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LEE, HU JONG (이후종)

Dept of Physics(물리학과)

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TRANSITION:9||VORTICES:8||STATE:7||intrinsic Josephson junctions:7||SINGLECRYSTALS:7||JUNCTIONS:5||MODES:5||SUPERCURRENT:5||SUPERCONDUCTOR:5||CONDUCTANCE:5||HIGHTEMPERATURE SUPERCONDUCTORS:5||TRANSPORT:5||PHASE:5||FILMS:4||LOCALIZATION:4||SINGLE DIRAC CONE:4||WIRES:4||MAGNETICFIELD:4||STEPS:3||ELECTRONS:3||proximity effect:3||MODEL:3||ARRAYS:3||INTERFERENCE:3||fluxon dynamics:3||HETEROSTRUCTURES:3||INSULATOR:3||Andreev reflection:3||electronic transport:3||FISKE:3||superconductor:2||ZnO:2||quantum point contact:2||METAL:2||DYNAMICS:2||interlayer Josephson coupling:2||SUPERCONDUCTORS:2||YBA2CU3O7DELTA:2||LAYER:2||DOTS:2||quantum dot:2||Article:2||TRANSISTORS:2||CARBON NANOTUBES:2||GAP:2||MECHANISM:2||LINE:2||GIANT SHAPIRO STEPS:2||LAYERS:2||electron energy loss spectroscopy:2||physical phenomena:2||scanning electron microscopy:2||HGTE QUANTUMWELLS:2||BI2TE3:2||SPECTROSCOPY:2||PNJUNCTIONS:2||spinpolarized tunneling:2||INTRINSIC JOSEPHSONJUNCTIONS:2||FIELDS:2||positive magnetoresistance:2||dilute magnetic semiconductor:2||magnetic field:2||scanning transmission electron microscopy:2||QUANTUM OSCILLATIONS:2||TRANSPORTPROPERTIES:2||surface pair current:2||MAGNETORESISTANCE:2||NANORIBBONS:2||INSTABILITY:2||ANDREEV REFLECTION:2||microwave irradiation:2||vertical graphene josephson junction:2||BI2SE3:2||CONDUCTIVITY:2||highTc superconductors:2||DIMENSIONAL ELECTRONGAS:2||graphene:2||Topological insulators:2||Josephson coupling Fraunhofer interference pattern:2||FERROMAGNET:2||DEPENDENCE:2||DETECTOR:2||COHERENCE:2||INJECTION:2||GRAPHENE:1||JOSEPHSONJUNCTIONS:1||LAYERED SUPERCONDUCTOR:1||mode splitting:1||BEHAVIOR:1||spinpolarized transport:1||SUPERCONDUCTING TRANSITION:1||microwave response:1||PSEUDOGAP:1||phase coherence:1||TRANSITIONS:1||Long Josephson junction:1||Charge detection:1||collective resonance modes:1||plasma oscillation modes:1||Superconducting proximity effect:1||Iron pnictide superconductor:1||McMillanRowell oscillations:1||ferromagnetic microstructure:1||superradiant state:1||VOLTAGE:1||branch splitting:1||TENSOR:1||INTERCALATION:1||insitu fabrication:1||NDGAO3:1||DISORDERED METALS:1||GAUGE GLASS:1||LOWTEMPERATURE TRANSPORT:1||spontaneous spin polarization model:1||BIAS:1||emission of electromagnetic waves:1||YBA2CU3O7/PRBA2CU3O7 SUPERLATTICES:1||BOHM:1||SHAPIRO STEPS:1||superconductor/ferromagnet interface:1||OXIDE:1||ANDREEVREFLECTION:1||SinFeAsO single crystal:1||COLLECTIVE MOTION:1||ANGULARDEPENDENCE:1||SUPERCONDUCTIVITY:1||BILAYER GRAPHENE:1||PHOTOLUMINESCENT PROPERTIES:1||SUPERCONDUCTING WEAK LINKS:1||intrinsic Josephson junctions geometrical resonance:1||intrinsic Josephson junction:1||MESOSCOPIC SPINVALVE:1||Bi2212 single crystals:1||intrinsic junctions:1||ANDREEV REFLECTIONS:1||normalmetal/superconductor interface:1||IBI2SR2CACU2OY:1||THERMAL FLUCTUATIONS:1||MIXED STATE:1||BI2.15SR1.85CACU2O8+DELTA:1||intrinsic Josephson effects:1||CACUO:1||QUANTUM POINT CONTACTS:1||resonant tunneling state:1||coherence length:1||NANOWIRE:1||GATES:1||Phase line:1||Thermal activation:1||QUANTUMDOT:1||superconducting proximity effect:1||Andreev interferometer:1||WIRE:1||Josephsonvortexflow branches:1||Bi2212 cuprates:1||LATTICE:1||demannetization effect:1||SUPERCONDUCTING MIRRORS:1||GAS:1||VALLEY TRANSPORT:1||ELECTRODES:1||DEPENDENT TRANSPORT:1||BORNOPPENHEIMER APPROXIMATION:1||collective plasma oscillations:1||fluxon resonance steps:1||STACKS:1||COLLECTIVE DYNAMICS:1||PAIRING SYMMETRY:1||MUON SPIN ROTATION:1||DIMENSIONAL CROSSOVER:1||Bi2Sr2CaCu2Oy highTc superconductors:1||heterojunctions:1||nanostructures:1||surfaces and interfaces:1||QUANTUM TRANSPORT:1||MICROJUNCTIONS:1||RESONATORS:1||STATES:1||FIELD:1||FLUCTUATIONS:1||SCATTERING:1||mode splitting of Josephson vortexflow branches:1||2D superconductivity:1||TRANSISTOR:1||ENERGYGAP:1||SUPERLATTICES:1||IRONBASED SUPERCONDUCTORS:1||PHASEDEPENDENT RESISTANCE:1||QUANTUM PHASETRANSITIONS:1||ELECTRICFIELD:1||HIGH MAGNETICFIELDS:1||NANOWIRE HETEROSTRUCTURES:1||ZNO:1||pair breaking.:1||SUPERCONDUCTING PB:1||domain formation:1||FORCE MICROSCOPY:1||RELAXATION:1||PLASMA RESONANCE:1||coupled Josephson junctions:1||COPPEROXIDE SUPERCONDUCTORS:1||CROSSOVER:1||SIMULATIONS:1||LOWTEMPERATURE:1||CONDUCTORS:1||METALINSULATORTRANSITION:1||SEMICONDUCTOR:1||FIELDEFFECT TRANSISTORS:1||ZEROVOLTAGE STATE:1||constanttemperature interlayer tunneling spectroscopy:1||Josephson supercurrent:1||BIPOLAR SUPERCURRENT:1||Interaction between Josephson and pancake vortices:1||flux jump:1||coaxial heterojunction nanorod:1||Natural Josephson coupling:1||BI2SR2CACU2O8+DELTA:1||VORTEX FLOW:1||TC SUPERCONDUCTORS:1||charge imbalance:1||Andreev diffractometer:1||intercalation:1||surface junction:1||Bi2212:1||tunnelling:1||GRAPHITE:1||GROWTH:1||collective transverse plasma modes:1||GAN:1||Macroscopic quantum tunneling:1||Fluctuation conductivity:1||Abovegap conductance jump:1||Josephson vortex motion:1||Intrinsic Josephson junctions:1||LAYERED SUPERCONDUCTORS:1||BI2SR2CACU2O8+Y:1||INTERFACES:1||BREAKDOWN:1||SYSTEMS:1||Anisotropy ratio:1||Josephson vortex:1||spin relaxation in superconductors:1||bibased single crystals:1||MESOSCOPIC PROXIMITY SUPERCONDUCTOR:1||reentrance of conductance:1||interlayer pair tunneling:1||JOSEPHSON:1||DISORDERED 2DIMENSIONAL SUPERCONDUCTORS:1||INDIUM FILMS:1||excited state:1||REGIME:1||triplet superconductivity:1||FILM:1||SCHOTTKY DIODES:1||peakdiphump structure:1||Kondo effect:1||REENTRANCE:1||Graphene:1||CONTACT:1||BERRYS PHASE:1||2DIMENSIONAL SUPERCONDUCTORS:1||Coulomb diamond:1||magnetic domain:1||spin injection:1||RESONANCE:1||plasma excitation modes:1||FLOW:1||OVERDOPED BI2SR2CACU2O8+DELTA:1||hole doping:1||chemical synthesis:1||phase transitions:1||superconductors:1||VORTEXGLASS SUPERCONDUCTIVITY:1||Kondorelated model:1||RADIATION:1||DOT:1||NANOBELTS:1||Complementarity:1||Closedloop AharonovBohm interferometer:1||pair breaking:1||interlayer phase fluctuation:1||MgB2 thin film:1||CONFINEMENT:1||WALLED CARBON NANOTUBES:1||TRANSITION:9||VORTICES:8||STATE:7||intrinsic Josephson junctions:7||SINGLECRYSTALS:7||JUNCTIONS:5||MODES:5||SUPERCURRENT:5||SUPERCONDUCTOR:5||CONDUCTANCE:5||HIGHTEMPERATURE SUPERCONDUCTORS:5||TRANSPORT:5||PHASE:5||FILMS:4||LOCALIZATION:4||SINGLE DIRAC CONE:4||WIRES:4||MAGNETICFIELD:4||STEPS:3||ELECTRONS:3||proximity effect:3||MODEL:3||ARRAYS:3||INTERFERENCE:3||fluxon dynamics:3||HETEROSTRUCTURES:3||INSULATOR:3||Andreev reflection:3||electronic transport:3||FISKE:3||superconductor:2||ZnO:2||quantum point contact:2||METAL:2||DYNAMICS:2||interlayer Josephson coupling:2||SUPERCONDUCTORS:2||YBA2CU3O7DELTA:2||LAYER:2||DOTS:2||quantum dot:2||Article:2||TRANSISTORS:2||CARBON NANOTUBES:2||GAP:2||MECHANISM:2||LINE:2||GIANT SHAPIRO STEPS:2||LAYERS:2||electron energy loss spectroscopy:2||physical phenomena:2||scanning electron microscopy:2||HGTE QUANTUMWELLS:2||BI2TE3:2||SPECTROSCOPY:2||PNJUNCTIONS:2||spinpolarized tunneling:2||INTRINSIC JOSEPHSONJUNCTIONS:2||FIELDS:2||positive magnetoresistance:2||dilute magnetic semiconductor:2||magnetic field:2||scanning transmission electron microscopy:2||QUANTUM OSCILLATIONS:2||TRANSPORTPROPERTIES:2||surface pair current:2||MAGNETORESISTANCE:2||NANORIBBONS:2||INSTABILITY:2||ANDREEV REFLECTION:2||microwave irradiation:2||vertical graphene josephson junction:2||BI2SE3:2||CONDUCTIVITY:2||highTc superconductors:2||DIMENSIONAL ELECTRONGAS:2||graphene:2||Topological insulators:2||Josephson coupling Fraunhofer interference pattern:2||FERROMAGNET:2||DEPENDENCE:2||DETECTOR:2||COHERENCE:2||INJECTION:2||GRAPHENE:1||JOSEPHSONJUNCTIONS:1||LAYERED SUPERCONDUCTOR:1||mode splitting:1||BEHAVIOR:1||spinpolarized transport:1||SUPERCONDUCTING TRANSITION:1||microwave response:1||PSEUDOGAP:1||phase coherence:1||TRANSITIONS:1||Long Josephson junction:1||Charge detection:1||collective resonance modes:1||plasma oscillation modes:1||Superconducting proximity effect:1||Iron pnictide superconductor:1||McMillanRowell oscillations:1||ferromagnetic microstructure:1||superradiant state:1||VOLTAGE:1||branch splitting:1||TENSOR:1||INTERCALATION:1||insitu fabrication:1||NDGAO3:1||DISORDERED METALS:1||GAUGE GLASS:1||LOWTEMPERATURE TRANSPORT:1||spontaneous spin polarization model:1||BIAS:1||emission of electromagnetic waves:1||YBA2CU3O7/PRBA2CU3O7 SUPERLATTICES:1||BOHM:1||SHAPIRO STEPS:1||superconductor/ferromagnet interface:1||OXIDE:1||ANDREEVREFLECTION:1||SinFeAsO single crystal:1||COLLECTIVE MOTION:1||ANGULARDEPENDENCE:1||SUPERCONDUCTIVITY:1||BILAYER GRAPHENE:1||PHOTOLUMINESCENT PROPERTIES:1||SUPERCONDUCTING WEAK LINKS:1||intrinsic Josephson junctions geometrical resonance:1||intrinsic Josephson junction:1||MESOSCOPIC SPINVALVE:1||Bi2212 single crystals:1||intrinsic junctions:1||ANDREEV REFLECTIONS:1||normalmetal/superconductor interface:1||IBI2SR2CACU2OY:1||THERMAL FLUCTUATIONS:1||MIXED STATE:1||BI2.15SR1.85CACU2O8+DELTA:1||intrinsic Josephson effects:1||CACUO:1||QUANTUM POINT CONTACTS:1||resonant tunneling state:1||coherence length:1||NANOWIRE:1||GATES:1||Phase line:1||Thermal activation:1||QUANTUMDOT:1||superconducting proximity effect:1||Andreev interferometer:1||WIRE:1||Josephsonvortexflow branches:1||Bi2212 cuprates:1||LATTICE:1||demannetization effect:1||SUPERCONDUCTING MIRRORS:1||GAS:1||VALLEY TRANSPORT:1||ELECTRODES:1||DEPENDENT TRANSPORT:1||BORNOPPENHEIMER APPROXIMATION:1||collective plasma oscillations:1||fluxon resonance steps:1||STACKS:1||COLLECTIVE DYNAMICS:1||PAIRING SYMMETRY:1||MUON SPIN ROTATION:1||DIMENSIONAL CROSSOVER:1||Bi2Sr2CaCu2Oy highTc superconductors:1||heterojunctions:1||nanostructures:1||surfaces and interfaces:1||QUANTUM TRANSPORT:1||MICROJUNCTIONS:1||RESONATORS:1||STATES:1||FIELD:1||FLUCTUATIONS:1||SCATTERING:1||mode splitting of Josephson vortexflow branches:1||2D superconductivity:1||TRANSISTOR:1||ENERGYGAP:1||SUPERLATTICES:1||IRONBASED SUPERCONDUCTORS:1||PHASEDEPENDENT RESISTANCE:1||QUANTUM PHASETRANSITIONS:1||ELECTRICFIELD:1||HIGH MAGNETICFIELDS:1||NANOWIRE HETEROSTRUCTURES:1||ZNO:1||pair breaking.:1||SUPERCONDUCTING PB:1||domain formation:1||FORCE MICROSCOPY:1||RELAXATION:1||PLASMA RESONANCE:1||coupled Josephson junctions:1||COPPEROXIDE SUPERCONDUCTORS:1||CROSSOVER:1||SIMULATIONS:1||LOWTEMPERATURE:1||CONDUCTORS:1||METALINSULATORTRANSITION:1||SEMICONDUCTOR:1||FIELDEFFECT TRANSISTORS:1||ZEROVOLTAGE STATE:1||constanttemperature interlayer tunneling spectroscopy:1||Josephson supercurrent:1||BIPOLAR SUPERCURRENT:1||Interaction between Josephson and pancake vortices:1||flux jump:1||coaxial heterojunction nanorod:1||Natural Josephson coupling:1||BI2SR2CACU2O8+DELTA:1||VORTEX FLOW:1||TC SUPERCONDUCTORS:1||charge imbalance:1||Andreev diffractometer:1||intercalation:1||surface junction:1||Bi2212:1||tunnelling:1||GRAPHITE:1||GROWTH:1||collective transverse plasma modes:1||GAN:1||Macroscopic quantum tunneling:1||Fluctuation conductivity:1||Abovegap conductance jump:1||Josephson vortex motion:1||Intrinsic Josephson junctions:1||LAYERED SUPERCONDUCTORS:1||BI2SR2CACU2O8+Y:1||INTERFACES:1||BREAKDOWN:1||SYSTEMS:1||Anisotropy ratio:1||Josephson vortex:1||spin relaxation in superconductors:1||bibased single crystals:1||MESOSCOPIC PROXIMITY SUPERCONDUCTOR:1||reentrance of conductance:1||interlayer pair tunneling:1||JOSEPHSON:1||DISORDERED 2DIMENSIONAL SUPERCONDUCTORS:1||INDIUM FILMS:1||excited state:1||REGIME:1||triplet superconductivity:1||FILM:1||SCHOTTKY DIODES:1||peakdiphump structure:1||Kondo effect:1||REENTRANCE:1||Graphene:1||CONTACT:1||BERRYS PHASE:1||2DIMENSIONAL SUPERCONDUCTORS:1||Coulomb diamond:1||magnetic domain:1||spin injection:1||RESONANCE:1||plasma excitation modes:1||FLOW:1||OVERDOPED BI2SR2CACU2O8+DELTA:1||hole doping:1||chemical synthesis:1||phase transitions:1||superconductors:1||VORTEXGLASS SUPERCONDUCTIVITY:1||Kondorelated model:1||RADIATION:1||DOT:1||NANOBELTS:1||Complementarity:1||Closedloop AharonovBohm interferometer:1||pair breaking:1||interlayer phase fluctuation:1||MgB2 thin film:1||CONFINEMENT:1||WALLED CARBON NANOTUBES:1||TRANSITION:9||VORTICES:8||STATE:7||intrinsic Josephson junctions:7||SINGLECRYSTALS:7||JUNCTIONS:5||MODES:5||SUPERCURRENT:5||SUPERCONDUCTOR:5||CONDUCTANCE:5||HIGHTEMPERATURE SUPERCONDUCTORS:5||TRANSPORT:5||PHASE:5||FILMS:4||LOCALIZATION:4||SINGLE DIRAC CONE:4||WIRES:4||MAGNETICFIELD:4||STEPS:3||ELECTRONS:3||proximity effect:3||MODEL:3||ARRAYS:3||INTERFERENCE:3||fluxon dynamics:3||HETEROSTRUCTURES:3||INSULATOR:3||Andreev reflection:3||electronic transport:3||FISKE:3||superconductor:2||ZnO:2||quantum point contact:2||METAL:2||DYNAMICS:2||interlayer Josephson coupling:2||SUPERCONDUCTORS:2||YBA2CU3O7DELTA:2||LAYER:2||DOTS:2||quantum dot:2||Article:2||TRANSISTORS:2||CARBON NANOTUBES:2||GAP:2||MECHANISM:2||LINE:2||GIANT SHAPIRO STEPS:2||LAYERS:2||electron energy loss spectroscopy:2||physical phenomena:2||scanning electron microscopy:2||HGTE QUANTUMWELLS:2||BI2TE3:2||SPECTROSCOPY:2||PNJUNCTIONS:2||spinpolarized tunneling:2||INTRINSIC JOSEPHSONJUNCTIONS:2||FIELDS:2||positive magnetoresistance:2||dilute magnetic semiconductor:2||magnetic field:2||scanning transmission electron microscopy:2||QUANTUM OSCILLATIONS:2||TRANSPORTPROPERTIES:2||surface pair current:2||MAGNETORESISTANCE:2||NANORIBBONS:2||INSTABILITY:2||ANDREEV REFLECTION:2||microwave irradiation:2||vertical graphene josephson junction:2||BI2SE3:2||CONDUCTIVITY:2||highTc superconductors:2||DIMENSIONAL ELECTRONGAS:2||graphene:2||Topological insulators:2||Josephson coupling Fraunhofer interference pattern:2||FERROMAGNET:2||DEPENDENCE:2||DETECTOR:2||COHERENCE:2||INJECTION:2||GRAPHENE:1||JOSEPHSONJUNCTIONS:1||LAYERED SUPERCONDUCTOR:1||mode splitting:1||BEHAVIOR:1||spinpolarized transport:1||SUPERCONDUCTING TRANSITION:1||microwave response:1||PSEUDOGAP:1||phase coherence:1||TRANSITIONS:1||Long Josephson junction:1||Charge detection:1||collective resonance modes:1||plasma oscillation modes:1||Superconducting proximity effect:1||Iron pnictide superconductor:1||McMillanRowell oscillations:1||ferromagnetic microstructure:1||superradiant state:1||VOLTAGE:1||branch splitting:1||TENSOR:1||INTERCALATION:1||insitu fabrication:1||NDGAO3:1||DISORDERED METALS:1||GAUGE GLASS:1||LOWTEMPERATURE TRANSPORT:1||spontaneous spin polarization model:1||BIAS:1||emission of electromagnetic waves:1||YBA2CU3O7/PRBA2CU3O7 SUPERLATTICES:1||BOHM:1||SHAPIRO STEPS:1||superconductor/ferromagnet interface:1||OXIDE:1||ANDREEVREFLECTION:1||SinFeAsO single crystal:1||COLLECTIVE MOTION:1||ANGULARDEPENDENCE:1||SUPERCONDUCTIVITY:1||BILAYER GRAPHENE:1||PHOTOLUMINESCENT PROPERTIES:1||SUPERCONDUCTING WEAK LINKS:1||intrinsic Josephson junctions geometrical resonance:1||intrinsic Josephson junction:1||MESOSCOPIC SPINVALVE:1||Bi2212 single crystals:1||intrinsic junctions:1||ANDREEV REFLECTIONS:1||normalmetal/superconductor interface:1||IBI2SR2CACU2OY:1||THERMAL FLUCTUATIONS:1||MIXED STATE:1||BI2.15SR1.85CACU2O8+DELTA:1||intrinsic Josephson effects:1||CACUO:1||QUANTUM POINT CONTACTS:1||resonant tunneling state:1||coherence length:1||NANOWIRE:1||GATES:1||Phase line:1||Thermal activation:1||QUANTUMDOT:1||superconducting proximity effect:1||Andreev interferometer:1||WIRE:1||Josephsonvortexflow branches:1||Bi2212 cuprates:1||LATTICE:1||demannetization effect:1||SUPERCONDUCTING MIRRORS:1||GAS:1||VALLEY TRANSPORT:1||ELECTRODES:1||DEPENDENT TRANSPORT:1||BORNOPPENHEIMER APPROXIMATION:1||collective plasma oscillations:1||fluxon resonance steps:1||STACKS:1||COLLECTIVE DYNAMICS:1||PAIRING SYMMETRY:1||MUON SPIN ROTATION:1||DIMENSIONAL CROSSOVER:1||Bi2Sr2CaCu2Oy highTc superconductors:1||heterojunctions:1||nanostructures:1||surfaces and interfaces:1||QUANTUM TRANSPORT:1||MICROJUNCTIONS:1||RESONATORS:1||STATES:1||FIELD:1||FLUCTUATIONS:1||SCATTERING:1||mode splitting of Josephson vortexflow branches:1||2D superconductivity:1||TRANSISTOR:1||ENERGYGAP:1||SUPERLATTICES:1||IRONBASED SUPERCONDUCTORS:1||PHASEDEPENDENT RESISTANCE:1||QUANTUM PHASETRANSITIONS:1||ELECTRICFIELD:1||HIGH MAGNETICFIELDS:1||NANOWIRE HETEROSTRUCTURES:1||ZNO:1||pair breaking.:1||SUPERCONDUCTING PB:1||domain formation:1||FORCE MICROSCOPY:1||RELAXATION:1||PLASMA RESONANCE:1||coupled Josephson junctions:1||COPPEROXIDE SUPERCONDUCTORS:1||CROSSOVER:1||SIMULATIONS:1||LOWTEMPERATURE:1||CONDUCTORS:1||METALINSULATORTRANSITION:1||SEMICONDUCTOR:1||FIELDEFFECT TRANSISTORS:1||ZEROVOLTAGE STATE:1||constanttemperature interlayer tunneling spectroscopy:1||Josephson supercurrent:1||BIPOLAR SUPERCURRENT:1||Interaction between Josephson and pancake vortices:1||flux jump:1||coaxial heterojunction nanorod:1||Natural Josephson coupling:1||BI2SR2CACU2O8+DELTA:1||VORTEX FLOW:1||TC SUPERCONDUCTORS:1||charge imbalance:1||Andreev diffractometer:1||intercalation:1||surface junction:1||Bi2212:1||tunnelling:1||GRAPHITE:1||GROWTH:1||collective transverse plasma modes:1||GAN:1||Macroscopic quantum tunneling:1||Fluctuation conductivity:1||Abovegap conductance jump:1||Josephson vortex motion:1||Intrinsic Josephson junctions:1||LAYERED SUPERCONDUCTORS:1||BI2SR2CACU2O8+Y:1||INTERFACES:1||BREAKDOWN:1||SYSTEMS:1||Anisotropy ratio:1||Josephson vortex:1||spin relaxation in superconductors:1||bibased single crystals:1||MESOSCOPIC PROXIMITY SUPERCONDUCTOR:1||reentrance of conductance:1||interlayer pair tunneling:1||JOSEPHSON:1||DISORDERED 2DIMENSIONAL SUPERCONDUCTORS:1||INDIUM FILMS:1||excited state:1||REGIME:1||triplet superconductivity:1||FILM:1||SCHOTTKY DIODES:1||peakdiphump structure:1||Kondo effect:1||REENTRANCE:1||Graphene:1||CONTACT:1||BERRYS PHASE:1||2DIMENSIONAL SUPERCONDUCTORS:1||Coulomb diamond:1||magnetic domain:1||spin injection:1||RESONANCE:1||plasma excitation modes:1||FLOW:1||OVERDOPED BI2SR2CACU2O8+DELTA:1||hole doping:1||chemical synthesis:1||phase transitions:1||superconductors:1||VORTEXGLASS SUPERCONDUCTIVITY:1||Kondorelated model:1||RADIATION:1||DOT:1||NANOBELTS:1||Complementarity:1||Closedloop AharonovBohm interferometer:1||pair breaking:1||interlayer phase fluctuation:1||MgB2 thin film:1||CONFINEMENT:1||WALLED CARBON NANOTUBES:1||TRANSITION:9||VORTICES:8||STATE:7||intrinsic Josephson junctions:7||SINGLECRYSTALS:7||JUNCTIONS:5||MODES:5||SUPERCURRENT:5||SUPERCONDUCTOR:5||CONDUCTANCE:5||HIGHTEMPERATURE SUPERCONDUCTORS:5||TRANSPORT:5||PHASE:5||FILMS:4||LOCALIZATION:4||SINGLE DIRAC CONE:4||WIRES:4||MAGNETICFIELD:4||STEPS:3||ELECTRONS:3||proximity effect:3||MODEL:3||ARRAYS:3||INTERFERENCE:3||fluxon dynamics:3||HETEROSTRUCTURES:3||INSULATOR:3||Andreev reflection:3||electronic transport:3||FISKE:3||superconductor:2||ZnO:2||quantum point contact:2||METAL:2||DYNAMICS:2||interlayer Josephson coupling:2||SUPERCONDUCTORS:2||YBA2CU3O7DELTA:2||LAYER:2||DOTS:2||quantum dot:2||Article:2||TRANSISTORS:2||CARBON NANOTUBES:2||GAP:2||MECHANISM:2||LINE:2||GIANT SHAPIRO STEPS:2||LAYERS:2||electron energy loss spectroscopy:2||physical phenomena:2||scanning electron microscopy:2||HGTE QUANTUMWELLS:2||BI2TE3:2||SPECTROSCOPY:2||PNJUNCTIONS:2||spinpolarized tunneling:2||INTRINSIC JOSEPHSONJUNCTIONS:2||FIELDS:2||positive magnetoresistance:2||dilute magnetic semiconductor:2||magnetic field:2||scanning transmission electron microscopy:2||QUANTUM OSCILLATIONS:2||TRANSPORTPROPERTIES:2||surface pair current:2||MAGNETORESISTANCE:2||NANORIBBONS:2||INSTABILITY:2||ANDREEV REFLECTION:2||microwave irradiation:2||vertical graphene josephson junction:2||BI2SE3:2||CONDUCTIVITY:2||highTc superconductors:2||DIMENSIONAL ELECTRONGAS:2||graphene:2||Topological insulators:2||Josephson coupling Fraunhofer interference pattern:2||FERROMAGNET:2||DEPENDENCE:2||DETECTOR:2||COHERENCE:2||INJECTION:2||GRAPHENE:1||JOSEPHSONJUNCTIONS:1||LAYERED SUPERCONDUCTOR:1||mode splitting:1||BEHAVIOR:1||spinpolarized transport:1||SUPERCONDUCTING TRANSITION:1||microwave response:1||PSEUDOGAP:1||phase coherence:1||TRANSITIONS:1||Long Josephson junction:1||Charge detection:1||collective resonance modes:1||plasma oscillation modes:1||Superconducting proximity effect:1||Iron pnictide superconductor:1||McMillanRowell oscillations:1||ferromagnetic microstructure:1||superradiant state:1||VOLTAGE:1||branch splitting:1||TENSOR:1||INTERCALATION:1||insitu fabrication:1||NDGAO3:1||DISORDERED METALS:1||GAUGE GLASS:1||LOWTEMPERATURE TRANSPORT:1||spontaneous spin polarization model:1||BIAS:1||emission of electromagnetic waves:1||YBA2CU3O7/PRBA2CU3O7 SUPERLATTICES:1||BOHM:1||SHAPIRO STEPS:1||superconductor/ferromagnet interface:1||OXIDE:1||ANDREEVREFLECTION:1||SinFeAsO single crystal:1||COLLECTIVE MOTION:1||ANGULARDEPENDENCE:1||SUPERCONDUCTIVITY:1||BILAYER GRAPHENE:1||PHOTOLUMINESCENT PROPERTIES:1||SUPERCONDUCTING WEAK LINKS:1||intrinsic Josephson junctions geometrical resonance:1||intrinsic Josephson junction:1||MESOSCOPIC SPINVALVE:1||Bi2212 single crystals:1||intrinsic junctions:1||ANDREEV REFLECTIONS:1||normalmetal/superconductor interface:1||IBI2SR2CACU2OY:1||THERMAL FLUCTUATIONS:1||MIXED STATE:1||BI2.15SR1.85CACU2O8+DELTA:1||intrinsic Josephson effects:1||CACUO:1||QUANTUM POINT CONTACTS:1||resonant tunneling state:1||coherence length:1||NANOWIRE:1||GATES:1||Phase line:1||Thermal activation:1||QUANTUMDOT:1||superconducting proximity effect:1||Andreev interferometer:1||WIRE:1||Josephsonvortexflow branches:1||Bi2212 cuprates:1||LATTICE:1||demannetization effect:1||SUPERCONDUCTING MIRRORS:1||GAS:1||VALLEY TRANSPORT:1||ELECTRODES:1||DEPENDENT TRANSPORT:1||BORNOPPENHEIMER APPROXIMATION:1||collective plasma oscillations:1||fluxon resonance steps:1||STACKS:1||COLLECTIVE DYNAMICS:1||PAIRING SYMMETRY:1||MUON SPIN ROTATION:1||DIMENSIONAL CROSSOVER:1||Bi2Sr2CaCu2Oy highTc superconductors:1||heterojunctions:1||nanostructures:1||surfaces and interfaces:1||QUANTUM TRANSPORT:1||MICROJUNCTIONS:1||RESONATORS:1||STATES:1||FIELD:1||FLUCTUATIONS:1||SCATTERING:1||mode splitting of Josephson vortexflow branches:1||2D superconductivity:1||TRANSISTOR:1||ENERGYGAP:1||SUPERLATTICES:1||IRONBASED SUPERCONDUCTORS:1||PHASEDEPENDENT RESISTANCE:1||QUANTUM PHASETRANSITIONS:1||ELECTRICFIELD:1||HIGH MAGNETICFIELDS:1||NANOWIRE HETEROSTRUCTURES:1||ZNO:1||pair breaking.:1||SUPERCONDUCTING PB:1||domain formation:1||FORCE MICROSCOPY:1||RELAXATION:1||PLASMA RESONANCE:1||coupled Josephson junctions:1||COPPEROXIDE SUPERCONDUCTORS:1||CROSSOVER:1||SIMULATIONS:1||LOWTEMPERATURE:1||CONDUCTORS:1||METALINSULATORTRANSITION:1||SEMICONDUCTOR:1||FIELDEFFECT TRANSISTORS:1||ZEROVOLTAGE STATE:1||constanttemperature interlayer tunneling spectroscopy:1||Josephson supercurrent:1||BIPOLAR SUPERCURRENT:1||Interaction between Josephson and pancake vortices:1||flux jump:1||coaxial heterojunction nanorod:1||Natural Josephson coupling:1||BI2SR2CACU2O8+DELTA:1||VORTEX FLOW:1||TC SUPERCONDUCTORS:1||charge imbalance:1||Andreev diffractometer:1||intercalation:1||surface junction:1||Bi2212:1||tunnelling:1||GRAPHITE:1||GROWTH:1||collective transverse plasma modes:1||GAN:1||Macroscopic quantum tunneling:1||Fluctuation conductivity:1||Abovegap conductance jump:1||Josephson vortex motion:1||Intrinsic Josephson junctions:1||LAYERED SUPERCONDUCTORS:1||BI2SR2CACU2O8+Y:1||INTERFACES:1||BREAKDOWN:1||SYSTEMS:1||Anisotropy ratio:1||Josephson vortex:1||spin relaxation in superconductors:1||bibased single crystals:1||MESOSCOPIC PROXIMITY SUPERCONDUCTOR:1||reentrance of conductance:1||interlayer pair tunneling:1||JOSEPHSON:1||DISORDERED 2DIMENSIONAL SUPERCONDUCTORS:1||INDIUM FILMS:1||excited state:1||REGIME:1||triplet superconductivity:1||FILM:1||SCHOTTKY DIODES:1||peakdiphump structure:1||Kondo effect:1||REENTRANCE:1||Graphene:1||CONTACT:1||BERRYS PHASE:1||2DIMENSIONAL SUPERCONDUCTORS:1||Coulomb diamond:1||magnetic domain:1||spin injection:1||RESONANCE:1||plasma excitation modes:1||FLOW:1||OVERDOPED BI2SR2CACU2O8+DELTA:1||hole doping:1||chemical synthesis:1||phase transitions:1||superconductors:1||VORTEXGLASS SUPERCONDUCTIVITY:1||Kondorelated model:1||RADIATION:1||DOT:1||NANOBELTS:1||Complementarity:1||Closedloop AharonovBohm interferometer:1||pair breaking:1||interlayer phase fluctuation:1||MgB2 thin film:1||CONFINEMENT:1||WALLED CARBON NANOTUBES:1||TRANSITION:9||VORTICES:8||STATE:7||intrinsic Josephson junctions:7||SINGLECRYSTALS:7||JUNCTIONS:5||MODES:5||SUPERCURRENT:5||SUPERCONDUCTOR:5||CONDUCTANCE:5||HIGHTEMPERATURE SUPERCONDUCTORS:5||TRANSPORT:5||PHASE:5||FILMS:4||LOCALIZATION:4||SINGLE DIRAC CONE:4||WIRES:4||MAGNETICFIELD:4||STEPS:3||ELECTRONS:3||proximity effect:3||MODEL:3||ARRAYS:3||INTERFERENCE:3||fluxon dynamics:3||HETEROSTRUCTURES:3||INSULATOR:3||Andreev reflection:3||electronic transport:3||FISKE:3||superconductor:2||ZnO:2||quantum point contact:2||METAL:2||DYNAMICS:2||interlayer Josephson coupling:2||SUPERCONDUCTORS:2||YBA2CU3O7DELTA:2||LAYER:2||DOTS:2||quantum dot:2||Article:2||TRANSISTORS:2||CARBON NANOTUBES:2||GAP:2||MECHANISM:2||LINE:2||GIANT SHAPIRO STEPS:2||LAYERS:2||electron energy loss spectroscopy:2||physical phenomena:2||scanning electron microscopy:2||HGTE QUANTUMWELLS:2||BI2TE3:2||SPECTROSCOPY:2||PNJUNCTIONS:2||spinpolarized tunneling:2||INTRINSIC JOSEPHSONJUNCTIONS:2||FIELDS:2||positive magnetoresistance:2||dilute magnetic semiconductor:2||magnetic field:2||scanning transmission electron microscopy:2||QUANTUM OSCILLATIONS:2||TRANSPORTPROPERTIES:2||surface pair current:2||MAGNETORESISTANCE:2||NANORIBBONS:2||INSTABILITY:2||ANDREEV REFLECTION:2||microwave irradiation:2||vertical graphene josephson junction:2||BI2SE3:2||CONDUCTIVITY:2||highTc superconductors:2||DIMENSIONAL ELECTRONGAS:2||graphene:2||Topological insulators:2||Josephson coupling Fraunhofer interference pattern:2||FERROMAGNET:2||DEPENDENCE:2||DETECTOR:2||COHERENCE:2||INJECTION:2||GRAPHENE:1||JOSEPHSONJUNCTIONS:1||LAYERED SUPERCONDUCTOR:1||mode splitting:1||BEHAVIOR:1||spinpolarized transport:1||SUPERCONDUCTING TRANSITION:1||microwave response:1||PSEUDOGAP:1||phase coherence:1||TRANSITIONS:1||Long Josephson junction:1||Charge detection:1||collective resonance modes:1||plasma oscillation modes:1||Superconducting proximity effect:1||Iron pnictide superconductor:1||McMillanRowell oscillations:1||ferromagnetic microstructure:1||superradiant state:1||VOLTAGE:1||branch splitting:1||TENSOR:1||INTERCALATION:1||insitu fabrication:1||NDGAO3:1||DISORDERED METALS:1||GAUGE GLASS:1||LOWTEMPERATURE TRANSPORT:1||spontaneous spin polarization model:1||BIAS:1||emission of electromagnetic waves:1||YBA2CU3O7/PRBA2CU3O7 SUPERLATTICES:1||BOHM:1||SHAPIRO STEPS:1||superconductor/ferromagnet interface:1||OXIDE:1||ANDREEVREFLECTION:1||SinFeAsO single crystal:1||COLLECTIVE MOTION:1||ANGULARDEPENDENCE:1||SUPERCONDUCTIVITY:1||BILAYER GRAPHENE:1||PHOTOLUMINESCENT PROPERTIES:1||SUPERCONDUCTING WEAK LINKS:1||intrinsic Josephson junctions geometrical resonance:1||intrinsic Josephson junction:1||MESOSCOPIC SPINVALVE:1||Bi2212 single crystals:1||intrinsic junctions:1||ANDREEV REFLECTIONS:1||normalmetal/superconductor interface:1||IBI2SR2CACU2OY:1||THERMAL FLUCTUATIONS:1||MIXED STATE:1||BI2.15SR1.85CACU2O8+DELTA:1||intrinsic Josephson effects:1||CACUO:1||QUANTUM POINT CONTACTS:1||resonant tunneling state:1||coherence length:1||NANOWIRE:1||GATES:1||Phase line:1||Thermal activation:1||QUANTUMDOT:1||superconducting proximity effect:1||Andreev interferometer:1||WIRE:1||Josephsonvortexflow branches:1||Bi2212 cuprates:1||LATTICE:1||demannetization effect:1||SUPERCONDUCTING MIRRORS:1||GAS:1||VALLEY TRANSPORT:1||ELECTRODES:1||DEPENDENT TRANSPORT:1||BORNOPPENHEIMER APPROXIMATION:1||collective plasma oscillations:1||fluxon resonance steps:1||STACKS:1||COLLECTIVE DYNAMICS:1||PAIRING SYMMETRY:1||MUON SPIN ROTATION:1||DIMENSIONAL CROSSOVER:1||Bi2Sr2CaCu2Oy highTc superconductors:1||heterojunctions:1||nanostructures:1||surfaces and interfaces:1||QUANTUM TRANSPORT:1||MICROJUNCTIONS:1||RESONATORS:1||STATES:1||FIELD:1||FLUCTUATIONS:1||SCATTERING:1||mode splitting of Josephson vortexflow branches:1||2D superconductivity:1||TRANSISTOR:1||ENERGYGAP:1||SUPERLATTICES:1||IRONBASED SUPERCONDUCTORS:1||PHASEDEPENDENT RESISTANCE:1||QUANTUM PHASETRANSITIONS:1||ELECTRICFIELD:1||HIGH MAGNETICFIELDS:1||NANOWIRE HETEROSTRUCTURES:1||ZNO:1||pair breaking.:1||SUPERCONDUCTING PB:1||domain formation:1||FORCE MICROSCOPY:1||RELAXATION:1||PLASMA RESONANCE:1||coupled Josephson junctions:1||COPPEROXIDE SUPERCONDUCTORS:1||CROSSOVER:1||SIMULATIONS:1||LOWTEMPERATURE:1||CONDUCTORS:1||METALINSULATORTRANSITION:1||SEMICONDUCTOR:1||FIELDEFFECT TRANSISTORS:1||ZEROVOLTAGE STATE:1||constanttemperature interlayer tunneling spectroscopy:1||Josephson supercurrent:1||BIPOLAR SUPERCURRENT:1||Interaction between Josephson and pancake vortices:1||flux jump:1||coaxial heterojunction nanorod:1||Natural Josephson coupling:1||BI2SR2CACU2O8+DELTA:1||VORTEX FLOW:1||TC SUPERCONDUCTORS:1||charge imbalance:1||Andreev diffractometer:1||intercalation:1||surface junction:1||Bi2212:1||tunnelling:1||GRAPHITE:1||GROWTH:1||collective transverse plasma modes:1||GAN:1||Macroscopic quantum tunneling:1||Fluctuation conductivity:1||Abovegap conductance jump:1||Josephson vortex motion:1||Intrinsic Josephson junctions:1||LAYERED SUPERCONDUCTORS:1||BI2SR2CACU2O8+Y:1||INTERFACES:1||BREAKDOWN:1||SYSTEMS:1||Anisotropy ratio:1||Josephson vortex:1||spin relaxation in superconductors:1||bibased single crystals:1||MESOSCOPIC PROXIMITY SUPERCONDUCTOR:1||reentrance of conductance:1||interlayer pair tunneling:1||JOSEPHSON:1||DISORDERED 2DIMENSIONAL SUPERCONDUCTORS:1||INDIUM FILMS:1||excited state:1||REGIME:1||triplet superconductivity:1||FILM:1||SCHOTTKY DIODES:1||peakdiphump structure:1||Kondo effect:1||REENTRANCE:1||Graphene:1||CONTACT:1||BERRYS PHASE:1||2DIMENSIONAL SUPERCONDUCTORS:1||Coulomb diamond:1||magnetic domain:1||spin injection:1||RESONANCE:1||plasma excitation modes:1||FLOW:1||OVERDOPED BI2SR2CACU2O8+DELTA:1||hole doping:1||chemical synthesis:1||phase transitions:1||superconductors:1||VORTEXGLASS SUPERCONDUCTIVITY:1||Kondorelated model:1||RADIATION:1||DOT:1||NANOBELTS:1||Complementarity:1||Closedloop AharonovBohm interferometer:1||pair breaking:1||interlayer phase fluctuation:1||MgB2 thin film:1||CONFINEMENT:1||WALLED CARBON NANOTUBES:1||TRANSITION:9||VORTICES:8||STATE:7||intrinsic Josephson junctions:7||SINGLECRYSTALS:7||JUNCTIONS:5||MODES:5||SUPERCURRENT:5||SUPERCONDUCTOR:5||CONDUCTANCE:5||HIGHTEMPERATURE SUPERCONDUCTORS:5||TRANSPORT:5||PHASE:5||FILMS:4||LOCALIZATION:4||SINGLE DIRAC CONE:4||WIRES:4||MAGNETICFIELD:4||STEPS:3||ELECTRONS:3||proximity effect:3||MODEL:3||ARRAYS:3||INTERFERENCE:3||fluxon dynamics:3||HETEROSTRUCTURES:3||INSULATOR:3||Andreev reflection:3||electronic transport:3||FISKE:3||superconductor:2||ZnO:2||quantum point contact:2||METAL:2||DYNAMICS:2||interlayer Josephson coupling:2||SUPERCONDUCTORS:2||YBA2CU3O7DELTA:2||LAYER:2||DOTS:2||quantum dot:2||Article:2||TRANSISTORS:2||CARBON NANOTUBES:2||GAP:2||MECHANISM:2||LINE:2||GIANT SHAPIRO STEPS:2||LAYERS:2||electron energy loss spectroscopy:2||physical phenomena:2||scanning electron microscopy:2||HGTE QUANTUMWELLS:2||BI2TE3:2||SPECTROSCOPY:2||PNJUNCTIONS:2||spinpolarized tunneling:2||INTRINSIC JOSEPHSONJUNCTIONS:2||FIELDS:2||positive magnetoresistance:2||dilute magnetic semiconductor:2||magnetic field:2||scanning transmission electron microscopy:2||QUANTUM OSCILLATIONS:2||TRANSPORTPROPERTIES:2||surface pair current:2||MAGNETORESISTANCE:2||NANORIBBONS:2||INSTABILITY:2||ANDREEV REFLECTION:2||microwave irradiation:2||vertical graphene josephson junction:2||BI2SE3:2||CONDUCTIVITY:2||highTc superconductors:2||DIMENSIONAL ELECTRONGAS:2||graphene:2||Topological insulators:2||Josephson coupling Fraunhofer interference pattern:2||FERROMAGNET:2||DEPENDENCE:2||DETECTOR:2||COHERENCE:2||INJECTION:2||GRAPHENE:1||JOSEPHSONJUNCTIONS:1||LAYERED SUPERCONDUCTOR:1||mode splitting:1||BEHAVIOR:1||spinpolarized transport:1||SUPERCONDUCTING TRANSITION:1||microwave response:1||PSEUDOGAP:1||phase coherence:1||TRANSITIONS:1||Long Josephson junction:1||Charge detection:1||collective resonance modes:1||plasma oscillation modes:1||Superconducting proximity effect:1||Iron pnictide superconductor:1||McMillanRowell oscillations:1||ferromagnetic microstructure:1||superradiant state:1||VOLTAGE:1||branch splitting:1||TENSOR:1||INTERCALATION:1||insitu fabrication:1||NDGAO3:1||DISORDERED METALS:1||GAUGE GLASS:1||LOWTEMPERATURE TRANSPORT:1||spontaneous spin polarization model:1||BIAS:1||emission of electromagnetic waves:1||YBA2CU3O7/PRBA2CU3O7 SUPERLATTICES:1||BOHM:1||SHAPIRO STEPS:1||superconductor/ferromagnet interface:1||OXIDE:1||ANDREEVREFLECTION:1||SinFeAsO single crystal:1||COLLECTIVE MOTION:1||ANGULARDEPENDENCE:1||SUPERCONDUCTIVITY:1||BILAYER GRAPHENE:1||PHOTOLUMINESCENT PROPERTIES:1||SUPERCONDUCTING WEAK LINKS:1||intrinsic Josephson junctions geometrical resonance:1||intrinsic Josephson junction:1||MESOSCOPIC SPINVALVE:1||Bi2212 single crystals:1||intrinsic junctions:1||ANDREEV REFLECTIONS:1||normalmetal/superconductor interface:1||IBI2SR2CACU2OY:1||THERMAL FLUCTUATIONS:1||MIXED STATE:1||BI2.15SR1.85CACU2O8+DELTA:1||intrinsic Josephson effects:1||CACUO:1||QUANTUM POINT CONTACTS:1||resonant tunneling state:1||coherence length:1||NANOWIRE:1||GATES:1||Phase line:1||Thermal activation:1||QUANTUMDOT:1||superconducting proximity effect:1||Andreev interferometer:1||WIRE:1||Josephsonvortexflow branches:1||Bi2212 cuprates:1||LATTICE:1||demannetization effect:1||SUPERCONDUCTING MIRRORS:1||GAS:1||VALLEY TRANSPORT:1||ELECTRODES:1||DEPENDENT TRANSPORT:1||BORNOPPENHEIMER APPROXIMATION:1||collective plasma oscillations:1||fluxon resonance steps:1||STACKS:1||COLLECTIVE DYNAMICS:1||PAIRING SYMMETRY:1||MUON SPIN ROTATION:1||DIMENSIONAL CROSSOVER:1||Bi2Sr2CaCu2Oy highTc superconductors:1||heterojunctions:1||nanostructures:1||surfaces and interfaces:1||QUANTUM TRANSPORT:1||MICROJUNCTIONS:1||RESONATORS:1||STATES:1||FIELD:1||FLUCTUATIONS:1||SCATTERING:1||mode splitting of Josephson vortexflow branches:1||2D superconductivity:1||TRANSISTOR:1||ENERGYGAP:1||SUPERLATTICES:1||IRONBASED SUPERCONDUCTORS:1||PHASEDEPENDENT RESISTANCE:1||QUANTUM PHASETRANSITIONS:1||ELECTRICFIELD:1||HIGH MAGNETICFIELDS:1||NANOWIRE HETEROSTRUCTURES:1||ZNO:1||pair breaking.:1||SUPERCONDUCTING PB:1||domain formation:1||FORCE MICROSCOPY:1||RELAXATION:1||PLASMA RESONANCE:1||coupled Josephson junctions:1||COPPEROXIDE SUPERCONDUCTORS:1||CROSSOVER:1||SIMULATIONS:1||LOWTEMPERATURE:1||CONDUCTORS:1||METALINSULATORTRANSITION:1||SEMICONDUCTOR:1||FIELDEFFECT TRANSISTORS:1||ZEROVOLTAGE STATE:1||constanttemperature interlayer tunneling spectroscopy:1||Josephson supercurrent:1||BIPOLAR SUPERCURRENT:1||Interaction between Josephson and pancake vortices:1||flux jump:1||coaxial heterojunction nanorod:1||Natural Josephson coupling:1||BI2SR2CACU2O8+DELTA:1||VORTEX FLOW:1||TC SUPERCONDUCTORS:1||charge imbalance:1||Andreev diffractometer:1||intercalation:1||surface junction:1||Bi2212:1||tunnelling:1||GRAPHITE:1||GROWTH:1||collective transverse plasma modes:1||GAN:1||Macroscopic quantum tunneling:1||Fluctuation conductivity:1||Abovegap conductance jump:1||Josephson vortex motion:1||Intrinsic Josephson junctions:1||LAYERED SUPERCONDUCTORS:1||BI2SR2CACU2O8+Y:1||INTERFACES:1||BREAKDOWN:1||SYSTEMS:1||Anisotropy ratio:1||Josephson vortex:1||spin relaxation in superconductors:1||bibased single crystals:1||MESOSCOPIC PROXIMITY SUPERCONDUCTOR:1||reentrance of conductance:1||interlayer pair tunneling:1||JOSEPHSON:1||DISORDERED 2DIMENSIONAL SUPERCONDUCTORS:1||INDIUM FILMS:1||excited state:1||REGIME:1||triplet superconductivity:1||FILM:1||SCHOTTKY DIODES:1||peakdiphump structure:1||Kondo effect:1||REENTRANCE:1||Graphene:1||CONTACT:1||BERRYS PHASE:1||2DIMENSIONAL SUPERCONDUCTORS:1||Coulomb diamond:1||magnetic domain:1||spin injection:1||RESONANCE:1||plasma excitation modes:1||FLOW:1||OVERDOPED BI2SR2CACU2O8+DELTA:1||hole doping:1||chemical synthesis:1||phase transitions:1||superconductors:1||VORTEXGLASS SUPERCONDUCTIVITY:1||Kondorelated model:1||RADIATION:1||DOT:1||NANOBELTS:1||Complementarity:1||Closedloop AharonovBohm interferometer:1||pair breaking:1||interlayer phase fluctuation:1||MgB2 thin film:1||CONFINEMENT:1||WALLED CARBON NANOTUBES:1||TRANSITION:9||VORTICES:8||STATE:7||intrinsic Josephson junctions:7||SINGLECRYSTALS:7||JUNCTIONS:5||MODES:5||SUPERCURRENT:5||SUPERCONDUCTOR:5||CONDUCTANCE:5||HIGHTEMPERATURE SUPERCONDUCTORS:5||TRANSPORT:5||PHASE:5||FILMS:4||LOCALIZATION:4||SINGLE DIRAC CONE:4||WIRES:4||MAGNETICFIELD:4||STEPS:3||ELECTRONS:3||proximity effect:3||MODEL:3||ARRAYS:3||INTERFERENCE:3||fluxon dynamics:3||HETEROSTRUCTURES:3||INSULATOR:3||Andreev reflection:3||electronic transport:3||FISKE:3||superconductor:2||ZnO:2||quantum point contact:2||METAL:2||DYNAMICS:2||interlayer Josephson coupling:2||SUPERCONDUCTORS:2||YBA2CU3O7DELTA:2||LAYER:2||DOTS:2||quantum dot:2||Article:2||TRANSISTORS:2||CARBON NANOTUBES:2||GAP:2||MECHANISM:2||LINE:2||GIANT SHAPIRO STEPS:2||LAYERS:2||electron energy loss spectroscopy:2||physical phenomena:2||scanning electron microscopy:2||HGTE QUANTUMWELLS:2||BI2TE3:2||SPECTROSCOPY:2||PNJUNCTIONS:2||spinpolarized tunneling:2||INTRINSIC JOSEPHSONJUNCTIONS:2||FIELDS:2||positive magnetoresistance:2||dilute magnetic semiconductor:2||magnetic field:2||scanning transmission electron microscopy:2||QUANTUM OSCILLATIONS:2||TRANSPORTPROPERTIES:2||surface pair current:2||MAGNETORESISTANCE:2||NANORIBBONS:2||INSTABILITY:2||ANDREEV REFLECTION:2||microwave irradiation:2||vertical graphene josephson junction:2||BI2SE3:2||CONDUCTIVITY:2||highTc superconductors:2||DIMENSIONAL ELECTRONGAS:2||graphene:2||Topological insulators:2||Josephson coupling Fraunhofer interference pattern:2||FERROMAGNET:2||DEPENDENCE:2||DETECTOR:2||COHERENCE:2||INJECTION:2||GRAPHENE:1||JOSEPHSONJUNCTIONS:1||LAYERED SUPERCONDUCTOR:1||mode splitting:1||BEHAVIOR:1||spinpolarized transport:1||SUPERCONDUCTING TRANSITION:1||microwave response:1||PSEUDOGAP:1||phase coherence:1||TRANSITIONS:1||Long Josephson junction:1||Charge detection:1||collective resonance modes:1||plasma oscillation modes:1||Superconducting proximity effect:1||Iron pnictide superconductor:1||McMillanRowell oscillations:1||ferromagnetic microstructure:1||superradiant state:1||VOLTAGE:1||branch splitting:1||TENSOR:1||INTERCALATION:1||insitu fabrication:1||NDGAO3:1||DISORDERED METALS:1||GAUGE GLASS:1||LOWTEMPERATURE TRANSPORT:1||spontaneous spin polarization model:1||BIAS:1||emission of electromagnetic waves:1||YBA2CU3O7/PRBA2CU3O7 SUPERLATTICES:1||BOHM:1||SHAPIRO STEPS:1||superconductor/ferromagnet interface:1||OXIDE:1||ANDREEVREFLECTION:1||SinFeAsO single crystal:1||COLLECTIVE MOTION:1||ANGULARDEPENDENCE:1||SUPERCONDUCTIVITY:1||BILAYER GRAPHENE:1||PHOTOLUMINESCENT PROPERTIES:1||SUPERCONDUCTING WEAK LINKS:1||intrinsic Josephson junctions geometrical resonance:1||intrinsic Josephson junction:1||MESOSCOPIC SPINVALVE:1||Bi2212 single crystals:1||intrinsic junctions:1||ANDREEV REFLECTIONS:1||normalmetal/superconductor interface:1||IBI2SR2CACU2OY:1||THERMAL FLUCTUATIONS:1||MIXED STATE:1||BI2.15SR1.85CACU2O8+DELTA:1||intrinsic Josephson effects:1||CACUO:1||QUANTUM POINT CONTACTS:1||resonant tunneling state:1||coherence length:1||NANOWIRE:1||GATES:1||Phase line:1||Thermal activation:1||QUANTUMDOT:1||superconducting proximity effect:1||Andreev interferometer:1||WIRE:1||Josephsonvortexflow branches:1||Bi2212 cuprates:1||LATTICE:1||demannetization effect:1||SUPERCONDUCTING MIRRORS:1||GAS:1||VALLEY TRANSPORT:1||ELECTRODES:1||DEPENDENT TRANSPORT:1||BORNOPPENHEIMER APPROXIMATION:1||collective plasma oscillations:1||fluxon resonance steps:1||STACKS:1||COLLECTIVE DYNAMICS:1||PAIRING SYMMETRY:1||MUON SPIN ROTATION:1||DIMENSIONAL CROSSOVER:1||Bi2Sr2CaCu2Oy highTc superconductors:1||heterojunctions:1||nanostructures:1||surfaces and interfaces:1||QUANTUM TRANSPORT:1||MICROJUNCTIONS:1||RESONATORS:1||STATES:1||FIELD:1||FLUCTUATIONS:1||SCATTERING:1||mode splitting of Josephson vortexflow branches:1||2D superconductivity:1||TRANSISTOR:1||ENERGYGAP:1||SUPERLATTICES:1||IRONBASED SUPERCONDUCTORS:1||PHASEDEPENDENT RESISTANCE:1||QUANTUM PHASETRANSITIONS:1||ELECTRICFIELD:1||HIGH MAGNETICFIELDS:1||NANOWIRE HETEROSTRUCTURES:1||ZNO:1||pair breaking.:1||SUPERCONDUCTING PB:1||domain formation:1||FORCE MICROSCOPY:1||RELAXATION:1||PLASMA RESONANCE:1||coupled Josephson junctions:1||COPPEROXIDE SUPERCONDUCTORS:1||CROSSOVER:1||SIMULATIONS:1||LOWTEMPERATURE:1||CONDUCTORS:1||METALINSULATORTRANSITION:1||SEMICONDUCTOR:1||FIELDEFFECT TRANSISTORS:1||ZEROVOLTAGE STATE:1||constanttemperature interlayer tunneling spectroscopy:1||Josephson supercurrent:1||BIPOLAR SUPERCURRENT:1||Interaction between Josephson and pancake vortices:1||flux jump:1||coaxial heterojunction nanorod:1||Natural Josephson coupling:1||BI2SR2CACU2O8+DELTA:1||VORTEX FLOW:1||TC SUPERCONDUCTORS:1||charge imbalance:1||Andreev diffractometer:1||intercalation:1||surface junction:1||Bi2212:1||tunnelling:1||GRAPHITE:1||GROWTH:1||collective transverse plasma modes:1||GAN:1||Macroscopic quantum tunneling:1||Fluctuation conductivity:1||Abovegap conductance jump:1||Josephson vortex motion:1||Intrinsic Josephson junctions:1||LAYERED SUPERCONDUCTORS:1||BI2SR2CACU2O8+Y:1||INTERFACES:1||BREAKDOWN:1||SYSTEMS:1||Anisotropy ratio:1||Josephson vortex:1||spin relaxation in superconductors:1||bibased single crystals:1||MESOSCOPIC PROXIMITY SUPERCONDUCTOR:1||reentrance of conductance:1||interlayer pair tunneling:1||JOSEPHSON:1||DISORDERED 2DIMENSIONAL SUPERCONDUCTORS:1||INDIUM FILMS:1||excited state:1||REGIME:1||triplet superconductivity:1||FILM:1||SCHOTTKY DIODES:1||peakdiphump structure:1||Kondo effect:1||REENTRANCE:1||Graphene:1||CONTACT:1||BERRYS PHASE:1||2DIMENSIONAL SUPERCONDUCTORS:1||Coulomb diamond:1||magnetic domain:1||spin injection:1||RESONANCE:1||plasma excitation modes:1||FLOW:1||OVERDOPED BI2SR2CACU2O8+DELTA:1||hole doping:1||chemical synthesis:1||phase transitions:1||superconductors:1||VORTEXGLASS SUPERCONDUCTIVITY:1||Kondorelated model:1||RADIATION:1||DOT:1||NANOBELTS:1||Complementarity:1||Closedloop AharonovBohm interferometer:1||pair breaking:1||interlayer phase fluctuation:1||MgB2 thin film:1||CONFINEMENT:1||WALLED CARBON NANOTUBES:1||TRANSITION:9||VORTICES:8||STATE:7||intrinsic Josephson junctions:7||SINGLECRYSTALS:7||JUNCTIONS:5||MODES:5||SUPERCURRENT:5||SUPERCONDUCTOR:5||CONDUCTANCE:5||HIGHTEMPERATURE SUPERCONDUCTORS:5||TRANSPORT:5||PHASE:5||FILMS:4||LOCALIZATION:4||SINGLE DIRAC CONE:4||WIRES:4||MAGNETICFIELD:4||STEPS:3||ELECTRONS:3||proximity effect:3||MODEL:3||ARRAYS:3||INTERFERENCE:3||fluxon dynamics:3||HETEROSTRUCTURES:3||INSULATOR:3||Andreev reflection:3||electronic transport:3||FISKE:3||superconductor:2||ZnO:2||quantum point contact:2||METAL:2||DYNAMICS:2||interlayer Josephson coupling:2||SUPERCONDUCTORS:2||YBA2CU3O7DELTA:2||LAYER:2||DOTS:2||quantum dot:2||Article:2||TRANSISTORS:2||CARBON NANOTUBES:2||GAP:2||MECHANISM:2||LINE:2||GIANT SHAPIRO STEPS:2||LAYERS:2||electron energy loss spectroscopy:2||physical phenomena:2||scanning electron microscopy:2||HGTE QUANTUMWELLS:2||BI2TE3:2||SPECTROSCOPY:2||PNJUNCTIONS:2||spinpolarized tunneling:2||INTRINSIC JOSEPHSONJUNCTIONS:2||FIELDS:2||positive magnetoresistance:2||dilute magnetic semiconductor:2||magnetic field:2||scanning transmission electron microscopy:2||QUANTUM OSCILLATIONS:2||TRANSPORTPROPERTIES:2||surface pair current:2||MAGNETORESISTANCE:2||NANORIBBONS:2||INSTABILITY:2||ANDREEV REFLECTION:2||microwave irradiation:2||vertical graphene josephson junction:2||BI2SE3:2||CONDUCTIVITY:2||highTc superconductors:2||DIMENSIONAL ELECTRONGAS:2||graphene:2||Topological insulators:2||Josephson coupling Fraunhofer interference pattern:2||FERROMAGNET:2||DEPENDENCE:2||DETECTOR:2||COHERENCE:2||INJECTION:2||GRAPHENE:1||JOSEPHSONJUNCTIONS:1||LAYERED SUPERCONDUCTOR:1||mode splitting:1||BEHAVIOR:1||spinpolarized transport:1||SUPERCONDUCTING TRANSITION:1||microwave response:1||PSEUDOGAP:1||phase coherence:1||TRANSITIONS:1||Long Josephson junction:1||Charge detection:1||collective resonance modes:1||plasma oscillation modes:1||Superconducting proximity effect:1||Iron pnictide superconductor:1||McMillanRowell oscillations:1||ferromagnetic microstructure:1||superradiant state:1||VOLTAGE:1||branch splitting:1||TENSOR:1||INTERCALATION:1||insitu fabrication:1||NDGAO3:1||DISORDERED METALS:1||GAUGE GLASS:1||LOWTEMPERATURE TRANSPORT:1||spontaneous spin polarization model:1||BIAS:1||emission of electromagnetic waves:1||YBA2CU3O7/PRBA2CU3O7 SUPERLATTICES:1||BOHM:1||SHAPIRO STEPS:1||superconductor/ferromagnet interface:1||OXIDE:1||ANDREEVREFLECTION:1||SinFeAsO single crystal:1||COLLECTIVE MOTION:1||ANGULARDEPENDENCE:1||SUPERCONDUCTIVITY:1||BILAYER GRAPHENE:1||PHOTOLUMINESCENT PROPERTIES:1||SUPERCONDUCTING WEAK LINKS:1||intrinsic Josephson junctions geometrical resonance:1||intrinsic Josephson junction:1||MESOSCOPIC SPINVALVE:1||Bi2212 single crystals:1||intrinsic junctions:1||ANDREEV REFLECTIONS:1||normalmetal/superconductor interface:1||IBI2SR2CACU2OY:1||THERMAL FLUCTUATIONS:1||MIXED STATE:1||BI2.15SR1.85CACU2O8+DELTA:1||intrinsic Josephson effects:1||CACUO:1||QUANTUM POINT CONTACTS:1||resonant tunneling state:1||coherence length:1||NANOWIRE:1||GATES:1||Phase line:1||Thermal activation:1||QUANTUMDOT:1||superconducting proximity effect:1||Andreev interferometer:1||WIRE:1||Josephsonvortexflow branches:1||Bi2212 cuprates:1||LATTICE:1||demannetization effect:1||SUPERCONDUCTING MIRRORS:1||GAS:1||VALLEY TRANSPORT:1||ELECTRODES:1||DEPENDENT TRANSPORT:1||BORNOPPENHEIMER APPROXIMATION:1||collective plasma oscillations:1||fluxon resonance steps:1||STACKS:1||COLLECTIVE DYNAMICS:1||PAIRING SYMMETRY:1||MUON SPIN ROTATION:1||DIMENSIONAL CROSSOVER:1||Bi2Sr2CaCu2Oy highTc superconductors:1||heterojunctions:1||nanostructures:1||surfaces and interfaces:1||QUANTUM TRANSPORT:1||MICROJUNCTIONS:1||RESONATORS:1||STATES:1||FIELD:1||FLUCTUATIONS:1||SCATTERING:1||mode splitting of Josephson vortexflow branches:1||2D superconductivity:1||TRANSISTOR:1||ENERGYGAP:1||SUPERLATTICES:1||IRONBASED SUPERCONDUCTORS:1||PHASEDEPENDENT RESISTANCE:1||QUANTUM PHASETRANSITIONS:1||ELECTRICFIELD:1||HIGH MAGNETICFIELDS:1||NANOWIRE HETEROSTRUCTURES:1||ZNO:1||pair breaking.:1||SUPERCONDUCTING PB:1||domain formation:1||FORCE MICROSCOPY:1||RELAXATION:1||PLASMA RESONANCE:1||coupled Josephson junctions:1||COPPEROXIDE SUPERCONDUCTORS:1||CROSSOVER:1||SIMULATIONS:1||LOWTEMPERATURE:1||CONDUCTORS:1||METALINSULATORTRANSITION:1||SEMICONDUCTOR:1||FIELDEFFECT TRANSISTORS:1||ZEROVOLTAGE STATE:1||constanttemperature interlayer tunneling spectroscopy:1||Josephson supercurrent:1||BIPOLAR SUPERCURRENT:1||Interaction between Josephson and pancake vortices:1||flux jump:1||coaxial heterojunction nanorod:1||Natural Josephson coupling:1||BI2SR2CACU2O8+DELTA:1||VORTEX FLOW:1||TC SUPERCONDUCTORS:1||charge imbalance:1||Andreev diffractometer:1||intercalation:1||surface junction:1||Bi2212:1||tunnelling:1||GRAPHITE:1||GROWTH:1||collective transverse plasma modes:1||GAN:1||Macroscopic quantum tunneling:1||Fluctuation conductivity:1||Abovegap conductance jump:1||Josephson vortex motion:1||Intrinsic Josephson junctions:1||LAYERED SUPERCONDUCTORS:1||BI2SR2CACU2O8+Y:1||INTERFACES:1||BREAKDOWN:1||SYSTEMS:1||Anisotropy ratio:1||Josephson vortex:1||spin relaxation in superconductors:1||bibased single crystals:1||MESOSCOPIC PROXIMITY SUPERCONDUCTOR:1||reentrance of conductance:1||interlayer pair tunneling:1||JOSEPHSON:1||DISORDERED 2DIMENSIONAL SUPERCONDUCTORS:1||INDIUM FILMS:1||excited state:1||REGIME:1||triplet superconductivity:1||FILM:1||SCHOTTKY DIODES:1||peakdiphump structure:1||Kondo effect:1||REENTRANCE:1||Graphene:1||CONTACT:1||BERRYS PHASE:1||2DIMENSIONAL SUPERCONDUCTORS:1||Coulomb diamond:1||magnetic domain:1||spin injection:1||RESONANCE:1||plasma excitation modes:1||FLOW:1||OVERDOPED BI2SR2CACU2O8+DELTA:1||hole doping:1||chemical synthesis:1||phase transitions:1||superconductors:1||VORTEXGLASS SUPERCONDUCTIVITY:1||Kondorelated model:1||RADIATION:1||DOT:1||NANOBELTS:1||Complementarity:1||Closedloop AharonovBohm interferometer:1||pair breaking:1||interlayer phase fluctuation:1||MgB2 thin film:1||CONFINEMENT:1||WALLED CARBON NANOTUBES:1||TRANSITION:9||VORTICES:8||STATE:7||intrinsic Josephson junctions:7||SINGLECRYSTALS:7||JUNCTIONS:5||MODES:5||SUPERCURRENT:5||SUPERCONDUCTOR:5||CONDUCTANCE:5||HIGHTEMPERATURE SUPERCONDUCTORS:5||TRANSPORT:5||PHASE:5||FILMS:4||LOCALIZATION:4||SINGLE DIRAC CONE:4||WIRES:4||MAGNETICFIELD:4||STEPS:3||ELECTRONS:3||proximity effect:3||MODEL:3||ARRAYS:3||INTERFERENCE:3||fluxon dynamics:3||HETEROSTRUCTURES:3||INSULATOR:3||Andreev reflection:3||electronic transport:3||FISKE:3||superconductor:2||ZnO:2||quantum point contact:2||METAL:2||DYNAMICS:2||interlayer Josephson coupling:2||SUPERCONDUCTORS:2||YBA2CU3O7DELTA:2||LAYER:2||DOTS:2||quantum dot:2||Article:2||TRANSISTORS:2||CARBON NANOTUBES:2||GAP:2||MECHANISM:2||LINE:2||GIANT SHAPIRO STEPS:2||LAYERS:2||electron energy loss spectroscopy:2||physical phenomena:2||scanning electron microscopy:2||HGTE QUANTUMWELLS:2||BI2TE3:2||SPECTROSCOPY:2||PNJUNCTIONS:2||spinpolarized tunneling:2||INTRINSIC JOSEPHSONJUNCTIONS:2||FIELDS:2||positive magnetoresistance:2||dilute magnetic semiconductor:2||magnetic field:2||scanning transmission electron microscopy:2||QUANTUM OSCILLATIONS:2||TRANSPORTPROPERTIES:2||surface pair current:2||MAGNETORESISTANCE:2||NANORIBBONS:2||INSTABILITY:2||ANDREEV REFLECTION:2||microwave irradiation:2||vertical graphene josephson junction:2||BI2SE3:2||CONDUCTIVITY:2||highTc superconductors:2||DIMENSIONAL ELECTRONGAS:2||graphene:2||Topological insulators:2||Josephson coupling Fraunhofer interference pattern:2||FERROMAGNET:2||DEPENDENCE:2||DETECTOR:2||COHERENCE:2||INJECTION:2||GRAPHENE:1||JOSEPHSONJUNCTIONS:1||LAYERED SUPERCONDUCTOR:1||mode splitting:1||BEHAVIOR:1||spinpolarized transport:1||SUPERCONDUCTING TRANSITION:1||microwave response:1||PSEUDOGAP:1||phase coherence:1||TRANSITIONS:1||Long Josephson junction:1||Charge detection:1||collective resonance modes:1||plasma oscillation modes:1||Superconducting proximity effect:1||Iron pnictide superconductor:1||McMillanRowell oscillations:1||ferromagnetic microstructure:1||superradiant state:1||VOLTAGE:1||branch splitting:1||TENSOR:1||INTERCALATION:1||insitu fabrication:1||NDGAO3:1||DISORDERED METALS:1||GAUGE GLASS:1||LOWTEMPERATURE TRANSPORT:1||spontaneous spin polarization model:1||BIAS:1||emission of electromagnetic waves:1||YBA2CU3O7/PRBA2CU3O7 SUPERLATTICES:1||BOHM:1||SHAPIRO STEPS:1||superconductor/ferromagnet interface:1||OXIDE:1||ANDREEVREFLECTION:1||SinFeAsO single crystal:1||COLLECTIVE MOTION:1||ANGULARDEPENDENCE:1||SUPERCONDUCTIVITY:1||BILAYER GRAPHENE:1||PHOTOLUMINESCENT PROPERTIES:1||SUPERCONDUCTING WEAK LINKS:1||intrinsic Josephson junctions geometrical resonance:1||intrinsic Josephson junction:1||MESOSCOPIC SPINVALVE:1||Bi2212 single crystals:1||intrinsic junctions:1||ANDREEV REFLECTIONS:1||normalmetal/superconductor interface:1||IBI2SR2CACU2OY:1||THERMAL FLUCTUATIONS:1||MIXED STATE:1||BI2.15SR1.85CACU2O8+DELTA:1||intrinsic Josephson effects:1||CACUO:1||QUANTUM POINT CONTACTS:1||resonant tunneling state:1||coherence length:1||NANOWIRE:1||GATES:1||Phase line:1||Thermal activation:1||QUANTUMDOT:1||superconducting proximity effect:1||Andreev interferometer:1||WIRE:1||Josephsonvortexflow branches:1||Bi2212 cuprates:1||LATTICE:1||demannetization effect:1||SUPERCONDUCTING MIRRORS:1||GAS:1||VALLEY TRANSPORT:1||ELECTRODES:1||DEPENDENT TRANSPORT:1||BORNOPPENHEIMER APPROXIMATION:1||collective plasma oscillations:1||fluxon resonance steps:1||STACKS:1||COLLECTIVE DYNAMICS:1||PAIRING SYMMETRY:1||MUON SPIN ROTATION:1||DIMENSIONAL CROSSOVER:1||Bi2Sr2CaCu2Oy highTc superconductors:1||heterojunctions:1||nanostructures:1||surfaces and interfaces:1||QUANTUM TRANSPORT:1||MICROJUNCTIONS:1||RESONATORS:1||STATES:1||FIELD:1||FLUCTUATIONS:1||SCATTERING:1||mode splitting of Josephson vortexflow branches:1||2D superconductivity:1||TRANSISTOR:1||ENERGYGAP:1||SUPERLATTICES:1||IRONBASED SUPERCONDUCTORS:1||PHASEDEPENDENT RESISTANCE:1||QUANTUM PHASETRANSITIONS:1||ELECTRICFIELD:1||HIGH MAGNETICFIELDS:1||NANOWIRE HETEROSTRUCTURES:1||ZNO:1||pair breaking.:1||SUPERCONDUCTING PB:1||domain formation:1||FORCE MICROSCOPY:1||RELAXATION:1||PLASMA RESONANCE:1||coupled Josephson junctions:1||COPPEROXIDE SUPERCONDUCTORS:1||CROSSOVER:1||SIMULATIONS:1||LOWTEMPERATURE:1||CONDUCTORS:1||METALINSULATORTRANSITION:1||SEMICONDUCTOR:1||FIELDEFFECT TRANSISTORS:1||ZEROVOLTAGE STATE:1||constanttemperature interlayer tunneling spectroscopy:1||Josephson supercurrent:1||BIPOLAR SUPERCURRENT:1||Interaction between Josephson and pancake vortices:1||flux jump:1||coaxial heterojunction nanorod:1||Natural Josephson coupling:1||BI2SR2CACU2O8+DELTA:1||VORTEX FLOW:1||TC SUPERCONDUCTORS:1||charge imbalance:1||Andreev diffractometer:1||intercalation:1||surface junction:1||Bi2212:1||tunnelling:1||GRAPHITE:1||GROWTH:1||collective transverse plasma modes:1||GAN:1||Macroscopic quantum tunneling:1||Fluctuation conductivity:1||Abovegap conductance jump:1||Josephson vortex motion:1||Intrinsic Josephson junctions:1||LAYERED SUPERCONDUCTORS:1||BI2SR2CACU2O8+Y:1||INTERFACES:1||BREAKDOWN:1||SYSTEMS:1||Anisotropy ratio:1||Josephson vortex:1||spin relaxation in superconductors:1||bibased single crystals:1||MESOSCOPIC PROXIMITY SUPERCONDUCTOR:1||reentrance of conductance:1||interlayer pair tunneling:1||JOSEPHSON:1||DISORDERED 2DIMENSIONAL SUPERCONDUCTORS:1||INDIUM FILMS:1||excited state:1||REGIME:1||triplet superconductivity:1||FILM:1||SCHOTTKY DIODES:1||peakdiphump structure:1||Kondo effect:1||REENTRANCE:1||Graphene:1||CONTACT:1||BERRYS PHASE:1||2DIMENSIONAL SUPERCONDUCTORS:1||Coulomb diamond:1||magnetic domain:1||spin injection:1||RESONANCE:1||plasma excitation modes:1||FLOW:1||OVERDOPED BI2SR2CACU2O8+DELTA:1||hole doping:1||chemical synthesis:1||phase transitions:1||superconductors:1||VORTEXGLASS SUPERCONDUCTIVITY:1||Kondorelated model:1||RADIATION:1||DOT:1||NANOBELTS:1||Complementarity:1||Closedloop AharonovBohm interferometer:1||pair breaking:1||interlayer phase fluctuation:1||MgB2 thin film:1||CONFINEMENT:1||WALLED CARBON NANOTUBES:1||TRANSITION:9||VORTICES:8||STATE:7||intrinsic Josephson junctions:7||SINGLECRYSTALS:7||JUNCTIONS:5||MODES:5||SUPERCURRENT:5||SUPERCONDUCTOR:5||CONDUCTANCE:5||HIGHTEMPERATURE SUPERCONDUCTORS:5||TRANSPORT:5||PHASE:5||FILMS:4||LOCALIZATION:4||SINGLE DIRAC CONE:4||WIRES:4||MAGNETICFIELD:4||STEPS:3||ELECTRONS:3||proximity effect:3||MODEL:3||ARRAYS:3||INTERFERENCE:3||fluxon dynamics:3||HETEROSTRUCTURES:3||INSULATOR:3||Andreev reflection:3||electronic transport:3||FISKE:3||superconductor:2||ZnO:2||quantum point contact:2||METAL:2||DYNAMICS:2||interlayer Josephson coupling:2||SUPERCONDUCTORS:2||YBA2CU3O7DELTA:2||LAYER:2||DOTS:2||quantum dot:2||Article:2||TRANSISTORS:2||CARBON NANOTUBES:2||GAP:2||MECHANISM:2||LINE:2||GIANT SHAPIRO STEPS:2||LAYERS:2||electron energy loss spectroscopy:2||physical phenomena:2||scanning electron microscopy:2||HGTE QUANTUMWELLS:2||BI2TE3:2||SPECTROSCOPY:2||PNJUNCTIONS:2||spinpolarized tunneling:2||INTRINSIC JOSEPHSONJUNCTIONS:2||FIELDS:2||positive magnetoresistance:2||dilute magnetic semiconductor:2||magnetic field:2||scanning transmission electron microscopy:2||QUANTUM OSCILLATIONS:2||TRANSPORTPROPERTIES:2||surface pair current:2||MAGNETORESISTANCE:2||NANORIBBONS:2||INSTABILITY:2||ANDREEV REFLECTION:2||microwave irradiation:2||vertical graphene josephson junction:2||BI2SE3:2||CONDUCTIVITY:2||highTc superconductors:2||DIMENSIONAL ELECTRONGAS:2||graphene:2||Topological insulators:2||Josephson coupling Fraunhofer interference pattern:2||FERROMAGNET:2||DEPENDENCE:2||DETECTOR:2||COHERENCE:2||INJECTION:2||GRAPHENE:1||JOSEPHSONJUNCTIONS:1||LAYERED SUPERCONDUCTOR:1||mode splitting:1||BEHAVIOR:1||spinpolarized transport:1||SUPERCONDUCTING TRANSITION:1||microwave response:1||PSEUDOGAP:1||phase coherence:1||TRANSITIONS:1||Long Josephson junction:1||Charge detection:1||collective resonance modes:1||plasma oscillation modes:1||Superconducting proximity effect:1||Iron pnictide superconductor:1||McMillanRowell oscillations:1||ferromagnetic microstructure:1||superradiant state:1||VOLTAGE:1||branch splitting:1||TENSOR:1||INTERCALATION:1||insitu fabrication:1||NDGAO3:1||DISORDERED METALS:1||GAUGE GLASS:1||LOWTEMPERATURE TRANSPORT:1||spontaneous spin polarization model:1||BIAS:1||emission of electromagnetic waves:1||YBA2CU3O7/PRBA2CU3O7 SUPERLATTICES:1||BOHM:1||SHAPIRO STEPS:1||superconductor/ferromagnet interface:1||OXIDE:1||ANDREEVREFLECTION:1||SinFeAsO single crystal:1||COLLECTIVE MOTION:1||ANGULARDEPENDENCE:1||SUPERCONDUCTIVITY:1||BILAYER GRAPHENE:1||PHOTOLUMINESCENT PROPERTIES:1||SUPERCONDUCTING WEAK LINKS:1||intrinsic Josephson junctions geometrical resonance:1||intrinsic Josephson junction:1||MESOSCOPIC SPINVALVE:1||Bi2212 single crystals:1||intrinsic junctions:1||ANDREEV REFLECTIONS:1||normalmetal/superconductor interface:1||IBI2SR2CACU2OY:1||THERMAL FLUCTUATIONS:1||MIXED STATE:1||BI2.15SR1.85CACU2O8+DELTA:1||intrinsic Josephson effects:1||CACUO:1||QUANTUM POINT CONTACTS:1||resonant tunneling state:1||coherence length:1||NANOWIRE:1||GATES:1||Phase line:1||Thermal activation:1||QUANTUMDOT:1||superconducting proximity effect:1||Andreev interferometer:1||WIRE:1||Josephsonvortexflow branches:1||Bi2212 cuprates:1||LATTICE:1||demannetization effect:1||SUPERCONDUCTING MIRRORS:1||GAS:1||VALLEY TRANSPORT:1||ELECTRODES:1||DEPENDENT TRANSPORT:1||BORNOPPENHEIMER APPROXIMATION:1||collective plasma oscillations:1||fluxon resonance steps:1||STACKS:1||COLLECTIVE DYNAMICS:1||PAIRING SYMMETRY:1||MUON SPIN ROTATION:1||DIMENSIONAL CROSSOVER:1||Bi2Sr2CaCu2Oy highTc superconductors:1||heterojunctions:1||nanostructures:1||surfaces and interfaces:1||QUANTUM TRANSPORT:1||MICROJUNCTIONS:1||RESONATORS:1||STATES:1||FIELD:1||FLUCTUATIONS:1||SCATTERING:1||mode splitting of Josephson vortexflow branches:1||2D superconductivity:1||TRANSISTOR:1||ENERGYGAP:1||SUPERLATTICES:1||IRONBASED SUPERCONDUCTORS:1||PHASEDEPENDENT RESISTANCE:1||QUANTUM PHASETRANSITIONS:1||ELECTRICFIELD:1||HIGH MAGNETICFIELDS:1||NANOWIRE HETEROSTRUCTURES:1||ZNO:1||pair breaking.:1||SUPERCONDUCTING PB:1||domain formation:1||FORCE MICROSCOPY:1||RELAXATION:1||PLASMA RESONANCE:1||coupled Josephson junctions:1||COPPEROXIDE SUPERCONDUCTORS:1||CROSSOVER:1||SIMULATIONS:1||LOWTEMPERATURE:1||CONDUCTORS:1||METALINSULATORTRANSITION:1||SEMICONDUCTOR:1||FIELDEFFECT TRANSISTORS:1||ZEROVOLTAGE STATE:1||constanttemperature interlayer tunneling spectroscopy:1||Josephson supercurrent:1||BIPOLAR SUPERCURRENT:1||Interaction between Josephson and pancake vortices:1||flux jump:1||coaxial heterojunction nanorod:1||Natural Josephson coupling:1||BI2SR2CACU2O8+DELTA:1||VORTEX FLOW:1||TC SUPERCONDUCTORS:1||charge imbalance:1||Andreev diffractometer:1||intercalation:1||surface junction:1||Bi2212:1||tunnelling:1||GRAPHITE:1||GROWTH:1||collective transverse plasma modes:1||GAN:1||Macroscopic quantum tunneling:1||Fluctuation conductivity:1||Abovegap conductance jump:1||Josephson vortex motion:1||Intrinsic Josephson junctions:1||LAYERED SUPERCONDUCTORS:1||BI2SR2CACU2O8+Y:1||INTERFACES:1||BREAKDOWN:1||SYSTEMS:1||Anisotropy ratio:1||Josephson vortex:1||spin relaxation in superconductors:1||bibased single crystals:1||MESOSCOPIC PROXIMITY SUPERCONDUCTOR:1||reentrance of conductance:1||interlayer pair tunneling:1||JOSEPHSON:1||DISORDERED 2DIMENSIONAL SUPERCONDUCTORS:1||INDIUM FILMS:1||excited state:1||REGIME:1||triplet superconductivity:1||FILM:1||SCHOTTKY DIODES:1||peakdiphump structure:1||Kondo effect:1||REENTRANCE:1||Graphene:1||CONTACT:1||BERRYS PHASE:1||2DIMENSIONAL SUPERCONDUCTORS:1||Coulomb diamond:1||magnetic domain:1||spin injection:1||RESONANCE:1||plasma excitation modes:1||FLOW:1||OVERDOPED BI2SR2CACU2O8+DELTA:1||hole doping:1||chemical synthesis:1||phase transitions:1||superconductors:1||VORTEXGLASS SUPERCONDUCTIVITY:1||Kondorelated model:1||RADIATION:1||DOT:1||NANOBELTS:1||Complementarity:1||Closedloop AharonovBohm interferometer:1||pair breaking:1||interlayer phase fluctuation:1||MgB2 thin film:1||CONFINEMENT:1||WALLED CARBON NANOTUBES:1||TRANSITION:9||VORTICES:8||STATE:7||intrinsic Josephson junctions:7||SINGLECRYSTALS:7||JUNCTIONS:5||MODES:5||SUPERCURRENT:5||SUPERCONDUCTOR:5||CONDUCTANCE:5||HIGHTEMPERATURE SUPERCONDUCTORS:5||TRANSPORT:5||PHASE:5||FILMS:4||LOCALIZATION:4||SINGLE DIRAC CONE:4||WIRES:4||MAGNETICFIELD:4||STEPS:3||ELECTRONS:3||proximity effect:3||MODEL:3||ARRAYS:3||INTERFERENCE:3||fluxon dynamics:3||HETEROSTRUCTURES:3||INSULATOR:3||Andreev reflection:3||electronic transport:3||FISKE:3||superconductor:2||ZnO:2||quantum point contact:2||METAL:2||DYNAMICS:2||interlayer Josephson coupling:2||SUPERCONDUCTORS:2||YBA2CU3O7DELTA:2||LAYER:2||DOTS:2||quantum dot:2||Article:2||TRANSISTORS:2||CARBON NANOTUBES:2||GAP:2||MECHANISM:2||LINE:2||GIANT SHAPIRO STEPS:2||LAYERS:2||electron energy loss spectroscopy:2||physical phenomena:2||scanning electron microscopy:2||HGTE QUANTUMWELLS:2||BI2TE3:2||SPECTROSCOPY:2||PNJUNCTIONS:2||spinpolarized tunneling:2||INTRINSIC JOSEPHSONJUNCTIONS:2||FIELDS:2||positive magnetoresistance:2||dilute magnetic semiconductor:2||magnetic field:2||scanning transmission electron microscopy:2||QUANTUM OSCILLATIONS:2||TRANSPORTPROPERTIES:2||surface pair current:2||MAGNETORESISTANCE:2||NANORIBBONS:2||INSTABILITY:2||ANDREEV REFLECTION:2||microwave irradiation:2||vertical graphene josephson junction:2||BI2SE3:2||CONDUCTIVITY:2||highTc superconductors:2||DIMENSIONAL ELECTRONGAS:2||graphene:2||Topological insulators:2||Josephson coupling Fraunhofer interference pattern:2||FERROMAGNET:2||DEPENDENCE:2||DETECTOR:2||COHERENCE:2||INJECTION:2||GRAPHENE:1||JOSEPHSONJUNCTIONS:1||LAYERED SUPERCONDUCTOR:1||mode splitting:1||BEHAVIOR:1||spinpolarized transport:1||SUPERCONDUCTING TRANSITION:1||microwave response:1||PSEUDOGAP:1||phase coherence:1||TRANSITIONS:1||Long Josephson junction:1||Charge detection:1||collective resonance modes:1||plasma oscillation modes:1||Superconducting proximity effect:1||Iron pnictide superconductor:1||McMillanRowell oscillations:1||ferromagnetic microstructure:1||superradiant state:1||VOLTAGE:1||branch splitting:1||TENSOR:1||INTERCALATION:1||insitu fabrication:1||NDGAO3:1||DISORDERED METALS:1||GAUGE GLASS:1||LOWTEMPERATURE TRANSPORT:1||spontaneous spin polarization model:1||BIAS:1||emission of electromagnetic waves:1||YBA2CU3O7/PRBA2CU3O7 SUPERLATTICES:1||BOHM:1||SHAPIRO STEPS:1||superconductor/ferromagnet interface:1||OXIDE:1||ANDREEVREFLECTION:1||SinFeAsO single crystal:1||COLLECTIVE MOTION:1||ANGULARDEPENDENCE:1||SUPERCONDUCTIVITY:1||BILAYER GRAPHENE:1||PHOTOLUMINESCENT PROPERTIES:1||SUPERCONDUCTING WEAK LINKS:1||intrinsic Josephson junctions geometrical resonance:1||intrinsic Josephson junction:1||MESOSCOPIC SPINVALVE:1||Bi2212 single crystals:1||intrinsic junctions:1||ANDREEV REFLECTIONS:1||normalmetal/superconductor interface:1||IBI2SR2CACU2OY:1||THERMAL FLUCTUATIONS:1||MIXED STATE:1||BI2.15SR1.85CACU2O8+DELTA:1||intrinsic Josephson effects:1||CACUO:1||QUANTUM POINT CONTACTS:1||resonant tunneling state:1||coherence length:1||NANOWIRE:1||GATES:1||Phase line:1||Thermal activation:1||QUANTUMDOT:1||superconducting proximity effect:1||Andreev interferometer:1||WIRE:1||Josephsonvortexflow branches:1||Bi2212 cuprates:1||LATTICE:1||demannetization effect:1||SUPERCONDUCTING MIRRORS:1||GAS:1||VALLEY TRANSPORT:1||ELECTRODES:1||DEPENDENT TRANSPORT:1||BORNOPPENHEIMER APPROXIMATION:1||collective plasma oscillations:1||fluxon resonance steps:1||STACKS:1||COLLECTIVE DYNAMICS:1||PAIRING SYMMETRY:1||MUON SPIN ROTATION:1||DIMENSIONAL CROSSOVER:1||Bi2Sr2CaCu2Oy highTc superconductors:1||heterojunctions:1||nanostructures:1||surfaces and interfaces:1||QUANTUM TRANSPORT:1||MICROJUNCTIONS:1||RESONATORS:1||STATES:1||FIELD:1||FLUCTUATIONS:1||SCATTERING:1||mode splitting of Josephson vortexflow branches:1||2D superconductivity:1||TRANSISTOR:1||ENERGYGAP:1||SUPERLATTICES:1||IRONBASED SUPERCONDUCTORS:1||PHASEDEPENDENT RESISTANCE:1||QUANTUM PHASETRANSITIONS:1||ELECTRICFIELD:1||HIGH MAGNETICFIELDS:1||NANOWIRE HETEROSTRUCTURES:1||ZNO:1||pair breaking.:1||SUPERCONDUCTING PB:1||domain formation:1||FORCE MICROSCOPY:1||RELAXATION:1||PLASMA RESONANCE:1||coupled Josephson junctions:1||COPPEROXIDE SUPERCONDUCTORS:1||CROSSOVER:1||SIMULATIONS:1||LOWTEMPERATURE:1||CONDUCTORS:1||METALINSULATORTRANSITION:1||SEMICONDUCTOR:1||FIELDEFFECT TRANSISTORS:1||ZEROVOLTAGE STATE:1||constanttemperature interlayer tunneling spectroscopy:1||Josephson supercurrent:1||BIPOLAR SUPERCURRENT:1||Interaction between Josephson and pancake vortices:1||flux jump:1||coaxial heterojunction nanorod:1||Natural Josephson coupling:1||BI2SR2CACU2O8+DELTA:1||VORTEX FLOW:1||TC SUPERCONDUCTORS:1||charge imbalance:1||Andreev diffractometer:1||intercalation:1||surface junction:1||Bi2212:1||tunnelling:1||GRAPHITE:1||GROWTH:1||collective transverse plasma modes:1||GAN:1||Macroscopic quantum tunneling:1||Fluctuation conductivity:1||Abovegap conductance jump:1||Josephson vortex motion:1||Intrinsic Josephson junctions:1||LAYERED SUPERCONDUCTORS:1||BI2SR2CACU2O8+Y:1||INTERFACES:1||BREAKDOWN:1||SYSTEMS:1||Anisotropy ratio:1||Josephson vortex:1||spin relaxation in superconductors:1||bibased single crystals:1||MESOSCOPIC PROXIMITY SUPERCONDUCTOR:1||reentrance of conductance:1||interlayer pair tunneling:1||JOSEPHSON:1||DISORDERED 2DIMENSIONAL SUPERCONDUCTORS:1||INDIUM FILMS:1||excited state:1||REGIME:1||triplet superconductivity:1||FILM:1||SCHOTTKY DIODES:1||peakdiphump structure:1||Kondo effect:1||REENTRANCE:1||Graphene:1||CONTACT:1||BERRYS PHASE:1||2DIMENSIONAL SUPERCONDUCTORS:1||Coulomb diamond:1||magnetic domain:1||spin injection:1||RESONANCE:1||plasma excitation modes:1||FLOW:1||OVERDOPED BI2SR2CACU2O8+DELTA:1||hole doping:1||chemical synthesis:1||phase transitions:1||superconductors:1||VORTEXGLASS SUPERCONDUCTIVITY:1||Kondorelated model:1||RADIATION:1||DOT:1||NANOBELTS:1||Complementarity:1||Closedloop AharonovBohm interferometer:1||pair breaking:1||interlayer phase fluctuation:1||MgB2 thin film:1||CONFINEMENT:1||WALLED CARBON NANOTUBES:1||TRANSITION:9||VORTICES:8||STATE:7||intrinsic Josephson junctions:7||SINGLECRYSTALS:7||JUNCTIONS:5||MODES:5||SUPERCURRENT:5||SUPERCONDUCTOR:5||CONDUCTANCE:5||HIGHTEMPERATURE SUPERCONDUCTORS:5||TRANSPORT:5||PHASE:5||FILMS:4||LOCALIZATION:4||SINGLE DIRAC CONE:4||WIRES:4||MAGNETICFIELD:4||STEPS:3||ELECTRONS:3||proximity effect:3||MODEL:3||ARRAYS:3||INTERFERENCE:3||fluxon dynamics:3||HETEROSTRUCTURES:3||INSULATOR:3||Andreev reflection:3||electronic transport:3||FISKE:3||superconductor:2||ZnO:2||quantum point contact:2||METAL:2||DYNAMICS:2||interlayer Josephson coupling:2||SUPERCONDUCTORS:2||YBA2CU3O7DELTA:2||LAYER:2||DOTS:2||quantum dot:2||Article:2||TRANSISTORS:2||CARBON NANOTUBES:2||GAP:2||MECHANISM:2||LINE:2||GIANT SHAPIRO STEPS:2||LAYERS:2||electron energy loss spectroscopy:2||physical phenomena:2||scanning electron microscopy:2||HGTE QUANTUMWELLS:2||BI2TE3:2||SPECTROSCOPY:2||PNJUNCTIONS:2||spinpolarized tunneling:2||INTRINSIC JOSEPHSONJUNCTIONS:2||FIELDS:2||positive magnetoresistance:2||dilute magnetic semiconductor:2||magnetic field:2||scanning transmission electron microscopy:2||QUANTUM OSCILLATIONS:2||TRANSPORTPROPERTIES:2||surface pair current:2||MAGNETORESISTANCE:2||NANORIBBONS:2||INSTABILITY:2||ANDREEV REFLECTION:2||microwave irradiation:2||vertical graphene josephson junction:2||BI2SE3:2||CONDUCTIVITY:2||highTc superconductors:2||DIMENSIONAL ELECTRONGAS:2||graphene:2||Topological insulators:2||Josephson coupling Fraunhofer interference pattern:2||FERROMAGNET:2||DEPENDENCE:2||DETECTOR:2||COHERENCE:2||INJECTION:2||GRAPHENE:1||JOSEPHSONJUNCTIONS:1||LAYERED SUPERCONDUCTOR:1||mode splitting:1||BEHAVIOR:1||spinpolarized transport:1||SUPERCONDUCTING TRANSITION:1||microwave response:1||PSEUDOGAP:1||phase coherence:1||TRANSITIONS:1||Long Josephson junction:1||Charge detection:1||collective resonance modes:1||plasma oscillation modes:1||Superconducting proximity effect:1||Iron pnictide superconductor:1||McMillanRowell oscillations:1||ferromagnetic microstructure:1||superradiant state:1||VOLTAGE:1||branch splitting:1||TENSOR:1||INTERCALATION:1||insitu fabrication:1||NDGAO3:1||DISORDERED METALS:1||GAUGE GLASS:1||LOWTEMPERATURE TRANSPORT:1||spontaneous spin polarization model:1||BIAS:1||emission of electromagnetic waves:1||YBA2CU3O7/PRBA2CU3O7 SUPERLATTICES:1||BOHM:1||SHAPIRO STEPS:1||superconductor/ferromagnet interface:1||OXIDE:1||ANDREEVREFLECTION:1||SinFeAsO single crystal:1||COLLECTIVE MOTION:1||ANGULARDEPENDENCE:1||SUPERCONDUCTIVITY:1||BILAYER GRAPHENE:1||PHOTOLUMINESCENT PROPERTIES:1||SUPERCONDUCTING WEAK LINKS:1||intrinsic Josephson junctions geometrical resonance:1||intrinsic Josephson junction:1||MESOSCOPIC SPINVALVE:1||Bi2212 single crystals:1||intrinsic junctions:1||ANDREEV REFLECTIONS:1||normalmetal/superconductor interface:1||IBI2SR2CACU2OY:1||THERMAL FLUCTUATIONS:1||MIXED STATE:1||BI2.15SR1.85CACU2O8+DELTA:1||intrinsic Josephson effects:1||CACUO:1||QUANTUM POINT CONTACTS:1||resonant tunneling state:1||coherence length:1||NANOWIRE:1||GATES:1||Phase line:1||Thermal activation:1||QUANTUMDOT:1||superconducting proximity effect:1||Andreev interferometer:1||WIRE:1||Josephsonvortexflow branches:1||Bi2212 cuprates:1||LATTICE:1||demannetization effect:1||SUPERCONDUCTING MIRRORS:1||GAS:1||VALLEY TRANSPORT:1||ELECTRODES:1||DEPENDENT TRANSPORT:1||BORNOPPENHEIMER APPROXIMATION:1||collective plasma oscillations:1||fluxon resonance steps:1||STACKS:1||COLLECTIVE DYNAMICS:1||PAIRING SYMMETRY:1||MUON SPIN ROTATION:1||DIMENSIONAL CROSSOVER:1||Bi2Sr2CaCu2Oy highTc superconductors:1||heterojunctions:1||nanostructures:1||surfaces and interfaces:1||QUANTUM TRANSPORT:1||MICROJUNCTIONS:1||RESONATORS:1||STATES:1||FIELD:1||FLUCTUATIONS:1||SCATTERING:1||mode splitting of Josephson vortexflow branches:1||2D superconductivity:1||TRANSISTOR:1||ENERGYGAP:1||SUPERLATTICES:1||IRONBASED SUPERCONDUCTORS:1||PHASEDEPENDENT RESISTANCE:1||QUANTUM PHASETRANSITIONS:1||ELECTRICFIELD:1||HIGH MAGNETICFIELDS:1||NANOWIRE HETEROSTRUCTURES:1||ZNO:1||pair breaking.:1||SUPERCONDUCTING PB:1||domain formation:1||FORCE MICROSCOPY:1||RELAXATION:1||PLASMA RESONANCE:1||coupled Josephson junctions:1||COPPEROXIDE SUPERCONDUCTORS:1||CROSSOVER:1||SIMULATIONS:1||LOWTEMPERATURE:1||CONDUCTORS:1||METALINSULATORTRANSITION:1||SEMICONDUCTOR:1||FIELDEFFECT TRANSISTORS:1||ZEROVOLTAGE STATE:1||constanttemperature interlayer tunneling spectroscopy:1||Josephson supercurrent:1||BIPOLAR SUPERCURRENT:1||Interaction between Josephson and pancake vortices:1||flux jump:1||coaxial heterojunction nanorod:1||Natural Josephson coupling:1||BI2SR2CACU2O8+DELTA:1||VORTEX FLOW:1||TC SUPERCONDUCTORS:1||charge imbalance:1||Andreev diffractometer:1||intercalation:1||surface junction:1||Bi2212:1||tunnelling:1||GRAPHITE:1||GROWTH:1||collective transverse plasma modes:1||GAN:1||Macroscopic quantum tunneling:1||Fluctuation conductivity:1||Abovegap conductance jump:1||Josephson vortex motion:1||Intrinsic Josephson junctions:1||LAYERED SUPERCONDUCTORS:1||BI2SR2CACU2O8+Y:1||INTERFACES:1||BREAKDOWN:1||SYSTEMS:1||Anisotropy ratio:1||Josephson vortex:1||spin relaxation in superconductors:1||bibased single crystals:1||MESOSCOPIC PROXIMITY SUPERCONDUCTOR:1||reentrance of conductance:1||interlayer pair tunneling:1||JOSEPHSON:1||DISORDERED 2DIMENSIONAL SUPERCONDUCTORS:1||INDIUM FILMS:1||excited state:1||REGIME:1||triplet superconductivity:1||FILM:1||SCHOTTKY DIODES:1||peakdiphump structure:1||Kondo effect:1||REENTRANCE:1||Graphene:1||CONTACT:1||BERRYS PHASE:1||2DIMENSIONAL SUPERCONDUCTORS:1||Coulomb diamond:1||magnetic domain:1||spin injection:1||RESONANCE:1||plasma excitation modes:1||FLOW:1||OVERDOPED BI2SR2CACU2O8+DELTA:1||hole doping:1||chemical synthesis:1||phase transitions:1||superconductors:1||VORTEXGLASS SUPERCONDUCTIVITY:1||Kondorelated model:1||RADIATION:1||DOT:1||NANOBELTS:1||Complementarity:1||Closedloop AharonovBohm interferometer:1||pair breaking:1||interlayer phase fluctuation:1||MgB2 thin film:1||CONFINEMENT:1||WALLED CARBON NANOTUBES:1||TRANSITION:9||VORTICES:8||STATE:7||intrinsic Josephson junctions:7||SINGLECRYSTALS:7||JUNCTIONS:5||MODES:5||SUPERCURRENT:5||SUPERCONDUCTOR:5||CONDUCTANCE:5||HIGHTEMPERATURE SUPERCONDUCTORS:5||TRANSPORT:5||PHASE:5||FILMS:4||LOCALIZATION:4||SINGLE DIRAC CONE:4||WIRES:4||MAGNETICFIELD:4||STEPS:3||ELECTRONS:3||proximity effect:3||MODEL:3||ARRAYS:3||INTERFERENCE:3||fluxon dynamics:3||HETEROSTRUCTURES:3||INSULATOR:3||Andreev reflection:3||electronic transport:3||FISKE:3||superconductor:2||ZnO:2||quantum point contact:2||METAL:2||DYNAMICS:2||interlayer Josephson coupling:2||SUPERCONDUCTORS:2||YBA2CU3O7DELTA:2||LAYER:2||DOTS:2||quantum dot:2||Article:2||TRANSISTORS:2||CARBON NANOTUBES:2||GAP:2||MECHANISM:2||LINE:2||GIANT SHAPIRO STEPS:2||LAYERS:2||electron energy loss spectroscopy:2||physical phenomena:2||scanning electron microscopy:2||HGTE QUANTUMWELLS:2||BI2TE3:2||SPECTROSCOPY:2||PNJUNCTIONS:2||spinpolarized tunneling:2||INTRINSIC JOSEPHSONJUNCTIONS:2||FIELDS:2||positive magnetoresistance:2||dilute magnetic semiconductor:2||magnetic field:2||scanning transmission electron microscopy:2||QUANTUM OSCILLATIONS:2||TRANSPORTPROPERTIES:2||surface pair current:2||MAGNETORESISTANCE:2||NANORIBBONS:2||INSTABILITY:2||ANDREEV REFLECTION:2||microwave irradiation:2||vertical graphene josephson junction:2||BI2SE3:2||CONDUCTIVITY:2||highTc superconductors:2||DIMENSIONAL ELECTRONGAS:2||graphene:2||Topological insulators:2||Josephson coupling Fraunhofer interference pattern:2||FERROMAGNET:2||DEPENDENCE:2||DETECTOR:2||COHERENCE:2||INJECTION:2||GRAPHENE:1||JOSEPHSONJUNCTIONS:1||LAYERED SUPERCONDUCTOR:1||mode splitting:1||BEHAVIOR:1||spinpolarized transport:1||SUPERCONDUCTING TRANSITION:1||microwave response:1||PSEUDOGAP:1||phase coherence:1||TRANSITIONS:1||Long Josephson junction:1||Charge detection:1||collective resonance modes:1||plasma oscillation modes:1||Superconducting proximity effect:1||Iron pnictide superconductor:1||McMillanRowell oscillations:1||ferromagnetic microstructure:1||superradiant state:1||VOLTAGE:1||branch splitting:1||TENSOR:1||INTERCALATION:1||insitu fabrication:1||NDGAO3:1||DISORDERED METALS:1||GAUGE GLASS:1||LOWTEMPERATURE TRANSPORT:1||spontaneous spin polarization model:1||BIAS:1||emission of electromagnetic waves:1||YBA2CU3O7/PRBA2CU3O7 SUPERLATTICES:1||BOHM:1||SHAPIRO STEPS:1||superconductor/ferromagnet interface:1||OXIDE:1||ANDREEVREFLECTION:1||SinFeAsO single crystal:1||COLLECTIVE MOTION:1||ANGULARDEPENDENCE:1||SUPERCONDUCTIVITY:1||BILAYER GRAPHENE:1||PHOTOLUMINESCENT PROPERTIES:1||SUPERCONDUCTING WEAK LINKS:1||intrinsic Josephson junctions geometrical resonance:1||intrinsic Josephson junction:1||MESOSCOPIC SPINVALVE:1||Bi2212 single crystals:1||intrinsic junctions:1||ANDREEV REFLECTIONS:1||normalmetal/superconductor interface:1||IBI2SR2CACU2OY:1||THERMAL FLUCTUATIONS:1||MIXED STATE:1||BI2.15SR1.85CACU2O8+DELTA:1||intrinsic Josephson effects:1||CACUO:1||QUANTUM POINT CONTACTS:1||resonant tunneling state:1||coherence length:1||NANOWIRE:1||GATES:1||Phase line:1||Thermal activation:1||QUANTUMDOT:1||superconducting proximity effect:1||Andreev interferometer:1||WIRE:1||Josephsonvortexflow branches:1||Bi2212 cuprates:1||LATTICE:1||demannetization effect:1||SUPERCONDUCTING MIRRORS:1||GAS:1||VALLEY TRANSPORT:1||ELECTRODES:1||DEPENDENT TRANSPORT:1||BORNOPPENHEIMER APPROXIMATION:1||collective plasma oscillations:1||fluxon resonance steps:1||STACKS:1||COLLECTIVE DYNAMICS:1||PAIRING SYMMETRY:1||MUON SPIN ROTATION:1||DIMENSIONAL CROSSOVER:1||Bi2Sr2CaCu2Oy highTc superconductors:1||heterojunctions:1||nanostructures:1||surfaces and interfaces:1||QUANTUM TRANSPORT:1||MICROJUNCTIONS:1||RESONATORS:1||STATES:1||FIELD:1||FLUCTUATIONS:1||SCATTERING:1||mode splitting of Josephson vortexflow branches:1||2D superconductivity:1||TRANSISTOR:1||ENERGYGAP:1||SUPERLATTICES:1||IRONBASED SUPERCONDUCTORS:1||PHASEDEPENDENT RESISTANCE:1||QUANTUM PHASETRANSITIONS:1||ELECTRICFIELD:1||HIGH MAGNETICFIELDS:1||NANOWIRE HETEROSTRUCTURES:1||ZNO:1||pair breaking.:1||SUPERCONDUCTING PB:1||domain formation:1||FORCE MICROSCOPY:1||RELAXATION:1||PLASMA RESONANCE:1||coupled Josephson junctions:1||COPPEROXIDE SUPERCONDUCTORS:1||CROSSOVER:1||SIMULATIONS:1||LOWTEMPERATURE:1||CONDUCTORS:1||METALINSULATORTRANSITION:1||SEMICONDUCTOR:1||FIELDEFFECT TRANSISTORS:1||ZEROVOLTAGE STATE:1||constanttemperature interlayer tunneling spectroscopy:1||Josephson supercurrent:1||BIPOLAR SUPERCURRENT:1||Interaction between Josephson and pancake vortices:1||flux jump:1||coaxial heterojunction nanorod:1||Natural Josephson coupling:1||BI2SR2CACU2O8+DELTA:1||VORTEX FLOW:1||TC SUPERCONDUCTORS:1||charge imbalance:1||Andreev diffractometer:1||intercalation:1||surface junction:1||Bi2212:1||tunnelling:1||GRAPHITE:1||GROWTH:1||collective transverse plasma modes:1||GAN:1||Macroscopic quantum tunneling:1||Fluctuation conductivity:1||Abovegap conductance jump:1||Josephson vortex motion:1||Intrinsic Josephson junctions:1||LAYERED SUPERCONDUCTORS:1||BI2SR2CACU2O8+Y:1||INTERFACES:1||BREAKDOWN:1||SYSTEMS:1||Anisotropy ratio:1||Josephson vortex:1||spin relaxation in superconductors:1||bibased single crystals:1||MESOSCOPIC PROXIMITY SUPERCONDUCTOR:1||reentrance of conductance:1||interlayer pair tunneling:1||JOSEPHSON:1||DISORDERED 2DIMENSIONAL SUPERCONDUCTORS:1||INDIUM FILMS:1||excited state:1||REGIME:1||triplet superconductivity:1||FILM:1||SCHOTTKY DIODES:1||peakdiphump structure:1||Kondo effect:1||REENTRANCE:1||Graphene:1||CONTACT:1||BERRYS PHASE:1||2DIMENSIONAL SUPERCONDUCTORS:1||Coulomb diamond:1||magnetic domain:1||spin injection:1||RESONANCE:1||plasma excitation modes:1||FLOW:1||OVERDOPED BI2SR2CACU2O8+DELTA:1||hole doping:1||chemical synthesis:1||phase transitions:1||superconductors:1||VORTEXGLASS SUPERCONDUCTIVITY:1||Kondorelated model:1||RADIATION:1||DOT:1||NANOBELTS:1||Complementarity:1||Closedloop AharonovBohm interferometer:1||pair breaking:1||interlayer phase fluctuation:1||MgB2 thin film:1||CONFINEMENT:1||WALLED CARBON NANOTUBES:1||TRANSITION:9||VORTICES:8||STATE:7||intrinsic Josephson junctions:7||SINGLECRYSTALS:7||JUNCTIONS:5||MODES:5||SUPERCURRENT:5||SUPERCONDUCTOR:5||CONDUCTANCE:5||HIGHTEMPERATURE SUPERCONDUCTORS:5||TRANSPORT:5||PHASE:5||FILMS:4||LOCALIZATION:4||SINGLE DIRAC CONE:4||WIRES:4||MAGNETICFIELD:4||STEPS:3||ELECTRONS:3||proximity effect:3||MODEL:3||ARRAYS:3||INTERFERENCE:3||fluxon dynamics:3||HETEROSTRUCTURES:3||INSULATOR:3||Andreev reflection:3||electronic transport:3||FISKE:3||superconductor:2||ZnO:2||quantum point contact:2||METAL:2||DYNAMICS:2||interlayer Josephson coupling:2||SUPERCONDUCTORS:2||YBA2CU3O7DELTA:2||LAYER:2||DOTS:2||quantum dot:2||Article:2||TRANSISTORS:2||CARBON NANOTUBES:2||GAP:2||MECHANISM:2||LINE:2||GIANT SHAPIRO STEPS:2||LAYERS:2||electron energy loss spectroscopy:2||physical phenomena:2||scanning electron microscopy:2||HGTE QUANTUMWELLS:2||BI2TE3:2||SPECTROSCOPY:2||PNJUNCTIONS:2||spinpolarized tunneling:2||INTRINSIC JOSEPHSONJUNCTIONS:2||FIELDS:2||positive magnetoresistance:2||dilute magnetic semiconductor:2||magnetic field:2||scanning transmission electron microscopy:2||QUANTUM OSCILLATIONS:2||TRANSPORTPROPERTIES:2||surface pair current:2||MAGNETORESISTANCE:2||NANORIBBONS:2||INSTABILITY:2||ANDREEV REFLECTION:2||microwave irradiation:2||vertical graphene josephson junction:2||BI2SE3:2||CONDUCTIVITY:2||highTc superconductors:2||DIMENSIONAL ELECTRONGAS:2||graphene:2||Topological insulators:2||Josephson coupling Fraunhofer interference pattern:2||FERROMAGNET:2||DEPENDENCE:2||DETECTOR:2||COHERENCE:2||INJECTION:2||GRAPHENE:1||JOSEPHSONJUNCTIONS:1||LAYERED SUPERCONDUCTOR:1||mode splitting:1||BEHAVIOR:1||spinpolarized transport:1||SUPERCONDUCTING TRANSITION:1||microwave response:1||PSEUDOGAP:1||phase coherence:1||TRANSITIONS:1||Long Josephson junction:1||Charge detection:1||collective resonance modes:1||plasma oscillation modes:1||Superconducting proximity effect:1||Iron pnictide superconductor:1||McMillanRowell oscillations:1||ferromagnetic microstructure:1||superradiant state:1||VOLTAGE:1||branch splitting:1||TENSOR:1||INTERCALATION:1||insitu fabrication:1||NDGAO3:1||DISORDERED METALS:1||GAUGE GLASS:1||LOWTEMPERATURE TRANSPORT:1||spontaneous spin polarization model:1||BIAS:1||emission of electromagnetic waves:1||YBA2CU3O7/PRBA2CU3O7 SUPERLATTICES:1||BOHM:1||SHAPIRO STEPS:1||superconductor/ferromagnet interface:1||OXIDE:1||ANDREEVREFLECTION:1||SinFeAsO single crystal:1||COLLECTIVE MOTION:1||ANGULARDEPENDENCE:1||SUPERCONDUCTIVITY:1||BILAYER GRAPHENE:1||PHOTOLUMINESCENT PROPERTIES:1||SUPERCONDUCTING WEAK LINKS:1||intrinsic Josephson junctions geometrical resonance:1||intrinsic Josephson junction:1||MESOSCOPIC SPINVALVE:1||Bi2212 single crystals:1||intrinsic junctions:1||ANDREEV REFLECTIONS:1||normalmetal/superconductor interface:1||IBI2SR2CACU2OY:1||THERMAL FLUCTUATIONS:1||MIXED STATE:1||BI2.15SR1.85CACU2O8+DELTA:1||intrinsic Josephson effects:1||CACUO:1||QUANTUM POINT CONTACTS:1||resonant tunneling state:1||coherence length:1||NANOWIRE:1||GATES:1||Phase line:1||Thermal activation:1||QUANTUMDOT:1||superconducting proximity effect:1||Andreev interferometer:1||WIRE:1||Josephsonvortexflow branches:1||Bi2212 cuprates:1||LATTICE:1||demannetization effect:1||SUPERCONDUCTING MIRRORS:1||GAS:1||VALLEY TRANSPORT:1||ELECTRODES:1||DEPENDENT TRANSPORT:1||BORNOPPENHEIMER APPROXIMATION:1||collective plasma oscillations:1||fluxon resonance steps:1||STACKS:1||COLLECTIVE DYNAMICS:1||PAIRING SYMMETRY:1||MUON SPIN ROTATION:1||DIMENSIONAL CROSSOVER:1||Bi2Sr2CaCu2Oy highTc superconductors:1||heterojunctions:1||nanostructures:1||surfaces and interfaces:1||QUANTUM TRANSPORT:1||MICROJUNCTIONS:1||RESONATORS:1||STATES:1||FIELD:1||FLUCTUATIONS:1||SCATTERING:1||mode splitting of Josephson vortexflow branches:1||2D superconductivity:1||TRANSISTOR:1||ENERGYGAP:1||SUPERLATTICES:1||IRONBASED SUPERCONDUCTORS:1||PHASEDEPENDENT RESISTANCE:1||QUANTUM PHASETRANSITIONS:1||ELECTRICFIELD:1||HIGH MAGNETICFIELDS:1||NANOWIRE HETEROSTRUCTURES:1||ZNO:1||pair breaking.:1||SUPERCONDUCTING PB:1||domain formation:1||FORCE MICROSCOPY:1||RELAXATION:1||PLASMA RESONANCE:1||coupled Josephson junctions:1||COPPEROXIDE SUPERCONDUCTORS:1||CROSSOVER:1||SIMULATIONS:1||LOWTEMPERATURE:1||CONDUCTORS:1||METALINSULATORTRANSITION:1||SEMICONDUCTOR:1||FIELDEFFECT TRANSISTORS:1||ZEROVOLTAGE STATE:1||constanttemperature interlayer tunneling spectroscopy:1||Josephson supercurrent:1||BIPOLAR SUPERCURRENT:1||Interaction between Josephson and pancake vortices:1||flux jump:1||coaxial heterojunction nanorod:1||Natural Josephson coupling:1||BI2SR2CACU2O8+DELTA:1||VORTEX FLOW:1||TC SUPERCONDUCTORS:1||charge imbalance:1||Andreev diffractometer:1||intercalation:1||surface junction:1||Bi2212:1||tunnelling:1||GRAPHITE:1||GROWTH:1||collective transverse plasma modes:1||GAN:1||Macroscopic quantum tunneling:1||Fluctuation conductivity:1||Abovegap conductance jump:1||Josephson vortex motion:1||Intrinsic Josephson junctions:1||LAYERED SUPERCONDUCTORS:1||BI2SR2CACU2O8+Y:1||INTERFACES:1||BREAKDOWN:1||SYSTEMS:1||Anisotropy ratio:1||Josephson vortex:1||spin relaxation in superconductors:1||bibased single crystals:1||MESOSCOPIC PROXIMITY SUPERCONDUCTOR:1||reentrance of conductance:1||interlayer pair tunneling:1||JOSEPHSON:1||DISORDERED 2DIMENSIONAL SUPERCONDUCTORS:1||INDIUM FILMS:1||excited state:1||REGIME:1||triplet superconductivity:1||FILM:1||SCHOTTKY DIODES:1||peakdiphump structure:1||Kondo effect:1||REENTRANCE:1||Graphene:1||CONTACT:1||BERRYS PHASE:1||2DIMENSIONAL SUPERCONDUCTORS:1||Coulomb diamond:1||magnetic domain:1||spin injection:1||RESONANCE:1||plasma excitation modes:1||FLOW:1||OVERDOPED BI2SR2CACU2O8+DELTA:1||hole doping:1||chemical synthesis:1||phase transitions:1||superconductors:1||VORTEXGLASS SUPERCONDUCTIVITY:1||Kondorelated model:1||RADIATION:1||DOT:1||NANOBELTS:1||Complementarity:1||Closedloop AharonovBohm interferometer:1||pair breaking:1||interlayer phase fluctuation:1||MgB2 thin film:1||CONFINEMENT:1||WALLED CARBON NANOTUBES:1||TRANSITION:9||VORTICES:8||STATE:7||intrinsic Josephson junctions:7||SINGLECRYSTALS:7||JUNCTIONS:5||MODES:5||SUPERCURRENT:5||SUPERCONDUCTOR:5||CONDUCTANCE:5||HIGHTEMPERATURE SUPERCONDUCTORS:5||TRANSPORT:5||PHASE:5||FILMS:4||LOCALIZATION:4||SINGLE DIRAC CONE:4||WIRES:4||MAGNETICFIELD:4||STEPS:3||ELECTRONS:3||proximity effect:3||MODEL:3||ARRAYS:3||INTERFERENCE:3||fluxon dynamics:3||HETEROSTRUCTURES:3||INSULATOR:3||Andreev reflection:3||electronic transport:3||FISKE:3||superconductor:2||ZnO:2||quantum point contact:2||METAL:2||DYNAMICS:2||interlayer Josephson coupling:2||SUPERCONDUCTORS:2||YBA2CU3O7DELTA:2||LAYER:2||DOTS:2||quantum dot:2||Article:2||TRANSISTORS:2||CARBON NANOTUBES:2||GAP:2||MECHANISM:2||LINE:2||GIANT SHAPIRO STEPS:2||LAYERS:2||electron energy loss spectroscopy:2||physical phenomena:2||scanning electron microscopy:2||HGTE QUANTUMWELLS:2||BI2TE3:2||SPECTROSCOPY:2||PNJUNCTIONS:2||spinpolarized tunneling:2||INTRINSIC JOSEPHSONJUNCTIONS:2||FIELDS:2||positive magnetoresistance:2||dilute magnetic semiconductor:2||magnetic field:2||scanning transmission electron microscopy:2||QUANTUM OSCILLATIONS:2||TRANSPORTPROPERTIES:2||surface pair current:2||MAGNETORESISTANCE:2||NANORIBBONS:2||INSTABILITY:2||ANDREEV REFLECTION:2||microwave irradiation:2||vertical graphene josephson junction:2||BI2SE3:2||CONDUCTIVITY:2||highTc superconductors:2||DIMENSIONAL ELECTRONGAS:2||graphene:2||Topological insulators:2||Josephson coupling Fraunhofer interference pattern:2||FERROMAGNET:2||DEPENDENCE:2||DETECTOR:2||COHERENCE:2||INJECTION:2||GRAPHENE:1||JOSEPHSONJUNCTIONS:1||LAYERED SUPERCONDUCTOR:1||mode splitting:1||BEHAVIOR:1||spinpolarized transport:1||SUPERCONDUCTING TRANSITION:1||microwave response:1||PSEUDOGAP:1||phase coherence:1||TRANSITIONS:1||Long Josephson junction:1||Charge detection:1||collective resonance modes:1||plasma oscillation modes:1||Superconducting proximity effect:1||Iron pnictide superconductor:1||McMillanRowell oscillations:1||ferromagnetic microstructure:1||superradiant state:1||VOLTAGE:1||branch splitting:1||TENSOR:1||INTERCALATION:1||insitu fabrication:1||NDGAO3:1||DISORDERED METALS:1||GAUGE GLASS:1||LOWTEMPERATURE TRANSPORT:1||spontaneous spin polarization model:1||BIAS:1||emission of electromagnetic waves:1||YBA2CU3O7/PRBA2CU3O7 SUPERLATTICES:1||BOHM:1||SHAPIRO STEPS:1||superconductor/ferromagnet interface:1||OXIDE:1||ANDREEVREFLECTION:1||SinFeAsO single crystal:1||COLLECTIVE MOTION:1||ANGULARDEPENDENCE:1||SUPERCONDUCTIVITY:1||BILAYER GRAPHENE:1||PHOTOLUMINESCENT PROPERTIES:1||SUPERCONDUCTING WEAK LINKS:1||intrinsic Josephson junctions geometrical resonance:1||intrinsic Josephson junction:1||MESOSCOPIC SPINVALVE:1||Bi2212 single crystals:1||intrinsic junctions:1||ANDREEV REFLECTIONS:1||normalmetal/superconductor interface:1||IBI2SR2CACU2OY:1||THERMAL FLUCTUATIONS:1||MIXED STATE:1||BI2.15SR1.85CACU2O8+DELTA:1||intrinsic Josephson effects:1||CACUO:1||QUANTUM POINT CONTACTS:1||resonant tunneling state:1||coherence length:1||NANOWIRE:1||GATES:1||Phase line:1||Thermal activation:1||QUANTUMDOT:1||superconducting proximity effect:1||Andreev interferometer:1||WIRE:1||Josephsonvortexflow branches:1||Bi2212 cuprates:1||LATTICE:1||demannetization effect:1||SUPERCONDUCTING MIRRORS:1||GAS:1||VALLEY TRANSPORT:1||ELECTRODES:1||DEPENDENT TRANSPORT:1||BORNOPPENHEIMER APPROXIMATION:1||collective plasma oscillations:1||fluxon resonance steps:1||STACKS:1||COLLECTIVE DYNAMICS:1||PAIRING SYMMETRY:1||MUON SPIN ROTATION:1||DIMENSIONAL CROSSOVER:1||Bi2Sr2CaCu2Oy highTc superconductors:1||heterojunctions:1||nanostructures:1||surfaces and interfaces:1||QUANTUM TRANSPORT:1||MICROJUNCTIONS:1||RESONATORS:1||STATES:1||FIELD:1||FLUCTUATIONS:1||SCATTERING:1||mode splitting of Josephson vortexflow branches:1||2D superconductivity:1||TRANSISTOR:1||ENERGYGAP:1||SUPERLATTICES:1||IRONBASED SUPERCONDUCTORS:1||PHASEDEPENDENT RESISTANCE:1||QUANTUM PHASETRANSITIONS:1||ELECTRICFIELD:1||HIGH MAGNETICFIELDS:1||NANOWIRE HETEROSTRUCTURES:1||ZNO:1||pair breaking.:1||SUPERCONDUCTING PB:1||domain formation:1||FORCE MICROSCOPY:1||RELAXATION:1||PLASMA RESONANCE:1||coupled Josephson junctions:1||COPPEROXIDE SUPERCONDUCTORS:1||CROSSOVER:1||SIMULATIONS:1||LOWTEMPERATURE:1||CONDUCTORS:1||METALINSULATORTRANSITION:1||SEMICONDUCTOR:1||FIELDEFFECT TRANSISTORS:1||ZEROVOLTAGE STATE:1||constanttemperature interlayer tunneling spectroscopy:1||Josephson supercurrent:1||BIPOLAR SUPERCURRENT:1||Interaction between Josephson and pancake vortices:1||flux jump:1||coaxial heterojunction nanorod:1||Natural Josephson coupling:1||BI2SR2CACU2O8+DELTA:1||VORTEX FLOW:1||TC SUPERCONDUCTORS:1||charge imbalance:1||Andreev diffractometer:1||intercalation:1||surface junction:1||Bi2212:1||tunnelling:1||GRAPHITE:1||GROWTH:1||collective transverse plasma modes:1||GAN:1||Macroscopic quantum tunneling:1||Fluctuation conductivity:1||Abovegap conductance jump:1||Josephson vortex motion:1||Intrinsic Josephson junctions:1||LAYERED SUPERCONDUCTORS:1||BI2SR2CACU2O8+Y:1||INTERFACES:1||BREAKDOWN:1||SYSTEMS:1||Anisotropy ratio:1||Josephson vortex:1||spin relaxation in superconductors:1||bibased single crystals:1||MESOSCOPIC PROXIMITY SUPERCONDUCTOR:1||reentrance of conductance:1||interlayer pair tunneling:1||JOSEPHSON:1||DISORDERED 2DIMENSIONAL SUPERCONDUCTORS:1||INDIUM FILMS:1||excited state:1||REGIME:1||triplet superconductivity:1||FILM:1||SCHOTTKY DIODES:1||peakdiphump structure:1||Kondo effect:1||REENTRANCE:1||Graphene:1||CONTACT:1||BERRYS PHASE:1||2DIMENSIONAL SUPERCONDUCTORS:1||Coulomb diamond:1||magnetic domain:1||spin injection:1||RESONANCE:1||plasma excitation modes:1||FLOW:1||OVERDOPED BI2SR2CACU2O8+DELTA:1||hole doping:1||chemical synthesis:1||phase transitions:1||superconductors:1||VORTEXGLASS SUPERCONDUCTIVITY:1||Kondorelated model:1||RADIATION:1||DOT:1||NANOBELTS:1||Complementarity:1||Closedloop AharonovBohm interferometer:1||pair breaking:1||interlayer phase fluctuation:1||MgB2 thin film:1||CONFINEMENT:1||WALLED CARBON NANOTUBES:1||TRANSITION:9||VORTICES:8||STATE:7||intrinsic Josephson junctions:7||SINGLECRYSTALS:7||JUNCTIONS:5||MODES:5||SUPERCURRENT:5||SUPERCONDUCTOR:5||CONDUCTANCE:5||HIGHTEMPERATURE SUPERCONDUCTORS:5||TRANSPORT:5||PHASE:5||FILMS:4||LOCALIZATION:4||SINGLE DIRAC CONE:4||WIRES:4||MAGNETICFIELD:4||STEPS:3||ELECTRONS:3||proximity effect:3||MODEL:3||ARRAYS:3||INTERFERENCE:3||fluxon dynamics:3||HETEROSTRUCTURES:3||INSULATOR:3||Andreev reflection:3||electronic transport:3||FISKE:3||superconductor:2||ZnO:2||quantum point contact:2||METAL:2||DYNAMICS:2||interlayer Josephson coupling:2||SUPERCONDUCTORS:2||YBA2CU3O7DELTA:2||LAYER:2||DOTS:2||quantum dot:2||Article:2||TRANSISTORS:2||CARBON NANOTUBES:2||GAP:2||MECHANISM:2||LINE:2||GIANT SHAPIRO STEPS:2||LAYERS:2||electron energy loss spectroscopy:2||physical phenomena:2||scanning electron microscopy:2||HGTE QUANTUMWELLS:2||BI2TE3:2||SPECTROSCOPY:2||PNJUNCTIONS:2||spinpolarized tunneling:2||INTRINSIC JOSEPHSONJUNCTIONS:2||FIELDS:2||positive magnetoresistance:2||dilute magnetic semiconductor:2||magnetic field:2||scanning transmission electron microscopy:2||QUANTUM OSCILLATIONS:2||TRANSPORTPROPERTIES:2||surface pair current:2||MAGNETORESISTANCE:2||NANORIBBONS:2||INSTABILITY:2||ANDREEV REFLECTION:2||microwave irradiation:2||vertical graphene josephson junction:2||BI2SE3:2||CONDUCTIVITY:2||highTc superconductors:2||DIMENSIONAL ELECTRONGAS:2||graphene:2||Topological insulators:2||Josephson coupling Fraunhofer interference pattern:2||FERROMAGNET:2||DEPENDENCE:2||DETECTOR:2||COHERENCE:2||INJECTION:2||GRAPHENE:1||JOSEPHSONJUNCTIONS:1||LAYERED SUPERCONDUCTOR:1||mode splitting:1||BEHAVIOR:1||spinpolarized transport:1||SUPERCONDUCTING TRANSITION:1||microwave response:1||PSEUDOGAP:1||phase coherence:1||TRANSITIONS:1||Long Josephson junction:1||Charge detection:1||collective resonance modes:1||plasma oscillation modes:1||Superconducting proximity effect:1||Iron pnictide superconductor:1||McMillanRowell oscillations:1||ferromagnetic microstructure:1||superradiant state:1||VOLTAGE:1||branch splitting:1||TENSOR:1||INTERCALATION:1||insitu fabrication:1||NDGAO3:1||DISORDERED METALS:1||GAUGE GLASS:1||LOWTEMPERATURE TRANSPORT:1||spontaneous spin polarization model:1||BIAS:1||emission of electromagnetic waves:1||YBA2CU3O7/PRBA2CU3O7 SUPERLATTICES:1||BOHM:1||SHAPIRO STEPS:1||superconductor/ferromagnet interface:1||OXIDE:1||ANDREEVREFLECTION:1||SinFeAsO single crystal:1||COLLECTIVE MOTION:1||ANGULARDEPENDENCE:1||SUPERCONDUCTIVITY:1||BILAYER GRAPHENE:1||PHOTOLUMINESCENT PROPERTIES:1||SUPERCONDUCTING WEAK LINKS:1||intrinsic Josephson junctions geometrical resonance:1||intrinsic Josephson junction:1||MESOSCOPIC SPINVALVE:1||Bi2212 single crystals:1||intrinsic junctions:1||ANDREEV REFLECTIONS:1||normalmetal/superconductor interface:1||IBI2SR2CACU2OY:1||THERMAL FLUCTUATIONS:1||MIXED STATE:1||BI2.15SR1.85CACU2O8+DELTA:1||intrinsic Josephson effects:1||CACUO:1||QUANTUM POINT CONTACTS:1||resonant tunneling state:1||coherence length:1||NANOWIRE:1||GATES:1||Phase line:1||Thermal activation:1||QUANTUMDOT:1||superconducting proximity effect:1||Andreev interferometer:1||WIRE:1||Josephsonvortexflow branches:1||Bi2212 cuprates:1||LATTICE:1||demannetization effect:1||SUPERCONDUCTING MIRRORS:1||GAS:1||VALLEY TRANSPORT:1||ELECTRODES:1||DEPENDENT TRANSPORT:1||BORNOPPENHEIMER APPROXIMATION:1||collective plasma oscillations:1||fluxon resonance steps:1||STACKS:1||COLLECTIVE DYNAMICS:1||PAIRING SYMMETRY:1||MUON SPIN ROTATION:1||DIMENSIONAL CROSSOVER:1||Bi2Sr2CaCu2Oy highTc superconductors:1||heterojunctions:1||nanostructures:1||surfaces and interfaces:1||QUANTUM TRANSPORT:1||MICROJUNCTIONS:1||RESONATORS:1||STATES:1||FIELD:1||FLUCTUATIONS:1||SCATTERING:1||mode splitting of Josephson vortexflow branches:1||2D superconductivity:1||TRANSISTOR:1||ENERGYGAP:1||SUPERLATTICES:1||IRONBASED SUPERCONDUCTORS:1||PHASEDEPENDENT RESISTANCE:1||QUANTUM PHASETRANSITIONS:1||ELECTRICFIELD:1||HIGH MAGNETICFIELDS:1||NANOWIRE HETEROSTRUCTURES:1||ZNO:1||pair breaking.:1||SUPERCONDUCTING PB:1||domain formation:1||FORCE MICROSCOPY:1||RELAXATION:1||PLASMA RESONANCE:1||coupled Josephson junctions:1||COPPEROXIDE SUPERCONDUCTORS:1||CROSSOVER:1||SIMULATIONS:1||LOWTEMPERATURE:1||CONDUCTORS:1||METALINSULATORTRANSITION:1||SEMICONDUCTOR:1||FIELDEFFECT TRANSISTORS:1||ZEROVOLTAGE STATE:1||constanttemperature interlayer tunneling spectroscopy:1||Josephson supercurrent:1||BIPOLAR SUPERCURRENT:1||Interaction between Josephson and pancake vortices:1||flux jump:1||coaxial heterojunction nanorod:1||Natural Josephson coupling:1||BI2SR2CACU2O8+DELTA:1||VORTEX FLOW:1||TC SUPERCONDUCTORS:1||charge imbalance:1||Andreev diffractometer:1||intercalation:1||surface junction:1||Bi2212:1||tunnelling:1||GRAPHITE:1||GROWTH:1||collective transverse plasma modes:1||GAN:1||Macroscopic quantum tunneling:1||Fluctuation conductivity:1||Abovegap conductance jump:1||Josephson vortex motion:1||Intrinsic Josephson junctions:1||LAYERED SUPERCONDUCTORS:1||BI2SR2CACU2O8+Y:1||INTERFACES:1||BREAKDOWN:1||SYSTEMS:1||Anisotropy ratio:1||Josephson vortex:1||spin relaxation in superconductors:1||bibased single crystals:1||MESOSCOPIC PROXIMITY SUPERCONDUCTOR:1||reentrance of conductance:1||interlayer pair tunneling:1||JOSEPHSON:1||DISORDERED 2DIMENSIONAL SUPERCONDUCTORS:1||INDIUM FILMS:1||excited state:1||REGIME:1||triplet superconductivity:1||FILM:1||SCHOTTKY DIODES:1||peakdiphump structure:1||Kondo effect:1||REENTRANCE:1||Graphene:1||CONTACT:1||BERRYS PHASE:1||2DIMENSIONAL SUPERCONDUCTORS:1||Coulomb diamond:1||magnetic domain:1||spin injection:1||RESONANCE:1||plasma excitation modes:1||FLOW:1||OVERDOPED BI2SR2CACU2O8+DELTA:1||hole doping:1||chemical synthesis:1||phase transitions:1||superconductors:1||VORTEXGLASS SUPERCONDUCTIVITY:1||Kondorelated model:1||RADIATION:1||DOT:1||NANOBELTS:1||Complementarity:1||Closedloop AharonovBohm interferometer:1||pair breaking:1||interlayer phase fluctuation:1||MgB2 thin film:1||CONFINEMENT:1||WALLED CARBON NANOTUBES:1||TRANSITION:9||VORTICES:8||STATE:7||intrinsic Josephson junctions:7||SINGLECRYSTALS:7||JUNCTIONS:5||MODES:5||SUPERCURRENT:5||SUPERCONDUCTOR:5||CONDUCTANCE:5||HIGHTEMPERATURE SUPERCONDUCTORS:5||TRANSPORT:5||PHASE:5||FILMS:4||LOCALIZATION:4||SINGLE DIRAC CONE:4||WIRES:4||MAGNETICFIELD:4||STEPS:3||ELECTRONS:3||proximity effect:3||MODEL:3||ARRAYS:3||INTERFERENCE:3||fluxon dynamics:3||HETEROSTRUCTURES:3||INSULATOR:3||Andreev reflection:3||electronic transport:3||FISKE:3||superconductor:2||ZnO:2||quantum point contact:2||METAL:2||DYNAMICS:2||interlayer Josephson coupling:2||SUPERCONDUCTORS:2||YBA2CU3O7DELTA:2||LAYER:2||DOTS:2||quantum dot:2||Article:2||TRANSISTORS:2||CARBON NANOTUBES:2||GAP:2||MECHANISM:2||LINE:2||GIANT SHAPIRO STEPS:2||LAYERS:2||electron energy loss spectroscopy:2||physical phenomena:2||scanning electron microscopy:2||HGTE QUANTUMWELLS:2||BI2TE3:2||SPECTROSCOPY:2||PNJUNCTIONS:2||spinpolarized tunneling:2||INTRINSIC JOSEPHSONJUNCTIONS:2||FIELDS:2||positive magnetoresistance:2||dilute magnetic semiconductor:2||magnetic field:2||scanning transmission electron microscopy:2||QUANTUM OSCILLATIONS:2||TRANSPORTPROPERTIES:2||surface pair current:2||MAGNETORESISTANCE:2||NANORIBBONS:2||INSTABILITY:2||ANDREEV REFLECTION:2||microwave irradiation:2||vertical graphene josephson junction:2||BI2SE3:2||CONDUCTIVITY:2||highTc superconductors:2||DIMENSIONAL ELECTRONGAS:2||graphene:2||Topological insulators:2||Josephson coupling Fraunhofer interference pattern:2||FERROMAGNET:2||DEPENDENCE:2||DETECTOR:2||COHERENCE:2||INJECTION:2||GRAPHENE:1||JOSEPHSONJUNCTIONS:1||LAYERED SUPERCONDUCTOR:1||mode splitting:1||BEHAVIOR:1||spinpolarized transport:1||SUPERCONDUCTING TRANSITION:1||microwave response:1||PSEUDOGAP:1||phase coherence:1||TRANSITIONS:1||Long Josephson junction:1||Charge detection:1||collective resonance modes:1||plasma oscillation modes:1||Superconducting proximity effect:1||Iron pnictide superconductor:1||McMillanRowell oscillations:1||ferromagnetic microstructure:1||superradiant state:1||VOLTAGE:1||branch splitting:1||TENSOR:1||INTERCALATION:1||insitu fabrication:1||NDGAO3:1||DISORDERED METALS:1||GAUGE GLASS:1||LOWTEMPERATURE TRANSPORT:1||spontaneous spin polarization model:1||BIAS:1||emission of electromagnetic waves:1||YBA2CU3O7/PRBA2CU3O7 SUPERLATTICES:1||BOHM:1||SHAPIRO STEPS:1||superconductor/ferromagnet interface:1||OXIDE:1||ANDREEVREFLECTION:1||SinFeAsO single crystal:1||COLLECTIVE MOTION:1||ANGULARDEPENDENCE:1||SUPERCONDUCTIVITY:1||BILAYER GRAPHENE:1||PHOTOLUMINESCENT PROPERTIES:1||SUPERCONDUCTING WEAK LINKS:1||intrinsic Josephson junctions geometrical resonance:1||intrinsic Josephson junction:1||MESOSCOPIC SPINVALVE:1||Bi2212 single crystals:1||intrinsic junctions:1||ANDREEV REFLECTIONS:1||normalmetal/superconductor interface:1||IBI2SR2CACU2OY:1||THERMAL FLUCTUATIONS:1||MIXED STATE:1||BI2.15SR1.85CACU2O8+DELTA:1||intrinsic Josephson effects:1||CACUO:1||QUANTUM POINT CONTACTS:1||resonant tunneling state:1||coherence length:1||NANOWIRE:1||GATES:1||Phase line:1||Thermal activation:1||QUANTUMDOT:1||superconducting proximity effect:1||Andreev interferometer:1||WIRE:1||Josephsonvortexflow branches:1||Bi2212 cuprates:1||LATTICE:1||demannetization effect:1||SUPERCONDUCTING MIRRORS:1||GAS:1||VALLEY TRANSPORT:1||ELECTRODES:1||DEPENDENT TRANSPORT:1||BORNOPPENHEIMER APPROXIMATION:1||collective plasma oscillations:1||fluxon resonance steps:1||STACKS:1||COLLECTIVE DYNAMICS:1||PAIRING SYMMETRY:1||MUON SPIN ROTATION:1||DIMENSIONAL CROSSOVER:1||Bi2Sr2CaCu2Oy highTc superconductors:1||heterojunctions:1||nanostructures:1||surfaces and interfaces:1||QUANTUM TRANSPORT:1||MICROJUNCTIONS:1||RESONATORS:1||STATES:1||FIELD:1||FLUCTUATIONS:1||SCATTERING:1||mode splitting of Josephson vortexflow branches:1||2D superconductivity:1||TRANSISTOR:1||ENERGYGAP:1||SUPERLATTICES:1||IRONBASED SUPERCONDUCTORS:1||PHASEDEPENDENT RESISTANCE:1||QUANTUM PHASETRANSITIONS:1||ELECTRICFIELD:1||HIGH MAGNETICFIELDS:1||NANOWIRE HETEROSTRUCTURES:1||ZNO:1||pair breaking.:1||SUPERCONDUCTING PB:1||domain formation:1||FORCE MICROSCOPY:1||RELAXATION:1||PLASMA RESONANCE:1||coupled Josephson junctions:1||COPPEROXIDE SUPERCONDUCTORS:1||CROSSOVER:1||SIMULATIONS:1||LOWTEMPERATURE:1||CONDUCTORS:1||METALINSULATORTRANSITION:1||SEMICONDUCTOR:1||FIELDEFFECT TRANSISTORS:1||ZEROVOLTAGE STATE:1||constanttemperature interlayer tunneling spectroscopy:1||Josephson supercurrent:1||BIPOLAR SUPERCURRENT:1||Interaction between Josephson and pancake vortices:1||flux jump:1||coaxial heterojunction nanorod:1||Natural Josephson coupling:1||BI2SR2CACU2O8+DELTA:1||VORTEX FLOW:1||TC SUPERCONDUCTORS:1||charge imbalance:1||Andreev diffractometer:1||intercalation:1||surface junction:1||Bi2212:1||tunnelling:1||GRAPHITE:1||GROWTH:1||collective transverse plasma modes:1||GAN:1||Macroscopic quantum tunneling:1||Fluctuation conductivity:1||Abovegap conductance jump:1||Josephson vortex motion:1||Intrinsic Josephson junctions:1||LAYERED SUPERCONDUCTORS:1||BI2SR2CACU2O8+Y:1||INTERFACES:1||BREAKDOWN:1||SYSTEMS:1||Anisotropy ratio:1||Josephson vortex:1||spin relaxation in superconductors:1||bibased single crystals:1||MESOSCOPIC PROXIMITY SUPERCONDUCTOR:1||reentrance of conductance:1||interlayer pair tunneling:1||JOSEPHSON:1||DISORDERED 2DIMENSIONAL SUPERCONDUCTORS:1||INDIUM FILMS:1||excited state:1||REGIME:1||triplet superconductivity:1||FILM:1||SCHOTTKY DIODES:1||peakdiphump structure:1||Kondo effect:1||REENTRANCE:1||Graphene:1||CONTACT:1||BERRYS PHASE:1||2DIMENSIONAL SUPERCONDUCTORS:1||Coulomb diamond:1||magnetic domain:1||spin injection:1||RESONANCE:1||plasma excitation modes:1||FLOW:1||OVERDOPED BI2SR2CACU2O8+DELTA:1||hole doping:1||chemical synthesis:1||phase transitions:1||superconductors:1||VORTEXGLASS SUPERCONDUCTIVITY:1||Kondorelated model:1||RADIATION:1||DOT:1||NANOBELTS:1||Complementarity:1||Closedloop AharonovBohm interferometer:1||pair breaking:1||interlayer phase fluctuation:1||MgB2 thin film:1||CONFINEMENT:1||WALLED CARBON NANOTUBES:1||TRANSITION:9||VORTICES:8||STATE:7||intrinsic Josephson junctions:7||SINGLECRYSTALS:7||JUNCTIONS:5||MODES:5||SUPERCURRENT:5||SUPERCONDUCTOR:5||CONDUCTANCE:5||HIGHTEMPERATURE SUPERCONDUCTORS:5||TRANSPORT:5||PHASE:5||FILMS:4||LOCALIZATION:4||SINGLE DIRAC CONE:4||WIRES:4||MAGNETICFIELD:4||STEPS:3||ELECTRONS:3||proximity effect:3||MODEL:3||ARRAYS:3||INTERFERENCE:3||fluxon dynamics:3||HETEROSTRUCTURES:3||INSULATOR:3||Andreev reflection:3||electronic transport:3||FISKE:3||superconductor:2||ZnO:2||quantum point contact:2||METAL:2||DYNAMICS:2||interlayer Josephson coupling:2||SUPERCONDUCTORS:2||YBA2CU3O7DELTA:2||LAYER:2||DOTS:2||quantum dot:2||Article:2||TRANSISTORS:2||CARBON NANOTUBES:2||GAP:2||MECHANISM:2||LINE:2||GIANT SHAPIRO STEPS:2||LAYERS:2||electron energy loss spectroscopy:2||physical phenomena:2||scanning electron microscopy:2||HGTE QUANTUMWELLS:2||BI2TE3:2||SPECTROSCOPY:2||PNJUNCTIONS:2||spinpolarized tunneling:2||INTRINSIC JOSEPHSONJUNCTIONS:2||FIELDS:2||positive magnetoresistance:2||dilute magnetic semiconductor:2||magnetic field:2||scanning transmission electron microscopy:2||QUANTUM OSCILLATIONS:2||TRANSPORTPROPERTIES:2||surface pair current:2||MAGNETORESISTANCE:2||NANORIBBONS:2||INSTABILITY:2||ANDREEV REFLECTION:2||microwave irradiation:2||vertical graphene josephson junction:2||BI2SE3:2||CONDUCTIVITY:2||highTc superconductors:2||DIMENSIONAL ELECTRONGAS:2||graphene:2||Topological insulators:2||Josephson coupling Fraunhofer interference pattern:2||FERROMAGNET:2||DEPENDENCE:2||DETECTOR:2||COHERENCE:2||INJECTION:2||GRAPHENE:1||JOSEPHSONJUNCTIONS:1||LAYERED SUPERCONDUCTOR:1||mode splitting:1||BEHAVIOR:1||spinpolarized transport:1||SUPERCONDUCTING TRANSITION:1||microwave response:1||PSEUDOGAP:1||phase coherence:1||TRANSITIONS:1||Long Josephson junction:1||Charge detection:1||collective resonance modes:1||plasma oscillation modes:1||Superconducting proximity effect:1||Iron pnictide superconductor:1||McMillanRowell oscillations:1||ferromagnetic microstructure:1||superradiant state:1||VOLTAGE:1||branch splitting:1||TENSOR:1||INTERCALATION:1||insitu fabrication:1||NDGAO3:1||DISORDERED METALS:1||GAUGE GLASS:1||LOWTEMPERATURE TRANSPORT:1||spontaneous spin polarization model:1||BIAS:1||emission of electromagnetic waves:1||YBA2CU3O7/PRBA2CU3O7 SUPERLATTICES:1||BOHM:1||SHAPIRO STEPS:1||superconductor/ferromagnet interface:1||OXIDE:1||ANDREEVREFLECTION:1||SinFeAsO single crystal:1||COLLECTIVE MOTION:1||ANGULARDEPENDENCE:1||SUPERCONDUCTIVITY:1||BILAYER GRAPHENE:1||PHOTOLUMINESCENT PROPERTIES:1||SUPERCONDUCTING WEAK LINKS:1||intrinsic Josephson junctions geometrical resonance:1||intrinsic Josephson junction:1||MESOSCOPIC SPINVALVE:1||Bi2212 single crystals:1||intrinsic junctions:1||ANDREEV REFLECTIONS:1||normalmetal/superconductor interface:1||IBI2SR2CACU2OY:1||THERMAL FLUCTUATIONS:1||MIXED STATE:1||BI2.15SR1.85CACU2O8+DELTA:1||intrinsic Josephson effects:1||CACUO:1||QUANTUM POINT CONTACTS:1||resonant tunneling state:1||coherence length:1||NANOWIRE:1||GATES:1||Phase line:1||Thermal activation:1||QUANTUMDOT:1||superconducting proximity effect:1||Andreev interferometer:1||WIRE:1||Josephsonvortexflow branches:1||Bi2212 cuprates:1||LATTICE:1||demannetization effect:1||SUPERCONDUCTING MIRRORS:1||GAS:1||VALLEY TRANSPORT:1||ELECTRODES:1||DEPENDENT TRANSPORT:1||BORNOPPENHEIMER APPROXIMATION:1||collective plasma oscillations:1||fluxon resonance steps:1||STACKS:1||COLLECTIVE DYNAMICS:1||PAIRING SYMMETRY:1||MUON SPIN ROTATION:1||DIMENSIONAL CROSSOVER:1||Bi2Sr2CaCu2Oy highTc superconductors:1||heterojunctions:1||nanostructures:1||surfaces and interfaces:1||QUANTUM TRANSPORT:1||MICROJUNCTIONS:1||RESONATORS:1||STATES:1||FIELD:1||FLUCTUATIONS:1||SCATTERING:1||mode splitting of Josephson vortexflow branches:1||2D superconductivity:1||TRANSISTOR:1||ENERGYGAP:1||SUPERLATTICES:1||IRONBASED SUPERCONDUCTORS:1||PHASEDEPENDENT RESISTANCE:1||QUANTUM PHASETRANSITIONS:1||ELECTRICFIELD:1||HIGH MAGNETICFIELDS:1||NANOWIRE HETEROSTRUCTURES:1||ZNO:1||pair breaking.:1||SUPERCONDUCTING PB:1||domain formation:1||FORCE MICROSCOPY:1||RELAXATION:1||PLASMA RESONANCE:1||coupled Josephson junctions:1||COPPEROXIDE SUPERCONDUCTORS:1||CROSSOVER:1||SIMULATIONS:1||LOWTEMPERATURE:1||CONDUCTORS:1||METALINSULATORTRANSITION:1||SEMICONDUCTOR:1||FIELDEFFECT TRANSISTORS:1||ZEROVOLTAGE STATE:1||constanttemperature interlayer tunneling spectroscopy:1||Josephson supercurrent:1||BIPOLAR SUPERCURRENT:1||Interaction between Josephson and pancake vortices:1||flux jump:1||coaxial heterojunction nanorod:1||Natural Josephson coupling:1||BI2SR2CACU2O8+DELTA:1||VORTEX FLOW:1||TC SUPERCONDUCTORS:1||charge imbalance:1||Andreev diffractometer:1||intercalation:1||surface junction:1||Bi2212:1||tunnelling:1||GRAPHITE:1||GROWTH:1||collective transverse plasma modes:1||GAN:1||Macroscopic quantum tunneling:1||Fluctuation conductivity:1||Abovegap conductance jump:1||Josephson vortex motion:1||Intrinsic Josephson junctions:1||LAYERED SUPERCONDUCTORS:1||BI2SR2CACU2O8+Y:1||INTERFACES:1||BREAKDOWN:1||SYSTEMS:1||Anisotropy ratio:1||Josephson vortex:1||spin relaxation in superconductors:1||bibased single crystals:1||MESOSCOPIC PROXIMITY SUPERCONDUCTOR:1||reentrance of conductance:1||interlayer pair tunneling:1||JOSEPHSON:1||DISORDERED 2DIMENSIONAL SUPERCONDUCTORS:1||INDIUM FILMS:1||excited state:1||REGIME:1||triplet superconductivity:1||FILM:1||SCHOTTKY DIODES:1||peakdiphump structure:1||Kondo effect:1||REENTRANCE:1||Graphene:1||CONTACT:1||BERRYS PHASE:1||2DIMENSIONAL SUPERCONDUCTORS:1||Coulomb diamond:1||magnetic domain:1||spin injection:1||RESONANCE:1||plasma excitation modes:1||FLOW:1||OVERDOPED BI2SR2CACU2O8+DELTA:1||hole doping:1||chemical synthesis:1||phase transitions:1||superconductors:1||VORTEXGLASS SUPERCONDUCTIVITY:1||Kondorelated model:1||RADIATION:1||DOT:1||NANOBELTS:1||Complementarity:1||Closedloop AharonovBohm interferometer:1||pair breaking:1||interlayer phase fluctuation:1||MgB2 thin film:1||CONFINEMENT:1||WALLED CARBON NANOTUBES:1||TRANSITION:9||VORTICES:8||STATE:7||intrinsic Josephson junctions:7||SINGLECRYSTALS:7||JUNCTIONS:5||MODES:5||SUPERCURRENT:5||SUPERCONDUCTOR:5||CONDUCTANCE:5||HIGHTEMPERATURE SUPERCONDUCTORS:5||TRANSPORT:5||PHASE:5||FILMS:4||LOCALIZATION:4||SINGLE DIRAC CONE:4||WIRES:4||MAGNETICFIELD:4||STEPS:3||ELECTRONS:3||proximity effect:3||MODEL:3||ARRAYS:3||INTERFERENCE:3||fluxon dynamics:3||HETEROSTRUCTURES:3||INSULATOR:3||Andreev reflection:3||electronic transport:3||FISKE:3||superconductor:2||ZnO:2||quantum point contact:2||METAL:2||DYNAMICS:2||interlayer Josephson coupling:2||SUPERCONDUCTORS:2||YBA2CU3O7DELTA:2||LAYER:2||DOTS:2||quantum dot:2||Article:2||TRANSISTORS:2||CARBON NANOTUBES:2||GAP:2||MECHANISM:2||LINE:2||GIANT SHAPIRO STEPS:2||LAYERS:2||electron energy loss spectroscopy:2||physical phenomena:2||scanning electron microscopy:2||HGTE QUANTUMWELLS:2||BI2TE3:2||SPECTROSCOPY:2||PNJUNCTIONS:2||spinpolarized tunneling:2||INTRINSIC JOSEPHSONJUNCTIONS:2||FIELDS:2||positive magnetoresistance:2||dilute magnetic semiconductor:2||magnetic field:2||scanning transmission electron microscopy:2||QUANTUM OSCILLATIONS:2||TRANSPORTPROPERTIES:2||surface pair current:2||MAGNETORESISTANCE:2||NANORIBBONS:2||INSTABILITY:2||ANDREEV REFLECTION:2||microwave irradiation:2||vertical graphene josephson junction:2||BI2SE3:2||CONDUCTIVITY:2||highTc superconductors:2||DIMENSIONAL ELECTRONGAS:2||graphene:2||Topological insulators:2||Josephson coupling Fraunhofer interference pattern:2||FERROMAGNET:2||DEPENDENCE:2||DETECTOR:2||COHERENCE:2||INJECTION:2||GRAPHENE:1||JOSEPHSONJUNCTIONS:1||LAYERED SUPERCONDUCTOR:1||mode splitting:1||BEHAVIOR:1||spinpolarized transport:1||SUPERCONDUCTING TRANSITION:1||microwave response:1||PSEUDOGAP:1||phase coherence:1||TRANSITIONS:1||Long Josephson junction:1||Charge detection:1||collective resonance modes:1||plasma oscillation modes:1||Superconducting proximity effect:1||Iron pnictide superconductor:1||McMillanRowell oscillations:1||ferromagnetic microstructure:1||superradiant state:1||VOLTAGE:1||branch splitting:1||TENSOR:1||INTERCALATION:1||insitu fabrication:1||NDGAO3:1||DISORDERED METALS:1||GAUGE GLASS:1||LOWTEMPERATURE TRANSPORT:1||spontaneous spin polarization model:1||BIAS:1||emission of electromagnetic waves:1||YBA2CU3O7/PRBA2CU3O7 SUPERLATTICES:1||BOHM:1||SHAPIRO STEPS:1||superconductor/ferromagnet interface:1||OXIDE:1||ANDREEVREFLECTION:1||SinFeAsO single crystal:1||COLLECTIVE MOTION:1||ANGULARDEPENDENCE:1||SUPERCONDUCTIVITY:1||BILAYER GRAPHENE:1||PHOTOLUMINESCENT PROPERTIES:1||SUPERCONDUCTING WEAK LINKS:1||intrinsic Josephson junctions geometrical resonance:1||intrinsic Josephson junction:1||MESOSCOPIC SPINVALVE:1||Bi2212 single crystals:1||intrinsic junctions:1||ANDREEV REFLECTIONS:1||normalmetal/superconductor interface:1||IBI2SR2CACU2OY:1||THERMAL FLUCTUATIONS:1||MIXED STATE:1||BI2.15SR1.85CACU2O8+DELTA:1||intrinsic Josephson effects:1||CACUO:1||QUANTUM POINT CONTACTS:1||resonant tunneling state:1||coherence length:1||NANOWIRE:1||GATES:1||Phase line:1||Thermal activation:1||QUANTUMDOT:1||superconducting proximity effect:1||Andreev interferometer:1||WIRE:1||Josephsonvortexflow branches:1||Bi2212 cuprates:1||LATTICE:1||demannetization effect:1||SUPERCONDUCTING MIRRORS:1||GAS:1||VALLEY TRANSPORT:1||ELECTRODES:1||DEPENDENT TRANSPORT:1||BORNOPPENHEIMER APPROXIMATION:1||collective plasma oscillations:1||fluxon resonance steps:1||STACKS:1||COLLECTIVE DYNAMICS:1||PAIRING SYMMETRY:1||MUON SPIN ROTATION:1||DIMENSIONAL CROSSOVER:1||Bi2Sr2CaCu2Oy highTc superconductors:1||heterojunctions:1||nanostructures:1||surfaces and interfaces:1||QUANTUM TRANSPORT:1||MICROJUNCTIONS:1||RESONATORS:1||STATES:1||FIELD:1||FLUCTUATIONS:1||SCATTERING:1||mode splitting of Josephson vortexflow branches:1||2D superconductivity:1||TRANSISTOR:1||ENERGYGAP:1||SUPERLATTICES:1||IRONBASED SUPERCONDUCTORS:1||PHASEDEPENDENT RESISTANCE:1||QUANTUM PHASETRANSITIONS:1||ELECTRICFIELD:1||HIGH MAGNETICFIELDS:1||NANOWIRE HETEROSTRUCTURES:1||ZNO:1||pair breaking.:1||SUPERCONDUCTING PB:1||domain formation:1||FORCE MICROSCOPY:1||RELAXATION:1||PLASMA RESONANCE:1||coupled Josephson junctions:1||COPPEROXIDE SUPERCONDUCTORS:1||CROSSOVER:1||SIMULATIONS:1||LOWTEMPERATURE:1||CONDUCTORS:1||METALINSULATORTRANSITION:1||SEMICONDUCTOR:1||FIELDEFFECT TRANSISTORS:1||ZEROVOLTAGE STATE:1||constanttemperature interlayer tunneling spectroscopy:1||Josephson supercurrent:1||BIPOLAR SUPERCURRENT:1||Interaction between Josephson and pancake vortices:1||flux jump:1||coaxial heterojunction nanorod:1||Natural Josephson coupling:1||BI2SR2CACU2O8+DELTA:1||VORTEX FLOW:1||TC SUPERCONDUCTORS:1||charge imbalance:1||Andreev diffractometer:1||intercalation:1||surface junction:1||Bi2212:1||tunnelling:1||GRAPHITE:1||GROWTH:1||collective transverse plasma modes:1||GAN:1||Macroscopic quantum tunneling:1||Fluctuation conductivity:1||Abovegap conductance jump:1||Josephson vortex motion:1||Intrinsic Josephson junctions:1||LAYERED SUPERCONDUCTORS:1||BI2SR2CACU2O8+Y:1||INTERFACES:1||BREAKDOWN:1||SYSTEMS:1||Anisotropy ratio:1||Josephson vortex:1||spin relaxation in superconductors:1||bibased single crystals:1||MESOSCOPIC PROXIMITY SUPERCONDUCTOR:1||reentrance of conductance:1||interlayer pair tunneling:1||JOSEPHSON:1||DISORDERED 2DIMENSIONAL SUPERCONDUCTORS:1||INDIUM FILMS:1||excited state:1||REGIME:1||triplet superconductivity:1||FILM:1||SCHOTTKY DIODES:1||peakdiphump structure:1||Kondo effect:1||REENTRANCE:1||Graphene:1||CONTACT:1||BERRYS PHASE:1||2DIMENSIONAL SUPERCONDUCTORS:1||Coulomb diamond:1||magnetic domain:1||spin injection:1||RESONANCE:1||plasma excitation modes:1||FLOW:1||OVERDOPED BI2SR2CACU2O8+DELTA:1||hole doping:1||chemical synthesis:1||phase transitions:1||superconductors:1||VORTEXGLASS SUPERCONDUCTIVITY:1||Kondorelated model:1||RADIATION:1||DOT:1||NANOBELTS:1||Complementarity:1||Closedloop AharonovBohm interferometer:1||pair breaking:1||interlayer phase fluctuation:1||MgB2 thin film:1||CONFINEMENT:1||WALLED CARBON NANOTUBES:1||TRANSITION:9||VORTICES:8||STATE:7||intrinsic Josephson junctions:7||SINGLECRYSTALS:7||JUNCTIONS:5||MODES:5||SUPERCURRENT:5||SUPERCONDUCTOR:5||CONDUCTANCE:5||HIGHTEMPERATURE SUPERCONDUCTORS:5||TRANSPORT:5||PHASE:5||FILMS:4||LOCALIZATION:4||SINGLE DIRAC CONE:4||WIRES:4||MAGNETICFIELD:4||STEPS:3||ELECTRONS:3||proximity effect:3||MODEL:3||ARRAYS:3||INTERFERENCE:3||fluxon dynamics:3||HETEROSTRUCTURES:3||INSULATOR:3||Andreev reflection:3||electronic transport:3||FISKE:3||superconductor:2||ZnO:2||quantum point contact:2||METAL:2||DYNAMICS:2||interlayer Josephson coupling:2||SUPERCONDUCTORS:2||YBA2CU3O7DELTA:2||LAYER:2||DOTS:2||quantum dot:2||Article:2||TRANSISTORS:2||CARBON NANOTUBES:2||GAP:2||MECHANISM:2||LINE:2||GIANT SHAPIRO STEPS:2||LAYERS:2||electron energy loss spectroscopy:2||physical phenomena:2||scanning electron microscopy:2||HGTE QUANTUMWELLS:2||BI2TE3:2||SPECTROSCOPY:2||PNJUNCTIONS:2||spinpolarized tunneling:2||INTRINSIC JOSEPHSONJUNCTIONS:2||FIELDS:2||positive magnetoresistance:2||dilute magnetic semiconductor:2||magnetic field:2||scanning transmission electron microscopy:2||QUANTUM OSCILLATIONS:2||TRANSPORTPROPERTIES:2||surface pair current:2||MAGNETORESISTANCE:2||NANORIBBONS:2||INSTABILITY:2||ANDREEV REFLECTION:2||microwave irradiation:2||vertical graphene josephson junction:2||BI2SE3:2||CONDUCTIVITY:2||highTc superconductors:2||DIMENSIONAL ELECTRONGAS:2||graphene:2||Topological insulators:2||Josephson coupling Fraunhofer interference pattern:2||FERROMAGNET:2||DEPENDENCE:2||DETECTOR:2||COHERENCE:2||INJECTION:2||GRAPHENE:1||JOSEPHSONJUNCTIONS:1||LAYERED SUPERCONDUCTOR:1||mode splitting:1||BEHAVIOR:1||spinpolarized transport:1||SUPERCONDUCTING TRANSITION:1||microwave response:1||PSEUDOGAP:1||phase coherence:1||TRANSITIONS:1||Long Josephson junction:1||Charge detection:1||collective resonance modes:1||plasma oscillation modes:1||Superconducting proximity effect:1||Iron pnictide superconductor:1||McMillanRowell oscillations:1||ferromagnetic microstructure:1||superradiant state:1||VOLTAGE:1||branch splitting:1||TENSOR:1||INTERCALATION:1||insitu fabrication:1||NDGAO3:1||DISORDERED METALS:1||GAUGE GLASS:1||LOWTEMPERATURE TRANSPORT:1||spontaneous spin polarization model:1||BIAS:1||emission of electromagnetic waves:1||YBA2CU3O7/PRBA2CU3O7 SUPERLATTICES:1||BOHM:1||SHAPIRO STEPS:1||superconductor/ferromagnet interface:1||OXIDE:1||ANDREEVREFLECTION:1||SinFeAsO single crystal:1||COLLECTIVE MOTION:1||ANGULARDEPENDENCE:1||SUPERCONDUCTIVITY:1||BILAYER GRAPHENE:1||PHOTOLUMINESCENT PROPERTIES:1||SUPERCONDUCTING WEAK LINKS:1||intrinsic Josephson junctions geometrical resonance:1||intrinsic Josephson junction:1||MESOSCOPIC SPINVALVE:1||Bi2212 single crystals:1||intrinsic junctions:1||ANDREEV REFLECTIONS:1||normalmetal/superconductor interface:1||IBI2SR2CACU2OY:1||THERMAL FLUCTUATIONS:1||MIXED STATE:1||BI2.15SR1.85CACU2O8+DELTA:1||intrinsic Josephson effects:1||CACUO:1||QUANTUM POINT CONTACTS:1||resonant tunneling state:1||coherence length:1||NANOWIRE:1||GATES:1||Phase line:1||Thermal activation:1||QUANTUMDOT:1||superconducting proximity effect:1||Andreev interferometer:1||WIRE:1||Josephsonvortexflow branches:1||Bi2212 cuprates:1||LATTICE:1||demannetization effect:1||SUPERCONDUCTING MIRRORS:1||GAS:1||VALLEY TRANSPORT:1||ELECTRODES:1||DEPENDENT TRANSPORT:1||BORNOPPENHEIMER APPROXIMATION:1||collective plasma oscillations:1||fluxon resonance steps:1||STACKS:1||COLLECTIVE DYNAMICS:1||PAIRING SYMMETRY:1||MUON SPIN ROTATION:1||DIMENSIONAL CROSSOVER:1||Bi2Sr2CaCu2Oy highTc superconductors:1||heterojunctions:1||nanostructures:1||surfaces and interfaces:1||QUANTUM TRANSPORT:1||MICROJUNCTIONS:1||RESONATORS:1||STATES:1||FIELD:1||FLUCTUATIONS:1||SCATTERING:1||mode splitting of Josephson vortexflow branches:1||2D superconductivity:1||TRANSISTOR:1||ENERGYGAP:1||SUPERLATTICES:1||IRONBASED SUPERCONDUCTORS:1||PHASEDEPENDENT RESISTANCE:1||QUANTUM PHASETRANSITIONS:1||ELECTRICFIELD:1||HIGH MAGNETICFIELDS:1||NANOWIRE HETEROSTRUCTURES:1||ZNO:1||pair breaking.:1||SUPERCONDUCTING PB:1||domain formation:1||FORCE MICROSCOPY:1||RELAXATION:1||PLASMA RESONANCE:1||coupled Josephson junctions:1||COPPEROXIDE SUPERCONDUCTORS:1||CROSSOVER:1||SIMULATIONS:1||LOWTEMPERATURE:1||CONDUCTORS:1||METALINSULATORTRANSITION:1||SEMICONDUCTOR:1||FIELDEFFECT TRANSISTORS:1||ZEROVOLTAGE STATE:1||constanttemperature interlayer tunneling spectroscopy:1||Josephson supercurrent:1||BIPOLAR SUPERCURRENT:1||Interaction between Josephson and pancake vortices:1||flux jump:1||coaxial heterojunction nanorod:1||Natural Josephson coupling:1||BI2SR2CACU2O8+DELTA:1||VORTEX FLOW:1||TC SUPERCONDUCTORS:1||charge imbalance:1||Andreev diffractometer:1||intercalation:1||surface junction:1||Bi2212:1||tunnelling:1||GRAPHITE:1||GROWTH:1||collective transverse plasma modes:1||GAN:1||Macroscopic quantum tunneling:1||Fluctuation conductivity:1||Abovegap conductance jump:1||Josephson vortex motion:1||Intrinsic Josephson junctions:1||LAYERED SUPERCONDUCTORS:1||BI2SR2CACU2O8+Y:1||INTERFACES:1||BREAKDOWN:1||SYSTEMS:1||Anisotropy ratio:1||Josephson vortex:1||spin relaxation in superconductors:1||bibased single crystals:1||MESOSCOPIC PROXIMITY SUPERCONDUCTOR:1||reentrance of conductance:1||interlayer pair tunneling:1||JOSEPHSON:1||DISORDERED 2DIMENSIONAL SUPERCONDUCTORS:1||INDIUM FILMS:1||excited state:1||REGIME:1||triplet superconductivity:1||FILM:1||SCHOTTKY DIODES:1||peakdiphump structure:1||Kondo effect:1||REENTRANCE:1||Graphene:1||CONTACT:1||BERRYS PHASE:1||2DIMENSIONAL SUPERCONDUCTORS:1||Coulomb diamond:1||magnetic domain:1||spin injection:1||RESONANCE:1||plasma excitation modes:1||FLOW:1||OVERDOPED BI2SR2CACU2O8+DELTA:1||hole doping:1||chemical synthesis:1||phase transitions:1||superconductors:1||VORTEXGLASS SUPERCONDUCTIVITY:1||Kondorelated model:1||RADIATION:1||DOT:1||NANOBELTS:1||Complementarity:1||Closedloop AharonovBohm interferometer:1||pair breaking:1||interlayer phase fluctuation:1||MgB2 thin film:1||CONFINEMENT:1||WALLED CARBON NANOTUBES:1||TRANSITION:9||VORTICES:8||STATE:7||intrinsic Josephson junctions:7||SINGLECRYSTALS:7||JUNCTIONS:5||MODES:5||SUPERCURRENT:5||SUPERCONDUCTOR:5||CONDUCTANCE:5||HIGHTEMPERATURE SUPERCONDUCTORS:5||TRANSPORT:5||PHASE:5||FILMS:4||LOCALIZATION:4||SINGLE DIRAC CONE:4||WIRES:4||MAGNETICFIELD:4||STEPS:3||ELECTRONS:3||proximity effect:3||MODEL:3||ARRAYS:3||INTERFERENCE:3||fluxon dynamics:3||HETEROSTRUCTURES:3||INSULATOR:3||Andreev reflection:3||electronic transport:3||FISKE:3||superconductor:2||ZnO:2||quantum point contact:2||METAL:2||DYNAMICS:2||interlayer Josephson coupling:2||SUPERCONDUCTORS:2||YBA2CU3O7DELTA:2||LAYER:2||DOTS:2||quantum dot:2||Article:2||TRANSISTORS:2||CARBON NANOTUBES:2||GAP:2||MECHANISM:2||LINE:2||GIANT SHAPIRO STEPS:2||LAYERS:2||electron energy loss spectroscopy:2||physical phenomena:2||scanning electron microscopy:2||HGTE QUANTUMWELLS:2||BI2TE3:2||SPECTROSCOPY:2||PNJUNCTIONS:2||spinpolarized tunneling:2||INTRINSIC JOSEPHSONJUNCTIONS:2||FIELDS:2||positive magnetoresistance:2||dilute magnetic semiconductor:2||magnetic field:2||scanning transmission electron microscopy:2||QUANTUM OSCILLATIONS:2||TRANSPORTPROPERTIES:2||surface pair current:2||MAGNETORESISTANCE:2||NANORIBBONS:2||INSTABILITY:2||ANDREEV REFLECTION:2||microwave irradiation:2||vertical graphene josephson junction:2||BI2SE3:2||CONDUCTIVITY:2||highTc superconductors:2||DIMENSIONAL ELECTRONGAS:2||graphene:2||Topological insulators:2||Josephson coupling Fraunhofer interference pattern:2||FERROMAGNET:2||DEPENDENCE:2||DETECTOR:2||COHERENCE:2||INJECTION:2||GRAPHENE:1||JOSEPHSONJUNCTIONS:1||LAYERED SUPERCONDUCTOR:1||mode splitting:1||BEHAVIOR:1||spinpolarized transport:1||SUPERCONDUCTING TRANSITION:1||microwave response:1||PSEUDOGAP:1||phase coherence:1||TRANSITIONS:1||Long Josephson junction:1||Charge detection:1||collective resonance modes:1||plasma oscillation modes:1||Superconducting proximity effect:1||Iron pnictide superconductor:1||McMillanRowell oscillations:1||ferromagnetic microstructure:1||superradiant state:1||VOLTAGE:1||branch splitting:1||TENSOR:1||INTERCALATION:1||insitu fabrication:1||NDGAO3:1||DISORDERED METALS:1||GAUGE GLASS:1||LOWTEMPERATURE TRANSPORT:1||spontaneous spin polarization model:1||BIAS:1||emission of electromagnetic waves:1||YBA2CU3O7/PRBA2CU3O7 SUPERLATTICES:1||BOHM:1||SHAPIRO STEPS:1||superconductor/ferromagnet interface:1||OXIDE:1||ANDREEVREFLECTION:1||SinFeAsO single crystal:1||COLLECTIVE MOTION:1||ANGULARDEPENDENCE:1||SUPERCONDUCTIVITY:1||BILAYER GRAPHENE:1||PHOTOLUMINESCENT PROPERTIES:1||SUPERCONDUCTING WEAK LINKS:1||intrinsic Josephson junctions geometrical resonance:1||intrinsic Josephson junction:1||MESOSCOPIC SPINVALVE:1||Bi2212 single crystals:1||intrinsic junctions:1||ANDREEV REFLECTIONS:1||normalmetal/superconductor interface:1||IBI2SR2CACU2OY:1||THERMAL FLUCTUATIONS:1||MIXED STATE:1||BI2.15SR1.85CACU2O8+DELTA:1||intrinsic Josephson effects:1||CACUO:1||QUANTUM POINT CONTACTS:1||resonant tunneling state:1||coherence length:1||NANOWIRE:1||GATES:1||Phase line:1||Thermal activation:1||QUANTUMDOT:1||superconducting proximity effect:1||Andreev interferometer:1||WIRE:1||Josephsonvortexflow branches:1||Bi2212 cuprates:1||LATTICE:1||demannetization effect:1||SUPERCONDUCTING MIRRORS:1||GAS:1||VALLEY TRANSPORT:1||ELECTRODES:1||DEPENDENT TRANSPORT:1||BORNOPPENHEIMER APPROXIMATION:1||collective plasma oscillations:1||fluxon resonance steps:1||STACKS:1||COLLECTIVE DYNAMICS:1||PAIRING SYMMETRY:1||MUON SPIN ROTATION:1||DIMENSIONAL CROSSOVER:1||Bi2Sr2CaCu2Oy highTc superconductors:1||heterojunctions:1||nanostructures:1||surfaces and interfaces:1||QUANTUM TRANSPORT:1||MICROJUNCTIONS:1||RESONATORS:1||STATES:1||FIELD:1||FLUCTUATIONS:1||SCATTERING:1||mode splitting of Josephson vortexflow branches:1||2D superconductivity:1||TRANSISTOR:1||ENERGYGAP:1||SUPERLATTICES:1||IRONBASED SUPERCONDUCTORS:1||PHASEDEPENDENT RESISTANCE:1||QUANTUM PHASETRANSITIONS:1||ELECTRICFIELD:1||HIGH MAGNETICFIELDS:1||NANOWIRE HETEROSTRUCTURES:1||ZNO:1||pair breaking.:1||SUPERCONDUCTING PB:1||domain formation:1||FORCE MICROSCOPY:1||RELAXATION:1||PLASMA RESONANCE:1||coupled Josephson junctions:1||COPPEROXIDE SUPERCONDUCTORS:1||CROSSOVER:1||SIMULATIONS:1||LOWTEMPERATURE:1||CONDUCTORS:1||METALINSULATORTRANSITION:1||SEMICONDUCTOR:1||FIELDEFFECT TRANSISTORS:1||ZEROVOLTAGE STATE:1||constanttemperature interlayer tunneling spectroscopy:1||Josephson supercurrent:1||BIPOLAR SUPERCURRENT:1||Interaction between Josephson and pancake vortices:1||flux jump:1||coaxial heterojunction nanorod:1||Natural Josephson coupling:1||BI2SR2CACU2O8+DELTA:1||VORTEX FLOW:1||TC SUPERCONDUCTORS:1||charge imbalance:1||Andreev diffractometer:1||intercalation:1||surface junction:1||Bi2212:1||tunnelling:1||GRAPHITE:1||GROWTH:1||collective transverse plasma modes:1||GAN:1||Macroscopic quantum tunneling:1||Fluctuation conductivity:1||Abovegap conductance jump:1||Josephson vortex motion:1||Intrinsic Josephson junctions:1||LAYERED SUPERCONDUCTORS:1||BI2SR2CACU2O8+Y:1||INTERFACES:1||BREAKDOWN:1||SYSTEMS:1||Anisotropy ratio:1||Josephson vortex:1||spin relaxation in superconductors:1||bibased single crystals:1||MESOSCOPIC PROXIMITY SUPERCONDUCTOR:1||reentrance of conductance:1||interlayer pair tunneling:1||JOSEPHSON:1||DISORDERED 2DIMENSIONAL SUPERCONDUCTORS:1||INDIUM FILMS:1||excited state:1||REGIME:1||triplet superconductivity:1||FILM:1||SCHOTTKY DIODES:1||peakdiphump structure:1||Kondo effect:1||REENTRANCE:1||Graphene:1||CONTACT:1||BERRYS PHASE:1||2DIMENSIONAL SUPERCONDUCTORS:1||Coulomb diamond:1||magnetic domain:1||spin injection:1||RESONANCE:1||plasma excitation modes:1||FLOW:1||OVERDOPED BI2SR2CACU2O8+DELTA:1||hole doping:1||chemical synthesis:1||phase transitions:1||superconductors:1||VORTEXGLASS SUPERCONDUCTIVITY:1||Kondorelated model:1||RADIATION:1||DOT:1||NANOBELTS:1||Complementarity:1||Closedloop AharonovBohm interferometer:1||pair breaking:1||interlayer phase fluctuation:1||MgB2 thin film:1||CONFINEMENT:1||WALLED CARBON NANOTUBES:1||TRANSITION:9||VORTICES:8||STATE:7||intrinsic Josephson junctions:7||SINGLECRYSTALS:7||JUNCTIONS:5||MODES:5||SUPERCURRENT:5||SUPERCONDUCTOR:5||CONDUCTANCE:5||HIGHTEMPERATURE SUPERCONDUCTORS:5||TRANSPORT:5||PHASE:5||FILMS:4||LOCALIZATION:4||SINGLE DIRAC CONE:4||WIRES:4||MAGNETICFIELD:4||STEPS:3||ELECTRONS:3||proximity effect:3||MODEL:3||ARRAYS:3||INTERFERENCE:3||fluxon dynamics:3||HETEROSTRUCTURES:3||INSULATOR:3||Andreev reflection:3||electronic transport:3||FISKE:3||superconductor:2||ZnO:2||quantum point contact:2||METAL:2||DYNAMICS:2||interlayer Josephson coupling:2||SUPERCONDUCTORS:2||YBA2CU3O7DELTA:2||LAYER:2||DOTS:2||quantum dot:2||Article:2||TRANSISTORS:2||CARBON NANOTUBES:2||GAP:2||MECHANISM:2||LINE:2||GIANT SHAPIRO STEPS:2||LAYERS:2||electron energy loss spectroscopy:2||physical phenomena:2||scanning electron microscopy:2||HGTE QUANTUMWELLS:2||BI2TE3:2||SPECTROSCOPY:2||PNJUNCTIONS:2||spinpolarized tunneling:2||INTRINSIC JOSEPHSONJUNCTIONS:2||FIELDS:2||positive magnetoresistance:2||dilute magnetic semiconductor:2||magnetic field:2||scanning transmission electron microscopy:2||QUANTUM OSCILLATIONS:2||TRANSPORTPROPERTIES:2||surface pair current:2||MAGNETORESISTANCE:2||NANORIBBONS:2||INSTABILITY:2||ANDREEV REFLECTION:2||microwave irradiation:2||vertical graphene josephson junction:2||BI2SE3:2||CONDUCTIVITY:2||highTc superconductors:2||DIMENSIONAL ELECTRONGAS:2||graphene:2||Topological insulators:2||Josephson coupling Fraunhofer interference pattern:2||FERROMAGNET:2||DEPENDENCE:2||DETECTOR:2||COHERENCE:2||INJECTION:2||GRAPHENE:1||JOSEPHSONJUNCTIONS:1||LAYERED SUPERCONDUCTOR:1||mode splitting:1||BEHAVIOR:1||spinpolarized transport:1||SUPERCONDUCTING TRANSITION:1||microwave response:1||PSEUDOGAP:1||phase coherence:1||TRANSITIONS:1||Long Josephson junction:1||Charge detection:1||collective resonance modes:1||plasma oscillation modes:1||Superconducting proximity effect:1||Iron pnictide superconductor:1||McMillanRowell oscillations:1||ferromagnetic microstructure:1||superradiant state:1||VOLTAGE:1||branch splitting:1||TENSOR:1||INTERCALATION:1||insitu fabrication:1||NDGAO3:1||DISORDERED METALS:1||GAUGE GLASS:1||LOWTEMPERATURE TRANSPORT:1||spontaneous spin polarization model:1||BIAS:1||emission of electromagnetic waves:1||YBA2CU3O7/PRBA2CU3O7 SUPERLATTICES:1||BOHM:1||SHAPIRO STEPS:1||superconductor/ferromagnet interface:1||OXIDE:1||ANDREEVREFLECTION:1||SinFeAsO single crystal:1||COLLECTIVE MOTION:1||ANGULARDEPENDENCE:1||SUPERCONDUCTIVITY:1||BILAYER GRAPHENE:1||PHOTOLUMINESCENT PROPERTIES:1||SUPERCONDUCTING WEAK LINKS:1||intrinsic Josephson junctions geometrical resonance:1||intrinsic Josephson junction:1||MESOSCOPIC SPINVALVE:1||Bi2212 single crystals:1||intrinsic junctions:1||ANDREEV REFLECTIONS:1||normalmetal/superconductor interface:1||IBI2SR2CACU2OY:1||THERMAL FLUCTUATIONS:1||MIXED STATE:1||BI2.15SR1.85CACU2O8+DELTA:1||intrinsic Josephson effects:1||CACUO:1||QUANTUM POINT CONTACTS:1||resonant tunneling state:1||coherence length:1||NANOWIRE:1||GATES:1||Phase line:1||Thermal activation:1||QUANTUMDOT:1||superconducting proximity effect:1||Andreev interferometer:1||WIRE:1||Josephsonvortexflow branches:1||Bi2212 cuprates:1||LATTICE:1||demannetization effect:1||SUPERCONDUCTING MIRRORS:1||GAS:1||VALLEY TRANSPORT:1||ELECTRODES:1||DEPENDENT TRANSPORT:1||BORNOPPENHEIMER APPROXIMATION:1||collective plasma oscillations:1||fluxon resonance steps:1||STACKS:1||COLLECTIVE DYNAMICS:1||PAIRING SYMMETRY:1||MUON SPIN ROTATION:1||DIMENSIONAL CROSSOVER:1||Bi2Sr2CaCu2Oy highTc superconductors:1||heterojunctions:1||nanostructures:1||surfaces and interfaces:1||QUANTUM TRANSPORT:1||MICROJUNCTIONS:1||RESONATORS:1||STATES:1||FIELD:1||FLUCTUATIONS:1||SCATTERING:1||mode splitting of Josephson vortexflow branches:1||2D superconductivity:1||TRANSISTOR:1||ENERGYGAP:1||SUPERLATTICES:1||IRONBASED SUPERCONDUCTORS:1||PHASEDEPENDENT RESISTANCE:1||QUANTUM PHASETRANSITIONS:1||ELECTRICFIELD:1||HIGH MAGNETICFIELDS:1||NANOWIRE HETEROSTRUCTURES:1||ZNO:1||pair breaking.:1||SUPERCONDUCTING PB:1||domain formation:1||FORCE MICROSCOPY:1||RELAXATION:1||PLASMA RESONANCE:1||coupled Josephson junctions:1||COPPEROXIDE SUPERCONDUCTORS:1||CROSSOVER:1||SIMULATIONS:1||LOWTEMPERATURE:1||CONDUCTORS:1||METALINSULATORTRANSITION:1||SEMICONDUCTOR:1||FIELDEFFECT TRANSISTORS:1||ZEROVOLTAGE STATE:1||constanttemperature interlayer tunneling spectroscopy:1||Josephson supercurrent:1||BIPOLAR SUPERCURRENT:1||Interaction between Josephson and pancake vortices:1||flux jump:1||coaxial heterojunction nanorod:1||Natural Josephson coupling:1||BI2SR2CACU2O8+DELTA:1||VORTEX FLOW:1||TC SUPERCONDUCTORS:1||charge imbalance:1||Andreev diffractometer:1||intercalation:1||surface junction:1||Bi2212:1||tunnelling:1||GRAPHITE:1||GROWTH:1||collective transverse plasma modes:1||GAN:1||Macroscopic quantum tunneling:1||Fluctuation conductivity:1||Abovegap conductance jump:1||Josephson vortex motion:1||Intrinsic Josephson junctions:1||LAYERED SUPERCONDUCTORS:1||BI2SR2CACU2O8+Y:1||INTERFACES:1||BREAKDOWN:1||SYSTEMS:1||Anisotropy ratio:1||Josephson vortex:1||spin relaxation in superconductors:1||bibased single crystals:1||MESOSCOPIC PROXIMITY SUPERCONDUCTOR:1||reentrance of conductance:1||interlayer pair tunneling:1||JOSEPHSON:1||DISORDERED 2DIMENSIONAL SUPERCONDUCTORS:1||INDIUM FILMS:1||excited state:1||REGIME:1||triplet superconductivity:1||FILM:1||SCHOTTKY DIODES:1||peakdiphump structure:1||Kondo effect:1||REENTRANCE:1||Graphene:1||CONTACT:1||BERRYS PHASE:1||2DIMENSIONAL SUPERCONDUCTORS:1||Coulomb diamond:1||magnetic domain:1||spin injection:1||RESONANCE:1||plasma excitation modes:1||FLOW:1||OVERDOPED BI2SR2CACU2O8+DELTA:1||hole doping:1||chemical synthesis:1||phase transitions:1||superconductors:1||VORTEXGLASS SUPERCONDUCTIVITY:1||Kondorelated model:1||RADIATION:1||DOT:1||NANOBELTS:1||Complementarity:1||Closedloop AharonovBohm interferometer:1||pair breaking:1||interlayer phase fluctuation:1||MgB2 thin film:1||CONFINEMENT:1||WALLED CARBON NANOTUBES:1||TRANSITION:9||VORTICES:8||STATE:7||intrinsic Josephson junctions:7||SINGLECRYSTALS:7||JUNCTIONS:5||MODES:5||SUPERCURRENT:5||SUPERCONDUCTOR:5||CONDUCTANCE:5||HIGHTEMPERATURE SUPERCONDUCTORS:5||TRANSPORT:5||PHASE:5||FILMS:4||LOCALIZATION:4||SINGLE DIRAC CONE:4||WIRES:4||MAGNETICFIELD:4||STEPS:3||ELECTRONS:3||proximity effect:3||MODEL:3||ARRAYS:3||INTERFERENCE:3||fluxon dynamics:3||HETEROSTRUCTURES:3||INSULATOR:3||Andreev reflection:3||electronic transport:3||FISKE:3||superconductor:2||ZnO:2||quantum point contact:2||METAL:2||DYNAMICS:2||interlayer Josephson coupling:2||SUPERCONDUCTORS:2||YBA2CU3O7DELTA:2||LAYER:2||DOTS:2||quantum dot:2||Article:2||TRANSISTORS:2||CARBON NANOTUBES:2||GAP:2||MECHANISM:2||LINE:2||GIANT SHAPIRO STEPS:2||LAYERS:2||electron energy loss spectroscopy:2||physical phenomena:2||scanning electron microscopy:2||HGTE QUANTUMWELLS:2||BI2TE3:2||SPECTROSCOPY:2||PNJUNCTIONS:2||spinpolarized tunneling:2||INTRINSIC JOSEPHSONJUNCTIONS:2||FIELDS:2||positive magnetoresistance:2||dilute magnetic semiconductor:2||magnetic field:2||scanning transmission electron microscopy:2||QUANTUM OSCILLATIONS:2||TRANSPORTPROPERTIES:2||surface pair current:2||MAGNETORESISTANCE:2||NANORIBBONS:2||INSTABILITY:2||ANDREEV REFLECTION:2||microwave irradiation:2||vertical graphene josephson junction:2||BI2SE3:2||CONDUCTIVITY:2||highTc superconductors:2||DIMENSIONAL ELECTRONGAS:2||graphene:2||Topological insulators:2||Josephson coupling Fraunhofer interference pattern:2||FERROMAGNET:2||DEPENDENCE:2||DETECTOR:2||COHERENCE:2||INJECTION:2||GRAPHENE:1||JOSEPHSONJUNCTIONS:1||LAYERED SUPERCONDUCTOR:1||mode splitting:1||BEHAVIOR:1||spinpolarized transport:1||SUPERCONDUCTING TRANSITION:1||microwave response:1||PSEUDOGAP:1||phase coherence:1||TRANSITIONS:1||Long Josephson junction:1||Charge detection:1||collective resonance modes:1||plasma oscillation modes:1||Superconducting proximity effect:1||Iron pnictide superconductor:1||McMillanRowell oscillations:1||ferromagnetic microstructure:1||superradiant state:1||VOLTAGE:1||branch splitting:1||TENSOR:1||INTERCALATION:1||insitu fabrication:1||NDGAO3:1||DISORDERED METALS:1||GAUGE GLASS:1||LOWTEMPERATURE TRANSPORT:1||spontaneous spin polarization model:1||BIAS:1||emission of electromagnetic waves:1||YBA2CU3O7/PRBA2CU3O7 SUPERLATTICES:1||BOHM:1||SHAPIRO STEPS:1||superconductor/ferromagnet interface:1||OXIDE:1||ANDREEVREFLECTION:1||SinFeAsO single crystal:1||COLLECTIVE MOTION:1||ANGULARDEPENDENCE:1||SUPERCONDUCTIVITY:1||BILAYER GRAPHENE:1||PHOTOLUMINESCENT PROPERTIES:1||SUPERCONDUCTING WEAK LINKS:1||intrinsic Josephson junctions geometrical resonance:1||intrinsic Josephson junction:1||MESOSCOPIC SPINVALVE:1||Bi2212 single crystals:1||intrinsic junctions:1||ANDREEV REFLECTIONS:1||normalmetal/superconductor interface:1||IBI2SR2CACU2OY:1||THERMAL FLUCTUATIONS:1||MIXED STATE:1||BI2.15SR1.85CACU2O8+DELTA:1||intrinsic Josephson effects:1||CACUO:1||QUANTUM POINT CONTACTS:1||resonant tunneling state:1||coherence length:1||NANOWIRE:1||GATES:1||Phase line:1||Thermal activation:1||QUANTUMDOT:1||superconducting proximity effect:1||Andreev interferometer:1||WIRE:1||Josephsonvortexflow branches:1||Bi2212 cuprates:1||LATTICE:1||demannetization effect:1||SUPERCONDUCTING MIRRORS:1||GAS:1||VALLEY TRANSPORT:1||ELECTRODES:1||DEPENDENT TRANSPORT:1||BORNOPPENHEIMER APPROXIMATION:1||collective plasma oscillations:1||fluxon resonance steps:1||STACKS:1||COLLECTIVE DYNAMICS:1||PAIRING SYMMETRY:1||MUON SPIN ROTATION:1||DIMENSIONAL CROSSOVER:1||Bi2Sr2CaCu2Oy highTc superconductors:1||heterojunctions:1||nanostructures:1||surfaces and interfaces:1||QUANTUM TRANSPORT:1||MICROJUNCTIONS:1||RESONATORS:1||STATES:1||FIELD:1||FLUCTUATIONS:1||SCATTERING:1||mode splitting of Josephson vortexflow branches:1||2D superconductivity:1||TRANSISTOR:1||ENERGYGAP:1||SUPERLATTICES:1||IRONBASED SUPERCONDUCTORS:1||PHASEDEPENDENT RESISTANCE:1||QUANTUM PHASETRANSITIONS:1||ELECTRICFIELD:1||HIGH MAGNETICFIELDS:1||NANOWIRE HETEROSTRUCTURES:1||ZNO:1||pair breaking.:1||SUPERCONDUCTING PB:1||domain formation:1||FORCE MICROSCOPY:1||RELAXATION:1||PLASMA RESONANCE:1||coupled Josephson junctions:1||COPPEROXIDE SUPERCONDUCTORS:1||CROSSOVER:1||SIMULATIONS:1||LOWTEMPERATURE:1||CONDUCTORS:1||METALINSULATORTRANSITION:1||SEMICONDUCTOR:1||FIELDEFFECT TRANSISTORS:1||ZEROVOLTAGE STATE:1||constanttemperature interlayer tunneling spectroscopy:1||Josephson supercurrent:1||BIPOLAR SUPERCURRENT:1||Interaction between Josephson and pancake vortices:1||flux jump:1||coaxial heterojunction nanorod:1||Natural Josephson coupling:1||BI2SR2CACU2O8+DELTA:1||VORTEX FLOW:1||TC SUPERCONDUCTORS:1||charge imbalance:1||Andreev diffractometer:1||intercalation:1||surface junction:1||Bi2212:1||tunnelling:1||GRAPHITE:1||GROWTH:1||collective transverse plasma modes:1||GAN:1||Macroscopic quantum tunneling:1||Fluctuation conductivity:1||Abovegap conductance jump:1||Josephson vortex motion:1||Intrinsic Josephson junctions:1||LAYERED SUPERCONDUCTORS:1||BI2SR2CACU2O8+Y:1||INTERFACES:1||BREAKDOWN:1||SYSTEMS:1||Anisotropy ratio:1||Josephson vortex:1||spin relaxation in superconductors:1||bibased single crystals:1||MESOSCOPIC PROXIMITY SUPERCONDUCTOR:1||reentrance of conductance:1||interlayer pair tunneling:1||JOSEPHSON:1||DISORDERED 2DIMENSIONAL SUPERCONDUCTORS:1||INDIUM FILMS:1||excited state:1||REGIME:1||triplet superconductivity:1||FILM:1||SCHOTTKY DIODES:1||peakdiphump structure:1||Kondo effect:1||REENTRANCE:1||Graphene:1||CONTACT:1||BERRYS PHASE:1||2DIMENSIONAL SUPERCONDUCTORS:1||Coulomb diamond:1||magnetic domain:1||spin injection:1||RESONANCE:1||plasma excitation modes:1||FLOW:1||OVERDOPED BI2SR2CACU2O8+DELTA:1||hole doping:1||chemical synthesis:1||phase transitions:1||superconductors:1||VORTEXGLASS SUPERCONDUCTIVITY:1||Kondorelated model:1||RADIATION:1||DOT:1||NANOBELTS:1||Complementarity:1||Closedloop AharonovBohm interferometer:1||pair breaking:1||interlayer phase fluctuation:1||MgB2 thin film:1||CONFINEMENT:1||WALLED CARBON NANOTUBES:1||TRANSITION:9||VORTICES:8||STATE:7||intrinsic Josephson junctions:7||SINGLECRYSTALS:7||JUNCTIONS:5||MODES:5||SUPERCURRENT:5||SUPERCONDUCTOR:5||CONDUCTANCE:5||HIGHTEMPERATURE SUPERCONDUCTORS:5||TRANSPORT:5||PHASE:5||FILMS:4||LOCALIZATION:4||SINGLE DIRAC CONE:4||WIRES:4||MAGNETICFIELD:4||STEPS:3||ELECTRONS:3||proximity effect:3||MODEL:3||ARRAYS:3||INTERFERENCE:3||fluxon dynamics:3||HETEROSTRUCTURES:3||INSULATOR:3||Andreev reflection:3||electronic transport:3||FISKE:3||superconductor:2||ZnO:2||quantum point contact:2||METAL:2||DYNAMICS:2||interlayer Josephson coupling:2||SUPERCONDUCTORS:2||YBA2CU3O7DELTA:2||LAYER:2||DOTS:2||quantum dot:2||Article:2||TRANSISTORS:2||CARBON NANOTUBES:2||GAP:2||MECHANISM:2||LINE:2||GIANT SHAPIRO STEPS:2||LAYERS:2||electron energy loss spectroscopy:2||physical phenomena:2||scanning electron microscopy:2||HGTE QUANTUMWELLS:2||BI2TE3:2||SPECTROSCOPY:2||PNJUNCTIONS:2||spinpolarized tunneling:2||INTRINSIC JOSEPHSONJUNCTIONS:2||FIELDS:2||positive magnetoresistance:2||dilute magnetic semiconductor:2||magnetic field:2||scanning transmission electron microscopy:2||QUANTUM OSCILLATIONS:2||TRANSPORTPROPERTIES:2||surface pair current:2||MAGNETORESISTANCE:2||NANORIBBONS:2||INSTABILITY:2||ANDREEV REFLECTION:2||microwave irradiation:2||vertical graphene josephson junction:2||BI2SE3:2||CONDUCTIVITY:2||highTc superconductors:2||DIMENSIONAL ELECTRONGAS:2||graphene:2||Topological insulators:2||Josephson coupling Fraunhofer interference pattern:2||FERROMAGNET:2||DEPENDENCE:2||DETECTOR:2||COHERENCE:2||INJECTION:2||GRAPHENE:1||JOSEPHSONJUNCTIONS:1||LAYERED SUPERCONDUCTOR:1||mode splitting:1||BEHAVIOR:1||spinpolarized transport:1||SUPERCONDUCTING TRANSITION:1||microwave response:1||PSEUDOGAP:1||phase coherence:1||TRANSITIONS:1||Long Josephson junction:1||Charge detection:1||collective resonance modes:1||plasma oscillation modes:1||Superconducting proximity effect:1||Iron pnictide superconductor:1||McMillanRowell oscillations:1||ferromagnetic microstructure:1||superradiant state:1||VOLTAGE:1||branch splitting:1||TENSOR:1||INTERCALATION:1||insitu fabrication:1||NDGAO3:1||DISORDERED METALS:1||GAUGE GLASS:1||LOWTEMPERATURE TRANSPORT:1||spontaneous spin polarization model:1||BIAS:1||emission of electromagnetic waves:1||YBA2CU3O7/PRBA2CU3O7 SUPERLATTICES:1||BOHM:1||SHAPIRO STEPS:1||superconductor/ferromagnet interface:1||OXIDE:1||ANDREEVREFLECTION:1||SinFeAsO single crystal:1||COLLECTIVE MOTION:1||ANGULARDEPENDENCE:1||SUPERCONDUCTIVITY:1||BILAYER GRAPHENE:1||PHOTOLUMINESCENT PROPERTIES:1||SUPERCONDUCTING WEAK LINKS:1||intrinsic Josephson junctions geometrical resonance:1||intrinsic Josephson junction:1||MESOSCOPIC SPINVALVE:1||Bi2212 single crystals:1||intrinsic junctions:1||ANDREEV REFLECTIONS:1||normalmetal/superconductor interface:1||IBI2SR2CACU2OY:1||THERMAL FLUCTUATIONS:1||MIXED STATE:1||BI2.15SR1.85CACU2O8+DELTA:1||intrinsic Josephson effects:1||CACUO:1||QUANTUM POINT CONTACTS:1||resonant tunneling state:1||coherence length:1||NANOWIRE:1||GATES:1||Phase line:1||Thermal activation:1||QUANTUMDOT:1||superconducting proximity effect:1||Andreev interferometer:1||WIRE:1||Josephsonvortexflow branches:1||Bi2212 cuprates:1||LATTICE:1||demannetization effect:1||SUPERCONDUCTING MIRRORS:1||GAS:1||VALLEY TRANSPORT:1||ELECTRODES:1||DEPENDENT TRANSPORT:1||BORNOPPENHEIMER APPROXIMATION:1||collective plasma oscillations:1||fluxon resonance steps:1||STACKS:1||COLLECTIVE DYNAMICS:1||PAIRING SYMMETRY:1||MUON SPIN ROTATION:1||DIMENSIONAL CROSSOVER:1||Bi2Sr2CaCu2Oy highTc superconductors:1||heterojunctions:1||nanostructures:1||surfaces and interfaces:1||QUANTUM TRANSPORT:1||MICROJUNCTIONS:1||RESONATORS:1||STATES:1||FIELD:1||FLUCTUATIONS:1||SCATTERING:1||mode splitting of Josephson vortexflow branches:1||2D superconductivity:1||TRANSISTOR:1||ENERGYGAP:1||SUPERLATTICES:1||IRONBASED SUPERCONDUCTORS:1||PHASEDEPENDENT RESISTANCE:1||QUANTUM PHASETRANSITIONS:1||ELECTRICFIELD:1||HIGH MAGNETICFIELDS:1||NANOWIRE HETEROSTRUCTURES:1||ZNO:1||pair breaking.:1||SUPERCONDUCTING PB:1||domain formation:1||FORCE MICROSCOPY:1||RELAXATION:1||PLASMA RESONANCE:1||coupled Josephson junctions:1||COPPEROXIDE SUPERCONDUCTORS:1||CROSSOVER:1||SIMULATIONS:1||LOWTEMPERATURE:1||CONDUCTORS:1||METALINSULATORTRANSITION:1||SEMICONDUCTOR:1||FIELDEFFECT TRANSISTORS:1||ZEROVOLTAGE STATE:1||constanttemperature interlayer tunneling spectroscopy:1||Josephson supercurrent:1||BIPOLAR SUPERCURRENT:1||Interaction between Josephson and pancake vortices:1||flux jump:1||coaxial heterojunction nanorod:1||Natural Josephson coupling:1||BI2SR2CACU2O8+DELTA:1||VORTEX FLOW:1||TC SUPERCONDUCTORS:1||charge imbalance:1||Andreev diffractometer:1||intercalation:1||surface junction:1||Bi2212:1||tunnelling:1||GRAPHITE:1||GROWTH:1||collective transverse plasma modes:1||GAN:1||Macroscopic quantum tunneling:1||Fluctuation conductivity:1||Abovegap conductance jump:1||Josephson vortex motion:1||Intrinsic Josephson junctions:1||LAYERED SUPERCONDUCTORS:1||BI2SR2CACU2O8+Y:1||INTERFACES:1||BREAKDOWN:1||SYSTEMS:1||Anisotropy ratio:1||Josephson vortex:1||spin relaxation in superconductors:1||bibased single crystals:1||MESOSCOPIC PROXIMITY SUPERCONDUCTOR:1||reentrance of conductance:1||interlayer pair tunneling:1||JOSEPHSON:1||DISORDERED 2DIMENSIONAL SUPERCONDUCTORS:1||INDIUM FILMS:1||excited state:1||REGIME:1||triplet superconductivity:1||FILM:1||SCHOTTKY DIODES:1||peakdiphump structure:1||Kondo effect:1||REENTRANCE:1||Graphene:1||CONTACT:1||BERRYS PHASE:1||2DIMENSIONAL SUPERCONDUCTORS:1||Coulomb diamond:1||magnetic domain:1||spin injection:1||RESONANCE:1||plasma excitation modes:1||FLOW:1||OVERDOPED BI2SR2CACU2O8+DELTA:1||hole doping:1||chemical synthesis:1||phase transitions:1||superconductors:1||VORTEXGLASS SUPERCONDUCTIVITY:1||Kondorelated model:1||RADIATION:1||DOT:1||NANOBELTS:1||Complementarity:1||Closedloop AharonovBohm interferometer:1||pair breaking:1||interlayer phase fluctuation:1||MgB2 thin film:1||CONFINEMENT:1||WALLED CARBON NANOTUBES:1||TRANSITION:9||VORTICES:8||STATE:7||intrinsic Josephson junctions:7||SINGLECRYSTALS:7||JUNCTIONS:5||MODES:5||SUPERCURRENT:5||SUPERCONDUCTOR:5||CONDUCTANCE:5||HIGHTEMPERATURE SUPERCONDUCTORS:5||TRANSPORT:5||PHASE:5||FILMS:4||LOCALIZATION:4||SINGLE DIRAC CONE:4||WIRES:4||MAGNETICFIELD:4||STEPS:3||ELECTRONS:3||proximity effect:3||MODEL:3||ARRAYS:3||INTERFERENCE:3||fluxon dynamics:3||HETEROSTRUCTURES:3||INSULATOR:3||Andreev reflection:3||electronic transport:3||FISKE:3||superconductor:2||ZnO:2||quantum point contact:2||METAL:2||DYNAMICS:2||interlayer Josephson coupling:2||SUPERCONDUCTORS:2||YBA2CU3O7DELTA:2||LAYER:2||DOTS:2||quantum dot:2||Article:2||TRANSISTORS:2||CARBON NANOTUBES:2||GAP:2||MECHANISM:2||LINE:2||GIANT SHAPIRO STEPS:2||LAYERS:2||electron energy loss spectroscopy:2||physical phenomena:2||scanning electron microscopy:2||HGTE QUANTUMWELLS:2||BI2TE3:2||SPECTROSCOPY:2||PNJUNCTIONS:2||spinpolarized tunneling:2||INTRINSIC JOSEPHSONJUNCTIONS:2||FIELDS:2||positive magnetoresistance:2||dilute magnetic semiconductor:2||magnetic field:2||scanning transmission electron microscopy:2||QUANTUM OSCILLATIONS:2||TRANSPORTPROPERTIES:2||surface pair current:2||MAGNETORESISTANCE:2||NANORIBBONS:2||INSTABILITY:2||ANDREEV REFLECTION:2||microwave irradiation:2||vertical graphene josephson junction:2||BI2SE3:2||CONDUCTIVITY:2||highTc superconductors:2||DIMENSIONAL ELECTRONGAS:2||graphene:2||Topological insulators:2||Josephson coupling Fraunhofer interference pattern:2||FERROMAGNET:2||DEPENDENCE:2||DETECTOR:2||COHERENCE:2||INJECTION:2||GRAPHENE:1||JOSEPHSONJUNCTIONS:1||LAYERED SUPERCONDUCTOR:1||mode splitting:1||BEHAVIOR:1||spinpolarized transport:1||SUPERCONDUCTING TRANSITION:1||microwave response:1||PSEUDOGAP:1||phase coherence:1||TRANSITIONS:1||Long Josephson junction:1||Charge detection:1||collective resonance modes:1||plasma oscillation modes:1||Superconducting proximity effect:1||Iron pnictide superconductor:1||McMillanRowell oscillations:1||ferromagnetic microstructure:1||superradiant state:1||VOLTAGE:1||branch splitting:1||TENSOR:1||INTERCALATION:1||insitu fabrication:1||NDGAO3:1||DISORDERED METALS:1||GAUGE GLASS:1||LOWTEMPERATURE TRANSPORT:1||spontaneous spin polarization model:1||BIAS:1||emission of electromagnetic waves:1||YBA2CU3O7/PRBA2CU3O7 SUPERLATTICES:1||BOHM:1||SHAPIRO STEPS:1||superconductor/ferromagnet interface:1||OXIDE:1||ANDREEVREFLECTION:1||SinFeAsO single crystal:1||COLLECTIVE MOTION:1||ANGULARDEPENDENCE:1||SUPERCONDUCTIVITY:1||BILAYER GRAPHENE:1||PHOTOLUMINESCENT PROPERTIES:1||SUPERCONDUCTING WEAK LINKS:1||intrinsic Josephson junctions geometrical resonance:1||intrinsic Josephson junction:1||MESOSCOPIC SPINVALVE:1||Bi2212 single crystals:1||intrinsic junctions:1||ANDREEV REFLECTIONS:1||normalmetal/superconductor interface:1||IBI2SR2CACU2OY:1||THERMAL FLUCTUATIONS:1||MIXED STATE:1||BI2.15SR1.85CACU2O8+DELTA:1||intrinsic Josephson effects:1||CACUO:1||QUANTUM POINT CONTACTS:1||resonant tunneling state:1||coherence length:1||NANOWIRE:1||GATES:1||Phase line:1||Thermal activation:1||QUANTUMDOT:1||superconducting proximity effect:1||Andreev interferometer:1||WIRE:1||Josephsonvortexflow branches:1||Bi2212 cuprates:1||LATTICE:1||demannetization effect:1||SUPERCONDUCTING MIRRORS:1||GAS:1||VALLEY TRANSPORT:1||ELECTRODES:1||DEPENDENT TRANSPORT:1||BORNOPPENHEIMER APPROXIMATION:1||collective plasma oscillations:1||fluxon resonance steps:1||STACKS:1||COLLECTIVE DYNAMICS:1||PAIRING SYMMETRY:1||MUON SPIN ROTATION:1||DIMENSIONAL CROSSOVER:1||Bi2Sr2CaCu2Oy highTc superconductors:1||heterojunctions:1||nanostructures:1||surfaces and interfaces:1||QUANTUM TRANSPORT:1||MICROJUNCTIONS:1||RESONATORS:1||STATES:1||FIELD:1||FLUCTUATIONS:1||SCATTERING:1||mode splitting of Josephson vortexflow branches:1||2D superconductivity:1||TRANSISTOR:1||ENERGYGAP:1||SUPERLATTICES:1||IRONBASED SUPERCONDUCTORS:1||PHASEDEPENDENT RESISTANCE:1||QUANTUM PHASETRANSITIONS:1||ELECTRICFIELD:1||HIGH MAGNETICFIELDS:1||NANOWIRE HETEROSTRUCTURES:1||ZNO:1||pair breaking.:1||SUPERCONDUCTING PB:1||domain formation:1||FORCE MICROSCOPY:1||RELAXATION:1||PLASMA RESONANCE:1||coupled Josephson junctions:1||COPPEROXIDE SUPERCONDUCTORS:1||CROSSOVER:1||SIMULATIONS:1||LOWTEMPERATURE:1||CONDUCTORS:1||METALINSULATORTRANSITION:1||SEMICONDUCTOR:1||FIELDEFFECT TRANSISTORS:1||ZEROVOLTAGE STATE:1||constanttemperature interlayer tunneling spectroscopy:1||Josephson supercurrent:1||BIPOLAR SUPERCURRENT:1||Interaction between Josephson and pancake vortices:1||flux jump:1||coaxial heterojunction nanorod:1||Natural Josephson coupling:1||BI2SR2CACU2O8+DELTA:1||VORTEX FLOW:1||TC SUPERCONDUCTORS:1||charge imbalance:1||Andreev diffractometer:1||intercalation:1||surface junction:1||Bi2212:1||tunnelling:1||GRAPHITE:1||GROWTH:1||collective transverse plasma modes:1||GAN:1||Macroscopic quantum tunneling:1||Fluctuation conductivity:1||Abovegap conductance jump:1||Josephson vortex motion:1||Intrinsic Josephson junctions:1||LAYERED SUPERCONDUCTORS:1||BI2SR2CACU2O8+Y:1||INTERFACES:1||BREAKDOWN:1||SYSTEMS:1||Anisotropy ratio:1||Josephson vortex:1||spin relaxation in superconductors:1||bibased single crystals:1||MESOSCOPIC PROXIMITY SUPERCONDUCTOR:1||reentrance of conductance:1||interlayer pair tunneling:1||JOSEPHSON:1||DISORDERED 2DIMENSIONAL SUPERCONDUCTORS:1||INDIUM FILMS:1||excited state:1||REGIME:1||triplet superconductivity:1||FILM:1||SCHOTTKY DIODES:1||peakdiphump structure:1||Kondo effect:1||REENTRANCE:1||Graphene:1||CONTACT:1||BERRYS PHASE:1||2DIMENSIONAL SUPERCONDUCTORS:1||Coulomb diamond:1||magnetic domain:1||spin injection:1||RESONANCE:1||plasma excitation modes:1||FLOW:1||OVERDOPED BI2SR2CACU2O8+DELTA:1||hole doping:1||chemical synthesis:1||phase transitions:1||superconductors:1||VORTEXGLASS SUPERCONDUCTIVITY:1||Kondorelated model:1||RADIATION:1||DOT:1||NANOBELTS:1||Complementarity:1||Closedloop AharonovBohm interferometer:1||pair breaking:1||interlayer phase fluctuation:1||MgB2 thin film:1||CONFINEMENT:1||WALLED CARBON NANOTUBES:1||TRANSITION:9||VORTICES:8||STATE:7||intrinsic Josephson junctions:7||SINGLECRYSTALS:7||JUNCTIONS:5||MODES:5||SUPERCURRENT:5||SUPERCONDUCTOR:5||CONDUCTANCE:5||HIGHTEMPERATURE SUPERCONDUCTORS:5||TRANSPORT:5||PHASE:5||FILMS:4||LOCALIZATION:4||SINGLE DIRAC CONE:4||WIRES:4||MAGNETICFIELD:4||STEPS:3||ELECTRONS:3||proximity effect:3||MODEL:3||ARRAYS:3||INTERFERENCE:3||fluxon dynamics:3||HETEROSTRUCTURES:3||INSULATOR:3||Andreev reflection:3||electronic transport:3||FISKE:3||superconductor:2||ZnO:2||quantum point contact:2||METAL:2||DYNAMICS:2||interlayer Josephson coupling:2||SUPERCONDUCTORS:2||YBA2CU3O7DELTA:2||LAYER:2||DOTS:2||quantum dot:2||Article:2||TRANSISTORS:2||CARBON NANOTUBES:2||GAP:2||MECHANISM:2||LINE:2||GIANT SHAPIRO STEPS:2||LAYERS:2||electron energy loss spectroscopy:2||physical phenomena:2||scanning electron microscopy:2||HGTE QUANTUMWELLS:2||BI2TE3:2||SPECTROSCOPY:2||PNJUNCTIONS:2||spinpolarized tunneling:2||INTRINSIC JOSEPHSONJUNCTIONS:2||FIELDS:2||positive magnetoresistance:2||dilute magnetic semiconductor:2||magnetic field:2||scanning transmission electron microscopy:2||QUANTUM OSCILLATIONS:2||TRANSPORTPROPERTIES:2||surface pair current:2||MAGNETORESISTANCE:2||NANORIBBONS:2||INSTABILITY:2||ANDREEV REFLECTION:2||microwave irradiation:2||vertical graphene josephson junction:2||BI2SE3:2||CONDUCTIVITY:2||highTc superconductors:2||DIMENSIONAL ELECTRONGAS:2||graphene:2||Topological insulators:2||Josephson coupling Fraunhofer interference pattern:2||FERROMAGNET:2||DEPENDENCE:2||DETECTOR:2||COHERENCE:2||INJECTION:2||GRAPHENE:1||JOSEPHSONJUNCTIONS:1||LAYERED SUPERCONDUCTOR:1||mode splitting:1||BEHAVIOR:1||spinpolarized transport:1||SUPERCONDUCTING TRANSITION:1||microwave response:1||PSEUDOGAP:1||phase coherence:1||TRANSITIONS:1||Long Josephson junction:1||Charge detection:1||collective resonance modes:1||plasma oscillation modes:1||Superconducting proximity effect:1||Iron pnictide superconductor:1||McMillanRowell oscillations:1||ferromagnetic microstructure:1||superradiant state:1||VOLTAGE:1||branch splitting:1||TENSOR:1||INTERCALATION:1||insitu fabrication:1||NDGAO3:1||DISORDERED METALS:1||GAUGE GLASS:1||LOWTEMPERATURE TRANSPORT:1||spontaneous spin polarization model:1||BIAS:1||emission of electromagnetic waves:1||YBA2CU3O7/PRBA2CU3O7 SUPERLATTICES:1||BOHM:1||SHAPIRO STEPS:1||superconductor/ferromagnet interface:1||OXIDE:1||ANDREEVREFLECTION:1||SinFeAsO single crystal:1||COLLECTIVE MOTION:1||ANGULARDEPENDENCE:1||SUPERCONDUCTIVITY:1||BILAYER GRAPHENE:1||PHOTOLUMINESCENT PROPERTIES:1||SUPERCONDUCTING WEAK LINKS:1||intrinsic Josephson junctions geometrical resonance:1||intrinsic Josephson junction:1||MESOSCOPIC SPINVALVE:1||Bi2212 single crystals:1||intrinsic junctions:1||ANDREEV REFLECTIONS:1||normalmetal/superconductor interface:1||IBI2SR2CACU2OY:1||THERMAL FLUCTUATIONS:1||MIXED STATE:1||BI2.15SR1.85CACU2O8+DELTA:1||intrinsic Josephson effects:1||CACUO:1||QUANTUM POINT CONTACTS:1||resonant tunneling state:1||coherence length:1||NANOWIRE:1||GATES:1||Phase line:1||Thermal activation:1||QUANTUMDOT:1||superconducting proximity effect:1||Andreev interferometer:1||WIRE:1||Josephsonvortexflow branches:1||Bi2212 cuprates:1||LATTICE:1||demannetization effect:1||SUPERCONDUCTING MIRRORS:1||GAS:1||VALLEY TRANSPORT:1||ELECTRODES:1||DEPENDENT TRANSPORT:1||BORNOPPENHEIMER APPROXIMATION:1||collective plasma oscillations:1||fluxon resonance steps:1||STACKS:1||COLLECTIVE DYNAMICS:1||PAIRING SYMMETRY:1||MUON SPIN ROTATION:1||DIMENSIONAL CROSSOVER:1||Bi2Sr2CaCu2Oy highTc superconductors:1||heterojunctions:1||nanostructures:1||surfaces and interfaces:1||QUANTUM TRANSPORT:1||MICROJUNCTIONS:1||RESONATORS:1||STATES:1||FIELD:1||FLUCTUATIONS:1||SCATTERING:1||mode splitting of Josephson vortexflow branches:1||2D superconductivity:1||TRANSISTOR:1||ENERGYGAP:1||SUPERLATTICES:1||IRONBASED SUPERCONDUCTORS:1||PHASEDEPENDENT RESISTANCE:1||QUANTUM PHASETRANSITIONS:1||ELECTRICFIELD:1||HIGH MAGNETICFIELDS:1||NANOWIRE HETEROSTRUCTURES:1||ZNO:1||pair breaking.:1||SUPERCONDUCTING PB:1||domain formation:1||FORCE MICROSCOPY:1||RELAXATION:1||PLASMA RESONANCE:1||coupled Josephson junctions:1||COPPEROXIDE SUPERCONDUCTORS:1||CROSSOVER:1||SIMULATIONS:1||LOWTEMPERATURE:1||CONDUCTORS:1||METALINSULATORTRANSITION:1||SEMICONDUCTOR:1||FIELDEFFECT TRANSISTORS:1||ZEROVOLTAGE STATE:1||constanttemperature interlayer tunneling spectroscopy:1||Josephson supercurrent:1||BIPOLAR SUPERCURRENT:1||Interaction between Josephson and pancake vortices:1||flux jump:1||coaxial heterojunction nanorod:1||Natural Josephson coupling:1||BI2SR2CACU2O8+DELTA:1||VORTEX FLOW:1||TC SUPERCONDUCTORS:1||charge imbalance:1||Andreev diffractometer:1||intercalation:1||surface junction:1||Bi2212:1||tunnelling:1||GRAPHITE:1||GROWTH:1||collective transverse plasma modes:1||GAN:1||Macroscopic quantum tunneling:1||Fluctuation conductivity:1||Abovegap conductance jump:1||Josephson vortex motion:1||Intrinsic Josephson junctions:1||LAYERED SUPERCONDUCTORS:1||BI2SR2CACU2O8+Y:1||INTERFACES:1||BREAKDOWN:1||SYSTEMS:1||Anisotropy ratio:1||Josephson vortex:1||spin relaxation in superconductors:1||bibased single crystals:1||MESOSCOPIC PROXIMITY SUPERCONDUCTOR:1||reentrance of conductance:1||interlayer pair tunneling:1||JOSEPHSON:1||DISORDERED 2DIMENSIONAL SUPERCONDUCTORS:1||INDIUM FILMS:1||excited state:1||REGIME:1||triplet superconductivity:1||FILM:1||SCHOTTKY DIODES:1||peakdiphump structure:1||Kondo effect:1||REENTRANCE:1||Graphene:1||CONTACT:1||BERRYS PHASE:1||2DIMENSIONAL SUPERCONDUCTORS:1||Coulomb diamond:1||magnetic domain:1||spin injection:1||RESONANCE:1||plasma excitation modes:1||FLOW:1||OVERDOPED BI2SR2CACU2O8+DELTA:1||hole doping:1||chemical synthesis:1||phase transitions:1||superconductors:1||VORTEXGLASS SUPERCONDUCTIVITY:1||Kondorelated model:1||RADIATION:1||DOT:1||NANOBELTS:1||Complementarity:1||Closedloop AharonovBohm interferometer:1||pair breaking:1||interlayer phase fluctuation:1||MgB2 thin film:1||CONFINEMENT:1||WALLED CARBON NANOTUBES:1||TRANSITION:9||VORTICES:8||STATE:7||intrinsic Josephson junctions:7||SINGLECRYSTALS:7||JUNCTIONS:5||MODES:5||SUPERCURRENT:5||SUPERCONDUCTOR:5||CONDUCTANCE:5||HIGHTEMPERATURE SUPERCONDUCTORS:5||TRANSPORT:5||PHASE:5||FILMS:4||LOCALIZATION:4||SINGLE DIRAC CONE:4||WIRES:4||MAGNETICFIELD:4||STEPS:3||ELECTRONS:3||proximity effect:3||MODEL:3||ARRAYS:3||INTERFERENCE:3||fluxon dynamics:3||HETEROSTRUCTURES:3||INSULATOR:3||Andreev reflection:3||electronic transport:3||FISKE:3||superconductor:2||ZnO:2||quantum point contact:2||METAL:2||DYNAMICS:2||interlayer Josephson coupling:2||SUPERCONDUCTORS:2||YBA2CU3O7DELTA:2||LAYER:2||DOTS:2||quantum dot:2||Article:2||TRANSISTORS:2||CARBON NANOTUBES:2||GAP:2||MECHANISM:2||LINE:2||GIANT SHAPIRO STEPS:2||LAYERS:2||electron energy loss spectroscopy:2||physical phenomena:2||scanning electron microscopy:2||HGTE QUANTUMWELLS:2||BI2TE3:2||SPECTROSCOPY:2||PNJUNCTIONS:2||spinpolarized tunneling:2||INTRINSIC JOSEPHSONJUNCTIONS:2||FIELDS:2||positive magnetoresistance:2||dilute magnetic semiconductor:2||magnetic field:2||scanning transmission electron microscopy:2||QUANTUM OSCILLATIONS:2||TRANSPORTPROPERTIES:2||surface pair current:2||MAGNETORESISTANCE:2||NANORIBBONS:2||INSTABILITY:2||ANDREEV REFLECTION:2||microwave irradiation:2||vertical graphene josephson junction:2||BI2SE3:2||CONDUCTIVITY:2||highTc superconductors:2||DIMENSIONAL ELECTRONGAS:2||graphene:2||Topological insulators:2||Josephson coupling Fraunhofer interference pattern:2||FERROMAGNET:2||DEPENDENCE:2||DETECTOR:2||COHERENCE:2||INJECTION:2||GRAPHENE:1||JOSEPHSONJUNCTIONS:1||LAYERED SUPERCONDUCTOR:1||mode splitting:1||BEHAVIOR:1||spinpolarized transport:1||SUPERCONDUCTING TRANSITION:1||microwave response:1||PSEUDOGAP:1||phase coherence:1||TRANSITIONS:1||Long Josephson junction:1||Charge detection:1||collective resonance modes:1||plasma oscillation modes:1||Superconducting proximity effect:1||Iron pnictide superconductor:1||McMillanRowell oscillations:1||ferromagnetic microstructure:1||superradiant state:1||VOLTAGE:1||branch splitting:1||TENSOR:1||INTERCALATION:1||insitu fabrication:1||NDGAO3:1||DISORDERED METALS:1||GAUGE GLASS:1||LOWTEMPERATURE TRANSPORT:1||spontaneous spin polarization model:1||BIAS:1||emission of electromagnetic waves:1||YBA2CU3O7/PRBA2CU3O7 SUPERLATTICES:1||BOHM:1||SHAPIRO STEPS:1||superconductor/ferromagnet interface:1||OXIDE:1||ANDREEVREFLECTION:1||SinFeAsO single crystal:1||COLLECTIVE MOTION:1||ANGULARDEPENDENCE:1||SUPERCONDUCTIVITY:1||BILAYER GRAPHENE:1||PHOTOLUMINESCENT PROPERTIES:1||SUPERCONDUCTING WEAK LINKS:1||intrinsic Josephson junctions geometrical resonance:1||intrinsic Josephson junction:1||MESOSCOPIC SPINVALVE:1||Bi2212 single crystals:1||intrinsic junctions:1||ANDREEV REFLECTIONS:1||normalmetal/superconductor interface:1||IBI2SR2CACU2OY:1||THERMAL FLUCTUATIONS:1||MIXED STATE:1||BI2.15SR1.85CACU2O8+DELTA:1||intrinsic Josephson effects:1||CACUO:1||QUANTUM POINT CONTACTS:1||resonant tunneling state:1||coherence length:1||NANOWIRE:1||GATES:1||Phase line:1||Thermal activation:1||QUANTUMDOT:1||superconducting proximity effect:1||Andreev interferometer:1||WIRE:1||Josephsonvortexflow branches:1||Bi2212 cuprates:1||LATTICE:1||demannetization effect:1||SUPERCONDUCTING MIRRORS:1||GAS:1||VALLEY TRANSPORT:1||ELECTRODES:1||DEPENDENT TRANSPORT:1||BORNOPPENHEIMER APPROXIMATION:1||collective plasma oscillations:1||fluxon resonance steps:1||STACKS:1||COLLECTIVE DYNAMICS:1||PAIRING SYMMETRY:1||MUON SPIN ROTATION:1||DIMENSIONAL CROSSOVER:1||Bi2Sr2CaCu2Oy highTc superconductors:1||heterojunctions:1||nanostructures:1||surfaces and interfaces:1||QUANTUM TRANSPORT:1||MICROJUNCTIONS:1||RESONATORS:1||STATES:1||FIELD:1||FLUCTUATIONS:1||SCATTERING:1||mode splitting of Josephson vortexflow branches:1||2D superconductivity:1||TRANSISTOR:1||ENERGYGAP:1||SUPERLATTICES:1||IRONBASED SUPERCONDUCTORS:1||PHASEDEPENDENT RESISTANCE:1||QUANTUM PHASETRANSITIONS:1||ELECTRICFIELD:1||HIGH MAGNETICFIELDS:1||NANOWIRE HETEROSTRUCTURES:1||ZNO:1||pair breaking.:1||SUPERCONDUCTING PB:1||domain formation:1||FORCE MICROSCOPY:1||RELAXATION:1||PLASMA RESONANCE:1||coupled Josephson junctions:1||COPPEROXIDE SUPERCONDUCTORS:1||CROSSOVER:1||SIMULATIONS:1||LOWTEMPERATURE:1||CONDUCTORS:1||METALINSULATORTRANSITION:1||SEMICONDUCTOR:1||FIELDEFFECT TRANSISTORS:1||ZEROVOLTAGE STATE:1||constanttemperature interlayer tunneling spectroscopy:1||Josephson supercurrent:1||BIPOLAR SUPERCURRENT:1||Interaction between Josephson and pancake vortices:1||flux jump:1||coaxial heterojunction nanorod:1||Natural Josephson coupling:1||BI2SR2CACU2O8+DELTA:1||VORTEX FLOW:1||TC SUPERCONDUCTORS:1||charge imbalance:1||Andreev diffractometer:1||intercalation:1||surface junction:1||Bi2212:1||tunnelling:1||GRAPHITE:1||GROWTH:1||collective transverse plasma modes:1||GAN:1||Macroscopic quantum tunneling:1||Fluctuation conductivity:1||Abovegap conductance jump:1||Josephson vortex motion:1||Intrinsic Josephson junctions:1||LAYERED SUPERCONDUCTORS:1||BI2SR2CACU2O8+Y:1||INTERFACES:1||BREAKDOWN:1||SYSTEMS:1||Anisotropy ratio:1||Josephson vortex:1||spin relaxation in superconductors:1||bibased single crystals:1||MESOSCOPIC PROXIMITY SUPERCONDUCTOR:1||reentrance of conductance:1||interlayer pair tunneling:1||JOSEPHSON:1||DISORDERED 2DIMENSIONAL SUPERCONDUCTORS:1||INDIUM FILMS:1||excited state:1||REGIME:1||triplet superconductivity:1||FILM:1||SCHOTTKY DIODES:1||peakdiphump structure:1||Kondo effect:1||REENTRANCE:1||Graphene:1||CONTACT:1||BERRYS PHASE:1||2DIMENSIONAL SUPERCONDUCTORS:1||Coulomb diamond:1||magnetic domain:1||spin injection:1||RESONANCE:1||plasma excitation modes:1||FLOW:1||OVERDOPED BI2SR2CACU2O8+DELTA:1||hole doping:1||chemical synthesis:1||phase transitions:1||superconductors:1||VORTEXGLASS SUPERCONDUCTIVITY:1||Kondorelated model:1||RADIATION:1||DOT:1||NANOBELTS:1||Complementarity:1||Closedloop AharonovBohm interferometer:1||pair breaking:1||interlayer phase fluctuation:1||MgB2 thin film:1||CONFINEMENT:1||WALLED CARBON NANOTUBES:1||TRANSITION:9||VORTICES:8||STATE:7||intrinsic Josephson junctions:7||SINGLECRYSTALS:7||JUNCTIONS:5||MODES:5||SUPERCURRENT:5||SUPERCONDUCTOR:5||CONDUCTANCE:5||HIGHTEMPERATURE SUPERCONDUCTORS:5||TRANSPORT:5||PHASE:5||FILMS:4||LOCALIZATION:4||SINGLE DIRAC CONE:4||WIRES:4||MAGNETICFIELD:4||STEPS:3||ELECTRONS:3||proximity effect:3||MODEL:3||ARRAYS:3||INTERFERENCE:3||fluxon dynamics:3||HETEROSTRUCTURES:3||INSULATOR:3||Andreev reflection:3||electronic transport:3||FISKE:3||superconductor:2||ZnO:2||quantum point contact:2||METAL:2||DYNAMICS:2||interlayer Josephson coupling:2||SUPERCONDUCTORS:2||YBA2CU3O7DELTA:2||LAYER:2||DOTS:2||quantum dot:2||Article:2||TRANSISTORS:2||CARBON NANOTUBES:2||GAP:2||MECHANISM:2||LINE:2||GIANT SHAPIRO STEPS:2||LAYERS:2||electron energy loss spectroscopy:2||physical phenomena:2||scanning electron microscopy:2||HGTE QUANTUMWELLS:2||BI2TE3:2||SPECTROSCOPY:2||PNJUNCTIONS:2||spinpolarized tunneling:2||INTRINSIC JOSEPHSONJUNCTIONS:2||FIELDS:2||positive magnetoresistance:2||dilute magnetic semiconductor:2||magnetic field:2||scanning transmission electron microscopy:2||QUANTUM OSCILLATIONS:2||TRANSPORTPROPERTIES:2||surface pair current:2||MAGNETORESISTANCE:2||NANORIBBONS:2||INSTABILITY:2||ANDREEV REFLECTION:2||microwave irradiation:2||vertical graphene josephson junction:2||BI2SE3:2||CONDUCTIVITY:2||highTc superconductors:2||DIMENSIONAL ELECTRONGAS:2||graphene:2||Topological insulators:2||Josephson coupling Fraunhofer interference pattern:2||FERROMAGNET:2||DEPENDENCE:2||DETECTOR:2||COHERENCE:2||INJECTION:2||GRAPHENE:1||JOSEPHSONJUNCTIONS:1||LAYERED SUPERCONDUCTOR:1||mode splitting:1||BEHAVIOR:1||spinpolarized transport:1||SUPERCONDUCTING TRANSITION:1||microwave response:1||PSEUDOGAP:1||phase coherence:1||TRANSITIONS:1||Long Josephson junction:1||Charge detection:1||collective resonance modes:1||plasma oscillation modes:1||Superconducting proximity effect:1||Iron pnictide superconductor:1||McMillanRowell oscillations:1||ferromagnetic microstructure:1||superradiant state:1||VOLTAGE:1||branch splitting:1||TENSOR:1||INTERCALATION:1||insitu fabrication:1||NDGAO3:1||DISORDERED METALS:1||GAUGE GLASS:1||LOWTEMPERATURE TRANSPORT:1||spontaneous spin polarization model:1||BIAS:1||emission of electromagnetic waves:1||YBA2CU3O7/PRBA2CU3O7 SUPERLATTICES:1||BOHM:1||SHAPIRO STEPS:1||superconductor/ferromagnet interface:1||OXIDE:1||ANDREEVREFLECTION:1||SinFeAsO single crystal:1||COLLECTIVE MOTION:1||ANGULARDEPENDENCE:1||SUPERCONDUCTIVITY:1||BILAYER GRAPHENE:1||PHOTOLUMINESCENT PROPERTIES:1||SUPERCONDUCTING WEAK LINKS:1||intrinsic Josephson junctions geometrical resonance:1||intrinsic Josephson junction:1||MESOSCOPIC SPINVALVE:1||Bi2212 single crystals:1||intrinsic junctions:1||ANDREEV REFLECTIONS:1||normalmetal/superconductor interface:1||IBI2SR2CACU2OY:1||THERMAL FLUCTUATIONS:1||MIXED STATE:1||BI2.15SR1.85CACU2O8+DELTA:1||intrinsic Josephson effects:1||CACUO:1||QUANTUM POINT CONTACTS:1||resonant tunneling state:1||coherence length:1||NANOWIRE:1||GATES:1||Phase line:1||Thermal activation:1||QUANTUMDOT:1||superconducting proximity effect:1||Andreev interferometer:1||WIRE:1||Josephsonvortexflow branches:1||Bi2212 cuprates:1||LATTICE:1||demannetization effect:1||SUPERCONDUCTING MIRRORS:1||GAS:1||VALLEY TRANSPORT:1||ELECTRODES:1||DEPENDENT TRANSPORT:1||BORNOPPENHEIMER APPROXIMATION:1||collective plasma oscillations:1||fluxon resonance steps:1||STACKS:1||COLLECTIVE DYNAMICS:1||PAIRING SYMMETRY:1||MUON SPIN ROTATION:1||DIMENSIONAL CROSSOVER:1||Bi2Sr2CaCu2Oy highTc superconductors:1||heterojunctions:1||nanostructures:1||surfaces and interfaces:1||QUANTUM TRANSPORT:1||MICROJUNCTIONS:1||RESONATORS:1||STATES:1||FIELD:1||FLUCTUATIONS:1||SCATTERING:1||mode splitting of Josephson vortexflow branches:1||2D superconductivity:1||TRANSISTOR:1||ENERGYGAP:1||SUPERLATTICES:1||IRONBASED SUPERCONDUCTORS:1||PHASEDEPENDENT RESISTANCE:1||QUANTUM PHASETRANSITIONS:1||ELECTRICFIELD:1||HIGH MAGNETICFIELDS:1||NANOWIRE HETEROSTRUCTURES:1||ZNO:1||pair breaking.:1||SUPERCONDUCTING PB:1||domain formation:1||FORCE MICROSCOPY:1||RELAXATION:1||PLASMA RESONANCE:1||coupled Josephson junctions:1||COPPEROXIDE SUPERCONDUCTORS:1||CROSSOVER:1||SIMULATIONS:1||LOWTEMPERATURE:1||CONDUCTORS:1||METALINSULATORTRANSITION:1||SEMICONDUCTOR:1||FIELDEFFECT TRANSISTORS:1||ZEROVOLTAGE STATE:1||constanttemperature interlayer tunneling spectroscopy:1||Josephson supercurrent:1||BIPOLAR SUPERCURRENT:1||Interaction between Josephson and pancake vortices:1||flux jump:1||coaxial heterojunction nanorod:1||Natural Josephson coupling:1||BI2SR2CACU2O8+DELTA:1||VORTEX FLOW:1||TC SUPERCONDUCTORS:1||charge imbalance:1||Andreev diffractometer:1||intercalation:1||surface junction:1||Bi2212:1||tunnelling:1||GRAPHITE:1||GROWTH:1||collective transverse plasma modes:1||GAN:1||Macroscopic quantum tunneling:1||Fluctuation conductivity:1||Abovegap conductance jump:1||Josephson vortex motion:1||Intrinsic Josephson junctions:1||LAYERED SUPERCONDUCTORS:1||BI2SR2CACU2O8+Y:1||INTERFACES:1||BREAKDOWN:1||SYSTEMS:1||Anisotropy ratio:1||Josephson vortex:1||spin relaxation in superconductors:1||bibased single crystals:1||MESOSCOPIC PROXIMITY SUPERCONDUCTOR:1||reentrance of conductance:1||interlayer pair tunneling:1||JOSEPHSON:1||DISORDERED 2DIMENSIONAL SUPERCONDUCTORS:1||INDIUM FILMS:1||excited state:1||REGIME:1||triplet superconductivity:1||FILM:1||SCHOTTKY DIODES:1||peakdiphump structure:1||Kondo effect:1||REENTRANCE:1||Graphene:1||CONTACT:1||BERRYS PHASE:1||2DIMENSIONAL SUPERCONDUCTORS:1||Coulomb diamond:1||magnetic domain:1||spin injection:1||RESONANCE:1||plasma excitation modes:1||FLOW:1||OVERDOPED BI2SR2CACU2O8+DELTA:1||hole doping:1||chemical synthesis:1||phase transitions:1||superconductors:1||VORTEXGLASS SUPERCONDUCTIVITY:1||Kondorelated model:1||RADIATION:1||DOT:1||NANOBELTS:1||Complementarity:1||Closedloop AharonovBohm interferometer:1||pair breaking:1||interlayer phase fluctuation:1||MgB2 thin film:1||CONFINEMENT:1||WALLED CARBON NANOTUBES:1||TRANSITION:9||VORTICES:8||STATE:7||intrinsic Josephson junctions:7||SINGLECRYSTALS:7||JUNCTIONS:5||MODES:5||SUPERCURRENT:5||SUPERCONDUCTOR:5||CONDUCTANCE:5||HIGHTEMPERATURE SUPERCONDUCTORS:5||TRANSPORT:5||PHASE:5||FILMS:4||LOCALIZATION:4||SINGLE DIRAC CONE:4||WIRES:4||MAGNETICFIELD:4||STEPS:3||ELECTRONS:3||proximity effect:3||MODEL:3||ARRAYS:3||INTERFERENCE:3||fluxon dynamics:3||HETEROSTRUCTURES:3||INSULATOR:3||Andreev reflection:3||electronic transport:3||FISKE:3||superconductor:2||ZnO:2||quantum point contact:2||METAL:2||DYNAMICS:2||interlayer Josephson coupling:2||SUPERCONDUCTORS:2||YBA2CU3O7DELTA:2||LAYER:2||DOTS:2||quantum dot:2||Article:2||TRANSISTORS:2||CARBON NANOTUBES:2||GAP:2||MECHANISM:2||LINE:2||GIANT SHAPIRO STEPS:2||LAYERS:2||electron energy loss spectroscopy:2||physical phenomena:2||scanning electron microscopy:2||HGTE QUANTUMWELLS:2||BI2TE3:2||SPECTROSCOPY:2||PNJUNCTIONS:2||spinpolarized tunneling:2||INTRINSIC JOSEPHSONJUNCTIONS:2||FIELDS:2||positive magnetoresistance:2||dilute magnetic semiconductor:2||magnetic field:2||scanning transmission electron microscopy:2||QUANTUM OSCILLATIONS:2||TRANSPORTPROPERTIES:2||surface pair current:2||MAGNETORESISTANCE:2||NANORIBBONS:2||INSTABILITY:2||ANDREEV REFLECTION:2||microwave irradiation:2||vertical graphene josephson junction:2||BI2SE3:2||CONDUCTIVITY:2||highTc superconductors:2||DIMENSIONAL ELECTRONGAS:2||graphene:2||Topological insulators:2||Josephson coupling Fraunhofer interference pattern:2||FERROMAGNET:2||DEPENDENCE:2||DETECTOR:2||COHERENCE:2||INJECTION:2||GRAPHENE:1||JOSEPHSONJUNCTIONS:1||LAYERED SUPERCONDUCTOR:1||mode splitting:1||BEHAVIOR:1||spinpolarized transport:1||SUPERCONDUCTING TRANSITION:1||microwave response:1||PSEUDOGAP:1||phase coherence:1||TRANSITIONS:1||Long Josephson junction:1||Charge detection:1||collective resonance modes:1||plasma oscillation modes:1||Superconducting proximity effect:1||Iron pnictide superconductor:1||McMillanRowell oscillations:1||ferromagnetic microstructure:1||superradiant state:1||VOLTAGE:1||branch splitting:1||TENSOR:1||INTERCALATION:1||insitu fabrication:1||NDGAO3:1||DISORDERED METALS:1||GAUGE GLASS:1||LOWTEMPERATURE TRANSPORT:1||spontaneous spin polarization model:1||BIAS:1||emission of electromagnetic waves:1||YBA2CU3O7/PRBA2CU3O7 SUPERLATTICES:1||BOHM:1||SHAPIRO STEPS:1||superconductor/ferromagnet interface:1||OXIDE:1||ANDREEVREFLECTION:1||SinFeAsO single crystal:1||COLLECTIVE MOTION:1||ANGULARDEPENDENCE:1||SUPERCONDUCTIVITY:1||BILAYER GRAPHENE:1||PHOTOLUMINESCENT PROPERTIES:1||SUPERCONDUCTING WEAK LINKS:1||intrinsic Josephson junctions geometrical resonance:1||intrinsic Josephson junction:1||MESOSCOPIC SPINVALVE:1||Bi2212 single crystals:1||intrinsic junctions:1||ANDREEV REFLECTIONS:1||normalmetal/superconductor interface:1||IBI2SR2CACU2OY:1||THERMAL FLUCTUATIONS:1||MIXED STATE:1||BI2.15SR1.85CACU2O8+DELTA:1||intrinsic Josephson effects:1||CACUO:1||QUANTUM POINT CONTACTS:1||resonant tunneling state:1||coherence length:1||NANOWIRE:1||GATES:1||Phase line:1||Thermal activation:1||QUANTUMDOT:1||superconducting proximity effect:1||Andreev interferometer:1||WIRE:1||Josephsonvortexflow branches:1||Bi2212 cuprates:1||LATTICE:1||demannetization effect:1||SUPERCONDUCTING MIRRORS:1||GAS:1||VALLEY TRANSPORT:1||ELECTRODES:1||DEPENDENT TRANSPORT:1||BORNOPPENHEIMER APPROXIMATION:1||collective plasma oscillations:1||fluxon resonance steps:1||STACKS:1||COLLECTIVE DYNAMICS:1||PAIRING SYMMETRY:1||MUON SPIN ROTATION:1||DIMENSIONAL CROSSOVER:1||Bi2Sr2CaCu2Oy highTc superconductors:1||heterojunctions:1||nanostructures:1||surfaces and interfaces:1||QUANTUM TRANSPORT:1||MICROJUNCTIONS:1||RESONATORS:1||STATES:1||FIELD:1||FLUCTUATIONS:1||SCATTERING:1||mode splitting of Josephson vortexflow branches:1||2D superconductivity:1||TRANSISTOR:1||ENERGYGAP:1||SUPERLATTICES:1||IRONBASED SUPERCONDUCTORS:1||PHASEDEPENDENT RESISTANCE:1||QUANTUM PHASETRANSITIONS:1||ELECTRICFIELD:1||HIGH MAGNETICFIELDS:1||NANOWIRE HETEROSTRUCTURES:1||ZNO:1||pair breaking.:1||SUPERCONDUCTING PB:1||domain formation:1||FORCE MICROSCOPY:1||RELAXATION:1||PLASMA RESONANCE:1||coupled Josephson junctions:1||COPPEROXIDE SUPERCONDUCTORS:1||CROSSOVER:1||SIMULATIONS:1||LOWTEMPERATURE:1||CONDUCTORS:1||METALINSULATORTRANSITION:1||SEMICONDUCTOR:1||FIELDEFFECT TRANSISTORS:1||ZEROVOLTAGE STATE:1||constanttemperature interlayer tunneling spectroscopy:1||Josephson supercurrent:1||BIPOLAR SUPERCURRENT:1||Interaction between Josephson and pancake vortices:1||flux jump:1||coaxial heterojunction nanorod:1||Natural Josephson coupling:1||BI2SR2CACU2O8+DELTA:1||VORTEX FLOW:1||TC SUPERCONDUCTORS:1||charge imbalance:1||Andreev diffractometer:1||intercalation:1||surface junction:1||Bi2212:1||tunnelling:1||GRAPHITE:1||GROWTH:1||collective transverse plasma modes:1||GAN:1||Macroscopic quantum tunneling:1||Fluctuation conductivity:1||Abovegap conductance jump:1||Josephson vortex motion:1||Intrinsic Josephson junctions:1||LAYERED SUPERCONDUCTORS:1||BI2SR2CACU2O8+Y:1||INTERFACES:1||BREAKDOWN:1||SYSTEMS:1||Anisotropy ratio:1||Josephson vortex:1||spin relaxation in superconductors:1||bibased single crystals:1||MESOSCOPIC PROXIMITY SUPERCONDUCTOR:1||reentrance of conductance:1||interlayer pair tunneling:1||JOSEPHSON:1||DISORDERED 2DIMENSIONAL SUPERCONDUCTORS:1||INDIUM FILMS:1||excited state:1||REGIME:1||triplet superconductivity:1||FILM:1||SCHOTTKY DIODES:1||peakdiphump structure:1||Kondo effect:1||REENTRANCE:1||Graphene:1||CONTACT:1||BERRYS PHASE:1||2DIMENSIONAL SUPERCONDUCTORS:1||Coulomb diamond:1||magnetic domain:1||spin injection:1||RESONANCE:1||plasma excitation modes:1||FLOW:1||OVERDOPED BI2SR2CACU2O8+DELTA:1||hole doping:1||chemical synthesis:1||phase transitions:1||superconductors:1||VORTEXGLASS SUPERCONDUCTIVITY:1||Kondorelated model:1||RADIATION:1||DOT:1||NANOBELTS:1||Complementarity:1||Closedloop AharonovBohm interferometer:1||pair breaking:1||interlayer phase fluctuation:1||MgB2 thin film:1||CONFINEMENT:1||WALLED CARBON NANOTUBES:1||TRANSITION:9||VORTICES:8||STATE:7||intrinsic Josephson junctions:7||SINGLECRYSTALS:7||JUNCTIONS:5||MODES:5||SUPERCURRENT:5||SUPERCONDUCTOR:5||CONDUCTANCE:5||HIGHTEMPERATURE SUPERCONDUCTORS:5||TRANSPORT:5||PHASE:5||FILMS:4||LOCALIZATION:4||SINGLE DIRAC CONE:4||WIRES:4||MAGNETICFIELD:4||STEPS:3||ELECTRONS:3||proximity effect:3||MODEL:3||ARRAYS:3||INTERFERENCE:3||fluxon dynamics:3||HETEROSTRUCTURES:3||INSULATOR:3||Andreev reflection:3||electronic transport:3||FISKE:3||superconductor:2||ZnO:2||quantum point contact:2||METAL:2||DYNAMICS:2||interlayer Josephson coupling:2||SUPERCONDUCTORS:2||YBA2CU3O7DELTA:2||LAYER:2||DOTS:2||quantum dot:2||Article:2||TRANSISTORS:2||CARBON NANOTUBES:2||GAP:2||MECHANISM:2||LINE:2||GIANT SHAPIRO STEPS:2||LAYERS:2||electron energy loss spectroscopy:2||physical phenomena:2||scanning electron microscopy:2||HGTE QUANTUMWELLS:2||BI2TE3:2||SPECTROSCOPY:2||PNJUNCTIONS:2||spinpolarized tunneling:2||INTRINSIC JOSEPHSONJUNCTIONS:2||FIELDS:2||positive magnetoresistance:2||dilute magnetic semiconductor:2||magnetic field:2||scanning transmission electron microscopy:2||QUANTUM OSCILLATIONS:2||TRANSPORTPROPERTIES:2||surface pair current:2||MAGNETORESISTANCE:2||NANORIBBONS:2||INSTABILITY:2||ANDREEV REFLECTION:2||microwave irradiation:2||vertical graphene josephson junction:2||BI2SE3:2||CONDUCTIVITY:2||highTc superconductors:2||DIMENSIONAL ELECTRONGAS:2||graphene:2||Topological insulators:2||Josephson coupling Fraunhofer interference pattern:2||FERROMAGNET:2||DEPENDENCE:2||DETECTOR:2||COHERENCE:2||INJECTION:2||GRAPHENE:1||JOSEPHSONJUNCTIONS:1||LAYERED SUPERCONDUCTOR:1||mode splitting:1||BEHAVIOR:1||spinpolarized transport:1||SUPERCONDUCTING TRANSITION:1||microwave response:1||PSEUDOGAP:1||phase coherence:1||TRANSITIONS:1||Long Josephson junction:1||Charge detection:1||collective resonance modes:1||plasma oscillation modes:1||Superconducting proximity effect:1||Iron pnictide superconductor:1||McMillanRowell oscillations:1||ferromagnetic microstructure:1||superradiant state:1||VOLTAGE:1||branch splitting:1||TENSOR:1||INTERCALATION:1||insitu fabrication:1||NDGAO3:1||DISORDERED METALS:1||GAUGE GLASS:1||LOWTEMPERATURE TRANSPORT:1||spontaneous spin polarization model:1||BIAS:1||emission of electromagnetic waves:1||YBA2CU3O7/PRBA2CU3O7 SUPERLATTICES:1||BOHM:1||SHAPIRO STEPS:1||superconductor/ferromagnet interface:1||OXIDE:1||ANDREEVREFLECTION:1||SinFeAsO single crystal:1||COLLECTIVE MOTION:1||ANGULARDEPENDENCE:1||SUPERCONDUCTIVITY:1||BILAYER GRAPHENE:1||PHOTOLUMINESCENT PROPERTIES:1||SUPERCONDUCTING WEAK LINKS:1||intrinsic Josephson junctions geometrical resonance:1||intrinsic Josephson junction:1||MESOSCOPIC SPINVALVE:1||Bi2212 single crystals:1||intrinsic junctions:1||ANDREEV REFLECTIONS:1||normalmetal/superconductor interface:1||IBI2SR2CACU2OY:1||THERMAL FLUCTUATIONS:1||MIXED STATE:1||BI2.15SR1.85CACU2O8+DELTA:1||intrinsic Josephson effects:1||CACUO:1||QUANTUM POINT CONTACTS:1||resonant tunneling state:1||coherence length:1||NANOWIRE:1||GATES:1||Phase line:1||Thermal activation:1||QUANTUMDOT:1||superconducting proximity effect:1||Andreev interferometer:1||WIRE:1||Josephsonvortexflow branches:1||Bi2212 cuprates:1||LATTICE:1||demannetization effect:1||SUPERCONDUCTING MIRRORS:1||GAS:1||VALLEY TRANSPORT:1||ELECTRODES:1||DEPENDENT TRANSPORT:1||BORNOPPENHEIMER APPROXIMATION:1||collective plasma oscillations:1||fluxon resonance steps:1||STACKS:1||COLLECTIVE DYNAMICS:1||PAIRING SYMMETRY:1||MUON SPIN ROTATION:1||DIMENSIONAL CROSSOVER:1||Bi2Sr2CaCu2Oy highTc superconductors:1||heterojunctions:1||nanostructures:1||surfaces and interfaces:1||QUANTUM TRANSPORT:1||MICROJUNCTIONS:1||RESONATORS:1||STATES:1||FIELD:1||FLUCTUATIONS:1||SCATTERING:1||mode splitting of Josephson vortexflow branches:1||2D superconductivity:1||TRANSISTOR:1||ENERGYGAP:1||SUPERLATTICES:1||IRONBASED SUPERCONDUCTORS:1||PHASEDEPENDENT RESISTANCE:1||QUANTUM PHASETRANSITIONS:1||ELECTRICFIELD:1||HIGH MAGNETICFIELDS:1||NANOWIRE HETEROSTRUCTURES:1||ZNO:1||pair breaking.:1||SUPERCONDUCTING PB:1||domain formation:1||FORCE MICROSCOPY:1||RELAXATION:1||PLASMA RESONANCE:1||coupled Josephson junctions:1||COPPEROXIDE SUPERCONDUCTORS:1||CROSSOVER:1||SIMULATIONS:1||LOWTEMPERATURE:1||CONDUCTORS:1||METALINSULATORTRANSITION:1||SEMICONDUCTOR:1||FIELDEFFECT TRANSISTORS:1||ZEROVOLTAGE STATE:1||constanttemperature interlayer tunneling spectroscopy:1||Josephson supercurrent:1||BIPOLAR SUPERCURRENT:1||Interaction between Josephson and pancake vortices:1||flux jump:1||coaxial heterojunction nanorod:1||Natural Josephson coupling:1||BI2SR2CACU2O8+DELTA:1||VORTEX FLOW:1||TC SUPERCONDUCTORS:1||charge imbalance:1||Andreev diffractometer:1||intercalation:1||surface junction:1||Bi2212:1||tunnelling:1||GRAPHITE:1||GROWTH:1||collective transverse plasma modes:1||GAN:1||Macroscopic quantum tunneling:1||Fluctuation conductivity:1||Abovegap conductance jump:1||Josephson vortex motion:1||Intrinsic Josephson junctions:1||LAYERED SUPERCONDUCTORS:1||BI2SR2CACU2O8+Y:1||INTERFACES:1||BREAKDOWN:1||SYSTEMS:1||Anisotropy ratio:1||Josephson vortex:1||spin relaxation in superconductors:1||bibased single crystals:1||MESOSCOPIC PROXIMITY SUPERCONDUCTOR:1||reentrance of conductance:1||interlayer pair tunneling:1||JOSEPHSON:1||DISORDERED 2DIMENSIONAL SUPERCONDUCTORS:1||INDIUM FILMS:1||excited state:1||REGIME:1||triplet superconductivity:1||FILM:1||SCHOTTKY DIODES:1||peakdiphump structure:1||Kondo effect:1||REENTRANCE:1||Graphene:1||CONTACT:1||BERRYS PHASE:1||2DIMENSIONAL SUPERCONDUCTORS:1||Coulomb diamond:1||magnetic domain:1||spin injection:1||RESONANCE:1||plasma excitation modes:1||FLOW:1||OVERDOPED BI2SR2CACU2O8+DELTA:1||hole doping:1||chemical synthesis:1||phase transitions:1||superconductors:1||VORTEXGLASS SUPERCONDUCTIVITY:1||Kondorelated model:1||RADIATION:1||DOT:1||NANOBELTS:1||Complementarity:1||Closedloop AharonovBohm interferometer:1||pair breaking:1||interlayer phase fluctuation:1||MgB2 thin film:1||CONFINEMENT:1||WALLED CARBON NANOTUBES:1||TRANSITION:9||VORTICES:8||STATE:7||intrinsic Josephson junctions:7||SINGLECRYSTALS:7||JUNCTIONS:5||MODES:5||SUPERCURRENT:5||SUPERCONDUCTOR:5||CONDUCTANCE:5||HIGHTEMPERATURE SUPERCONDUCTORS:5||TRANSPORT:5||PHASE:5||FILMS:4||LOCALIZATION:4||SINGLE DIRAC CONE:4||WIRES:4||MAGNETICFIELD:4||STEPS:3||ELECTRONS:3||proximity effect:3||MODEL:3||ARRAYS:3||INTERFERENCE:3||fluxon dynamics:3||HETEROSTRUCTURES:3||INSULATOR:3||Andreev reflection:3||electronic transport:3||FISKE:3||superconductor:2||ZnO:2||quantum point contact:2||METAL:2||DYNAMICS:2||interlayer Josephson coupling:2||SUPERCONDUCTORS:2||YBA2CU3O7DELTA:2||LAYER:2||DOTS:2||quantum dot:2||Article:2||TRANSISTORS:2||CARBON NANOTUBES:2||GAP:2||MECHANISM:2||LINE:2||GIANT SHAPIRO STEPS:2||LAYERS:2||electron energy loss spectroscopy:2||physical phenomena:2||scanning electron microscopy:2||HGTE QUANTUMWELLS:2||BI2TE3:2||SPECTROSCOPY:2||PNJUNCTIONS:2||spinpolarized tunneling:2||INTRINSIC JOSEPHSONJUNCTIONS:2||FIELDS:2||positive magnetoresistance:2||dilute magnetic semiconductor:2||magnetic field:2||scanning transmission electron microscopy:2||QUANTUM OSCILLATIONS:2||TRANSPORTPROPERTIES:2||surface pair current:2||MAGNETORESISTANCE:2||NANORIBBONS:2||INSTABILITY:2||ANDREEV REFLECTION:2||microwave irradiation:2||vertical graphene josephson junction:2||BI2SE3:2||CONDUCTIVITY:2||highTc superconductors:2||DIMENSIONAL ELECTRONGAS:2||graphene:2||Topological insulators:2||Josephson coupling Fraunhofer interference pattern:2||FERROMAGNET:2||DEPENDENCE:2||DETECTOR:2||COHERENCE:2||INJECTION:2||GRAPHENE:1||JOSEPHSONJUNCTIONS:1||LAYERED SUPERCONDUCTOR:1||mode splitting:1||BEHAVIOR:1||spinpolarized transport:1||SUPERCONDUCTING TRANSITION:1||microwave response:1||PSEUDOGAP:1||phase coherence:1||TRANSITIONS:1||Long Josephson junction:1||Charge detection:1||collective resonance modes:1||plasma oscillation modes:1||Superconducting proximity effect:1||Iron pnictide superconductor:1||McMillanRowell oscillations:1||ferromagnetic microstructure:1||superradiant state:1||VOLTAGE:1||branch splitting:1||TENSOR:1||INTERCALATION:1||insitu fabrication:1||NDGAO3:1||DISORDERED METALS:1||GAUGE GLASS:1||LOWTEMPERATURE TRANSPORT:1||spontaneous spin polarization model:1||BIAS:1||emission of electromagnetic waves:1||YBA2CU3O7/PRBA2CU3O7 SUPERLATTICES:1||BOHM:1||SHAPIRO STEPS:1||superconductor/ferromagnet interface:1||OXIDE:1||ANDREEVREFLECTION:1||SinFeAsO single crystal:1||COLLECTIVE MOTION:1||ANGULARDEPENDENCE:1||SUPERCONDUCTIVITY:1||BILAYER GRAPHENE:1||PHOTOLUMINESCENT PROPERTIES:1||SUPERCONDUCTING WEAK LINKS:1||intrinsic Josephson junctions geometrical resonance:1||intrinsic Josephson junction:1||MESOSCOPIC SPINVALVE:1||Bi2212 single crystals:1||intrinsic junctions:1||ANDREEV REFLECTIONS:1||normalmetal/superconductor interface:1||IBI2SR2CACU2OY:1||THERMAL FLUCTUATIONS:1||MIXED STATE:1||BI2.15SR1.85CACU2O8+DELTA:1||intrinsic Josephson effects:1||CACUO:1||QUANTUM POINT CONTACTS:1||resonant tunneling state:1||coherence length:1||NANOWIRE:1||GATES:1||Phase line:1||Thermal activation:1||QUANTUMDOT:1||superconducting proximity effect:1||Andreev interferometer:1||WIRE:1||Josephsonvortexflow branches:1||Bi2212 cuprates:1||LATTICE:1||demannetization effect:1||SUPERCONDUCTING MIRRORS:1||GAS:1||VALLEY TRANSPORT:1||ELECTRODES:1||DEPENDENT TRANSPORT:1||BORNOPPENHEIMER APPROXIMATION:1||collective plasma oscillations:1||fluxon resonance steps:1||STACKS:1||COLLECTIVE DYNAMICS:1||PAIRING SYMMETRY:1||MUON SPIN ROTATION:1||DIMENSIONAL CROSSOVER:1||Bi2Sr2CaCu2Oy highTc superconductors:1||heterojunctions:1||nanostructures:1||surfaces and interfaces:1||QUANTUM TRANSPORT:1||MICROJUNCTIONS:1||RESONATORS:1||STATES:1||FIELD:1||FLUCTUATIONS:1||SCATTERING:1||mode splitting of Josephson vortexflow branches:1||2D superconductivity:1||TRANSISTOR:1||ENERGYGAP:1||SUPERLATTICES:1||IRONBASED SUPERCONDUCTORS:1||PHASEDEPENDENT RESISTANCE:1||QUANTUM PHASETRANSITIONS:1||ELECTRICFIELD:1||HIGH MAGNETICFIELDS:1||NANOWIRE HETEROSTRUCTURES:1||ZNO:1||pair breaking.:1||SUPERCONDUCTING PB:1||domain formation:1||FORCE MICROSCOPY:1||RELAXATION:1||PLASMA RESONANCE:1||coupled Josephson junctions:1||COPPEROXIDE SUPERCONDUCTORS:1||CROSSOVER:1||SIMULATIONS:1||LOWTEMPERATURE:1||CONDUCTORS:1||METALINSULATORTRANSITION:1||SEMICONDUCTOR:1||FIELDEFFECT TRANSISTORS:1||ZEROVOLTAGE STATE:1||constanttemperature interlayer tunneling spectroscopy:1||Josephson supercurrent:1||BIPOLAR SUPERCURRENT:1||Interaction between Josephson and pancake vortices:1||flux jump:1||coaxial heterojunction nanorod:1||Natural Josephson coupling:1||BI2SR2CACU2O8+DELTA:1||VORTEX FLOW:1||TC SUPERCONDUCTORS:1||charge imbalance:1||Andreev diffractometer:1||intercalation:1||surface junction:1||Bi2212:1||tunnelling:1||GRAPHITE:1||GROWTH:1||collective transverse plasma modes:1||GAN:1||Macroscopic quantum tunneling:1||Fluctuation conductivity:1||Abovegap conductance jump:1||Josephson vortex motion:1||Intrinsic Josephson junctions:1||LAYERED SUPERCONDUCTORS:1||BI2SR2CACU2O8+Y:1||INTERFACES:1||BREAKDOWN:1||SYSTEMS:1||Anisotropy ratio:1||Josephson vortex:1||spin relaxation in superconductors:1||bibased single crystals:1||MESOSCOPIC PROXIMITY SUPERCONDUCTOR:1||reentrance of conductance:1||interlayer pair tunneling:1||JOSEPHSON:1||DISORDERED 2DIMENSIONAL SUPERCONDUCTORS:1||INDIUM FILMS:1||excited state:1||REGIME:1||triplet superconductivity:1||FILM:1||SCHOTTKY DIODES:1||peakdiphump structure:1||Kondo effect:1||REENTRANCE:1||Graphene:1||CONTACT:1||BERRYS PHASE:1||2DIMENSIONAL SUPERCONDUCTORS:1||Coulomb diamond:1||magnetic domain:1||spin injection:1||RESONANCE:1||plasma excitation modes:1||FLOW:1||OVERDOPED BI2SR2CACU2O8+DELTA:1||hole doping:1||chemical synthesis:1||phase transitions:1||superconductors:1||VORTEXGLASS SUPERCONDUCTIVITY:1||Kondorelated model:1||RADIATION:1||DOT:1||NANOBELTS:1||Complementarity:1||Closedloop AharonovBohm interferometer:1||pair breaking:1||interlayer phase fluctuation:1||MgB2 thin film:1||CONFINEMENT:1||WALLED CARBON NANOTUBES:1||TRANSITION:9||VORTICES:8||STATE:7||intrinsic Josephson junctions:7||SINGLECRYSTALS:7||JUNCTIONS:5||MODES:5||SUPERCURRENT:5||SUPERCONDUCTOR:5||CONDUCTANCE:5||HIGHTEMPERATURE SUPERCONDUCTORS:5||TRANSPORT:5||PHASE:5||FILMS:4||LOCALIZATION:4||SINGLE DIRAC CONE:4||WIRES:4||MAGNETICFIELD:4||STEPS:3||ELECTRONS:3||proximity effect:3||MODEL:3||ARRAYS:3||INTERFERENCE:3||fluxon dynamics:3||HETEROSTRUCTURES:3||INSULATOR:3||Andreev reflection:3||electronic transport:3||FISKE:3||superconductor:2||ZnO:2||quantum point contact:2||METAL:2||DYNAMICS:2||interlayer Josephson coupling:2||SUPERCONDUCTORS:2||YBA2CU3O7DELTA:2||LAYER:2||DOTS:2||quantum dot:2||Article:2||TRANSISTORS:2||CARBON NANOTUBES:2||GAP:2||MECHANISM:2||LINE:2||GIANT SHAPIRO STEPS:2||LAYERS:2||electron energy loss spectroscopy:2||physical phenomena:2||scanning electron microscopy:2||HGTE QUANTUMWELLS:2||BI2TE3:2||SPECTROSCOPY:2||PNJUNCTIONS:2||spinpolarized tunneling:2||INTRINSIC JOSEPHSONJUNCTIONS:2||FIELDS:2||positive magnetoresistance:2||dilute magnetic semiconductor:2||magnetic field:2||scanning transmission electron microscopy:2||QUANTUM OSCILLATIONS:2||TRANSPORTPROPERTIES:2||surface pair current:2||MAGNETORESISTANCE:2||NANORIBBONS:2||INSTABILITY:2||ANDREEV REFLECTION:2||microwave irradiation:2||vertical graphene josephson junction:2||BI2SE3:2||CONDUCTIVITY:2||highTc superconductors:2||DIMENSIONAL ELECTRONGAS:2||graphene:2||Topological insulators:2||Josephson coupling Fraunhofer interference pattern:2||FERROMAGNET:2||DEPENDENCE:2||DETECTOR:2||COHERENCE:2||INJECTION:2||GRAPHENE:1||JOSEPHSONJUNCTIONS:1||LAYERED SUPERCONDUCTOR:1||mode splitting:1||BEHAVIOR:1||spinpolarized transport:1||SUPERCONDUCTING TRANSITION:1||microwave response:1||PSEUDOGAP:1||phase coherence:1||TRANSITIONS:1||Long Josephson junction:1||Charge detection:1||collective resonance modes:1||plasma oscillation modes:1||Superconducting proximity effect:1||Iron pnictide superconductor:1||McMillanRowell oscillations:1||ferromagnetic microstructure:1||superradiant state:1||VOLTAGE:1||branch splitting:1||TENSOR:1||INTERCALATION:1||insitu fabrication:1||NDGAO3:1||DISORDERED METALS:1||GAUGE GLASS:1||LOWTEMPERATURE TRANSPORT:1||spontaneous spin polarization model:1||BIAS:1||emission of electromagnetic waves:1||YBA2CU3O7/PRBA2CU3O7 SUPERLATTICES:1||BOHM:1||SHAPIRO STEPS:1||superconductor/ferromagnet interface:1||OXIDE:1||ANDREEVREFLECTION:1||SinFeAsO single crystal:1||COLLECTIVE MOTION:1||ANGULARDEPENDENCE:1||SUPERCONDUCTIVITY:1||BILAYER GRAPHENE:1||PHOTOLUMINESCENT PROPERTIES:1||SUPERCONDUCTING WEAK LINKS:1||intrinsic Josephson junctions geometrical resonance:1||intrinsic Josephson junction:1||MESOSCOPIC SPINVALVE:1||Bi2212 single crystals:1||intrinsic junctions:1||ANDREEV REFLECTIONS:1||normalmetal/superconductor interface:1||IBI2SR2CACU2OY:1||THERMAL FLUCTUATIONS:1||MIXED STATE:1||BI2.15SR1.85CACU2O8+DELTA:1||intrinsic Josephson effects:1||CACUO:1||QUANTUM POINT CONTACTS:1||resonant tunneling state:1||coherence length:1||NANOWIRE:1||GATES:1||Phase line:1||Thermal activation:1||QUANTUMDOT:1||superconducting proximity effect:1||Andreev interferometer:1||WIRE:1||Josephsonvortexflow branches:1||Bi2212 cuprates:1||LATTICE:1||demannetization effect:1||SUPERCONDUCTING MIRRORS:1||GAS:1||VALLEY TRANSPORT:1||ELECTRODES:1||DEPENDENT TRANSPORT:1||BORNOPPENHEIMER APPROXIMATION:1||collective plasma oscillations:1||fluxon resonance steps:1||STACKS:1||COLLECTIVE DYNAMICS:1||PAIRING SYMMETRY:1||MUON SPIN ROTATION:1||DIMENSIONAL CROSSOVER:1||Bi2Sr2CaCu2Oy highTc superconductors:1||heterojunctions:1||nanostructures:1||surfaces and interfaces:1||QUANTUM TRANSPORT:1||MICROJUNCTIONS:1||RESONATORS:1||STATES:1||FIELD:1||FLUCTUATIONS:1||SCATTERING:1||mode splitting of Josephson vortexflow branches:1||2D superconductivity:1||TRANSISTOR:1||ENERGYGAP:1||SUPERLATTICES:1||IRONBASED SUPERCONDUCTORS:1||PHASEDEPENDENT RESISTANCE:1||QUANTUM PHASETRANSITIONS:1||ELECTRICFIELD:1||HIGH MAGNETICFIELDS:1||NANOWIRE HETEROSTRUCTURES:1||ZNO:1||pair breaking.:1||SUPERCONDUCTING PB:1||domain formation:1||FORCE MICROSCOPY:1||RELAXATION:1||PLASMA RESONANCE:1||coupled Josephson junctions:1||COPPEROXIDE SUPERCONDUCTORS:1||CROSSOVER:1||SIMULATIONS:1||LOWTEMPERATURE:1||CONDUCTORS:1||METALINSULATORTRANSITION:1||SEMICONDUCTOR:1||FIELDEFFECT TRANSISTORS:1||ZEROVOLTAGE STATE:1||constanttemperature interlayer tunneling spectroscopy:1||Josephson supercurrent:1||BIPOLAR SUPERCURRENT:1||Interaction between Josephson and pancake vortices:1||flux jump:1||coaxial heterojunction nanorod:1||Natural Josephson coupling:1||BI2SR2CACU2O8+DELTA:1||VORTEX FLOW:1||TC SUPERCONDUCTORS:1||charge imbalance:1||Andreev diffractometer:1||intercalation:1||surface junction:1||Bi2212:1||tunnelling:1||GRAPHITE:1||GROWTH:1||collective transverse plasma modes:1||GAN:1||Macroscopic quantum tunneling:1||Fluctuation conductivity:1||Abovegap conductance jump:1||Josephson vortex motion:1||Intrinsic Josephson junctions:1||LAYERED SUPERCONDUCTORS:1||BI2SR2CACU2O8+Y:1||INTERFACES:1||BREAKDOWN:1||SYSTEMS:1||Anisotropy ratio:1||Josephson vortex:1||spin relaxation in superconductors:1||bibased single crystals:1||MESOSCOPIC PROXIMITY SUPERCONDUCTOR:1||reentrance of conductance:1||interlayer pair tunneling:1||JOSEPHSON:1||DISORDERED 2DIMENSIONAL SUPERCONDUCTORS:1||INDIUM FILMS:1||excited state:1||REGIME:1||triplet superconductivity:1||FILM:1||SCHOTTKY DIODES:1||peakdiphump structure:1||Kondo effect:1||REENTRANCE:1||Graphene:1||CONTACT:1||BERRYS PHASE:1||2DIMENSIONAL SUPERCONDUCTORS:1||Coulomb diamond:1||magnetic domain:1||spin injection:1||RESONANCE:1||plasma excitation modes:1||FLOW:1||OVERDOPED BI2SR2CACU2O8+DELTA:1||hole doping:1||chemical synthesis:1||phase transitions:1||superconductors:1||VORTEXGLASS SUPERCONDUCTIVITY:1||Kondorelated model:1||RADIATION:1||DOT:1||NANOBELTS:1||Complementarity:1||Closedloop AharonovBohm interferometer:1||pair breaking:1||interlayer phase fluctuation:1||MgB2 thin film:1||CONFINEMENT:1||WALLED CARBON NANOTUBES:1||TRANSITION:9||VORTICES:8||STATE:7||intrinsic Josephson junctions:7||SINGLECRYSTALS:7||JUNCTIONS:5||MODES:5||SUPERCURRENT:5||SUPERCONDUCTOR:5||CONDUCTANCE:5||HIGHTEMPERATURE SUPERCONDUCTORS:5||TRANSPORT:5||PHASE:5||FILMS:4||LOCALIZATION:4||SINGLE DIRAC CONE:4||WIRES:4||MAGNETICFIELD:4||STEPS:3||ELECTRONS:3||proximity effect:3||MODEL:3||ARRAYS:3||INTERFERENCE:3||fluxon dynamics:3||HETEROSTRUCTURES:3||INSULATOR:3||Andreev reflection:3||electronic transport:3||FISKE:3||superconductor:2||ZnO:2||quantum point contact:2||METAL:2||DYNAMICS:2||interlayer Josephson coupling:2||SUPERCONDUCTORS:2||YBA2CU3O7DELTA:2||LAYER:2||DOTS:2||quantum dot:2||Article:2||TRANSISTORS:2||CARBON NANOTUBES:2||GAP:2||MECHANISM:2||LINE:2||GIANT SHAPIRO STEPS:2||LAYERS:2||electron energy loss spectroscopy:2||physical phenomena:2||scanning electron microscopy:2||HGTE QUANTUMWELLS:2||BI2TE3:2||SPECTROSCOPY:2||PNJUNCTIONS:2||spinpolarized tunneling:2||INTRINSIC JOSEPHSONJUNCTIONS:2||FIELDS:2||positive magnetoresistance:2||dilute magnetic semiconductor:2||magnetic field:2||scanning transmission electron microscopy:2||QUANTUM OSCILLATIONS:2||TRANSPORTPROPERTIES:2||surface pair current:2||MAGNETORESISTANCE:2||NANORIBBONS:2||INSTABILITY:2||ANDREEV REFLECTION:2||microwave irradiation:2||vertical graphene josephson junction:2||BI2SE3:2||CONDUCTIVITY:2||highTc superconductors:2||DIMENSIONAL ELECTRONGAS:2||graphene:2||Topological insulators:2||Josephson coupling Fraunhofer interference pattern:2||FERROMAGNET:2||DEPENDENCE:2||DETECTOR:2||COHERENCE:2||INJECTION:2||GRAPHENE:1||JOSEPHSONJUNCTIONS:1||LAYERED SUPERCONDUCTOR:1||mode splitting:1||BEHAVIOR:1||spinpolarized transport:1||SUPERCONDUCTING TRANSITION:1||microwave response:1||PSEUDOGAP:1||phase coherence:1||TRANSITIONS:1||Long Josephson junction:1||Charge detection:1||collective resonance modes:1||plasma oscillation modes:1||Superconducting proximity effect:1||Iron pnictide superconductor:1||McMillanRowell oscillations:1||ferromagnetic microstructure:1||superradiant state:1||VOLTAGE:1||branch splitting:1||TENSOR:1||INTERCALATION:1||insitu fabrication:1||NDGAO3:1||DISORDERED METALS:1||GAUGE GLASS:1||LOWTEMPERATURE TRANSPORT:1||spontaneous spin polarization model:1||BIAS:1||emission of electromagnetic waves:1||YBA2CU3O7/PRBA2CU3O7 SUPERLATTICES:1||BOHM:1||SHAPIRO STEPS:1||superconductor/ferromagnet interface:1||OXIDE:1||ANDREEVREFLECTION:1||SinFeAsO single crystal:1||COLLECTIVE MOTION:1||ANGULARDEPENDENCE:1||SUPERCONDUCTIVITY:1||BILAYER GRAPHENE:1||PHOTOLUMINESCENT PROPERTIES:1||SUPERCONDUCTING WEAK LINKS:1||intrinsic Josephson junctions geometrical resonance:1||intrinsic Josephson junction:1||MESOSCOPIC SPINVALVE:1||Bi2212 single crystals:1||intrinsic junctions:1||ANDREEV REFLECTIONS:1||normalmetal/superconductor interface:1||IBI2SR2CACU2OY:1||THERMAL FLUCTUATIONS:1||MIXED STATE:1||BI2.15SR1.85CACU2O8+DELTA:1||intrinsic Josephson effects:1||CACUO:1||QUANTUM POINT CONTACTS:1||resonant tunneling state:1||coherence length:1||NANOWIRE:1||GATES:1||Phase line:1||Thermal activation:1||QUANTUMDOT:1||superconducting proximity effect:1||Andreev interferometer:1||WIRE:1||Josephsonvortexflow branches:1||Bi2212 cuprates:1||LATTICE:1||demannetization effect:1||SUPERCONDUCTING MIRRORS:1||GAS:1||VALLEY TRANSPORT:1||ELECTRODES:1||DEPENDENT TRANSPORT:1||BORNOPPENHEIMER APPROXIMATION:1||collective plasma oscillations:1||fluxon resonance steps:1||STACKS:1||COLLECTIVE DYNAMICS:1||PAIRING SYMMETRY:1||MUON SPIN ROTATION:1||DIMENSIONAL CROSSOVER:1||Bi2Sr2CaCu2Oy highTc superconductors:1||heterojunctions:1||nanostructures:1||surfaces and interfaces:1||QUANTUM TRANSPORT:1||MICROJUNCTIONS:1||RESONATORS:1||STATES:1||FIELD:1||FLUCTUATIONS:1||SCATTERING:1||mode splitting of Josephson vortexflow branches:1||2D superconductivity:1||TRANSISTOR:1||ENERGYGAP:1||SUPERLATTICES:1||IRONBASED SUPERCONDUCTORS:1||PHASEDEPENDENT RESISTANCE:1||QUANTUM PHASETRANSITIONS:1||ELECTRICFIELD:1||HIGH MAGNETICFIELDS:1||NANOWIRE HETEROSTRUCTURES:1||ZNO:1||pair breaking.:1||SUPERCONDUCTING PB:1||domain formation:1||FORCE MICROSCOPY:1||RELAXATION:1||PLASMA RESONANCE:1||coupled Josephson junctions:1||COPPEROXIDE SUPERCONDUCTORS:1||CROSSOVER:1||SIMULATIONS:1||LOWTEMPERATURE:1||CONDUCTORS:1||METALINSULATORTRANSITION:1||SEMICONDUCTOR:1||FIELDEFFECT TRANSISTORS:1||ZEROVOLTAGE STATE:1||constanttemperature interlayer tunneling spectroscopy:1||Josephson supercurrent:1||BIPOLAR SUPERCURRENT:1||Interaction between Josephson and pancake vortices:1||flux jump:1||coaxial heterojunction nanorod:1||Natural Josephson coupling:1||BI2SR2CACU2O8+DELTA:1||VORTEX FLOW:1||TC SUPERCONDUCTORS:1||charge imbalance:1||Andreev diffractometer:1||intercalation:1||surface junction:1||Bi2212:1||tunnelling:1||GRAPHITE:1||GROWTH:1||collective transverse plasma modes:1||GAN:1||Macroscopic quantum tunneling:1||Fluctuation conductivity:1||Abovegap conductance jump:1||Josephson vortex motion:1||Intrinsic Josephson junctions:1||LAYERED SUPERCONDUCTORS:1||BI2SR2CACU2O8+Y:1||INTERFACES:1||BREAKDOWN:1||SYSTEMS:1||Anisotropy ratio:1||Josephson vortex:1||spin relaxation in superconductors:1||bibased single crystals:1||MESOSCOPIC PROXIMITY SUPERCONDUCTOR:1||reentrance of conductance:1||interlayer pair tunneling:1||JOSEPHSON:1||DISORDERED 2DIMENSIONAL SUPERCONDUCTORS:1||INDIUM FILMS:1||excited state:1||REGIME:1||triplet superconductivity:1||FILM:1||SCHOTTKY DIODES:1||peakdiphump structure:1||Kondo effect:1||REENTRANCE:1||Graphene:1||CONTACT:1||BERRYS PHASE:1||2DIMENSIONAL SUPERCONDUCTORS:1||Coulomb diamond:1||magnetic domain:1||spin injection:1||RESONANCE:1||plasma excitation modes:1||FLOW:1||OVERDOPED BI2SR2CACU2O8+DELTA:1||hole doping:1||chemical synthesis:1||phase transitions:1||superconductors:1||VORTEXGLASS SUPERCONDUCTIVITY:1||Kondorelated model:1||RADIATION:1||DOT:1||NANOBELTS:1||Complementarity:1||Closedloop AharonovBohm interferometer:1||pair breaking:1||interlayer phase fluctuation:1||MgB2 thin film:1||CONFINEMENT:1||WALLED CARBON NANOTUBES:1||TRANSITION:9||VORTICES:8||STATE:7||intrinsic Josephson junctions:7||SINGLECRYSTALS:7||JUNCTIONS:5||MODES:5||SUPERCURRENT:5||SUPERCONDUCTOR:5||CONDUCTANCE:5||HIGHTEMPERATURE SUPERCONDUCTORS:5||TRANSPORT:5||PHASE:5||FILMS:4||LOCALIZATION:4||SINGLE DIRAC CONE:4||WIRES:4||MAGNETICFIELD:4||STEPS:3||ELECTRONS:3||proximity effect:3||MODEL:3||ARRAYS:3||INTERFERENCE:3||fluxon dynamics:3||HETEROSTRUCTURES:3||INSULATOR:3||Andreev reflection:3||electronic transport:3||FISKE:3||superconductor:2||ZnO:2||quantum point contact:2||METAL:2||DYNAMICS:2||interlayer Josephson coupling:2||SUPERCONDUCTORS:2||YBA2CU3O7DELTA:2||LAYER:2||DOTS:2||quantum dot:2||Article:2||TRANSISTORS:2||CARBON NANOTUBES:2||GAP:2||MECHANISM:2||LINE:2||GIANT SHAPIRO STEPS:2||LAYERS:2||electron energy loss spectroscopy:2||physical phenomena:2||scanning electron microscopy:2||HGTE QUANTUMWELLS:2||BI2TE3:2||SPECTROSCOPY:2||PNJUNCTIONS:2||spinpolarized tunneling:2||INTRINSIC JOSEPHSONJUNCTIONS:2||FIELDS:2||positive magnetoresistance:2||dilute magnetic semiconductor:2||magnetic field:2||scanning transmission electron microscopy:2||QUANTUM OSCILLATIONS:2||TRANSPORTPROPERTIES:2||surface pair current:2||MAGNETORESISTANCE:2||NANORIBBONS:2||INSTABILITY:2||ANDREEV REFLECTION:2||microwave irradiation:2||vertical graphene josephson junction:2||BI2SE3:2||CONDUCTIVITY:2||highTc superconductors:2||DIMENSIONAL ELECTRONGAS:2||graphene:2||Topological insulators:2||Josephson coupling Fraunhofer interference pattern:2||FERROMAGNET:2||DEPENDENCE:2||DETECTOR:2||COHERENCE:2||INJECTION:2||GRAPHENE:1||JOSEPHSONJUNCTIONS:1||LAYERED SUPERCONDUCTOR:1||mode splitting:1||BEHAVIOR:1||spinpolarized transport:1||SUPERCONDUCTING TRANSITION:1||microwave response:1||PSEUDOGAP:1||phase coherence:1||TRANSITIONS:1||Long Josephson junction:1||Charge detection:1||collective resonance modes:1||plasma oscillation modes:1||Superconducting proximity effect:1||Iron pnictide superconductor:1||McMillanRowell oscillations:1||ferromagnetic microstructure:1||superradiant state:1||VOLTAGE:1||branch splitting:1||TENSOR:1||INTERCALATION:1||insitu fabrication:1||NDGAO3:1||DISORDERED METALS:1||GAUGE GLASS:1||LOWTEMPERATURE TRANSPORT:1||spontaneous spin polarization model:1||BIAS:1||emission of electromagnetic waves:1||YBA2CU3O7/PRBA2CU3O7 SUPERLATTICES:1||BOHM:1||SHAPIRO STEPS:1||superconductor/ferromagnet interface:1||OXIDE:1||ANDREEVREFLECTION:1||SinFeAsO single crystal:1||COLLECTIVE MOTION:1||ANGULARDEPENDENCE:1||SUPERCONDUCTIVITY:1||BILAYER GRAPHENE:1||PHOTOLUMINESCENT PROPERTIES:1||SUPERCONDUCTING WEAK LINKS:1||intrinsic Josephson junctions geometrical resonance:1||intrinsic Josephson junction:1||MESOSCOPIC SPINVALVE:1||Bi2212 single crystals:1||intrinsic junctions:1||ANDREEV REFLECTIONS:1||normalmetal/superconductor interface:1||IBI2SR2CACU2OY:1||THERMAL FLUCTUATIONS:1||MIXED STATE:1||BI2.15SR1.85CACU2O8+DELTA:1||intrinsic Josephson effects:1||CACUO:1||QUANTUM POINT CONTACTS:1||resonant tunneling state:1||coherence length:1||NANOWIRE:1||GATES:1||Phase line:1||Thermal activation:1||QUANTUMDOT:1||superconducting proximity effect:1||Andreev interferometer:1||WIRE:1||Josephsonvortexflow branches:1||Bi2212 cuprates:1||LATTICE:1||demannetization effect:1||SUPERCONDUCTING MIRRORS:1||GAS:1||VALLEY TRANSPORT:1||ELECTRODES:1||DEPENDENT TRANSPORT:1||BORNOPPENHEIMER APPROXIMATION:1||collective plasma oscillations:1||fluxon resonance steps:1||STACKS:1||COLLECTIVE DYNAMICS:1||PAIRING SYMMETRY:1||MUON SPIN ROTATION:1||DIMENSIONAL CROSSOVER:1||Bi2Sr2CaCu2Oy highTc superconductors:1||heterojunctions:1||nanostructures:1||surfaces and interfaces:1||QUANTUM TRANSPORT:1||MICROJUNCTIONS:1||RESONATORS:1||STATES:1||FIELD:1||FLUCTUATIONS:1||SCATTERING:1||mode splitting of Josephson vortexflow branches:1||2D superconductivity:1||TRANSISTOR:1||ENERGYGAP:1||SUPERLATTICES:1||IRONBASED SUPERCONDUCTORS:1||PHASEDEPENDENT RESISTANCE:1||QUANTUM PHASETRANSITIONS:1||ELECTRICFIELD:1||HIGH MAGNETICFIELDS:1||NANOWIRE HETEROSTRUCTURES:1||ZNO:1||pair breaking.:1||SUPERCONDUCTING PB:1||domain formation:1||FORCE MICROSCOPY:1||RELAXATION:1||PLASMA RESONANCE:1||coupled Josephson junctions:1||COPPEROXIDE SUPERCONDUCTORS:1||CROSSOVER:1||SIMULATIONS:1||LOWTEMPERATURE:1||CONDUCTORS:1||METALINSULATORTRANSITION:1||SEMICONDUCTOR:1||FIELDEFFECT TRANSISTORS:1||ZEROVOLTAGE STATE:1||constanttemperature interlayer tunneling spectroscopy:1||Josephson supercurrent:1||BIPOLAR SUPERCURRENT:1||Interaction between Josephson and pancake vortices:1||flux jump:1||coaxial heterojunction nanorod:1||Natural Josephson coupling:1||BI2SR2CACU2O8+DELTA:1||VORTEX FLOW:1||TC SUPERCONDUCTORS:1||charge imbalance:1||Andreev diffractometer:1||intercalation:1||surface junction:1||Bi2212:1||tunnelling:1||GRAPHITE:1||GROWTH:1||collective transverse plasma modes:1||GAN:1||Macroscopic quantum tunneling:1||Fluctuation conductivity:1||Abovegap conductance jump:1||Josephson vortex motion:1||Intrinsic Josephson junctions:1||LAYERED SUPERCONDUCTORS:1||BI2SR2CACU2O8+Y:1||INTERFACES:1||BREAKDOWN:1||SYSTEMS:1||Anisotropy ratio:1||Josephson vortex:1||spin relaxation in superconductors:1||bibased single crystals:1||MESOSCOPIC PROXIMITY SUPERCONDUCTOR:1||reentrance of conductance:1||interlayer pair tunneling:1||JOSEPHSON:1||DISORDERED 2DIMENSIONAL SUPERCONDUCTORS:1||INDIUM FILMS:1||excited state:1||REGIME:1||triplet superconductivity:1||FILM:1||SCHOTTKY DIODES:1||peakdiphump structure:1||Kondo effect:1||REENTRANCE:1||Graphene:1||CONTACT:1||BERRYS PHASE:1||2DIMENSIONAL SUPERCONDUCTORS:1||Coulomb diamond:1||magnetic domain:1||spin injection:1||RESONANCE:1||plasma excitation modes:1||FLOW:1||OVERDOPED BI2SR2CACU2O8+DELTA:1||hole doping:1||chemical synthesis:1||phase transitions:1||superconductors:1||VORTEXGLASS SUPERCONDUCTIVITY:1||Kondorelated model:1||RADIATION:1||DOT:1||NANOBELTS:1||Complementarity:1||Closedloop AharonovBohm interferometer:1||pair breaking:1||interlayer phase fluctuation:1||MgB2 thin film:1||CONFINEMENT:1||WALLED CARBON NANOTUBES:1||TRANSITION:9||VORTICES:8||STATE:7||intrinsic Josephson junctions:7||SINGLECRYSTALS:7||JUNCTIONS:5||MODES:5||SUPERCURRENT:5||SUPERCONDUCTOR:5||CONDUCTANCE:5||HIGHTEMPERATURE SUPERCONDUCTORS:5||TRANSPORT:5||PHASE:5||FILMS:4||LOCALIZATION:4||SINGLE DIRAC CONE:4||WIRES:4||MAGNETICFIELD:4||STEPS:3||ELECTRONS:3||proximity effect:3||MODEL:3||ARRAYS:3||INTERFERENCE:3||fluxon dynamics:3||HETEROSTRUCTURES:3||INSULATOR:3||Andreev reflection:3||electronic transport:3||FISKE:3||superconductor:2||ZnO:2||quantum point contact:2||METAL:2||DYNAMICS:2||interlayer Josephson coupling:2||SUPERCONDUCTORS:2||YBA2CU3O7DELTA:2||LAYER:2||DOTS:2||quantum dot:2||Article:2||TRANSISTORS:2||CARBON NANOTUBES:2||GAP:2||MECHANISM:2||LINE:2||GIANT SHAPIRO STEPS:2||LAYERS:2||electron energy loss spectroscopy:2||physical phenomena:2||scanning electron microscopy:2||HGTE QUANTUMWELLS:2||BI2TE3:2||SPECTROSCOPY:2||PNJUNCTIONS:2||spinpolarized tunneling:2||INTRINSIC JOSEPHSONJUNCTIONS:2||FIELDS:2||positive magnetoresistance:2||dilute magnetic semiconductor:2||magnetic field:2||scanning transmission electron microscopy:2||QUANTUM OSCILLATIONS:2||TRANSPORTPROPERTIES:2||surface pair current:2||MAGNETORESISTANCE:2||NANORIBBONS:2||INSTABILITY:2||ANDREEV REFLECTION:2||microwave irradiation:2||vertical graphene josephson junction:2||BI2SE3:2||CONDUCTIVITY:2||highTc superconductors:2||DIMENSIONAL ELECTRONGAS:2||graphene:2||Topological insulators:2||Josephson coupling Fraunhofer interference pattern:2||FERROMAGNET:2||DEPENDENCE:2||DETECTOR:2||COHERENCE:2||INJECTION:2||GRAPHENE:1||JOSEPHSONJUNCTIONS:1||LAYERED SUPERCONDUCTOR:1||mode splitting:1||BEHAVIOR:1||spinpolarized transport:1||SUPERCONDUCTING TRANSITION:1||microwave response:1||PSEUDOGAP:1||phase coherence:1||TRANSITIONS:1||Long Josephson junction:1||Charge detection:1||collective resonance modes:1||plasma oscillation modes:1||Superconducting proximity effect:1||Iron pnictide superconductor:1||McMillanRowell oscillations:1||ferromagnetic microstructure:1||superradiant state:1||VOLTAGE:1||branch splitting:1||TENSOR:1||INTERCALATION:1||insitu fabrication:1||NDGAO3:1||DISORDERED METALS:1||GAUGE GLASS:1||LOWTEMPERATURE TRANSPORT:1||spontaneous spin polarization model:1||BIAS:1||emission of electromagnetic waves:1||YBA2CU3O7/PRBA2CU3O7 SUPERLATTICES:1||BOHM:1||SHAPIRO STEPS:1||superconductor/ferromagnet interface:1||OXIDE:1||ANDREEVREFLECTION:1||SinFeAsO single crystal:1||COLLECTIVE MOTION:1||ANGULARDEPENDENCE:1||SUPERCONDUCTIVITY:1||BILAYER GRAPHENE:1||PHOTOLUMINESCENT PROPERTIES:1||SUPERCONDUCTING WEAK LINKS:1||intrinsic Josephson junctions geometrical resonance:1||intrinsic Josephson junction:1||MESOSCOPIC SPINVALVE:1||Bi2212 single crystals:1||intrinsic junctions:1||ANDREEV REFLECTIONS:1||normalmetal/superconductor interface:1||IBI2SR2CACU2OY:1||THERMAL FLUCTUATIONS:1||MIXED STATE:1||BI2.15SR1.85CACU2O8+DELTA:1||intrinsic Josephson effects:1||CACUO:1||QUANTUM POINT CONTACTS:1||resonant tunneling state:1||coherence length:1||NANOWIRE:1||GATES:1||Phase line:1||Thermal activation:1||QUANTUMDOT:1||superconducting proximity effect:1||Andreev interferometer:1||WIRE:1||Josephsonvortexflow branches:1||Bi2212 cuprates:1||LATTICE:1||demannetization effect:1||SUPERCONDUCTING MIRRORS:1||GAS:1||VALLEY TRANSPORT:1||ELECTRODES:1||DEPENDENT TRANSPORT:1||BORNOPPENHEIMER APPROXIMATION:1||collective plasma oscillations:1||fluxon resonance steps:1||STACKS:1||COLLECTIVE DYNAMICS:1||PAIRING SYMMETRY:1||MUON SPIN ROTATION:1||DIMENSIONAL CROSSOVER:1||Bi2Sr2CaCu2Oy highTc superconductors:1||heterojunctions:1||nanostructures:1||surfaces and interfaces:1||QUANTUM TRANSPORT:1||MICROJUNCTIONS:1||RESONATORS:1||STATES:1||FIELD:1||FLUCTUATIONS:1||SCATTERING:1||mode splitting of Josephson vortexflow branches:1||2D superconductivity:1||TRANSISTOR:1||ENERGYGAP:1||SUPERLATTICES:1||IRONBASED SUPERCONDUCTORS:1||PHASEDEPENDENT RESISTANCE:1||QUANTUM PHASETRANSITIONS:1||ELECTRICFIELD:1||HIGH MAGNETICFIELDS:1||NANOWIRE HETEROSTRUCTURES:1||ZNO:1||pair breaking.:1||SUPERCONDUCTING PB:1||domain formation:1||FORCE MICROSCOPY:1||RELAXATION:1||PLASMA RESONANCE:1||coupled Josephson junctions:1||COPPEROXIDE SUPERCONDUCTORS:1||CROSSOVER:1||SIMULATIONS:1||LOWTEMPERATURE:1||CONDUCTORS:1||METALINSULATORTRANSITION:1||SEMICONDUCTOR:1||FIELDEFFECT TRANSISTORS:1||ZEROVOLTAGE STATE:1||constanttemperature interlayer tunneling spectroscopy:1||Josephson supercurrent:1||BIPOLAR SUPERCURRENT:1||Interaction between Josephson and pancake vortices:1||flux jump:1||coaxial heterojunction nanorod:1||Natural Josephson coupling:1||BI2SR2CACU2O8+DELTA:1||VORTEX FLOW:1||TC SUPERCONDUCTORS:1||charge imbalance:1||Andreev diffractometer:1||intercalation:1||surface junction:1||Bi2212:1||tunnelling:1||GRAPHITE:1||GROWTH:1||collective transverse plasma modes:1||GAN:1||Macroscopic quantum tunneling:1||Fluctuation conductivity:1||Abovegap conductance jump:1||Josephson vortex motion:1||Intrinsic Josephson junctions:1||LAYERED SUPERCONDUCTORS:1||BI2SR2CACU2O8+Y:1||INTERFACES:1||BREAKDOWN:1||SYSTEMS:1||Anisotropy ratio:1||Josephson vortex:1||spin relaxation in superconductors:1||bibased single crystals:1||MESOSCOPIC PROXIMITY SUPERCONDUCTOR:1||reentrance of conductance:1||interlayer pair tunneling:1||JOSEPHSON:1||DISORDERED 2DIMENSIONAL SUPERCONDUCTORS:1||INDIUM FILMS:1||excited state:1||REGIME:1||triplet superconductivity:1||FILM:1||SCHOTTKY DIODES:1||peakdiphump structure:1||Kondo effect:1||REENTRANCE:1||Graphene:1||CONTACT:1||BERRYS PHASE:1||2DIMENSIONAL SUPERCONDUCTORS:1||Coulomb diamond:1||magnetic domain:1||spin injection:1||RESONANCE:1||plasma excitation modes:1||FLOW:1||OVERDOPED BI2SR2CACU2O8+DELTA:1||hole doping:1||chemical synthesis:1||phase transitions:1||superconductors:1||VORTEXGLASS SUPERCONDUCTIVITY:1||Kondorelated model:1||RADIATION:1||DOT:1||NANOBELTS:1||Complementarity:1||Closedloop AharonovBohm interferometer:1||pair breaking:1||interlayer phase fluctuation:1||MgB2 thin film:1||CONFINEMENT:1||WALLED CARBON NANOTUBES:1||TRANSITION:9||VORTICES:8||STATE:7||intrinsic Josephson junctions:7||SINGLECRYSTALS:7||JUNCTIONS:5||MODES:5||SUPERCURRENT:5||SUPERCONDUCTOR:5||CONDUCTANCE:5||HIGHTEMPERATURE SUPERCONDUCTORS:5||TRANSPORT:5||PHASE:5||FILMS:4||LOCALIZATION:4||SINGLE DIRAC CONE:4||WIRES:4||MAGNETICFIELD:4||STEPS:3||ELECTRONS:3||proximity effect:3||MODEL:3||ARRAYS:3||INTERFERENCE:3||fluxon dynamics:3||HETEROSTRUCTURES:3||INSULATOR:3||Andreev reflection:3||electronic transport:3||FISKE:3||superconductor:2||ZnO:2||quantum point contact:2||METAL:2||DYNAMICS:2||interlayer Josephson coupling:2||SUPERCONDUCTORS:2||YBA2CU3O7DELTA:2||LAYER:2||DOTS:2||quantum dot:2||Article:2||TRANSISTORS:2||CARBON NANOTUBES:2||GAP:2||MECHANISM:2||LINE:2||GIANT SHAPIRO STEPS:2||LAYERS:2||electron energy loss spectroscopy:2||physical phenomena:2||scanning electron microscopy:2||HGTE QUANTUMWELLS:2||BI2TE3:2||SPECTROSCOPY:2||PNJUNCTIONS:2||spinpolarized tunneling:2||INTRINSIC JOSEPHSONJUNCTIONS:2||FIELDS:2||positive magnetoresistance:2||dilute magnetic semiconductor:2||magnetic field:2||scanning transmission electron microscopy:2||QUANTUM OSCILLATIONS:2||TRANSPORTPROPERTIES:2||surface pair current:2||MAGNETORESISTANCE:2||NANORIBBONS:2||INSTABILITY:2||ANDREEV REFLECTION:2||microwave irradiation:2||vertical graphene josephson junction:2||BI2SE3:2||CONDUCTIVITY:2||highTc superconductors:2||DIMENSIONAL ELECTRONGAS:2||graphene:2||Topological insulators:2||Josephson coupling Fraunhofer interference pattern:2||FERROMAGNET:2||DEPENDENCE:2||DETECTOR:2||COHERENCE:2||INJECTION:2||GRAPHENE:1||JOSEPHSONJUNCTIONS:1||LAYERED SUPERCONDUCTOR:1||mode splitting:1||BEHAVIOR:1||spinpolarized transport:1||SUPERCONDUCTING TRANSITION:1||microwave response:1||PSEUDOGAP:1||phase coherence:1||TRANSITIONS:1||Long Josephson junction:1||Charge detection:1||collective resonance modes:1||plasma oscillation modes:1||Superconducting proximity effect:1||Iron pnictide superconductor:1||McMillanRowell oscillations:1||ferromagnetic microstructure:1||superradiant state:1||VOLTAGE:1||branch splitting:1||TENSOR:1||INTERCALATION:1||insitu fabrication:1||NDGAO3:1||DISORDERED METALS:1||GAUGE GLASS:1||LOWTEMPERATURE TRANSPORT:1||spontaneous spin polarization model:1||BIAS:1||emission of electromagnetic waves:1||YBA2CU3O7/PRBA2CU3O7 SUPERLATTICES:1||BOHM:1||SHAPIRO STEPS:1||superconductor/ferromagnet interface:1||OXIDE:1||ANDREEVREFLECTION:1||SinFeAsO single crystal:1||COLLECTIVE MOTION:1||ANGULARDEPENDENCE:1||SUPERCONDUCTIVITY:1||BILAYER GRAPHENE:1||PHOTOLUMINESCENT PROPERTIES:1||SUPERCONDUCTING WEAK LINKS:1||intrinsic Josephson junctions geometrical resonance:1||intrinsic Josephson junction:1||MESOSCOPIC SPINVALVE:1||Bi2212 single crystals:1||intrinsic junctions:1||ANDREEV REFLECTIONS:1||normalmetal/superconductor interface:1||IBI2SR2CACU2OY:1||THERMAL FLUCTUATIONS:1||MIXED STATE:1||BI2.15SR1.85CACU2O8+DELTA:1||intrinsic Josephson effects:1||CACUO:1||QUANTUM POINT CONTACTS:1||resonant tunneling state:1||coherence length:1||NANOWIRE:1||GATES:1||Phase line:1||Thermal activation:1||QUANTUMDOT:1||superconducting proximity effect:1||Andreev interferometer:1||WIRE:1||Josephsonvortexflow branches:1||Bi2212 cuprates:1||LATTICE:1||demannetization effect:1||SUPERCONDUCTING MIRRORS:1||GAS:1||VALLEY TRANSPORT:1||ELECTRODES:1||DEPENDENT TRANSPORT:1||BORNOPPENHEIMER APPROXIMATION:1||collective plasma oscillations:1||fluxon resonance steps:1||STACKS:1||COLLECTIVE DYNAMICS:1||PAIRING SYMMETRY:1||MUON SPIN ROTATION:1||DIMENSIONAL CROSSOVER:1||Bi2Sr2CaCu2Oy highTc superconductors:1||heterojunctions:1||nanostructures:1||surfaces and interfaces:1||QUANTUM TRANSPORT:1||MICROJUNCTIONS:1||RESONATORS:1||STATES:1||FIELD:1||FLUCTUATIONS:1||SCATTERING:1||mode splitting of Josephson vortexflow branches:1||2D superconductivity:1||TRANSISTOR:1||ENERGYGAP:1||SUPERLATTICES:1||IRONBASED SUPERCONDUCTORS:1||PHASEDEPENDENT RESISTANCE:1||QUANTUM PHASETRANSITIONS:1||ELECTRICFIELD:1||HIGH MAGNETICFIELDS:1||NANOWIRE HETEROSTRUCTURES:1||ZNO:1||pair breaking.:1||SUPERCONDUCTING PB:1||domain formation:1||FORCE MICROSCOPY:1||RELAXATION:1||PLASMA RESONANCE:1||coupled Josephson junctions:1||COPPEROXIDE SUPERCONDUCTORS:1||CROSSOVER:1||SIMULATIONS:1||LOWTEMPERATURE:1||CONDUCTORS:1||METALINSULATORTRANSITION:1||SEMICONDUCTOR:1||FIELDEFFECT TRANSISTORS:1||ZEROVOLTAGE STATE:1||constanttemperature interlayer tunneling spectroscopy:1||Josephson supercurrent:1||BIPOLAR SUPERCURRENT:1||Interaction between Josephson and pancake vortices:1||flux jump:1||coaxial heterojunction nanorod:1||Natural Josephson coupling:1||BI2SR2CACU2O8+DELTA:1||VORTEX FLOW:1||TC SUPERCONDUCTORS:1||charge imbalance:1||Andreev diffractometer:1||intercalation:1||surface junction:1||Bi2212:1||tunnelling:1||GRAPHITE:1||GROWTH:1||collective transverse plasma modes:1||GAN:1||Macroscopic quantum tunneling:1||Fluctuation conductivity:1||Abovegap conductance jump:1||Josephson vortex motion:1||Intrinsic Josephson junctions:1||LAYERED SUPERCONDUCTORS:1||BI2SR2CACU2O8+Y:1||INTERFACES:1||BREAKDOWN:1||SYSTEMS:1||Anisotropy ratio:1||Josephson vortex:1||spin relaxation in superconductors:1||bibased single crystals:1||MESOSCOPIC PROXIMITY SUPERCONDUCTOR:1||reentrance of conductance:1||interlayer pair tunneling:1||JOSEPHSON:1||DISORDERED 2DIMENSIONAL SUPERCONDUCTORS:1||INDIUM FILMS:1||excited state:1||REGIME:1||triplet superconductivity:1||FILM:1||SCHOTTKY DIODES:1||peakdiphump structure:1||Kondo effect:1||REENTRANCE:1||Graphene:1||CONTACT:1||BERRYS PHASE:1||2DIMENSIONAL SUPERCONDUCTORS:1||Coulomb diamond:1||magnetic domain:1||spin injection:1||RESONANCE:1||plasma excitation modes:1||FLOW:1||OVERDOPED BI2SR2CACU2O8+DELTA:1||hole doping:1||chemical synthesis:1||phase transitions:1||superconductors:1||VORTEXGLASS SUPERCONDUCTIVITY:1||Kondorelated model:1||RADIATION:1||DOT:1||NANOBELTS:1||Complementarity:1||Closedloop AharonovBohm interferometer:1||pair breaking:1||interlayer phase fluctuation:1||MgB2 thin film:1||CONFINEMENT:1||WALLED CARBON NANOTUBES:1||TRANSITION:9||VORTICES:8||STATE:7||intrinsic Josephson junctions:7||SINGLECRYSTALS:7||JUNCTIONS:5||MODES:5||SUPERCURRENT:5||SUPERCONDUCTOR:5||CONDUCTANCE:5||HIGHTEMPERATURE SUPERCONDUCTORS:5||TRANSPORT:5||PHASE:5||FILMS:4||LOCALIZATION:4||SINGLE DIRAC CONE:4||WIRES:4||MAGNETICFIELD:4||STEPS:3||ELECTRONS:3||proximity effect:3||MODEL:3||ARRAYS:3||INTERFERENCE:3||fluxon dynamics:3||HETEROSTRUCTURES:3||INSULATOR:3||Andreev reflection:3||electronic transport:3||FISKE:3||superconductor:2||ZnO:2||quantum point contact:2||METAL:2||DYNAMICS:2||interlayer Josephson coupling:2||SUPERCONDUCTORS:2||YBA2CU3O7DELTA:2||LAYER:2||DOTS:2||quantum dot:2||Article:2||TRANSISTORS:2||CARBON NANOTUBES:2||GAP:2||MECHANISM:2||LINE:2||GIANT SHAPIRO STEPS:2||LAYERS:2||electron energy loss spectroscopy:2||physical phenomena:2||scanning electron microscopy:2||HGTE QUANTUMWELLS:2||BI2TE3:2||SPECTROSCOPY:2||PNJUNCTIONS:2||spinpolarized tunneling:2||INTRINSIC JOSEPHSONJUNCTIONS:2||FIELDS:2||positive magnetoresistance:2||dilute magnetic semiconductor:2||magnetic field:2||scanning transmission electron microscopy:2||QUANTUM OSCILLATIONS:2||TRANSPORTPROPERTIES:2||surface pair current:2||MAGNETORESISTANCE:2||NANORIBBONS:2||INSTABILITY:2||ANDREEV REFLECTION:2||microwave irradiation:2||vertical graphene josephson junction:2||BI2SE3:2||CONDUCTIVITY:2||highTc superconductors:2||DIMENSIONAL ELECTRONGAS:2||graphene:2||Topological insulators:2||Josephson coupling Fraunhofer interference pattern:2||FERROMAGNET:2||DEPENDENCE:2||DETECTOR:2||COHERENCE:2||INJECTION:2||GRAPHENE:1||JOSEPHSONJUNCTIONS:1||LAYERED SUPERCONDUCTOR:1||mode splitting:1||BEHAVIOR:1||spinpolarized transport:1||SUPERCONDUCTING TRANSITION:1||microwave response:1||PSEUDOGAP:1||phase coherence:1||TRANSITIONS:1||Long Josephson junction:1||Charge detection:1||collective resonance modes:1||plasma oscillation modes:1||Superconducting proximity effect:1||Iron pnictide superconductor:1||McMillanRowell oscillations:1||ferromagnetic microstructure:1||superradiant state:1||VOLTAGE:1||branch splitting:1||TENSOR:1||INTERCALATION:1||insitu fabrication:1||NDGAO3:1||DISORDERED METALS:1||GAUGE GLASS:1||LOWTEMPERATURE TRANSPORT:1||spontaneous spin polarization model:1||BIAS:1||emission of electromagnetic waves:1||YBA2CU3O7/PRBA2CU3O7 SUPERLATTICES:1||BOHM:1||SHAPIRO STEPS:1||superconductor/ferromagnet interface:1||OXIDE:1||ANDREEVREFLECTION:1||SinFeAsO single crystal:1||COLLECTIVE MOTION:1||ANGULARDEPENDENCE:1||SUPERCONDUCTIVITY:1||BILAYER GRAPHENE:1||PHOTOLUMINESCENT PROPERTIES:1||SUPERCONDUCTING WEAK LINKS:1||intrinsic Josephson junctions geometrical resonance:1||intrinsic Josephson junction:1||MESOSCOPIC SPINVALVE:1||Bi2212 single crystals:1||intrinsic junctions:1||ANDREEV REFLECTIONS:1||normalmetal/superconductor interface:1||IBI2SR2CACU2OY:1||THERMAL FLUCTUATIONS:1||MIXED STATE:1||BI2.15SR1.85CACU2O8+DELTA:1||intrinsic Josephson effects:1||CACUO:1||QUANTUM POINT CONTACTS:1||resonant tunneling state:1||coherence length:1||NANOWIRE:1||GATES:1||Phase line:1||Thermal activation:1||QUANTUMDOT:1||superconducting proximity effect:1||Andreev interferometer:1||WIRE:1||Josephsonvortexflow branches:1||Bi2212 cuprates:1||LATTICE:1||demannetization effect:1||SUPERCONDUCTING MIRRORS:1||GAS:1||VALLEY TRANSPORT:1||ELECTRODES:1||DEPENDENT TRANSPORT:1||BORNOPPENHEIMER APPROXIMATION:1||collective plasma oscillations:1||fluxon resonance steps:1||STACKS:1||COLLECTIVE DYNAMICS:1||PAIRING SYMMETRY:1||MUON SPIN ROTATION:1||DIMENSIONAL CROSSOVER:1||Bi2Sr2CaCu2Oy highTc superconductors:1||heterojunctions:1||nanostructures:1||surfaces and interfaces:1||QUANTUM TRANSPORT:1||MICROJUNCTIONS:1||RESONATORS:1||STATES:1||FIELD:1||FLUCTUATIONS:1||SCATTERING:1||mode splitting of Josephson vortexflow branches:1||2D superconductivity:1||TRANSISTOR:1||ENERGYGAP:1||SUPERLATTICES:1||IRONBASED SUPERCONDUCTORS:1||PHASEDEPENDENT RESISTANCE:1||QUANTUM PHASETRANSITIONS:1||ELECTRICFIELD:1||HIGH MAGNETICFIELDS:1||NANOWIRE HETEROSTRUCTURES:1||ZNO:1||pair breaking.:1||SUPERCONDUCTING PB:1||domain formation:1||FORCE MICROSCOPY:1||RELAXATION:1||PLASMA RESONANCE:1||coupled Josephson junctions:1||COPPEROXIDE SUPERCONDUCTORS:1||CROSSOVER:1||SIMULATIONS:1||LOWTEMPERATURE:1||CONDUCTORS:1||METALINSULATORTRANSITION:1||SEMICONDUCTOR:1||FIELDEFFECT TRANSISTORS:1||ZEROVOLTAGE STATE:1||constanttemperature interlayer tunneling spectroscopy:1||Josephson supercurrent:1||BIPOLAR SUPERCURRENT:1||Interaction between Josephson and pancake vortices:1||flux jump:1||coaxial heterojunction nanorod:1||Natural Josephson coupling:1||BI2SR2CACU2O8+DELTA:1||VORTEX FLOW:1||TC SUPERCONDUCTORS:1||charge imbalance:1||Andreev diffractometer:1||intercalation:1||surface junction:1||Bi2212:1||tunnelling:1||GRAPHITE:1||GROWTH:1||collective transverse plasma modes:1||GAN:1||Macroscopic quantum tunneling:1||Fluctuation conductivity:1||Abovegap conductance jump:1||Josephson vortex motion:1||Intrinsic Josephson junctions:1||LAYERED SUPERCONDUCTORS:1||BI2SR2CACU2O8+Y:1||INTERFACES:1||BREAKDOWN:1||SYSTEMS:1||Anisotropy ratio:1||Josephson vortex:1||spin relaxation in superconductors:1||bibased single crystals:1||MESOSCOPIC PROXIMITY SUPERCONDUCTOR:1||reentrance of conductance:1||interlayer pair tunneling:1||JOSEPHSON:1||DISORDERED 2DIMENSIONAL SUPERCONDUCTORS:1||INDIUM FILMS:1||excited state:1||REGIME:1||triplet superconductivity:1||FILM:1||SCHOTTKY DIODES:1||peakdiphump structure:1||Kondo effect:1||REENTRANCE:1||Graphene:1||CONTACT:1||BERRYS PHASE:1||2DIMENSIONAL SUPERCONDUCTORS:1||Coulomb diamond:1||magnetic domain:1||spin injection:1||RESONANCE:1||plasma excitation modes:1||FLOW:1||OVERDOPED BI2SR2CACU2O8+DELTA:1||hole doping:1||chemical synthesis:1||phase transitions:1||superconductors:1||VORTEXGLASS SUPERCONDUCTIVITY:1||Kondorelated model:1||RADIATION:1||DOT:1||NANOBELTS:1||Complementarity:1||Closedloop AharonovBohm interferometer:1||pair breaking:1||interlayer phase fluctuation:1||MgB2 thin film:1||CONFINEMENT:1||WALLED CARBON NANOTUBES:1||TRANSITION:9||VORTICES:8||STATE:7||intrinsic Josephson junctions:7||SINGLECRYSTALS:7||JUNCTIONS:5||MODES:5||SUPERCURRENT:5||SUPERCONDUCTOR:5||CONDUCTANCE:5||HIGHTEMPERATURE SUPERCONDUCTORS:5||TRANSPORT:5||PHASE:5||FILMS:4||LOCALIZATION:4||SINGLE DIRAC CONE:4||WIRES:4||MAGNETICFIELD:4||STEPS:3||ELECTRONS:3||proximity effect:3||MODEL:3||ARRAYS:3||INTERFERENCE:3||fluxon dynamics:3||HETEROSTRUCTURES:3||INSULATOR:3||Andreev reflection:3||electronic transport:3||FISKE:3||superconductor:2||ZnO:2||quantum point contact:2||METAL:2||DYNAMICS:2||interlayer Josephson coupling:2||SUPERCONDUCTORS:2||YBA2CU3O7DELTA:2||LAYER:2||DOTS:2||quantum dot:2||Article:2||TRANSISTORS:2||CARBON NANOTUBES:2||GAP:2||MECHANISM:2||LINE:2||GIANT SHAPIRO STEPS:2||LAYERS:2||electron energy loss spectroscopy:2||physical phenomena:2||scanning electron microscopy:2||HGTE QUANTUMWELLS:2||BI2TE3:2||SPECTROSCOPY:2||PNJUNCTIONS:2||spinpolarized tunneling:2||INTRINSIC JOSEPHSONJUNCTIONS:2||FIELDS:2||positive magnetoresistance:2||dilute magnetic semiconductor:2||magnetic field:2||scanning transmission electron microscopy:2||QUANTUM OSCILLATIONS:2||TRANSPORTPROPERTIES:2||surface pair current:2||MAGNETORESISTANCE:2||NANORIBBONS:2||INSTABILITY:2||ANDREEV REFLECTION:2||microwave irradiation:2||vertical graphene josephson junction:2||BI2SE3:2||CONDUCTIVITY:2||highTc superconductors:2||DIMENSIONAL ELECTRONGAS:2||graphene:2||Topological insulators:2||Josephson coupling Fraunhofer interference pattern:2||FERROMAGNET:2||DEPENDENCE:2||DETECTOR:2||COHERENCE:2||INJECTION:2||GRAPHENE:1||JOSEPHSONJUNCTIONS:1||LAYERED SUPERCONDUCTOR:1||mode splitting:1||BEHAVIOR:1||spinpolarized transport:1||SUPERCONDUCTING TRANSITION:1||microwave response:1||PSEUDOGAP:1||phase coherence:1||TRANSITIONS:1||Long Josephson junction:1||Charge detection:1||collective resonance modes:1||plasma oscillation modes:1||Superconducting proximity effect:1||Iron pnictide superconductor:1||McMillanRowell oscillations:1||ferromagnetic microstructure:1||superradiant state:1||VOLTAGE:1||branch splitting:1||TENSOR:1||INTERCALATION:1||insitu fabrication:1||NDGAO3:1||DISORDERED METALS:1||GAUGE GLASS:1||LOWTEMPERATURE TRANSPORT:1||spontaneous spin polarization model:1||BIAS:1||emission of electromagnetic waves:1||YBA2CU3O7/PRBA2CU3O7 SUPERLATTICES:1||BOHM:1||SHAPIRO STEPS:1||superconductor/ferromagnet interface:1||OXIDE:1||ANDREEVREFLECTION:1||SinFeAsO single crystal:1||COLLECTIVE MOTION:1||ANGULARDEPENDENCE:1||SUPERCONDUCTIVITY:1||BILAYER GRAPHENE:1||PHOTOLUMINESCENT PROPERTIES:1||SUPERCONDUCTING WEAK LINKS:1||intrinsic Josephson junctions geometrical resonance:1||intrinsic Josephson junction:1||MESOSCOPIC SPINVALVE:1||Bi2212 single crystals:1||intrinsic junctions:1||ANDREEV REFLECTIONS:1||normalmetal/superconductor interface:1||IBI2SR2CACU2OY:1||THERMAL FLUCTUATIONS:1||MIXED STATE:1||BI2.15SR1.85CACU2O8+DELTA:1||intrinsic Josephson effects:1||CACUO:1||QUANTUM POINT CONTACTS:1||resonant tunneling state:1||coherence length:1||NANOWIRE:1||GATES:1||Phase line:1||Thermal activation:1||QUANTUMDOT:1||superconducting proximity effect:1||Andreev interferometer:1||WIRE:1||Josephsonvortexflow branches:1||Bi2212 cuprates:1||LATTICE:1||demannetization effect:1||SUPERCONDUCTING MIRRORS:1||GAS:1||VALLEY TRANSPORT:1||ELECTRODES:1||DEPENDENT TRANSPORT:1||BORNOPPENHEIMER APPROXIMATION:1||collective plasma oscillations:1||fluxon resonance steps:1||STACKS:1||COLLECTIVE DYNAMICS:1||PAIRING SYMMETRY:1||MUON SPIN ROTATION:1||DIMENSIONAL CROSSOVER:1||Bi2Sr2CaCu2Oy highTc superconductors:1||heterojunctions:1||nanostructures:1||surfaces and interfaces:1||QUANTUM TRANSPORT:1||MICROJUNCTIONS:1||RESONATORS:1||STATES:1||FIELD:1||FLUCTUATIONS:1||SCATTERING:1||mode splitting of Josephson vortexflow branches:1||2D superconductivity:1||TRANSISTOR:1||ENERGYGAP:1||SUPERLATTICES:1||IRONBASED SUPERCONDUCTORS:1||PHASEDEPENDENT RESISTANCE:1||QUANTUM PHASETRANSITIONS:1||ELECTRICFIELD:1||HIGH MAGNETICFIELDS:1||NANOWIRE HETEROSTRUCTURES:1||ZNO:1||pair breaking.:1||SUPERCONDUCTING PB:1||domain formation:1||FORCE MICROSCOPY:1||RELAXATION:1||PLASMA RESONANCE:1||coupled Josephson junctions:1||COPPEROXIDE SUPERCONDUCTORS:1||CROSSOVER:1||SIMULATIONS:1||LOWTEMPERATURE:1||CONDUCTORS:1||METALINSULATORTRANSITION:1||SEMICONDUCTOR:1||FIELDEFFECT TRANSISTORS:1||ZEROVOLTAGE STATE:1||constanttemperature interlayer tunneling spectroscopy:1||Josephson supercurrent:1||BIPOLAR SUPERCURRENT:1||Interaction between Josephson and pancake vortices:1||flux jump:1||coaxial heterojunction nanorod:1||Natural Josephson coupling:1||BI2SR2CACU2O8+DELTA:1||VORTEX FLOW:1||TC SUPERCONDUCTORS:1||charge imbalance:1||Andreev diffractometer:1||intercalation:1||surface junction:1||Bi2212:1||tunnelling:1||GRAPHITE:1||GROWTH:1||collective transverse plasma modes:1||GAN:1||Macroscopic quantum tunneling:1||Fluctuation conductivity:1||Abovegap conductance jump:1||Josephson vortex motion:1||Intrinsic Josephson junctions:1||LAYERED SUPERCONDUCTORS:1||BI2SR2CACU2O8+Y:1||INTERFACES:1||BREAKDOWN:1||SYSTEMS:1||Anisotropy ratio:1||Josephson vortex:1||spin relaxation in superconductors:1||bibased single crystals:1||MESOSCOPIC PROXIMITY SUPERCONDUCTOR:1||reentrance of conductance:1||interlayer pair tunneling:1||JOSEPHSON:1||DISORDERED 2DIMENSIONAL SUPERCONDUCTORS:1||INDIUM FILMS:1||excited state:1||REGIME:1||triplet superconductivity:1||FILM:1||SCHOTTKY DIODES:1||peakdiphump structure:1||Kondo effect:1||REENTRANCE:1||Graphene:1||CONTACT:1||BERRYS PHASE:1||2DIMENSIONAL SUPERCONDUCTORS:1||Coulomb diamond:1||magnetic domain:1||spin injection:1||RESONANCE:1||plasma excitation modes:1||FLOW:1||OVERDOPED BI2SR2CACU2O8+DELTA:1||hole doping:1||chemical synthesis:1||phase transitions:1||superconductors:1||VORTEXGLASS SUPERCONDUCTIVITY:1||Kondorelated model:1||RADIATION:1||DOT:1||NANOBELTS:1||Complementarity:1||Closedloop AharonovBohm interferometer:1||pair breaking:1||interlayer phase fluctuation:1||MgB2 thin film:1||CONFINEMENT:1||WALLED CARBON NANOTUBES:1||TRANSITION:9||VORTICES:8||STATE:7||intrinsic Josephson junctions:7||SINGLECRYSTALS:7||JUNCTIONS:5||MODES:5||SUPERCURRENT:5||SUPERCONDUCTOR:5||CONDUCTANCE:5||HIGHTEMPERATURE SUPERCONDUCTORS:5||TRANSPORT:5||PHASE:5||FILMS:4||LOCALIZATION:4||SINGLE DIRAC CONE:4||WIRES:4||MAGNETICFIELD:4||STEPS:3||ELECTRONS:3||proximity effect:3||MODEL:3||ARRAYS:3||INTERFERENCE:3||fluxon dynamics:3||HETEROSTRUCTURES:3||INSULATOR:3||Andreev reflection:3||electronic transport:3||FISKE:3||superconductor:2||ZnO:2||quantum point contact:2||METAL:2||DYNAMICS:2||interlayer Josephson coupling:2||SUPERCONDUCTORS:2||YBA2CU3O7DELTA:2||LAYER:2||DOTS:2||quantum dot:2||Article:2||TRANSISTORS:2||CARBON NANOTUBES:2||GAP:2||MECHANISM:2||LINE:2||GIANT SHAPIRO STEPS:2||LAYERS:2||electron energy loss spectroscopy:2||physical phenomena:2||scanning electron microscopy:2||HGTE QUANTUMWELLS:2||BI2TE3:2||SPECTROSCOPY:2||PNJUNCTIONS:2||spinpolarized tunneling:2||INTRINSIC JOSEPHSONJUNCTIONS:2||FIELDS:2||positive magnetoresistance:2||dilute magnetic semiconductor:2||magnetic field:2||scanning transmission electron microscopy:2||QUANTUM OSCILLATIONS:2||TRANSPORTPROPERTIES:2||surface pair current:2||MAGNETORESISTANCE:2||NANORIBBONS:2||INSTABILITY:2||ANDREEV REFLECTION:2||microwave irradiation:2||vertical graphene josephson junction:2||BI2SE3:2||CONDUCTIVITY:2||highTc superconductors:2||DIMENSIONAL ELECTRONGAS:2||graphene:2||Topological insulators:2||Josephson coupling Fraunhofer interference pattern:2||FERROMAGNET:2||DEPENDENCE:2||DETECTOR:2||COHERENCE:2||INJECTION:2||GRAPHENE:1||JOSEPHSONJUNCTIONS:1||LAYERED SUPERCONDUCTOR:1||mode splitting:1||BEHAVIOR:1||spinpolarized transport:1||SUPERCONDUCTING TRANSITION:1||microwave response:1||PSEUDOGAP:1||phase coherence:1||TRANSITIONS:1||Long Josephson junction:1||Charge detection:1||collective resonance modes:1||plasma oscillation modes:1||Superconducting proximity effect:1||Iron pnictide superconductor:1||McMillanRowell oscillations:1||ferromagnetic microstructure:1||superradiant state:1||VOLTAGE:1||branch splitting:1||TENSOR:1||INTERCALATION:1||insitu fabrication:1||NDGAO3:1||DISORDERED METALS:1||GAUGE GLASS:1||LOWTEMPERATURE TRANSPORT:1||spontaneous spin polarization model:1||BIAS:1||emission of electromagnetic waves:1||YBA2CU3O7/PRBA2CU3O7 SUPERLATTICES:1||BOHM:1||SHAPIRO STEPS:1||superconductor/ferromagnet interface:1||OXIDE:1||ANDREEVREFLECTION:1||SinFeAsO single crystal:1||COLLECTIVE MOTION:1||ANGULARDEPENDENCE:1||SUPERCONDUCTIVITY:1||BILAYER GRAPHENE:1||PHOTOLUMINESCENT PROPERTIES:1||SUPERCONDUCTING WEAK LINKS:1||intrinsic Josephson junctions geometrical resonance:1||intrinsic Josephson junction:1||MESOSCOPIC SPINVALVE:1||Bi2212 single crystals:1||intrinsic junctions:1||ANDREEV REFLECTIONS:1||normalmetal/superconductor interface:1||IBI2SR2CACU2OY:1||THERMAL FLUCTUATIONS:1||MIXED STATE:1||BI2.15SR1.85CACU2O8+DELTA:1||intrinsic Josephson effects:1||CACUO:1||QUANTUM POINT CONTACTS:1||resonant tunneling state:1||coherence length:1||NANOWIRE:1||GATES:1||Phase line:1||Thermal activation:1||QUANTUMDOT:1||superconducting proximity effect:1||Andreev interferometer:1||WIRE:1||Josephsonvortexflow branches:1||Bi2212 cuprates:1||LATTICE:1||demannetization effect:1||SUPERCONDUCTING MIRRORS:1||GAS:1||VALLEY TRANSPORT:1||ELECTRODES:1||DEPENDENT TRANSPORT:1||BORNOPPENHEIMER APPROXIMATION:1||collective plasma oscillations:1||fluxon resonance steps:1||STACKS:1||COLLECTIVE DYNAMICS:1||PAIRING SYMMETRY:1||MUON SPIN ROTATION:1||DIMENSIONAL CROSSOVER:1||Bi2Sr2CaCu2Oy highTc superconductors:1||heterojunctions:1||nanostructures:1||surfaces and interfaces:1||QUANTUM TRANSPORT:1||MICROJUNCTIONS:1||RESONATORS:1||STATES:1||FIELD:1||FLUCTUATIONS:1||SCATTERING:1||mode splitting of Josephson vortexflow branches:1||2D superconductivity:1||TRANSISTOR:1||ENERGYGAP:1||SUPERLATTICES:1||IRONBASED SUPERCONDUCTORS:1||PHASEDEPENDENT RESISTANCE:1||QUANTUM PHASETRANSITIONS:1||ELECTRICFIELD:1||HIGH MAGNETICFIELDS:1||NANOWIRE HETEROSTRUCTURES:1||ZNO:1||pair breaking.:1||SUPERCONDUCTING PB:1||domain formation:1||FORCE MICROSCOPY:1||RELAXATION:1||PLASMA RESONANCE:1||coupled Josephson junctions:1||COPPEROXIDE SUPERCONDUCTORS:1||CROSSOVER:1||SIMULATIONS:1||LOWTEMPERATURE:1||CONDUCTORS:1||METALINSULATORTRANSITION:1||SEMICONDUCTOR:1||FIELDEFFECT TRANSISTORS:1||ZEROVOLTAGE STATE:1||constanttemperature interlayer tunneling spectroscopy:1||Josephson supercurrent:1||BIPOLAR SUPERCURRENT:1||Interaction between Josephson and pancake vortices:1||flux jump:1||coaxial heterojunction nanorod:1||Natural Josephson coupling:1||BI2SR2CACU2O8+DELTA:1||VORTEX FLOW:1||TC SUPERCONDUCTORS:1||charge imbalance:1||Andreev diffractometer:1||intercalation:1||surface junction:1||Bi2212:1||tunnelling:1||GRAPHITE:1||GROWTH:1||collective transverse plasma modes:1||GAN:1||Macroscopic quantum tunneling:1||Fluctuation conductivity:1||Abovegap conductance jump:1||Josephson vortex motion:1||Intrinsic Josephson junctions:1||LAYERED SUPERCONDUCTORS:1||BI2SR2CACU2O8+Y:1||INTERFACES:1||BREAKDOWN:1||SYSTEMS:1||Anisotropy ratio:1||Josephson vortex:1||spin relaxation in superconductors:1||bibased single crystals:1||MESOSCOPIC PROXIMITY SUPERCONDUCTOR:1||reentrance of conductance:1||interlayer pair tunneling:1||JOSEPHSON:1||DISORDERED 2DIMENSIONAL SUPERCONDUCTORS:1||INDIUM FILMS:1||excited state:1||REGIME:1||triplet superconductivity:1||FILM:1||SCHOTTKY DIODES:1||peakdiphump structure:1||Kondo effect:1||REENTRANCE:1||Graphene:1||CONTACT:1||BERRYS PHASE:1||2DIMENSIONAL SUPERCONDUCTORS:1||Coulomb diamond:1||magnetic domain:1||spin injection:1||RESONANCE:1||plasma excitation modes:1||FLOW:1||OVERDOPED BI2SR2CACU2O8+DELTA:1||hole doping:1||chemical synthesis:1||phase transitions:1||superconductors:1||VORTEXGLASS SUPERCONDUCTIVITY:1||Kondorelated model:1||RADIATION:1||DOT:1||NANOBELTS:1||Complementarity:1||Closedloop AharonovBohm interferometer:1||pair breaking:1||interlayer phase fluctuation:1||MgB2 thin film:1||CONFINEMENT:1||WALLED CARBON NANOTUBES:1||TRANSITION:9||VORTICES:8||STATE:7||intrinsic Josephson junctions:7||SINGLECRYSTALS:7||JUNCTIONS:5||MODES:5||SUPERCURRENT:5||SUPERCONDUCTOR:5||CONDUCTANCE:5||HIGHTEMPERATURE SUPERCONDUCTORS:5||TRANSPORT:5||PHASE:5||FILMS:4||LOCALIZATION:4||SINGLE DIRAC CONE:4||WIRES:4||MAGNETICFIELD:4||STEPS:3||ELECTRONS:3||proximity effect:3||MODEL:3||ARRAYS:3||INTERFERENCE:3||fluxon dynamics:3||HETEROSTRUCTURES:3||INSULATOR:3||Andreev reflection:3||electronic transport:3||FISKE:3||superconductor:2||ZnO:2||quantum point contact:2||METAL:2||DYNAMICS:2||interlayer Josephson coupling:2||SUPERCONDUCTORS:2||YBA2CU3O7DELTA:2||LAYER:2||DOTS:2||quantum dot:2||Article:2||TRANSISTORS:2||CARBON NANOTUBES:2||GAP:2||MECHANISM:2||LINE:2||GIANT SHAPIRO STEPS:2||LAYERS:2||electron energy loss spectroscopy:2||physical phenomena:2||scanning electron microscopy:2||HGTE QUANTUMWELLS:2||BI2TE3:2||SPECTROSCOPY:2||PNJUNCTIONS:2||spinpolarized tunneling:2||INTRINSIC JOSEPHSONJUNCTIONS:2||FIELDS:2||positive magnetoresistance:2||dilute magnetic semiconductor:2||magnetic field:2||scanning transmission electron microscopy:2||QUANTUM OSCILLATIONS:2||TRANSPORTPROPERTIES:2||surface pair current:2||MAGNETORESISTANCE:2||NANORIBBONS:2||INSTABILITY:2||ANDREEV REFLECTION:2||microwave irradiation:2||vertical graphene josephson junction:2||BI2SE3:2||CONDUCTIVITY:2||highTc superconductors:2||DIMENSIONAL ELECTRONGAS:2||graphene:2||Topological insulators:2||Josephson coupling Fraunhofer interference pattern:2||FERROMAGNET:2||DEPENDENCE:2||DETECTOR:2||COHERENCE:2||INJECTION:2||GRAPHENE:1||JOSEPHSONJUNCTIONS:1||LAYERED SUPERCONDUCTOR:1||mode splitting:1||BEHAVIOR:1||spinpolarized transport:1||SUPERCONDUCTING TRANSITION:1||microwave response:1||PSEUDOGAP:1||phase coherence:1||TRANSITIONS:1||Long Josephson junction:1||Charge detection:1||collective resonance modes:1||plasma oscillation modes:1||Superconducting proximity effect:1||Iron pnictide superconductor:1||McMillanRowell oscillations:1||ferromagnetic microstructure:1||superradiant state:1||VOLTAGE:1||branch splitting:1||TENSOR:1||INTERCALATION:1||insitu fabrication:1||NDGAO3:1||DISORDERED METALS:1||GAUGE GLASS:1||LOWTEMPERATURE TRANSPORT:1||spontaneous spin polarization model:1||BIAS:1||emission of electromagnetic waves:1||YBA2CU3O7/PRBA2CU3O7 SUPERLATTICES:1||BOHM:1||SHAPIRO STEPS:1||superconductor/ferromagnet interface:1||OXIDE:1||ANDREEVREFLECTION:1||SinFeAsO single crystal:1||COLLECTIVE MOTION:1||ANGULARDEPENDENCE:1||SUPERCONDUCTIVITY:1||BILAYER GRAPHENE:1||PHOTOLUMINESCENT PROPERTIES:1||SUPERCONDUCTING WEAK LINKS:1||intrinsic Josephson junctions geometrical resonance:1||intrinsic Josephson junction:1||MESOSCOPIC SPINVALVE:1||Bi2212 single crystals:1||intrinsic junctions:1||ANDREEV REFLECTIONS:1||normalmetal/superconductor interface:1||IBI2SR2CACU2OY:1||THERMAL FLUCTUATIONS:1||MIXED STATE:1||BI2.15SR1.85CACU2O8+DELTA:1||intrinsic Josephson effects:1||CACUO:1||QUANTUM POINT CONTACTS:1||resonant tunneling state:1||coherence length:1||NANOWIRE:1||GATES:1||Phase line:1||Thermal activation:1||QUANTUMDOT:1||superconducting proximity effect:1||Andreev interferometer:1||WIRE:1||Josephsonvortexflow branches:1||Bi2212 cuprates:1||LATTICE:1||demannetization effect:1||SUPERCONDUCTING MIRRORS:1||GAS:1||VALLEY TRANSPORT:1||ELECTRODES:1||DEPENDENT TRANSPORT:1||BORNOPPENHEIMER APPROXIMATION:1||collective plasma oscillations:1||fluxon resonance steps:1||STACKS:1||COLLECTIVE DYNAMICS:1||PAIRING SYMMETRY:1||MUON SPIN ROTATION:1||DIMENSIONAL CROSSOVER:1||Bi2Sr2CaCu2Oy highTc superconductors:1||heterojunctions:1||nanostructures:1||surfaces and interfaces:1||QUANTUM TRANSPORT:1||MICROJUNCTIONS:1||RESONATORS:1||STATES:1||FIELD:1||FLUCTUATIONS:1||SCATTERING:1||mode splitting of Josephson vortexflow branches:1||2D superconductivity:1||TRANSISTOR:1||ENERGYGAP:1||SUPERLATTICES:1||IRONBASED SUPERCONDUCTORS:1||PHASEDEPENDENT RESISTANCE:1||QUANTUM PHASETRANSITIONS:1||ELECTRICFIELD:1||HIGH MAGNETICFIELDS:1||NANOWIRE HETEROSTRUCTURES:1||ZNO:1||pair breaking.:1||SUPERCONDUCTING PB:1||domain formation:1||FORCE MICROSCOPY:1||RELAXATION:1||PLASMA RESONANCE:1||coupled Josephson junctions:1||COPPEROXIDE SUPERCONDUCTORS:1||CROSSOVER:1||SIMULATIONS:1||LOWTEMPERATURE:1||CONDUCTORS:1||METALINSULATORTRANSITION:1||SEMICONDUCTOR:1||FIELDEFFECT TRANSISTORS:1||ZEROVOLTAGE STATE:1||constanttemperature interlayer tunneling spectroscopy:1||Josephson supercurrent:1||BIPOLAR SUPERCURRENT:1||Interaction between Josephson and pancake vortices:1||flux jump:1||coaxial heterojunction nanorod:1||Natural Josephson coupling:1||BI2SR2CACU2O8+DELTA:1||VORTEX FLOW:1||TC SUPERCONDUCTORS:1||charge imbalance:1||Andreev diffractometer:1||intercalation:1||surface junction:1||Bi2212:1||tunnelling:1||GRAPHITE:1||GROWTH:1||collective transverse plasma modes:1||GAN:1||Macroscopic quantum tunneling:1||Fluctuation conductivity:1||Abovegap conductance jump:1||Josephson vortex motion:1||Intrinsic Josephson junctions:1||LAYERED SUPERCONDUCTORS:1||BI2SR2CACU2O8+Y:1||INTERFACES:1||BREAKDOWN:1||SYSTEMS:1||Anisotropy ratio:1||Josephson vortex:1||spin relaxation in superconductors:1||bibased single crystals:1||MESOSCOPIC PROXIMITY SUPERCONDUCTOR:1||reentrance of conductance:1||interlayer pair tunneling:1||JOSEPHSON:1||DISORDERED 2DIMENSIONAL SUPERCONDUCTORS:1||INDIUM FILMS:1||excited state:1||REGIME:1||triplet superconductivity:1||FILM:1||SCHOTTKY DIODES:1||peakdiphump structure:1||Kondo effect:1||REENTRANCE:1||Graphene:1||CONTACT:1||BERRYS PHASE:1||2DIMENSIONAL SUPERCONDUCTORS:1||Coulomb diamond:1||magnetic domain:1||spin injection:1||RESONANCE:1||plasma excitation modes:1||FLOW:1||OVERDOPED BI2SR2CACU2O8+DELTA:1||hole doping:1||chemical synthesis:1||phase transitions:1||superconductors:1||VORTEXGLASS SUPERCONDUCTIVITY:1||Kondorelated model:1||RADIATION:1||DOT:1||NANOBELTS:1||Complementarity:1||Closedloop AharonovBohm interferometer:1||pair breaking:1||interlayer phase fluctuation:1||MgB2 thin film:1||CONFINEMENT:1||WALLED CARBON NANOTUBES:1||TRANSITION:9||VORTICES:8||STATE:7||intrinsic Josephson junctions:7||SINGLECRYSTALS:7||JUNCTIONS:5||MODES:5||SUPERCURRENT:5||SUPERCONDUCTOR:5||CONDUCTANCE:5||HIGHTEMPERATURE SUPERCONDUCTORS:5||TRANSPORT:5||PHASE:5||FILMS:4||LOCALIZATION:4||SINGLE DIRAC CONE:4||WIRES:4||MAGNETICFIELD:4||STEPS:3||ELECTRONS:3||proximity effect:3||MODEL:3||ARRAYS:3||INTERFERENCE:3||fluxon dynamics:3||HETEROSTRUCTURES:3||INSULATOR:3||Andreev reflection:3||electronic transport:3||FISKE:3||superconductor:2||ZnO:2||quantum point contact:2||METAL:2||DYNAMICS:2||interlayer Josephson coupling:2||SUPERCONDUCTORS:2||YBA2CU3O7DELTA:2||LAYER:2||DOTS:2||quantum dot:2||Article:2||TRANSISTORS:2||CARBON NANOTUBES:2||GAP:2||MECHANISM:2||LINE:2||GIANT SHAPIRO STEPS:2||LAYERS:2||electron energy loss spectroscopy:2||physical phenomena:2||scanning electron microscopy:2||HGTE QUANTUMWELLS:2||BI2TE3:2||SPECTROSCOPY:2||PNJUNCTIONS:2||spinpolarized tunneling:2||INTRINSIC JOSEPHSONJUNCTIONS:2||FIELDS:2||positive magnetoresistance:2||dilute magnetic semiconductor:2||magnetic field:2||scanning transmission electron microscopy:2||QUANTUM OSCILLATIONS:2||TRANSPORTPROPERTIES:2||surface pair current:2||MAGNETORESISTANCE:2||NANORIBBONS:2||INSTABILITY:2||ANDREEV REFLECTION:2||microwave irradiation:2||vertical graphene josephson junction:2||BI2SE3:2||CONDUCTIVITY:2||highTc superconductors:2||DIMENSIONAL ELECTRONGAS:2||graphene:2||Topological insulators:2||Josephson coupling Fraunhofer interference pattern:2||FERROMAGNET:2||DEPENDENCE:2||DETECTOR:2||COHERENCE:2||INJECTION:2||GRAPHENE:1||JOSEPHSONJUNCTIONS:1||LAYERED SUPERCONDUCTOR:1||mode splitting:1||BEHAVIOR:1||spinpolarized transport:1||SUPERCONDUCTING TRANSITION:1||microwave response:1||PSEUDOGAP:1||phase coherence:1||TRANSITIONS:1||Long Josephson junction:1||Charge detection:1||collective resonance modes:1||plasma oscillation modes:1||Superconducting proximity effect:1||Iron pnictide superconductor:1||McMillanRowell oscillations:1||ferromagnetic microstructure:1||superradiant state:1||VOLTAGE:1||branch splitting:1||TENSOR:1||INTERCALATION:1||insitu fabrication:1||NDGAO3:1||DISORDERED METALS:1||GAUGE GLASS:1||LOWTEMPERATURE TRANSPORT:1||spontaneous spin polarization model:1||BIAS:1||emission of electromagnetic waves:1||YBA2CU3O7/PRBA2CU3O7 SUPERLATTICES:1||BOHM:1||SHAPIRO STEPS:1||superconductor/ferromagnet interface:1||OXIDE:1||ANDREEVREFLECTION:1||SinFeAsO single crystal:1||COLLECTIVE MOTION:1||ANGULARDEPENDENCE:1||SUPERCONDUCTIVITY:1||BILAYER GRAPHENE:1||PHOTOLUMINESCENT PROPERTIES:1||SUPERCONDUCTING WEAK LINKS:1||intrinsic Josephson junctions geometrical resonance:1||intrinsic Josephson junction:1||MESOSCOPIC SPINVALVE:1||Bi2212 single crystals:1||intrinsic junctions:1||ANDREEV REFLECTIONS:1||normalmetal/superconductor interface:1||IBI2SR2CACU2OY:1||THERMAL FLUCTUATIONS:1||MIXED STATE:1||BI2.15SR1.85CACU2O8+DELTA:1||intrinsic Josephson effects:1||CACUO:1||QUANTUM POINT CONTACTS:1||resonant tunneling state:1||coherence length:1||NANOWIRE:1||GATES:1||Phase line:1||Thermal activation:1||QUANTUMDOT:1||superconducting proximity effect:1||Andreev interferometer:1||WIRE:1||Josephsonvortexflow branches:1||Bi2212 cuprates:1||LATTICE:1||demannetization effect:1||SUPERCONDUCTING MIRRORS:1||GAS:1||VALLEY TRANSPORT:1||ELECTRODES:1||DEPENDENT TRANSPORT:1||BORNOPPENHEIMER APPROXIMATION:1||collective plasma oscillations:1||fluxon resonance steps:1||STACKS:1||COLLECTIVE DYNAMICS:1||PAIRING SYMMETRY:1||MUON SPIN ROTATION:1||DIMENSIONAL CROSSOVER:1||Bi2Sr2CaCu2Oy highTc superconductors:1||heterojunctions:1||nanostructures:1||surfaces and interfaces:1||QUANTUM TRANSPORT:1||MICROJUNCTIONS:1||RESONATORS:1||STATES:1||FIELD:1||FLUCTUATIONS:1||SCATTERING:1||mode splitting of Josephson vortexflow branches:1||2D superconductivity:1||TRANSISTOR:1||ENERGYGAP:1||SUPERLATTICES:1||IRONBASED SUPERCONDUCTORS:1||PHASEDEPENDENT RESISTANCE:1||QUANTUM PHASETRANSITIONS:1||ELECTRICFIELD:1||HIGH MAGNETICFIELDS:1||NANOWIRE HETEROSTRUCTURES:1||ZNO:1||pair breaking.:1||SUPERCONDUCTING PB:1||domain formation:1||FORCE MICROSCOPY:1||RELAXATION:1||PLASMA RESONANCE:1||coupled Josephson junctions:1||COPPEROXIDE SUPERCONDUCTORS:1||CROSSOVER:1||SIMULATIONS:1||LOWTEMPERATURE:1||CONDUCTORS:1||METALINSULATORTRANSITION:1||SEMICONDUCTOR:1||FIELDEFFECT TRANSISTORS:1||ZEROVOLTAGE STATE:1||constanttemperature interlayer tunneling spectroscopy:1||Josephson supercurrent:1||BIPOLAR SUPERCURRENT:1||Interaction between Josephson and pancake vortices:1||flux jump:1||coaxial heterojunction nanorod:1||Natural Josephson coupling:1||BI2SR2CACU2O8+DELTA:1||VORTEX FLOW:1||TC SUPERCONDUCTORS:1||charge imbalance:1||Andreev diffractometer:1||intercalation:1||surface junction:1||Bi2212:1||tunnelling:1||GRAPHITE:1||GROWTH:1||collective transverse plasma modes:1||GAN:1||Macroscopic quantum tunneling:1||Fluctuation conductivity:1||Abovegap conductance jump:1||Josephson vortex motion:1||Intrinsic Josephson junctions:1||LAYERED SUPERCONDUCTORS:1||BI2SR2CACU2O8+Y:1||INTERFACES:1||BREAKDOWN:1||SYSTEMS:1||Anisotropy ratio:1||Josephson vortex:1||spin relaxation in superconductors:1||bibased single crystals:1||MESOSCOPIC PROXIMITY SUPERCONDUCTOR:1||reentrance of conductance:1||interlayer pair tunneling:1||JOSEPHSON:1||DISORDERED 2DIMENSIONAL SUPERCONDUCTORS:1||INDIUM FILMS:1||excited state:1||REGIME:1||triplet superconductivity:1||FILM:1||SCHOTTKY DIODES:1||peakdiphump structure:1||Kondo effect:1||REENTRANCE:1||Graphene:1||CONTACT:1||BERRYS PHASE:1||2DIMENSIONAL SUPERCONDUCTORS:1||Coulomb diamond:1||magnetic domain:1||spin injection:1||RESONANCE:1||plasma excitation modes:1||FLOW:1||OVERDOPED BI2SR2CACU2O8+DELTA:1||hole doping:1||chemical synthesis:1||phase transitions:1||superconductors:1||VORTEXGLASS SUPERCONDUCTIVITY:1||Kondorelated model:1||RADIATION:1||DOT:1||NANOBELTS:1||Complementarity:1||Closedloop AharonovBohm interferometer:1||pair breaking:1||interlayer phase fluctuation:1||MgB2 thin film:1||CONFINEMENT:1||WALLED CARBON NANOTUBES:1||TRANSITION:9||VORTICES:8||STATE:7||intrinsic Josephson junctions:7||SINGLECRYSTALS:7||JUNCTIONS:5||MODES:5||SUPERCURRENT:5||SUPERCONDUCTOR:5||CONDUCTANCE:5||HIGHTEMPERATURE SUPERCONDUCTORS:5||TRANSPORT:5||PHASE:5||FILMS:4||LOCALIZATION:4||SINGLE DIRAC CONE:4||WIRES:4||MAGNETICFIELD:4||STEPS:3||ELECTRONS:3||proximity effect:3||MODEL:3||ARRAYS:3||INTERFERENCE:3||fluxon dynamics:3||HETEROSTRUCTURES:3||INSULATOR:3||Andreev reflection:3||electronic transport:3||FISKE:3||superconductor:2||ZnO:2||quantum point contact:2||METAL:2||DYNAMICS:2||interlayer Josephson coupling:2||SUPERCONDUCTORS:2||YBA2CU3O7DELTA:2||LAYER:2||DOTS:2||quantum dot:2||Article:2||TRANSISTORS:2||CARBON NANOTUBES:2||GAP:2||MECHANISM:2||LINE:2||GIANT SHAPIRO STEPS:2||LAYERS:2||electron energy loss spectroscopy:2||physical phenomena:2||scanning electron microscopy:2||HGTE QUANTUMWELLS:2||BI2TE3:2||SPECTROSCOPY:2||PNJUNCTIONS:2||spinpolarized tunneling:2||INTRINSIC JOSEPHSONJUNCTIONS:2||FIELDS:2||positive magnetoresistance:2||dilute magnetic semiconductor:2||magnetic field:2||scanning transmission electron microscopy:2||QUANTUM OSCILLATIONS:2||TRANSPORTPROPERTIES:2||surface pair current:2||MAGNETORESISTANCE:2||NANORIBBONS:2||INSTABILITY:2||ANDREEV REFLECTION:2||microwave irradiation:2||vertical graphene josephson junction:2||BI2SE3:2||CONDUCTIVITY:2||highTc superconductors:2||DIMENSIONAL ELECTRONGAS:2||graphene:2||Topological insulators:2||Josephson coupling Fraunhofer interference pattern:2||FERROMAGNET:2||DEPENDENCE:2||DETECTOR:2||COHERENCE:2||INJECTION:2||GRAPHENE:1||JOSEPHSONJUNCTIONS:1||LAYERED SUPERCONDUCTOR:1||mode splitting:1||BEHAVIOR:1||spinpolarized transport:1||SUPERCONDUCTING TRANSITION:1||microwave response:1||PSEUDOGAP:1||phase coherence:1||TRANSITIONS:1||Long Josephson junction:1||Charge detection:1||collective resonance modes:1||plasma oscillation modes:1||Superconducting proximity effect:1||Iron pnictide superconductor:1||McMillanRowell oscillations:1||ferromagnetic microstructure:1||superradiant state:1||VOLTAGE:1||branch splitting:1||TENSOR:1||INTERCALATION:1||insitu fabrication:1||NDGAO3:1||DISORDERED METALS:1||GAUGE GLASS:1||LOWTEMPERATURE TRANSPORT:1||spontaneous spin polarization model:1||BIAS:1||emission of electromagnetic waves:1||YBA2CU3O7/PRBA2CU3O7 SUPERLATTICES:1||BOHM:1||SHAPIRO STEPS:1||superconductor/ferromagnet interface:1||OXIDE:1||ANDREEVREFLECTION:1||SinFeAsO single crystal:1||COLLECTIVE MOTION:1||ANGULARDEPENDENCE:1||SUPERCONDUCTIVITY:1||BILAYER GRAPHENE:1||PHOTOLUMINESCENT PROPERTIES:1||SUPERCONDUCTING WEAK LINKS:1||intrinsic Josephson junctions geometrical resonance:1||intrinsic Josephson junction:1||MESOSCOPIC SPINVALVE:1||Bi2212 single crystals:1||intrinsic junctions:1||ANDREEV REFLECTIONS:1||normalmetal/superconductor interface:1||IBI2SR2CACU2OY:1||THERMAL FLUCTUATIONS:1||MIXED STATE:1||BI2.15SR1.85CACU2O8+DELTA:1||intrinsic Josephson effects:1||CACUO:1||QUANTUM POINT CONTACTS:1||resonant tunneling state:1||coherence length:1||NANOWIRE:1||GATES:1||Phase line:1||Thermal activation:1||QUANTUMDOT:1||superconducting proximity effect:1||Andreev interferometer:1||WIRE:1||Josephsonvortexflow branches:1||Bi2212 cuprates:1||LATTICE:1||demannetization effect:1||SUPERCONDUCTING MIRRORS:1||GAS:1||VALLEY TRANSPORT:1||ELECTRODES:1||DEPENDENT TRANSPORT:1||BORNOPPENHEIMER APPROXIMATION:1||collective plasma oscillations:1||fluxon resonance steps:1||STACKS:1||COLLECTIVE DYNAMICS:1||PAIRING SYMMETRY:1||MUON SPIN ROTATION:1||DIMENSIONAL CROSSOVER:1||Bi2Sr2CaCu2Oy highTc superconductors:1||heterojunctions:1||nanostructures:1||surfaces and interfaces:1||QUANTUM TRANSPORT:1||MICROJUNCTIONS:1||RESONATORS:1||STATES:1||FIELD:1||FLUCTUATIONS:1||SCATTERING:1||mode splitting of Josephson vortexflow branches:1||2D superconductivity:1||TRANSISTOR:1||ENERGYGAP:1||SUPERLATTICES:1||IRONBASED SUPERCONDUCTORS:1||PHASEDEPENDENT RESISTANCE:1||QUANTUM PHASETRANSITIONS:1||ELECTRICFIELD:1||HIGH MAGNETICFIELDS:1||NANOWIRE HETEROSTRUCTURES:1||ZNO:1||pair breaking.:1||SUPERCONDUCTING PB:1||domain formation:1||FORCE MICROSCOPY:1||RELAXATION:1||PLASMA RESONANCE:1||coupled Josephson junctions:1||COPPEROXIDE SUPERCONDUCTORS:1||CROSSOVER:1||SIMULATIONS:1||LOWTEMPERATURE:1||CONDUCTORS:1||METALINSULATORTRANSITION:1||SEMICONDUCTOR:1||FIELDEFFECT TRANSISTORS:1||ZEROVOLTAGE STATE:1||constanttemperature interlayer tunneling spectroscopy:1||Josephson supercurrent:1||BIPOLAR SUPERCURRENT:1||Interaction between Josephson and pancake vortices:1||flux jump:1||coaxial heterojunction nanorod:1||Natural Josephson coupling:1||BI2SR2CACU2O8+DELTA:1||VORTEX FLOW:1||TC SUPERCONDUCTORS:1||charge imbalance:1||Andreev diffractometer:1||intercalation:1||surface junction:1||Bi2212:1||tunnelling:1||GRAPHITE:1||GROWTH:1||collective transverse plasma modes:1||GAN:1||Macroscopic quantum tunneling:1||Fluctuation conductivity:1||Abovegap conductance jump:1||Josephson vortex motion:1||Intrinsic Josephson junctions:1||LAYERED SUPERCONDUCTORS:1||BI2SR2CACU2O8+Y:1||INTERFACES:1||BREAKDOWN:1||SYSTEMS:1||Anisotropy ratio:1||Josephson vortex:1||spin relaxation in superconductors:1||bibased single crystals:1||MESOSCOPIC PROXIMITY SUPERCONDUCTOR:1||reentrance of conductance:1||interlayer pair tunneling:1||JOSEPHSON:1||DISORDERED 2DIMENSIONAL SUPERCONDUCTORS:1||INDIUM FILMS:1||excited state:1||REGIME:1||triplet superconductivity:1||FILM:1||SCHOTTKY DIODES:1||peakdiphump structure:1||Kondo effect:1||REENTRANCE:1||Graphene:1||CONTACT:1||BERRYS PHASE:1||2DIMENSIONAL SUPERCONDUCTORS:1||Coulomb diamond:1||magnetic domain:1||spin injection:1||RESONANCE:1||plasma excitation modes:1||FLOW:1||OVERDOPED BI2SR2CACU2O8+DELTA:1||hole doping:1||chemical synthesis:1||phase transitions:1||superconductors:1||VORTEXGLASS SUPERCONDUCTIVITY:1||Kondorelated model:1||RADIATION:1||DOT:1||NANOBELTS:1||Complementarity:1||Closedloop AharonovBohm interferometer:1||pair breaking:1||interlayer phase fluctuation:1||MgB2 thin film:1||CONFINEMENT:1||WALLED CARBON NANOTUBES:1||TRANSITION:9||VORTICES:8||STATE:7||intrinsic Josephson junctions:7||SINGLECRYSTALS:7||JUNCTIONS:5||MODES:5||SUPERCURRENT:5||SUPERCONDUCTOR:5||CONDUCTANCE:5||HIGHTEMPERATURE SUPERCONDUCTORS:5||TRANSPORT:5||PHASE:5||FILMS:4||LOCALIZATION:4||SINGLE DIRAC CONE:4||WIRES:4||MAGNETICFIELD:4||STEPS:3||ELECTRONS:3||proximity effect:3||MODEL:3||ARRAYS:3||INTERFERENCE:3||fluxon dynamics:3||HETEROSTRUCTURES:3||INSULATOR:3||Andreev reflection:3||electronic transport:3||FISKE:3||superconductor:2||ZnO:2||quantum point contact:2||METAL:2||DYNAMICS:2||interlayer Josephson coupling:2||SUPERCONDUCTORS:2||YBA2CU3O7DELTA:2||LAYER:2||DOTS:2||quantum dot:2||Article:2||TRANSISTORS:2||CARBON NANOTUBES:2||GAP:2||MECHANISM:2||LINE:2||GIANT SHAPIRO STEPS:2||LAYERS:2||electron energy loss spectroscopy:2||physical phenomena:2||scanning electron microscopy:2||HGTE QUANTUMWELLS:2||BI2TE3:2||SPECTROSCOPY:2||PNJUNCTIONS:2||spinpolarized tunneling:2||INTRINSIC JOSEPHSONJUNCTIONS:2||FIELDS:2||positive magnetoresistance:2||dilute magnetic semiconductor:2||magnetic field:2||scanning transmission electron microscopy:2||QUANTUM OSCILLATIONS:2||TRANSPORTPROPERTIES:2||surface pair current:2||MAGNETORESISTANCE:2||NANORIBBONS:2||INSTABILITY:2||ANDREEV REFLECTION:2||microwave irradiation:2||vertical graphene josephson junction:2||BI2SE3:2||CONDUCTIVITY:2||highTc superconductors:2||DIMENSIONAL ELECTRONGAS:2||graphene:2||Topological insulators:2||Josephson coupling Fraunhofer interference pattern:2||FERROMAGNET:2||DEPENDENCE:2||DETECTOR:2||COHERENCE:2||INJECTION:2||GRAPHENE:1||JOSEPHSONJUNCTIONS:1||LAYERED SUPERCONDUCTOR:1||mode splitting:1||BEHAVIOR:1||spinpolarized transport:1||SUPERCONDUCTING TRANSITION:1||microwave response:1||PSEUDOGAP:1||phase coherence:1||TRANSITIONS:1||Long Josephson junction:1||Charge detection:1||collective resonance modes:1||plasma oscillation modes:1||Superconducting proximity effect:1||Iron pnictide superconductor:1||McMillanRowell oscillations:1||ferromagnetic microstructure:1||superradiant state:1||VOLTAGE:1||branch splitting:1||TENSOR:1||INTERCALATION:1||insitu fabrication:1||NDGAO3:1||DISORDERED METALS:1||GAUGE GLASS:1||LOWTEMPERATURE TRANSPORT:1||spontaneous spin polarization model:1||BIAS:1||emission of electromagnetic waves:1||YBA2CU3O7/PRBA2CU3O7 SUPERLATTICES:1||BOHM:1||SHAPIRO STEPS:1||superconductor/ferromagnet interface:1||OXIDE:1||ANDREEVREFLECTION:1||SinFeAsO single crystal:1||COLLECTIVE MOTION:1||ANGULARDEPENDENCE:1||SUPERCONDUCTIVITY:1||BILAYER GRAPHENE:1||PHOTOLUMINESCENT PROPERTIES:1||SUPERCONDUCTING WEAK LINKS:1||intrinsic Josephson junctions geometrical resonance:1||intrinsic Josephson junction:1||MESOSCOPIC SPINVALVE:1||Bi2212 single crystals:1||intrinsic junctions:1||ANDREEV REFLECTIONS:1||normalmetal/superconductor interface:1||IBI2SR2CACU2OY:1||THERMAL FLUCTUATIONS:1||MIXED STATE:1||BI2.15SR1.85CACU2O8+DELTA:1||intrinsic Josephson effects:1||CACUO:1||QUANTUM POINT CONTACTS:1||resonant tunneling state:1||coherence length:1||NANOWIRE:1||GATES:1||Phase line:1||Thermal activation:1||QUANTUMDOT:1||superconducting proximity effect:1||Andreev interferometer:1||WIRE:1||Josephsonvortexflow branches:1||Bi2212 cuprates:1||LATTICE:1||demannetization effect:1||SUPERCONDUCTING MIRRORS:1||GAS:1||VALLEY TRANSPORT:1||ELECTRODES:1||DEPENDENT TRANSPORT:1||BORNOPPENHEIMER APPROXIMATION:1||collective plasma oscillations:1||fluxon resonance steps:1||STACKS:1||COLLECTIVE DYNAMICS:1||PAIRING SYMMETRY:1||MUON SPIN ROTATION:1||DIMENSIONAL CROSSOVER:1||Bi2Sr2CaCu2Oy highTc superconductors:1||heterojunctions:1||nanostructures:1||surfaces and interfaces:1||QUANTUM TRANSPORT:1||MICROJUNCTIONS:1||RESONATORS:1||STATES:1||FIELD:1||FLUCTUATIONS:1||SCATTERING:1||mode splitting of Josephson vortexflow branches:1||2D superconductivity:1||TRANSISTOR:1||ENERGYGAP:1||SUPERLATTICES:1||IRONBASED SUPERCONDUCTORS:1||PHASEDEPENDENT RESISTANCE:1||QUANTUM PHASETRANSITIONS:1||ELECTRICFIELD:1||HIGH MAGNETICFIELDS:1||NANOWIRE HETEROSTRUCTURES:1||ZNO:1||pair breaking.:1||SUPERCONDUCTING PB:1||domain formation:1||FORCE MICROSCOPY:1||RELAXATION:1||PLASMA RESONANCE:1||coupled Josephson junctions:1||COPPEROXIDE SUPERCONDUCTORS:1||CROSSOVER:1||SIMULATIONS:1||LOWTEMPERATURE:1||CONDUCTORS:1||METALINSULATORTRANSITION:1||SEMICONDUCTOR:1||FIELDEFFECT TRANSISTORS:1||ZEROVOLTAGE STATE:1||constanttemperature interlayer tunneling spectroscopy:1||Josephson supercurrent:1||BIPOLAR SUPERCURRENT:1||Interaction between Josephson and pancake vortices:1||flux jump:1||coaxial heterojunction nanorod:1||Natural Josephson coupling:1||BI2SR2CACU2O8+DELTA:1||VORTEX FLOW:1||TC SUPERCONDUCTORS:1||charge imbalance:1||Andreev diffractometer:1||intercalation:1||surface junction:1||Bi2212:1||tunnelling:1||GRAPHITE:1||GROWTH:1||collective transverse plasma modes:1||GAN:1||Macroscopic quantum tunneling:1||Fluctuation conductivity:1||Abovegap conductance jump:1||Josephson vortex motion:1||Intrinsic Josephson junctions:1||LAYERED SUPERCONDUCTORS:1||BI2SR2CACU2O8+Y:1||INTERFACES:1||BREAKDOWN:1||SYSTEMS:1||Anisotropy ratio:1||Josephson vortex:1||spin relaxation in superconductors:1||bibased single crystals:1||MESOSCOPIC PROXIMITY SUPERCONDUCTOR:1||reentrance of conductance:1||interlayer pair tunneling:1||JOSEPHSON:1||DISORDERED 2DIMENSIONAL SUPERCONDUCTORS:1||INDIUM FILMS:1||excited state:1||REGIME:1||triplet superconductivity:1||FILM:1||SCHOTTKY DIODES:1||peakdiphump structure:1||Kondo effect:1||REENTRANCE:1||Graphene:1||CONTACT:1||BERRYS PHASE:1||2DIMENSIONAL SUPERCONDUCTORS:1||Coulomb diamond:1||magnetic domain:1||spin injection:1||RESONANCE:1||plasma excitation modes:1||FLOW:1||OVERDOPED BI2SR2CACU2O8+DELTA:1||hole doping:1||chemical synthesis:1||phase transitions:1||superconductors:1||VORTEXGLASS SUPERCONDUCTIVITY:1||Kondorelated model:1||RADIATION:1||DOT:1||NANOBELTS:1||Complementarity:1||Closedloop AharonovBohm interferometer:1||pair breaking:1||interlayer phase fluctuation:1||MgB2 thin film:1||CONFINEMENT:1||WALLED CARBON NANOTUBES:1||TRANSITION:9||VORTICES:8||STATE:7||intrinsic Josephson junctions:7||SINGLECRYSTALS:7||JUNCTIONS:5||MODES:5||SUPERCURRENT:5||SUPERCONDUCTOR:5||CONDUCTANCE:5||HIGHTEMPERATURE SUPERCONDUCTORS:5||TRANSPORT:5||PHASE:5||FILMS:4||LOCALIZATION:4||SINGLE DIRAC CONE:4||WIRES:4||MAGNETICFIELD:4||STEPS:3||ELECTRONS:3||proximity effect:3||MODEL:3||ARRAYS:3||INTERFERENCE:3||fluxon dynamics:3||HETEROSTRUCTURES:3||INSULATOR:3||Andreev reflection:3||electronic transport:3||FISKE:3||superconductor:2||ZnO:2||quantum point contact:2||METAL:2||DYNAMICS:2||interlayer Josephson coupling:2||SUPERCONDUCTORS:2||YBA2CU3O7DELTA:2||LAYER:2||DOTS:2||quantum dot:2||Article:2||TRANSISTORS:2||CARBON NANOTUBES:2||GAP:2||MECHANISM:2||LINE:2||GIANT SHAPIRO STEPS:2||LAYERS:2||electron energy loss spectroscopy:2||physical phenomena:2||scanning electron microscopy:2||HGTE QUANTUMWELLS:2||BI2TE3:2||SPECTROSCOPY:2||PNJUNCTIONS:2||spinpolarized tunneling:2||INTRINSIC JOSEPHSONJUNCTIONS:2||FIELDS:2||positive magnetoresistance:2||dilute magnetic semiconductor:2||magnetic field:2||scanning transmission electron microscopy:2||QUANTUM OSCILLATIONS:2||TRANSPORTPROPERTIES:2||surface pair current:2||MAGNETORESISTANCE:2||NANORIBBONS:2||INSTABILITY:2||ANDREEV REFLECTION:2||microwave irradiation:2||vertical graphene josephson junction:2||BI2SE3:2||CONDUCTIVITY:2||highTc superconductors:2||DIMENSIONAL ELECTRONGAS:2||graphene:2||Topological insulators:2||Josephson coupling Fraunhofer interference pattern:2||FERROMAGNET:2||DEPENDENCE:2||DETECTOR:2||COHERENCE:2||INJECTION:2||GRAPHENE:1||JOSEPHSONJUNCTIONS:1||LAYERED SUPERCONDUCTOR:1||mode splitting:1||BEHAVIOR:1||spinpolarized transport:1||SUPERCONDUCTING TRANSITION:1||microwave response:1||PSEUDOGAP:1||phase coherence:1||TRANSITIONS:1||Long Josephson junction:1||Charge detection:1||collective resonance modes:1||plasma oscillation modes:1||Superconducting proximity effect:1||Iron pnictide superconductor:1||McMillanRowell oscillations:1||ferromagnetic microstructure:1||superradiant state:1||VOLTAGE:1||branch splitting:1||TENSOR:1||INTERCALATION:1||insitu fabrication:1||NDGAO3:1||DISORDERED METALS:1||GAUGE GLASS:1||LOWTEMPERATURE TRANSPORT:1||spontaneous spin polarization model:1||BIAS:1||emission of electromagnetic waves:1||YBA2CU3O7/PRBA2CU3O7 SUPERLATTICES:1||BOHM:1||SHAPIRO STEPS:1||superconductor/ferromagnet interface:1||OXIDE:1||ANDREEVREFLECTION:1||SinFeAsO single crystal:1||COLLECTIVE MOTION:1||ANGULARDEPENDENCE:1||SUPERCONDUCTIVITY:1||BILAYER GRAPHENE:1||PHOTOLUMINESCENT PROPERTIES:1||SUPERCONDUCTING WEAK LINKS:1||intrinsic Josephson junctions geometrical resonance:1||intrinsic Josephson junction:1||MESOSCOPIC SPINVALVE:1||Bi2212 single crystals:1||intrinsic junctions:1||ANDREEV REFLECTIONS:1||normalmetal/superconductor interface:1||IBI2SR2CACU2OY:1||THERMAL FLUCTUATIONS:1||MIXED STATE:1||BI2.15SR1.85CACU2O8+DELTA:1||intrinsic Josephson effects:1||CACUO:1||QUANTUM POINT CONTACTS:1||resonant tunneling state:1||coherence length:1||NANOWIRE:1||GATES:1||Phase line:1||Thermal activation:1||QUANTUMDOT:1||superconducting proximity effect:1||Andreev interferometer:1||WIRE:1||Josephsonvortexflow branches:1||Bi2212 cuprates:1||LATTICE:1||demannetization effect:1||SUPERCONDUCTING MIRRORS:1||GAS:1||VALLEY TRANSPORT:1||ELECTRODES:1||DEPENDENT TRANSPORT:1||BORNOPPENHEIMER APPROXIMATION:1||collective plasma oscillations:1||fluxon resonance steps:1||STACKS:1||COLLECTIVE DYNAMICS:1||PAIRING SYMMETRY:1||MUON SPIN ROTATION:1||DIMENSIONAL CROSSOVER:1||Bi2Sr2CaCu2Oy highTc superconductors:1||heterojunctions:1||nanostructures:1||surfaces and interfaces:1||QUANTUM TRANSPORT:1||MICROJUNCTIONS:1||RESONATORS:1||STATES:1||FIELD:1||FLUCTUATIONS:1||SCATTERING:1||mode splitting of Josephson vortexflow branches:1||2D superconductivity:1||TRANSISTOR:1||ENERGYGAP:1||SUPERLATTICES:1||IRONBASED SUPERCONDUCTORS:1||PHASEDEPENDENT RESISTANCE:1||QUANTUM PHASETRANSITIONS:1||ELECTRICFIELD:1||HIGH MAGNETICFIELDS:1||NANOWIRE HETEROSTRUCTURES:1||ZNO:1||pair breaking.:1||SUPERCONDUCTING PB:1||domain formation:1||FORCE MICROSCOPY:1||RELAXATION:1||PLASMA RESONANCE:1||coupled Josephson junctions:1||COPPEROXIDE SUPERCONDUCTORS:1||CROSSOVER:1||SIMULATIONS:1||LOWTEMPERATURE:1||CONDUCTORS:1||METALINSULATORTRANSITION:1||SEMICONDUCTOR:1||FIELDEFFECT TRANSISTORS:1||ZEROVOLTAGE STATE:1||constanttemperature interlayer tunneling spectroscopy:1||Josephson supercurrent:1||BIPOLAR SUPERCURRENT:1||Interaction between Josephson and pancake vortices:1||flux jump:1||coaxial heterojunction nanorod:1||Natural Josephson coupling:1||BI2SR2CACU2O8+DELTA:1||VORTEX FLOW:1||TC SUPERCONDUCTORS:1||charge imbalance:1||Andreev diffractometer:1||intercalation:1||surface junction:1||Bi2212:1||tunnelling:1||GRAPHITE:1||GROWTH:1||collective transverse plasma modes:1||GAN:1||Macroscopic quantum tunneling:1||Fluctuation conductivity:1||Abovegap conductance jump:1||Josephson vortex motion:1||Intrinsic Josephson junctions:1||LAYERED SUPERCONDUCTORS:1||BI2SR2CACU2O8+Y:1||INTERFACES:1||BREAKDOWN:1||SYSTEMS:1||Anisotropy ratio:1||Josephson vortex:1||spin relaxation in superconductors:1||bibased single crystals:1||MESOSCOPIC PROXIMITY SUPERCONDUCTOR:1||reentrance of conductance:1||interlayer pair tunneling:1||JOSEPHSON:1||DISORDERED 2DIMENSIONAL SUPERCONDUCTORS:1||INDIUM FILMS:1||excited state:1||REGIME:1||triplet superconductivity:1||FILM:1||SCHOTTKY DIODES:1||peakdiphump structure:1||Kondo effect:1||REENTRANCE:1||Graphene:1||CONTACT:1||BERRYS PHASE:1||2DIMENSIONAL SUPERCONDUCTORS:1||Coulomb diamond:1||magnetic domain:1||spin injection:1||RESONANCE:1||plasma excitation modes:1||FLOW:1||OVERDOPED BI2SR2CACU2O8+DELTA:1||hole doping:1||chemical synthesis:1||phase transitions:1||superconductors:1||VORTEXGLASS SUPERCONDUCTIVITY:1||Kondorelated model:1||RADIATION:1||DOT:1||NANOBELTS:1||Complementarity:1||Closedloop AharonovBohm interferometer:1||pair breaking:1||interlayer phase fluctuation:1||MgB2 thin film:1||CONFINEMENT:1||WALLED CARBON NANOTUBES:1||TRANSITION:9||VORTICES:8||STATE:7||intrinsic Josephson junctions:7||SINGLECRYSTALS:7||JUNCTIONS:5||MODES:5||SUPERCURRENT:5||SUPERCONDUCTOR:5||CONDUCTANCE:5||HIGHTEMPERATURE SUPERCONDUCTORS:5||TRANSPORT:5||PHASE:5||FILMS:4||LOCALIZATION:4||SINGLE DIRAC CONE:4||WIRES:4||MAGNETICFIELD:4||STEPS:3||ELECTRONS:3||proximity effect:3||MODEL:3||ARRAYS:3||INTERFERENCE:3||fluxon dynamics:3||HETEROSTRUCTURES:3||INSULATOR:3||Andreev reflection:3||electronic transport:3||FISKE:3||superconductor:2||ZnO:2||quantum point contact:2||METAL:2||DYNAMICS:2||interlayer Josephson coupling:2||SUPERCONDUCTORS:2||YBA2CU3O7DELTA:2||LAYER:2||DOTS:2||quantum dot:2||Article:2||TRANSISTORS:2||CARBON NANOTUBES:2||GAP:2||MECHANISM:2||LINE:2||GIANT SHAPIRO STEPS:2||LAYERS:2||electron energy loss spectroscopy:2||physical phenomena:2||scanning electron microscopy:2||HGTE QUANTUMWELLS:2||BI2TE3:2||SPECTROSCOPY:2||PNJUNCTIONS:2||spinpolarized tunneling:2||INTRINSIC JOSEPHSONJUNCTIONS:2||FIELDS:2||positive magnetoresistance:2||dilute magnetic semiconductor:2||magnetic field:2||scanning transmission electron microscopy:2||QUANTUM OSCILLATIONS:2||TRANSPORTPROPERTIES:2||surface pair current:2||MAGNETORESISTANCE:2||NANORIBBONS:2||INSTABILITY:2||ANDREEV REFLECTION:2||microwave irradiation:2||vertical graphene josephson junction:2||BI2SE3:2||CONDUCTIVITY:2||highTc superconductors:2||DIMENSIONAL ELECTRONGAS:2||graphene:2||Topological insulators:2||Josephson coupling Fraunhofer interference pattern:2||FERROMAGNET:2||DEPENDENCE:2||DETECTOR:2||COHERENCE:2||INJECTION:2||GRAPHENE:1||JOSEPHSONJUNCTIONS:1||LAYERED SUPERCONDUCTOR:1||mode splitting:1||BEHAVIOR:1||spinpolarized transport:1||SUPERCONDUCTING TRANSITION:1||microwave response:1||PSEUDOGAP:1||phase coherence:1||TRANSITIONS:1||Long Josephson junction:1||Charge detection:1||collective resonance modes:1||plasma oscillation modes:1||Superconducting proximity effect:1||Iron pnictide superconductor:1||McMillanRowell oscillations:1||ferromagnetic microstructure:1||superradiant state:1||VOLTAGE:1||branch splitting:1||TENSOR:1||INTERCALATION:1||insitu fabrication:1||NDGAO3:1||DISORDERED METALS:1||GAUGE GLASS:1||LOWTEMPERATURE TRANSPORT:1||spontaneous spin polarization model:1||BIAS:1||emission of electromagnetic waves:1||YBA2CU3O7/PRBA2CU3O7 SUPERLATTICES:1||BOHM:1||SHAPIRO STEPS:1||superconductor/ferromagnet interface:1||OXIDE:1||ANDREEVREFLECTION:1||SinFeAsO single crystal:1||COLLECTIVE MOTION:1||ANGULARDEPENDENCE:1||SUPERCONDUCTIVITY:1||BILAYER GRAPHENE:1||PHOTOLUMINESCENT PROPERTIES:1||SUPERCONDUCTING WEAK LINKS:1||intrinsic Josephson junctions geometrical resonance:1||intrinsic Josephson junction:1||MESOSCOPIC SPINVALVE:1||Bi2212 single crystals:1||intrinsic junctions:1||ANDREEV REFLECTIONS:1||normalmetal/superconductor interface:1||IBI2SR2CACU2OY:1||THERMAL FLUCTUATIONS:1||MIXED STATE:1||BI2.15SR1.85CACU2O8+DELTA:1||intrinsic Josephson effects:1||CACUO:1||QUANTUM POINT CONTACTS:1||resonant tunneling state:1||coherence length:1||NANOWIRE:1||GATES:1||Phase line:1||Thermal activation:1||QUANTUMDOT:1||superconducting proximity effect:1||Andreev interferometer:1||WIRE:1||Josephsonvortexflow branches:1||Bi2212 cuprates:1||LATTICE:1||demannetization effect:1||SUPERCONDUCTING MIRRORS:1||GAS:1||VALLEY TRANSPORT:1||ELECTRODES:1||DEPENDENT TRANSPORT:1||BORNOPPENHEIMER APPROXIMATION:1||collective plasma oscillations:1||fluxon resonance steps:1||STACKS:1||COLLECTIVE DYNAMICS:1||PAIRING SYMMETRY:1||MUON SPIN ROTATION:1||DIMENSIONAL CROSSOVER:1||Bi2Sr2CaCu2Oy highTc superconductors:1||heterojunctions:1||nanostructures:1||surfaces and interfaces:1||QUANTUM TRANSPORT:1||MICROJUNCTIONS:1||RESONATORS:1||STATES:1||FIELD:1||FLUCTUATIONS:1||SCATTERING:1||mode splitting of Josephson vortexflow branches:1||2D superconductivity:1||TRANSISTOR:1||ENERGYGAP:1||SUPERLATTICES:1||IRONBASED SUPERCONDUCTORS:1||PHASEDEPENDENT RESISTANCE:1||QUANTUM PHASETRANSITIONS:1||ELECTRICFIELD:1||HIGH MAGNETICFIELDS:1||NANOWIRE HETEROSTRUCTURES:1||ZNO:1||pair breaking.:1||SUPERCONDUCTING PB:1||domain formation:1||FORCE MICROSCOPY:1||RELAXATION:1||PLASMA RESONANCE:1||coupled Josephson junctions:1||COPPEROXIDE SUPERCONDUCTORS:1||CROSSOVER:1||SIMULATIONS:1||LOWTEMPERATURE:1||CONDUCTORS:1||METALINSULATORTRANSITION:1||SEMICONDUCTOR:1||FIELDEFFECT TRANSISTORS:1||ZEROVOLTAGE STATE:1||constanttemperature interlayer tunneling spectroscopy:1||Josephson supercurrent:1||BIPOLAR SUPERCURRENT:1||Interaction between Josephson and pancake vortices:1||flux jump:1||coaxial heterojunction nanorod:1||Natural Josephson coupling:1||BI2SR2CACU2O8+DELTA:1||VORTEX FLOW:1||TC SUPERCONDUCTORS:1||charge imbalance:1||Andreev diffractometer:1||intercalation:1||surface junction:1||Bi2212:1||tunnelling:1||GRAPHITE:1||GROWTH:1||collective transverse plasma modes:1||GAN:1||Macroscopic quantum tunneling:1||Fluctuation conductivity:1||Abovegap conductance jump:1||Josephson vortex motion:1||Intrinsic Josephson junctions:1||LAYERED SUPERCONDUCTORS:1||BI2SR2CACU2O8+Y:1||INTERFACES:1||BREAKDOWN:1||SYSTEMS:1||Anisotropy ratio:1||Josephson vortex:1||spin relaxation in superconductors:1||bibased single crystals:1||MESOSCOPIC PROXIMITY SUPERCONDUCTOR:1||reentrance of conductance:1||interlayer pair tunneling:1||JOSEPHSON:1||DISORDERED 2DIMENSIONAL SUPERCONDUCTORS:1||INDIUM FILMS:1||excited state:1||REGIME:1||triplet superconductivity:1||FILM:1||SCHOTTKY DIODES:1||peakdiphump structure:1||Kondo effect:1||REENTRANCE:1||Graphene:1||CONTACT:1||BERRYS PHASE:1||2DIMENSIONAL SUPERCONDUCTORS:1||Coulomb diamond:1||magnetic domain:1||spin injection:1||RESONANCE:1||plasma excitation modes:1||FLOW:1||OVERDOPED BI2SR2CACU2O8+DELTA:1||hole doping:1||chemical synthesis:1||phase transitions:1||superconductors:1||VORTEXGLASS SUPERCONDUCTIVITY:1||Kondorelated model:1||RADIATION:1||DOT:1||NANOBELTS:1||Complementarity:1||Closedloop AharonovBohm interferometer:1||pair breaking:1||interlayer phase fluctuation:1||MgB2 thin film:1||CONFINEMENT:1||WALLED CARBON NANOTUBES:1||TRANSITION:9||VORTICES:8||STATE:7||intrinsic Josephson junctions:7||SINGLECRYSTALS:7||JUNCTIONS:5||MODES:5||SUPERCURRENT:5||SUPERCONDUCTOR:5||CONDUCTANCE:5||HIGHTEMPERATURE SUPERCONDUCTORS:5||TRANSPORT:5||PHASE:5||FILMS:4||LOCALIZATION:4||SINGLE DIRAC CONE:4||WIRES:4||MAGNETICFIELD:4||STEPS:3||ELECTRONS:3||proximity effect:3||MODEL:3||ARRAYS:3||INTERFERENCE:3||fluxon dynamics:3||HETEROSTRUCTURES:3||INSULATOR:3||Andreev reflection:3||electronic transport:3||FISKE:3||superconductor:2||ZnO:2||quantum point contact:2||METAL:2||DYNAMICS:2||interlayer Josephson coupling:2||SUPERCONDUCTORS:2||YBA2CU3O7DELTA:2||LAYER:2||DOTS:2||quantum dot:2||Article:2||TRANSISTORS:2||CARBON NANOTUBES:2||GAP:2||MECHANISM:2||LINE:2||GIANT SHAPIRO STEPS:2||LAYERS:2||electron energy loss spectroscopy:2||physical phenomena:2||scanning electron microscopy:2||HGTE QUANTUMWELLS:2||BI2TE3:2||SPECTROSCOPY:2||PNJUNCTIONS:2||spinpolarized tunneling:2||INTRINSIC JOSEPHSONJUNCTIONS:2||FIELDS:2||positive magnetoresistance:2||dilute magnetic semiconductor:2||magnetic field:2||scanning transmission electron microscopy:2||QUANTUM OSCILLATIONS:2||TRANSPORTPROPERTIES:2||surface pair current:2||MAGNETORESISTANCE:2||NANORIBBONS:2||INSTABILITY:2||ANDREEV REFLECTION:2||microwave irradiation:2||vertical graphene josephson junction:2||BI2SE3:2||CONDUCTIVITY:2||highTc superconductors:2||DIMENSIONAL ELECTRONGAS:2||graphene:2||Topological insulators:2||Josephson coupling Fraunhofer interference pattern:2||FERROMAGNET:2||DEPENDENCE:2||DETECTOR:2||COHERENCE:2||INJECTION:2||GRAPHENE:1||JOSEPHSONJUNCTIONS:1||LAYERED SUPERCONDUCTOR:1||mode splitting:1||BEHAVIOR:1||spinpolarized transport:1||SUPERCONDUCTING TRANSITION:1||microwave response:1||PSEUDOGAP:1||phase coherence:1||TRANSITIONS:1||Long Josephson junction:1||Charge detection:1||collective resonance modes:1||plasma oscillation modes:1||Superconducting proximity effect:1||Iron pnictide superconductor:1||McMillanRowell oscillations:1||ferromagnetic microstructure:1||superradiant state:1||VOLTAGE:1||branch splitting:1||TENSOR:1||INTERCALATION:1||insitu fabrication:1||NDGAO3:1||DISORDERED METALS:1||GAUGE GLASS:1||LOWTEMPERATURE TRANSPORT:1||spontaneous spin polarization model:1||BIAS:1||emission of electromagnetic waves:1||YBA2CU3O7/PRBA2CU3O7 SUPERLATTICES:1||BOHM:1||SHAPIRO STEPS:1||superconductor/ferromagnet interface:1||OXIDE:1||ANDREEVREFLECTION:1||SinFeAsO single crystal:1||COLLECTIVE MOTION:1||ANGULARDEPENDENCE:1||SUPERCONDUCTIVITY:1||BILAYER GRAPHENE:1||PHOTOLUMINESCENT PROPERTIES:1||SUPERCONDUCTING WEAK LINKS:1||intrinsic Josephson junctions geometrical resonance:1||intrinsic Josephson junction:1||MESOSCOPIC SPINVALVE:1||Bi2212 single crystals:1||intrinsic junctions:1||ANDREEV REFLECTIONS:1||normalmetal/superconductor interface:1||IBI2SR2CACU2OY:1||THERMAL FLUCTUATIONS:1||MIXED STATE:1||BI2.15SR1.85CACU2O8+DELTA:1||intrinsic Josephson effects:1||CACUO:1||QUANTUM POINT CONTACTS:1||resonant tunneling state:1||coherence length:1||NANOWIRE:1||GATES:1||Phase line:1||Thermal activation:1||QUANTUMDOT:1||superconducting proximity effect:1||Andreev interferometer:1||WIRE:1||Josephsonvortexflow branches:1||Bi2212 cuprates:1||LATTICE:1||demannetization effect:1||SUPERCONDUCTING MIRRORS:1||GAS:1||VALLEY TRANSPORT:1||ELECTRODES:1||DEPENDENT TRANSPORT:1||BORNOPPENHEIMER APPROXIMATION:1||collective plasma oscillations:1||fluxon resonance steps:1||STACKS:1||COLLECTIVE DYNAMICS:1||PAIRING SYMMETRY:1||MUON SPIN ROTATION:1||DIMENSIONAL CROSSOVER:1||Bi2Sr2CaCu2Oy highTc superconductors:1||heterojunctions:1||nanostructures:1||surfaces and interfaces:1||QUANTUM TRANSPORT:1||MICROJUNCTIONS:1||RESONATORS:1||STATES:1||FIELD:1||FLUCTUATIONS:1||SCATTERING:1||mode splitting of Josephson vortexflow branches:1||2D superconductivity:1||TRANSISTOR:1||ENERGYGAP:1||SUPERLATTICES:1||IRONBASED SUPERCONDUCTORS:1||PHASEDEPENDENT RESISTANCE:1||QUANTUM PHASETRANSITIONS:1||ELECTRICFIELD:1||HIGH MAGNETICFIELDS:1||NANOWIRE HETEROSTRUCTURES:1||ZNO:1||pair breaking.:1||SUPERCONDUCTING PB:1||domain formation:1||FORCE MICROSCOPY:1||RELAXATION:1||PLASMA RESONANCE:1||coupled Josephson junctions:1||COPPEROXIDE SUPERCONDUCTORS:1||CROSSOVER:1||SIMULATIONS:1||LOWTEMPERATURE:1||CONDUCTORS:1||METALINSULATORTRANSITION:1||SEMICONDUCTOR:1||FIELDEFFECT TRANSISTORS:1||ZEROVOLTAGE STATE:1||constanttemperature interlayer tunneling spectroscopy:1||Josephson supercurrent:1||BIPOLAR SUPERCURRENT:1||Interaction between Josephson and pancake vortices:1||flux jump:1||coaxial heterojunction nanorod:1||Natural Josephson coupling:1||BI2SR2CACU2O8+DELTA:1||VORTEX FLOW:1||TC SUPERCONDUCTORS:1||charge imbalance:1||Andreev diffractometer:1||intercalation:1||surface junction:1||Bi2212:1||tunnelling:1||GRAPHITE:1||GROWTH:1||collective transverse plasma modes:1||GAN:1||Macroscopic quantum tunneling:1||Fluctuation conductivity:1||Abovegap conductance jump:1||Josephson vortex motion:1||Intrinsic Josephson junctions:1||LAYERED SUPERCONDUCTORS:1||BI2SR2CACU2O8+Y:1||INTERFACES:1||BREAKDOWN:1||SYSTEMS:1||Anisotropy ratio:1||Josephson vortex:1||spin relaxation in superconductors:1||bibased single crystals:1||MESOSCOPIC PROXIMITY SUPERCONDUCTOR:1||reentrance of conductance:1||interlayer pair tunneling:1||JOSEPHSON:1||DISORDERED 2DIMENSIONAL SUPERCONDUCTORS:1||INDIUM FILMS:1||excited state:1||REGIME:1||triplet superconductivity:1||FILM:1||SCHOTTKY DIODES:1||peakdiphump structure:1||Kondo effect:1||REENTRANCE:1||Graphene:1||CONTACT:1||BERRYS PHASE:1||2DIMENSIONAL SUPERCONDUCTORS:1||Coulomb diamond:1||magnetic domain:1||spin injection:1||RESONANCE:1||plasma excitation modes:1||FLOW:1||OVERDOPED BI2SR2CACU2O8+DELTA:1||hole doping:1||chemical synthesis:1||phase transitions:1||superconductors:1||VORTEXGLASS SUPERCONDUCTIVITY:1||Kondorelated model:1||RADIATION:1||DOT:1||NANOBELTS:1||Complementarity:1||Closedloop AharonovBohm interferometer:1||pair breaking:1||interlayer phase fluctuation:1||MgB2 thin film:1||CONFINEMENT:1||WALLED CARBON NANOTUBES:1||TRANSITION:9||VORTICES:8||STATE:7||intrinsic Josephson junctions:7||SINGLECRYSTALS:7||JUNCTIONS:5||MODES:5||SUPERCURRENT:5||SUPERCONDUCTOR:5||CONDUCTANCE:5||HIGHTEMPERATURE SUPERCONDUCTORS:5||TRANSPORT:5||PHASE:5||FILMS:4||LOCALIZATION:4||SINGLE DIRAC CONE:4||WIRES:4||MAGNETICFIELD:4||STEPS:3||ELECTRONS:3||proximity effect:3||MODEL:3||ARRAYS:3||INTERFERENCE:3||fluxon dynamics:3||HETEROSTRUCTURES:3||INSULATOR:3||Andreev reflection:3||electronic transport:3||FISKE:3||superconductor:2||ZnO:2||quantum point contact:2||METAL:2||DYNAMICS:2||interlayer Josephson coupling:2||SUPERCONDUCTORS:2||YBA2CU3O7DELTA:2||LAYER:2||DOTS:2||quantum dot:2||Article:2||TRANSISTORS:2||CARBON NANOTUBES:2||GAP:2||MECHANISM:2||LINE:2||GIANT SHAPIRO STEPS:2||LAYERS:2||electron energy loss spectroscopy:2||physical phenomena:2||scanning electron microscopy:2||HGTE QUANTUMWELLS:2||BI2TE3:2||SPECTROSCOPY:2||PNJUNCTIONS:2||spinpolarized tunneling:2||INTRINSIC JOSEPHSONJUNCTIONS:2||FIELDS:2||positive magnetoresistance:2||dilute magnetic semiconductor:2||magnetic field:2||scanning transmission electron microscopy:2||QUANTUM OSCILLATIONS:2||TRANSPORTPROPERTIES:2||surface pair current:2||MAGNETORESISTANCE:2||NANORIBBONS:2||INSTABILITY:2||ANDREEV REFLECTION:2||microwave irradiation:2||vertical graphene josephson junction:2||BI2SE3:2||CONDUCTIVITY:2||highTc superconductors:2||DIMENSIONAL ELECTRONGAS:2||graphene:2||Topological insulators:2||Josephson coupling Fraunhofer interference pattern:2||FERROMAGNET:2||DEPENDENCE:2||DETECTOR:2||COHERENCE:2||INJECTION:2||GRAPHENE:1||JOSEPHSONJUNCTIONS:1||LAYERED SUPERCONDUCTOR:1||mode splitting:1||BEHAVIOR:1||spinpolarized transport:1||SUPERCONDUCTING TRANSITION:1||microwave response:1||PSEUDOGAP:1||phase coherence:1||TRANSITIONS:1||Long Josephson junction:1||Charge detection:1||collective resonance modes:1||plasma oscillation modes:1||Superconducting proximity effect:1||Iron pnictide superconductor:1||McMillanRowell oscillations:1||ferromagnetic microstructure:1||superradiant state:1||VOLTAGE:1||branch splitting:1||TENSOR:1||INTERCALATION:1||insitu fabrication:1||NDGAO3:1||DISORDERED METALS:1||GAUGE GLASS:1||LOWTEMPERATURE TRANSPORT:1||spontaneous spin polarization model:1||BIAS:1||emission of electromagnetic waves:1||YBA2CU3O7/PRBA2CU3O7 SUPERLATTICES:1||BOHM:1||SHAPIRO STEPS:1||superconductor/ferromagnet interface:1||OXIDE:1||ANDREEVREFLECTION:1||SinFeAsO single crystal:1||COLLECTIVE MOTION:1||ANGULARDEPENDENCE:1||SUPERCONDUCTIVITY:1||BILAYER GRAPHENE:1||PHOTOLUMINESCENT PROPERTIES:1||SUPERCONDUCTING WEAK LINKS:1||intrinsic Josephson junctions geometrical resonance:1||intrinsic Josephson junction:1||MESOSCOPIC SPINVALVE:1||Bi2212 single crystals:1||intrinsic junctions:1||ANDREEV REFLECTIONS:1||normalmetal/superconductor interface:1||IBI2SR2CACU2OY:1||THERMAL FLUCTUATIONS:1||MIXED STATE:1||BI2.15SR1.85CACU2O8+DELTA:1||intrinsic Josephson effects:1||CACUO:1||QUANTUM POINT CONTACTS:1||resonant tunneling state:1||coherence length:1||NANOWIRE:1||GATES:1||Phase line:1||Thermal activation:1||QUANTUMDOT:1||superconducting proximity effect:1||Andreev interferometer:1||WIRE:1||Josephsonvortexflow branches:1||Bi2212 cuprates:1||LATTICE:1||demannetization effect:1||SUPERCONDUCTING MIRRORS:1||GAS:1||VALLEY TRANSPORT:1||ELECTRODES:1||DEPENDENT TRANSPORT:1||BORNOPPENHEIMER APPROXIMATION:1||collective plasma oscillations:1||fluxon resonance steps:1||STACKS:1||COLLECTIVE DYNAMICS:1||PAIRING SYMMETRY:1||MUON SPIN ROTATION:1||DIMENSIONAL CROSSOVER:1||Bi2Sr2CaCu2Oy highTc superconductors:1||heterojunctions:1||nanostructures:1||surfaces and interfaces:1||QUANTUM TRANSPORT:1||MICROJUNCTIONS:1||RESONATORS:1||STATES:1||FIELD:1||FLUCTUATIONS:1||SCATTERING:1||mode splitting of Josephson vortexflow branches:1||2D superconductivity:1||TRANSISTOR:1||ENERGYGAP:1||SUPERLATTICES:1||IRONBASED SUPERCONDUCTORS:1||PHASEDEPENDENT RESISTANCE:1||QUANTUM PHASETRANSITIONS:1||ELECTRICFIELD:1||HIGH MAGNETICFIELDS:1||NANOWIRE HETEROSTRUCTURES:1||ZNO:1||pair breaking.:1||SUPERCONDUCTING PB:1||domain formation:1||FORCE MICROSCOPY:1||RELAXATION:1||PLASMA RESONANCE:1||coupled Josephson junctions:1||COPPEROXIDE SUPERCONDUCTORS:1||CROSSOVER:1||SIMULATIONS:1||LOWTEMPERATURE:1||CONDUCTORS:1||METALINSULATORTRANSITION:1||SEMICONDUCTOR:1||FIELDEFFECT TRANSISTORS:1||ZEROVOLTAGE STATE:1||constanttemperature interlayer tunneling spectroscopy:1||Josephson supercurrent:1||BIPOLAR SUPERCURRENT:1||Interaction between Josephson and pancake vortices:1||flux jump:1||coaxial heterojunction nanorod:1||Natural Josephson coupling:1||BI2SR2CACU2O8+DELTA:1||VORTEX FLOW:1||TC SUPERCONDUCTORS:1||charge imbalance:1||Andreev diffractometer:1||intercalation:1||surface junction:1||Bi2212:1||tunnelling:1||GRAPHITE:1||GROWTH:1||collective transverse plasma modes:1||GAN:1||Macroscopic quantum tunneling:1||Fluctuation conductivity:1||Abovegap conductance jump:1||Josephson vortex motion:1||Intrinsic Josephson junctions:1||LAYERED SUPERCONDUCTORS:1||BI2SR2CACU2O8+Y:1||INTERFACES:1||BREAKDOWN:1||SYSTEMS:1||Anisotropy ratio:1||Josephson vortex:1||spin relaxation in superconductors:1||bibased single crystals:1||MESOSCOPIC PROXIMITY SUPERCONDUCTOR:1||reentrance of conductance:1||interlayer pair tunneling:1||JOSEPHSON:1||DISORDERED 2DIMENSIONAL SUPERCONDUCTORS:1||INDIUM FILMS:1||excited state:1||REGIME:1||triplet superconductivity:1||FILM:1||SCHOTTKY DIODES:1||peakdiphump structure:1||Kondo effect:1||REENTRANCE:1||Graphene:1||CONTACT:1||BERRYS PHASE:1||2DIMENSIONAL SUPERCONDUCTORS:1||Coulomb diamond:1||magnetic domain:1||spin injection:1||RESONANCE:1||plasma excitation modes:1||FLOW:1||OVERDOPED BI2SR2CACU2O8+DELTA:1||hole doping:1||chemical synthesis:1||phase transitions:1||superconductors:1||VORTEXGLASS SUPERCONDUCTIVITY:1||Kondorelated model:1||RADIATION:1||DOT:1||NANOBELTS:1||Complementarity:1||Closedloop AharonovBohm interferometer:1||pair breaking:1||interlayer phase fluctuation:1||MgB2 thin film:1||CONFINEMENT:1||WALLED CARBON NANOTUBES:1||TRANSITION:9||VORTICES:8||STATE:7||intrinsic Josephson junctions:7||SINGLECRYSTALS:7||JUNCTIONS:5||MODES:5||SUPERCURRENT:5||SUPERCONDUCTOR:5||CONDUCTANCE:5||HIGHTEMPERATURE SUPERCONDUCTORS:5||TRANSPORT:5||PHASE:5||FILMS:4||LOCALIZATION:4||SINGLE DIRAC CONE:4||WIRES:4||MAGNETICFIELD:4||STEPS:3||ELECTRONS:3||proximity effect:3||MODEL:3||ARRAYS:3||INTERFERENCE:3||fluxon dynamics:3||HETEROSTRUCTURES:3||INSULATOR:3||Andreev reflection:3||electronic transport:3||FISKE:3||superconductor:2||ZnO:2||quantum point contact:2||METAL:2||DYNAMICS:2||interlayer Josephson coupling:2||SUPERCONDUCTORS:2||YBA2CU3O7DELTA:2||LAYER:2||DOTS:2||quantum dot:2||Article:2||TRANSISTORS:2||CARBON NANOTUBES:2||GAP:2||MECHANISM:2||LINE:2||GIANT SHAPIRO STEPS:2||LAYERS:2||electron energy loss spectroscopy:2||physical phenomena:2||scanning electron microscopy:2||HGTE QUANTUMWELLS:2||BI2TE3:2||SPECTROSCOPY:2||PNJUNCTIONS:2||spinpolarized tunneling:2||INTRINSIC JOSEPHSONJUNCTIONS:2||FIELDS:2||positive magnetoresistance:2||dilute magnetic semiconductor:2||magnetic field:2||scanning transmission electron microscopy:2||QUANTUM OSCILLATIONS:2||TRANSPORTPROPERTIES:2||surface pair current:2||MAGNETORESISTANCE:2||NANORIBBONS:2||INSTABILITY:2||ANDREEV REFLECTION:2||microwave irradiation:2||vertical graphene josephson junction:2||BI2SE3:2||CONDUCTIVITY:2||highTc superconductors:2||DIMENSIONAL ELECTRONGAS:2||graphene:2||Topological insulators:2||Josephson coupling Fraunhofer interference pattern:2||FERROMAGNET:2||DEPENDENCE:2||DETECTOR:2||COHERENCE:2||INJECTION:2||GRAPHENE:1||JOSEPHSONJUNCTIONS:1||LAYERED SUPERCONDUCTOR:1||mode splitting:1||BEHAVIOR:1||spinpolarized transport:1||SUPERCONDUCTING TRANSITION:1||microwave response:1||PSEUDOGAP:1||phase coherence:1||TRANSITIONS:1||Long Josephson junction:1||Charge detection:1||collective resonance modes:1||plasma oscillation modes:1||Superconducting proximity effect:1||Iron pnictide superconductor:1||McMillanRowell oscillations:1||ferromagnetic microstructure:1||superradiant state:1||VOLTAGE:1||branch splitting:1||TENSOR:1||INTERCALATION:1||insitu fabrication:1||NDGAO3:1||DISORDERED METALS:1||GAUGE GLASS:1||LOWTEMPERATURE TRANSPORT:1||spontaneous spin polarization model:1||BIAS:1||emission of electromagnetic waves:1||YBA2CU3O7/PRBA2CU3O7 SUPERLATTICES:1||BOHM:1||SHAPIRO STEPS:1||superconductor/ferromagnet interface:1||OXIDE:1||ANDREEVREFLECTION:1||SinFeAsO single crystal:1||COLLECTIVE MOTION:1||ANGULARDEPENDENCE:1||SUPERCONDUCTIVITY:1||BILAYER GRAPHENE:1||PHOTOLUMINESCENT PROPERTIES:1||SUPERCONDUCTING WEAK LINKS:1||intrinsic Josephson junctions geometrical resonance:1||intrinsic Josephson junction:1||MESOSCOPIC SPINVALVE:1||Bi2212 single crystals:1||intrinsic junctions:1||ANDREEV REFLECTIONS:1||normalmetal/superconductor interface:1||IBI2SR2CACU2OY:1||THERMAL FLUCTUATIONS:1||MIXED STATE:1||BI2.15SR1.85CACU2O8+DELTA:1||intrinsic Josephson effects:1||CACUO:1||QUANTUM POINT CONTACTS:1||resonant tunneling state:1||coherence length:1||NANOWIRE:1||GATES:1||Phase line:1||Thermal activation:1||QUANTUMDOT:1||superconducting proximity effect:1||Andreev interferometer:1||WIRE:1||Josephsonvortexflow branches:1||Bi2212 cuprates:1||LATTICE:1||demannetization effect:1||SUPERCONDUCTING MIRRORS:1||GAS:1||VALLEY TRANSPORT:1||ELECTRODES:1||DEPENDENT TRANSPORT:1||BORNOPPENHEIMER APPROXIMATION:1||collective plasma oscillations:1||fluxon resonance steps:1||STACKS:1||COLLECTIVE DYNAMICS:1||PAIRING SYMMETRY:1||MUON SPIN ROTATION:1||DIMENSIONAL CROSSOVER:1||Bi2Sr2CaCu2Oy highTc superconductors:1||heterojunctions:1||nanostructures:1||surfaces and interfaces:1||QUANTUM TRANSPORT:1||MICROJUNCTIONS:1||RESONATORS:1||STATES:1||FIELD:1||FLUCTUATIONS:1||SCATTERING:1||mode splitting of Josephson vortexflow branches:1||2D superconductivity:1||TRANSISTOR:1||ENERGYGAP:1||SUPERLATTICES:1||IRONBASED SUPERCONDUCTORS:1||PHASEDEPENDENT RESISTANCE:1||QUANTUM PHASETRANSITIONS:1||ELECTRICFIELD:1||HIGH MAGNETICFIELDS:1||NANOWIRE HETEROSTRUCTURES:1||ZNO:1||pair breaking.:1||SUPERCONDUCTING PB:1||domain formation:1||FORCE MICROSCOPY:1||RELAXATION:1||PLASMA RESONANCE:1||coupled Josephson junctions:1||COPPEROXIDE SUPERCONDUCTORS:1||CROSSOVER:1||SIMULATIONS:1||LOWTEMPERATURE:1||CONDUCTORS:1||METALINSULATORTRANSITION:1||SEMICONDUCTOR:1||FIELDEFFECT TRANSISTORS:1||ZEROVOLTAGE STATE:1||constanttemperature interlayer tunneling spectroscopy:1||Josephson supercurrent:1||BIPOLAR SUPERCURRENT:1||Interaction between Josephson and pancake vortices:1||flux jump:1||coaxial heterojunction nanorod:1||Natural Josephson coupling:1||BI2SR2CACU2O8+DELTA:1||VORTEX FLOW:1||TC SUPERCONDUCTORS:1||charge imbalance:1||Andreev diffractometer:1||intercalation:1||surface junction:1||Bi2212:1||tunnelling:1||GRAPHITE:1||GROWTH:1||collective transverse plasma modes:1||GAN:1||Macroscopic quantum tunneling:1||Fluctuation conductivity:1||Abovegap conductance jump:1||Josephson vortex motion:1||Intrinsic Josephson junctions:1||LAYERED SUPERCONDUCTORS:1||BI2SR2CACU2O8+Y:1||INTERFACES:1||BREAKDOWN:1||SYSTEMS:1||Anisotropy ratio:1||Josephson vortex:1||spin relaxation in superconductors:1||bibased single crystals:1||MESOSCOPIC PROXIMITY SUPERCONDUCTOR:1||reentrance of conductance:1||interlayer pair tunneling:1||JOSEPHSON:1||DISORDERED 2DIMENSIONAL SUPERCONDUCTORS:1||INDIUM FILMS:1||excited state:1||REGIME:1||triplet superconductivity:1||FILM:1||SCHOTTKY DIODES:1||peakdiphump structure:1||Kondo effect:1||REENTRANCE:1||Graphene:1||CONTACT:1||BERRYS PHASE:1||2DIMENSIONAL SUPERCONDUCTORS:1||Coulomb diamond:1||magnetic domain:1||spin injection:1||RESONANCE:1||plasma excitation modes:1||FLOW:1||OVERDOPED BI2SR2CACU2O8+DELTA:1||hole doping:1||chemical synthesis:1||phase transitions:1||superconductors:1||VORTEXGLASS SUPERCONDUCTIVITY:1||Kondorelated model:1||RADIATION:1||DOT:1||NANOBELTS:1||Complementarity:1||Closedloop AharonovBohm interferometer:1||pair breaking:1||interlayer phase fluctuation:1||MgB2 thin film:1||CONFINEMENT:1||WALLED CARBON NANOTUBES:1||TRANSITION:9||VORTICES:8||STATE:7||intrinsic Josephson junctions:7||SINGLECRYSTALS:7||JUNCTIONS:5||MODES:5||SUPERCURRENT:5||SUPERCONDUCTOR:5||CONDUCTANCE:5||HIGHTEMPERATURE SUPERCONDUCTORS:5||TRANSPORT:5||PHASE:5||FILMS:4||LOCALIZATION:4||SINGLE DIRAC CONE:4||WIRES:4||MAGNETICFIELD:4||STEPS:3||ELECTRONS:3||proximity effect:3||MODEL:3||ARRAYS:3||INTERFERENCE:3||fluxon dynamics:3||HETEROSTRUCTURES:3||INSULATOR:3||Andreev reflection:3||electronic transport:3||FISKE:3||superconductor:2||ZnO:2||quantum point contact:2||METAL:2||DYNAMICS:2||interlayer Josephson coupling:2||SUPERCONDUCTORS:2||YBA2CU3O7DELTA:2||LAYER:2||DOTS:2||quantum dot:2||Article:2||TRANSISTORS:2||CARBON NANOTUBES:2||GAP:2||MECHANISM:2||LINE:2||GIANT SHAPIRO STEPS:2||LAYERS:2||electron energy loss spectroscopy:2||physical phenomena:2||scanning electron microscopy:2||HGTE QUANTUMWELLS:2||BI2TE3:2||SPECTROSCOPY:2||PNJUNCTIONS:2||spinpolarized tunneling:2||INTRINSIC JOSEPHSONJUNCTIONS:2||FIELDS:2||positive magnetoresistance:2||dilute magnetic semiconductor:2||magnetic field:2||scanning transmission electron microscopy:2||QUANTUM OSCILLATIONS:2||TRANSPORTPROPERTIES:2||surface pair current:2||MAGNETORESISTANCE:2||NANORIBBONS:2||INSTABILITY:2||ANDREEV REFLECTION:2||microwave irradiation:2||vertical graphene josephson junction:2||BI2SE3:2||CONDUCTIVITY:2||highTc superconductors:2||DIMENSIONAL ELECTRONGAS:2||graphene:2||Topological insulators:2||Josephson coupling Fraunhofer interference pattern:2||FERROMAGNET:2||DEPENDENCE:2||DETECTOR:2||COHERENCE:2||INJECTION:2||GRAPHENE:1||JOSEPHSONJUNCTIONS:1||LAYERED SUPERCONDUCTOR:1||mode splitting:1||BEHAVIOR:1||spinpolarized transport:1||SUPERCONDUCTING TRANSITION:1||microwave response:1||PSEUDOGAP:1||phase coherence:1||TRANSITIONS:1||Long Josephson junction:1||Charge detection:1||collective resonance modes:1||plasma oscillation modes:1||Superconducting proximity effect:1||Iron pnictide superconductor:1||McMillanRowell oscillations:1||ferromagnetic microstructure:1||superradiant state:1||VOLTAGE:1||branch splitting:1||TENSOR:1||INTERCALATION:1||insitu fabrication:1||NDGAO3:1||DISORDERED METALS:1||GAUGE GLASS:1||LOWTEMPERATURE TRANSPORT:1||spontaneous spin polarization model:1||BIAS:1||emission of electromagnetic waves:1||YBA2CU3O7/PRBA2CU3O7 SUPERLATTICES:1||BOHM:1||SHAPIRO STEPS:1||superconductor/ferromagnet interface:1||OXIDE:1||ANDREEVREFLECTION:1||SinFeAsO single crystal:1||COLLECTIVE MOTION:1||ANGULARDEPENDENCE:1||SUPERCONDUCTIVITY:1||BILAYER GRAPHENE:1||PHOTOLUMINESCENT PROPERTIES:1||SUPERCONDUCTING WEAK LINKS:1||intrinsic Josephson junctions geometrical resonance:1||intrinsic Josephson junction:1||MESOSCOPIC SPINVALVE:1||Bi2212 single crystals:1||intrinsic junctions:1||ANDREEV REFLECTIONS:1||normalmetal/superconductor interface:1||IBI2SR2CACU2OY:1||THERMAL FLUCTUATIONS:1||MIXED STATE:1||BI2.15SR1.85CACU2O8+DELTA:1||intrinsic Josephson effects:1||CACUO:1||QUANTUM POINT CONTACTS:1||resonant tunneling state:1||coherence length:1||NANOWIRE:1||GATES:1||Phase line:1||Thermal activation:1||QUANTUMDOT:1||superconducting proximity effect:1||Andreev interferometer:1||WIRE:1||Josephsonvortexflow branches:1||Bi2212 cuprates:1||LATTICE:1||demannetization effect:1||SUPERCONDUCTING MIRRORS:1||GAS:1||VALLEY TRANSPORT:1||ELECTRODES:1||DEPENDENT TRANSPORT:1||BORNOPPENHEIMER APPROXIMATION:1||collective plasma oscillations:1||fluxon resonance steps:1||STACKS:1||COLLECTIVE DYNAMICS:1||PAIRING SYMMETRY:1||MUON SPIN ROTATION:1||DIMENSIONAL CROSSOVER:1||Bi2Sr2CaCu2Oy highTc superconductors:1||heterojunctions:1||nanostructures:1||surfaces and interfaces:1||QUANTUM TRANSPORT:1||MICROJUNCTIONS:1||RESONATORS:1||STATES:1||FIELD:1||FLUCTUATIONS:1||SCATTERING:1||mode splitting of Josephson vortexflow branches:1||2D superconductivity:1||TRANSISTOR:1||ENERGYGAP:1||SUPERLATTICES:1||IRONBASED SUPERCONDUCTORS:1||PHASEDEPENDENT RESISTANCE:1||QUANTUM PHASETRANSITIONS:1||ELECTRICFIELD:1||HIGH MAGNETICFIELDS:1||NANOWIRE HETEROSTRUCTURES:1||ZNO:1||pair breaking.:1||SUPERCONDUCTING PB:1||domain formation:1||FORCE MICROSCOPY:1||RELAXATION:1||PLASMA RESONANCE:1||coupled Josephson junctions:1||COPPEROXIDE SUPERCONDUCTORS:1||CROSSOVER:1||SIMULATIONS:1||LOWTEMPERATURE:1||CONDUCTORS:1||METALINSULATORTRANSITION:1||SEMICONDUCTOR:1||FIELDEFFECT TRANSISTORS:1||ZEROVOLTAGE STATE:1||constanttemperature interlayer tunneling spectroscopy:1||Josephson supercurrent:1||BIPOLAR SUPERCURRENT:1||Interaction between Josephson and pancake vortices:1||flux jump:1||coaxial heterojunction nanorod:1||Natural Josephson coupling:1||BI2SR2CACU2O8+DELTA:1||VORTEX FLOW:1||TC SUPERCONDUCTORS:1||charge imbalance:1||Andreev diffractometer:1||intercalation:1||surface junction:1||Bi2212:1||tunnelling:1||GRAPHITE:1||GROWTH:1||collective transverse plasma modes:1||GAN:1||Macroscopic quantum tunneling:1||Fluctuation conductivity:1||Abovegap conductance jump:1||Josephson vortex motion:1||Intrinsic Josephson junctions:1||LAYERED SUPERCONDUCTORS:1||BI2SR2CACU2O8+Y:1||INTERFACES:1||BREAKDOWN:1||SYSTEMS:1||Anisotropy ratio:1||Josephson vortex:1||spin relaxation in superconductors:1||bibased single crystals:1||MESOSCOPIC PROXIMITY SUPERCONDUCTOR:1||reentrance of conductance:1||interlayer pair tunneling:1||JOSEPHSON:1||DISORDERED 2DIMENSIONAL SUPERCONDUCTORS:1||INDIUM FILMS:1||excited state:1||REGIME:1||triplet superconductivity:1||FILM:1||SCHOTTKY DIODES:1||peakdiphump structure:1||Kondo effect:1||REENTRANCE:1||Graphene:1||CONTACT:1||BERRYS PHASE:1||2DIMENSIONAL SUPERCONDUCTORS:1||Coulomb diamond:1||magnetic domain:1||spin injection:1||RESONANCE:1||plasma excitation modes:1||FLOW:1||OVERDOPED BI2SR2CACU2O8+DELTA:1||hole doping:1||chemical synthesis:1||phase transitions:1||superconductors:1||VORTEXGLASS SUPERCONDUCTIVITY:1||Kondorelated model:1||RADIATION:1||DOT:1||NANOBELTS:1||Complementarity:1||Closedloop AharonovBohm interferometer:1||pair breaking:1||interlayer phase fluctuation:1||MgB2 thin film:1||CONFINEMENT:1||WALLED CARBON NANOTUBES:1||TRANSITION:9||VORTICES:8||STATE:7||intrinsic Josephson junctions:7||SINGLECRYSTALS:7||JUNCTIONS:5||MODES:5||SUPERCURRENT:5||SUPERCONDUCTOR:5||CONDUCTANCE:5||HIGHTEMPERATURE SUPERCONDUCTORS:5||TRANSPORT:5||PHASE:5||FILMS:4||LOCALIZATION:4||SINGLE DIRAC CONE:4||WIRES:4||MAGNETICFIELD:4||STEPS:3||ELECTRONS:3||proximity effect:3||MODEL:3||ARRAYS:3||INTERFERENCE:3||fluxon dynamics:3||HETEROSTRUCTURES:3||INSULATOR:3||Andreev reflection:3||electronic transport:3||FISKE:3||superconductor:2||ZnO:2||quantum point contact:2||METAL:2||DYNAMICS:2||interlayer Josephson coupling:2||SUPERCONDUCTORS:2||YBA2CU3O7DELTA:2||LAYER:2||DOTS:2||quantum dot:2||Article:2||TRANSISTORS:2||CARBON NANOTUBES:2||GAP:2||MECHANISM:2||LINE:2||GIANT SHAPIRO STEPS:2||LAYERS:2||electron energy loss spectroscopy:2||physical phenomena:2||scanning electron microscopy:2||HGTE QUANTUMWELLS:2||BI2TE3:2||SPECTROSCOPY:2||PNJUNCTIONS:2||spinpolarized tunneling:2||INTRINSIC JOSEPHSONJUNCTIONS:2||FIELDS:2||positive magnetoresistance:2||dilute magnetic semiconductor:2||magnetic field:2||scanning transmission electron microscopy:2||QUANTUM OSCILLATIONS:2||TRANSPORTPROPERTIES:2||surface pair current:2||MAGNETORESISTANCE:2||NANORIBBONS:2||INSTABILITY:2||ANDREEV REFLECTION:2||microwave irradiation:2||vertical graphene josephson junction:2||BI2SE3:2||CONDUCTIVITY:2||highTc superconductors:2||DIMENSIONAL ELECTRONGAS:2||graphene:2||Topological insulators:2||Josephson coupling Fraunhofer interference pattern:2||FERROMAGNET:2||DEPENDENCE:2||DETECTOR:2||COHERENCE:2||INJECTION:2||GRAPHENE:1||JOSEPHSONJUNCTIONS:1||LAYERED SUPERCONDUCTOR:1||mode splitting:1||BEHAVIOR:1||spinpolarized transport:1||SUPERCONDUCTING TRANSITION:1||microwave response:1||PSEUDOGAP:1||phase coherence:1||TRANSITIONS:1||Long Josephson junction:1||Charge detection:1||collective resonance modes:1||plasma oscillation modes:1||Superconducting proximity effect:1||Iron pnictide superconductor:1||McMillanRowell oscillations:1||ferromagnetic microstructure:1||superradiant state:1||VOLTAGE:1||branch splitting:1||TENSOR:1||INTERCALATION:1||insitu fabrication:1||NDGAO3:1||DISORDERED METALS:1||GAUGE GLASS:1||LOWTEMPERATURE TRANSPORT:1||spontaneous spin polarization model:1||BIAS:1||emission of electromagnetic waves:1||YBA2CU3O7/PRBA2CU3O7 SUPERLATTICES:1||BOHM:1||SHAPIRO STEPS:1||superconductor/ferromagnet interface:1||OXIDE:1||ANDREEVREFLECTION:1||SinFeAsO single crystal:1||COLLECTIVE MOTION:1||ANGULARDEPENDENCE:1||SUPERCONDUCTIVITY:1||BILAYER GRAPHENE:1||PHOTOLUMINESCENT PROPERTIES:1||SUPERCONDUCTING WEAK LINKS:1||intrinsic Josephson junctions geometrical resonance:1||intrinsic Josephson junction:1||MESOSCOPIC SPINVALVE:1||Bi2212 single crystals:1||intrinsic junctions:1||ANDREEV REFLECTIONS:1||normalmetal/superconductor interface:1||IBI2SR2CACU2OY:1||THERMAL FLUCTUATIONS:1||MIXED STATE:1||BI2.15SR1.85CACU2O8+DELTA:1||intrinsic Josephson effects:1||CACUO:1||QUANTUM POINT CONTACTS:1||resonant tunneling state:1||coherence length:1||NANOWIRE:1||GATES:1||Phase line:1||Thermal activation:1||QUANTUMDOT:1||superconducting proximity effect:1||Andreev interferometer:1||WIRE:1||Josephsonvortexflow branches:1||Bi2212 cuprates:1||LATTICE:1||demannetization effect:1||SUPERCONDUCTING MIRRORS:1||GAS:1||VALLEY TRANSPORT:1||ELECTRODES:1||DEPENDENT TRANSPORT:1||BORNOPPENHEIMER APPROXIMATION:1||collective plasma oscillations:1||fluxon resonance steps:1||STACKS:1||COLLECTIVE DYNAMICS:1||PAIRING SYMMETRY:1||MUON SPIN ROTATION:1||DIMENSIONAL CROSSOVER:1||Bi2Sr2CaCu2Oy highTc superconductors:1||heterojunctions:1||nanostructures:1||surfaces and interfaces:1||QUANTUM TRANSPORT:1||MICROJUNCTIONS:1||RESONATORS:1||STATES:1||FIELD:1||FLUCTUATIONS:1||SCATTERING:1||mode splitting of Josephson vortexflow branches:1||2D superconductivity:1||TRANSISTOR:1||ENERGYGAP:1||SUPERLATTICES:1||IRONBASED SUPERCONDUCTORS:1||PHASEDEPENDENT RESISTANCE:1||QUANTUM PHASETRANSITIONS:1||ELECTRICFIELD:1||HIGH MAGNETICFIELDS:1||NANOWIRE HETEROSTRUCTURES:1||ZNO:1||pair breaking.:1||SUPERCONDUCTING PB:1||domain formation:1||FORCE MICROSCOPY:1||RELAXATION:1||PLASMA RESONANCE:1||coupled Josephson junctions:1||COPPEROXIDE SUPERCONDUCTORS:1||CROSSOVER:1||SIMULATIONS:1||LOWTEMPERATURE:1||CONDUCTORS:1||METALINSULATORTRANSITION:1||SEMICONDUCTOR:1||FIELDEFFECT TRANSISTORS:1||ZEROVOLTAGE STATE:1||constanttemperature interlayer tunneling spectroscopy:1||Josephson supercurrent:1||BIPOLAR SUPERCURRENT:1||Interaction between Josephson and pancake vortices:1||flux jump:1||coaxial heterojunction nanorod:1||Natural Josephson coupling:1||BI2SR2CACU2O8+DELTA:1||VORTEX FLOW:1||TC SUPERCONDUCTORS:1||charge imbalance:1||Andreev diffractometer:1||intercalation:1||surface junction:1||Bi2212:1||tunnelling:1||GRAPHITE:1||GROWTH:1||collective transverse plasma modes:1||GAN:1||Macroscopic quantum tunneling:1||Fluctuation conductivity:1||Abovegap conductance jump:1||Josephson vortex motion:1||Intrinsic Josephson junctions:1||LAYERED SUPERCONDUCTORS:1||BI2SR2CACU2O8+Y:1||INTERFACES:1||BREAKDOWN:1||SYSTEMS:1||Anisotropy ratio:1||Josephson vortex:1||spin relaxation in superconductors:1||bibased single crystals:1||MESOSCOPIC PROXIMITY SUPERCONDUCTOR:1||reentrance of conductance:1||interlayer pair tunneling:1||JOSEPHSON:1||DISORDERED 2DIMENSIONAL SUPERCONDUCTORS:1||INDIUM FILMS:1||excited state:1||REGIME:1||triplet superconductivity:1||FILM:1||SCHOTTKY DIODES:1||peakdiphump structure:1||Kondo effect:1||REENTRANCE:1||Graphene:1||CONTACT:1||BERRYS PHASE:1||2DIMENSIONAL SUPERCONDUCTORS:1||Coulomb diamond:1||magnetic domain:1||spin injection:1||RESONANCE:1||plasma excitation modes:1||FLOW:1||OVERDOPED BI2SR2CACU2O8+DELTA:1||hole doping:1||chemical synthesis:1||phase transitions:1||superconductors:1||VORTEXGLASS SUPERCONDUCTIVITY:1||Kondorelated model:1||RADIATION:1||DOT:1||NANOBELTS:1||Complementarity:1||Closedloop AharonovBohm interferometer:1||pair breaking:1||interlayer phase fluctuation:1||MgB2 thin film:1||CONFINEMENT:1||WALLED CARBON NANOTUBES:1||TRANSITION:9||VORTICES:8||STATE:7||intrinsic Josephson junctions:7||SINGLECRYSTALS:7||JUNCTIONS:5||MODES:5||SUPERCURRENT:5||SUPERCONDUCTOR:5||CONDUCTANCE:5||HIGHTEMPERATURE SUPERCONDUCTORS:5||TRANSPORT:5||PHASE:5||FILMS:4||LOCALIZATION:4||SINGLE DIRAC CONE:4||WIRES:4||MAGNETICFIELD:4||STEPS:3||ELECTRONS:3||proximity effect:3||MODEL:3||ARRAYS:3||INTERFERENCE:3||fluxon dynamics:3||HETEROSTRUCTURES:3||INSULATOR:3||Andreev reflection:3||electronic transport:3||FISKE:3||superconductor:2||ZnO:2||quantum point contact:2||METAL:2||DYNAMICS:2||interlayer Josephson coupling:2||SUPERCONDUCTORS:2||YBA2CU3O7DELTA:2||LAYER:2||DOTS:2||quantum dot:2||Article:2||TRANSISTORS:2||CARBON NANOTUBES:2||GAP:2||MECHANISM:2||LINE:2||GIANT SHAPIRO STEPS:2||LAYERS:2||electron energy loss spectroscopy:2||physical phenomena:2||scanning electron microscopy:2||HGTE QUANTUMWELLS:2||BI2TE3:2||SPECTROSCOPY:2||PNJUNCTIONS:2||spinpolarized tunneling:2||INTRINSIC JOSEPHSONJUNCTIONS:2||FIELDS:2||positive magnetoresistance:2||dilute magnetic semiconductor:2||magnetic field:2||scanning transmission electron microscopy:2||QUANTUM OSCILLATIONS:2||TRANSPORTPROPERTIES:2||surface pair current:2||MAGNETORESISTANCE:2||NANORIBBONS:2||INSTABILITY:2||ANDREEV REFLECTION:2||microwave irradiation:2||vertical graphene josephson junction:2||BI2SE3:2||CONDUCTIVITY:2||highTc superconductors:2||DIMENSIONAL ELECTRONGAS:2||graphene:2||Topological insulators:2||Josephson coupling Fraunhofer interference pattern:2||FERROMAGNET:2||DEPENDENCE:2||DETECTOR:2||COHERENCE:2||INJECTION:2||GRAPHENE:1||JOSEPHSONJUNCTIONS:1||LAYERED SUPERCONDUCTOR:1||mode splitting:1||BEHAVIOR:1||spinpolarized transport:1||SUPERCONDUCTING TRANSITION:1||microwave response:1||PSEUDOGAP:1||phase coherence:1||TRANSITIONS:1||Long Josephson junction:1||Charge detection:1||collective resonance modes:1||plasma oscillation modes:1||Superconducting proximity effect:1||Iron pnictide superconductor:1||McMillanRowell oscillations:1||ferromagnetic microstructure:1||superradiant state:1||VOLTAGE:1||branch splitting:1||TENSOR:1||INTERCALATION:1||insitu fabrication:1||NDGAO3:1||DISORDERED METALS:1||GAUGE GLASS:1||LOWTEMPERATURE TRANSPORT:1||spontaneous spin polarization model:1||BIAS:1||emission of electromagnetic waves:1||YBA2CU3O7/PRBA2CU3O7 SUPERLATTICES:1||BOHM:1||SHAPIRO STEPS:1||superconductor/ferromagnet interface:1||OXIDE:1||ANDREEVREFLECTION:1||SinFeAsO single crystal:1||COLLECTIVE MOTION:1||ANGULARDEPENDENCE:1||SUPERCONDUCTIVITY:1||BILAYER GRAPHENE:1||PHOTOLUMINESCENT PROPERTIES:1||SUPERCONDUCTING WEAK LINKS:1||intrinsic Josephson junctions geometrical resonance:1||intrinsic Josephson junction:1||MESOSCOPIC SPINVALVE:1||Bi2212 single crystals:1||intrinsic junctions:1||ANDREEV REFLECTIONS:1||normalmetal/superconductor interface:1||IBI2SR2CACU2OY:1||THERMAL FLUCTUATIONS:1||MIXED STATE:1||BI2.15SR1.85CACU2O8+DELTA:1||intrinsic Josephson effects:1||CACUO:1||QUANTUM POINT CONTACTS:1||resonant tunneling state:1||coherence length:1||NANOWIRE:1||GATES:1||Phase line:1||Thermal activation:1||QUANTUMDOT:1||superconducting proximity effect:1||Andreev interferometer:1||WIRE:1||Josephsonvortexflow branches:1||Bi2212 cuprates:1||LATTICE:1||demannetization effect:1||SUPERCONDUCTING MIRRORS:1||GAS:1||VALLEY TRANSPORT:1||ELECTRODES:1||DEPENDENT TRANSPORT:1||BORNOPPENHEIMER APPROXIMATION:1||collective plasma oscillations:1||fluxon resonance steps:1||STACKS:1||COLLECTIVE DYNAMICS:1||PAIRING SYMMETRY:1||MUON SPIN ROTATION:1||DIMENSIONAL CROSSOVER:1||Bi2Sr2CaCu2Oy highTc superconductors:1||heterojunctions:1||nanostructures:1||surfaces and interfaces:1||QUANTUM TRANSPORT:1||MICROJUNCTIONS:1||RESONATORS:1||STATES:1||FIELD:1||FLUCTUATIONS:1||SCATTERING:1||mode splitting of Josephson vortexflow branches:1||2D superconductivity:1||TRANSISTOR:1||ENERGYGAP:1||SUPERLATTICES:1||IRONBASED SUPERCONDUCTORS:1||PHASEDEPENDENT RESISTANCE:1||QUANTUM PHASETRANSITIONS:1||ELECTRICFIELD:1||HIGH MAGNETICFIELDS:1||NANOWIRE HETEROSTRUCTURES:1||ZNO:1||pair breaking.:1||SUPERCONDUCTING PB:1||domain formation:1||FORCE MICROSCOPY:1||RELAXATION:1||PLASMA RESONANCE:1||coupled Josephson junctions:1||COPPEROXIDE SUPERCONDUCTORS:1||CROSSOVER:1||SIMULATIONS:1||LOWTEMPERATURE:1||CONDUCTORS:1||METALINSULATORTRANSITION:1||SEMICONDUCTOR:1||FIELDEFFECT TRANSISTORS:1||ZEROVOLTAGE STATE:1||constanttemperature interlayer tunneling spectroscopy:1||Josephson supercurrent:1||BIPOLAR SUPERCURRENT:1||Interaction between Josephson and pancake vortices:1||flux jump:1||coaxial heterojunction nanorod:1||Natural Josephson coupling:1||BI2SR2CACU2O8+DELTA:1||VORTEX FLOW:1||TC SUPERCONDUCTORS:1||charge imbalance:1||Andreev diffractometer:1||intercalation:1||surface junction:1||Bi2212:1||tunnelling:1||GRAPHITE:1||GROWTH:1||collective transverse plasma modes:1||GAN:1||Macroscopic quantum tunneling:1||Fluctuation conductivity:1||Abovegap conductance jump:1||Josephson vortex motion:1||Intrinsic Josephson junctions:1||LAYERED SUPERCONDUCTORS:1||BI2SR2CACU2O8+Y:1||INTERFACES:1||BREAKDOWN:1||SYSTEMS:1||Anisotropy ratio:1||Josephson vortex:1||spin relaxation in superconductors:1||bibased single crystals:1||MESOSCOPIC PROXIMITY SUPERCONDUCTOR:1||reentrance of conductance:1||interlayer pair tunneling:1||JOSEPHSON:1||DISORDERED 2DIMENSIONAL SUPERCONDUCTORS:1||INDIUM FILMS:1||excited state:1||REGIME:1||triplet superconductivity:1||FILM:1||SCHOTTKY DIODES:1||peakdiphump structure:1||Kondo effect:1||REENTRANCE:1||Graphene:1||CONTACT:1||BERRYS PHASE:1||2DIMENSIONAL SUPERCONDUCTORS:1||Coulomb diamond:1||magnetic domain:1||spin injection:1||RESONANCE:1||plasma excitation modes:1||FLOW:1||OVERDOPED BI2SR2CACU2O8+DELTA:1||hole doping:1||chemical synthesis:1||phase transitions:1||superconductors:1||VORTEXGLASS SUPERCONDUCTIVITY:1||Kondorelated model:1||RADIATION:1||DOT:1||NANOBELTS:1||Complementarity:1||Closedloop AharonovBohm interferometer:1||pair breaking:1||interlayer phase fluctuation:1||MgB2 thin film:1||CONFINEMENT:1||WALLED CARBON NANOTUBES:1||TRANSITION:9||VORTICES:8||STATE:7||intrinsic Josephson junctions:7||SINGLECRYSTALS:7||JUNCTIONS:5||MODES:5||SUPERCURRENT:5||SUPERCONDUCTOR:5||CONDUCTANCE:5||HIGHTEMPERATURE SUPERCONDUCTORS:5||TRANSPORT:5||PHASE:5||FILMS:4||LOCALIZATION:4||SINGLE DIRAC CONE:4||WIRES:4||MAGNETICFIELD:4||STEPS:3||ELECTRONS:3||proximity effect:3||MODEL:3||ARRAYS:3||INTERFERENCE:3||fluxon dynamics:3||HETEROSTRUCTURES:3||INSULATOR:3||Andreev reflection:3||electronic transport:3||FISKE:3||superconductor:2||ZnO:2||quantum point contact:2||METAL:2||DYNAMICS:2||interlayer Josephson coupling:2||SUPERCONDUCTORS:2||YBA2CU3O7DELTA:2||LAYER:2||DOTS:2||quantum dot:2||Article:2||TRANSISTORS:2||CARBON NANOTUBES:2||GAP:2||MECHANISM:2||LINE:2||GIANT SHAPIRO STEPS:2||LAYERS:2||electron energy loss spectroscopy:2||physical phenomena:2||scanning electron microscopy:2||HGTE QUANTUMWELLS:2||BI2TE3:2||SPECTROSCOPY:2||PNJUNCTIONS:2||spinpolarized tunneling:2||INTRINSIC JOSEPHSONJUNCTIONS:2||FIELDS:2||positive magnetoresistance:2||dilute magnetic semiconductor:2||magnetic field:2||scanning transmission electron microscopy:2||QUANTUM OSCILLATIONS:2||TRANSPORTPROPERTIES:2||surface pair current:2||MAGNETORESISTANCE:2||NANORIBBONS:2||INSTABILITY:2||ANDREEV REFLECTION:2||microwave irradiation:2||vertical graphene josephson junction:2||BI2SE3:2||CONDUCTIVITY:2||highTc superconductors:2||DIMENSIONAL ELECTRONGAS:2||graphene:2||Topological insulators:2||Josephson coupling Fraunhofer interference pattern:2||FERROMAGNET:2||DEPENDENCE:2||DETECTOR:2||COHERENCE:2||INJECTION:2||GRAPHENE:1||JOSEPHSONJUNCTIONS:1||LAYERED SUPERCONDUCTOR:1||mode splitting:1||BEHAVIOR:1||spinpolarized transport:1||SUPERCONDUCTING TRANSITION:1||microwave response:1||PSEUDOGAP:1||phase coherence:1||TRANSITIONS:1||Long Josephson junction:1||Charge detection:1||collective resonance modes:1||plasma oscillation modes:1||Superconducting proximity effect:1||Iron pnictide superconductor:1||McMillanRowell oscillations:1||ferromagnetic microstructure:1||superradiant state:1||VOLTAGE:1||branch splitting:1||TENSOR:1||INTERCALATION:1||insitu fabrication:1||NDGAO3:1||DISORDERED METALS:1||GAUGE GLASS:1||LOWTEMPERATURE TRANSPORT:1||spontaneous spin polarization model:1||BIAS:1||emission of electromagnetic waves:1||YBA2CU3O7/PRBA2CU3O7 SUPERLATTICES:1||BOHM:1||SHAPIRO STEPS:1||superconductor/ferromagnet interface:1||OXIDE:1||ANDREEVREFLECTION:1||SinFeAsO single crystal:1||COLLECTIVE MOTION:1||ANGULARDEPENDENCE:1||SUPERCONDUCTIVITY:1||BILAYER GRAPHENE:1||PHOTOLUMINESCENT PROPERTIES:1||SUPERCONDUCTING WEAK LINKS:1||intrinsic Josephson junctions geometrical resonance:1||intrinsic Josephson junction:1||MESOSCOPIC SPINVALVE:1||Bi2212 single crystals:1||intrinsic junctions:1||ANDREEV REFLECTIONS:1||normalmetal/superconductor interface:1||IBI2SR2CACU2OY:1||THERMAL FLUCTUATIONS:1||MIXED STATE:1||BI2.15SR1.85CACU2O8+DELTA:1||intrinsic Josephson effects:1||CACUO:1||QUANTUM POINT CONTACTS:1||resonant tunneling state:1||coherence length:1||NANOWIRE:1||GATES:1||Phase line:1||Thermal activation:1||QUANTUMDOT:1||superconducting proximity effect:1||Andreev interferometer:1||WIRE:1||Josephsonvortexflow branches:1||Bi2212 cuprates:1||LATTICE:1||demannetization effect:1||SUPERCONDUCTING MIRRORS:1||GAS:1||VALLEY TRANSPORT:1||ELECTRODES:1||DEPENDENT TRANSPORT:1||BORNOPPENHEIMER APPROXIMATION:1||collective plasma oscillations:1||fluxon resonance steps:1||STACKS:1||COLLECTIVE DYNAMICS:1||PAIRING SYMMETRY:1||MUON SPIN ROTATION:1||DIMENSIONAL CROSSOVER:1||Bi2Sr2CaCu2Oy highTc superconductors:1||heterojunctions:1||nanostructures:1||surfaces and interfaces:1||QUANTUM TRANSPORT:1||MICROJUNCTIONS:1||RESONATORS:1||STATES:1||FIELD:1||FLUCTUATIONS:1||SCATTERING:1||mode splitting of Josephson vortexflow branches:1||2D superconductivity:1||TRANSISTOR:1||ENERGYGAP:1||SUPERLATTICES:1||IRONBASED SUPERCONDUCTORS:1||PHASEDEPENDENT RESISTANCE:1||QUANTUM PHASETRANSITIONS:1||ELECTRICFIELD:1||HIGH MAGNETICFIELDS:1||NANOWIRE HETEROSTRUCTURES:1||ZNO:1||pair breaking.:1||SUPERCONDUCTING PB:1||domain formation:1||FORCE MICROSCOPY:1||RELAXATION:1||PLASMA RESONANCE:1||coupled Josephson junctions:1||COPPEROXIDE SUPERCONDUCTORS:1||CROSSOVER:1||SIMULATIONS:1||LOWTEMPERATURE:1||CONDUCTORS:1||METALINSULATORTRANSITION:1||SEMICONDUCTOR:1||FIELDEFFECT TRANSISTORS:1||ZEROVOLTAGE STATE:1||constanttemperature interlayer tunneling spectroscopy:1||Josephson supercurrent:1||BIPOLAR SUPERCURRENT:1||Interaction between Josephson and pancake vortices:1||flux jump:1||coaxial heterojunction nanorod:1||Natural Josephson coupling:1||BI2SR2CACU2O8+DELTA:1||VORTEX FLOW:1||TC SUPERCONDUCTORS:1||charge imbalance:1||Andreev diffractometer:1||intercalation:1||surface junction:1||Bi2212:1||tunnelling:1||GRAPHITE:1||GROWTH:1||collective transverse plasma modes:1||GAN:1||Macroscopic quantum tunneling:1||Fluctuation conductivity:1||Abovegap conductance jump:1||Josephson vortex motion:1||Intrinsic Josephson junctions:1||LAYERED SUPERCONDUCTORS:1||BI2SR2CACU2O8+Y:1||INTERFACES:1||BREAKDOWN:1||SYSTEMS:1||Anisotropy ratio:1||Josephson vortex:1||spin relaxation in superconductors:1||bibased single crystals:1||MESOSCOPIC PROXIMITY SUPERCONDUCTOR:1||reentrance of conductance:1||interlayer pair tunneling:1||JOSEPHSON:1||DISORDERED 2DIMENSIONAL SUPERCONDUCTORS:1||INDIUM FILMS:1||excited state:1||REGIME:1||triplet superconductivity:1||FILM:1||SCHOTTKY DIODES:1||peakdiphump structure:1||Kondo effect:1||REENTRANCE:1||Graphene:1||CONTACT:1||BERRYS PHASE:1||2DIMENSIONAL SUPERCONDUCTORS:1||Coulomb diamond:1||magnetic domain:1||spin injection:1||RESONANCE:1||plasma excitation modes:1||FLOW:1||OVERDOPED BI2SR2CACU2O8+DELTA:1||hole doping:1||chemical synthesis:1||phase transitions:1||superconductors:1||VORTEXGLASS SUPERCONDUCTIVITY:1||Kondorelated model:1||RADIATION:1||DOT:1||NANOBELTS:1||Complementarity:1||Closedloop AharonovBohm interferometer:1||pair breaking:1||interlayer phase fluctuation:1||MgB2 thin film:1||CONFINEMENT:1||WALLED CARBON NANOTUBES:1||TRANSITION:9||VORTICES:8||STATE:7||intrinsic Josephson junctions:7||SINGLECRYSTALS:7||JUNCTIONS:5||MODES:5||SUPERCURRENT:5||SUPERCONDUCTOR:5||CONDUCTANCE:5||HIGHTEMPERATURE SUPERCONDUCTORS:5||TRANSPORT:5||PHASE:5||FILMS:4||LOCALIZATION:4||SINGLE DIRAC CONE:4||WIRES:4||MAGNETICFIELD:4||STEPS:3||ELECTRONS:3||proximity effect:3||MODEL:3||ARRAYS:3||INTERFERENCE:3||fluxon dynamics:3||HETEROSTRUCTURES:3||INSULATOR:3||Andreev reflection:3||electronic transport:3||FISKE:3||superconductor:2||ZnO:2||quantum point contact:2||METAL:2||DYNAMICS:2||interlayer Josephson coupling:2||SUPERCONDUCTORS:2||YBA2CU3O7DELTA:2||LAYER:2||DOTS:2||quantum dot:2||Article:2||TRANSISTORS:2||CARBON NANOTUBES:2||GAP:2||MECHANISM:2||LINE:2||GIANT SHAPIRO STEPS:2||LAYERS:2||electron energy loss spectroscopy:2||physical phenomena:2||scanning electron microscopy:2||HGTE QUANTUMWELLS:2||BI2TE3:2||SPECTROSCOPY:2||PNJUNCTIONS:2||spinpolarized tunneling:2||INTRINSIC JOSEPHSONJUNCTIONS:2||FIELDS:2||positive magnetoresistance:2||dilute magnetic semiconductor:2||magnetic field:2||scanning transmission electron microscopy:2||QUANTUM OSCILLATIONS:2||TRANSPORTPROPERTIES:2||surface pair current:2||MAGNETORESISTANCE:2||NANORIBBONS:2||INSTABILITY:2||ANDREEV REFLECTION:2||microwave irradiation:2||vertical graphene josephson junction:2||BI2SE3:2||CONDUCTIVITY:2||highTc superconductors:2||DIMENSIONAL ELECTRONGAS:2||graphene:2||Topological insulators:2||Josephson coupling Fraunhofer interference pattern:2||FERROMAGNET:2||DEPENDENCE:2||DETECTOR:2||COHERENCE:2||INJECTION:2||GRAPHENE:1||JOSEPHSONJUNCTIONS:1||LAYERED SUPERCONDUCTOR:1||mode splitting:1||BEHAVIOR:1||spinpolarized transport:1||SUPERCONDUCTING TRANSITION:1||microwave response:1||PSEUDOGAP:1||phase coherence:1||TRANSITIONS:1||Long Josephson junction:1||Charge detection:1||collective resonance modes:1||plasma oscillation modes:1||Superconducting proximity effect:1||Iron pnictide superconductor:1||McMillanRowell oscillations:1||ferromagnetic microstructure:1||superradiant state:1||VOLTAGE:1||branch splitting:1||TENSOR:1||INTERCALATION:1||insitu fabrication:1||NDGAO3:1||DISORDERED METALS:1||GAUGE GLASS:1||LOWTEMPERATURE TRANSPORT:1||spontaneous spin polarization model:1||BIAS:1||emission of electromagnetic waves:1||YBA2CU3O7/PRBA2CU3O7 SUPERLATTICES:1||BOHM:1||SHAPIRO STEPS:1||superconductor/ferromagnet interface:1||OXIDE:1||ANDREEVREFLECTION:1||SinFeAsO single crystal:1||COLLECTIVE MOTION:1||ANGULARDEPENDENCE:1||SUPERCONDUCTIVITY:1||BILAYER GRAPHENE:1||PHOTOLUMINESCENT PROPERTIES:1||SUPERCONDUCTING WEAK LINKS:1||intrinsic Josephson junctions geometrical resonance:1||intrinsic Josephson junction:1||MESOSCOPIC SPINVALVE:1||Bi2212 single crystals:1||intrinsic junctions:1||ANDREEV REFLECTIONS:1||normalmetal/superconductor interface:1||IBI2SR2CACU2OY:1||THERMAL FLUCTUATIONS:1||MIXED STATE:1||BI2.15SR1.85CACU2O8+DELTA:1||intrinsic Josephson effects:1||CACUO:1||QUANTUM POINT CONTACTS:1||resonant tunneling state:1||coherence length:1||NANOWIRE:1||GATES:1||Phase line:1||Thermal activation:1||QUANTUMDOT:1||superconducting proximity effect:1||Andreev interferometer:1||WIRE:1||Josephsonvortexflow branches:1||Bi2212 cuprates:1||LATTICE:1||demannetization effect:1||SUPERCONDUCTING MIRRORS:1||GAS:1||VALLEY TRANSPORT:1||ELECTRODES:1||DEPENDENT TRANSPORT:1||BORNOPPENHEIMER APPROXIMATION:1||collective plasma oscillations:1||fluxon resonance steps:1||STACKS:1||COLLECTIVE DYNAMICS:1||PAIRING SYMMETRY:1||MUON SPIN ROTATION:1||DIMENSIONAL CROSSOVER:1||Bi2Sr2CaCu2Oy highTc superconductors:1||heterojunctions:1||nanostructures:1||surfaces and interfaces:1||QUANTUM TRANSPORT:1||MICROJUNCTIONS:1||RESONATORS:1||STATES:1||FIELD:1||FLUCTUATIONS:1||SCATTERING:1||mode splitting of Josephson vortexflow branches:1||2D superconductivity:1||TRANSISTOR:1||ENERGYGAP:1||SUPERLATTICES:1||IRONBASED SUPERCONDUCTORS:1||PHASEDEPENDENT RESISTANCE:1||QUANTUM PHASETRANSITIONS:1||ELECTRICFIELD:1||HIGH MAGNETICFIELDS:1||NANOWIRE HETEROSTRUCTURES:1||ZNO:1||pair breaking.:1||SUPERCONDUCTING PB:1||domain formation:1||FORCE MICROSCOPY:1||RELAXATION:1||PLASMA RESONANCE:1||coupled Josephson junctions:1||COPPEROXIDE SUPERCONDUCTORS:1||CROSSOVER:1||SIMULATIONS:1||LOWTEMPERATURE:1||CONDUCTORS:1||METALINSULATORTRANSITION:1||SEMICONDUCTOR:1||FIELDEFFECT TRANSISTORS:1||ZEROVOLTAGE STATE:1||constanttemperature interlayer tunneling spectroscopy:1||Josephson supercurrent:1||BIPOLAR SUPERCURRENT:1||Interaction between Josephson and pancake vortices:1||flux jump:1||coaxial heterojunction nanorod:1||Natural Josephson coupling:1||BI2SR2CACU2O8+DELTA:1||VORTEX FLOW:1||TC SUPERCONDUCTORS:1||charge imbalance:1||Andreev diffractometer:1||intercalation:1||surface junction:1||Bi2212:1||tunnelling:1||GRAPHITE:1||GROWTH:1||collective transverse plasma modes:1||GAN:1||Macroscopic quantum tunneling:1||Fluctuation conductivity:1||Abovegap conductance jump:1||Josephson vortex motion:1||Intrinsic Josephson junctions:1||LAYERED SUPERCONDUCTORS:1||BI2SR2CACU2O8+Y:1||INTERFACES:1||BREAKDOWN:1||SYSTEMS:1||Anisotropy ratio:1||Josephson vortex:1||spin relaxation in superconductors:1||bibased single crystals:1||MESOSCOPIC PROXIMITY SUPERCONDUCTOR:1||reentrance of conductance:1||interlayer pair tunneling:1||JOSEPHSON:1||DISORDERED 2DIMENSIONAL SUPERCONDUCTORS:1||INDIUM FILMS:1||excited state:1||REGIME:1||triplet superconductivity:1||FILM:1||SCHOTTKY DIODES:1||peakdiphump structure:1||Kondo effect:1||REENTRANCE:1||Graphene:1||CONTACT:1||BERRYS PHASE:1||2DIMENSIONAL SUPERCONDUCTORS:1||Coulomb diamond:1||magnetic domain:1||spin injection:1||RESONANCE:1||plasma excitation modes:1||FLOW:1||OVERDOPED BI2SR2CACU2O8+DELTA:1||hole doping:1||chemical synthesis:1||phase transitions:1||superconductors:1||VORTEXGLASS SUPERCONDUCTIVITY:1||Kondorelated model:1||RADIATION:1||DOT:1||NANOBELTS:1||Complementarity:1||Closedloop AharonovBohm interferometer:1||pair breaking:1||interlayer phase fluctuation:1||MgB2 thin film:1||CONFINEMENT:1||WALLED CARBON NANOTUBES:1||TRANSITION:9||VORTICES:8||STATE:7||intrinsic Josephson junctions:7||SINGLECRYSTALS:7||JUNCTIONS:5||MODES:5||SUPERCURRENT:5||SUPERCONDUCTOR:5||CONDUCTANCE:5||HIGHTEMPERATURE SUPERCONDUCTORS:5||TRANSPORT:5||PHASE:5||FILMS:4||LOCALIZATION:4||SINGLE DIRAC CONE:4||WIRES:4||MAGNETICFIELD:4||STEPS:3||ELECTRONS:3||proximity effect:3||MODEL:3||ARRAYS:3||INTERFERENCE:3||fluxon dynamics:3||HETEROSTRUCTURES:3||INSULATOR:3||Andreev reflection:3||electronic transport:3||FISKE:3||superconductor:2||ZnO:2||quantum point contact:2||METAL:2||DYNAMICS:2||interlayer Josephson coupling:2||SUPERCONDUCTORS:2||YBA2CU3O7DELTA:2||LAYER:2||DOTS:2||quantum dot:2||Article:2||TRANSISTORS:2||CARBON NANOTUBES:2||GAP:2||MECHANISM:2||LINE:2||GIANT SHAPIRO STEPS:2||LAYERS:2||electron energy loss spectroscopy:2||physical phenomena:2||scanning electron microscopy:2||HGTE QUANTUMWELLS:2||BI2TE3:2||SPECTROSCOPY:2||PNJUNCTIONS:2||spinpolarized tunneling:2||INTRINSIC JOSEPHSONJUNCTIONS:2||FIELDS:2||positive magnetoresistance:2||dilute magnetic semiconductor:2||magnetic field:2||scanning transmission electron microscopy:2||QUANTUM OSCILLATIONS:2||TRANSPORTPROPERTIES:2||surface pair current:2||MAGNETORESISTANCE:2||NANORIBBONS:2||INSTABILITY:2||ANDREEV REFLECTION:2||microwave irradiation:2||vertical graphene josephson junction:2||BI2SE3:2||CONDUCTIVITY:2||highTc superconductors:2||DIMENSIONAL ELECTRONGAS:2||graphene:2||Topological insulators:2||Josephson coupling Fraunhofer interference pattern:2||FERROMAGNET:2||DEPENDENCE:2||DETECTOR:2||COHERENCE:2||INJECTION:2||GRAPHENE:1||JOSEPHSONJUNCTIONS:1||LAYERED SUPERCONDUCTOR:1||mode splitting:1||BEHAVIOR:1||spinpolarized transport:1||SUPERCONDUCTING TRANSITION:1||microwave response:1||PSEUDOGAP:1||phase coherence:1||TRANSITIONS:1||Long Josephson junction:1||Charge detection:1||collective resonance modes:1||plasma oscillation modes:1||Superconducting proximity effect:1||Iron pnictide superconductor:1||McMillanRowell oscillations:1||ferromagnetic microstructure:1||superradiant state:1||VOLTAGE:1||branch splitting:1||TENSOR:1||INTERCALATION:1||insitu fabrication:1||NDGAO3:1||DISORDERED METALS:1||GAUGE GLASS:1||LOWTEMPERATURE TRANSPORT:1||spontaneous spin polarization model:1||BIAS:1||emission of electromagnetic waves:1||YBA2CU3O7/PRBA2CU3O7 SUPERLATTICES:1||BOHM:1||SHAPIRO STEPS:1||superconductor/ferromagnet interface:1||OXIDE:1||ANDREEVREFLECTION:1||SinFeAsO single crystal:1||COLLECTIVE MOTION:1||ANGULARDEPENDENCE:1||SUPERCONDUCTIVITY:1||BILAYER GRAPHENE:1||PHOTOLUMINESCENT PROPERTIES:1||SUPERCONDUCTING WEAK LINKS:1||intrinsic Josephson junctions geometrical resonance:1||intrinsic Josephson junction:1||MESOSCOPIC SPINVALVE:1||Bi2212 single crystals:1||intrinsic junctions:1||ANDREEV REFLECTIONS:1||normalmetal/superconductor interface:1||IBI2SR2CACU2OY:1||THERMAL FLUCTUATIONS:1||MIXED STATE:1||BI2.15SR1.85CACU2O8+DELTA:1||intrinsic Josephson effects:1||CACUO:1||QUANTUM POINT CONTACTS:1||resonant tunneling state:1||coherence length:1||NANOWIRE:1||GATES:1||Phase line:1||Thermal activation:1||QUANTUMDOT:1||superconducting proximity effect:1||Andreev interferometer:1||WIRE:1||Josephsonvortexflow branches:1||Bi2212 cuprates:1||LATTICE:1||demannetization effect:1||SUPERCONDUCTING MIRRORS:1||GAS:1||VALLEY TRANSPORT:1||ELECTRODES:1||DEPENDENT TRANSPORT:1||BORNOPPENHEIMER APPROXIMATION:1||collective plasma oscillations:1||fluxon resonance steps:1||STACKS:1||COLLECTIVE DYNAMICS:1||PAIRING SYMMETRY:1||MUON SPIN ROTATION:1||DIMENSIONAL CROSSOVER:1||Bi2Sr2CaCu2Oy highTc superconductors:1||heterojunctions:1||nanostructures:1||surfaces and interfaces:1||QUANTUM TRANSPORT:1||MICROJUNCTIONS:1||RESONATORS:1||STATES:1||FIELD:1||FLUCTUATIONS:1||SCATTERING:1||mode splitting of Josephson vortexflow branches:1||2D superconductivity:1||TRANSISTOR:1||ENERGYGAP:1||SUPERLATTICES:1||IRONBASED SUPERCONDUCTORS:1||PHASEDEPENDENT RESISTANCE:1||QUANTUM PHASETRANSITIONS:1||ELECTRICFIELD:1||HIGH MAGNETICFIELDS:1||NANOWIRE HETEROSTRUCTURES:1||ZNO:1||pair breaking.:1||SUPERCONDUCTING PB:1||domain formation:1||FORCE MICROSCOPY:1||RELAXATION:1||PLASMA RESONANCE:1||coupled Josephson junctions:1||COPPEROXIDE SUPERCONDUCTORS:1||CROSSOVER:1||SIMULATIONS:1||LOWTEMPERATURE:1||CONDUCTORS:1||METALINSULATORTRANSITION:1||SEMICONDUCTOR:1||FIELDEFFECT TRANSISTORS:1||ZEROVOLTAGE STATE:1||constanttemperature interlayer tunneling spectroscopy:1||Josephson supercurrent:1||BIPOLAR SUPERCURRENT:1||Interaction between Josephson and pancake vortices:1||flux jump:1||coaxial heterojunction nanorod:1||Natural Josephson coupling:1||BI2SR2CACU2O8+DELTA:1||VORTEX FLOW:1||TC SUPERCONDUCTORS:1||charge imbalance:1||Andreev diffractometer:1||intercalation:1||surface junction:1||Bi2212:1||tunnelling:1||GRAPHITE:1||GROWTH:1||collective transverse plasma modes:1||GAN:1||Macroscopic quantum tunneling:1||Fluctuation conductivity:1||Abovegap conductance jump:1||Josephson vortex motion:1||Intrinsic Josephson junctions:1||LAYERED SUPERCONDUCTORS:1||BI2SR2CACU2O8+Y:1||INTERFACES:1||BREAKDOWN:1||SYSTEMS:1||Anisotropy ratio:1||Josephson vortex:1||spin relaxation in superconductors:1||bibased single crystals:1||MESOSCOPIC PROXIMITY SUPERCONDUCTOR:1||reentrance of conductance:1||interlayer pair tunneling:1||JOSEPHSON:1||DISORDERED 2DIMENSIONAL SUPERCONDUCTORS:1||INDIUM FILMS:1||excited state:1||REGIME:1||triplet superconductivity:1||FILM:1||SCHOTTKY DIODES:1||peakdiphump structure:1||Kondo effect:1||REENTRANCE:1||Graphene:1||CONTACT:1||BERRYS PHASE:1||2DIMENSIONAL SUPERCONDUCTORS:1||Coulomb diamond:1||magnetic domain:1||spin injection:1||RESONANCE:1||plasma excitation modes:1||FLOW:1||OVERDOPED BI2SR2CACU2O8+DELTA:1||hole doping:1||chemical synthesis:1||phase transitions:1||superconductors:1||VORTEXGLASS SUPERCONDUCTIVITY:1||Kondorelated model:1||RADIATION:1||DOT:1||NANOBELTS:1||Complementarity:1||Closedloop AharonovBohm interferometer:1||pair breaking:1||interlayer phase fluctuation:1||MgB2 thin film:1||CONFINEMENT:1||WALLED CARBON NANOTUBES:1||TRANSITION:9||VORTICES:8||STATE:7||intrinsic Josephson junctions:7||SINGLECRYSTALS:7||JUNCTIONS:5||MODES:5||SUPERCURRENT:5||SUPERCONDUCTOR:5||CONDUCTANCE:5||HIGHTEMPERATURE SUPERCONDUCTORS:5||TRANSPORT:5||PHASE:5||FILMS:4||LOCALIZATION:4||SINGLE DIRAC CONE:4||WIRES:4||MAGNETICFIELD:4||STEPS:3||ELECTRONS:3||proximity effect:3||MODEL:3||ARRAYS:3||INTERFERENCE:3||fluxon dynamics:3||HETEROSTRUCTURES:3||INSULATOR:3||Andreev reflection:3||electronic transport:3||FISKE:3||superconductor:2||ZnO:2||quantum point contact:2||METAL:2||DYNAMICS:2||interlayer Josephson coupling:2||SUPERCONDUCTORS:2||YBA2CU3O7DELTA:2||LAYER:2||DOTS:2||quantum dot:2||Article:2||TRANSISTORS:2||CARBON NANOTUBES:2||GAP:2||MECHANISM:2||LINE:2||GIANT SHAPIRO STEPS:2||LAYERS:2||electron energy loss spectroscopy:2||physical phenomena:2||scanning electron microscopy:2||HGTE QUANTUMWELLS:2||BI2TE3:2||SPECTROSCOPY:2||PNJUNCTIONS:2||spinpolarized tunneling:2||INTRINSIC JOSEPHSONJUNCTIONS:2||FIELDS:2||positive magnetoresistance:2||dilute magnetic semiconductor:2||magnetic field:2||scanning transmission electron microscopy:2||QUANTUM OSCILLATIONS:2||TRANSPORTPROPERTIES:2||surface pair current:2||MAGNETORESISTANCE:2||NANORIBBONS:2||INSTABILITY:2||ANDREEV REFLECTION:2||microwave irradiation:2||vertical graphene josephson junction:2||BI2SE3:2||CONDUCTIVITY:2||highTc superconductors:2||DIMENSIONAL ELECTRONGAS:2||graphene:2||Topological insulators:2||Josephson coupling Fraunhofer interference pattern:2||FERROMAGNET:2||DEPENDENCE:2||DETECTOR:2||COHERENCE:2||INJECTION:2||GRAPHENE:1||JOSEPHSONJUNCTIONS:1||LAYERED SUPERCONDUCTOR:1||mode splitting:1||BEHAVIOR:1||spinpolarized transport:1||SUPERCONDUCTING TRANSITION:1||microwave response:1||PSEUDOGAP:1||phase coherence:1||TRANSITIONS:1||Long Josephson junction:1||Charge detection:1||collective resonance modes:1||plasma oscillation modes:1||Superconducting proximity effect:1||Iron pnictide superconductor:1||McMillanRowell oscillations:1||ferromagnetic microstructure:1||superradiant state:1||VOLTAGE:1||branch splitting:1||TENSOR:1||INTERCALATION:1||insitu fabrication:1||NDGAO3:1||DISORDERED METALS:1||GAUGE GLASS:1||LOWTEMPERATURE TRANSPORT:1||spontaneous spin polarization model:1||BIAS:1||emission of electromagnetic waves:1||YBA2CU3O7/PRBA2CU3O7 SUPERLATTICES:1||BOHM:1||SHAPIRO STEPS:1||superconductor/ferromagnet interface:1||OXIDE:1||ANDREEVREFLECTION:1||SinFeAsO single crystal:1||COLLECTIVE MOTION:1||ANGULARDEPENDENCE:1||SUPERCONDUCTIVITY:1||BILAYER GRAPHENE:1||PHOTOLUMINESCENT PROPERTIES:1||SUPERCONDUCTING WEAK LINKS:1||intrinsic Josephson junctions geometrical resonance:1||intrinsic Josephson junction:1||MESOSCOPIC SPINVALVE:1||Bi2212 single crystals:1||intrinsic junctions:1||ANDREEV REFLECTIONS:1||normalmetal/superconductor interface:1||IBI2SR2CACU2OY:1||THERMAL FLUCTUATIONS:1||MIXED STATE:1||BI2.15SR1.85CACU2O8+DELTA:1||intrinsic Josephson effects:1||CACUO:1||QUANTUM POINT CONTACTS:1||resonant tunneling state:1||coherence length:1||NANOWIRE:1||GATES:1||Phase line:1||Thermal activation:1||QUANTUMDOT:1||superconducting proximity effect:1||Andreev interferometer:1||WIRE:1||Josephsonvortexflow branches:1||Bi2212 cuprates:1||LATTICE:1||demannetization effect:1||SUPERCONDUCTING MIRRORS:1||GAS:1||VALLEY TRANSPORT:1||ELECTRODES:1||DEPENDENT TRANSPORT:1||BORNOPPENHEIMER APPROXIMATION:1||collective plasma oscillations:1||fluxon resonance steps:1||STACKS:1||COLLECTIVE DYNAMICS:1||PAIRING SYMMETRY:1||MUON SPIN ROTATION:1||DIMENSIONAL CROSSOVER:1||Bi2Sr2CaCu2Oy highTc superconductors:1||heterojunctions:1||nanostructures:1||surfaces and interfaces:1||QUANTUM TRANSPORT:1||MICROJUNCTIONS:1||RESONATORS:1||STATES:1||FIELD:1||FLUCTUATIONS:1||SCATTERING:1||mode splitting of Josephson vortexflow branches:1||2D superconductivity:1||TRANSISTOR:1||ENERGYGAP:1||SUPERLATTICES:1||IRONBASED SUPERCONDUCTORS:1||PHASEDEPENDENT RESISTANCE:1||QUANTUM PHASETRANSITIONS:1||ELECTRICFIELD:1||HIGH MAGNETICFIELDS:1||NANOWIRE HETEROSTRUCTURES:1||ZNO:1||pair breaking.:1||SUPERCONDUCTING PB:1||domain formation:1||FORCE MICROSCOPY:1||RELAXATION:1||PLASMA RESONANCE:1||coupled Josephson junctions:1||COPPEROXIDE SUPERCONDUCTORS:1||CROSSOVER:1||SIMULATIONS:1||LOWTEMPERATURE:1||CONDUCTORS:1||METALINSULATORTRANSITION:1||SEMICONDUCTOR:1||FIELDEFFECT TRANSISTORS:1||ZEROVOLTAGE STATE:1||constanttemperature interlayer tunneling spectroscopy:1||Josephson supercurrent:1||BIPOLAR SUPERCURRENT:1||Interaction between Josephson and pancake vortices:1||flux jump:1||coaxial heterojunction nanorod:1||Natural Josephson coupling:1||BI2SR2CACU2O8+DELTA:1||VORTEX FLOW:1||TC SUPERCONDUCTORS:1||charge imbalance:1||Andreev diffractometer:1||intercalation:1||surface junction:1||Bi2212:1||tunnelling:1||GRAPHITE:1||GROWTH:1||collective transverse plasma modes:1||GAN:1||Macroscopic quantum tunneling:1||Fluctuation conductivity:1||Abovegap conductance jump:1||Josephson vortex motion:1||Intrinsic Josephson junctions:1||LAYERED SUPERCONDUCTORS:1||BI2SR2CACU2O8+Y:1||INTERFACES:1||BREAKDOWN:1||SYSTEMS:1||Anisotropy ratio:1||Josephson vortex:1||spin relaxation in superconductors:1||bibased single crystals:1||MESOSCOPIC PROXIMITY SUPERCONDUCTOR:1||reentrance of conductance:1||interlayer pair tunneling:1||JOSEPHSON:1||DISORDERED 2DIMENSIONAL SUPERCONDUCTORS:1||INDIUM FILMS:1||excited state:1||REGIME:1||triplet superconductivity:1||FILM:1||SCHOTTKY DIODES:1||peakdiphump structure:1||Kondo effect:1||REENTRANCE:1||Graphene:1||CONTACT:1||BERRYS PHASE:1||2DIMENSIONAL SUPERCONDUCTORS:1||Coulomb diamond:1||magnetic domain:1||spin injection:1||RESONANCE:1||plasma excitation modes:1||FLOW:1||OVERDOPED BI2SR2CACU2O8+DELTA:1||hole doping:1||chemical synthesis:1||phase transitions:1||superconductors:1||VORTEXGLASS SUPERCONDUCTIVITY:1||Kondorelated model:1||RADIATION:1||DOT:1||NANOBELTS:1||Complementarity:1||Closedloop AharonovBohm interferometer:1||pair breaking:1||interlayer phase fluctuation:1||MgB2 thin film:1||CONFINEMENT:1||WALLED CARBON NANOTUBES:1||TRANSITION:9||VORTICES:8||STATE:7||intrinsic Josephson junctions:7||SINGLECRYSTALS:7||JUNCTIONS:5||MODES:5||SUPERCURRENT:5||SUPERCONDUCTOR:5||CONDUCTANCE:5||HIGHTEMPERATURE SUPERCONDUCTORS:5||TRANSPORT:5||PHASE:5||FILMS:4||LOCALIZATION:4||SINGLE DIRAC CONE:4||WIRES:4||MAGNETICFIELD:4||STEPS:3||ELECTRONS:3||proximity effect:3||MODEL:3||ARRAYS:3||INTERFERENCE:3||fluxon dynamics:3||HETEROSTRUCTURES:3||INSULATOR:3||Andreev reflection:3||electronic transport:3||FISKE:3||superconductor:2||ZnO:2||quantum point contact:2||METAL:2||DYNAMICS:2||interlayer Josephson coupling:2||SUPERCONDUCTORS:2||YBA2CU3O7DELTA:2||LAYER:2||DOTS:2||quantum dot:2||Article:2||TRANSISTORS:2||CARBON NANOTUBES:2||GAP:2||MECHANISM:2||LINE:2||GIANT SHAPIRO STEPS:2||LAYERS:2||electron energy loss spectroscopy:2||physical phenomena:2||scanning electron microscopy:2||HGTE QUANTUMWELLS:2||BI2TE3:2||SPECTROSCOPY:2||PNJUNCTIONS:2||spinpolarized tunneling:2||INTRINSIC JOSEPHSONJUNCTIONS:2||FIELDS:2||positive magnetoresistance:2||dilute magnetic semiconductor:2||magnetic field:2||scanning transmission electron microscopy:2||QUANTUM OSCILLATIONS:2||TRANSPORTPROPERTIES:2||surface pair current:2||MAGNETORESISTANCE:2||NANORIBBONS:2||INSTABILITY:2||ANDREEV REFLECTION:2||microwave irradiation:2||vertical graphene josephson junction:2||BI2SE3:2||CONDUCTIVITY:2||highTc superconductors:2||DIMENSIONAL ELECTRONGAS:2||graphene:2||Topological insulators:2||Josephson coupling Fraunhofer interference pattern:2||FERROMAGNET:2||DEPENDENCE:2||DETECTOR:2||COHERENCE:2||INJECTION:2||GRAPHENE:1||JOSEPHSONJUNCTIONS:1||LAYERED SUPERCONDUCTOR:1||mode splitting:1||BEHAVIOR:1||spinpolarized transport:1||SUPERCONDUCTING TRANSITION:1||microwave response:1||PSEUDOGAP:1||phase coherence:1||TRANSITIONS:1||Long Josephson junction:1||Charge detection:1||collective resonance modes:1||plasma oscillation modes:1||Superconducting proximity effect:1||Iron pnictide superconductor:1||McMillanRowell oscillations:1||ferromagnetic microstructure:1||superradiant state:1||VOLTAGE:1||branch splitting:1||TENSOR:1||INTERCALATION:1||insitu fabrication:1||NDGAO3:1||DISORDERED METALS:1||GAUGE GLASS:1||LOWTEMPERATURE TRANSPORT:1||spontaneous spin polarization model:1||BIAS:1||emission of electromagnetic waves:1||YBA2CU3O7/PRBA2CU3O7 SUPERLATTICES:1||BOHM:1||SHAPIRO STEPS:1||superconductor/ferromagnet interface:1||OXIDE:1||ANDREEVREFLECTION:1||SinFeAsO single crystal:1||COLLECTIVE MOTION:1||ANGULARDEPENDENCE:1||SUPERCONDUCTIVITY:1||BILAYER GRAPHENE:1||PHOTOLUMINESCENT PROPERTIES:1||SUPERCONDUCTING WEAK LINKS:1||intrinsic Josephson junctions geometrical resonance:1||intrinsic Josephson junction:1||MESOSCOPIC SPINVALVE:1||Bi2212 single crystals:1||intrinsic junctions:1||ANDREEV REFLECTIONS:1||normalmetal/superconductor interface:1||IBI2SR2CACU2OY:1||THERMAL FLUCTUATIONS:1||MIXED STATE:1||BI2.15SR1.85CACU2O8+DELTA:1||intrinsic Josephson effects:1||CACUO:1||QUANTUM POINT CONTACTS:1||resonant tunneling state:1||coherence length:1||NANOWIRE:1||GATES:1||Phase line:1||Thermal activation:1||QUANTUMDOT:1||superconducting proximity effect:1||Andreev interferometer:1||WIRE:1||Josephsonvortexflow branches:1||Bi2212 cuprates:1||LATTICE:1||demannetization effect:1||SUPERCONDUCTING MIRRORS:1||GAS:1||VALLEY TRANSPORT:1||ELECTRODES:1||DEPENDENT TRANSPORT:1||BORNOPPENHEIMER APPROXIMATION:1||collective plasma oscillations:1||fluxon resonance steps:1||STACKS:1||COLLECTIVE DYNAMICS:1||PAIRING SYMMETRY:1||MUON SPIN ROTATION:1||DIMENSIONAL CROSSOVER:1||Bi2Sr2CaCu2Oy highTc superconductors:1||heterojunctions:1||nanostructures:1||surfaces and interfaces:1||QUANTUM TRANSPORT:1||MICROJUNCTIONS:1||RESONATORS:1||STATES:1||FIELD:1||FLUCTUATIONS:1||SCATTERING:1||mode splitting of Josephson vortexflow branches:1||2D superconductivity:1||TRANSISTOR:1||ENERGYGAP:1||SUPERLATTICES:1||IRONBASED SUPERCONDUCTORS:1||PHASEDEPENDENT RESISTANCE:1||QUANTUM PHASETRANSITIONS:1||ELECTRICFIELD:1||HIGH MAGNETICFIELDS:1||NANOWIRE HETEROSTRUCTURES:1||ZNO:1||pair breaking.:1||SUPERCONDUCTING PB:1||domain formation:1||FORCE MICROSCOPY:1||RELAXATION:1||PLASMA RESONANCE:1||coupled Josephson junctions:1||COPPEROXIDE SUPERCONDUCTORS:1||CROSSOVER:1||SIMULATIONS:1||LOWTEMPERATURE:1||CONDUCTORS:1||METALINSULATORTRANSITION:1||SEMICONDUCTOR:1||FIELDEFFECT TRANSISTORS:1||ZEROVOLTAGE STATE:1||constanttemperature interlayer tunneling spectroscopy:1||Josephson supercurrent:1||BIPOLAR SUPERCURRENT:1||Interaction between Josephson and pancake vortices:1||flux jump:1||coaxial heterojunction nanorod:1||Natural Josephson coupling:1||BI2SR2CACU2O8+DELTA:1||VORTEX FLOW:1||TC SUPERCONDUCTORS:1||charge imbalance:1||Andreev diffractometer:1||intercalation:1||surface junction:1||Bi2212:1||tunnelling:1||GRAPHITE:1||GROWTH:1||collective transverse plasma modes:1||GAN:1||Macroscopic quantum tunneling:1||Fluctuation conductivity:1||Abovegap conductance jump:1||Josephson vortex motion:1||Intrinsic Josephson junctions:1||LAYERED SUPERCONDUCTORS:1||BI2SR2CACU2O8+Y:1||INTERFACES:1||BREAKDOWN:1||SYSTEMS:1||Anisotropy ratio:1||Josephson vortex:1||spin relaxation in superconductors:1||bibased single crystals:1||MESOSCOPIC PROXIMITY SUPERCONDUCTOR:1||reentrance of conductance:1||interlayer pair tunneling:1||JOSEPHSON:1||DISORDERED 2DIMENSIONAL SUPERCONDUCTORS:1||INDIUM FILMS:1||excited state:1||REGIME:1||triplet superconductivity:1||FILM:1||SCHOTTKY DIODES:1||peakdiphump structure:1||Kondo effect:1||REENTRANCE:1||Graphene:1||CONTACT:1||BERRYS PHASE:1||2DIMENSIONAL SUPERCONDUCTORS:1||Coulomb diamond:1||magnetic domain:1||spin injection:1||RESONANCE:1||plasma excitation modes:1||FLOW:1||OVERDOPED BI2SR2CACU2O8+DELTA:1||hole doping:1||chemical synthesis:1||phase transitions:1||superconductors:1||VORTEXGLASS SUPERCONDUCTIVITY:1||Kondorelated model:1||RADIATION:1||DOT:1||NANOBELTS:1||Complementarity:1||Closedloop AharonovBohm interferometer:1||pair breaking:1||interlayer phase fluctuation:1||MgB2 thin film:1||CONFINEMENT:1||WALLED CARBON NANOTUBES:1||TRANSITION:9||VORTICES:8||STATE:7||intrinsic Josephson junctions:7||SINGLECRYSTALS:7||JUNCTIONS:5||MODES:5||SUPERCURRENT:5||SUPERCONDUCTOR:5||CONDUCTANCE:5||HIGHTEMPERATURE SUPERCONDUCTORS:5||TRANSPORT:5||PHASE:5||FILMS:4||LOCALIZATION:4||SINGLE DIRAC CONE:4||WIRES:4||MAGNETICFIELD:4||STEPS:3||ELECTRONS:3||proximity effect:3||MODEL:3||ARRAYS:3||INTERFERENCE:3||fluxon dynamics:3||HETEROSTRUCTURES:3||INSULATOR:3||Andreev reflection:3||electronic transport:3||FISKE:3||superconductor:2||ZnO:2||quantum point contact:2||METAL:2||DYNAMICS:2||interlayer Josephson coupling:2||SUPERCONDUCTORS:2||YBA2CU3O7DELTA:2||LAYER:2||DOTS:2||quantum dot:2||Article:2||TRANSISTORS:2||CARBON NANOTUBES:2||GAP:2||MECHANISM:2||LINE:2||GIANT SHAPIRO STEPS:2||LAYERS:2||electron energy loss spectroscopy:2||physical phenomena:2||scanning electron microscopy:2||HGTE QUANTUMWELLS:2||BI2TE3:2||SPECTROSCOPY:2||PNJUNCTIONS:2||spinpolarized tunneling:2||INTRINSIC JOSEPHSONJUNCTIONS:2||FIELDS:2||positive magnetoresistance:2||dilute magnetic semiconductor:2||magnetic field:2||scanning transmission electron microscopy:2||QUANTUM OSCILLATIONS:2||TRANSPORTPROPERTIES:2||surface pair current:2||MAGNETORESISTANCE:2||NANORIBBONS:2||INSTABILITY:2||ANDREEV REFLECTION:2||microwave irradiation:2||vertical graphene josephson junction:2||BI2SE3:2||CONDUCTIVITY:2||highTc superconductors:2||DIMENSIONAL ELECTRONGAS:2||graphene:2||Topological insulators:2||Josephson coupling Fraunhofer interference pattern:2||FERROMAGNET:2||DEPENDENCE:2||DETECTOR:2||COHERENCE:2||INJECTION:2||GRAPHENE:1||JOSEPHSONJUNCTIONS:1||LAYERED SUPERCONDUCTOR:1||mode splitting:1||BEHAVIOR:1||spinpolarized transport:1||SUPERCONDUCTING TRANSITION:1||microwave response:1||PSEUDOGAP:1||phase coherence:1||TRANSITIONS:1||Long Josephson junction:1||Charge detection:1||collective resonance modes:1||plasma oscillation modes:1||Superconducting proximity effect:1||Iron pnictide superconductor:1||McMillanRowell oscillations:1||ferromagnetic microstructure:1||superradiant state:1||VOLTAGE:1||branch splitting:1||TENSOR:1||INTERCALATION:1||insitu fabrication:1||NDGAO3:1||DISORDERED METALS:1||GAUGE GLASS:1||LOWTEMPERATURE TRANSPORT:1||spontaneous spin polarization model:1||BIAS:1||emission of electromagnetic waves:1||YBA2CU3O7/PRBA2CU3O7 SUPERLATTICES:1||BOHM:1||SHAPIRO STEPS:1||superconductor/ferromagnet interface:1||OXIDE:1||ANDREEVREFLECTION:1||SinFeAsO single crystal:1||COLLECTIVE MOTION:1||ANGULARDEPENDENCE:1||SUPERCONDUCTIVITY:1||BILAYER GRAPHENE:1||PHOTOLUMINESCENT PROPERTIES:1||SUPERCONDUCTING WEAK LINKS:1||intrinsic Josephson junctions geometrical resonance:1||intrinsic Josephson junction:1||MESOSCOPIC SPINVALVE:1||Bi2212 single crystals:1||intrinsic junctions:1||ANDREEV REFLECTIONS:1||normalmetal/superconductor interface:1||IBI2SR2CACU2OY:1||THERMAL FLUCTUATIONS:1||MIXED STATE:1||BI2.15SR1.85CACU2O8+DELTA:1||intrinsic Josephson effects:1||CACUO:1||QUANTUM POINT CONTACTS:1||resonant tunneling state:1||coherence length:1||NANOWIRE:1||GATES:1||Phase line:1||Thermal activation:1||QUANTUMDOT:1||superconducting proximity effect:1||Andreev interferometer:1||WIRE:1||Josephsonvortexflow branches:1||Bi2212 cuprates:1||LATTICE:1||demannetization effect:1||SUPERCONDUCTING MIRRORS:1||GAS:1||VALLEY TRANSPORT:1||ELECTRODES:1||DEPENDENT TRANSPORT:1||BORNOPPENHEIMER APPROXIMATION:1||collective plasma oscillations:1||fluxon resonance steps:1||STACKS:1||COLLECTIVE DYNAMICS:1||PAIRING SYMMETRY:1||MUON SPIN ROTATION:1||DIMENSIONAL CROSSOVER:1||Bi2Sr2CaCu2Oy highTc superconductors:1||heterojunctions:1||nanostructures:1||surfaces and interfaces:1||QUANTUM TRANSPORT:1||MICROJUNCTIONS:1||RESONATORS:1||STATES:1||FIELD:1||FLUCTUATIONS:1||SCATTERING:1||mode splitting of Josephson vortexflow branches:1||2D superconductivity:1||TRANSISTOR:1||ENERGYGAP:1||SUPERLATTICES:1||IRONBASED SUPERCONDUCTORS:1||PHASEDEPENDENT RESISTANCE:1||QUANTUM PHASETRANSITIONS:1||ELECTRICFIELD:1||HIGH MAGNETICFIELDS:1||NANOWIRE HETEROSTRUCTURES:1||ZNO:1||pair breaking.:1||SUPERCONDUCTING PB:1||domain formation:1||FORCE MICROSCOPY:1||RELAXATION:1||PLASMA RESONANCE:1||coupled Josephson junctions:1||COPPEROXIDE SUPERCONDUCTORS:1||CROSSOVER:1||SIMULATIONS:1||LOWTEMPERATURE:1||CONDUCTORS:1||METALINSULATORTRANSITION:1||SEMICONDUCTOR:1||FIELDEFFECT TRANSISTORS:1||ZEROVOLTAGE STATE:1||constanttemperature interlayer tunneling spectroscopy:1||Josephson supercurrent:1||BIPOLAR SUPERCURRENT:1||Interaction between Josephson and pancake vortices:1||flux jump:1||coaxial heterojunction nanorod:1||Natural Josephson coupling:1||BI2SR2CACU2O8+DELTA:1||VORTEX FLOW:1||TC SUPERCONDUCTORS:1||charge imbalance:1||Andreev diffractometer:1||intercalation:1||surface junction:1||Bi2212:1||tunnelling:1||GRAPHITE:1||GROWTH:1||collective transverse plasma modes:1||GAN:1||Macroscopic quantum tunneling:1||Fluctuation conductivity:1||Abovegap conductance jump:1||Josephson vortex motion:1||Intrinsic Josephson junctions:1||LAYERED SUPERCONDUCTORS:1||BI2SR2CACU2O8+Y:1||INTERFACES:1||BREAKDOWN:1||SYSTEMS:1||Anisotropy ratio:1||Josephson vortex:1||spin relaxation in superconductors:1||bibased single crystals:1||MESOSCOPIC PROXIMITY SUPERCONDUCTOR:1||reentrance of conductance:1||interlayer pair tunneling:1||JOSEPHSON:1||DISORDERED 2DIMENSIONAL SUPERCONDUCTORS:1||INDIUM FILMS:1||excited state:1||REGIME:1||triplet superconductivity:1||FILM:1||SCHOTTKY DIODES:1||peakdiphump structure:1||Kondo effect:1||REENTRANCE:1||Graphene:1||CONTACT:1||BERRYS PHASE:1||2DIMENSIONAL SUPERCONDUCTORS:1||Coulomb diamond:1||magnetic domain:1||spin injection:1||RESONANCE:1||plasma excitation modes:1||FLOW:1||OVERDOPED BI2SR2CACU2O8+DELTA:1||hole doping:1||chemical synthesis:1||phase transitions:1||superconductors:1||VORTEXGLASS SUPERCONDUCTIVITY:1||Kondorelated model:1||RADIATION:1||DOT:1||NANOBELTS:1||Complementarity:1||Closedloop AharonovBohm interferometer:1||pair breaking:1||interlayer phase fluctuation:1||MgB2 thin film:1||CONFINEMENT:1||WALLED CARBON NANOTUBES:1||TRANSITION:9||VORTICES:8||STATE:7||intrinsic Josephson junctions:7||SINGLECRYSTALS:7||JUNCTIONS:5||MODES:5||SUPERCURRENT:5||SUPERCONDUCTOR:5||CONDUCTANCE:5||HIGHTEMPERATURE SUPERCONDUCTORS:5||TRANSPORT:5||PHASE:5||FILMS:4||LOCALIZATION:4||SINGLE DIRAC CONE:4||WIRES:4||MAGNETICFIELD:4||STEPS:3||ELECTRONS:3||proximity effect:3||MODEL:3||ARRAYS:3||INTERFERENCE:3||fluxon dynamics:3||HETEROSTRUCTURES:3||INSULATOR:3||Andreev reflection:3||electronic transport:3||FISKE:3||superconductor:2||ZnO:2||quantum point contact:2||METAL:2||DYNAMICS:2||interlayer Josephson coupling:2||SUPERCONDUCTORS:2||YBA2CU3O7DELTA:2||LAYER:2||DOTS:2||quantum dot:2||Article:2||TRANSISTORS:2||CARBON NANOTUBES:2||GAP:2||MECHANISM:2||LINE:2||GIANT SHAPIRO STEPS:2||LAYERS:2||electron energy loss spectroscopy:2||physical phenomena:2||scanning electron microscopy:2||HGTE QUANTUMWELLS:2||BI2TE3:2||SPECTROSCOPY:2||PNJUNCTIONS:2||spinpolarized tunneling:2||INTRINSIC JOSEPHSONJUNCTIONS:2||FIELDS:2||positive magnetoresistance:2||dilute magnetic semiconductor:2||magnetic field:2||scanning transmission electron microscopy:2||QUANTUM OSCILLATIONS:2||TRANSPORTPROPERTIES:2||surface pair current:2||MAGNETORESISTANCE:2||NANORIBBONS:2||INSTABILITY:2||ANDREEV REFLECTION:2||microwave irradiation:2||vertical graphene josephson junction:2||BI2SE3:2||CONDUCTIVITY:2||highTc superconductors:2||DIMENSIONAL ELECTRONGAS:2||graphene:2||Topological insulators:2||Josephson coupling Fraunhofer interference pattern:2||FERROMAGNET:2||DEPENDENCE:2||DETECTOR:2||COHERENCE:2||INJECTION:2||GRAPHENE:1||JOSEPHSONJUNCTIONS:1||LAYERED SUPERCONDUCTOR:1||mode splitting:1||BEHAVIOR:1||spinpolarized transport:1||SUPERCONDUCTING TRANSITION:1||microwave response:1||PSEUDOGAP:1||phase coherence:1||TRANSITIONS:1||Long Josephson junction:1||Charge detection:1||collective resonance modes:1||plasma oscillation modes:1||Superconducting proximity effect:1||Iron pnictide superconductor:1||McMillanRowell oscillations:1||ferromagnetic microstructure:1||superradiant state:1||VOLTAGE:1||branch splitting:1||TENSOR:1||INTERCALATION:1||insitu fabrication:1||NDGAO3:1||DISORDERED METALS:1||GAUGE GLASS:1||LOWTEMPERATURE TRANSPORT:1||spontaneous spin polarization model:1||BIAS:1||emission of electromagnetic waves:1||YBA2CU3O7/PRBA2CU3O7 SUPERLATTICES:1||BOHM:1||SHAPIRO STEPS:1||superconductor/ferromagnet interface:1||OXIDE:1||ANDREEVREFLECTION:1||SinFeAsO single crystal:1||COLLECTIVE MOTION:1||ANGULARDEPENDENCE:1||SUPERCONDUCTIVITY:1||BILAYER GRAPHENE:1||PHOTOLUMINESCENT PROPERTIES:1||SUPERCONDUCTING WEAK LINKS:1||intrinsic Josephson junctions geometrical resonance:1||intrinsic Josephson junction:1||MESOSCOPIC SPINVALVE:1||Bi2212 single crystals:1||intrinsic junctions:1||ANDREEV REFLECTIONS:1||normalmetal/superconductor interface:1||IBI2SR2CACU2OY:1||THERMAL FLUCTUATIONS:1||MIXED STATE:1||BI2.15SR1.85CACU2O8+DELTA:1||intrinsic Josephson effects:1||CACUO:1||QUANTUM POINT CONTACTS:1||resonant tunneling state:1||coherence length:1||NANOWIRE:1||GATES:1||Phase line:1||Thermal activation:1||QUANTUMDOT:1||superconducting proximity effect:1||Andreev interferometer:1||WIRE:1||Josephsonvortexflow branches:1||Bi2212 cuprates:1||LATTICE:1||demannetization effect:1||SUPERCONDUCTING MIRRORS:1||GAS:1||VALLEY TRANSPORT:1||ELECTRODES:1||DEPENDENT TRANSPORT:1||BORNOPPENHEIMER APPROXIMATION:1||collective plasma oscillations:1||fluxon resonance steps:1||STACKS:1||COLLECTIVE DYNAMICS:1||PAIRING SYMMETRY:1||MUON SPIN ROTATION:1||DIMENSIONAL CROSSOVER:1||Bi2Sr2CaCu2Oy highTc superconductors:1||heterojunctions:1||nanostructures:1||surfaces and interfaces:1||QUANTUM TRANSPORT:1||MICROJUNCTIONS:1||RESONATORS:1||STATES:1||FIELD:1||FLUCTUATIONS:1||SCATTERING:1||mode splitting of Josephson vortexflow branches:1||2D superconductivity:1||TRANSISTOR:1||ENERGYGAP:1||SUPERLATTICES:1||IRONBASED SUPERCONDUCTORS:1||PHASEDEPENDENT RESISTANCE:1||QUANTUM PHASETRANSITIONS:1||ELECTRICFIELD:1||HIGH MAGNETICFIELDS:1||NANOWIRE HETEROSTRUCTURES:1||ZNO:1||pair breaking.:1||SUPERCONDUCTING PB:1||domain formation:1||FORCE MICROSCOPY:1||RELAXATION:1||PLASMA RESONANCE:1||coupled Josephson junctions:1||COPPEROXIDE SUPERCONDUCTORS:1||CROSSOVER:1||SIMULATIONS:1||LOWTEMPERATURE:1||CONDUCTORS:1||METALINSULATORTRANSITION:1||SEMICONDUCTOR:1||FIELDEFFECT TRANSISTORS:1||ZEROVOLTAGE STATE:1||constanttemperature interlayer tunneling spectroscopy:1||Josephson supercurrent:1||BIPOLAR SUPERCURRENT:1||Interaction between Josephson and pancake vortices:1||flux jump:1||coaxial heterojunction nanorod:1||Natural Josephson coupling:1||BI2SR2CACU2O8+DELTA:1||VORTEX FLOW:1||TC SUPERCONDUCTORS:1||charge imbalance:1||Andreev diffractometer:1||intercalation:1||surface junction:1||Bi2212:1||tunnelling:1||GRAPHITE:1||GROWTH:1||collective transverse plasma modes:1||GAN:1||Macroscopic quantum tunneling:1||Fluctuation conductivity:1||Abovegap conductance jump:1||Josephson vortex motion:1||Intrinsic Josephson junctions:1||LAYERED SUPERCONDUCTORS:1||BI2SR2CACU2O8+Y:1||INTERFACES:1||BREAKDOWN:1||SYSTEMS:1||Anisotropy ratio:1||Josephson vortex:1||spin relaxation in superconductors:1||bibased single crystals:1||MESOSCOPIC PROXIMITY SUPERCONDUCTOR:1||reentrance of conductance:1||interlayer pair tunneling:1||JOSEPHSON:1||DISORDERED 2DIMENSIONAL SUPERCONDUCTORS:1||INDIUM FILMS:1||excited state:1||REGIME:1||triplet superconductivity:1||FILM:1||SCHOTTKY DIODES:1||peakdiphump structure:1||Kondo effect:1||REENTRANCE:1||Graphene:1||CONTACT:1||BERRYS PHASE:1||2DIMENSIONAL SUPERCONDUCTORS:1||Coulomb diamond:1||magnetic domain:1||spin injection:1||RESONANCE:1||plasma excitation modes:1||FLOW:1||OVERDOPED BI2SR2CACU2O8+DELTA:1||hole doping:1||chemical synthesis:1||phase transitions:1||superconductors:1||VORTEXGLASS SUPERCONDUCTIVITY:1||Kondorelated model:1||RADIATION:1||DOT:1||NANOBELTS:1||Complementarity:1||Closedloop AharonovBohm interferometer:1||pair breaking:1||interlayer phase fluctuation:1||MgB2 thin film:1||CONFINEMENT:1||WALLED CARBON NANOTUBES:1||TRANSITION:9||VORTICES:8||STATE:7||intrinsic Josephson junctions:7||SINGLECRYSTALS:7||JUNCTIONS:5||MODES:5||SUPERCURRENT:5||SUPERCONDUCTOR:5||CONDUCTANCE:5||HIGHTEMPERATURE SUPERCONDUCTORS:5||TRANSPORT:5||PHASE:5||FILMS:4||LOCALIZATION:4||SINGLE DIRAC CONE:4||WIRES:4||MAGNETICFIELD:4||STEPS:3||ELECTRONS:3||proximity effect:3||MODEL:3||ARRAYS:3||INTERFERENCE:3||fluxon dynamics:3||HETEROSTRUCTURES:3||INSULATOR:3||Andreev reflection:3||electronic transport:3||FISKE:3||superconductor:2||ZnO:2||quantum point contact:2||METAL:2||DYNAMICS:2||interlayer Josephson coupling:2||SUPERCONDUCTORS:2||YBA2CU3O7DELTA:2||LAYER:2||DOTS:2||quantum dot:2||Article:2||TRANSISTORS:2||CARBON NANOTUBES:2||GAP:2||MECHANISM:2||LINE:2||GIANT SHAPIRO STEPS:2||LAYERS:2||electron energy loss spectroscopy:2||physical phenomena:2||scanning electron microscopy:2||HGTE QUANTUMWELLS:2||BI2TE3:2||SPECTROSCOPY:2||PNJUNCTIONS:2||spinpolarized tunneling:2||INTRINSIC JOSEPHSONJUNCTIONS:2||FIELDS:2||positive magnetoresistance:2||dilute magnetic semiconductor:2||magnetic field:2||scanning transmission electron microscopy:2||QUANTUM OSCILLATIONS:2||TRANSPORTPROPERTIES:2||surface pair current:2||MAGNETORESISTANCE:2||NANORIBBONS:2||INSTABILITY:2||ANDREEV REFLECTION:2||microwave irradiation:2||vertical graphene josephson junction:2||BI2SE3:2||CONDUCTIVITY:2||highTc superconductors:2||DIMENSIONAL ELECTRONGAS:2||graphene:2||Topological insulators:2||Josephson coupling Fraunhofer interference pattern:2||FERROMAGNET:2||DEPENDENCE:2||DETECTOR:2||COHERENCE:2||INJECTION:2||GRAPHENE:1||JOSEPHSONJUNCTIONS:1||LAYERED SUPERCONDUCTOR:1||mode splitting:1||BEHAVIOR:1||spinpolarized transport:1||SUPERCONDUCTING TRANSITION:1||microwave response:1||PSEUDOGAP:1||phase coherence:1||TRANSITIONS:1||Long Josephson junction:1||Charge detection:1||collective resonance modes:1||plasma oscillation modes:1||Superconducting proximity effect:1||Iron pnictide superconductor:1||McMillanRowell oscillations:1||ferromagnetic microstructure:1||superradiant state:1||VOLTAGE:1||branch splitting:1||TENSOR:1||INTERCALATION:1||insitu fabrication:1||NDGAO3:1||DISORDERED METALS:1||GAUGE GLASS:1||LOWTEMPERATURE TRANSPORT:1||spontaneous spin polarization model:1||BIAS:1||emission of electromagnetic waves:1||YBA2CU3O7/PRBA2CU3O7 SUPERLATTICES:1||BOHM:1||SHAPIRO STEPS:1||superconductor/ferromagnet interface:1||OXIDE:1||ANDREEVREFLECTION:1||SinFeAsO single crystal:1||COLLECTIVE MOTION:1||ANGULARDEPENDENCE:1||SUPERCONDUCTIVITY:1||BILAYER GRAPHENE:1||PHOTOLUMINESCENT PROPERTIES:1||SUPERCONDUCTING WEAK LINKS:1||intrinsic Josephson junctions geometrical resonance:1||intrinsic Josephson junction:1||MESOSCOPIC SPINVALVE:1||Bi2212 single crystals:1||intrinsic junctions:1||ANDREEV REFLECTIONS:1||normalmetal/superconductor interface:1||IBI2SR2CACU2OY:1||THERMAL FLUCTUATIONS:1||MIXED STATE:1||BI2.15SR1.85CACU2O8+DELTA:1||intrinsic Josephson effects:1||CACUO:1||QUANTUM POINT CONTACTS:1||resonant tunneling state:1||coherence length:1||NANOWIRE:1||GATES:1||Phase line:1||Thermal activation:1||QUANTUMDOT:1||superconducting proximity effect:1||Andreev interferometer:1||WIRE:1||Josephsonvortexflow branches:1||Bi2212 cuprates:1||LATTICE:1||demannetization effect:1||SUPERCONDUCTING MIRRORS:1||GAS:1||VALLEY TRANSPORT:1||ELECTRODES:1||DEPENDENT TRANSPORT:1||BORNOPPENHEIMER APPROXIMATION:1||collective plasma oscillations:1||fluxon resonance steps:1||STACKS:1||COLLECTIVE DYNAMICS:1||PAIRING SYMMETRY:1||MUON SPIN ROTATION:1||DIMENSIONAL CROSSOVER:1||Bi2Sr2CaCu2Oy highTc superconductors:1||heterojunctions:1||nanostructures:1||surfaces and interfaces:1||QUANTUM TRANSPORT:1||MICROJUNCTIONS:1||RESONATORS:1||STATES:1||FIELD:1||FLUCTUATIONS:1||SCATTERING:1||mode splitting of Josephson vortexflow branches:1||2D superconductivity:1||TRANSISTOR:1||ENERGYGAP:1||SUPERLATTICES:1||IRONBASED SUPERCONDUCTORS:1||PHASEDEPENDENT RESISTANCE:1||QUANTUM PHASETRANSITIONS:1||ELECTRICFIELD:1||HIGH MAGNETICFIELDS:1||NANOWIRE HETEROSTRUCTURES:1||ZNO:1||pair breaking.:1||SUPERCONDUCTING PB:1||domain formation:1||FORCE MICROSCOPY:1||RELAXATION:1||PLASMA RESONANCE:1||coupled Josephson junctions:1||COPPEROXIDE SUPERCONDUCTORS:1||CROSSOVER:1||SIMULATIONS:1||LOWTEMPERATURE:1||CONDUCTORS:1||METALINSULATORTRANSITION:1||SEMICONDUCTOR:1||FIELDEFFECT TRANSISTORS:1||ZEROVOLTAGE STATE:1||constanttemperature interlayer tunneling spectroscopy:1||Josephson supercurrent:1||BIPOLAR SUPERCURRENT:1||Interaction between Josephson and pancake vortices:1||flux jump:1||coaxial heterojunction nanorod:1||Natural Josephson coupling:1||BI2SR2CACU2O8+DELTA:1||VORTEX FLOW:1||TC SUPERCONDUCTORS:1||charge imbalance:1||Andreev diffractometer:1||intercalation:1||surface junction:1||Bi2212:1||tunnelling:1||GRAPHITE:1||GROWTH:1||collective transverse plasma modes:1||GAN:1||Macroscopic quantum tunneling:1||Fluctuation conductivity:1||Abovegap conductance jump:1||Josephson vortex motion:1||Intrinsic Josephson junctions:1||LAYERED SUPERCONDUCTORS:1||BI2SR2CACU2O8+Y:1||INTERFACES:1||BREAKDOWN:1||SYSTEMS:1||Anisotropy ratio:1||Josephson vortex:1||spin relaxation in superconductors:1||bibased single crystals:1||MESOSCOPIC PROXIMITY SUPERCONDUCTOR:1||reentrance of conductance:1||interlayer pair tunneling:1||JOSEPHSON:1||DISORDERED 2DIMENSIONAL SUPERCONDUCTORS:1||INDIUM FILMS:1||excited state:1||REGIME:1||triplet superconductivity:1||FILM:1||SCHOTTKY DIODES:1||peakdiphump structure:1||Kondo effect:1||REENTRANCE:1||Graphene:1||CONTACT:1||BERRYS PHASE:1||2DIMENSIONAL SUPERCONDUCTORS:1||Coulomb diamond:1||magnetic domain:1||spin injection:1||RESONANCE:1||plasma excitation modes:1||FLOW:1||OVERDOPED BI2SR2CACU2O8+DELTA:1||hole doping:1||chemical synthesis:1||phase transitions:1||superconductors:1||VORTEXGLASS SUPERCONDUCTIVITY:1||Kondorelated model:1||RADIATION:1||DOT:1||NANOBELTS:1||Complementarity:1||Closedloop AharonovBohm interferometer:1||pair breaking:1||interlayer phase fluctuation:1||MgB2 thin film:1||CONFINEMENT:1||WALLED CARBON NANOTUBES:1||TRANSITION:9||VORTICES:8||STATE:7||intrinsic Josephson junctions:7||SINGLECRYSTALS:7||JUNCTIONS:5||MODES:5||SUPERCURRENT:5||SUPERCONDUCTOR:5||CONDUCTANCE:5||HIGHTEMPERATURE SUPERCONDUCTORS:5||TRANSPORT:5||PHASE:5||FILMS:4||LOCALIZATION:4||SINGLE DIRAC CONE:4||WIRES:4||MAGNETICFIELD:4||STEPS:3||ELECTRONS:3||proximity effect:3||MODEL:3||ARRAYS:3||INTERFERENCE:3||fluxon dynamics:3||HETEROSTRUCTURES:3||INSULATOR:3||Andreev reflection:3||electronic transport:3||FISKE:3||superconductor:2||ZnO:2||quantum point contact:2||METAL:2||DYNAMICS:2||interlayer Josephson coupling:2||SUPERCONDUCTORS:2||YBA2CU3O7DELTA:2||LAYER:2||DOTS:2||quantum dot:2||Article:2||TRANSISTORS:2||CARBON NANOTUBES:2||GAP:2||MECHANISM:2||LINE:2||GIANT SHAPIRO STEPS:2||LAYERS:2||electron energy loss spectroscopy:2||physical phenomena:2||scanning electron microscopy:2||HGTE QUANTUMWELLS:2||BI2TE3:2||SPECTROSCOPY:2||PNJUNCTIONS:2||spinpolarized tunneling:2||INTRINSIC JOSEPHSONJUNCTIONS:2||FIELDS:2||positive magnetoresistance:2||dilute magnetic semiconductor:2||magnetic field:2||scanning transmission electron microscopy:2||QUANTUM OSCILLATIONS:2||TRANSPORTPROPERTIES:2||surface pair current:2||MAGNETORESISTANCE:2||NANORIBBONS:2||INSTABILITY:2||ANDREEV REFLECTION:2||microwave irradiation:2||vertical graphene josephson junction:2||BI2SE3:2||CONDUCTIVITY:2||highTc superconductors:2||DIMENSIONAL ELECTRONGAS:2||graphene:2||Topological insulators:2||Josephson coupling Fraunhofer interference pattern:2||FERROMAGNET:2||DEPENDENCE:2||DETECTOR:2||COHERENCE:2||INJECTION:2||GRAPHENE:1||JOSEPHSONJUNCTIONS:1||LAYERED SUPERCONDUCTOR:1||mode splitting:1||BEHAVIOR:1||spinpolarized transport:1||SUPERCONDUCTING TRANSITION:1||microwave response:1||PSEUDOGAP:1||phase coherence:1||TRANSITIONS:1||Long Josephson junction:1||Charge detection:1||collective resonance modes:1||plasma oscillation modes:1||Superconducting proximity effect:1||Iron pnictide superconductor:1||McMillanRowell oscillations:1||ferromagnetic microstructure:1||superradiant state:1||VOLTAGE:1||branch splitting:1||TENSOR:1||INTERCALATION:1||insitu fabrication:1||NDGAO3:1||DISORDERED METALS:1||GAUGE GLASS:1||LOWTEMPERATURE TRANSPORT:1||spontaneous spin polarization model:1||BIAS:1||emission of electromagnetic waves:1||YBA2CU3O7/PRBA2CU3O7 SUPERLATTICES:1||BOHM:1||SHAPIRO STEPS:1||superconductor/ferromagnet interface:1||OXIDE:1||ANDREEVREFLECTION:1||SinFeAsO single crystal:1||COLLECTIVE MOTION:1||ANGULARDEPENDENCE:1||SUPERCONDUCTIVITY:1||BILAYER GRAPHENE:1||PHOTOLUMINESCENT PROPERTIES:1||SUPERCONDUCTING WEAK LINKS:1||intrinsic Josephson junctions geometrical resonance:1||intrinsic Josephson junction:1||MESOSCOPIC SPINVALVE:1||Bi2212 single crystals:1||intrinsic junctions:1||ANDREEV REFLECTIONS:1||normalmetal/superconductor interface:1||IBI2SR2CACU2OY:1||THERMAL FLUCTUATIONS:1||MIXED STATE:1||BI2.15SR1.85CACU2O8+DELTA:1||intrinsic Josephson effects:1||CACUO:1||QUANTUM POINT CONTACTS:1||resonant tunneling state:1||coherence length:1||NANOWIRE:1||GATES:1||Phase line:1||Thermal activation:1||QUANTUMDOT:1||superconducting proximity effect:1||Andreev interferometer:1||WIRE:1||Josephsonvortexflow branches:1||Bi2212 cuprates:1||LATTICE:1||demannetization effect:1||SUPERCONDUCTING MIRRORS:1||GAS:1||VALLEY TRANSPORT:1||ELECTRODES:1||DEPENDENT TRANSPORT:1||BORNOPPENHEIMER APPROXIMATION:1||collective plasma oscillations:1||fluxon resonance steps:1||STACKS:1||COLLECTIVE DYNAMICS:1||PAIRING SYMMETRY:1||MUON SPIN ROTATION:1||DIMENSIONAL CROSSOVER:1||Bi2Sr2CaCu2Oy highTc superconductors:1||heterojunctions:1||nanostructures:1||surfaces and interfaces:1||QUANTUM TRANSPORT:1||MICROJUNCTIONS:1||RESONATORS:1||STATES:1||FIELD:1||FLUCTUATIONS:1||SCATTERING:1||mode splitting of Josephson vortexflow branches:1||2D superconductivity:1||TRANSISTOR:1||ENERGYGAP:1||SUPERLATTICES:1||IRONBASED SUPERCONDUCTORS:1||PHASEDEPENDENT RESISTANCE:1||QUANTUM PHASETRANSITIONS:1||ELECTRICFIELD:1||HIGH MAGNETICFIELDS:1||NANOWIRE HETEROSTRUCTURES:1||ZNO:1||pair breaking.:1||SUPERCONDUCTING PB:1||domain formation:1||FORCE MICROSCOPY:1||RELAXATION:1||PLASMA RESONANCE:1||coupled Josephson junctions:1||COPPEROXIDE SUPERCONDUCTORS:1||CROSSOVER:1||SIMULATIONS:1||LOWTEMPERATURE:1||CONDUCTORS:1||METALINSULATORTRANSITION:1||SEMICONDUCTOR:1||FIELDEFFECT TRANSISTORS:1||ZEROVOLTAGE STATE:1||constanttemperature interlayer tunneling spectroscopy:1||Josephson supercurrent:1||BIPOLAR SUPERCURRENT:1||Interaction between Josephson and pancake vortices:1||flux jump:1||coaxial heterojunction nanorod:1||Natural Josephson coupling:1||BI2SR2CACU2O8+DELTA:1||VORTEX FLOW:1||TC SUPERCONDUCTORS:1||charge imbalance:1||Andreev diffractometer:1||intercalation:1||surface junction:1||Bi2212:1||tunnelling:1||GRAPHITE:1||GROWTH:1||collective transverse plasma modes:1||GAN:1||Macroscopic quantum tunneling:1||Fluctuation conductivity:1||Abovegap conductance jump:1||Josephson vortex motion:1||Intrinsic Josephson junctions:1||LAYERED SUPERCONDUCTORS:1||BI2SR2CACU2O8+Y:1||INTERFACES:1||BREAKDOWN:1||SYSTEMS:1||Anisotropy ratio:1||Josephson vortex:1||spin relaxation in superconductors:1||bibased single crystals:1||MESOSCOPIC PROXIMITY SUPERCONDUCTOR:1||reentrance of conductance:1||interlayer pair tunneling:1||JOSEPHSON:1||DISORDERED 2DIMENSIONAL SUPERCONDUCTORS:1||INDIUM FILMS:1||excited state:1||REGIME:1||triplet superconductivity:1||FILM:1||SCHOTTKY DIODES:1||peakdiphump structure:1||Kondo effect:1||REENTRANCE:1||Graphene:1||CONTACT:1||BERRYS PHASE:1||2DIMENSIONAL SUPERCONDUCTORS:1||Coulomb diamond:1||magnetic domain:1||spin injection:1||RESONANCE:1||plasma excitation modes:1||FLOW:1||OVERDOPED BI2SR2CACU2O8+DELTA:1||hole doping:1||chemical synthesis:1||phase transitions:1||superconductors:1||VORTEXGLASS SUPERCONDUCTIVITY:1||Kondorelated model:1||RADIATION:1||DOT:1||NANOBELTS:1||Complementarity:1||Closedloop AharonovBohm interferometer:1||pair breaking:1||interlayer phase fluctuation:1||MgB2 thin film:1||CONFINEMENT:1||WALLED CARBON NANOTUBES:1||TRANSITION:9||VORTICES:8||STATE:7||intrinsic Josephson junctions:7||SINGLECRYSTALS:7||JUNCTIONS:5||MODES:5||SUPERCURRENT:5||SUPERCONDUCTOR:5||CONDUCTANCE:5||HIGHTEMPERATURE SUPERCONDUCTORS:5||TRANSPORT:5||PHASE:5||FILMS:4||LOCALIZATION:4||SINGLE DIRAC CONE:4||WIRES:4||MAGNETICFIELD:4||STEPS:3||ELECTRONS:3||proximity effect:3||MODEL:3||ARRAYS:3||INTERFERENCE:3||fluxon dynamics:3||HETEROSTRUCTURES:3||INSULATOR:3||Andreev reflection:3||electronic transport:3||FISKE:3||superconductor:2||ZnO:2||quantum point contact:2||METAL:2||DYNAMICS:2||interlayer Josephson coupling:2||SUPERCONDUCTORS:2||YBA2CU3O7DELTA:2||LAYER:2||DOTS:2||quantum dot:2||Article:2||TRANSISTORS:2||CARBON NANOTUBES:2||GAP:2||MECHANISM:2||LINE:2||GIANT SHAPIRO STEPS:2||LAYERS:2||electron energy loss spectroscopy:2||physical phenomena:2||scanning electron microscopy:2||HGTE QUANTUMWELLS:2||BI2TE3:2||SPECTROSCOPY:2||PNJUNCTIONS:2||spinpolarized tunneling:2||INTRINSIC JOSEPHSONJUNCTIONS:2||FIELDS:2||positive magnetoresistance:2||dilute magnetic semiconductor:2||magnetic field:2||scanning transmission electron microscopy:2||QUANTUM OSCILLATIONS:2||TRANSPORTPROPERTIES:2||surface pair current:2||MAGNETORESISTANCE:2||NANORIBBONS:2||INSTABILITY:2||ANDREEV REFLECTION:2||microwave irradiation:2||vertical graphene josephson junction:2||BI2SE3:2||CONDUCTIVITY:2||highTc superconductors:2||DIMENSIONAL ELECTRONGAS:2||graphene:2||Topological insulators:2||Josephson coupling Fraunhofer interference pattern:2||FERROMAGNET:2||DEPENDENCE:2||DETECTOR:2||COHERENCE:2||INJECTION:2||GRAPHENE:1||JOSEPHSONJUNCTIONS:1||LAYERED SUPERCONDUCTOR:1||mode splitting:1||BEHAVIOR:1||spinpolarized transport:1||SUPERCONDUCTING TRANSITION:1||microwave response:1||PSEUDOGAP:1||phase coherence:1||TRANSITIONS:1||Long Josephson junction:1||Charge detection:1||collective resonance modes:1||plasma oscillation modes:1||Superconducting proximity effect:1||Iron pnictide superconductor:1||McMillanRowell oscillations:1||ferromagnetic microstructure:1||superradiant state:1||VOLTAGE:1||branch splitting:1||TENSOR:1||INTERCALATION:1||insitu fabrication:1||NDGAO3:1||DISORDERED METALS:1||GAUGE GLASS:1||LOWTEMPERATURE TRANSPORT:1||spontaneous spin polarization model:1||BIAS:1||emission of electromagnetic waves:1||YBA2CU3O7/PRBA2CU3O7 SUPERLATTICES:1||BOHM:1||SHAPIRO STEPS:1||superconductor/ferromagnet interface:1||OXIDE:1||ANDREEVREFLECTION:1||SinFeAsO single crystal:1||COLLECTIVE MOTION:1||ANGULARDEPENDENCE:1||SUPERCONDUCTIVITY:1||BILAYER GRAPHENE:1||PHOTOLUMINESCENT PROPERTIES:1||SUPERCONDUCTING WEAK LINKS:1||intrinsic Josephson junctions geometrical resonance:1||intrinsic Josephson junction:1||MESOSCOPIC SPINVALVE:1||Bi2212 single crystals:1||intrinsic junctions:1||ANDREEV REFLECTIONS:1||normalmetal/superconductor interface:1||IBI2SR2CACU2OY:1||THERMAL FLUCTUATIONS:1||MIXED STATE:1||BI2.15SR1.85CACU2O8+DELTA:1||intrinsic Josephson effects:1||CACUO:1||QUANTUM POINT CONTACTS:1||resonant tunneling state:1||coherence length:1||NANOWIRE:1||GATES:1||Phase line:1||Thermal activation:1||QUANTUMDOT:1||superconducting proximity effect:1||Andreev interferometer:1||WIRE:1||Josephsonvortexflow branches:1||Bi2212 cuprates:1||LATTICE:1||demannetization effect:1||SUPERCONDUCTING MIRRORS:1||GAS:1||VALLEY TRANSPORT:1||ELECTRODES:1||DEPENDENT TRANSPORT:1||BORNOPPENHEIMER APPROXIMATION:1||collective plasma oscillations:1||fluxon resonance steps:1||STACKS:1||COLLECTIVE DYNAMICS:1||PAIRING SYMMETRY:1||MUON SPIN ROTATION:1||DIMENSIONAL CROSSOVER:1||Bi2Sr2CaCu2Oy highTc superconductors:1||heterojunctions:1||nanostructures:1||surfaces and interfaces:1||QUANTUM TRANSPORT:1||MICROJUNCTIONS:1||RESONATORS:1||STATES:1||FIELD:1||FLUCTUATIONS:1||SCATTERING:1||mode splitting of Josephson vortexflow branches:1||2D superconductivity:1||TRANSISTOR:1||ENERGYGAP:1||SUPERLATTICES:1||IRONBASED SUPERCONDUCTORS:1||PHASEDEPENDENT RESISTANCE:1||QUANTUM PHASETRANSITIONS:1||ELECTRICFIELD:1||HIGH MAGNETICFIELDS:1||NANOWIRE HETEROSTRUCTURES:1||ZNO:1||pair breaking.:1||SUPERCONDUCTING PB:1||domain formation:1||FORCE MICROSCOPY:1||RELAXATION:1||PLASMA RESONANCE:1||coupled Josephson junctions:1||COPPEROXIDE SUPERCONDUCTORS:1||CROSSOVER:1||SIMULATIONS:1||LOWTEMPERATURE:1||CONDUCTORS:1||METALINSULATORTRANSITION:1||SEMICONDUCTOR:1||FIELDEFFECT TRANSISTORS:1||ZEROVOLTAGE STATE:1||constanttemperature interlayer tunneling spectroscopy:1||Josephson supercurrent:1||BIPOLAR SUPERCURRENT:1||Interaction between Josephson and pancake vortices:1||flux jump:1||coaxial heterojunction nanorod:1||Natural Josephson coupling:1||BI2SR2CACU2O8+DELTA:1||VORTEX FLOW:1||TC SUPERCONDUCTORS:1||charge imbalance:1||Andreev diffractometer:1||intercalation:1||surface junction:1||Bi2212:1||tunnelling:1||GRAPHITE:1||GROWTH:1||collective transverse plasma modes:1||GAN:1||Macroscopic quantum tunneling:1||Fluctuation conductivity:1||Abovegap conductance jump:1||Josephson vortex motion:1||Intrinsic Josephson junctions:1||LAYERED SUPERCONDUCTORS:1||BI2SR2CACU2O8+Y:1||INTERFACES:1||BREAKDOWN:1||SYSTEMS:1||Anisotropy ratio:1||Josephson vortex:1||spin relaxation in superconductors:1||bibased single crystals:1||MESOSCOPIC PROXIMITY SUPERCONDUCTOR:1||reentrance of conductance:1||interlayer pair tunneling:1||JOSEPHSON:1||DISORDERED 2DIMENSIONAL SUPERCONDUCTORS:1||INDIUM FILMS:1||excited state:1||REGIME:1||triplet superconductivity:1||FILM:1||SCHOTTKY DIODES:1||peakdiphump structure:1||Kondo effect:1||REENTRANCE:1||Graphene:1||CONTACT:1||BERRYS PHASE:1||2DIMENSIONAL SUPERCONDUCTORS:1||Coulomb diamond:1||magnetic domain:1||spin injection:1||RESONANCE:1||plasma excitation modes:1||FLOW:1||OVERDOPED BI2SR2CACU2O8+DELTA:1||hole doping:1||chemical synthesis:1||phase transitions:1||superconductors:1||VORTEXGLASS SUPERCONDUCTIVITY:1||Kondorelated model:1||RADIATION:1||DOT:1||NANOBELTS:1||Complementarity:1||Closedloop AharonovBohm interferometer:1||pair breaking:1||interlayer phase fluctuation:1||MgB2 thin film:1||CONFINEMENT:1||WALLED CARBON NANOTUBES:1||TRANSITION:9||VORTICES:8||STATE:7||intrinsic Josephson junctions:7||SINGLECRYSTALS:7||JUNCTIONS:5||MODES:5||SUPERCURRENT:5||SUPERCONDUCTOR:5||CONDUCTANCE:5||HIGHTEMPERATURE SUPERCONDUCTORS:5||TRANSPORT:5||PHASE:5||FILMS:4||LOCALIZATION:4||SINGLE DIRAC CONE:4||WIRES:4||MAGNETICFIELD:4||STEPS:3||ELECTRONS:3||proximity effect:3||MODEL:3||ARRAYS:3||INTERFERENCE:3||fluxon dynamics:3||HETEROSTRUCTURES:3||INSULATOR:3||Andreev reflection:3||electronic transport:3||FISKE:3||superconductor:2||ZnO:2||quantum point contact:2||METAL:2||DYNAMICS:2||interlayer Josephson coupling:2||SUPERCONDUCTORS:2||YBA2CU3O7DELTA:2||LAYER:2||DOTS:2||quantum dot:2||Article:2||TRANSISTORS:2||CARBON NANOTUBES:2||GAP:2||MECHANISM:2||LINE:2||GIANT SHAPIRO STEPS:2||LAYERS:2||electron energy loss spectroscopy:2||physical phenomena:2||scanning electron microscopy:2||HGTE QUANTUMWELLS:2||BI2TE3:2||SPECTROSCOPY:2||PNJUNCTIONS:2||spinpolarized tunneling:2||INTRINSIC JOSEPHSONJUNCTIONS:2||FIELDS:2||positive magnetoresistance:2||dilute magnetic semiconductor:2||magnetic field:2||scanning transmission electron microscopy:2||QUANTUM OSCILLATIONS:2||TRANSPORTPROPERTIES:2||surface pair current:2||MAGNETORESISTANCE:2||NANORIBBONS:2||INSTABILITY:2||ANDREEV REFLECTION:2||microwave irradiation:2||vertical graphene josephson junction:2||BI2SE3:2||CONDUCTIVITY:2||highTc superconductors:2||DIMENSIONAL ELECTRONGAS:2||graphene:2||Topological insulators:2||Josephson coupling Fraunhofer interference pattern:2||FERROMAGNET:2||DEPENDENCE:2||DETECTOR:2||COHERENCE:2||INJECTION:2||GRAPHENE:1||JOSEPHSONJUNCTIONS:1||LAYERED SUPERCONDUCTOR:1||mode splitting:1||BEHAVIOR:1||spinpolarized transport:1||SUPERCONDUCTING TRANSITION:1||microwave response:1||PSEUDOGAP:1||phase coherence:1||TRANSITIONS:1||Long Josephson junction:1||Charge detection:1||collective resonance modes:1||plasma oscillation modes:1||Superconducting proximity effect:1||Iron pnictide superconductor:1||McMillanRowell oscillations:1||ferromagnetic microstructure:1||superradiant state:1||VOLTAGE:1||branch splitting:1||TENSOR:1||INTERCALATION:1||insitu fabrication:1||NDGAO3:1||DISORDERED METALS:1||GAUGE GLASS:1||LOWTEMPERATURE TRANSPORT:1||spontaneous spin polarization model:1||BIAS:1||emission of electromagnetic waves:1||YBA2CU3O7/PRBA2CU3O7 SUPERLATTICES:1||BOHM:1||SHAPIRO STEPS:1||superconductor/ferromagnet interface:1||OXIDE:1||ANDREEVREFLECTION:1||SinFeAsO single crystal:1||COLLECTIVE MOTION:1||ANGULARDEPENDENCE:1||SUPERCONDUCTIVITY:1||BILAYER GRAPHENE:1||PHOTOLUMINESCENT PROPERTIES:1||SUPERCONDUCTING WEAK LINKS:1||intrinsic Josephson junctions geometrical resonance:1||intrinsic Josephson junction:1||MESOSCOPIC SPINVALVE:1||Bi2212 single crystals:1||intrinsic junctions:1||ANDREEV REFLECTIONS:1||normalmetal/superconductor interface:1||IBI2SR2CACU2OY:1||THERMAL FLUCTUATIONS:1||MIXED STATE:1||BI2.15SR1.85CACU2O8+DELTA:1||intrinsic Josephson effects:1||CACUO:1||QUANTUM POINT CONTACTS:1||resonant tunneling state:1||coherence length:1||NANOWIRE:1||GATES:1||Phase line:1||Thermal activation:1||QUANTUMDOT:1||superconducting proximity effect:1||Andreev interferometer:1||WIRE:1||Josephsonvortexflow branches:1||Bi2212 cuprates:1||LATTICE:1||demannetization effect:1||SUPERCONDUCTING MIRRORS:1||GAS:1||VALLEY TRANSPORT:1||ELECTRODES:1||DEPENDENT TRANSPORT:1||BORNOPPENHEIMER APPROXIMATION:1||collective plasma oscillations:1||fluxon resonance steps:1||STACKS:1||COLLECTIVE DYNAMICS:1||PAIRING SYMMETRY:1||MUON SPIN ROTATION:1||DIMENSIONAL CROSSOVER:1||Bi2Sr2CaCu2Oy highTc superconductors:1||heterojunctions:1||nanostructures:1||surfaces and interfaces:1||QUANTUM TRANSPORT:1||MICROJUNCTIONS:1||RESONATORS:1||STATES:1||FIELD:1||FLUCTUATIONS:1||SCATTERING:1||mode splitting of Josephson vortexflow branches:1||2D superconductivity:1||TRANSISTOR:1||ENERGYGAP:1||SUPERLATTICES:1||IRONBASED SUPERCONDUCTORS:1||PHASEDEPENDENT RESISTANCE:1||QUANTUM PHASETRANSITIONS:1||ELECTRICFIELD:1||HIGH MAGNETICFIELDS:1||NANOWIRE HETEROSTRUCTURES:1||ZNO:1||pair breaking.:1||SUPERCONDUCTING PB:1||domain formation:1||FORCE MICROSCOPY:1||RELAXATION:1||PLASMA RESONANCE:1||coupled Josephson junctions:1||COPPEROXIDE SUPERCONDUCTORS:1||CROSSOVER:1||SIMULATIONS:1||LOWTEMPERATURE:1||CONDUCTORS:1||METALINSULATORTRANSITION:1||SEMICONDUCTOR:1||FIELDEFFECT TRANSISTORS:1||ZEROVOLTAGE STATE:1||constanttemperature interlayer tunneling spectroscopy:1||Josephson supercurrent:1||BIPOLAR SUPERCURRENT:1||Interaction between Josephson and pancake vortices:1||flux jump:1||coaxial heterojunction nanorod:1||Natural Josephson coupling:1||BI2SR2CACU2O8+DELTA:1||VORTEX FLOW:1||TC SUPERCONDUCTORS:1||charge imbalance:1||Andreev diffractometer:1||intercalation:1||surface junction:1||Bi2212:1||tunnelling:1||GRAPHITE:1||GROWTH:1||collective transverse plasma modes:1||GAN:1||Macroscopic quantum tunneling:1||Fluctuation conductivity:1||Abovegap conductance jump:1||Josephson vortex motion:1||Intrinsic Josephson junctions:1||LAYERED SUPERCONDUCTORS:1||BI2SR2CACU2O8+Y:1||INTERFACES:1||BREAKDOWN:1||SYSTEMS:1||Anisotropy ratio:1||Josephson vortex:1||spin relaxation in superconductors:1||bibased single crystals:1||MESOSCOPIC PROXIMITY SUPERCONDUCTOR:1||reentrance of conductance:1||interlayer pair tunneling:1||JOSEPHSON:1||DISORDERED 2DIMENSIONAL SUPERCONDUCTORS:1||INDIUM FILMS:1||excited state:1||REGIME:1||triplet superconductivity:1||FILM:1||SCHOTTKY DIODES:1||peakdiphump structure:1||Kondo effect:1||REENTRANCE:1||Graphene:1||CONTACT:1||BERRYS PHASE:1||2DIMENSIONAL SUPERCONDUCTORS:1||Coulomb diamond:1||magnetic domain:1||spin injection:1||RESONANCE:1||plasma excitation modes:1||FLOW:1||OVERDOPED BI2SR2CACU2O8+DELTA:1||hole doping:1||chemical synthesis:1||phase transitions:1||superconductors:1||VORTEXGLASS SUPERCONDUCTIVITY:1||Kondorelated model:1||RADIATION:1||DOT:1||NANOBELTS:1||Complementarity:1||Closedloop AharonovBohm interferometer:1||pair breaking:1||interlayer phase fluctuation:1||MgB2 thin film:1||CONFINEMENT:1||WALLED CARBON NANOTUBES:1||TRANSITION:9||VORTICES:8||STATE:7||intrinsic Josephson junctions:7||SINGLECRYSTALS:7||JUNCTIONS:5||MODES:5||SUPERCURRENT:5||SUPERCONDUCTOR:5||CONDUCTANCE:5||HIGHTEMPERATURE SUPERCONDUCTORS:5||TRANSPORT:5||PHASE:5||FILMS:4||LOCALIZATION:4||SINGLE DIRAC CONE:4||WIRES:4||MAGNETICFIELD:4||STEPS:3||ELECTRONS:3||proximity effect:3||MODEL:3||ARRAYS:3||INTERFERENCE:3||fluxon dynamics:3||HETEROSTRUCTURES:3||INSULATOR:3||Andreev reflection:3||electronic transport:3||FISKE:3||superconductor:2||ZnO:2||quantum point contact:2||METAL:2||DYNAMICS:2||interlayer Josephson coupling:2||SUPERCONDUCTORS:2||YBA2CU3O7DELTA:2||LAYER:2||DOTS:2||quantum dot:2||Article:2||TRANSISTORS:2||CARBON NANOTUBES:2||GAP:2||MECHANISM:2||LINE:2||GIANT SHAPIRO STEPS:2||LAYERS:2||electron energy loss spectroscopy:2||physical phenomena:2||scanning electron microscopy:2||HGTE QUANTUMWELLS:2||BI2TE3:2||SPECTROSCOPY:2||PNJUNCTIONS:2||spinpolarized tunneling:2||INTRINSIC JOSEPHSONJUNCTIONS:2||FIELDS:2||positive magnetoresistance:2||dilute magnetic semiconductor:2||magnetic field:2||scanning transmission electron microscopy:2||QUANTUM OSCILLATIONS:2||TRANSPORTPROPERTIES:2||surface pair current:2||MAGNETORESISTANCE:2||NANORIBBONS:2||INSTABILITY:2||ANDREEV REFLECTION:2||microwave irradiation:2||vertical graphene josephson junction:2||BI2SE3:2||CONDUCTIVITY:2||highTc superconductors:2||DIMENSIONAL ELECTRONGAS:2||graphene:2||Topological insulators:2||Josephson coupling Fraunhofer interference pattern:2||FERROMAGNET:2||DEPENDENCE:2||DETECTOR:2||COHERENCE:2||INJECTION:2||GRAPHENE:1||JOSEPHSONJUNCTIONS:1||LAYERED SUPERCONDUCTOR:1||mode splitting:1||BEHAVIOR:1||spinpolarized transport:1||SUPERCONDUCTING TRANSITION:1||microwave response:1||PSEUDOGAP:1||phase coherence:1||TRANSITIONS:1||Long Josephson junction:1||Charge detection:1||collective resonance modes:1||plasma oscillation modes:1||Superconducting proximity effect:1||Iron pnictide superconductor:1||McMillanRowell oscillations:1||ferromagnetic microstructure:1||superradiant state:1||VOLTAGE:1||branch splitting:1||TENSOR:1||INTERCALATION:1||insitu fabrication:1||NDGAO3:1||DISORDERED METALS:1||GAUGE GLASS:1||LOWTEMPERATURE TRANSPORT:1||spontaneous spin polarization model:1||BIAS:1||emission of electromagnetic waves:1||YBA2CU3O7/PRBA2CU3O7 SUPERLATTICES:1||BOHM:1||SHAPIRO STEPS:1||superconductor/ferromagnet interface:1||OXIDE:1||ANDREEVREFLECTION:1||SinFeAsO single crystal:1||COLLECTIVE MOTION:1||ANGULARDEPENDENCE:1||SUPERCONDUCTIVITY:1||BILAYER GRAPHENE:1||PHOTOLUMINESCENT PROPERTIES:1||SUPERCONDUCTING WEAK LINKS:1||intrinsic Josephson junctions geometrical resonance:1||intrinsic Josephson junction:1||MESOSCOPIC SPINVALVE:1||Bi2212 single crystals:1||intrinsic junctions:1||ANDREEV REFLECTIONS:1||normalmetal/superconductor interface:1||IBI2SR2CACU2OY:1||THERMAL FLUCTUATIONS:1||MIXED STATE:1||BI2.15SR1.85CACU2O8+DELTA:1||intrinsic Josephson effects:1||CACUO:1||QUANTUM POINT CONTACTS:1||resonant tunneling state:1||coherence length:1||NANOWIRE:1||GATES:1||Phase line:1||Thermal activation:1||QUANTUMDOT:1||superconducting proximity effect:1||Andreev interferometer:1||WIRE:1||Josephsonvortexflow branches:1||Bi2212 cuprates:1||LATTICE:1||demannetization effect:1||SUPERCONDUCTING MIRRORS:1||GAS:1||VALLEY TRANSPORT:1||ELECTRODES:1||DEPENDENT TRANSPORT:1||BORNOPPENHEIMER APPROXIMATION:1||collective plasma oscillations:1||fluxon resonance steps:1||STACKS:1||COLLECTIVE DYNAMICS:1||PAIRING SYMMETRY:1||MUON SPIN ROTATION:1||DIMENSIONAL CROSSOVER:1||Bi2Sr2CaCu2Oy highTc superconductors:1||heterojunctions:1||nanostructures:1||surfaces and interfaces:1||QUANTUM TRANSPORT:1||MICROJUNCTIONS:1||RESONATORS:1||STATES:1||FIELD:1||FLUCTUATIONS:1||SCATTERING:1||mode splitting of Josephson vortexflow branches:1||2D superconductivity:1||TRANSISTOR:1||ENERGYGAP:1||SUPERLATTICES:1||IRONBASED SUPERCONDUCTORS:1||PHASEDEPENDENT RESISTANCE:1||QUANTUM PHASETRANSITIONS:1||ELECTRICFIELD:1||HIGH MAGNETICFIELDS:1||NANOWIRE HETEROSTRUCTURES:1||ZNO:1||pair breaking.:1||SUPERCONDUCTING PB:1||domain formation:1||FORCE MICROSCOPY:1||RELAXATION:1||PLASMA RESONANCE:1||coupled Josephson junctions:1||COPPEROXIDE SUPERCONDUCTORS:1||CROSSOVER:1||SIMULATIONS:1||LOWTEMPERATURE:1||CONDUCTORS:1||METALINSULATORTRANSITION:1||SEMICONDUCTOR:1||FIELDEFFECT TRANSISTORS:1||ZEROVOLTAGE STATE:1||constanttemperature interlayer tunneling spectroscopy:1||Josephson supercurrent:1||BIPOLAR SUPERCURRENT:1||Interaction between Josephson and pancake vortices:1||flux jump:1||coaxial heterojunction nanorod:1||Natural Josephson coupling:1||BI2SR2CACU2O8+DELTA:1||VORTEX FLOW:1||TC SUPERCONDUCTORS:1||charge imbalance:1||Andreev diffractometer:1||intercalation:1||surface junction:1||Bi2212:1||tunnelling:1||GRAPHITE:1||GROWTH:1||collective transverse plasma modes:1||GAN:1||Macroscopic quantum tunneling:1||Fluctuation conductivity:1||Abovegap conductance jump:1||Josephson vortex motion:1||Intrinsic Josephson junctions:1||LAYERED SUPERCONDUCTORS:1||BI2SR2CACU2O8+Y:1||INTERFACES:1||BREAKDOWN:1||SYSTEMS:1||Anisotropy ratio:1||Josephson vortex:1||spin relaxation in superconductors:1||bibased single crystals:1||MESOSCOPIC PROXIMITY SUPERCONDUCTOR:1||reentrance of conductance:1||interlayer pair tunneling:1||JOSEPHSON:1||DISORDERED 2DIMENSIONAL SUPERCONDUCTORS:1||INDIUM FILMS:1||excited state:1||REGIME:1||triplet superconductivity:1||FILM:1||SCHOTTKY DIODES:1||peakdiphump structure:1||Kondo effect:1||REENTRANCE:1||Graphene:1||CONTACT:1||BERRYS PHASE:1||2DIMENSIONAL SUPERCONDUCTORS:1||Coulomb diamond:1||magnetic domain:1||spin injection:1||RESONANCE:1||plasma excitation modes:1||FLOW:1||OVERDOPED BI2SR2CACU2O8+DELTA:1||hole doping:1||chemical synthesis:1||phase transitions:1||superconductors:1||VORTEXGLASS SUPERCONDUCTIVITY:1||Kondorelated model:1||RADIATION:1||DOT:1||NANOBELTS:1||Complementarity:1||Closedloop AharonovBohm interferometer:1||pair breaking:1||interlayer phase fluctuation:1||MgB2 thin film:1||CONFINEMENT:1||WALLED CARBON NANOTUBES:1||TRANSITION:9||VORTICES:8||STATE:7||intrinsic Josephson junctions:7||SINGLECRYSTALS:7||JUNCTIONS:5||MODES:5||SUPERCURRENT:5||SUPERCONDUCTOR:5||CONDUCTANCE:5||HIGHTEMPERATURE SUPERCONDUCTORS:5||TRANSPORT:5||PHASE:5||FILMS:4||LOCALIZATION:4||SINGLE DIRAC CONE:4||WIRES:4||MAGNETICFIELD:4||STEPS:3||ELECTRONS:3||proximity effect:3||MODEL:3||ARRAYS:3||INTERFERENCE:3||fluxon dynamics:3||HETEROSTRUCTURES:3||INSULATOR:3||Andreev reflection:3||electronic transport:3||FISKE:3||superconductor:2||ZnO:2||quantum point contact:2||METAL:2||DYNAMICS:2||interlayer Josephson coupling:2||SUPERCONDUCTORS:2||YBA2CU3O7DELTA:2||LAYER:2||DOTS:2||quantum dot:2||Article:2||TRANSISTORS:2||CARBON NANOTUBES:2||GAP:2||MECHANISM:2||LINE:2||GIANT SHAPIRO STEPS:2||LAYERS:2||electron energy loss spectroscopy:2||physical phenomena:2||scanning electron microscopy:2||HGTE QUANTUMWELLS:2||BI2TE3:2||SPECTROSCOPY:2||PNJUNCTIONS:2||spinpolarized tunneling:2||INTRINSIC JOSEPHSONJUNCTIONS:2||FIELDS:2||positive magnetoresistance:2||dilute magnetic semiconductor:2||magnetic field:2||scanning transmission electron microscopy:2||QUANTUM OSCILLATIONS:2||TRANSPORTPROPERTIES:2||surface pair current:2||MAGNETORESISTANCE:2||NANORIBBONS:2||INSTABILITY:2||ANDREEV REFLECTION:2||microwave irradiation:2||vertical graphene josephson junction:2||BI2SE3:2||CONDUCTIVITY:2||highTc superconductors:2||DIMENSIONAL ELECTRONGAS:2||graphene:2||Topological insulators:2||Josephson coupling Fraunhofer interference pattern:2||FERROMAGNET:2||DEPENDENCE:2||DETECTOR:2||COHERENCE:2||INJECTION:2||GRAPHENE:1||JOSEPHSONJUNCTIONS:1||LAYERED SUPERCONDUCTOR:1||mode splitting:1||BEHAVIOR:1||spinpolarized transport:1||SUPERCONDUCTING TRANSITION:1||microwave response:1||PSEUDOGAP:1||phase coherence:1||TRANSITIONS:1||Long Josephson junction:1||Charge detection:1||collective resonance modes:1||plasma oscillation modes:1||Superconducting proximity effect:1||Iron pnictide superconductor:1||McMillanRowell oscillations:1||ferromagnetic microstructure:1||superradiant state:1||VOLTAGE:1||branch splitting:1||TENSOR:1||INTERCALATION:1||insitu fabrication:1||NDGAO3:1||DISORDERED METALS:1||GAUGE GLASS:1||LOWTEMPERATURE TRANSPORT:1||spontaneous spin polarization model:1||BIAS:1||emission of electromagnetic waves:1||YBA2CU3O7/PRBA2CU3O7 SUPERLATTICES:1||BOHM:1||SHAPIRO STEPS:1||superconductor/ferromagnet interface:1||OXIDE:1||ANDREEVREFLECTION:1||SinFeAsO single crystal:1||COLLECTIVE MOTION:1||ANGULARDEPENDENCE:1||SUPERCONDUCTIVITY:1||BILAYER GRAPHENE:1||PHOTOLUMINESCENT PROPERTIES:1||SUPERCONDUCTING WEAK LINKS:1||intrinsic Josephson junctions geometrical resonance:1||intrinsic Josephson junction:1||MESOSCOPIC SPINVALVE:1||Bi2212 single crystals:1||intrinsic junctions:1||ANDREEV REFLECTIONS:1||normalmetal/superconductor interface:1||IBI2SR2CACU2OY:1||THERMAL FLUCTUATIONS:1||MIXED STATE:1||BI2.15SR1.85CACU2O8+DELTA:1||intrinsic Josephson effects:1||CACUO:1||QUANTUM POINT CONTACTS:1||resonant tunneling state:1||coherence length:1||NANOWIRE:1||GATES:1||Phase line:1||Thermal activation:1||QUANTUMDOT:1||superconducting proximity effect:1||Andreev interferometer:1||WIRE:1||Josephsonvortexflow branches:1||Bi2212 cuprates:1||LATTICE:1||demannetization effect:1||SUPERCONDUCTING MIRRORS:1||GAS:1||VALLEY TRANSPORT:1||ELECTRODES:1||DEPENDENT TRANSPORT:1||BORNOPPENHEIMER APPROXIMATION:1||collective plasma oscillations:1||fluxon resonance steps:1||STACKS:1||COLLECTIVE DYNAMICS:1||PAIRING SYMMETRY:1||MUON SPIN ROTATION:1||DIMENSIONAL CROSSOVER:1||Bi2Sr2CaCu2Oy highTc superconductors:1||heterojunctions:1||nanostructures:1||surfaces and interfaces:1||QUANTUM TRANSPORT:1||MICROJUNCTIONS:1||RESONATORS:1||STATES:1||FIELD:1||FLUCTUATIONS:1||SCATTERING:1||mode splitting of Josephson vortexflow branches:1||2D superconductivity:1||TRANSISTOR:1||ENERGYGAP:1||SUPERLATTICES:1||IRONBASED SUPERCONDUCTORS:1||PHASEDEPENDENT RESISTANCE:1||QUANTUM PHASETRANSITIONS:1||ELECTRICFIELD:1||HIGH MAGNETICFIELDS:1||NANOWIRE HETEROSTRUCTURES:1||ZNO:1||pair breaking.:1||SUPERCONDUCTING PB:1||domain formation:1||FORCE MICROSCOPY:1||RELAXATION:1||PLASMA RESONANCE:1||coupled Josephson junctions:1||COPPEROXIDE SUPERCONDUCTORS:1||CROSSOVER:1||SIMULATIONS:1||LOWTEMPERATURE:1||CONDUCTORS:1||METALINSULATORTRANSITION:1||SEMICONDUCTOR:1||FIELDEFFECT TRANSISTORS:1||ZEROVOLTAGE STATE:1||constanttemperature interlayer tunneling spectroscopy:1||Josephson supercurrent:1||BIPOLAR SUPERCURRENT:1||Interaction between Josephson and pancake vortices:1||flux jump:1||coaxial heterojunction nanorod:1||Natural Josephson coupling:1||BI2SR2CACU2O8+DELTA:1||VORTEX FLOW:1||TC SUPERCONDUCTORS:1||charge imbalance:1||Andreev diffractometer:1||intercalation:1||surface junction:1||Bi2212:1||tunnelling:1||GRAPHITE:1||GROWTH:1||collective transverse plasma modes:1||GAN:1||Macroscopic quantum tunneling:1||Fluctuation conductivity:1||Abovegap conductance jump:1||Josephson vortex motion:1||Intrinsic Josephson junctions:1||LAYERED SUPERCONDUCTORS:1||BI2SR2CACU2O8+Y:1||INTERFACES:1||BREAKDOWN:1||SYSTEMS:1||Anisotropy ratio:1||Josephson vortex:1||spin relaxation in superconductors:1||bibased single crystals:1||MESOSCOPIC PROXIMITY SUPERCONDUCTOR:1||reentrance of conductance:1||interlayer pair tunneling:1||JOSEPHSON:1||DISORDERED 2DIMENSIONAL SUPERCONDUCTORS:1||INDIUM FILMS:1||excited state:1||REGIME:1||triplet superconductivity:1||FILM:1||SCHOTTKY DIODES:1||peakdiphump structure:1||Kondo effect:1||REENTRANCE:1||Graphene:1||CONTACT:1||BERRYS PHASE:1||2DIMENSIONAL SUPERCONDUCTORS:1||Coulomb diamond:1||magnetic domain:1||spin injection:1||RESONANCE:1||plasma excitation modes:1||FLOW:1||OVERDOPED BI2SR2CACU2O8+DELTA:1||hole doping:1||chemical synthesis:1||phase transitions:1||superconductors:1||VORTEXGLASS SUPERCONDUCTIVITY:1||Kondorelated model:1||RADIATION:1||DOT:1||NANOBELTS:1||Complementarity:1||Closedloop AharonovBohm interferometer:1||pair breaking:1||interlayer phase fluctuation:1||MgB2 thin film:1||CONFINEMENT:1||WALLED CARBON NANOTUBES:1||TRANSITION:9||VORTICES:8||STATE:7||intrinsic Josephson junctions:7||SINGLECRYSTALS:7||JUNCTIONS:5||MODES:5||SUPERCURRENT:5||SUPERCONDUCTOR:5||CONDUCTANCE:5||HIGHTEMPERATURE SUPERCONDUCTORS:5||TRANSPORT:5||PHASE:5||FILMS:4||LOCALIZATION:4||SINGLE DIRAC CONE:4||WIRES:4||MAGNETICFIELD:4||STEPS:3||ELECTRONS:3||proximity effect:3||MODEL:3||ARRAYS:3||INTERFERENCE:3||fluxon dynamics:3||HETEROSTRUCTURES:3||INSULATOR:3||Andreev reflection:3||electronic transport:3||FISKE:3||superconductor:2||ZnO:2||quantum point contact:2||METAL:2||DYNAMICS:2||interlayer Josephson coupling:2||SUPERCONDUCTORS:2||YBA2CU3O7DELTA:2||LAYER:2||DOTS:2||quantum dot:2||Article:2||TRANSISTORS:2||CARBON NANOTUBES:2||GAP:2||MECHANISM:2||LINE:2||GIANT SHAPIRO STEPS:2||LAYERS:2||electron energy loss spectroscopy:2||physical phenomena:2||scanning electron microscopy:2||HGTE QUANTUMWELLS:2||BI2TE3:2||SPECTROSCOPY:2||PNJUNCTIONS:2||spinpolarized tunneling:2||INTRINSIC JOSEPHSONJUNCTIONS:2||FIELDS:2||positive magnetoresistance:2||dilute magnetic semiconductor:2||magnetic field:2||scanning transmission electron microscopy:2||QUANTUM OSCILLATIONS:2||TRANSPORTPROPERTIES:2||surface pair current:2||MAGNETORESISTANCE:2||NANORIBBONS:2||INSTABILITY:2||ANDREEV REFLECTION:2||microwave irradiation:2||vertical graphene josephson junction:2||BI2SE3:2||CONDUCTIVITY:2||highTc superconductors:2||DIMENSIONAL ELECTRONGAS:2||graphene:2||Topological insulators:2||Josephson coupling Fraunhofer interference pattern:2||FERROMAGNET:2||DEPENDENCE:2||DETECTOR:2||COHERENCE:2||INJECTION:2||GRAPHENE:1||JOSEPHSONJUNCTIONS:1||LAYERED SUPERCONDUCTOR:1||mode splitting:1||BEHAVIOR:1||spinpolarized transport:1||SUPERCONDUCTING TRANSITION:1||microwave response:1||PSEUDOGAP:1||phase coherence:1||TRANSITIONS:1||Long Josephson junction:1||Charge detection:1||collective resonance modes:1||plasma oscillation modes:1||Superconducting proximity effect:1||Iron pnictide superconductor:1||McMillanRowell oscillations:1||ferromagnetic microstructure:1||superradiant state:1||VOLTAGE:1||branch splitting:1||TENSOR:1||INTERCALATION:1||insitu fabrication:1||NDGAO3:1||DISORDERED METALS:1||GAUGE GLASS:1||LOWTEMPERATURE TRANSPORT:1||spontaneous spin polarization model:1||BIAS:1||emission of electromagnetic waves:1||YBA2CU3O7/PRBA2CU3O7 SUPERLATTICES:1||BOHM:1||SHAPIRO STEPS:1||superconductor/ferromagnet interface:1||OXIDE:1||ANDREEVREFLECTION:1||SinFeAsO single crystal:1||COLLECTIVE MOTION:1||ANGULARDEPENDENCE:1||SUPERCONDUCTIVITY:1||BILAYER GRAPHENE:1||PHOTOLUMINESCENT PROPERTIES:1||SUPERCONDUCTING WEAK LINKS:1||intrinsic Josephson junctions geometrical resonance:1||intrinsic Josephson junction:1||MESOSCOPIC SPINVALVE:1||Bi2212 single crystals:1||intrinsic junctions:1||ANDREEV REFLECTIONS:1||normalmetal/superconductor interface:1||IBI2SR2CACU2OY:1||THERMAL FLUCTUATIONS:1||MIXED STATE:1||BI2.15SR1.85CACU2O8+DELTA:1||intrinsic Josephson effects:1||CACUO:1||QUANTUM POINT CONTACTS:1||resonant tunneling state:1||coherence length:1||NANOWIRE:1||GATES:1||Phase line:1||Thermal activation:1||QUANTUMDOT:1||superconducting proximity effect:1||Andreev interferometer:1||WIRE:1||Josephsonvortexflow branches:1||Bi2212 cuprates:1||LATTICE:1||demannetization effect:1||SUPERCONDUCTING MIRRORS:1||GAS:1||VALLEY TRANSPORT:1||ELECTRODES:1||DEPENDENT TRANSPORT:1||BORNOPPENHEIMER APPROXIMATION:1||collective plasma oscillations:1||fluxon resonance steps:1||STACKS:1||COLLECTIVE DYNAMICS:1||PAIRING SYMMETRY:1||MUON SPIN ROTATION:1||DIMENSIONAL CROSSOVER:1||Bi2Sr2CaCu2Oy highTc superconductors:1||heterojunctions:1||nanostructures:1||surfaces and interfaces:1||QUANTUM TRANSPORT:1||MICROJUNCTIONS:1||RESONATORS:1||STATES:1||FIELD:1||FLUCTUATIONS:1||SCATTERING:1||mode splitting of Josephson vortexflow branches:1||2D superconductivity:1||TRANSISTOR:1||ENERGYGAP:1||SUPERLATTICES:1||IRONBASED SUPERCONDUCTORS:1||PHASEDEPENDENT RESISTANCE:1||QUANTUM PHASETRANSITIONS:1||ELECTRICFIELD:1||HIGH MAGNETICFIELDS:1||NANOWIRE HETEROSTRUCTURES:1||ZNO:1||pair breaking.:1||SUPERCONDUCTING PB:1||domain formation:1||FORCE MICROSCOPY:1||RELAXATION:1||PLASMA RESONANCE:1||coupled Josephson junctions:1||COPPEROXIDE SUPERCONDUCTORS:1||CROSSOVER:1||SIMULATIONS:1||LOWTEMPERATURE:1||CONDUCTORS:1||METALINSULATORTRANSITION:1||SEMICONDUCTOR:1||FIELDEFFECT TRANSISTORS:1||ZEROVOLTAGE STATE:1||constanttemperature interlayer tunneling spectroscopy:1||Josephson supercurrent:1||BIPOLAR SUPERCURRENT:1||Interaction between Josephson and pancake vortices:1||flux jump:1||coaxial heterojunction nanorod:1||Natural Josephson coupling:1||BI2SR2CACU2O8+DELTA:1||VORTEX FLOW:1||TC SUPERCONDUCTORS:1||charge imbalance:1||Andreev diffractometer:1||intercalation:1||surface junction:1||Bi2212:1||tunnelling:1||GRAPHITE:1||GROWTH:1||collective transverse plasma modes:1||GAN:1||Macroscopic quantum tunneling:1||Fluctuation conductivity:1||Abovegap conductance jump:1||Josephson vortex motion:1||Intrinsic Josephson junctions:1||LAYERED SUPERCONDUCTORS:1||BI2SR2CACU2O8+Y:1||INTERFACES:1||BREAKDOWN:1||SYSTEMS:1||Anisotropy ratio:1||Josephson vortex:1||spin relaxation in superconductors:1||bibased single crystals:1||MESOSCOPIC PROXIMITY SUPERCONDUCTOR:1||reentrance of conductance:1||interlayer pair tunneling:1||JOSEPHSON:1||DISORDERED 2DIMENSIONAL SUPERCONDUCTORS:1||INDIUM FILMS:1||excited state:1||REGIME:1||triplet superconductivity:1||FILM:1||SCHOTTKY DIODES:1||peakdiphump structure:1||Kondo effect:1||REENTRANCE:1||Graphene:1||CONTACT:1||BERRYS PHASE:1||2DIMENSIONAL SUPERCONDUCTORS:1||Coulomb diamond:1||magnetic domain:1||spin injection:1||RESONANCE:1||plasma excitation modes:1||FLOW:1||OVERDOPED BI2SR2CACU2O8+DELTA:1||hole doping:1||chemical synthesis:1||phase transitions:1||superconductors:1||VORTEXGLASS SUPERCONDUCTIVITY:1||Kondorelated model:1||RADIATION:1||DOT:1||NANOBELTS:1||Complementarity:1||Closedloop AharonovBohm interferometer:1||pair breaking:1||interlayer phase fluctuation:1||MgB2 thin film:1||CONFINEMENT:1||WALLED CARBON NANOTUBES:1||TRANSITION:9||VORTICES:8||STATE:7||intrinsic Josephson junctions:7||SINGLECRYSTALS:7||JUNCTIONS:5||MODES:5||SUPERCURRENT:5||SUPERCONDUCTOR:5||CONDUCTANCE:5||HIGHTEMPERATURE SUPERCONDUCTORS:5||TRANSPORT:5||PHASE:5||FILMS:4||LOCALIZATION:4||SINGLE DIRAC CONE:4||WIRES:4||MAGNETICFIELD:4||STEPS:3||ELECTRONS:3||proximity effect:3||MODEL:3||ARRAYS:3||INTERFERENCE:3||fluxon dynamics:3||HETEROSTRUCTURES:3||INSULATOR:3||Andreev reflection:3||electronic transport:3||FISKE:3||superconductor:2||ZnO:2||quantum point contact:2||METAL:2||DYNAMICS:2||interlayer Josephson coupling:2||SUPERCONDUCTORS:2||YBA2CU3O7DELTA:2||LAYER:2||DOTS:2||quantum dot:2||Article:2||TRANSISTORS:2||CARBON NANOTUBES:2||GAP:2||MECHANISM:2||LINE:2||GIANT SHAPIRO STEPS:2||LAYERS:2||electron energy loss spectroscopy:2||physical phenomena:2||scanning electron microscopy:2||HGTE QUANTUMWELLS:2||BI2TE3:2||SPECTROSCOPY:2||PNJUNCTIONS:2||spinpolarized tunneling:2||INTRINSIC JOSEPHSONJUNCTIONS:2||FIELDS:2||positive magnetoresistance:2||dilute magnetic semiconductor:2||magnetic field:2||scanning transmission electron microscopy:2||QUANTUM OSCILLATIONS:2||TRANSPORTPROPERTIES:2||surface pair current:2||MAGNETORESISTANCE:2||NANORIBBONS:2||INSTABILITY:2||ANDREEV REFLECTION:2||microwave irradiation:2||vertical graphene josephson junction:2||BI2SE3:2||CONDUCTIVITY:2||highTc superconductors:2||DIMENSIONAL ELECTRONGAS:2||graphene:2||Topological insulators:2||Josephson coupling Fraunhofer interference pattern:2||FERROMAGNET:2||DEPENDENCE:2||DETECTOR:2||COHERENCE:2||INJECTION:2||GRAPHENE:1||JOSEPHSONJUNCTIONS:1||LAYERED SUPERCONDUCTOR:1||mode splitting:1||BEHAVIOR:1||spinpolarized transport:1||SUPERCONDUCTING TRANSITION:1||microwave response:1||PSEUDOGAP:1||phase coherence:1||TRANSITIONS:1||Long Josephson junction:1||Charge detection:1||collective resonance modes:1||plasma oscillation modes:1||Superconducting proximity effect:1||Iron pnictide superconductor:1||McMillanRowell oscillations:1||ferromagnetic microstructure:1||superradiant state:1||VOLTAGE:1||branch splitting:1||TENSOR:1||INTERCALATION:1||insitu fabrication:1||NDGAO3:1||DISORDERED METALS:1||GAUGE GLASS:1||LOWTEMPERATURE TRANSPORT:1||spontaneous spin polarization model:1||BIAS:1||emission of electromagnetic waves:1||YBA2CU3O7/PRBA2CU3O7 SUPERLATTICES:1||BOHM:1||SHAPIRO STEPS:1||superconductor/ferromagnet interface:1||OXIDE:1||ANDREEVREFLECTION:1||SinFeAsO single crystal:1||COLLECTIVE MOTION:1||ANGULARDEPENDENCE:1||SUPERCONDUCTIVITY:1||BILAYER GRAPHENE:1||PHOTOLUMINESCENT PROPERTIES:1||SUPERCONDUCTING WEAK LINKS:1||intrinsic Josephson junctions geometrical resonance:1||intrinsic Josephson junction:1||MESOSCOPIC SPINVALVE:1||Bi2212 single crystals:1||intrinsic junctions:1||ANDREEV REFLECTIONS:1||normalmetal/superconductor interface:1||IBI2SR2CACU2OY:1||THERMAL FLUCTUATIONS:1||MIXED STATE:1||BI2.15SR1.85CACU2O8+DELTA:1||intrinsic Josephson effects:1||CACUO:1||QUANTUM POINT CONTACTS:1||resonant tunneling state:1||coherence length:1||NANOWIRE:1||GATES:1||Phase line:1||Thermal activation:1||QUANTUMDOT:1||superconducting proximity effect:1||Andreev interferometer:1||WIRE:1||Josephsonvortexflow branches:1||Bi2212 cuprates:1||LATTICE:1||demannetization effect:1||SUPERCONDUCTING MIRRORS:1||GAS:1||VALLEY TRANSPORT:1||ELECTRODES:1||DEPENDENT TRANSPORT:1||BORNOPPENHEIMER APPROXIMATION:1||collective plasma oscillations:1||fluxon resonance steps:1||STACKS:1||COLLECTIVE DYNAMICS:1||PAIRING SYMMETRY:1||MUON SPIN ROTATION:1||DIMENSIONAL CROSSOVER:1||Bi2Sr2CaCu2Oy highTc superconductors:1||heterojunctions:1||nanostructures:1||surfaces and interfaces:1||QUANTUM TRANSPORT:1||MICROJUNCTIONS:1||RESONATORS:1||STATES:1||FIELD:1||FLUCTUATIONS:1||SCATTERING:1||mode splitting of Josephson vortexflow branches:1||2D superconductivity:1||TRANSISTOR:1||ENERGYGAP:1||SUPERLATTICES:1||IRONBASED SUPERCONDUCTORS:1||PHASEDEPENDENT RESISTANCE:1||QUANTUM PHASETRANSITIONS:1||ELECTRICFIELD:1||HIGH MAGNETICFIELDS:1||NANOWIRE HETEROSTRUCTURES:1||ZNO:1||pair breaking.:1||SUPERCONDUCTING PB:1||domain formation:1||FORCE MICROSCOPY:1||RELAXATION:1||PLASMA RESONANCE:1||coupled Josephson junctions:1||COPPEROXIDE SUPERCONDUCTORS:1||CROSSOVER:1||SIMULATIONS:1||LOWTEMPERATURE:1||CONDUCTORS:1||METALINSULATORTRANSITION:1||SEMICONDUCTOR:1||FIELDEFFECT TRANSISTORS:1||ZEROVOLTAGE STATE:1||constanttemperature interlayer tunneling spectroscopy:1||Josephson supercurrent:1||BIPOLAR SUPERCURRENT:1||Interaction between Josephson and pancake vortices:1||flux jump:1||coaxial heterojunction nanorod:1||Natural Josephson coupling:1||BI2SR2CACU2O8+DELTA:1||VORTEX FLOW:1||TC SUPERCONDUCTORS:1||charge imbalance:1||Andreev diffractometer:1||intercalation:1||surface junction:1||Bi2212:1||tunnelling:1||GRAPHITE:1||GROWTH:1||collective transverse plasma modes:1||GAN:1||Macroscopic quantum tunneling:1||Fluctuation conductivity:1||Abovegap conductance jump:1||Josephson vortex motion:1||Intrinsic Josephson junctions:1||LAYERED SUPERCONDUCTORS:1||BI2SR2CACU2O8+Y:1||INTERFACES:1||BREAKDOWN:1||SYSTEMS:1||Anisotropy ratio:1||Josephson vortex:1||spin relaxation in superconductors:1||bibased single crystals:1||MESOSCOPIC PROXIMITY SUPERCONDUCTOR:1||reentrance of conductance:1||interlayer pair tunneling:1||JOSEPHSON:1||DISORDERED 2DIMENSIONAL SUPERCONDUCTORS:1||INDIUM FILMS:1||excited state:1||REGIME:1||triplet superconductivity:1||FILM:1||SCHOTTKY DIODES:1||peakdiphump structure:1||Kondo effect:1||REENTRANCE:1||Graphene:1||CONTACT:1||BERRYS PHASE:1||2DIMENSIONAL SUPERCONDUCTORS:1||Coulomb diamond:1||magnetic domain:1||spin injection:1||RESONANCE:1||plasma excitation modes:1||FLOW:1||OVERDOPED BI2SR2CACU2O8+DELTA:1||hole doping:1||chemical synthesis:1||phase transitions:1||superconductors:1||VORTEXGLASS SUPERCONDUCTIVITY:1||Kondorelated model:1||RADIATION:1||DOT:1||NANOBELTS:1||Complementarity:1||Closedloop AharonovBohm interferometer:1||pair breaking:1||interlayer phase fluctuation:1||MgB2 thin film:1||CONFINEMENT:1||WALLED CARBON NANOTUBES:1||TRANSITION:9||VORTICES:8||STATE:7||intrinsic Josephson junctions:7||SINGLECRYSTALS:7||JUNCTIONS:5||MODES:5||SUPERCURRENT:5||SUPERCONDUCTOR:5||CONDUCTANCE:5||HIGHTEMPERATURE SUPERCONDUCTORS:5||TRANSPORT:5||PHASE:5||FILMS:4||LOCALIZATION:4||SINGLE DIRAC CONE:4||WIRES:4||MAGNETICFIELD:4||STEPS:3||ELECTRONS:3||proximity effect:3||MODEL:3||ARRAYS:3||INTERFERENCE:3||fluxon dynamics:3||HETEROSTRUCTURES:3||INSULATOR:3||Andreev reflection:3||electronic transport:3||FISKE:3||superconductor:2||ZnO:2||quantum point contact:2||METAL:2||DYNAMICS:2||interlayer Josephson coupling:2||SUPERCONDUCTORS:2||YBA2CU3O7DELTA:2||LAYER:2||DOTS:2||quantum dot:2||Article:2||TRANSISTORS:2||CARBON NANOTUBES:2||GAP:2||MECHANISM:2||LINE:2||GIANT SHAPIRO STEPS:2||LAYERS:2||electron energy loss spectroscopy:2||physical phenomena:2||scanning electron microscopy:2||HGTE QUANTUMWELLS:2||BI2TE3:2||SPECTROSCOPY:2||PNJUNCTIONS:2||spinpolarized tunneling:2||INTRINSIC JOSEPHSONJUNCTIONS:2||FIELDS:2||positive magnetoresistance:2||dilute magnetic semiconductor:2||magnetic field:2||scanning transmission electron microscopy:2||QUANTUM OSCILLATIONS:2||TRANSPORTPROPERTIES:2||surface pair current:2||MAGNETORESISTANCE:2||NANORIBBONS:2||INSTABILITY:2||ANDREEV REFLECTION:2||microwave irradiation:2||vertical graphene josephson junction:2||BI2SE3:2||CONDUCTIVITY:2||highTc superconductors:2||DIMENSIONAL ELECTRONGAS:2||graphene:2||Topological insulators:2||Josephson coupling Fraunhofer interference pattern:2||FERROMAGNET:2||DEPENDENCE:2||DETECTOR:2||COHERENCE:2||INJECTION:2||GRAPHENE:1||JOSEPHSONJUNCTIONS:1||LAYERED SUPERCONDUCTOR:1||mode splitting:1||BEHAVIOR:1||spinpolarized transport:1||SUPERCONDUCTING TRANSITION:1||microwave response:1||PSEUDOGAP:1||phase coherence:1||TRANSITIONS:1||Long Josephson junction:1||Charge detection:1||collective resonance modes:1||plasma oscillation modes:1||Superconducting proximity effect:1||Iron pnictide superconductor:1||McMillanRowell oscillations:1||ferromagnetic microstructure:1||superradiant state:1||VOLTAGE:1||branch splitting:1||TENSOR:1||INTERCALATION:1||insitu fabrication:1||NDGAO3:1||DISORDERED METALS:1||GAUGE GLASS:1||LOWTEMPERATURE TRANSPORT:1||spontaneous spin polarization model:1||BIAS:1||emission of electromagnetic waves:1||YBA2CU3O7/PRBA2CU3O7 SUPERLATTICES:1||BOHM:1||SHAPIRO STEPS:1||superconductor/ferromagnet interface:1||OXIDE:1||ANDREEVREFLECTION:1||SinFeAsO single crystal:1||COLLECTIVE MOTION:1||ANGULARDEPENDENCE:1||SUPERCONDUCTIVITY:1||BILAYER GRAPHENE:1||PHOTOLUMINESCENT PROPERTIES:1||SUPERCONDUCTING WEAK LINKS:1||intrinsic Josephson junctions geometrical resonance:1||intrinsic Josephson junction:1||MESOSCOPIC SPINVALVE:1||Bi2212 single crystals:1||intrinsic junctions:1||ANDREEV REFLECTIONS:1||normalmetal/superconductor interface:1||IBI2SR2CACU2OY:1||THERMAL FLUCTUATIONS:1||MIXED STATE:1||BI2.15SR1.85CACU2O8+DELTA:1||intrinsic Josephson effects:1||CACUO:1||QUANTUM POINT CONTACTS:1||resonant tunneling state:1||coherence length:1||NANOWIRE:1||GATES:1||Phase line:1||Thermal activation:1||QUANTUMDOT:1||superconducting proximity effect:1||Andreev interferometer:1||WIRE:1||Josephsonvortexflow branches:1||Bi2212 cuprates:1||LATTICE:1||demannetization effect:1||SUPERCONDUCTING MIRRORS:1||GAS:1||VALLEY TRANSPORT:1||ELECTRODES:1||DEPENDENT TRANSPORT:1||BORNOPPENHEIMER APPROXIMATION:1||collective plasma oscillations:1||fluxon resonance steps:1||STACKS:1||COLLECTIVE DYNAMICS:1||PAIRING SYMMETRY:1||MUON SPIN ROTATION:1||DIMENSIONAL CROSSOVER:1||Bi2Sr2CaCu2Oy highTc superconductors:1||heterojunctions:1||nanostructures:1||surfaces and interfaces:1||QUANTUM TRANSPORT:1||MICROJUNCTIONS:1||RESONATORS:1||STATES:1||FIELD:1||FLUCTUATIONS:1||SCATTERING:1||mode splitting of Josephson vortexflow branches:1||2D superconductivity:1||TRANSISTOR:1||ENERGYGAP:1||SUPERLATTICES:1||IRONBASED SUPERCONDUCTORS:1||PHASEDEPENDENT RESISTANCE:1||QUANTUM PHASETRANSITIONS:1||ELECTRICFIELD:1||HIGH MAGNETICFIELDS:1||NANOWIRE HETEROSTRUCTURES:1||ZNO:1||pair breaking.:1||SUPERCONDUCTING PB:1||domain formation:1||FORCE MICROSCOPY:1||RELAXATION:1||PLASMA RESONANCE:1||coupled Josephson junctions:1||COPPEROXIDE SUPERCONDUCTORS:1||CROSSOVER:1||SIMULATIONS:1||LOWTEMPERATURE:1||CONDUCTORS:1||METALINSULATORTRANSITION:1||SEMICONDUCTOR:1||FIELDEFFECT TRANSISTORS:1||ZEROVOLTAGE STATE:1||constanttemperature interlayer tunneling spectroscopy:1||Josephson supercurrent:1||BIPOLAR SUPERCURRENT:1||Interaction between Josephson and pancake vortices:1||flux jump:1||coaxial heterojunction nanorod:1||Natural Josephson coupling:1||BI2SR2CACU2O8+DELTA:1||VORTEX FLOW:1||TC SUPERCONDUCTORS:1||charge imbalance:1||Andreev diffractometer:1||intercalation:1||surface junction:1||Bi2212:1||tunnelling:1||GRAPHITE:1||GROWTH:1||collective transverse plasma modes:1||GAN:1||Macroscopic quantum tunneling:1||Fluctuation conductivity:1||Abovegap conductance jump:1||Josephson vortex motion:1||Intrinsic Josephson junctions:1||LAYERED SUPERCONDUCTORS:1||BI2SR2CACU2O8+Y:1||INTERFACES:1||BREAKDOWN:1||SYSTEMS:1||Anisotropy ratio:1||Josephson vortex:1||spin relaxation in superconductors:1||bibased single crystals:1||MESOSCOPIC PROXIMITY SUPERCONDUCTOR:1||reentrance of conductance:1||interlayer pair tunneling:1||JOSEPHSON:1||DISORDERED 2DIMENSIONAL SUPERCONDUCTORS:1||INDIUM FILMS:1||excited state:1||REGIME:1||triplet superconductivity:1||FILM:1||SCHOTTKY DIODES:1||peakdiphump structure:1||Kondo effect:1||REENTRANCE:1||Graphene:1||CONTACT:1||BERRYS PHASE:1||2DIMENSIONAL SUPERCONDUCTORS:1||Coulomb diamond:1||magnetic domain:1||spin injection:1||RESONANCE:1||plasma excitation modes:1||FLOW:1||OVERDOPED BI2SR2CACU2O8+DELTA:1||hole doping:1||chemical synthesis:1||phase transitions:1||superconductors:1||VORTEXGLASS SUPERCONDUCTIVITY:1||Kondorelated model:1||RADIATION:1||DOT:1||NANOBELTS:1||Complementarity:1||Closedloop AharonovBohm interferometer:1||pair breaking:1||interlayer phase fluctuation:1||MgB2 thin film:1||CONFINEMENT:1||WALLED CARBON NANOTUBES:1||TRANSITION:9||VORTICES:8||STATE:7||intrinsic Josephson junctions:7||SINGLECRYSTALS:7||JUNCTIONS:5||MODES:5||SUPERCURRENT:5||SUPERCONDUCTOR:5||CONDUCTANCE:5||HIGHTEMPERATURE SUPERCONDUCTORS:5||TRANSPORT:5||PHASE:5||FILMS:4||LOCALIZATION:4||SINGLE DIRAC CONE:4||WIRES:4||MAGNETICFIELD:4||STEPS:3||ELECTRONS:3||proximity effect:3||MODEL:3||ARRAYS:3||INTERFERENCE:3||fluxon dynamics:3||HETEROSTRUCTURES:3||INSULATOR:3||Andreev reflection:3||electronic transport:3||FISKE:3||superconductor:2||ZnO:2||quantum point contact:2||METAL:2||DYNAMICS:2||interlayer Josephson coupling:2||SUPERCONDUCTORS:2||YBA2CU3O7DELTA:2||LAYER:2||DOTS:2||quantum dot:2||Article:2||TRANSISTORS:2||CARBON NANOTUBES:2||GAP:2||MECHANISM:2||LINE:2||GIANT SHAPIRO STEPS:2||LAYERS:2||electron energy loss spectroscopy:2||physical phenomena:2||scanning electron microscopy:2||HGTE QUANTUMWELLS:2||BI2TE3:2||SPECTROSCOPY:2||PNJUNCTIONS:2||spinpolarized tunneling:2||INTRINSIC JOSEPHSONJUNCTIONS:2||FIELDS:2||positive magnetoresistance:2||dilute magnetic semiconductor:2||magnetic field:2||scanning transmission electron microscopy:2||QUANTUM OSCILLATIONS:2||TRANSPORTPROPERTIES:2||surface pair current:2||MAGNETORESISTANCE:2||NANORIBBONS:2||INSTABILITY:2||ANDREEV REFLECTION:2||microwave irradiation:2||vertical graphene josephson junction:2||BI2SE3:2||CONDUCTIVITY:2||highTc superconductors:2||DIMENSIONAL ELECTRONGAS:2||graphene:2||Topological insulators:2||Josephson coupling Fraunhofer interference pattern:2||FERROMAGNET:2||DEPENDENCE:2||DETECTOR:2||COHERENCE:2||INJECTION:2||GRAPHENE:1||JOSEPHSONJUNCTIONS:1||LAYERED SUPERCONDUCTOR:1||mode splitting:1||BEHAVIOR:1||spinpolarized transport:1||SUPERCONDUCTING TRANSITION:1||microwave response:1||PSEUDOGAP:1||phase coherence:1||TRANSITIONS:1||Long Josephson junction:1||Charge detection:1||collective resonance modes:1||plasma oscillation modes:1||Superconducting proximity effect:1||Iron pnictide superconductor:1||McMillanRowell oscillations:1||ferromagnetic microstructure:1||superradiant state:1||VOLTAGE:1||branch splitting:1||TENSOR:1||INTERCALATION:1||insitu fabrication:1||NDGAO3:1||DISORDERED METALS:1||GAUGE GLASS:1||LOWTEMPERATURE TRANSPORT:1||spontaneous spin polarization model:1||BIAS:1||emission of electromagnetic waves:1||YBA2CU3O7/PRBA2CU3O7 SUPERLATTICES:1||BOHM:1||SHAPIRO STEPS:1||superconductor/ferromagnet interface:1||OXIDE:1||ANDREEVREFLECTION:1||SinFeAsO single crystal:1||COLLECTIVE MOTION:1||ANGULARDEPENDENCE:1||SUPERCONDUCTIVITY:1||BILAYER GRAPHENE:1||PHOTOLUMINESCENT PROPERTIES:1||SUPERCONDUCTING WEAK LINKS:1||intrinsic Josephson junctions geometrical resonance:1||intrinsic Josephson junction:1||MESOSCOPIC SPINVALVE:1||Bi2212 single crystals:1||intrinsic junctions:1||ANDREEV REFLECTIONS:1||normalmetal/superconductor interface:1||IBI2SR2CACU2OY:1||THERMAL FLUCTUATIONS:1||MIXED STATE:1||BI2.15SR1.85CACU2O8+DELTA:1||intrinsic Josephson effects:1||CACUO:1||QUANTUM POINT CONTACTS:1||resonant tunneling state:1||coherence length:1||NANOWIRE:1||GATES:1||Phase line:1||Thermal activation:1||QUANTUMDOT:1||superconducting proximity effect:1||Andreev interferometer:1||WIRE:1||Josephsonvortexflow branches:1||Bi2212 cuprates:1||LATTICE:1||demannetization effect:1||SUPERCONDUCTING MIRRORS:1||GAS:1||VALLEY TRANSPORT:1||ELECTRODES:1||DEPENDENT TRANSPORT:1||BORNOPPENHEIMER APPROXIMATION:1||collective plasma oscillations:1||fluxon resonance steps:1||STACKS:1||COLLECTIVE DYNAMICS:1||PAIRING SYMMETRY:1||MUON SPIN ROTATION:1||DIMENSIONAL CROSSOVER:1||Bi2Sr2CaCu2Oy highTc superconductors:1||heterojunctions:1||nanostructures:1||surfaces and interfaces:1||QUANTUM TRANSPORT:1||MICROJUNCTIONS:1||RESONATORS:1||STATES:1||FIELD:1||FLUCTUATIONS:1||SCATTERING:1||mode splitting of Josephson vortexflow branches:1||2D superconductivity:1||TRANSISTOR:1||ENERGYGAP:1||SUPERLATTICES:1||IRONBASED SUPERCONDUCTORS:1||PHASEDEPENDENT RESISTANCE:1||QUANTUM PHASETRANSITIONS:1||ELECTRICFIELD:1||HIGH MAGNETICFIELDS:1||NANOWIRE HETEROSTRUCTURES:1||ZNO:1||pair breaking.:1||SUPERCONDUCTING PB:1||domain formation:1||FORCE MICROSCOPY:1||RELAXATION:1||PLASMA RESONANCE:1||coupled Josephson junctions:1||COPPEROXIDE SUPERCONDUCTORS:1||CROSSOVER:1||SIMULATIONS:1||LOWTEMPERATURE:1||CONDUCTORS:1||METALINSULATORTRANSITION:1||SEMICONDUCTOR:1||FIELDEFFECT TRANSISTORS:1||ZEROVOLTAGE STATE:1||constanttemperature interlayer tunneling spectroscopy:1||Josephson supercurrent:1||BIPOLAR SUPERCURRENT:1||Interaction between Josephson and pancake vortices:1||flux jump:1||coaxial heterojunction nanorod:1||Natural Josephson coupling:1||BI2SR2CACU2O8+DELTA:1||VORTEX FLOW:1||TC SUPERCONDUCTORS:1||charge imbalance:1||Andreev diffractometer:1||intercalation:1||surface junction:1||Bi2212:1||tunnelling:1||GRAPHITE:1||GROWTH:1||collective transverse plasma modes:1||GAN:1||Macroscopic quantum tunneling:1||Fluctuation conductivity:1||Abovegap conductance jump:1||Josephson vortex motion:1||Intrinsic Josephson junctions:1||LAYERED SUPERCONDUCTORS:1||BI2SR2CACU2O8+Y:1||INTERFACES:1||BREAKDOWN:1||SYSTEMS:1||Anisotropy ratio:1||Josephson vortex:1||spin relaxation in superconductors:1||bibased single crystals:1||MESOSCOPIC PROXIMITY SUPERCONDUCTOR:1||reentrance of conductance:1||interlayer pair tunneling:1||JOSEPHSON:1||DISORDERED 2DIMENSIONAL SUPERCONDUCTORS:1||INDIUM FILMS:1||excited state:1||REGIME:1||triplet superconductivity:1||FILM:1||SCHOTTKY DIODES:1||peakdiphump structure:1||Kondo effect:1||REENTRANCE:1||Graphene:1||CONTACT:1||BERRYS PHASE:1||2DIMENSIONAL SUPERCONDUCTORS:1||Coulomb diamond:1||magnetic domain:1||spin injection:1||RESONANCE:1||plasma excitation modes:1||FLOW:1||OVERDOPED BI2SR2CACU2O8+DELTA:1||hole doping:1||chemical synthesis:1||phase transitions:1||superconductors:1||VORTEXGLASS SUPERCONDUCTIVITY:1||Kondorelated model:1||RADIATION:1||DOT:1||NANOBELTS:1||Complementarity:1||Closedloop AharonovBohm interferometer:1||pair breaking:1||interlayer phase fluctuation:1||MgB2 thin film:1||CONFINEMENT:1||WALLED CARBON NANOTUBES:1||TRANSITION:9||VORTICES:8||STATE:7||intrinsic Josephson junctions:7||SINGLECRYSTALS:7||JUNCTIONS:5||MODES:5||SUPERCURRENT:5||SUPERCONDUCTOR:5||CONDUCTANCE:5||HIGHTEMPERATURE SUPERCONDUCTORS:5||TRANSPORT:5||PHASE:5||FILMS:4||LOCALIZATION:4||SINGLE DIRAC CONE:4||WIRES:4||MAGNETICFIELD:4||STEPS:3||ELECTRONS:3||proximity effect:3||MODEL:3||ARRAYS:3||INTERFERENCE:3||fluxon dynamics:3||HETEROSTRUCTURES:3||INSULATOR:3||Andreev reflection:3||electronic transport:3||FISKE:3||superconductor:2||ZnO:2||quantum point contact:2||METAL:2||DYNAMICS:2||interlayer Josephson coupling:2||SUPERCONDUCTORS:2||YBA2CU3O7DELTA:2||LAYER:2||DOTS:2||quantum dot:2||Article:2||TRANSISTORS:2||CARBON NANOTUBES:2||GAP:2||MECHANISM:2||LINE:2||GIANT SHAPIRO STEPS:2||LAYERS:2||electron energy loss spectroscopy:2||physical phenomena:2||scanning electron microscopy:2||HGTE QUANTUMWELLS:2||BI2TE3:2||SPECTROSCOPY:2||PNJUNCTIONS:2||spinpolarized tunneling:2||INTRINSIC JOSEPHSONJUNCTIONS:2||FIELDS:2||positive magnetoresistance:2||dilute magnetic semiconductor:2||magnetic field:2||scanning transmission electron microscopy:2||QUANTUM OSCILLATIONS:2||TRANSPORTPROPERTIES:2||surface pair current:2||MAGNETORESISTANCE:2||NANORIBBONS:2||INSTABILITY:2||ANDREEV REFLECTION:2||microwave irradiation:2||vertical graphene josephson junction:2||BI2SE3:2||CONDUCTIVITY:2||highTc superconductors:2||DIMENSIONAL ELECTRONGAS:2||graphene:2||Topological insulators:2||Josephson coupling Fraunhofer interference pattern:2||FERROMAGNET:2||DEPENDENCE:2||DETECTOR:2||COHERENCE:2||INJECTION:2||GRAPHENE:1||JOSEPHSONJUNCTIONS:1||LAYERED SUPERCONDUCTOR:1||mode splitting:1||BEHAVIOR:1||spinpolarized transport:1||SUPERCONDUCTING TRANSITION:1||microwave response:1||PSEUDOGAP:1||phase coherence:1||TRANSITIONS:1||Long Josephson junction:1||Charge detection:1||collective resonance modes:1||plasma oscillation modes:1||Superconducting proximity effect:1||Iron pnictide superconductor:1||McMillanRowell oscillations:1||ferromagnetic microstructure:1||superradiant state:1||VOLTAGE:1||branch splitting:1||TENSOR:1||INTERCALATION:1||insitu fabrication:1||NDGAO3:1||DISORDERED METALS:1||GAUGE GLASS:1||LOWTEMPERATURE TRANSPORT:1||spontaneous spin polarization model:1||BIAS:1||emission of electromagnetic waves:1||YBA2CU3O7/PRBA2CU3O7 SUPERLATTICES:1||BOHM:1||SHAPIRO STEPS:1||superconductor/ferromagnet interface:1||OXIDE:1||ANDREEVREFLECTION:1||SinFeAsO single crystal:1||COLLECTIVE MOTION:1||ANGULARDEPENDENCE:1||SUPERCONDUCTIVITY:1||BILAYER GRAPHENE:1||PHOTOLUMINESCENT PROPERTIES:1||SUPERCONDUCTING WEAK LINKS:1||intrinsic Josephson junctions geometrical resonance:1||intrinsic Josephson junction:1||MESOSCOPIC SPINVALVE:1||Bi2212 single crystals:1||intrinsic junctions:1||ANDREEV REFLECTIONS:1||normalmetal/superconductor interface:1||IBI2SR2CACU2OY:1||THERMAL FLUCTUATIONS:1||MIXED STATE:1||BI2.15SR1.85CACU2O8+DELTA:1||intrinsic Josephson effects:1||CACUO:1||QUANTUM POINT CONTACTS:1||resonant tunneling state:1||coherence length:1||NANOWIRE:1||GATES:1||Phase line:1||Thermal activation:1||QUANTUMDOT:1||superconducting proximity effect:1||Andreev interferometer:1||WIRE:1||Josephsonvortexflow branches:1||Bi2212 cuprates:1||LATTICE:1||demannetization effect:1||SUPERCONDUCTING MIRRORS:1||GAS:1||VALLEY TRANSPORT:1||ELECTRODES:1||DEPENDENT TRANSPORT:1||BORNOPPENHEIMER APPROXIMATION:1||collective plasma oscillations:1||fluxon resonance steps:1||STACKS:1||COLLECTIVE DYNAMICS:1||PAIRING SYMMETRY:1||MUON SPIN ROTATION:1||DIMENSIONAL CROSSOVER:1||Bi2Sr2CaCu2Oy highTc superconductors:1||heterojunctions:1||nanostructures:1||surfaces and interfaces:1||QUANTUM TRANSPORT:1||MICROJUNCTIONS:1||RESONATORS:1||STATES:1||FIELD:1||FLUCTUATIONS:1||SCATTERING:1||mode splitting of Josephson vortexflow branches:1||2D superconductivity:1||TRANSISTOR:1||ENERGYGAP:1||SUPERLATTICES:1||IRONBASED SUPERCONDUCTORS:1||PHASEDEPENDENT RESISTANCE:1||QUANTUM PHASETRANSITIONS:1||ELECTRICFIELD:1||HIGH MAGNETICFIELDS:1||NANOWIRE HETEROSTRUCTURES:1||ZNO:1||pair breaking.:1||SUPERCONDUCTING PB:1||domain formation:1||FORCE MICROSCOPY:1||RELAXATION:1||PLASMA RESONANCE:1||coupled Josephson junctions:1||COPPEROXIDE SUPERCONDUCTORS:1||CROSSOVER:1||SIMULATIONS:1||LOWTEMPERATURE:1||CONDUCTORS:1||METALINSULATORTRANSITION:1||SEMICONDUCTOR:1||FIELDEFFECT TRANSISTORS:1||ZEROVOLTAGE STATE:1||constanttemperature interlayer tunneling spectroscopy:1||Josephson supercurrent:1||BIPOLAR SUPERCURRENT:1||Interaction between Josephson and pancake vortices:1||flux jump:1||coaxial heterojunction nanorod:1||Natural Josephson coupling:1||BI2SR2CACU2O8+DELTA:1||VORTEX FLOW:1||TC SUPERCONDUCTORS:1||charge imbalance:1||Andreev diffractometer:1||intercalation:1||surface junction:1||Bi2212:1||tunnelling:1||GRAPHITE:1||GROWTH:1||collective transverse plasma modes:1||GAN:1||Macroscopic quantum tunneling:1||Fluctuation conductivity:1||Abovegap conductance jump:1||Josephson vortex motion:1||Intrinsic Josephson junctions:1||LAYERED SUPERCONDUCTORS:1||BI2SR2CACU2O8+Y:1||INTERFACES:1||BREAKDOWN:1||SYSTEMS:1||Anisotropy ratio:1||Josephson vortex:1||spin relaxation in superconductors:1||bibased single crystals:1||MESOSCOPIC PROXIMITY SUPERCONDUCTOR:1||reentrance of conductance:1||interlayer pair tunneling:1||JOSEPHSON:1||DISORDERED 2DIMENSIONAL SUPERCONDUCTORS:1||INDIUM FILMS:1||excited state:1||REGIME:1||triplet superconductivity:1||FILM:1||SCHOTTKY DIODES:1||peakdiphump structure:1||Kondo effect:1||REENTRANCE:1||Graphene:1||CONTACT:1||BERRYS PHASE:1||2DIMENSIONAL SUPERCONDUCTORS:1||Coulomb diamond:1||magnetic domain:1||spin injection:1||RESONANCE:1||plasma excitation modes:1||FLOW:1||OVERDOPED BI2SR2CACU2O8+DELTA:1||hole doping:1||chemical synthesis:1||phase transitions:1||superconductors:1||VORTEXGLASS SUPERCONDUCTIVITY:1||Kondorelated model:1||RADIATION:1||DOT:1||NANOBELTS:1||Complementarity:1||Closedloop AharonovBohm interferometer:1||pair breaking:1||interlayer phase fluctuation:1||MgB2 thin film:1||CONFINEMENT:1||WALLED CARBON NANOTUBES:1||TRANSITION:9||VORTICES:8||STATE:7||intrinsic Josephson junctions:7||SINGLECRYSTALS:7||JUNCTIONS:5||MODES:5||SUPERCURRENT:5||SUPERCONDUCTOR:5||CONDUCTANCE:5||HIGHTEMPERATURE SUPERCONDUCTORS:5||TRANSPORT:5||PHASE:5||FILMS:4||LOCALIZATION:4||SINGLE DIRAC CONE:4||WIRES:4||MAGNETICFIELD:4||STEPS:3||ELECTRONS:3||proximity effect:3||MODEL:3||ARRAYS:3||INTERFERENCE:3||fluxon dynamics:3||HETEROSTRUCTURES:3||INSULATOR:3||Andreev reflection:3||electronic transport:3||FISKE:3||superconductor:2||ZnO:2||quantum point contact:2||METAL:2||DYNAMICS:2||interlayer Josephson coupling:2||SUPERCONDUCTORS:2||YBA2CU3O7DELTA:2||LAYER:2||DOTS:2||quantum dot:2||Article:2||TRANSISTORS:2||CARBON NANOTUBES:2||GAP:2||MECHANISM:2||LINE:2||GIANT SHAPIRO STEPS:2||LAYERS:2||electron energy loss spectroscopy:2||physical phenomena:2||scanning electron microscopy:2||HGTE QUANTUMWELLS:2||BI2TE3:2||SPECTROSCOPY:2||PNJUNCTIONS:2||spinpolarized tunneling:2||INTRINSIC JOSEPHSONJUNCTIONS:2||FIELDS:2||positive magnetoresistance:2||dilute magnetic semiconductor:2||magnetic field:2||scanning transmission electron microscopy:2||QUANTUM OSCILLATIONS:2||TRANSPORTPROPERTIES:2||surface pair current:2||MAGNETORESISTANCE:2||NANORIBBONS:2||INSTABILITY:2||ANDREEV REFLECTION:2||microwave irradiation:2||vertical graphene josephson junction:2||BI2SE3:2||CONDUCTIVITY:2||highTc superconductors:2||DIMENSIONAL ELECTRONGAS:2||graphene:2||Topological insulators:2||Josephson coupling Fraunhofer interference pattern:2||FERROMAGNET:2||DEPENDENCE:2||DETECTOR:2||COHERENCE:2||INJECTION:2||GRAPHENE:1||JOSEPHSONJUNCTIONS:1||LAYERED SUPERCONDUCTOR:1||mode splitting:1||BEHAVIOR:1||spinpolarized transport:1||SUPERCONDUCTING TRANSITION:1||microwave response:1||PSEUDOGAP:1||phase coherence:1||TRANSITIONS:1||Long Josephson junction:1||Charge detection:1||collective resonance modes:1||plasma oscillation modes:1||Superconducting proximity effect:1||Iron pnictide superconductor:1||McMillanRowell oscillations:1||ferromagnetic microstructure:1||superradiant state:1||VOLTAGE:1||branch splitting:1||TENSOR:1||INTERCALATION:1||insitu fabrication:1||NDGAO3:1||DISORDERED METALS:1||GAUGE GLASS:1||LOWTEMPERATURE TRANSPORT:1||spontaneous spin polarization model:1||BIAS:1||emission of electromagnetic waves:1||YBA2CU3O7/PRBA2CU3O7 SUPERLATTICES:1||BOHM:1||SHAPIRO STEPS:1||superconductor/ferromagnet interface:1||OXIDE:1||ANDREEVREFLECTION:1||SinFeAsO single crystal:1||COLLECTIVE MOTION:1||ANGULARDEPENDENCE:1||SUPERCONDUCTIVITY:1||BILAYER GRAPHENE:1||PHOTOLUMINESCENT PROPERTIES:1||SUPERCONDUCTING WEAK LINKS:1||intrinsic Josephson junctions geometrical resonance:1||intrinsic Josephson junction:1||MESOSCOPIC SPINVALVE:1||Bi2212 single crystals:1||intrinsic junctions:1||ANDREEV REFLECTIONS:1||normalmetal/superconductor interface:1||IBI2SR2CACU2OY:1||THERMAL FLUCTUATIONS:1||MIXED STATE:1||BI2.15SR1.85CACU2O8+DELTA:1||intrinsic Josephson effects:1||CACUO:1||QUANTUM POINT CONTACTS:1||resonant tunneling state:1||coherence length:1||NANOWIRE:1||GATES:1||Phase line:1||Thermal activation:1||QUANTUMDOT:1||superconducting proximity effect:1||Andreev interferometer:1||WIRE:1||Josephsonvortexflow branches:1||Bi2212 cuprates:1||LATTICE:1||demannetization effect:1||SUPERCONDUCTING MIRRORS:1||GAS:1||VALLEY TRANSPORT:1||ELECTRODES:1||DEPENDENT TRANSPORT:1||BORNOPPENHEIMER APPROXIMATION:1||collective plasma oscillations:1||fluxon resonance steps:1||STACKS:1||COLLECTIVE DYNAMICS:1||PAIRING SYMMETRY:1||MUON SPIN ROTATION:1||DIMENSIONAL CROSSOVER:1||Bi2Sr2CaCu2Oy highTc superconductors:1||heterojunctions:1||nanostructures:1||surfaces and interfaces:1||QUANTUM TRANSPORT:1||MICROJUNCTIONS:1||RESONATORS:1||STATES:1||FIELD:1||FLUCTUATIONS:1||SCATTERING:1||mode splitting of Josephson vortexflow branches:1||2D superconductivity:1||TRANSISTOR:1||ENERGYGAP:1||SUPERLATTICES:1||IRONBASED SUPERCONDUCTORS:1||PHASEDEPENDENT RESISTANCE:1||QUANTUM PHASETRANSITIONS:1||ELECTRICFIELD:1||HIGH MAGNETICFIELDS:1||NANOWIRE HETEROSTRUCTURES:1||ZNO:1||pair breaking.:1||SUPERCONDUCTING PB:1||domain formation:1||FORCE MICROSCOPY:1||RELAXATION:1||PLASMA RESONANCE:1||coupled Josephson junctions:1||COPPEROXIDE SUPERCONDUCTORS:1||CROSSOVER:1||SIMULATIONS:1||LOWTEMPERATURE:1||CONDUCTORS:1||METALINSULATORTRANSITION:1||SEMICONDUCTOR:1||FIELDEFFECT TRANSISTORS:1||ZEROVOLTAGE STATE:1||constanttemperature interlayer tunneling spectroscopy:1||Josephson supercurrent:1||BIPOLAR SUPERCURRENT:1||Interaction between Josephson and pancake vortices:1||flux jump:1||coaxial heterojunction nanorod:1||Natural Josephson coupling:1||BI2SR2CACU2O8+DELTA:1||VORTEX FLOW:1||TC SUPERCONDUCTORS:1||charge imbalance:1||Andreev diffractometer:1||intercalation:1||surface junction:1||Bi2212:1||tunnelling:1||GRAPHITE:1||GROWTH:1||collective transverse plasma modes:1||GAN:1||Macroscopic quantum tunneling:1||Fluctuation conductivity:1||Abovegap conductance jump:1||Josephson vortex motion:1||Intrinsic Josephson junctions:1||LAYERED SUPERCONDUCTORS:1||BI2SR2CACU2O8+Y:1||INTERFACES:1||BREAKDOWN:1||SYSTEMS:1||Anisotropy ratio:1||Josephson vortex:1||spin relaxation in superconductors:1||bibased single crystals:1||MESOSCOPIC PROXIMITY SUPERCONDUCTOR:1||reentrance of conductance:1||interlayer pair tunneling:1||JOSEPHSON:1||DISORDERED 2DIMENSIONAL SUPERCONDUCTORS:1||INDIUM FILMS:1||excited state:1||REGIME:1||triplet superconductivity:1||FILM:1||SCHOTTKY DIODES:1||peakdiphump structure:1||Kondo effect:1||REENTRANCE:1||Graphene:1||CONTACT:1||BERRYS PHASE:1||2DIMENSIONAL SUPERCONDUCTORS:1||Coulomb diamond:1||magnetic domain:1||spin injection:1||RESONANCE:1||plasma excitation modes:1||FLOW:1||OVERDOPED BI2SR2CACU2O8+DELTA:1||hole doping:1||chemical synthesis:1||phase transitions:1||superconductors:1||VORTEXGLASS SUPERCONDUCTIVITY:1||Kondorelated model:1||RADIATION:1||DOT:1||NANOBELTS:1||Complementarity:1||Closedloop AharonovBohm interferometer:1||pair breaking:1||interlayer phase fluctuation:1||MgB2 thin film:1||CONFINEMENT:1||WALLED CARBON NANOTUBES:1||TRANSITION:9||VORTICES:8||STATE:7||intrinsic Josephson junctions:7||SINGLECRYSTALS:7||JUNCTIONS:5||MODES:5||SUPERCURRENT:5||SUPERCONDUCTOR:5||CONDUCTANCE:5||HIGHTEMPERATURE SUPERCONDUCTORS:5||TRANSPORT:5||PHASE:5||FILMS:4||LOCALIZATION:4||SINGLE DIRAC CONE:4||WIRES:4||MAGNETICFIELD:4||STEPS:3||ELECTRONS:3||proximity effect:3||MODEL:3||ARRAYS:3||INTERFERENCE:3||fluxon dynamics:3||HETEROSTRUCTURES:3||INSULATOR:3||Andreev reflection:3||electronic transport:3||FISKE:3||superconductor:2||ZnO:2||quantum point contact:2||METAL:2||DYNAMICS:2||interlayer Josephson coupling:2||SUPERCONDUCTORS:2||YBA2CU3O7DELTA:2||LAYER:2||DOTS:2||quantum dot:2||Article:2||TRANSISTORS:2||CARBON NANOTUBES:2||GAP:2||MECHANISM:2||LINE:2||GIANT SHAPIRO STEPS:2||LAYERS:2||electron energy loss spectroscopy:2||physical phenomena:2||scanning electron microscopy:2||HGTE QUANTUMWELLS:2||BI2TE3:2||SPECTROSCOPY:2||PNJUNCTIONS:2||spinpolarized tunneling:2||INTRINSIC JOSEPHSONJUNCTIONS:2||FIELDS:2||positive magnetoresistance:2||dilute magnetic semiconductor:2||magnetic field:2||scanning transmission electron microscopy:2||QUANTUM OSCILLATIONS:2||TRANSPORTPROPERTIES:2||surface pair current:2||MAGNETORESISTANCE:2||NANORIBBONS:2||INSTABILITY:2||ANDREEV REFLECTION:2||microwave irradiation:2||vertical graphene josephson junction:2||BI2SE3:2||CONDUCTIVITY:2||highTc superconductors:2||DIMENSIONAL ELECTRONGAS:2||graphene:2||Topological insulators:2||Josephson coupling Fraunhofer interference pattern:2||FERROMAGNET:2||DEPENDENCE:2||DETECTOR:2||COHERENCE:2||INJECTION:2||GRAPHENE:1||JOSEPHSONJUNCTIONS:1||LAYERED SUPERCONDUCTOR:1||mode splitting:1||BEHAVIOR:1||spinpolarized transport:1||SUPERCONDUCTING TRANSITION:1||microwave response:1||PSEUDOGAP:1||phase coherence:1||TRANSITIONS:1||Long Josephson junction:1||Charge detection:1||collective resonance modes:1||plasma oscillation modes:1||Superconducting proximity effect:1||Iron pnictide superconductor:1||McMillanRowell oscillations:1||ferromagnetic microstructure:1||superradiant state:1||VOLTAGE:1||branch splitting:1||TENSOR:1||INTERCALATION:1||insitu fabrication:1||NDGAO3:1||DISORDERED METALS:1||GAUGE GLASS:1||LOWTEMPERATURE TRANSPORT:1||spontaneous spin polarization model:1||BIAS:1||emission of electromagnetic waves:1||YBA2CU3O7/PRBA2CU3O7 SUPERLATTICES:1||BOHM:1||SHAPIRO STEPS:1||superconductor/ferromagnet interface:1||OXIDE:1||ANDREEVREFLECTION:1||SinFeAsO single crystal:1||COLLECTIVE MOTION:1||ANGULARDEPENDENCE:1||SUPERCONDUCTIVITY:1||BILAYER GRAPHENE:1||PHOTOLUMINESCENT PROPERTIES:1||SUPERCONDUCTING WEAK LINKS:1||intrinsic Josephson junctions geometrical resonance:1||intrinsic Josephson junction:1||MESOSCOPIC SPINVALVE:1||Bi2212 single crystals:1||intrinsic junctions:1||ANDREEV REFLECTIONS:1||normalmetal/superconductor interface:1||IBI2SR2CACU2OY:1||THERMAL FLUCTUATIONS:1||MIXED STATE:1||BI2.15SR1.85CACU2O8+DELTA:1||intrinsic Josephson effects:1||CACUO:1||QUANTUM POINT CONTACTS:1||resonant tunneling state:1||coherence length:1||NANOWIRE:1||GATES:1||Phase line:1||Thermal activation:1||QUANTUMDOT:1||superconducting proximity effect:1||Andreev interferometer:1||WIRE:1||Josephsonvortexflow branches:1||Bi2212 cuprates:1||LATTICE:1||demannetization effect:1||SUPERCONDUCTING MIRRORS:1||GAS:1||VALLEY TRANSPORT:1||ELECTRODES:1||DEPENDENT TRANSPORT:1||BORNOPPENHEIMER APPROXIMATION:1||collective plasma oscillations:1||fluxon resonance steps:1||STACKS:1||COLLECTIVE DYNAMICS:1||PAIRING SYMMETRY:1||MUON SPIN ROTATION:1||DIMENSIONAL CROSSOVER:1||Bi2Sr2CaCu2Oy highTc superconductors:1||heterojunctions:1||nanostructures:1||surfaces and interfaces:1||QUANTUM TRANSPORT:1||MICROJUNCTIONS:1||RESONATORS:1||STATES:1||FIELD:1||FLUCTUATIONS:1||SCATTERING:1||mode splitting of Josephson vortexflow branches:1||2D superconductivity:1||TRANSISTOR:1||ENERGYGAP:1||SUPERLATTICES:1||IRONBASED SUPERCONDUCTORS:1||PHASEDEPENDENT RESISTANCE:1||QUANTUM PHASETRANSITIONS:1||ELECTRICFIELD:1||HIGH MAGNETICFIELDS:1||NANOWIRE HETEROSTRUCTURES:1||ZNO:1||pair breaking.:1||SUPERCONDUCTING PB:1||domain formation:1||FORCE MICROSCOPY:1||RELAXATION:1||PLASMA RESONANCE:1||coupled Josephson junctions:1||COPPEROXIDE SUPERCONDUCTORS:1||CROSSOVER:1||SIMULATIONS:1||LOWTEMPERATURE:1||CONDUCTORS:1||METALINSULATORTRANSITION:1||SEMICONDUCTOR:1||FIELDEFFECT TRANSISTORS:1||ZEROVOLTAGE STATE:1||constanttemperature interlayer tunneling spectroscopy:1||Josephson supercurrent:1||BIPOLAR SUPERCURRENT:1||Interaction between Josephson and pancake vortices:1||flux jump:1||coaxial heterojunction nanorod:1||Natural Josephson coupling:1||BI2SR2CACU2O8+DELTA:1||VORTEX FLOW:1||TC SUPERCONDUCTORS:1||charge imbalance:1||Andreev diffractometer:1||intercalation:1||surface junction:1||Bi2212:1||tunnelling:1||GRAPHITE:1||GROWTH:1||collective transverse plasma modes:1||GAN:1||Macroscopic quantum tunneling:1||Fluctuation conductivity:1||Abovegap conductance jump:1||Josephson vortex motion:1||Intrinsic Josephson junctions:1||LAYERED SUPERCONDUCTORS:1||BI2SR2CACU2O8+Y:1||INTERFACES:1||BREAKDOWN:1||SYSTEMS:1||Anisotropy ratio:1||Josephson vortex:1||spin relaxation in superconductors:1||bibased single crystals:1||MESOSCOPIC PROXIMITY SUPERCONDUCTOR:1||reentrance of conductance:1||interlayer pair tunneling:1||JOSEPHSON:1||DISORDERED 2DIMENSIONAL SUPERCONDUCTORS:1||INDIUM FILMS:1||excited state:1||REGIME:1||triplet superconductivity:1||FILM:1||SCHOTTKY DIODES:1||peakdiphump structure:1||Kondo effect:1||REENTRANCE:1||Graphene:1||CONTACT:1||BERRYS PHASE:1||2DIMENSIONAL SUPERCONDUCTORS:1||Coulomb diamond:1||magnetic domain:1||spin injection:1||RESONANCE:1||plasma excitation modes:1||FLOW:1||OVERDOPED BI2SR2CACU2O8+DELTA:1||hole doping:1||chemical synthesis:1||phase transitions:1||superconductors:1||VORTEXGLASS SUPERCONDUCTIVITY:1||Kondorelated model:1||RADIATION:1||DOT:1||NANOBELTS:1||Complementarity:1||Closedloop AharonovBohm interferometer:1||pair breaking:1||interlayer phase fluctuation:1||MgB2 thin film:1||CONFINEMENT:1||WALLED CARBON NANOTUBES:1||TRANSITION:9||VORTICES:8||STATE:7||intrinsic Josephson junctions:7||SINGLECRYSTALS:7||JUNCTIONS:5||MODES:5||SUPERCURRENT:5||SUPERCONDUCTOR:5||CONDUCTANCE:5||HIGHTEMPERATURE SUPERCONDUCTORS:5||TRANSPORT:5||PHASE:5||FILMS:4||LOCALIZATION:4||SINGLE DIRAC CONE:4||WIRES:4||MAGNETICFIELD:4||STEPS:3||ELECTRONS:3||proximity effect:3||MODEL:3||ARRAYS:3||INTERFERENCE:3||fluxon dynamics:3||HETEROSTRUCTURES:3||INSULATOR:3||Andreev reflection:3||electronic transport:3||FISKE:3||superconductor:2||ZnO:2||quantum point contact:2||METAL:2||DYNAMICS:2||interlayer Josephson coupling:2||SUPERCONDUCTORS:2||YBA2CU3O7DELTA:2||LAYER:2||DOTS:2||quantum dot:2||Article:2||TRANSISTORS:2||CARBON NANOTUBES:2||GAP:2||MECHANISM:2||LINE:2||GIANT SHAPIRO STEPS:2||LAYERS:2||electron energy loss spectroscopy:2||physical phenomena:2||scanning electron microscopy:2||HGTE QUANTUMWELLS:2||BI2TE3:2||SPECTROSCOPY:2||PNJUNCTIONS:2||spinpolarized tunneling:2||INTRINSIC JOSEPHSONJUNCTIONS:2||FIELDS:2||positive magnetoresistance:2||dilute magnetic semiconductor:2||magnetic field:2||scanning transmission electron microscopy:2||QUANTUM OSCILLATIONS:2||TRANSPORTPROPERTIES:2||surface pair current:2||MAGNETORESISTANCE:2||NANORIBBONS:2||INSTABILITY:2||ANDREEV REFLECTION:2||microwave irradiation:2||vertical graphene josephson junction:2||BI2SE3:2||CONDUCTIVITY:2||highTc superconductors:2||DIMENSIONAL ELECTRONGAS:2||graphene:2||Topological insulators:2||Josephson coupling Fraunhofer interference pattern:2||FERROMAGNET:2||DEPENDENCE:2||DETECTOR:2||COHERENCE:2||INJECTION:2||GRAPHENE:1||JOSEPHSONJUNCTIONS:1||LAYERED SUPERCONDUCTOR:1||mode splitting:1||BEHAVIOR:1||spinpolarized transport:1||SUPERCONDUCTING TRANSITION:1||microwave response:1||PSEUDOGAP:1||phase coherence:1||TRANSITIONS:1||Long Josephson junction:1||Charge detection:1||collective resonance modes:1||plasma oscillation modes:1||Superconducting proximity effect:1||Iron pnictide superconductor:1||McMillanRowell oscillations:1||ferromagnetic microstructure:1||superradiant state:1||VOLTAGE:1||branch splitting:1||TENSOR:1||INTERCALATION:1||insitu fabrication:1||NDGAO3:1||DISORDERED METALS:1||GAUGE GLASS:1||LOWTEMPERATURE TRANSPORT:1||spontaneous spin polarization model:1||BIAS:1||emission of electromagnetic waves:1||YBA2CU3O7/PRBA2CU3O7 SUPERLATTICES:1||BOHM:1||SHAPIRO STEPS:1||superconductor/ferromagnet interface:1||OXIDE:1||ANDREEVREFLECTION:1||SinFeAsO single crystal:1||COLLECTIVE MOTION:1||ANGULARDEPENDENCE:1||SUPERCONDUCTIVITY:1||BILAYER GRAPHENE:1||PHOTOLUMINESCENT PROPERTIES:1||SUPERCONDUCTING WEAK LINKS:1||intrinsic Josephson junctions geometrical resonance:1||intrinsic Josephson junction:1||MESOSCOPIC SPINVALVE:1||Bi2212 single crystals:1||intrinsic junctions:1||ANDREEV REFLECTIONS:1||normalmetal/superconductor interface:1||IBI2SR2CACU2OY:1||THERMAL FLUCTUATIONS:1||MIXED STATE:1||BI2.15SR1.85CACU2O8+DELTA:1||intrinsic Josephson effects:1||CACUO:1||QUANTUM POINT CONTACTS:1||resonant tunneling state:1||coherence length:1||NANOWIRE:1||GATES:1||Phase line:1||Thermal activation:1||QUANTUMDOT:1||superconducting proximity effect:1||Andreev interferometer:1||WIRE:1||Josephsonvortexflow branches:1||Bi2212 cuprates:1||LATTICE:1||demannetization effect:1||SUPERCONDUCTING MIRRORS:1||GAS:1||VALLEY TRANSPORT:1||ELECTRODES:1||DEPENDENT TRANSPORT:1||BORNOPPENHEIMER APPROXIMATION:1||collective plasma oscillations:1||fluxon resonance steps:1||STACKS:1||COLLECTIVE DYNAMICS:1||PAIRING SYMMETRY:1||MUON SPIN ROTATION:1||DIMENSIONAL CROSSOVER:1||Bi2Sr2CaCu2Oy highTc superconductors:1||heterojunctions:1||nanostructures:1||surfaces and interfaces:1||QUANTUM TRANSPORT:1||MICROJUNCTIONS:1||RESONATORS:1||STATES:1||FIELD:1||FLUCTUATIONS:1||SCATTERING:1||mode splitting of Josephson vortexflow branches:1||2D superconductivity:1||TRANSISTOR:1||ENERGYGAP:1||SUPERLATTICES:1||IRONBASED SUPERCONDUCTORS:1||PHASEDEPENDENT RESISTANCE:1||QUANTUM PHASETRANSITIONS:1||ELECTRICFIELD:1||HIGH MAGNETICFIELDS:1||NANOWIRE HETEROSTRUCTURES:1||ZNO:1||pair breaking.:1||SUPERCONDUCTING PB:1||domain formation:1||FORCE MICROSCOPY:1||RELAXATION:1||PLASMA RESONANCE:1||coupled Josephson junctions:1||COPPEROXIDE SUPERCONDUCTORS:1||CROSSOVER:1||SIMULATIONS:1||LOWTEMPERATURE:1||CONDUCTORS:1||METALINSULATORTRANSITION:1||SEMICONDUCTOR:1||FIELDEFFECT TRANSISTORS:1||ZEROVOLTAGE STATE:1||constanttemperature interlayer tunneling spectroscopy:1||Josephson supercurrent:1||BIPOLAR SUPERCURRENT:1||Interaction between Josephson and pancake vortices:1||flux jump:1||coaxial heterojunction nanorod:1||Natural Josephson coupling:1||BI2SR2CACU2O8+DELTA:1||VORTEX FLOW:1||TC SUPERCONDUCTORS:1||charge imbalance:1||Andreev diffractometer:1||intercalation:1||surface junction:1||Bi2212:1||tunnelling:1||GRAPHITE:1||GROWTH:1||collective transverse plasma modes:1||GAN:1||Macroscopic quantum tunneling:1||Fluctuation conductivity:1||Abovegap conductance jump:1||Josephson vortex motion:1||Intrinsic Josephson junctions:1||LAYERED SUPERCONDUCTORS:1||BI2SR2CACU2O8+Y:1||INTERFACES:1||BREAKDOWN:1||SYSTEMS:1||Anisotropy ratio:1||Josephson vortex:1||spin relaxation in superconductors:1||bibased single crystals:1||MESOSCOPIC PROXIMITY SUPERCONDUCTOR:1||reentrance of conductance:1||interlayer pair tunneling:1||JOSEPHSON:1||DISORDERED 2DIMENSIONAL SUPERCONDUCTORS:1||INDIUM FILMS:1||excited state:1||REGIME:1||triplet superconductivity:1||FILM:1||SCHOTTKY DIODES:1||peakdiphump structure:1||Kondo effect:1||REENTRANCE:1||Graphene:1||CONTACT:1||BERRYS PHASE:1||2DIMENSIONAL SUPERCONDUCTORS:1||Coulomb diamond:1||magnetic domain:1||spin injection:1||RESONANCE:1||plasma excitation modes:1||FLOW:1||OVERDOPED BI2SR2CACU2O8+DELTA:1||hole doping:1||chemical synthesis:1||phase transitions:1||superconductors:1||VORTEXGLASS SUPERCONDUCTIVITY:1||Kondorelated model:1||RADIATION:1||DOT:1||NANOBELTS:1||Complementarity:1||Closedloop AharonovBohm interferometer:1||pair breaking:1||interlayer phase fluctuation:1||MgB2 thin film:1||CONFINEMENT:1||WALLED CARBON NANOTUBES:1||TRANSITION:9||VORTICES:8||STATE:7||intrinsic Josephson junctions:7||SINGLECRYSTALS:7||JUNCTIONS:5||MODES:5||SUPERCURRENT:5||SUPERCONDUCTOR:5||CONDUCTANCE:5||HIGHTEMPERATURE SUPERCONDUCTORS:5||TRANSPORT:5||PHASE:5||FILMS:4||LOCALIZATION:4||SINGLE DIRAC CONE:4||WIRES:4||MAGNETICFIELD:4||STEPS:3||ELECTRONS:3||proximity effect:3||MODEL:3||ARRAYS:3||INTERFERENCE:3||fluxon dynamics:3||HETEROSTRUCTURES:3||INSULATOR:3||Andreev reflection:3||electronic transport:3||FISKE:3||superconductor:2||ZnO:2||quantum point contact:2||METAL:2||DYNAMICS:2||interlayer Josephson coupling:2||SUPERCONDUCTORS:2||YBA2CU3O7DELTA:2||LAYER:2||DOTS:2||quantum dot:2||Article:2||TRANSISTORS:2||CARBON NANOTUBES:2||GAP:2||MECHANISM:2||LINE:2||GIANT SHAPIRO STEPS:2||LAYERS:2||electron energy loss spectroscopy:2||physical phenomena:2||scanning electron microscopy:2||HGTE QUANTUMWELLS:2||BI2TE3:2||SPECTROSCOPY:2||PNJUNCTIONS:2||spinpolarized tunneling:2||INTRINSIC JOSEPHSONJUNCTIONS:2||FIELDS:2||positive magnetoresistance:2||dilute magnetic semiconductor:2||magnetic field:2||scanning transmission electron microscopy:2||QUANTUM OSCILLATIONS:2||TRANSPORTPROPERTIES:2||surface pair current:2||MAGNETORESISTANCE:2||NANORIBBONS:2||INSTABILITY:2||ANDREEV REFLECTION:2||microwave irradiation:2||vertical graphene josephson junction:2||BI2SE3:2||CONDUCTIVITY:2||highTc superconductors:2||DIMENSIONAL ELECTRONGAS:2||graphene:2||Topological insulators:2||Josephson coupling Fraunhofer interference pattern:2||FERROMAGNET:2||DEPENDENCE:2||DETECTOR:2||COHERENCE:2||INJECTION:2||GRAPHENE:1||JOSEPHSONJUNCTIONS:1||LAYERED SUPERCONDUCTOR:1||mode splitting:1||BEHAVIOR:1||spinpolarized transport:1||SUPERCONDUCTING TRANSITION:1||microwave response:1||PSEUDOGAP:1||phase coherence:1||TRANSITIONS:1||Long Josephson junction:1||Charge detection:1||collective resonance modes:1||plasma oscillation modes:1||Superconducting proximity effect:1||Iron pnictide superconductor:1||McMillanRowell oscillations:1||ferromagnetic microstructure:1||superradiant state:1||VOLTAGE:1||branch splitting:1||TENSOR:1||INTERCALATION:1||insitu fabrication:1||NDGAO3:1||DISORDERED METALS:1||GAUGE GLASS:1||LOWTEMPERATURE TRANSPORT:1||spontaneous spin polarization model:1||BIAS:1||emission of electromagnetic waves:1||YBA2CU3O7/PRBA2CU3O7 SUPERLATTICES:1||BOHM:1||SHAPIRO STEPS:1||superconductor/ferromagnet interface:1||OXIDE:1||ANDREEVREFLECTION:1||SinFeAsO single crystal:1||COLLECTIVE MOTION:1||ANGULARDEPENDENCE:1||SUPERCONDUCTIVITY:1||BILAYER GRAPHENE:1||PHOTOLUMINESCENT PROPERTIES:1||SUPERCONDUCTING WEAK LINKS:1||intrinsic Josephson junctions geometrical resonance:1||intrinsic Josephson junction:1||MESOSCOPIC SPINVALVE:1||Bi2212 single crystals:1||intrinsic junctions:1||ANDREEV REFLECTIONS:1||normalmetal/superconductor interface:1||IBI2SR2CACU2OY:1||THERMAL FLUCTUATIONS:1||MIXED STATE:1||BI2.15SR1.85CACU2O8+DELTA:1||intrinsic Josephson effects:1||CACUO:1||QUANTUM POINT CONTACTS:1||resonant tunneling state:1||coherence length:1||NANOWIRE:1||GATES:1||Phase line:1||Thermal activation:1||QUANTUMDOT:1||superconducting proximity effect:1||Andreev interferometer:1||WIRE:1||Josephsonvortexflow branches:1||Bi2212 cuprates:1||LATTICE:1||demannetization effect:1||SUPERCONDUCTING MIRRORS:1||GAS:1||VALLEY TRANSPORT:1||ELECTRODES:1||DEPENDENT TRANSPORT:1||BORNOPPENHEIMER APPROXIMATION:1||collective plasma oscillations:1||fluxon resonance steps:1||STACKS:1||COLLECTIVE DYNAMICS:1||PAIRING SYMMETRY:1||MUON SPIN ROTATION:1||DIMENSIONAL CROSSOVER:1||Bi2Sr2CaCu2Oy highTc superconductors:1||heterojunctions:1||nanostructures:1||surfaces and interfaces:1||QUANTUM TRANSPORT:1||MICROJUNCTIONS:1||RESONATORS:1||STATES:1||FIELD:1||FLUCTUATIONS:1||SCATTERING:1||mode splitting of Josephson vortexflow branches:1||2D superconductivity:1||TRANSISTOR:1||ENERGYGAP:1||SUPERLATTICES:1||IRONBASED SUPERCONDUCTORS:1||PHASEDEPENDENT RESISTANCE:1||QUANTUM PHASETRANSITIONS:1||ELECTRICFIELD:1||HIGH MAGNETICFIELDS:1||NANOWIRE HETEROSTRUCTURES:1||ZNO:1||pair breaking.:1||SUPERCONDUCTING PB:1||domain formation:1||FORCE MICROSCOPY:1||RELAXATION:1||PLASMA RESONANCE:1||coupled Josephson junctions:1||COPPEROXIDE SUPERCONDUCTORS:1||CROSSOVER:1||SIMULATIONS:1||LOWTEMPERATURE:1||CONDUCTORS:1||METALINSULATORTRANSITION:1||SEMICONDUCTOR:1||FIELDEFFECT TRANSISTORS:1||ZEROVOLTAGE STATE:1||constanttemperature interlayer tunneling spectroscopy:1||Josephson supercurrent:1||BIPOLAR SUPERCURRENT:1||Interaction between Josephson and pancake vortices:1||flux jump:1||coaxial heterojunction nanorod:1||Natural Josephson coupling:1||BI2SR2CACU2O8+DELTA:1||VORTEX FLOW:1||TC SUPERCONDUCTORS:1||charge imbalance:1||Andreev diffractometer:1||intercalation:1||surface junction:1||Bi2212:1||tunnelling:1||GRAPHITE:1||GROWTH:1||collective transverse plasma modes:1||GAN:1||Macroscopic quantum tunneling:1||Fluctuation conductivity:1||Abovegap conductance jump:1||Josephson vortex motion:1||Intrinsic Josephson junctions:1||LAYERED SUPERCONDUCTORS:1||BI2SR2CACU2O8+Y:1||INTERFACES:1||BREAKDOWN:1||SYSTEMS:1||Anisotropy ratio:1||Josephson vortex:1||spin relaxation in superconductors:1||bibased single crystals:1||MESOSCOPIC PROXIMITY SUPERCONDUCTOR:1||reentrance of conductance:1||interlayer pair tunneling:1||JOSEPHSON:1||DISORDERED 2DIMENSIONAL SUPERCONDUCTORS:1||INDIUM FILMS:1||excited state:1||REGIME:1||triplet superconductivity:1||FILM:1||SCHOTTKY DIODES:1||peakdiphump structure:1||Kondo effect:1||REENTRANCE:1||Graphene:1||CONTACT:1||BERRYS PHASE:1||2DIMENSIONAL SUPERCONDUCTORS:1||Coulomb diamond:1||magnetic domain:1||spin injection:1||RESONANCE:1||plasma excitation modes:1||FLOW:1||OVERDOPED BI2SR2CACU2O8+DELTA:1||hole doping:1||chemical synthesis:1||phase transitions:1||superconductors:1||VORTEXGLASS SUPERCONDUCTIVITY:1||Kondorelated model:1||RADIATION:1||DOT:1||NANOBELTS:1||Complementarity:1||Closedloop AharonovBohm interferometer:1||pair breaking:1||interlayer phase fluctuation:1||MgB2 thin film:1||CONFINEMENT:1||WALLED CARBON NANOTUBES:1||TRANSITION:9||VORTICES:8||STATE:7||intrinsic Josephson junctions:7||SINGLECRYSTALS:7||JUNCTIONS:5||MODES:5||SUPERCURRENT:5||SUPERCONDUCTOR:5||CONDUCTANCE:5||HIGHTEMPERATURE SUPERCONDUCTORS:5||TRANSPORT:5||PHASE:5||FILMS:4||LOCALIZATION:4||SINGLE DIRAC CONE:4||WIRES:4||MAGNETICFIELD:4||STEPS:3||ELECTRONS:3||proximity effect:3||MODEL:3||ARRAYS:3||INTERFERENCE:3||fluxon dynamics:3||HETEROSTRUCTURES:3||INSULATOR:3||Andreev reflection:3||electronic transport:3||FISKE:3||superconductor:2||ZnO:2||quantum point contact:2||METAL:2||DYNAMICS:2||interlayer Josephson coupling:2||SUPERCONDUCTORS:2||YBA2CU3O7DELTA:2||LAYER:2||DOTS:2||quantum dot:2||Article:2||TRANSISTORS:2||CARBON NANOTUBES:2||GAP:2||MECHANISM:2||LINE:2||GIANT SHAPIRO STEPS:2||LAYERS:2||electron energy loss spectroscopy:2||physical phenomena:2||scanning electron microscopy:2||HGTE QUANTUMWELLS:2||BI2TE3:2||SPECTROSCOPY:2||PNJUNCTIONS:2||spinpolarized tunneling:2||INTRINSIC JOSEPHSONJUNCTIONS:2||FIELDS:2||positive magnetoresistance:2||dilute magnetic semiconductor:2||magnetic field:2||scanning transmission electron microscopy:2||QUANTUM OSCILLATIONS:2||TRANSPORTPROPERTIES:2||surface pair current:2||MAGNETORESISTANCE:2||NANORIBBONS:2||INSTABILITY:2||ANDREEV REFLECTION:2||microwave irradiation:2||vertical graphene josephson junction:2||BI2SE3:2||CONDUCTIVITY:2||highTc superconductors:2||DIMENSIONAL ELECTRONGAS:2||graphene:2||Topological insulators:2||Josephson coupling Fraunhofer interference pattern:2||FERROMAGNET:2||DEPENDENCE:2||DETECTOR:2||COHERENCE:2||INJECTION:2||GRAPHENE:1||JOSEPHSONJUNCTIONS:1||LAYERED SUPERCONDUCTOR:1||mode splitting:1||BEHAVIOR:1||spinpolarized transport:1||SUPERCONDUCTING TRANSITION:1||microwave response:1||PSEUDOGAP:1||phase coherence:1||TRANSITIONS:1||Long Josephson junction:1||Charge detection:1||collective resonance modes:1||plasma oscillation modes:1||Superconducting proximity effect:1||Iron pnictide superconductor:1||McMillanRowell oscillations:1||ferromagnetic microstructure:1||superradiant state:1||VOLTAGE:1||branch splitting:1||TENSOR:1||INTERCALATION:1||insitu fabrication:1||NDGAO3:1||DISORDERED METALS:1||GAUGE GLASS:1||LOWTEMPERATURE TRANSPORT:1||spontaneous spin polarization model:1||BIAS:1||emission of electromagnetic waves:1||YBA2CU3O7/PRBA2CU3O7 SUPERLATTICES:1||BOHM:1||SHAPIRO STEPS:1||superconductor/ferromagnet interface:1||OXIDE:1||ANDREEVREFLECTION:1||SinFeAsO single crystal:1||COLLECTIVE MOTION:1||ANGULARDEPENDENCE:1||SUPERCONDUCTIVITY:1||BILAYER GRAPHENE:1||PHOTOLUMINESCENT PROPERTIES:1||SUPERCONDUCTING WEAK LINKS:1||intrinsic Josephson junctions geometrical resonance:1||intrinsic Josephson junction:1||MESOSCOPIC SPINVALVE:1||Bi2212 single crystals:1||intrinsic junctions:1||ANDREEV REFLECTIONS:1||normalmetal/superconductor interface:1||IBI2SR2CACU2OY:1||THERMAL FLUCTUATIONS:1||MIXED STATE:1||BI2.15SR1.85CACU2O8+DELTA:1||intrinsic Josephson effects:1||CACUO:1||QUANTUM POINT CONTACTS:1||resonant tunneling state:1||coherence length:1||NANOWIRE:1||GATES:1||Phase line:1||Thermal activation:1||QUANTUMDOT:1||superconducting proximity effect:1||Andreev interferometer:1||WIRE:1||Josephsonvortexflow branches:1||Bi2212 cuprates:1||LATTICE:1||demannetization effect:1||SUPERCONDUCTING MIRRORS:1||GAS:1||VALLEY TRANSPORT:1||ELECTRODES:1||DEPENDENT TRANSPORT:1||BORNOPPENHEIMER APPROXIMATION:1||collective plasma oscillations:1||fluxon resonance steps:1||STACKS:1||COLLECTIVE DYNAMICS:1||PAIRING SYMMETRY:1||MUON SPIN ROTATION:1||DIMENSIONAL CROSSOVER:1||Bi2Sr2CaCu2Oy highTc superconductors:1||heterojunctions:1||nanostructures:1||surfaces and interfaces:1||QUANTUM TRANSPORT:1||MICROJUNCTIONS:1||RESONATORS:1||STATES:1||FIELD:1||FLUCTUATIONS:1||SCATTERING:1||mode splitting of Josephson vortexflow branches:1||2D superconductivity:1||TRANSISTOR:1||ENERGYGAP:1||SUPERLATTICES:1||IRONBASED SUPERCONDUCTORS:1||PHASEDEPENDENT RESISTANCE:1||QUANTUM PHASETRANSITIONS:1||ELECTRICFIELD:1||HIGH MAGNETICFIELDS:1||NANOWIRE HETEROSTRUCTURES:1||ZNO:1||pair breaking.:1||SUPERCONDUCTING PB:1||domain formation:1||FORCE MICROSCOPY:1||RELAXATION:1||PLASMA RESONANCE:1||coupled Josephson junctions:1||COPPEROXIDE SUPERCONDUCTORS:1||CROSSOVER:1||SIMULATIONS:1||LOWTEMPERATURE:1||CONDUCTORS:1||METALINSULATORTRANSITION:1||SEMICONDUCTOR:1||FIELDEFFECT TRANSISTORS:1||ZEROVOLTAGE STATE:1||constanttemperature interlayer tunneling spectroscopy:1||Josephson supercurrent:1||BIPOLAR SUPERCURRENT:1||Interaction between Josephson and pancake vortices:1||flux jump:1||coaxial heterojunction nanorod:1||Natural Josephson coupling:1||BI2SR2CACU2O8+DELTA:1||VORTEX FLOW:1||TC SUPERCONDUCTORS:1||charge imbalance:1||Andreev diffractometer:1||intercalation:1||surface junction:1||Bi2212:1||tunnelling:1||GRAPHITE:1||GROWTH:1||collective transverse plasma modes:1||GAN:1||Macroscopic quantum tunneling:1||Fluctuation conductivity:1||Abovegap conductance jump:1||Josephson vortex motion:1||Intrinsic Josephson junctions:1||LAYERED SUPERCONDUCTORS:1||BI2SR2CACU2O8+Y:1||INTERFACES:1||BREAKDOWN:1||SYSTEMS:1||Anisotropy ratio:1||Josephson vortex:1||spin relaxation in superconductors:1||bibased single crystals:1||MESOSCOPIC PROXIMITY SUPERCONDUCTOR:1||reentrance of conductance:1||interlayer pair tunneling:1||JOSEPHSON:1||DISORDERED 2DIMENSIONAL SUPERCONDUCTORS:1||INDIUM FILMS:1||excited state:1||REGIME:1||triplet superconductivity:1||FILM:1||SCHOTTKY DIODES:1||peakdiphump structure:1||Kondo effect:1||REENTRANCE:1||Graphene:1||CONTACT:1||BERRYS PHASE:1||2DIMENSIONAL SUPERCONDUCTORS:1||Coulomb diamond:1||magnetic domain:1||spin injection:1||RESONANCE:1||plasma excitation modes:1||FLOW:1||OVERDOPED BI2SR2CACU2O8+DELTA:1||hole doping:1||chemical synthesis:1||phase transitions:1||superconductors:1||VORTEXGLASS SUPERCONDUCTIVITY:1||Kondorelated model:1||RADIATION:1||DOT:1||NANOBELTS:1||Complementarity:1||Closedloop AharonovBohm interferometer:1||pair breaking:1||interlayer phase fluctuation:1||MgB2 thin film:1||CONFINEMENT:1||WALLED CARBON NANOTUBES:1||TRANSITION:9||VORTICES:8||STATE:7||intrinsic Josephson junctions:7||SINGLECRYSTALS:7||JUNCTIONS:5||MODES:5||SUPERCURRENT:5||SUPERCONDUCTOR:5||CONDUCTANCE:5||HIGHTEMPERATURE SUPERCONDUCTORS:5||TRANSPORT:5||PHASE:5||FILMS:4||LOCALIZATION:4||SINGLE DIRAC CONE:4||WIRES:4||MAGNETICFIELD:4||STEPS:3||ELECTRONS:3||proximity effect:3||MODEL:3||ARRAYS:3||INTERFERENCE:3||fluxon dynamics:3||HETEROSTRUCTURES:3||INSULATOR:3||Andreev reflection:3||electronic transport:3||FISKE:3||superconductor:2||ZnO:2||quantum point contact:2||METAL:2||DYNAMICS:2||interlayer Josephson coupling:2||SUPERCONDUCTORS:2||YBA2CU3O7DELTA:2||LAYER:2||DOTS:2||quantum dot:2||Article:2||TRANSISTORS:2||CARBON NANOTUBES:2||GAP:2||MECHANISM:2||LINE:2||GIANT SHAPIRO STEPS:2||LAYERS:2||electron energy loss spectroscopy:2||physical phenomena:2||scanning electron microscopy:2||HGTE QUANTUMWELLS:2||BI2TE3:2||SPECTROSCOPY:2||PNJUNCTIONS:2||spinpolarized tunneling:2||INTRINSIC JOSEPHSONJUNCTIONS:2||FIELDS:2||positive magnetoresistance:2||dilute magnetic semiconductor:2||magnetic field:2||scanning transmission electron microscopy:2||QUANTUM OSCILLATIONS:2||TRANSPORTPROPERTIES:2||surface pair current:2||MAGNETORESISTANCE:2||NANORIBBONS:2||INSTABILITY:2||ANDREEV REFLECTION:2||microwave irradiation:2||vertical graphene josephson junction:2||BI2SE3:2||CONDUCTIVITY:2||highTc superconductors:2||DIMENSIONAL ELECTRONGAS:2||graphene:2||Topological insulators:2||Josephson coupling Fraunhofer interference pattern:2||FERROMAGNET:2||DEPENDENCE:2||DETECTOR:2||COHERENCE:2||INJECTION:2||GRAPHENE:1||JOSEPHSONJUNCTIONS:1||LAYERED SUPERCONDUCTOR:1||mode splitting:1||BEHAVIOR:1||spinpolarized transport:1||SUPERCONDUCTING TRANSITION:1||microwave response:1||PSEUDOGAP:1||phase coherence:1||TRANSITIONS:1||Long Josephson junction:1||Charge detection:1||collective resonance modes:1||plasma oscillation modes:1||Superconducting proximity effect:1||Iron pnictide superconductor:1||McMillanRowell oscillations:1||ferromagnetic microstructure:1||superradiant state:1||VOLTAGE:1||branch splitting:1||TENSOR:1||INTERCALATION:1||insitu fabrication:1||NDGAO3:1||DISORDERED METALS:1||GAUGE GLASS:1||LOWTEMPERATURE TRANSPORT:1||spontaneous spin polarization model:1||BIAS:1||emission of electromagnetic waves:1||YBA2CU3O7/PRBA2CU3O7 SUPERLATTICES:1||BOHM:1||SHAPIRO STEPS:1||superconductor/ferromagnet interface:1||OXIDE:1||ANDREEVREFLECTION:1||SinFeAsO single crystal:1||COLLECTIVE MOTION:1||ANGULARDEPENDENCE:1||SUPERCONDUCTIVITY:1||BILAYER GRAPHENE:1||PHOTOLUMINESCENT PROPERTIES:1||SUPERCONDUCTING WEAK LINKS:1||intrinsic Josephson junctions geometrical resonance:1||intrinsic Josephson junction:1||MESOSCOPIC SPINVALVE:1||Bi2212 single crystals:1||intrinsic junctions:1||ANDREEV REFLECTIONS:1||normalmetal/superconductor interface:1||IBI2SR2CACU2OY:1||THERMAL FLUCTUATIONS:1||MIXED STATE:1||BI2.15SR1.85CACU2O8+DELTA:1||intrinsic Josephson effects:1||CACUO:1||QUANTUM POINT CONTACTS:1||resonant tunneling state:1||coherence length:1||NANOWIRE:1||GATES:1||Phase line:1||Thermal activation:1||QUANTUMDOT:1||superconducting proximity effect:1||Andreev interferometer:1||WIRE:1||Josephsonvortexflow branches:1||Bi2212 cuprates:1||LATTICE:1||demannetization effect:1||SUPERCONDUCTING MIRRORS:1||GAS:1||VALLEY TRANSPORT:1||ELECTRODES:1||DEPENDENT TRANSPORT:1||BORNOPPENHEIMER APPROXIMATION:1||collective plasma oscillations:1||fluxon resonance steps:1||STACKS:1||COLLECTIVE DYNAMICS:1||PAIRING SYMMETRY:1||MUON SPIN ROTATION:1||DIMENSIONAL CROSSOVER:1||Bi2Sr2CaCu2Oy highTc superconductors:1||heterojunctions:1||nanostructures:1||surfaces and interfaces:1||QUANTUM TRANSPORT:1||MICROJUNCTIONS:1||RESONATORS:1||STATES:1||FIELD:1||FLUCTUATIONS:1||SCATTERING:1||mode splitting of Josephson vortexflow branches:1||2D superconductivity:1||TRANSISTOR:1||ENERGYGAP:1||SUPERLATTICES:1||IRONBASED SUPERCONDUCTORS:1||PHASEDEPENDENT RESISTANCE:1||QUANTUM PHASETRANSITIONS:1||ELECTRICFIELD:1||HIGH MAGNETICFIELDS:1||NANOWIRE HETEROSTRUCTURES:1||ZNO:1||pair breaking.:1||SUPERCONDUCTING PB:1||domain formation:1||FORCE MICROSCOPY:1||RELAXATION:1||PLASMA RESONANCE:1||coupled Josephson junctions:1||COPPEROXIDE SUPERCONDUCTORS:1||CROSSOVER:1||SIMULATIONS:1||LOWTEMPERATURE:1||CONDUCTORS:1||METALINSULATORTRANSITION:1||SEMICONDUCTOR:1||FIELDEFFECT TRANSISTORS:1||ZEROVOLTAGE STATE:1||constanttemperature interlayer tunneling spectroscopy:1||Josephson supercurrent:1||BIPOLAR SUPERCURRENT:1||Interaction between Josephson and pancake vortices:1||flux jump:1||coaxial heterojunction nanorod:1||Natural Josephson coupling:1||BI2SR2CACU2O8+DELTA:1||VORTEX FLOW:1||TC SUPERCONDUCTORS:1||charge imbalance:1||Andreev diffractometer:1||intercalation:1||surface junction:1||Bi2212:1||tunnelling:1||GRAPHITE:1||GROWTH:1||collective transverse plasma modes:1||GAN:1||Macroscopic quantum tunneling:1||Fluctuation conductivity:1||Abovegap conductance jump:1||Josephson vortex motion:1||Intrinsic Josephson junctions:1||LAYERED SUPERCONDUCTORS:1||BI2SR2CACU2O8+Y:1||INTERFACES:1||BREAKDOWN:1||SYSTEMS:1||Anisotropy ratio:1||Josephson vortex:1||spin relaxation in superconductors:1||bibased single crystals:1||MESOSCOPIC PROXIMITY SUPERCONDUCTOR:1||reentrance of conductance:1||interlayer pair tunneling:1||JOSEPHSON:1||DISORDERED 2DIMENSIONAL SUPERCONDUCTORS:1||INDIUM FILMS:1||excited state:1||REGIME:1||triplet superconductivity:1||FILM:1||SCHOTTKY DIODES:1||peakdiphump structure:1||Kondo effect:1||REENTRANCE:1||Graphene:1||CONTACT:1||BERRYS PHASE:1||2DIMENSIONAL SUPERCONDUCTORS:1||Coulomb diamond:1||magnetic domain:1||spin injection:1||RESONANCE:1||plasma excitation modes:1||FLOW:1||OVERDOPED BI2SR2CACU2O8+DELTA:1||hole doping:1||chemical synthesis:1||phase transitions:1||superconductors:1||VORTEXGLASS SUPERCONDUCTIVITY:1||Kondorelated model:1||RADIATION:1||DOT:1||NANOBELTS:1||Complementarity:1||Closedloop AharonovBohm interferometer:1||pair breaking:1||interlayer phase fluctuation:1||MgB2 thin film:1||CONFINEMENT:1||WALLED CARBON NANOTUBES:1||TRANSITION:9||VORTICES:8||STATE:7||intrinsic Josephson junctions:7||SINGLECRYSTALS:7||JUNCTIONS:5||MODES:5||SUPERCURRENT:5||SUPERCONDUCTOR:5||CONDUCTANCE:5||HIGHTEMPERATURE SUPERCONDUCTORS:5||TRANSPORT:5||PHASE:5||FILMS:4||LOCALIZATION:4||SINGLE DIRAC CONE:4||WIRES:4||MAGNETICFIELD:4||STEPS:3||ELECTRONS:3||proximity effect:3||MODEL:3||ARRAYS:3||INTERFERENCE:3||fluxon dynamics:3||HETEROSTRUCTURES:3||INSULATOR:3||Andreev reflection:3||electronic transport:3||FISKE:3||superconductor:2||ZnO:2||quantum point contact:2||METAL:2||DYNAMICS:2||interlayer Josephson coupling:2||SUPERCONDUCTORS:2||YBA2CU3O7DELTA:2||LAYER:2||DOTS:2||quantum dot:2||Article:2||TRANSISTORS:2||CARBON NANOTUBES:2||GAP:2||MECHANISM:2||LINE:2||GIANT SHAPIRO STEPS:2||LAYERS:2||electron energy loss spectroscopy:2||physical phenomena:2||scanning electron microscopy:2||HGTE QUANTUMWELLS:2||BI2TE3:2||SPECTROSCOPY:2||PNJUNCTIONS:2||spinpolarized tunneling:2||INTRINSIC JOSEPHSONJUNCTIONS:2||FIELDS:2||positive magnetoresistance:2||dilute magnetic semiconductor:2||magnetic field:2||scanning transmission electron microscopy:2||QUANTUM OSCILLATIONS:2||TRANSPORTPROPERTIES:2||surface pair current:2||MAGNETORESISTANCE:2||NANORIBBONS:2||INSTABILITY:2||ANDREEV REFLECTION:2||microwave irradiation:2||vertical graphene josephson junction:2||BI2SE3:2||CONDUCTIVITY:2||highTc superconductors:2||DIMENSIONAL ELECTRONGAS:2||graphene:2||Topological insulators:2||Josephson coupling Fraunhofer interference pattern:2||FERROMAGNET:2||DEPENDENCE:2||DETECTOR:2||COHERENCE:2||INJECTION:2||GRAPHENE:1||JOSEPHSONJUNCTIONS:1||LAYERED SUPERCONDUCTOR:1||mode splitting:1||BEHAVIOR:1||spinpolarized transport:1||SUPERCONDUCTING TRANSITION:1||microwave response:1||PSEUDOGAP:1||phase coherence:1||TRANSITIONS:1||Long Josephson junction:1||Charge detection:1||collective resonance modes:1||plasma oscillation modes:1||Superconducting proximity effect:1||Iron pnictide superconductor:1||McMillanRowell oscillations:1||ferromagnetic microstructure:1||superradiant state:1||VOLTAGE:1||branch splitting:1||TENSOR:1||INTERCALATION:1||insitu fabrication:1||NDGAO3:1||DISORDERED METALS:1||GAUGE GLASS:1||LOWTEMPERATURE TRANSPORT:1||spontaneous spin polarization model:1||BIAS:1||emission of electromagnetic waves:1||YBA2CU3O7/PRBA2CU3O7 SUPERLATTICES:1||BOHM:1||SHAPIRO STEPS:1||superconductor/ferromagnet interface:1||OXIDE:1||ANDREEVREFLECTION:1||SinFeAsO single crystal:1||COLLECTIVE MOTION:1||ANGULARDEPENDENCE:1||SUPERCONDUCTIVITY:1||BILAYER GRAPHENE:1||PHOTOLUMINESCENT PROPERTIES:1||SUPERCONDUCTING WEAK LINKS:1||intrinsic Josephson junctions geometrical resonance:1||intrinsic Josephson junction:1||MESOSCOPIC SPINVALVE:1||Bi2212 single crystals:1||intrinsic junctions:1||ANDREEV REFLECTIONS:1||normalmetal/superconductor interface:1||IBI2SR2CACU2OY:1||THERMAL FLUCTUATIONS:1||MIXED STATE:1||BI2.15SR1.85CACU2O8+DELTA:1||intrinsic Josephson effects:1||CACUO:1||QUANTUM POINT CONTACTS:1||resonant tunneling state:1||coherence length:1||NANOWIRE:1||GATES:1||Phase line:1||Thermal activation:1||QUANTUMDOT:1||superconducting proximity effect:1||Andreev interferometer:1||WIRE:1||Josephsonvortexflow branches:1||Bi2212 cuprates:1||LATTICE:1||demannetization effect:1||SUPERCONDUCTING MIRRORS:1||GAS:1||VALLEY TRANSPORT:1||ELECTRODES:1||DEPENDENT TRANSPORT:1||BORNOPPENHEIMER APPROXIMATION:1||collective plasma oscillations:1||fluxon resonance steps:1||STACKS:1||COLLECTIVE DYNAMICS:1||PAIRING SYMMETRY:1||MUON SPIN ROTATION:1||DIMENSIONAL CROSSOVER:1||Bi2Sr2CaCu2Oy highTc superconductors:1||heterojunctions:1||nanostructures:1||surfaces and interfaces:1||QUANTUM TRANSPORT:1||MICROJUNCTIONS:1||RESONATORS:1||STATES:1||FIELD:1||FLUCTUATIONS:1||SCATTERING:1||mode splitting of Josephson vortexflow branches:1||2D superconductivity:1||TRANSISTOR:1||ENERGYGAP:1||SUPERLATTICES:1||IRONBASED SUPERCONDUCTORS:1||PHASEDEPENDENT RESISTANCE:1||QUANTUM PHASETRANSITIONS:1||ELECTRICFIELD:1||HIGH MAGNETICFIELDS:1||NANOWIRE HETEROSTRUCTURES:1||ZNO:1||pair breaking.:1||SUPERCONDUCTING PB:1||domain formation:1||FORCE MICROSCOPY:1||RELAXATION:1||PLASMA RESONANCE:1||coupled Josephson junctions:1||COPPEROXIDE SUPERCONDUCTORS:1||CROSSOVER:1||SIMULATIONS:1||LOWTEMPERATURE:1||CONDUCTORS:1||METALINSULATORTRANSITION:1||SEMICONDUCTOR:1||FIELDEFFECT TRANSISTORS:1||ZEROVOLTAGE STATE:1||constanttemperature interlayer tunneling spectroscopy:1||Josephson supercurrent:1||BIPOLAR SUPERCURRENT:1||Interaction between Josephson and pancake vortices:1||flux jump:1||coaxial heterojunction nanorod:1||Natural Josephson coupling:1||BI2SR2CACU2O8+DELTA:1||VORTEX FLOW:1||TC SUPERCONDUCTORS:1||charge imbalance:1||Andreev diffractometer:1||intercalation:1||surface junction:1||Bi2212:1||tunnelling:1||GRAPHITE:1||GROWTH:1||collective transverse plasma modes:1||GAN:1||Macroscopic quantum tunneling:1||Fluctuation conductivity:1||Abovegap conductance jump:1||Josephson vortex motion:1||Intrinsic Josephson junctions:1||LAYERED SUPERCONDUCTORS:1||BI2SR2CACU2O8+Y:1||INTERFACES:1||BREAKDOWN:1||SYSTEMS:1||Anisotropy ratio:1||Josephson vortex:1||spin relaxation in superconductors:1||bibased single crystals:1||MESOSCOPIC PROXIMITY SUPERCONDUCTOR:1||reentrance of conductance:1||interlayer pair tunneling:1||JOSEPHSON:1||DISORDERED 2DIMENSIONAL SUPERCONDUCTORS:1||INDIUM FILMS:1||excited state:1||REGIME:1||triplet superconductivity:1||FILM:1||SCHOTTKY DIODES:1||peakdiphump structure:1||Kondo effect:1||REENTRANCE:1||Graphene:1||CONTACT:1||BERRYS PHASE:1||2DIMENSIONAL SUPERCONDUCTORS:1||Coulomb diamond:1||magnetic domain:1||spin injection:1||RESONANCE:1||plasma excitation modes:1||FLOW:1||OVERDOPED BI2SR2CACU2O8+DELTA:1||hole doping:1||chemical synthesis:1||phase transitions:1||superconductors:1||VORTEXGLASS SUPERCONDUCTIVITY:1||Kondorelated model:1||RADIATION:1||DOT:1||NANOBELTS:1||Complementarity:1||Closedloop AharonovBohm interferometer:1||pair breaking:1||interlayer phase fluctuation:1||MgB2 thin film:1||CONFINEMENT:1||WALLED CARBON NANOTUBES:1||TRANSITION:9||VORTICES:8||STATE:7||intrinsic Josephson junctions:7||SINGLECRYSTALS:7||JUNCTIONS:5||MODES:5||SUPERCURRENT:5||SUPERCONDUCTOR:5||CONDUCTANCE:5||HIGHTEMPERATURE SUPERCONDUCTORS:5||TRANSPORT:5||PHASE:5||FILMS:4||LOCALIZATION:4||SINGLE DIRAC CONE:4||WIRES:4||MAGNETICFIELD:4||STEPS:3||ELECTRONS:3||proximity effect:3||MODEL:3||ARRAYS:3||INTERFERENCE:3||fluxon dynamics:3||HETEROSTRUCTURES:3||INSULATOR:3||Andreev reflection:3||electronic transport:3||FISKE:3||superconductor:2||ZnO:2||quantum point contact:2||METAL:2||DYNAMICS:2||interlayer Josephson coupling:2||SUPERCONDUCTORS:2||YBA2CU3O7DELTA:2||LAYER:2||DOTS:2||quantum dot:2||Article:2||TRANSISTORS:2||CARBON NANOTUBES:2||GAP:2||MECHANISM:2||LINE:2||GIANT SHAPIRO STEPS:2||LAYERS:2||electron energy loss spectroscopy:2||physical phenomena:2||scanning electron microscopy:2||HGTE QUANTUMWELLS:2||BI2TE3:2||SPECTROSCOPY:2||PNJUNCTIONS:2||spinpolarized tunneling:2||INTRINSIC JOSEPHSONJUNCTIONS:2||FIELDS:2||positive magnetoresistance:2||dilute magnetic semiconductor:2||magnetic field:2||scanning transmission electron microscopy:2||QUANTUM OSCILLATIONS:2||TRANSPORTPROPERTIES:2||surface pair current:2||MAGNETORESISTANCE:2||NANORIBBONS:2||INSTABILITY:2||ANDREEV REFLECTION:2||microwave irradiation:2||vertical graphene josephson junction:2||BI2SE3:2||CONDUCTIVITY:2||highTc superconductors:2||DIMENSIONAL ELECTRONGAS:2||graphene:2||Topological insulators:2||Josephson coupling Fraunhofer interference pattern:2||FERROMAGNET:2||DEPENDENCE:2||DETECTOR:2||COHERENCE:2||INJECTION:2||GRAPHENE:1||JOSEPHSONJUNCTIONS:1||LAYERED SUPERCONDUCTOR:1||mode splitting:1||BEHAVIOR:1||spinpolarized transport:1||SUPERCONDUCTING TRANSITION:1||microwave response:1||PSEUDOGAP:1||phase coherence:1||TRANSITIONS:1||Long Josephson junction:1||Charge detection:1||collective resonance modes:1||plasma oscillation modes:1||Superconducting proximity effect:1||Iron pnictide superconductor:1||McMillanRowell oscillations:1||ferromagnetic microstructure:1||superradiant state:1||VOLTAGE:1||branch splitting:1||TENSOR:1||INTERCALATION:1||insitu fabrication:1||NDGAO3:1||DISORDERED METALS:1||GAUGE GLASS:1||LOWTEMPERATURE TRANSPORT:1||spontaneous spin polarization model:1||BIAS:1||emission of electromagnetic waves:1||YBA2CU3O7/PRBA2CU3O7 SUPERLATTICES:1||BOHM:1||SHAPIRO STEPS:1||superconductor/ferromagnet interface:1||OXIDE:1||ANDREEVREFLECTION:1||SinFeAsO single crystal:1||COLLECTIVE MOTION:1||ANGULARDEPENDENCE:1||SUPERCONDUCTIVITY:1||BILAYER GRAPHENE:1||PHOTOLUMINESCENT PROPERTIES:1||SUPERCONDUCTING WEAK LINKS:1||intrinsic Josephson junctions geometrical resonance:1||intrinsic Josephson junction:1||MESOSCOPIC SPINVALVE:1||Bi2212 single crystals:1||intrinsic junctions:1||ANDREEV REFLECTIONS:1||normalmetal/superconductor interface:1||IBI2SR2CACU2OY:1||THERMAL FLUCTUATIONS:1||MIXED STATE:1||BI2.15SR1.85CACU2O8+DELTA:1||intrinsic Josephson effects:1||CACUO:1||QUANTUM POINT CONTACTS:1||resonant tunneling state:1||coherence length:1||NANOWIRE:1||GATES:1||Phase line:1||Thermal activation:1||QUANTUMDOT:1||superconducting proximity effect:1||Andreev interferometer:1||WIRE:1||Josephsonvortexflow branches:1||Bi2212 cuprates:1||LATTICE:1||demannetization effect:1||SUPERCONDUCTING MIRRORS:1||GAS:1||VALLEY TRANSPORT:1||ELECTRODES:1||DEPENDENT TRANSPORT:1||BORNOPPENHEIMER APPROXIMATION:1||collective plasma oscillations:1||fluxon resonance steps:1||STACKS:1||COLLECTIVE DYNAMICS:1||PAIRING SYMMETRY:1||MUON SPIN ROTATION:1||DIMENSIONAL CROSSOVER:1||Bi2Sr2CaCu2Oy highTc superconductors:1||heterojunctions:1||nanostructures:1||surfaces and interfaces:1||QUANTUM TRANSPORT:1||MICROJUNCTIONS:1||RESONATORS:1||STATES:1||FIELD:1||FLUCTUATIONS:1||SCATTERING:1||mode splitting of Josephson vortexflow branches:1||2D superconductivity:1||TRANSISTOR:1||ENERGYGAP:1||SUPERLATTICES:1||IRONBASED SUPERCONDUCTORS:1||PHASEDEPENDENT RESISTANCE:1||QUANTUM PHASETRANSITIONS:1||ELECTRICFIELD:1||HIGH MAGNETICFIELDS:1||NANOWIRE HETEROSTRUCTURES:1||ZNO:1||pair breaking.:1||SUPERCONDUCTING PB:1||domain formation:1||FORCE MICROSCOPY:1||RELAXATION:1||PLASMA RESONANCE:1||coupled Josephson junctions:1||COPPEROXIDE SUPERCONDUCTORS:1||CROSSOVER:1||SIMULATIONS:1||LOWTEMPERATURE:1||CONDUCTORS:1||METALINSULATORTRANSITION:1||SEMICONDUCTOR:1||FIELDEFFECT TRANSISTORS:1||ZEROVOLTAGE STATE:1||constanttemperature interlayer tunneling spectroscopy:1||Josephson supercurrent:1||BIPOLAR SUPERCURRENT:1||Interaction between Josephson and pancake vortices:1||flux jump:1||coaxial heterojunction nanorod:1||Natural Josephson coupling:1||BI2SR2CACU2O8+DELTA:1||VORTEX FLOW:1||TC SUPERCONDUCTORS:1||charge imbalance:1||Andreev diffractometer:1||intercalation:1||surface junction:1||Bi2212:1||tunnelling:1||GRAPHITE:1||GROWTH:1||collective transverse plasma modes:1||GAN:1||Macroscopic quantum tunneling:1||Fluctuation conductivity:1||Abovegap conductance jump:1||Josephson vortex motion:1||Intrinsic Josephson junctions:1||LAYERED SUPERCONDUCTORS:1||BI2SR2CACU2O8+Y:1||INTERFACES:1||BREAKDOWN:1||SYSTEMS:1||Anisotropy ratio:1||Josephson vortex:1||spin relaxation in superconductors:1||bibased single crystals:1||MESOSCOPIC PROXIMITY SUPERCONDUCTOR:1||reentrance of conductance:1||interlayer pair tunneling:1||JOSEPHSON:1||DISORDERED 2DIMENSIONAL SUPERCONDUCTORS:1||INDIUM FILMS:1||excited state:1||REGIME:1||triplet superconductivity:1||FILM:1||SCHOTTKY DIODES:1||peakdiphump structure:1||Kondo effect:1||REENTRANCE:1||Graphene:1||CONTACT:1||BERRYS PHASE:1||2DIMENSIONAL SUPERCONDUCTORS:1||Coulomb diamond:1||magnetic domain:1||spin injection:1||RESONANCE:1||plasma excitation modes:1||FLOW:1||OVERDOPED BI2SR2CACU2O8+DELTA:1||hole doping:1||chemical synthesis:1||phase transitions:1||superconductors:1||VORTEXGLASS SUPERCONDUCTIVITY:1||Kondorelated model:1||RADIATION:1||DOT:1||NANOBELTS:1||Complementarity:1||Closedloop AharonovBohm interferometer:1||pair breaking:1||interlayer phase fluctuation:1||MgB2 thin film:1||CONFINEMENT:1||WALLED CARBON NANOTUBES:1||TRANSITION:9||VORTICES:8||STATE:7||intrinsic Josephson junctions:7||SINGLECRYSTALS:7||JUNCTIONS:5||MODES:5||SUPERCURRENT:5||SUPERCONDUCTOR:5||CONDUCTANCE:5||HIGHTEMPERATURE SUPERCONDUCTORS:5||TRANSPORT:5||PHASE:5||FILMS:4||LOCALIZATION:4||SINGLE DIRAC CONE:4||WIRES:4||MAGNETICFIELD:4||STEPS:3||ELECTRONS:3||proximity effect:3||MODEL:3||ARRAYS:3||INTERFERENCE:3||fluxon dynamics:3||HETEROSTRUCTURES:3||INSULATOR:3||Andreev reflection:3||electronic transport:3||FISKE:3||superconductor:2||ZnO:2||quantum point contact:2||METAL:2||DYNAMICS:2||interlayer Josephson coupling:2||SUPERCONDUCTORS:2||YBA2CU3O7DELTA:2||LAYER:2||DOTS:2||quantum dot:2||Article:2||TRANSISTORS:2||CARBON NANOTUBES:2||GAP:2||MECHANISM:2||LINE:2||GIANT SHAPIRO STEPS:2||LAYERS:2||electron energy loss spectroscopy:2||physical phenomena:2||scanning electron microscopy:2||HGTE QUANTUMWELLS:2||BI2TE3:2||SPECTROSCOPY:2||PNJUNCTIONS:2||spinpolarized tunneling:2||INTRINSIC JOSEPHSONJUNCTIONS:2||FIELDS:2||positive magnetoresistance:2||dilute magnetic semiconductor:2||magnetic field:2||scanning transmission electron microscopy:2||QUANTUM OSCILLATIONS:2||TRANSPORTPROPERTIES:2||surface pair current:2||MAGNETORESISTANCE:2||NANORIBBONS:2||INSTABILITY:2||ANDREEV REFLECTION:2||microwave irradiation:2||vertical graphene josephson junction:2||BI2SE3:2||CONDUCTIVITY:2||highTc superconductors:2||DIMENSIONAL ELECTRONGAS:2||graphene:2||Topological insulators:2||Josephson coupling Fraunhofer interference pattern:2||FERROMAGNET:2||DEPENDENCE:2||DETECTOR:2||COHERENCE:2||INJECTION:2||GRAPHENE:1||JOSEPHSONJUNCTIONS:1||LAYERED SUPERCONDUCTOR:1||mode splitting:1||BEHAVIOR:1||spinpolarized transport:1||SUPERCONDUCTING TRANSITION:1||microwave response:1||PSEUDOGAP:1||phase coherence:1||TRANSITIONS:1||Long Josephson junction:1||Charge detection:1||collective resonance modes:1||plasma oscillation modes:1||Superconducting proximity effect:1||Iron pnictide superconductor:1||McMillanRowell oscillations:1||ferromagnetic microstructure:1||superradiant state:1||VOLTAGE:1||branch splitting:1||TENSOR:1||INTERCALATION:1||insitu fabrication:1||NDGAO3:1||DISORDERED METALS:1||GAUGE GLASS:1||LOWTEMPERATURE TRANSPORT:1||spontaneous spin polarization model:1||BIAS:1||emission of electromagnetic waves:1||YBA2CU3O7/PRBA2CU3O7 SUPERLATTICES:1||BOHM:1||SHAPIRO STEPS:1||superconductor/ferromagnet interface:1||OXIDE:1||ANDREEVREFLECTION:1||SinFeAsO single crystal:1||COLLECTIVE MOTION:1||ANGULARDEPENDENCE:1||SUPERCONDUCTIVITY:1||BILAYER GRAPHENE:1||PHOTOLUMINESCENT PROPERTIES:1||SUPERCONDUCTING WEAK LINKS:1||intrinsic Josephson junctions geometrical resonance:1||intrinsic Josephson junction:1||MESOSCOPIC SPINVALVE:1||Bi2212 single crystals:1||intrinsic junctions:1||ANDREEV REFLECTIONS:1||normalmetal/superconductor interface:1||IBI2SR2CACU2OY:1||THERMAL FLUCTUATIONS:1||MIXED STATE:1||BI2.15SR1.85CACU2O8+DELTA:1||intrinsic Josephson effects:1||CACUO:1||QUANTUM POINT CONTACTS:1||resonant tunneling state:1||coherence length:1||NANOWIRE:1||GATES:1||Phase line:1||Thermal activation:1||QUANTUMDOT:1||superconducting proximity effect:1||Andreev interferometer:1||WIRE:1||Josephsonvortexflow branches:1||Bi2212 cuprates:1||LATTICE:1||demannetization effect:1||SUPERCONDUCTING MIRRORS:1||GAS:1||VALLEY TRANSPORT:1||ELECTRODES:1||DEPENDENT TRANSPORT:1||BORNOPPENHEIMER APPROXIMATION:1||collective plasma oscillations:1||fluxon resonance steps:1||STACKS:1||COLLECTIVE DYNAMICS:1||PAIRING SYMMETRY:1||MUON SPIN ROTATION:1||DIMENSIONAL CROSSOVER:1||Bi2Sr2CaCu2Oy highTc superconductors:1||heterojunctions:1||nanostructures:1||surfaces and interfaces:1||QUANTUM TRANSPORT:1||MICROJUNCTIONS:1||RESONATORS:1||STATES:1||FIELD:1||FLUCTUATIONS:1||SCATTERING:1||mode splitting of Josephson vortexflow branches:1||2D superconductivity:1||TRANSISTOR:1||ENERGYGAP:1||SUPERLATTICES:1||IRONBASED SUPERCONDUCTORS:1||PHASEDEPENDENT RESISTANCE:1||QUANTUM PHASETRANSITIONS:1||ELECTRICFIELD:1||HIGH MAGNETICFIELDS:1||NANOWIRE HETEROSTRUCTURES:1||ZNO:1||pair breaking.:1||SUPERCONDUCTING PB:1||domain formation:1||FORCE MICROSCOPY:1||RELAXATION:1||PLASMA RESONANCE:1||coupled Josephson junctions:1||COPPEROXIDE SUPERCONDUCTORS:1||CROSSOVER:1||SIMULATIONS:1||LOWTEMPERATURE:1||CONDUCTORS:1||METALINSULATORTRANSITION:1||SEMICONDUCTOR:1||FIELDEFFECT TRANSISTORS:1||ZEROVOLTAGE STATE:1||constanttemperature interlayer tunneling spectroscopy:1||Josephson supercurrent:1||BIPOLAR SUPERCURRENT:1||Interaction between Josephson and pancake vortices:1||flux jump:1||coaxial heterojunction nanorod:1||Natural Josephson coupling:1||BI2SR2CACU2O8+DELTA:1||VORTEX FLOW:1||TC SUPERCONDUCTORS:1||charge imbalance:1||Andreev diffractometer:1||intercalation:1||surface junction:1||Bi2212:1||tunnelling:1||GRAPHITE:1||GROWTH:1||collective transverse plasma modes:1||GAN:1||Macroscopic quantum tunneling:1||Fluctuation conductivity:1||Abovegap conductance jump:1||Josephson vortex motion:1||Intrinsic Josephson junctions:1||LAYERED SUPERCONDUCTORS:1||BI2SR2CACU2O8+Y:1||INTERFACES:1||BREAKDOWN:1||SYSTEMS:1||Anisotropy ratio:1||Josephson vortex:1||spin relaxation in superconductors:1||bibased single crystals:1||MESOSCOPIC PROXIMITY SUPERCONDUCTOR:1||reentrance of conductance:1||interlayer pair tunneling:1||JOSEPHSON:1||DISORDERED 2DIMENSIONAL SUPERCONDUCTORS:1||INDIUM FILMS:1||excited state:1||REGIME:1||triplet superconductivity:1||FILM:1||SCHOTTKY DIODES:1||peakdiphump structure:1||Kondo effect:1||REENTRANCE:1||Graphene:1||CONTACT:1||BERRYS PHASE:1||2DIMENSIONAL SUPERCONDUCTORS:1||Coulomb diamond:1||magnetic domain:1||spin injection:1||RESONANCE:1||plasma excitation modes:1||FLOW:1||OVERDOPED BI2SR2CACU2O8+DELTA:1||hole doping:1||chemical synthesis:1||phase transitions:1||superconductors:1||VORTEXGLASS SUPERCONDUCTIVITY:1||Kondorelated model:1||RADIATION:1||DOT:1||NANOBELTS:1||Complementarity:1||Closedloop AharonovBohm interferometer:1||pair breaking:1||interlayer phase fluctuation:1||MgB2 thin film:1||CONFINEMENT:1||WALLED CARBON NANOTUBES:1||TRANSITION:9||VORTICES:8||STATE:7||intrinsic Josephson junctions:7||SINGLECRYSTALS:7||JUNCTIONS:5||MODES:5||SUPERCURRENT:5||SUPERCONDUCTOR:5||CONDUCTANCE:5||HIGHTEMPERATURE SUPERCONDUCTORS:5||TRANSPORT:5||PHASE:5||FILMS:4||LOCALIZATION:4||SINGLE DIRAC CONE:4||WIRES:4||MAGNETICFIELD:4||STEPS:3||ELECTRONS:3||proximity effect:3||MODEL:3||ARRAYS:3||INTERFERENCE:3||fluxon dynamics:3||HETEROSTRUCTURES:3||INSULATOR:3||Andreev reflection:3||electronic transport:3||FISKE:3||superconductor:2||ZnO:2||quantum point contact:2||METAL:2||DYNAMICS:2||interlayer Josephson coupling:2||SUPERCONDUCTORS:2||YBA2CU3O7DELTA:2||LAYER:2||DOTS:2||quantum dot:2||Article:2||TRANSISTORS:2||CARBON NANOTUBES:2||GAP:2||MECHANISM:2||LINE:2||GIANT SHAPIRO STEPS:2||LAYERS:2||electron energy loss spectroscopy:2||physical phenomena:2||scanning electron microscopy:2||HGTE QUANTUMWELLS:2||BI2TE3:2||SPECTROSCOPY:2||PNJUNCTIONS:2||spinpolarized tunneling:2||INTRINSIC JOSEPHSONJUNCTIONS:2||FIELDS:2||positive magnetoresistance:2||dilute magnetic semiconductor:2||magnetic field:2||scanning transmission electron microscopy:2||QUANTUM OSCILLATIONS:2||TRANSPORTPROPERTIES:2||surface pair current:2||MAGNETORESISTANCE:2||NANORIBBONS:2||INSTABILITY:2||ANDREEV REFLECTION:2||microwave irradiation:2||vertical graphene josephson junction:2||BI2SE3:2||CONDUCTIVITY:2||highTc superconductors:2||DIMENSIONAL ELECTRONGAS:2||graphene:2||Topological insulators:2||Josephson coupling Fraunhofer interference pattern:2||FERROMAGNET:2||DEPENDENCE:2||DETECTOR:2||COHERENCE:2||INJECTION:2||GRAPHENE:1||JOSEPHSONJUNCTIONS:1||LAYERED SUPERCONDUCTOR:1||mode splitting:1||BEHAVIOR:1||spinpolarized transport:1||SUPERCONDUCTING TRANSITION:1||microwave response:1||PSEUDOGAP:1||phase coherence:1||TRANSITIONS:1||Long Josephson junction:1||Charge detection:1||collective resonance modes:1||plasma oscillation modes:1||Superconducting proximity effect:1||Iron pnictide superconductor:1||McMillanRowell oscillations:1||ferromagnetic microstructure:1||superradiant state:1||VOLTAGE:1||branch splitting:1||TENSOR:1||INTERCALATION:1||insitu fabrication:1||NDGAO3:1||DISORDERED METALS:1||GAUGE GLASS:1||LOWTEMPERATURE TRANSPORT:1||spontaneous spin polarization model:1||BIAS:1||emission of electromagnetic waves:1||YBA2CU3O7/PRBA2CU3O7 SUPERLATTICES:1||BOHM:1||SHAPIRO STEPS:1||superconductor/ferromagnet interface:1||OXIDE:1||ANDREEVREFLECTION:1||SinFeAsO single crystal:1||COLLECTIVE MOTION:1||ANGULARDEPENDENCE:1||SUPERCONDUCTIVITY:1||BILAYER GRAPHENE:1||PHOTOLUMINESCENT PROPERTIES:1||SUPERCONDUCTING WEAK LINKS:1||intrinsic Josephson junctions geometrical resonance:1||intrinsic Josephson junction:1||MESOSCOPIC SPINVALVE:1||Bi2212 single crystals:1||intrinsic junctions:1||ANDREEV REFLECTIONS:1||normalmetal/superconductor interface:1||IBI2SR2CACU2OY:1||THERMAL FLUCTUATIONS:1||MIXED STATE:1||BI2.15SR1.85CACU2O8+DELTA:1||intrinsic Josephson effects:1||CACUO:1||QUANTUM POINT CONTACTS:1||resonant tunneling state:1||coherence length:1||NANOWIRE:1||GATES:1||Phase line:1||Thermal activation:1||QUANTUMDOT:1||superconducting proximity effect:1||Andreev interferometer:1||WIRE:1||Josephsonvortexflow branches:1||Bi2212 cuprates:1||LATTICE:1||demannetization effect:1||SUPERCONDUCTING MIRRORS:1||GAS:1||VALLEY TRANSPORT:1||ELECTRODES:1||DEPENDENT TRANSPORT:1||BORNOPPENHEIMER APPROXIMATION:1||collective plasma oscillations:1||fluxon resonance steps:1||STACKS:1||COLLECTIVE DYNAMICS:1||PAIRING SYMMETRY:1||MUON SPIN ROTATION:1||DIMENSIONAL CROSSOVER:1||Bi2Sr2CaCu2Oy highTc superconductors:1||heterojunctions:1||nanostructures:1||surfaces and interfaces:1||QUANTUM TRANSPORT:1||MICROJUNCTIONS:1||RESONATORS:1||STATES:1||FIELD:1||FLUCTUATIONS:1||SCATTERING:1||mode splitting of Josephson vortexflow branches:1||2D superconductivity:1||TRANSISTOR:1||ENERGYGAP:1||SUPERLATTICES:1||IRONBASED SUPERCONDUCTORS:1||PHASEDEPENDENT RESISTANCE:1||QUANTUM PHASETRANSITIONS:1||ELECTRICFIELD:1||HIGH MAGNETICFIELDS:1||NANOWIRE HETEROSTRUCTURES:1||ZNO:1||pair breaking.:1||SUPERCONDUCTING PB:1||domain formation:1||FORCE MICROSCOPY:1||RELAXATION:1||PLASMA RESONANCE:1||coupled Josephson junctions:1||COPPEROXIDE SUPERCONDUCTORS:1||CROSSOVER:1||SIMULATIONS:1||LOWTEMPERATURE:1||CONDUCTORS:1||METALINSULATORTRANSITION:1||SEMICONDUCTOR:1||FIELDEFFECT TRANSISTORS:1||ZEROVOLTAGE STATE:1||constanttemperature interlayer tunneling spectroscopy:1||Josephson supercurrent:1||BIPOLAR SUPERCURRENT:1||Interaction between Josephson and pancake vortices:1||flux jump:1||coaxial heterojunction nanorod:1||Natural Josephson coupling:1||BI2SR2CACU2O8+DELTA:1||VORTEX FLOW:1||TC SUPERCONDUCTORS:1||charge imbalance:1||Andreev diffractometer:1||intercalation:1||surface junction:1||Bi2212:1||tunnelling:1||GRAPHITE:1||GROWTH:1||collective transverse plasma modes:1||GAN:1||Macroscopic quantum tunneling:1||Fluctuation conductivity:1||Abovegap conductance jump:1||Josephson vortex motion:1||Intrinsic Josephson junctions:1||LAYERED SUPERCONDUCTORS:1||BI2SR2CACU2O8+Y:1||INTERFACES:1||BREAKDOWN:1||SYSTEMS:1||Anisotropy ratio:1||Josephson vortex:1||spin relaxation in superconductors:1||bibased single crystals:1||MESOSCOPIC PROXIMITY SUPERCONDUCTOR:1||reentrance of conductance:1||interlayer pair tunneling:1||JOSEPHSON:1||DISORDERED 2DIMENSIONAL SUPERCONDUCTORS:1||INDIUM FILMS:1||excited state:1||REGIME:1||triplet superconductivity:1||FILM:1||SCHOTTKY DIODES:1||peakdiphump structure:1||Kondo effect:1||REENTRANCE:1||Graphene:1||CONTACT:1||BERRYS PHASE:1||2DIMENSIONAL SUPERCONDUCTORS:1||Coulomb diamond:1||magnetic domain:1||spin injection:1||RESONANCE:1||plasma excitation modes:1||FLOW:1||OVERDOPED BI2SR2CACU2O8+DELTA:1||hole doping:1||chemical synthesis:1||phase transitions:1||superconductors:1||VORTEXGLASS SUPERCONDUCTIVITY:1||Kondorelated model:1||RADIATION:1||DOT:1||NANOBELTS:1||Complementarity:1||Closedloop AharonovBohm interferometer:1||pair breaking:1||interlayer phase fluctuation:1||MgB2 thin film:1||CONFINEMENT:1||WALLED CARBON NANOTUBES:1||TRANSITION:9||VORTICES:8||STATE:7||intrinsic Josephson junctions:7||SINGLECRYSTALS:7||JUNCTIONS:5||MODES:5||SUPERCURRENT:5||SUPERCONDUCTOR:5||CONDUCTANCE:5||HIGHTEMPERATURE SUPERCONDUCTORS:5||TRANSPORT:5||PHASE:5||FILMS:4||LOCALIZATION:4||SINGLE DIRAC CONE:4||WIRES:4||MAGNETICFIELD:4||STEPS:3||ELECTRONS:3||proximity effect:3||MODEL:3||ARRAYS:3||INTERFERENCE:3||fluxon dynamics:3||HETEROSTRUCTURES:3||INSULATOR:3||Andreev reflection:3||electronic transport:3||FISKE:3||superconductor:2||ZnO:2||quantum point contact:2||METAL:2||DYNAMICS:2||interlayer Josephson coupling:2||SUPERCONDUCTORS:2||YBA2CU3O7DELTA:2||LAYER:2||DOTS:2||quantum dot:2||Article:2||TRANSISTORS:2||CARBON NANOTUBES:2||GAP:2||MECHANISM:2||LINE:2||GIANT SHAPIRO STEPS:2||LAYERS:2||electron energy loss spectroscopy:2||physical phenomena:2||scanning electron microscopy:2||HGTE QUANTUMWELLS:2||BI2TE3:2||SPECTROSCOPY:2||PNJUNCTIONS:2||spinpolarized tunneling:2||INTRINSIC JOSEPHSONJUNCTIONS:2||FIELDS:2||positive magnetoresistance:2||dilute magnetic semiconductor:2||magnetic field:2||scanning transmission electron microscopy:2||QUANTUM OSCILLATIONS:2||TRANSPORTPROPERTIES:2||surface pair current:2||MAGNETORESISTANCE:2||NANORIBBONS:2||INSTABILITY:2||ANDREEV REFLECTION:2||microwave irradiation:2||vertical graphene josephson junction:2||BI2SE3:2||CONDUCTIVITY:2||highTc superconductors:2||DIMENSIONAL ELECTRONGAS:2||graphene:2||Topological insulators:2||Josephson coupling Fraunhofer interference pattern:2||FERROMAGNET:2||DEPENDENCE:2||DETECTOR:2||COHERENCE:2||INJECTION:2||GRAPHENE:1||JOSEPHSONJUNCTIONS:1||LAYERED SUPERCONDUCTOR:1||mode splitting:1||BEHAVIOR:1||spinpolarized transport:1||SUPERCONDUCTING TRANSITION:1||microwave response:1||PSEUDOGAP:1||phase coherence:1||TRANSITIONS:1||Long Josephson junction:1||Charge detection:1||collective resonance modes:1||plasma oscillation modes:1||Superconducting proximity effect:1||Iron pnictide superconductor:1||McMillanRowell oscillations:1||ferromagnetic microstructure:1||superradiant state:1||VOLTAGE:1||branch splitting:1||TENSOR:1||INTERCALATION:1||insitu fabrication:1||NDGAO3:1||DISORDERED METALS:1||GAUGE GLASS:1||LOWTEMPERATURE TRANSPORT:1||spontaneous spin polarization model:1||BIAS:1||emission of electromagnetic waves:1||YBA2CU3O7/PRBA2CU3O7 SUPERLATTICES:1||BOHM:1||SHAPIRO STEPS:1||superconductor/ferromagnet interface:1||OXIDE:1||ANDREEVREFLECTION:1||SinFeAsO single crystal:1||COLLECTIVE MOTION:1||ANGULARDEPENDENCE:1||SUPERCONDUCTIVITY:1||BILAYER GRAPHENE:1||PHOTOLUMINESCENT PROPERTIES:1||SUPERCONDUCTING WEAK LINKS:1||intrinsic Josephson junctions geometrical resonance:1||intrinsic Josephson junction:1||MESOSCOPIC SPINVALVE:1||Bi2212 single crystals:1||intrinsic junctions:1||ANDREEV REFLECTIONS:1||normalmetal/superconductor interface:1||IBI2SR2CACU2OY:1||THERMAL FLUCTUATIONS:1||MIXED STATE:1||BI2.15SR1.85CACU2O8+DELTA:1||intrinsic Josephson effects:1||CACUO:1||QUANTUM POINT CONTACTS:1||resonant tunneling state:1||coherence length:1||NANOWIRE:1||GATES:1||Phase line:1||Thermal activation:1||QUANTUMDOT:1||superconducting proximity effect:1||Andreev interferometer:1||WIRE:1||Josephsonvortexflow branches:1||Bi2212 cuprates:1||LATTICE:1||demannetization effect:1||SUPERCONDUCTING MIRRORS:1||GAS:1||VALLEY TRANSPORT:1||ELECTRODES:1||DEPENDENT TRANSPORT:1||BORNOPPENHEIMER APPROXIMATION:1||collective plasma oscillations:1||fluxon resonance steps:1||STACKS:1||COLLECTIVE DYNAMICS:1||PAIRING SYMMETRY:1||MUON SPIN ROTATION:1||DIMENSIONAL CROSSOVER:1||Bi2Sr2CaCu2Oy highTc superconductors:1||heterojunctions:1||nanostructures:1||surfaces and interfaces:1||QUANTUM TRANSPORT:1||MICROJUNCTIONS:1||RESONATORS:1||STATES:1||FIELD:1||FLUCTUATIONS:1||SCATTERING:1||mode splitting of Josephson vortexflow branches:1||2D superconductivity:1||TRANSISTOR:1||ENERGYGAP:1||SUPERLATTICES:1||IRONBASED SUPERCONDUCTORS:1||PHASEDEPENDENT RESISTANCE:1||QUANTUM PHASETRANSITIONS:1||ELECTRICFIELD:1||HIGH MAGNETICFIELDS:1||NANOWIRE HETEROSTRUCTURES:1||ZNO:1||pair breaking.:1||SUPERCONDUCTING PB:1||domain formation:1||FORCE MICROSCOPY:1||RELAXATION:1||PLASMA RESONANCE:1||coupled Josephson junctions:1||COPPEROXIDE SUPERCONDUCTORS:1||CROSSOVER:1||SIMULATIONS:1||LOWTEMPERATURE:1||CONDUCTORS:1||METALINSULATORTRANSITION:1||SEMICONDUCTOR:1||FIELDEFFECT TRANSISTORS:1||ZEROVOLTAGE STATE:1||constanttemperature interlayer tunneling spectroscopy:1||Josephson supercurrent:1||BIPOLAR SUPERCURRENT:1||Interaction between Josephson and pancake vortices:1||flux jump:1||coaxial heterojunction nanorod:1||Natural Josephson coupling:1||BI2SR2CACU2O8+DELTA:1||VORTEX FLOW:1||TC SUPERCONDUCTORS:1||charge imbalance:1||Andreev diffractometer:1||intercalation:1||surface junction:1||Bi2212:1||tunnelling:1||GRAPHITE:1||GROWTH:1||collective transverse plasma modes:1||GAN:1||Macroscopic quantum tunneling:1||Fluctuation conductivity:1||Abovegap conductance jump:1||Josephson vortex motion:1||Intrinsic Josephson junctions:1||LAYERED SUPERCONDUCTORS:1||BI2SR2CACU2O8+Y:1||INTERFACES:1||BREAKDOWN:1||SYSTEMS:1||Anisotropy ratio:1||Josephson vortex:1||spin relaxation in superconductors:1||bibased single crystals:1||MESOSCOPIC PROXIMITY SUPERCONDUCTOR:1||reentrance of conductance:1||interlayer pair tunneling:1||JOSEPHSON:1||DISORDERED 2DIMENSIONAL SUPERCONDUCTORS:1||INDIUM FILMS:1||excited state:1||REGIME:1||triplet superconductivity:1||FILM:1||SCHOTTKY DIODES:1||peakdiphump structure:1||Kondo effect:1||REENTRANCE:1||Graphene:1||CONTACT:1||BERRYS PHASE:1||2DIMENSIONAL SUPERCONDUCTORS:1||Coulomb diamond:1||magnetic domain:1||spin injection:1||RESONANCE:1||plasma excitation modes:1||FLOW:1||OVERDOPED BI2SR2CACU2O8+DELTA:1||hole doping:1||chemical synthesis:1||phase transitions:1||superconductors:1||VORTEXGLASS SUPERCONDUCTIVITY:1||Kondorelated model:1||RADIATION:1||DOT:1||NANOBELTS:1||Complementarity:1||Closedloop AharonovBohm interferometer:1||pair breaking:1||interlayer phase fluctuation:1||MgB2 thin film:1||CONFINEMENT:1||WALLED CARBON NANOTUBES:1||TRANSITION:9||VORTICES:8||STATE:7||intrinsic Josephson junctions:7||SINGLECRYSTALS:7||JUNCTIONS:5||MODES:5||SUPERCURRENT:5||SUPERCONDUCTOR:5||CONDUCTANCE:5||HIGHTEMPERATURE SUPERCONDUCTORS:5||TRANSPORT:5||PHASE:5||FILMS:4||LOCALIZATION:4||SINGLE DIRAC CONE:4||WIRES:4||MAGNETICFIELD:4||STEPS:3||ELECTRONS:3||proximity effect:3||MODEL:3||ARRAYS:3||INTERFERENCE:3||fluxon dynamics:3||HETEROSTRUCTURES:3||INSULATOR:3||Andreev reflection:3||electronic transport:3||FISKE:3||superconductor:2||ZnO:2||quantum point contact:2||METAL:2||DYNAMICS:2||interlayer Josephson coupling:2||SUPERCONDUCTORS:2||YBA2CU3O7DELTA:2||LAYER:2||DOTS:2||quantum dot:2||Article:2||TRANSISTORS:2||CARBON NANOTUBES:2||GAP:2||MECHANISM:2||LINE:2||GIANT SHAPIRO STEPS:2||LAYERS:2||electron energy loss spectroscopy:2||physical phenomena:2||scanning electron microscopy:2||HGTE QUANTUMWELLS:2||BI2TE3:2||SPECTROSCOPY:2||PNJUNCTIONS:2||spinpolarized tunneling:2||INTRINSIC JOSEPHSONJUNCTIONS:2||FIELDS:2||positive magnetoresistance:2||dilute magnetic semiconductor:2||magnetic field:2||scanning transmission electron microscopy:2||QUANTUM OSCILLATIONS:2||TRANSPORTPROPERTIES:2||surface pair current:2||MAGNETORESISTANCE:2||NANORIBBONS:2||INSTABILITY:2||ANDREEV REFLECTION:2||microwave irradiation:2||vertical graphene josephson junction:2||BI2SE3:2||CONDUCTIVITY:2||highTc superconductors:2||DIMENSIONAL ELECTRONGAS:2||graphene:2||Topological insulators:2||Josephson coupling Fraunhofer interference pattern:2||FERROMAGNET:2||DEPENDENCE:2||DETECTOR:2||COHERENCE:2||INJECTION:2||GRAPHENE:1||JOSEPHSONJUNCTIONS:1||LAYERED SUPERCONDUCTOR:1||mode splitting:1||BEHAVIOR:1||spinpolarized transport:1||SUPERCONDUCTING TRANSITION:1||microwave response:1||PSEUDOGAP:1||phase coherence:1||TRANSITIONS:1||Long Josephson junction:1||Charge detection:1||collective resonance modes:1||plasma oscillation modes:1||Superconducting proximity effect:1||Iron pnictide superconductor:1||McMillanRowell oscillations:1||ferromagnetic microstructure:1||superradiant state:1||VOLTAGE:1||branch splitting:1||TENSOR:1||INTERCALATION:1||insitu fabrication:1||NDGAO3:1||DISORDERED METALS:1||GAUGE GLASS:1||LOWTEMPERATURE TRANSPORT:1||spontaneous spin polarization model:1||BIAS:1||emission of electromagnetic waves:1||YBA2CU3O7/PRBA2CU3O7 SUPERLATTICES:1||BOHM:1||SHAPIRO STEPS:1||superconductor/ferromagnet interface:1||OXIDE:1||ANDREEVREFLECTION:1||SinFeAsO single crystal:1||COLLECTIVE MOTION:1||ANGULARDEPENDENCE:1||SUPERCONDUCTIVITY:1||BILAYER GRAPHENE:1||PHOTOLUMINESCENT PROPERTIES:1||SUPERCONDUCTING WEAK LINKS:1||intrinsic Josephson junctions geometrical resonance:1||intrinsic Josephson junction:1||MESOSCOPIC SPINVALVE:1||Bi2212 single crystals:1||intrinsic junctions:1||ANDREEV REFLECTIONS:1||normalmetal/superconductor interface:1||IBI2SR2CACU2OY:1||THERMAL FLUCTUATIONS:1||MIXED STATE:1||BI2.15SR1.85CACU2O8+DELTA:1||intrinsic Josephson effects:1||CACUO:1||QUANTUM POINT CONTACTS:1||resonant tunneling state:1||coherence length:1||NANOWIRE:1||GATES:1||Phase line:1||Thermal activation:1||QUANTUMDOT:1||superconducting proximity effect:1||Andreev interferometer:1||WIRE:1||Josephsonvortexflow branches:1||Bi2212 cuprates:1||LATTICE:1||demannetization effect:1||SUPERCONDUCTING MIRRORS:1||GAS:1||VALLEY TRANSPORT:1||ELECTRODES:1||DEPENDENT TRANSPORT:1||BORNOPPENHEIMER APPROXIMATION:1||collective plasma oscillations:1||fluxon resonance steps:1||STACKS:1||COLLECTIVE DYNAMICS:1||PAIRING SYMMETRY:1||MUON SPIN ROTATION:1||DIMENSIONAL CROSSOVER:1||Bi2Sr2CaCu2Oy highTc superconductors:1||heterojunctions:1||nanostructures:1||surfaces and interfaces:1||QUANTUM TRANSPORT:1||MICROJUNCTIONS:1||RESONATORS:1||STATES:1||FIELD:1||FLUCTUATIONS:1||SCATTERING:1||mode splitting of Josephson vortexflow branches:1||2D superconductivity:1||TRANSISTOR:1||ENERGYGAP:1||SUPERLATTICES:1||IRONBASED SUPERCONDUCTORS:1||PHASEDEPENDENT RESISTANCE:1||QUANTUM PHASETRANSITIONS:1||ELECTRICFIELD:1||HIGH MAGNETICFIELDS:1||NANOWIRE HETEROSTRUCTURES:1||ZNO:1||pair breaking.:1||SUPERCONDUCTING PB:1||domain formation:1||FORCE MICROSCOPY:1||RELAXATION:1||PLASMA RESONANCE:1||coupled Josephson junctions:1||COPPEROXIDE SUPERCONDUCTORS:1||CROSSOVER:1||SIMULATIONS:1||LOWTEMPERATURE:1||CONDUCTORS:1||METALINSULATORTRANSITION:1||SEMICONDUCTOR:1||FIELDEFFECT TRANSISTORS:1||ZEROVOLTAGE STATE:1||constanttemperature interlayer tunneling spectroscopy:1||Josephson supercurrent:1||BIPOLAR SUPERCURRENT:1||Interaction between Josephson and pancake vortices:1||flux jump:1||coaxial heterojunction nanorod:1||Natural Josephson coupling:1||BI2SR2CACU2O8+DELTA:1||VORTEX FLOW:1||TC SUPERCONDUCTORS:1||charge imbalance:1||Andreev diffractometer:1||intercalation:1||surface junction:1||Bi2212:1||tunnelling:1||GRAPHITE:1||GROWTH:1||collective transverse plasma modes:1||GAN:1||Macroscopic quantum tunneling:1||Fluctuation conductivity:1||Abovegap conductance jump:1||Josephson vortex motion:1||Intrinsic Josephson junctions:1||LAYERED SUPERCONDUCTORS:1||BI2SR2CACU2O8+Y:1||INTERFACES:1||BREAKDOWN:1||SYSTEMS:1||Anisotropy ratio:1||Josephson vortex:1||spin relaxation in superconductors:1||bibased single crystals:1||MESOSCOPIC PROXIMITY SUPERCONDUCTOR:1||reentrance of conductance:1||interlayer pair tunneling:1||JOSEPHSON:1||DISORDERED 2DIMENSIONAL SUPERCONDUCTORS:1||INDIUM FILMS:1||excited state:1||REGIME:1||triplet superconductivity:1||FILM:1||SCHOTTKY DIODES:1||peakdiphump structure:1||Kondo effect:1||REENTRANCE:1||Graphene:1||CONTACT:1||BERRYS PHASE:1||2DIMENSIONAL SUPERCONDUCTORS:1||Coulomb diamond:1||magnetic domain:1||spin injection:1||RESONANCE:1||plasma excitation modes:1||FLOW:1||OVERDOPED BI2SR2CACU2O8+DELTA:1||hole doping:1||chemical synthesis:1||phase transitions:1||superconductors:1||VORTEXGLASS SUPERCONDUCTIVITY:1||Kondorelated model:1||RADIATION:1||DOT:1||NANOBELTS:1||Complementarity:1||Closedloop AharonovBohm interferometer:1||pair breaking:1||interlayer phase fluctuation:1||MgB2 thin film:1||CONFINEMENT:1||WALLED CARBON NANOTUBES:1||TRANSITION:9||VORTICES:8||STATE:7||intrinsic Josephson junctions:7||SINGLECRYSTALS:7||JUNCTIONS:5||MODES:5||SUPERCURRENT:5||SUPERCONDUCTOR:5||CONDUCTANCE:5||HIGHTEMPERATURE SUPERCONDUCTORS:5||TRANSPORT:5||PHASE:5||FILMS:4||LOCALIZATION:4||SINGLE DIRAC CONE:4||WIRES:4||MAGNETICFIELD:4||STEPS:3||ELECTRONS:3||proximity effect:3||MODEL:3||ARRAYS:3||INTERFERENCE:3||fluxon dynamics:3||HETEROSTRUCTURES:3||INSULATOR:3||Andreev reflection:3||electronic transport:3||FISKE:3||superconductor:2||ZnO:2||quantum point contact:2||METAL:2||DYNAMICS:2||interlayer Josephson coupling:2||SUPERCONDUCTORS:2||YBA2CU3O7DELTA:2||LAYER:2||DOTS:2||quantum dot:2||Article:2||TRANSISTORS:2||CARBON NANOTUBES:2||GAP:2||MECHANISM:2||LINE:2||GIANT SHAPIRO STEPS:2||LAYERS:2||electron energy loss spectroscopy:2||physical phenomena:2||scanning electron microscopy:2||HGTE QUANTUMWELLS:2||BI2TE3:2||SPECTROSCOPY:2||PNJUNCTIONS:2||spinpolarized tunneling:2||INTRINSIC JOSEPHSONJUNCTIONS:2||FIELDS:2||positive magnetoresistance:2||dilute magnetic semiconductor:2||magnetic field:2||scanning transmission electron microscopy:2||QUANTUM OSCILLATIONS:2||TRANSPORTPROPERTIES:2||surface pair current:2||MAGNETORESISTANCE:2||NANORIBBONS:2||INSTABILITY:2||ANDREEV REFLECTION:2||microwave irradiation:2||vertical graphene josephson junction:2||BI2SE3:2||CONDUCTIVITY:2||highTc superconductors:2||DIMENSIONAL ELECTRONGAS:2||graphene:2||Topological insulators:2||Josephson coupling Fraunhofer interference pattern:2||FERROMAGNET:2||DEPENDENCE:2||DETECTOR:2||COHERENCE:2||INJECTION:2||GRAPHENE:1||JOSEPHSONJUNCTIONS:1||LAYERED SUPERCONDUCTOR:1||mode splitting:1||BEHAVIOR:1||spinpolarized transport:1||SUPERCONDUCTING TRANSITION:1||microwave response:1||PSEUDOGAP:1||phase coherence:1||TRANSITIONS:1||Long Josephson junction:1||Charge detection:1||collective resonance modes:1||plasma oscillation modes:1||Superconducting proximity effect:1||Iron pnictide superconductor:1||McMillanRowell oscillations:1||ferromagnetic microstructure:1||superradiant state:1||VOLTAGE:1||branch splitting:1||TENSOR:1||INTERCALATION:1||insitu fabrication:1||NDGAO3:1||DISORDERED METALS:1||GAUGE GLASS:1||LOWTEMPERATURE TRANSPORT:1||spontaneous spin polarization model:1||BIAS:1||emission of electromagnetic waves:1||YBA2CU3O7/PRBA2CU3O7 SUPERLATTICES:1||BOHM:1||SHAPIRO STEPS:1||superconductor/ferromagnet interface:1||OXIDE:1||ANDREEVREFLECTION:1||SinFeAsO single crystal:1||COLLECTIVE MOTION:1||ANGULARDEPENDENCE:1||SUPERCONDUCTIVITY:1||BILAYER GRAPHENE:1||PHOTOLUMINESCENT PROPERTIES:1||SUPERCONDUCTING WEAK LINKS:1||intrinsic Josephson junctions geometrical resonance:1||intrinsic Josephson junction:1||MESOSCOPIC SPINVALVE:1||Bi2212 single crystals:1||intrinsic junctions:1||ANDREEV REFLECTIONS:1||normalmetal/superconductor interface:1||IBI2SR2CACU2OY:1||THERMAL FLUCTUATIONS:1||MIXED STATE:1||BI2.15SR1.85CACU2O8+DELTA:1||intrinsic Josephson effects:1||CACUO:1||QUANTUM POINT CONTACTS:1||resonant tunneling state:1||coherence length:1||NANOWIRE:1||GATES:1||Phase line:1||Thermal activation:1||QUANTUMDOT:1||superconducting proximity effect:1||Andreev interferometer:1||WIRE:1||Josephsonvortexflow branches:1||Bi2212 cuprates:1||LATTICE:1||demannetization effect:1||SUPERCONDUCTING MIRRORS:1||GAS:1||VALLEY TRANSPORT:1||ELECTRODES:1||DEPENDENT TRANSPORT:1||BORNOPPENHEIMER APPROXIMATION:1||collective plasma oscillations:1||fluxon resonance steps:1||STACKS:1||COLLECTIVE DYNAMICS:1||PAIRING SYMMETRY:1||MUON SPIN ROTATION:1||DIMENSIONAL CROSSOVER:1||Bi2Sr2CaCu2Oy highTc superconductors:1||heterojunctions:1||nanostructures:1||surfaces and interfaces:1||QUANTUM TRANSPORT:1||MICROJUNCTIONS:1||RESONATORS:1||STATES:1||FIELD:1||FLUCTUATIONS:1||SCATTERING:1||mode splitting of Josephson vortexflow branches:1||2D superconductivity:1||TRANSISTOR:1||ENERGYGAP:1||SUPERLATTICES:1||IRONBASED SUPERCONDUCTORS:1||PHASEDEPENDENT RESISTANCE:1||QUANTUM PHASETRANSITIONS:1||ELECTRICFIELD:1||HIGH MAGNETICFIELDS:1||NANOWIRE HETEROSTRUCTURES:1||ZNO:1||pair breaking.:1||SUPERCONDUCTING PB:1||domain formation:1||FORCE MICROSCOPY:1||RELAXATION:1||PLASMA RESONANCE:1||coupled Josephson junctions:1||COPPEROXIDE SUPERCONDUCTORS:1||CROSSOVER:1||SIMULATIONS:1||LOWTEMPERATURE:1||CONDUCTORS:1||METALINSULATORTRANSITION:1||SEMICONDUCTOR:1||FIELDEFFECT TRANSISTORS:1||ZEROVOLTAGE STATE:1||constanttemperature interlayer tunneling spectroscopy:1||Josephson supercurrent:1||BIPOLAR SUPERCURRENT:1||Interaction between Josephson and pancake vortices:1||flux jump:1||coaxial heterojunction nanorod:1||Natural Josephson coupling:1||BI2SR2CACU2O8+DELTA:1||VORTEX FLOW:1||TC SUPERCONDUCTORS:1||charge imbalance:1||Andreev diffractometer:1||intercalation:1||surface junction:1||Bi2212:1||tunnelling:1||GRAPHITE:1||GROWTH:1||collective transverse plasma modes:1||GAN:1||Macroscopic quantum tunneling:1||Fluctuation conductivity:1||Abovegap conductance jump:1||Josephson vortex motion:1||Intrinsic Josephson junctions:1||LAYERED SUPERCONDUCTORS:1||BI2SR2CACU2O8+Y:1||INTERFACES:1||BREAKDOWN:1||SYSTEMS:1||Anisotropy ratio:1||Josephson vortex:1||spin relaxation in superconductors:1||bibased single crystals:1||MESOSCOPIC PROXIMITY SUPERCONDUCTOR:1||reentrance of conductance:1||interlayer pair tunneling:1||JOSEPHSON:1||DISORDERED 2DIMENSIONAL SUPERCONDUCTORS:1||INDIUM FILMS:1||excited state:1||REGIME:1||triplet superconductivity:1||FILM:1||SCHOTTKY DIODES:1||peakdiphump structure:1||Kondo effect:1||REENTRANCE:1||Graphene:1||CONTACT:1||BERRYS PHASE:1||2DIMENSIONAL SUPERCONDUCTORS:1||Coulomb diamond:1||magnetic domain:1||spin injection:1||RESONANCE:1||plasma excitation modes:1||FLOW:1||OVERDOPED BI2SR2CACU2O8+DELTA:1||hole doping:1||chemical synthesis:1||phase transitions:1||superconductors:1||VORTEXGLASS SUPERCONDUCTIVITY:1||Kondorelated model:1||RADIATION:1||DOT:1||NANOBELTS:1||Complementarity:1||Closedloop AharonovBohm interferometer:1||pair breaking:1||interlayer phase fluctuation:1||MgB2 thin film:1||CONFINEMENT:1||WALLED CARBON NANOTUBES:1||TRANSITION:9||VORTICES:8||STATE:7||intrinsic Josephson junctions:7||SINGLECRYSTALS:7||JUNCTIONS:5||MODES:5||SUPERCURRENT:5||SUPERCONDUCTOR:5||CONDUCTANCE:5||HIGHTEMPERATURE SUPERCONDUCTORS:5||TRANSPORT:5||PHASE:5||FILMS:4||LOCALIZATION:4||SINGLE DIRAC CONE:4||WIRES:4||MAGNETICFIELD:4||STEPS:3||ELECTRONS:3||proximity effect:3||MODEL:3||ARRAYS:3||INTERFERENCE:3||fluxon dynamics:3||HETEROSTRUCTURES:3||INSULATOR:3||Andreev reflection:3||electronic transport:3||FISKE:3||superconductor:2||ZnO:2||quantum point contact:2||METAL:2||DYNAMICS:2||interlayer Josephson coupling:2||SUPERCONDUCTORS:2||YBA2CU3O7DELTA:2||LAYER:2||DOTS:2||quantum dot:2||Article:2||TRANSISTORS:2||CARBON NANOTUBES:2||GAP:2||MECHANISM:2||LINE:2||GIANT SHAPIRO STEPS:2||LAYERS:2||electron energy loss spectroscopy:2||physical phenomena:2||scanning electron microscopy:2||HGTE QUANTUMWELLS:2||BI2TE3:2||SPECTROSCOPY:2||PNJUNCTIONS:2||spinpolarized tunneling:2||INTRINSIC JOSEPHSONJUNCTIONS:2||FIELDS:2||positive magnetoresistance:2||dilute magnetic semiconductor:2||magnetic field:2||scanning transmission electron microscopy:2||QUANTUM OSCILLATIONS:2||TRANSPORTPROPERTIES:2||surface pair current:2||MAGNETORESISTANCE:2||NANORIBBONS:2||INSTABILITY:2||ANDREEV REFLECTION:2||microwave irradiation:2||vertical graphene josephson junction:2||BI2SE3:2||CONDUCTIVITY:2||highTc superconductors:2||DIMENSIONAL ELECTRONGAS:2||graphene:2||Topological insulators:2||Josephson coupling Fraunhofer interference pattern:2||FERROMAGNET:2||DEPENDENCE:2||DETECTOR:2||COHERENCE:2||INJECTION:2||GRAPHENE:1||JOSEPHSONJUNCTIONS:1||LAYERED SUPERCONDUCTOR:1||mode splitting:1||BEHAVIOR:1||spinpolarized transport:1||SUPERCONDUCTING TRANSITION:1||microwave response:1||PSEUDOGAP:1||phase coherence:1||TRANSITIONS:1||Long Josephson junction:1||Charge detection:1||collective resonance modes:1||plasma oscillation modes:1||Superconducting proximity effect:1||Iron pnictide superconductor:1||McMillanRowell oscillations:1||ferromagnetic microstructure:1||superradiant state:1||VOLTAGE:1||branch splitting:1||TENSOR:1||INTERCALATION:1||insitu fabrication:1||NDGAO3:1||DISORDERED METALS:1||GAUGE GLASS:1||LOWTEMPERATURE TRANSPORT:1||spontaneous spin polarization model:1||BIAS:1||emission of electromagnetic waves:1||YBA2CU3O7/PRBA2CU3O7 SUPERLATTICES:1||BOHM:1||SHAPIRO STEPS:1||superconductor/ferromagnet interface:1||OXIDE:1||ANDREEVREFLECTION:1||SinFeAsO single crystal:1||COLLECTIVE MOTION:1||ANGULARDEPENDENCE:1||SUPERCONDUCTIVITY:1||BILAYER GRAPHENE:1||PHOTOLUMINESCENT PROPERTIES:1||SUPERCONDUCTING WEAK LINKS:1||intrinsic Josephson junctions geometrical resonance:1||intrinsic Josephson junction:1||MESOSCOPIC SPINVALVE:1||Bi2212 single crystals:1||intrinsic junctions:1||ANDREEV REFLECTIONS:1||normalmetal/superconductor interface:1||IBI2SR2CACU2OY:1||THERMAL FLUCTUATIONS:1||MIXED STATE:1||BI2.15SR1.85CACU2O8+DELTA:1||intrinsic Josephson effects:1||CACUO:1||QUANTUM POINT CONTACTS:1||resonant tunneling state:1||coherence length:1||NANOWIRE:1||GATES:1||Phase line:1||Thermal activation:1||QUANTUMDOT:1||superconducting proximity effect:1||Andreev interferometer:1||WIRE:1||Josephsonvortexflow branches:1||Bi2212 cuprates:1||LATTICE:1||demannetization effect:1||SUPERCONDUCTING MIRRORS:1||GAS:1||VALLEY TRANSPORT:1||ELECTRODES:1||DEPENDENT TRANSPORT:1||BORNOPPENHEIMER APPROXIMATION:1||collective plasma oscillations:1||fluxon resonance steps:1||STACKS:1||COLLECTIVE DYNAMICS:1||PAIRING SYMMETRY:1||MUON SPIN ROTATION:1||DIMENSIONAL CROSSOVER:1||Bi2Sr2CaCu2Oy highTc superconductors:1||heterojunctions:1||nanostructures:1||surfaces and interfaces:1||QUANTUM TRANSPORT:1||MICROJUNCTIONS:1||RESONATORS:1||STATES:1||FIELD:1||FLUCTUATIONS:1||SCATTERING:1||mode splitting of Josephson vortexflow branches:1||2D superconductivity:1||TRANSISTOR:1||ENERGYGAP:1||SUPERLATTICES:1||IRONBASED SUPERCONDUCTORS:1||PHASEDEPENDENT RESISTANCE:1||QUANTUM PHASETRANSITIONS:1||ELECTRICFIELD:1||HIGH MAGNETICFIELDS:1||NANOWIRE HETEROSTRUCTURES:1||ZNO:1||pair breaking.:1||SUPERCONDUCTING PB:1||domain formation:1||FORCE MICROSCOPY:1||RELAXATION:1||PLASMA RESONANCE:1||coupled Josephson junctions:1||COPPEROXIDE SUPERCONDUCTORS:1||CROSSOVER:1||SIMULATIONS:1||LOWTEMPERATURE:1||CONDUCTORS:1||METALINSULATORTRANSITION:1||SEMICONDUCTOR:1||FIELDEFFECT TRANSISTORS:1||ZEROVOLTAGE STATE:1||constanttemperature interlayer tunneling spectroscopy:1||Josephson supercurrent:1||BIPOLAR SUPERCURRENT:1||Interaction between Josephson and pancake vortices:1||flux jump:1||coaxial heterojunction nanorod:1||Natural Josephson coupling:1||BI2SR2CACU2O8+DELTA:1||VORTEX FLOW:1||TC SUPERCONDUCTORS:1||charge imbalance:1||Andreev diffractometer:1||intercalation:1||surface junction:1||Bi2212:1||tunnelling:1||GRAPHITE:1||GROWTH:1||collective transverse plasma modes:1||GAN:1||Macroscopic quantum tunneling:1||Fluctuation conductivity:1||Abovegap conductance jump:1||Josephson vortex motion:1||Intrinsic Josephson junctions:1||LAYERED SUPERCONDUCTORS:1||BI2SR2CACU2O8+Y:1||INTERFACES:1||BREAKDOWN:1||SYSTEMS:1||Anisotropy ratio:1||Josephson vortex:1||spin relaxation in superconductors:1||bibased single crystals:1||MESOSCOPIC PROXIMITY SUPERCONDUCTOR:1||reentrance of conductance:1||interlayer pair tunneling:1||JOSEPHSON:1||DISORDERED 2DIMENSIONAL SUPERCONDUCTORS:1||INDIUM FILMS:1||excited state:1||REGIME:1||triplet superconductivity:1||FILM:1||SCHOTTKY DIODES:1||peakdiphump structure:1||Kondo effect:1||REENTRANCE:1||Graphene:1||CONTACT:1||BERRYS PHASE:1||2DIMENSIONAL SUPERCONDUCTORS:1||Coulomb diamond:1||magnetic domain:1||spin injection:1||RESONANCE:1||plasma excitation modes:1||FLOW:1||OVERDOPED BI2SR2CACU2O8+DELTA:1||hole doping:1||chemical synthesis:1||phase transitions:1||superconductors:1||VORTEXGLASS SUPERCONDUCTIVITY:1||Kondorelated model:1||RADIATION:1||DOT:1||NANOBELTS:1||Complementarity:1||Closedloop AharonovBohm interferometer:1||pair breaking:1||interlayer phase fluctuation:1||MgB2 thin film:1||CONFINEMENT:1||WALLED CARBON NANOTUBES:1||TRANSITION:9||VORTICES:8||STATE:7||intrinsic Josephson junctions:7||SINGLECRYSTALS:7||JUNCTIONS:5||MODES:5||SUPERCURRENT:5||SUPERCONDUCTOR:5||CONDUCTANCE:5||HIGHTEMPERATURE SUPERCONDUCTORS:5||TRANSPORT:5||PHASE:5||FILMS:4||LOCALIZATION:4||SINGLE DIRAC CONE:4||WIRES:4||MAGNETICFIELD:4||STEPS:3||ELECTRONS:3||proximity effect:3||MODEL:3||ARRAYS:3||INTERFERENCE:3||fluxon dynamics:3||HETEROSTRUCTURES:3||INSULATOR:3||Andreev reflection:3||electronic transport:3||FISKE:3||superconductor:2||ZnO:2||quantum point contact:2||METAL:2||DYNAMICS:2||interlayer Josephson coupling:2||SUPERCONDUCTORS:2||YBA2CU3O7DELTA:2||LAYER:2||DOTS:2||quantum dot:2||Article:2||TRANSISTORS:2||CARBON NANOTUBES:2||GAP:2||MECHANISM:2||LINE:2||GIANT SHAPIRO STEPS:2||LAYERS:2||electron energy loss spectroscopy:2||physical phenomena:2||scanning electron microscopy:2||HGTE QUANTUMWELLS:2||BI2TE3:2||SPECTROSCOPY:2||PNJUNCTIONS:2||spinpolarized tunneling:2||INTRINSIC JOSEPHSONJUNCTIONS:2||FIELDS:2||positive magnetoresistance:2||dilute magnetic semiconductor:2||magnetic field:2||scanning transmission electron microscopy:2||QUANTUM OSCILLATIONS:2||TRANSPORTPROPERTIES:2||surface pair current:2||MAGNETORESISTANCE:2||NANORIBBONS:2||INSTABILITY:2||ANDREEV REFLECTION:2||microwave irradiation:2||vertical graphene josephson junction:2||BI2SE3:2||CONDUCTIVITY:2||highTc superconductors:2||DIMENSIONAL ELECTRONGAS:2||graphene:2||Topological insulators:2||Josephson coupling Fraunhofer interference pattern:2||FERROMAGNET:2||DEPENDENCE:2||DETECTOR:2||COHERENCE:2||INJECTION:2||GRAPHENE:1||JOSEPHSONJUNCTIONS:1||LAYERED SUPERCONDUCTOR:1||mode splitting:1||BEHAVIOR:1||spinpolarized transport:1||SUPERCONDUCTING TRANSITION:1||microwave response:1||PSEUDOGAP:1||phase coherence:1||TRANSITIONS:1||Long Josephson junction:1||Charge detection:1||collective resonance modes:1||plasma oscillation modes:1||Superconducting proximity effect:1||Iron pnictide superconductor:1||McMillanRowell oscillations:1||ferromagnetic microstructure:1||superradiant state:1||VOLTAGE:1||branch splitting:1||TENSOR:1||INTERCALATION:1||insitu fabrication:1||NDGAO3:1||DISORDERED METALS:1||GAUGE GLASS:1||LOWTEMPERATURE TRANSPORT:1||spontaneous spin polarization model:1||BIAS:1||emission of electromagnetic waves:1||YBA2CU3O7/PRBA2CU3O7 SUPERLATTICES:1||BOHM:1||SHAPIRO STEPS:1||superconductor/ferromagnet interface:1||OXIDE:1||ANDREEVREFLECTION:1||SinFeAsO single crystal:1||COLLECTIVE MOTION:1||ANGULARDEPENDENCE:1||SUPERCONDUCTIVITY:1||BILAYER GRAPHENE:1||PHOTOLUMINESCENT PROPERTIES:1||SUPERCONDUCTING WEAK LINKS:1||intrinsic Josephson junctions geometrical resonance:1||intrinsic Josephson junction:1||MESOSCOPIC SPINVALVE:1||Bi2212 single crystals:1||intrinsic junctions:1||ANDREEV REFLECTIONS:1||normalmetal/superconductor interface:1||IBI2SR2CACU2OY:1||THERMAL FLUCTUATIONS:1||MIXED STATE:1||BI2.15SR1.85CACU2O8+DELTA:1||intrinsic Josephson effects:1||CACUO:1||QUANTUM POINT CONTACTS:1||resonant tunneling state:1||coherence length:1||NANOWIRE:1||GATES:1||Phase line:1||Thermal activation:1||QUANTUMDOT:1||superconducting proximity effect:1||Andreev interferometer:1||WIRE:1||Josephsonvortexflow branches:1||Bi2212 cuprates:1||LATTICE:1||demannetization effect:1||SUPERCONDUCTING MIRRORS:1||GAS:1||VALLEY TRANSPORT:1||ELECTRODES:1||DEPENDENT TRANSPORT:1||BORNOPPENHEIMER APPROXIMATION:1||collective plasma oscillations:1||fluxon resonance steps:1||STACKS:1||COLLECTIVE DYNAMICS:1||PAIRING SYMMETRY:1||MUON SPIN ROTATION:1||DIMENSIONAL CROSSOVER:1||Bi2Sr2CaCu2Oy highTc superconductors:1||heterojunctions:1||nanostructures:1||surfaces and interfaces:1||QUANTUM TRANSPORT:1||MICROJUNCTIONS:1||RESONATORS:1||STATES:1||FIELD:1||FLUCTUATIONS:1||SCATTERING:1||mode splitting of Josephson vortexflow branches:1||2D superconductivity:1||TRANSISTOR:1||ENERGYGAP:1||SUPERLATTICES:1||IRONBASED SUPERCONDUCTORS:1||PHASEDEPENDENT RESISTANCE:1||QUANTUM PHASETRANSITIONS:1||ELECTRICFIELD:1||HIGH MAGNETICFIELDS:1||NANOWIRE HETEROSTRUCTURES:1||ZNO:1||pair breaking.:1||SUPERCONDUCTING PB:1||domain formation:1||FORCE MICROSCOPY:1||RELAXATION:1||PLASMA RESONANCE:1||coupled Josephson junctions:1||COPPEROXIDE SUPERCONDUCTORS:1||CROSSOVER:1||SIMULATIONS:1||LOWTEMPERATURE:1||CONDUCTORS:1||METALINSULATORTRANSITION:1||SEMICONDUCTOR:1||FIELDEFFECT TRANSISTORS:1||ZEROVOLTAGE STATE:1||constanttemperature interlayer tunneling spectroscopy:1||Josephson supercurrent:1||BIPOLAR SUPERCURRENT:1||Interaction between Josephson and pancake vortices:1||flux jump:1||coaxial heterojunction nanorod:1||Natural Josephson coupling:1||BI2SR2CACU2O8+DELTA:1||VORTEX FLOW:1||TC SUPERCONDUCTORS:1||charge imbalance:1||Andreev diffractometer:1||intercalation:1||surface junction:1||Bi2212:1||tunnelling:1||GRAPHITE:1||GROWTH:1||collective transverse plasma modes:1||GAN:1||Macroscopic quantum tunneling:1||Fluctuation conductivity:1||Abovegap conductance jump:1||Josephson vortex motion:1||Intrinsic Josephson junctions:1||LAYERED SUPERCONDUCTORS:1||BI2SR2CACU2O8+Y:1||INTERFACES:1||BREAKDOWN:1||SYSTEMS:1||Anisotropy ratio:1||Josephson vortex:1||spin relaxation in superconductors:1||bibased single crystals:1||MESOSCOPIC PROXIMITY SUPERCONDUCTOR:1||reentrance of conductance:1||interlayer pair tunneling:1||JOSEPHSON:1||DISORDERED 2DIMENSIONAL SUPERCONDUCTORS:1||INDIUM FILMS:1||excited state:1||REGIME:1||triplet superconductivity:1||FILM:1||SCHOTTKY DIODES:1||peakdiphump structure:1||Kondo effect:1||REENTRANCE:1||Graphene:1||CONTACT:1||BERRYS PHASE:1||2DIMENSIONAL SUPERCONDUCTORS:1||Coulomb diamond:1||magnetic domain:1||spin injection:1||RESONANCE:1||plasma excitation modes:1||FLOW:1||OVERDOPED BI2SR2CACU2O8+DELTA:1||hole doping:1||chemical synthesis:1||phase transitions:1||superconductors:1||VORTEXGLASS SUPERCONDUCTIVITY:1||Kondorelated model:1||RADIATION:1||DOT:1||NANOBELTS:1||Complementarity:1||Closedloop AharonovBohm interferometer:1||pair breaking:1||interlayer phase fluctuation:1||MgB2 thin film:1||CONFINEMENT:1||WALLED CARBON NANOTUBES:1||TRANSITION:9||VORTICES:8||STATE:7||intrinsic Josephson junctions:7||SINGLECRYSTALS:7||JUNCTIONS:5||MODES:5||SUPERCURRENT:5||SUPERCONDUCTOR:5||CONDUCTANCE:5||HIGHTEMPERATURE SUPERCONDUCTORS:5||TRANSPORT:5||PHASE:5||FILMS:4||LOCALIZATION:4||SINGLE DIRAC CONE:4||WIRES:4||MAGNETICFIELD:4||STEPS:3||ELECTRONS:3||proximity effect:3||MODEL:3||ARRAYS:3||INTERFERENCE:3||fluxon dynamics:3||HETEROSTRUCTURES:3||INSULATOR:3||Andreev reflection:3||electronic transport:3||FISKE:3||superconductor:2||ZnO:2||quantum point contact:2||METAL:2||DYNAMICS:2||interlayer Josephson coupling:2||SUPERCONDUCTORS:2||YBA2CU3O7DELTA:2||LAYER:2||DOTS:2||quantum dot:2||Article:2||TRANSISTORS:2||CARBON NANOTUBES:2||GAP:2||MECHANISM:2||LINE:2||GIANT SHAPIRO STEPS:2||LAYERS:2||electron energy loss spectroscopy:2||physical phenomena:2||scanning electron microscopy:2||HGTE QUANTUMWELLS:2||BI2TE3:2||SPECTROSCOPY:2||PNJUNCTIONS:2||spinpolarized tunneling:2||INTRINSIC JOSEPHSONJUNCTIONS:2||FIELDS:2||positive magnetoresistance:2||dilute magnetic semiconductor:2||magnetic field:2||scanning transmission electron microscopy:2||QUANTUM OSCILLATIONS:2||TRANSPORTPROPERTIES:2||surface pair current:2||MAGNETORESISTANCE:2||NANORIBBONS:2||INSTABILITY:2||ANDREEV REFLECTION:2||microwave irradiation:2||vertical graphene josephson junction:2||BI2SE3:2||CONDUCTIVITY:2||highTc superconductors:2||DIMENSIONAL ELECTRONGAS:2||graphene:2||Topological insulators:2||Josephson coupling Fraunhofer interference pattern:2||FERROMAGNET:2||DEPENDENCE:2||DETECTOR:2||COHERENCE:2||INJECTION:2||GRAPHENE:1||JOSEPHSONJUNCTIONS:1||LAYERED SUPERCONDUCTOR:1||mode splitting:1||BEHAVIOR:1||spinpolarized transport:1||SUPERCONDUCTING TRANSITION:1||microwave response:1||PSEUDOGAP:1||phase coherence:1||TRANSITIONS:1||Long Josephson junction:1||Charge detection:1||collective resonance modes:1||plasma oscillation modes:1||Superconducting proximity effect:1||Iron pnictide superconductor:1||McMillanRowell oscillations:1||ferromagnetic microstructure:1||superradiant state:1||VOLTAGE:1||branch splitting:1||TENSOR:1||INTERCALATION:1||insitu fabrication:1||NDGAO3:1||DISORDERED METALS:1||GAUGE GLASS:1||LOWTEMPERATURE TRANSPORT:1||spontaneous spin polarization model:1||BIAS:1||emission of electromagnetic waves:1||YBA2CU3O7/PRBA2CU3O7 SUPERLATTICES:1||BOHM:1||SHAPIRO STEPS:1||superconductor/ferromagnet interface:1||OXIDE:1||ANDREEVREFLECTION:1||SinFeAsO single crystal:1||COLLECTIVE MOTION:1||ANGULARDEPENDENCE:1||SUPERCONDUCTIVITY:1||BILAYER GRAPHENE:1||PHOTOLUMINESCENT PROPERTIES:1||SUPERCONDUCTING WEAK LINKS:1||intrinsic Josephson junctions geometrical resonance:1||intrinsic Josephson junction:1||MESOSCOPIC SPINVALVE:1||Bi2212 single crystals:1||intrinsic junctions:1||ANDREEV REFLECTIONS:1||normalmetal/superconductor interface:1||IBI2SR2CACU2OY:1||THERMAL FLUCTUATIONS:1||MIXED STATE:1||BI2.15SR1.85CACU2O8+DELTA:1||intrinsic Josephson effects:1||CACUO:1||QUANTUM POINT CONTACTS:1||resonant tunneling state:1||coherence length:1||NANOWIRE:1||GATES:1||Phase line:1||Thermal activation:1||QUANTUMDOT:1||superconducting proximity effect:1||Andreev interferometer:1||WIRE:1||Josephsonvortexflow branches:1||Bi2212 cuprates:1||LATTICE:1||demannetization effect:1||SUPERCONDUCTING MIRRORS:1||GAS:1||VALLEY TRANSPORT:1||ELECTRODES:1||DEPENDENT TRANSPORT:1||BORNOPPENHEIMER APPROXIMATION:1||collective plasma oscillations:1||fluxon resonance steps:1||STACKS:1||COLLECTIVE DYNAMICS:1||PAIRING SYMMETRY:1||MUON SPIN ROTATION:1||DIMENSIONAL CROSSOVER:1||Bi2Sr2CaCu2Oy highTc superconductors:1||heterojunctions:1||nanostructures:1||surfaces and interfaces:1||QUANTUM TRANSPORT:1||MICROJUNCTIONS:1||RESONATORS:1||STATES:1||FIELD:1||FLUCTUATIONS:1||SCATTERING:1||mode splitting of Josephson vortexflow branches:1||2D superconductivity:1||TRANSISTOR:1||ENERGYGAP:1||SUPERLATTICES:1||IRONBASED SUPERCONDUCTORS:1||PHASEDEPENDENT RESISTANCE:1||QUANTUM PHASETRANSITIONS:1||ELECTRICFIELD:1||HIGH MAGNETICFIELDS:1||NANOWIRE HETEROSTRUCTURES:1||ZNO:1||pair breaking.:1||SUPERCONDUCTING PB:1||domain formation:1||FORCE MICROSCOPY:1||RELAXATION:1||PLASMA RESONANCE:1||coupled Josephson junctions:1||COPPEROXIDE SUPERCONDUCTORS:1||CROSSOVER:1||SIMULATIONS:1||LOWTEMPERATURE:1||CONDUCTORS:1||METALINSULATORTRANSITION:1||SEMICONDUCTOR:1||FIELDEFFECT TRANSISTORS:1||ZEROVOLTAGE STATE:1||constanttemperature interlayer tunneling spectroscopy:1||Josephson supercurrent:1||BIPOLAR SUPERCURRENT:1||Interaction between Josephson and pancake vortices:1||flux jump:1||coaxial heterojunction nanorod:1||Natural Josephson coupling:1||BI2SR2CACU2O8+DELTA:1||VORTEX FLOW:1||TC SUPERCONDUCTORS:1||charge imbalance:1||Andreev diffractometer:1||intercalation:1||surface junction:1||Bi2212:1||tunnelling:1||GRAPHITE:1||GROWTH:1||collective transverse plasma modes:1||GAN:1||Macroscopic quantum tunneling:1||Fluctuation conductivity:1||Abovegap conductance jump:1||Josephson vortex motion:1||Intrinsic Josephson junctions:1||LAYERED SUPERCONDUCTORS:1||BI2SR2CACU2O8+Y:1||INTERFACES:1||BREAKDOWN:1||SYSTEMS:1||Anisotropy ratio:1||Josephson vortex:1||spin relaxation in superconductors:1||bibased single crystals:1||MESOSCOPIC PROXIMITY SUPERCONDUCTOR:1||reentrance of conductance:1||interlayer pair tunneling:1||JOSEPHSON:1||DISORDERED 2DIMENSIONAL SUPERCONDUCTORS:1||INDIUM FILMS:1||excited state:1||REGIME:1||triplet superconductivity:1||FILM:1||SCHOTTKY DIODES:1||peakdiphump structure:1||Kondo effect:1||REENTRANCE:1||Graphene:1||CONTACT:1||BERRYS PHASE:1||2DIMENSIONAL SUPERCONDUCTORS:1||Coulomb diamond:1||magnetic domain:1||spin injection:1||RESONANCE:1||plasma excitation modes:1||FLOW:1||OVERDOPED BI2SR2CACU2O8+DELTA:1||hole doping:1||chemical synthesis:1||phase transitions:1||superconductors:1||VORTEXGLASS SUPERCONDUCTIVITY:1||Kondorelated model:1||RADIATION:1||DOT:1||NANOBELTS:1||Complementarity:1||Closedloop AharonovBohm interferometer:1||pair breaking:1||interlayer phase fluctuation:1||MgB2 thin film:1||CONFINEMENT:1||WALLED CARBON NANOTUBES:1||TRANSITION:9||VORTICES:8||STATE:7||intrinsic Josephson junctions:7||SINGLECRYSTALS:7||JUNCTIONS:5||MODES:5||SUPERCURRENT:5||SUPERCONDUCTOR:5||CONDUCTANCE:5||HIGHTEMPERATURE SUPERCONDUCTORS:5||TRANSPORT:5||PHASE:5||FILMS:4||LOCALIZATION:4||SINGLE DIRAC CONE:4||WIRES:4||MAGNETICFIELD:4||STEPS:3||ELECTRONS:3||proximity effect:3||MODEL:3||ARRAYS:3||INTERFERENCE:3||fluxon dynamics:3||HETEROSTRUCTURES:3||INSULATOR:3||Andreev reflection:3||electronic transport:3||FISKE:3||superconductor:2||ZnO:2||quantum point contact:2||METAL:2||DYNAMICS:2||interlayer Josephson coupling:2||SUPERCONDUCTORS:2||YBA2CU3O7DELTA:2||LAYER:2||DOTS:2||quantum dot:2||Article:2||TRANSISTORS:2||CARBON NANOTUBES:2||GAP:2||MECHANISM:2||LINE:2||GIANT SHAPIRO STEPS:2||LAYERS:2||electron energy loss spectroscopy:2||physical phenomena:2||scanning electron microscopy:2||HGTE QUANTUMWELLS:2||BI2TE3:2||SPECTROSCOPY:2||PNJUNCTIONS:2||spinpolarized tunneling:2||INTRINSIC JOSEPHSONJUNCTIONS:2||FIELDS:2||positive magnetoresistance:2||dilute magnetic semiconductor:2||magnetic field:2||scanning transmission electron microscopy:2||QUANTUM OSCILLATIONS:2||TRANSPORTPROPERTIES:2||surface pair current:2||MAGNETORESISTANCE:2||NANORIBBONS:2||INSTABILITY:2||ANDREEV REFLECTION:2||microwave irradiation:2||vertical graphene josephson junction:2||BI2SE3:2||CONDUCTIVITY:2||highTc superconductors:2||DIMENSIONAL ELECTRONGAS:2||graphene:2||Topological insulators:2||Josephson coupling Fraunhofer interference pattern:2||FERROMAGNET:2||DEPENDENCE:2||DETECTOR:2||COHERENCE:2||INJECTION:2||GRAPHENE:1||JOSEPHSONJUNCTIONS:1||LAYERED SUPERCONDUCTOR:1||mode splitting:1||BEHAVIOR:1||spinpolarized transport:1||SUPERCONDUCTING TRANSITION:1||microwave response:1||PSEUDOGAP:1||phase coherence:1||TRANSITIONS:1||Long Josephson junction:1||Charge detection:1||collective resonance modes:1||plasma oscillation modes:1||Superconducting proximity effect:1||Iron pnictide superconductor:1||McMillanRowell oscillations:1||ferromagnetic microstructure:1||superradiant state:1||VOLTAGE:1||branch splitting:1||TENSOR:1||INTERCALATION:1||insitu fabrication:1||NDGAO3:1||DISORDERED METALS:1||GAUGE GLASS:1||LOWTEMPERATURE TRANSPORT:1||spontaneous spin polarization model:1||BIAS:1||emission of electromagnetic waves:1||YBA2CU3O7/PRBA2CU3O7 SUPERLATTICES:1||BOHM:1||SHAPIRO STEPS:1||superconductor/ferromagnet interface:1||OXIDE:1||ANDREEVREFLECTION:1||SinFeAsO single crystal:1||COLLECTIVE MOTION:1||ANGULARDEPENDENCE:1||SUPERCONDUCTIVITY:1||BILAYER GRAPHENE:1||PHOTOLUMINESCENT PROPERTIES:1||SUPERCONDUCTING WEAK LINKS:1||intrinsic Josephson junctions geometrical resonance:1||intrinsic Josephson junction:1||MESOSCOPIC SPINVALVE:1||Bi2212 single crystals:1||intrinsic junctions:1||ANDREEV REFLECTIONS:1||normalmetal/superconductor interface:1||IBI2SR2CACU2OY:1||THERMAL FLUCTUATIONS:1||MIXED STATE:1||BI2.15SR1.85CACU2O8+DELTA:1||intrinsic Josephson effects:1||CACUO:1||QUANTUM POINT CONTACTS:1||resonant tunneling state:1||coherence length:1||NANOWIRE:1||GATES:1||Phase line:1||Thermal activation:1||QUANTUMDOT:1||superconducting proximity effect:1||Andreev interferometer:1||WIRE:1||Josephsonvortexflow branches:1||Bi2212 cuprates:1||LATTICE:1||demannetization effect:1||SUPERCONDUCTING MIRRORS:1||GAS:1||VALLEY TRANSPORT:1||ELECTRODES:1||DEPENDENT TRANSPORT:1||BORNOPPENHEIMER APPROXIMATION:1||collective plasma oscillations:1||fluxon resonance steps:1||STACKS:1||COLLECTIVE DYNAMICS:1||PAIRING SYMMETRY:1||MUON SPIN ROTATION:1||DIMENSIONAL CROSSOVER:1||Bi2Sr2CaCu2Oy highTc superconductors:1||heterojunctions:1||nanostructures:1||surfaces and interfaces:1||QUANTUM TRANSPORT:1||MICROJUNCTIONS:1||RESONATORS:1||STATES:1||FIELD:1||FLUCTUATIONS:1||SCATTERING:1||mode splitting of Josephson vortexflow branches:1||2D superconductivity:1||TRANSISTOR:1||ENERGYGAP:1||SUPERLATTICES:1||IRONBASED SUPERCONDUCTORS:1||PHASEDEPENDENT RESISTANCE:1||QUANTUM PHASETRANSITIONS:1||ELECTRICFIELD:1||HIGH MAGNETICFIELDS:1||NANOWIRE HETEROSTRUCTURES:1||ZNO:1||pair breaking.:1||SUPERCONDUCTING PB:1||domain formation:1||FORCE MICROSCOPY:1||RELAXATION:1||PLASMA RESONANCE:1||coupled Josephson junctions:1||COPPEROXIDE SUPERCONDUCTORS:1||CROSSOVER:1||SIMULATIONS:1||LOWTEMPERATURE:1||CONDUCTORS:1||METALINSULATORTRANSITION:1||SEMICONDUCTOR:1||FIELDEFFECT TRANSISTORS:1||ZEROVOLTAGE STATE:1||constanttemperature interlayer tunneling spectroscopy:1||Josephson supercurrent:1||BIPOLAR SUPERCURRENT:1||Interaction between Josephson and pancake vortices:1||flux jump:1||coaxial heterojunction nanorod:1||Natural Josephson coupling:1||BI2SR2CACU2O8+DELTA:1||VORTEX FLOW:1||TC SUPERCONDUCTORS:1||charge imbalance:1||Andreev diffractometer:1||intercalation:1||surface junction:1||Bi2212:1||tunnelling:1||GRAPHITE:1||GROWTH:1||collective transverse plasma modes:1||GAN:1||Macroscopic quantum tunneling:1||Fluctuation conductivity:1||Abovegap conductance jump:1||Josephson vortex motion:1||Intrinsic Josephson junctions:1||LAYERED SUPERCONDUCTORS:1||BI2SR2CACU2O8+Y:1||INTERFACES:1||BREAKDOWN:1||SYSTEMS:1||Anisotropy ratio:1||Josephson vortex:1||spin relaxation in superconductors:1||bibased single crystals:1||MESOSCOPIC PROXIMITY SUPERCONDUCTOR:1||reentrance of conductance:1||interlayer pair tunneling:1||JOSEPHSON:1||DISORDERED 2DIMENSIONAL SUPERCONDUCTORS:1||INDIUM FILMS:1||excited state:1||REGIME:1||triplet superconductivity:1||FILM:1||SCHOTTKY DIODES:1||peakdiphump structure:1||Kondo effect:1||REENTRANCE:1||Graphene:1||CONTACT:1||BERRYS PHASE:1||2DIMENSIONAL SUPERCONDUCTORS:1||Coulomb diamond:1||magnetic domain:1||spin injection:1||RESONANCE:1||plasma excitation modes:1||FLOW:1||OVERDOPED BI2SR2CACU2O8+DELTA:1||hole doping:1||chemical synthesis:1||phase transitions:1||superconductors:1||VORTEXGLASS SUPERCONDUCTIVITY:1||Kondorelated model:1||RADIATION:1||DOT:1||NANOBELTS:1||Complementarity:1||Closedloop AharonovBohm interferometer:1||pair breaking:1||interlayer phase fluctuation:1||MgB2 thin film:1||CONFINEMENT:1||WALLED CARBON NANOTUBES:1||TRANSITION:9||VORTICES:8||STATE:7||intrinsic Josephson junctions:7||SINGLECRYSTALS:7||JUNCTIONS:5||MODES:5||SUPERCURRENT:5||SUPERCONDUCTOR:5||CONDUCTANCE:5||HIGHTEMPERATURE SUPERCONDUCTORS:5||TRANSPORT:5||PHASE:5||FILMS:4||LOCALIZATION:4||SINGLE DIRAC CONE:4||WIRES:4||MAGNETICFIELD:4||STEPS:3||ELECTRONS:3||proximity effect:3||MODEL:3||ARRAYS:3||INTERFERENCE:3||fluxon dynamics:3||HETEROSTRUCTURES:3||INSULATOR:3||Andreev reflection:3||electronic transport:3||FISKE:3||superconductor:2||ZnO:2||quantum point contact:2||METAL:2||DYNAMICS:2||interlayer Josephson coupling:2||SUPERCONDUCTORS:2||YBA2CU3O7DELTA:2||LAYER:2||DOTS:2||quantum dot:2||Article:2||TRANSISTORS:2||CARBON NANOTUBES:2||GAP:2||MECHANISM:2||LINE:2||GIANT SHAPIRO STEPS:2||LAYERS:2||electron energy loss spectroscopy:2||physical phenomena:2||scanning electron microscopy:2||HGTE QUANTUMWELLS:2||BI2TE3:2||SPECTROSCOPY:2||PNJUNCTIONS:2||spinpolarized tunneling:2||INTRINSIC JOSEPHSONJUNCTIONS:2||FIELDS:2||positive magnetoresistance:2||dilute magnetic semiconductor:2||magnetic field:2||scanning transmission electron microscopy:2||QUANTUM OSCILLATIONS:2||TRANSPORTPROPERTIES:2||surface pair current:2||MAGNETORESISTANCE:2||NANORIBBONS:2||INSTABILITY:2||ANDREEV REFLECTION:2||microwave irradiation:2||vertical graphene josephson junction:2||BI2SE3:2||CONDUCTIVITY:2||highTc superconductors:2||DIMENSIONAL ELECTRONGAS:2||graphene:2||Topological insulators:2||Josephson coupling Fraunhofer interference pattern:2||FERROMAGNET:2||DEPENDENCE:2||DETECTOR:2||COHERENCE:2||INJECTION:2||GRAPHENE:1||JOSEPHSONJUNCTIONS:1||LAYERED SUPERCONDUCTOR:1||mode splitting:1||BEHAVIOR:1||spinpolarized transport:1||SUPERCONDUCTING TRANSITION:1||microwave response:1||PSEUDOGAP:1||phase coherence:1||TRANSITIONS:1||Long Josephson junction:1||Charge detection:1||collective resonance modes:1||plasma oscillation modes:1||Superconducting proximity effect:1||Iron pnictide superconductor:1||McMillanRowell oscillations:1||ferromagnetic microstructure:1||superradiant state:1||VOLTAGE:1||branch splitting:1||TENSOR:1||INTERCALATION:1||insitu fabrication:1||NDGAO3:1||DISORDERED METALS:1||GAUGE GLASS:1||LOWTEMPERATURE TRANSPORT:1||spontaneous spin polarization model:1||BIAS:1||emission of electromagnetic waves:1||YBA2CU3O7/PRBA2CU3O7 SUPERLATTICES:1||BOHM:1||SHAPIRO STEPS:1||superconductor/ferromagnet interface:1||OXIDE:1||ANDREEVREFLECTION:1||SinFeAsO single crystal:1||COLLECTIVE MOTION:1||ANGULARDEPENDENCE:1||SUPERCONDUCTIVITY:1||BILAYER GRAPHENE:1||PHOTOLUMINESCENT PROPERTIES:1||SUPERCONDUCTING WEAK LINKS:1||intrinsic Josephson junctions geometrical resonance:1||intrinsic Josephson junction:1||MESOSCOPIC SPINVALVE:1||Bi2212 single crystals:1||intrinsic junctions:1||ANDREEV REFLECTIONS:1||normalmetal/superconductor interface:1||IBI2SR2CACU2OY:1||THERMAL FLUCTUATIONS:1||MIXED STATE:1||BI2.15SR1.85CACU2O8+DELTA:1||intrinsic Josephson effects:1||CACUO:1||QUANTUM POINT CONTACTS:1||resonant tunneling state:1||coherence length:1||NANOWIRE:1||GATES:1||Phase line:1||Thermal activation:1||QUANTUMDOT:1||superconducting proximity effect:1||Andreev interferometer:1||WIRE:1||Josephsonvortexflow branches:1||Bi2212 cuprates:1||LATTICE:1||demannetization effect:1||SUPERCONDUCTING MIRRORS:1||GAS:1||VALLEY TRANSPORT:1||ELECTRODES:1||DEPENDENT TRANSPORT:1||BORNOPPENHEIMER APPROXIMATION:1||collective plasma oscillations:1||fluxon resonance steps:1||STACKS:1||COLLECTIVE DYNAMICS:1||PAIRING SYMMETRY:1||MUON SPIN ROTATION:1||DIMENSIONAL CROSSOVER:1||Bi2Sr2CaCu2Oy highTc superconductors:1||heterojunctions:1||nanostructures:1||surfaces and interfaces:1||QUANTUM TRANSPORT:1||MICROJUNCTIONS:1||RESONATORS:1||STATES:1||FIELD:1||FLUCTUATIONS:1||SCATTERING:1||mode splitting of Josephson vortexflow branches:1||2D superconductivity:1||TRANSISTOR:1||ENERGYGAP:1||SUPERLATTICES:1||IRONBASED SUPERCONDUCTORS:1||PHASEDEPENDENT RESISTANCE:1||QUANTUM PHASETRANSITIONS:1||ELECTRICFIELD:1||HIGH MAGNETICFIELDS:1||NANOWIRE HETEROSTRUCTURES:1||ZNO:1||pair breaking.:1||SUPERCONDUCTING PB:1||domain formation:1||FORCE MICROSCOPY:1||RELAXATION:1||PLASMA RESONANCE:1||coupled Josephson junctions:1||COPPEROXIDE SUPERCONDUCTORS:1||CROSSOVER:1||SIMULATIONS:1||LOWTEMPERATURE:1||CONDUCTORS:1||METALINSULATORTRANSITION:1||SEMICONDUCTOR:1||FIELDEFFECT TRANSISTORS:1||ZEROVOLTAGE STATE:1||constanttemperature interlayer tunneling spectroscopy:1||Josephson supercurrent:1||BIPOLAR SUPERCURRENT:1||Interaction between Josephson and pancake vortices:1||flux jump:1||coaxial heterojunction nanorod:1||Natural Josephson coupling:1||BI2SR2CACU2O8+DELTA:1||VORTEX FLOW:1||TC SUPERCONDUCTORS:1||charge imbalance:1||Andreev diffractometer:1||intercalation:1||surface junction:1||Bi2212:1||tunnelling:1||GRAPHITE:1||GROWTH:1||collective transverse plasma modes:1||GAN:1||Macroscopic quantum tunneling:1||Fluctuation conductivity:1||Abovegap conductance jump:1||Josephson vortex motion:1||Intrinsic Josephson junctions:1||LAYERED SUPERCONDUCTORS:1||BI2SR2CACU2O8+Y:1||INTERFACES:1||BREAKDOWN:1||SYSTEMS:1||Anisotropy ratio:1||Josephson vortex:1||spin relaxation in superconductors:1||bibased single crystals:1||MESOSCOPIC PROXIMITY SUPERCONDUCTOR:1||reentrance of conductance:1||interlayer pair tunneling:1||JOSEPHSON:1||DISORDERED 2DIMENSIONAL SUPERCONDUCTORS:1||INDIUM FILMS:1||excited state:1||REGIME:1||triplet superconductivity:1||FILM:1||SCHOTTKY DIODES:1||peakdiphump structure:1||Kondo effect:1||REENTRANCE:1||Graphene:1||CONTACT:1||BERRYS PHASE:1||2DIMENSIONAL SUPERCONDUCTORS:1||Coulomb diamond:1||magnetic domain:1||spin injection:1||RESONANCE:1||plasma excitation modes:1||FLOW:1||OVERDOPED BI2SR2CACU2O8+DELTA:1||hole doping:1||chemical synthesis:1||phase transitions:1||superconductors:1||VORTEXGLASS SUPERCONDUCTIVITY:1||Kondorelated model:1||RADIATION:1||DOT:1||NANOBELTS:1||Complementarity:1||Closedloop AharonovBohm interferometer:1||pair breaking:1||interlayer phase fluctuation:1||MgB2 thin film:1||CONFINEMENT:1||WALLED CARBON NANOTUBES:1||TRANSITION:9||VORTICES:8||STATE:7||intrinsic Josephson junctions:7||SINGLECRYSTALS:7||JUNCTIONS:5||MODES:5||SUPERCURRENT:5||SUPERCONDUCTOR:5||CONDUCTANCE:5||HIGHTEMPERATURE SUPERCONDUCTORS:5||TRANSPORT:5||PHASE:5||FILMS:4||LOCALIZATION:4||SINGLE DIRAC CONE:4||WIRES:4||MAGNETICFIELD:4||STEPS:3||ELECTRONS:3||proximity effect:3||MODEL:3||ARRAYS:3||INTERFERENCE:3||fluxon dynamics:3||HETEROSTRUCTURES:3||INSULATOR:3||Andreev reflection:3||electronic transport:3||FISKE:3||superconductor:2||ZnO:2||quantum point contact:2||METAL:2||DYNAMICS:2||interlayer Josephson coupling:2||SUPERCONDUCTORS:2||YBA2CU3O7DELTA:2||LAYER:2||DOTS:2||quantum dot:2||Article:2||TRANSISTORS:2||CARBON NANOTUBES:2||GAP:2||MECHANISM:2||LINE:2||GIANT SHAPIRO STEPS:2||LAYERS:2||electron energy loss spectroscopy:2||physical phenomena:2||scanning electron microscopy:2||HGTE QUANTUMWELLS:2||BI2TE3:2||SPECTROSCOPY:2||PNJUNCTIONS:2||spinpolarized tunneling:2||INTRINSIC JOSEPHSONJUNCTIONS:2||FIELDS:2||positive magnetoresistance:2||dilute magnetic semiconductor:2||magnetic field:2||scanning transmission electron microscopy:2||QUANTUM OSCILLATIONS:2||TRANSPORTPROPERTIES:2||surface pair current:2||MAGNETORESISTANCE:2||NANORIBBONS:2||INSTABILITY:2||ANDREEV REFLECTION:2||microwave irradiation:2||vertical graphene josephson junction:2||BI2SE3:2||CONDUCTIVITY:2||highTc superconductors:2||DIMENSIONAL ELECTRONGAS:2||graphene:2||Topological insulators:2||Josephson coupling Fraunhofer interference pattern:2||FERROMAGNET:2||DEPENDENCE:2||DETECTOR:2||COHERENCE:2||INJECTION:2||GRAPHENE:1||JOSEPHSONJUNCTIONS:1||LAYERED SUPERCONDUCTOR:1||mode splitting:1||BEHAVIOR:1||spinpolarized transport:1||SUPERCONDUCTING TRANSITION:1||microwave response:1||PSEUDOGAP:1||phase coherence:1||TRANSITIONS:1||Long Josephson junction:1||Charge detection:1||collective resonance modes:1||plasma oscillation modes:1||Superconducting proximity effect:1||Iron pnictide superconductor:1||McMillanRowell oscillations:1||ferromagnetic microstructure:1||superradiant state:1||VOLTAGE:1||branch splitting:1||TENSOR:1||INTERCALATION:1||insitu fabrication:1||NDGAO3:1||DISORDERED METALS:1||GAUGE GLASS:1||LOWTEMPERATURE TRANSPORT:1||spontaneous spin polarization model:1||BIAS:1||emission of electromagnetic waves:1||YBA2CU3O7/PRBA2CU3O7 SUPERLATTICES:1||BOHM:1||SHAPIRO STEPS:1||superconductor/ferromagnet interface:1||OXIDE:1||ANDREEVREFLECTION:1||SinFeAsO single crystal:1||COLLECTIVE MOTION:1||ANGULARDEPENDENCE:1||SUPERCONDUCTIVITY:1||BILAYER GRAPHENE:1||PHOTOLUMINESCENT PROPERTIES:1||SUPERCONDUCTING WEAK LINKS:1||intrinsic Josephson junctions geometrical resonance:1||intrinsic Josephson junction:1||MESOSCOPIC SPINVALVE:1||Bi2212 single crystals:1||intrinsic junctions:1||ANDREEV REFLECTIONS:1||normalmetal/superconductor interface:1||IBI2SR2CACU2OY:1||THERMAL FLUCTUATIONS:1||MIXED STATE:1||BI2.15SR1.85CACU2O8+DELTA:1||intrinsic Josephson effects:1||CACUO:1||QUANTUM POINT CONTACTS:1||resonant tunneling state:1||coherence length:1||NANOWIRE:1||GATES:1||Phase line:1||Thermal activation:1||QUANTUMDOT:1||superconducting proximity effect:1||Andreev interferometer:1||WIRE:1||Josephsonvortexflow branches:1||Bi2212 cuprates:1||LATTICE:1||demannetization effect:1||SUPERCONDUCTING MIRRORS:1||GAS:1||VALLEY TRANSPORT:1||ELECTRODES:1||DEPENDENT TRANSPORT:1||BORNOPPENHEIMER APPROXIMATION:1||collective plasma oscillations:1||fluxon resonance steps:1||STACKS:1||COLLECTIVE DYNAMICS:1||PAIRING SYMMETRY:1||MUON SPIN ROTATION:1||DIMENSIONAL CROSSOVER:1||Bi2Sr2CaCu2Oy highTc superconductors:1||heterojunctions:1||nanostructures:1||surfaces and interfaces:1||QUANTUM TRANSPORT:1||MICROJUNCTIONS:1||RESONATORS:1||STATES:1||FIELD:1||FLUCTUATIONS:1||SCATTERING:1||mode splitting of Josephson vortexflow branches:1||2D superconductivity:1||TRANSISTOR:1||ENERGYGAP:1||SUPERLATTICES:1||IRONBASED SUPERCONDUCTORS:1||PHASEDEPENDENT RESISTANCE:1||QUANTUM PHASETRANSITIONS:1||ELECTRICFIELD:1||HIGH MAGNETICFIELDS:1||NANOWIRE HETEROSTRUCTURES:1||ZNO:1||pair breaking.:1||SUPERCONDUCTING PB:1||domain formation:1||FORCE MICROSCOPY:1||RELAXATION:1||PLASMA RESONANCE:1||coupled Josephson junctions:1||COPPEROXIDE SUPERCONDUCTORS:1||CROSSOVER:1||SIMULATIONS:1||LOWTEMPERATURE:1||CONDUCTORS:1||METALINSULATORTRANSITION:1||SEMICONDUCTOR:1||FIELDEFFECT TRANSISTORS:1||ZEROVOLTAGE STATE:1||constanttemperature interlayer tunneling spectroscopy:1||Josephson supercurrent:1||BIPOLAR SUPERCURRENT:1||Interaction between Josephson and pancake vortices:1||flux jump:1||coaxial heterojunction nanorod:1||Natural Josephson coupling:1||BI2SR2CACU2O8+DELTA:1||VORTEX FLOW:1||TC SUPERCONDUCTORS:1||charge imbalance:1||Andreev diffractometer:1||intercalation:1||surface junction:1||Bi2212:1||tunnelling:1||GRAPHITE:1||GROWTH:1||collective transverse plasma modes:1||GAN:1||Macroscopic quantum tunneling:1||Fluctuation conductivity:1||Abovegap conductance jump:1||Josephson vortex motion:1||Intrinsic Josephson junctions:1||LAYERED SUPERCONDUCTORS:1||BI2SR2CACU2O8+Y:1||INTERFACES:1||BREAKDOWN:1||SYSTEMS:1||Anisotropy ratio:1||Josephson vortex:1||spin relaxation in superconductors:1||bibased single crystals:1||MESOSCOPIC PROXIMITY SUPERCONDUCTOR:1||reentrance of conductance:1||interlayer pair tunneling:1||JOSEPHSON:1||DISORDERED 2DIMENSIONAL SUPERCONDUCTORS:1||INDIUM FILMS:1||excited state:1||REGIME:1||triplet superconductivity:1||FILM:1||SCHOTTKY DIODES:1||peakdiphump structure:1||Kondo effect:1||REENTRANCE:1||Graphene:1||CONTACT:1||BERRYS PHASE:1||2DIMENSIONAL SUPERCONDUCTORS:1||Coulomb diamond:1||magnetic domain:1||spin injection:1||RESONANCE:1||plasma excitation modes:1||FLOW:1||OVERDOPED BI2SR2CACU2O8+DELTA:1||hole doping:1||chemical synthesis:1||phase transitions:1||superconductors:1||VORTEXGLASS SUPERCONDUCTIVITY:1||Kondorelated model:1||RADIATION:1||DOT:1||NANOBELTS:1||Complementarity:1||Closedloop AharonovBohm interferometer:1||pair breaking:1||interlayer phase fluctuation:1||MgB2 thin film:1||CONFINEMENT:1||WALLED CARBON NANOTUBES:1||TRANSITION:9||VORTICES:8||STATE:7||intrinsic Josephson junctions:7||SINGLECRYSTALS:7||JUNCTIONS:5||MODES:5||SUPERCURRENT:5||SUPERCONDUCTOR:5||CONDUCTANCE:5||HIGHTEMPERATURE SUPERCONDUCTORS:5||TRANSPORT:5||PHASE:5||FILMS:4||LOCALIZATION:4||SINGLE DIRAC CONE:4||WIRES:4||MAGNETICFIELD:4||STEPS:3||ELECTRONS:3||proximity effect:3||MODEL:3||ARRAYS:3||INTERFERENCE:3||fluxon dynamics:3||HETEROSTRUCTURES:3||INSULATOR:3||Andreev reflection:3||electronic transport:3||FISKE:3||superconductor:2||ZnO:2||quantum point contact:2||METAL:2||DYNAMICS:2||interlayer Josephson coupling:2||SUPERCONDUCTORS:2||YBA2CU3O7DELTA:2||LAYER:2||DOTS:2||quantum dot:2||Article:2||TRANSISTORS:2||CARBON NANOTUBES:2||GAP:2||MECHANISM:2||LINE:2||GIANT SHAPIRO STEPS:2||LAYERS:2||electron energy loss spectroscopy:2||physical phenomena:2||scanning electron microscopy:2||HGTE QUANTUMWELLS:2||BI2TE3:2||SPECTROSCOPY:2||PNJUNCTIONS:2||spinpolarized tunneling:2||INTRINSIC JOSEPHSONJUNCTIONS:2||FIELDS:2||positive magnetoresistance:2||dilute magnetic semiconductor:2||magnetic field:2||scanning transmission electron microscopy:2||QUANTUM OSCILLATIONS:2||TRANSPORTPROPERTIES:2||surface pair current:2||MAGNETORESISTANCE:2||NANORIBBONS:2||INSTABILITY:2||ANDREEV REFLECTION:2||microwave irradiation:2||vertical graphene josephson junction:2||BI2SE3:2||CONDUCTIVITY:2||highTc superconductors:2||DIMENSIONAL ELECTRONGAS:2||graphene:2||Topological insulators:2||Josephson coupling Fraunhofer interference pattern:2||FERROMAGNET:2||DEPENDENCE:2||DETECTOR:2||COHERENCE:2||INJECTION:2||GRAPHENE:1||JOSEPHSONJUNCTIONS:1||LAYERED SUPERCONDUCTOR:1||mode splitting:1||BEHAVIOR:1||spinpolarized transport:1||SUPERCONDUCTING TRANSITION:1||microwave response:1||PSEUDOGAP:1||phase coherence:1||TRANSITIONS:1||Long Josephson junction:1||Charge detection:1||collective resonance modes:1||plasma oscillation modes:1||Superconducting proximity effect:1||Iron pnictide superconductor:1||McMillanRowell oscillations:1||ferromagnetic microstructure:1||superradiant state:1||VOLTAGE:1||branch splitting:1||TENSOR:1||INTERCALATION:1||insitu fabrication:1||NDGAO3:1||DISORDERED METALS:1||GAUGE GLASS:1||LOWTEMPERATURE TRANSPORT:1||spontaneous spin polarization model:1||BIAS:1||emission of electromagnetic waves:1||YBA2CU3O7/PRBA2CU3O7 SUPERLATTICES:1||BOHM:1||SHAPIRO STEPS:1||superconductor/ferromagnet interface:1||OXIDE:1||ANDREEVREFLECTION:1||SinFeAsO single crystal:1||COLLECTIVE MOTION:1||ANGULARDEPENDENCE:1||SUPERCONDUCTIVITY:1||BILAYER GRAPHENE:1||PHOTOLUMINESCENT PROPERTIES:1||SUPERCONDUCTING WEAK LINKS:1||intrinsic Josephson junctions geometrical resonance:1||intrinsic Josephson junction:1||MESOSCOPIC SPINVALVE:1||Bi2212 single crystals:1||intrinsic junctions:1||ANDREEV REFLECTIONS:1||normalmetal/superconductor interface:1||IBI2SR2CACU2OY:1||THERMAL FLUCTUATIONS:1||MIXED STATE:1||BI2.15SR1.85CACU2O8+DELTA:1||intrinsic Josephson effects:1||CACUO:1||QUANTUM POINT CONTACTS:1||resonant tunneling state:1||coherence length:1||NANOWIRE:1||GATES:1||Phase line:1||Thermal activation:1||QUANTUMDOT:1||superconducting proximity effect:1||Andreev interferometer:1||WIRE:1||Josephsonvortexflow branches:1||Bi2212 cuprates:1||LATTICE:1||demannetization effect:1||SUPERCONDUCTING MIRRORS:1||GAS:1||VALLEY TRANSPORT:1||ELECTRODES:1||DEPENDENT TRANSPORT:1||BORNOPPENHEIMER APPROXIMATION:1||collective plasma oscillations:1||fluxon resonance steps:1||STACKS:1||COLLECTIVE DYNAMICS:1||PAIRING SYMMETRY:1||MUON SPIN ROTATION:1||DIMENSIONAL CROSSOVER:1||Bi2Sr2CaCu2Oy highTc superconductors:1||heterojunctions:1||nanostructures:1||surfaces and interfaces:1||QUANTUM TRANSPORT:1||MICROJUNCTIONS:1||RESONATORS:1||STATES:1||FIELD:1||FLUCTUATIONS:1||SCATTERING:1||mode splitting of Josephson vortexflow branches:1||2D superconductivity:1||TRANSISTOR:1||ENERGYGAP:1||SUPERLATTICES:1||IRONBASED SUPERCONDUCTORS:1||PHASEDEPENDENT RESISTANCE:1||QUANTUM PHASETRANSITIONS:1||ELECTRICFIELD:1||HIGH MAGNETICFIELDS:1||NANOWIRE HETEROSTRUCTURES:1||ZNO:1||pair breaking.:1||SUPERCONDUCTING PB:1||domain formation:1||FORCE MICROSCOPY:1||RELAXATION:1||PLASMA RESONANCE:1||coupled Josephson junctions:1||COPPEROXIDE SUPERCONDUCTORS:1||CROSSOVER:1||SIMULATIONS:1||LOWTEMPERATURE:1||CONDUCTORS:1||METALINSULATORTRANSITION:1||SEMICONDUCTOR:1||FIELDEFFECT TRANSISTORS:1||ZEROVOLTAGE STATE:1||constanttemperature interlayer tunneling spectroscopy:1||Josephson supercurrent:1||BIPOLAR SUPERCURRENT:1||Interaction between Josephson and pancake vortices:1||flux jump:1||coaxial heterojunction nanorod:1||Natural Josephson coupling:1||BI2SR2CACU2O8+DELTA:1||VORTEX FLOW:1||TC SUPERCONDUCTORS:1||charge imbalance:1||Andreev diffractometer:1||intercalation:1||surface junction:1||Bi2212:1||tunnelling:1||GRAPHITE:1||GROWTH:1||collective transverse plasma modes:1||GAN:1||Macroscopic quantum tunneling:1||Fluctuation conductivity:1||Abovegap conductance jump:1||Josephson vortex motion:1||Intrinsic Josephson junctions:1||LAYERED SUPERCONDUCTORS:1||BI2SR2CACU2O8+Y:1||INTERFACES:1||BREAKDOWN:1||SYSTEMS:1||Anisotropy ratio:1||Josephson vortex:1||spin relaxation in superconductors:1||bibased single crystals:1||MESOSCOPIC PROXIMITY SUPERCONDUCTOR:1||reentrance of conductance:1||interlayer pair tunneling:1||JOSEPHSON:1||DISORDERED 2DIMENSIONAL SUPERCONDUCTORS:1||INDIUM FILMS:1||excited state:1||REGIME:1||triplet superconductivity:1||FILM:1||SCHOTTKY DIODES:1||peakdiphump structure:1||Kondo effect:1||REENTRANCE:1||Graphene:1||CONTACT:1||BERRYS PHASE:1||2DIMENSIONAL SUPERCONDUCTORS:1||Coulomb diamond:1||magnetic domain:1||spin injection:1||RESONANCE:1||plasma excitation modes:1||FLOW:1||OVERDOPED BI2SR2CACU2O8+DELTA:1||hole doping:1||chemical synthesis:1||phase transitions:1||superconductors:1||VORTEXGLASS SUPERCONDUCTIVITY:1||Kondorelated model:1||RADIATION:1||DOT:1||NANOBELTS:1||Complementarity:1||Closedloop AharonovBohm interferometer:1||pair breaking:1||interlayer phase fluctuation:1||MgB2 thin film:1||CONFINEMENT:1||WALLED CARBON NANOTUBES:1||TRANSITION:9||VORTICES:8||STATE:7||intrinsic Josephson junctions:7||SINGLECRYSTALS:7||JUNCTIONS:5||MODES:5||SUPERCURRENT:5||SUPERCONDUCTOR:5||CONDUCTANCE:5||HIGHTEMPERATURE SUPERCONDUCTORS:5||TRANSPORT:5||PHASE:5||FILMS:4||LOCALIZATION:4||SINGLE DIRAC CONE:4||WIRES:4||MAGNETICFIELD:4||STEPS:3||ELECTRONS:3||proximity effect:3||MODEL:3||ARRAYS:3||INTERFERENCE:3||fluxon dynamics:3||HETEROSTRUCTURES:3||INSULATOR:3||Andreev reflection:3||electronic transport:3||FISKE:3||superconductor:2||ZnO:2||quantum point contact:2||METAL:2||DYNAMICS:2||interlayer Josephson coupling:2||SUPERCONDUCTORS:2||YBA2CU3O7DELTA:2||LAYER:2||DOTS:2||quantum dot:2||Article:2||TRANSISTORS:2||CARBON NANOTUBES:2||GAP:2||MECHANISM:2||LINE:2||GIANT SHAPIRO STEPS:2||LAYERS:2||electron energy loss spectroscopy:2||physical phenomena:2||scanning electron microscopy:2||HGTE QUANTUMWELLS:2||BI2TE3:2||SPECTROSCOPY:2||PNJUNCTIONS:2||spinpolarized tunneling:2||INTRINSIC JOSEPHSONJUNCTIONS:2||FIELDS:2||positive magnetoresistance:2||dilute magnetic semiconductor:2||magnetic field:2||scanning transmission electron microscopy:2||QUANTUM OSCILLATIONS:2||TRANSPORTPROPERTIES:2||surface pair current:2||MAGNETORESISTANCE:2||NANORIBBONS:2||INSTABILITY:2||ANDREEV REFLECTION:2||microwave irradiation:2||vertical graphene josephson junction:2||BI2SE3:2||CONDUCTIVITY:2||highTc superconductors:2||DIMENSIONAL ELECTRONGAS:2||graphene:2||Topological insulators:2||Josephson coupling Fraunhofer interference pattern:2||FERROMAGNET:2||DEPENDENCE:2||DETECTOR:2||COHERENCE:2||INJECTION:2||GRAPHENE:1||JOSEPHSONJUNCTIONS:1||LAYERED SUPERCONDUCTOR:1||mode splitting:1||BEHAVIOR:1||spinpolarized transport:1||SUPERCONDUCTING TRANSITION:1||microwave response:1||PSEUDOGAP:1||phase coherence:1||TRANSITIONS:1||Long Josephson junction:1||Charge detection:1||collective resonance modes:1||plasma oscillation modes:1||Superconducting proximity effect:1||Iron pnictide superconductor:1||McMillanRowell oscillations:1||ferromagnetic microstructure:1||superradiant state:1||VOLTAGE:1||branch splitting:1||TENSOR:1||INTERCALATION:1||insitu fabrication:1||NDGAO3:1||DISORDERED METALS:1||GAUGE GLASS:1||LOWTEMPERATURE TRANSPORT:1||spontaneous spin polarization model:1||BIAS:1||emission of electromagnetic waves:1||YBA2CU3O7/PRBA2CU3O7 SUPERLATTICES:1||BOHM:1||SHAPIRO STEPS:1||superconductor/ferromagnet interface:1||OXIDE:1||ANDREEVREFLECTION:1||SinFeAsO single crystal:1||COLLECTIVE MOTION:1||ANGULARDEPENDENCE:1||SUPERCONDUCTIVITY:1||BILAYER GRAPHENE:1||PHOTOLUMINESCENT PROPERTIES:1||SUPERCONDUCTING WEAK LINKS:1||intrinsic Josephson junctions geometrical resonance:1||intrinsic Josephson junction:1||MESOSCOPIC SPINVALVE:1||Bi2212 single crystals:1||intrinsic junctions:1||ANDREEV REFLECTIONS:1||normalmetal/superconductor interface:1||IBI2SR2CACU2OY:1||THERMAL FLUCTUATIONS:1||MIXED STATE:1||BI2.15SR1.85CACU2O8+DELTA:1||intrinsic Josephson effects:1||CACUO:1||QUANTUM POINT CONTACTS:1||resonant tunneling state:1||coherence length:1||NANOWIRE:1||GATES:1||Phase line:1||Thermal activation:1||QUANTUMDOT:1||superconducting proximity effect:1||Andreev interferometer:1||WIRE:1||Josephsonvortexflow branches:1||Bi2212 cuprates:1||LATTICE:1||demannetization effect:1||SUPERCONDUCTING MIRRORS:1||GAS:1||VALLEY TRANSPORT:1||ELECTRODES:1||DEPENDENT TRANSPORT:1||BORNOPPENHEIMER APPROXIMATION:1||collective plasma oscillations:1||fluxon resonance steps:1||STACKS:1||COLLECTIVE DYNAMICS:1||PAIRING SYMMETRY:1||MUON SPIN ROTATION:1||DIMENSIONAL CROSSOVER:1||Bi2Sr2CaCu2Oy highTc superconductors:1||heterojunctions:1||nanostructures:1||surfaces and interfaces:1||QUANTUM TRANSPORT:1||MICROJUNCTIONS:1||RESONATORS:1||STATES:1||FIELD:1||FLUCTUATIONS:1||SCATTERING:1||mode splitting of Josephson vortexflow branches:1||2D superconductivity:1||TRANSISTOR:1||ENERGYGAP:1||SUPERLATTICES:1||IRONBASED SUPERCONDUCTORS:1||PHASEDEPENDENT RESISTANCE:1||QUANTUM PHASETRANSITIONS:1||ELECTRICFIELD:1||HIGH MAGNETICFIELDS:1||NANOWIRE HETEROSTRUCTURES:1||ZNO:1||pair breaking.:1||SUPERCONDUCTING PB:1||domain formation:1||FORCE MICROSCOPY:1||RELAXATION:1||PLASMA RESONANCE:1||coupled Josephson junctions:1||COPPEROXIDE SUPERCONDUCTORS:1||CROSSOVER:1||SIMULATIONS:1||LOWTEMPERATURE:1||CONDUCTORS:1||METALINSULATORTRANSITION:1||SEMICONDUCTOR:1||FIELDEFFECT TRANSISTORS:1||ZEROVOLTAGE STATE:1||constanttemperature interlayer tunneling spectroscopy:1||Josephson supercurrent:1||BIPOLAR SUPERCURRENT:1||Interaction between Josephson and pancake vortices:1||flux jump:1||coaxial heterojunction nanorod:1||Natural Josephson coupling:1||BI2SR2CACU2O8+DELTA:1||VORTEX FLOW:1||TC SUPERCONDUCTORS:1||charge imbalance:1||Andreev diffractometer:1||intercalation:1||surface junction:1||Bi2212:1||tunnelling:1||GRAPHITE:1||GROWTH:1||collective transverse plasma modes:1||GAN:1||Macroscopic quantum tunneling:1||Fluctuation conductivity:1||Abovegap conductance jump:1||Josephson vortex motion:1||Intrinsic Josephson junctions:1||LAYERED SUPERCONDUCTORS:1||BI2SR2CACU2O8+Y:1||INTERFACES:1||BREAKDOWN:1||SYSTEMS:1||Anisotropy ratio:1||Josephson vortex:1||spin relaxation in superconductors:1||bibased single crystals:1||MESOSCOPIC PROXIMITY SUPERCONDUCTOR:1||reentrance of conductance:1||interlayer pair tunneling:1||JOSEPHSON:1||DISORDERED 2DIMENSIONAL SUPERCONDUCTORS:1||INDIUM FILMS:1||excited state:1||REGIME:1||triplet superconductivity:1||FILM:1||SCHOTTKY DIODES:1||peakdiphump structure:1||Kondo effect:1||REENTRANCE:1||Graphene:1||CONTACT:1||BERRYS PHASE:1||2DIMENSIONAL SUPERCONDUCTORS:1||Coulomb diamond:1||magnetic domain:1||spin injection:1||RESONANCE:1||plasma excitation modes:1||FLOW:1||OVERDOPED BI2SR2CACU2O8+DELTA:1||hole doping:1||chemical synthesis:1||phase transitions:1||superconductors:1||VORTEXGLASS SUPERCONDUCTIVITY:1||Kondorelated model:1||RADIATION:1||DOT:1||NANOBELTS:1||Complementarity:1||Closedloop AharonovBohm interferometer:1||pair breaking:1||interlayer phase fluctuation:1||MgB2 thin film:1||CONFINEMENT:1||WALLED CARBON NANOTUBES:1||TRANSITION:9||VORTICES:8||STATE:7||intrinsic Josephson junctions:7||SINGLECRYSTALS:7||JUNCTIONS:5||MODES:5||SUPERCURRENT:5||SUPERCONDUCTOR:5||CONDUCTANCE:5||HIGHTEMPERATURE SUPERCONDUCTORS:5||TRANSPORT:5||PHASE:5||FILMS:4||LOCALIZATION:4||SINGLE DIRAC CONE:4||WIRES:4||MAGNETICFIELD:4||STEPS:3||ELECTRONS:3||proximity effect:3||MODEL:3||ARRAYS:3||INTERFERENCE:3||fluxon dynamics:3||HETEROSTRUCTURES:3||INSULATOR:3||Andreev reflection:3||electronic transport:3||FISKE:3||superconductor:2||ZnO:2||quantum point contact:2||METAL:2||DYNAMICS:2||interlayer Josephson coupling:2||SUPERCONDUCTORS:2||YBA2CU3O7DELTA:2||LAYER:2||DOTS:2||quantum dot:2||Article:2||TRANSISTORS:2||CARBON NANOTUBES:2||GAP:2||MECHANISM:2||LINE:2||GIANT SHAPIRO STEPS:2||LAYERS:2||electron energy loss spectroscopy:2||physical phenomena:2||scanning electron microscopy:2||HGTE QUANTUMWELLS:2||BI2TE3:2||SPECTROSCOPY:2||PNJUNCTIONS:2||spinpolarized tunneling:2||INTRINSIC JOSEPHSONJUNCTIONS:2||FIELDS:2||positive magnetoresistance:2||dilute magnetic semiconductor:2||magnetic field:2||scanning transmission electron microscopy:2||QUANTUM OSCILLATIONS:2||TRANSPORTPROPERTIES:2||surface pair current:2||MAGNETORESISTANCE:2||NANORIBBONS:2||INSTABILITY:2||ANDREEV REFLECTION:2||microwave irradiation:2||vertical graphene josephson junction:2||BI2SE3:2||CONDUCTIVITY:2||highTc superconductors:2||DIMENSIONAL ELECTRONGAS:2||graphene:2||Topological insulators:2||Josephson coupling Fraunhofer interference pattern:2||FERROMAGNET:2||DEPENDENCE:2||DETECTOR:2||COHERENCE:2||INJECTION:2||GRAPHENE:1||JOSEPHSONJUNCTIONS:1||LAYERED SUPERCONDUCTOR:1||mode splitting:1||BEHAVIOR:1||spinpolarized transport:1||SUPERCONDUCTING TRANSITION:1||microwave response:1||PSEUDOGAP:1||phase coherence:1||TRANSITIONS:1||Long Josephson junction:1||Charge detection:1||collective resonance modes:1||plasma oscillation modes:1||Superconducting proximity effect:1||Iron pnictide superconductor:1||McMillanRowell oscillations:1||ferromagnetic microstructure:1||superradiant state:1||VOLTAGE:1||branch splitting:1||TENSOR:1||INTERCALATION:1||insitu fabrication:1||NDGAO3:1||DISORDERED METALS:1||GAUGE GLASS:1||LOWTEMPERATURE TRANSPORT:1||spontaneous spin polarization model:1||BIAS:1||emission of electromagnetic waves:1||YBA2CU3O7/PRBA2CU3O7 SUPERLATTICES:1||BOHM:1||SHAPIRO STEPS:1||superconductor/ferromagnet interface:1||OXIDE:1||ANDREEVREFLECTION:1||SinFeAsO single crystal:1||COLLECTIVE MOTION:1||ANGULARDEPENDENCE:1||SUPERCONDUCTIVITY:1||BILAYER GRAPHENE:1||PHOTOLUMINESCENT PROPERTIES:1||SUPERCONDUCTING WEAK LINKS:1||intrinsic Josephson junctions geometrical resonance:1||intrinsic Josephson junction:1||MESOSCOPIC SPINVALVE:1||Bi2212 single crystals:1||intrinsic junctions:1||ANDREEV REFLECTIONS:1||normalmetal/superconductor interface:1||IBI2SR2CACU2OY:1||THERMAL FLUCTUATIONS:1||MIXED STATE:1||BI2.15SR1.85CACU2O8+DELTA:1||intrinsic Josephson effects:1||CACUO:1||QUANTUM POINT CONTACTS:1||resonant tunneling state:1||coherence length:1||NANOWIRE:1||GATES:1||Phase line:1||Thermal activation:1||QUANTUMDOT:1||superconducting proximity effect:1||Andreev interferometer:1||WIRE:1||Josephsonvortexflow branches:1||Bi2212 cuprates:1||LATTICE:1||demannetization effect:1||SUPERCONDUCTING MIRRORS:1||GAS:1||VALLEY TRANSPORT:1||ELECTRODES:1||DEPENDENT TRANSPORT:1||BORNOPPENHEIMER APPROXIMATION:1||collective plasma oscillations:1||fluxon resonance steps:1||STACKS:1||COLLECTIVE DYNAMICS:1||PAIRING SYMMETRY:1||MUON SPIN ROTATION:1||DIMENSIONAL CROSSOVER:1||Bi2Sr2CaCu2Oy highTc superconductors:1||heterojunctions:1||nanostructures:1||surfaces and interfaces:1||QUANTUM TRANSPORT:1||MICROJUNCTIONS:1||RESONATORS:1||STATES:1||FIELD:1||FLUCTUATIONS:1||SCATTERING:1||mode splitting of Josephson vortexflow branches:1||2D superconductivity:1||TRANSISTOR:1||ENERGYGAP:1||SUPERLATTICES:1||IRONBASED SUPERCONDUCTORS:1||PHASEDEPENDENT RESISTANCE:1||QUANTUM PHASETRANSITIONS:1||ELECTRICFIELD:1||HIGH MAGNETICFIELDS:1||NANOWIRE HETEROSTRUCTURES:1||ZNO:1||pair breaking.:1||SUPERCONDUCTING PB:1||domain formation:1||FORCE MICROSCOPY:1||RELAXATION:1||PLASMA RESONANCE:1||coupled Josephson junctions:1||COPPEROXIDE SUPERCONDUCTORS:1||CROSSOVER:1||SIMULATIONS:1||LOWTEMPERATURE:1||CONDUCTORS:1||METALINSULATORTRANSITION:1||SEMICONDUCTOR:1||FIELDEFFECT TRANSISTORS:1||ZEROVOLTAGE STATE:1||constanttemperature interlayer tunneling spectroscopy:1||Josephson supercurrent:1||BIPOLAR SUPERCURRENT:1||Interaction between Josephson and pancake vortices:1||flux jump:1||coaxial heterojunction nanorod:1||Natural Josephson coupling:1||BI2SR2CACU2O8+DELTA:1||VORTEX FLOW:1||TC SUPERCONDUCTORS:1||charge imbalance:1||Andreev diffractometer:1||intercalation:1||surface junction:1||Bi2212:1||tunnelling:1||GRAPHITE:1||GROWTH:1||collective transverse plasma modes:1||GAN:1||Macroscopic quantum tunneling:1||Fluctuation conductivity:1||Abovegap conductance jump:1||Josephson vortex motion:1||Intrinsic Josephson junctions:1||LAYERED SUPERCONDUCTORS:1||BI2SR2CACU2O8+Y:1||INTERFACES:1||BREAKDOWN:1||SYSTEMS:1||Anisotropy ratio:1||Josephson vortex:1||spin relaxation in superconductors:1||bibased single crystals:1||MESOSCOPIC PROXIMITY SUPERCONDUCTOR:1||reentrance of conductance:1||interlayer pair tunneling:1||JOSEPHSON:1||DISORDERED 2DIMENSIONAL SUPERCONDUCTORS:1||INDIUM FILMS:1||excited state:1||REGIME:1||triplet superconductivity:1||FILM:1||SCHOTTKY DIODES:1||peakdiphump structure:1||Kondo effect:1||REENTRANCE:1||Graphene:1||CONTACT:1||BERRYS PHASE:1||2DIMENSIONAL SUPERCONDUCTORS:1||Coulomb diamond:1||magnetic domain:1||spin injection:1||RESONANCE:1||plasma excitation modes:1||FLOW:1||OVERDOPED BI2SR2CACU2O8+DELTA:1||hole doping:1||chemical synthesis:1||phase transitions:1||superconductors:1||VORTEXGLASS SUPERCONDUCTIVITY:1||Kondorelated model:1||RADIATION:1||DOT:1||NANOBELTS:1||Complementarity:1||Closedloop AharonovBohm interferometer:1||pair breaking:1||interlayer phase fluctuation:1||MgB2 thin film:1||CONFINEMENT:1||WALLED CARBON NANOTUBES:1||TRANSITION:9||VORTICES:8||STATE:7||intrinsic Josephson junctions:7||SINGLECRYSTALS:7||JUNCTIONS:5||MODES:5||SUPERCURRENT:5||SUPERCONDUCTOR:5||CONDUCTANCE:5||HIGHTEMPERATURE SUPERCONDUCTORS:5||TRANSPORT:5||PHASE:5||FILMS:4||LOCALIZATION:4||SINGLE DIRAC CONE:4||WIRES:4||MAGNETICFIELD:4||STEPS:3||ELECTRONS:3||proximity effect:3||MODEL:3||ARRAYS:3||INTERFERENCE:3||fluxon dynamics:3||HETEROSTRUCTURES:3||INSULATOR:3||Andreev reflection:3||electronic transport:3||FISKE:3||superconductor:2||ZnO:2||quantum point contact:2||METAL:2||DYNAMICS:2||interlayer Josephson coupling:2||SUPERCONDUCTORS:2||YBA2CU3O7DELTA:2||LAYER:2||DOTS:2||quantum dot:2||Article:2||TRANSISTORS:2||CARBON NANOTUBES:2||GAP:2||MECHANISM:2||LINE:2||GIANT SHAPIRO STEPS:2||LAYERS:2||electron energy loss spectroscopy:2||physical phenomena:2||scanning electron microscopy:2||HGTE QUANTUMWELLS:2||BI2TE3:2||SPECTROSCOPY:2||PNJUNCTIONS:2||spinpolarized tunneling:2||INTRINSIC JOSEPHSONJUNCTIONS:2||FIELDS:2||positive magnetoresistance:2||dilute magnetic semiconductor:2||magnetic field:2||scanning transmission electron microscopy:2||QUANTUM OSCILLATIONS:2||TRANSPORTPROPERTIES:2||surface pair current:2||MAGNETORESISTANCE:2||NANORIBBONS:2||INSTABILITY:2||ANDREEV REFLECTION:2||microwave irradiation:2||vertical graphene josephson junction:2||BI2SE3:2||CONDUCTIVITY:2||highTc superconductors:2||DIMENSIONAL ELECTRONGAS:2||graphene:2||Topological insulators:2||Josephson coupling Fraunhofer interference pattern:2||FERROMAGNET:2||DEPENDENCE:2||DETECTOR:2||COHERENCE:2||INJECTION:2||GRAPHENE:1||JOSEPHSONJUNCTIONS:1||LAYERED SUPERCONDUCTOR:1||mode splitting:1||BEHAVIOR:1||spinpolarized transport:1||SUPERCONDUCTING TRANSITION:1||microwave response:1||PSEUDOGAP:1||phase coherence:1||TRANSITIONS:1||Long Josephson junction:1||Charge detection:1||collective resonance modes:1||plasma oscillation modes:1||Superconducting proximity effect:1||Iron pnictide superconductor:1||McMillanRowell oscillations:1||ferromagnetic microstructure:1||superradiant state:1||VOLTAGE:1||branch splitting:1||TENSOR:1||INTERCALATION:1||insitu fabrication:1||NDGAO3:1||DISORDERED METALS:1||GAUGE GLASS:1||LOWTEMPERATURE TRANSPORT:1||spontaneous spin polarization model:1||BIAS:1||emission of electromagnetic waves:1||YBA2CU3O7/PRBA2CU3O7 SUPERLATTICES:1||BOHM:1||SHAPIRO STEPS:1||superconductor/ferromagnet interface:1||OXIDE:1||ANDREEVREFLECTION:1||SinFeAsO single crystal:1||COLLECTIVE MOTION:1||ANGULARDEPENDENCE:1||SUPERCONDUCTIVITY:1||BILAYER GRAPHENE:1||PHOTOLUMINESCENT PROPERTIES:1||SUPERCONDUCTING WEAK LINKS:1||intrinsic Josephson junctions geometrical resonance:1||intrinsic Josephson junction:1||MESOSCOPIC SPINVALVE:1||Bi2212 single crystals:1||intrinsic junctions:1||ANDREEV REFLECTIONS:1||normalmetal/superconductor interface:1||IBI2SR2CACU2OY:1||THERMAL FLUCTUATIONS:1||MIXED STATE:1||BI2.15SR1.85CACU2O8+DELTA:1||intrinsic Josephson effects:1||CACUO:1||QUANTUM POINT CONTACTS:1||resonant tunneling state:1||coherence length:1||NANOWIRE:1||GATES:1||Phase line:1||Thermal activation:1||QUANTUMDOT:1||superconducting proximity effect:1||Andreev interferometer:1||WIRE:1||Josephsonvortexflow branches:1||Bi2212 cuprates:1||LATTICE:1||demannetization effect:1||SUPERCONDUCTING MIRRORS:1||GAS:1||VALLEY TRANSPORT:1||ELECTRODES:1||DEPENDENT TRANSPORT:1||BORNOPPENHEIMER APPROXIMATION:1||collective plasma oscillations:1||fluxon resonance steps:1||STACKS:1||COLLECTIVE DYNAMICS:1||PAIRING SYMMETRY:1||MUON SPIN ROTATION:1||DIMENSIONAL CROSSOVER:1||Bi2Sr2CaCu2Oy highTc superconductors:1||heterojunctions:1||nanostructures:1||surfaces and interfaces:1||QUANTUM TRANSPORT:1||MICROJUNCTIONS:1||RESONATORS:1||STATES:1||FIELD:1||FLUCTUATIONS:1||SCATTERING:1||mode splitting of Josephson vortexflow branches:1||2D superconductivity:1||TRANSISTOR:1||ENERGYGAP:1||SUPERLATTICES:1||IRONBASED SUPERCONDUCTORS:1||PHASEDEPENDENT RESISTANCE:1||QUANTUM PHASETRANSITIONS:1||ELECTRICFIELD:1||HIGH MAGNETICFIELDS:1||NANOWIRE HETEROSTRUCTURES:1||ZNO:1||pair breaking.:1||SUPERCONDUCTING PB:1||domain formation:1||FORCE MICROSCOPY:1||RELAXATION:1||PLASMA RESONANCE:1||coupled Josephson junctions:1||COPPEROXIDE SUPERCONDUCTORS:1||CROSSOVER:1||SIMULATIONS:1||LOWTEMPERATURE:1||CONDUCTORS:1||METALINSULATORTRANSITION:1||SEMICONDUCTOR:1||FIELDEFFECT TRANSISTORS:1||ZEROVOLTAGE STATE:1||constanttemperature interlayer tunneling spectroscopy:1||Josephson supercurrent:1||BIPOLAR SUPERCURRENT:1||Interaction between Josephson and pancake vortices:1||flux jump:1||coaxial heterojunction nanorod:1||Natural Josephson coupling:1||BI2SR2CACU2O8+DELTA:1||VORTEX FLOW:1||TC SUPERCONDUCTORS:1||charge imbalance:1||Andreev diffractometer:1||intercalation:1||surface junction:1||Bi2212:1||tunnelling:1||GRAPHITE:1||GROWTH:1||collective transverse plasma modes:1||GAN:1||Macroscopic quantum tunneling:1||Fluctuation conductivity:1||Abovegap conductance jump:1||Josephson vortex motion:1||Intrinsic Josephson junctions:1||LAYERED SUPERCONDUCTORS:1||BI2SR2CACU2O8+Y:1||INTERFACES:1||BREAKDOWN:1||SYSTEMS:1||Anisotropy ratio:1||Josephson vortex:1||spin relaxation in superconductors:1||bibased single crystals:1||MESOSCOPIC PROXIMITY SUPERCONDUCTOR:1||reentrance of conductance:1||interlayer pair tunneling:1||JOSEPHSON:1||DISORDERED 2DIMENSIONAL SUPERCONDUCTORS:1||INDIUM FILMS:1||excited state:1||REGIME:1||triplet superconductivity:1||FILM:1||SCHOTTKY DIODES:1||peakdiphump structure:1||Kondo effect:1||REENTRANCE:1||Graphene:1||CONTACT:1||BERRYS PHASE:1||2DIMENSIONAL SUPERCONDUCTORS:1||Coulomb diamond:1||magnetic domain:1||spin injection:1||RESONANCE:1||plasma excitation modes:1||FLOW:1||OVERDOPED BI2SR2CACU2O8+DELTA:1||hole doping:1||chemical synthesis:1||phase transitions:1||superconductors:1||VORTEXGLASS SUPERCONDUCTIVITY:1||Kondorelated model:1||RADIATION:1||DOT:1||NANOBELTS:1||Complementarity:1||Closedloop AharonovBohm interferometer:1||pair breaking:1||interlayer phase fluctuation:1||MgB2 thin film:1||CONFINEMENT:1||WALLED CARBON NANOTUBES:1||TRANSITION:9||VORTICES:8||STATE:7||intrinsic Josephson junctions:7||SINGLECRYSTALS:7||JUNCTIONS:5||MODES:5||SUPERCURRENT:5||SUPERCONDUCTOR:5||CONDUCTANCE:5||HIGHTEMPERATURE SUPERCONDUCTORS:5||TRANSPORT:5||PHASE:5||FILMS:4||LOCALIZATION:4||SINGLE DIRAC CONE:4||WIRES:4||MAGNETICFIELD:4||STEPS:3||ELECTRONS:3||proximity effect:3||MODEL:3||ARRAYS:3||INTERFERENCE:3||fluxon dynamics:3||HETEROSTRUCTURES:3||INSULATOR:3||Andreev reflection:3||electronic transport:3||FISKE:3||superconductor:2||ZnO:2||quantum point contact:2||METAL:2||DYNAMICS:2||interlayer Josephson coupling:2||SUPERCONDUCTORS:2||YBA2CU3O7DELTA:2||LAYER:2||DOTS:2||quantum dot:2||Article:2||TRANSISTORS:2||CARBON NANOTUBES:2||GAP:2||MECHANISM:2||LINE:2||GIANT SHAPIRO STEPS:2||LAYERS:2||electron energy loss spectroscopy:2||physical phenomena:2||scanning electron microscopy:2||HGTE QUANTUMWELLS:2||BI2TE3:2||SPECTROSCOPY:2||PNJUNCTIONS:2||spinpolarized tunneling:2||INTRINSIC JOSEPHSONJUNCTIONS:2||FIELDS:2||positive magnetoresistance:2||dilute magnetic semiconductor:2||magnetic field:2||scanning transmission electron microscopy:2||QUANTUM OSCILLATIONS:2||TRANSPORTPROPERTIES:2||surface pair current:2||MAGNETORESISTANCE:2||NANORIBBONS:2||INSTABILITY:2||ANDREEV REFLECTION:2||microwave irradiation:2||vertical graphene josephson junction:2||BI2SE3:2||CONDUCTIVITY:2||highTc superconductors:2||DIMENSIONAL ELECTRONGAS:2||graphene:2||Topological insulators:2||Josephson coupling Fraunhofer interference pattern:2||FERROMAGNET:2||DEPENDENCE:2||DETECTOR:2||COHERENCE:2||INJECTION:2||GRAPHENE:1||JOSEPHSONJUNCTIONS:1||LAYERED SUPERCONDUCTOR:1||mode splitting:1||BEHAVIOR:1||spinpolarized transport:1||SUPERCONDUCTING TRANSITION:1||microwave response:1||PSEUDOGAP:1||phase coherence:1||TRANSITIONS:1||Long Josephson junction:1||Charge detection:1||collective resonance modes:1||plasma oscillation modes:1||Superconducting proximity effect:1||Iron pnictide superconductor:1||McMillanRowell oscillations:1||ferromagnetic microstructure:1||superradiant state:1||VOLTAGE:1||branch splitting:1||TENSOR:1||INTERCALATION:1||insitu fabrication:1||NDGAO3:1||DISORDERED METALS:1||GAUGE GLASS:1||LOWTEMPERATURE TRANSPORT:1||spontaneous spin polarization model:1||BIAS:1||emission of electromagnetic waves:1||YBA2CU3O7/PRBA2CU3O7 SUPERLATTICES:1||BOHM:1||SHAPIRO STEPS:1||superconductor/ferromagnet interface:1||OXIDE:1||ANDREEVREFLECTION:1||SinFeAsO single crystal:1||COLLECTIVE MOTION:1||ANGULARDEPENDENCE:1||SUPERCONDUCTIVITY:1||BILAYER GRAPHENE:1||PHOTOLUMINESCENT PROPERTIES:1||SUPERCONDUCTING WEAK LINKS:1||intrinsic Josephson junctions geometrical resonance:1||intrinsic Josephson junction:1||MESOSCOPIC SPINVALVE:1||Bi2212 single crystals:1||intrinsic junctions:1||ANDREEV REFLECTIONS:1||normalmetal/superconductor interface:1||IBI2SR2CACU2OY:1||THERMAL FLUCTUATIONS:1||MIXED STATE:1||BI2.15SR1.85CACU2O8+DELTA:1||intrinsic Josephson effects:1||CACUO:1||QUANTUM POINT CONTACTS:1||resonant tunneling state:1||coherence length:1||NANOWIRE:1||GATES:1||Phase line:1||Thermal activation:1||QUANTUMDOT:1||superconducting proximity effect:1||Andreev interferometer:1||WIRE:1||Josephsonvortexflow branches:1||Bi2212 cuprates:1||LATTICE:1||demannetization effect:1||SUPERCONDUCTING MIRRORS:1||GAS:1||VALLEY TRANSPORT:1||ELECTRODES:1||DEPENDENT TRANSPORT:1||BORNOPPENHEIMER APPROXIMATION:1||collective plasma oscillations:1||fluxon resonance steps:1||STACKS:1||COLLECTIVE DYNAMICS:1||PAIRING SYMMETRY:1||MUON SPIN ROTATION:1||DIMENSIONAL CROSSOVER:1||Bi2Sr2CaCu2Oy highTc superconductors:1||heterojunctions:1||nanostructures:1||surfaces and interfaces:1||QUANTUM TRANSPORT:1||MICROJUNCTIONS:1||RESONATORS:1||STATES:1||FIELD:1||FLUCTUATIONS:1||SCATTERING:1||mode splitting of Josephson vortexflow branches:1||2D superconductivity:1||TRANSISTOR:1||ENERGYGAP:1||SUPERLATTICES:1||IRONBASED SUPERCONDUCTORS:1||PHASEDEPENDENT RESISTANCE:1||QUANTUM PHASETRANSITIONS:1||ELECTRICFIELD:1||HIGH MAGNETICFIELDS:1||NANOWIRE HETEROSTRUCTURES:1||ZNO:1||pair breaking.:1||SUPERCONDUCTING PB:1||domain formation:1||FORCE MICROSCOPY:1||RELAXATION:1||PLASMA RESONANCE:1||coupled Josephson junctions:1||COPPEROXIDE SUPERCONDUCTORS:1||CROSSOVER:1||SIMULATIONS:1||LOWTEMPERATURE:1||CONDUCTORS:1||METALINSULATORTRANSITION:1||SEMICONDUCTOR:1||FIELDEFFECT TRANSISTORS:1||ZEROVOLTAGE STATE:1||constanttemperature interlayer tunneling spectroscopy:1||Josephson supercurrent:1||BIPOLAR SUPERCURRENT:1||Interaction between Josephson and pancake vortices:1||flux jump:1||coaxial heterojunction nanorod:1||Natural Josephson coupling:1||BI2SR2CACU2O8+DELTA:1||VORTEX FLOW:1||TC SUPERCONDUCTORS:1||charge imbalance:1||Andreev diffractometer:1||intercalation:1||surface junction:1||Bi2212:1||tunnelling:1||GRAPHITE:1||GROWTH:1||collective transverse plasma modes:1||GAN:1||Macroscopic quantum tunneling:1||Fluctuation conductivity:1||Abovegap conductance jump:1||Josephson vortex motion:1||Intrinsic Josephson junctions:1||LAYERED SUPERCONDUCTORS:1||BI2SR2CACU2O8+Y:1||INTERFACES:1||BREAKDOWN:1||SYSTEMS:1||Anisotropy ratio:1||Josephson vortex:1||spin relaxation in superconductors:1||bibased single crystals:1||MESOSCOPIC PROXIMITY SUPERCONDUCTOR:1||reentrance of conductance:1||interlayer pair tunneling:1||JOSEPHSON:1||DISORDERED 2DIMENSIONAL SUPERCONDUCTORS:1||INDIUM FILMS:1||excited state:1||REGIME:1||triplet superconductivity:1||FILM:1||SCHOTTKY DIODES:1||peakdiphump structure:1||Kondo effect:1||REENTRANCE:1||Graphene:1||CONTACT:1||BERRYS PHASE:1||2DIMENSIONAL SUPERCONDUCTORS:1||Coulomb diamond:1||magnetic domain:1||spin injection:1||RESONANCE:1||plasma excitation modes:1||FLOW:1||OVERDOPED BI2SR2CACU2O8+DELTA:1||hole doping:1||chemical synthesis:1||phase transitions:1||superconductors:1||VORTEXGLASS SUPERCONDUCTIVITY:1||Kondorelated model:1||RADIATION:1||DOT:1||NANOBELTS:1||Complementarity:1||Closedloop AharonovBohm interferometer:1||pair breaking:1||interlayer phase fluctuation:1||MgB2 thin film:1||CONFINEMENT:1||WALLED CARBON NANOTUBES:1||TRANSITION:9||VORTICES:8||STATE:7||intrinsic Josephson junctions:7||SINGLECRYSTALS:7||JUNCTIONS:5||MODES:5||SUPERCURRENT:5||SUPERCONDUCTOR:5||CONDUCTANCE:5||HIGHTEMPERATURE SUPERCONDUCTORS:5||TRANSPORT:5||PHASE:5||FILMS:4||LOCALIZATION:4||SINGLE DIRAC CONE:4||WIRES:4||MAGNETICFIELD:4||STEPS:3||ELECTRONS:3||proximity effect:3||MODEL:3||ARRAYS:3||INTERFERENCE:3||fluxon dynamics:3||HETEROSTRUCTURES:3||INSULATOR:3||Andreev reflection:3||electronic transport:3||FISKE:3||superconductor:2||ZnO:2||quantum point contact:2||METAL:2||DYNAMICS:2||interlayer Josephson coupling:2||SUPERCONDUCTORS:2||YBA2CU3O7DELTA:2||LAYER:2||DOTS:2||quantum dot:2||Article:2||TRANSISTORS:2||CARBON NANOTUBES:2||GAP:2||MECHANISM:2||LINE:2||GIANT SHAPIRO STEPS:2||LAYERS:2||electron energy loss spectroscopy:2||physical phenomena:2||scanning electron microscopy:2||HGTE QUANTUMWELLS:2||BI2TE3:2||SPECTROSCOPY:2||PNJUNCTIONS:2||spinpolarized tunneling:2||INTRINSIC JOSEPHSONJUNCTIONS:2||FIELDS:2||positive magnetoresistance:2||dilute magnetic semiconductor:2||magnetic field:2||scanning transmission electron microscopy:2||QUANTUM OSCILLATIONS:2||TRANSPORTPROPERTIES:2||surface pair current:2||MAGNETORESISTANCE:2||NANORIBBONS:2||INSTABILITY:2||ANDREEV REFLECTION:2||microwave irradiation:2||vertical graphene josephson junction:2||BI2SE3:2||CONDUCTIVITY:2||highTc superconductors:2||DIMENSIONAL ELECTRONGAS:2||graphene:2||Topological insulators:2||Josephson coupling Fraunhofer interference pattern:2||FERROMAGNET:2||DEPENDENCE:2||DETECTOR:2||COHERENCE:2||INJECTION:2||GRAPHENE:1||JOSEPHSONJUNCTIONS:1||LAYERED SUPERCONDUCTOR:1||mode splitting:1||BEHAVIOR:1||spinpolarized transport:1||SUPERCONDUCTING TRANSITION:1||microwave response:1||PSEUDOGAP:1||phase coherence:1||TRANSITIONS:1||Long Josephson junction:1||Charge detection:1||collective resonance modes:1||plasma oscillation modes:1||Superconducting proximity effect:1||Iron pnictide superconductor:1||McMillanRowell oscillations:1||ferromagnetic microstructure:1||superradiant state:1||VOLTAGE:1||branch splitting:1||TENSOR:1||INTERCALATION:1||insitu fabrication:1||NDGAO3:1||DISORDERED METALS:1||GAUGE GLASS:1||LOWTEMPERATURE TRANSPORT:1||spontaneous spin polarization model:1||BIAS:1||emission of electromagnetic waves:1||YBA2CU3O7/PRBA2CU3O7 SUPERLATTICES:1||BOHM:1||SHAPIRO STEPS:1||superconductor/ferromagnet interface:1||OXIDE:1||ANDREEVREFLECTION:1||SinFeAsO single crystal:1||COLLECTIVE MOTION:1||ANGULARDEPENDENCE:1||SUPERCONDUCTIVITY:1||BILAYER GRAPHENE:1||PHOTOLUMINESCENT PROPERTIES:1||SUPERCONDUCTING WEAK LINKS:1||intrinsic Josephson junctions geometrical resonance:1||intrinsic Josephson junction:1||MESOSCOPIC SPINVALVE:1||Bi2212 single crystals:1||intrinsic junctions:1||ANDREEV REFLECTIONS:1||normalmetal/superconductor interface:1||IBI2SR2CACU2OY:1||THERMAL FLUCTUATIONS:1||MIXED STATE:1||BI2.15SR1.85CACU2O8+DELTA:1||intrinsic Josephson effects:1||CACUO:1||QUANTUM POINT CONTACTS:1||resonant tunneling state:1||coherence length:1||NANOWIRE:1||GATES:1||Phase line:1||Thermal activation:1||QUANTUMDOT:1||superconducting proximity effect:1||Andreev interferometer:1||WIRE:1||Josephsonvortexflow branches:1||Bi2212 cuprates:1||LATTICE:1||demannetization effect:1||SUPERCONDUCTING MIRRORS:1||GAS:1||VALLEY TRANSPORT:1||ELECTRODES:1||DEPENDENT TRANSPORT:1||BORNOPPENHEIMER APPROXIMATION:1||collective plasma oscillations:1||fluxon resonance steps:1||STACKS:1||COLLECTIVE DYNAMICS:1||PAIRING SYMMETRY:1||MUON SPIN ROTATION:1||DIMENSIONAL CROSSOVER:1||Bi2Sr2CaCu2Oy highTc superconductors:1||heterojunctions:1||nanostructures:1||surfaces and interfaces:1||QUANTUM TRANSPORT:1||MICROJUNCTIONS:1||RESONATORS:1||STATES:1||FIELD:1||FLUCTUATIONS:1||SCATTERING:1||mode splitting of Josephson vortexflow branches:1||2D superconductivity:1||TRANSISTOR:1||ENERGYGAP:1||SUPERLATTICES:1||IRONBASED SUPERCONDUCTORS:1||PHASEDEPENDENT RESISTANCE:1||QUANTUM PHASETRANSITIONS:1||ELECTRICFIELD:1||HIGH MAGNETICFIELDS:1||NANOWIRE HETEROSTRUCTURES:1||ZNO:1||pair breaking.:1||SUPERCONDUCTING PB:1||domain formation:1||FORCE MICROSCOPY:1||RELAXATION:1||PLASMA RESONANCE:1||coupled Josephson junctions:1||COPPEROXIDE SUPERCONDUCTORS:1||CROSSOVER:1||SIMULATIONS:1||LOWTEMPERATURE:1||CONDUCTORS:1||METALINSULATORTRANSITION:1||SEMICONDUCTOR:1||FIELDEFFECT TRANSISTORS:1||ZEROVOLTAGE STATE:1||constanttemperature interlayer tunneling spectroscopy:1||Josephson supercurrent:1||BIPOLAR SUPERCURRENT:1||Interaction between Josephson and pancake vortices:1||flux jump:1||coaxial heterojunction nanorod:1||Natural Josephson coupling:1||BI2SR2CACU2O8+DELTA:1||VORTEX FLOW:1||TC SUPERCONDUCTORS:1||charge imbalance:1||Andreev diffractometer:1||intercalation:1||surface junction:1||Bi2212:1||tunnelling:1||GRAPHITE:1||GROWTH:1||collective transverse plasma modes:1||GAN:1||Macroscopic quantum tunneling:1||Fluctuation conductivity:1||Abovegap conductance jump:1||Josephson vortex motion:1||Intrinsic Josephson junctions:1||LAYERED SUPERCONDUCTORS:1||BI2SR2CACU2O8+Y:1||INTERFACES:1||BREAKDOWN:1||SYSTEMS:1||Anisotropy ratio:1||Josephson vortex:1||spin relaxation in superconductors:1||bibased single crystals:1||MESOSCOPIC PROXIMITY SUPERCONDUCTOR:1||reentrance of conductance:1||interlayer pair tunneling:1||JOSEPHSON:1||DISORDERED 2DIMENSIONAL SUPERCONDUCTORS:1||INDIUM FILMS:1||excited state:1||REGIME:1||triplet superconductivity:1||FILM:1||SCHOTTKY DIODES:1||peakdiphump structure:1||Kondo effect:1||REENTRANCE:1||Graphene:1||CONTACT:1||BERRYS PHASE:1||2DIMENSIONAL SUPERCONDUCTORS:1||Coulomb diamond:1||magnetic domain:1||spin injection:1||RESONANCE:1||plasma excitation modes:1||FLOW:1||OVERDOPED BI2SR2CACU2O8+DELTA:1||hole doping:1||chemical synthesis:1||phase transitions:1||superconductors:1||VORTEXGLASS SUPERCONDUCTIVITY:1||Kondorelated model:1||RADIATION:1||DOT:1||NANOBELTS:1||Complementarity:1||Closedloop AharonovBohm interferometer:1||pair breaking:1||interlayer phase fluctuation:1||MgB2 thin film:1||CONFINEMENT:1||WALLED CARBON NANOTUBES:1||TRANSITION:9||VORTICES:8||STATE:7||intrinsic Josephson junctions:7||SINGLECRYSTALS:7||JUNCTIONS:5||MODES:5||SUPERCURRENT:5||SUPERCONDUCTOR:5||CONDUCTANCE:5||HIGHTEMPERATURE SUPERCONDUCTORS:5||TRANSPORT:5||PHASE:5||FILMS:4||LOCALIZATION:4||SINGLE DIRAC CONE:4||WIRES:4||MAGNETICFIELD:4||STEPS:3||ELECTRONS:3||proximity effect:3||MODEL:3||ARRAYS:3||INTERFERENCE:3||fluxon dynamics:3||HETEROSTRUCTURES:3||INSULATOR:3||Andreev reflection:3||electronic transport:3||FISKE:3||superconductor:2||ZnO:2||quantum point contact:2||METAL:2||DYNAMICS:2||interlayer Josephson coupling:2||SUPERCONDUCTORS:2||YBA2CU3O7DELTA:2||LAYER:2||DOTS:2||quantum dot:2||Article:2||TRANSISTORS:2||CARBON NANOTUBES:2||GAP:2||MECHANISM:2||LINE:2||GIANT SHAPIRO STEPS:2||LAYERS:2||electron energy loss spectroscopy:2||physical phenomena:2||scanning electron microscopy:2||HGTE QUANTUMWELLS:2||BI2TE3:2||SPECTROSCOPY:2||PNJUNCTIONS:2||spinpolarized tunneling:2||INTRINSIC JOSEPHSONJUNCTIONS:2||FIELDS:2||positive magnetoresistance:2||dilute magnetic semiconductor:2||magnetic field:2||scanning transmission electron microscopy:2||QUANTUM OSCILLATIONS:2||TRANSPORTPROPERTIES:2||surface pair current:2||MAGNETORESISTANCE:2||NANORIBBONS:2||INSTABILITY:2||ANDREEV REFLECTION:2||microwave irradiation:2||vertical graphene josephson junction:2||BI2SE3:2||CONDUCTIVITY:2||highTc superconductors:2||DIMENSIONAL ELECTRONGAS:2||graphene:2||Topological insulators:2||Josephson coupling Fraunhofer interference pattern:2||FERROMAGNET:2||DEPENDENCE:2||DETECTOR:2||COHERENCE:2||INJECTION:2||GRAPHENE:1||JOSEPHSONJUNCTIONS:1||LAYERED SUPERCONDUCTOR:1||mode splitting:1||BEHAVIOR:1||spinpolarized transport:1||SUPERCONDUCTING TRANSITION:1||microwave response:1||PSEUDOGAP:1||phase coherence:1||TRANSITIONS:1||Long Josephson junction:1||Charge detection:1||collective resonance modes:1||plasma oscillation modes:1||Superconducting proximity effect:1||Iron pnictide superconductor:1||McMillanRowell oscillations:1||ferromagnetic microstructure:1||superradiant state:1||VOLTAGE:1||branch splitting:1||TENSOR:1||INTERCALATION:1||insitu fabrication:1||NDGAO3:1||DISORDERED METALS:1||GAUGE GLASS:1||LOWTEMPERATURE TRANSPORT:1||spontaneous spin polarization model:1||BIAS:1||emission of electromagnetic waves:1||YBA2CU3O7/PRBA2CU3O7 SUPERLATTICES:1||BOHM:1||SHAPIRO STEPS:1||superconductor/ferromagnet interface:1||OXIDE:1||ANDREEVREFLECTION:1||SinFeAsO single crystal:1||COLLECTIVE MOTION:1||ANGULARDEPENDENCE:1||SUPERCONDUCTIVITY:1||BILAYER GRAPHENE:1||PHOTOLUMINESCENT PROPERTIES:1||SUPERCONDUCTING WEAK LINKS:1||intrinsic Josephson junctions geometrical resonance:1||intrinsic Josephson junction:1||MESOSCOPIC SPINVALVE:1||Bi2212 single crystals:1||intrinsic junctions:1||ANDREEV REFLECTIONS:1||normalmetal/superconductor interface:1||IBI2SR2CACU2OY:1||THERMAL FLUCTUATIONS:1||MIXED STATE:1||BI2.15SR1.85CACU2O8+DELTA:1||intrinsic Josephson effects:1||CACUO:1||QUANTUM POINT CONTACTS:1||resonant tunneling state:1||coherence length:1||NANOWIRE:1||GATES:1||Phase line:1||Thermal activation:1||QUANTUMDOT:1||superconducting proximity effect:1||Andreev interferometer:1||WIRE:1||Josephsonvortexflow branches:1||Bi2212 cuprates:1||LATTICE:1||demannetization effect:1||SUPERCONDUCTING MIRRORS:1||GAS:1||VALLEY TRANSPORT:1||ELECTRODES:1||DEPENDENT TRANSPORT:1||BORNOPPENHEIMER APPROXIMATION:1||collective plasma oscillations:1||fluxon resonance steps:1||STACKS:1||COLLECTIVE DYNAMICS:1||PAIRING SYMMETRY:1||MUON SPIN ROTATION:1||DIMENSIONAL CROSSOVER:1||Bi2Sr2CaCu2Oy highTc superconductors:1||heterojunctions:1||nanostructures:1||surfaces and interfaces:1||QUANTUM TRANSPORT:1||MICROJUNCTIONS:1||RESONATORS:1||STATES:1||FIELD:1||FLUCTUATIONS:1||SCATTERING:1||mode splitting of Josephson vortexflow branches:1||2D superconductivity:1||TRANSISTOR:1||ENERGYGAP:1||SUPERLATTICES:1||IRONBASED SUPERCONDUCTORS:1||PHASEDEPENDENT RESISTANCE:1||QUANTUM PHASETRANSITIONS:1||ELECTRICFIELD:1||HIGH MAGNETICFIELDS:1||NANOWIRE HETEROSTRUCTURES:1||ZNO:1||pair breaking.:1||SUPERCONDUCTING PB:1||domain formation:1||FORCE MICROSCOPY:1||RELAXATION:1||PLASMA RESONANCE:1||coupled Josephson junctions:1||COPPEROXIDE SUPERCONDUCTORS:1||CROSSOVER:1||SIMULATIONS:1||LOWTEMPERATURE:1||CONDUCTORS:1||METALINSULATORTRANSITION:1||SEMICONDUCTOR:1||FIELDEFFECT TRANSISTORS:1||ZEROVOLTAGE STATE:1||constanttemperature interlayer tunneling spectroscopy:1||Josephson supercurrent:1||BIPOLAR SUPERCURRENT:1||Interaction between Josephson and pancake vortices:1||flux jump:1||coaxial heterojunction nanorod:1||Natural Josephson coupling:1||BI2SR2CACU2O8+DELTA:1||VORTEX FLOW:1||TC SUPERCONDUCTORS:1||charge imbalance:1||Andreev diffractometer:1||intercalation:1||surface junction:1||Bi2212:1||tunnelling:1||GRAPHITE:1||GROWTH:1||collective transverse plasma modes:1||GAN:1||Macroscopic quantum tunneling:1||Fluctuation conductivity:1||Abovegap conductance jump:1||Josephson vortex motion:1||Intrinsic Josephson junctions:1||LAYERED SUPERCONDUCTORS:1||BI2SR2CACU2O8+Y:1||INTERFACES:1||BREAKDOWN:1||SYSTEMS:1||Anisotropy ratio:1||Josephson vortex:1||spin relaxation in superconductors:1||bibased single crystals:1||MESOSCOPIC PROXIMITY SUPERCONDUCTOR:1||reentrance of conductance:1||interlayer pair tunneling:1||JOSEPHSON:1||DISORDERED 2DIMENSIONAL SUPERCONDUCTORS:1||INDIUM FILMS:1||excited state:1||REGIME:1||triplet superconductivity:1||FILM:1||SCHOTTKY DIODES:1||peakdiphump structure:1||Kondo effect:1||REENTRANCE:1||Graphene:1||CONTACT:1||BERRYS PHASE:1||2DIMENSIONAL SUPERCONDUCTORS:1||Coulomb diamond:1||magnetic domain:1||spin injection:1||RESONANCE:1||plasma excitation modes:1||FLOW:1||OVERDOPED BI2SR2CACU2O8+DELTA:1||hole doping:1||chemical synthesis:1||phase transitions:1||superconductors:1||VORTEXGLASS SUPERCONDUCTIVITY:1||Kondorelated model:1||RADIATION:1||DOT:1||NANOBELTS:1||Complementarity:1||Closedloop AharonovBohm interferometer:1||pair breaking:1||interlayer phase fluctuation:1||MgB2 thin film:1||CONFINEMENT:1||WALLED CARBON NANOTUBES:1||TRANSITION:9||VORTICES:8||STATE:7||intrinsic Josephson junctions:7||SINGLECRYSTALS:7||JUNCTIONS:5||MODES:5||SUPERCURRENT:5||SUPERCONDUCTOR:5||CONDUCTANCE:5||HIGHTEMPERATURE SUPERCONDUCTORS:5||TRANSPORT:5||PHASE:5||FILMS:4||LOCALIZATION:4||SINGLE DIRAC CONE:4||WIRES:4||MAGNETICFIELD:4||STEPS:3||ELECTRONS:3||proximity effect:3||MODEL:3||ARRAYS:3||INTERFERENCE:3||fluxon dynamics:3||HETEROSTRUCTURES:3||INSULATOR:3||Andreev reflection:3||electronic transport:3||FISKE:3||superconductor:2||ZnO:2||quantum point contact:2||METAL:2||DYNAMICS:2||interlayer Josephson coupling:2||SUPERCONDUCTORS:2||YBA2CU3O7DELTA:2||LAYER:2||DOTS:2||quantum dot:2||Article:2||TRANSISTORS:2||CARBON NANOTUBES:2||GAP:2||MECHANISM:2||LINE:2||GIANT SHAPIRO STEPS:2||LAYERS:2||electron energy loss spectroscopy:2||physical phenomena:2||scanning electron microscopy:2||HGTE QUANTUMWELLS:2||BI2TE3:2||SPECTROSCOPY:2||PNJUNCTIONS:2||spinpolarized tunneling:2||INTRINSIC JOSEPHSONJUNCTIONS:2||FIELDS:2||positive magnetoresistance:2||dilute magnetic semiconductor:2||magnetic field:2||scanning transmission electron microscopy:2||QUANTUM OSCILLATIONS:2||TRANSPORTPROPERTIES:2||surface pair current:2||MAGNETORESISTANCE:2||NANORIBBONS:2||INSTABILITY:2||ANDREEV REFLECTION:2||microwave irradiation:2||vertical graphene josephson junction:2||BI2SE3:2||CONDUCTIVITY:2||highTc superconductors:2||DIMENSIONAL ELECTRONGAS:2||graphene:2||Topological insulators:2||Josephson coupling Fraunhofer interference pattern:2||FERROMAGNET:2||DEPENDENCE:2||DETECTOR:2||COHERENCE:2||INJECTION:2||GRAPHENE:1||JOSEPHSONJUNCTIONS:1||LAYERED SUPERCONDUCTOR:1||mode splitting:1||BEHAVIOR:1||spinpolarized transport:1||SUPERCONDUCTING TRANSITION:1||microwave response:1||PSEUDOGAP:1||phase coherence:1||TRANSITIONS:1||Long Josephson junction:1||Charge detection:1||collective resonance modes:1||plasma oscillation modes:1||Superconducting proximity effect:1||Iron pnictide superconductor:1||McMillanRowell oscillations:1||ferromagnetic microstructure:1||superradiant state:1||VOLTAGE:1||branch splitting:1||TENSOR:1||INTERCALATION:1||insitu fabrication:1||NDGAO3:1||DISORDERED METALS:1||GAUGE GLASS:1||LOWTEMPERATURE TRANSPORT:1||spontaneous spin polarization model:1||BIAS:1||emission of electromagnetic waves:1||YBA2CU3O7/PRBA2CU3O7 SUPERLATTICES:1||BOHM:1||SHAPIRO STEPS:1||superconductor/ferromagnet interface:1||OXIDE:1||ANDREEVREFLECTION:1||SinFeAsO single crystal:1||COLLECTIVE MOTION:1||ANGULARDEPENDENCE:1||SUPERCONDUCTIVITY:1||BILAYER GRAPHENE:1||PHOTOLUMINESCENT PROPERTIES:1||SUPERCONDUCTING WEAK LINKS:1||intrinsic Josephson junctions geometrical resonance:1||intrinsic Josephson junction:1||MESOSCOPIC SPINVALVE:1||Bi2212 single crystals:1||intrinsic junctions:1||ANDREEV REFLECTIONS:1||normalmetal/superconductor interface:1||IBI2SR2CACU2OY:1||THERMAL FLUCTUATIONS:1||MIXED STATE:1||BI2.15SR1.85CACU2O8+DELTA:1||intrinsic Josephson effects:1||CACUO:1||QUANTUM POINT CONTACTS:1||resonant tunneling state:1||coherence length:1||NANOWIRE:1||GATES:1||Phase line:1||Thermal activation:1||QUANTUMDOT:1||superconducting proximity effect:1||Andreev interferometer:1||WIRE:1||Josephsonvortexflow branches:1||Bi2212 cuprates:1||LATTICE:1||demannetization effect:1||SUPERCONDUCTING MIRRORS:1||GAS:1||VALLEY TRANSPORT:1||ELECTRODES:1||DEPENDENT TRANSPORT:1||BORNOPPENHEIMER APPROXIMATION:1||collective plasma oscillations:1||fluxon resonance steps:1||STACKS:1||COLLECTIVE DYNAMICS:1||PAIRING SYMMETRY:1||MUON SPIN ROTATION:1||DIMENSIONAL CROSSOVER:1||Bi2Sr2CaCu2Oy highTc superconductors:1||heterojunctions:1||nanostructures:1||surfaces and interfaces:1||QUANTUM TRANSPORT:1||MICROJUNCTIONS:1||RESONATORS:1||STATES:1||FIELD:1||FLUCTUATIONS:1||SCATTERING:1||mode splitting of Josephson vortexflow branches:1||2D superconductivity:1||TRANSISTOR:1||ENERGYGAP:1||SUPERLATTICES:1||IRONBASED SUPERCONDUCTORS:1||PHASEDEPENDENT RESISTANCE:1||QUANTUM PHASETRANSITIONS:1||ELECTRICFIELD:1||HIGH MAGNETICFIELDS:1||NANOWIRE HETEROSTRUCTURES:1||ZNO:1||pair breaking.:1||SUPERCONDUCTING PB:1||domain formation:1||FORCE MICROSCOPY:1||RELAXATION:1||PLASMA RESONANCE:1||coupled Josephson junctions:1||COPPEROXIDE SUPERCONDUCTORS:1||CROSSOVER:1||SIMULATIONS:1||LOWTEMPERATURE:1||CONDUCTORS:1||METALINSULATORTRANSITION:1||SEMICONDUCTOR:1||FIELDEFFECT TRANSISTORS:1||ZEROVOLTAGE STATE:1||constanttemperature interlayer tunneling spectroscopy:1||Josephson supercurrent:1||BIPOLAR SUPERCURRENT:1||Interaction between Josephson and pancake vortices:1||flux jump:1||coaxial heterojunction nanorod:1||Natural Josephson coupling:1||BI2SR2CACU2O8+DELTA:1||VORTEX FLOW:1||TC SUPERCONDUCTORS:1||charge imbalance:1||Andreev diffractometer:1||intercalation:1||surface junction:1||Bi2212:1||tunnelling:1||GRAPHITE:1||GROWTH:1||collective transverse plasma modes:1||GAN:1||Macroscopic quantum tunneling:1||Fluctuation conductivity:1||Abovegap conductance jump:1||Josephson vortex motion:1||Intrinsic Josephson junctions:1||LAYERED SUPERCONDUCTORS:1||BI2SR2CACU2O8+Y:1||INTERFACES:1||BREAKDOWN:1||SYSTEMS:1||Anisotropy ratio:1||Josephson vortex:1||spin relaxation in superconductors:1||bibased single crystals:1||MESOSCOPIC PROXIMITY SUPERCONDUCTOR:1||reentrance of conductance:1||interlayer pair tunneling:1||JOSEPHSON:1||DISORDERED 2DIMENSIONAL SUPERCONDUCTORS:1||INDIUM FILMS:1||excited state:1||REGIME:1||triplet superconductivity:1||FILM:1||SCHOTTKY DIODES:1||peakdiphump structure:1||Kondo effect:1||REENTRANCE:1||Graphene:1||CONTACT:1||BERRYS PHASE:1||2DIMENSIONAL SUPERCONDUCTORS:1||Coulomb diamond:1||magnetic domain:1||spin injection:1||RESONANCE:1||plasma excitation modes:1||FLOW:1||OVERDOPED BI2SR2CACU2O8+DELTA:1||hole doping:1||chemical synthesis:1||phase transitions:1||superconductors:1||VORTEXGLASS SUPERCONDUCTIVITY:1||Kondorelated model:1||RADIATION:1||DOT:1||NANOBELTS:1||Complementarity:1||Closedloop AharonovBohm interferometer:1||pair breaking:1||interlayer phase fluctuation:1||MgB2 thin film:1||CONFINEMENT:1||WALLED CARBON NANOTUBES:1||TRANSITION:9||VORTICES:8||STATE:7||intrinsic Josephson junctions:7||SINGLECRYSTALS:7||JUNCTIONS:5||MODES:5||SUPERCURRENT:5||SUPERCONDUCTOR:5||CONDUCTANCE:5||HIGHTEMPERATURE SUPERCONDUCTORS:5||TRANSPORT:5||PHASE:5||FILMS:4||LOCALIZATION:4||SINGLE DIRAC CONE:4||WIRES:4||MAGNETICFIELD:4||STEPS:3||ELECTRONS:3||proximity effect:3||MODEL:3||ARRAYS:3||INTERFERENCE:3||fluxon dynamics:3||HETEROSTRUCTURES:3||INSULATOR:3||Andreev reflection:3||electronic transport:3||FISKE:3||superconductor:2||ZnO:2||quantum point contact:2||METAL:2||DYNAMICS:2||interlayer Josephson coupling:2||SUPERCONDUCTORS:2||YBA2CU3O7DELTA:2||LAYER:2||DOTS:2||quantum dot:2||Article:2||TRANSISTORS:2||CARBON NANOTUBES:2||GAP:2||MECHANISM:2||LINE:2||GIANT SHAPIRO STEPS:2||LAYERS:2||electron energy loss spectroscopy:2||physical phenomena:2||scanning electron microscopy:2||HGTE QUANTUMWELLS:2||BI2TE3:2||SPECTROSCOPY:2||PNJUNCTIONS:2||spinpolarized tunneling:2||INTRINSIC JOSEPHSONJUNCTIONS:2||FIELDS:2||positive magnetoresistance:2||dilute magnetic semiconductor:2||magnetic field:2||scanning transmission electron microscopy:2||QUANTUM OSCILLATIONS:2||TRANSPORTPROPERTIES:2||surface pair current:2||MAGNETORESISTANCE:2||NANORIBBONS:2||INSTABILITY:2||ANDREEV REFLECTION:2||microwave irradiation:2||vertical graphene josephson junction:2||BI2SE3:2||CONDUCTIVITY:2||highTc superconductors:2||DIMENSIONAL ELECTRONGAS:2||graphene:2||Topological insulators:2||Josephson coupling Fraunhofer interference pattern:2||FERROMAGNET:2||DEPENDENCE:2||DETECTOR:2||COHERENCE:2||INJECTION:2||GRAPHENE:1||JOSEPHSONJUNCTIONS:1||LAYERED SUPERCONDUCTOR:1||mode splitting:1||BEHAVIOR:1||spinpolarized transport:1||SUPERCONDUCTING TRANSITION:1||microwave response:1||PSEUDOGAP:1||phase coherence:1||TRANSITIONS:1||Long Josephson junction:1||Charge detection:1||collective resonance modes:1||plasma oscillation modes:1||Superconducting proximity effect:1||Iron pnictide superconductor:1||McMillanRowell oscillations:1||ferromagnetic microstructure:1||superradiant state:1||VOLTAGE:1||branch splitting:1||TENSOR:1||INTERCALATION:1||insitu fabrication:1||NDGAO3:1||DISORDERED METALS:1||GAUGE GLASS:1||LOWTEMPERATURE TRANSPORT:1||spontaneous spin polarization model:1||BIAS:1||emission of electromagnetic waves:1||YBA2CU3O7/PRBA2CU3O7 SUPERLATTICES:1||BOHM:1||SHAPIRO STEPS:1||superconductor/ferromagnet interface:1||OXIDE:1||ANDREEVREFLECTION:1||SinFeAsO single crystal:1||COLLECTIVE MOTION:1||ANGULARDEPENDENCE:1||SUPERCONDUCTIVITY:1||BILAYER GRAPHENE:1||PHOTOLUMINESCENT PROPERTIES:1||SUPERCONDUCTING WEAK LINKS:1||intrinsic Josephson junctions geometrical resonance:1||intrinsic Josephson junction:1||MESOSCOPIC SPINVALVE:1||Bi2212 single crystals:1||intrinsic junctions:1||ANDREEV REFLECTIONS:1||normalmetal/superconductor interface:1||IBI2SR2CACU2OY:1||THERMAL FLUCTUATIONS:1||MIXED STATE:1||BI2.15SR1.85CACU2O8+DELTA:1||intrinsic Josephson effects:1||CACUO:1||QUANTUM POINT CONTACTS:1||resonant tunneling state:1||coherence length:1||NANOWIRE:1||GATES:1||Phase line:1||Thermal activation:1||QUANTUMDOT:1||superconducting proximity effect:1||Andreev interferometer:1||WIRE:1||Josephsonvortexflow branches:1||Bi2212 cuprates:1||LATTICE:1||demannetization effect:1||SUPERCONDUCTING MIRRORS:1||GAS:1||VALLEY TRANSPORT:1||ELECTRODES:1||DEPENDENT TRANSPORT:1||BORNOPPENHEIMER APPROXIMATION:1||collective plasma oscillations:1||fluxon resonance steps:1||STACKS:1||COLLECTIVE DYNAMICS:1||PAIRING SYMMETRY:1||MUON SPIN ROTATION:1||DIMENSIONAL CROSSOVER:1||Bi2Sr2CaCu2Oy highTc superconductors:1||heterojunctions:1||nanostructures:1||surfaces and interfaces:1||QUANTUM TRANSPORT:1||MICROJUNCTIONS:1||RESONATORS:1||STATES:1||FIELD:1||FLUCTUATIONS:1||SCATTERING:1||mode splitting of Josephson vortexflow branches:1||2D superconductivity:1||TRANSISTOR:1||ENERGYGAP:1||SUPERLATTICES:1||IRONBASED SUPERCONDUCTORS:1||PHASEDEPENDENT RESISTANCE:1||QUANTUM PHASETRANSITIONS:1||ELECTRICFIELD:1||HIGH MAGNETICFIELDS:1||NANOWIRE HETEROSTRUCTURES:1||ZNO:1||pair breaking.:1||SUPERCONDUCTING PB:1||domain formation:1||FORCE MICROSCOPY:1||RELAXATION:1||PLASMA RESONANCE:1||coupled Josephson junctions:1||COPPEROXIDE SUPERCONDUCTORS:1||CROSSOVER:1||SIMULATIONS:1||LOWTEMPERATURE:1||CONDUCTORS:1||METALINSULATORTRANSITION:1||SEMICONDUCTOR:1||FIELDEFFECT TRANSISTORS:1||ZEROVOLTAGE STATE:1||constanttemperature interlayer tunneling spectroscopy:1||Josephson supercurrent:1||BIPOLAR SUPERCURRENT:1||Interaction between Josephson and pancake vortices:1||flux jump:1||coaxial heterojunction nanorod:1||Natural Josephson coupling:1||BI2SR2CACU2O8+DELTA:1||VORTEX FLOW:1||TC SUPERCONDUCTORS:1||charge imbalance:1||Andreev diffractometer:1||intercalation:1||surface junction:1||Bi2212:1||tunnelling:1||GRAPHITE:1||GROWTH:1||collective transverse plasma modes:1||GAN:1||Macroscopic quantum tunneling:1||Fluctuation conductivity:1||Abovegap conductance jump:1||Josephson vortex motion:1||Intrinsic Josephson junctions:1||LAYERED SUPERCONDUCTORS:1||BI2SR2CACU2O8+Y:1||INTERFACES:1||BREAKDOWN:1||SYSTEMS:1||Anisotropy ratio:1||Josephson vortex:1||spin relaxation in superconductors:1||bibased single crystals:1||MESOSCOPIC PROXIMITY SUPERCONDUCTOR:1||reentrance of conductance:1||interlayer pair tunneling:1||JOSEPHSON:1||DISORDERED 2DIMENSIONAL SUPERCONDUCTORS:1||INDIUM FILMS:1||excited state:1||REGIME:1||triplet superconductivity:1||FILM:1||SCHOTTKY DIODES:1||peakdiphump structure:1||Kondo effect:1||REENTRANCE:1||Graphene:1||CONTACT:1||BERRYS PHASE:1||2DIMENSIONAL SUPERCONDUCTORS:1||Coulomb diamond:1||magnetic domain:1||spin injection:1||RESONANCE:1||plasma excitation modes:1||FLOW:1||OVERDOPED BI2SR2CACU2O8+DELTA:1||hole doping:1||chemical synthesis:1||phase transitions:1||superconductors:1||VORTEXGLASS SUPERCONDUCTIVITY:1||Kondorelated model:1||RADIATION:1||DOT:1||NANOBELTS:1||Complementarity:1||Closedloop AharonovBohm interferometer:1||pair breaking:1||interlayer phase fluctuation:1||MgB2 thin film:1||CONFINEMENT:1||WALLED CARBON NANOTUBES:1||TRANSITION:9||VORTICES:8||STATE:7||intrinsic Josephson junctions:7||SINGLECRYSTALS:7||JUNCTIONS:5||MODES:5||SUPERCURRENT:5||SUPERCONDUCTOR:5||CONDUCTANCE:5||HIGHTEMPERATURE SUPERCONDUCTORS:5||TRANSPORT:5||PHASE:5||FILMS:4||LOCALIZATION:4||SINGLE DIRAC CONE:4||WIRES:4||MAGNETICFIELD:4||STEPS:3||ELECTRONS:3||proximity effect:3||MODEL:3||ARRAYS:3||INTERFERENCE:3||fluxon dynamics:3||HETEROSTRUCTURES:3||INSULATOR:3||Andreev reflection:3||electronic transport:3||FISKE:3||superconductor:2||ZnO:2||quantum point contact:2||METAL:2||DYNAMICS:2||interlayer Josephson coupling:2||SUPERCONDUCTORS:2||YBA2CU3O7DELTA:2||LAYER:2||DOTS:2||quantum dot:2||Article:2||TRANSISTORS:2||CARBON NANOTUBES:2||GAP:2||MECHANISM:2||LINE:2||GIANT SHAPIRO STEPS:2||LAYERS:2||electron energy loss spectroscopy:2||physical phenomena:2||scanning electron microscopy:2||HGTE QUANTUMWELLS:2||BI2TE3:2||SPECTROSCOPY:2||PNJUNCTIONS:2||spinpolarized tunneling:2||INTRINSIC JOSEPHSONJUNCTIONS:2||FIELDS:2||positive magnetoresistance:2||dilute magnetic semiconductor:2||magnetic field:2||scanning transmission electron microscopy:2||QUANTUM OSCILLATIONS:2||TRANSPORTPROPERTIES:2||surface pair current:2||MAGNETORESISTANCE:2||NANORIBBONS:2||INSTABILITY:2||ANDREEV REFLECTION:2||microwave irradiation:2||vertical graphene josephson junction:2||BI2SE3:2||CONDUCTIVITY:2||highTc superconductors:2||DIMENSIONAL ELECTRONGAS:2||graphene:2||Topological insulators:2||Josephson coupling Fraunhofer interference pattern:2||FERROMAGNET:2||DEPENDENCE:2||DETECTOR:2||COHERENCE:2||INJECTION:2||GRAPHENE:1||JOSEPHSONJUNCTIONS:1||LAYERED SUPERCONDUCTOR:1||mode splitting:1||BEHAVIOR:1||spinpolarized transport:1||SUPERCONDUCTING TRANSITION:1||microwave response:1||PSEUDOGAP:1||phase coherence:1||TRANSITIONS:1||Long Josephson junction:1||Charge detection:1||collective resonance modes:1||plasma oscillation modes:1||Superconducting proximity effect:1||Iron pnictide superconductor:1||McMillanRowell oscillations:1||ferromagnetic microstructure:1||superradiant state:1||VOLTAGE:1||branch splitting:1||TENSOR:1||INTERCALATION:1||insitu fabrication:1||NDGAO3:1||DISORDERED METALS:1||GAUGE GLASS:1||LOWTEMPERATURE TRANSPORT:1||spontaneous spin polarization model:1||BIAS:1||emission of electromagnetic waves:1||YBA2CU3O7/PRBA2CU3O7 SUPERLATTICES:1||BOHM:1||SHAPIRO STEPS:1||superconductor/ferromagnet interface:1||OXIDE:1||ANDREEVREFLECTION:1||SinFeAsO single crystal:1||COLLECTIVE MOTION:1||ANGULARDEPENDENCE:1||SUPERCONDUCTIVITY:1||BILAYER GRAPHENE:1||PHOTOLUMINESCENT PROPERTIES:1||SUPERCONDUCTING WEAK LINKS:1||intrinsic Josephson junctions geometrical resonance:1||intrinsic Josephson junction:1||MESOSCOPIC SPINVALVE:1||Bi2212 single crystals:1||intrinsic junctions:1||ANDREEV REFLECTIONS:1||normalmetal/superconductor interface:1||IBI2SR2CACU2OY:1||THERMAL FLUCTUATIONS:1||MIXED STATE:1||BI2.15SR1.85CACU2O8+DELTA:1||intrinsic Josephson effects:1||CACUO:1||QUANTUM POINT CONTACTS:1||resonant tunneling state:1||coherence length:1||NANOWIRE:1||GATES:1||Phase line:1||Thermal activation:1||QUANTUMDOT:1||superconducting proximity effect:1||Andreev interferometer:1||WIRE:1||Josephsonvortexflow branches:1||Bi2212 cuprates:1||LATTICE:1||demannetization effect:1||SUPERCONDUCTING MIRRORS:1||GAS:1||VALLEY TRANSPORT:1||ELECTRODES:1||DEPENDENT TRANSPORT:1||BORNOPPENHEIMER APPROXIMATION:1||collective plasma oscillations:1||fluxon resonance steps:1||STACKS:1||COLLECTIVE DYNAMICS:1||PAIRING SYMMETRY:1||MUON SPIN ROTATION:1||DIMENSIONAL CROSSOVER:1||Bi2Sr2CaCu2Oy highTc superconductors:1||heterojunctions:1||nanostructures:1||surfaces and interfaces:1||QUANTUM TRANSPORT:1||MICROJUNCTIONS:1||RESONATORS:1||STATES:1||FIELD:1||FLUCTUATIONS:1||SCATTERING:1||mode splitting of Josephson vortexflow branches:1||2D superconductivity:1||TRANSISTOR:1||ENERGYGAP:1||SUPERLATTICES:1||IRONBASED SUPERCONDUCTORS:1||PHASEDEPENDENT RESISTANCE:1||QUANTUM PHASETRANSITIONS:1||ELECTRICFIELD:1||HIGH MAGNETICFIELDS:1||NANOWIRE HETEROSTRUCTURES:1||ZNO:1||pair breaking.:1||SUPERCONDUCTING PB:1||domain formation:1||FORCE MICROSCOPY:1||RELAXATION:1||PLASMA RESONANCE:1||coupled Josephson junctions:1||COPPEROXIDE SUPERCONDUCTORS:1||CROSSOVER:1||SIMULATIONS:1||LOWTEMPERATURE:1||CONDUCTORS:1||METALINSULATORTRANSITION:1||SEMICONDUCTOR:1||FIELDEFFECT TRANSISTORS:1||ZEROVOLTAGE STATE:1||constanttemperature interlayer tunneling spectroscopy:1||Josephson supercurrent:1||BIPOLAR SUPERCURRENT:1||Interaction between Josephson and pancake vortices:1||flux jump:1||coaxial heterojunction nanorod:1||Natural Josephson coupling:1||BI2SR2CACU2O8+DELTA:1||VORTEX FLOW:1||TC SUPERCONDUCTORS:1||charge imbalance:1||Andreev diffractometer:1||intercalation:1||surface junction:1||Bi2212:1||tunnelling:1||GRAPHITE:1||GROWTH:1||collective transverse plasma modes:1||GAN:1||Macroscopic quantum tunneling:1||Fluctuation conductivity:1||Abovegap conductance jump:1||Josephson vortex motion:1||Intrinsic Josephson junctions:1||LAYERED SUPERCONDUCTORS:1||BI2SR2CACU2O8+Y:1||INTERFACES:1||BREAKDOWN:1||SYSTEMS:1||Anisotropy ratio:1||Josephson vortex:1||spin relaxation in superconductors:1||bibased single crystals:1||MESOSCOPIC PROXIMITY SUPERCONDUCTOR:1||reentrance of conductance:1||interlayer pair tunneling:1||JOSEPHSON:1||DISORDERED 2DIMENSIONAL SUPERCONDUCTORS:1||INDIUM FILMS:1||excited state:1||REGIME:1||triplet superconductivity:1||FILM:1||SCHOTTKY DIODES:1||peakdiphump structure:1||Kondo effect:1||REENTRANCE:1||Graphene:1||CONTACT:1||BERRYS PHASE:1||2DIMENSIONAL SUPERCONDUCTORS:1||Coulomb diamond:1||magnetic domain:1||spin injection:1||RESONANCE:1||plasma excitation modes:1||FLOW:1||OVERDOPED BI2SR2CACU2O8+DELTA:1||hole doping:1||chemical synthesis:1||phase transitions:1||superconductors:1||VORTEXGLASS SUPERCONDUCTIVITY:1||Kondorelated model:1||RADIATION:1||DOT:1||NANOBELTS:1||Complementarity:1||Closedloop AharonovBohm interferometer:1||pair breaking:1||interlayer phase fluctuation:1||MgB2 thin film:1||CONFINEMENT:1||WALLED CARBON NANOTUBES:1||TRANSITION:9||VORTICES:8||STATE:7||intrinsic Josephson junctions:7||SINGLECRYSTALS:7||JUNCTIONS:5||MODES:5||SUPERCURRENT:5||SUPERCONDUCTOR:5||CONDUCTANCE:5||HIGHTEMPERATURE SUPERCONDUCTORS:5||TRANSPORT:5||PHASE:5||FILMS:4||LOCALIZATION:4||SINGLE DIRAC CONE:4||WIRES:4||MAGNETICFIELD:4||STEPS:3||ELECTRONS:3||proximity effect:3||MODEL:3||ARRAYS:3||INTERFERENCE:3||fluxon dynamics:3||HETEROSTRUCTURES:3||INSULATOR:3||Andreev reflection:3||electronic transport:3||FISKE:3||superconductor:2||ZnO:2||quantum point contact:2||METAL:2||DYNAMICS:2||interlayer Josephson coupling:2||SUPERCONDUCTORS:2||YBA2CU3O7DELTA:2||LAYER:2||DOTS:2||quantum dot:2||Article:2||TRANSISTORS:2||CARBON NANOTUBES:2||GAP:2||MECHANISM:2||LINE:2||GIANT SHAPIRO STEPS:2||LAYERS:2||electron energy loss spectroscopy:2||physical phenomena:2||scanning electron microscopy:2||HGTE QUANTUMWELLS:2||BI2TE3:2||SPECTROSCOPY:2||PNJUNCTIONS:2||spinpolarized tunneling:2||INTRINSIC JOSEPHSONJUNCTIONS:2||FIELDS:2||positive magnetoresistance:2||dilute magnetic semiconductor:2||magnetic field:2||scanning transmission electron microscopy:2||QUANTUM OSCILLATIONS:2||TRANSPORTPROPERTIES:2||surface pair current:2||MAGNETORESISTANCE:2||NANORIBBONS:2||INSTABILITY:2||ANDREEV REFLECTION:2||microwave irradiation:2||vertical graphene josephson junction:2||BI2SE3:2||CONDUCTIVITY:2||highTc superconductors:2||DIMENSIONAL ELECTRONGAS:2||graphene:2||Topological insulators:2||Josephson coupling Fraunhofer interference pattern:2||FERROMAGNET:2||DEPENDENCE:2||DETECTOR:2||COHERENCE:2||INJECTION:2||GRAPHENE:1||JOSEPHSONJUNCTIONS:1||LAYERED SUPERCONDUCTOR:1||mode splitting:1||BEHAVIOR:1||spinpolarized transport:1||SUPERCONDUCTING TRANSITION:1||microwave response:1||PSEUDOGAP:1||phase coherence:1||TRANSITIONS:1||Long Josephson junction:1||Charge detection:1||collective resonance modes:1||plasma oscillation modes:1||Superconducting proximity effect:1||Iron pnictide superconductor:1||McMillanRowell oscillations:1||ferromagnetic microstructure:1||superradiant state:1||VOLTAGE:1||branch splitting:1||TENSOR:1||INTERCALATION:1||insitu fabrication:1||NDGAO3:1||DISORDERED METALS:1||GAUGE GLASS:1||LOWTEMPERATURE TRANSPORT:1||spontaneous spin polarization model:1||BIAS:1||emission of electromagnetic waves:1||YBA2CU3O7/PRBA2CU3O7 SUPERLATTICES:1||BOHM:1||SHAPIRO STEPS:1||superconductor/ferromagnet interface:1||OXIDE:1||ANDREEVREFLECTION:1||SinFeAsO single crystal:1||COLLECTIVE MOTION:1||ANGULARDEPENDENCE:1||SUPERCONDUCTIVITY:1||BILAYER GRAPHENE:1||PHOTOLUMINESCENT PROPERTIES:1||SUPERCONDUCTING WEAK LINKS:1||intrinsic Josephson junctions geometrical resonance:1||intrinsic Josephson junction:1||MESOSCOPIC SPINVALVE:1||Bi2212 single crystals:1||intrinsic junctions:1||ANDREEV REFLECTIONS:1||normalmetal/superconductor interface:1||IBI2SR2CACU2OY:1||THERMAL FLUCTUATIONS:1||MIXED STATE:1||BI2.15SR1.85CACU2O8+DELTA:1||intrinsic Josephson effects:1||CACUO:1||QUANTUM POINT CONTACTS:1||resonant tunneling state:1||coherence length:1||NANOWIRE:1||GATES:1||Phase line:1||Thermal activation:1||QUANTUMDOT:1||superconducting proximity effect:1||Andreev interferometer:1||WIRE:1||Josephsonvortexflow branches:1||Bi2212 cuprates:1||LATTICE:1||demannetization effect:1||SUPERCONDUCTING MIRRORS:1||GAS:1||VALLEY TRANSPORT:1||ELECTRODES:1||DEPENDENT TRANSPORT:1||BORNOPPENHEIMER APPROXIMATION:1||collective plasma oscillations:1||fluxon resonance steps:1||STACKS:1||COLLECTIVE DYNAMICS:1||PAIRING SYMMETRY:1||MUON SPIN ROTATION:1||DIMENSIONAL CROSSOVER:1||Bi2Sr2CaCu2Oy highTc superconductors:1||heterojunctions:1||nanostructures:1||surfaces and interfaces:1||QUANTUM TRANSPORT:1||MICROJUNCTIONS:1||RESONATORS:1||STATES:1||FIELD:1||FLUCTUATIONS:1||SCATTERING:1||mode splitting of Josephson vortexflow branches:1||2D superconductivity:1||TRANSISTOR:1||ENERGYGAP:1||SUPERLATTICES:1||IRONBASED SUPERCONDUCTORS:1||PHASEDEPENDENT RESISTANCE:1||QUANTUM PHASETRANSITIONS:1||ELECTRICFIELD:1||HIGH MAGNETICFIELDS:1||NANOWIRE HETEROSTRUCTURES:1||ZNO:1||pair breaking.:1||SUPERCONDUCTING PB:1||domain formation:1||FORCE MICROSCOPY:1||RELAXATION:1||PLASMA RESONANCE:1||coupled Josephson junctions:1||COPPEROXIDE SUPERCONDUCTORS:1||CROSSOVER:1||SIMULATIONS:1||LOWTEMPERATURE:1||CONDUCTORS:1||METALINSULATORTRANSITION:1||SEMICONDUCTOR:1||FIELDEFFECT TRANSISTORS:1||ZEROVOLTAGE STATE:1||constanttemperature interlayer tunneling spectroscopy:1||Josephson supercurrent:1||BIPOLAR SUPERCURRENT:1||Interaction between Josephson and pancake vortices:1||flux jump:1||coaxial heterojunction nanorod:1||Natural Josephson coupling:1||BI2SR2CACU2O8+DELTA:1||VORTEX FLOW:1||TC SUPERCONDUCTORS:1||charge imbalance:1||Andreev diffractometer:1||intercalation:1||surface junction:1||Bi2212:1||tunnelling:1||GRAPHITE:1||GROWTH:1||collective transverse plasma modes:1||GAN:1||Macroscopic quantum tunneling:1||Fluctuation conductivity:1||Abovegap conductance jump:1||Josephson vortex motion:1||Intrinsic Josephson junctions:1||LAYERED SUPERCONDUCTORS:1||BI2SR2CACU2O8+Y:1||INTERFACES:1||BREAKDOWN:1||SYSTEMS:1||Anisotropy ratio:1||Josephson vortex:1||spin relaxation in superconductors:1||bibased single crystals:1||MESOSCOPIC PROXIMITY SUPERCONDUCTOR:1||reentrance of conductance:1||interlayer pair tunneling:1||JOSEPHSON:1||DISORDERED 2DIMENSIONAL SUPERCONDUCTORS:1||INDIUM FILMS:1||excited state:1||REGIME:1||triplet superconductivity:1||FILM:1||SCHOTTKY DIODES:1||peakdiphump structure:1||Kondo effect:1||REENTRANCE:1||Graphene:1||CONTACT:1||BERRYS PHASE:1||2DIMENSIONAL SUPERCONDUCTORS:1||Coulomb diamond:1||magnetic domain:1||spin injection:1||RESONANCE:1||plasma excitation modes:1||FLOW:1||OVERDOPED BI2SR2CACU2O8+DELTA:1||hole doping:1||chemical synthesis:1||phase transitions:1||superconductors:1||VORTEXGLASS SUPERCONDUCTIVITY:1||Kondorelated model:1||RADIATION:1||DOT:1||NANOBELTS:1||Complementarity:1||Closedloop AharonovBohm interferometer:1||pair breaking:1||interlayer phase fluctuation:1||MgB2 thin film:1||CONFINEMENT:1||WALLED CARBON NANOTUBES:1||TRANSITION:9||VORTICES:8||STATE:7||intrinsic Josephson junctions:7||SINGLECRYSTALS:7||JUNCTIONS:5||MODES:5||SUPERCURRENT:5||SUPERCONDUCTOR:5||CONDUCTANCE:5||HIGHTEMPERATURE SUPERCONDUCTORS:5||TRANSPORT:5||PHASE:5||FILMS:4||LOCALIZATION:4||SINGLE DIRAC CONE:4||WIRES:4||MAGNETICFIELD:4||STEPS:3||ELECTRONS:3||proximity effect:3||MODEL:3||ARRAYS:3||INTERFERENCE:3||fluxon dynamics:3||HETEROSTRUCTURES:3||INSULATOR:3||Andreev reflection:3||electronic transport:3||FISKE:3||superconductor:2||ZnO:2||quantum point contact:2||METAL:2||DYNAMICS:2||interlayer Josephson coupling:2||SUPERCONDUCTORS:2||YBA2CU3O7DELTA:2||LAYER:2||DOTS:2||quantum dot:2||Article:2||TRANSISTORS:2||CARBON NANOTUBES:2||GAP:2||MECHANISM:2||LINE:2||GIANT SHAPIRO STEPS:2||LAYERS:2||electron energy loss spectroscopy:2||physical phenomena:2||scanning electron microscopy:2||HGTE QUANTUMWELLS:2||BI2TE3:2||SPECTROSCOPY:2||PNJUNCTIONS:2||spinpolarized tunneling:2||INTRINSIC JOSEPHSONJUNCTIONS:2||FIELDS:2||positive magnetoresistance:2||dilute magnetic semiconductor:2||magnetic field:2||scanning transmission electron microscopy:2||QUANTUM OSCILLATIONS:2||TRANSPORTPROPERTIES:2||surface pair current:2||MAGNETORESISTANCE:2||NANORIBBONS:2||INSTABILITY:2||ANDREEV REFLECTION:2||microwave irradiation:2||vertical graphene josephson junction:2||BI2SE3:2||CONDUCTIVITY:2||highTc superconductors:2||DIMENSIONAL ELECTRONGAS:2||graphene:2||Topological insulators:2||Josephson coupling Fraunhofer interference pattern:2||FERROMAGNET:2||DEPENDENCE:2||DETECTOR:2||COHERENCE:2||INJECTION:2||GRAPHENE:1||JOSEPHSONJUNCTIONS:1||LAYERED SUPERCONDUCTOR:1||mode splitting:1||BEHAVIOR:1||spinpolarized transport:1||SUPERCONDUCTING TRANSITION:1||microwave response:1||PSEUDOGAP:1||phase coherence:1||TRANSITIONS:1||Long Josephson junction:1||Charge detection:1||collective resonance modes:1||plasma oscillation modes:1||Superconducting proximity effect:1||Iron pnictide superconductor:1||McMillanRowell oscillations:1||ferromagnetic microstructure:1||superradiant state:1||VOLTAGE:1||branch splitting:1||TENSOR:1||INTERCALATION:1||insitu fabrication:1||NDGAO3:1||DISORDERED METALS:1||GAUGE GLASS:1||LOWTEMPERATURE TRANSPORT:1||spontaneous spin polarization model:1||BIAS:1||emission of electromagnetic waves:1||YBA2CU3O7/PRBA2CU3O7 SUPERLATTICES:1||BOHM:1||SHAPIRO STEPS:1||superconductor/ferromagnet interface:1||OXIDE:1||ANDREEVREFLECTION:1||SinFeAsO single crystal:1||COLLECTIVE MOTION:1||ANGULARDEPENDENCE:1||SUPERCONDUCTIVITY:1||BILAYER GRAPHENE:1||PHOTOLUMINESCENT PROPERTIES:1||SUPERCONDUCTING WEAK LINKS:1||intrinsic Josephson junctions geometrical resonance:1||intrinsic Josephson junction:1||MESOSCOPIC SPINVALVE:1||Bi2212 single crystals:1||intrinsic junctions:1||ANDREEV REFLECTIONS:1||normalmetal/superconductor interface:1||IBI2SR2CACU2OY:1||THERMAL FLUCTUATIONS:1||MIXED STATE:1||BI2.15SR1.85CACU2O8+DELTA:1||intrinsic Josephson effects:1||CACUO:1||QUANTUM POINT CONTACTS:1||resonant tunneling state:1||coherence length:1||NANOWIRE:1||GATES:1||Phase line:1||Thermal activation:1||QUANTUMDOT:1||superconducting proximity effect:1||Andreev interferometer:1||WIRE:1||Josephsonvortexflow branches:1||Bi2212 cuprates:1||LATTICE:1||demannetization effect:1||SUPERCONDUCTING MIRRORS:1||GAS:1||VALLEY TRANSPORT:1||ELECTRODES:1||DEPENDENT TRANSPORT:1||BORNOPPENHEIMER APPROXIMATION:1||collective plasma oscillations:1||fluxon resonance steps:1||STACKS:1||COLLECTIVE DYNAMICS:1||PAIRING SYMMETRY:1||MUON SPIN ROTATION:1||DIMENSIONAL CROSSOVER:1||Bi2Sr2CaCu2Oy highTc superconductors:1||heterojunctions:1||nanostructures:1||surfaces and interfaces:1||QUANTUM TRANSPORT:1||MICROJUNCTIONS:1||RESONATORS:1||STATES:1||FIELD:1||FLUCTUATIONS:1||SCATTERING:1||mode splitting of Josephson vortexflow branches:1||2D superconductivity:1||TRANSISTOR:1||ENERGYGAP:1||SUPERLATTICES:1||IRONBASED SUPERCONDUCTORS:1||PHASEDEPENDENT RESISTANCE:1||QUANTUM PHASETRANSITIONS:1||ELECTRICFIELD:1||HIGH MAGNETICFIELDS:1||NANOWIRE HETEROSTRUCTURES:1||ZNO:1||pair breaking.:1||SUPERCONDUCTING PB:1||domain formation:1||FORCE MICROSCOPY:1||RELAXATION:1||PLASMA RESONANCE:1||coupled Josephson junctions:1||COPPEROXIDE SUPERCONDUCTORS:1||CROSSOVER:1||SIMULATIONS:1||LOWTEMPERATURE:1||CONDUCTORS:1||METALINSULATORTRANSITION:1||SEMICONDUCTOR:1||FIELDEFFECT TRANSISTORS:1||ZEROVOLTAGE STATE:1||constanttemperature interlayer tunneling spectroscopy:1||Josephson supercurrent:1||BIPOLAR SUPERCURRENT:1||Interaction between Josephson and pancake vortices:1||flux jump:1||coaxial heterojunction nanorod:1||Natural Josephson coupling:1||BI2SR2CACU2O8+DELTA:1||VORTEX FLOW:1||TC SUPERCONDUCTORS:1||charge imbalance:1||Andreev diffractometer:1||intercalation:1||surface junction:1||Bi2212:1||tunnelling:1||GRAPHITE:1||GROWTH:1||collective transverse plasma modes:1||GAN:1||Macroscopic quantum tunneling:1||Fluctuation conductivity:1||Abovegap conductance jump:1||Josephson vortex motion:1||Intrinsic Josephson junctions:1||LAYERED SUPERCONDUCTORS:1||BI2SR2CACU2O8+Y:1||INTERFACES:1||BREAKDOWN:1||SYSTEMS:1||Anisotropy ratio:1||Josephson vortex:1||spin relaxation in superconductors:1||bibased single crystals:1||MESOSCOPIC PROXIMITY SUPERCONDUCTOR:1||reentrance of conductance:1||interlayer pair tunneling:1||JOSEPHSON:1||DISORDERED 2DIMENSIONAL SUPERCONDUCTORS:1||INDIUM FILMS:1||excited state:1||REGIME:1||triplet superconductivity:1||FILM:1||SCHOTTKY DIODES:1||peakdiphump structure:1||Kondo effect:1||REENTRANCE:1||Graphene:1||CONTACT:1||BERRYS PHASE:1||2DIMENSIONAL SUPERCONDUCTORS:1||Coulomb diamond:1||magnetic domain:1||spin injection:1||RESONANCE:1||plasma excitation modes:1||FLOW:1||OVERDOPED BI2SR2CACU2O8+DELTA:1||hole doping:1||chemical synthesis:1||phase transitions:1||superconductors:1||VORTEXGLASS SUPERCONDUCTIVITY:1||Kondorelated model:1||RADIATION:1||DOT:1||NANOBELTS:1||Complementarity:1||Closedloop AharonovBohm interferometer:1||pair breaking:1||interlayer phase fluctuation:1||MgB2 thin film:1||CONFINEMENT:1||WALLED CARBON NANOTUBES:1||TRANSITION:9||VORTICES:8||STATE:7||intrinsic Josephson junctions:7||SINGLECRYSTALS:7||JUNCTIONS:5||MODES:5||SUPERCURRENT:5||SUPERCONDUCTOR:5||CONDUCTANCE:5||HIGHTEMPERATURE SUPERCONDUCTORS:5||TRANSPORT:5||PHASE:5||FILMS:4||LOCALIZATION:4||SINGLE DIRAC CONE:4||WIRES:4||MAGNETICFIELD:4||STEPS:3||ELECTRONS:3||proximity effect:3||MODEL:3||ARRAYS:3||INTERFERENCE:3||fluxon dynamics:3||HETEROSTRUCTURES:3||INSULATOR:3||Andreev reflection:3||electronic transport:3||FISKE:3||superconductor:2||ZnO:2||quantum point contact:2||METAL:2||DYNAMICS:2||interlayer Josephson coupling:2||SUPERCONDUCTORS:2||YBA2CU3O7DELTA:2||LAYER:2||DOTS:2||quantum dot:2||Article:2||TRANSISTORS:2||CARBON NANOTUBES:2||GAP:2||MECHANISM:2||LINE:2||GIANT SHAPIRO STEPS:2||LAYERS:2||electron energy loss spectroscopy:2||physical phenomena:2||scanning electron microscopy:2||HGTE QUANTUMWELLS:2||BI2TE3:2||SPECTROSCOPY:2||PNJUNCTIONS:2||spinpolarized tunneling:2||INTRINSIC JOSEPHSONJUNCTIONS:2||FIELDS:2||positive magnetoresistance:2||dilute magnetic semiconductor:2||magnetic field:2||scanning transmission electron microscopy:2||QUANTUM OSCILLATIONS:2||TRANSPORTPROPERTIES:2||surface pair current:2||MAGNETORESISTANCE:2||NANORIBBONS:2||INSTABILITY:2||ANDREEV REFLECTION:2||microwave irradiation:2||vertical graphene josephson junction:2||BI2SE3:2||CONDUCTIVITY:2||highTc superconductors:2||DIMENSIONAL ELECTRONGAS:2||graphene:2||Topological insulators:2||Josephson coupling Fraunhofer interference pattern:2||FERROMAGNET:2||DEPENDENCE:2||DETECTOR:2||COHERENCE:2||INJECTION:2||GRAPHENE:1||JOSEPHSONJUNCTIONS:1||LAYERED SUPERCONDUCTOR:1||mode splitting:1||BEHAVIOR:1||spinpolarized transport:1||SUPERCONDUCTING TRANSITION:1||microwave response:1||PSEUDOGAP:1||phase coherence:1||TRANSITIONS:1||Long Josephson junction:1||Charge detection:1||collective resonance modes:1||plasma oscillation modes:1||Superconducting proximity effect:1||Iron pnictide superconductor:1||McMillanRowell oscillations:1||ferromagnetic microstructure:1||superradiant state:1||VOLTAGE:1||branch splitting:1||TENSOR:1||INTERCALATION:1||insitu fabrication:1||NDGAO3:1||DISORDERED METALS:1||GAUGE GLASS:1||LOWTEMPERATURE TRANSPORT:1||spontaneous spin polarization model:1||BIAS:1||emission of electromagnetic waves:1||YBA2CU3O7/PRBA2CU3O7 SUPERLATTICES:1||BOHM:1||SHAPIRO STEPS:1||superconductor/ferromagnet interface:1||OXIDE:1||ANDREEVREFLECTION:1||SinFeAsO single crystal:1||COLLECTIVE MOTION:1||ANGULARDEPENDENCE:1||SUPERCONDUCTIVITY:1||BILAYER GRAPHENE:1||PHOTOLUMINESCENT PROPERTIES:1||SUPERCONDUCTING WEAK LINKS:1||intrinsic Josephson junctions geometrical resonance:1||intrinsic Josephson junction:1||MESOSCOPIC SPINVALVE:1||Bi2212 single crystals:1||intrinsic junctions:1||ANDREEV REFLECTIONS:1||normalmetal/superconductor interface:1||IBI2SR2CACU2OY:1||THERMAL FLUCTUATIONS:1||MIXED STATE:1||BI2.15SR1.85CACU2O8+DELTA:1||intrinsic Josephson effects:1||CACUO:1||QUANTUM POINT CONTACTS:1||resonant tunneling state:1||coherence length:1||NANOWIRE:1||GATES:1||Phase line:1||Thermal activation:1||QUANTUMDOT:1||superconducting proximity effect:1||Andreev interferometer:1||WIRE:1||Josephsonvortexflow branches:1||Bi2212 cuprates:1||LATTICE:1||demannetization effect:1||SUPERCONDUCTING MIRRORS:1||GAS:1||VALLEY TRANSPORT:1||ELECTRODES:1||DEPENDENT TRANSPORT:1||BORNOPPENHEIMER APPROXIMATION:1||collective plasma oscillations:1||fluxon resonance steps:1||STACKS:1||COLLECTIVE DYNAMICS:1||PAIRING SYMMETRY:1||MUON SPIN ROTATION:1||DIMENSIONAL CROSSOVER:1||Bi2Sr2CaCu2Oy highTc superconductors:1||heterojunctions:1||nanostructures:1||surfaces and interfaces:1||QUANTUM TRANSPORT:1||MICROJUNCTIONS:1||RESONATORS:1||STATES:1||FIELD:1||FLUCTUATIONS:1||SCATTERING:1||mode splitting of Josephson vortexflow branches:1||2D superconductivity:1||TRANSISTOR:1||ENERGYGAP:1||SUPERLATTICES:1||IRONBASED SUPERCONDUCTORS:1||PHASEDEPENDENT RESISTANCE:1||QUANTUM PHASETRANSITIONS:1||ELECTRICFIELD:1||HIGH MAGNETICFIELDS:1||NANOWIRE HETEROSTRUCTURES:1||ZNO:1||pair breaking.:1||SUPERCONDUCTING PB:1||domain formation:1||FORCE MICROSCOPY:1||RELAXATION:1||PLASMA RESONANCE:1||coupled Josephson junctions:1||COPPEROXIDE SUPERCONDUCTORS:1||CROSSOVER:1||SIMULATIONS:1||LOWTEMPERATURE:1||CONDUCTORS:1||METALINSULATORTRANSITION:1||SEMICONDUCTOR:1||FIELDEFFECT TRANSISTORS:1||ZEROVOLTAGE STATE:1||constanttemperature interlayer tunneling spectroscopy:1||Josephson supercurrent:1||BIPOLAR SUPERCURRENT:1||Interaction between Josephson and pancake vortices:1||flux jump:1||coaxial heterojunction nanorod:1||Natural Josephson coupling:1||BI2SR2CACU2O8+DELTA:1||VORTEX FLOW:1||TC SUPERCONDUCTORS:1||charge imbalance:1||Andreev diffractometer:1||intercalation:1||surface junction:1||Bi2212:1||tunnelling:1||GRAPHITE:1||GROWTH:1||collective transverse plasma modes:1||GAN:1||Macroscopic quantum tunneling:1||Fluctuation conductivity:1||Abovegap conductance jump:1||Josephson vortex motion:1||Intrinsic Josephson junctions:1||LAYERED SUPERCONDUCTORS:1||BI2SR2CACU2O8+Y:1||INTERFACES:1||BREAKDOWN:1||SYSTEMS:1||Anisotropy ratio:1||Josephson vortex:1||spin relaxation in superconductors:1||bibased single crystals:1||MESOSCOPIC PROXIMITY SUPERCONDUCTOR:1||reentrance of conductance:1||interlayer pair tunneling:1||JOSEPHSON:1||DISORDERED 2DIMENSIONAL SUPERCONDUCTORS:1||INDIUM FILMS:1||excited state:1||REGIME:1||triplet superconductivity:1||FILM:1||SCHOTTKY DIODES:1||peakdiphump structure:1||Kondo effect:1||REENTRANCE:1||Graphene:1||CONTACT:1||BERRYS PHASE:1||2DIMENSIONAL SUPERCONDUCTORS:1||Coulomb diamond:1||magnetic domain:1||spin injection:1||RESONANCE:1||plasma excitation modes:1||FLOW:1||OVERDOPED BI2SR2CACU2O8+DELTA:1||hole doping:1||chemical synthesis:1||phase transitions:1||superconductors:1||VORTEXGLASS SUPERCONDUCTIVITY:1||Kondorelated model:1||RADIATION:1||DOT:1||NANOBELTS:1||Complementarity:1||Closedloop AharonovBohm interferometer:1||pair breaking:1||interlayer phase fluctuation:1||MgB2 thin film:1||CONFINEMENT:1||WALLED CARBON NANOTUBES:1||TRANSITION:9||VORTICES:8||STATE:7||intrinsic Josephson junctions:7||SINGLECRYSTALS:7||JUNCTIONS:5||MODES:5||SUPERCURRENT:5||SUPERCONDUCTOR:5||CONDUCTANCE:5||HIGHTEMPERATURE SUPERCONDUCTORS:5||TRANSPORT:5||PHASE:5||FILMS:4||LOCALIZATION:4||SINGLE DIRAC CONE:4||WIRES:4||MAGNETICFIELD:4||STEPS:3||ELECTRONS:3||proximity effect:3||MODEL:3||ARRAYS:3||INTERFERENCE:3||fluxon dynamics:3||HETEROSTRUCTURES:3||INSULATOR:3||Andreev reflection:3||electronic transport:3||FISKE:3||superconductor:2||ZnO:2||quantum point contact:2||METAL:2||DYNAMICS:2||interlayer Josephson coupling:2||SUPERCONDUCTORS:2||YBA2CU3O7DELTA:2||LAYER:2||DOTS:2||quantum dot:2||Article:2||TRANSISTORS:2||CARBON NANOTUBES:2||GAP:2||MECHANISM:2||LINE:2||GIANT SHAPIRO STEPS:2||LAYERS:2||electron energy loss spectroscopy:2||physical phenomena:2||scanning electron microscopy:2||HGTE QUANTUMWELLS:2||BI2TE3:2||SPECTROSCOPY:2||PNJUNCTIONS:2||spinpolarized tunneling:2||INTRINSIC JOSEPHSONJUNCTIONS:2||FIELDS:2||positive magnetoresistance:2||dilute magnetic semiconductor:2||magnetic field:2||scanning transmission electron microscopy:2||QUANTUM OSCILLATIONS:2||TRANSPORTPROPERTIES:2||surface pair current:2||MAGNETORESISTANCE:2||NANORIBBONS:2||INSTABILITY:2||ANDREEV REFLECTION:2||microwave irradiation:2||vertical graphene josephson junction:2||BI2SE3:2||CONDUCTIVITY:2||highTc superconductors:2||DIMENSIONAL ELECTRONGAS:2||graphene:2||Topological insulators:2||Josephson coupling Fraunhofer interference pattern:2||FERROMAGNET:2||DEPENDENCE:2||DETECTOR:2||COHERENCE:2||INJECTION:2||GRAPHENE:1||JOSEPHSONJUNCTIONS:1||LAYERED SUPERCONDUCTOR:1||mode splitting:1||BEHAVIOR:1||spinpolarized transport:1||SUPERCONDUCTING TRANSITION:1||microwave response:1||PSEUDOGAP:1||phase coherence:1||TRANSITIONS:1||Long Josephson junction:1||Charge detection:1||collective resonance modes:1||plasma oscillation modes:1||Superconducting proximity effect:1||Iron pnictide superconductor:1||McMillanRowell oscillations:1||ferromagnetic microstructure:1||superradiant state:1||VOLTAGE:1||branch splitting:1||TENSOR:1||INTERCALATION:1||insitu fabrication:1||NDGAO3:1||DISORDERED METALS:1||GAUGE GLASS:1||LOWTEMPERATURE TRANSPORT:1||spontaneous spin polarization model:1||BIAS:1||emission of electromagnetic waves:1||YBA2CU3O7/PRBA2CU3O7 SUPERLATTICES:1||BOHM:1||SHAPIRO STEPS:1||superconductor/ferromagnet interface:1||OXIDE:1||ANDREEVREFLECTION:1||SinFeAsO single crystal:1||COLLECTIVE MOTION:1||ANGULARDEPENDENCE:1||SUPERCONDUCTIVITY:1||BILAYER GRAPHENE:1||PHOTOLUMINESCENT PROPERTIES:1||SUPERCONDUCTING WEAK LINKS:1||intrinsic Josephson junctions geometrical resonance:1||intrinsic Josephson junction:1||MESOSCOPIC SPINVALVE:1||Bi2212 single crystals:1||intrinsic junctions:1||ANDREEV REFLECTIONS:1||normalmetal/superconductor interface:1||IBI2SR2CACU2OY:1||THERMAL FLUCTUATIONS:1||MIXED STATE:1||BI2.15SR1.85CACU2O8+DELTA:1||intrinsic Josephson effects:1||CACUO:1||QUANTUM POINT CONTACTS:1||resonant tunneling state:1||coherence length:1||NANOWIRE:1||GATES:1||Phase line:1||Thermal activation:1||QUANTUMDOT:1||superconducting proximity effect:1||Andreev interferometer:1||WIRE:1||Josephsonvortexflow branches:1||Bi2212 cuprates:1||LATTICE:1||demannetization effect:1||SUPERCONDUCTING MIRRORS:1||GAS:1||VALLEY TRANSPORT:1||ELECTRODES:1||DEPENDENT TRANSPORT:1||BORNOPPENHEIMER APPROXIMATION:1||collective plasma oscillations:1||fluxon resonance steps:1||STACKS:1||COLLECTIVE DYNAMICS:1||PAIRING SYMMETRY:1||MUON SPIN ROTATION:1||DIMENSIONAL CROSSOVER:1||Bi2Sr2CaCu2Oy highTc superconductors:1||heterojunctions:1||nanostructures:1||surfaces and interfaces:1||QUANTUM TRANSPORT:1||MICROJUNCTIONS:1||RESONATORS:1||STATES:1||FIELD:1||FLUCTUATIONS:1||SCATTERING:1||mode splitting of Josephson vortexflow branches:1||2D superconductivity:1||TRANSISTOR:1||ENERGYGAP:1||SUPERLATTICES:1||IRONBASED SUPERCONDUCTORS:1||PHASEDEPENDENT RESISTANCE:1||QUANTUM PHASETRANSITIONS:1||ELECTRICFIELD:1||HIGH MAGNETICFIELDS:1||NANOWIRE HETEROSTRUCTURES:1||ZNO:1||pair breaking.:1||SUPERCONDUCTING PB:1||domain formation:1||FORCE MICROSCOPY:1||RELAXATION:1||PLASMA RESONANCE:1||coupled Josephson junctions:1||COPPEROXIDE SUPERCONDUCTORS:1||CROSSOVER:1||SIMULATIONS:1||LOWTEMPERATURE:1||CONDUCTORS:1||METALINSULATORTRANSITION:1||SEMICONDUCTOR:1||FIELDEFFECT TRANSISTORS:1||ZEROVOLTAGE STATE:1||constanttemperature interlayer tunneling spectroscopy:1||Josephson supercurrent:1||BIPOLAR SUPERCURRENT:1||Interaction between Josephson and pancake vortices:1||flux jump:1||coaxial heterojunction nanorod:1||Natural Josephson coupling:1||BI2SR2CACU2O8+DELTA:1||VORTEX FLOW:1||TC SUPERCONDUCTORS:1||charge imbalance:1||Andreev diffractometer:1||intercalation:1||surface junction:1||Bi2212:1||tunnelling:1||GRAPHITE:1||GROWTH:1||collective transverse plasma modes:1||GAN:1||Macroscopic quantum tunneling:1||Fluctuation conductivity:1||Abovegap conductance jump:1||Josephson vortex motion:1||Intrinsic Josephson junctions:1||LAYERED SUPERCONDUCTORS:1||BI2SR2CACU2O8+Y:1||INTERFACES:1||BREAKDOWN:1||SYSTEMS:1||Anisotropy ratio:1||Josephson vortex:1||spin relaxation in superconductors:1||bibased single crystals:1||MESOSCOPIC PROXIMITY SUPERCONDUCTOR:1||reentrance of conductance:1||interlayer pair tunneling:1||JOSEPHSON:1||DISORDERED 2DIMENSIONAL SUPERCONDUCTORS:1||INDIUM FILMS:1||excited state:1||REGIME:1||triplet superconductivity:1||FILM:1||SCHOTTKY DIODES:1||peakdiphump structure:1||Kondo effect:1||REENTRANCE:1||Graphene:1||CONTACT:1||BERRYS PHASE:1||2DIMENSIONAL SUPERCONDUCTORS:1||Coulomb diamond:1||magnetic domain:1||spin injection:1||RESONANCE:1||plasma excitation modes:1||FLOW:1||OVERDOPED BI2SR2CACU2O8+DELTA:1||hole doping:1||chemical synthesis:1||phase transitions:1||superconductors:1||VORTEXGLASS SUPERCONDUCTIVITY:1||Kondorelated model:1||RADIATION:1||DOT:1||NANOBELTS:1||Complementarity:1||Closedloop AharonovBohm interferometer:1||pair breaking:1||interlayer phase fluctuation:1||MgB2 thin film:1||CONFINEMENT:1||WALLED CARBON NANOTUBES:1||TRANSITION:9||VORTICES:8||STATE:7||intrinsic Josephson junctions:7||SINGLECRYSTALS:7||JUNCTIONS:5||MODES:5||SUPERCURRENT:5||SUPERCONDUCTOR:5||CONDUCTANCE:5||HIGHTEMPERATURE SUPERCONDUCTORS:5||TRANSPORT:5||PHASE:5||FILMS:4||LOCALIZATION:4||SINGLE DIRAC CONE:4||WIRES:4||MAGNETICFIELD:4||STEPS:3||ELECTRONS:3||proximity effect:3||MODEL:3||ARRAYS:3||INTERFERENCE:3||fluxon dynamics:3||HETEROSTRUCTURES:3||INSULATOR:3||Andreev reflection:3||electronic transport:3||FISKE:3||superconductor:2||ZnO:2||quantum point contact:2||METAL:2||DYNAMICS:2||interlayer Josephson coupling:2||SUPERCONDUCTORS:2||YBA2CU3O7DELTA:2||LAYER:2||DOTS:2||quantum dot:2||Article:2||TRANSISTORS:2||CARBON NANOTUBES:2||GAP:2||MECHANISM:2||LINE:2||GIANT SHAPIRO STEPS:2||LAYERS:2||electron energy loss spectroscopy:2||physical phenomena:2||scanning electron microscopy:2||HGTE QUANTUMWELLS:2||BI2TE3:2||SPECTROSCOPY:2||PNJUNCTIONS:2||spinpolarized tunneling:2||INTRINSIC JOSEPHSONJUNCTIONS:2||FIELDS:2||positive magnetoresistance:2||dilute magnetic semiconductor:2||magnetic field:2||scanning transmission electron microscopy:2||QUANTUM OSCILLATIONS:2||TRANSPORTPROPERTIES:2||surface pair current:2||MAGNETORESISTANCE:2||NANORIBBONS:2||INSTABILITY:2||ANDREEV REFLECTION:2||microwave irradiation:2||vertical graphene josephson junction:2||BI2SE3:2||CONDUCTIVITY:2||highTc superconductors:2||DIMENSIONAL ELECTRONGAS:2||graphene:2||Topological insulators:2||Josephson coupling Fraunhofer interference pattern:2||FERROMAGNET:2||DEPENDENCE:2||DETECTOR:2||COHERENCE:2||INJECTION:2||GRAPHENE:1||JOSEPHSONJUNCTIONS:1||LAYERED SUPERCONDUCTOR:1||mode splitting:1||BEHAVIOR:1||spinpolarized transport:1||SUPERCONDUCTING TRANSITION:1||microwave response:1||PSEUDOGAP:1||phase coherence:1||TRANSITIONS:1||Long Josephson junction:1||Charge detection:1||collective resonance modes:1||plasma oscillation modes:1||Superconducting proximity effect:1||Iron pnictide superconductor:1||McMillanRowell oscillations:1||ferromagnetic microstructure:1||superradiant state:1||VOLTAGE:1||branch splitting:1||TENSOR:1||INTERCALATION:1||insitu fabrication:1||NDGAO3:1||DISORDERED METALS:1||GAUGE GLASS:1||LOWTEMPERATURE TRANSPORT:1||spontaneous spin polarization model:1||BIAS:1||emission of electromagnetic waves:1||YBA2CU3O7/PRBA2CU3O7 SUPERLATTICES:1||BOHM:1||SHAPIRO STEPS:1||superconductor/ferromagnet interface:1||OXIDE:1||ANDREEVREFLECTION:1||SinFeAsO single crystal:1||COLLECTIVE MOTION:1||ANGULARDEPENDENCE:1||SUPERCONDUCTIVITY:1||BILAYER GRAPHENE:1||PHOTOLUMINESCENT PROPERTIES:1||SUPERCONDUCTING WEAK LINKS:1||intrinsic Josephson junctions geometrical resonance:1||intrinsic Josephson junction:1||MESOSCOPIC SPINVALVE:1||Bi2212 single crystals:1||intrinsic junctions:1||ANDREEV REFLECTIONS:1||normalmetal/superconductor interface:1||IBI2SR2CACU2OY:1||THERMAL FLUCTUATIONS:1||MIXED STATE:1||BI2.15SR1.85CACU2O8+DELTA:1||intrinsic Josephson effects:1||CACUO:1||QUANTUM POINT CONTACTS:1||resonant tunneling state:1||coherence length:1||NANOWIRE:1||GATES:1||Phase line:1||Thermal activation:1||QUANTUMDOT:1||superconducting proximity effect:1||Andreev interferometer:1||WIRE:1||Josephsonvortexflow branches:1||Bi2212 cuprates:1||LATTICE:1||demannetization effect:1||SUPERCONDUCTING MIRRORS:1||GAS:1||VALLEY TRANSPORT:1||ELECTRODES:1||DEPENDENT TRANSPORT:1||BORNOPPENHEIMER APPROXIMATION:1||collective plasma oscillations:1||fluxon resonance steps:1||STACKS:1||COLLECTIVE DYNAMICS:1||PAIRING SYMMETRY:1||MUON SPIN ROTATION:1||DIMENSIONAL CROSSOVER:1||Bi2Sr2CaCu2Oy highTc superconductors:1||heterojunctions:1||nanostructures:1||surfaces and interfaces:1||QUANTUM TRANSPORT:1||MICROJUNCTIONS:1||RESONATORS:1||STATES:1||FIELD:1||FLUCTUATIONS:1||SCATTERING:1||mode splitting of Josephson vortexflow branches:1||2D superconductivity:1||TRANSISTOR:1||ENERGYGAP:1||SUPERLATTICES:1||IRONBASED SUPERCONDUCTORS:1||PHASEDEPENDENT RESISTANCE:1||QUANTUM PHASETRANSITIONS:1||ELECTRICFIELD:1||HIGH MAGNETICFIELDS:1||NANOWIRE HETEROSTRUCTURES:1||ZNO:1||pair breaking.:1||SUPERCONDUCTING PB:1||domain formation:1||FORCE MICROSCOPY:1||RELAXATION:1||PLASMA RESONANCE:1||coupled Josephson junctions:1||COPPEROXIDE SUPERCONDUCTORS:1||CROSSOVER:1||SIMULATIONS:1||LOWTEMPERATURE:1||CONDUCTORS:1||METALINSULATORTRANSITION:1||SEMICONDUCTOR:1||FIELDEFFECT TRANSISTORS:1||ZEROVOLTAGE STATE:1||constanttemperature interlayer tunneling spectroscopy:1||Josephson supercurrent:1||BIPOLAR SUPERCURRENT:1||Interaction between Josephson and pancake vortices:1||flux jump:1||coaxial heterojunction nanorod:1||Natural Josephson coupling:1||BI2SR2CACU2O8+DELTA:1||VORTEX FLOW:1||TC SUPERCONDUCTORS:1||charge imbalance:1||Andreev diffractometer:1||intercalation:1||surface junction:1||Bi2212:1||tunnelling:1||GRAPHITE:1||GROWTH:1||collective transverse plasma modes:1||GAN:1||Macroscopic quantum tunneling:1||Fluctuation conductivity:1||Abovegap conductance jump:1||Josephson vortex motion:1||Intrinsic Josephson junctions:1||LAYERED SUPERCONDUCTORS:1||BI2SR2CACU2O8+Y:1||INTERFACES:1||BREAKDOWN:1||SYSTEMS:1||Anisotropy ratio:1||Josephson vortex:1||spin relaxation in superconductors:1||bibased single crystals:1||MESOSCOPIC PROXIMITY SUPERCONDUCTOR:1||reentrance of conductance:1||interlayer pair tunneling:1||JOSEPHSON:1||DISORDERED 2DIMENSIONAL SUPERCONDUCTORS:1||INDIUM FILMS:1||excited state:1||REGIME:1||triplet superconductivity:1||FILM:1||SCHOTTKY DIODES:1||peakdiphump structure:1||Kondo effect:1||REENTRANCE:1||Graphene:1||CONTACT:1||BERRYS PHASE:1||2DIMENSIONAL SUPERCONDUCTORS:1||Coulomb diamond:1||magnetic domain:1||spin injection:1||RESONANCE:1||plasma excitation modes:1||FLOW:1||OVERDOPED BI2SR2CACU2O8+DELTA:1||hole doping:1||chemical synthesis:1||phase transitions:1||superconductors:1||VORTEXGLASS SUPERCONDUCTIVITY:1||Kondorelated model:1||RADIATION:1||DOT:1||NANOBELTS:1||Complementarity:1||Closedloop AharonovBohm interferometer:1||pair breaking:1||interlayer phase fluctuation:1||MgB2 thin film:1||CONFINEMENT:1||WALLED CARBON NANOTUBES:1||TRANSITION:9||VORTICES:8||STATE:7||intrinsic Josephson junctions:7||SINGLECRYSTALS:7||JUNCTIONS:5||MODES:5||SUPERCURRENT:5||SUPERCONDUCTOR:5||CONDUCTANCE:5||HIGHTEMPERATURE SUPERCONDUCTORS:5||TRANSPORT:5||PHASE:5||FILMS:4||LOCALIZATION:4||SINGLE DIRAC CONE:4||WIRES:4||MAGNETICFIELD:4||STEPS:3||ELECTRONS:3||proximity effect:3||MODEL:3||ARRAYS:3||INTERFERENCE:3||fluxon dynamics:3||HETEROSTRUCTURES:3||INSULATOR:3||Andreev reflection:3||electronic transport:3||FISKE:3||superconductor:2||ZnO:2||quantum point contact:2||METAL:2||DYNAMICS:2||interlayer Josephson coupling:2||SUPERCONDUCTORS:2||YBA2CU3O7DELTA:2||LAYER:2||DOTS:2||quantum dot:2||Article:2||TRANSISTORS:2||CARBON NANOTUBES:2||GAP:2||MECHANISM:2||LINE:2||GIANT SHAPIRO STEPS:2||LAYERS:2||electron energy loss spectroscopy:2||physical phenomena:2||scanning electron microscopy:2||HGTE QUANTUMWELLS:2||BI2TE3:2||SPECTROSCOPY:2||PNJUNCTIONS:2||spinpolarized tunneling:2||INTRINSIC JOSEPHSONJUNCTIONS:2||FIELDS:2||positive magnetoresistance:2||dilute magnetic semiconductor:2||magnetic field:2||scanning transmission electron microscopy:2||QUANTUM OSCILLATIONS:2||TRANSPORTPROPERTIES:2||surface pair current:2||MAGNETORESISTANCE:2||NANORIBBONS:2||INSTABILITY:2||ANDREEV REFLECTION:2||microwave irradiation:2||vertical graphene josephson junction:2||BI2SE3:2||CONDUCTIVITY:2||highTc superconductors:2||DIMENSIONAL ELECTRONGAS:2||graphene:2||Topological insulators:2||Josephson coupling Fraunhofer interference pattern:2||FERROMAGNET:2||DEPENDENCE:2||DETECTOR:2||COHERENCE:2||INJECTION:2||GRAPHENE:1||JOSEPHSONJUNCTIONS:1||LAYERED SUPERCONDUCTOR:1||mode splitting:1||BEHAVIOR:1||spinpolarized transport:1||SUPERCONDUCTING TRANSITION:1||microwave response:1||PSEUDOGAP:1||phase coherence:1||TRANSITIONS:1||Long Josephson junction:1||Charge detection:1||collective resonance modes:1||plasma oscillation modes:1||Superconducting proximity effect:1||Iron pnictide superconductor:1||McMillanRowell oscillations:1||ferromagnetic microstructure:1||superradiant state:1||VOLTAGE:1||branch splitting:1||TENSOR:1||INTERCALATION:1||insitu fabrication:1||NDGAO3:1||DISORDERED METALS:1||GAUGE GLASS:1||LOWTEMPERATURE TRANSPORT:1||spontaneous spin polarization model:1||BIAS:1||emission of electromagnetic waves:1||YBA2CU3O7/PRBA2CU3O7 SUPERLATTICES:1||BOHM:1||SHAPIRO STEPS:1||superconductor/ferromagnet interface:1||OXIDE:1||ANDREEVREFLECTION:1||SinFeAsO single crystal:1||COLLECTIVE MOTION:1||ANGULARDEPENDENCE:1||SUPERCONDUCTIVITY:1||BILAYER GRAPHENE:1||PHOTOLUMINESCENT PROPERTIES:1||SUPERCONDUCTING WEAK LINKS:1||intrinsic Josephson junctions geometrical resonance:1||intrinsic Josephson junction:1||MESOSCOPIC SPINVALVE:1||Bi2212 single crystals:1||intrinsic junctions:1||ANDREEV REFLECTIONS:1||normalmetal/superconductor interface:1||IBI2SR2CACU2OY:1||THERMAL FLUCTUATIONS:1||MIXED STATE:1||BI2.15SR1.85CACU2O8+DELTA:1||intrinsic Josephson effects:1||CACUO:1||QUANTUM POINT CONTACTS:1||resonant tunneling state:1||coherence length:1||NANOWIRE:1||GATES:1||Phase line:1||Thermal activation:1||QUANTUMDOT:1||superconducting proximity effect:1||Andreev interferometer:1||WIRE:1||Josephsonvortexflow branches:1||Bi2212 cuprates:1||LATTICE:1||demannetization effect:1||SUPERCONDUCTING MIRRORS:1||GAS:1||VALLEY TRANSPORT:1||ELECTRODES:1||DEPENDENT TRANSPORT:1||BORNOPPENHEIMER APPROXIMATION:1||collective plasma oscillations:1||fluxon resonance steps:1||STACKS:1||COLLECTIVE DYNAMICS:1||PAIRING SYMMETRY:1||MUON SPIN ROTATION:1||DIMENSIONAL CROSSOVER:1||Bi2Sr2CaCu2Oy highTc superconductors:1||heterojunctions:1||nanostructures:1||surfaces and interfaces:1||QUANTUM TRANSPORT:1||MICROJUNCTIONS:1||RESONATORS:1||STATES:1||FIELD:1||FLUCTUATIONS:1||SCATTERING:1||mode splitting of Josephson vortexflow branches:1||2D superconductivity:1||TRANSISTOR:1||ENERGYGAP:1||SUPERLATTICES:1||IRONBASED SUPERCONDUCTORS:1||PHASEDEPENDENT RESISTANCE:1||QUANTUM PHASETRANSITIONS:1||ELECTRICFIELD:1||HIGH MAGNETICFIELDS:1||NANOWIRE HETEROSTRUCTURES:1||ZNO:1||pair breaking.:1||SUPERCONDUCTING PB:1||domain formation:1||FORCE MICROSCOPY:1||RELAXATION:1||PLASMA RESONANCE:1||coupled Josephson junctions:1||COPPEROXIDE SUPERCONDUCTORS:1||CROSSOVER:1||SIMULATIONS:1||LOWTEMPERATURE:1||CONDUCTORS:1||METALINSULATORTRANSITION:1||SEMICONDUCTOR:1||FIELDEFFECT TRANSISTORS:1||ZEROVOLTAGE STATE:1||constanttemperature interlayer tunneling spectroscopy:1||Josephson supercurrent:1||BIPOLAR SUPERCURRENT:1||Interaction between Josephson and pancake vortices:1||flux jump:1||coaxial heterojunction nanorod:1||Natural Josephson coupling:1||BI2SR2CACU2O8+DELTA:1||VORTEX FLOW:1||TC SUPERCONDUCTORS:1||charge imbalance:1||Andreev diffractometer:1||intercalation:1||surface junction:1||Bi2212:1||tunnelling:1||GRAPHITE:1||GROWTH:1||collective transverse plasma modes:1||GAN:1||Macroscopic quantum tunneling:1||Fluctuation conductivity:1||Abovegap conductance jump:1||Josephson vortex motion:1||Intrinsic Josephson junctions:1||LAYERED SUPERCONDUCTORS:1||BI2SR2CACU2O8+Y:1||INTERFACES:1||BREAKDOWN:1||SYSTEMS:1||Anisotropy ratio:1||Josephson vortex:1||spin relaxation in superconductors:1||bibased single crystals:1||MESOSCOPIC PROXIMITY SUPERCONDUCTOR:1||reentrance of conductance:1||interlayer pair tunneling:1||JOSEPHSON:1||DISORDERED 2DIMENSIONAL SUPERCONDUCTORS:1||INDIUM FILMS:1||excited state:1||REGIME:1||triplet superconductivity:1||FILM:1||SCHOTTKY DIODES:1||peakdiphump structure:1||Kondo effect:1||REENTRANCE:1||Graphene:1||CONTACT:1||BERRYS PHASE:1||2DIMENSIONAL SUPERCONDUCTORS:1||Coulomb diamond:1||magnetic domain:1||spin injection:1||RESONANCE:1||plasma excitation modes:1||FLOW:1||OVERDOPED BI2SR2CACU2O8+DELTA:1||hole doping:1||chemical synthesis:1||phase transitions:1||superconductors:1||VORTEXGLASS SUPERCONDUCTIVITY:1||Kondorelated model:1||RADIATION:1||DOT:1||NANOBELTS:1||Complementarity:1||Closedloop AharonovBohm interferometer:1||pair breaking:1||interlayer phase fluctuation:1||MgB2 thin film:1||CONFINEMENT:1||WALLED CARBON NANOTUBES:1||TRANSITION:9||VORTICES:8||STATE:7||intrinsic Josephson junctions:7||SINGLECRYSTALS:7||JUNCTIONS:5||MODES:5||SUPERCURRENT:5||SUPERCONDUCTOR:5||CONDUCTANCE:5||HIGHTEMPERATURE SUPERCONDUCTORS:5||TRANSPORT:5||PHASE:5||FILMS:4||LOCALIZATION:4||SINGLE DIRAC CONE:4||WIRES:4||MAGNETICFIELD:4||STEPS:3||ELECTRONS:3||proximity effect:3||MODEL:3||ARRAYS:3||INTERFERENCE:3||fluxon dynamics:3||HETEROSTRUCTURES:3||INSULATOR:3||Andreev reflection:3||electronic transport:3||FISKE:3||superconductor:2||ZnO:2||quantum point contact:2||METAL:2||DYNAMICS:2||interlayer Josephson coupling:2||SUPERCONDUCTORS:2||YBA2CU3O7DELTA:2||LAYER:2||DOTS:2||quantum dot:2||Article:2||TRANSISTORS:2||CARBON NANOTUBES:2||GAP:2||MECHANISM:2||LINE:2||GIANT SHAPIRO STEPS:2||LAYERS:2||electron energy loss spectroscopy:2||physical phenomena:2||scanning electron microscopy:2||HGTE QUANTUMWELLS:2||BI2TE3:2||SPECTROSCOPY:2||PNJUNCTIONS:2||spinpolarized tunneling:2||INTRINSIC JOSEPHSONJUNCTIONS:2||FIELDS:2||positive magnetoresistance:2||dilute magnetic semiconductor:2||magnetic field:2||scanning transmission electron microscopy:2||QUANTUM OSCILLATIONS:2||TRANSPORTPROPERTIES:2||surface pair current:2||MAGNETORESISTANCE:2||NANORIBBONS:2||INSTABILITY:2||ANDREEV REFLECTION:2||microwave irradiation:2||vertical graphene josephson junction:2||BI2SE3:2||CONDUCTIVITY:2||highTc superconductors:2||DIMENSIONAL ELECTRONGAS:2||graphene:2||Topological insulators:2||Josephson coupling Fraunhofer interference pattern:2||FERROMAGNET:2||DEPENDENCE:2||DETECTOR:2||COHERENCE:2||INJECTION:2||GRAPHENE:1||JOSEPHSONJUNCTIONS:1||LAYERED SUPERCONDUCTOR:1||mode splitting:1||BEHAVIOR:1||spinpolarized transport:1||SUPERCONDUCTING TRANSITION:1||microwave response:1||PSEUDOGAP:1||phase coherence:1||TRANSITIONS:1||Long Josephson junction:1||Charge detection:1||collective resonance modes:1||plasma oscillation modes:1||Superconducting proximity effect:1||Iron pnictide superconductor:1||McMillanRowell oscillations:1||ferromagnetic microstructure:1||superradiant state:1||VOLTAGE:1||branch splitting:1||TENSOR:1||INTERCALATION:1||insitu fabrication:1||NDGAO3:1||DISORDERED METALS:1||GAUGE GLASS:1||LOWTEMPERATURE TRANSPORT:1||spontaneous spin polarization model:1||BIAS:1||emission of electromagnetic waves:1||YBA2CU3O7/PRBA2CU3O7 SUPERLATTICES:1||BOHM:1||SHAPIRO STEPS:1||superconductor/ferromagnet interface:1||OXIDE:1||ANDREEVREFLECTION:1||SinFeAsO single crystal:1||COLLECTIVE MOTION:1||ANGULARDEPENDENCE:1||SUPERCONDUCTIVITY:1||BILAYER GRAPHENE:1||PHOTOLUMINESCENT PROPERTIES:1||SUPERCONDUCTING WEAK LINKS:1||intrinsic Josephson junctions geometrical resonance:1||intrinsic Josephson junction:1||MESOSCOPIC SPINVALVE:1||Bi2212 single crystals:1||intrinsic junctions:1||ANDREEV REFLECTIONS:1||normalmetal/superconductor interface:1||IBI2SR2CACU2OY:1||THERMAL FLUCTUATIONS:1||MIXED STATE:1||BI2.15SR1.85CACU2O8+DELTA:1||intrinsic Josephson effects:1||CACUO:1||QUANTUM POINT CONTACTS:1||resonant tunneling state:1||coherence length:1||NANOWIRE:1||GATES:1||Phase line:1||Thermal activation:1||QUANTUMDOT:1||superconducting proximity effect:1||Andreev interferometer:1||WIRE:1||Josephsonvortexflow branches:1||Bi2212 cuprates:1||LATTICE:1||demannetization effect:1||SUPERCONDUCTING MIRRORS:1||GAS:1||VALLEY TRANSPORT:1||ELECTRODES:1||DEPENDENT TRANSPORT:1||BORNOPPENHEIMER APPROXIMATION:1||collective plasma oscillations:1||fluxon resonance steps:1||STACKS:1||COLLECTIVE DYNAMICS:1||PAIRING SYMMETRY:1||MUON SPIN ROTATION:1||DIMENSIONAL CROSSOVER:1||Bi2Sr2CaCu2Oy highTc superconductors:1||heterojunctions:1||nanostructures:1||surfaces and interfaces:1||QUANTUM TRANSPORT:1||MICROJUNCTIONS:1||RESONATORS:1||STATES:1||FIELD:1||FLUCTUATIONS:1||SCATTERING:1||mode splitting of Josephson vortexflow branches:1||2D superconductivity:1||TRANSISTOR:1||ENERGYGAP:1||SUPERLATTICES:1||IRONBASED SUPERCONDUCTORS:1||PHASEDEPENDENT RESISTANCE:1||QUANTUM PHASETRANSITIONS:1||ELECTRICFIELD:1||HIGH MAGNETICFIELDS:1||NANOWIRE HETEROSTRUCTURES:1||ZNO:1||pair breaking.:1||SUPERCONDUCTING PB:1||domain formation:1||FORCE MICROSCOPY:1||RELAXATION:1||PLASMA RESONANCE:1||coupled Josephson junctions:1||COPPEROXIDE SUPERCONDUCTORS:1||CROSSOVER:1||SIMULATIONS:1||LOWTEMPERATURE:1||CONDUCTORS:1||METALINSULATORTRANSITION:1||SEMICONDUCTOR:1||FIELDEFFECT TRANSISTORS:1||ZEROVOLTAGE STATE:1||constanttemperature interlayer tunneling spectroscopy:1||Josephson supercurrent:1||BIPOLAR SUPERCURRENT:1||Interaction between Josephson and pancake vortices:1||flux jump:1||coaxial heterojunction nanorod:1||Natural Josephson coupling:1||BI2SR2CACU2O8+DELTA:1||VORTEX FLOW:1||TC SUPERCONDUCTORS:1||charge imbalance:1||Andreev diffractometer:1||intercalation:1||surface junction:1||Bi2212:1||tunnelling:1||GRAPHITE:1||GROWTH:1||collective transverse plasma modes:1||GAN:1||Macroscopic quantum tunneling:1||Fluctuation conductivity:1||Abovegap conductance jump:1||Josephson vortex motion:1||Intrinsic Josephson junctions:1||LAYERED SUPERCONDUCTORS:1||BI2SR2CACU2O8+Y:1||INTERFACES:1||BREAKDOWN:1||SYSTEMS:1||Anisotropy ratio:1||Josephson vortex:1||spin relaxation in superconductors:1||bibased single crystals:1||MESOSCOPIC PROXIMITY SUPERCONDUCTOR:1||reentrance of conductance:1||interlayer pair tunneling:1||JOSEPHSON:1||DISORDERED 2DIMENSIONAL SUPERCONDUCTORS:1||INDIUM FILMS:1||excited state:1||REGIME:1||triplet superconductivity:1||FILM:1||SCHOTTKY DIODES:1||peakdiphump structure:1||Kondo effect:1||REENTRANCE:1||Graphene:1||CONTACT:1||BERRYS PHASE:1||2DIMENSIONAL SUPERCONDUCTORS:1||Coulomb diamond:1||magnetic domain:1||spin injection:1||RESONANCE:1||plasma excitation modes:1||FLOW:1||OVERDOPED BI2SR2CACU2O8+DELTA:1||hole doping:1||chemical synthesis:1||phase transitions:1||superconductors:1||VORTEXGLASS SUPERCONDUCTIVITY:1||Kondorelated model:1||RADIATION:1||DOT:1||NANOBELTS:1||Complementarity:1||Closedloop AharonovBohm interferometer:1||pair breaking:1||interlayer phase fluctuation:1||MgB2 thin film:1||CONFINEMENT:1||WALLED CARBON NANOTUBES:1||TRANSITION:9||VORTICES:8||STATE:7||intrinsic Josephson junctions:7||SINGLECRYSTALS:7||JUNCTIONS:5||MODES:5||SUPERCURRENT:5||SUPERCONDUCTOR:5||CONDUCTANCE:5||HIGHTEMPERATURE SUPERCONDUCTORS:5||TRANSPORT:5||PHASE:5||FILMS:4||LOCALIZATION:4||SINGLE DIRAC CONE:4||WIRES:4||MAGNETICFIELD:4||STEPS:3||ELECTRONS:3||proximity effect:3||MODEL:3||ARRAYS:3||INTERFERENCE:3||fluxon dynamics:3||HETEROSTRUCTURES:3||INSULATOR:3||Andreev reflection:3||electronic transport:3||FISKE:3||superconductor:2||ZnO:2||quantum point contact:2||METAL:2||DYNAMICS:2||interlayer Josephson coupling:2||SUPERCONDUCTORS:2||YBA2CU3O7DELTA:2||LAYER:2||DOTS:2||quantum dot:2||Article:2||TRANSISTORS:2||CARBON NANOTUBES:2||GAP:2||MECHANISM:2||LINE:2||GIANT SHAPIRO STEPS:2||LAYERS:2||electron energy loss spectroscopy:2||physical phenomena:2||scanning electron microscopy:2||HGTE QUANTUMWELLS:2||BI2TE3:2||SPECTROSCOPY:2||PNJUNCTIONS:2||spinpolarized tunneling:2||INTRINSIC JOSEPHSONJUNCTIONS:2||FIELDS:2||positive magnetoresistance:2||dilute magnetic semiconductor:2||magnetic field:2||scanning transmission electron microscopy:2||QUANTUM OSCILLATIONS:2||TRANSPORTPROPERTIES:2||surface pair current:2||MAGNETORESISTANCE:2||NANORIBBONS:2||INSTABILITY:2||ANDREEV REFLECTION:2||microwave irradiation:2||vertical graphene josephson junction:2||BI2SE3:2||CONDUCTIVITY:2||highTc superconductors:2||DIMENSIONAL ELECTRONGAS:2||graphene:2||Topological insulators:2||Josephson coupling Fraunhofer interference pattern:2||FERROMAGNET:2||DEPENDENCE:2||DETECTOR:2||COHERENCE:2||INJECTION:2||GRAPHENE:1||JOSEPHSONJUNCTIONS:1||LAYERED SUPERCONDUCTOR:1||mode splitting:1||BEHAVIOR:1||spinpolarized transport:1||SUPERCONDUCTING TRANSITION:1||microwave response:1||PSEUDOGAP:1||phase coherence:1||TRANSITIONS:1||Long Josephson junction:1||Charge detection:1||collective resonance modes:1||plasma oscillation modes:1||Superconducting proximity effect:1||Iron pnictide superconductor:1||McMillanRowell oscillations:1||ferromagnetic microstructure:1||superradiant state:1||VOLTAGE:1||branch splitting:1||TENSOR:1||INTERCALATION:1||insitu fabrication:1||NDGAO3:1||DISORDERED METALS:1||GAUGE GLASS:1||LOWTEMPERATURE TRANSPORT:1||spontaneous spin polarization model:1||BIAS:1||emission of electromagnetic waves:1||YBA2CU3O7/PRBA2CU3O7 SUPERLATTICES:1||BOHM:1||SHAPIRO STEPS:1||superconductor/ferromagnet interface:1||OXIDE:1||ANDREEVREFLECTION:1||SinFeAsO single crystal:1||COLLECTIVE MOTION:1||ANGULARDEPENDENCE:1||SUPERCONDUCTIVITY:1||BILAYER GRAPHENE:1||PHOTOLUMINESCENT PROPERTIES:1||SUPERCONDUCTING WEAK LINKS:1||intrinsic Josephson junctions geometrical resonance:1||intrinsic Josephson junction:1||MESOSCOPIC SPINVALVE:1||Bi2212 single crystals:1||intrinsic junctions:1||ANDREEV REFLECTIONS:1||normalmetal/superconductor interface:1||IBI2SR2CACU2OY:1||THERMAL FLUCTUATIONS:1||MIXED STATE:1||BI2.15SR1.85CACU2O8+DELTA:1||intrinsic Josephson effects:1||CACUO:1||QUANTUM POINT CONTACTS:1||resonant tunneling state:1||coherence length:1||NANOWIRE:1||GATES:1||Phase line:1||Thermal activation:1||QUANTUMDOT:1||superconducting proximity effect:1||Andreev interferometer:1||WIRE:1||Josephsonvortexflow branches:1||Bi2212 cuprates:1||LATTICE:1||demannetization effect:1||SUPERCONDUCTING MIRRORS:1||GAS:1||VALLEY TRANSPORT:1||ELECTRODES:1||DEPENDENT TRANSPORT:1||BORNOPPENHEIMER APPROXIMATION:1||collective plasma oscillations:1||fluxon resonance steps:1||STACKS:1||COLLECTIVE DYNAMICS:1||PAIRING SYMMETRY:1||MUON SPIN ROTATION:1||DIMENSIONAL CROSSOVER:1||Bi2Sr2CaCu2Oy highTc superconductors:1||heterojunctions:1||nanostructures:1||surfaces and interfaces:1||QUANTUM TRANSPORT:1||MICROJUNCTIONS:1||RESONATORS:1||STATES:1||FIELD:1||FLUCTUATIONS:1||SCATTERING:1||mode splitting of Josephson vortexflow branches:1||2D superconductivity:1||TRANSISTOR:1||ENERGYGAP:1||SUPERLATTICES:1||IRONBASED SUPERCONDUCTORS:1||PHASEDEPENDENT RESISTANCE:1||QUANTUM PHASETRANSITIONS:1||ELECTRICFIELD:1||HIGH MAGNETICFIELDS:1||NANOWIRE HETEROSTRUCTURES:1||ZNO:1||pair breaking.:1||SUPERCONDUCTING PB:1||domain formation:1||FORCE MICROSCOPY:1||RELAXATION:1||PLASMA RESONANCE:1||coupled Josephson junctions:1||COPPEROXIDE SUPERCONDUCTORS:1||CROSSOVER:1||SIMULATIONS:1||LOWTEMPERATURE:1||CONDUCTORS:1||METALINSULATORTRANSITION:1||SEMICONDUCTOR:1||FIELDEFFECT TRANSISTORS:1||ZEROVOLTAGE STATE:1||constanttemperature interlayer tunneling spectroscopy:1||Josephson supercurrent:1||BIPOLAR SUPERCURRENT:1||Interaction between Josephson and pancake vortices:1||flux jump:1||coaxial heterojunction nanorod:1||Natural Josephson coupling:1||BI2SR2CACU2O8+DELTA:1||VORTEX FLOW:1||TC SUPERCONDUCTORS:1||charge imbalance:1||Andreev diffractometer:1||intercalation:1||surface junction:1||Bi2212:1||tunnelling:1||GRAPHITE:1||GROWTH:1||collective transverse plasma modes:1||GAN:1||Macroscopic quantum tunneling:1||Fluctuation conductivity:1||Abovegap conductance jump:1||Josephson vortex motion:1||Intrinsic Josephson junctions:1||LAYERED SUPERCONDUCTORS:1||BI2SR2CACU2O8+Y:1||INTERFACES:1||BREAKDOWN:1||SYSTEMS:1||Anisotropy ratio:1||Josephson vortex:1||spin relaxation in superconductors:1||bibased single crystals:1||MESOSCOPIC PROXIMITY SUPERCONDUCTOR:1||reentrance of conductance:1||interlayer pair tunneling:1||JOSEPHSON:1||DISORDERED 2DIMENSIONAL SUPERCONDUCTORS:1||INDIUM FILMS:1||excited state:1||REGIME:1||triplet superconductivity:1||FILM:1||SCHOTTKY DIODES:1||peakdiphump structure:1||Kondo effect:1||REENTRANCE:1||Graphene:1||CONTACT:1||BERRYS PHASE:1||2DIMENSIONAL SUPERCONDUCTORS:1||Coulomb diamond:1||magnetic domain:1||spin injection:1||RESONANCE:1||plasma excitation modes:1||FLOW:1||OVERDOPED BI2SR2CACU2O8+DELTA:1||hole doping:1||chemical synthesis:1||phase transitions:1||superconductors:1||VORTEXGLASS SUPERCONDUCTIVITY:1||Kondorelated model:1||RADIATION:1||DOT:1||NANOBELTS:1||Complementarity:1||Closedloop AharonovBohm interferometer:1||pair breaking:1||interlayer phase fluctuation:1||MgB2 thin film:1||CONFINEMENT:1||WALLED CARBON NANOTUBES:1||TRANSITION:9||VORTICES:8||STATE:7||intrinsic Josephson junctions:7||SINGLECRYSTALS:7||JUNCTIONS:5||MODES:5||SUPERCURRENT:5||SUPERCONDUCTOR:5||CONDUCTANCE:5||HIGHTEMPERATURE SUPERCONDUCTORS:5||TRANSPORT:5||PHASE:5||FILMS:4||LOCALIZATION:4||SINGLE DIRAC CONE:4||WIRES:4||MAGNETICFIELD:4||STEPS:3||ELECTRONS:3||proximity effect:3||MODEL:3||ARRAYS:3||INTERFERENCE:3||fluxon dynamics:3||HETEROSTRUCTURES:3||INSULATOR:3||Andreev reflection:3||electronic transport:3||FISKE:3||superconductor:2||ZnO:2||quantum point contact:2||METAL:2||DYNAMICS:2||interlayer Josephson coupling:2||SUPERCONDUCTORS:2||YBA2CU3O7DELTA:2||LAYER:2||DOTS:2||quantum dot:2||Article:2||TRANSISTORS:2||CARBON NANOTUBES:2||GAP:2||MECHANISM:2||LINE:2||GIANT SHAPIRO STEPS:2||LAYERS:2||electron energy loss spectroscopy:2||physical phenomena:2||scanning electron microscopy:2||HGTE QUANTUMWELLS:2||BI2TE3:2||SPECTROSCOPY:2||PNJUNCTIONS:2||spinpolarized tunneling:2||INTRINSIC JOSEPHSONJUNCTIONS:2||FIELDS:2||positive magnetoresistance:2||dilute magnetic semiconductor:2||magnetic field:2||scanning transmission electron microscopy:2||QUANTUM OSCILLATIONS:2||TRANSPORTPROPERTIES:2||surface pair current:2||MAGNETORESISTANCE:2||NANORIBBONS:2||INSTABILITY:2||ANDREEV REFLECTION:2||microwave irradiation:2||vertical graphene josephson junction:2||BI2SE3:2||CONDUCTIVITY:2||highTc superconductors:2||DIMENSIONAL ELECTRONGAS:2||graphene:2||Topological insulators:2||Josephson coupling Fraunhofer interference pattern:2||FERROMAGNET:2||DEPENDENCE:2||DETECTOR:2||COHERENCE:2||INJECTION:2||GRAPHENE:1||JOSEPHSONJUNCTIONS:1||LAYERED SUPERCONDUCTOR:1||mode splitting:1||BEHAVIOR:1||spinpolarized transport:1||SUPERCONDUCTING TRANSITION:1||microwave response:1||PSEUDOGAP:1||phase coherence:1||TRANSITIONS:1||Long Josephson junction:1||Charge detection:1||collective resonance modes:1||plasma oscillation modes:1||Superconducting proximity effect:1||Iron pnictide superconductor:1||McMillanRowell oscillations:1||ferromagnetic microstructure:1||superradiant state:1||VOLTAGE:1||branch splitting:1||TENSOR:1||INTERCALATION:1||insitu fabrication:1||NDGAO3:1||DISORDERED METALS:1||GAUGE GLASS:1||LOWTEMPERATURE TRANSPORT:1||spontaneous spin polarization model:1||BIAS:1||emission of electromagnetic waves:1||YBA2CU3O7/PRBA2CU3O7 SUPERLATTICES:1||BOHM:1||SHAPIRO STEPS:1||superconductor/ferromagnet interface:1||OXIDE:1||ANDREEVREFLECTION:1||SinFeAsO single crystal:1||COLLECTIVE MOTION:1||ANGULARDEPENDENCE:1||SUPERCONDUCTIVITY:1||BILAYER GRAPHENE:1||PHOTOLUMINESCENT PROPERTIES:1||SUPERCONDUCTING WEAK LINKS:1||intrinsic Josephson junctions geometrical resonance:1||intrinsic Josephson junction:1||MESOSCOPIC SPINVALVE:1||Bi2212 single crystals:1||intrinsic junctions:1||ANDREEV REFLECTIONS:1||normalmetal/superconductor interface:1||IBI2SR2CACU2OY:1||THERMAL FLUCTUATIONS:1||MIXED STATE:1||BI2.15SR1.85CACU2O8+DELTA:1||intrinsic Josephson effects:1||CACUO:1||QUANTUM POINT CONTACTS:1||resonant tunneling state:1||coherence length:1||NANOWIRE:1||GATES:1||Phase line:1||Thermal activation:1||QUANTUMDOT:1||superconducting proximity effect:1||Andreev interferometer:1||WIRE:1||Josephsonvortexflow branches:1||Bi2212 cuprates:1||LATTICE:1||demannetization effect:1||SUPERCONDUCTING MIRRORS:1||GAS:1||VALLEY TRANSPORT:1||ELECTRODES:1||DEPENDENT TRANSPORT:1||BORNOPPENHEIMER APPROXIMATION:1||collective plasma oscillations:1||fluxon resonance steps:1||STACKS:1||COLLECTIVE DYNAMICS:1||PAIRING SYMMETRY:1||MUON SPIN ROTATION:1||DIMENSIONAL CROSSOVER:1||Bi2Sr2CaCu2Oy highTc superconductors:1||heterojunctions:1||nanostructures:1||surfaces and interfaces:1||QUANTUM TRANSPORT:1||MICROJUNCTIONS:1||RESONATORS:1||STATES:1||FIELD:1||FLUCTUATIONS:1||SCATTERING:1||mode splitting of Josephson vortexflow branches:1||2D superconductivity:1||TRANSISTOR:1||ENERGYGAP:1||SUPERLATTICES:1||IRONBASED SUPERCONDUCTORS:1||PHASEDEPENDENT RESISTANCE:1||QUANTUM PHASETRANSITIONS:1||ELECTRICFIELD:1||HIGH MAGNETICFIELDS:1||NANOWIRE HETEROSTRUCTURES:1||ZNO:1||pair breaking.:1||SUPERCONDUCTING PB:1||domain formation:1||FORCE MICROSCOPY:1||RELAXATION:1||PLASMA RESONANCE:1||coupled Josephson junctions:1||COPPEROXIDE SUPERCONDUCTORS:1||CROSSOVER:1||SIMULATIONS:1||LOWTEMPERATURE:1||CONDUCTORS:1||METALINSULATORTRANSITION:1||SEMICONDUCTOR:1||FIELDEFFECT TRANSISTORS:1||ZEROVOLTAGE STATE:1||constanttemperature interlayer tunneling spectroscopy:1||Josephson supercurrent:1||BIPOLAR SUPERCURRENT:1||Interaction between Josephson and pancake vortices:1||flux jump:1||coaxial heterojunction nanorod:1||Natural Josephson coupling:1||BI2SR2CACU2O8+DELTA:1||VORTEX FLOW:1||TC SUPERCONDUCTORS:1||charge imbalance:1||Andreev diffractometer:1||intercalation:1||surface junction:1||Bi2212:1||tunnelling:1||GRAPHITE:1||GROWTH:1||collective transverse plasma modes:1||GAN:1||Macroscopic quantum tunneling:1||Fluctuation conductivity:1||Abovegap conductance jump:1||Josephson vortex motion:1||Intrinsic Josephson junctions:1||LAYERED SUPERCONDUCTORS:1||BI2SR2CACU2O8+Y:1||INTERFACES:1||BREAKDOWN:1||SYSTEMS:1||Anisotropy ratio:1||Josephson vortex:1||spin relaxation in superconductors:1||bibased single crystals:1||MESOSCOPIC PROXIMITY SUPERCONDUCTOR:1||reentrance of conductance:1||interlayer pair tunneling:1||JOSEPHSON:1||DISORDERED 2DIMENSIONAL SUPERCONDUCTORS:1||INDIUM FILMS:1||excited state:1||REGIME:1||triplet superconductivity:1||FILM:1||SCHOTTKY DIODES:1||peakdiphump structure:1||Kondo effect:1||REENTRANCE:1||Graphene:1||CONTACT:1||BERRYS PHASE:1||2DIMENSIONAL SUPERCONDUCTORS:1||Coulomb diamond:1||magnetic domain:1||spin injection:1||RESONANCE:1||plasma excitation modes:1||FLOW:1||OVERDOPED BI2SR2CACU2O8+DELTA:1||hole doping:1||chemical synthesis:1||phase transitions:1||superconductors:1||VORTEXGLASS SUPERCONDUCTIVITY:1||Kondorelated model:1||RADIATION:1||DOT:1||NANOBELTS:1||Complementarity:1||Closedloop AharonovBohm interferometer:1||pair breaking:1||interlayer phase fluctuation:1||MgB2 thin film:1||CONFINEMENT:1||WALLED CARBON NANOTUBES:1||TRANSITION:9||VORTICES:8||STATE:7||intrinsic Josephson junctions:7||SINGLECRYSTALS:7||JUNCTIONS:5||MODES:5||SUPERCURRENT:5||SUPERCONDUCTOR:5||CONDUCTANCE:5||HIGHTEMPERATURE SUPERCONDUCTORS:5||TRANSPORT:5||PHASE:5||FILMS:4||LOCALIZATION:4||SINGLE DIRAC CONE:4||WIRES:4||MAGNETICFIELD:4||STEPS:3||ELECTRONS:3||proximity effect:3||MODEL:3||ARRAYS:3||INTERFERENCE:3||fluxon dynamics:3||HETEROSTRUCTURES:3||INSULATOR:3||Andreev reflection:3||electronic transport:3||FISKE:3||superconductor:2||ZnO:2||quantum point contact:2||METAL:2||DYNAMICS:2||interlayer Josephson coupling:2||SUPERCONDUCTORS:2||YBA2CU3O7DELTA:2||LAYER:2||DOTS:2||quantum dot:2||Article:2||TRANSISTORS:2||CARBON NANOTUBES:2||GAP:2||MECHANISM:2||LINE:2||GIANT SHAPIRO STEPS:2||LAYERS:2||electron energy loss spectroscopy:2||physical phenomena:2||scanning electron microscopy:2||HGTE QUANTUMWELLS:2||BI2TE3:2||SPECTROSCOPY:2||PNJUNCTIONS:2||spinpolarized tunneling:2||INTRINSIC JOSEPHSONJUNCTIONS:2||FIELDS:2||positive magnetoresistance:2||dilute magnetic semiconductor:2||magnetic field:2||scanning transmission electron microscopy:2||QUANTUM OSCILLATIONS:2||TRANSPORTPROPERTIES:2||surface pair current:2||MAGNETORESISTANCE:2||NANORIBBONS:2||INSTABILITY:2||ANDREEV REFLECTION:2||microwave irradiation:2||vertical graphene josephson junction:2||BI2SE3:2||CONDUCTIVITY:2||highTc superconductors:2||DIMENSIONAL ELECTRONGAS:2||graphene:2||Topological insulators:2||Josephson coupling Fraunhofer interference pattern:2||FERROMAGNET:2||DEPENDENCE:2||DETECTOR:2||COHERENCE:2||INJECTION:2||GRAPHENE:1||JOSEPHSONJUNCTIONS:1||LAYERED SUPERCONDUCTOR:1||mode splitting:1||BEHAVIOR:1||spinpolarized transport:1||SUPERCONDUCTING TRANSITION:1||microwave response:1||PSEUDOGAP:1||phase coherence:1||TRANSITIONS:1||Long Josephson junction:1||Charge detection:1||collective resonance modes:1||plasma oscillation modes:1||Superconducting proximity effect:1||Iron pnictide superconductor:1||McMillanRowell oscillations:1||ferromagnetic microstructure:1||superradiant state:1||VOLTAGE:1||branch splitting:1||TENSOR:1||INTERCALATION:1||insitu fabrication:1||NDGAO3:1||DISORDERED METALS:1||GAUGE GLASS:1||LOWTEMPERATURE TRANSPORT:1||spontaneous spin polarization model:1||BIAS:1||emission of electromagnetic waves:1||YBA2CU3O7/PRBA2CU3O7 SUPERLATTICES:1||BOHM:1||SHAPIRO STEPS:1||superconductor/ferromagnet interface:1||OXIDE:1||ANDREEVREFLECTION:1||SinFeAsO single crystal:1||COLLECTIVE MOTION:1||ANGULARDEPENDENCE:1||SUPERCONDUCTIVITY:1||BILAYER GRAPHENE:1||PHOTOLUMINESCENT PROPERTIES:1||SUPERCONDUCTING WEAK LINKS:1||intrinsic Josephson junctions geometrical resonance:1||intrinsic Josephson junction:1||MESOSCOPIC SPINVALVE:1||Bi2212 single crystals:1||intrinsic junctions:1||ANDREEV REFLECTIONS:1||normalmetal/superconductor interface:1||IBI2SR2CACU2OY:1||THERMAL FLUCTUATIONS:1||MIXED STATE:1||BI2.15SR1.85CACU2O8+DELTA:1||intrinsic Josephson effects:1||CACUO:1||QUANTUM POINT CONTACTS:1||resonant tunneling state:1||coherence length:1||NANOWIRE:1||GATES:1||Phase line:1||Thermal activation:1||QUANTUMDOT:1||superconducting proximity effect:1||Andreev interferometer:1||WIRE:1||Josephsonvortexflow branches:1||Bi2212 cuprates:1||LATTICE:1||demannetization effect:1||SUPERCONDUCTING MIRRORS:1||GAS:1||VALLEY TRANSPORT:1||ELECTRODES:1||DEPENDENT TRANSPORT:1||BORNOPPENHEIMER APPROXIMATION:1||collective plasma oscillations:1||fluxon resonance steps:1||STACKS:1||COLLECTIVE DYNAMICS:1||PAIRING SYMMETRY:1||MUON SPIN ROTATION:1||DIMENSIONAL CROSSOVER:1||Bi2Sr2CaCu2Oy highTc superconductors:1||heterojunctions:1||nanostructures:1||surfaces and interfaces:1||QUANTUM TRANSPORT:1||MICROJUNCTIONS:1||RESONATORS:1||STATES:1||FIELD:1||FLUCTUATIONS:1||SCATTERING:1||mode splitting of Josephson vortexflow branches:1||2D superconductivity:1||TRANSISTOR:1||ENERGYGAP:1||SUPERLATTICES:1||IRONBASED SUPERCONDUCTORS:1||PHASEDEPENDENT RESISTANCE:1||QUANTUM PHASETRANSITIONS:1||ELECTRICFIELD:1||HIGH MAGNETICFIELDS:1||NANOWIRE HETEROSTRUCTURES:1||ZNO:1||pair breaking.:1||SUPERCONDUCTING PB:1||domain formation:1||FORCE MICROSCOPY:1||RELAXATION:1||PLASMA RESONANCE:1||coupled Josephson junctions:1||COPPEROXIDE SUPERCONDUCTORS:1||CROSSOVER:1||SIMULATIONS:1||LOWTEMPERATURE:1||CONDUCTORS:1||METALINSULATORTRANSITION:1||SEMICONDUCTOR:1||FIELDEFFECT TRANSISTORS:1||ZEROVOLTAGE STATE:1||constanttemperature interlayer tunneling spectroscopy:1||Josephson supercurrent:1||BIPOLAR SUPERCURRENT:1||Interaction between Josephson and pancake vortices:1||flux jump:1||coaxial heterojunction nanorod:1||Natural Josephson coupling:1||BI2SR2CACU2O8+DELTA:1||VORTEX FLOW:1||TC SUPERCONDUCTORS:1||charge imbalance:1||Andreev diffractometer:1||intercalation:1||surface junction:1||Bi2212:1||tunnelling:1||GRAPHITE:1||GROWTH:1||collective transverse plasma modes:1||GAN:1||Macroscopic quantum tunneling:1||Fluctuation conductivity:1||Abovegap conductance jump:1||Josephson vortex motion:1||Intrinsic Josephson junctions:1||LAYERED SUPERCONDUCTORS:1||BI2SR2CACU2O8+Y:1||INTERFACES:1||BREAKDOWN:1||SYSTEMS:1||Anisotropy ratio:1||Josephson vortex:1||spin relaxation in superconductors:1||bibased single crystals:1||MESOSCOPIC PROXIMITY SUPERCONDUCTOR:1||reentrance of conductance:1||interlayer pair tunneling:1||JOSEPHSON:1||DISORDERED 2DIMENSIONAL SUPERCONDUCTORS:1||INDIUM FILMS:1||excited state:1||REGIME:1||triplet superconductivity:1||FILM:1||SCHOTTKY DIODES:1||peakdiphump structure:1||Kondo effect:1||REENTRANCE:1||Graphene:1||CONTACT:1||BERRYS PHASE:1||2DIMENSIONAL SUPERCONDUCTORS:1||Coulomb diamond:1||magnetic domain:1||spin injection:1||RESONANCE:1||plasma excitation modes:1||FLOW:1||OVERDOPED BI2SR2CACU2O8+DELTA:1||hole doping:1||chemical synthesis:1||phase transitions:1||superconductors:1||VORTEXGLASS SUPERCONDUCTIVITY:1||Kondorelated model:1||RADIATION:1||DOT:1||NANOBELTS:1||Complementarity:1||Closedloop AharonovBohm interferometer:1||pair breaking:1||interlayer phase fluctuation:1||MgB2 thin film:1||CONFINEMENT:1||WALLED CARBON NANOTUBES:1||TRANSITION:9||VORTICES:8||STATE:7||intrinsic Josephson junctions:7||SINGLECRYSTALS:7||JUNCTIONS:5||MODES:5||SUPERCURRENT:5||SUPERCONDUCTOR:5||CONDUCTANCE:5||HIGHTEMPERATURE SUPERCONDUCTORS:5||TRANSPORT:5||PHASE:5||FILMS:4||LOCALIZATION:4||SINGLE DIRAC CONE:4||WIRES:4||MAGNETICFIELD:4||STEPS:3||ELECTRONS:3||proximity effect:3||MODEL:3||ARRAYS:3||INTERFERENCE:3||fluxon dynamics:3||HETEROSTRUCTURES:3||INSULATOR:3||Andreev reflection:3||electronic transport:3||FISKE:3||superconductor:2||ZnO:2||quantum point contact:2||METAL:2||DYNAMICS:2||interlayer Josephson coupling:2||SUPERCONDUCTORS:2||YBA2CU3O7DELTA:2||LAYER:2||DOTS:2||quantum dot:2||Article:2||TRANSISTORS:2||CARBON NANOTUBES:2||GAP:2||MECHANISM:2||LINE:2||GIANT SHAPIRO STEPS:2||LAYERS:2||electron energy loss spectroscopy:2||physical phenomena:2||scanning electron microscopy:2||HGTE QUANTUMWELLS:2||BI2TE3:2||SPECTROSCOPY:2||PNJUNCTIONS:2||spinpolarized tunneling:2||INTRINSIC JOSEPHSONJUNCTIONS:2||FIELDS:2||positive magnetoresistance:2||dilute magnetic semiconductor:2||magnetic field:2||scanning transmission electron microscopy:2||QUANTUM OSCILLATIONS:2||TRANSPORTPROPERTIES:2||surface pair current:2||MAGNETORESISTANCE:2||NANORIBBONS:2||INSTABILITY:2||ANDREEV REFLECTION:2||microwave irradiation:2||vertical graphene josephson junction:2||BI2SE3:2||CONDUCTIVITY:2||highTc superconductors:2||DIMENSIONAL ELECTRONGAS:2||graphene:2||Topological insulators:2||Josephson coupling Fraunhofer interference pattern:2||FERROMAGNET:2||DEPENDENCE:2||DETECTOR:2||COHERENCE:2||INJECTION:2||GRAPHENE:1||JOSEPHSONJUNCTIONS:1||LAYERED SUPERCONDUCTOR:1||mode splitting:1||BEHAVIOR:1||spinpolarized transport:1||SUPERCONDUCTING TRANSITION:1||microwave response:1||PSEUDOGAP:1||phase coherence:1||TRANSITIONS:1||Long Josephson junction:1||Charge detection:1||collective resonance modes:1||plasma oscillation modes:1||Superconducting proximity effect:1||Iron pnictide superconductor:1||McMillanRowell oscillations:1||ferromagnetic microstructure:1||superradiant state:1||VOLTAGE:1||branch splitting:1||TENSOR:1||INTERCALATION:1||insitu fabrication:1||NDGAO3:1||DISORDERED METALS:1||GAUGE GLASS:1||LOWTEMPERATURE TRANSPORT:1||spontaneous spin polarization model:1||BIAS:1||emission of electromagnetic waves:1||YBA2CU3O7/PRBA2CU3O7 SUPERLATTICES:1||BOHM:1||SHAPIRO STEPS:1||superconductor/ferromagnet interface:1||OXIDE:1||ANDREEVREFLECTION:1||SinFeAsO single crystal:1||COLLECTIVE MOTION:1||ANGULARDEPENDENCE:1||SUPERCONDUCTIVITY:1||BILAYER GRAPHENE:1||PHOTOLUMINESCENT PROPERTIES:1||SUPERCONDUCTING WEAK LINKS:1||intrinsic Josephson junctions geometrical resonance:1||intrinsic Josephson junction:1||MESOSCOPIC SPINVALVE:1||Bi2212 single crystals:1||intrinsic junctions:1||ANDREEV REFLECTIONS:1||normalmetal/superconductor interface:1||IBI2SR2CACU2OY:1||THERMAL FLUCTUATIONS:1||MIXED STATE:1||BI2.15SR1.85CACU2O8+DELTA:1||intrinsic Josephson effects:1||CACUO:1||QUANTUM POINT CONTACTS:1||resonant tunneling state:1||coherence length:1||NANOWIRE:1||GATES:1||Phase line:1||Thermal activation:1||QUANTUMDOT:1||superconducting proximity effect:1||Andreev interferometer:1||WIRE:1||Josephsonvortexflow branches:1||Bi2212 cuprates:1||LATTICE:1||demannetization effect:1||SUPERCONDUCTING MIRRORS:1||GAS:1||VALLEY TRANSPORT:1||ELECTRODES:1||DEPENDENT TRANSPORT:1||BORNOPPENHEIMER APPROXIMATION:1||collective plasma oscillations:1||fluxon resonance steps:1||STACKS:1||COLLECTIVE DYNAMICS:1||PAIRING SYMMETRY:1||MUON SPIN ROTATION:1||DIMENSIONAL CROSSOVER:1||Bi2Sr2CaCu2Oy highTc superconductors:1||heterojunctions:1||nanostructures:1||surfaces and interfaces:1||QUANTUM TRANSPORT:1||MICROJUNCTIONS:1||RESONATORS:1||STATES:1||FIELD:1||FLUCTUATIONS:1||SCATTERING:1||mode splitting of Josephson vortexflow branches:1||2D superconductivity:1||TRANSISTOR:1||ENERGYGAP:1||SUPERLATTICES:1||IRONBASED SUPERCONDUCTORS:1||PHASEDEPENDENT RESISTANCE:1||QUANTUM PHASETRANSITIONS:1||ELECTRICFIELD:1||HIGH MAGNETICFIELDS:1||NANOWIRE HETEROSTRUCTURES:1||ZNO:1||pair breaking.:1||SUPERCONDUCTING PB:1||domain formation:1||FORCE MICROSCOPY:1||RELAXATION:1||PLASMA RESONANCE:1||coupled Josephson junctions:1||COPPEROXIDE SUPERCONDUCTORS:1||CROSSOVER:1||SIMULATIONS:1||LOWTEMPERATURE:1||CONDUCTORS:1||METALINSULATORTRANSITION:1||SEMICONDUCTOR:1||FIELDEFFECT TRANSISTORS:1||ZEROVOLTAGE STATE:1||constanttemperature interlayer tunneling spectroscopy:1||Josephson supercurrent:1||BIPOLAR SUPERCURRENT:1||Interaction between Josephson and pancake vortices:1||flux jump:1||coaxial heterojunction nanorod:1||Natural Josephson coupling:1||BI2SR2CACU2O8+DELTA:1||VORTEX FLOW:1||TC SUPERCONDUCTORS:1||charge imbalance:1||Andreev diffractometer:1||intercalation:1||surface junction:1||Bi2212:1||tunnelling:1||GRAPHITE:1||GROWTH:1||collective transverse plasma modes:1||GAN:1||Macroscopic quantum tunneling:1||Fluctuation conductivity:1||Abovegap conductance jump:1||Josephson vortex motion:1||Intrinsic Josephson junctions:1||LAYERED SUPERCONDUCTORS:1||BI2SR2CACU2O8+Y:1||INTERFACES:1||BREAKDOWN:1||SYSTEMS:1||Anisotropy ratio:1||Josephson vortex:1||spin relaxation in superconductors:1||bibased single crystals:1||MESOSCOPIC PROXIMITY SUPERCONDUCTOR:1||reentrance of conductance:1||interlayer pair tunneling:1||JOSEPHSON:1||DISORDERED 2DIMENSIONAL SUPERCONDUCTORS:1||INDIUM FILMS:1||excited state:1||REGIME:1||triplet superconductivity:1||FILM:1||SCHOTTKY DIODES:1||peakdiphump structure:1||Kondo effect:1||REENTRANCE:1||Graphene:1||CONTACT:1||BERRYS PHASE:1||2DIMENSIONAL SUPERCONDUCTORS:1||Coulomb diamond:1||magnetic domain:1||spin injection:1||RESONANCE:1||plasma excitation modes:1||FLOW:1||OVERDOPED BI2SR2CACU2O8+DELTA:1||hole doping:1||chemical synthesis:1||phase transitions:1||superconductors:1||VORTEXGLASS SUPERCONDUCTIVITY:1||Kondorelated model:1||RADIATION:1||DOT:1||NANOBELTS:1||Complementarity:1||Closedloop AharonovBohm interferometer:1||pair breaking:1||interlayer phase fluctuation:1||MgB2 thin film:1||CONFINEMENT:1||WALLED CARBON NANOTUBES:1||TRANSITION:9||VORTICES:8||STATE:7||intrinsic Josephson junctions:7||SINGLECRYSTALS:7||JUNCTIONS:5||MODES:5||SUPERCURRENT:5||SUPERCONDUCTOR:5||CONDUCTANCE:5||HIGHTEMPERATURE SUPERCONDUCTORS:5||TRANSPORT:5||PHASE:5||FILMS:4||LOCALIZATION:4||SINGLE DIRAC CONE:4||WIRES:4||MAGNETICFIELD:4||STEPS:3||ELECTRONS:3||proximity effect:3||MODEL:3||ARRAYS:3||INTERFERENCE:3||fluxon dynamics:3||HETEROSTRUCTURES:3||INSULATOR:3||Andreev reflection:3||electronic transport:3||FISKE:3||superconductor:2||ZnO:2||quantum point contact:2||METAL:2||DYNAMICS:2||interlayer Josephson coupling:2||SUPERCONDUCTORS:2||YBA2CU3O7DELTA:2||LAYER:2||DOTS:2||quantum dot:2||Article:2||TRANSISTORS:2||CARBON NANOTUBES:2||GAP:2||MECHANISM:2||LINE:2||GIANT SHAPIRO STEPS:2||LAYERS:2||electron energy loss spectroscopy:2||physical phenomena:2||scanning electron microscopy:2||HGTE QUANTUMWELLS:2||BI2TE3:2||SPECTROSCOPY:2||PNJUNCTIONS:2||spinpolarized tunneling:2||INTRINSIC JOSEPHSONJUNCTIONS:2||FIELDS:2||positive magnetoresistance:2||dilute magnetic semiconductor:2||magnetic field:2||scanning transmission electron microscopy:2||QUANTUM OSCILLATIONS:2||TRANSPORTPROPERTIES:2||surface pair current:2||MAGNETORESISTANCE:2||NANORIBBONS:2||INSTABILITY:2||ANDREEV REFLECTION:2||microwave irradiation:2||vertical graphene josephson junction:2||BI2SE3:2||CONDUCTIVITY:2||highTc superconductors:2||DIMENSIONAL ELECTRONGAS:2||graphene:2||Topological insulators:2||Josephson coupling Fraunhofer interference pattern:2||FERROMAGNET:2||DEPENDENCE:2||DETECTOR:2||COHERENCE:2||INJECTION:2||GRAPHENE:1||JOSEPHSONJUNCTIONS:1||LAYERED SUPERCONDUCTOR:1||mode splitting:1||BEHAVIOR:1||spinpolarized transport:1||SUPERCONDUCTING TRANSITION:1||microwave response:1||PSEUDOGAP:1||phase coherence:1||TRANSITIONS:1||Long Josephson junction:1||Charge detection:1||collective resonance modes:1||plasma oscillation modes:1||Superconducting proximity effect:1||Iron pnictide superconductor:1||McMillanRowell oscillations:1||ferromagnetic microstructure:1||superradiant state:1||VOLTAGE:1||branch splitting:1||TENSOR:1||INTERCALATION:1||insitu fabrication:1||NDGAO3:1||DISORDERED METALS:1||GAUGE GLASS:1||LOWTEMPERATURE TRANSPORT:1||spontaneous spin polarization model:1||BIAS:1||emission of electromagnetic waves:1||YBA2CU3O7/PRBA2CU3O7 SUPERLATTICES:1||BOHM:1||SHAPIRO STEPS:1||superconductor/ferromagnet interface:1||OXIDE:1||ANDREEVREFLECTION:1||SinFeAsO single crystal:1||COLLECTIVE MOTION:1||ANGULARDEPENDENCE:1||SUPERCONDUCTIVITY:1||BILAYER GRAPHENE:1||PHOTOLUMINESCENT PROPERTIES:1||SUPERCONDUCTING WEAK LINKS:1||intrinsic Josephson junctions geometrical resonance:1||intrinsic Josephson junction:1||MESOSCOPIC SPINVALVE:1||Bi2212 single crystals:1||intrinsic junctions:1||ANDREEV REFLECTIONS:1||normalmetal/superconductor interface:1||IBI2SR2CACU2OY:1||THERMAL FLUCTUATIONS:1||MIXED STATE:1||BI2.15SR1.85CACU2O8+DELTA:1||intrinsic Josephson effects:1||CACUO:1||QUANTUM POINT CONTACTS:1||resonant tunneling state:1||coherence length:1||NANOWIRE:1||GATES:1||Phase line:1||Thermal activation:1||QUANTUMDOT:1||superconducting proximity effect:1||Andreev interferometer:1||WIRE:1||Josephsonvortexflow branches:1||Bi2212 cuprates:1||LATTICE:1||demannetization effect:1||SUPERCONDUCTING MIRRORS:1||GAS:1||VALLEY TRANSPORT:1||ELECTRODES:1||DEPENDENT TRANSPORT:1||BORNOPPENHEIMER APPROXIMATION:1||collective plasma oscillations:1||fluxon resonance steps:1||STACKS:1||COLLECTIVE DYNAMICS:1||PAIRING SYMMETRY:1||MUON SPIN ROTATION:1||DIMENSIONAL CROSSOVER:1||Bi2Sr2CaCu2Oy highTc superconductors:1||heterojunctions:1||nanostructures:1||surfaces and interfaces:1||QUANTUM TRANSPORT:1||MICROJUNCTIONS:1||RESONATORS:1||STATES:1||FIELD:1||FLUCTUATIONS:1||SCATTERING:1||mode splitting of Josephson vortexflow branches:1||2D superconductivity:1||TRANSISTOR:1||ENERGYGAP:1||SUPERLATTICES:1||IRONBASED SUPERCONDUCTORS:1||PHASEDEPENDENT RESISTANCE:1||QUANTUM PHASETRANSITIONS:1||ELECTRICFIELD:1||HIGH MAGNETICFIELDS:1||NANOWIRE HETEROSTRUCTURES:1||ZNO:1||pair breaking.:1||SUPERCONDUCTING PB:1||domain formation:1||FORCE MICROSCOPY:1||RELAXATION:1||PLASMA RESONANCE:1||coupled Josephson junctions:1||COPPEROXIDE SUPERCONDUCTORS:1||CROSSOVER:1||SIMULATIONS:1||LOWTEMPERATURE:1||CONDUCTORS:1||METALINSULATORTRANSITION:1||SEMICONDUCTOR:1||FIELDEFFECT TRANSISTORS:1||ZEROVOLTAGE STATE:1||constanttemperature interlayer tunneling spectroscopy:1||Josephson supercurrent:1||BIPOLAR SUPERCURRENT:1||Interaction between Josephson and pancake vortices:1||flux jump:1||coaxial heterojunction nanorod:1||Natural Josephson coupling:1||BI2SR2CACU2O8+DELTA:1||VORTEX FLOW:1||TC SUPERCONDUCTORS:1||charge imbalance:1||Andreev diffractometer:1||intercalation:1||surface junction:1||Bi2212:1||tunnelling:1||GRAPHITE:1||GROWTH:1||collective transverse plasma modes:1||GAN:1||Macroscopic quantum tunneling:1||Fluctuation conductivity:1||Abovegap conductance jump:1||Josephson vortex motion:1||Intrinsic Josephson junctions:1||LAYERED SUPERCONDUCTORS:1||BI2SR2CACU2O8+Y:1||INTERFACES:1||BREAKDOWN:1||SYSTEMS:1||Anisotropy ratio:1||Josephson vortex:1||spin relaxation in superconductors:1||bibased single crystals:1||MESOSCOPIC PROXIMITY SUPERCONDUCTOR:1||reentrance of conductance:1||interlayer pair tunneling:1||JOSEPHSON:1||DISORDERED 2DIMENSIONAL SUPERCONDUCTORS:1||INDIUM FILMS:1||excited state:1||REGIME:1||triplet superconductivity:1||FILM:1||SCHOTTKY DIODES:1||peakdiphump structure:1||Kondo effect:1||REENTRANCE:1||Graphene:1||CONTACT:1||BERRYS PHASE:1||2DIMENSIONAL SUPERCONDUCTORS:1||Coulomb diamond:1||magnetic domain:1||spin injection:1||RESONANCE:1||plasma excitation modes:1||FLOW:1||OVERDOPED BI2SR2CACU2O8+DELTA:1||hole doping:1||chemical synthesis:1||phase transitions:1||superconductors:1||VORTEXGLASS SUPERCONDUCTIVITY:1||Kondorelated model:1||RADIATION:1||DOT:1||NANOBELTS:1||Complementarity:1||Closedloop AharonovBohm interferometer:1||pair breaking:1||interlayer phase fluctuation:1||MgB2 thin film:1||CONFINEMENT:1||WALLED CARBON NANOTUBES:1||TRANSITION:9||VORTICES:8||STATE:7||intrinsic Josephson junctions:7||SINGLECRYSTALS:7||JUNCTIONS:5||MODES:5||SUPERCURRENT:5||SUPERCONDUCTOR:5||CONDUCTANCE:5||HIGHTEMPERATURE SUPERCONDUCTORS:5||TRANSPORT:5||PHASE:5||FILMS:4||LOCALIZATION:4||SINGLE DIRAC CONE:4||WIRES:4||MAGNETICFIELD:4||STEPS:3||ELECTRONS:3||proximity effect:3||MODEL:3||ARRAYS:3||INTERFERENCE:3||fluxon dynamics:3||HETEROSTRUCTURES:3||INSULATOR:3||Andreev reflection:3||electronic transport:3||FISKE:3||superconductor:2||ZnO:2||quantum point contact:2||METAL:2||DYNAMICS:2||interlayer Josephson coupling:2||SUPERCONDUCTORS:2||YBA2CU3O7DELTA:2||LAYER:2||DOTS:2||quantum dot:2||Article:2||TRANSISTORS:2||CARBON NANOTUBES:2||GAP:2||MECHANISM:2||LINE:2||GIANT SHAPIRO STEPS:2||LAYERS:2||electron energy loss spectroscopy:2||physical phenomena:2||scanning electron microscopy:2||HGTE QUANTUMWELLS:2||BI2TE3:2||SPECTROSCOPY:2||PNJUNCTIONS:2||spinpolarized tunneling:2||INTRINSIC JOSEPHSONJUNCTIONS:2||FIELDS:2||positive magnetoresistance:2||dilute magnetic semiconductor:2||magnetic field:2||scanning transmission electron microscopy:2||QUANTUM OSCILLATIONS:2||TRANSPORTPROPERTIES:2||surface pair current:2||MAGNETORESISTANCE:2||NANORIBBONS:2||INSTABILITY:2||ANDREEV REFLECTION:2||microwave irradiation:2||vertical graphene josephson junction:2||BI2SE3:2||CONDUCTIVITY:2||highTc superconductors:2||DIMENSIONAL ELECTRONGAS:2||graphene:2||Topological insulators:2||Josephson coupling Fraunhofer interference pattern:2||FERROMAGNET:2||DEPENDENCE:2||DETECTOR:2||COHERENCE:2||INJECTION:2||GRAPHENE:1||JOSEPHSONJUNCTIONS:1||LAYERED SUPERCONDUCTOR:1||mode splitting:1||BEHAVIOR:1||spinpolarized transport:1||SUPERCONDUCTING TRANSITION:1||microwave response:1||PSEUDOGAP:1||phase coherence:1||TRANSITIONS:1||Long Josephson junction:1||Charge detection:1||collective resonance modes:1||plasma oscillation modes:1||Superconducting proximity effect:1||Iron pnictide superconductor:1||McMillanRowell oscillations:1||ferromagnetic microstructure:1||superradiant state:1||VOLTAGE:1||branch splitting:1||TENSOR:1||INTERCALATION:1||insitu fabrication:1||NDGAO3:1||DISORDERED METALS:1||GAUGE GLASS:1||LOWTEMPERATURE TRANSPORT:1||spontaneous spin polarization model:1||BIAS:1||emission of electromagnetic waves:1||YBA2CU3O7/PRBA2CU3O7 SUPERLATTICES:1||BOHM:1||SHAPIRO STEPS:1||superconductor/ferromagnet interface:1||OXIDE:1||ANDREEVREFLECTION:1||SinFeAsO single crystal:1||COLLECTIVE MOTION:1||ANGULARDEPENDENCE:1||SUPERCONDUCTIVITY:1||BILAYER GRAPHENE:1||PHOTOLUMINESCENT PROPERTIES:1||SUPERCONDUCTING WEAK LINKS:1||intrinsic Josephson junctions geometrical resonance:1||intrinsic Josephson junction:1||MESOSCOPIC SPINVALVE:1||Bi2212 single crystals:1||intrinsic junctions:1||ANDREEV REFLECTIONS:1||normalmetal/superconductor interface:1||IBI2SR2CACU2OY:1||THERMAL FLUCTUATIONS:1||MIXED STATE:1||BI2.15SR1.85CACU2O8+DELTA:1||intrinsic Josephson effects:1||CACUO:1||QUANTUM POINT CONTACTS:1||resonant tunneling state:1||coherence length:1||NANOWIRE:1||GATES:1||Phase line:1||Thermal activation:1||QUANTUMDOT:1||superconducting proximity effect:1||Andreev interferometer:1||WIRE:1||Josephsonvortexflow branches:1||Bi2212 cuprates:1||LATTICE:1||demannetization effect:1||SUPERCONDUCTING MIRRORS:1||GAS:1||VALLEY TRANSPORT:1||ELECTRODES:1||DEPENDENT TRANSPORT:1||BORNOPPENHEIMER APPROXIMATION:1||collective plasma oscillations:1||fluxon resonance steps:1||STACKS:1||COLLECTIVE DYNAMICS:1||PAIRING SYMMETRY:1||MUON SPIN ROTATION:1||DIMENSIONAL CROSSOVER:1||Bi2Sr2CaCu2Oy highTc superconductors:1||heterojunctions:1||nanostructures:1||surfaces and interfaces:1||QUANTUM TRANSPORT:1||MICROJUNCTIONS:1||RESONATORS:1||STATES:1||FIELD:1||FLUCTUATIONS:1||SCATTERING:1||mode splitting of Josephson vortexflow branches:1||2D superconductivity:1||TRANSISTOR:1||ENERGYGAP:1||SUPERLATTICES:1||IRONBASED SUPERCONDUCTORS:1||PHASEDEPENDENT RESISTANCE:1||QUANTUM PHASETRANSITIONS:1||ELECTRICFIELD:1||HIGH MAGNETICFIELDS:1||NANOWIRE HETEROSTRUCTURES:1||ZNO:1||pair breaking.:1||SUPERCONDUCTING PB:1||domain formation:1||FORCE MICROSCOPY:1||RELAXATION:1||PLASMA RESONANCE:1||coupled Josephson junctions:1||COPPEROXIDE SUPERCONDUCTORS:1||CROSSOVER:1||SIMULATIONS:1||LOWTEMPERATURE:1||CONDUCTORS:1||METALINSULATORTRANSITION:1||SEMICONDUCTOR:1||FIELDEFFECT TRANSISTORS:1||ZEROVOLTAGE STATE:1||constanttemperature interlayer tunneling spectroscopy:1||Josephson supercurrent:1||BIPOLAR SUPERCURRENT:1||Interaction between Josephson and pancake vortices:1||flux jump:1||coaxial heterojunction nanorod:1||Natural Josephson coupling:1||BI2SR2CACU2O8+DELTA:1||VORTEX FLOW:1||TC SUPERCONDUCTORS:1||charge imbalance:1||Andreev diffractometer:1||intercalation:1||surface junction:1||Bi2212:1||tunnelling:1||GRAPHITE:1||GROWTH:1||collective transverse plasma modes:1||GAN:1||Macroscopic quantum tunneling:1||Fluctuation conductivity:1||Abovegap conductance jump:1||Josephson vortex motion:1||Intrinsic Josephson junctions:1||LAYERED SUPERCONDUCTORS:1||BI2SR2CACU2O8+Y:1||INTERFACES:1||BREAKDOWN:1||SYSTEMS:1||Anisotropy ratio:1||Josephson vortex:1||spin relaxation in superconductors:1||bibased single crystals:1||MESOSCOPIC PROXIMITY SUPERCONDUCTOR:1||reentrance of conductance:1||interlayer pair tunneling:1||JOSEPHSON:1||DISORDERED 2DIMENSIONAL SUPERCONDUCTORS:1||INDIUM FILMS:1||excited state:1||REGIME:1||triplet superconductivity:1||FILM:1||SCHOTTKY DIODES:1||peakdiphump structure:1||Kondo effect:1||REENTRANCE:1||Graphene:1||CONTACT:1||BERRYS PHASE:1||2DIMENSIONAL SUPERCONDUCTORS:1||Coulomb diamond:1||magnetic domain:1||spin injection:1||RESONANCE:1||plasma excitation modes:1||FLOW:1||OVERDOPED BI2SR2CACU2O8+DELTA:1||hole doping:1||chemical synthesis:1||phase transitions:1||superconductors:1||VORTEXGLASS SUPERCONDUCTIVITY:1||Kondorelated model:1||RADIATION:1||DOT:1||NANOBELTS:1||Complementarity:1||Closedloop AharonovBohm interferometer:1||pair breaking:1||interlayer phase fluctuation:1||MgB2 thin film:1||CONFINEMENT:1||WALLED CARBON NANOTUBES:1||TRANSITION:9||VORTICES:8||STATE:7||intrinsic Josephson junctions:7||SINGLECRYSTALS:7||JUNCTIONS:5||MODES:5||SUPERCURRENT:5||SUPERCONDUCTOR:5||CONDUCTANCE:5||HIGHTEMPERATURE SUPERCONDUCTORS:5||TRANSPORT:5||PHASE:5||FILMS:4||LOCALIZATION:4||SINGLE DIRAC CONE:4||WIRES:4||MAGNETICFIELD:4||STEPS:3||ELECTRONS:3||proximity effect:3||MODEL:3||ARRAYS:3||INTERFERENCE:3||fluxon dynamics:3||HETEROSTRUCTURES:3||INSULATOR:3||Andreev reflection:3||electronic transport:3||FISKE:3||superconductor:2||ZnO:2||quantum point contact:2||METAL:2||DYNAMICS:2||interlayer Josephson coupling:2||SUPERCONDUCTORS:2||YBA2CU3O7DELTA:2||LAYER:2||DOTS:2||quantum dot:2||Article:2||TRANSISTORS:2||CARBON NANOTUBES:2||GAP:2||MECHANISM:2||LINE:2||GIANT SHAPIRO STEPS:2||LAYERS:2||electron energy loss spectroscopy:2||physical phenomena:2||scanning electron microscopy:2||HGTE QUANTUMWELLS:2||BI2TE3:2||SPECTROSCOPY:2||PNJUNCTIONS:2||spinpolarized tunneling:2||INTRINSIC JOSEPHSONJUNCTIONS:2||FIELDS:2||positive magnetoresistance:2||dilute magnetic semiconductor:2||magnetic field:2||scanning transmission electron microscopy:2||QUANTUM OSCILLATIONS:2||TRANSPORTPROPERTIES:2||surface pair current:2||MAGNETORESISTANCE:2||NANORIBBONS:2||INSTABILITY:2||ANDREEV REFLECTION:2||microwave irradiation:2||vertical graphene josephson junction:2||BI2SE3:2||CONDUCTIVITY:2||highTc superconductors:2||DIMENSIONAL ELECTRONGAS:2||graphene:2||Topological insulators:2||Josephson coupling Fraunhofer interference pattern:2||FERROMAGNET:2||DEPENDENCE:2||DETECTOR:2||COHERENCE:2||INJECTION:2||GRAPHENE:1||JOSEPHSONJUNCTIONS:1||LAYERED SUPERCONDUCTOR:1||mode splitting:1||BEHAVIOR:1||spinpolarized transport:1||SUPERCONDUCTING TRANSITION:1||microwave response:1||PSEUDOGAP:1||phase coherence:1||TRANSITIONS:1||Long Josephson junction:1||Charge detection:1||collective resonance modes:1||plasma oscillation modes:1||Superconducting proximity effect:1||Iron pnictide superconductor:1||McMillanRowell oscillations:1||ferromagnetic microstructure:1||superradiant state:1||VOLTAGE:1||branch splitting:1||TENSOR:1||INTERCALATION:1||insitu fabrication:1||NDGAO3:1||DISORDERED METALS:1||GAUGE GLASS:1||LOWTEMPERATURE TRANSPORT:1||spontaneous spin polarization model:1||BIAS:1||emission of electromagnetic waves:1||YBA2CU3O7/PRBA2CU3O7 SUPERLATTICES:1||BOHM:1||SHAPIRO STEPS:1||superconductor/ferromagnet interface:1||OXIDE:1||ANDREEVREFLECTION:1||SinFeAsO single crystal:1||COLLECTIVE MOTION:1||ANGULARDEPENDENCE:1||SUPERCONDUCTIVITY:1||BILAYER GRAPHENE:1||PHOTOLUMINESCENT PROPERTIES:1||SUPERCONDUCTING WEAK LINKS:1||intrinsic Josephson junctions geometrical resonance:1||intrinsic Josephson junction:1||MESOSCOPIC SPINVALVE:1||Bi2212 single crystals:1||intrinsic junctions:1||ANDREEV REFLECTIONS:1||normalmetal/superconductor interface:1||IBI2SR2CACU2OY:1||THERMAL FLUCTUATIONS:1||MIXED STATE:1||BI2.15SR1.85CACU2O8+DELTA:1||intrinsic Josephson effects:1||CACUO:1||QUANTUM POINT CONTACTS:1||resonant tunneling state:1||coherence length:1||NANOWIRE:1||GATES:1||Phase line:1||Thermal activation:1||QUANTUMDOT:1||superconducting proximity effect:1||Andreev interferometer:1||WIRE:1||Josephsonvortexflow branches:1||Bi2212 cuprates:1||LATTICE:1||demannetization effect:1||SUPERCONDUCTING MIRRORS:1||GAS:1||VALLEY TRANSPORT:1||ELECTRODES:1||DEPENDENT TRANSPORT:1||BORNOPPENHEIMER APPROXIMATION:1||collective plasma oscillations:1||fluxon resonance steps:1||STACKS:1||COLLECTIVE DYNAMICS:1||PAIRING SYMMETRY:1||MUON SPIN ROTATION:1||DIMENSIONAL CROSSOVER:1||Bi2Sr2CaCu2Oy highTc superconductors:1||heterojunctions:1||nanostructures:1||surfaces and interfaces:1||QUANTUM TRANSPORT:1||MICROJUNCTIONS:1||RESONATORS:1||STATES:1||FIELD:1||FLUCTUATIONS:1||SCATTERING:1||mode splitting of Josephson vortexflow branches:1||2D superconductivity:1||TRANSISTOR:1||ENERGYGAP:1||SUPERLATTICES:1||IRONBASED SUPERCONDUCTORS:1||PHASEDEPENDENT RESISTANCE:1||QUANTUM PHASETRANSITIONS:1||ELECTRICFIELD:1||HIGH MAGNETICFIELDS:1||NANOWIRE HETEROSTRUCTURES:1||ZNO:1||pair breaking.:1||SUPERCONDUCTING PB:1||domain formation:1||FORCE MICROSCOPY:1||RELAXATION:1||PLASMA RESONANCE:1||coupled Josephson junctions:1||COPPEROXIDE SUPERCONDUCTORS:1||CROSSOVER:1||SIMULATIONS:1||LOWTEMPERATURE:1||CONDUCTORS:1||METALINSULATORTRANSITION:1||SEMICONDUCTOR:1||FIELDEFFECT TRANSISTORS:1||ZEROVOLTAGE STATE:1||constanttemperature interlayer tunneling spectroscopy:1||Josephson supercurrent:1||BIPOLAR SUPERCURRENT:1||Interaction between Josephson and pancake vortices:1||flux jump:1||coaxial heterojunction nanorod:1||Natural Josephson coupling:1||BI2SR2CACU2O8+DELTA:1||VORTEX FLOW:1||TC SUPERCONDUCTORS:1||charge imbalance:1||Andreev diffractometer:1||intercalation:1||surface junction:1||Bi2212:1||tunnelling:1||GRAPHITE:1||GROWTH:1||collective transverse plasma modes:1||GAN:1||Macroscopic quantum tunneling:1||Fluctuation conductivity:1||Abovegap conductance jump:1||Josephson vortex motion:1||Intrinsic Josephson junctions:1||LAYERED SUPERCONDUCTORS:1||BI2SR2CACU2O8+Y:1||INTERFACES:1||BREAKDOWN:1||SYSTEMS:1||Anisotropy ratio:1||Josephson vortex:1||spin relaxation in superconductors:1||bibased single crystals:1||MESOSCOPIC PROXIMITY SUPERCONDUCTOR:1||reentrance of conductance:1||interlayer pair tunneling:1||JOSEPHSON:1||DISORDERED 2DIMENSIONAL SUPERCONDUCTORS:1||INDIUM FILMS:1||excited state:1||REGIME:1||triplet superconductivity:1||FILM:1||SCHOTTKY DIODES:1||peakdiphump structure:1||Kondo effect:1||REENTRANCE:1||Graphene:1||CONTACT:1||BERRYS PHASE:1||2DIMENSIONAL SUPERCONDUCTORS:1||Coulomb diamond:1||magnetic domain:1||spin injection:1||RESONANCE:1||plasma excitation modes:1||FLOW:1||OVERDOPED BI2SR2CACU2O8+DELTA:1||hole doping:1||chemical synthesis:1||phase transitions:1||superconductors:1||VORTEXGLASS SUPERCONDUCTIVITY:1||Kondorelated model:1||RADIATION:1||DOT:1||NANOBELTS:1||Complementarity:1||Closedloop AharonovBohm interferometer:1||pair breaking:1||interlayer phase fluctuation:1||MgB2 thin film:1||CONFINEMENT:1||WALLED CARBON NANOTUBES:1||TRANSITION:9||VORTICES:8||STATE:7||intrinsic Josephson junctions:7||SINGLECRYSTALS:7||JUNCTIONS:5||MODES:5||SUPERCURRENT:5||SUPERCONDUCTOR:5||CONDUCTANCE:5||HIGHTEMPERATURE SUPERCONDUCTORS:5||TRANSPORT:5||PHASE:5||FILMS:4||LOCALIZATION:4||SINGLE DIRAC CONE:4||WIRES:4||MAGNETICFIELD:4||STEPS:3||ELECTRONS:3||proximity effect:3||MODEL:3||ARRAYS:3||INTERFERENCE:3||fluxon dynamics:3||HETEROSTRUCTURES:3||INSULATOR:3||Andreev reflection:3||electronic transport:3||FISKE:3||superconductor:2||ZnO:2||quantum point contact:2||METAL:2||DYNAMICS:2||interlayer Josephson coupling:2||SUPERCONDUCTORS:2||YBA2CU3O7DELTA:2||LAYER:2||DOTS:2||quantum dot:2||Article:2||TRANSISTORS:2||CARBON NANOTUBES:2||GAP:2||MECHANISM:2||LINE:2||GIANT SHAPIRO STEPS:2||LAYERS:2||electron energy loss spectroscopy:2||physical phenomena:2||scanning electron microscopy:2||HGTE QUANTUMWELLS:2||BI2TE3:2||SPECTROSCOPY:2||PNJUNCTIONS:2||spinpolarized tunneling:2||INTRINSIC JOSEPHSONJUNCTIONS:2||FIELDS:2||positive magnetoresistance:2||dilute magnetic semiconductor:2||magnetic field:2||scanning transmission electron microscopy:2||QUANTUM OSCILLATIONS:2||TRANSPORTPROPERTIES:2||surface pair current:2||MAGNETORESISTANCE:2||NANORIBBONS:2||INSTABILITY:2||ANDREEV REFLECTION:2||microwave irradiation:2||vertical graphene josephson junction:2||BI2SE3:2||CONDUCTIVITY:2||highTc superconductors:2||DIMENSIONAL ELECTRONGAS:2||graphene:2||Topological insulators:2||Josephson coupling Fraunhofer interference pattern:2||FERROMAGNET:2||DEPENDENCE:2||DETECTOR:2||COHERENCE:2||INJECTION:2||GRAPHENE:1||JOSEPHSONJUNCTIONS:1||LAYERED SUPERCONDUCTOR:1||mode splitting:1||BEHAVIOR:1||spinpolarized transport:1||SUPERCONDUCTING TRANSITION:1||microwave response:1||PSEUDOGAP:1||phase coherence:1||TRANSITIONS:1||Long Josephson junction:1||Charge detection:1||collective resonance modes:1||plasma oscillation modes:1||Superconducting proximity effect:1||Iron pnictide superconductor:1||McMillanRowell oscillations:1||ferromagnetic microstructure:1||superradiant state:1||VOLTAGE:1||branch splitting:1||TENSOR:1||INTERCALATION:1||insitu fabrication:1||NDGAO3:1||DISORDERED METALS:1||GAUGE GLASS:1||LOWTEMPERATURE TRANSPORT:1||spontaneous spin polarization model:1||BIAS:1||emission of electromagnetic waves:1||YBA2CU3O7/PRBA2CU3O7 SUPERLATTICES:1||BOHM:1||SHAPIRO STEPS:1||superconductor/ferromagnet interface:1||OXIDE:1||ANDREEVREFLECTION:1||SinFeAsO single crystal:1||COLLECTIVE MOTION:1||ANGULARDEPENDENCE:1||SUPERCONDUCTIVITY:1||BILAYER GRAPHENE:1||PHOTOLUMINESCENT PROPERTIES:1||SUPERCONDUCTING WEAK LINKS:1||intrinsic Josephson junctions geometrical resonance:1||intrinsic Josephson junction:1||MESOSCOPIC SPINVALVE:1||Bi2212 single crystals:1||intrinsic junctions:1||ANDREEV REFLECTIONS:1||normalmetal/superconductor interface:1||IBI2SR2CACU2OY:1||THERMAL FLUCTUATIONS:1||MIXED STATE:1||BI2.15SR1.85CACU2O8+DELTA:1||intrinsic Josephson effects:1||CACUO:1||QUANTUM POINT CONTACTS:1||resonant tunneling state:1||coherence length:1||NANOWIRE:1||GATES:1||Phase line:1||Thermal activation:1||QUANTUMDOT:1||superconducting proximity effect:1||Andreev interferometer:1||WIRE:1||Josephsonvortexflow branches:1||Bi2212 cuprates:1||LATTICE:1||demannetization effect:1||SUPERCONDUCTING MIRRORS:1||GAS:1||VALLEY TRANSPORT:1||ELECTRODES:1||DEPENDENT TRANSPORT:1||BORNOPPENHEIMER APPROXIMATION:1||collective plasma oscillations:1||fluxon resonance steps:1||STACKS:1||COLLECTIVE DYNAMICS:1||PAIRING SYMMETRY:1||MUON SPIN ROTATION:1||DIMENSIONAL CROSSOVER:1||Bi2Sr2CaCu2Oy highTc superconductors:1||heterojunctions:1||nanostructures:1||surfaces and interfaces:1||QUANTUM TRANSPORT:1||MICROJUNCTIONS:1||RESONATORS:1||STATES:1||FIELD:1||FLUCTUATIONS:1||SCATTERING:1||mode splitting of Josephson vortexflow branches:1||2D superconductivity:1||TRANSISTOR:1||ENERGYGAP:1||SUPERLATTICES:1||IRONBASED SUPERCONDUCTORS:1||PHASEDEPENDENT RESISTANCE:1||QUANTUM PHASETRANSITIONS:1||ELECTRICFIELD:1||HIGH MAGNETICFIELDS:1||NANOWIRE HETEROSTRUCTURES:1||ZNO:1||pair breaking.:1||SUPERCONDUCTING PB:1||domain formation:1||FORCE MICROSCOPY:1||RELAXATION:1||PLASMA RESONANCE:1||coupled Josephson junctions:1||COPPEROXIDE SUPERCONDUCTORS:1||CROSSOVER:1||SIMULATIONS:1||LOWTEMPERATURE:1||CONDUCTORS:1||METALINSULATORTRANSITION:1||SEMICONDUCTOR:1||FIELDEFFECT TRANSISTORS:1||ZEROVOLTAGE STATE:1||constanttemperature interlayer tunneling spectroscopy:1||Josephson supercurrent:1||BIPOLAR SUPERCURRENT:1||Interaction between Josephson and pancake vortices:1||flux jump:1||coaxial heterojunction nanorod:1||Natural Josephson coupling:1||BI2SR2CACU2O8+DELTA:1||VORTEX FLOW:1||TC SUPERCONDUCTORS:1||charge imbalance:1||Andreev diffractometer:1||intercalation:1||surface junction:1||Bi2212:1||tunnelling:1||GRAPHITE:1||GROWTH:1||collective transverse plasma modes:1||GAN:1||Macroscopic quantum tunneling:1||Fluctuation conductivity:1||Abovegap conductance jump:1||Josephson vortex motion:1||Intrinsic Josephson junctions:1||LAYERED SUPERCONDUCTORS:1||BI2SR2CACU2O8+Y:1||INTERFACES:1||BREAKDOWN:1||SYSTEMS:1||Anisotropy ratio:1||Josephson vortex:1||spin relaxation in superconductors:1||bibased single crystals:1||MESOSCOPIC PROXIMITY SUPERCONDUCTOR:1||reentrance of conductance:1||interlayer pair tunneling:1||JOSEPHSON:1||DISORDERED 2DIMENSIONAL SUPERCONDUCTORS:1||INDIUM FILMS:1||excited state:1||REGIME:1||triplet superconductivity:1||FILM:1||SCHOTTKY DIODES:1||peakdiphump structure:1||Kondo effect:1||REENTRANCE:1||Graphene:1||CONTACT:1||BERRYS PHASE:1||2DIMENSIONAL SUPERCONDUCTORS:1||Coulomb diamond:1||magnetic domain:1||spin injection:1||RESONANCE:1||plasma excitation modes:1||FLOW:1||OVERDOPED BI2SR2CACU2O8+DELTA:1||hole doping:1||chemical synthesis:1||phase transitions:1||superconductors:1||VORTEXGLASS SUPERCONDUCTIVITY:1||Kondorelated model:1||RADIATION:1||DOT:1||NANOBELTS:1||Complementarity:1||Closedloop AharonovBohm interferometer:1||pair breaking:1||interlayer phase fluctuation:1||MgB2 thin film:1||CONFINEMENT:1||WALLED CARBON NANOTUBES:1||TRANSITION:9||VORTICES:8||STATE:7||intrinsic Josephson junctions:7||SINGLECRYSTALS:7||JUNCTIONS:5||MODES:5||SUPERCURRENT:5||SUPERCONDUCTOR:5||CONDUCTANCE:5||HIGHTEMPERATURE SUPERCONDUCTORS:5||TRANSPORT:5||PHASE:5||FILMS:4||LOCALIZATION:4||SINGLE DIRAC CONE:4||WIRES:4||MAGNETICFIELD:4||STEPS:3||ELECTRONS:3||proximity effect:3||MODEL:3||ARRAYS:3||INTERFERENCE:3||fluxon dynamics:3||HETEROSTRUCTURES:3||INSULATOR:3||Andreev reflection:3||electronic transport:3||FISKE:3||superconductor:2||ZnO:2||quantum point contact:2||METAL:2||DYNAMICS:2||interlayer Josephson coupling:2||SUPERCONDUCTORS:2||YBA2CU3O7DELTA:2||LAYER:2||DOTS:2||quantum dot:2||Article:2||TRANSISTORS:2||CARBON NANOTUBES:2||GAP:2||MECHANISM:2||LINE:2||GIANT SHAPIRO STEPS:2||LAYERS:2||electron energy loss spectroscopy:2||physical phenomena:2||scanning electron microscopy:2||HGTE QUANTUMWELLS:2||BI2TE3:2||SPECTROSCOPY:2||PNJUNCTIONS:2||spinpolarized tunneling:2||INTRINSIC JOSEPHSONJUNCTIONS:2||FIELDS:2||positive magnetoresistance:2||dilute magnetic semiconductor:2||magnetic field:2||scanning transmission electron microscopy:2||QUANTUM OSCILLATIONS:2||TRANSPORTPROPERTIES:2||surface pair current:2||MAGNETORESISTANCE:2||NANORIBBONS:2||INSTABILITY:2||ANDREEV REFLECTION:2||microwave irradiation:2||vertical graphene josephson junction:2||BI2SE3:2||CONDUCTIVITY:2||highTc superconductors:2||DIMENSIONAL ELECTRONGAS:2||graphene:2||Topological insulators:2||Josephson coupling Fraunhofer interference pattern:2||FERROMAGNET:2||DEPENDENCE:2||DETECTOR:2||COHERENCE:2||INJECTION:2||GRAPHENE:1||JOSEPHSONJUNCTIONS:1||LAYERED SUPERCONDUCTOR:1||mode splitting:1||BEHAVIOR:1||spinpolarized transport:1||SUPERCONDUCTING TRANSITION:1||microwave response:1||PSEUDOGAP:1||phase coherence:1||TRANSITIONS:1||Long Josephson junction:1||Charge detection:1||collective resonance modes:1||plasma oscillation modes:1||Superconducting proximity effect:1||Iron pnictide superconductor:1||McMillanRowell oscillations:1||ferromagnetic microstructure:1||superradiant state:1||VOLTAGE:1||branch splitting:1||TENSOR:1||INTERCALATION:1||insitu fabrication:1||NDGAO3:1||DISORDERED METALS:1||GAUGE GLASS:1||LOWTEMPERATURE TRANSPORT:1||spontaneous spin polarization model:1||BIAS:1||emission of electromagnetic waves:1||YBA2CU3O7/PRBA2CU3O7 SUPERLATTICES:1||BOHM:1||SHAPIRO STEPS:1||superconductor/ferromagnet interface:1||OXIDE:1||ANDREEVREFLECTION:1||SinFeAsO single crystal:1||COLLECTIVE MOTION:1||ANGULARDEPENDENCE:1||SUPERCONDUCTIVITY:1||BILAYER GRAPHENE:1||PHOTOLUMINESCENT PROPERTIES:1||SUPERCONDUCTING WEAK LINKS:1||intrinsic Josephson junctions geometrical resonance:1||intrinsic Josephson junction:1||MESOSCOPIC SPINVALVE:1||Bi2212 single crystals:1||intrinsic junctions:1||ANDREEV REFLECTIONS:1||normalmetal/superconductor interface:1||IBI2SR2CACU2OY:1||THERMAL FLUCTUATIONS:1||MIXED STATE:1||BI2.15SR1.85CACU2O8+DELTA:1||intrinsic Josephson effects:1||CACUO:1||QUANTUM POINT CONTACTS:1||resonant tunneling state:1||coherence length:1||NANOWIRE:1||GATES:1||Phase line:1||Thermal activation:1||QUANTUMDOT:1||superconducting proximity effect:1||Andreev interferometer:1||WIRE:1||Josephsonvortexflow branches:1||Bi2212 cuprates:1||LATTICE:1||demannetization effect:1||SUPERCONDUCTING MIRRORS:1||GAS:1||VALLEY TRANSPORT:1||ELECTRODES:1||DEPENDENT TRANSPORT:1||BORNOPPENHEIMER APPROXIMATION:1||collective plasma oscillations:1||fluxon resonance steps:1||STACKS:1||COLLECTIVE DYNAMICS:1||PAIRING SYMMETRY:1||MUON SPIN ROTATION:1||DIMENSIONAL CROSSOVER:1||Bi2Sr2CaCu2Oy highTc superconductors:1||heterojunctions:1||nanostructures:1||surfaces and interfaces:1||QUANTUM TRANSPORT:1||MICROJUNCTIONS:1||RESONATORS:1||STATES:1||FIELD:1||FLUCTUATIONS:1||SCATTERING:1||mode splitting of Josephson vortexflow branches:1||2D superconductivity:1||TRANSISTOR:1||ENERGYGAP:1||SUPERLATTICES:1||IRONBASED SUPERCONDUCTORS:1||PHASEDEPENDENT RESISTANCE:1||QUANTUM PHASETRANSITIONS:1||ELECTRICFIELD:1||HIGH MAGNETICFIELDS:1||NANOWIRE HETEROSTRUCTURES:1||ZNO:1||pair breaking.:1||SUPERCONDUCTING PB:1||domain formation:1||FORCE MICROSCOPY:1||RELAXATION:1||PLASMA RESONANCE:1||coupled Josephson junctions:1||COPPEROXIDE SUPERCONDUCTORS:1||CROSSOVER:1||SIMULATIONS:1||LOWTEMPERATURE:1||CONDUCTORS:1||METALINSULATORTRANSITION:1||SEMICONDUCTOR:1||FIELDEFFECT TRANSISTORS:1||ZEROVOLTAGE STATE:1||constanttemperature interlayer tunneling spectroscopy:1||Josephson supercurrent:1||BIPOLAR SUPERCURRENT:1||Interaction between Josephson and pancake vortices:1||flux jump:1||coaxial heterojunction nanorod:1||Natural Josephson coupling:1||BI2SR2CACU2O8+DELTA:1||VORTEX FLOW:1||TC SUPERCONDUCTORS:1||charge imbalance:1||Andreev diffractometer:1||intercalation:1||surface junction:1||Bi2212:1||tunnelling:1||GRAPHITE:1||GROWTH:1||collective transverse plasma modes:1||GAN:1||Macroscopic quantum tunneling:1||Fluctuation conductivity:1||Abovegap conductance jump:1||Josephson vortex motion:1||Intrinsic Josephson junctions:1||LAYERED SUPERCONDUCTORS:1||BI2SR2CACU2O8+Y:1||INTERFACES:1||BREAKDOWN:1||SYSTEMS:1||Anisotropy ratio:1||Josephson vortex:1||spin relaxation in superconductors:1||bibased single crystals:1||MESOSCOPIC PROXIMITY SUPERCONDUCTOR:1||reentrance of conductance:1||interlayer pair tunneling:1||JOSEPHSON:1||DISORDERED 2DIMENSIONAL SUPERCONDUCTORS:1||INDIUM FILMS:1||excited state:1||REGIME:1||triplet superconductivity:1||FILM:1||SCHOTTKY DIODES:1||peakdiphump structure:1||Kondo effect:1||REENTRANCE:1||Graphene:1||CONTACT:1||BERRYS PHASE:1||2DIMENSIONAL SUPERCONDUCTORS:1||Coulomb diamond:1||magnetic domain:1||spin injection:1||RESONANCE:1||plasma excitation modes:1||FLOW:1||OVERDOPED BI2SR2CACU2O8+DELTA:1||hole doping:1||chemical synthesis:1||phase transitions:1||superconductors:1||VORTEXGLASS SUPERCONDUCTIVITY:1||Kondorelated model:1||RADIATION:1||DOT:1||NANOBELTS:1||Complementarity:1||Closedloop AharonovBohm interferometer:1||pair breaking:1||interlayer phase fluctuation:1||MgB2 thin film:1||CONFINEMENT:1||WALLED CARBON NANOTUBES:1||TRANSITION:9||VORTICES:8||STATE:7||intrinsic Josephson junctions:7||SINGLECRYSTALS:7||JUNCTIONS:5||MODES:5||SUPERCURRENT:5||SUPERCONDUCTOR:5||CONDUCTANCE:5||HIGHTEMPERATURE SUPERCONDUCTORS:5||TRANSPORT:5||PHASE:5||FILMS:4||LOCALIZATION:4||SINGLE DIRAC CONE:4||WIRES:4||MAGNETICFIELD:4||STEPS:3||ELECTRONS:3||proximity effect:3||MODEL:3||ARRAYS:3||INTERFERENCE:3||fluxon dynamics:3||HETEROSTRUCTURES:3||INSULATOR:3||Andreev reflection:3||electronic transport:3||FISKE:3||superconductor:2||ZnO:2||quantum point contact:2||METAL:2||DYNAMICS:2||interlayer Josephson coupling:2||SUPERCONDUCTORS:2||YBA2CU3O7DELTA:2||LAYER:2||DOTS:2||quantum dot:2||Article:2||TRANSISTORS:2||CARBON NANOTUBES:2||GAP:2||MECHANISM:2||LINE:2||GIANT SHAPIRO STEPS:2||LAYERS:2||electron energy loss spectroscopy:2||physical phenomena:2||scanning electron microscopy:2||HGTE QUANTUMWELLS:2||BI2TE3:2||SPECTROSCOPY:2||PNJUNCTIONS:2||spinpolarized tunneling:2||INTRINSIC JOSEPHSONJUNCTIONS:2||FIELDS:2||positive magnetoresistance:2||dilute magnetic semiconductor:2||magnetic field:2||scanning transmission electron microscopy:2||QUANTUM OSCILLATIONS:2||TRANSPORTPROPERTIES:2||surface pair current:2||MAGNETORESISTANCE:2||NANORIBBONS:2||INSTABILITY:2||ANDREEV REFLECTION:2||microwave irradiation:2||vertical graphene josephson junction:2||BI2SE3:2||CONDUCTIVITY:2||highTc superconductors:2||DIMENSIONAL ELECTRONGAS:2||graphene:2||Topological insulators:2||Josephson coupling Fraunhofer interference pattern:2||FERROMAGNET:2||DEPENDENCE:2||DETECTOR:2||COHERENCE:2||INJECTION:2||GRAPHENE:1||JOSEPHSONJUNCTIONS:1||LAYERED SUPERCONDUCTOR:1||mode splitting:1||BEHAVIOR:1||spinpolarized transport:1||SUPERCONDUCTING TRANSITION:1||microwave response:1||PSEUDOGAP:1||phase coherence:1||TRANSITIONS:1||Long Josephson junction:1||Charge detection:1||collective resonance modes:1||plasma oscillation modes:1||Superconducting proximity effect:1||Iron pnictide superconductor:1||McMillanRowell oscillations:1||ferromagnetic microstructure:1||superradiant state:1||VOLTAGE:1||branch splitting:1||TENSOR:1||INTERCALATION:1||insitu fabrication:1||NDGAO3:1||DISORDERED METALS:1||GAUGE GLASS:1||LOWTEMPERATURE TRANSPORT:1||spontaneous spin polarization model:1||BIAS:1||emission of electromagnetic waves:1||YBA2CU3O7/PRBA2CU3O7 SUPERLATTICES:1||BOHM:1||SHAPIRO STEPS:1||superconductor/ferromagnet interface:1||OXIDE:1||ANDREEVREFLECTION:1||SinFeAsO single crystal:1||COLLECTIVE MOTION:1||ANGULARDEPENDENCE:1||SUPERCONDUCTIVITY:1||BILAYER GRAPHENE:1||PHOTOLUMINESCENT PROPERTIES:1||SUPERCONDUCTING WEAK LINKS:1||intrinsic Josephson junctions geometrical resonance:1||intrinsic Josephson junction:1||MESOSCOPIC SPINVALVE:1||Bi2212 single crystals:1||intrinsic junctions:1||ANDREEV REFLECTIONS:1||normalmetal/superconductor interface:1||IBI2SR2CACU2OY:1||THERMAL FLUCTUATIONS:1||MIXED STATE:1||BI2.15SR1.85CACU2O8+DELTA:1||intrinsic Josephson effects:1||CACUO:1||QUANTUM POINT CONTACTS:1||resonant tunneling state:1||coherence length:1||NANOWIRE:1||GATES:1||Phase line:1||Thermal activation:1||QUANTUMDOT:1||superconducting proximity effect:1||Andreev interferometer:1||WIRE:1||Josephsonvortexflow branches:1||Bi2212 cuprates:1||LATTICE:1||demannetization effect:1||SUPERCONDUCTING MIRRORS:1||GAS:1||VALLEY TRANSPORT:1||ELECTRODES:1||DEPENDENT TRANSPORT:1||BORNOPPENHEIMER APPROXIMATION:1||collective plasma oscillations:1||fluxon resonance steps:1||STACKS:1||COLLECTIVE DYNAMICS:1||PAIRING SYMMETRY:1||MUON SPIN ROTATION:1||DIMENSIONAL CROSSOVER:1||Bi2Sr2CaCu2Oy highTc superconductors:1||heterojunctions:1||nanostructures:1||surfaces and interfaces:1||QUANTUM TRANSPORT:1||MICROJUNCTIONS:1||RESONATORS:1||STATES:1||FIELD:1||FLUCTUATIONS:1||SCATTERING:1||mode splitting of Josephson vortexflow branches:1||2D superconductivity:1||TRANSISTOR:1||ENERGYGAP:1||SUPERLATTICES:1||IRONBASED SUPERCONDUCTORS:1||PHASEDEPENDENT RESISTANCE:1||QUANTUM PHASETRANSITIONS:1||ELECTRICFIELD:1||HIGH MAGNETICFIELDS:1||NANOWIRE HETEROSTRUCTURES:1||ZNO:1||pair breaking.:1||SUPERCONDUCTING PB:1||domain formation:1||FORCE MICROSCOPY:1||RELAXATION:1||PLASMA RESONANCE:1||coupled Josephson junctions:1||COPPEROXIDE SUPERCONDUCTORS:1||CROSSOVER:1||SIMULATIONS:1||LOWTEMPERATURE:1||CONDUCTORS:1||METALINSULATORTRANSITION:1||SEMICONDUCTOR:1||FIELDEFFECT TRANSISTORS:1||ZEROVOLTAGE STATE:1||constanttemperature interlayer tunneling spectroscopy:1||Josephson supercurrent:1||BIPOLAR SUPERCURRENT:1||Interaction between Josephson and pancake vortices:1||flux jump:1||coaxial heterojunction nanorod:1||Natural Josephson coupling:1||BI2SR2CACU2O8+DELTA:1||VORTEX FLOW:1||TC SUPERCONDUCTORS:1||charge imbalance:1||Andreev diffractometer:1||intercalation:1||surface junction:1||Bi2212:1||tunnelling:1||GRAPHITE:1||GROWTH:1||collective transverse plasma modes:1||GAN:1||Macroscopic quantum tunneling:1||Fluctuation conductivity:1||Abovegap conductance jump:1||Josephson vortex motion:1||Intrinsic Josephson junctions:1||LAYERED SUPERCONDUCTORS:1||BI2SR2CACU2O8+Y:1||INTERFACES:1||BREAKDOWN:1||SYSTEMS:1||Anisotropy ratio:1||Josephson vortex:1||spin relaxation in superconductors:1||bibased single crystals:1||MESOSCOPIC PROXIMITY SUPERCONDUCTOR:1||reentrance of conductance:1||interlayer pair tunneling:1||JOSEPHSON:1||DISORDERED 2DIMENSIONAL SUPERCONDUCTORS:1||INDIUM FILMS:1||excited state:1||REGIME:1||triplet superconductivity:1||FILM:1||SCHOTTKY DIODES:1||peakdiphump structure:1||Kondo effect:1||REENTRANCE:1||Graphene:1||CONTACT:1||BERRYS PHASE:1||2DIMENSIONAL SUPERCONDUCTORS:1||Coulomb diamond:1||magnetic domain:1||spin injection:1||RESONANCE:1||plasma excitation modes:1||FLOW:1||OVERDOPED BI2SR2CACU2O8+DELTA:1||hole doping:1||chemical synthesis:1||phase transitions:1||superconductors:1||VORTEXGLASS SUPERCONDUCTIVITY:1||Kondorelated model:1||RADIATION:1||DOT:1||NANOBELTS:1||Complementarity:1||Closedloop AharonovBohm interferometer:1||pair breaking:1||interlayer phase fluctuation:1||MgB2 thin film:1||CONFINEMENT:1||WALLED CARBON NANOTUBES:1||TRANSITION:9||VORTICES:8||STATE:7||intrinsic Josephson junctions:7||SINGLECRYSTALS:7||JUNCTIONS:5||MODES:5||SUPERCURRENT:5||SUPERCONDUCTOR:5||CONDUCTANCE:5||HIGHTEMPERATURE SUPERCONDUCTORS:5||TRANSPORT:5||PHASE:5||FILMS:4||LOCALIZATION:4||SINGLE DIRAC CONE:4||WIRES:4||MAGNETICFIELD:4||STEPS:3||ELECTRONS:3||proximity effect:3||MODEL:3||ARRAYS:3||INTERFERENCE:3||fluxon dynamics:3||HETEROSTRUCTURES:3||INSULATOR:3||Andreev reflection:3||electronic transport:3||FISKE:3||superconductor:2||ZnO:2||quantum point contact:2||METAL:2||DYNAMICS:2||interlayer Josephson coupling:2||SUPERCONDUCTORS:2||YBA2CU3O7DELTA:2||LAYER:2||DOTS:2||quantum dot:2||Article:2||TRANSISTORS:2||CARBON NANOTUBES:2||GAP:2||MECHANISM:2||LINE:2||GIANT SHAPIRO STEPS:2||LAYERS:2||electron energy loss spectroscopy:2||physical phenomena:2||scanning electron microscopy:2||HGTE QUANTUMWELLS:2||BI2TE3:2||SPECTROSCOPY:2||PNJUNCTIONS:2||spinpolarized tunneling:2||INTRINSIC JOSEPHSONJUNCTIONS:2||FIELDS:2||positive magnetoresistance:2||dilute magnetic semiconductor:2||magnetic field:2||scanning transmission electron microscopy:2||QUANTUM OSCILLATIONS:2||TRANSPORTPROPERTIES:2||surface pair current:2||MAGNETORESISTANCE:2||NANORIBBONS:2||INSTABILITY:2||ANDREEV REFLECTION:2||microwave irradiation:2||vertical graphene josephson junction:2||BI2SE3:2||CONDUCTIVITY:2||highTc superconductors:2||DIMENSIONAL ELECTRONGAS:2||graphene:2||Topological insulators:2||Josephson coupling Fraunhofer interference pattern:2||FERROMAGNET:2||DEPENDENCE:2||DETECTOR:2||COHERENCE:2||INJECTION:2||GRAPHENE:1||JOSEPHSONJUNCTIONS:1||LAYERED SUPERCONDUCTOR:1||mode splitting:1||BEHAVIOR:1||spinpolarized transport:1||SUPERCONDUCTING TRANSITION:1||microwave response:1||PSEUDOGAP:1||phase coherence:1||TRANSITIONS:1||Long Josephson junction:1||Charge detection:1||collective resonance modes:1||plasma oscillation modes:1||Superconducting proximity effect:1||Iron pnictide superconductor:1||McMillanRowell oscillations:1||ferromagnetic microstructure:1||superradiant state:1||VOLTAGE:1||branch splitting:1||TENSOR:1||INTERCALATION:1||insitu fabrication:1||NDGAO3:1||DISORDERED METALS:1||GAUGE GLASS:1||LOWTEMPERATURE TRANSPORT:1||spontaneous spin polarization model:1||BIAS:1||emission of electromagnetic waves:1||YBA2CU3O7/PRBA2CU3O7 SUPERLATTICES:1||BOHM:1||SHAPIRO STEPS:1||superconductor/ferromagnet interface:1||OXIDE:1||ANDREEVREFLECTION:1||SinFeAsO single crystal:1||COLLECTIVE MOTION:1||ANGULARDEPENDENCE:1||SUPERCONDUCTIVITY:1||BILAYER GRAPHENE:1||PHOTOLUMINESCENT PROPERTIES:1||SUPERCONDUCTING WEAK LINKS:1||intrinsic Josephson junctions geometrical resonance:1||intrinsic Josephson junction:1||MESOSCOPIC SPINVALVE:1||Bi2212 single crystals:1||intrinsic junctions:1||ANDREEV REFLECTIONS:1||normalmetal/superconductor interface:1||IBI2SR2CACU2OY:1||THERMAL FLUCTUATIONS:1||MIXED STATE:1||BI2.15SR1.85CACU2O8+DELTA:1||intrinsic Josephson effects:1||CACUO:1||QUANTUM POINT CONTACTS:1||resonant tunneling state:1||coherence length:1||NANOWIRE:1||GATES:1||Phase line:1||Thermal activation:1||QUANTUMDOT:1||superconducting proximity effect:1||Andreev interferometer:1||WIRE:1||Josephsonvortexflow branches:1||Bi2212 cuprates:1||LATTICE:1||demannetization effect:1||SUPERCONDUCTING MIRRORS:1||GAS:1||VALLEY TRANSPORT:1||ELECTRODES:1||DEPENDENT TRANSPORT:1||BORNOPPENHEIMER APPROXIMATION:1||collective plasma oscillations:1||fluxon resonance steps:1||STACKS:1||COLLECTIVE DYNAMICS:1||PAIRING SYMMETRY:1||MUON SPIN ROTATION:1||DIMENSIONAL CROSSOVER:1||Bi2Sr2CaCu2Oy highTc superconductors:1||heterojunctions:1||nanostructures:1||surfaces and interfaces:1||QUANTUM TRANSPORT:1||MICROJUNCTIONS:1||RESONATORS:1||STATES:1||FIELD:1||FLUCTUATIONS:1||SCATTERING:1||mode splitting of Josephson vortexflow branches:1||2D superconductivity:1||TRANSISTOR:1||ENERGYGAP:1||SUPERLATTICES:1||IRONBASED SUPERCONDUCTORS:1||PHASEDEPENDENT RESISTANCE:1||QUANTUM PHASETRANSITIONS:1||ELECTRICFIELD:1||HIGH MAGNETICFIELDS:1||NANOWIRE HETEROSTRUCTURES:1||ZNO:1||pair breaking.:1||SUPERCONDUCTING PB:1||domain formation:1||FORCE MICROSCOPY:1||RELAXATION:1||PLASMA RESONANCE:1||coupled Josephson junctions:1||COPPEROXIDE SUPERCONDUCTORS:1||CROSSOVER:1||SIMULATIONS:1||LOWTEMPERATURE:1||CONDUCTORS:1||METALINSULATORTRANSITION:1||SEMICONDUCTOR:1||FIELDEFFECT TRANSISTORS:1||ZEROVOLTAGE STATE:1||constanttemperature interlayer tunneling spectroscopy:1||Josephson supercurrent:1||BIPOLAR SUPERCURRENT:1||Interaction between Josephson and pancake vortices:1||flux jump:1||coaxial heterojunction nanorod:1||Natural Josephson coupling:1||BI2SR2CACU2O8+DELTA:1||VORTEX FLOW:1||TC SUPERCONDUCTORS:1||charge imbalance:1||Andreev diffractometer:1||intercalation:1||surface junction:1||Bi2212:1||tunnelling:1||GRAPHITE:1||GROWTH:1||collective transverse plasma modes:1||GAN:1||Macroscopic quantum tunneling:1||Fluctuation conductivity:1||Abovegap conductance jump:1||Josephson vortex motion:1||Intrinsic Josephson junctions:1||LAYERED SUPERCONDUCTORS:1||BI2SR2CACU2O8+Y:1||INTERFACES:1||BREAKDOWN:1||SYSTEMS:1||Anisotropy ratio:1||Josephson vortex:1||spin relaxation in superconductors:1||bibased single crystals:1||MESOSCOPIC PROXIMITY SUPERCONDUCTOR:1||reentrance of conductance:1||interlayer pair tunneling:1||JOSEPHSON:1||DISORDERED 2DIMENSIONAL SUPERCONDUCTORS:1||INDIUM FILMS:1||excited state:1||REGIME:1||triplet superconductivity:1||FILM:1||SCHOTTKY DIODES:1||peakdiphump structure:1||Kondo effect:1||REENTRANCE:1||Graphene:1||CONTACT:1||BERRYS PHASE:1||2DIMENSIONAL SUPERCONDUCTORS:1||Coulomb diamond:1||magnetic domain:1||spin injection:1||RESONANCE:1||plasma excitation modes:1||FLOW:1||OVERDOPED BI2SR2CACU2O8+DELTA:1||hole doping:1||chemical synthesis:1||phase transitions:1||superconductors:1||VORTEXGLASS SUPERCONDUCTIVITY:1||Kondorelated model:1||RADIATION:1||DOT:1||NANOBELTS:1||Complementarity:1||Closedloop AharonovBohm interferometer:1||pair breaking:1||interlayer phase fluctuation:1||MgB2 thin film:1||CONFINEMENT:1||WALLED CARBON NANOTUBES:1||TRANSITION:9||VORTICES:8||STATE:7||intrinsic Josephson junctions:7||SINGLECRYSTALS:7||JUNCTIONS:5||MODES:5||SUPERCURRENT:5||SUPERCONDUCTOR:5||CONDUCTANCE:5||HIGHTEMPERATURE SUPERCONDUCTORS:5||TRANSPORT:5||PHASE:5||FILMS:4||LOCALIZATION:4||SINGLE DIRAC CONE:4||WIRES:4||MAGNETICFIELD:4||STEPS:3||ELECTRONS:3||proximity effect:3||MODEL:3||ARRAYS:3||INTERFERENCE:3||fluxon dynamics:3||HETEROSTRUCTURES:3||INSULATOR:3||Andreev reflection:3||electronic transport:3||FISKE:3||superconductor:2||ZnO:2||quantum point contact:2||METAL:2||DYNAMICS:2||interlayer Josephson coupling:2||SUPERCONDUCTORS:2||YBA2CU3O7DELTA:2||LAYER:2||DOTS:2||quantum dot:2||Article:2||TRANSISTORS:2||CARBON NANOTUBES:2||GAP:2||MECHANISM:2||LINE:2||GIANT SHAPIRO STEPS:2||LAYERS:2||electron energy loss spectroscopy:2||physical phenomena:2||scanning electron microscopy:2||HGTE QUANTUMWELLS:2||BI2TE3:2||SPECTROSCOPY:2||PNJUNCTIONS:2||spinpolarized tunneling:2||INTRINSIC JOSEPHSONJUNCTIONS:2||FIELDS:2||positive magnetoresistance:2||dilute magnetic semiconductor:2||magnetic field:2||scanning transmission electron microscopy:2||QUANTUM OSCILLATIONS:2||TRANSPORTPROPERTIES:2||surface pair current:2||MAGNETORESISTANCE:2||NANORIBBONS:2||INSTABILITY:2||ANDREEV REFLECTION:2||microwave irradiation:2||vertical graphene josephson junction:2||BI2SE3:2||CONDUCTIVITY:2||highTc superconductors:2||DIMENSIONAL ELECTRONGAS:2||graphene:2||Topological insulators:2||Josephson coupling Fraunhofer interference pattern:2||FERROMAGNET:2||DEPENDENCE:2||DETECTOR:2||COHERENCE:2||INJECTION:2||GRAPHENE:1||JOSEPHSONJUNCTIONS:1||LAYERED SUPERCONDUCTOR:1||mode splitting:1||BEHAVIOR:1||spinpolarized transport:1||SUPERCONDUCTING TRANSITION:1||microwave response:1||PSEUDOGAP:1||phase coherence:1||TRANSITIONS:1||Long Josephson junction:1||Charge detection:1||collective resonance modes:1||plasma oscillation modes:1||Superconducting proximity effect:1||Iron pnictide superconductor:1||McMillanRowell oscillations:1||ferromagnetic microstructure:1||superradiant state:1||VOLTAGE:1||branch splitting:1||TENSOR:1||INTERCALATION:1||insitu fabrication:1||NDGAO3:1||DISORDERED METALS:1||GAUGE GLASS:1||LOWTEMPERATURE TRANSPORT:1||spontaneous spin polarization model:1||BIAS:1||emission of electromagnetic waves:1||YBA2CU3O7/PRBA2CU3O7 SUPERLATTICES:1||BOHM:1||SHAPIRO STEPS:1||superconductor/ferromagnet interface:1||OXIDE:1||ANDREEVREFLECTION:1||SinFeAsO single crystal:1||COLLECTIVE MOTION:1||ANGULARDEPENDENCE:1||SUPERCONDUCTIVITY:1||BILAYER GRAPHENE:1||PHOTOLUMINESCENT PROPERTIES:1||SUPERCONDUCTING WEAK LINKS:1||intrinsic Josephson junctions geometrical resonance:1||intrinsic Josephson junction:1||MESOSCOPIC SPINVALVE:1||Bi2212 single crystals:1||intrinsic junctions:1||ANDREEV REFLECTIONS:1||normalmetal/superconductor interface:1||IBI2SR2CACU2OY:1||THERMAL FLUCTUATIONS:1||MIXED STATE:1||BI2.15SR1.85CACU2O8+DELTA:1||intrinsic Josephson effects:1||CACUO:1||QUANTUM POINT CONTACTS:1||resonant tunneling state:1||coherence length:1||NANOWIRE:1||GATES:1||Phase line:1||Thermal activation:1||QUANTUMDOT:1||superconducting proximity effect:1||Andreev interferometer:1||WIRE:1||Josephsonvortexflow branches:1||Bi2212 cuprates:1||LATTICE:1||demannetization effect:1||SUPERCONDUCTING MIRRORS:1||GAS:1||VALLEY TRANSPORT:1||ELECTRODES:1||DEPENDENT TRANSPORT:1||BORNOPPENHEIMER APPROXIMATION:1||collective plasma oscillations:1||fluxon resonance steps:1||STACKS:1||COLLECTIVE DYNAMICS:1||PAIRING SYMMETRY:1||MUON SPIN ROTATION:1||DIMENSIONAL CROSSOVER:1||Bi2Sr2CaCu2Oy highTc superconductors:1||heterojunctions:1||nanostructures:1||surfaces and interfaces:1||QUANTUM TRANSPORT:1||MICROJUNCTIONS:1||RESONATORS:1||STATES:1||FIELD:1||FLUCTUATIONS:1||SCATTERING:1||mode splitting of Josephson vortexflow branches:1||2D superconductivity:1||TRANSISTOR:1||ENERGYGAP:1||SUPERLATTICES:1||IRONBASED SUPERCONDUCTORS:1||PHASEDEPENDENT RESISTANCE:1||QUANTUM PHASETRANSITIONS:1||ELECTRICFIELD:1||HIGH MAGNETICFIELDS:1||NANOWIRE HETEROSTRUCTURES:1||ZNO:1||pair breaking.:1||SUPERCONDUCTING PB:1||domain formation:1||FORCE MICROSCOPY:1||RELAXATION:1||PLASMA RESONANCE:1||coupled Josephson junctions:1||COPPEROXIDE SUPERCONDUCTORS:1||CROSSOVER:1||SIMULATIONS:1||LOWTEMPERATURE:1||CONDUCTORS:1||METALINSULATORTRANSITION:1||SEMICONDUCTOR:1||FIELDEFFECT TRANSISTORS:1||ZEROVOLTAGE STATE:1||constanttemperature interlayer tunneling spectroscopy:1||Josephson supercurrent:1||BIPOLAR SUPERCURRENT:1||Interaction between Josephson and pancake vortices:1||flux jump:1||coaxial heterojunction nanorod:1||Natural Josephson coupling:1||BI2SR2CACU2O8+DELTA:1||VORTEX FLOW:1||TC SUPERCONDUCTORS:1||charge imbalance:1||Andreev diffractometer:1||intercalation:1||surface junction:1||Bi2212:1||tunnelling:1||GRAPHITE:1||GROWTH:1||collective transverse plasma modes:1||GAN:1||Macroscopic quantum tunneling:1||Fluctuation conductivity:1||Abovegap conductance jump:1||Josephson vortex motion:1||Intrinsic Josephson junctions:1||LAYERED SUPERCONDUCTORS:1||BI2SR2CACU2O8+Y:1||INTERFACES:1||BREAKDOWN:1||SYSTEMS:1||Anisotropy ratio:1||Josephson vortex:1||spin relaxation in superconductors:1||bibased single crystals:1||MESOSCOPIC PROXIMITY SUPERCONDUCTOR:1||reentrance of conductance:1||interlayer pair tunneling:1||JOSEPHSON:1||DISORDERED 2DIMENSIONAL SUPERCONDUCTORS:1||INDIUM FILMS:1||excited state:1||REGIME:1||triplet superconductivity:1||FILM:1||SCHOTTKY DIODES:1||peakdiphump structure:1||Kondo effect:1||REENTRANCE:1||Graphene:1||CONTACT:1||BERRYS PHASE:1||2DIMENSIONAL SUPERCONDUCTORS:1||Coulomb diamond:1||magnetic domain:1||spin injection:1||RESONANCE:1||plasma excitation modes:1||FLOW:1||OVERDOPED BI2SR2CACU2O8+DELTA:1||hole doping:1||chemical synthesis:1||phase transitions:1||superconductors:1||VORTEXGLASS SUPERCONDUCTIVITY:1||Kondorelated model:1||RADIATION:1||DOT:1||NANOBELTS:1||Complementarity:1||Closedloop AharonovBohm interferometer:1||pair breaking:1||interlayer phase fluctuation:1||MgB2 thin film:1||CONFINEMENT:1||WALLED CARBON NANOTUBES:1||TRANSITION:9||VORTICES:8||STATE:7||intrinsic Josephson junctions:7||SINGLECRYSTALS:7||JUNCTIONS:5||MODES:5||SUPERCURRENT:5||SUPERCONDUCTOR:5||CONDUCTANCE:5||HIGHTEMPERATURE SUPERCONDUCTORS:5||TRANSPORT:5||PHASE:5||FILMS:4||LOCALIZATION:4||SINGLE DIRAC CONE:4||WIRES:4||MAGNETICFIELD:4||STEPS:3||ELECTRONS:3||proximity effect:3||MODEL:3||ARRAYS:3||INTERFERENCE:3||fluxon dynamics:3||HETEROSTRUCTURES:3||INSULATOR:3||Andreev reflection:3||electronic transport:3||FISKE:3||superconductor:2||ZnO:2||quantum point contact:2||METAL:2||DYNAMICS:2||interlayer Josephson coupling:2||SUPERCONDUCTORS:2||YBA2CU3O7DELTA:2||LAYER:2||DOTS:2||quantum dot:2||Article:2||TRANSISTORS:2||CARBON NANOTUBES:2||GAP:2||MECHANISM:2||LINE:2||GIANT SHAPIRO STEPS:2||LAYERS:2||electron energy loss spectroscopy:2||physical phenomena:2||scanning electron microscopy:2||HGTE QUANTUMWELLS:2||BI2TE3:2||SPECTROSCOPY:2||PNJUNCTIONS:2||spinpolarized tunneling:2||INTRINSIC JOSEPHSONJUNCTIONS:2||FIELDS:2||positive magnetoresistance:2||dilute magnetic semiconductor:2||magnetic field:2||scanning transmission electron microscopy:2||QUANTUM OSCILLATIONS:2||TRANSPORTPROPERTIES:2||surface pair current:2||MAGNETORESISTANCE:2||NANORIBBONS:2||INSTABILITY:2||ANDREEV REFLECTION:2||microwave irradiation:2||vertical graphene josephson junction:2||BI2SE3:2||CONDUCTIVITY:2||highTc superconductors:2||DIMENSIONAL ELECTRONGAS:2||graphene:2||Topological insulators:2||Josephson coupling Fraunhofer interference pattern:2||FERROMAGNET:2||DEPENDENCE:2||DETECTOR:2||COHERENCE:2||INJECTION:2||GRAPHENE:1||JOSEPHSONJUNCTIONS:1||LAYERED SUPERCONDUCTOR:1||mode splitting:1||BEHAVIOR:1||spinpolarized transport:1||SUPERCONDUCTING TRANSITION:1||microwave response:1||PSEUDOGAP:1||phase coherence:1||TRANSITIONS:1||Long Josephson junction:1||Charge detection:1||collective resonance modes:1||plasma oscillation modes:1||Superconducting proximity effect:1||Iron pnictide superconductor:1||McMillanRowell oscillations:1||ferromagnetic microstructure:1||superradiant state:1||VOLTAGE:1||branch splitting:1||TENSOR:1||INTERCALATION:1||insitu fabrication:1||NDGAO3:1||DISORDERED METALS:1||GAUGE GLASS:1||LOWTEMPERATURE TRANSPORT:1||spontaneous spin polarization model:1||BIAS:1||emission of electromagnetic waves:1||YBA2CU3O7/PRBA2CU3O7 SUPERLATTICES:1||BOHM:1||SHAPIRO STEPS:1||superconductor/ferromagnet interface:1||OXIDE:1||ANDREEVREFLECTION:1||SinFeAsO single crystal:1||COLLECTIVE MOTION:1||ANGULARDEPENDENCE:1||SUPERCONDUCTIVITY:1||BILAYER GRAPHENE:1||PHOTOLUMINESCENT PROPERTIES:1||SUPERCONDUCTING WEAK LINKS:1||intrinsic Josephson junctions geometrical resonance:1||intrinsic Josephson junction:1||MESOSCOPIC SPINVALVE:1||Bi2212 single crystals:1||intrinsic junctions:1||ANDREEV REFLECTIONS:1||normalmetal/superconductor interface:1||IBI2SR2CACU2OY:1||THERMAL FLUCTUATIONS:1||MIXED STATE:1||BI2.15SR1.85CACU2O8+DELTA:1||intrinsic Josephson effects:1||CACUO:1||QUANTUM POINT CONTACTS:1||resonant tunneling state:1||coherence length:1||NANOWIRE:1||GATES:1||Phase line:1||Thermal activation:1||QUANTUMDOT:1||superconducting proximity effect:1||Andreev interferometer:1||WIRE:1||Josephsonvortexflow branches:1||Bi2212 cuprates:1||LATTICE:1||demannetization effect:1||SUPERCONDUCTING MIRRORS:1||GAS:1||VALLEY TRANSPORT:1||ELECTRODES:1||DEPENDENT TRANSPORT:1||BORNOPPENHEIMER APPROXIMATION:1||collective plasma oscillations:1||fluxon resonance steps:1||STACKS:1||COLLECTIVE DYNAMICS:1||PAIRING SYMMETRY:1||MUON SPIN ROTATION:1||DIMENSIONAL CROSSOVER:1||Bi2Sr2CaCu2Oy highTc superconductors:1||heterojunctions:1||nanostructures:1||surfaces and interfaces:1||QUANTUM TRANSPORT:1||MICROJUNCTIONS:1||RESONATORS:1||STATES:1||FIELD:1||FLUCTUATIONS:1||SCATTERING:1||mode splitting of Josephson vortexflow branches:1||2D superconductivity:1||TRANSISTOR:1||ENERGYGAP:1||SUPERLATTICES:1||IRONBASED SUPERCONDUCTORS:1||PHASEDEPENDENT RESISTANCE:1||QUANTUM PHASETRANSITIONS:1||ELECTRICFIELD:1||HIGH MAGNETICFIELDS:1||NANOWIRE HETEROSTRUCTURES:1||ZNO:1||pair breaking.:1||SUPERCONDUCTING PB:1||domain formation:1||FORCE MICROSCOPY:1||RELAXATION:1||PLASMA RESONANCE:1||coupled Josephson junctions:1||COPPEROXIDE SUPERCONDUCTORS:1||CROSSOVER:1||SIMULATIONS:1||LOWTEMPERATURE:1||CONDUCTORS:1||METALINSULATORTRANSITION:1||SEMICONDUCTOR:1||FIELDEFFECT TRANSISTORS:1||ZEROVOLTAGE STATE:1||constanttemperature interlayer tunneling spectroscopy:1||Josephson supercurrent:1||BIPOLAR SUPERCURRENT:1||Interaction between Josephson and pancake vortices:1||flux jump:1||coaxial heterojunction nanorod:1||Natural Josephson coupling:1||BI2SR2CACU2O8+DELTA:1||VORTEX FLOW:1||TC SUPERCONDUCTORS:1||charge imbalance:1||Andreev diffractometer:1||intercalation:1||surface junction:1||Bi2212:1||tunnelling:1||GRAPHITE:1||GROWTH:1||collective transverse plasma modes:1||GAN:1||Macroscopic quantum tunneling:1||Fluctuation conductivity:1||Abovegap conductance jump:1||Josephson vortex motion:1||Intrinsic Josephson junctions:1||LAYERED SUPERCONDUCTORS:1||BI2SR2CACU2O8+Y:1||INTERFACES:1||BREAKDOWN:1||SYSTEMS:1||Anisotropy ratio:1||Josephson vortex:1||spin relaxation in superconductors:1||bibased single crystals:1||MESOSCOPIC PROXIMITY SUPERCONDUCTOR:1||reentrance of conductance:1||interlayer pair tunneling:1||JOSEPHSON:1||DISORDERED 2DIMENSIONAL SUPERCONDUCTORS:1||INDIUM FILMS:1||excited state:1||REGIME:1||triplet superconductivity:1||FILM:1||SCHOTTKY DIODES:1||peakdiphump structure:1||Kondo effect:1||REENTRANCE:1||Graphene:1||CONTACT:1||BERRYS PHASE:1||2DIMENSIONAL SUPERCONDUCTORS:1||Coulomb diamond:1||magnetic domain:1||spin injection:1||RESONANCE:1||plasma excitation modes:1||FLOW:1||OVERDOPED BI2SR2CACU2O8+DELTA:1||hole doping:1||chemical synthesis:1||phase transitions:1||superconductors:1||VORTEXGLASS SUPERCONDUCTIVITY:1||Kondorelated model:1||RADIATION:1||DOT:1||NANOBELTS:1||Complementarity:1||Closedloop AharonovBohm interferometer:1||pair breaking:1||interlayer phase fluctuation:1||MgB2 thin film:1||CONFINEMENT:1||WALLED CARBON NANOTUBES:1||TRANSITION:9||VORTICES:8||STATE:7||intrinsic Josephson junctions:7||SINGLECRYSTALS:7||JUNCTIONS:5||MODES:5||SUPERCURRENT:5||SUPERCONDUCTOR:5||CONDUCTANCE:5||HIGHTEMPERATURE SUPERCONDUCTORS:5||TRANSPORT:5||PHASE:5||FILMS:4||LOCALIZATION:4||SINGLE DIRAC CONE:4||WIRES:4||MAGNETICFIELD:4||STEPS:3||ELECTRONS:3||proximity effect:3||MODEL:3||ARRAYS:3||INTERFERENCE:3||fluxon dynamics:3||HETEROSTRUCTURES:3||INSULATOR:3||Andreev reflection:3||electronic transport:3||FISKE:3||superconductor:2||ZnO:2||quantum point contact:2||METAL:2||DYNAMICS:2||interlayer Josephson coupling:2||SUPERCONDUCTORS:2||YBA2CU3O7DELTA:2||LAYER:2||DOTS:2||quantum dot:2||Article:2||TRANSISTORS:2||CARBON NANOTUBES:2||GAP:2||MECHANISM:2||LINE:2||GIANT SHAPIRO STEPS:2||LAYERS:2||electron energy loss spectroscopy:2||physical phenomena:2||scanning electron microscopy:2||HGTE QUANTUMWELLS:2||BI2TE3:2||SPECTROSCOPY:2||PNJUNCTIONS:2||spinpolarized tunneling:2||INTRINSIC JOSEPHSONJUNCTIONS:2||FIELDS:2||positive magnetoresistance:2||dilute magnetic semiconductor:2||magnetic field:2||scanning transmission electron microscopy:2||QUANTUM OSCILLATIONS:2||TRANSPORTPROPERTIES:2||surface pair current:2||MAGNETORESISTANCE:2||NANORIBBONS:2||INSTABILITY:2||ANDREEV REFLECTION:2||microwave irradiation:2||vertical graphene josephson junction:2||BI2SE3:2||CONDUCTIVITY:2||highTc superconductors:2||DIMENSIONAL ELECTRONGAS:2||graphene:2||Topological insulators:2||Josephson coupling Fraunhofer interference pattern:2||FERROMAGNET:2||DEPENDENCE:2||DETECTOR:2||COHERENCE:2||INJECTION:2||GRAPHENE:1||JOSEPHSONJUNCTIONS:1||LAYERED SUPERCONDUCTOR:1||mode splitting:1||BEHAVIOR:1||spinpolarized transport:1||SUPERCONDUCTING TRANSITION:1||microwave response:1||PSEUDOGAP:1||phase coherence:1||TRANSITIONS:1||Long Josephson junction:1||Charge detection:1||collective resonance modes:1||plasma oscillation modes:1||Superconducting proximity effect:1||Iron pnictide superconductor:1||McMillanRowell oscillations:1||ferromagnetic microstructure:1||superradiant state:1||VOLTAGE:1||branch splitting:1||TENSOR:1||INTERCALATION:1||insitu fabrication:1||NDGAO3:1||DISORDERED METALS:1||GAUGE GLASS:1||LOWTEMPERATURE TRANSPORT:1||spontaneous spin polarization model:1||BIAS:1||emission of electromagnetic waves:1||YBA2CU3O7/PRBA2CU3O7 SUPERLATTICES:1||BOHM:1||SHAPIRO STEPS:1||superconductor/ferromagnet interface:1||OXIDE:1||ANDREEVREFLECTION:1||SinFeAsO single crystal:1||COLLECTIVE MOTION:1||ANGULARDEPENDENCE:1||SUPERCONDUCTIVITY:1||BILAYER GRAPHENE:1||PHOTOLUMINESCENT PROPERTIES:1||SUPERCONDUCTING WEAK LINKS:1||intrinsic Josephson junctions geometrical resonance:1||intrinsic Josephson junction:1||MESOSCOPIC SPINVALVE:1||Bi2212 single crystals:1||intrinsic junctions:1||ANDREEV REFLECTIONS:1||normalmetal/superconductor interface:1||IBI2SR2CACU2OY:1||THERMAL FLUCTUATIONS:1||MIXED STATE:1||BI2.15SR1.85CACU2O8+DELTA:1||intrinsic Josephson effects:1||CACUO:1||QUANTUM POINT CONTACTS:1||resonant tunneling state:1||coherence length:1||NANOWIRE:1||GATES:1||Phase line:1||Thermal activation:1||QUANTUMDOT:1||superconducting proximity effect:1||Andreev interferometer:1||WIRE:1||Josephsonvortexflow branches:1||Bi2212 cuprates:1||LATTICE:1||demannetization effect:1||SUPERCONDUCTING MIRRORS:1||GAS:1||VALLEY TRANSPORT:1||ELECTRODES:1||DEPENDENT TRANSPORT:1||BORNOPPENHEIMER APPROXIMATION:1||collective plasma oscillations:1||fluxon resonance steps:1||STACKS:1||COLLECTIVE DYNAMICS:1||PAIRING SYMMETRY:1||MUON SPIN ROTATION:1||DIMENSIONAL CROSSOVER:1||Bi2Sr2CaCu2Oy highTc superconductors:1||heterojunctions:1||nanostructures:1||surfaces and interfaces:1||QUANTUM TRANSPORT:1||MICROJUNCTIONS:1||RESONATORS:1||STATES:1||FIELD:1||FLUCTUATIONS:1||SCATTERING:1||mode splitting of Josephson vortexflow branches:1||2D superconductivity:1||TRANSISTOR:1||ENERGYGAP:1||SUPERLATTICES:1||IRONBASED SUPERCONDUCTORS:1||PHASEDEPENDENT RESISTANCE:1||QUANTUM PHASETRANSITIONS:1||ELECTRICFIELD:1||HIGH MAGNETICFIELDS:1||NANOWIRE HETEROSTRUCTURES:1||ZNO:1||pair breaking.:1||SUPERCONDUCTING PB:1||domain formation:1||FORCE MICROSCOPY:1||RELAXATION:1||PLASMA RESONANCE:1||coupled Josephson junctions:1||COPPEROXIDE SUPERCONDUCTORS:1||CROSSOVER:1||SIMULATIONS:1||LOWTEMPERATURE:1||CONDUCTORS:1||METALINSULATORTRANSITION:1||SEMICONDUCTOR:1||FIELDEFFECT TRANSISTORS:1||ZEROVOLTAGE STATE:1||constanttemperature interlayer tunneling spectroscopy:1||Josephson supercurrent:1||BIPOLAR SUPERCURRENT:1||Interaction between Josephson and pancake vortices:1||flux jump:1||coaxial heterojunction nanorod:1||Natural Josephson coupling:1||BI2SR2CACU2O8+DELTA:1||VORTEX FLOW:1||TC SUPERCONDUCTORS:1||charge imbalance:1||Andreev diffractometer:1||intercalation:1||surface junction:1||Bi2212:1||tunnelling:1||GRAPHITE:1||GROWTH:1||collective transverse plasma modes:1||GAN:1||Macroscopic quantum tunneling:1||Fluctuation conductivity:1||Abovegap conductance jump:1||Josephson vortex motion:1||Intrinsic Josephson junctions:1||LAYERED SUPERCONDUCTORS:1||BI2SR2CACU2O8+Y:1||INTERFACES:1||BREAKDOWN:1||SYSTEMS:1||Anisotropy ratio:1||Josephson vortex:1||spin relaxation in superconductors:1||bibased single crystals:1||MESOSCOPIC PROXIMITY SUPERCONDUCTOR:1||reentrance of conductance:1||interlayer pair tunneling:1||JOSEPHSON:1||DISORDERED 2DIMENSIONAL SUPERCONDUCTORS:1||INDIUM FILMS:1||excited state:1||REGIME:1||triplet superconductivity:1||FILM:1||SCHOTTKY DIODES:1||peakdiphump structure:1||Kondo effect:1||REENTRANCE:1||Graphene:1||CONTACT:1||BERRYS PHASE:1||2DIMENSIONAL SUPERCONDUCTORS:1||Coulomb diamond:1||magnetic domain:1||spin injection:1||RESONANCE:1||plasma excitation modes:1||FLOW:1||OVERDOPED BI2SR2CACU2O8+DELTA:1||hole doping:1||chemical synthesis:1||phase transitions:1||superconductors:1||VORTEXGLASS SUPERCONDUCTIVITY:1||Kondorelated model:1||RADIATION:1||DOT:1||NANOBELTS:1||Complementarity:1||Closedloop AharonovBohm interferometer:1||pair breaking:1||interlayer phase fluctuation:1||MgB2 thin film:1||CONFINEMENT:1||WALLED CARBON NANOTUBES:1||TRANSITION:9||VORTICES:8||STATE:7||intrinsic Josephson junctions:7||SINGLECRYSTALS:7||JUNCTIONS:5||MODES:5||SUPERCURRENT:5||SUPERCONDUCTOR:5||CONDUCTANCE:5||HIGHTEMPERATURE SUPERCONDUCTORS:5||TRANSPORT:5||PHASE:5||FILMS:4||LOCALIZATION:4||SINGLE DIRAC CONE:4||WIRES:4||MAGNETICFIELD:4||STEPS:3||ELECTRONS:3||proximity effect:3||MODEL:3||ARRAYS:3||INTERFERENCE:3||fluxon dynamics:3||HETEROSTRUCTURES:3||INSULATOR:3||Andreev reflection:3||electronic transport:3||FISKE:3||superconductor:2||ZnO:2||quantum point contact:2||METAL:2||DYNAMICS:2||interlayer Josephson coupling:2||SUPERCONDUCTORS:2||YBA2CU3O7DELTA:2||LAYER:2||DOTS:2||quantum dot:2||Article:2||TRANSISTORS:2||CARBON NANOTUBES:2||GAP:2||MECHANISM:2||LINE:2||GIANT SHAPIRO STEPS:2||LAYERS:2||electron energy loss spectroscopy:2||physical phenomena:2||scanning electron microscopy:2||HGTE QUANTUMWELLS:2||BI2TE3:2||SPECTROSCOPY:2||PNJUNCTIONS:2||spinpolarized tunneling:2||INTRINSIC JOSEPHSONJUNCTIONS:2||FIELDS:2||positive magnetoresistance:2||dilute magnetic semiconductor:2||magnetic field:2||scanning transmission electron microscopy:2||QUANTUM OSCILLATIONS:2||TRANSPORTPROPERTIES:2||surface pair current:2||MAGNETORESISTANCE:2||NANORIBBONS:2||INSTABILITY:2||ANDREEV REFLECTION:2||microwave irradiation:2||vertical graphene josephson junction:2||BI2SE3:2||CONDUCTIVITY:2||highTc superconductors:2||DIMENSIONAL ELECTRONGAS:2||graphene:2||Topological insulators:2||Josephson coupling Fraunhofer interference pattern:2||FERROMAGNET:2||DEPENDENCE:2||DETECTOR:2||COHERENCE:2||INJECTION:2||GRAPHENE:1||JOSEPHSONJUNCTIONS:1||LAYERED SUPERCONDUCTOR:1||mode splitting:1||BEHAVIOR:1||spinpolarized transport:1||SUPERCONDUCTING TRANSITION:1||microwave response:1||PSEUDOGAP:1||phase coherence:1||TRANSITIONS:1||Long Josephson junction:1||Charge detection:1||collective resonance modes:1||plasma oscillation modes:1||Superconducting proximity effect:1||Iron pnictide superconductor:1||McMillanRowell oscillations:1||ferromagnetic microstructure:1||superradiant state:1||VOLTAGE:1||branch splitting:1||TENSOR:1||INTERCALATION:1||insitu fabrication:1||NDGAO3:1||DISORDERED METALS:1||GAUGE GLASS:1||LOWTEMPERATURE TRANSPORT:1||spontaneous spin polarization model:1||BIAS:1||emission of electromagnetic waves:1||YBA2CU3O7/PRBA2CU3O7 SUPERLATTICES:1||BOHM:1||SHAPIRO STEPS:1||superconductor/ferromagnet interface:1||OXIDE:1||ANDREEVREFLECTION:1||SinFeAsO single crystal:1||COLLECTIVE MOTION:1||ANGULARDEPENDENCE:1||SUPERCONDUCTIVITY:1||BILAYER GRAPHENE:1||PHOTOLUMINESCENT PROPERTIES:1||SUPERCONDUCTING WEAK LINKS:1||intrinsic Josephson junctions geometrical resonance:1||intrinsic Josephson junction:1||MESOSCOPIC SPINVALVE:1||Bi2212 single crystals:1||intrinsic junctions:1||ANDREEV REFLECTIONS:1||normalmetal/superconductor interface:1||IBI2SR2CACU2OY:1||THERMAL FLUCTUATIONS:1||MIXED STATE:1||BI2.15SR1.85CACU2O8+DELTA:1||intrinsic Josephson effects:1||CACUO:1||QUANTUM POINT CONTACTS:1||resonant tunneling state:1||coherence length:1||NANOWIRE:1||GATES:1||Phase line:1||Thermal activation:1||QUANTUMDOT:1||superconducting proximity effect:1||Andreev interferometer:1||WIRE:1||Josephsonvortexflow branches:1||Bi2212 cuprates:1||LATTICE:1||demannetization effect:1||SUPERCONDUCTING MIRRORS:1||GAS:1||VALLEY TRANSPORT:1||ELECTRODES:1||DEPENDENT TRANSPORT:1||BORNOPPENHEIMER APPROXIMATION:1||collective plasma oscillations:1||fluxon resonance steps:1||STACKS:1||COLLECTIVE DYNAMICS:1||PAIRING SYMMETRY:1||MUON SPIN ROTATION:1||DIMENSIONAL CROSSOVER:1||Bi2Sr2CaCu2Oy highTc superconductors:1||heterojunctions:1||nanostructures:1||surfaces and interfaces:1||QUANTUM TRANSPORT:1||MICROJUNCTIONS:1||RESONATORS:1||STATES:1||FIELD:1||FLUCTUATIONS:1||SCATTERING:1||mode splitting of Josephson vortexflow branches:1||2D superconductivity:1||TRANSISTOR:1||ENERGYGAP:1||SUPERLATTICES:1||IRONBASED SUPERCONDUCTORS:1||PHASEDEPENDENT RESISTANCE:1||QUANTUM PHASETRANSITIONS:1||ELECTRICFIELD:1||HIGH MAGNETICFIELDS:1||NANOWIRE HETEROSTRUCTURES:1||ZNO:1||pair breaking.:1||SUPERCONDUCTING PB:1||domain formation:1||FORCE MICROSCOPY:1||RELAXATION:1||PLASMA RESONANCE:1||coupled Josephson junctions:1||COPPEROXIDE SUPERCONDUCTORS:1||CROSSOVER:1||SIMULATIONS:1||LOWTEMPERATURE:1||CONDUCTORS:1||METALINSULATORTRANSITION:1||SEMICONDUCTOR:1||FIELDEFFECT TRANSISTORS:1||ZEROVOLTAGE STATE:1||constanttemperature interlayer tunneling spectroscopy:1||Josephson supercurrent:1||BIPOLAR SUPERCURRENT:1||Interaction between Josephson and pancake vortices:1||flux jump:1||coaxial heterojunction nanorod:1||Natural Josephson coupling:1||BI2SR2CACU2O8+DELTA:1||VORTEX FLOW:1||TC SUPERCONDUCTORS:1||charge imbalance:1||Andreev diffractometer:1||intercalation:1||surface junction:1||Bi2212:1||tunnelling:1||GRAPHITE:1||GROWTH:1||collective transverse plasma modes:1||GAN:1||Macroscopic quantum tunneling:1||Fluctuation conductivity:1||Abovegap conductance jump:1||Josephson vortex motion:1||Intrinsic Josephson junctions:1||LAYERED SUPERCONDUCTORS:1||BI2SR2CACU2O8+Y:1||INTERFACES:1||BREAKDOWN:1||SYSTEMS:1||Anisotropy ratio:1||Josephson vortex:1||spin relaxation in superconductors:1||bibased single crystals:1||MESOSCOPIC PROXIMITY SUPERCONDUCTOR:1||reentrance of conductance:1||interlayer pair tunneling:1||JOSEPHSON:1||DISORDERED 2DIMENSIONAL SUPERCONDUCTORS:1||INDIUM FILMS:1||excited state:1||REGIME:1||triplet superconductivity:1||FILM:1||SCHOTTKY DIODES:1||peakdiphump structure:1||Kondo effect:1||REENTRANCE:1||Graphene:1||CONTACT:1||BERRYS PHASE:1||2DIMENSIONAL SUPERCONDUCTORS:1||Coulomb diamond:1||magnetic domain:1||spin injection:1||RESONANCE:1||plasma excitation modes:1||FLOW:1||OVERDOPED BI2SR2CACU2O8+DELTA:1||hole doping:1||chemical synthesis:1||phase transitions:1||superconductors:1||VORTEXGLASS SUPERCONDUCTIVITY:1||Kondorelated model:1||RADIATION:1||DOT:1||NANOBELTS:1||Complementarity:1||Closedloop AharonovBohm interferometer:1||pair breaking:1||interlayer phase fluctuation:1||MgB2 thin film:1||CONFINEMENT:1||WALLED CARBON NANOTUBES:1||TRANSITION:9||VORTICES:8||STATE:7||intrinsic Josephson junctions:7||SINGLECRYSTALS:7||JUNCTIONS:5||MODES:5||SUPERCURRENT:5||SUPERCONDUCTOR:5||CONDUCTANCE:5||HIGHTEMPERATURE SUPERCONDUCTORS:5||TRANSPORT:5||PHASE:5||FILMS:4||LOCALIZATION:4||SINGLE DIRAC CONE:4||WIRES:4||MAGNETICFIELD:4||STEPS:3||ELECTRONS:3||proximity effect:3||MODEL:3||ARRAYS:3||INTERFERENCE:3||fluxon dynamics:3||HETEROSTRUCTURES:3||INSULATOR:3||Andreev reflection:3||electronic transport:3||FISKE:3||superconductor:2||ZnO:2||quantum point contact:2||METAL:2||DYNAMICS:2||interlayer Josephson coupling:2||SUPERCONDUCTORS:2||YBA2CU3O7DELTA:2||LAYER:2||DOTS:2||quantum dot:2||Article:2||TRANSISTORS:2||CARBON NANOTUBES:2||GAP:2||MECHANISM:2||LINE:2||GIANT SHAPIRO STEPS:2||LAYERS:2||electron energy loss spectroscopy:2||physical phenomena:2||scanning electron microscopy:2||HGTE QUANTUMWELLS:2||BI2TE3:2||SPECTROSCOPY:2||PNJUNCTIONS:2||spinpolarized tunneling:2||INTRINSIC JOSEPHSONJUNCTIONS:2||FIELDS:2||positive magnetoresistance:2||dilute magnetic semiconductor:2||magnetic field:2||scanning transmission electron microscopy:2||QUANTUM OSCILLATIONS:2||TRANSPORTPROPERTIES:2||surface pair current:2||MAGNETORESISTANCE:2||NANORIBBONS:2||INSTABILITY:2||ANDREEV REFLECTION:2||microwave irradiation:2||vertical graphene josephson junction:2||BI2SE3:2||CONDUCTIVITY:2||highTc superconductors:2||DIMENSIONAL ELECTRONGAS:2||graphene:2||Topological insulators:2||Josephson coupling Fraunhofer interference pattern:2||FERROMAGNET:2||DEPENDENCE:2||DETECTOR:2||COHERENCE:2||INJECTION:2||GRAPHENE:1||JOSEPHSONJUNCTIONS:1||LAYERED SUPERCONDUCTOR:1||mode splitting:1||BEHAVIOR:1||spinpolarized transport:1||SUPERCONDUCTING TRANSITION:1||microwave response:1||PSEUDOGAP:1||phase coherence:1||TRANSITIONS:1||Long Josephson junction:1||Charge detection:1||collective resonance modes:1||plasma oscillation modes:1||Superconducting proximity effect:1||Iron pnictide superconductor:1||McMillanRowell oscillations:1||ferromagnetic microstructure:1||superradiant state:1||VOLTAGE:1||branch splitting:1||TENSOR:1||INTERCALATION:1||insitu fabrication:1||NDGAO3:1||DISORDERED METALS:1||GAUGE GLASS:1||LOWTEMPERATURE TRANSPORT:1||spontaneous spin polarization model:1||BIAS:1||emission of electromagnetic waves:1||YBA2CU3O7/PRBA2CU3O7 SUPERLATTICES:1||BOHM:1||SHAPIRO STEPS:1||superconductor/ferromagnet interface:1||OXIDE:1||ANDREEVREFLECTION:1||SinFeAsO single crystal:1||COLLECTIVE MOTION:1||ANGULARDEPENDENCE:1||SUPERCONDUCTIVITY:1||BILAYER GRAPHENE:1||PHOTOLUMINESCENT PROPERTIES:1||SUPERCONDUCTING WEAK LINKS:1||intrinsic Josephson junctions geometrical resonance:1||intrinsic Josephson junction:1||MESOSCOPIC SPINVALVE:1||Bi2212 single crystals:1||intrinsic junctions:1||ANDREEV REFLECTIONS:1||normalmetal/superconductor interface:1||IBI2SR2CACU2OY:1||THERMAL FLUCTUATIONS:1||MIXED STATE:1||BI2.15SR1.85CACU2O8+DELTA:1||intrinsic Josephson effects:1||CACUO:1||QUANTUM POINT CONTACTS:1||resonant tunneling state:1||coherence length:1||NANOWIRE:1||GATES:1||Phase line:1||Thermal activation:1||QUANTUMDOT:1||superconducting proximity effect:1||Andreev interferometer:1||WIRE:1||Josephsonvortexflow branches:1||Bi2212 cuprates:1||LATTICE:1||demannetization effect:1||SUPERCONDUCTING MIRRORS:1||GAS:1||VALLEY TRANSPORT:1||ELECTRODES:1||DEPENDENT TRANSPORT:1||BORNOPPENHEIMER APPROXIMATION:1||collective plasma oscillations:1||fluxon resonance steps:1||STACKS:1||COLLECTIVE DYNAMICS:1||PAIRING SYMMETRY:1||MUON SPIN ROTATION:1||DIMENSIONAL CROSSOVER:1||Bi2Sr2CaCu2Oy highTc superconductors:1||heterojunctions:1||nanostructures:1||surfaces and interfaces:1||QUANTUM TRANSPORT:1||MICROJUNCTIONS:1||RESONATORS:1||STATES:1||FIELD:1||FLUCTUATIONS:1||SCATTERING:1||mode splitting of Josephson vortexflow branches:1||2D superconductivity:1||TRANSISTOR:1||ENERGYGAP:1||SUPERLATTICES:1||IRONBASED SUPERCONDUCTORS:1||PHASEDEPENDENT RESISTANCE:1||QUANTUM PHASETRANSITIONS:1||ELECTRICFIELD:1||HIGH MAGNETICFIELDS:1||NANOWIRE HETEROSTRUCTURES:1||ZNO:1||pair breaking.:1||SUPERCONDUCTING PB:1||domain formation:1||FORCE MICROSCOPY:1||RELAXATION:1||PLASMA RESONANCE:1||coupled Josephson junctions:1||COPPEROXIDE SUPERCONDUCTORS:1||CROSSOVER:1||SIMULATIONS:1||LOWTEMPERATURE:1||CONDUCTORS:1||METALINSULATORTRANSITION:1||SEMICONDUCTOR:1||FIELDEFFECT TRANSISTORS:1||ZEROVOLTAGE STATE:1||constanttemperature interlayer tunneling spectroscopy:1||Josephson supercurrent:1||BIPOLAR SUPERCURRENT:1||Interaction between Josephson and pancake vortices:1||flux jump:1||coaxial heterojunction nanorod:1||Natural Josephson coupling:1||BI2SR2CACU2O8+DELTA:1||VORTEX FLOW:1||TC SUPERCONDUCTORS:1||charge imbalance:1||Andreev diffractometer:1||intercalation:1||surface junction:1||Bi2212:1||tunnelling:1||GRAPHITE:1||GROWTH:1||collective transverse plasma modes:1||GAN:1||Macroscopic quantum tunneling:1||Fluctuation conductivity:1||Abovegap conductance jump:1||Josephson vortex motion:1||Intrinsic Josephson junctions:1||LAYERED SUPERCONDUCTORS:1||BI2SR2CACU2O8+Y:1||INTERFACES:1||BREAKDOWN:1||SYSTEMS:1||Anisotropy ratio:1||Josephson vortex:1||spin relaxation in superconductors:1||bibased single crystals:1||MESOSCOPIC PROXIMITY SUPERCONDUCTOR:1||reentrance of conductance:1||interlayer pair tunneling:1||JOSEPHSON:1||DISORDERED 2DIMENSIONAL SUPERCONDUCTORS:1||INDIUM FILMS:1||excited state:1||REGIME:1||triplet superconductivity:1||FILM:1||SCHOTTKY DIODES:1||peakdiphump structure:1||Kondo effect:1||REENTRANCE:1||Graphene:1||CONTACT:1||BERRYS PHASE:1||2DIMENSIONAL SUPERCONDUCTORS:1||Coulomb diamond:1||magnetic domain:1||spin injection:1||RESONANCE:1||plasma excitation modes:1||FLOW:1||OVERDOPED BI2SR2CACU2O8+DELTA:1||hole doping:1||chemical synthesis:1||phase transitions:1||superconductors:1||VORTEXGLASS SUPERCONDUCTIVITY:1||Kondorelated model:1||RADIATION:1||DOT:1||NANOBELTS:1||Complementarity:1||Closedloop AharonovBohm interferometer:1||pair breaking:1||interlayer phase fluctuation:1||MgB2 thin film:1||CONFINEMENT:1||WALLED CARBON NANOTUBES:1||TRANSITION:9||VORTICES:8||STATE:7||intrinsic Josephson junctions:7||SINGLECRYSTALS:7||JUNCTIONS:5||MODES:5||SUPERCURRENT:5||SUPERCONDUCTOR:5||CONDUCTANCE:5||HIGHTEMPERATURE SUPERCONDUCTORS:5||TRANSPORT:5||PHASE:5||FILMS:4||LOCALIZATION:4||SINGLE DIRAC CONE:4||WIRES:4||MAGNETICFIELD:4||STEPS:3||ELECTRONS:3||proximity effect:3||MODEL:3||ARRAYS:3||INTERFERENCE:3||fluxon dynamics:3||HETEROSTRUCTURES:3||INSULATOR:3||Andreev reflection:3||electronic transport:3||FISKE:3||superconductor:2||ZnO:2||quantum point contact:2||METAL:2||DYNAMICS:2||interlayer Josephson coupling:2||SUPERCONDUCTORS:2||YBA2CU3O7DELTA:2||LAYER:2||DOTS:2||quantum dot:2||Article:2||TRANSISTORS:2||CARBON NANOTUBES:2||GAP:2||MECHANISM:2||LINE:2||GIANT SHAPIRO STEPS:2||LAYERS:2||electron energy loss spectroscopy:2||physical phenomena:2||scanning electron microscopy:2||HGTE QUANTUMWELLS:2||BI2TE3:2||SPECTROSCOPY:2||PNJUNCTIONS:2||spinpolarized tunneling:2||INTRINSIC JOSEPHSONJUNCTIONS:2||FIELDS:2||positive magnetoresistance:2||dilute magnetic semiconductor:2||magnetic field:2||scanning transmission electron microscopy:2||QUANTUM OSCILLATIONS:2||TRANSPORTPROPERTIES:2||surface pair current:2||MAGNETORESISTANCE:2||NANORIBBONS:2||INSTABILITY:2||ANDREEV REFLECTION:2||microwave irradiation:2||vertical graphene josephson junction:2||BI2SE3:2||CONDUCTIVITY:2||highTc superconductors:2||DIMENSIONAL ELECTRONGAS:2||graphene:2||Topological insulators:2||Josephson coupling Fraunhofer interference pattern:2||FERROMAGNET:2||DEPENDENCE:2||DETECTOR:2||COHERENCE:2||INJECTION:2||GRAPHENE:1||JOSEPHSONJUNCTIONS:1||LAYERED SUPERCONDUCTOR:1||mode splitting:1||BEHAVIOR:1||spinpolarized transport:1||SUPERCONDUCTING TRANSITION:1||microwave response:1||PSEUDOGAP:1||phase coherence:1||TRANSITIONS:1||Long Josephson junction:1||Charge detection:1||collective resonance modes:1||plasma oscillation modes:1||Superconducting proximity effect:1||Iron pnictide superconductor:1||McMillanRowell oscillations:1||ferromagnetic microstructure:1||superradiant state:1||VOLTAGE:1||branch splitting:1||TENSOR:1||INTERCALATION:1||insitu fabrication:1||NDGAO3:1||DISORDERED METALS:1||GAUGE GLASS:1||LOWTEMPERATURE TRANSPORT:1||spontaneous spin polarization model:1||BIAS:1||emission of electromagnetic waves:1||YBA2CU3O7/PRBA2CU3O7 SUPERLATTICES:1||BOHM:1||SHAPIRO STEPS:1||superconductor/ferromagnet interface:1||OXIDE:1||ANDREEVREFLECTION:1||SinFeAsO single crystal:1||COLLECTIVE MOTION:1||ANGULARDEPENDENCE:1||SUPERCONDUCTIVITY:1||BILAYER GRAPHENE:1||PHOTOLUMINESCENT PROPERTIES:1||SUPERCONDUCTING WEAK LINKS:1||intrinsic Josephson junctions geometrical resonance:1||intrinsic Josephson junction:1||MESOSCOPIC SPINVALVE:1||Bi2212 single crystals:1||intrinsic junctions:1||ANDREEV REFLECTIONS:1||normalmetal/superconductor interface:1||IBI2SR2CACU2OY:1||THERMAL FLUCTUATIONS:1||MIXED STATE:1||BI2.15SR1.85CACU2O8+DELTA:1||intrinsic Josephson effects:1||CACUO:1||QUANTUM POINT CONTACTS:1||resonant tunneling state:1||coherence length:1||NANOWIRE:1||GATES:1||Phase line:1||Thermal activation:1||QUANTUMDOT:1||superconducting proximity effect:1||Andreev interferometer:1||WIRE:1||Josephsonvortexflow branches:1||Bi2212 cuprates:1||LATTICE:1||demannetization effect:1||SUPERCONDUCTING MIRRORS:1||GAS:1||VALLEY TRANSPORT:1||ELECTRODES:1||DEPENDENT TRANSPORT:1||BORNOPPENHEIMER APPROXIMATION:1||collective plasma oscillations:1||fluxon resonance steps:1||STACKS:1||COLLECTIVE DYNAMICS:1||PAIRING SYMMETRY:1||MUON SPIN ROTATION:1||DIMENSIONAL CROSSOVER:1||Bi2Sr2CaCu2Oy highTc superconductors:1||heterojunctions:1||nanostructures:1||surfaces and interfaces:1||QUANTUM TRANSPORT:1||MICROJUNCTIONS:1||RESONATORS:1||STATES:1||FIELD:1||FLUCTUATIONS:1||SCATTERING:1||mode splitting of Josephson vortexflow branches:1||2D superconductivity:1||TRANSISTOR:1||ENERGYGAP:1||SUPERLATTICES:1||IRONBASED SUPERCONDUCTORS:1||PHASEDEPENDENT RESISTANCE:1||QUANTUM PHASETRANSITIONS:1||ELECTRICFIELD:1||HIGH MAGNETICFIELDS:1||NANOWIRE HETEROSTRUCTURES:1||ZNO:1||pair breaking.:1||SUPERCONDUCTING PB:1||domain formation:1||FORCE MICROSCOPY:1||RELAXATION:1||PLASMA RESONANCE:1||coupled Josephson junctions:1||COPPEROXIDE SUPERCONDUCTORS:1||CROSSOVER:1||SIMULATIONS:1||LOWTEMPERATURE:1||CONDUCTORS:1||METALINSULATORTRANSITION:1||SEMICONDUCTOR:1||FIELDEFFECT TRANSISTORS:1||ZEROVOLTAGE STATE:1||constanttemperature interlayer tunneling spectroscopy:1||Josephson supercurrent:1||BIPOLAR SUPERCURRENT:1||Interaction between Josephson and pancake vortices:1||flux jump:1||coaxial heterojunction nanorod:1||Natural Josephson coupling:1||BI2SR2CACU2O8+DELTA:1||VORTEX FLOW:1||TC SUPERCONDUCTORS:1||charge imbalance:1||Andreev diffractometer:1||intercalation:1||surface junction:1||Bi2212:1||tunnelling:1||GRAPHITE:1||GROWTH:1||collective transverse plasma modes:1||GAN:1||Macroscopic quantum tunneling:1||Fluctuation conductivity:1||Abovegap conductance jump:1||Josephson vortex motion:1||Intrinsic Josephson junctions:1||LAYERED SUPERCONDUCTORS:1||BI2SR2CACU2O8+Y:1||INTERFACES:1||BREAKDOWN:1||SYSTEMS:1||Anisotropy ratio:1||Josephson vortex:1||spin relaxation in superconductors:1||bibased single crystals:1||MESOSCOPIC PROXIMITY SUPERCONDUCTOR:1||reentrance of conductance:1||interlayer pair tunneling:1||JOSEPHSON:1||DISORDERED 2DIMENSIONAL SUPERCONDUCTORS:1||INDIUM FILMS:1||excited state:1||REGIME:1||triplet superconductivity:1||FILM:1||SCHOTTKY DIODES:1||peakdiphump structure:1||Kondo effect:1||REENTRANCE:1||Graphene:1||CONTACT:1||BERRYS PHASE:1||2DIMENSIONAL SUPERCONDUCTORS:1||Coulomb diamond:1||magnetic domain:1||spin injection:1||RESONANCE:1||plasma excitation modes:1||FLOW:1||OVERDOPED BI2SR2CACU2O8+DELTA:1||hole doping:1||chemical synthesis:1||phase transitions:1||superconductors:1||VORTEXGLASS SUPERCONDUCTIVITY:1||Kondorelated model:1||RADIATION:1||DOT:1||NANOBELTS:1||Complementarity:1||Closedloop AharonovBohm interferometer:1||pair breaking:1||interlayer phase fluctuation:1||MgB2 thin film:1||CONFINEMENT:1||WALLED CARBON NANOTUBES:1||TRANSITION:9||VORTICES:8||STATE:7||intrinsic Josephson junctions:7||SINGLECRYSTALS:7||JUNCTIONS:5||MODES:5||SUPERCURRENT:5||SUPERCONDUCTOR:5||CONDUCTANCE:5||HIGHTEMPERATURE SUPERCONDUCTORS:5||TRANSPORT:5||PHASE:5||FILMS:4||LOCALIZATION:4||SINGLE DIRAC CONE:4||WIRES:4||MAGNETICFIELD:4||STEPS:3||ELECTRONS:3||proximity effect:3||MODEL:3||ARRAYS:3||INTERFERENCE:3||fluxon dynamics:3||HETEROSTRUCTURES:3||INSULATOR:3||Andreev reflection:3||electronic transport:3||FISKE:3||superconductor:2||ZnO:2||quantum point contact:2||METAL:2||DYNAMICS:2||interlayer Josephson coupling:2||SUPERCONDUCTORS:2||YBA2CU3O7DELTA:2||LAYER:2||DOTS:2||quantum dot:2||Article:2||TRANSISTORS:2||CARBON NANOTUBES:2||GAP:2||MECHANISM:2||LINE:2||GIANT SHAPIRO STEPS:2||LAYERS:2||electron energy loss spectroscopy:2||physical phenomena:2||scanning electron microscopy:2||HGTE QUANTUMWELLS:2||BI2TE3:2||SPECTROSCOPY:2||PNJUNCTIONS:2||spinpolarized tunneling:2||INTRINSIC JOSEPHSONJUNCTIONS:2||FIELDS:2||positive magnetoresistance:2||dilute magnetic semiconductor:2||magnetic field:2||scanning transmission electron microscopy:2||QUANTUM OSCILLATIONS:2||TRANSPORTPROPERTIES:2||surface pair current:2||MAGNETORESISTANCE:2||NANORIBBONS:2||INSTABILITY:2||ANDREEV REFLECTION:2||microwave irradiation:2||vertical graphene josephson junction:2||BI2SE3:2||CONDUCTIVITY:2||highTc superconductors:2||DIMENSIONAL ELECTRONGAS:2||graphene:2||Topological insulators:2||Josephson coupling Fraunhofer interference pattern:2||FERROMAGNET:2||DEPENDENCE:2||DETECTOR:2||COHERENCE:2||INJECTION:2||GRAPHENE:1||JOSEPHSONJUNCTIONS:1||LAYERED SUPERCONDUCTOR:1||mode splitting:1||BEHAVIOR:1||spinpolarized transport:1||SUPERCONDUCTING TRANSITION:1||microwave response:1||PSEUDOGAP:1||phase coherence:1||TRANSITIONS:1||Long Josephson junction:1||Charge detection:1||collective resonance modes:1||plasma oscillation modes:1||Superconducting proximity effect:1||Iron pnictide superconductor:1||McMillanRowell oscillations:1||ferromagnetic microstructure:1||superradiant state:1||VOLTAGE:1||branch splitting:1||TENSOR:1||INTERCALATION:1||insitu fabrication:1||NDGAO3:1||DISORDERED METALS:1||GAUGE GLASS:1||LOWTEMPERATURE TRANSPORT:1||spontaneous spin polarization model:1||BIAS:1||emission of electromagnetic waves:1||YBA2CU3O7/PRBA2CU3O7 SUPERLATTICES:1||BOHM:1||SHAPIRO STEPS:1||superconductor/ferromagnet interface:1||OXIDE:1||ANDREEVREFLECTION:1||SinFeAsO single crystal:1||COLLECTIVE MOTION:1||ANGULARDEPENDENCE:1||SUPERCONDUCTIVITY:1||BILAYER GRAPHENE:1||PHOTOLUMINESCENT PROPERTIES:1||SUPERCONDUCTING WEAK LINKS:1||intrinsic Josephson junctions geometrical resonance:1||intrinsic Josephson junction:1||MESOSCOPIC SPINVALVE:1||Bi2212 single crystals:1||intrinsic junctions:1||ANDREEV REFLECTIONS:1||normalmetal/superconductor interface:1||IBI2SR2CACU2OY:1||THERMAL FLUCTUATIONS:1||MIXED STATE:1||BI2.15SR1.85CACU2O8+DELTA:1||intrinsic Josephson effects:1||CACUO:1||QUANTUM POINT CONTACTS:1||resonant tunneling state:1||coherence length:1||NANOWIRE:1||GATES:1||Phase line:1||Thermal activation:1||QUANTUMDOT:1||superconducting proximity effect:1||Andreev interferometer:1||WIRE:1||Josephsonvortexflow branches:1||Bi2212 cuprates:1||LATTICE:1||demannetization effect:1||SUPERCONDUCTING MIRRORS:1||GAS:1||VALLEY TRANSPORT:1||ELECTRODES:1||DEPENDENT TRANSPORT:1||BORNOPPENHEIMER APPROXIMATION:1||collective plasma oscillations:1||fluxon resonance steps:1||STACKS:1||COLLECTIVE DYNAMICS:1||PAIRING SYMMETRY:1||MUON SPIN ROTATION:1||DIMENSIONAL CROSSOVER:1||Bi2Sr2CaCu2Oy highTc superconductors:1||heterojunctions:1||nanostructures:1||surfaces and interfaces:1||QUANTUM TRANSPORT:1||MICROJUNCTIONS:1||RESONATORS:1||STATES:1||FIELD:1||FLUCTUATIONS:1||SCATTERING:1||mode splitting of Josephson vortexflow branches:1||2D superconductivity:1||TRANSISTOR:1||ENERGYGAP:1||SUPERLATTICES:1||IRONBASED SUPERCONDUCTORS:1||PHASEDEPENDENT RESISTANCE:1||QUANTUM PHASETRANSITIONS:1||ELECTRICFIELD:1||HIGH MAGNETICFIELDS:1||NANOWIRE HETEROSTRUCTURES:1||ZNO:1||pair breaking.:1||SUPERCONDUCTING PB:1||domain formation:1||FORCE MICROSCOPY:1||RELAXATION:1||PLASMA RESONANCE:1||coupled Josephson junctions:1||COPPEROXIDE SUPERCONDUCTORS:1||CROSSOVER:1||SIMULATIONS:1||LOWTEMPERATURE:1||CONDUCTORS:1||METALINSULATORTRANSITION:1||SEMICONDUCTOR:1||FIELDEFFECT TRANSISTORS:1||ZEROVOLTAGE STATE:1||constanttemperature interlayer tunneling spectroscopy:1||Josephson supercurrent:1||BIPOLAR SUPERCURRENT:1||Interaction between Josephson and pancake vortices:1||flux jump:1||coaxial heterojunction nanorod:1||Natural Josephson coupling:1||BI2SR2CACU2O8+DELTA:1||VORTEX FLOW:1||TC SUPERCONDUCTORS:1||charge imbalance:1||Andreev diffractometer:1||intercalation:1||surface junction:1||Bi2212:1||tunnelling:1||GRAPHITE:1||GROWTH:1||collective transverse plasma modes:1||GAN:1||Macroscopic quantum tunneling:1||Fluctuation conductivity:1||Abovegap conductance jump:1||Josephson vortex motion:1||Intrinsic Josephson junctions:1||LAYERED SUPERCONDUCTORS:1||BI2SR2CACU2O8+Y:1||INTERFACES:1||BREAKDOWN:1||SYSTEMS:1||Anisotropy ratio:1||Josephson vortex:1||spin relaxation in superconductors:1||bibased single crystals:1||MESOSCOPIC PROXIMITY SUPERCONDUCTOR:1||reentrance of conductance:1||interlayer pair tunneling:1||JOSEPHSON:1||DISORDERED 2DIMENSIONAL SUPERCONDUCTORS:1||INDIUM FILMS:1||excited state:1||REGIME:1||triplet superconductivity:1||FILM:1||SCHOTTKY DIODES:1||peakdiphump structure:1||Kondo effect:1||REENTRANCE:1||Graphene:1||CONTACT:1||BERRYS PHASE:1||2DIMENSIONAL SUPERCONDUCTORS:1||Coulomb diamond:1||magnetic domain:1||spin injection:1||RESONANCE:1||plasma excitation modes:1||FLOW:1||OVERDOPED BI2SR2CACU2O8+DELTA:1||hole doping:1||chemical synthesis:1||phase transitions:1||superconductors:1||VORTEXGLASS SUPERCONDUCTIVITY:1||Kondorelated model:1||RADIATION:1||DOT:1||NANOBELTS:1||Complementarity:1||Closedloop AharonovBohm interferometer:1||pair breaking:1||interlayer phase fluctuation:1||MgB2 thin film:1||CONFINEMENT:1||WALLED CARBON NANOTUBES:1||TRANSITION:9||VORTICES:8||STATE:7||intrinsic Josephson junctions:7||SINGLECRYSTALS:7||JUNCTIONS:5||MODES:5||SUPERCURRENT:5||SUPERCONDUCTOR:5||CONDUCTANCE:5||HIGHTEMPERATURE SUPERCONDUCTORS:5||TRANSPORT:5||PHASE:5||FILMS:4||LOCALIZATION:4||SINGLE DIRAC CONE:4||WIRES:4||MAGNETICFIELD:4||STEPS:3||ELECTRONS:3||proximity effect:3||MODEL:3||ARRAYS:3||INTERFERENCE:3||fluxon dynamics:3||HETEROSTRUCTURES:3||INSULATOR:3||Andreev reflection:3||electronic transport:3||FISKE:3||superconductor:2||ZnO:2||quantum point contact:2||METAL:2||DYNAMICS:2||interlayer Josephson coupling:2||SUPERCONDUCTORS:2||YBA2CU3O7DELTA:2||LAYER:2||DOTS:2||quantum dot:2||Article:2||TRANSISTORS:2||CARBON NANOTUBES:2||GAP:2||MECHANISM:2||LINE:2||GIANT SHAPIRO STEPS:2||LAYERS:2||electron energy loss spectroscopy:2||physical phenomena:2||scanning electron microscopy:2||HGTE QUANTUMWELLS:2||BI2TE3:2||SPECTROSCOPY:2||PNJUNCTIONS:2||spinpolarized tunneling:2||INTRINSIC JOSEPHSONJUNCTIONS:2||FIELDS:2||positive magnetoresistance:2||dilute magnetic semiconductor:2||magnetic field:2||scanning transmission electron microscopy:2||QUANTUM OSCILLATIONS:2||TRANSPORTPROPERTIES:2||surface pair current:2||MAGNETORESISTANCE:2||NANORIBBONS:2||INSTABILITY:2||ANDREEV REFLECTION:2||microwave irradiation:2||vertical graphene josephson junction:2||BI2SE3:2||CONDUCTIVITY:2||highTc superconductors:2||DIMENSIONAL ELECTRONGAS:2||graphene:2||Topological insulators:2||Josephson coupling Fraunhofer interference pattern:2||FERROMAGNET:2||DEPENDENCE:2||DETECTOR:2||COHERENCE:2||INJECTION:2||GRAPHENE:1||JOSEPHSONJUNCTIONS:1||LAYERED SUPERCONDUCTOR:1||mode splitting:1||BEHAVIOR:1||spinpolarized transport:1||SUPERCONDUCTING TRANSITION:1||microwave response:1||PSEUDOGAP:1||phase coherence:1||TRANSITIONS:1||Long Josephson junction:1||Charge detection:1||collective resonance modes:1||plasma oscillation modes:1||Superconducting proximity effect:1||Iron pnictide superconductor:1||McMillanRowell oscillations:1||ferromagnetic microstructure:1||superradiant state:1||VOLTAGE:1||branch splitting:1||TENSOR:1||INTERCALATION:1||insitu fabrication:1||NDGAO3:1||DISORDERED METALS:1||GAUGE GLASS:1||LOWTEMPERATURE TRANSPORT:1||spontaneous spin polarization model:1||BIAS:1||emission of electromagnetic waves:1||YBA2CU3O7/PRBA2CU3O7 SUPERLATTICES:1||BOHM:1||SHAPIRO STEPS:1||superconductor/ferromagnet interface:1||OXIDE:1||ANDREEVREFLECTION:1||SinFeAsO single crystal:1||COLLECTIVE MOTION:1||ANGULARDEPENDENCE:1||SUPERCONDUCTIVITY:1||BILAYER GRAPHENE:1||PHOTOLUMINESCENT PROPERTIES:1||SUPERCONDUCTING WEAK LINKS:1||intrinsic Josephson junctions geometrical resonance:1||intrinsic Josephson junction:1||MESOSCOPIC SPINVALVE:1||Bi2212 single crystals:1||intrinsic junctions:1||ANDREEV REFLECTIONS:1||normalmetal/superconductor interface:1||IBI2SR2CACU2OY:1||THERMAL FLUCTUATIONS:1||MIXED STATE:1||BI2.15SR1.85CACU2O8+DELTA:1||intrinsic Josephson effects:1||CACUO:1||QUANTUM POINT CONTACTS:1||resonant tunneling state:1||coherence length:1||NANOWIRE:1||GATES:1||Phase line:1||Thermal activation:1||QUANTUMDOT:1||superconducting proximity effect:1||Andreev interferometer:1||WIRE:1||Josephsonvortexflow branches:1||Bi2212 cuprates:1||LATTICE:1||demannetization effect:1||SUPERCONDUCTING MIRRORS:1||GAS:1||VALLEY TRANSPORT:1||ELECTRODES:1||DEPENDENT TRANSPORT:1||BORNOPPENHEIMER APPROXIMATION:1||collective plasma oscillations:1||fluxon resonance steps:1||STACKS:1||COLLECTIVE DYNAMICS:1||PAIRING SYMMETRY:1||MUON SPIN ROTATION:1||DIMENSIONAL CROSSOVER:1||Bi2Sr2CaCu2Oy highTc superconductors:1||heterojunctions:1||nanostructures:1||surfaces and interfaces:1||QUANTUM TRANSPORT:1||MICROJUNCTIONS:1||RESONATORS:1||STATES:1||FIELD:1||FLUCTUATIONS:1||SCATTERING:1||mode splitting of Josephson vortexflow branches:1||2D superconductivity:1||TRANSISTOR:1||ENERGYGAP:1||SUPERLATTICES:1||IRONBASED SUPERCONDUCTORS:1||PHASEDEPENDENT RESISTANCE:1||QUANTUM PHASETRANSITIONS:1||ELECTRICFIELD:1||HIGH MAGNETICFIELDS:1||NANOWIRE HETEROSTRUCTURES:1||ZNO:1||pair breaking.:1||SUPERCONDUCTING PB:1||domain formation:1||FORCE MICROSCOPY:1||RELAXATION:1||PLASMA RESONANCE:1||coupled Josephson junctions:1||COPPEROXIDE SUPERCONDUCTORS:1||CROSSOVER:1||SIMULATIONS:1||LOWTEMPERATURE:1||CONDUCTORS:1||METALINSULATORTRANSITION:1||SEMICONDUCTOR:1||FIELDEFFECT TRANSISTORS:1||ZEROVOLTAGE STATE:1||constanttemperature interlayer tunneling spectroscopy:1||Josephson supercurrent:1||BIPOLAR SUPERCURRENT:1||Interaction between Josephson and pancake vortices:1||flux jump:1||coaxial heterojunction nanorod:1||Natural Josephson coupling:1||BI2SR2CACU2O8+DELTA:1||VORTEX FLOW:1||TC SUPERCONDUCTORS:1||charge imbalance:1||Andreev diffractometer:1||intercalation:1||surface junction:1||Bi2212:1||tunnelling:1||GRAPHITE:1||GROWTH:1||collective transverse plasma modes:1||GAN:1||Macroscopic quantum tunneling:1||Fluctuation conductivity:1||Abovegap conductance jump:1||Josephson vortex motion:1||Intrinsic Josephson junctions:1||LAYERED SUPERCONDUCTORS:1||BI2SR2CACU2O8+Y:1||INTERFACES:1||BREAKDOWN:1||SYSTEMS:1||Anisotropy ratio:1||Josephson vortex:1||spin relaxation in superconductors:1||bibased single crystals:1||MESOSCOPIC PROXIMITY SUPERCONDUCTOR:1||reentrance of conductance:1||interlayer pair tunneling:1||JOSEPHSON:1||DISORDERED 2DIMENSIONAL SUPERCONDUCTORS:1||INDIUM FILMS:1||excited state:1||REGIME:1||triplet superconductivity:1||FILM:1||SCHOTTKY DIODES:1||peakdiphump structure:1||Kondo effect:1||REENTRANCE:1||Graphene:1||CONTACT:1||BERRYS PHASE:1||2DIMENSIONAL SUPERCONDUCTORS:1||Coulomb diamond:1||magnetic domain:1||spin injection:1||RESONANCE:1||plasma excitation modes:1||FLOW:1||OVERDOPED BI2SR2CACU2O8+DELTA:1||hole doping:1||chemical synthesis:1||phase transitions:1||superconductors:1||VORTEXGLASS SUPERCONDUCTIVITY:1||Kondorelated model:1||RADIATION:1||DOT:1||NANOBELTS:1||Complementarity:1||Closedloop AharonovBohm interferometer:1||pair breaking:1||interlayer phase fluctuation:1||MgB2 thin film:1||CONFINEMENT:1||WALLED CARBON NANOTUBES:1||TRANSITION:9||VORTICES:8||STATE:7||intrinsic Josephson junctions:7||SINGLECRYSTALS:7||JUNCTIONS:5||MODES:5||SUPERCURRENT:5||SUPERCONDUCTOR:5||CONDUCTANCE:5||HIGHTEMPERATURE SUPERCONDUCTORS:5||TRANSPORT:5||PHASE:5||FILMS:4||LOCALIZATION:4||SINGLE DIRAC CONE:4||WIRES:4||MAGNETICFIELD:4||STEPS:3||ELECTRONS:3||proximity effect:3||MODEL:3||ARRAYS:3||INTERFERENCE:3||fluxon dynamics:3||HETEROSTRUCTURES:3||INSULATOR:3||Andreev reflection:3||electronic transport:3||FISKE:3||superconductor:2||ZnO:2||quantum point contact:2||METAL:2||DYNAMICS:2||interlayer Josephson coupling:2||SUPERCONDUCTORS:2||YBA2CU3O7DELTA:2||LAYER:2||DOTS:2||quantum dot:2||Article:2||TRANSISTORS:2||CARBON NANOTUBES:2||GAP:2||MECHANISM:2||LINE:2||GIANT SHAPIRO STEPS:2||LAYERS:2||electron energy loss spectroscopy:2||physical phenomena:2||scanning electron microscopy:2||HGTE QUANTUMWELLS:2||BI2TE3:2||SPECTROSCOPY:2||PNJUNCTIONS:2||spinpolarized tunneling:2||INTRINSIC JOSEPHSONJUNCTIONS:2||FIELDS:2||positive magnetoresistance:2||dilute magnetic semiconductor:2||magnetic field:2||scanning transmission electron microscopy:2||QUANTUM OSCILLATIONS:2||TRANSPORTPROPERTIES:2||surface pair current:2||MAGNETORESISTANCE:2||NANORIBBONS:2||INSTABILITY:2||ANDREEV REFLECTION:2||microwave irradiation:2||vertical graphene josephson junction:2||BI2SE3:2||CONDUCTIVITY:2||highTc superconductors:2||DIMENSIONAL ELECTRONGAS:2||graphene:2||Topological insulators:2||Josephson coupling Fraunhofer interference pattern:2||FERROMAGNET:2||DEPENDENCE:2||DETECTOR:2||COHERENCE:2||INJECTION:2||GRAPHENE:1||JOSEPHSONJUNCTIONS:1||LAYERED SUPERCONDUCTOR:1||mode splitting:1||BEHAVIOR:1||spinpolarized transport:1||SUPERCONDUCTING TRANSITION:1||microwave response:1||PSEUDOGAP:1||phase coherence:1||TRANSITIONS:1||Long Josephson junction:1||Charge detection:1||collective resonance modes:1||plasma oscillation modes:1||Superconducting proximity effect:1||Iron pnictide superconductor:1||McMillanRowell oscillations:1||ferromagnetic microstructure:1||superradiant state:1||VOLTAGE:1||branch splitting:1||TENSOR:1||INTERCALATION:1||insitu fabrication:1||NDGAO3:1||DISORDERED METALS:1||GAUGE GLASS:1||LOWTEMPERATURE TRANSPORT:1||spontaneous spin polarization model:1||BIAS:1||emission of electromagnetic waves:1||YBA2CU3O7/PRBA2CU3O7 SUPERLATTICES:1||BOHM:1||SHAPIRO STEPS:1||superconductor/ferromagnet interface:1||OXIDE:1||ANDREEVREFLECTION:1||SinFeAsO single crystal:1||COLLECTIVE MOTION:1||ANGULARDEPENDENCE:1||SUPERCONDUCTIVITY:1||BILAYER GRAPHENE:1||PHOTOLUMINESCENT PROPERTIES:1||SUPERCONDUCTING WEAK LINKS:1||intrinsic Josephson junctions geometrical resonance:1||intrinsic Josephson junction:1||MESOSCOPIC SPINVALVE:1||Bi2212 single crystals:1||intrinsic junctions:1||ANDREEV REFLECTIONS:1||normalmetal/superconductor interface:1||IBI2SR2CACU2OY:1||THERMAL FLUCTUATIONS:1||MIXED STATE:1||BI2.15SR1.85CACU2O8+DELTA:1||intrinsic Josephson effects:1||CACUO:1||QUANTUM POINT CONTACTS:1||resonant tunneling state:1||coherence length:1||NANOWIRE:1||GATES:1||Phase line:1||Thermal activation:1||QUANTUMDOT:1||superconducting proximity effect:1||Andreev interferometer:1||WIRE:1||Josephsonvortexflow branches:1||Bi2212 cuprates:1||LATTICE:1||demannetization effect:1||SUPERCONDUCTING MIRRORS:1||GAS:1||VALLEY TRANSPORT:1||ELECTRODES:1||DEPENDENT TRANSPORT:1||BORNOPPENHEIMER APPROXIMATION:1||collective plasma oscillations:1||fluxon resonance steps:1||STACKS:1||COLLECTIVE DYNAMICS:1||PAIRING SYMMETRY:1||MUON SPIN ROTATION:1||DIMENSIONAL CROSSOVER:1||Bi2Sr2CaCu2Oy highTc superconductors:1||heterojunctions:1||nanostructures:1||surfaces and interfaces:1||QUANTUM TRANSPORT:1||MICROJUNCTIONS:1||RESONATORS:1||STATES:1||FIELD:1||FLUCTUATIONS:1||SCATTERING:1||mode splitting of Josephson vortexflow branches:1||2D superconductivity:1||TRANSISTOR:1||ENERGYGAP:1||SUPERLATTICES:1||IRONBASED SUPERCONDUCTORS:1||PHASEDEPENDENT RESISTANCE:1||QUANTUM PHASETRANSITIONS:1||ELECTRICFIELD:1||HIGH MAGNETICFIELDS:1||NANOWIRE HETEROSTRUCTURES:1||ZNO:1||pair breaking.:1||SUPERCONDUCTING PB:1||domain formation:1||FORCE MICROSCOPY:1||RELAXATION:1||PLASMA RESONANCE:1||coupled Josephson junctions:1||COPPEROXIDE SUPERCONDUCTORS:1||CROSSOVER:1||SIMULATIONS:1||LOWTEMPERATURE:1||CONDUCTORS:1||METALINSULATORTRANSITION:1||SEMICONDUCTOR:1||FIELDEFFECT TRANSISTORS:1||ZEROVOLTAGE STATE:1||constanttemperature interlayer tunneling spectroscopy:1||Josephson supercurrent:1||BIPOLAR SUPERCURRENT:1||Interaction between Josephson and pancake vortices:1||flux jump:1||coaxial heterojunction nanorod:1||Natural Josephson coupling:1||BI2SR2CACU2O8+DELTA:1||VORTEX FLOW:1||TC SUPERCONDUCTORS:1||charge imbalance:1||Andreev diffractometer:1||intercalation:1||surface junction:1||Bi2212:1||tunnelling:1||GRAPHITE:1||GROWTH:1||collective transverse plasma modes:1||GAN:1||Macroscopic quantum tunneling:1||Fluctuation conductivity:1||Abovegap conductance jump:1||Josephson vortex motion:1||Intrinsic Josephson junctions:1||LAYERED SUPERCONDUCTORS:1||BI2SR2CACU2O8+Y:1||INTERFACES:1||BREAKDOWN:1||SYSTEMS:1||Anisotropy ratio:1||Josephson vortex:1||spin relaxation in superconductors:1||bibased single crystals:1||MESOSCOPIC PROXIMITY SUPERCONDUCTOR:1||reentrance of conductance:1||interlayer pair tunneling:1||JOSEPHSON:1||DISORDERED 2DIMENSIONAL SUPERCONDUCTORS:1||INDIUM FILMS:1||excited state:1||REGIME:1||triplet superconductivity:1||FILM:1||SCHOTTKY DIODES:1||peakdiphump structure:1||Kondo effect:1||REENTRANCE:1||Graphene:1||CONTACT:1||BERRYS PHASE:1||2DIMENSIONAL SUPERCONDUCTORS:1||Coulomb diamond:1||magnetic domain:1||spin injection:1||RESONANCE:1||plasma excitation modes:1||FLOW:1||OVERDOPED BI2SR2CACU2O8+DELTA:1||hole doping:1||chemical synthesis:1||phase transitions:1||superconductors:1||VORTEXGLASS SUPERCONDUCTIVITY:1||Kondorelated model:1||RADIATION:1||DOT:1||NANOBELTS:1||Complementarity:1||Closedloop AharonovBohm interferometer:1||pair breaking:1||interlayer phase fluctuation:1||MgB2 thin film:1||CONFINEMENT:1||WALLED CARBON NANOTUBES:1||TRANSITION:9||VORTICES:8||STATE:7||intrinsic Josephson junctions:7||SINGLECRYSTALS:7||JUNCTIONS:5||MODES:5||SUPERCURRENT:5||SUPERCONDUCTOR:5||CONDUCTANCE:5||HIGHTEMPERATURE SUPERCONDUCTORS:5||TRANSPORT:5||PHASE:5||FILMS:4||LOCALIZATION:4||SINGLE DIRAC CONE:4||WIRES:4||MAGNETICFIELD:4||STEPS:3||ELECTRONS:3||proximity effect:3||MODEL:3||ARRAYS:3||INTERFERENCE:3||fluxon dynamics:3||HETEROSTRUCTURES:3||INSULATOR:3||Andreev reflection:3||electronic transport:3||FISKE:3||superconductor:2||ZnO:2||quantum point contact:2||METAL:2||DYNAMICS:2||interlayer Josephson coupling:2||SUPERCONDUCTORS:2||YBA2CU3O7DELTA:2||LAYER:2||DOTS:2||quantum dot:2||Article:2||TRANSISTORS:2||CARBON NANOTUBES:2||GAP:2||MECHANISM:2||LINE:2||GIANT SHAPIRO STEPS:2||LAYERS:2||electron energy loss spectroscopy:2||physical phenomena:2||scanning electron microscopy:2||HGTE QUANTUMWELLS:2||BI2TE3:2||SPECTROSCOPY:2||PNJUNCTIONS:2||spinpolarized tunneling:2||INTRINSIC JOSEPHSONJUNCTIONS:2||FIELDS:2||positive magnetoresistance:2||dilute magnetic semiconductor:2||magnetic field:2||scanning transmission electron microscopy:2||QUANTUM OSCILLATIONS:2||TRANSPORTPROPERTIES:2||surface pair current:2||MAGNETORESISTANCE:2||NANORIBBONS:2||INSTABILITY:2||ANDREEV REFLECTION:2||microwave irradiation:2||vertical graphene josephson junction:2||BI2SE3:2||CONDUCTIVITY:2||highTc superconductors:2||DIMENSIONAL ELECTRONGAS:2||graphene:2||Topological insulators:2||Josephson coupling Fraunhofer interference pattern:2||FERROMAGNET:2||DEPENDENCE:2||DETECTOR:2||COHERENCE:2||INJECTION:2||GRAPHENE:1||JOSEPHSONJUNCTIONS:1||LAYERED SUPERCONDUCTOR:1||mode splitting:1||BEHAVIOR:1||spinpolarized transport:1||SUPERCONDUCTING TRANSITION:1||microwave response:1||PSEUDOGAP:1||phase coherence:1||TRANSITIONS:1||Long Josephson junction:1||Charge detection:1||collective resonance modes:1||plasma oscillation modes:1||Superconducting proximity effect:1||Iron pnictide superconductor:1||McMillanRowell oscillations:1||ferromagnetic microstructure:1||superradiant state:1||VOLTAGE:1||branch splitting:1||TENSOR:1||INTERCALATION:1||insitu fabrication:1||NDGAO3:1||DISORDERED METALS:1||GAUGE GLASS:1||LOWTEMPERATURE TRANSPORT:1||spontaneous spin polarization model:1||BIAS:1||emission of electromagnetic waves:1||YBA2CU3O7/PRBA2CU3O7 SUPERLATTICES:1||BOHM:1||SHAPIRO STEPS:1||superconductor/ferromagnet interface:1||OXIDE:1||ANDREEVREFLECTION:1||SinFeAsO single crystal:1||COLLECTIVE MOTION:1||ANGULARDEPENDENCE:1||SUPERCONDUCTIVITY:1||BILAYER GRAPHENE:1||PHOTOLUMINESCENT PROPERTIES:1||SUPERCONDUCTING WEAK LINKS:1||intrinsic Josephson junctions geometrical resonance:1||intrinsic Josephson junction:1||MESOSCOPIC SPINVALVE:1||Bi2212 single crystals:1||intrinsic junctions:1||ANDREEV REFLECTIONS:1||normalmetal/superconductor interface:1||IBI2SR2CACU2OY:1||THERMAL FLUCTUATIONS:1||MIXED STATE:1||BI2.15SR1.85CACU2O8+DELTA:1||intrinsic Josephson effects:1||CACUO:1||QUANTUM POINT CONTACTS:1||resonant tunneling state:1||coherence length:1||NANOWIRE:1||GATES:1||Phase line:1||Thermal activation:1||QUANTUMDOT:1||superconducting proximity effect:1||Andreev interferometer:1||WIRE:1||Josephsonvortexflow branches:1||Bi2212 cuprates:1||LATTICE:1||demannetization effect:1||SUPERCONDUCTING MIRRORS:1||GAS:1||VALLEY TRANSPORT:1||ELECTRODES:1||DEPENDENT TRANSPORT:1||BORNOPPENHEIMER APPROXIMATION:1||collective plasma oscillations:1||fluxon resonance steps:1||STACKS:1||COLLECTIVE DYNAMICS:1||PAIRING SYMMETRY:1||MUON SPIN ROTATION:1||DIMENSIONAL CROSSOVER:1||Bi2Sr2CaCu2Oy highTc superconductors:1||heterojunctions:1||nanostructures:1||surfaces and interfaces:1||QUANTUM TRANSPORT:1||MICROJUNCTIONS:1||RESONATORS:1||STATES:1||FIELD:1||FLUCTUATIONS:1||SCATTERING:1||mode splitting of Josephson vortexflow branches:1||2D superconductivity:1||TRANSISTOR:1||ENERGYGAP:1||SUPERLATTICES:1||IRONBASED SUPERCONDUCTORS:1||PHASEDEPENDENT RESISTANCE:1||QUANTUM PHASETRANSITIONS:1||ELECTRICFIELD:1||HIGH MAGNETICFIELDS:1||NANOWIRE HETEROSTRUCTURES:1||ZNO:1||pair breaking.:1||SUPERCONDUCTING PB:1||domain formation:1||FORCE MICROSCOPY:1||RELAXATION:1||PLASMA RESONANCE:1||coupled Josephson junctions:1||COPPEROXIDE SUPERCONDUCTORS:1||CROSSOVER:1||SIMULATIONS:1||LOWTEMPERATURE:1||CONDUCTORS:1||METALINSULATORTRANSITION:1||SEMICONDUCTOR:1||FIELDEFFECT TRANSISTORS:1||ZEROVOLTAGE STATE:1||constanttemperature interlayer tunneling spectroscopy:1||Josephson supercurrent:1||BIPOLAR SUPERCURRENT:1||Interaction between Josephson and pancake vortices:1||flux jump:1||coaxial heterojunction nanorod:1||Natural Josephson coupling:1||BI2SR2CACU2O8+DELTA:1||VORTEX FLOW:1||TC SUPERCONDUCTORS:1||charge imbalance:1||Andreev diffractometer:1||intercalation:1||surface junction:1||Bi2212:1||tunnelling:1||GRAPHITE:1||GROWTH:1||collective transverse plasma modes:1||GAN:1||Macroscopic quantum tunneling:1||Fluctuation conductivity:1||Abovegap conductance jump:1||Josephson vortex motion:1||Intrinsic Josephson junctions:1||LAYERED SUPERCONDUCTORS:1||BI2SR2CACU2O8+Y:1||INTERFACES:1||BREAKDOWN:1||SYSTEMS:1||Anisotropy ratio:1||Josephson vortex:1||spin relaxation in superconductors:1||bibased single crystals:1||MESOSCOPIC PROXIMITY SUPERCONDUCTOR:1||reentrance of conductance:1||interlayer pair tunneling:1||JOSEPHSON:1||DISORDERED 2DIMENSIONAL SUPERCONDUCTORS:1||INDIUM FILMS:1||excited state:1||REGIME:1||triplet superconductivity:1||FILM:1||SCHOTTKY DIODES:1||peakdiphump structure:1||Kondo effect:1||REENTRANCE:1||Graphene:1||CONTACT:1||BERRYS PHASE:1||2DIMENSIONAL SUPERCONDUCTORS:1||Coulomb diamond:1||magnetic domain:1||spin injection:1||RESONANCE:1||plasma excitation modes:1||FLOW:1||OVERDOPED BI2SR2CACU2O8+DELTA:1||hole doping:1||chemical synthesis:1||phase transitions:1||superconductors:1||VORTEXGLASS SUPERCONDUCTIVITY:1||Kondorelated model:1||RADIATION:1||DOT:1||NANOBELTS:1||Complementarity:1||Closedloop AharonovBohm interferometer:1||pair breaking:1||interlayer phase fluctuation:1||MgB2 thin film:1||CONFINEMENT:1||WALLED CARBON NANOTUBES:1||TRANSITION:9||VORTICES:8||STATE:7||intrinsic Josephson junctions:7||SINGLECRYSTALS:7||JUNCTIONS:5||MODES:5||SUPERCURRENT:5||SUPERCONDUCTOR:5||CONDUCTANCE:5||HIGHTEMPERATURE SUPERCONDUCTORS:5||TRANSPORT:5||PHASE:5||FILMS:4||LOCALIZATION:4||SINGLE DIRAC CONE:4||WIRES:4||MAGNETICFIELD:4||STEPS:3||ELECTRONS:3||proximity effect:3||MODEL:3||ARRAYS:3||INTERFERENCE:3||fluxon dynamics:3||HETEROSTRUCTURES:3||INSULATOR:3||Andreev reflection:3||electronic transport:3||FISKE:3||superconductor:2||ZnO:2||quantum point contact:2||METAL:2||DYNAMICS:2||interlayer Josephson coupling:2||SUPERCONDUCTORS:2||YBA2CU3O7DELTA:2||LAYER:2||DOTS:2||quantum dot:2||Article:2||TRANSISTORS:2||CARBON NANOTUBES:2||GAP:2||MECHANISM:2||LINE:2||GIANT SHAPIRO STEPS:2||LAYERS:2||electron energy loss spectroscopy:2||physical phenomena:2||scanning electron microscopy:2||HGTE QUANTUMWELLS:2||BI2TE3:2||SPECTROSCOPY:2||PNJUNCTIONS:2||spinpolarized tunneling:2||INTRINSIC JOSEPHSONJUNCTIONS:2||FIELDS:2||positive magnetoresistance:2||dilute magnetic semiconductor:2||magnetic field:2||scanning transmission electron microscopy:2||QUANTUM OSCILLATIONS:2||TRANSPORTPROPERTIES:2||surface pair current:2||MAGNETORESISTANCE:2||NANORIBBONS:2||INSTABILITY:2||ANDREEV REFLECTION:2||microwave irradiation:2||vertical graphene josephson junction:2||BI2SE3:2||CONDUCTIVITY:2||highTc superconductors:2||DIMENSIONAL ELECTRONGAS:2||graphene:2||Topological insulators:2||Josephson coupling Fraunhofer interference pattern:2||FERROMAGNET:2||DEPENDENCE:2||DETECTOR:2||COHERENCE:2||INJECTION:2||GRAPHENE:1||JOSEPHSONJUNCTIONS:1||LAYERED SUPERCONDUCTOR:1||mode splitting:1||BEHAVIOR:1||spinpolarized transport:1||SUPERCONDUCTING TRANSITION:1||microwave response:1||PSEUDOGAP:1||phase coherence:1||TRANSITIONS:1||Long Josephson junction:1||Charge detection:1||collective resonance modes:1||plasma oscillation modes:1||Superconducting proximity effect:1||Iron pnictide superconductor:1||McMillanRowell oscillations:1||ferromagnetic microstructure:1||superradiant state:1||VOLTAGE:1||branch splitting:1||TENSOR:1||INTERCALATION:1||insitu fabrication:1||NDGAO3:1||DISORDERED METALS:1||GAUGE GLASS:1||LOWTEMPERATURE TRANSPORT:1||spontaneous spin polarization model:1||BIAS:1||emission of electromagnetic waves:1||YBA2CU3O7/PRBA2CU3O7 SUPERLATTICES:1||BOHM:1||SHAPIRO STEPS:1||superconductor/ferromagnet interface:1||OXIDE:1||ANDREEVREFLECTION:1||SinFeAsO single crystal:1||COLLECTIVE MOTION:1||ANGULARDEPENDENCE:1||SUPERCONDUCTIVITY:1||BILAYER GRAPHENE:1||PHOTOLUMINESCENT PROPERTIES:1||SUPERCONDUCTING WEAK LINKS:1||intrinsic Josephson junctions geometrical resonance:1||intrinsic Josephson junction:1||MESOSCOPIC SPINVALVE:1||Bi2212 single crystals:1||intrinsic junctions:1||ANDREEV REFLECTIONS:1||normalmetal/superconductor interface:1||IBI2SR2CACU2OY:1||THERMAL FLUCTUATIONS:1||MIXED STATE:1||BI2.15SR1.85CACU2O8+DELTA:1||intrinsic Josephson effects:1||CACUO:1||QUANTUM POINT CONTACTS:1||resonant tunneling state:1||coherence length:1||NANOWIRE:1||GATES:1||Phase line:1||Thermal activation:1||QUANTUMDOT:1||superconducting proximity effect:1||Andreev interferometer:1||WIRE:1||Josephsonvortexflow branches:1||Bi2212 cuprates:1||LATTICE:1||demannetization effect:1||SUPERCONDUCTING MIRRORS:1||GAS:1||VALLEY TRANSPORT:1||ELECTRODES:1||DEPENDENT TRANSPORT:1||BORNOPPENHEIMER APPROXIMATION:1||collective plasma oscillations:1||fluxon resonance steps:1||STACKS:1||COLLECTIVE DYNAMICS:1||PAIRING SYMMETRY:1||MUON SPIN ROTATION:1||DIMENSIONAL CROSSOVER:1||Bi2Sr2CaCu2Oy highTc superconductors:1||heterojunctions:1||nanostructures:1||surfaces and interfaces:1||QUANTUM TRANSPORT:1||MICROJUNCTIONS:1||RESONATORS:1||STATES:1||FIELD:1||FLUCTUATIONS:1||SCATTERING:1||mode splitting of Josephson vortexflow branches:1||2D superconductivity:1||TRANSISTOR:1||ENERGYGAP:1||SUPERLATTICES:1||IRONBASED SUPERCONDUCTORS:1||PHASEDEPENDENT RESISTANCE:1||QUANTUM PHASETRANSITIONS:1||ELECTRICFIELD:1||HIGH MAGNETICFIELDS:1||NANOWIRE HETEROSTRUCTURES:1||ZNO:1||pair breaking.:1||SUPERCONDUCTING PB:1||domain formation:1||FORCE MICROSCOPY:1||RELAXATION:1||PLASMA RESONANCE:1||coupled Josephson junctions:1||COPPEROXIDE SUPERCONDUCTORS:1||CROSSOVER:1||SIMULATIONS:1||LOWTEMPERATURE:1||CONDUCTORS:1||METALINSULATORTRANSITION:1||SEMICONDUCTOR:1||FIELDEFFECT TRANSISTORS:1||ZEROVOLTAGE STATE:1||constanttemperature interlayer tunneling spectroscopy:1||Josephson supercurrent:1||BIPOLAR SUPERCURRENT:1||Interaction between Josephson and pancake vortices:1||flux jump:1||coaxial heterojunction nanorod:1||Natural Josephson coupling:1||BI2SR2CACU2O8+DELTA:1||VORTEX FLOW:1||TC SUPERCONDUCTORS:1||charge imbalance:1||Andreev diffractometer:1||intercalation:1||surface junction:1||Bi2212:1||tunnelling:1||GRAPHITE:1||GROWTH:1||collective transverse plasma modes:1||GAN:1||Macroscopic quantum tunneling:1||Fluctuation conductivity:1||Abovegap conductance jump:1||Josephson vortex motion:1||Intrinsic Josephson junctions:1||LAYERED SUPERCONDUCTORS:1||BI2SR2CACU2O8+Y:1||INTERFACES:1||BREAKDOWN:1||SYSTEMS:1||Anisotropy ratio:1||Josephson vortex:1||spin relaxation in superconductors:1||bibased single crystals:1||MESOSCOPIC PROXIMITY SUPERCONDUCTOR:1||reentrance of conductance:1||interlayer pair tunneling:1||JOSEPHSON:1||DISORDERED 2DIMENSIONAL SUPERCONDUCTORS:1||INDIUM FILMS:1||excited state:1||REGIME:1||triplet superconductivity:1||FILM:1||SCHOTTKY DIODES:1||peakdiphump structure:1||Kondo effect:1||REENTRANCE:1||Graphene:1||CONTACT:1||BERRYS PHASE:1||2DIMENSIONAL SUPERCONDUCTORS:1||Coulomb diamond:1||magnetic domain:1||spin injection:1||RESONANCE:1||plasma excitation modes:1||FLOW:1||OVERDOPED BI2SR2CACU2O8+DELTA:1||hole doping:1||chemical synthesis:1||phase transitions:1||superconductors:1||VORTEXGLASS SUPERCONDUCTIVITY:1||Kondorelated model:1||RADIATION:1||DOT:1||NANOBELTS:1||Complementarity:1||Closedloop AharonovBohm interferometer:1||pair breaking:1||interlayer phase fluctuation:1||MgB2 thin film:1||CONFINEMENT:1||WALLED CARBON NANOTUBES:1||TRANSITION:9||VORTICES:8||STATE:7||intrinsic Josephson junctions:7||SINGLECRYSTALS:7||JUNCTIONS:5||MODES:5||SUPERCURRENT:5||SUPERCONDUCTOR:5||CONDUCTANCE:5||HIGHTEMPERATURE SUPERCONDUCTORS:5||TRANSPORT:5||PHASE:5||FILMS:4||LOCALIZATION:4||SINGLE DIRAC CONE:4||WIRES:4||MAGNETICFIELD:4||STEPS:3||ELECTRONS:3||proximity effect:3||MODEL:3||ARRAYS:3||INTERFERENCE:3||fluxon dynamics:3||HETEROSTRUCTURES:3||INSULATOR:3||Andreev reflection:3||electronic transport:3||FISKE:3||superconductor:2||ZnO:2||quantum point contact:2||METAL:2||DYNAMICS:2||interlayer Josephson coupling:2||SUPERCONDUCTORS:2||YBA2CU3O7DELTA:2||LAYER:2||DOTS:2||quantum dot:2||Article:2||TRANSISTORS:2||CARBON NANOTUBES:2||GAP:2||MECHANISM:2||LINE:2||GIANT SHAPIRO STEPS:2||LAYERS:2||electron energy loss spectroscopy:2||physical phenomena:2||scanning electron microscopy:2||HGTE QUANTUMWELLS:2||BI2TE3:2||SPECTROSCOPY:2||PNJUNCTIONS:2||spinpolarized tunneling:2||INTRINSIC JOSEPHSONJUNCTIONS:2||FIELDS:2||positive magnetoresistance:2||dilute magnetic semiconductor:2||magnetic field:2||scanning transmission electron microscopy:2||QUANTUM OSCILLATIONS:2||TRANSPORTPROPERTIES:2||surface pair current:2||MAGNETORESISTANCE:2||NANORIBBONS:2||INSTABILITY:2||ANDREEV REFLECTION:2||microwave irradiation:2||vertical graphene josephson junction:2||BI2SE3:2||CONDUCTIVITY:2||highTc superconductors:2||DIMENSIONAL ELECTRONGAS:2||graphene:2||Topological insulators:2||Josephson coupling Fraunhofer interference pattern:2||FERROMAGNET:2||DEPENDENCE:2||DETECTOR:2||COHERENCE:2||INJECTION:2||GRAPHENE:1||JOSEPHSONJUNCTIONS:1||LAYERED SUPERCONDUCTOR:1||mode splitting:1||BEHAVIOR:1||spinpolarized transport:1||SUPERCONDUCTING TRANSITION:1||microwave response:1||PSEUDOGAP:1||phase coherence:1||TRANSITIONS:1||Long Josephson junction:1||Charge detection:1||collective resonance modes:1||plasma oscillation modes:1||Superconducting proximity effect:1||Iron pnictide superconductor:1||McMillanRowell oscillations:1||ferromagnetic microstructure:1||superradiant state:1||VOLTAGE:1||branch splitting:1||TENSOR:1||INTERCALATION:1||insitu fabrication:1||NDGAO3:1||DISORDERED METALS:1||GAUGE GLASS:1||LOWTEMPERATURE TRANSPORT:1||spontaneous spin polarization model:1||BIAS:1||emission of electromagnetic waves:1||YBA2CU3O7/PRBA2CU3O7 SUPERLATTICES:1||BOHM:1||SHAPIRO STEPS:1||superconductor/ferromagnet interface:1||OXIDE:1||ANDREEVREFLECTION:1||SinFeAsO single crystal:1||COLLECTIVE MOTION:1||ANGULARDEPENDENCE:1||SUPERCONDUCTIVITY:1||BILAYER GRAPHENE:1||PHOTOLUMINESCENT PROPERTIES:1||SUPERCONDUCTING WEAK LINKS:1||intrinsic Josephson junctions geometrical resonance:1||intrinsic Josephson junction:1||MESOSCOPIC SPINVALVE:1||Bi2212 single crystals:1||intrinsic junctions:1||ANDREEV REFLECTIONS:1||normalmetal/superconductor interface:1||IBI2SR2CACU2OY:1||THERMAL FLUCTUATIONS:1||MIXED STATE:1||BI2.15SR1.85CACU2O8+DELTA:1||intrinsic Josephson effects:1||CACUO:1||QUANTUM POINT CONTACTS:1||resonant tunneling state:1||coherence length:1||NANOWIRE:1||GATES:1||Phase line:1||Thermal activation:1||QUANTUMDOT:1||superconducting proximity effect:1||Andreev interferometer:1||WIRE:1||Josephsonvortexflow branches:1||Bi2212 cuprates:1||LATTICE:1||demannetization effect:1||SUPERCONDUCTING MIRRORS:1||GAS:1||VALLEY TRANSPORT:1||ELECTRODES:1||DEPENDENT TRANSPORT:1||BORNOPPENHEIMER APPROXIMATION:1||collective plasma oscillations:1||fluxon resonance steps:1||STACKS:1||COLLECTIVE DYNAMICS:1||PAIRING SYMMETRY:1||MUON SPIN ROTATION:1||DIMENSIONAL CROSSOVER:1||Bi2Sr2CaCu2Oy highTc superconductors:1||heterojunctions:1||nanostructures:1||surfaces and interfaces:1||QUANTUM TRANSPORT:1||MICROJUNCTIONS:1||RESONATORS:1||STATES:1||FIELD:1||FLUCTUATIONS:1||SCATTERING:1||mode splitting of Josephson vortexflow branches:1||2D superconductivity:1||TRANSISTOR:1||ENERGYGAP:1||SUPERLATTICES:1||IRONBASED SUPERCONDUCTORS:1||PHASEDEPENDENT RESISTANCE:1||QUANTUM PHASETRANSITIONS:1||ELECTRICFIELD:1||HIGH MAGNETICFIELDS:1||NANOWIRE HETEROSTRUCTURES:1||ZNO:1||pair breaking.:1||SUPERCONDUCTING PB:1||domain formation:1||FORCE MICROSCOPY:1||RELAXATION:1||PLASMA RESONANCE:1||coupled Josephson junctions:1||COPPEROXIDE SUPERCONDUCTORS:1||CROSSOVER:1||SIMULATIONS:1||LOWTEMPERATURE:1||CONDUCTORS:1||METALINSULATORTRANSITION:1||SEMICONDUCTOR:1||FIELDEFFECT TRANSISTORS:1||ZEROVOLTAGE STATE:1||constanttemperature interlayer tunneling spectroscopy:1||Josephson supercurrent:1||BIPOLAR SUPERCURRENT:1||Interaction between Josephson and pancake vortices:1||flux jump:1||coaxial heterojunction nanorod:1||Natural Josephson coupling:1||BI2SR2CACU2O8+DELTA:1||VORTEX FLOW:1||TC SUPERCONDUCTORS:1||charge imbalance:1||Andreev diffractometer:1||intercalation:1||surface junction:1||Bi2212:1||tunnelling:1||GRAPHITE:1||GROWTH:1||collective transverse plasma modes:1||GAN:1||Macroscopic quantum tunneling:1||Fluctuation conductivity:1||Abovegap conductance jump:1||Josephson vortex motion:1||Intrinsic Josephson junctions:1||LAYERED SUPERCONDUCTORS:1||BI2SR2CACU2O8+Y:1||INTERFACES:1||BREAKDOWN:1||SYSTEMS:1||Anisotropy ratio:1||Josephson vortex:1||spin relaxation in superconductors:1||bibased single crystals:1||MESOSCOPIC PROXIMITY SUPERCONDUCTOR:1||reentrance of conductance:1||interlayer pair tunneling:1||JOSEPHSON:1||DISORDERED 2DIMENSIONAL SUPERCONDUCTORS:1||INDIUM FILMS:1||excited state:1||REGIME:1||triplet superconductivity:1||FILM:1||SCHOTTKY DIODES:1||peakdiphump structure:1||Kondo effect:1||REENTRANCE:1||Graphene:1||CONTACT:1||BERRYS PHASE:1||2DIMENSIONAL SUPERCONDUCTORS:1||Coulomb diamond:1||magnetic domain:1||spin injection:1||RESONANCE:1||plasma excitation modes:1||FLOW:1||OVERDOPED BI2SR2CACU2O8+DELTA:1||hole doping:1||chemical synthesis:1||phase transitions:1||superconductors:1||VORTEXGLASS SUPERCONDUCTIVITY:1||Kondorelated model:1||RADIATION:1||DOT:1||NANOBELTS:1||Complementarity:1||Closedloop AharonovBohm interferometer:1||pair breaking:1||interlayer phase fluctuation:1||MgB2 thin film:1||CONFINEMENT:1||WALLED CARBON NANOTUBES:1||TRANSITION:9||VORTICES:8||STATE:7||intrinsic Josephson junctions:7||SINGLECRYSTALS:7||JUNCTIONS:5||MODES:5||SUPERCURRENT:5||SUPERCONDUCTOR:5||CONDUCTANCE:5||HIGHTEMPERATURE SUPERCONDUCTORS:5||TRANSPORT:5||PHASE:5||FILMS:4||LOCALIZATION:4||SINGLE DIRAC CONE:4||WIRES:4||MAGNETICFIELD:4||STEPS:3||ELECTRONS:3||proximity effect:3||MODEL:3||ARRAYS:3||INTERFERENCE:3||fluxon dynamics:3||HETEROSTRUCTURES:3||INSULATOR:3||Andreev reflection:3||electronic transport:3||FISKE:3||superconductor:2||ZnO:2||quantum point contact:2||METAL:2||DYNAMICS:2||interlayer Josephson coupling:2||SUPERCONDUCTORS:2||YBA2CU3O7DELTA:2||LAYER:2||DOTS:2||quantum dot:2||Article:2||TRANSISTORS:2||CARBON NANOTUBES:2||GAP:2||MECHANISM:2||LINE:2||GIANT SHAPIRO STEPS:2||LAYERS:2||electron energy loss spectroscopy:2||physical phenomena:2||scanning electron microscopy:2||HGTE QUANTUMWELLS:2||BI2TE3:2||SPECTROSCOPY:2||PNJUNCTIONS:2||spinpolarized tunneling:2||INTRINSIC JOSEPHSONJUNCTIONS:2||FIELDS:2||positive magnetoresistance:2||dilute magnetic semiconductor:2||magnetic field:2||scanning transmission electron microscopy:2||QUANTUM OSCILLATIONS:2||TRANSPORTPROPERTIES:2||surface pair current:2||MAGNETORESISTANCE:2||NANORIBBONS:2||INSTABILITY:2||ANDREEV REFLECTION:2||microwave irradiation:2||vertical graphene josephson junction:2||BI2SE3:2||CONDUCTIVITY:2||highTc superconductors:2||DIMENSIONAL ELECTRONGAS:2||graphene:2||Topological insulators:2||Josephson coupling Fraunhofer interference pattern:2||FERROMAGNET:2||DEPENDENCE:2||DETECTOR:2||COHERENCE:2||INJECTION:2||GRAPHENE:1||JOSEPHSONJUNCTIONS:1||LAYERED SUPERCONDUCTOR:1||mode splitting:1||BEHAVIOR:1||spinpolarized transport:1||SUPERCONDUCTING TRANSITION:1||microwave response:1||PSEUDOGAP:1||phase coherence:1||TRANSITIONS:1||Long Josephson junction:1||Charge detection:1||collective resonance modes:1||plasma oscillation modes:1||Superconducting proximity effect:1||Iron pnictide superconductor:1||McMillanRowell oscillations:1||ferromagnetic microstructure:1||superradiant state:1||VOLTAGE:1||branch splitting:1||TENSOR:1||INTERCALATION:1||insitu fabrication:1||NDGAO3:1||DISORDERED METALS:1||GAUGE GLASS:1||LOWTEMPERATURE TRANSPORT:1||spontaneous spin polarization model:1||BIAS:1||emission of electromagnetic waves:1||YBA2CU3O7/PRBA2CU3O7 SUPERLATTICES:1||BOHM:1||SHAPIRO STEPS:1||superconductor/ferromagnet interface:1||OXIDE:1||ANDREEVREFLECTION:1||SinFeAsO single crystal:1||COLLECTIVE MOTION:1||ANGULARDEPENDENCE:1||SUPERCONDUCTIVITY:1||BILAYER GRAPHENE:1||PHOTOLUMINESCENT PROPERTIES:1||SUPERCONDUCTING WEAK LINKS:1||intrinsic Josephson junctions geometrical resonance:1||intrinsic Josephson junction:1||MESOSCOPIC SPINVALVE:1||Bi2212 single crystals:1||intrinsic junctions:1||ANDREEV REFLECTIONS:1||normalmetal/superconductor interface:1||IBI2SR2CACU2OY:1||THERMAL FLUCTUATIONS:1||MIXED STATE:1||BI2.15SR1.85CACU2O8+DELTA:1||intrinsic Josephson effects:1||CACUO:1||QUANTUM POINT CONTACTS:1||resonant tunneling state:1||coherence length:1||NANOWIRE:1||GATES:1||Phase line:1||Thermal activation:1||QUANTUMDOT:1||superconducting proximity effect:1||Andreev interferometer:1||WIRE:1||Josephsonvortexflow branches:1||Bi2212 cuprates:1||LATTICE:1||demannetization effect:1||SUPERCONDUCTING MIRRORS:1||GAS:1||VALLEY TRANSPORT:1||ELECTRODES:1||DEPENDENT TRANSPORT:1||BORNOPPENHEIMER APPROXIMATION:1||collective plasma oscillations:1||fluxon resonance steps:1||STACKS:1||COLLECTIVE DYNAMICS:1||PAIRING SYMMETRY:1||MUON SPIN ROTATION:1||DIMENSIONAL CROSSOVER:1||Bi2Sr2CaCu2Oy highTc superconductors:1||heterojunctions:1||nanostructures:1||surfaces and interfaces:1||QUANTUM TRANSPORT:1||MICROJUNCTIONS:1||RESONATORS:1||STATES:1||FIELD:1||FLUCTUATIONS:1||SCATTERING:1||mode splitting of Josephson vortexflow branches:1||2D superconductivity:1||TRANSISTOR:1||ENERGYGAP:1||SUPERLATTICES:1||IRONBASED SUPERCONDUCTORS:1||PHASEDEPENDENT RESISTANCE:1||QUANTUM PHASETRANSITIONS:1||ELECTRICFIELD:1||HIGH MAGNETICFIELDS:1||NANOWIRE HETEROSTRUCTURES:1||ZNO:1||pair breaking.:1||SUPERCONDUCTING PB:1||domain formation:1||FORCE MICROSCOPY:1||RELAXATION:1||PLASMA RESONANCE:1||coupled Josephson junctions:1||COPPEROXIDE SUPERCONDUCTORS:1||CROSSOVER:1||SIMULATIONS:1||LOWTEMPERATURE:1||CONDUCTORS:1||METALINSULATORTRANSITION:1||SEMICONDUCTOR:1||FIELDEFFECT TRANSISTORS:1||ZEROVOLTAGE STATE:1||constanttemperature interlayer tunneling spectroscopy:1||Josephson supercurrent:1||BIPOLAR SUPERCURRENT:1||Interaction between Josephson and pancake vortices:1||flux jump:1||coaxial heterojunction nanorod:1||Natural Josephson coupling:1||BI2SR2CACU2O8+DELTA:1||VORTEX FLOW:1||TC SUPERCONDUCTORS:1||charge imbalance:1||Andreev diffractometer:1||intercalation:1||surface junction:1||Bi2212:1||tunnelling:1||GRAPHITE:1||GROWTH:1||collective transverse plasma modes:1||GAN:1||Macroscopic quantum tunneling:1||Fluctuation conductivity:1||Abovegap conductance jump:1||Josephson vortex motion:1||Intrinsic Josephson junctions:1||LAYERED SUPERCONDUCTORS:1||BI2SR2CACU2O8+Y:1||INTERFACES:1||BREAKDOWN:1||SYSTEMS:1||Anisotropy ratio:1||Josephson vortex:1||spin relaxation in superconductors:1||bibased single crystals:1||MESOSCOPIC PROXIMITY SUPERCONDUCTOR:1||reentrance of conductance:1||interlayer pair tunneling:1||JOSEPHSON:1||DISORDERED 2DIMENSIONAL SUPERCONDUCTORS:1||INDIUM FILMS:1||excited state:1||REGIME:1||triplet superconductivity:1||FILM:1||SCHOTTKY DIODES:1||peakdiphump structure:1||Kondo effect:1||REENTRANCE:1||Graphene:1||CONTACT:1||BERRYS PHASE:1||2DIMENSIONAL SUPERCONDUCTORS:1||Coulomb diamond:1||magnetic domain:1||spin injection:1||RESONANCE:1||plasma excitation modes:1||FLOW:1||OVERDOPED BI2SR2CACU2O8+DELTA:1||hole doping:1||chemical synthesis:1||phase transitions:1||superconductors:1||VORTEXGLASS SUPERCONDUCTIVITY:1||Kondorelated model:1||RADIATION:1||DOT:1||NANOBELTS:1||Complementarity:1||Closedloop AharonovBohm interferometer:1||pair breaking:1||interlayer phase fluctuation:1||MgB2 thin film:1||CONFINEMENT:1||WALLED CARBON NANOTUBES:1||TRANSITION:9||VORTICES:8||STATE:7||intrinsic Josephson junctions:7||SINGLECRYSTALS:7||JUNCTIONS:5||MODES:5||SUPERCURRENT:5||SUPERCONDUCTOR:5||CONDUCTANCE:5||HIGHTEMPERATURE SUPERCONDUCTORS:5||TRANSPORT:5||PHASE:5||FILMS:4||LOCALIZATION:4||SINGLE DIRAC CONE:4||WIRES:4||MAGNETICFIELD:4||STEPS:3||ELECTRONS:3||proximity effect:3||MODEL:3||ARRAYS:3||INTERFERENCE:3||fluxon dynamics:3||HETEROSTRUCTURES:3||INSULATOR:3||Andreev reflection:3||electronic transport:3||FISKE:3||superconductor:2||ZnO:2||quantum point contact:2||METAL:2||DYNAMICS:2||interlayer Josephson coupling:2||SUPERCONDUCTORS:2||YBA2CU3O7DELTA:2||LAYER:2||DOTS:2||quantum dot:2||Article:2||TRANSISTORS:2||CARBON NANOTUBES:2||GAP:2||MECHANISM:2||LINE:2||GIANT SHAPIRO STEPS:2||LAYERS:2||electron energy loss spectroscopy:2||physical phenomena:2||scanning electron microscopy:2||HGTE QUANTUMWELLS:2||BI2TE3:2||SPECTROSCOPY:2||PNJUNCTIONS:2||spinpolarized tunneling:2||INTRINSIC JOSEPHSONJUNCTIONS:2||FIELDS:2||positive magnetoresistance:2||dilute magnetic semiconductor:2||magnetic field:2||scanning transmission electron microscopy:2||QUANTUM OSCILLATIONS:2||TRANSPORTPROPERTIES:2||surface pair current:2||MAGNETORESISTANCE:2||NANORIBBONS:2||INSTABILITY:2||ANDREEV REFLECTION:2||microwave irradiation:2||vertical graphene josephson junction:2||BI2SE3:2||CONDUCTIVITY:2||highTc superconductors:2||DIMENSIONAL ELECTRONGAS:2||graphene:2||Topological insulators:2||Josephson coupling Fraunhofer interference pattern:2||FERROMAGNET:2||DEPENDENCE:2||DETECTOR:2||COHERENCE:2||INJECTION:2||GRAPHENE:1||JOSEPHSONJUNCTIONS:1||LAYERED SUPERCONDUCTOR:1||mode splitting:1||BEHAVIOR:1||spinpolarized transport:1||SUPERCONDUCTING TRANSITION:1||microwave response:1||PSEUDOGAP:1||phase coherence:1||TRANSITIONS:1||Long Josephson junction:1||Charge detection:1||collective resonance modes:1||plasma oscillation modes:1||Superconducting proximity effect:1||Iron pnictide superconductor:1||McMillanRowell oscillations:1||ferromagnetic microstructure:1||superradiant state:1||VOLTAGE:1||branch splitting:1||TENSOR:1||INTERCALATION:1||insitu fabrication:1||NDGAO3:1||DISORDERED METALS:1||GAUGE GLASS:1||LOWTEMPERATURE TRANSPORT:1||spontaneous spin polarization model:1||BIAS:1||emission of electromagnetic waves:1||YBA2CU3O7/PRBA2CU3O7 SUPERLATTICES:1||BOHM:1||SHAPIRO STEPS:1||superconductor/ferromagnet interface:1||OXIDE:1||ANDREEVREFLECTION:1||SinFeAsO single crystal:1||COLLECTIVE MOTION:1||ANGULARDEPENDENCE:1||SUPERCONDUCTIVITY:1||BILAYER GRAPHENE:1||PHOTOLUMINESCENT PROPERTIES:1||SUPERCONDUCTING WEAK LINKS:1||intrinsic Josephson junctions geometrical resonance:1||intrinsic Josephson junction:1||MESOSCOPIC SPINVALVE:1||Bi2212 single crystals:1||intrinsic junctions:1||ANDREEV REFLECTIONS:1||normalmetal/superconductor interface:1||IBI2SR2CACU2OY:1||THERMAL FLUCTUATIONS:1||MIXED STATE:1||BI2.15SR1.85CACU2O8+DELTA:1||intrinsic Josephson effects:1||CACUO:1||QUANTUM POINT CONTACTS:1||resonant tunneling state:1||coherence length:1||NANOWIRE:1||GATES:1||Phase line:1||Thermal activation:1||QUANTUMDOT:1||superconducting proximity effect:1||Andreev interferometer:1||WIRE:1||Josephsonvortexflow branches:1||Bi2212 cuprates:1||LATTICE:1||demannetization effect:1||SUPERCONDUCTING MIRRORS:1||GAS:1||VALLEY TRANSPORT:1||ELECTRODES:1||DEPENDENT TRANSPORT:1||BORNOPPENHEIMER APPROXIMATION:1||collective plasma oscillations:1||fluxon resonance steps:1||STACKS:1||COLLECTIVE DYNAMICS:1||PAIRING SYMMETRY:1||MUON SPIN ROTATION:1||DIMENSIONAL CROSSOVER:1||Bi2Sr2CaCu2Oy highTc superconductors:1||heterojunctions:1||nanostructures:1||surfaces and interfaces:1||QUANTUM TRANSPORT:1||MICROJUNCTIONS:1||RESONATORS:1||STATES:1||FIELD:1||FLUCTUATIONS:1||SCATTERING:1||mode splitting of Josephson vortexflow branches:1||2D superconductivity:1||TRANSISTOR:1||ENERGYGAP:1||SUPERLATTICES:1||IRONBASED SUPERCONDUCTORS:1||PHASEDEPENDENT RESISTANCE:1||QUANTUM PHASETRANSITIONS:1||ELECTRICFIELD:1||HIGH MAGNETICFIELDS:1||NANOWIRE HETEROSTRUCTURES:1||ZNO:1||pair breaking.:1||SUPERCONDUCTING PB:1||domain formation:1||FORCE MICROSCOPY:1||RELAXATION:1||PLASMA RESONANCE:1||coupled Josephson junctions:1||COPPEROXIDE SUPERCONDUCTORS:1||CROSSOVER:1||SIMULATIONS:1||LOWTEMPERATURE:1||CONDUCTORS:1||METALINSULATORTRANSITION:1||SEMICONDUCTOR:1||FIELDEFFECT TRANSISTORS:1||ZEROVOLTAGE STATE:1||constanttemperature interlayer tunneling spectroscopy:1||Josephson supercurrent:1||BIPOLAR SUPERCURRENT:1||Interaction between Josephson and pancake vortices:1||flux jump:1||coaxial heterojunction nanorod:1||Natural Josephson coupling:1||BI2SR2CACU2O8+DELTA:1||VORTEX FLOW:1||TC SUPERCONDUCTORS:1||charge imbalance:1||Andreev diffractometer:1||intercalation:1||surface junction:1||Bi2212:1||tunnelling:1||GRAPHITE:1||GROWTH:1||collective transverse plasma modes:1||GAN:1||Macroscopic quantum tunneling:1||Fluctuation conductivity:1||Abovegap conductance jump:1||Josephson vortex motion:1||Intrinsic Josephson junctions:1||LAYERED SUPERCONDUCTORS:1||BI2SR2CACU2O8+Y:1||INTERFACES:1||BREAKDOWN:1||SYSTEMS:1||Anisotropy ratio:1||Josephson vortex:1||spin relaxation in superconductors:1||bibased single crystals:1||MESOSCOPIC PROXIMITY SUPERCONDUCTOR:1||reentrance of conductance:1||interlayer pair tunneling:1||JOSEPHSON:1||DISORDERED 2DIMENSIONAL SUPERCONDUCTORS:1||INDIUM FILMS:1||excited state:1||REGIME:1||triplet superconductivity:1||FILM:1||SCHOTTKY DIODES:1||peakdiphump structure:1||Kondo effect:1||REENTRANCE:1||Graphene:1||CONTACT:1||BERRYS PHASE:1||2DIMENSIONAL SUPERCONDUCTORS:1||Coulomb diamond:1||magnetic domain:1||spin injection:1||RESONANCE:1||plasma excitation modes:1||FLOW:1||OVERDOPED BI2SR2CACU2O8+DELTA:1||hole doping:1||chemical synthesis:1||phase transitions:1||superconductors:1||VORTEXGLASS SUPERCONDUCTIVITY:1||Kondorelated model:1||RADIATION:1||DOT:1||NANOBELTS:1||Complementarity:1||Closedloop AharonovBohm interferometer:1||pair breaking:1||interlayer phase fluctuation:1||MgB2 thin film:1||CONFINEMENT:1||WALLED CARBON NANOTUBES:1||TRANSITION:9||VORTICES:8||STATE:7||intrinsic Josephson junctions:7||SINGLECRYSTALS:7||JUNCTIONS:5||MODES:5||SUPERCURRENT:5||SUPERCONDUCTOR:5||CONDUCTANCE:5||HIGHTEMPERATURE SUPERCONDUCTORS:5||TRANSPORT:5||PHASE:5||FILMS:4||LOCALIZATION:4||SINGLE DIRAC CONE:4||WIRES:4||MAGNETICFIELD:4||STEPS:3||ELECTRONS:3||proximity effect:3||MODEL:3||ARRAYS:3||INTERFERENCE:3||fluxon dynamics:3||HETEROSTRUCTURES:3||INSULATOR:3||Andreev reflection:3||electronic transport:3||FISKE:3||superconductor:2||ZnO:2||quantum point contact:2||METAL:2||DYNAMICS:2||interlayer Josephson coupling:2||SUPERCONDUCTORS:2||YBA2CU3O7DELTA:2||LAYER:2||DOTS:2||quantum dot:2||Article:2||TRANSISTORS:2||CARBON NANOTUBES:2||GAP:2||MECHANISM:2||LINE:2||GIANT SHAPIRO STEPS:2||LAYERS:2||electron energy loss spectroscopy:2||physical phenomena:2||scanning electron microscopy:2||HGTE QUANTUMWELLS:2||BI2TE3:2||SPECTROSCOPY:2||PNJUNCTIONS:2||spinpolarized tunneling:2||INTRINSIC JOSEPHSONJUNCTIONS:2||FIELDS:2||positive magnetoresistance:2||dilute magnetic semiconductor:2||magnetic field:2||scanning transmission electron microscopy:2||QUANTUM OSCILLATIONS:2||TRANSPORTPROPERTIES:2||surface pair current:2||MAGNETORESISTANCE:2||NANORIBBONS:2||INSTABILITY:2||ANDREEV REFLECTION:2||microwave irradiation:2||vertical graphene josephson junction:2||BI2SE3:2||CONDUCTIVITY:2||highTc superconductors:2||DIMENSIONAL ELECTRONGAS:2||graphene:2||Topological insulators:2||Josephson coupling Fraunhofer interference pattern:2||FERROMAGNET:2||DEPENDENCE:2||DETECTOR:2||COHERENCE:2||INJECTION:2||GRAPHENE:1||JOSEPHSONJUNCTIONS:1||LAYERED SUPERCONDUCTOR:1||mode splitting:1||BEHAVIOR:1||spinpolarized transport:1||SUPERCONDUCTING TRANSITION:1||microwave response:1||PSEUDOGAP:1||phase coherence:1||TRANSITIONS:1||Long Josephson junction:1||Charge detection:1||collective resonance modes:1||plasma oscillation modes:1||Superconducting proximity effect:1||Iron pnictide superconductor:1||McMillanRowell oscillations:1||ferromagnetic microstructure:1||superradiant state:1||VOLTAGE:1||branch splitting:1||TENSOR:1||INTERCALATION:1||insitu fabrication:1||NDGAO3:1||DISORDERED METALS:1||GAUGE GLASS:1||LOWTEMPERATURE TRANSPORT:1||spontaneous spin polarization model:1||BIAS:1||emission of electromagnetic waves:1||YBA2CU3O7/PRBA2CU3O7 SUPERLATTICES:1||BOHM:1||SHAPIRO STEPS:1||superconductor/ferromagnet interface:1||OXIDE:1||ANDREEVREFLECTION:1||SinFeAsO single crystal:1||COLLECTIVE MOTION:1||ANGULARDEPENDENCE:1||SUPERCONDUCTIVITY:1||BILAYER GRAPHENE:1||PHOTOLUMINESCENT PROPERTIES:1||SUPERCONDUCTING WEAK LINKS:1||intrinsic Josephson junctions geometrical resonance:1||intrinsic Josephson junction:1||MESOSCOPIC SPINVALVE:1||Bi2212 single crystals:1||intrinsic junctions:1||ANDREEV REFLECTIONS:1||normalmetal/superconductor interface:1||IBI2SR2CACU2OY:1||THERMAL FLUCTUATIONS:1||MIXED STATE:1||BI2.15SR1.85CACU2O8+DELTA:1||intrinsic Josephson effects:1||CACUO:1||QUANTUM POINT CONTACTS:1||resonant tunneling state:1||coherence length:1||NANOWIRE:1||GATES:1||Phase line:1||Thermal activation:1||QUANTUMDOT:1||superconducting proximity effect:1||Andreev interferometer:1||WIRE:1||Josephsonvortexflow branches:1||Bi2212 cuprates:1||LATTICE:1||demannetization effect:1||SUPERCONDUCTING MIRRORS:1||GAS:1||VALLEY TRANSPORT:1||ELECTRODES:1||DEPENDENT TRANSPORT:1||BORNOPPENHEIMER APPROXIMATION:1||collective plasma oscillations:1||fluxon resonance steps:1||STACKS:1||COLLECTIVE DYNAMICS:1||PAIRING SYMMETRY:1||MUON SPIN ROTATION:1||DIMENSIONAL CROSSOVER:1||Bi2Sr2CaCu2Oy highTc superconductors:1||heterojunctions:1||nanostructures:1||surfaces and interfaces:1||QUANTUM TRANSPORT:1||MICROJUNCTIONS:1||RESONATORS:1||STATES:1||FIELD:1||FLUCTUATIONS:1||SCATTERING:1||mode splitting of Josephson vortexflow branches:1||2D superconductivity:1||TRANSISTOR:1||ENERGYGAP:1||SUPERLATTICES:1||IRONBASED SUPERCONDUCTORS:1||PHASEDEPENDENT RESISTANCE:1||QUANTUM PHASETRANSITIONS:1||ELECTRICFIELD:1||HIGH MAGNETICFIELDS:1||NANOWIRE HETEROSTRUCTURES:1||ZNO:1||pair breaking.:1||SUPERCONDUCTING PB:1||domain formation:1||FORCE MICROSCOPY:1||RELAXATION:1||PLASMA RESONANCE:1||coupled Josephson junctions:1||COPPEROXIDE SUPERCONDUCTORS:1||CROSSOVER:1||SIMULATIONS:1||LOWTEMPERATURE:1||CONDUCTORS:1||METALINSULATORTRANSITION:1||SEMICONDUCTOR:1||FIELDEFFECT TRANSISTORS:1||ZEROVOLTAGE STATE:1||constanttemperature interlayer tunneling spectroscopy:1||Josephson supercurrent:1||BIPOLAR SUPERCURRENT:1||Interaction between Josephson and pancake vortices:1||flux jump:1||coaxial heterojunction nanorod:1||Natural Josephson coupling:1||BI2SR2CACU2O8+DELTA:1||VORTEX FLOW:1||TC SUPERCONDUCTORS:1||charge imbalance:1||Andreev diffractometer:1||intercalation:1||surface junction:1||Bi2212:1||tunnelling:1||GRAPHITE:1||GROWTH:1||collective transverse plasma modes:1||GAN:1||Macroscopic quantum tunneling:1||Fluctuation conductivity:1||Abovegap conductance jump:1||Josephson vortex motion:1||Intrinsic Josephson junctions:1||LAYERED SUPERCONDUCTORS:1||BI2SR2CACU2O8+Y:1||INTERFACES:1||BREAKDOWN:1||SYSTEMS:1||Anisotropy ratio:1||Josephson vortex:1||spin relaxation in superconductors:1||bibased single crystals:1||MESOSCOPIC PROXIMITY SUPERCONDUCTOR:1||reentrance of conductance:1||interlayer pair tunneling:1||JOSEPHSON:1||DISORDERED 2DIMENSIONAL SUPERCONDUCTORS:1||INDIUM FILMS:1||excited state:1||REGIME:1||triplet superconductivity:1||FILM:1||SCHOTTKY DIODES:1||peakdiphump structure:1||Kondo effect:1||REENTRANCE:1||Graphene:1||CONTACT:1||BERRYS PHASE:1||2DIMENSIONAL SUPERCONDUCTORS:1||Coulomb diamond:1||magnetic domain:1||spin injection:1||RESONANCE:1||plasma excitation modes:1||FLOW:1||OVERDOPED BI2SR2CACU2O8+DELTA:1||hole doping:1||chemical synthesis:1||phase transitions:1||superconductors:1||VORTEXGLASS SUPERCONDUCTIVITY:1||Kondorelated model:1||RADIATION:1||DOT:1||NANOBELTS:1||Complementarity:1||Closedloop AharonovBohm interferometer:1||pair breaking:1||interlayer phase fluctuation:1||MgB2 thin film:1||CONFINEMENT:1||WALLED CARBON NANOTUBES:1||TRANSITION:9||VORTICES:8||STATE:7||intrinsic Josephson junctions:7||SINGLECRYSTALS:7||JUNCTIONS:5||MODES:5||SUPERCURRENT:5||SUPERCONDUCTOR:5||CONDUCTANCE:5||HIGHTEMPERATURE SUPERCONDUCTORS:5||TRANSPORT:5||PHASE:5||FILMS:4||LOCALIZATION:4||SINGLE DIRAC CONE:4||WIRES:4||MAGNETICFIELD:4||STEPS:3||ELECTRONS:3||proximity effect:3||MODEL:3||ARRAYS:3||INTERFERENCE:3||fluxon dynamics:3||HETEROSTRUCTURES:3||INSULATOR:3||Andreev reflection:3||electronic transport:3||FISKE:3||superconductor:2||ZnO:2||quantum point contact:2||METAL:2||DYNAMICS:2||interlayer Josephson coupling:2||SUPERCONDUCTORS:2||YBA2CU3O7DELTA:2||LAYER:2||DOTS:2||quantum dot:2||Article:2||TRANSISTORS:2||CARBON NANOTUBES:2||GAP:2||MECHANISM:2||LINE:2||GIANT SHAPIRO STEPS:2||LAYERS:2||electron energy loss spectroscopy:2||physical phenomena:2||scanning electron microscopy:2||HGTE QUANTUMWELLS:2||BI2TE3:2||SPECTROSCOPY:2||PNJUNCTIONS:2||spinpolarized tunneling:2||INTRINSIC JOSEPHSONJUNCTIONS:2||FIELDS:2||positive magnetoresistance:2||dilute magnetic semiconductor:2||magnetic field:2||scanning transmission electron microscopy:2||QUANTUM OSCILLATIONS:2||TRANSPORTPROPERTIES:2||surface pair current:2||MAGNETORESISTANCE:2||NANORIBBONS:2||INSTABILITY:2||ANDREEV REFLECTION:2||microwave irradiation:2||vertical graphene josephson junction:2||BI2SE3:2||CONDUCTIVITY:2||highTc superconductors:2||DIMENSIONAL ELECTRONGAS:2||graphene:2||Topological insulators:2||Josephson coupling Fraunhofer interference pattern:2||FERROMAGNET:2||DEPENDENCE:2||DETECTOR:2||COHERENCE:2||INJECTION:2||GRAPHENE:1||JOSEPHSONJUNCTIONS:1||LAYERED SUPERCONDUCTOR:1||mode splitting:1||BEHAVIOR:1||spinpolarized transport:1||SUPERCONDUCTING TRANSITION:1||microwave response:1||PSEUDOGAP:1||phase coherence:1||TRANSITIONS:1||Long Josephson junction:1||Charge detection:1||collective resonance modes:1||plasma oscillation modes:1||Superconducting proximity effect:1||Iron pnictide superconductor:1||McMillanRowell oscillations:1||ferromagnetic microstructure:1||superradiant state:1||VOLTAGE:1||branch splitting:1||TENSOR:1||INTERCALATION:1||insitu fabrication:1||NDGAO3:1||DISORDERED METALS:1||GAUGE GLASS:1||LOWTEMPERATURE TRANSPORT:1||spontaneous spin polarization model:1||BIAS:1||emission of electromagnetic waves:1||YBA2CU3O7/PRBA2CU3O7 SUPERLATTICES:1||BOHM:1||SHAPIRO STEPS:1||superconductor/ferromagnet interface:1||OXIDE:1||ANDREEVREFLECTION:1||SinFeAsO single crystal:1||COLLECTIVE MOTION:1||ANGULARDEPENDENCE:1||SUPERCONDUCTIVITY:1||BILAYER GRAPHENE:1||PHOTOLUMINESCENT PROPERTIES:1||SUPERCONDUCTING WEAK LINKS:1||intrinsic Josephson junctions geometrical resonance:1||intrinsic Josephson junction:1||MESOSCOPIC SPINVALVE:1||Bi2212 single crystals:1||intrinsic junctions:1||ANDREEV REFLECTIONS:1||normalmetal/superconductor interface:1||IBI2SR2CACU2OY:1||THERMAL FLUCTUATIONS:1||MIXED STATE:1||BI2.15SR1.85CACU2O8+DELTA:1||intrinsic Josephson effects:1||CACUO:1||QUANTUM POINT CONTACTS:1||resonant tunneling state:1||coherence length:1||NANOWIRE:1||GATES:1||Phase line:1||Thermal activation:1||QUANTUMDOT:1||superconducting proximity effect:1||Andreev interferometer:1||WIRE:1||Josephsonvortexflow branches:1||Bi2212 cuprates:1||LATTICE:1||demannetization effect:1||SUPERCONDUCTING MIRRORS:1||GAS:1||VALLEY TRANSPORT:1||ELECTRODES:1||DEPENDENT TRANSPORT:1||BORNOPPENHEIMER APPROXIMATION:1||collective plasma oscillations:1||fluxon resonance steps:1||STACKS:1||COLLECTIVE DYNAMICS:1||PAIRING SYMMETRY:1||MUON SPIN ROTATION:1||DIMENSIONAL CROSSOVER:1||Bi2Sr2CaCu2Oy highTc superconductors:1||heterojunctions:1||nanostructures:1||surfaces and interfaces:1||QUANTUM TRANSPORT:1||MICROJUNCTIONS:1||RESONATORS:1||STATES:1||FIELD:1||FLUCTUATIONS:1||SCATTERING:1||mode splitting of Josephson vortexflow branches:1||2D superconductivity:1||TRANSISTOR:1||ENERGYGAP:1||SUPERLATTICES:1||IRONBASED SUPERCONDUCTORS:1||PHASEDEPENDENT RESISTANCE:1||QUANTUM PHASETRANSITIONS:1||ELECTRICFIELD:1||HIGH MAGNETICFIELDS:1||NANOWIRE HETEROSTRUCTURES:1||ZNO:1||pair breaking.:1||SUPERCONDUCTING PB:1||domain formation:1||FORCE MICROSCOPY:1||RELAXATION:1||PLASMA RESONANCE:1||coupled Josephson junctions:1||COPPEROXIDE SUPERCONDUCTORS:1||CROSSOVER:1||SIMULATIONS:1||LOWTEMPERATURE:1||CONDUCTORS:1||METALINSULATORTRANSITION:1||SEMICONDUCTOR:1||FIELDEFFECT TRANSISTORS:1||ZEROVOLTAGE STATE:1||constanttemperature interlayer tunneling spectroscopy:1||Josephson supercurrent:1||BIPOLAR SUPERCURRENT:1||Interaction between Josephson and pancake vortices:1||flux jump:1||coaxial heterojunction nanorod:1||Natural Josephson coupling:1||BI2SR2CACU2O8+DELTA:1||VORTEX FLOW:1||TC SUPERCONDUCTORS:1||charge imbalance:1||Andreev diffractometer:1||intercalation:1||surface junction:1||Bi2212:1||tunnelling:1||GRAPHITE:1||GROWTH:1||collective transverse plasma modes:1||GAN:1||Macroscopic quantum tunneling:1||Fluctuation conductivity:1||Abovegap conductance jump:1||Josephson vortex motion:1||Intrinsic Josephson junctions:1||LAYERED SUPERCONDUCTORS:1||BI2SR2CACU2O8+Y:1||INTERFACES:1||BREAKDOWN:1||SYSTEMS:1||Anisotropy ratio:1||Josephson vortex:1||spin relaxation in superconductors:1||bibased single crystals:1||MESOSCOPIC PROXIMITY SUPERCONDUCTOR:1||reentrance of conductance:1||interlayer pair tunneling:1||JOSEPHSON:1||DISORDERED 2DIMENSIONAL SUPERCONDUCTORS:1||INDIUM FILMS:1||excited state:1||REGIME:1||triplet superconductivity:1||FILM:1||SCHOTTKY DIODES:1||peakdiphump structure:1||Kondo effect:1||REENTRANCE:1||Graphene:1||CONTACT:1||BERRYS PHASE:1||2DIMENSIONAL SUPERCONDUCTORS:1||Coulomb diamond:1||magnetic domain:1||spin injection:1||RESONANCE:1||plasma excitation modes:1||FLOW:1||OVERDOPED BI2SR2CACU2O8+DELTA:1||hole doping:1||chemical synthesis:1||phase transitions:1||superconductors:1||VORTEXGLASS SUPERCONDUCTIVITY:1||Kondorelated model:1||RADIATION:1||DOT:1||NANOBELTS:1||Complementarity:1||Closedloop AharonovBohm interferometer:1||pair breaking:1||interlayer phase fluctuation:1||MgB2 thin film:1||CONFINEMENT:1||WALLED CARBON NANOTUBES:1||TRANSITION:9||VORTICES:8||STATE:7||intrinsic Josephson junctions:7||SINGLECRYSTALS:7||JUNCTIONS:5||MODES:5||SUPERCURRENT:5||SUPERCONDUCTOR:5||CONDUCTANCE:5||HIGHTEMPERATURE SUPERCONDUCTORS:5||TRANSPORT:5||PHASE:5||FILMS:4||LOCALIZATION:4||SINGLE DIRAC CONE:4||WIRES:4||MAGNETICFIELD:4||STEPS:3||ELECTRONS:3||proximity effect:3||MODEL:3||ARRAYS:3||INTERFERENCE:3||fluxon dynamics:3||HETEROSTRUCTURES:3||INSULATOR:3||Andreev reflection:3||electronic transport:3||FISKE:3||superconductor:2||ZnO:2||quantum point contact:2||METAL:2||DYNAMICS:2||interlayer Josephson coupling:2||SUPERCONDUCTORS:2||YBA2CU3O7DELTA:2||LAYER:2||DOTS:2||quantum dot:2||Article:2||TRANSISTORS:2||CARBON NANOTUBES:2||GAP:2||MECHANISM:2||LINE:2||GIANT SHAPIRO STEPS:2||LAYERS:2||electron energy loss spectroscopy:2||physical phenomena:2||scanning electron microscopy:2||HGTE QUANTUMWELLS:2||BI2TE3:2||SPECTROSCOPY:2||PNJUNCTIONS:2||spinpolarized tunneling:2||INTRINSIC JOSEPHSONJUNCTIONS:2||FIELDS:2||positive magnetoresistance:2||dilute magnetic semiconductor:2||magnetic field:2||scanning transmission electron microscopy:2||QUANTUM OSCILLATIONS:2||TRANSPORTPROPERTIES:2||surface pair current:2||MAGNETORESISTANCE:2||NANORIBBONS:2||INSTABILITY:2||ANDREEV REFLECTION:2||microwave irradiation:2||vertical graphene josephson junction:2||BI2SE3:2||CONDUCTIVITY:2||highTc superconductors:2||DIMENSIONAL ELECTRONGAS:2||graphene:2||Topological insulators:2||Josephson coupling Fraunhofer interference pattern:2||FERROMAGNET:2||DEPENDENCE:2||DETECTOR:2||COHERENCE:2||INJECTION:2||GRAPHENE:1||JOSEPHSONJUNCTIONS:1||LAYERED SUPERCONDUCTOR:1||mode splitting:1||BEHAVIOR:1||spinpolarized transport:1||SUPERCONDUCTING TRANSITION:1||microwave response:1||PSEUDOGAP:1||phase coherence:1||TRANSITIONS:1||Long Josephson junction:1||Charge detection:1||collective resonance modes:1||plasma oscillation modes:1||Superconducting proximity effect:1||Iron pnictide superconductor:1||McMillanRowell oscillations:1||ferromagnetic microstructure:1||superradiant state:1||VOLTAGE:1||branch splitting:1||TENSOR:1||INTERCALATION:1||insitu fabrication:1||NDGAO3:1||DISORDERED METALS:1||GAUGE GLASS:1||LOWTEMPERATURE TRANSPORT:1||spontaneous spin polarization model:1||BIAS:1||emission of electromagnetic waves:1||YBA2CU3O7/PRBA2CU3O7 SUPERLATTICES:1||BOHM:1||SHAPIRO STEPS:1||superconductor/ferromagnet interface:1||OXIDE:1||ANDREEVREFLECTION:1||SinFeAsO single crystal:1||COLLECTIVE MOTION:1||ANGULARDEPENDENCE:1||SUPERCONDUCTIVITY:1||BILAYER GRAPHENE:1||PHOTOLUMINESCENT PROPERTIES:1||SUPERCONDUCTING WEAK LINKS:1||intrinsic Josephson junctions geometrical resonance:1||intrinsic Josephson junction:1||MESOSCOPIC SPINVALVE:1||Bi2212 single crystals:1||intrinsic junctions:1||ANDREEV REFLECTIONS:1||normalmetal/superconductor interface:1||IBI2SR2CACU2OY:1||THERMAL FLUCTUATIONS:1||MIXED STATE:1||BI2.15SR1.85CACU2O8+DELTA:1||intrinsic Josephson effects:1||CACUO:1||QUANTUM POINT CONTACTS:1||resonant tunneling state:1||coherence length:1||NANOWIRE:1||GATES:1||Phase line:1||Thermal activation:1||QUANTUMDOT:1||superconducting proximity effect:1||Andreev interferometer:1||WIRE:1||Josephsonvortexflow branches:1||Bi2212 cuprates:1||LATTICE:1||demannetization effect:1||SUPERCONDUCTING MIRRORS:1||GAS:1||VALLEY TRANSPORT:1||ELECTRODES:1||DEPENDENT TRANSPORT:1||BORNOPPENHEIMER APPROXIMATION:1||collective plasma oscillations:1||fluxon resonance steps:1||STACKS:1||COLLECTIVE DYNAMICS:1||PAIRING SYMMETRY:1||MUON SPIN ROTATION:1||DIMENSIONAL CROSSOVER:1||Bi2Sr2CaCu2Oy highTc superconductors:1||heterojunctions:1||nanostructures:1||surfaces and interfaces:1||QUANTUM TRANSPORT:1||MICROJUNCTIONS:1||RESONATORS:1||STATES:1||FIELD:1||FLUCTUATIONS:1||SCATTERING:1||mode splitting of Josephson vortexflow branches:1||2D superconductivity:1||TRANSISTOR:1||ENERGYGAP:1||SUPERLATTICES:1||IRONBASED SUPERCONDUCTORS:1||PHASEDEPENDENT RESISTANCE:1||QUANTUM PHASETRANSITIONS:1||ELECTRICFIELD:1||HIGH MAGNETICFIELDS:1||NANOWIRE HETEROSTRUCTURES:1||ZNO:1||pair breaking.:1||SUPERCONDUCTING PB:1||domain formation:1||FORCE MICROSCOPY:1||RELAXATION:1||PLASMA RESONANCE:1||coupled Josephson junctions:1||COPPEROXIDE SUPERCONDUCTORS:1||CROSSOVER:1||SIMULATIONS:1||LOWTEMPERATURE:1||CONDUCTORS:1||METALINSULATORTRANSITION:1||SEMICONDUCTOR:1||FIELDEFFECT TRANSISTORS:1||ZEROVOLTAGE STATE:1||constanttemperature interlayer tunneling spectroscopy:1||Josephson supercurrent:1||BIPOLAR SUPERCURRENT:1||Interaction between Josephson and pancake vortices:1||flux jump:1||coaxial heterojunction nanorod:1||Natural Josephson coupling:1||BI2SR2CACU2O8+DELTA:1||VORTEX FLOW:1||TC SUPERCONDUCTORS:1||charge imbalance:1||Andreev diffractometer:1||intercalation:1||surface junction:1||Bi2212:1||tunnelling:1||GRAPHITE:1||GROWTH:1||collective transverse plasma modes:1||GAN:1||Macroscopic quantum tunneling:1||Fluctuation conductivity:1||Abovegap conductance jump:1||Josephson vortex motion:1||Intrinsic Josephson junctions:1||LAYERED SUPERCONDUCTORS:1||BI2SR2CACU2O8+Y:1||INTERFACES:1||BREAKDOWN:1||SYSTEMS:1||Anisotropy ratio:1||Josephson vortex:1||spin relaxation in superconductors:1||bibased single crystals:1||MESOSCOPIC PROXIMITY SUPERCONDUCTOR:1||reentrance of conductance:1||interlayer pair tunneling:1||JOSEPHSON:1||DISORDERED 2DIMENSIONAL SUPERCONDUCTORS:1||INDIUM FILMS:1||excited state:1||REGIME:1||triplet superconductivity:1||FILM:1||SCHOTTKY DIODES:1||peakdiphump structure:1||Kondo effect:1||REENTRANCE:1||Graphene:1||CONTACT:1||BERRYS PHASE:1||2DIMENSIONAL SUPERCONDUCTORS:1||Coulomb diamond:1||magnetic domain:1||spin injection:1||RESONANCE:1||plasma excitation modes:1||FLOW:1||OVERDOPED BI2SR2CACU2O8+DELTA:1||hole doping:1||chemical synthesis:1||phase transitions:1||superconductors:1||VORTEXGLASS SUPERCONDUCTIVITY:1||Kondorelated model:1||RADIATION:1||DOT:1||NANOBELTS:1||Complementarity:1||Closedloop AharonovBohm interferometer:1||pair breaking:1||interlayer phase fluctuation:1||MgB2 thin film:1||CONFINEMENT:1||WALLED CARBON NANOTUBES:1||TRANSITION:9||VORTICES:8||STATE:7||intrinsic Josephson junctions:7||SINGLECRYSTALS:7||JUNCTIONS:5||MODES:5||SUPERCURRENT:5||SUPERCONDUCTOR:5||CONDUCTANCE:5||HIGHTEMPERATURE SUPERCONDUCTORS:5||TRANSPORT:5||PHASE:5||FILMS:4||LOCALIZATION:4||SINGLE DIRAC CONE:4||WIRES:4||MAGNETICFIELD:4||STEPS:3||ELECTRONS:3||proximity effect:3||MODEL:3||ARRAYS:3||INTERFERENCE:3||fluxon dynamics:3||HETEROSTRUCTURES:3||INSULATOR:3||Andreev reflection:3||electronic transport:3||FISKE:3||superconductor:2||ZnO:2||quantum point contact:2||METAL:2||DYNAMICS:2||interlayer Josephson coupling:2||SUPERCONDUCTORS:2||YBA2CU3O7DELTA:2||LAYER:2||DOTS:2||quantum dot:2||Article:2||TRANSISTORS:2||CARBON NANOTUBES:2||GAP:2||MECHANISM:2||LINE:2||GIANT SHAPIRO STEPS:2||LAYERS:2||electron energy loss spectroscopy:2||physical phenomena:2||scanning electron microscopy:2||HGTE QUANTUMWELLS:2||BI2TE3:2||SPECTROSCOPY:2||PNJUNCTIONS:2||spinpolarized tunneling:2||INTRINSIC JOSEPHSONJUNCTIONS:2||FIELDS:2||positive magnetoresistance:2||dilute magnetic semiconductor:2||magnetic field:2||scanning transmission electron microscopy:2||QUANTUM OSCILLATIONS:2||TRANSPORTPROPERTIES:2||surface pair current:2||MAGNETORESISTANCE:2||NANORIBBONS:2||INSTABILITY:2||ANDREEV REFLECTION:2||microwave irradiation:2||vertical graphene josephson junction:2||BI2SE3:2||CONDUCTIVITY:2||highTc superconductors:2||DIMENSIONAL ELECTRONGAS:2||graphene:2||Topological insulators:2||Josephson coupling Fraunhofer interference pattern:2||FERROMAGNET:2||DEPENDENCE:2||DETECTOR:2||COHERENCE:2||INJECTION:2||GRAPHENE:1||JOSEPHSONJUNCTIONS:1||LAYERED SUPERCONDUCTOR:1||mode splitting:1||BEHAVIOR:1||spinpolarized transport:1||SUPERCONDUCTING TRANSITION:1||microwave response:1||PSEUDOGAP:1||phase coherence:1||TRANSITIONS:1||Long Josephson junction:1||Charge detection:1||collective resonance modes:1||plasma oscillation modes:1||Superconducting proximity effect:1||Iron pnictide superconductor:1||McMillanRowell oscillations:1||ferromagnetic microstructure:1||superradiant state:1||VOLTAGE:1||branch splitting:1||TENSOR:1||INTERCALATION:1||insitu fabrication:1||NDGAO3:1||DISORDERED METALS:1||GAUGE GLASS:1||LOWTEMPERATURE TRANSPORT:1||spontaneous spin polarization model:1||BIAS:1||emission of electromagnetic waves:1||YBA2CU3O7/PRBA2CU3O7 SUPERLATTICES:1||BOHM:1||SHAPIRO STEPS:1||superconductor/ferromagnet interface:1||OXIDE:1||ANDREEVREFLECTION:1||SinFeAsO single crystal:1||COLLECTIVE MOTION:1||ANGULARDEPENDENCE:1||SUPERCONDUCTIVITY:1||BILAYER GRAPHENE:1||PHOTOLUMINESCENT PROPERTIES:1||SUPERCONDUCTING WEAK LINKS:1||intrinsic Josephson junctions geometrical resonance:1||intrinsic Josephson junction:1||MESOSCOPIC SPINVALVE:1||Bi2212 single crystals:1||intrinsic junctions:1||ANDREEV REFLECTIONS:1||normalmetal/superconductor interface:1||IBI2SR2CACU2OY:1||THERMAL FLUCTUATIONS:1||MIXED STATE:1||BI2.15SR1.85CACU2O8+DELTA:1||intrinsic Josephson effects:1||CACUO:1||QUANTUM POINT CONTACTS:1||resonant tunneling state:1||coherence length:1||NANOWIRE:1||GATES:1||Phase line:1||Thermal activation:1||QUANTUMDOT:1||superconducting proximity effect:1||Andreev interferometer:1||WIRE:1||Josephsonvortexflow branches:1||Bi2212 cuprates:1||LATTICE:1||demannetization effect:1||SUPERCONDUCTING MIRRORS:1||GAS:1||VALLEY TRANSPORT:1||ELECTRODES:1||DEPENDENT TRANSPORT:1||BORNOPPENHEIMER APPROXIMATION:1||collective plasma oscillations:1||fluxon resonance steps:1||STACKS:1||COLLECTIVE DYNAMICS:1||PAIRING SYMMETRY:1||MUON SPIN ROTATION:1||DIMENSIONAL CROSSOVER:1||Bi2Sr2CaCu2Oy highTc superconductors:1||heterojunctions:1||nanostructures:1||surfaces and interfaces:1||QUANTUM TRANSPORT:1||MICROJUNCTIONS:1||RESONATORS:1||STATES:1||FIELD:1||FLUCTUATIONS:1||SCATTERING:1||mode splitting of Josephson vortexflow branches:1||2D superconductivity:1||TRANSISTOR:1||ENERGYGAP:1||SUPERLATTICES:1||IRONBASED SUPERCONDUCTORS:1||PHASEDEPENDENT RESISTANCE:1||QUANTUM PHASETRANSITIONS:1||ELECTRICFIELD:1||HIGH MAGNETICFIELDS:1||NANOWIRE HETEROSTRUCTURES:1||ZNO:1||pair breaking.:1||SUPERCONDUCTING PB:1||domain formation:1||FORCE MICROSCOPY:1||RELAXATION:1||PLASMA RESONANCE:1||coupled Josephson junctions:1||COPPEROXIDE SUPERCONDUCTORS:1||CROSSOVER:1||SIMULATIONS:1||LOWTEMPERATURE:1||CONDUCTORS:1||METALINSULATORTRANSITION:1||SEMICONDUCTOR:1||FIELDEFFECT TRANSISTORS:1||ZEROVOLTAGE STATE:1||constanttemperature interlayer tunneling spectroscopy:1||Josephson supercurrent:1||BIPOLAR SUPERCURRENT:1||Interaction between Josephson and pancake vortices:1||flux jump:1||coaxial heterojunction nanorod:1||Natural Josephson coupling:1||BI2SR2CACU2O8+DELTA:1||VORTEX FLOW:1||TC SUPERCONDUCTORS:1||charge imbalance:1||Andreev diffractometer:1||intercalation:1||surface junction:1||Bi2212:1||tunnelling:1||GRAPHITE:1||GROWTH:1||collective transverse plasma modes:1||GAN:1||Macroscopic quantum tunneling:1||Fluctuation conductivity:1||Abovegap conductance jump:1||Josephson vortex motion:1||Intrinsic Josephson junctions:1||LAYERED SUPERCONDUCTORS:1||BI2SR2CACU2O8+Y:1||INTERFACES:1||BREAKDOWN:1||SYSTEMS:1||Anisotropy ratio:1||Josephson vortex:1||spin relaxation in superconductors:1||bibased single crystals:1||MESOSCOPIC PROXIMITY SUPERCONDUCTOR:1||reentrance of conductance:1||interlayer pair tunneling:1||JOSEPHSON:1||DISORDERED 2DIMENSIONAL SUPERCONDUCTORS:1||INDIUM FILMS:1||excited state:1||REGIME:1||triplet superconductivity:1||FILM:1||SCHOTTKY DIODES:1||peakdiphump structure:1||Kondo effect:1||REENTRANCE:1||Graphene:1||CONTACT:1||BERRYS PHASE:1||2DIMENSIONAL SUPERCONDUCTORS:1||Coulomb diamond:1||magnetic domain:1||spin injection:1||RESONANCE:1||plasma excitation modes:1||FLOW:1||OVERDOPED BI2SR2CACU2O8+DELTA:1||hole doping:1||chemical synthesis:1||phase transitions:1||superconductors:1||VORTEXGLASS SUPERCONDUCTIVITY:1||Kondorelated model:1||RADIATION:1||DOT:1||NANOBELTS:1||Complementarity:1||Closedloop AharonovBohm interferometer:1||pair breaking:1||interlayer phase fluctuation:1||MgB2 thin film:1||CONFINEMENT:1||WALLED CARBON NANOTUBES:1||TRANSITION:9||VORTICES:8||STATE:7||intrinsic Josephson junctions:7||SINGLECRYSTALS:7||JUNCTIONS:5||MODES:5||SUPERCURRENT:5||SUPERCONDUCTOR:5||CONDUCTANCE:5||HIGHTEMPERATURE SUPERCONDUCTORS:5||TRANSPORT:5||PHASE:5||FILMS:4||LOCALIZATION:4||SINGLE DIRAC CONE:4||WIRES:4||MAGNETICFIELD:4||STEPS:3||ELECTRONS:3||proximity effect:3||MODEL:3||ARRAYS:3||INTERFERENCE:3||fluxon dynamics:3||HETEROSTRUCTURES:3||INSULATOR:3||Andreev reflection:3||electronic transport:3||FISKE:3||superconductor:2||ZnO:2||quantum point contact:2||METAL:2||DYNAMICS:2||interlayer Josephson coupling:2||SUPERCONDUCTORS:2||YBA2CU3O7DELTA:2||LAYER:2||DOTS:2||quantum dot:2||Article:2||TRANSISTORS:2||CARBON NANOTUBES:2||GAP:2||MECHANISM:2||LINE:2||GIANT SHAPIRO STEPS:2||LAYERS:2||electron energy loss spectroscopy:2||physical phenomena:2||scanning electron microscopy:2||HGTE QUANTUMWELLS:2||BI2TE3:2||SPECTROSCOPY:2||PNJUNCTIONS:2||spinpolarized tunneling:2||INTRINSIC JOSEPHSONJUNCTIONS:2||FIELDS:2||positive magnetoresistance:2||dilute magnetic semiconductor:2||magnetic field:2||scanning transmission electron microscopy:2||QUANTUM OSCILLATIONS:2||TRANSPORTPROPERTIES:2||surface pair current:2||MAGNETORESISTANCE:2||NANORIBBONS:2||INSTABILITY:2||ANDREEV REFLECTION:2||microwave irradiation:2||vertical graphene josephson junction:2||BI2SE3:2||CONDUCTIVITY:2||highTc superconductors:2||DIMENSIONAL ELECTRONGAS:2||graphene:2||Topological insulators:2||Josephson coupling Fraunhofer interference pattern:2||FERROMAGNET:2||DEPENDENCE:2||DETECTOR:2||COHERENCE:2||INJECTION:2||GRAPHENE:1||JOSEPHSONJUNCTIONS:1||LAYERED SUPERCONDUCTOR:1||mode splitting:1||BEHAVIOR:1||spinpolarized transport:1||SUPERCONDUCTING TRANSITION:1||microwave response:1||PSEUDOGAP:1||phase coherence:1||TRANSITIONS:1||Long Josephson junction:1||Charge detection:1||collective resonance modes:1||plasma oscillation modes:1||Superconducting proximity effect:1||Iron pnictide superconductor:1||McMillanRowell oscillations:1||ferromagnetic microstructure:1||superradiant state:1||VOLTAGE:1||branch splitting:1||TENSOR:1||INTERCALATION:1||insitu fabrication:1||NDGAO3:1||DISORDERED METALS:1||GAUGE GLASS:1||LOWTEMPERATURE TRANSPORT:1||spontaneous spin polarization model:1||BIAS:1||emission of electromagnetic waves:1||YBA2CU3O7/PRBA2CU3O7 SUPERLATTICES:1||BOHM:1||SHAPIRO STEPS:1||superconductor/ferromagnet interface:1||OXIDE:1||ANDREEVREFLECTION:1||SinFeAsO single crystal:1||COLLECTIVE MOTION:1||ANGULARDEPENDENCE:1||SUPERCONDUCTIVITY:1||BILAYER GRAPHENE:1||PHOTOLUMINESCENT PROPERTIES:1||SUPERCONDUCTING WEAK LINKS:1||intrinsic Josephson junctions geometrical resonance:1||intrinsic Josephson junction:1||MESOSCOPIC SPINVALVE:1||Bi2212 single crystals:1||intrinsic junctions:1||ANDREEV REFLECTIONS:1||normalmetal/superconductor interface:1||IBI2SR2CACU2OY:1||THERMAL FLUCTUATIONS:1||MIXED STATE:1||BI2.15SR1.85CACU2O8+DELTA:1||intrinsic Josephson effects:1||CACUO:1||QUANTUM POINT CONTACTS:1||resonant tunneling state:1||coherence length:1||NANOWIRE:1||GATES:1||Phase line:1||Thermal activation:1||QUANTUMDOT:1||superconducting proximity effect:1||Andreev interferometer:1||WIRE:1||Josephsonvortexflow branches:1||Bi2212 cuprates:1||LATTICE:1||demannetization effect:1||SUPERCONDUCTING MIRRORS:1||GAS:1||VALLEY TRANSPORT:1||ELECTRODES:1||DEPENDENT TRANSPORT:1||BORNOPPENHEIMER APPROXIMATION:1||collective plasma oscillations:1||fluxon resonance steps:1||STACKS:1||COLLECTIVE DYNAMICS:1||PAIRING SYMMETRY:1||MUON SPIN ROTATION:1||DIMENSIONAL CROSSOVER:1||Bi2Sr2CaCu2Oy highTc superconductors:1||heterojunctions:1||nanostructures:1||surfaces and interfaces:1||QUANTUM TRANSPORT:1||MICROJUNCTIONS:1||RESONATORS:1||STATES:1||FIELD:1||FLUCTUATIONS:1||SCATTERING:1||mode splitting of Josephson vortexflow branches:1||2D superconductivity:1||TRANSISTOR:1||ENERGYGAP:1||SUPERLATTICES:1||IRONBASED SUPERCONDUCTORS:1||PHASEDEPENDENT RESISTANCE:1||QUANTUM PHASETRANSITIONS:1||ELECTRICFIELD:1||HIGH MAGNETICFIELDS:1||NANOWIRE HETEROSTRUCTURES:1||ZNO:1||pair breaking.:1||SUPERCONDUCTING PB:1||domain formation:1||FORCE MICROSCOPY:1||RELAXATION:1||PLASMA RESONANCE:1||coupled Josephson junctions:1||COPPEROXIDE SUPERCONDUCTORS:1||CROSSOVER:1||SIMULATIONS:1||LOWTEMPERATURE:1||CONDUCTORS:1||METALINSULATORTRANSITION:1||SEMICONDUCTOR:1||FIELDEFFECT TRANSISTORS:1||ZEROVOLTAGE STATE:1||constanttemperature interlayer tunneling spectroscopy:1||Josephson supercurrent:1||BIPOLAR SUPERCURRENT:1||Interaction between Josephson and pancake vortices:1||flux jump:1||coaxial heterojunction nanorod:1||Natural Josephson coupling:1||BI2SR2CACU2O8+DELTA:1||VORTEX FLOW:1||TC SUPERCONDUCTORS:1||charge imbalance:1||Andreev diffractometer:1||intercalation:1||surface junction:1||Bi2212:1||tunnelling:1||GRAPHITE:1||GROWTH:1||collective transverse plasma modes:1||GAN:1||Macroscopic quantum tunneling:1||Fluctuation conductivity:1||Abovegap conductance jump:1||Josephson vortex motion:1||Intrinsic Josephson junctions:1||LAYERED SUPERCONDUCTORS:1||BI2SR2CACU2O8+Y:1||INTERFACES:1||BREAKDOWN:1||SYSTEMS:1||Anisotropy ratio:1||Josephson vortex:1||spin relaxation in superconductors:1||bibased single crystals:1||MESOSCOPIC PROXIMITY SUPERCONDUCTOR:1||reentrance of conductance:1||interlayer pair tunneling:1||JOSEPHSON:1||DISORDERED 2DIMENSIONAL SUPERCONDUCTORS:1||INDIUM FILMS:1||excited state:1||REGIME:1||triplet superconductivity:1||FILM:1||SCHOTTKY DIODES:1||peakdiphump structure:1||Kondo effect:1||REENTRANCE:1||Graphene:1||CONTACT:1||BERRYS PHASE:1||2DIMENSIONAL SUPERCONDUCTORS:1||Coulomb diamond:1||magnetic domain:1||spin injection:1||RESONANCE:1||plasma excitation modes:1||FLOW:1||OVERDOPED BI2SR2CACU2O8+DELTA:1||hole doping:1||chemical synthesis:1||phase transitions:1||superconductors:1||VORTEXGLASS SUPERCONDUCTIVITY:1||Kondorelated model:1||RADIATION:1||DOT:1||NANOBELTS:1||Complementarity:1||Closedloop AharonovBohm interferometer:1||pair breaking:1||interlayer phase fluctuation:1||MgB2 thin film:1||CONFINEMENT:1||WALLED CARBON NANOTUBES:1||TRANSITION:9||VORTICES:8||STATE:7||intrinsic Josephson junctions:7||SINGLECRYSTALS:7||JUNCTIONS:5||MODES:5||SUPERCURRENT:5||SUPERCONDUCTOR:5||CONDUCTANCE:5||HIGHTEMPERATURE SUPERCONDUCTORS:5||TRANSPORT:5||PHASE:5||FILMS:4||LOCALIZATION:4||SINGLE DIRAC CONE:4||WIRES:4||MAGNETICFIELD:4||STEPS:3||ELECTRONS:3||proximity effect:3||MODEL:3||ARRAYS:3||INTERFERENCE:3||fluxon dynamics:3||HETEROSTRUCTURES:3||INSULATOR:3||Andreev reflection:3||electronic transport:3||FISKE:3||superconductor:2||ZnO:2||quantum point contact:2||METAL:2||DYNAMICS:2||interlayer Josephson coupling:2||SUPERCONDUCTORS:2||YBA2CU3O7DELTA:2||LAYER:2||DOTS:2||quantum dot:2||Article:2||TRANSISTORS:2||CARBON NANOTUBES:2||GAP:2||MECHANISM:2||LINE:2||GIANT SHAPIRO STEPS:2||LAYERS:2||electron energy loss spectroscopy:2||physical phenomena:2||scanning electron microscopy:2||HGTE QUANTUMWELLS:2||BI2TE3:2||SPECTROSCOPY:2||PNJUNCTIONS:2||spinpolarized tunneling:2||INTRINSIC JOSEPHSONJUNCTIONS:2||FIELDS:2||positive magnetoresistance:2||dilute magnetic semiconductor:2||magnetic field:2||scanning transmission electron microscopy:2||QUANTUM OSCILLATIONS:2||TRANSPORTPROPERTIES:2||surface pair current:2||MAGNETORESISTANCE:2||NANORIBBONS:2||INSTABILITY:2||ANDREEV REFLECTION:2||microwave irradiation:2||vertical graphene josephson junction:2||BI2SE3:2||CONDUCTIVITY:2||highTc superconductors:2||DIMENSIONAL ELECTRONGAS:2||graphene:2||Topological insulators:2||Josephson coupling Fraunhofer interference pattern:2||FERROMAGNET:2||DEPENDENCE:2||DETECTOR:2||COHERENCE:2||INJECTION:2||GRAPHENE:1||JOSEPHSONJUNCTIONS:1||LAYERED SUPERCONDUCTOR:1||mode splitting:1||BEHAVIOR:1||spinpolarized transport:1||SUPERCONDUCTING TRANSITION:1||microwave response:1||PSEUDOGAP:1||phase coherence:1||TRANSITIONS:1||Long Josephson junction:1||Charge detection:1||collective resonance modes:1||plasma oscillation modes:1||Superconducting proximity effect:1||Iron pnictide superconductor:1||McMillanRowell oscillations:1||ferromagnetic microstructure:1||superradiant state:1||VOLTAGE:1||branch splitting:1||TENSOR:1||INTERCALATION:1||insitu fabrication:1||NDGAO3:1||DISORDERED METALS:1||GAUGE GLASS:1||LOWTEMPERATURE TRANSPORT:1||spontaneous spin polarization model:1||BIAS:1||emission of electromagnetic waves:1||YBA2CU3O7/PRBA2CU3O7 SUPERLATTICES:1||BOHM:1||SHAPIRO STEPS:1||superconductor/ferromagnet interface:1||OXIDE:1||ANDREEVREFLECTION:1||SinFeAsO single crystal:1||COLLECTIVE MOTION:1||ANGULARDEPENDENCE:1||SUPERCONDUCTIVITY:1||BILAYER GRAPHENE:1||PHOTOLUMINESCENT PROPERTIES:1||SUPERCONDUCTING WEAK LINKS:1||intrinsic Josephson junctions geometrical resonance:1||intrinsic Josephson junction:1||MESOSCOPIC SPINVALVE:1||Bi2212 single crystals:1||intrinsic junctions:1||ANDREEV REFLECTIONS:1||normalmetal/superconductor interface:1||IBI2SR2CACU2OY:1||THERMAL FLUCTUATIONS:1||MIXED STATE:1||BI2.15SR1.85CACU2O8+DELTA:1||intrinsic Josephson effects:1||CACUO:1||QUANTUM POINT CONTACTS:1||resonant tunneling state:1||coherence length:1||NANOWIRE:1||GATES:1||Phase line:1||Thermal activation:1||QUANTUMDOT:1||superconducting proximity effect:1||Andreev interferometer:1||WIRE:1||Josephsonvortexflow branches:1||Bi2212 cuprates:1||LATTICE:1||demannetization effect:1||SUPERCONDUCTING MIRRORS:1||GAS:1||VALLEY TRANSPORT:1||ELECTRODES:1||DEPENDENT TRANSPORT:1||BORNOPPENHEIMER APPROXIMATION:1||collective plasma oscillations:1||fluxon resonance steps:1||STACKS:1||COLLECTIVE DYNAMICS:1||PAIRING SYMMETRY:1||MUON SPIN ROTATION:1||DIMENSIONAL CROSSOVER:1||Bi2Sr2CaCu2Oy highTc superconductors:1||heterojunctions:1||nanostructures:1||surfaces and interfaces:1||QUANTUM TRANSPORT:1||MICROJUNCTIONS:1||RESONATORS:1||STATES:1||FIELD:1||FLUCTUATIONS:1||SCATTERING:1||mode splitting of Josephson vortexflow branches:1||2D superconductivity:1||TRANSISTOR:1||ENERGYGAP:1||SUPERLATTICES:1||IRONBASED SUPERCONDUCTORS:1||PHASEDEPENDENT RESISTANCE:1||QUANTUM PHASETRANSITIONS:1||ELECTRICFIELD:1||HIGH MAGNETICFIELDS:1||NANOWIRE HETEROSTRUCTURES:1||ZNO:1||pair breaking.:1||SUPERCONDUCTING PB:1||domain formation:1||FORCE MICROSCOPY:1||RELAXATION:1||PLASMA RESONANCE:1||coupled Josephson junctions:1||COPPEROXIDE SUPERCONDUCTORS:1||CROSSOVER:1||SIMULATIONS:1||LOWTEMPERATURE:1||CONDUCTORS:1||METALINSULATORTRANSITION:1||SEMICONDUCTOR:1||FIELDEFFECT TRANSISTORS:1||ZEROVOLTAGE STATE:1||constanttemperature interlayer tunneling spectroscopy:1||Josephson supercurrent:1||BIPOLAR SUPERCURRENT:1||Interaction between Josephson and pancake vortices:1||flux jump:1||coaxial heterojunction nanorod:1||Natural Josephson coupling:1||BI2SR2CACU2O8+DELTA:1||VORTEX FLOW:1||TC SUPERCONDUCTORS:1||charge imbalance:1||Andreev diffractometer:1||intercalation:1||surface junction:1||Bi2212:1||tunnelling:1||GRAPHITE:1||GROWTH:1||collective transverse plasma modes:1||GAN:1||Macroscopic quantum tunneling:1||Fluctuation conductivity:1||Abovegap conductance jump:1||Josephson vortex motion:1||Intrinsic Josephson junctions:1||LAYERED SUPERCONDUCTORS:1||BI2SR2CACU2O8+Y:1||INTERFACES:1||BREAKDOWN:1||SYSTEMS:1||Anisotropy ratio:1||Josephson vortex:1||spin relaxation in superconductors:1||bibased single crystals:1||MESOSCOPIC PROXIMITY SUPERCONDUCTOR:1||reentrance of conductance:1||interlayer pair tunneling:1||JOSEPHSON:1||DISORDERED 2DIMENSIONAL SUPERCONDUCTORS:1||INDIUM FILMS:1||excited state:1||REGIME:1||triplet superconductivity:1||FILM:1||SCHOTTKY DIODES:1||peakdiphump structure:1||Kondo effect:1||REENTRANCE:1||Graphene:1||CONTACT:1||BERRYS PHASE:1||2DIMENSIONAL SUPERCONDUCTORS:1||Coulomb diamond:1||magnetic domain:1||spin injection:1||RESONANCE:1||plasma excitation modes:1||FLOW:1||OVERDOPED BI2SR2CACU2O8+DELTA:1||hole doping:1||chemical synthesis:1||phase transitions:1||superconductors:1||VORTEXGLASS SUPERCONDUCTIVITY:1||Kondorelated model:1||RADIATION:1||DOT:1||NANOBELTS:1||Complementarity:1||Closedloop AharonovBohm interferometer:1||pair breaking:1||interlayer phase fluctuation:1||MgB2 thin film:1||CONFINEMENT:1||WALLED CARBON NANOTUBES:1||TRANSITION:9||VORTICES:8||STATE:7||intrinsic Josephson junctions:7||SINGLECRYSTALS:7||JUNCTIONS:5||MODES:5||SUPERCURRENT:5||SUPERCONDUCTOR:5||CONDUCTANCE:5||HIGHTEMPERATURE SUPERCONDUCTORS:5||TRANSPORT:5||PHASE:5||FILMS:4||LOCALIZATION:4||SINGLE DIRAC CONE:4||WIRES:4||MAGNETICFIELD:4||STEPS:3||ELECTRONS:3||proximity effect:3||MODEL:3||ARRAYS:3||INTERFERENCE:3||fluxon dynamics:3||HETEROSTRUCTURES:3||INSULATOR:3||Andreev reflection:3||electronic transport:3||FISKE:3||superconductor:2||ZnO:2||quantum point contact:2||METAL:2||DYNAMICS:2||interlayer Josephson coupling:2||SUPERCONDUCTORS:2||YBA2CU3O7DELTA:2||LAYER:2||DOTS:2||quantum dot:2||Article:2||TRANSISTORS:2||CARBON NANOTUBES:2||GAP:2||MECHANISM:2||LINE:2||GIANT SHAPIRO STEPS:2||LAYERS:2||electron energy loss spectroscopy:2||physical phenomena:2||scanning electron microscopy:2||HGTE QUANTUMWELLS:2||BI2TE3:2||SPECTROSCOPY:2||PNJUNCTIONS:2||spinpolarized tunneling:2||INTRINSIC JOSEPHSONJUNCTIONS:2||FIELDS:2||positive magnetoresistance:2||dilute magnetic semiconductor:2||magnetic field:2||scanning transmission electron microscopy:2||QUANTUM OSCILLATIONS:2||TRANSPORTPROPERTIES:2||surface pair current:2||MAGNETORESISTANCE:2||NANORIBBONS:2||INSTABILITY:2||ANDREEV REFLECTION:2||microwave irradiation:2||vertical graphene josephson junction:2||BI2SE3:2||CONDUCTIVITY:2||highTc superconductors:2||DIMENSIONAL ELECTRONGAS:2||graphene:2||Topological insulators:2||Josephson coupling Fraunhofer interference pattern:2||FERROMAGNET:2||DEPENDENCE:2||DETECTOR:2||COHERENCE:2||INJECTION:2||GRAPHENE:1||JOSEPHSONJUNCTIONS:1||LAYERED SUPERCONDUCTOR:1||mode splitting:1||BEHAVIOR:1||spinpolarized transport:1||SUPERCONDUCTING TRANSITION:1||microwave response:1||PSEUDOGAP:1||phase coherence:1||TRANSITIONS:1||Long Josephson junction:1||Charge detection:1||collective resonance modes:1||plasma oscillation modes:1||Superconducting proximity effect:1||Iron pnictide superconductor:1||McMillanRowell oscillations:1||ferromagnetic microstructure:1||superradiant state:1||VOLTAGE:1||branch splitting:1||TENSOR:1||INTERCALATION:1||insitu fabrication:1||NDGAO3:1||DISORDERED METALS:1||GAUGE GLASS:1||LOWTEMPERATURE TRANSPORT:1||spontaneous spin polarization model:1||BIAS:1||emission of electromagnetic waves:1||YBA2CU3O7/PRBA2CU3O7 SUPERLATTICES:1||BOHM:1||SHAPIRO STEPS:1||superconductor/ferromagnet interface:1||OXIDE:1||ANDREEVREFLECTION:1||SinFeAsO single crystal:1||COLLECTIVE MOTION:1||ANGULARDEPENDENCE:1||SUPERCONDUCTIVITY:1||BILAYER GRAPHENE:1||PHOTOLUMINESCENT PROPERTIES:1||SUPERCONDUCTING WEAK LINKS:1||intrinsic Josephson junctions geometrical resonance:1||intrinsic Josephson junction:1||MESOSCOPIC SPINVALVE:1||Bi2212 single crystals:1||intrinsic junctions:1||ANDREEV REFLECTIONS:1||normalmetal/superconductor interface:1||IBI2SR2CACU2OY:1||THERMAL FLUCTUATIONS:1||MIXED STATE:1||BI2.15SR1.85CACU2O8+DELTA:1||intrinsic Josephson effects:1||CACUO:1||QUANTUM POINT CONTACTS:1||resonant tunneling state:1||coherence length:1||NANOWIRE:1||GATES:1||Phase line:1||Thermal activation:1||QUANTUMDOT:1||superconducting proximity effect:1||Andreev interferometer:1||WIRE:1||Josephsonvortexflow branches:1||Bi2212 cuprates:1||LATTICE:1||demannetization effect:1||SUPERCONDUCTING MIRRORS:1||GAS:1||VALLEY TRANSPORT:1||ELECTRODES:1||DEPENDENT TRANSPORT:1||BORNOPPENHEIMER APPROXIMATION:1||collective plasma oscillations:1||fluxon resonance steps:1||STACKS:1||COLLECTIVE DYNAMICS:1||PAIRING SYMMETRY:1||MUON SPIN ROTATION:1||DIMENSIONAL CROSSOVER:1||Bi2Sr2CaCu2Oy highTc superconductors:1||heterojunctions:1||nanostructures:1||surfaces and interfaces:1||QUANTUM TRANSPORT:1||MICROJUNCTIONS:1||RESONATORS:1||STATES:1||FIELD:1||FLUCTUATIONS:1||SCATTERING:1||mode splitting of Josephson vortexflow branches:1||2D superconductivity:1||TRANSISTOR:1||ENERGYGAP:1||SUPERLATTICES:1||IRONBASED SUPERCONDUCTORS:1||PHASEDEPENDENT RESISTANCE:1||QUANTUM PHASETRANSITIONS:1||ELECTRICFIELD:1||HIGH MAGNETICFIELDS:1||NANOWIRE HETEROSTRUCTURES:1||ZNO:1||pair breaking.:1||SUPERCONDUCTING PB:1||domain formation:1||FORCE MICROSCOPY:1||RELAXATION:1||PLASMA RESONANCE:1||coupled Josephson junctions:1||COPPEROXIDE SUPERCONDUCTORS:1||CROSSOVER:1||SIMULATIONS:1||LOWTEMPERATURE:1||CONDUCTORS:1||METALINSULATORTRANSITION:1||SEMICONDUCTOR:1||FIELDEFFECT TRANSISTORS:1||ZEROVOLTAGE STATE:1||constanttemperature interlayer tunneling spectroscopy:1||Josephson supercurrent:1||BIPOLAR SUPERCURRENT:1||Interaction between Josephson and pancake vortices:1||flux jump:1||coaxial heterojunction nanorod:1||Natural Josephson coupling:1||BI2SR2CACU2O8+DELTA:1||VORTEX FLOW:1||TC SUPERCONDUCTORS:1||charge imbalance:1||Andreev diffractometer:1||intercalation:1||surface junction:1||Bi2212:1||tunnelling:1||GRAPHITE:1||GROWTH:1||collective transverse plasma modes:1||GAN:1||Macroscopic quantum tunneling:1||Fluctuation conductivity:1||Abovegap conductance jump:1||Josephson vortex motion:1||Intrinsic Josephson junctions:1||LAYERED SUPERCONDUCTORS:1||BI2SR2CACU2O8+Y:1||INTERFACES:1||BREAKDOWN:1||SYSTEMS:1||Anisotropy ratio:1||Josephson vortex:1||spin relaxation in superconductors:1||bibased single crystals:1||MESOSCOPIC PROXIMITY SUPERCONDUCTOR:1||reentrance of conductance:1||interlayer pair tunneling:1||JOSEPHSON:1||DISORDERED 2DIMENSIONAL SUPERCONDUCTORS:1||INDIUM FILMS:1||excited state:1||REGIME:1||triplet superconductivity:1||FILM:1||SCHOTTKY DIODES:1||peakdiphump structure:1||Kondo effect:1||REENTRANCE:1||Graphene:1||CONTACT:1||BERRYS PHASE:1||2DIMENSIONAL SUPERCONDUCTORS:1||Coulomb diamond:1||magnetic domain:1||spin injection:1||RESONANCE:1||plasma excitation modes:1||FLOW:1||OVERDOPED BI2SR2CACU2O8+DELTA:1||hole doping:1||chemical synthesis:1||phase transitions:1||superconductors:1||VORTEXGLASS SUPERCONDUCTIVITY:1||Kondorelated model:1||RADIATION:1||DOT:1||NANOBELTS:1||Complementarity:1||Closedloop AharonovBohm interferometer:1||pair breaking:1||interlayer phase fluctuation:1||MgB2 thin film:1||CONFINEMENT:1||WALLED CARBON NANOTUBES:1||TRANSITION:9||VORTICES:8||STATE:7||intrinsic Josephson junctions:7||SINGLECRYSTALS:7||JUNCTIONS:5||MODES:5||SUPERCURRENT:5||SUPERCONDUCTOR:5||CONDUCTANCE:5||HIGHTEMPERATURE SUPERCONDUCTORS:5||TRANSPORT:5||PHASE:5||FILMS:4||LOCALIZATION:4||SINGLE DIRAC CONE:4||WIRES:4||MAGNETICFIELD:4||STEPS:3||ELECTRONS:3||proximity effect:3||MODEL:3||ARRAYS:3||INTERFERENCE:3||fluxon dynamics:3||HETEROSTRUCTURES:3||INSULATOR:3||Andreev reflection:3||electronic transport:3||FISKE:3||superconductor:2||ZnO:2||quantum point contact:2||METAL:2||DYNAMICS:2||interlayer Josephson coupling:2||SUPERCONDUCTORS:2||YBA2CU3O7DELTA:2||LAYER:2||DOTS:2||quantum dot:2||Article:2||TRANSISTORS:2||CARBON NANOTUBES:2||GAP:2||MECHANISM:2||LINE:2||GIANT SHAPIRO STEPS:2||LAYERS:2||electron energy loss spectroscopy:2||physical phenomena:2||scanning electron microscopy:2||HGTE QUANTUMWELLS:2||BI2TE3:2||SPECTROSCOPY:2||PNJUNCTIONS:2||spinpolarized tunneling:2||INTRINSIC JOSEPHSONJUNCTIONS:2||FIELDS:2||positive magnetoresistance:2||dilute magnetic semiconductor:2||magnetic field:2||scanning transmission electron microscopy:2||QUANTUM OSCILLATIONS:2||TRANSPORTPROPERTIES:2||surface pair current:2||MAGNETORESISTANCE:2||NANORIBBONS:2||INSTABILITY:2||ANDREEV REFLECTION:2||microwave irradiation:2||vertical graphene josephson junction:2||BI2SE3:2||CONDUCTIVITY:2||highTc superconductors:2||DIMENSIONAL ELECTRONGAS:2||graphene:2||Topological insulators:2||Josephson coupling Fraunhofer interference pattern:2||FERROMAGNET:2||DEPENDENCE:2||DETECTOR:2||COHERENCE:2||INJECTION:2||GRAPHENE:1||JOSEPHSONJUNCTIONS:1||LAYERED SUPERCONDUCTOR:1||mode splitting:1||BEHAVIOR:1||spinpolarized transport:1||SUPERCONDUCTING TRANSITION:1||microwave response:1||PSEUDOGAP:1||phase coherence:1||TRANSITIONS:1||Long Josephson junction:1||Charge detection:1||collective resonance modes:1||plasma oscillation modes:1||Superconducting proximity effect:1||Iron pnictide superconductor:1||McMillanRowell oscillations:1||ferromagnetic microstructure:1||superradiant state:1||VOLTAGE:1||branch splitting:1||TENSOR:1||INTERCALATION:1||insitu fabrication:1||NDGAO3:1||DISORDERED METALS:1||GAUGE GLASS:1||LOWTEMPERATURE TRANSPORT:1||spontaneous spin polarization model:1||BIAS:1||emission of electromagnetic waves:1||YBA2CU3O7/PRBA2CU3O7 SUPERLATTICES:1||BOHM:1||SHAPIRO STEPS:1||superconductor/ferromagnet interface:1||OXIDE:1||ANDREEVREFLECTION:1||SinFeAsO single crystal:1||COLLECTIVE MOTION:1||ANGULARDEPENDENCE:1||SUPERCONDUCTIVITY:1||BILAYER GRAPHENE:1||PHOTOLUMINESCENT PROPERTIES:1||SUPERCONDUCTING WEAK LINKS:1||intrinsic Josephson junctions geometrical resonance:1||intrinsic Josephson junction:1||MESOSCOPIC SPINVALVE:1||Bi2212 single crystals:1||intrinsic junctions:1||ANDREEV REFLECTIONS:1||normalmetal/superconductor interface:1||IBI2SR2CACU2OY:1||THERMAL FLUCTUATIONS:1||MIXED STATE:1||BI2.15SR1.85CACU2O8+DELTA:1||intrinsic Josephson effects:1||CACUO:1||QUANTUM POINT CONTACTS:1||resonant tunneling state:1||coherence length:1||NANOWIRE:1||GATES:1||Phase line:1||Thermal activation:1||QUANTUMDOT:1||superconducting proximity effect:1||Andreev interferometer:1||WIRE:1||Josephsonvortexflow branches:1||Bi2212 cuprates:1||LATTICE:1||demannetization effect:1||SUPERCONDUCTING MIRRORS:1||GAS:1||VALLEY TRANSPORT:1||ELECTRODES:1||DEPENDENT TRANSPORT:1||BORNOPPENHEIMER APPROXIMATION:1||collective plasma oscillations:1||fluxon resonance steps:1||STACKS:1||COLLECTIVE DYNAMICS:1||PAIRING SYMMETRY:1||MUON SPIN ROTATION:1||DIMENSIONAL CROSSOVER:1||Bi2Sr2CaCu2Oy highTc superconductors:1||heterojunctions:1||nanostructures:1||surfaces and interfaces:1||QUANTUM TRANSPORT:1||MICROJUNCTIONS:1||RESONATORS:1||STATES:1||FIELD:1||FLUCTUATIONS:1||SCATTERING:1||mode splitting of Josephson vortexflow branches:1||2D superconductivity:1||TRANSISTOR:1||ENERGYGAP:1||SUPERLATTICES:1||IRONBASED SUPERCONDUCTORS:1||PHASEDEPENDENT RESISTANCE:1||QUANTUM PHASETRANSITIONS:1||ELECTRICFIELD:1||HIGH MAGNETICFIELDS:1||NANOWIRE HETEROSTRUCTURES:1||ZNO:1||pair breaking.:1||SUPERCONDUCTING PB:1||domain formation:1||FORCE MICROSCOPY:1||RELAXATION:1||PLASMA RESONANCE:1||coupled Josephson junctions:1||COPPEROXIDE SUPERCONDUCTORS:1||CROSSOVER:1||SIMULATIONS:1||LOWTEMPERATURE:1||CONDUCTORS:1||METALINSULATORTRANSITION:1||SEMICONDUCTOR:1||FIELDEFFECT TRANSISTORS:1||ZEROVOLTAGE STATE:1||constanttemperature interlayer tunneling spectroscopy:1||Josephson supercurrent:1||BIPOLAR SUPERCURRENT:1||Interaction between Josephson and pancake vortices:1||flux jump:1||coaxial heterojunction nanorod:1||Natural Josephson coupling:1||BI2SR2CACU2O8+DELTA:1||VORTEX FLOW:1||TC SUPERCONDUCTORS:1||charge imbalance:1||Andreev diffractometer:1||intercalation:1||surface junction:1||Bi2212:1||tunnelling:1||GRAPHITE:1||GROWTH:1||collective transverse plasma modes:1||GAN:1||Macroscopic quantum tunneling:1||Fluctuation conductivity:1||Abovegap conductance jump:1||Josephson vortex motion:1||Intrinsic Josephson junctions:1||LAYERED SUPERCONDUCTORS:1||BI2SR2CACU2O8+Y:1||INTERFACES:1||BREAKDOWN:1||SYSTEMS:1||Anisotropy ratio:1||Josephson vortex:1||spin relaxation in superconductors:1||bibased single crystals:1||MESOSCOPIC PROXIMITY SUPERCONDUCTOR:1||reentrance of conductance:1||interlayer pair tunneling:1||JOSEPHSON:1||DISORDERED 2DIMENSIONAL SUPERCONDUCTORS:1||INDIUM FILMS:1||excited state:1||REGIME:1||triplet superconductivity:1||FILM:1||SCHOTTKY DIODES:1||peakdiphump structure:1||Kondo effect:1||REENTRANCE:1||Graphene:1||CONTACT:1||BERRYS PHASE:1||2DIMENSIONAL SUPERCONDUCTORS:1||Coulomb diamond:1||magnetic domain:1||spin injection:1||RESONANCE:1||plasma excitation modes:1||FLOW:1||OVERDOPED BI2SR2CACU2O8+DELTA:1||hole doping:1||chemical synthesis:1||phase transitions:1||superconductors:1||VORTEXGLASS SUPERCONDUCTIVITY:1||Kondorelated model:1||RADIATION:1||DOT:1||NANOBELTS:1||Complementarity:1||Closedloop AharonovBohm interferometer:1||pair breaking:1||interlayer phase fluctuation:1||MgB2 thin film:1||CONFINEMENT:1||WALLED CARBON NANOTUBES:1||TRANSITION:9||VORTICES:8||STATE:7||intrinsic Josephson junctions:7||SINGLECRYSTALS:7||JUNCTIONS:5||MODES:5||SUPERCURRENT:5||SUPERCONDUCTOR:5||CONDUCTANCE:5||HIGHTEMPERATURE SUPERCONDUCTORS:5||TRANSPORT:5||PHASE:5||FILMS:4||LOCALIZATION:4||SINGLE DIRAC CONE:4||WIRES:4||MAGNETICFIELD:4||STEPS:3||ELECTRONS:3||proximity effect:3||MODEL:3||ARRAYS:3||INTERFERENCE:3||fluxon dynamics:3||HETEROSTRUCTURES:3||INSULATOR:3||Andreev reflection:3||electronic transport:3||FISKE:3||superconductor:2||ZnO:2||quantum point contact:2||METAL:2||DYNAMICS:2||interlayer Josephson coupling:2||SUPERCONDUCTORS:2||YBA2CU3O7DELTA:2||LAYER:2||DOTS:2||quantum dot:2||Article:2||TRANSISTORS:2||CARBON NANOTUBES:2||GAP:2||MECHANISM:2||LINE:2||GIANT SHAPIRO STEPS:2||LAYERS:2||electron energy loss spectroscopy:2||physical phenomena:2||scanning electron microscopy:2||HGTE QUANTUMWELLS:2||BI2TE3:2||SPECTROSCOPY:2||PNJUNCTIONS:2||spinpolarized tunneling:2||INTRINSIC JOSEPHSONJUNCTIONS:2||FIELDS:2||positive magnetoresistance:2||dilute magnetic semiconductor:2||magnetic field:2||scanning transmission electron microscopy:2||QUANTUM OSCILLATIONS:2||TRANSPORTPROPERTIES:2||surface pair current:2||MAGNETORESISTANCE:2||NANORIBBONS:2||INSTABILITY:2||ANDREEV REFLECTION:2||microwave irradiation:2||vertical graphene josephson junction:2||BI2SE3:2||CONDUCTIVITY:2||highTc superconductors:2||DIMENSIONAL ELECTRONGAS:2||graphene:2||Topological insulators:2||Josephson coupling Fraunhofer interference pattern:2||FERROMAGNET:2||DEPENDENCE:2||DETECTOR:2||COHERENCE:2||INJECTION:2||GRAPHENE:1||JOSEPHSONJUNCTIONS:1||LAYERED SUPERCONDUCTOR:1||mode splitting:1||BEHAVIOR:1||spinpolarized transport:1||SUPERCONDUCTING TRANSITION:1||microwave response:1||PSEUDOGAP:1||phase coherence:1||TRANSITIONS:1||Long Josephson junction:1||Charge detection:1||collective resonance modes:1||plasma oscillation modes:1||Superconducting proximity effect:1||Iron pnictide superconductor:1||McMillanRowell oscillations:1||ferromagnetic microstructure:1||superradiant state:1||VOLTAGE:1||branch splitting:1||TENSOR:1||INTERCALATION:1||insitu fabrication:1||NDGAO3:1||DISORDERED METALS:1||GAUGE GLASS:1||LOWTEMPERATURE TRANSPORT:1||spontaneous spin polarization model:1||BIAS:1||emission of electromagnetic waves:1||YBA2CU3O7/PRBA2CU3O7 SUPERLATTICES:1||BOHM:1||SHAPIRO STEPS:1||superconductor/ferromagnet interface:1||OXIDE:1||ANDREEVREFLECTION:1||SinFeAsO single crystal:1||COLLECTIVE MOTION:1||ANGULARDEPENDENCE:1||SUPERCONDUCTIVITY:1||BILAYER GRAPHENE:1||PHOTOLUMINESCENT PROPERTIES:1||SUPERCONDUCTING WEAK LINKS:1||intrinsic Josephson junctions geometrical resonance:1||intrinsic Josephson junction:1||MESOSCOPIC SPINVALVE:1||Bi2212 single crystals:1||intrinsic junctions:1||ANDREEV REFLECTIONS:1||normalmetal/superconductor interface:1||IBI2SR2CACU2OY:1||THERMAL FLUCTUATIONS:1||MIXED STATE:1||BI2.15SR1.85CACU2O8+DELTA:1||intrinsic Josephson effects:1||CACUO:1||QUANTUM POINT CONTACTS:1||resonant tunneling state:1||coherence length:1||NANOWIRE:1||GATES:1||Phase line:1||Thermal activation:1||QUANTUMDOT:1||superconducting proximity effect:1||Andreev interferometer:1||WIRE:1||Josephsonvortexflow branches:1||Bi2212 cuprates:1||LATTICE:1||demannetization effect:1||SUPERCONDUCTING MIRRORS:1||GAS:1||VALLEY TRANSPORT:1||ELECTRODES:1||DEPENDENT TRANSPORT:1||BORNOPPENHEIMER APPROXIMATION:1||collective plasma oscillations:1||fluxon resonance steps:1||STACKS:1||COLLECTIVE DYNAMICS:1||PAIRING SYMMETRY:1||MUON SPIN ROTATION:1||DIMENSIONAL CROSSOVER:1||Bi2Sr2CaCu2Oy highTc superconductors:1||heterojunctions:1||nanostructures:1||surfaces and interfaces:1||QUANTUM TRANSPORT:1||MICROJUNCTIONS:1||RESONATORS:1||STATES:1||FIELD:1||FLUCTUATIONS:1||SCATTERING:1||mode splitting of Josephson vortexflow branches:1||2D superconductivity:1||TRANSISTOR:1||ENERGYGAP:1||SUPERLATTICES:1||IRONBASED SUPERCONDUCTORS:1||PHASEDEPENDENT RESISTANCE:1||QUANTUM PHASETRANSITIONS:1||ELECTRICFIELD:1||HIGH MAGNETICFIELDS:1||NANOWIRE HETEROSTRUCTURES:1||ZNO:1||pair breaking.:1||SUPERCONDUCTING PB:1||domain formation:1||FORCE MICROSCOPY:1||RELAXATION:1||PLASMA RESONANCE:1||coupled Josephson junctions:1||COPPEROXIDE SUPERCONDUCTORS:1||CROSSOVER:1||SIMULATIONS:1||LOWTEMPERATURE:1||CONDUCTORS:1||METALINSULATORTRANSITION:1||SEMICONDUCTOR:1||FIELDEFFECT TRANSISTORS:1||ZEROVOLTAGE STATE:1||constanttemperature interlayer tunneling spectroscopy:1||Josephson supercurrent:1||BIPOLAR SUPERCURRENT:1||Interaction between Josephson and pancake vortices:1||flux jump:1||coaxial heterojunction nanorod:1||Natural Josephson coupling:1||BI2SR2CACU2O8+DELTA:1||VORTEX FLOW:1||TC SUPERCONDUCTORS:1||charge imbalance:1||Andreev diffractometer:1||intercalation:1||surface junction:1||Bi2212:1||tunnelling:1||GRAPHITE:1||GROWTH:1||collective transverse plasma modes:1||GAN:1||Macroscopic quantum tunneling:1||Fluctuation conductivity:1||Abovegap conductance jump:1||Josephson vortex motion:1||Intrinsic Josephson junctions:1||LAYERED SUPERCONDUCTORS:1||BI2SR2CACU2O8+Y:1||INTERFACES:1||BREAKDOWN:1||SYSTEMS:1||Anisotropy ratio:1||Josephson vortex:1||spin relaxation in superconductors:1||bibased single crystals:1||MESOSCOPIC PROXIMITY SUPERCONDUCTOR:1||reentrance of conductance:1||interlayer pair tunneling:1||JOSEPHSON:1||DISORDERED 2DIMENSIONAL SUPERCONDUCTORS:1||INDIUM FILMS:1||excited state:1||REGIME:1||triplet superconductivity:1||FILM:1||SCHOTTKY DIODES:1||peakdiphump structure:1||Kondo effect:1||REENTRANCE:1||Graphene:1||CONTACT:1||BERRYS PHASE:1||2DIMENSIONAL SUPERCONDUCTORS:1||Coulomb diamond:1||magnetic domain:1||spin injection:1||RESONANCE:1||plasma excitation modes:1||FLOW:1||OVERDOPED BI2SR2CACU2O8+DELTA:1||hole doping:1||chemical synthesis:1||phase transitions:1||superconductors:1||VORTEXGLASS SUPERCONDUCTIVITY:1||Kondorelated model:1||RADIATION:1||DOT:1||NANOBELTS:1||Complementarity:1||Closedloop AharonovBohm interferometer:1||pair breaking:1||interlayer phase fluctuation:1||MgB2 thin film:1||CONFINEMENT:1||WALLED CARBON NANOTUBES:1||TRANSITION:9||VORTICES:8||STATE:7||intrinsic Josephson junctions:7||SINGLECRYSTALS:7||JUNCTIONS:5||MODES:5||SUPERCURRENT:5||SUPERCONDUCTOR:5||CONDUCTANCE:5||HIGHTEMPERATURE SUPERCONDUCTORS:5||TRANSPORT:5||PHASE:5||FILMS:4||LOCALIZATION:4||SINGLE DIRAC CONE:4||WIRES:4||MAGNETICFIELD:4||STEPS:3||ELECTRONS:3||proximity effect:3||MODEL:3||ARRAYS:3||INTERFERENCE:3||fluxon dynamics:3||HETEROSTRUCTURES:3||INSULATOR:3||Andreev reflection:3||electronic transport:3||FISKE:3||superconductor:2||ZnO:2||quantum point contact:2||METAL:2||DYNAMICS:2||interlayer Josephson coupling:2||SUPERCONDUCTORS:2||YBA2CU3O7DELTA:2||LAYER:2||DOTS:2||quantum dot:2||Article:2||TRANSISTORS:2||CARBON NANOTUBES:2||GAP:2||MECHANISM:2||LINE:2||GIANT SHAPIRO STEPS:2||LAYERS:2||electron energy loss spectroscopy:2||physical phenomena:2||scanning electron microscopy:2||HGTE QUANTUMWELLS:2||BI2TE3:2||SPECTROSCOPY:2||PNJUNCTIONS:2||spinpolarized tunneling:2||INTRINSIC JOSEPHSONJUNCTIONS:2||FIELDS:2||positive magnetoresistance:2||dilute magnetic semiconductor:2||magnetic field:2||scanning transmission electron microscopy:2||QUANTUM OSCILLATIONS:2||TRANSPORTPROPERTIES:2||surface pair current:2||MAGNETORESISTANCE:2||NANORIBBONS:2||INSTABILITY:2||ANDREEV REFLECTION:2||microwave irradiation:2||vertical graphene josephson junction:2||BI2SE3:2||CONDUCTIVITY:2||highTc superconductors:2||DIMENSIONAL ELECTRONGAS:2||graphene:2||Topological insulators:2||Josephson coupling Fraunhofer interference pattern:2||FERROMAGNET:2||DEPENDENCE:2||DETECTOR:2||COHERENCE:2||INJECTION:2||GRAPHENE:1||JOSEPHSONJUNCTIONS:1||LAYERED SUPERCONDUCTOR:1||mode splitting:1||BEHAVIOR:1||spinpolarized transport:1||SUPERCONDUCTING TRANSITION:1||microwave response:1||PSEUDOGAP:1||phase coherence:1||TRANSITIONS:1||Long Josephson junction:1||Charge detection:1||collective resonance modes:1||plasma oscillation modes:1||Superconducting proximity effect:1||Iron pnictide superconductor:1||McMillanRowell oscillations:1||ferromagnetic microstructure:1||superradiant state:1||VOLTAGE:1||branch splitting:1||TENSOR:1||INTERCALATION:1||insitu fabrication:1||NDGAO3:1||DISORDERED METALS:1||GAUGE GLASS:1||LOWTEMPERATURE TRANSPORT:1||spontaneous spin polarization model:1||BIAS:1||emission of electromagnetic waves:1||YBA2CU3O7/PRBA2CU3O7 SUPERLATTICES:1||BOHM:1||SHAPIRO STEPS:1||superconductor/ferromagnet interface:1||OXIDE:1||ANDREEVREFLECTION:1||SinFeAsO single crystal:1||COLLECTIVE MOTION:1||ANGULARDEPENDENCE:1||SUPERCONDUCTIVITY:1||BILAYER GRAPHENE:1||PHOTOLUMINESCENT PROPERTIES:1||SUPERCONDUCTING WEAK LINKS:1||intrinsic Josephson junctions geometrical resonance:1||intrinsic Josephson junction:1||MESOSCOPIC SPINVALVE:1||Bi2212 single crystals:1||intrinsic junctions:1||ANDREEV REFLECTIONS:1||normalmetal/superconductor interface:1||IBI2SR2CACU2OY:1||THERMAL FLUCTUATIONS:1||MIXED STATE:1||BI2.15SR1.85CACU2O8+DELTA:1||intrinsic Josephson effects:1||CACUO:1||QUANTUM POINT CONTACTS:1||resonant tunneling state:1||coherence length:1||NANOWIRE:1||GATES:1||Phase line:1||Thermal activation:1||QUANTUMDOT:1||superconducting proximity effect:1||Andreev interferometer:1||WIRE:1||Josephsonvortexflow branches:1||Bi2212 cuprates:1||LATTICE:1||demannetization effect:1||SUPERCONDUCTING MIRRORS:1||GAS:1||VALLEY TRANSPORT:1||ELECTRODES:1||DEPENDENT TRANSPORT:1||BORNOPPENHEIMER APPROXIMATION:1||collective plasma oscillations:1||fluxon resonance steps:1||STACKS:1||COLLECTIVE DYNAMICS:1||PAIRING SYMMETRY:1||MUON SPIN ROTATION:1||DIMENSIONAL CROSSOVER:1||Bi2Sr2CaCu2Oy highTc superconductors:1||heterojunctions:1||nanostructures:1||surfaces and interfaces:1||QUANTUM TRANSPORT:1||MICROJUNCTIONS:1||RESONATORS:1||STATES:1||FIELD:1||FLUCTUATIONS:1||SCATTERING:1||mode splitting of Josephson vortexflow branches:1||2D superconductivity:1||TRANSISTOR:1||ENERGYGAP:1||SUPERLATTICES:1||IRONBASED SUPERCONDUCTORS:1||PHASEDEPENDENT RESISTANCE:1||QUANTUM PHASETRANSITIONS:1||ELECTRICFIELD:1||HIGH MAGNETICFIELDS:1||NANOWIRE HETEROSTRUCTURES:1||ZNO:1||pair breaking.:1||SUPERCONDUCTING PB:1||domain formation:1||FORCE MICROSCOPY:1||RELAXATION:1||PLASMA RESONANCE:1||coupled Josephson junctions:1||COPPEROXIDE SUPERCONDUCTORS:1||CROSSOVER:1||SIMULATIONS:1||LOWTEMPERATURE:1||CONDUCTORS:1||METALINSULATORTRANSITION:1||SEMICONDUCTOR:1||FIELDEFFECT TRANSISTORS:1||ZEROVOLTAGE STATE:1||constanttemperature interlayer tunneling spectroscopy:1||Josephson supercurrent:1||BIPOLAR SUPERCURRENT:1||Interaction between Josephson and pancake vortices:1||flux jump:1||coaxial heterojunction nanorod:1||Natural Josephson coupling:1||BI2SR2CACU2O8+DELTA:1||VORTEX FLOW:1||TC SUPERCONDUCTORS:1||charge imbalance:1||Andreev diffractometer:1||intercalation:1||surface junction:1||Bi2212:1||tunnelling:1||GRAPHITE:1||GROWTH:1||collective transverse plasma modes:1||GAN:1||Macroscopic quantum tunneling:1||Fluctuation conductivity:1||Abovegap conductance jump:1||Josephson vortex motion:1||Intrinsic Josephson junctions:1||LAYERED SUPERCONDUCTORS:1||BI2SR2CACU2O8+Y:1||INTERFACES:1||BREAKDOWN:1||SYSTEMS:1||Anisotropy ratio:1||Josephson vortex:1||spin relaxation in superconductors:1||bibased single crystals:1||MESOSCOPIC PROXIMITY SUPERCONDUCTOR:1||reentrance of conductance:1||interlayer pair tunneling:1||JOSEPHSON:1||DISORDERED 2DIMENSIONAL SUPERCONDUCTORS:1||INDIUM FILMS:1||excited state:1||REGIME:1||triplet superconductivity:1||FILM:1||SCHOTTKY DIODES:1||peakdiphump structure:1||Kondo effect:1||REENTRANCE:1||Graphene:1||CONTACT:1||BERRYS PHASE:1||2DIMENSIONAL SUPERCONDUCTORS:1||Coulomb diamond:1||magnetic domain:1||spin injection:1||RESONANCE:1||plasma excitation modes:1||FLOW:1||OVERDOPED BI2SR2CACU2O8+DELTA:1||hole doping:1||chemical synthesis:1||phase transitions:1||superconductors:1||VORTEXGLASS SUPERCONDUCTIVITY:1||Kondorelated model:1||RADIATION:1||DOT:1||NANOBELTS:1||Complementarity:1||Closedloop AharonovBohm interferometer:1||pair breaking:1||interlayer phase fluctuation:1||MgB2 thin film:1||CONFINEMENT:1||WALLED CARBON NANOTUBES:1||TRANSITION:9||VORTICES:8||STATE:7||intrinsic Josephson junctions:7||SINGLECRYSTALS:7||JUNCTIONS:5||MODES:5||SUPERCURRENT:5||SUPERCONDUCTOR:5||CONDUCTANCE:5||HIGHTEMPERATURE SUPERCONDUCTORS:5||TRANSPORT:5||PHASE:5||FILMS:4||LOCALIZATION:4||SINGLE DIRAC CONE:4||WIRES:4||MAGNETICFIELD:4||STEPS:3||ELECTRONS:3||proximity effect:3||MODEL:3||ARRAYS:3||INTERFERENCE:3||fluxon dynamics:3||HETEROSTRUCTURES:3||INSULATOR:3||Andreev reflection:3||electronic transport:3||FISKE:3||superconductor:2||ZnO:2||quantum point contact:2||METAL:2||DYNAMICS:2||interlayer Josephson coupling:2||SUPERCONDUCTORS:2||YBA2CU3O7DELTA:2||LAYER:2||DOTS:2||quantum dot:2||Article:2||TRANSISTORS:2||CARBON NANOTUBES:2||GAP:2||MECHANISM:2||LINE:2||GIANT SHAPIRO STEPS:2||LAYERS:2||electron energy loss spectroscopy:2||physical phenomena:2||scanning electron microscopy:2||HGTE QUANTUMWELLS:2||BI2TE3:2||SPECTROSCOPY:2||PNJUNCTIONS:2||spinpolarized tunneling:2||INTRINSIC JOSEPHSONJUNCTIONS:2||FIELDS:2||positive magnetoresistance:2||dilute magnetic semiconductor:2||magnetic field:2||scanning transmission electron microscopy:2||QUANTUM OSCILLATIONS:2||TRANSPORTPROPERTIES:2||surface pair current:2||MAGNETORESISTANCE:2||NANORIBBONS:2||INSTABILITY:2||ANDREEV REFLECTION:2||microwave irradiation:2||vertical graphene josephson junction:2||BI2SE3:2||CONDUCTIVITY:2||highTc superconductors:2||DIMENSIONAL ELECTRONGAS:2||graphene:2||Topological insulators:2||Josephson coupling Fraunhofer interference pattern:2||FERROMAGNET:2||DEPENDENCE:2||DETECTOR:2||COHERENCE:2||INJECTION:2||GRAPHENE:1||JOSEPHSONJUNCTIONS:1||LAYERED SUPERCONDUCTOR:1||mode splitting:1||BEHAVIOR:1||spinpolarized transport:1||SUPERCONDUCTING TRANSITION:1||microwave response:1||PSEUDOGAP:1||phase coherence:1||TRANSITIONS:1||Long Josephson junction:1||Charge detection:1||collective resonance modes:1||plasma oscillation modes:1||Superconducting proximity effect:1||Iron pnictide superconductor:1||McMillanRowell oscillations:1||ferromagnetic microstructure:1||superradiant state:1||VOLTAGE:1||branch splitting:1||TENSOR:1||INTERCALATION:1||insitu fabrication:1||NDGAO3:1||DISORDERED METALS:1||GAUGE GLASS:1||LOWTEMPERATURE TRANSPORT:1||spontaneous spin polarization model:1||BIAS:1||emission of electromagnetic waves:1||YBA2CU3O7/PRBA2CU3O7 SUPERLATTICES:1||BOHM:1||SHAPIRO STEPS:1||superconductor/ferromagnet interface:1||OXIDE:1||ANDREEVREFLECTION:1||SinFeAsO single crystal:1||COLLECTIVE MOTION:1||ANGULARDEPENDENCE:1||SUPERCONDUCTIVITY:1||BILAYER GRAPHENE:1||PHOTOLUMINESCENT PROPERTIES:1||SUPERCONDUCTING WEAK LINKS:1||intrinsic Josephson junctions geometrical resonance:1||intrinsic Josephson junction:1||MESOSCOPIC SPINVALVE:1||Bi2212 single crystals:1||intrinsic junctions:1||ANDREEV REFLECTIONS:1||normalmetal/superconductor interface:1||IBI2SR2CACU2OY:1||THERMAL FLUCTUATIONS:1||MIXED STATE:1||BI2.15SR1.85CACU2O8+DELTA:1||intrinsic Josephson effects:1||CACUO:1||QUANTUM POINT CONTACTS:1||resonant tunneling state:1||coherence length:1||NANOWIRE:1||GATES:1||Phase line:1||Thermal activation:1||QUANTUMDOT:1||superconducting proximity effect:1||Andreev interferometer:1||WIRE:1||Josephsonvortexflow branches:1||Bi2212 cuprates:1||LATTICE:1||demannetization effect:1||SUPERCONDUCTING MIRRORS:1||GAS:1||VALLEY TRANSPORT:1||ELECTRODES:1||DEPENDENT TRANSPORT:1||BORNOPPENHEIMER APPROXIMATION:1||collective plasma oscillations:1||fluxon resonance steps:1||STACKS:1||COLLECTIVE DYNAMICS:1||PAIRING SYMMETRY:1||MUON SPIN ROTATION:1||DIMENSIONAL CROSSOVER:1||Bi2Sr2CaCu2Oy highTc superconductors:1||heterojunctions:1||nanostructures:1||surfaces and interfaces:1||QUANTUM TRANSPORT:1||MICROJUNCTIONS:1||RESONATORS:1||STATES:1||FIELD:1||FLUCTUATIONS:1||SCATTERING:1||mode splitting of Josephson vortexflow branches:1||2D superconductivity:1||TRANSISTOR:1||ENERGYGAP:1||SUPERLATTICES:1||IRONBASED SUPERCONDUCTORS:1||PHASEDEPENDENT RESISTANCE:1||QUANTUM PHASETRANSITIONS:1||ELECTRICFIELD:1||HIGH MAGNETICFIELDS:1||NANOWIRE HETEROSTRUCTURES:1||ZNO:1||pair breaking.:1||SUPERCONDUCTING PB:1||domain formation:1||FORCE MICROSCOPY:1||RELAXATION:1||PLASMA RESONANCE:1||coupled Josephson junctions:1||COPPEROXIDE SUPERCONDUCTORS:1||CROSSOVER:1||SIMULATIONS:1||LOWTEMPERATURE:1||CONDUCTORS:1||METALINSULATORTRANSITION:1||SEMICONDUCTOR:1||FIELDEFFECT TRANSISTORS:1||ZEROVOLTAGE STATE:1||constanttemperature interlayer tunneling spectroscopy:1||Josephson supercurrent:1||BIPOLAR SUPERCURRENT:1||Interaction between Josephson and pancake vortices:1||flux jump:1||coaxial heterojunction nanorod:1||Natural Josephson coupling:1||BI2SR2CACU2O8+DELTA:1||VORTEX FLOW:1||TC SUPERCONDUCTORS:1||charge imbalance:1||Andreev diffractometer:1||intercalation:1||surface junction:1||Bi2212:1||tunnelling:1||GRAPHITE:1||GROWTH:1||collective transverse plasma modes:1||GAN:1||Macroscopic quantum tunneling:1||Fluctuation conductivity:1||Abovegap conductance jump:1||Josephson vortex motion:1||Intrinsic Josephson junctions:1||LAYERED SUPERCONDUCTORS:1||BI2SR2CACU2O8+Y:1||INTERFACES:1||BREAKDOWN:1||SYSTEMS:1||Anisotropy ratio:1||Josephson vortex:1||spin relaxation in superconductors:1||bibased single crystals:1||MESOSCOPIC PROXIMITY SUPERCONDUCTOR:1||reentrance of conductance:1||interlayer pair tunneling:1||JOSEPHSON:1||DISORDERED 2DIMENSIONAL SUPERCONDUCTORS:1||INDIUM FILMS:1||excited state:1||REGIME:1||triplet superconductivity:1||FILM:1||SCHOTTKY DIODES:1||peakdiphump structure:1||Kondo effect:1||REENTRANCE:1||Graphene:1||CONTACT:1||BERRYS PHASE:1||2DIMENSIONAL SUPERCONDUCTORS:1||Coulomb diamond:1||magnetic domain:1||spin injection:1||RESONANCE:1||plasma excitation modes:1||FLOW:1||OVERDOPED BI2SR2CACU2O8+DELTA:1||hole doping:1||chemical synthesis:1||phase transitions:1||superconductors:1||VORTEXGLASS SUPERCONDUCTIVITY:1||Kondorelated model:1||RADIATION:1||DOT:1||NANOBELTS:1||Complementarity:1||Closedloop AharonovBohm interferometer:1||pair breaking:1||interlayer phase fluctuation:1||MgB2 thin film:1||CONFINEMENT:1||WALLED CARBON NANOTUBES:1||TRANSITION:9||VORTICES:8||STATE:7||intrinsic Josephson junctions:7||SINGLECRYSTALS:7||JUNCTIONS:5||MODES:5||SUPERCURRENT:5||SUPERCONDUCTOR:5||CONDUCTANCE:5||HIGHTEMPERATURE SUPERCONDUCTORS:5||TRANSPORT:5||PHASE:5||FILMS:4||LOCALIZATION:4||SINGLE DIRAC CONE:4||WIRES:4||MAGNETICFIELD:4||STEPS:3||ELECTRONS:3||proximity effect:3||MODEL:3||ARRAYS:3||INTERFERENCE:3||fluxon dynamics:3||HETEROSTRUCTURES:3||INSULATOR:3||Andreev reflection:3||electronic transport:3||FISKE:3||superconductor:2||ZnO:2||quantum point contact:2||METAL:2||DYNAMICS:2||interlayer Josephson coupling:2||SUPERCONDUCTORS:2||YBA2CU3O7DELTA:2||LAYER:2||DOTS:2||quantum dot:2||Article:2||TRANSISTORS:2||CARBON NANOTUBES:2||GAP:2||MECHANISM:2||LINE:2||GIANT SHAPIRO STEPS:2||LAYERS:2||electron energy loss spectroscopy:2||physical phenomena:2||scanning electron microscopy:2||HGTE QUANTUMWELLS:2||BI2TE3:2||SPECTROSCOPY:2||PNJUNCTIONS:2||spinpolarized tunneling:2||INTRINSIC JOSEPHSONJUNCTIONS:2||FIELDS:2||positive magnetoresistance:2||dilute magnetic semiconductor:2||magnetic field:2||scanning transmission electron microscopy:2||QUANTUM OSCILLATIONS:2||TRANSPORTPROPERTIES:2||surface pair current:2||MAGNETORESISTANCE:2||NANORIBBONS:2||INSTABILITY:2||ANDREEV REFLECTION:2||microwave irradiation:2||vertical graphene josephson junction:2||BI2SE3:2||CONDUCTIVITY:2||highTc superconductors:2||DIMENSIONAL ELECTRONGAS:2||graphene:2||Topological insulators:2||Josephson coupling Fraunhofer interference pattern:2||FERROMAGNET:2||DEPENDENCE:2||DETECTOR:2||COHERENCE:2||INJECTION:2||GRAPHENE:1||JOSEPHSONJUNCTIONS:1||LAYERED SUPERCONDUCTOR:1||mode splitting:1||BEHAVIOR:1||spinpolarized transport:1||SUPERCONDUCTING TRANSITION:1||microwave response:1||PSEUDOGAP:1||phase coherence:1||TRANSITIONS:1||Long Josephson junction:1||Charge detection:1||collective resonance modes:1||plasma oscillation modes:1||Superconducting proximity effect:1||Iron pnictide superconductor:1||McMillanRowell oscillations:1||ferromagnetic microstructure:1||superradiant state:1||VOLTAGE:1||branch splitting:1||TENSOR:1||INTERCALATION:1||insitu fabrication:1||NDGAO3:1||DISORDERED METALS:1||GAUGE GLASS:1||LOWTEMPERATURE TRANSPORT:1||spontaneous spin polarization model:1||BIAS:1||emission of electromagnetic waves:1||YBA2CU3O7/PRBA2CU3O7 SUPERLATTICES:1||BOHM:1||SHAPIRO STEPS:1||superconductor/ferromagnet interface:1||OXIDE:1||ANDREEVREFLECTION:1||SinFeAsO single crystal:1||COLLECTIVE MOTION:1||ANGULARDEPENDENCE:1||SUPERCONDUCTIVITY:1||BILAYER GRAPHENE:1||PHOTOLUMINESCENT PROPERTIES:1||SUPERCONDUCTING WEAK LINKS:1||intrinsic Josephson junctions geometrical resonance:1||intrinsic Josephson junction:1||MESOSCOPIC SPINVALVE:1||Bi2212 single crystals:1||intrinsic junctions:1||ANDREEV REFLECTIONS:1||normalmetal/superconductor interface:1||IBI2SR2CACU2OY:1||THERMAL FLUCTUATIONS:1||MIXED STATE:1||BI2.15SR1.85CACU2O8+DELTA:1||intrinsic Josephson effects:1||CACUO:1||QUANTUM POINT CONTACTS:1||resonant tunneling state:1||coherence length:1||NANOWIRE:1||GATES:1||Phase line:1||Thermal activation:1||QUANTUMDOT:1||superconducting proximity effect:1||Andreev interferometer:1||WIRE:1||Josephsonvortexflow branches:1||Bi2212 cuprates:1||LATTICE:1||demannetization effect:1||SUPERCONDUCTING MIRRORS:1||GAS:1||VALLEY TRANSPORT:1||ELECTRODES:1||DEPENDENT TRANSPORT:1||BORNOPPENHEIMER APPROXIMATION:1||collective plasma oscillations:1||fluxon resonance steps:1||STACKS:1||COLLECTIVE DYNAMICS:1||PAIRING SYMMETRY:1||MUON SPIN ROTATION:1||DIMENSIONAL CROSSOVER:1||Bi2Sr2CaCu2Oy highTc superconductors:1||heterojunctions:1||nanostructures:1||surfaces and interfaces:1||QUANTUM TRANSPORT:1||MICROJUNCTIONS:1||RESONATORS:1||STATES:1||FIELD:1||FLUCTUATIONS:1||SCATTERING:1||mode splitting of Josephson vortexflow branches:1||2D superconductivity:1||TRANSISTOR:1||ENERGYGAP:1||SUPERLATTICES:1||IRONBASED SUPERCONDUCTORS:1||PHASEDEPENDENT RESISTANCE:1||QUANTUM PHASETRANSITIONS:1||ELECTRICFIELD:1||HIGH MAGNETICFIELDS:1||NANOWIRE HETEROSTRUCTURES:1||ZNO:1||pair breaking.:1||SUPERCONDUCTING PB:1||domain formation:1||FORCE MICROSCOPY:1||RELAXATION:1||PLASMA RESONANCE:1||coupled Josephson junctions:1||COPPEROXIDE SUPERCONDUCTORS:1||CROSSOVER:1||SIMULATIONS:1||LOWTEMPERATURE:1||CONDUCTORS:1||METALINSULATORTRANSITION:1||SEMICONDUCTOR:1||FIELDEFFECT TRANSISTORS:1||ZEROVOLTAGE STATE:1||constanttemperature interlayer tunneling spectroscopy:1||Josephson supercurrent:1||BIPOLAR SUPERCURRENT:1||Interaction between Josephson and pancake vortices:1||flux jump:1||coaxial heterojunction nanorod:1||Natural Josephson coupling:1||BI2SR2CACU2O8+DELTA:1||VORTEX FLOW:1||TC SUPERCONDUCTORS:1||charge imbalance:1||Andreev diffractometer:1||intercalation:1||surface junction:1||Bi2212:1||tunnelling:1||GRAPHITE:1||GROWTH:1||collective transverse plasma modes:1||GAN:1||Macroscopic quantum tunneling:1||Fluctuation conductivity:1||Abovegap conductance jump:1||Josephson vortex motion:1||Intrinsic Josephson junctions:1||LAYERED SUPERCONDUCTORS:1||BI2SR2CACU2O8+Y:1||INTERFACES:1||BREAKDOWN:1||SYSTEMS:1||Anisotropy ratio:1||Josephson vortex:1||spin relaxation in superconductors:1||bibased single crystals:1||MESOSCOPIC PROXIMITY SUPERCONDUCTOR:1||reentrance of conductance:1||interlayer pair tunneling:1||JOSEPHSON:1||DISORDERED 2DIMENSIONAL SUPERCONDUCTORS:1||INDIUM FILMS:1||excited state:1||REGIME:1||triplet superconductivity:1||FILM:1||SCHOTTKY DIODES:1||peakdiphump structure:1||Kondo effect:1||REENTRANCE:1||Graphene:1||CONTACT:1||BERRYS PHASE:1||2DIMENSIONAL SUPERCONDUCTORS:1||Coulomb diamond:1||magnetic domain:1||spin injection:1||RESONANCE:1||plasma excitation modes:1||FLOW:1||OVERDOPED BI2SR2CACU2O8+DELTA:1||hole doping:1||chemical synthesis:1||phase transitions:1||superconductors:1||VORTEXGLASS SUPERCONDUCTIVITY:1||Kondorelated model:1||RADIATION:1||DOT:1||NANOBELTS:1||Complementarity:1||Closedloop AharonovBohm interferometer:1||pair breaking:1||interlayer phase fluctuation:1||MgB2 thin film:1||CONFINEMENT:1||WALLED CARBON NANOTUBES:1||TRANSITION:9||VORTICES:8||STATE:7||intrinsic Josephson junctions:7||SINGLECRYSTALS:7||JUNCTIONS:5||MODES:5||SUPERCURRENT:5||SUPERCONDUCTOR:5||CONDUCTANCE:5||HIGHTEMPERATURE SUPERCONDUCTORS:5||TRANSPORT:5||PHASE:5||FILMS:4||LOCALIZATION:4||SINGLE DIRAC CONE:4||WIRES:4||MAGNETICFIELD:4||STEPS:3||ELECTRONS:3||proximity effect:3||MODEL:3||ARRAYS:3||INTERFERENCE:3||fluxon dynamics:3||HETEROSTRUCTURES:3||INSULATOR:3||Andreev reflection:3||electronic transport:3||FISKE:3||superconductor:2||ZnO:2||quantum point contact:2||METAL:2||DYNAMICS:2||interlayer Josephson coupling:2||SUPERCONDUCTORS:2||YBA2CU3O7DELTA:2||LAYER:2||DOTS:2||quantum dot:2||Article:2||TRANSISTORS:2||CARBON NANOTUBES:2||GAP:2||MECHANISM:2||LINE:2||GIANT SHAPIRO STEPS:2||LAYERS:2||electron energy loss spectroscopy:2||physical phenomena:2||scanning electron microscopy:2||HGTE QUANTUMWELLS:2||BI2TE3:2||SPECTROSCOPY:2||PNJUNCTIONS:2||spinpolarized tunneling:2||INTRINSIC JOSEPHSONJUNCTIONS:2||FIELDS:2||positive magnetoresistance:2||dilute magnetic semiconductor:2||magnetic field:2||scanning transmission electron microscopy:2||QUANTUM OSCILLATIONS:2||TRANSPORTPROPERTIES:2||surface pair current:2||MAGNETORESISTANCE:2||NANORIBBONS:2||INSTABILITY:2||ANDREEV REFLECTION:2||microwave irradiation:2||vertical graphene josephson junction:2||BI2SE3:2||CONDUCTIVITY:2||highTc superconductors:2||DIMENSIONAL ELECTRONGAS:2||graphene:2||Topological insulators:2||Josephson coupling Fraunhofer interference pattern:2||FERROMAGNET:2||DEPENDENCE:2||DETECTOR:2||COHERENCE:2||INJECTION:2||GRAPHENE:1||JOSEPHSONJUNCTIONS:1||LAYERED SUPERCONDUCTOR:1||mode splitting:1||BEHAVIOR:1||spinpolarized transport:1||SUPERCONDUCTING TRANSITION:1||microwave response:1||PSEUDOGAP:1||phase coherence:1||TRANSITIONS:1||Long Josephson junction:1||Charge detection:1||collective resonance modes:1||plasma oscillation modes:1||Superconducting proximity effect:1||Iron pnictide superconductor:1||McMillanRowell oscillations:1||ferromagnetic microstructure:1||superradiant state:1||VOLTAGE:1||branch splitting:1||TENSOR:1||INTERCALATION:1||insitu fabrication:1||NDGAO3:1||DISORDERED METALS:1||GAUGE GLASS:1||LOWTEMPERATURE TRANSPORT:1||spontaneous spin polarization model:1||BIAS:1||emission of electromagnetic waves:1||YBA2CU3O7/PRBA2CU3O7 SUPERLATTICES:1||BOHM:1||SHAPIRO STEPS:1||superconductor/ferromagnet interface:1||OXIDE:1||ANDREEVREFLECTION:1||SinFeAsO single crystal:1||COLLECTIVE MOTION:1||ANGULARDEPENDENCE:1||SUPERCONDUCTIVITY:1||BILAYER GRAPHENE:1||PHOTOLUMINESCENT PROPERTIES:1||SUPERCONDUCTING WEAK LINKS:1||intrinsic Josephson junctions geometrical resonance:1||intrinsic Josephson junction:1||MESOSCOPIC SPINVALVE:1||Bi2212 single crystals:1||intrinsic junctions:1||ANDREEV REFLECTIONS:1||normalmetal/superconductor interface:1||IBI2SR2CACU2OY:1||THERMAL FLUCTUATIONS:1||MIXED STATE:1||BI2.15SR1.85CACU2O8+DELTA:1||intrinsic Josephson effects:1||CACUO:1||QUANTUM POINT CONTACTS:1||resonant tunneling state:1||coherence length:1||NANOWIRE:1||GATES:1||Phase line:1||Thermal activation:1||QUANTUMDOT:1||superconducting proximity effect:1||Andreev interferometer:1||WIRE:1||Josephsonvortexflow branches:1||Bi2212 cuprates:1||LATTICE:1||demannetization effect:1||SUPERCONDUCTING MIRRORS:1||GAS:1||VALLEY TRANSPORT:1||ELECTRODES:1||DEPENDENT TRANSPORT:1||BORNOPPENHEIMER APPROXIMATION:1||collective plasma oscillations:1||fluxon resonance steps:1||STACKS:1||COLLECTIVE DYNAMICS:1||PAIRING SYMMETRY:1||MUON SPIN ROTATION:1||DIMENSIONAL CROSSOVER:1||Bi2Sr2CaCu2Oy highTc superconductors:1||heterojunctions:1||nanostructures:1||surfaces and interfaces:1||QUANTUM TRANSPORT:1||MICROJUNCTIONS:1||RESONATORS:1||STATES:1||FIELD:1||FLUCTUATIONS:1||SCATTERING:1||mode splitting of Josephson vortexflow branches:1||2D superconductivity:1||TRANSISTOR:1||ENERGYGAP:1||SUPERLATTICES:1||IRONBASED SUPERCONDUCTORS:1||PHASEDEPENDENT RESISTANCE:1||QUANTUM PHASETRANSITIONS:1||ELECTRICFIELD:1||HIGH MAGNETICFIELDS:1||NANOWIRE HETEROSTRUCTURES:1||ZNO:1||pair breaking.:1||SUPERCONDUCTING PB:1||domain formation:1||FORCE MICROSCOPY:1||RELAXATION:1||PLASMA RESONANCE:1||coupled Josephson junctions:1||COPPEROXIDE SUPERCONDUCTORS:1||CROSSOVER:1||SIMULATIONS:1||LOWTEMPERATURE:1||CONDUCTORS:1||METALINSULATORTRANSITION:1||SEMICONDUCTOR:1||FIELDEFFECT TRANSISTORS:1||ZEROVOLTAGE STATE:1||constanttemperature interlayer tunneling spectroscopy:1||Josephson supercurrent:1||BIPOLAR SUPERCURRENT:1||Interaction between Josephson and pancake vortices:1||flux jump:1||coaxial heterojunction nanorod:1||Natural Josephson coupling:1||BI2SR2CACU2O8+DELTA:1||VORTEX FLOW:1||TC SUPERCONDUCTORS:1||charge imbalance:1||Andreev diffractometer:1||intercalation:1||surface junction:1||Bi2212:1||tunnelling:1||GRAPHITE:1||GROWTH:1||collective transverse plasma modes:1||GAN:1||Macroscopic quantum tunneling:1||Fluctuation conductivity:1||Abovegap conductance jump:1||Josephson vortex motion:1||Intrinsic Josephson junctions:1||LAYERED SUPERCONDUCTORS:1||BI2SR2CACU2O8+Y:1||INTERFACES:1||BREAKDOWN:1||SYSTEMS:1||Anisotropy ratio:1||Josephson vortex:1||spin relaxation in superconductors:1||bibased single crystals:1||MESOSCOPIC PROXIMITY SUPERCONDUCTOR:1||reentrance of conductance:1||interlayer pair tunneling:1||JOSEPHSON:1||DISORDERED 2DIMENSIONAL SUPERCONDUCTORS:1||INDIUM FILMS:1||excited state:1||REGIME:1||triplet superconductivity:1||FILM:1||SCHOTTKY DIODES:1||peakdiphump structure:1||Kondo effect:1||REENTRANCE:1||Graphene:1||CONTACT:1||BERRYS PHASE:1||2DIMENSIONAL SUPERCONDUCTORS:1||Coulomb diamond:1||magnetic domain:1||spin injection:1||RESONANCE:1||plasma excitation modes:1||FLOW:1||OVERDOPED BI2SR2CACU2O8+DELTA:1||hole doping:1||chemical synthesis:1||phase transitions:1||superconductors:1||VORTEXGLASS SUPERCONDUCTIVITY:1||Kondorelated model:1||RADIATION:1||DOT:1||NANOBELTS:1||Complementarity:1||Closedloop AharonovBohm interferometer:1||pair breaking:1||interlayer phase fluctuation:1||MgB2 thin film:1||CONFINEMENT:1||WALLED CARBON NANOTUBES:1||TRANSITION:9||VORTICES:8||STATE:7||intrinsic Josephson junctions:7||SINGLECRYSTALS:7||JUNCTIONS:5||MODES:5||SUPERCURRENT:5||SUPERCONDUCTOR:5||CONDUCTANCE:5||HIGHTEMPERATURE SUPERCONDUCTORS:5||TRANSPORT:5||PHASE:5||FILMS:4||LOCALIZATION:4||SINGLE DIRAC CONE:4||WIRES:4||MAGNETICFIELD:4||STEPS:3||ELECTRONS:3||proximity effect:3||MODEL:3||ARRAYS:3||INTERFERENCE:3||fluxon dynamics:3||HETEROSTRUCTURES:3||INSULATOR:3||Andreev reflection:3||electronic transport:3||FISKE:3||superconductor:2||ZnO:2||quantum point contact:2||METAL:2||DYNAMICS:2||interlayer Josephson coupling:2||SUPERCONDUCTORS:2||YBA2CU3O7DELTA:2||LAYER:2||DOTS:2||quantum dot:2||Article:2||TRANSISTORS:2||CARBON NANOTUBES:2||GAP:2||MECHANISM:2||LINE:2||GIANT SHAPIRO STEPS:2||LAYERS:2||electron energy loss spectroscopy:2||physical phenomena:2||scanning electron microscopy:2||HGTE QUANTUMWELLS:2||BI2TE3:2||SPECTROSCOPY:2||PNJUNCTIONS:2||spinpolarized tunneling:2||INTRINSIC JOSEPHSONJUNCTIONS:2||FIELDS:2||positive magnetoresistance:2||dilute magnetic semiconductor:2||magnetic field:2||scanning transmission electron microscopy:2||QUANTUM OSCILLATIONS:2||TRANSPORTPROPERTIES:2||surface pair current:2||MAGNETORESISTANCE:2||NANORIBBONS:2||INSTABILITY:2||ANDREEV REFLECTION:2||microwave irradiation:2||vertical graphene josephson junction:2||BI2SE3:2||CONDUCTIVITY:2||highTc superconductors:2||DIMENSIONAL ELECTRONGAS:2||graphene:2||Topological insulators:2||Josephson coupling Fraunhofer interference pattern:2||FERROMAGNET:2||DEPENDENCE:2||DETECTOR:2||COHERENCE:2||INJECTION:2||GRAPHENE:1||JOSEPHSONJUNCTIONS:1||LAYERED SUPERCONDUCTOR:1||mode splitting:1||BEHAVIOR:1||spinpolarized transport:1||SUPERCONDUCTING TRANSITION:1||microwave response:1||PSEUDOGAP:1||phase coherence:1||TRANSITIONS:1||Long Josephson junction:1||Charge detection:1||collective resonance modes:1||plasma oscillation modes:1||Superconducting proximity effect:1||Iron pnictide superconductor:1||McMillanRowell oscillations:1||ferromagnetic microstructure:1||superradiant state:1||VOLTAGE:1||branch splitting:1||TENSOR:1||INTERCALATION:1||insitu fabrication:1||NDGAO3:1||DISORDERED METALS:1||GAUGE GLASS:1||LOWTEMPERATURE TRANSPORT:1||spontaneous spin polarization model:1||BIAS:1||emission of electromagnetic waves:1||YBA2CU3O7/PRBA2CU3O7 SUPERLATTICES:1||BOHM:1||SHAPIRO STEPS:1||superconductor/ferromagnet interface:1||OXIDE:1||ANDREEVREFLECTION:1||SinFeAsO single crystal:1||COLLECTIVE MOTION:1||ANGULARDEPENDENCE:1||SUPERCONDUCTIVITY:1||BILAYER GRAPHENE:1||PHOTOLUMINESCENT PROPERTIES:1||SUPERCONDUCTING WEAK LINKS:1||intrinsic Josephson junctions geometrical resonance:1||intrinsic Josephson junction:1||MESOSCOPIC SPINVALVE:1||Bi2212 single crystals:1||intrinsic junctions:1||ANDREEV REFLECTIONS:1||normalmetal/superconductor interface:1||IBI2SR2CACU2OY:1||THERMAL FLUCTUATIONS:1||MIXED STATE:1||BI2.15SR1.85CACU2O8+DELTA:1||intrinsic Josephson effects:1||CACUO:1||QUANTUM POINT CONTACTS:1||resonant tunneling state:1||coherence length:1||NANOWIRE:1||GATES:1||Phase line:1||Thermal activation:1||QUANTUMDOT:1||superconducting proximity effect:1||Andreev interferometer:1||WIRE:1||Josephsonvortexflow branches:1||Bi2212 cuprates:1||LATTICE:1||demannetization effect:1||SUPERCONDUCTING MIRRORS:1||GAS:1||VALLEY TRANSPORT:1||ELECTRODES:1||DEPENDENT TRANSPORT:1||BORNOPPENHEIMER APPROXIMATION:1||collective plasma oscillations:1||fluxon resonance steps:1||STACKS:1||COLLECTIVE DYNAMICS:1||PAIRING SYMMETRY:1||MUON SPIN ROTATION:1||DIMENSIONAL CROSSOVER:1||Bi2Sr2CaCu2Oy highTc superconductors:1||heterojunctions:1||nanostructures:1||surfaces and interfaces:1||QUANTUM TRANSPORT:1||MICROJUNCTIONS:1||RESONATORS:1||STATES:1||FIELD:1||FLUCTUATIONS:1||SCATTERING:1||mode splitting of Josephson vortexflow branches:1||2D superconductivity:1||TRANSISTOR:1||ENERGYGAP:1||SUPERLATTICES:1||IRONBASED SUPERCONDUCTORS:1||PHASEDEPENDENT RESISTANCE:1||QUANTUM PHASETRANSITIONS:1||ELECTRICFIELD:1||HIGH MAGNETICFIELDS:1||NANOWIRE HETEROSTRUCTURES:1||ZNO:1||pair breaking.:1||SUPERCONDUCTING PB:1||domain formation:1||FORCE MICROSCOPY:1||RELAXATION:1||PLASMA RESONANCE:1||coupled Josephson junctions:1||COPPEROXIDE SUPERCONDUCTORS:1||CROSSOVER:1||SIMULATIONS:1||LOWTEMPERATURE:1||CONDUCTORS:1||METALINSULATORTRANSITION:1||SEMICONDUCTOR:1||FIELDEFFECT TRANSISTORS:1||ZEROVOLTAGE STATE:1||constanttemperature interlayer tunneling spectroscopy:1||Josephson supercurrent:1||BIPOLAR SUPERCURRENT:1||Interaction between Josephson and pancake vortices:1||flux jump:1||coaxial heterojunction nanorod:1||Natural Josephson coupling:1||BI2SR2CACU2O8+DELTA:1||VORTEX FLOW:1||TC SUPERCONDUCTORS:1||charge imbalance:1||Andreev diffractometer:1||intercalation:1||surface junction:1||Bi2212:1||tunnelling:1||GRAPHITE:1||GROWTH:1||collective transverse plasma modes:1||GAN:1||Macroscopic quantum tunneling:1||Fluctuation conductivity:1||Abovegap conductance jump:1||Josephson vortex motion:1||Intrinsic Josephson junctions:1||LAYERED SUPERCONDUCTORS:1||BI2SR2CACU2O8+Y:1||INTERFACES:1||BREAKDOWN:1||SYSTEMS:1||Anisotropy ratio:1||Josephson vortex:1||spin relaxation in superconductors:1||bibased single crystals:1||MESOSCOPIC PROXIMITY SUPERCONDUCTOR:1||reentrance of conductance:1||interlayer pair tunneling:1||JOSEPHSON:1||DISORDERED 2DIMENSIONAL SUPERCONDUCTORS:1||INDIUM FILMS:1||excited state:1||REGIME:1||triplet superconductivity:1||FILM:1||SCHOTTKY DIODES:1||peakdiphump structure:1||Kondo effect:1||REENTRANCE:1||Graphene:1||CONTACT:1||BERRYS PHASE:1||2DIMENSIONAL SUPERCONDUCTORS:1||Coulomb diamond:1||magnetic domain:1||spin injection:1||RESONANCE:1||plasma excitation modes:1||FLOW:1||OVERDOPED BI2SR2CACU2O8+DELTA:1||hole doping:1||chemical synthesis:1||phase transitions:1||superconductors:1||VORTEXGLASS SUPERCONDUCTIVITY:1||Kondorelated model:1||RADIATION:1||DOT:1||NANOBELTS:1||Complementarity:1||Closedloop AharonovBohm interferometer:1||pair breaking:1||interlayer phase fluctuation:1||MgB2 thin film:1||CONFINEMENT:1||WALLED CARBON NANOTUBES:1||TRANSITION:9||VORTICES:8||STATE:7||intrinsic Josephson junctions:7||SINGLECRYSTALS:7||JUNCTIONS:5||MODES:5||SUPERCURRENT:5||SUPERCONDUCTOR:5||CONDUCTANCE:5||HIGHTEMPERATURE SUPERCONDUCTORS:5||TRANSPORT:5||PHASE:5||FILMS:4||LOCALIZATION:4||SINGLE DIRAC CONE:4||WIRES:4||MAGNETICFIELD:4||STEPS:3||ELECTRONS:3||proximity effect:3||MODEL:3||ARRAYS:3||INTERFERENCE:3||fluxon dynamics:3||HETEROSTRUCTURES:3||INSULATOR:3||Andreev reflection:3||electronic transport:3||FISKE:3||superconductor:2||ZnO:2||quantum point contact:2||METAL:2||DYNAMICS:2||interlayer Josephson coupling:2||SUPERCONDUCTORS:2||YBA2CU3O7DELTA:2||LAYER:2||DOTS:2||quantum dot:2||Article:2||TRANSISTORS:2||CARBON NANOTUBES:2||GAP:2||MECHANISM:2||LINE:2||GIANT SHAPIRO STEPS:2||LAYERS:2||electron energy loss spectroscopy:2||physical phenomena:2||scanning electron microscopy:2||HGTE QUANTUMWELLS:2||BI2TE3:2||SPECTROSCOPY:2||PNJUNCTIONS:2||spinpolarized tunneling:2||INTRINSIC JOSEPHSONJUNCTIONS:2||FIELDS:2||positive magnetoresistance:2||dilute magnetic semiconductor:2||magnetic field:2||scanning transmission electron microscopy:2||QUANTUM OSCILLATIONS:2||TRANSPORTPROPERTIES:2||surface pair current:2||MAGNETORESISTANCE:2||NANORIBBONS:2||INSTABILITY:2||ANDREEV REFLECTION:2||microwave irradiation:2||vertical graphene josephson junction:2||BI2SE3:2||CONDUCTIVITY:2||highTc superconductors:2||DIMENSIONAL ELECTRONGAS:2||graphene:2||Topological insulators:2||Josephson coupling Fraunhofer interference pattern:2||FERROMAGNET:2||DEPENDENCE:2||DETECTOR:2||COHERENCE:2||INJECTION:2||GRAPHENE:1||JOSEPHSONJUNCTIONS:1||LAYERED SUPERCONDUCTOR:1||mode splitting:1||BEHAVIOR:1||spinpolarized transport:1||SUPERCONDUCTING TRANSITION:1||microwave response:1||PSEUDOGAP:1||phase coherence:1||TRANSITIONS:1||Long Josephson junction:1||Charge detection:1||collective resonance modes:1||plasma oscillation modes:1||Superconducting proximity effect:1||Iron pnictide superconductor:1||McMillanRowell oscillations:1||ferromagnetic microstructure:1||superradiant state:1||VOLTAGE:1||branch splitting:1||TENSOR:1||INTERCALATION:1||insitu fabrication:1||NDGAO3:1||DISORDERED METALS:1||GAUGE GLASS:1||LOWTEMPERATURE TRANSPORT:1||spontaneous spin polarization model:1||BIAS:1||emission of electromagnetic waves:1||YBA2CU3O7/PRBA2CU3O7 SUPERLATTICES:1||BOHM:1||SHAPIRO STEPS:1||superconductor/ferromagnet interface:1||OXIDE:1||ANDREEVREFLECTION:1||SinFeAsO single crystal:1||COLLECTIVE MOTION:1||ANGULARDEPENDENCE:1||SUPERCONDUCTIVITY:1||BILAYER GRAPHENE:1||PHOTOLUMINESCENT PROPERTIES:1||SUPERCONDUCTING WEAK LINKS:1||intrinsic Josephson junctions geometrical resonance:1||intrinsic Josephson junction:1||MESOSCOPIC SPINVALVE:1||Bi2212 single crystals:1||intrinsic junctions:1||ANDREEV REFLECTIONS:1||normalmetal/superconductor interface:1||IBI2SR2CACU2OY:1||THERMAL FLUCTUATIONS:1||MIXED STATE:1||BI2.15SR1.85CACU2O8+DELTA:1||intrinsic Josephson effects:1||CACUO:1||QUANTUM POINT CONTACTS:1||resonant tunneling state:1||coherence length:1||NANOWIRE:1||GATES:1||Phase line:1||Thermal activation:1||QUANTUMDOT:1||superconducting proximity effect:1||Andreev interferometer:1||WIRE:1||Josephsonvortexflow branches:1||Bi2212 cuprates:1||LATTICE:1||demannetization effect:1||SUPERCONDUCTING MIRRORS:1||GAS:1||VALLEY TRANSPORT:1||ELECTRODES:1||DEPENDENT TRANSPORT:1||BORNOPPENHEIMER APPROXIMATION:1||collective plasma oscillations:1||fluxon resonance steps:1||STACKS:1||COLLECTIVE DYNAMICS:1||PAIRING SYMMETRY:1||MUON SPIN ROTATION:1||DIMENSIONAL CROSSOVER:1||Bi2Sr2CaCu2Oy highTc superconductors:1||heterojunctions:1||nanostructures:1||surfaces and interfaces:1||QUANTUM TRANSPORT:1||MICROJUNCTIONS:1||RESONATORS:1||STATES:1||FIELD:1||FLUCTUATIONS:1||SCATTERING:1||mode splitting of Josephson vortexflow branches:1||2D superconductivity:1||TRANSISTOR:1||ENERGYGAP:1||SUPERLATTICES:1||IRONBASED SUPERCONDUCTORS:1||PHASEDEPENDENT RESISTANCE:1||QUANTUM PHASETRANSITIONS:1||ELECTRICFIELD:1||HIGH MAGNETICFIELDS:1||NANOWIRE HETEROSTRUCTURES:1||ZNO:1||pair breaking.:1||SUPERCONDUCTING PB:1||domain formation:1||FORCE MICROSCOPY:1||RELAXATION:1||PLASMA RESONANCE:1||coupled Josephson junctions:1||COPPEROXIDE SUPERCONDUCTORS:1||CROSSOVER:1||SIMULATIONS:1||LOWTEMPERATURE:1||CONDUCTORS:1||METALINSULATORTRANSITION:1||SEMICONDUCTOR:1||FIELDEFFECT TRANSISTORS:1||ZEROVOLTAGE STATE:1||constanttemperature interlayer tunneling spectroscopy:1||Josephson supercurrent:1||BIPOLAR SUPERCURRENT:1||Interaction between Josephson and pancake vortices:1||flux jump:1||coaxial heterojunction nanorod:1||Natural Josephson coupling:1||BI2SR2CACU2O8+DELTA:1||VORTEX FLOW:1||TC SUPERCONDUCTORS:1||charge imbalance:1||Andreev diffractometer:1||intercalation:1||surface junction:1||Bi2212:1||tunnelling:1||GRAPHITE:1||GROWTH:1||collective transverse plasma modes:1||GAN:1||Macroscopic quantum tunneling:1||Fluctuation conductivity:1||Abovegap conductance jump:1||Josephson vortex motion:1||Intrinsic Josephson junctions:1||LAYERED SUPERCONDUCTORS:1||BI2SR2CACU2O8+Y:1||INTERFACES:1||BREAKDOWN:1||SYSTEMS:1||Anisotropy ratio:1||Josephson vortex:1||spin relaxation in superconductors:1||bibased single crystals:1||MESOSCOPIC PROXIMITY SUPERCONDUCTOR:1||reentrance of conductance:1||interlayer pair tunneling:1||JOSEPHSON:1||DISORDERED 2DIMENSIONAL SUPERCONDUCTORS:1||INDIUM FILMS:1||excited state:1||REGIME:1||triplet superconductivity:1||FILM:1||SCHOTTKY DIODES:1||peakdiphump structure:1||Kondo effect:1||REENTRANCE:1||Graphene:1||CONTACT:1||BERRYS PHASE:1||2DIMENSIONAL SUPERCONDUCTORS:1||Coulomb diamond:1||magnetic domain:1||spin injection:1||RESONANCE:1||plasma excitation modes:1||FLOW:1||OVERDOPED BI2SR2CACU2O8+DELTA:1||hole doping:1||chemical synthesis:1||phase transitions:1||superconductors:1||VORTEXGLASS SUPERCONDUCTIVITY:1||Kondorelated model:1||RADIATION:1||DOT:1||NANOBELTS:1||Complementarity:1||Closedloop AharonovBohm interferometer:1||pair breaking:1||interlayer phase fluctuation:1||MgB2 thin film:1||CONFINEMENT:1||WALLED CARBON NANOTUBES:1||TRANSITION:9||VORTICES:8||STATE:7||intrinsic Josephson junctions:7||SINGLECRYSTALS:7||JUNCTIONS:5||MODES:5||SUPERCURRENT:5||SUPERCONDUCTOR:5||CONDUCTANCE:5||HIGHTEMPERATURE SUPERCONDUCTORS:5||TRANSPORT:5||PHASE:5||FILMS:4||LOCALIZATION:4||SINGLE DIRAC CONE:4||WIRES:4||MAGNETICFIELD:4||STEPS:3||ELECTRONS:3||proximity effect:3||MODEL:3||ARRAYS:3||INTERFERENCE:3||fluxon dynamics:3||HETEROSTRUCTURES:3||INSULATOR:3||Andreev reflection:3||electronic transport:3||FISKE:3||superconductor:2||ZnO:2||quantum point contact:2||METAL:2||DYNAMICS:2||interlayer Josephson coupling:2||SUPERCONDUCTORS:2||YBA2CU3O7DELTA:2||LAYER:2||DOTS:2||quantum dot:2||Article:2||TRANSISTORS:2||CARBON NANOTUBES:2||GAP:2||MECHANISM:2||LINE:2||GIANT SHAPIRO STEPS:2||LAYERS:2||electron energy loss spectroscopy:2||physical phenomena:2||scanning electron microscopy:2||HGTE QUANTUMWELLS:2||BI2TE3:2||SPECTROSCOPY:2||PNJUNCTIONS:2||spinpolarized tunneling:2||INTRINSIC JOSEPHSONJUNCTIONS:2||FIELDS:2||positive magnetoresistance:2||dilute magnetic semiconductor:2||magnetic field:2||scanning transmission electron microscopy:2||QUANTUM OSCILLATIONS:2||TRANSPORTPROPERTIES:2||surface pair current:2||MAGNETORESISTANCE:2||NANORIBBONS:2||INSTABILITY:2||ANDREEV REFLECTION:2||microwave irradiation:2||vertical graphene josephson junction:2||BI2SE3:2||CONDUCTIVITY:2||highTc superconductors:2||DIMENSIONAL ELECTRONGAS:2||graphene:2||Topological insulators:2||Josephson coupling Fraunhofer interference pattern:2||FERROMAGNET:2||DEPENDENCE:2||DETECTOR:2||COHERENCE:2||INJECTION:2||GRAPHENE:1||JOSEPHSONJUNCTIONS:1||LAYERED SUPERCONDUCTOR:1||mode splitting:1||BEHAVIOR:1||spinpolarized transport:1||SUPERCONDUCTING TRANSITION:1||microwave response:1||PSEUDOGAP:1||phase coherence:1||TRANSITIONS:1||Long Josephson junction:1||Charge detection:1||collective resonance modes:1||plasma oscillation modes:1||Superconducting proximity effect:1||Iron pnictide superconductor:1||McMillanRowell oscillations:1||ferromagnetic microstructure:1||superradiant state:1||VOLTAGE:1||branch splitting:1||TENSOR:1||INTERCALATION:1||insitu fabrication:1||NDGAO3:1||DISORDERED METALS:1||GAUGE GLASS:1||LOWTEMPERATURE TRANSPORT:1||spontaneous spin polarization model:1||BIAS:1||emission of electromagnetic waves:1||YBA2CU3O7/PRBA2CU3O7 SUPERLATTICES:1||BOHM:1||SHAPIRO STEPS:1||superconductor/ferromagnet interface:1||OXIDE:1||ANDREEVREFLECTION:1||SinFeAsO single crystal:1||COLLECTIVE MOTION:1||ANGULARDEPENDENCE:1||SUPERCONDUCTIVITY:1||BILAYER GRAPHENE:1||PHOTOLUMINESCENT PROPERTIES:1||SUPERCONDUCTING WEAK LINKS:1||intrinsic Josephson junctions geometrical resonance:1||intrinsic Josephson junction:1||MESOSCOPIC SPINVALVE:1||Bi2212 single crystals:1||intrinsic junctions:1||ANDREEV REFLECTIONS:1||normalmetal/superconductor interface:1||IBI2SR2CACU2OY:1||THERMAL FLUCTUATIONS:1||MIXED STATE:1||BI2.15SR1.85CACU2O8+DELTA:1||intrinsic Josephson effects:1||CACUO:1||QUANTUM POINT CONTACTS:1||resonant tunneling state:1||coherence length:1||NANOWIRE:1||GATES:1||Phase line:1||Thermal activation:1||QUANTUMDOT:1||superconducting proximity effect:1||Andreev interferometer:1||WIRE:1||Josephsonvortexflow branches:1||Bi2212 cuprates:1||LATTICE:1||demannetization effect:1||SUPERCONDUCTING MIRRORS:1||GAS:1||VALLEY TRANSPORT:1||ELECTRODES:1||DEPENDENT TRANSPORT:1||BORNOPPENHEIMER APPROXIMATION:1||collective plasma oscillations:1||fluxon resonance steps:1||STACKS:1||COLLECTIVE DYNAMICS:1||PAIRING SYMMETRY:1||MUON SPIN ROTATION:1||DIMENSIONAL CROSSOVER:1||Bi2Sr2CaCu2Oy highTc superconductors:1||heterojunctions:1||nanostructures:1||surfaces and interfaces:1||QUANTUM TRANSPORT:1||MICROJUNCTIONS:1||RESONATORS:1||STATES:1||FIELD:1||FLUCTUATIONS:1||SCATTERING:1||mode splitting of Josephson vortexflow branches:1||2D superconductivity:1||TRANSISTOR:1||ENERGYGAP:1||SUPERLATTICES:1||IRONBASED SUPERCONDUCTORS:1||PHASEDEPENDENT RESISTANCE:1||QUANTUM PHASETRANSITIONS:1||ELECTRICFIELD:1||HIGH MAGNETICFIELDS:1||NANOWIRE HETEROSTRUCTURES:1||ZNO:1||pair breaking.:1||SUPERCONDUCTING PB:1||domain formation:1||FORCE MICROSCOPY:1||RELAXATION:1||PLASMA RESONANCE:1||coupled Josephson junctions:1||COPPEROXIDE SUPERCONDUCTORS:1||CROSSOVER:1||SIMULATIONS:1||LOWTEMPERATURE:1||CONDUCTORS:1||METALINSULATORTRANSITION:1||SEMICONDUCTOR:1||FIELDEFFECT TRANSISTORS:1||ZEROVOLTAGE STATE:1||constanttemperature interlayer tunneling spectroscopy:1||Josephson supercurrent:1||BIPOLAR SUPERCURRENT:1||Interaction between Josephson and pancake vortices:1||flux jump:1||coaxial heterojunction nanorod:1||Natural Josephson coupling:1||BI2SR2CACU2O8+DELTA:1||VORTEX FLOW:1||TC SUPERCONDUCTORS:1||charge imbalance:1||Andreev diffractometer:1||intercalation:1||surface junction:1||Bi2212:1||tunnelling:1||GRAPHITE:1||GROWTH:1||collective transverse plasma modes:1||GAN:1||Macroscopic quantum tunneling:1||Fluctuation conductivity:1||Abovegap conductance jump:1||Josephson vortex motion:1||Intrinsic Josephson junctions:1||LAYERED SUPERCONDUCTORS:1||BI2SR2CACU2O8+Y:1||INTERFACES:1||BREAKDOWN:1||SYSTEMS:1||Anisotropy ratio:1||Josephson vortex:1||spin relaxation in superconductors:1||bibased single crystals:1||MESOSCOPIC PROXIMITY SUPERCONDUCTOR:1||reentrance of conductance:1||interlayer pair tunneling:1||JOSEPHSON:1||DISORDERED 2DIMENSIONAL SUPERCONDUCTORS:1||INDIUM FILMS:1||excited state:1||REGIME:1||triplet superconductivity:1||FILM:1||SCHOTTKY DIODES:1||peakdiphump structure:1||Kondo effect:1||REENTRANCE:1||Graphene:1||CONTACT:1||BERRYS PHASE:1||2DIMENSIONAL SUPERCONDUCTORS:1||Coulomb diamond:1||magnetic domain:1||spin injection:1||RESONANCE:1||plasma excitation modes:1||FLOW:1||OVERDOPED BI2SR2CACU2O8+DELTA:1||hole doping:1||chemical synthesis:1||phase transitions:1||superconductors:1||VORTEXGLASS SUPERCONDUCTIVITY:1||Kondorelated model:1||RADIATION:1||DOT:1||NANOBELTS:1||Complementarity:1||Closedloop AharonovBohm interferometer:1||pair breaking:1||interlayer phase fluctuation:1||MgB2 thin film:1||CONFINEMENT:1||WALLED CARBON NANOTUBES:1||TRANSITION:9||VORTICES:8||STATE:7||intrinsic Josephson junctions:7||SINGLECRYSTALS:7||JUNCTIONS:5||MODES:5||SUPERCURRENT:5||SUPERCONDUCTOR:5||CONDUCTANCE:5||HIGHTEMPERATURE SUPERCONDUCTORS:5||TRANSPORT:5||PHASE:5||FILMS:4||LOCALIZATION:4||SINGLE DIRAC CONE:4||WIRES:4||MAGNETICFIELD:4||STEPS:3||ELECTRONS:3||proximity effect:3||MODEL:3||ARRAYS:3||INTERFERENCE:3||fluxon dynamics:3||HETEROSTRUCTURES:3||INSULATOR:3||Andreev reflection:3||electronic transport:3||FISKE:3||superconductor:2||ZnO:2||quantum point contact:2||METAL:2||DYNAMICS:2||interlayer Josephson coupling:2||SUPERCONDUCTORS:2||YBA2CU3O7DELTA:2||LAYER:2||DOTS:2||quantum dot:2||Article:2||TRANSISTORS:2||CARBON NANOTUBES:2||GAP:2||MECHANISM:2||LINE:2||GIANT SHAPIRO STEPS:2||LAYERS:2||electron energy loss spectroscopy:2||physical phenomena:2||scanning electron microscopy:2||HGTE QUANTUMWELLS:2||BI2TE3:2||SPECTROSCOPY:2||PNJUNCTIONS:2||spinpolarized tunneling:2||INTRINSIC JOSEPHSONJUNCTIONS:2||FIELDS:2||positive magnetoresistance:2||dilute magnetic semiconductor:2||magnetic field:2||scanning transmission electron microscopy:2||QUANTUM OSCILLATIONS:2||TRANSPORTPROPERTIES:2||surface pair current:2||MAGNETORESISTANCE:2||NANORIBBONS:2||INSTABILITY:2||ANDREEV REFLECTION:2||microwave irradiation:2||vertical graphene josephson junction:2||BI2SE3:2||CONDUCTIVITY:2||highTc superconductors:2||DIMENSIONAL ELECTRONGAS:2||graphene:2||Topological insulators:2||Josephson coupling Fraunhofer interference pattern:2||FERROMAGNET:2||DEPENDENCE:2||DETECTOR:2||COHERENCE:2||INJECTION:2||GRAPHENE:1||JOSEPHSONJUNCTIONS:1||LAYERED SUPERCONDUCTOR:1||mode splitting:1||BEHAVIOR:1||spinpolarized transport:1||SUPERCONDUCTING TRANSITION:1||microwave response:1||PSEUDOGAP:1||phase coherence:1||TRANSITIONS:1||Long Josephson junction:1||Charge detection:1||collective resonance modes:1||plasma oscillation modes:1||Superconducting proximity effect:1||Iron pnictide superconductor:1||McMillanRowell oscillations:1||ferromagnetic microstructure:1||superradiant state:1||VOLTAGE:1||branch splitting:1||TENSOR:1||INTERCALATION:1||insitu fabrication:1||NDGAO3:1||DISORDERED METALS:1||GAUGE GLASS:1||LOWTEMPERATURE TRANSPORT:1||spontaneous spin polarization model:1||BIAS:1||emission of electromagnetic waves:1||YBA2CU3O7/PRBA2CU3O7 SUPERLATTICES:1||BOHM:1||SHAPIRO STEPS:1||superconductor/ferromagnet interface:1||OXIDE:1||ANDREEVREFLECTION:1||SinFeAsO single crystal:1||COLLECTIVE MOTION:1||ANGULARDEPENDENCE:1||SUPERCONDUCTIVITY:1||BILAYER GRAPHENE:1||PHOTOLUMINESCENT PROPERTIES:1||SUPERCONDUCTING WEAK LINKS:1||intrinsic Josephson junctions geometrical resonance:1||intrinsic Josephson junction:1||MESOSCOPIC SPINVALVE:1||Bi2212 single crystals:1||intrinsic junctions:1||ANDREEV REFLECTIONS:1||normalmetal/superconductor interface:1||IBI2SR2CACU2OY:1||THERMAL FLUCTUATIONS:1||MIXED STATE:1||BI2.15SR1.85CACU2O8+DELTA:1||intrinsic Josephson effects:1||CACUO:1||QUANTUM POINT CONTACTS:1||resonant tunneling state:1||coherence length:1||NANOWIRE:1||GATES:1||Phase line:1||Thermal activation:1||QUANTUMDOT:1||superconducting proximity effect:1||Andreev interferometer:1||WIRE:1||Josephsonvortexflow branches:1||Bi2212 cuprates:1||LATTICE:1||demannetization effect:1||SUPERCONDUCTING MIRRORS:1||GAS:1||VALLEY TRANSPORT:1||ELECTRODES:1||DEPENDENT TRANSPORT:1||BORNOPPENHEIMER APPROXIMATION:1||collective plasma oscillations:1||fluxon resonance steps:1||STACKS:1||COLLECTIVE DYNAMICS:1||PAIRING SYMMETRY:1||MUON SPIN ROTATION:1||DIMENSIONAL CROSSOVER:1||Bi2Sr2CaCu2Oy highTc superconductors:1||heterojunctions:1||nanostructures:1||surfaces and interfaces:1||QUANTUM TRANSPORT:1||MICROJUNCTIONS:1||RESONATORS:1||STATES:1||FIELD:1||FLUCTUATIONS:1||SCATTERING:1||mode splitting of Josephson vortexflow branches:1||2D superconductivity:1||TRANSISTOR:1||ENERGYGAP:1||SUPERLATTICES:1||IRONBASED SUPERCONDUCTORS:1||PHASEDEPENDENT RESISTANCE:1||QUANTUM PHASETRANSITIONS:1||ELECTRICFIELD:1||HIGH MAGNETICFIELDS:1||NANOWIRE HETEROSTRUCTURES:1||ZNO:1||pair breaking.:1||SUPERCONDUCTING PB:1||domain formation:1||FORCE MICROSCOPY:1||RELAXATION:1||PLASMA RESONANCE:1||coupled Josephson junctions:1||COPPEROXIDE SUPERCONDUCTORS:1||CROSSOVER:1||SIMULATIONS:1||LOWTEMPERATURE:1||CONDUCTORS:1||METALINSULATORTRANSITION:1||SEMICONDUCTOR:1||FIELDEFFECT TRANSISTORS:1||ZEROVOLTAGE STATE:1||constanttemperature interlayer tunneling spectroscopy:1||Josephson supercurrent:1||BIPOLAR SUPERCURRENT:1||Interaction between Josephson and pancake vortices:1||flux jump:1||coaxial heterojunction nanorod:1||Natural Josephson coupling:1||BI2SR2CACU2O8+DELTA:1||VORTEX FLOW:1||TC SUPERCONDUCTORS:1||charge imbalance:1||Andreev diffractometer:1||intercalation:1||surface junction:1||Bi2212:1||tunnelling:1||GRAPHITE:1||GROWTH:1||collective transverse plasma modes:1||GAN:1||Macroscopic quantum tunneling:1||Fluctuation conductivity:1||Abovegap conductance jump:1||Josephson vortex motion:1||Intrinsic Josephson junctions:1||LAYERED SUPERCONDUCTORS:1||BI2SR2CACU2O8+Y:1||INTERFACES:1||BREAKDOWN:1||SYSTEMS:1||Anisotropy ratio:1||Josephson vortex:1||spin relaxation in superconductors:1||bibased single crystals:1||MESOSCOPIC PROXIMITY SUPERCONDUCTOR:1||reentrance of conductance:1||interlayer pair tunneling:1||JOSEPHSON:1||DISORDERED 2DIMENSIONAL SUPERCONDUCTORS:1||INDIUM FILMS:1||excited state:1||REGIME:1||triplet superconductivity:1||FILM:1||SCHOTTKY DIODES:1||peakdiphump structure:1||Kondo effect:1||REENTRANCE:1||Graphene:1||CONTACT:1||BERRYS PHASE:1||2DIMENSIONAL SUPERCONDUCTORS:1||Coulomb diamond:1||magnetic domain:1||spin injection:1||RESONANCE:1||plasma excitation modes:1||FLOW:1||OVERDOPED BI2SR2CACU2O8+DELTA:1||hole doping:1||chemical synthesis:1||phase transitions:1||superconductors:1||VORTEXGLASS SUPERCONDUCTIVITY:1||Kondorelated model:1||RADIATION:1||DOT:1||NANOBELTS:1||Complementarity:1||Closedloop AharonovBohm interferometer:1||pair breaking:1||interlayer phase fluctuation:1||MgB2 thin film:1||CONFINEMENT:1||WALLED CARBON NANOTUBES:1||TRANSITION:9||VORTICES:8||STATE:7||intrinsic Josephson junctions:7||SINGLECRYSTALS:7||JUNCTIONS:5||MODES:5||SUPERCURRENT:5||SUPERCONDUCTOR:5||CONDUCTANCE:5||HIGHTEMPERATURE SUPERCONDUCTORS:5||TRANSPORT:5||PHASE:5||FILMS:4||LOCALIZATION:4||SINGLE DIRAC CONE:4||WIRES:4||MAGNETICFIELD:4||STEPS:3||ELECTRONS:3||proximity effect:3||MODEL:3||ARRAYS:3||INTERFERENCE:3||fluxon dynamics:3||HETEROSTRUCTURES:3||INSULATOR:3||Andreev reflection:3||electronic transport:3||FISKE:3||superconductor:2||ZnO:2||quantum point contact:2||METAL:2||DYNAMICS:2||interlayer Josephson coupling:2||SUPERCONDUCTORS:2||YBA2CU3O7DELTA:2||LAYER:2||DOTS:2||quantum dot:2||Article:2||TRANSISTORS:2||CARBON NANOTUBES:2||GAP:2||MECHANISM:2||LINE:2||GIANT SHAPIRO STEPS:2||LAYERS:2||electron energy loss spectroscopy:2||physical phenomena:2||scanning electron microscopy:2||HGTE QUANTUMWELLS:2||BI2TE3:2||SPECTROSCOPY:2||PNJUNCTIONS:2||spinpolarized tunneling:2||INTRINSIC JOSEPHSONJUNCTIONS:2||FIELDS:2||positive magnetoresistance:2||dilute magnetic semiconductor:2||magnetic field:2||scanning transmission electron microscopy:2||QUANTUM OSCILLATIONS:2||TRANSPORTPROPERTIES:2||surface pair current:2||MAGNETORESISTANCE:2||NANORIBBONS:2||INSTABILITY:2||ANDREEV REFLECTION:2||microwave irradiation:2||vertical graphene josephson junction:2||BI2SE3:2||CONDUCTIVITY:2||highTc superconductors:2||DIMENSIONAL ELECTRONGAS:2||graphene:2||Topological insulators:2||Josephson coupling Fraunhofer interference pattern:2||FERROMAGNET:2||DEPENDENCE:2||DETECTOR:2||COHERENCE:2||INJECTION:2||GRAPHENE:1||JOSEPHSONJUNCTIONS:1||LAYERED SUPERCONDUCTOR:1||mode splitting:1||BEHAVIOR:1||spinpolarized transport:1||SUPERCONDUCTING TRANSITION:1||microwave response:1||PSEUDOGAP:1||phase coherence:1||TRANSITIONS:1||Long Josephson junction:1||Charge detection:1||collective resonance modes:1||plasma oscillation modes:1||Superconducting proximity effect:1||Iron pnictide superconductor:1||McMillanRowell oscillations:1||ferromagnetic microstructure:1||superradiant state:1||VOLTAGE:1||branch splitting:1||TENSOR:1||INTERCALATION:1||insitu fabrication:1||NDGAO3:1||DISORDERED METALS:1||GAUGE GLASS:1||LOWTEMPERATURE TRANSPORT:1||spontaneous spin polarization model:1||BIAS:1||emission of electromagnetic waves:1||YBA2CU3O7/PRBA2CU3O7 SUPERLATTICES:1||BOHM:1||SHAPIRO STEPS:1||superconductor/ferromagnet interface:1||OXIDE:1||ANDREEVREFLECTION:1||SinFeAsO single crystal:1||COLLECTIVE MOTION:1||ANGULARDEPENDENCE:1||SUPERCONDUCTIVITY:1||BILAYER GRAPHENE:1||PHOTOLUMINESCENT PROPERTIES:1||SUPERCONDUCTING WEAK LINKS:1||intrinsic Josephson junctions geometrical resonance:1||intrinsic Josephson junction:1||MESOSCOPIC SPINVALVE:1||Bi2212 single crystals:1||intrinsic junctions:1||ANDREEV REFLECTIONS:1||normalmetal/superconductor interface:1||IBI2SR2CACU2OY:1||THERMAL FLUCTUATIONS:1||MIXED STATE:1||BI2.15SR1.85CACU2O8+DELTA:1||intrinsic Josephson effects:1||CACUO:1||QUANTUM POINT CONTACTS:1||resonant tunneling state:1||coherence length:1||NANOWIRE:1||GATES:1||Phase line:1||Thermal activation:1||QUANTUMDOT:1||superconducting proximity effect:1||Andreev interferometer:1||WIRE:1||Josephsonvortexflow branches:1||Bi2212 cuprates:1||LATTICE:1||demannetization effect:1||SUPERCONDUCTING MIRRORS:1||GAS:1||VALLEY TRANSPORT:1||ELECTRODES:1||DEPENDENT TRANSPORT:1||BORNOPPENHEIMER APPROXIMATION:1||collective plasma oscillations:1||fluxon resonance steps:1||STACKS:1||COLLECTIVE DYNAMICS:1||PAIRING SYMMETRY:1||MUON SPIN ROTATION:1||DIMENSIONAL CROSSOVER:1||Bi2Sr2CaCu2Oy highTc superconductors:1||heterojunctions:1||nanostructures:1||surfaces and interfaces:1||QUANTUM TRANSPORT:1||MICROJUNCTIONS:1||RESONATORS:1||STATES:1||FIELD:1||FLUCTUATIONS:1||SCATTERING:1||mode splitting of Josephson vortexflow branches:1||2D superconductivity:1||TRANSISTOR:1||ENERGYGAP:1||SUPERLATTICES:1||IRONBASED SUPERCONDUCTORS:1||PHASEDEPENDENT RESISTANCE:1||QUANTUM PHASETRANSITIONS:1||ELECTRICFIELD:1||HIGH MAGNETICFIELDS:1||NANOWIRE HETEROSTRUCTURES:1||ZNO:1||pair breaking.:1||SUPERCONDUCTING PB:1||domain formation:1||FORCE MICROSCOPY:1||RELAXATION:1||PLASMA RESONANCE:1||coupled Josephson junctions:1||COPPEROXIDE SUPERCONDUCTORS:1||CROSSOVER:1||SIMULATIONS:1||LOWTEMPERATURE:1||CONDUCTORS:1||METALINSULATORTRANSITION:1||SEMICONDUCTOR:1||FIELDEFFECT TRANSISTORS:1||ZEROVOLTAGE STATE:1||constanttemperature interlayer tunneling spectroscopy:1||Josephson supercurrent:1||BIPOLAR SUPERCURRENT:1||Interaction between Josephson and pancake vortices:1||flux jump:1||coaxial heterojunction nanorod:1||Natural Josephson coupling:1||BI2SR2CACU2O8+DELTA:1||VORTEX FLOW:1||TC SUPERCONDUCTORS:1||charge imbalance:1||Andreev diffractometer:1||intercalation:1||surface junction:1||Bi2212:1||tunnelling:1||GRAPHITE:1||GROWTH:1||collective transverse plasma modes:1||GAN:1||Macroscopic quantum tunneling:1||Fluctuation conductivity:1||Abovegap conductance jump:1||Josephson vortex motion:1||Intrinsic Josephson junctions:1||LAYERED SUPERCONDUCTORS:1||BI2SR2CACU2O8+Y:1||INTERFACES:1||BREAKDOWN:1||SYSTEMS:1||Anisotropy ratio:1||Josephson vortex:1||spin relaxation in superconductors:1||bibased single crystals:1||MESOSCOPIC PROXIMITY SUPERCONDUCTOR:1||reentrance of conductance:1||interlayer pair tunneling:1||JOSEPHSON:1||DISORDERED 2DIMENSIONAL SUPERCONDUCTORS:1||INDIUM FILMS:1||excited state:1||REGIME:1||triplet superconductivity:1||FILM:1||SCHOTTKY DIODES:1||peakdiphump structure:1||Kondo effect:1||REENTRANCE:1||Graphene:1||CONTACT:1||BERRYS PHASE:1||2DIMENSIONAL SUPERCONDUCTORS:1||Coulomb diamond:1||magnetic domain:1||spin injection:1||RESONANCE:1||plasma excitation modes:1||FLOW:1||OVERDOPED BI2SR2CACU2O8+DELTA:1||hole doping:1||chemical synthesis:1||phase transitions:1||superconductors:1||VORTEXGLASS SUPERCONDUCTIVITY:1||Kondorelated model:1||RADIATION:1||DOT:1||NANOBELTS:1||Complementarity:1||Closedloop AharonovBohm interferometer:1||pair breaking:1||interlayer phase fluctuation:1||MgB2 thin film:1||CONFINEMENT:1||WALLED CARBON NANOTUBES:1||TRANSITION:9||VORTICES:8||STATE:7||intrinsic Josephson junctions:7||SINGLECRYSTALS:7||JUNCTIONS:5||MODES:5||SUPERCURRENT:5||SUPERCONDUCTOR:5||CONDUCTANCE:5||HIGHTEMPERATURE SUPERCONDUCTORS:5||TRANSPORT:5||PHASE:5||FILMS:4||LOCALIZATION:4||SINGLE DIRAC CONE:4||WIRES:4||MAGNETICFIELD:4||STEPS:3||ELECTRONS:3||proximity effect:3||MODEL:3||ARRAYS:3||INTERFERENCE:3||fluxon dynamics:3||HETEROSTRUCTURES:3||INSULATOR:3||Andreev reflection:3||electronic transport:3||FISKE:3||superconductor:2||ZnO:2||quantum point contact:2||METAL:2||DYNAMICS:2||interlayer Josephson coupling:2||SUPERCONDUCTORS:2||YBA2CU3O7DELTA:2||LAYER:2||DOTS:2||quantum dot:2||Article:2||TRANSISTORS:2||CARBON NANOTUBES:2||GAP:2||MECHANISM:2||LINE:2||GIANT SHAPIRO STEPS:2||LAYERS:2||electron energy loss spectroscopy:2||physical phenomena:2||scanning electron microscopy:2||HGTE QUANTUMWELLS:2||BI2TE3:2||SPECTROSCOPY:2||PNJUNCTIONS:2||spinpolarized tunneling:2||INTRINSIC JOSEPHSONJUNCTIONS:2||FIELDS:2||positive magnetoresistance:2||dilute magnetic semiconductor:2||magnetic field:2||scanning transmission electron microscopy:2||QUANTUM OSCILLATIONS:2||TRANSPORTPROPERTIES:2||surface pair current:2||MAGNETORESISTANCE:2||NANORIBBONS:2||INSTABILITY:2||ANDREEV REFLECTION:2||microwave irradiation:2||vertical graphene josephson junction:2||BI2SE3:2||CONDUCTIVITY:2||highTc superconductors:2||DIMENSIONAL ELECTRONGAS:2||graphene:2||Topological insulators:2||Josephson coupling Fraunhofer interference pattern:2||FERROMAGNET:2||DEPENDENCE:2||DETECTOR:2||COHERENCE:2||INJECTION:2||GRAPHENE:1||JOSEPHSONJUNCTIONS:1||LAYERED SUPERCONDUCTOR:1||mode splitting:1||BEHAVIOR:1||spinpolarized transport:1||SUPERCONDUCTING TRANSITION:1||microwave response:1||PSEUDOGAP:1||phase coherence:1||TRANSITIONS:1||Long Josephson junction:1||Charge detection:1||collective resonance modes:1||plasma oscillation modes:1||Superconducting proximity effect:1||Iron pnictide superconductor:1||McMillanRowell oscillations:1||ferromagnetic microstructure:1||superradiant state:1||VOLTAGE:1||branch splitting:1||TENSOR:1||INTERCALATION:1||insitu fabrication:1||NDGAO3:1||DISORDERED METALS:1||GAUGE GLASS:1||LOWTEMPERATURE TRANSPORT:1||spontaneous spin polarization model:1||BIAS:1||emission of electromagnetic waves:1||YBA2CU3O7/PRBA2CU3O7 SUPERLATTICES:1||BOHM:1||SHAPIRO STEPS:1||superconductor/ferromagnet interface:1||OXIDE:1||ANDREEVREFLECTION:1||SinFeAsO single crystal:1||COLLECTIVE MOTION:1||ANGULARDEPENDENCE:1||SUPERCONDUCTIVITY:1||BILAYER GRAPHENE:1||PHOTOLUMINESCENT PROPERTIES:1||SUPERCONDUCTING WEAK LINKS:1||intrinsic Josephson junctions geometrical resonance:1||intrinsic Josephson junction:1||MESOSCOPIC SPINVALVE:1||Bi2212 single crystals:1||intrinsic junctions:1||ANDREEV REFLECTIONS:1||normalmetal/superconductor interface:1||IBI2SR2CACU2OY:1||THERMAL FLUCTUATIONS:1||MIXED STATE:1||BI2.15SR1.85CACU2O8+DELTA:1||intrinsic Josephson effects:1||CACUO:1||QUANTUM POINT CONTACTS:1||resonant tunneling state:1||coherence length:1||NANOWIRE:1||GATES:1||Phase line:1||Thermal activation:1||QUANTUMDOT:1||superconducting proximity effect:1||Andreev interferometer:1||WIRE:1||Josephsonvortexflow branches:1||Bi2212 cuprates:1||LATTICE:1||demannetization effect:1||SUPERCONDUCTING MIRRORS:1||GAS:1||VALLEY TRANSPORT:1||ELECTRODES:1||DEPENDENT TRANSPORT:1||BORNOPPENHEIMER APPROXIMATION:1||collective plasma oscillations:1||fluxon resonance steps:1||STACKS:1||COLLECTIVE DYNAMICS:1||PAIRING SYMMETRY:1||MUON SPIN ROTATION:1||DIMENSIONAL CROSSOVER:1||Bi2Sr2CaCu2Oy highTc superconductors:1||heterojunctions:1||nanostructures:1||surfaces and interfaces:1||QUANTUM TRANSPORT:1||MICROJUNCTIONS:1||RESONATORS:1||STATES:1||FIELD:1||FLUCTUATIONS:1||SCATTERING:1||mode splitting of Josephson vortexflow branches:1||2D superconductivity:1||TRANSISTOR:1||ENERGYGAP:1||SUPERLATTICES:1||IRONBASED SUPERCONDUCTORS:1||PHASEDEPENDENT RESISTANCE:1||QUANTUM PHASETRANSITIONS:1||ELECTRICFIELD:1||HIGH MAGNETICFIELDS:1||NANOWIRE HETEROSTRUCTURES:1||ZNO:1||pair breaking.:1||SUPERCONDUCTING PB:1||domain formation:1||FORCE MICROSCOPY:1||RELAXATION:1||PLASMA RESONANCE:1||coupled Josephson junctions:1||COPPEROXIDE SUPERCONDUCTORS:1||CROSSOVER:1||SIMULATIONS:1||LOWTEMPERATURE:1||CONDUCTORS:1||METALINSULATORTRANSITION:1||SEMICONDUCTOR:1||FIELDEFFECT TRANSISTORS:1||ZEROVOLTAGE STATE:1||constanttemperature interlayer tunneling spectroscopy:1||Josephson supercurrent:1||BIPOLAR SUPERCURRENT:1||Interaction between Josephson and pancake vortices:1||flux jump:1||coaxial heterojunction nanorod:1||Natural Josephson coupling:1||BI2SR2CACU2O8+DELTA:1||VORTEX FLOW:1||TC SUPERCONDUCTORS:1||charge imbalance:1||Andreev diffractometer:1||intercalation:1||surface junction:1||Bi2212:1||tunnelling:1||GRAPHITE:1||GROWTH:1||collective transverse plasma modes:1||GAN:1||Macroscopic quantum tunneling:1||Fluctuation conductivity:1||Abovegap conductance jump:1||Josephson vortex motion:1||Intrinsic Josephson junctions:1||LAYERED SUPERCONDUCTORS:1||BI2SR2CACU2O8+Y:1||INTERFACES:1||BREAKDOWN:1||SYSTEMS:1||Anisotropy ratio:1||Josephson vortex:1||spin relaxation in superconductors:1||bibased single crystals:1||MESOSCOPIC PROXIMITY SUPERCONDUCTOR:1||reentrance of conductance:1||interlayer pair tunneling:1||JOSEPHSON:1||DISORDERED 2DIMENSIONAL SUPERCONDUCTORS:1||INDIUM FILMS:1||excited state:1||REGIME:1||triplet superconductivity:1||FILM:1||SCHOTTKY DIODES:1||peakdiphump structure:1||Kondo effect:1||REENTRANCE:1||Graphene:1||CONTACT:1||BERRYS PHASE:1||2DIMENSIONAL SUPERCONDUCTORS:1||Coulomb diamond:1||magnetic domain:1||spin injection:1||RESONANCE:1||plasma excitation modes:1||FLOW:1||OVERDOPED BI2SR2CACU2O8+DELTA:1||hole doping:1||chemical synthesis:1||phase transitions:1||superconductors:1||VORTEXGLASS SUPERCONDUCTIVITY:1||Kondorelated model:1||RADIATION:1||DOT:1||NANOBELTS:1||Complementarity:1||Closedloop AharonovBohm interferometer:1||pair breaking:1||interlayer phase fluctuation:1||MgB2 thin film:1||CONFINEMENT:1||WALLED CARBON NANOTUBES:1||TRANSITION:9||VORTICES:8||STATE:7||intrinsic Josephson junctions:7||SINGLECRYSTALS:7||JUNCTIONS:5||MODES:5||SUPERCURRENT:5||SUPERCONDUCTOR:5||CONDUCTANCE:5||HIGHTEMPERATURE SUPERCONDUCTORS:5||TRANSPORT:5||PHASE:5||FILMS:4||LOCALIZATION:4||SINGLE DIRAC CONE:4||WIRES:4||MAGNETICFIELD:4||STEPS:3||ELECTRONS:3||proximity effect:3||MODEL:3||ARRAYS:3||INTERFERENCE:3||fluxon dynamics:3||HETEROSTRUCTURES:3||INSULATOR:3||Andreev reflection:3||electronic transport:3||FISKE:3||superconductor:2||ZnO:2||quantum point contact:2||METAL:2||DYNAMICS:2||interlayer Josephson coupling:2||SUPERCONDUCTORS:2||YBA2CU3O7DELTA:2||LAYER:2||DOTS:2||quantum dot:2||Article:2||TRANSISTORS:2||CARBON NANOTUBES:2||GAP:2||MECHANISM:2||LINE:2||GIANT SHAPIRO STEPS:2||LAYERS:2||electron energy loss spectroscopy:2||physical phenomena:2||scanning electron microscopy:2||HGTE QUANTUMWELLS:2||BI2TE3:2||SPECTROSCOPY:2||PNJUNCTIONS:2||spinpolarized tunneling:2||INTRINSIC JOSEPHSONJUNCTIONS:2||FIELDS:2||positive magnetoresistance:2||dilute magnetic semiconductor:2||magnetic field:2||scanning transmission electron microscopy:2||QUANTUM OSCILLATIONS:2||TRANSPORTPROPERTIES:2||surface pair current:2||MAGNETORESISTANCE:2||NANORIBBONS:2||INSTABILITY:2||ANDREEV REFLECTION:2||microwave irradiation:2||vertical graphene josephson junction:2||BI2SE3:2||CONDUCTIVITY:2||highTc superconductors:2||DIMENSIONAL ELECTRONGAS:2||graphene:2||Topological insulators:2||Josephson coupling Fraunhofer interference pattern:2||FERROMAGNET:2||DEPENDENCE:2||DETECTOR:2||COHERENCE:2||INJECTION:2||GRAPHENE:1||JOSEPHSONJUNCTIONS:1||LAYERED SUPERCONDUCTOR:1||mode splitting:1||BEHAVIOR:1||spinpolarized transport:1||SUPERCONDUCTING TRANSITION:1||microwave response:1||PSEUDOGAP:1||phase coherence:1||TRANSITIONS:1||Long Josephson junction:1||Charge detection:1||collective resonance modes:1||plasma oscillation modes:1||Superconducting proximity effect:1||Iron pnictide superconductor:1||McMillanRowell oscillations:1||ferromagnetic microstructure:1||superradiant state:1||VOLTAGE:1||branch splitting:1||TENSOR:1||INTERCALATION:1||insitu fabrication:1||NDGAO3:1||DISORDERED METALS:1||GAUGE GLASS:1||LOWTEMPERATURE TRANSPORT:1||spontaneous spin polarization model:1||BIAS:1||emission of electromagnetic waves:1||YBA2CU3O7/PRBA2CU3O7 SUPERLATTICES:1||BOHM:1||SHAPIRO STEPS:1||superconductor/ferromagnet interface:1||OXIDE:1||ANDREEVREFLECTION:1||SinFeAsO single crystal:1||COLLECTIVE MOTION:1||ANGULARDEPENDENCE:1||SUPERCONDUCTIVITY:1||BILAYER GRAPHENE:1||PHOTOLUMINESCENT PROPERTIES:1||SUPERCONDUCTING WEAK LINKS:1||intrinsic Josephson junctions geometrical resonance:1||intrinsic Josephson junction:1||MESOSCOPIC SPINVALVE:1||Bi2212 single crystals:1||intrinsic junctions:1||ANDREEV REFLECTIONS:1||normalmetal/superconductor interface:1||IBI2SR2CACU2OY:1||THERMAL FLUCTUATIONS:1||MIXED STATE:1||BI2.15SR1.85CACU2O8+DELTA:1||intrinsic Josephson effects:1||CACUO:1||QUANTUM POINT CONTACTS:1||resonant tunneling state:1||coherence length:1||NANOWIRE:1||GATES:1||Phase line:1||Thermal activation:1||QUANTUMDOT:1||superconducting proximity effect:1||Andreev interferometer:1||WIRE:1||Josephsonvortexflow branches:1||Bi2212 cuprates:1||LATTICE:1||demannetization effect:1||SUPERCONDUCTING MIRRORS:1||GAS:1||VALLEY TRANSPORT:1||ELECTRODES:1||DEPENDENT TRANSPORT:1||BORNOPPENHEIMER APPROXIMATION:1||collective plasma oscillations:1||fluxon resonance steps:1||STACKS:1||COLLECTIVE DYNAMICS:1||PAIRING SYMMETRY:1||MUON SPIN ROTATION:1||DIMENSIONAL CROSSOVER:1||Bi2Sr2CaCu2Oy highTc superconductors:1||heterojunctions:1||nanostructures:1||surfaces and interfaces:1||QUANTUM TRANSPORT:1||MICROJUNCTIONS:1||RESONATORS:1||STATES:1||FIELD:1||FLUCTUATIONS:1||SCATTERING:1||mode splitting of Josephson vortexflow branches:1||2D superconductivity:1||TRANSISTOR:1||ENERGYGAP:1||SUPERLATTICES:1||IRONBASED SUPERCONDUCTORS:1||PHASEDEPENDENT RESISTANCE:1||QUANTUM PHASETRANSITIONS:1||ELECTRICFIELD:1||HIGH MAGNETICFIELDS:1||NANOWIRE HETEROSTRUCTURES:1||ZNO:1||pair breaking.:1||SUPERCONDUCTING PB:1||domain formation:1||FORCE MICROSCOPY:1||RELAXATION:1||PLASMA RESONANCE:1||coupled Josephson junctions:1||COPPEROXIDE SUPERCONDUCTORS:1||CROSSOVER:1||SIMULATIONS:1||LOWTEMPERATURE:1||CONDUCTORS:1||METALINSULATORTRANSITION:1||SEMICONDUCTOR:1||FIELDEFFECT TRANSISTORS:1||ZEROVOLTAGE STATE:1||constanttemperature interlayer tunneling spectroscopy:1||Josephson supercurrent:1||BIPOLAR SUPERCURRENT:1||Interaction between Josephson and pancake vortices:1||flux jump:1||coaxial heterojunction nanorod:1||Natural Josephson coupling:1||BI2SR2CACU2O8+DELTA:1||VORTEX FLOW:1||TC SUPERCONDUCTORS:1||charge imbalance:1||Andreev diffractometer:1||intercalation:1||surface junction:1||Bi2212:1||tunnelling:1||GRAPHITE:1||GROWTH:1||collective transverse plasma modes:1||GAN:1||Macroscopic quantum tunneling:1||Fluctuation conductivity:1||Abovegap conductance jump:1||Josephson vortex motion:1||Intrinsic Josephson junctions:1||LAYERED SUPERCONDUCTORS:1||BI2SR2CACU2O8+Y:1||INTERFACES:1||BREAKDOWN:1||SYSTEMS:1||Anisotropy ratio:1||Josephson vortex:1||spin relaxation in superconductors:1||bibased single crystals:1||MESOSCOPIC PROXIMITY SUPERCONDUCTOR:1||reentrance of conductance:1||interlayer pair tunneling:1||JOSEPHSON:1||DISORDERED 2DIMENSIONAL SUPERCONDUCTORS:1||INDIUM FILMS:1||excited state:1||REGIME:1||triplet superconductivity:1||FILM:1||SCHOTTKY DIODES:1||peakdiphump structure:1||Kondo effect:1||REENTRANCE:1||Graphene:1||CONTACT:1||BERRYS PHASE:1||2DIMENSIONAL SUPERCONDUCTORS:1||Coulomb diamond:1||magnetic domain:1||spin injection:1||RESONANCE:1||plasma excitation modes:1||FLOW:1||OVERDOPED BI2SR2CACU2O8+DELTA:1||hole doping:1||chemical synthesis:1||phase transitions:1||superconductors:1||VORTEXGLASS SUPERCONDUCTIVITY:1||Kondorelated model:1||RADIATION:1||DOT:1||NANOBELTS:1||Complementarity:1||Closedloop AharonovBohm interferometer:1||pair breaking:1||interlayer phase fluctuation:1||MgB2 thin film:1||CONFINEMENT:1||WALLED CARBON NANOTUBES:1||TRANSITION:9||VORTICES:8||STATE:7||intrinsic Josephson junctions:7||SINGLECRYSTALS:7||JUNCTIONS:5||MODES:5||SUPERCURRENT:5||SUPERCONDUCTOR:5||CONDUCTANCE:5||HIGHTEMPERATURE SUPERCONDUCTORS:5||TRANSPORT:5||PHASE:5||FILMS:4||LOCALIZATION:4||SINGLE DIRAC CONE:4||WIRES:4||MAGNETICFIELD:4||STEPS:3||ELECTRONS:3||proximity effect:3||MODEL:3||ARRAYS:3||INTERFERENCE:3||fluxon dynamics:3||HETEROSTRUCTURES:3||INSULATOR:3||Andreev reflection:3||electronic transport:3||FISKE:3||superconductor:2||ZnO:2||quantum point contact:2||METAL:2||DYNAMICS:2||interlayer Josephson coupling:2||SUPERCONDUCTORS:2||YBA2CU3O7DELTA:2||LAYER:2||DOTS:2||quantum dot:2||Article:2||TRANSISTORS:2||CARBON NANOTUBES:2||GAP:2||MECHANISM:2||LINE:2||GIANT SHAPIRO STEPS:2||LAYERS:2||electron energy loss spectroscopy:2||physical phenomena:2||scanning electron microscopy:2||HGTE QUANTUMWELLS:2||BI2TE3:2||SPECTROSCOPY:2||PNJUNCTIONS:2||spinpolarized tunneling:2||INTRINSIC JOSEPHSONJUNCTIONS:2||FIELDS:2||positive magnetoresistance:2||dilute magnetic semiconductor:2||magnetic field:2||scanning transmission electron microscopy:2||QUANTUM OSCILLATIONS:2||TRANSPORTPROPERTIES:2||surface pair current:2||MAGNETORESISTANCE:2||NANORIBBONS:2||INSTABILITY:2||ANDREEV REFLECTION:2||microwave irradiation:2||vertical graphene josephson junction:2||BI2SE3:2||CONDUCTIVITY:2||highTc superconductors:2||DIMENSIONAL ELECTRONGAS:2||graphene:2||Topological insulators:2||Josephson coupling Fraunhofer interference pattern:2||FERROMAGNET:2||DEPENDENCE:2||DETECTOR:2||COHERENCE:2||INJECTION:2||GRAPHENE:1||JOSEPHSONJUNCTIONS:1||LAYERED SUPERCONDUCTOR:1||mode splitting:1||BEHAVIOR:1||spinpolarized transport:1||SUPERCONDUCTING TRANSITION:1||microwave response:1||PSEUDOGAP:1||phase coherence:1||TRANSITIONS:1||Long Josephson junction:1||Charge detection:1||collective resonance modes:1||plasma oscillation modes:1||Superconducting proximity effect:1||Iron pnictide superconductor:1||McMillanRowell oscillations:1||ferromagnetic microstructure:1||superradiant state:1||VOLTAGE:1||branch splitting:1||TENSOR:1||INTERCALATION:1||insitu fabrication:1||NDGAO3:1||DISORDERED METALS:1||GAUGE GLASS:1||LOWTEMPERATURE TRANSPORT:1||spontaneous spin polarization model:1||BIAS:1||emission of electromagnetic waves:1||YBA2CU3O7/PRBA2CU3O7 SUPERLATTICES:1||BOHM:1||SHAPIRO STEPS:1||superconductor/ferromagnet interface:1||OXIDE:1||ANDREEVREFLECTION:1||SinFeAsO single crystal:1||COLLECTIVE MOTION:1||ANGULARDEPENDENCE:1||SUPERCONDUCTIVITY:1||BILAYER GRAPHENE:1||PHOTOLUMINESCENT PROPERTIES:1||SUPERCONDUCTING WEAK LINKS:1||intrinsic Josephson junctions geometrical resonance:1||intrinsic Josephson junction:1||MESOSCOPIC SPINVALVE:1||Bi2212 single crystals:1||intrinsic junctions:1||ANDREEV REFLECTIONS:1||normalmetal/superconductor interface:1||IBI2SR2CACU2OY:1||THERMAL FLUCTUATIONS:1||MIXED STATE:1||BI2.15SR1.85CACU2O8+DELTA:1||intrinsic Josephson effects:1||CACUO:1||QUANTUM POINT CONTACTS:1||resonant tunneling state:1||coherence length:1||NANOWIRE:1||GATES:1||Phase line:1||Thermal activation:1||QUANTUMDOT:1||superconducting proximity effect:1||Andreev interferometer:1||WIRE:1||Josephsonvortexflow branches:1||Bi2212 cuprates:1||LATTICE:1||demannetization effect:1||SUPERCONDUCTING MIRRORS:1||GAS:1||VALLEY TRANSPORT:1||ELECTRODES:1||DEPENDENT TRANSPORT:1||BORNOPPENHEIMER APPROXIMATION:1||collective plasma oscillations:1||fluxon resonance steps:1||STACKS:1||COLLECTIVE DYNAMICS:1||PAIRING SYMMETRY:1||MUON SPIN ROTATION:1||DIMENSIONAL CROSSOVER:1||Bi2Sr2CaCu2Oy highTc superconductors:1||heterojunctions:1||nanostructures:1||surfaces and interfaces:1||QUANTUM TRANSPORT:1||MICROJUNCTIONS:1||RESONATORS:1||STATES:1||FIELD:1||FLUCTUATIONS:1||SCATTERING:1||mode splitting of Josephson vortexflow branches:1||2D superconductivity:1||TRANSISTOR:1||ENERGYGAP:1||SUPERLATTICES:1||IRONBASED SUPERCONDUCTORS:1||PHASEDEPENDENT RESISTANCE:1||QUANTUM PHASETRANSITIONS:1||ELECTRICFIELD:1||HIGH MAGNETICFIELDS:1||NANOWIRE HETEROSTRUCTURES:1||ZNO:1||pair breaking.:1||SUPERCONDUCTING PB:1||domain formation:1||FORCE MICROSCOPY:1||RELAXATION:1||PLASMA RESONANCE:1||coupled Josephson junctions:1||COPPEROXIDE SUPERCONDUCTORS:1||CROSSOVER:1||SIMULATIONS:1||LOWTEMPERATURE:1||CONDUCTORS:1||METALINSULATORTRANSITION:1||SEMICONDUCTOR:1||FIELDEFFECT TRANSISTORS:1||ZEROVOLTAGE STATE:1||constanttemperature interlayer tunneling spectroscopy:1||Josephson supercurrent:1||BIPOLAR SUPERCURRENT:1||Interaction between Josephson and pancake vortices:1||flux jump:1||coaxial heterojunction nanorod:1||Natural Josephson coupling:1||BI2SR2CACU2O8+DELTA:1||VORTEX FLOW:1||TC SUPERCONDUCTORS:1||charge imbalance:1||Andreev diffractometer:1||intercalation:1||surface junction:1||Bi2212:1||tunnelling:1||GRAPHITE:1||GROWTH:1||collective transverse plasma modes:1||GAN:1||Macroscopic quantum tunneling:1||Fluctuation conductivity:1||Abovegap conductance jump:1||Josephson vortex motion:1||Intrinsic Josephson junctions:1||LAYERED SUPERCONDUCTORS:1||BI2SR2CACU2O8+Y:1||INTERFACES:1||BREAKDOWN:1||SYSTEMS:1||Anisotropy ratio:1||Josephson vortex:1||spin relaxation in superconductors:1||bibased single crystals:1||MESOSCOPIC PROXIMITY SUPERCONDUCTOR:1||reentrance of conductance:1||interlayer pair tunneling:1||JOSEPHSON:1||DISORDERED 2DIMENSIONAL SUPERCONDUCTORS:1||INDIUM FILMS:1||excited state:1||REGIME:1||triplet superconductivity:1||FILM:1||SCHOTTKY DIODES:1||peakdiphump structure:1||Kondo effect:1||REENTRANCE:1||Graphene:1||CONTACT:1||BERRYS PHASE:1||2DIMENSIONAL SUPERCONDUCTORS:1||Coulomb diamond:1||magnetic domain:1||spin injection:1||RESONANCE:1||plasma excitation modes:1||FLOW:1||OVERDOPED BI2SR2CACU2O8+DELTA:1||hole doping:1||chemical synthesis:1||phase transitions:1||superconductors:1||VORTEXGLASS SUPERCONDUCTIVITY:1||Kondorelated model:1||RADIATION:1||DOT:1||NANOBELTS:1||Complementarity:1||Closedloop AharonovBohm interferometer:1||pair breaking:1||interlayer phase fluctuation:1||MgB2 thin film:1||CONFINEMENT:1||WALLED CARBON NANOTUBES:1||TRANSITION:9||VORTICES:8||STATE:7||intrinsic Josephson junctions:7||SINGLECRYSTALS:7||JUNCTIONS:5||MODES:5||SUPERCURRENT:5||SUPERCONDUCTOR:5||CONDUCTANCE:5||HIGHTEMPERATURE SUPERCONDUCTORS:5||TRANSPORT:5||PHASE:5||FILMS:4||LOCALIZATION:4||SINGLE DIRAC CONE:4||WIRES:4||MAGNETICFIELD:4||STEPS:3||ELECTRONS:3||proximity effect:3||MODEL:3||ARRAYS:3||INTERFERENCE:3||fluxon dynamics:3||HETEROSTRUCTURES:3||INSULATOR:3||Andreev reflection:3||electronic transport:3||FISKE:3||superconductor:2||ZnO:2||quantum point contact:2||METAL:2||DYNAMICS:2||interlayer Josephson coupling:2||SUPERCONDUCTORS:2||YBA2CU3O7DELTA:2||LAYER:2||DOTS:2||quantum dot:2||Article:2||TRANSISTORS:2||CARBON NANOTUBES:2||GAP:2||MECHANISM:2||LINE:2||GIANT SHAPIRO STEPS:2||LAYERS:2||electron energy loss spectroscopy:2||physical phenomena:2||scanning electron microscopy:2||HGTE QUANTUMWELLS:2||BI2TE3:2||SPECTROSCOPY:2||PNJUNCTIONS:2||spinpolarized tunneling:2||INTRINSIC JOSEPHSONJUNCTIONS:2||FIELDS:2||positive magnetoresistance:2||dilute magnetic semiconductor:2||magnetic field:2||scanning transmission electron microscopy:2||QUANTUM OSCILLATIONS:2||TRANSPORTPROPERTIES:2||surface pair current:2||MAGNETORESISTANCE:2||NANORIBBONS:2||INSTABILITY:2||ANDREEV REFLECTION:2||microwave irradiation:2||vertical graphene josephson junction:2||BI2SE3:2||CONDUCTIVITY:2||highTc superconductors:2||DIMENSIONAL ELECTRONGAS:2||graphene:2||Topological insulators:2||Josephson coupling Fraunhofer interference pattern:2||FERROMAGNET:2||DEPENDENCE:2||DETECTOR:2||COHERENCE:2||INJECTION:2||GRAPHENE:1||JOSEPHSONJUNCTIONS:1||LAYERED SUPERCONDUCTOR:1||mode splitting:1||BEHAVIOR:1||spinpolarized transport:1||SUPERCONDUCTING TRANSITION:1||microwave response:1||PSEUDOGAP:1||phase coherence:1||TRANSITIONS:1||Long Josephson junction:1||Charge detection:1||collective resonance modes:1||plasma oscillation modes:1||Superconducting proximity effect:1||Iron pnictide superconductor:1||McMillanRowell oscillations:1||ferromagnetic microstructure:1||superradiant state:1||VOLTAGE:1||branch splitting:1||TENSOR:1||INTERCALATION:1||insitu fabrication:1||NDGAO3:1||DISORDERED METALS:1||GAUGE GLASS:1||LOWTEMPERATURE TRANSPORT:1||spontaneous spin polarization model:1||BIAS:1||emission of electromagnetic waves:1||YBA2CU3O7/PRBA2CU3O7 SUPERLATTICES:1||BOHM:1||SHAPIRO STEPS:1||superconductor/ferromagnet interface:1||OXIDE:1||ANDREEVREFLECTION:1||SinFeAsO single crystal:1||COLLECTIVE MOTION:1||ANGULARDEPENDENCE:1||SUPERCONDUCTIVITY:1||BILAYER GRAPHENE:1||PHOTOLUMINESCENT PROPERTIES:1||SUPERCONDUCTING WEAK LINKS:1||intrinsic Josephson junctions geometrical resonance:1||intrinsic Josephson junction:1||MESOSCOPIC SPINVALVE:1||Bi2212 single crystals:1||intrinsic junctions:1||ANDREEV REFLECTIONS:1||normalmetal/superconductor interface:1||IBI2SR2CACU2OY:1||THERMAL FLUCTUATIONS:1||MIXED STATE:1||BI2.15SR1.85CACU2O8+DELTA:1||intrinsic Josephson effects:1||CACUO:1||QUANTUM POINT CONTACTS:1||resonant tunneling state:1||coherence length:1||NANOWIRE:1||GATES:1||Phase line:1||Thermal activation:1||QUANTUMDOT:1||superconducting proximity effect:1||Andreev interferometer:1||WIRE:1||Josephsonvortexflow branches:1||Bi2212 cuprates:1||LATTICE:1||demannetization effect:1||SUPERCONDUCTING MIRRORS:1||GAS:1||VALLEY TRANSPORT:1||ELECTRODES:1||DEPENDENT TRANSPORT:1||BORNOPPENHEIMER APPROXIMATION:1||collective plasma oscillations:1||fluxon resonance steps:1||STACKS:1||COLLECTIVE DYNAMICS:1||PAIRING SYMMETRY:1||MUON SPIN ROTATION:1||DIMENSIONAL CROSSOVER:1||Bi2Sr2CaCu2Oy highTc superconductors:1||heterojunctions:1||nanostructures:1||surfaces and interfaces:1||QUANTUM TRANSPORT:1||MICROJUNCTIONS:1||RESONATORS:1||STATES:1||FIELD:1||FLUCTUATIONS:1||SCATTERING:1||mode splitting of Josephson vortexflow branches:1||2D superconductivity:1||TRANSISTOR:1||ENERGYGAP:1||SUPERLATTICES:1||IRONBASED SUPERCONDUCTORS:1||PHASEDEPENDENT RESISTANCE:1||QUANTUM PHASETRANSITIONS:1||ELECTRICFIELD:1||HIGH MAGNETICFIELDS:1||NANOWIRE HETEROSTRUCTURES:1||ZNO:1||pair breaking.:1||SUPERCONDUCTING PB:1||domain formation:1||FORCE MICROSCOPY:1||RELAXATION:1||PLASMA RESONANCE:1||coupled Josephson junctions:1||COPPEROXIDE SUPERCONDUCTORS:1||CROSSOVER:1||SIMULATIONS:1||LOWTEMPERATURE:1||CONDUCTORS:1||METALINSULATORTRANSITION:1||SEMICONDUCTOR:1||FIELDEFFECT TRANSISTORS:1||ZEROVOLTAGE STATE:1||constanttemperature interlayer tunneling spectroscopy:1||Josephson supercurrent:1||BIPOLAR SUPERCURRENT:1||Interaction between Josephson and pancake vortices:1||flux jump:1||coaxial heterojunction nanorod:1||Natural Josephson coupling:1||BI2SR2CACU2O8+DELTA:1||VORTEX FLOW:1||TC SUPERCONDUCTORS:1||charge imbalance:1||Andreev diffractometer:1||intercalation:1||surface junction:1||Bi2212:1||tunnelling:1||GRAPHITE:1||GROWTH:1||collective transverse plasma modes:1||GAN:1||Macroscopic quantum tunneling:1||Fluctuation conductivity:1||Abovegap conductance jump:1||Josephson vortex motion:1||Intrinsic Josephson junctions:1||LAYERED SUPERCONDUCTORS:1||BI2SR2CACU2O8+Y:1||INTERFACES:1||BREAKDOWN:1||SYSTEMS:1||Anisotropy ratio:1||Josephson vortex:1||spin relaxation in superconductors:1||bibased single crystals:1||MESOSCOPIC PROXIMITY SUPERCONDUCTOR:1||reentrance of conductance:1||interlayer pair tunneling:1||JOSEPHSON:1||DISORDERED 2DIMENSIONAL SUPERCONDUCTORS:1||INDIUM FILMS:1||excited state:1||REGIME:1||triplet superconductivity:1||FILM:1||SCHOTTKY DIODES:1||peakdiphump structure:1||Kondo effect:1||REENTRANCE:1||Graphene:1||CONTACT:1||BERRYS PHASE:1||2DIMENSIONAL SUPERCONDUCTORS:1||Coulomb diamond:1||magnetic domain:1||spin injection:1||RESONANCE:1||plasma excitation modes:1||FLOW:1||OVERDOPED BI2SR2CACU2O8+DELTA:1||hole doping:1||chemical synthesis:1||phase transitions:1||superconductors:1||VORTEXGLASS SUPERCONDUCTIVITY:1||Kondorelated model:1||RADIATION:1||DOT:1||NANOBELTS:1||Complementarity:1||Closedloop AharonovBohm interferometer:1||pair breaking:1||interlayer phase fluctuation:1||MgB2 thin film:1||CONFINEMENT:1||WALLED CARBON NANOTUBES:1||TRANSITION:9||VORTICES:8||STATE:7||intrinsic Josephson junctions:7||SINGLECRYSTALS:7||JUNCTIONS:5||MODES:5||SUPERCURRENT:5||SUPERCONDUCTOR:5||CONDUCTANCE:5||HIGHTEMPERATURE SUPERCONDUCTORS:5||TRANSPORT:5||PHASE:5||FILMS:4||LOCALIZATION:4||SINGLE DIRAC CONE:4||WIRES:4||MAGNETICFIELD:4||STEPS:3||ELECTRONS:3||proximity effect:3||MODEL:3||ARRAYS:3||INTERFERENCE:3||fluxon dynamics:3||HETEROSTRUCTURES:3||INSULATOR:3||Andreev reflection:3||electronic transport:3||FISKE:3||superconductor:2||ZnO:2||quantum point contact:2||METAL:2||DYNAMICS:2||interlayer Josephson coupling:2||SUPERCONDUCTORS:2||YBA2CU3O7DELTA:2||LAYER:2||DOTS:2||quantum dot:2||Article:2||TRANSISTORS:2||CARBON NANOTUBES:2||GAP:2||MECHANISM:2||LINE:2||GIANT SHAPIRO STEPS:2||LAYERS:2||electron energy loss spectroscopy:2||physical phenomena:2||scanning electron microscopy:2||HGTE QUANTUMWELLS:2||BI2TE3:2||SPECTROSCOPY:2||PNJUNCTIONS:2||spinpolarized tunneling:2||INTRINSIC JOSEPHSONJUNCTIONS:2||FIELDS:2||positive magnetoresistance:2||dilute magnetic semiconductor:2||magnetic field:2||scanning transmission electron microscopy:2||QUANTUM OSCILLATIONS:2||TRANSPORTPROPERTIES:2||surface pair current:2||MAGNETORESISTANCE:2||NANORIBBONS:2||INSTABILITY:2||ANDREEV REFLECTION:2||microwave irradiation:2||vertical graphene josephson junction:2||BI2SE3:2||CONDUCTIVITY:2||highTc superconductors:2||DIMENSIONAL ELECTRONGAS:2||graphene:2||Topological insulators:2||Josephson coupling Fraunhofer interference pattern:2||FERROMAGNET:2||DEPENDENCE:2||DETECTOR:2||COHERENCE:2||INJECTION:2||GRAPHENE:1||JOSEPHSONJUNCTIONS:1||LAYERED SUPERCONDUCTOR:1||mode splitting:1||BEHAVIOR:1||spinpolarized transport:1||SUPERCONDUCTING TRANSITION:1||microwave response:1||PSEUDOGAP:1||phase coherence:1||TRANSITIONS:1||Long Josephson junction:1||Charge detection:1||collective resonance modes:1||plasma oscillation modes:1||Superconducting proximity effect:1||Iron pnictide superconductor:1||McMillanRowell oscillations:1||ferromagnetic microstructure:1||superradiant state:1||VOLTAGE:1||branch splitting:1||TENSOR:1||INTERCALATION:1||insitu fabrication:1||NDGAO3:1||DISORDERED METALS:1||GAUGE GLASS:1||LOWTEMPERATURE TRANSPORT:1||spontaneous spin polarization model:1||BIAS:1||emission of electromagnetic waves:1||YBA2CU3O7/PRBA2CU3O7 SUPERLATTICES:1||BOHM:1||SHAPIRO STEPS:1||superconductor/ferromagnet interface:1||OXIDE:1||ANDREEVREFLECTION:1||SinFeAsO single crystal:1||COLLECTIVE MOTION:1||ANGULARDEPENDENCE:1||SUPERCONDUCTIVITY:1||BILAYER GRAPHENE:1||PHOTOLUMINESCENT PROPERTIES:1||SUPERCONDUCTING WEAK LINKS:1||intrinsic Josephson junctions geometrical resonance:1||intrinsic Josephson junction:1||MESOSCOPIC SPINVALVE:1||Bi2212 single crystals:1||intrinsic junctions:1||ANDREEV REFLECTIONS:1||normalmetal/superconductor interface:1||IBI2SR2CACU2OY:1||THERMAL FLUCTUATIONS:1||MIXED STATE:1||BI2.15SR1.85CACU2O8+DELTA:1||intrinsic Josephson effects:1||CACUO:1||QUANTUM POINT CONTACTS:1||resonant tunneling state:1||coherence length:1||NANOWIRE:1||GATES:1||Phase line:1||Thermal activation:1||QUANTUMDOT:1||superconducting proximity effect:1||Andreev interferometer:1||WIRE:1||Josephsonvortexflow branches:1||Bi2212 cuprates:1||LATTICE:1||demannetization effect:1||SUPERCONDUCTING MIRRORS:1||GAS:1||VALLEY TRANSPORT:1||ELECTRODES:1||DEPENDENT TRANSPORT:1||BORNOPPENHEIMER APPROXIMATION:1||collective plasma oscillations:1||fluxon resonance steps:1||STACKS:1||COLLECTIVE DYNAMICS:1||PAIRING SYMMETRY:1||MUON SPIN ROTATION:1||DIMENSIONAL CROSSOVER:1||Bi2Sr2CaCu2Oy highTc superconductors:1||heterojunctions:1||nanostructures:1||surfaces and interfaces:1||QUANTUM TRANSPORT:1||MICROJUNCTIONS:1||RESONATORS:1||STATES:1||FIELD:1||FLUCTUATIONS:1||SCATTERING:1||mode splitting of Josephson vortexflow branches:1||2D superconductivity:1||TRANSISTOR:1||ENERGYGAP:1||SUPERLATTICES:1||IRONBASED SUPERCONDUCTORS:1||PHASEDEPENDENT RESISTANCE:1||QUANTUM PHASETRANSITIONS:1||ELECTRICFIELD:1||HIGH MAGNETICFIELDS:1||NANOWIRE HETEROSTRUCTURES:1||ZNO:1||pair breaking.:1||SUPERCONDUCTING PB:1||domain formation:1||FORCE MICROSCOPY:1||RELAXATION:1||PLASMA RESONANCE:1||coupled Josephson junctions:1||COPPEROXIDE SUPERCONDUCTORS:1||CROSSOVER:1||SIMULATIONS:1||LOWTEMPERATURE:1||CONDUCTORS:1||METALINSULATORTRANSITION:1||SEMICONDUCTOR:1||FIELDEFFECT TRANSISTORS:1||ZEROVOLTAGE STATE:1||constanttemperature interlayer tunneling spectroscopy:1||Josephson supercurrent:1||BIPOLAR SUPERCURRENT:1||Interaction between Josephson and pancake vortices:1||flux jump:1||coaxial heterojunction nanorod:1||Natural Josephson coupling:1||BI2SR2CACU2O8+DELTA:1||VORTEX FLOW:1||TC SUPERCONDUCTORS:1||charge imbalance:1||Andreev diffractometer:1||intercalation:1||surface junction:1||Bi2212:1||tunnelling:1||GRAPHITE:1||GROWTH:1||collective transverse plasma modes:1||GAN:1||Macroscopic quantum tunneling:1||Fluctuation conductivity:1||Abovegap conductance jump:1||Josephson vortex motion:1||Intrinsic Josephson junctions:1||LAYERED SUPERCONDUCTORS:1||BI2SR2CACU2O8+Y:1||INTERFACES:1||BREAKDOWN:1||SYSTEMS:1||Anisotropy ratio:1||Josephson vortex:1||spin relaxation in superconductors:1||bibased single crystals:1||MESOSCOPIC PROXIMITY SUPERCONDUCTOR:1||reentrance of conductance:1||interlayer pair tunneling:1||JOSEPHSON:1||DISORDERED 2DIMENSIONAL SUPERCONDUCTORS:1||INDIUM FILMS:1||excited state:1||REGIME:1||triplet superconductivity:1||FILM:1||SCHOTTKY DIODES:1||peakdiphump structure:1||Kondo effect:1||REENTRANCE:1||Graphene:1||CONTACT:1||BERRYS PHASE:1||2DIMENSIONAL SUPERCONDUCTORS:1||Coulomb diamond:1||magnetic domain:1||spin injection:1||RESONANCE:1||plasma excitation modes:1||FLOW:1||OVERDOPED BI2SR2CACU2O8+DELTA:1||hole doping:1||chemical synthesis:1||phase transitions:1||superconductors:1||VORTEXGLASS SUPERCONDUCTIVITY:1||Kondorelated model:1||RADIATION:1||DOT:1||NANOBELTS:1||Complementarity:1||Closedloop AharonovBohm interferometer:1||pair breaking:1||interlayer phase fluctuation:1||MgB2 thin film:1||CONFINEMENT:1||WALLED CARBON NANOTUBES:1||TRANSITION:9||VORTICES:8||STATE:7||intrinsic Josephson junctions:7||SINGLECRYSTALS:7||JUNCTIONS:5||MODES:5||SUPERCURRENT:5||SUPERCONDUCTOR:5||CONDUCTANCE:5||HIGHTEMPERATURE SUPERCONDUCTORS:5||TRANSPORT:5||PHASE:5||FILMS:4||LOCALIZATION:4||SINGLE DIRAC CONE:4||WIRES:4||MAGNETICFIELD:4||STEPS:3||ELECTRONS:3||proximity effect:3||MODEL:3||ARRAYS:3||INTERFERENCE:3||fluxon dynamics:3||HETEROSTRUCTURES:3||INSULATOR:3||Andreev reflection:3||electronic transport:3||FISKE:3||superconductor:2||ZnO:2||quantum point contact:2||METAL:2||DYNAMICS:2||interlayer Josephson coupling:2||SUPERCONDUCTORS:2||YBA2CU3O7DELTA:2||LAYER:2||DOTS:2||quantum dot:2||Article:2||TRANSISTORS:2||CARBON NANOTUBES:2||GAP:2||MECHANISM:2||LINE:2||GIANT SHAPIRO STEPS:2||LAYERS:2||electron energy loss spectroscopy:2||physical phenomena:2||scanning electron microscopy:2||HGTE QUANTUMWELLS:2||BI2TE3:2||SPECTROSCOPY:2||PNJUNCTIONS:2||spinpolarized tunneling:2||INTRINSIC JOSEPHSONJUNCTIONS:2||FIELDS:2||positive magnetoresistance:2||dilute magnetic semiconductor:2||magnetic field:2||scanning transmission electron microscopy:2||QUANTUM OSCILLATIONS:2||TRANSPORTPROPERTIES:2||surface pair current:2||MAGNETORESISTANCE:2||NANORIBBONS:2||INSTABILITY:2||ANDREEV REFLECTION:2||microwave irradiation:2||vertical graphene josephson junction:2||BI2SE3:2||CONDUCTIVITY:2||highTc superconductors:2||DIMENSIONAL ELECTRONGAS:2||graphene:2||Topological insulators:2||Josephson coupling Fraunhofer interference pattern:2||FERROMAGNET:2||DEPENDENCE:2||DETECTOR:2||COHERENCE:2||INJECTION:2||GRAPHENE:1||JOSEPHSONJUNCTIONS:1||LAYERED SUPERCONDUCTOR:1||mode splitting:1||BEHAVIOR:1||spinpolarized transport:1||SUPERCONDUCTING TRANSITION:1||microwave response:1||PSEUDOGAP:1||phase coherence:1||TRANSITIONS:1||Long Josephson junction:1||Charge detection:1||collective resonance modes:1||plasma oscillation modes:1||Superconducting proximity effect:1||Iron pnictide superconductor:1||McMillanRowell oscillations:1||ferromagnetic microstructure:1||superradiant state:1||VOLTAGE:1||branch splitting:1||TENSOR:1||INTERCALATION:1||insitu fabrication:1||NDGAO3:1||DISORDERED METALS:1||GAUGE GLASS:1||LOWTEMPERATURE TRANSPORT:1||spontaneous spin polarization model:1||BIAS:1||emission of electromagnetic waves:1||YBA2CU3O7/PRBA2CU3O7 SUPERLATTICES:1||BOHM:1||SHAPIRO STEPS:1||superconductor/ferromagnet interface:1||OXIDE:1||ANDREEVREFLECTION:1||SinFeAsO single crystal:1||COLLECTIVE MOTION:1||ANGULARDEPENDENCE:1||SUPERCONDUCTIVITY:1||BILAYER GRAPHENE:1||PHOTOLUMINESCENT PROPERTIES:1||SUPERCONDUCTING WEAK LINKS:1||intrinsic Josephson junctions geometrical resonance:1||intrinsic Josephson junction:1||MESOSCOPIC SPINVALVE:1||Bi2212 single crystals:1||intrinsic junctions:1||ANDREEV REFLECTIONS:1||normalmetal/superconductor interface:1||IBI2SR2CACU2OY:1||THERMAL FLUCTUATIONS:1||MIXED STATE:1||BI2.15SR1.85CACU2O8+DELTA:1||intrinsic Josephson effects:1||CACUO:1||QUANTUM POINT CONTACTS:1||resonant tunneling state:1||coherence length:1||NANOWIRE:1||GATES:1||Phase line:1||Thermal activation:1||QUANTUMDOT:1||superconducting proximity effect:1||Andreev interferometer:1||WIRE:1||Josephsonvortexflow branches:1||Bi2212 cuprates:1||LATTICE:1||demannetization effect:1||SUPERCONDUCTING MIRRORS:1||GAS:1||VALLEY TRANSPORT:1||ELECTRODES:1||DEPENDENT TRANSPORT:1||BORNOPPENHEIMER APPROXIMATION:1||collective plasma oscillations:1||fluxon resonance steps:1||STACKS:1||COLLECTIVE DYNAMICS:1||PAIRING SYMMETRY:1||MUON SPIN ROTATION:1||DIMENSIONAL CROSSOVER:1||Bi2Sr2CaCu2Oy highTc superconductors:1||heterojunctions:1||nanostructures:1||surfaces and interfaces:1||QUANTUM TRANSPORT:1||MICROJUNCTIONS:1||RESONATORS:1||STATES:1||FIELD:1||FLUCTUATIONS:1||SCATTERING:1||mode splitting of Josephson vortexflow branches:1||2D superconductivity:1||TRANSISTOR:1||ENERGYGAP:1||SUPERLATTICES:1||IRONBASED SUPERCONDUCTORS:1||PHASEDEPENDENT RESISTANCE:1||QUANTUM PHASETRANSITIONS:1||ELECTRICFIELD:1||HIGH MAGNETICFIELDS:1||NANOWIRE HETEROSTRUCTURES:1||ZNO:1||pair breaking.:1||SUPERCONDUCTING PB:1||domain formation:1||FORCE MICROSCOPY:1||RELAXATION:1||PLASMA RESONANCE:1||coupled Josephson junctions:1||COPPEROXIDE SUPERCONDUCTORS:1||CROSSOVER:1||SIMULATIONS:1||LOWTEMPERATURE:1||CONDUCTORS:1||METALINSULATORTRANSITION:1||SEMICONDUCTOR:1||FIELDEFFECT TRANSISTORS:1||ZEROVOLTAGE STATE:1||constanttemperature interlayer tunneling spectroscopy:1||Josephson supercurrent:1||BIPOLAR SUPERCURRENT:1||Interaction between Josephson and pancake vortices:1||flux jump:1||coaxial heterojunction nanorod:1||Natural Josephson coupling:1||BI2SR2CACU2O8+DELTA:1||VORTEX FLOW:1||TC SUPERCONDUCTORS:1||charge imbalance:1||Andreev diffractometer:1||intercalation:1||surface junction:1||Bi2212:1||tunnelling:1||GRAPHITE:1||GROWTH:1||collective transverse plasma modes:1||GAN:1||Macroscopic quantum tunneling:1||Fluctuation conductivity:1||Abovegap conductance jump:1||Josephson vortex motion:1||Intrinsic Josephson junctions:1||LAYERED SUPERCONDUCTORS:1||BI2SR2CACU2O8+Y:1||INTERFACES:1||BREAKDOWN:1||SYSTEMS:1||Anisotropy ratio:1||Josephson vortex:1||spin relaxation in superconductors:1||bibased single crystals:1||MESOSCOPIC PROXIMITY SUPERCONDUCTOR:1||reentrance of conductance:1||interlayer pair tunneling:1||JOSEPHSON:1||DISORDERED 2DIMENSIONAL SUPERCONDUCTORS:1||INDIUM FILMS:1||excited state:1||REGIME:1||triplet superconductivity:1||FILM:1||SCHOTTKY DIODES:1||peakdiphump structure:1||Kondo effect:1||REENTRANCE:1||Graphene:1||CONTACT:1||BERRYS PHASE:1||2DIMENSIONAL SUPERCONDUCTORS:1||Coulomb diamond:1||magnetic domain:1||spin injection:1||RESONANCE:1||plasma excitation modes:1||FLOW:1||OVERDOPED BI2SR2CACU2O8+DELTA:1||hole doping:1||chemical synthesis:1||phase transitions:1||superconductors:1||VORTEXGLASS SUPERCONDUCTIVITY:1||Kondorelated model:1||RADIATION:1||DOT:1||NANOBELTS:1||Complementarity:1||Closedloop AharonovBohm interferometer:1||pair breaking:1||interlayer phase fluctuation:1||MgB2 thin film:1||CONFINEMENT:1||WALLED CARBON NANOTUBES:1||TRANSITION:9||VORTICES:8||STATE:7||intrinsic Josephson junctions:7||SINGLECRYSTALS:7||JUNCTIONS:5||MODES:5||SUPERCURRENT:5||SUPERCONDUCTOR:5||CONDUCTANCE:5||HIGHTEMPERATURE SUPERCONDUCTORS:5||TRANSPORT:5||PHASE:5||FILMS:4||LOCALIZATION:4||SINGLE DIRAC CONE:4||WIRES:4||MAGNETICFIELD:4||STEPS:3||ELECTRONS:3||proximity effect:3||MODEL:3||ARRAYS:3||INTERFERENCE:3||fluxon dynamics:3||HETEROSTRUCTURES:3||INSULATOR:3||Andreev reflection:3||electronic transport:3||FISKE:3||superconductor:2||ZnO:2||quantum point contact:2||METAL:2||DYNAMICS:2||interlayer Josephson coupling:2||SUPERCONDUCTORS:2||YBA2CU3O7DELTA:2||LAYER:2||DOTS:2||quantum dot:2||Article:2||TRANSISTORS:2||CARBON NANOTUBES:2||GAP:2||MECHANISM:2||LINE:2||GIANT SHAPIRO STEPS:2||LAYERS:2||electron energy loss spectroscopy:2||physical phenomena:2||scanning electron microscopy:2||HGTE QUANTUMWELLS:2||BI2TE3:2||SPECTROSCOPY:2||PNJUNCTIONS:2||spinpolarized tunneling:2||INTRINSIC JOSEPHSONJUNCTIONS:2||FIELDS:2||positive magnetoresistance:2||dilute magnetic semiconductor:2||magnetic field:2||scanning transmission electron microscopy:2||QUANTUM OSCILLATIONS:2||TRANSPORTPROPERTIES:2||surface pair current:2||MAGNETORESISTANCE:2||NANORIBBONS:2||INSTABILITY:2||ANDREEV REFLECTION:2||microwave irradiation:2||vertical graphene josephson junction:2||BI2SE3:2||CONDUCTIVITY:2||highTc superconductors:2||DIMENSIONAL ELECTRONGAS:2||graphene:2||Topological insulators:2||Josephson coupling Fraunhofer interference pattern:2||FERROMAGNET:2||DEPENDENCE:2||DETECTOR:2||COHERENCE:2||INJECTION:2||GRAPHENE:1||JOSEPHSONJUNCTIONS:1||LAYERED SUPERCONDUCTOR:1||mode splitting:1||BEHAVIOR:1||spinpolarized transport:1||SUPERCONDUCTING TRANSITION:1||microwave response:1||PSEUDOGAP:1||phase coherence:1||TRANSITIONS:1||Long Josephson junction:1||Charge detection:1||collective resonance modes:1||plasma oscillation modes:1||Superconducting proximity effect:1||Iron pnictide superconductor:1||McMillanRowell oscillations:1||ferromagnetic microstructure:1||superradiant state:1||VOLTAGE:1||branch splitting:1||TENSOR:1||INTERCALATION:1||insitu fabrication:1||NDGAO3:1||DISORDERED METALS:1||GAUGE GLASS:1||LOWTEMPERATURE TRANSPORT:1||spontaneous spin polarization model:1||BIAS:1||emission of electromagnetic waves:1||YBA2CU3O7/PRBA2CU3O7 SUPERLATTICES:1||BOHM:1||SHAPIRO STEPS:1||superconductor/ferromagnet interface:1||OXIDE:1||ANDREEVREFLECTION:1||SinFeAsO single crystal:1||COLLECTIVE MOTION:1||ANGULARDEPENDENCE:1||SUPERCONDUCTIVITY:1||BILAYER GRAPHENE:1||PHOTOLUMINESCENT PROPERTIES:1||SUPERCONDUCTING WEAK LINKS:1||intrinsic Josephson junctions geometrical resonance:1||intrinsic Josephson junction:1||MESOSCOPIC SPINVALVE:1||Bi2212 single crystals:1||intrinsic junctions:1||ANDREEV REFLECTIONS:1||normalmetal/superconductor interface:1||IBI2SR2CACU2OY:1||THERMAL FLUCTUATIONS:1||MIXED STATE:1||BI2.15SR1.85CACU2O8+DELTA:1||intrinsic Josephson effects:1||CACUO:1||QUANTUM POINT CONTACTS:1||resonant tunneling state:1||coherence length:1||NANOWIRE:1||GATES:1||Phase line:1||Thermal activation:1||QUANTUMDOT:1||superconducting proximity effect:1||Andreev interferometer:1||WIRE:1||Josephsonvortexflow branches:1||Bi2212 cuprates:1||LATTICE:1||demannetization effect:1||SUPERCONDUCTING MIRRORS:1||GAS:1||VALLEY TRANSPORT:1||ELECTRODES:1||DEPENDENT TRANSPORT:1||BORNOPPENHEIMER APPROXIMATION:1||collective plasma oscillations:1||fluxon resonance steps:1||STACKS:1||COLLECTIVE DYNAMICS:1||PAIRING SYMMETRY:1||MUON SPIN ROTATION:1||DIMENSIONAL CROSSOVER:1||Bi2Sr2CaCu2Oy highTc superconductors:1||heterojunctions:1||nanostructures:1||surfaces and interfaces:1||QUANTUM TRANSPORT:1||MICROJUNCTIONS:1||RESONATORS:1||STATES:1||FIELD:1||FLUCTUATIONS:1||SCATTERING:1||mode splitting of Josephson vortexflow branches:1||2D superconductivity:1||TRANSISTOR:1||ENERGYGAP:1||SUPERLATTICES:1||IRONBASED SUPERCONDUCTORS:1||PHASEDEPENDENT RESISTANCE:1||QUANTUM PHASETRANSITIONS:1||ELECTRICFIELD:1||HIGH MAGNETICFIELDS:1||NANOWIRE HETEROSTRUCTURES:1||ZNO:1||pair breaking.:1||SUPERCONDUCTING PB:1||domain formation:1||FORCE MICROSCOPY:1||RELAXATION:1||PLASMA RESONANCE:1||coupled Josephson junctions:1||COPPEROXIDE SUPERCONDUCTORS:1||CROSSOVER:1||SIMULATIONS:1||LOWTEMPERATURE:1||CONDUCTORS:1||METALINSULATORTRANSITION:1||SEMICONDUCTOR:1||FIELDEFFECT TRANSISTORS:1||ZEROVOLTAGE STATE:1||constanttemperature interlayer tunneling spectroscopy:1||Josephson supercurrent:1||BIPOLAR SUPERCURRENT:1||Interaction between Josephson and pancake vortices:1||flux jump:1||coaxial heterojunction nanorod:1||Natural Josephson coupling:1||BI2SR2CACU2O8+DELTA:1||VORTEX FLOW:1||TC SUPERCONDUCTORS:1||charge imbalance:1||Andreev diffractometer:1||intercalation:1||surface junction:1||Bi2212:1||tunnelling:1||GRAPHITE:1||GROWTH:1||collective transverse plasma modes:1||GAN:1||Macroscopic quantum tunneling:1||Fluctuation conductivity:1||Abovegap conductance jump:1||Josephson vortex motion:1||Intrinsic Josephson junctions:1||LAYERED SUPERCONDUCTORS:1||BI2SR2CACU2O8+Y:1||INTERFACES:1||BREAKDOWN:1||SYSTEMS:1||Anisotropy ratio:1||Josephson vortex:1||spin relaxation in superconductors:1||bibased single crystals:1||MESOSCOPIC PROXIMITY SUPERCONDUCTOR:1||reentrance of conductance:1||interlayer pair tunneling:1||JOSEPHSON:1||DISORDERED 2DIMENSIONAL SUPERCONDUCTORS:1||INDIUM FILMS:1||excited state:1||REGIME:1||triplet superconductivity:1||FILM:1||SCHOTTKY DIODES:1||peakdiphump structure:1||Kondo effect:1||REENTRANCE:1||Graphene:1||CONTACT:1||BERRYS PHASE:1||2DIMENSIONAL SUPERCONDUCTORS:1||Coulomb diamond:1||magnetic domain:1||spin injection:1||RESONANCE:1||plasma excitation modes:1||FLOW:1||OVERDOPED BI2SR2CACU2O8+DELTA:1||hole doping:1||chemical synthesis:1||phase transitions:1||superconductors:1||VORTEXGLASS SUPERCONDUCTIVITY:1||Kondorelated model:1||RADIATION:1||DOT:1||NANOBELTS:1||Complementarity:1||Closedloop AharonovBohm interferometer:1||pair breaking:1||interlayer phase fluctuation:1||MgB2 thin film:1||CONFINEMENT:1||WALLED CARBON NANOTUBES:1||TRANSITION:9||VORTICES:8||STATE:7||intrinsic Josephson junctions:7||SINGLECRYSTALS:7||JUNCTIONS:5||MODES:5||SUPERCURRENT:5||SUPERCONDUCTOR:5||CONDUCTANCE:5||HIGHTEMPERATURE SUPERCONDUCTORS:5||TRANSPORT:5||PHASE:5||FILMS:4||LOCALIZATION:4||SINGLE DIRAC CONE:4||WIRES:4||MAGNETICFIELD:4||STEPS:3||ELECTRONS:3||proximity effect:3||MODEL:3||ARRAYS:3||INTERFERENCE:3||fluxon dynamics:3||HETEROSTRUCTURES:3||INSULATOR:3||Andreev reflection:3||electronic transport:3||FISKE:3||superconductor:2||ZnO:2||quantum point contact:2||METAL:2||DYNAMICS:2||interlayer Josephson coupling:2||SUPERCONDUCTORS:2||YBA2CU3O7DELTA:2||LAYER:2||DOTS:2||quantum dot:2||Article:2||TRANSISTORS:2||CARBON NANOTUBES:2||GAP:2||MECHANISM:2||LINE:2||GIANT SHAPIRO STEPS:2||LAYERS:2||electron energy loss spectroscopy:2||physical phenomena:2||scanning electron microscopy:2||HGTE QUANTUMWELLS:2||BI2TE3:2||SPECTROSCOPY:2||PNJUNCTIONS:2||spinpolarized tunneling:2||INTRINSIC JOSEPHSONJUNCTIONS:2||FIELDS:2||positive magnetoresistance:2||dilute magnetic semiconductor:2||magnetic field:2||scanning transmission electron microscopy:2||QUANTUM OSCILLATIONS:2||TRANSPORTPROPERTIES:2||surface pair current:2||MAGNETORESISTANCE:2||NANORIBBONS:2||INSTABILITY:2||ANDREEV REFLECTION:2||microwave irradiation:2||vertical graphene josephson junction:2||BI2SE3:2||CONDUCTIVITY:2||highTc superconductors:2||DIMENSIONAL ELECTRONGAS:2||graphene:2||Topological insulators:2||Josephson coupling Fraunhofer interference pattern:2||FERROMAGNET:2||DEPENDENCE:2||DETECTOR:2||COHERENCE:2||INJECTION:2||GRAPHENE:1||JOSEPHSONJUNCTIONS:1||LAYERED SUPERCONDUCTOR:1||mode splitting:1||BEHAVIOR:1||spinpolarized transport:1||SUPERCONDUCTING TRANSITION:1||microwave response:1||PSEUDOGAP:1||phase coherence:1||TRANSITIONS:1||Long Josephson junction:1||Charge detection:1||collective resonance modes:1||plasma oscillation modes:1||Superconducting proximity effect:1||Iron pnictide superconductor:1||McMillanRowell oscillations:1||ferromagnetic microstructure:1||superradiant state:1||VOLTAGE:1||branch splitting:1||TENSOR:1||INTERCALATION:1||insitu fabrication:1||NDGAO3:1||DISORDERED METALS:1||GAUGE GLASS:1||LOWTEMPERATURE TRANSPORT:1||spontaneous spin polarization model:1||BIAS:1||emission of electromagnetic waves:1||YBA2CU3O7/PRBA2CU3O7 SUPERLATTICES:1||BOHM:1||SHAPIRO STEPS:1||superconductor/ferromagnet interface:1||OXIDE:1||ANDREEVREFLECTION:1||SinFeAsO single crystal:1||COLLECTIVE MOTION:1||ANGULARDEPENDENCE:1||SUPERCONDUCTIVITY:1||BILAYER GRAPHENE:1||PHOTOLUMINESCENT PROPERTIES:1||SUPERCONDUCTING WEAK LINKS:1||intrinsic Josephson junctions geometrical resonance:1||intrinsic Josephson junction:1||MESOSCOPIC SPINVALVE:1||Bi2212 single crystals:1||intrinsic junctions:1||ANDREEV REFLECTIONS:1||normalmetal/superconductor interface:1||IBI2SR2CACU2OY:1||THERMAL FLUCTUATIONS:1||MIXED STATE:1||BI2.15SR1.85CACU2O8+DELTA:1||intrinsic Josephson effects:1||CACUO:1||QUANTUM POINT CONTACTS:1||resonant tunneling state:1||coherence length:1||NANOWIRE:1||GATES:1||Phase line:1||Thermal activation:1||QUANTUMDOT:1||superconducting proximity effect:1||Andreev interferometer:1||WIRE:1||Josephsonvortexflow branches:1||Bi2212 cuprates:1||LATTICE:1||demannetization effect:1||SUPERCONDUCTING MIRRORS:1||GAS:1||VALLEY TRANSPORT:1||ELECTRODES:1||DEPENDENT TRANSPORT:1||BORNOPPENHEIMER APPROXIMATION:1||collective plasma oscillations:1||fluxon resonance steps:1||STACKS:1||COLLECTIVE DYNAMICS:1||PAIRING SYMMETRY:1||MUON SPIN ROTATION:1||DIMENSIONAL CROSSOVER:1||Bi2Sr2CaCu2Oy highTc superconductors:1||heterojunctions:1||nanostructures:1||surfaces and interfaces:1||QUANTUM TRANSPORT:1||MICROJUNCTIONS:1||RESONATORS:1||STATES:1||FIELD:1||FLUCTUATIONS:1||SCATTERING:1||mode splitting of Josephson vortexflow branches:1||2D superconductivity:1||TRANSISTOR:1||ENERGYGAP:1||SUPERLATTICES:1||IRONBASED SUPERCONDUCTORS:1||PHASEDEPENDENT RESISTANCE:1||QUANTUM PHASETRANSITIONS:1||ELECTRICFIELD:1||HIGH MAGNETICFIELDS:1||NANOWIRE HETEROSTRUCTURES:1||ZNO:1||pair breaking.:1||SUPERCONDUCTING PB:1||domain formation:1||FORCE MICROSCOPY:1||RELAXATION:1||PLASMA RESONANCE:1||coupled Josephson junctions:1||COPPEROXIDE SUPERCONDUCTORS:1||CROSSOVER:1||SIMULATIONS:1||LOWTEMPERATURE:1||CONDUCTORS:1||METALINSULATORTRANSITION:1||SEMICONDUCTOR:1||FIELDEFFECT TRANSISTORS:1||ZEROVOLTAGE STATE:1||constanttemperature interlayer tunneling spectroscopy:1||Josephson supercurrent:1||BIPOLAR SUPERCURRENT:1||Interaction between Josephson and pancake vortices:1||flux jump:1||coaxial heterojunction nanorod:1||Natural Josephson coupling:1||BI2SR2CACU2O8+DELTA:1||VORTEX FLOW:1||TC SUPERCONDUCTORS:1||charge imbalance:1||Andreev diffractometer:1||intercalation:1||surface junction:1||Bi2212:1||tunnelling:1||GRAPHITE:1||GROWTH:1||collective transverse plasma modes:1||GAN:1||Macroscopic quantum tunneling:1||Fluctuation conductivity:1||Abovegap conductance jump:1||Josephson vortex motion:1||Intrinsic Josephson junctions:1||LAYERED SUPERCONDUCTORS:1||BI2SR2CACU2O8+Y:1||INTERFACES:1||BREAKDOWN:1||SYSTEMS:1||Anisotropy ratio:1||Josephson vortex:1||spin relaxation in superconductors:1||bibased single crystals:1||MESOSCOPIC PROXIMITY SUPERCONDUCTOR:1||reentrance of conductance:1||interlayer pair tunneling:1||JOSEPHSON:1||DISORDERED 2DIMENSIONAL SUPERCONDUCTORS:1||INDIUM FILMS:1||excited state:1||REGIME:1||triplet superconductivity:1||FILM:1||SCHOTTKY DIODES:1||peakdiphump structure:1||Kondo effect:1||REENTRANCE:1||Graphene:1||CONTACT:1||BERRYS PHASE:1||2DIMENSIONAL SUPERCONDUCTORS:1||Coulomb diamond:1||magnetic domain:1||spin injection:1||RESONANCE:1||plasma excitation modes:1||FLOW:1||OVERDOPED BI2SR2CACU2O8+DELTA:1||hole doping:1||chemical synthesis:1||phase transitions:1||superconductors:1||VORTEXGLASS SUPERCONDUCTIVITY:1||Kondorelated model:1||RADIATION:1||DOT:1||NANOBELTS:1||Complementarity:1||Closedloop AharonovBohm interferometer:1||pair breaking:1||interlayer phase fluctuation:1||MgB2 thin film:1||CONFINEMENT:1||WALLED CARBON NANOTUBES:1||TRANSITION:9||VORTICES:8||STATE:7||intrinsic Josephson junctions:7||SINGLECRYSTALS:7||JUNCTIONS:5||MODES:5||SUPERCURRENT:5||SUPERCONDUCTOR:5||CONDUCTANCE:5||HIGHTEMPERATURE SUPERCONDUCTORS:5||TRANSPORT:5||PHASE:5||FILMS:4||LOCALIZATION:4||SINGLE DIRAC CONE:4||WIRES:4||MAGNETICFIELD:4||STEPS:3||ELECTRONS:3||proximity effect:3||MODEL:3||ARRAYS:3||INTERFERENCE:3||fluxon dynamics:3||HETEROSTRUCTURES:3||INSULATOR:3||Andreev reflection:3||electronic transport:3||FISKE:3||superconductor:2||ZnO:2||quantum point contact:2||METAL:2||DYNAMICS:2||interlayer Josephson coupling:2||SUPERCONDUCTORS:2||YBA2CU3O7DELTA:2||LAYER:2||DOTS:2||quantum dot:2||Article:2||TRANSISTORS:2||CARBON NANOTUBES:2||GAP:2||MECHANISM:2||LINE:2||GIANT SHAPIRO STEPS:2||LAYERS:2||electron energy loss spectroscopy:2||physical phenomena:2||scanning electron microscopy:2||HGTE QUANTUMWELLS:2||BI2TE3:2||SPECTROSCOPY:2||PNJUNCTIONS:2||spinpolarized tunneling:2||INTRINSIC JOSEPHSONJUNCTIONS:2||FIELDS:2||positive magnetoresistance:2||dilute magnetic semiconductor:2||magnetic field:2||scanning transmission electron microscopy:2||QUANTUM OSCILLATIONS:2||TRANSPORTPROPERTIES:2||surface pair current:2||MAGNETORESISTANCE:2||NANORIBBONS:2||INSTABILITY:2||ANDREEV REFLECTION:2||microwave irradiation:2||vertical graphene josephson junction:2||BI2SE3:2||CONDUCTIVITY:2||highTc superconductors:2||DIMENSIONAL ELECTRONGAS:2||graphene:2||Topological insulators:2||Josephson coupling Fraunhofer interference pattern:2||FERROMAGNET:2||DEPENDENCE:2||DETECTOR:2||COHERENCE:2||INJECTION:2||GRAPHENE:1||JOSEPHSONJUNCTIONS:1||LAYERED SUPERCONDUCTOR:1||mode splitting:1||BEHAVIOR:1||spinpolarized transport:1||SUPERCONDUCTING TRANSITION:1||microwave response:1||PSEUDOGAP:1||phase coherence:1||TRANSITIONS:1||Long Josephson junction:1||Charge detection:1||collective resonance modes:1||plasma oscillation modes:1||Superconducting proximity effect:1||Iron pnictide superconductor:1||McMillanRowell oscillations:1||ferromagnetic microstructure:1||superradiant state:1||VOLTAGE:1||branch splitting:1||TENSOR:1||INTERCALATION:1||insitu fabrication:1||NDGAO3:1||DISORDERED METALS:1||GAUGE GLASS:1||LOWTEMPERATURE TRANSPORT:1||spontaneous spin polarization model:1||BIAS:1||emission of electromagnetic waves:1||YBA2CU3O7/PRBA2CU3O7 SUPERLATTICES:1||BOHM:1||SHAPIRO STEPS:1||superconductor/ferromagnet interface:1||OXIDE:1||ANDREEVREFLECTION:1||SinFeAsO single crystal:1||COLLECTIVE MOTION:1||ANGULARDEPENDENCE:1||SUPERCONDUCTIVITY:1||BILAYER GRAPHENE:1||PHOTOLUMINESCENT PROPERTIES:1||SUPERCONDUCTING WEAK LINKS:1||intrinsic Josephson junctions geometrical resonance:1||intrinsic Josephson junction:1||MESOSCOPIC SPINVALVE:1||Bi2212 single crystals:1||intrinsic junctions:1||ANDREEV REFLECTIONS:1||normalmetal/superconductor interface:1||IBI2SR2CACU2OY:1||THERMAL FLUCTUATIONS:1||MIXED STATE:1||BI2.15SR1.85CACU2O8+DELTA:1||intrinsic Josephson effects:1||CACUO:1||QUANTUM POINT CONTACTS:1||resonant tunneling state:1||coherence length:1||NANOWIRE:1||GATES:1||Phase line:1||Thermal activation:1||QUANTUMDOT:1||superconducting proximity effect:1||Andreev interferometer:1||WIRE:1||Josephsonvortexflow branches:1||Bi2212 cuprates:1||LATTICE:1||demannetization effect:1||SUPERCONDUCTING MIRRORS:1||GAS:1||VALLEY TRANSPORT:1||ELECTRODES:1||DEPENDENT TRANSPORT:1||BORNOPPENHEIMER APPROXIMATION:1||collective plasma oscillations:1||fluxon resonance steps:1||STACKS:1||COLLECTIVE DYNAMICS:1||PAIRING SYMMETRY:1||MUON SPIN ROTATION:1||DIMENSIONAL CROSSOVER:1||Bi2Sr2CaCu2Oy highTc superconductors:1||heterojunctions:1||nanostructures:1||surfaces and interfaces:1||QUANTUM TRANSPORT:1||MICROJUNCTIONS:1||RESONATORS:1||STATES:1||FIELD:1||FLUCTUATIONS:1||SCATTERING:1||mode splitting of Josephson vortexflow branches:1||2D superconductivity:1||TRANSISTOR:1||ENERGYGAP:1||SUPERLATTICES:1||IRONBASED SUPERCONDUCTORS:1||PHASEDEPENDENT RESISTANCE:1||QUANTUM PHASETRANSITIONS:1||ELECTRICFIELD:1||HIGH MAGNETICFIELDS:1||NANOWIRE HETEROSTRUCTURES:1||ZNO:1||pair breaking.:1||SUPERCONDUCTING PB:1||domain formation:1||FORCE MICROSCOPY:1||RELAXATION:1||PLASMA RESONANCE:1||coupled Josephson junctions:1||COPPEROXIDE SUPERCONDUCTORS:1||CROSSOVER:1||SIMULATIONS:1||LOWTEMPERATURE:1||CONDUCTORS:1||METALINSULATORTRANSITION:1||SEMICONDUCTOR:1||FIELDEFFECT TRANSISTORS:1||ZEROVOLTAGE STATE:1||constanttemperature interlayer tunneling spectroscopy:1||Josephson supercurrent:1||BIPOLAR SUPERCURRENT:1||Interaction between Josephson and pancake vortices:1||flux jump:1||coaxial heterojunction nanorod:1||Natural Josephson coupling:1||BI2SR2CACU2O8+DELTA:1||VORTEX FLOW:1||TC SUPERCONDUCTORS:1||charge imbalance:1||Andreev diffractometer:1||intercalation:1||surface junction:1||Bi2212:1||tunnelling:1||GRAPHITE:1||GROWTH:1||collective transverse plasma modes:1||GAN:1||Macroscopic quantum tunneling:1||Fluctuation conductivity:1||Abovegap conductance jump:1||Josephson vortex motion:1||Intrinsic Josephson junctions:1||LAYERED SUPERCONDUCTORS:1||BI2SR2CACU2O8+Y:1||INTERFACES:1||BREAKDOWN:1||SYSTEMS:1||Anisotropy ratio:1||Josephson vortex:1||spin relaxation in superconductors:1||bibased single crystals:1||MESOSCOPIC PROXIMITY SUPERCONDUCTOR:1||reentrance of conductance:1||interlayer pair tunneling:1||JOSEPHSON:1||DISORDERED 2DIMENSIONAL SUPERCONDUCTORS:1||INDIUM FILMS:1||excited state:1||REGIME:1||triplet superconductivity:1||FILM:1||SCHOTTKY DIODES:1||peakdiphump structure:1||Kondo effect:1||REENTRANCE:1||Graphene:1||CONTACT:1||BERRYS PHASE:1||2DIMENSIONAL SUPERCONDUCTORS:1||Coulomb diamond:1||magnetic domain:1||spin injection:1||RESONANCE:1||plasma excitation modes:1||FLOW:1||OVERDOPED BI2SR2CACU2O8+DELTA:1||hole doping:1||chemical synthesis:1||phase transitions:1||superconductors:1||VORTEXGLASS SUPERCONDUCTIVITY:1||Kondorelated model:1||RADIATION:1||DOT:1||NANOBELTS:1||Complementarity:1||Closedloop AharonovBohm interferometer:1||pair breaking:1||interlayer phase fluctuation:1||MgB2 thin film:1||CONFINEMENT:1||WALLED CARBON NANOTUBES:1||TRANSITION:9||VORTICES:8||STATE:7||intrinsic Josephson junctions:7||SINGLECRYSTALS:7||JUNCTIONS:5||MODES:5||SUPERCURRENT:5||SUPERCONDUCTOR:5||CONDUCTANCE:5||HIGHTEMPERATURE SUPERCONDUCTORS:5||TRANSPORT:5||PHASE:5||FILMS:4||LOCALIZATION:4||SINGLE DIRAC CONE:4||WIRES:4||MAGNETICFIELD:4||STEPS:3||ELECTRONS:3||proximity effect:3||MODEL:3||ARRAYS:3||INTERFERENCE:3||fluxon dynamics:3||HETEROSTRUCTURES:3||INSULATOR:3||Andreev reflection:3||electronic transport:3||FISKE:3||superconductor:2||ZnO:2||quantum point contact:2||METAL:2||DYNAMICS:2||interlayer Josephson coupling:2||SUPERCONDUCTORS:2||YBA2CU3O7DELTA:2||LAYER:2||DOTS:2||quantum dot:2||Article:2||TRANSISTORS:2||CARBON NANOTUBES:2||GAP:2||MECHANISM:2||LINE:2||GIANT SHAPIRO STEPS:2||LAYERS:2||electron energy loss spectroscopy:2||physical phenomena:2||scanning electron microscopy:2||HGTE QUANTUMWELLS:2||BI2TE3:2||SPECTROSCOPY:2||PNJUNCTIONS:2||spinpolarized tunneling:2||INTRINSIC JOSEPHSONJUNCTIONS:2||FIELDS:2||positive magnetoresistance:2||dilute magnetic semiconductor:2||magnetic field:2||scanning transmission electron microscopy:2||QUANTUM OSCILLATIONS:2||TRANSPORTPROPERTIES:2||surface pair current:2||MAGNETORESISTANCE:2||NANORIBBONS:2||INSTABILITY:2||ANDREEV REFLECTION:2||microwave irradiation:2||vertical graphene josephson junction:2||BI2SE3:2||CONDUCTIVITY:2||highTc superconductors:2||DIMENSIONAL ELECTRONGAS:2||graphene:2||Topological insulators:2||Josephson coupling Fraunhofer interference pattern:2||FERROMAGNET:2||DEPENDENCE:2||DETECTOR:2||COHERENCE:2||INJECTION:2||GRAPHENE:1||JOSEPHSONJUNCTIONS:1||LAYERED SUPERCONDUCTOR:1||mode splitting:1||BEHAVIOR:1||spinpolarized transport:1||SUPERCONDUCTING TRANSITION:1||microwave response:1||PSEUDOGAP:1||phase coherence:1||TRANSITIONS:1||Long Josephson junction:1||Charge detection:1||collective resonance modes:1||plasma oscillation modes:1||Superconducting proximity effect:1||Iron pnictide superconductor:1||McMillanRowell oscillations:1||ferromagnetic microstructure:1||superradiant state:1||VOLTAGE:1||branch splitting:1||TENSOR:1||INTERCALATION:1||insitu fabrication:1||NDGAO3:1||DISORDERED METALS:1||GAUGE GLASS:1||LOWTEMPERATURE TRANSPORT:1||spontaneous spin polarization model:1||BIAS:1||emission of electromagnetic waves:1||YBA2CU3O7/PRBA2CU3O7 SUPERLATTICES:1||BOHM:1||SHAPIRO STEPS:1||superconductor/ferromagnet interface:1||OXIDE:1||ANDREEVREFLECTION:1||SinFeAsO single crystal:1||COLLECTIVE MOTION:1||ANGULARDEPENDENCE:1||SUPERCONDUCTIVITY:1||BILAYER GRAPHENE:1||PHOTOLUMINESCENT PROPERTIES:1||SUPERCONDUCTING WEAK LINKS:1||intrinsic Josephson junctions geometrical resonance:1||intrinsic Josephson junction:1||MESOSCOPIC SPINVALVE:1||Bi2212 single crystals:1||intrinsic junctions:1||ANDREEV REFLECTIONS:1||normalmetal/superconductor interface:1||IBI2SR2CACU2OY:1||THERMAL FLUCTUATIONS:1||MIXED STATE:1||BI2.15SR1.85CACU2O8+DELTA:1||intrinsic Josephson effects:1||CACUO:1||QUANTUM POINT CONTACTS:1||resonant tunneling state:1||coherence length:1||NANOWIRE:1||GATES:1||Phase line:1||Thermal activation:1||QUANTUMDOT:1||superconducting proximity effect:1||Andreev interferometer:1||WIRE:1||Josephsonvortexflow branches:1||Bi2212 cuprates:1||LATTICE:1||demannetization effect:1||SUPERCONDUCTING MIRRORS:1||GAS:1||VALLEY TRANSPORT:1||ELECTRODES:1||DEPENDENT TRANSPORT:1||BORNOPPENHEIMER APPROXIMATION:1||collective plasma oscillations:1||fluxon resonance steps:1||STACKS:1||COLLECTIVE DYNAMICS:1||PAIRING SYMMETRY:1||MUON SPIN ROTATION:1||DIMENSIONAL CROSSOVER:1||Bi2Sr2CaCu2Oy highTc superconductors:1||heterojunctions:1||nanostructures:1||surfaces and interfaces:1||QUANTUM TRANSPORT:1||MICROJUNCTIONS:1||RESONATORS:1||STATES:1||FIELD:1||FLUCTUATIONS:1||SCATTERING:1||mode splitting of Josephson vortexflow branches:1||2D superconductivity:1||TRANSISTOR:1||ENERGYGAP:1||SUPERLATTICES:1||IRONBASED SUPERCONDUCTORS:1||PHASEDEPENDENT RESISTANCE:1||QUANTUM PHASETRANSITIONS:1||ELECTRICFIELD:1||HIGH MAGNETICFIELDS:1||NANOWIRE HETEROSTRUCTURES:1||ZNO:1||pair breaking.:1||SUPERCONDUCTING PB:1||domain formation:1||FORCE MICROSCOPY:1||RELAXATION:1||PLASMA RESONANCE:1||coupled Josephson junctions:1||COPPEROXIDE SUPERCONDUCTORS:1||CROSSOVER:1||SIMULATIONS:1||LOWTEMPERATURE:1||CONDUCTORS:1||METALINSULATORTRANSITION:1||SEMICONDUCTOR:1||FIELDEFFECT TRANSISTORS:1||ZEROVOLTAGE STATE:1||constanttemperature interlayer tunneling spectroscopy:1||Josephson supercurrent:1||BIPOLAR SUPERCURRENT:1||Interaction between Josephson and pancake vortices:1||flux jump:1||coaxial heterojunction nanorod:1||Natural Josephson coupling:1||BI2SR2CACU2O8+DELTA:1||VORTEX FLOW:1||TC SUPERCONDUCTORS:1||charge imbalance:1||Andreev diffractometer:1||intercalation:1||surface junction:1||Bi2212:1||tunnelling:1||GRAPHITE:1||GROWTH:1||collective transverse plasma modes:1||GAN:1||Macroscopic quantum tunneling:1||Fluctuation conductivity:1||Abovegap conductance jump:1||Josephson vortex motion:1||Intrinsic Josephson junctions:1||LAYERED SUPERCONDUCTORS:1||BI2SR2CACU2O8+Y:1||INTERFACES:1||BREAKDOWN:1||SYSTEMS:1||Anisotropy ratio:1||Josephson vortex:1||spin relaxation in superconductors:1||bibased single crystals:1||MESOSCOPIC PROXIMITY SUPERCONDUCTOR:1||reentrance of conductance:1||interlayer pair tunneling:1||JOSEPHSON:1||DISORDERED 2DIMENSIONAL SUPERCONDUCTORS:1||INDIUM FILMS:1||excited state:1||REGIME:1||triplet superconductivity:1||FILM:1||SCHOTTKY DIODES:1||peakdiphump structure:1||Kondo effect:1||REENTRANCE:1||Graphene:1||CONTACT:1||BERRYS PHASE:1||2DIMENSIONAL SUPERCONDUCTORS:1||Coulomb diamond:1||magnetic domain:1||spin injection:1||RESONANCE:1||plasma excitation modes:1||FLOW:1||OVERDOPED BI2SR2CACU2O8+DELTA:1||hole doping:1||chemical synthesis:1||phase transitions:1||superconductors:1||VORTEXGLASS SUPERCONDUCTIVITY:1||Kondorelated model:1||RADIATION:1||DOT:1||NANOBELTS:1||Complementarity:1||Closedloop AharonovBohm interferometer:1||pair breaking:1||interlayer phase fluctuation:1||MgB2 thin film:1||CONFINEMENT:1||WALLED CARBON NANOTUBES:1||TRANSITION:9||VORTICES:8||STATE:7||intrinsic Josephson junctions:7||SINGLECRYSTALS:7||JUNCTIONS:5||MODES:5||SUPERCURRENT:5||SUPERCONDUCTOR:5||CONDUCTANCE:5||HIGHTEMPERATURE SUPERCONDUCTORS:5||TRANSPORT:5||PHASE:5||FILMS:4||LOCALIZATION:4||SINGLE DIRAC CONE:4||WIRES:4||MAGNETICFIELD:4||STEPS:3||ELECTRONS:3||proximity effect:3||MODEL:3||ARRAYS:3||INTERFERENCE:3||fluxon dynamics:3||HETEROSTRUCTURES:3||INSULATOR:3||Andreev reflection:3||electronic transport:3||FISKE:3||superconductor:2||ZnO:2||quantum point contact:2||METAL:2||DYNAMICS:2||interlayer Josephson coupling:2||SUPERCONDUCTORS:2||YBA2CU3O7DELTA:2||LAYER:2||DOTS:2||quantum dot:2||Article:2||TRANSISTORS:2||CARBON NANOTUBES:2||GAP:2||MECHANISM:2||LINE:2||GIANT SHAPIRO STEPS:2||LAYERS:2||electron energy loss spectroscopy:2||physical phenomena:2||scanning electron microscopy:2||HGTE QUANTUMWELLS:2||BI2TE3:2||SPECTROSCOPY:2||PNJUNCTIONS:2||spinpolarized tunneling:2||INTRINSIC JOSEPHSONJUNCTIONS:2||FIELDS:2||positive magnetoresistance:2||dilute magnetic semiconductor:2||magnetic field:2||scanning transmission electron microscopy:2||QUANTUM OSCILLATIONS:2||TRANSPORTPROPERTIES:2||surface pair current:2||MAGNETORESISTANCE:2||NANORIBBONS:2||INSTABILITY:2||ANDREEV REFLECTION:2||microwave irradiation:2||vertical graphene josephson junction:2||BI2SE3:2||CONDUCTIVITY:2||highTc superconductors:2||DIMENSIONAL ELECTRONGAS:2||graphene:2||Topological insulators:2||Josephson coupling Fraunhofer interference pattern:2||FERROMAGNET:2||DEPENDENCE:2||DETECTOR:2||COHERENCE:2||INJECTION:2||GRAPHENE:1||JOSEPHSONJUNCTIONS:1||LAYERED SUPERCONDUCTOR:1||mode splitting:1||BEHAVIOR:1||spinpolarized transport:1||SUPERCONDUCTING TRANSITION:1||microwave response:1||PSEUDOGAP:1||phase coherence:1||TRANSITIONS:1||Long Josephson junction:1||Charge detection:1||collective resonance modes:1||plasma oscillation modes:1||Superconducting proximity effect:1||Iron pnictide superconductor:1||McMillanRowell oscillations:1||ferromagnetic microstructure:1||superradiant state:1||VOLTAGE:1||branch splitting:1||TENSOR:1||INTERCALATION:1||insitu fabrication:1||NDGAO3:1||DISORDERED METALS:1||GAUGE GLASS:1||LOWTEMPERATURE TRANSPORT:1||spontaneous spin polarization model:1||BIAS:1||emission of electromagnetic waves:1||YBA2CU3O7/PRBA2CU3O7 SUPERLATTICES:1||BOHM:1||SHAPIRO STEPS:1||superconductor/ferromagnet interface:1||OXIDE:1||ANDREEVREFLECTION:1||SinFeAsO single crystal:1||COLLECTIVE MOTION:1||ANGULARDEPENDENCE:1||SUPERCONDUCTIVITY:1||BILAYER GRAPHENE:1||PHOTOLUMINESCENT PROPERTIES:1||SUPERCONDUCTING WEAK LINKS:1||intrinsic Josephson junctions geometrical resonance:1||intrinsic Josephson junction:1||MESOSCOPIC SPINVALVE:1||Bi2212 single crystals:1||intrinsic junctions:1||ANDREEV REFLECTIONS:1||normalmetal/superconductor interface:1||IBI2SR2CACU2OY:1||THERMAL FLUCTUATIONS:1||MIXED STATE:1||BI2.15SR1.85CACU2O8+DELTA:1||intrinsic Josephson effects:1||CACUO:1||QUANTUM POINT CONTACTS:1||resonant tunneling state:1||coherence length:1||NANOWIRE:1||GATES:1||Phase line:1||Thermal activation:1||QUANTUMDOT:1||superconducting proximity effect:1||Andreev interferometer:1||WIRE:1||Josephsonvortexflow branches:1||Bi2212 cuprates:1||LATTICE:1||demannetization effect:1||SUPERCONDUCTING MIRRORS:1||GAS:1||VALLEY TRANSPORT:1||ELECTRODES:1||DEPENDENT TRANSPORT:1||BORNOPPENHEIMER APPROXIMATION:1||collective plasma oscillations:1||fluxon resonance steps:1||STACKS:1||COLLECTIVE DYNAMICS:1||PAIRING SYMMETRY:1||MUON SPIN ROTATION:1||DIMENSIONAL CROSSOVER:1||Bi2Sr2CaCu2Oy highTc superconductors:1||heterojunctions:1||nanostructures:1||surfaces and interfaces:1||QUANTUM TRANSPORT:1||MICROJUNCTIONS:1||RESONATORS:1||STATES:1||FIELD:1||FLUCTUATIONS:1||SCATTERING:1||mode splitting of Josephson vortexflow branches:1||2D superconductivity:1||TRANSISTOR:1||ENERGYGAP:1||SUPERLATTICES:1||IRONBASED SUPERCONDUCTORS:1||PHASEDEPENDENT RESISTANCE:1||QUANTUM PHASETRANSITIONS:1||ELECTRICFIELD:1||HIGH MAGNETICFIELDS:1||NANOWIRE HETEROSTRUCTURES:1||ZNO:1||pair breaking.:1||SUPERCONDUCTING PB:1||domain formation:1||FORCE MICROSCOPY:1||RELAXATION:1||PLASMA RESONANCE:1||coupled Josephson junctions:1||COPPEROXIDE SUPERCONDUCTORS:1||CROSSOVER:1||SIMULATIONS:1||LOWTEMPERATURE:1||CONDUCTORS:1||METALINSULATORTRANSITION:1||SEMICONDUCTOR:1||FIELDEFFECT TRANSISTORS:1||ZEROVOLTAGE STATE:1||constanttemperature interlayer tunneling spectroscopy:1||Josephson supercurrent:1||BIPOLAR SUPERCURRENT:1||Interaction between Josephson and pancake vortices:1||flux jump:1||coaxial heterojunction nanorod:1||Natural Josephson coupling:1||BI2SR2CACU2O8+DELTA:1||VORTEX FLOW:1||TC SUPERCONDUCTORS:1||charge imbalance:1||Andreev diffractometer:1||intercalation:1||surface junction:1||Bi2212:1||tunnelling:1||GRAPHITE:1||GROWTH:1||collective transverse plasma modes:1||GAN:1||Macroscopic quantum tunneling:1||Fluctuation conductivity:1||Abovegap conductance jump:1||Josephson vortex motion:1||Intrinsic Josephson junctions:1||LAYERED SUPERCONDUCTORS:1||BI2SR2CACU2O8+Y:1||INTERFACES:1||BREAKDOWN:1||SYSTEMS:1||Anisotropy ratio:1||Josephson vortex:1||spin relaxation in superconductors:1||bibased single crystals:1||MESOSCOPIC PROXIMITY SUPERCONDUCTOR:1||reentrance of conductance:1||interlayer pair tunneling:1||JOSEPHSON:1||DISORDERED 2DIMENSIONAL SUPERCONDUCTORS:1||INDIUM FILMS:1||excited state:1||REGIME:1||triplet superconductivity:1||FILM:1||SCHOTTKY DIODES:1||peakdiphump structure:1||Kondo effect:1||REENTRANCE:1||Graphene:1||CONTACT:1||BERRYS PHASE:1||2DIMENSIONAL SUPERCONDUCTORS:1||Coulomb diamond:1||magnetic domain:1||spin injection:1||RESONANCE:1||plasma excitation modes:1||FLOW:1||OVERDOPED BI2SR2CACU2O8+DELTA:1||hole doping:1||chemical synthesis:1||phase transitions:1||superconductors:1||VORTEXGLASS SUPERCONDUCTIVITY:1||Kondorelated model:1||RADIATION:1||DOT:1||NANOBELTS:1||Complementarity:1||Closedloop AharonovBohm interferometer:1||pair breaking:1||interlayer phase fluctuation:1||MgB2 thin film:1||CONFINEMENT:1||WALLED CARBON NANOTUBES:1||TRANSITION:9||VORTICES:8||STATE:7||intrinsic Josephson junctions:7||SINGLECRYSTALS:7||JUNCTIONS:5||MODES:5||SUPERCURRENT:5||SUPERCONDUCTOR:5||CONDUCTANCE:5||HIGHTEMPERATURE SUPERCONDUCTORS:5||TRANSPORT:5||PHASE:5||FILMS:4||LOCALIZATION:4||SINGLE DIRAC CONE:4||WIRES:4||MAGNETICFIELD:4||STEPS:3||ELECTRONS:3||proximity effect:3||MODEL:3||ARRAYS:3||INTERFERENCE:3||fluxon dynamics:3||HETEROSTRUCTURES:3||INSULATOR:3||Andreev reflection:3||electronic transport:3||FISKE:3||superconductor:2||ZnO:2||quantum point contact:2||METAL:2||DYNAMICS:2||interlayer Josephson coupling:2||SUPERCONDUCTORS:2||YBA2CU3O7DELTA:2||LAYER:2||DOTS:2||quantum dot:2||Article:2||TRANSISTORS:2||CARBON NANOTUBES:2||GAP:2||MECHANISM:2||LINE:2||GIANT SHAPIRO STEPS:2||LAYERS:2||electron energy loss spectroscopy:2||physical phenomena:2||scanning electron microscopy:2||HGTE QUANTUMWELLS:2||BI2TE3:2||SPECTROSCOPY:2||PNJUNCTIONS:2||spinpolarized tunneling:2||INTRINSIC JOSEPHSONJUNCTIONS:2||FIELDS:2||positive magnetoresistance:2||dilute magnetic semiconductor:2||magnetic field:2||scanning transmission electron microscopy:2||QUANTUM OSCILLATIONS:2||TRANSPORTPROPERTIES:2||surface pair current:2||MAGNETORESISTANCE:2||NANORIBBONS:2||INSTABILITY:2||ANDREEV REFLECTION:2||microwave irradiation:2||vertical graphene josephson junction:2||BI2SE3:2||CONDUCTIVITY:2||highTc superconductors:2||DIMENSIONAL ELECTRONGAS:2||graphene:2||Topological insulators:2||Josephson coupling Fraunhofer interference pattern:2||FERROMAGNET:2||DEPENDENCE:2||DETECTOR:2||COHERENCE:2||INJECTION:2||GRAPHENE:1||JOSEPHSONJUNCTIONS:1||LAYERED SUPERCONDUCTOR:1||mode splitting:1||BEHAVIOR:1||spinpolarized transport:1||SUPERCONDUCTING TRANSITION:1||microwave response:1||PSEUDOGAP:1||phase coherence:1||TRANSITIONS:1||Long Josephson junction:1||Charge detection:1||collective resonance modes:1||plasma oscillation modes:1||Superconducting proximity effect:1||Iron pnictide superconductor:1||McMillanRowell oscillations:1||ferromagnetic microstructure:1||superradiant state:1||VOLTAGE:1||branch splitting:1||TENSOR:1||INTERCALATION:1||insitu fabrication:1||NDGAO3:1||DISORDERED METALS:1||GAUGE GLASS:1||LOWTEMPERATURE TRANSPORT:1||spontaneous spin polarization model:1||BIAS:1||emission of electromagnetic waves:1||YBA2CU3O7/PRBA2CU3O7 SUPERLATTICES:1||BOHM:1||SHAPIRO STEPS:1||superconductor/ferromagnet interface:1||OXIDE:1||ANDREEVREFLECTION:1||SinFeAsO single crystal:1||COLLECTIVE MOTION:1||ANGULARDEPENDENCE:1||SUPERCONDUCTIVITY:1||BILAYER GRAPHENE:1||PHOTOLUMINESCENT PROPERTIES:1||SUPERCONDUCTING WEAK LINKS:1||intrinsic Josephson junctions geometrical resonance:1||intrinsic Josephson junction:1||MESOSCOPIC SPINVALVE:1||Bi2212 single crystals:1||intrinsic junctions:1||ANDREEV REFLECTIONS:1||normalmetal/superconductor interface:1||IBI2SR2CACU2OY:1||THERMAL FLUCTUATIONS:1||MIXED STATE:1||BI2.15SR1.85CACU2O8+DELTA:1||intrinsic Josephson effects:1||CACUO:1||QUANTUM POINT CONTACTS:1||resonant tunneling state:1||coherence length:1||NANOWIRE:1||GATES:1||Phase line:1||Thermal activation:1||QUANTUMDOT:1||superconducting proximity effect:1||Andreev interferometer:1||WIRE:1||Josephsonvortexflow branches:1||Bi2212 cuprates:1||LATTICE:1||demannetization effect:1||SUPERCONDUCTING MIRRORS:1||GAS:1||VALLEY TRANSPORT:1||ELECTRODES:1||DEPENDENT TRANSPORT:1||BORNOPPENHEIMER APPROXIMATION:1||collective plasma oscillations:1||fluxon resonance steps:1||STACKS:1||COLLECTIVE DYNAMICS:1||PAIRING SYMMETRY:1||MUON SPIN ROTATION:1||DIMENSIONAL CROSSOVER:1||Bi2Sr2CaCu2Oy highTc superconductors:1||heterojunctions:1||nanostructures:1||surfaces and interfaces:1||QUANTUM TRANSPORT:1||MICROJUNCTIONS:1||RESONATORS:1||STATES:1||FIELD:1||FLUCTUATIONS:1||SCATTERING:1||mode splitting of Josephson vortexflow branches:1||2D superconductivity:1||TRANSISTOR:1||ENERGYGAP:1||SUPERLATTICES:1||IRONBASED SUPERCONDUCTORS:1||PHASEDEPENDENT RESISTANCE:1||QUANTUM PHASETRANSITIONS:1||ELECTRICFIELD:1||HIGH MAGNETICFIELDS:1||NANOWIRE HETEROSTRUCTURES:1||ZNO:1||pair breaking.:1||SUPERCONDUCTING PB:1||domain formation:1||FORCE MICROSCOPY:1||RELAXATION:1||PLASMA RESONANCE:1||coupled Josephson junctions:1||COPPEROXIDE SUPERCONDUCTORS:1||CROSSOVER:1||SIMULATIONS:1||LOWTEMPERATURE:1||CONDUCTORS:1||METALINSULATORTRANSITION:1||SEMICONDUCTOR:1||FIELDEFFECT TRANSISTORS:1||ZEROVOLTAGE STATE:1||constanttemperature interlayer tunneling spectroscopy:1||Josephson supercurrent:1||BIPOLAR SUPERCURRENT:1||Interaction between Josephson and pancake vortices:1||flux jump:1||coaxial heterojunction nanorod:1||Natural Josephson coupling:1||BI2SR2CACU2O8+DELTA:1||VORTEX FLOW:1||TC SUPERCONDUCTORS:1||charge imbalance:1||Andreev diffractometer:1||intercalation:1||surface junction:1||Bi2212:1||tunnelling:1||GRAPHITE:1||GROWTH:1||collective transverse plasma modes:1||GAN:1||Macroscopic quantum tunneling:1||Fluctuation conductivity:1||Abovegap conductance jump:1||Josephson vortex motion:1||Intrinsic Josephson junctions:1||LAYERED SUPERCONDUCTORS:1||BI2SR2CACU2O8+Y:1||INTERFACES:1||BREAKDOWN:1||SYSTEMS:1||Anisotropy ratio:1||Josephson vortex:1||spin relaxation in superconductors:1||bibased single crystals:1||MESOSCOPIC PROXIMITY SUPERCONDUCTOR:1||reentrance of conductance:1||interlayer pair tunneling:1||JOSEPHSON:1||DISORDERED 2DIMENSIONAL SUPERCONDUCTORS:1||INDIUM FILMS:1||excited state:1||REGIME:1||triplet superconductivity:1||FILM:1||SCHOTTKY DIODES:1||peakdiphump structure:1||Kondo effect:1||REENTRANCE:1||Graphene:1||CONTACT:1||BERRYS PHASE:1||2DIMENSIONAL SUPERCONDUCTORS:1||Coulomb diamond:1||magnetic domain:1||spin injection:1||RESONANCE:1||plasma excitation modes:1||FLOW:1||OVERDOPED BI2SR2CACU2O8+DELTA:1||hole doping:1||chemical synthesis:1||phase transitions:1||superconductors:1||VORTEXGLASS SUPERCONDUCTIVITY:1||Kondorelated model:1||RADIATION:1||DOT:1||NANOBELTS:1||Complementarity:1||Closedloop AharonovBohm interferometer:1||pair breaking:1||interlayer phase fluctuation:1||MgB2 thin film:1||CONFINEMENT:1||WALLED CARBON NANOTUBES:1||TRANSITION:9||VORTICES:8||STATE:7||intrinsic Josephson junctions:7||SINGLECRYSTALS:7||JUNCTIONS:5||MODES:5||SUPERCURRENT:5||SUPERCONDUCTOR:5||CONDUCTANCE:5||HIGHTEMPERATURE SUPERCONDUCTORS:5||TRANSPORT:5||PHASE:5||FILMS:4||LOCALIZATION:4||SINGLE DIRAC CONE:4||WIRES:4||MAGNETICFIELD:4||STEPS:3||ELECTRONS:3||proximity effect:3||MODEL:3||ARRAYS:3||INTERFERENCE:3||fluxon dynamics:3||HETEROSTRUCTURES:3||INSULATOR:3||Andreev reflection:3||electronic transport:3||FISKE:3||superconductor:2||ZnO:2||quantum point contact:2||METAL:2||DYNAMICS:2||interlayer Josephson coupling:2||SUPERCONDUCTORS:2||YBA2CU3O7DELTA:2||LAYER:2||DOTS:2||quantum dot:2||Article:2||TRANSISTORS:2||CARBON NANOTUBES:2||GAP:2||MECHANISM:2||LINE:2||GIANT SHAPIRO STEPS:2||LAYERS:2||electron energy loss spectroscopy:2||physical phenomena:2||scanning electron microscopy:2||HGTE QUANTUMWELLS:2||BI2TE3:2||SPECTROSCOPY:2||PNJUNCTIONS:2||spinpolarized tunneling:2||INTRINSIC JOSEPHSONJUNCTIONS:2||FIELDS:2||positive magnetoresistance:2||dilute magnetic semiconductor:2||magnetic field:2||scanning transmission electron microscopy:2||QUANTUM OSCILLATIONS:2||TRANSPORTPROPERTIES:2||surface pair current:2||MAGNETORESISTANCE:2||NANORIBBONS:2||INSTABILITY:2||ANDREEV REFLECTION:2||microwave irradiation:2||vertical graphene josephson junction:2||BI2SE3:2||CONDUCTIVITY:2||highTc superconductors:2||DIMENSIONAL ELECTRONGAS:2||graphene:2||Topological insulators:2||Josephson coupling Fraunhofer interference pattern:2||FERROMAGNET:2||DEPENDENCE:2||DETECTOR:2||COHERENCE:2||INJECTION:2||GRAPHENE:1||JOSEPHSONJUNCTIONS:1||LAYERED SUPERCONDUCTOR:1||mode splitting:1||BEHAVIOR:1||spinpolarized transport:1||SUPERCONDUCTING TRANSITION:1||microwave response:1||PSEUDOGAP:1||phase coherence:1||TRANSITIONS:1||Long Josephson junction:1||Charge detection:1||collective resonance modes:1||plasma oscillation modes:1||Superconducting proximity effect:1||Iron pnictide superconductor:1||McMillanRowell oscillations:1||ferromagnetic microstructure:1||superradiant state:1||VOLTAGE:1||branch splitting:1||TENSOR:1||INTERCALATION:1||insitu fabrication:1||NDGAO3:1||DISORDERED METALS:1||GAUGE GLASS:1||LOWTEMPERATURE TRANSPORT:1||spontaneous spin polarization model:1||BIAS:1||emission of electromagnetic waves:1||YBA2CU3O7/PRBA2CU3O7 SUPERLATTICES:1||BOHM:1||SHAPIRO STEPS:1||superconductor/ferromagnet interface:1||OXIDE:1||ANDREEVREFLECTION:1||SinFeAsO single crystal:1||COLLECTIVE MOTION:1||ANGULARDEPENDENCE:1||SUPERCONDUCTIVITY:1||BILAYER GRAPHENE:1||PHOTOLUMINESCENT PROPERTIES:1||SUPERCONDUCTING WEAK LINKS:1||intrinsic Josephson junctions geometrical resonance:1||intrinsic Josephson junction:1||MESOSCOPIC SPINVALVE:1||Bi2212 single crystals:1||intrinsic junctions:1||ANDREEV REFLECTIONS:1||normalmetal/superconductor interface:1||IBI2SR2CACU2OY:1||THERMAL FLUCTUATIONS:1||MIXED STATE:1||BI2.15SR1.85CACU2O8+DELTA:1||intrinsic Josephson effects:1||CACUO:1||QUANTUM POINT CONTACTS:1||resonant tunneling state:1||coherence length:1||NANOWIRE:1||GATES:1||Phase line:1||Thermal activation:1||QUANTUMDOT:1||superconducting proximity effect:1||Andreev interferometer:1||WIRE:1||Josephsonvortexflow branches:1||Bi2212 cuprates:1||LATTICE:1||demannetization effect:1||SUPERCONDUCTING MIRRORS:1||GAS:1||VALLEY TRANSPORT:1||ELECTRODES:1||DEPENDENT TRANSPORT:1||BORNOPPENHEIMER APPROXIMATION:1||collective plasma oscillations:1||fluxon resonance steps:1||STACKS:1||COLLECTIVE DYNAMICS:1||PAIRING SYMMETRY:1||MUON SPIN ROTATION:1||DIMENSIONAL CROSSOVER:1||Bi2Sr2CaCu2Oy highTc superconductors:1||heterojunctions:1||nanostructures:1||surfaces and interfaces:1||QUANTUM TRANSPORT:1||MICROJUNCTIONS:1||RESONATORS:1||STATES:1||FIELD:1||FLUCTUATIONS:1||SCATTERING:1||mode splitting of Josephson vortexflow branches:1||2D superconductivity:1||TRANSISTOR:1||ENERGYGAP:1||SUPERLATTICES:1||IRONBASED SUPERCONDUCTORS:1||PHASEDEPENDENT RESISTANCE:1||QUANTUM PHASETRANSITIONS:1||ELECTRICFIELD:1||HIGH MAGNETICFIELDS:1||NANOWIRE HETEROSTRUCTURES:1||ZNO:1||pair breaking.:1||SUPERCONDUCTING PB:1||domain formation:1||FORCE MICROSCOPY:1||RELAXATION:1||PLASMA RESONANCE:1||coupled Josephson junctions:1||COPPEROXIDE SUPERCONDUCTORS:1||CROSSOVER:1||SIMULATIONS:1||LOWTEMPERATURE:1||CONDUCTORS:1||METALINSULATORTRANSITION:1||SEMICONDUCTOR:1||FIELDEFFECT TRANSISTORS:1||ZEROVOLTAGE STATE:1||constanttemperature interlayer tunneling spectroscopy:1||Josephson supercurrent:1||BIPOLAR SUPERCURRENT:1||Interaction between Josephson and pancake vortices:1||flux jump:1||coaxial heterojunction nanorod:1||Natural Josephson coupling:1||BI2SR2CACU2O8+DELTA:1||VORTEX FLOW:1||TC SUPERCONDUCTORS:1||charge imbalance:1||Andreev diffractometer:1||intercalation:1||surface junction:1||Bi2212:1||tunnelling:1||GRAPHITE:1||GROWTH:1||collective transverse plasma modes:1||GAN:1||Macroscopic quantum tunneling:1||Fluctuation conductivity:1||Abovegap conductance jump:1||Josephson vortex motion:1||Intrinsic Josephson junctions:1||LAYERED SUPERCONDUCTORS:1||BI2SR2CACU2O8+Y:1||INTERFACES:1||BREAKDOWN:1||SYSTEMS:1||Anisotropy ratio:1||Josephson vortex:1||spin relaxation in superconductors:1||bibased single crystals:1||MESOSCOPIC PROXIMITY SUPERCONDUCTOR:1||reentrance of conductance:1||interlayer pair tunneling:1||JOSEPHSON:1||DISORDERED 2DIMENSIONAL SUPERCONDUCTORS:1||INDIUM FILMS:1||excited state:1||REGIME:1||triplet superconductivity:1||FILM:1||SCHOTTKY DIODES:1||peakdiphump structure:1||Kondo effect:1||REENTRANCE:1||Graphene:1||CONTACT:1||BERRYS PHASE:1||2DIMENSIONAL SUPERCONDUCTORS:1||Coulomb diamond:1||magnetic domain:1||spin injection:1||RESONANCE:1||plasma excitation modes:1||FLOW:1||OVERDOPED BI2SR2CACU2O8+DELTA:1||hole doping:1||chemical synthesis:1||phase transitions:1||superconductors:1||VORTEXGLASS SUPERCONDUCTIVITY:1||Kondorelated model:1||RADIATION:1||DOT:1||NANOBELTS:1||Complementarity:1||Closedloop AharonovBohm interferometer:1||pair breaking:1||interlayer phase fluctuation:1||MgB2 thin film:1||CONFINEMENT:1||WALLED CARBON NANOTUBES:1||TRANSITION:9||VORTICES:8||STATE:7||intrinsic Josephson junctions:7||SINGLECRYSTALS:7||JUNCTIONS:5||MODES:5||SUPERCURRENT:5||SUPERCONDUCTOR:5||CONDUCTANCE:5||HIGHTEMPERATURE SUPERCONDUCTORS:5||TRANSPORT:5||PHASE:5||FILMS:4||LOCALIZATION:4||SINGLE DIRAC CONE:4||WIRES:4||MAGNETICFIELD:4||STEPS:3||ELECTRONS:3||proximity effect:3||MODEL:3||ARRAYS:3||INTERFERENCE:3||fluxon dynamics:3||HETEROSTRUCTURES:3||INSULATOR:3||Andreev reflection:3||electronic transport:3||FISKE:3||superconductor:2||ZnO:2||quantum point contact:2||METAL:2||DYNAMICS:2||interlayer Josephson coupling:2||SUPERCONDUCTORS:2||YBA2CU3O7DELTA:2||LAYER:2||DOTS:2||quantum dot:2||Article:2||TRANSISTORS:2||CARBON NANOTUBES:2||GAP:2||MECHANISM:2||LINE:2||GIANT SHAPIRO STEPS:2||LAYERS:2||electron energy loss spectroscopy:2||physical phenomena:2||scanning electron microscopy:2||HGTE QUANTUMWELLS:2||BI2TE3:2||SPECTROSCOPY:2||PNJUNCTIONS:2||spinpolarized tunneling:2||INTRINSIC JOSEPHSONJUNCTIONS:2||FIELDS:2||positive magnetoresistance:2||dilute magnetic semiconductor:2||magnetic field:2||scanning transmission electron microscopy:2||QUANTUM OSCILLATIONS:2||TRANSPORTPROPERTIES:2||surface pair current:2||MAGNETORESISTANCE:2||NANORIBBONS:2||INSTABILITY:2||ANDREEV REFLECTION:2||microwave irradiation:2||vertical graphene josephson junction:2||BI2SE3:2||CONDUCTIVITY:2||highTc superconductors:2||DIMENSIONAL ELECTRONGAS:2||graphene:2||Topological insulators:2||Josephson coupling Fraunhofer interference pattern:2||FERROMAGNET:2||DEPENDENCE:2||DETECTOR:2||COHERENCE:2||INJECTION:2||GRAPHENE:1||JOSEPHSONJUNCTIONS:1||LAYERED SUPERCONDUCTOR:1||mode splitting:1||BEHAVIOR:1||spinpolarized transport:1||SUPERCONDUCTING TRANSITION:1||microwave response:1||PSEUDOGAP:1||phase coherence:1||TRANSITIONS:1||Long Josephson junction:1||Charge detection:1||collective resonance modes:1||plasma oscillation modes:1||Superconducting proximity effect:1||Iron pnictide superconductor:1||McMillanRowell oscillations:1||ferromagnetic microstructure:1||superradiant state:1||VOLTAGE:1||branch splitting:1||TENSOR:1||INTERCALATION:1||insitu fabrication:1||NDGAO3:1||DISORDERED METALS:1||GAUGE GLASS:1||LOWTEMPERATURE TRANSPORT:1||spontaneous spin polarization model:1||BIAS:1||emission of electromagnetic waves:1||YBA2CU3O7/PRBA2CU3O7 SUPERLATTICES:1||BOHM:1||SHAPIRO STEPS:1||superconductor/ferromagnet interface:1||OXIDE:1||ANDREEVREFLECTION:1||SinFeAsO single crystal:1||COLLECTIVE MOTION:1||ANGULARDEPENDENCE:1||SUPERCONDUCTIVITY:1||BILAYER GRAPHENE:1||PHOTOLUMINESCENT PROPERTIES:1||SUPERCONDUCTING WEAK LINKS:1||intrinsic Josephson junctions geometrical resonance:1||intrinsic Josephson junction:1||MESOSCOPIC SPINVALVE:1||Bi2212 single crystals:1||intrinsic junctions:1||ANDREEV REFLECTIONS:1||normalmetal/superconductor interface:1||IBI2SR2CACU2OY:1||THERMAL FLUCTUATIONS:1||MIXED STATE:1||BI2.15SR1.85CACU2O8+DELTA:1||intrinsic Josephson effects:1||CACUO:1||QUANTUM POINT CONTACTS:1||resonant tunneling state:1||coherence length:1||NANOWIRE:1||GATES:1||Phase line:1||Thermal activation:1||QUANTUMDOT:1||superconducting proximity effect:1||Andreev interferometer:1||WIRE:1||Josephsonvortexflow branches:1||Bi2212 cuprates:1||LATTICE:1||demannetization effect:1||SUPERCONDUCTING MIRRORS:1||GAS:1||VALLEY TRANSPORT:1||ELECTRODES:1||DEPENDENT TRANSPORT:1||BORNOPPENHEIMER APPROXIMATION:1||collective plasma oscillations:1||fluxon resonance steps:1||STACKS:1||COLLECTIVE DYNAMICS:1||PAIRING SYMMETRY:1||MUON SPIN ROTATION:1||DIMENSIONAL CROSSOVER:1||Bi2Sr2CaCu2Oy highTc superconductors:1||heterojunctions:1||nanostructures:1||surfaces and interfaces:1||QUANTUM TRANSPORT:1||MICROJUNCTIONS:1||RESONATORS:1||STATES:1||FIELD:1||FLUCTUATIONS:1||SCATTERING:1||mode splitting of Josephson vortexflow branches:1||2D superconductivity:1||TRANSISTOR:1||ENERGYGAP:1||SUPERLATTICES:1||IRONBASED SUPERCONDUCTORS:1||PHASEDEPENDENT RESISTANCE:1||QUANTUM PHASETRANSITIONS:1||ELECTRICFIELD:1||HIGH MAGNETICFIELDS:1||NANOWIRE HETEROSTRUCTURES:1||ZNO:1||pair breaking.:1||SUPERCONDUCTING PB:1||domain formation:1||FORCE MICROSCOPY:1||RELAXATION:1||PLASMA RESONANCE:1||coupled Josephson junctions:1||COPPEROXIDE SUPERCONDUCTORS:1||CROSSOVER:1||SIMULATIONS:1||LOWTEMPERATURE:1||CONDUCTORS:1||METALINSULATORTRANSITION:1||SEMICONDUCTOR:1||FIELDEFFECT TRANSISTORS:1||ZEROVOLTAGE STATE:1||constanttemperature interlayer tunneling spectroscopy:1||Josephson supercurrent:1||BIPOLAR SUPERCURRENT:1||Interaction between Josephson and pancake vortices:1||flux jump:1||coaxial heterojunction nanorod:1||Natural Josephson coupling:1||BI2SR2CACU2O8+DELTA:1||VORTEX FLOW:1||TC SUPERCONDUCTORS:1||charge imbalance:1||Andreev diffractometer:1||intercalation:1||surface junction:1||Bi2212:1||tunnelling:1||GRAPHITE:1||GROWTH:1||collective transverse plasma modes:1||GAN:1||Macroscopic quantum tunneling:1||Fluctuation conductivity:1||Abovegap conductance jump:1||Josephson vortex motion:1||Intrinsic Josephson junctions:1||LAYERED SUPERCONDUCTORS:1||BI2SR2CACU2O8+Y:1||INTERFACES:1||BREAKDOWN:1||SYSTEMS:1||Anisotropy ratio:1||Josephson vortex:1||spin relaxation in superconductors:1||bibased single crystals:1||MESOSCOPIC PROXIMITY SUPERCONDUCTOR:1||reentrance of conductance:1||interlayer pair tunneling:1||JOSEPHSON:1||DISORDERED 2DIMENSIONAL SUPERCONDUCTORS:1||INDIUM FILMS:1||excited state:1||REGIME:1||triplet superconductivity:1||FILM:1||SCHOTTKY DIODES:1||peakdiphump structure:1||Kondo effect:1||REENTRANCE:1||Graphene:1||CONTACT:1||BERRYS PHASE:1||2DIMENSIONAL SUPERCONDUCTORS:1||Coulomb diamond:1||magnetic domain:1||spin injection:1||RESONANCE:1||plasma excitation modes:1||FLOW:1||OVERDOPED BI2SR2CACU2O8+DELTA:1||hole doping:1||chemical synthesis:1||phase transitions:1||superconductors:1||VORTEXGLASS SUPERCONDUCTIVITY:1||Kondorelated model:1||RADIATION:1||DOT:1||NANOBELTS:1||Complementarity:1||Closedloop AharonovBohm interferometer:1||pair breaking:1||interlayer phase fluctuation:1||MgB2 thin film:1||CONFINEMENT:1||WALLED CARBON NANOTUBES:1||TRANSITION:9||VORTICES:8||STATE:7||intrinsic Josephson junctions:7||SINGLECRYSTALS:7||JUNCTIONS:5||MODES:5||SUPERCURRENT:5||SUPERCONDUCTOR:5||CONDUCTANCE:5||HIGHTEMPERATURE SUPERCONDUCTORS:5||TRANSPORT:5||PHASE:5||FILMS:4||LOCALIZATION:4||SINGLE DIRAC CONE:4||WIRES:4||MAGNETICFIELD:4||STEPS:3||ELECTRONS:3||proximity effect:3||MODEL:3||ARRAYS:3||INTERFERENCE:3||fluxon dynamics:3||HETEROSTRUCTURES:3||INSULATOR:3||Andreev reflection:3||electronic transport:3||FISKE:3||superconductor:2||ZnO:2||quantum point contact:2||METAL:2||DYNAMICS:2||interlayer Josephson coupling:2||SUPERCONDUCTORS:2||YBA2CU3O7DELTA:2||LAYER:2||DOTS:2||quantum dot:2||Article:2||TRANSISTORS:2||CARBON NANOTUBES:2||GAP:2||MECHANISM:2||LINE:2||GIANT SHAPIRO STEPS:2||LAYERS:2||electron energy loss spectroscopy:2||physical phenomena:2||scanning electron microscopy:2||HGTE QUANTUMWELLS:2||BI2TE3:2||SPECTROSCOPY:2||PNJUNCTIONS:2||spinpolarized tunneling:2||INTRINSIC JOSEPHSONJUNCTIONS:2||FIELDS:2||positive magnetoresistance:2||dilute magnetic semiconductor:2||magnetic field:2||scanning transmission electron microscopy:2||QUANTUM OSCILLATIONS:2||TRANSPORTPROPERTIES:2||surface pair current:2||MAGNETORESISTANCE:2||NANORIBBONS:2||INSTABILITY:2||ANDREEV REFLECTION:2||microwave irradiation:2||vertical graphene josephson junction:2||BI2SE3:2||CONDUCTIVITY:2||highTc superconductors:2||DIMENSIONAL ELECTRONGAS:2||graphene:2||Topological insulators:2||Josephson coupling Fraunhofer interference pattern:2||FERROMAGNET:2||DEPENDENCE:2||DETECTOR:2||COHERENCE:2||INJECTION:2||GRAPHENE:1||JOSEPHSONJUNCTIONS:1||LAYERED SUPERCONDUCTOR:1||mode splitting:1||BEHAVIOR:1||spinpolarized transport:1||SUPERCONDUCTING TRANSITION:1||microwave response:1||PSEUDOGAP:1||phase coherence:1||TRANSITIONS:1||Long Josephson junction:1||Charge detection:1||collective resonance modes:1||plasma oscillation modes:1||Superconducting proximity effect:1||Iron pnictide superconductor:1||McMillanRowell oscillations:1||ferromagnetic microstructure:1||superradiant state:1||VOLTAGE:1||branch splitting:1||TENSOR:1||INTERCALATION:1||insitu fabrication:1||NDGAO3:1||DISORDERED METALS:1||GAUGE GLASS:1||LOWTEMPERATURE TRANSPORT:1||spontaneous spin polarization model:1||BIAS:1||emission of electromagnetic waves:1||YBA2CU3O7/PRBA2CU3O7 SUPERLATTICES:1||BOHM:1||SHAPIRO STEPS:1||superconductor/ferromagnet interface:1||OXIDE:1||ANDREEVREFLECTION:1||SinFeAsO single crystal:1||COLLECTIVE MOTION:1||ANGULARDEPENDENCE:1||SUPERCONDUCTIVITY:1||BILAYER GRAPHENE:1||PHOTOLUMINESCENT PROPERTIES:1||SUPERCONDUCTING WEAK LINKS:1||intrinsic Josephson junctions geometrical resonance:1||intrinsic Josephson junction:1||MESOSCOPIC SPINVALVE:1||Bi2212 single crystals:1||intrinsic junctions:1||ANDREEV REFLECTIONS:1||normalmetal/superconductor interface:1||IBI2SR2CACU2OY:1||THERMAL FLUCTUATIONS:1||MIXED STATE:1||BI2.15SR1.85CACU2O8+DELTA:1||intrinsic Josephson effects:1||CACUO:1||QUANTUM POINT CONTACTS:1||resonant tunneling state:1||coherence length:1||NANOWIRE:1||GATES:1||Phase line:1||Thermal activation:1||QUANTUMDOT:1||superconducting proximity effect:1||Andreev interferometer:1||WIRE:1||Josephsonvortexflow branches:1||Bi2212 cuprates:1||LATTICE:1||demannetization effect:1||SUPERCONDUCTING MIRRORS:1||GAS:1||VALLEY TRANSPORT:1||ELECTRODES:1||DEPENDENT TRANSPORT:1||BORNOPPENHEIMER APPROXIMATION:1||collective plasma oscillations:1||fluxon resonance steps:1||STACKS:1||COLLECTIVE DYNAMICS:1||PAIRING SYMMETRY:1||MUON SPIN ROTATION:1||DIMENSIONAL CROSSOVER:1||Bi2Sr2CaCu2Oy highTc superconductors:1||heterojunctions:1||nanostructures:1||surfaces and interfaces:1||QUANTUM TRANSPORT:1||MICROJUNCTIONS:1||RESONATORS:1||STATES:1||FIELD:1||FLUCTUATIONS:1||SCATTERING:1||mode splitting of Josephson vortexflow branches:1||2D superconductivity:1||TRANSISTOR:1||ENERGYGAP:1||SUPERLATTICES:1||IRONBASED SUPERCONDUCTORS:1||PHASEDEPENDENT RESISTANCE:1||QUANTUM PHASETRANSITIONS:1||ELECTRICFIELD:1||HIGH MAGNETICFIELDS:1||NANOWIRE HETEROSTRUCTURES:1||ZNO:1||pair breaking.:1||SUPERCONDUCTING PB:1||domain formation:1||FORCE MICROSCOPY:1||RELAXATION:1||PLASMA RESONANCE:1||coupled Josephson junctions:1||COPPEROXIDE SUPERCONDUCTORS:1||CROSSOVER:1||SIMULATIONS:1||LOWTEMPERATURE:1||CONDUCTORS:1||METALINSULATORTRANSITION:1||SEMICONDUCTOR:1||FIELDEFFECT TRANSISTORS:1||ZEROVOLTAGE STATE:1||constanttemperature interlayer tunneling spectroscopy:1||Josephson supercurrent:1||BIPOLAR SUPERCURRENT:1||Interaction between Josephson and pancake vortices:1||flux jump:1||coaxial heterojunction nanorod:1||Natural Josephson coupling:1||BI2SR2CACU2O8+DELTA:1||VORTEX FLOW:1||TC SUPERCONDUCTORS:1||charge imbalance:1||Andreev diffractometer:1||intercalation:1||surface junction:1||Bi2212:1||tunnelling:1||GRAPHITE:1||GROWTH:1||collective transverse plasma modes:1||GAN:1||Macroscopic quantum tunneling:1||Fluctuation conductivity:1||Abovegap conductance jump:1||Josephson vortex motion:1||Intrinsic Josephson junctions:1||LAYERED SUPERCONDUCTORS:1||BI2SR2CACU2O8+Y:1||INTERFACES:1||BREAKDOWN:1||SYSTEMS:1||Anisotropy ratio:1||Josephson vortex:1||spin relaxation in superconductors:1||bibased single crystals:1||MESOSCOPIC PROXIMITY SUPERCONDUCTOR:1||reentrance of conductance:1||interlayer pair tunneling:1||JOSEPHSON:1||DISORDERED 2DIMENSIONAL SUPERCONDUCTORS:1||INDIUM FILMS:1||excited state:1||REGIME:1||triplet superconductivity:1||FILM:1||SCHOTTKY DIODES:1||peakdiphump structure:1||Kondo effect:1||REENTRANCE:1||Graphene:1||CONTACT:1||BERRYS PHASE:1||2DIMENSIONAL SUPERCONDUCTORS:1||Coulomb diamond:1||magnetic domain:1||spin injection:1||RESONANCE:1||plasma excitation modes:1||FLOW:1||OVERDOPED BI2SR2CACU2O8+DELTA:1||hole doping:1||chemical synthesis:1||phase transitions:1||superconductors:1||VORTEXGLASS SUPERCONDUCTIVITY:1||Kondorelated model:1||RADIATION:1||DOT:1||NANOBELTS:1||Complementarity:1||Closedloop AharonovBohm interferometer:1||pair breaking:1||interlayer phase fluctuation:1||MgB2 thin film:1||CONFINEMENT:1||WALLED CARBON NANOTUBES:1||TRANSITION:9||VORTICES:8||STATE:7||intrinsic Josephson junctions:7||SINGLECRYSTALS:7||JUNCTIONS:5||MODES:5||SUPERCURRENT:5||SUPERCONDUCTOR:5||CONDUCTANCE:5||HIGHTEMPERATURE SUPERCONDUCTORS:5||TRANSPORT:5||PHASE:5||FILMS:4||LOCALIZATION:4||SINGLE DIRAC CONE:4||WIRES:4||MAGNETICFIELD:4||STEPS:3||ELECTRONS:3||proximity effect:3||MODEL:3||ARRAYS:3||INTERFERENCE:3||fluxon dynamics:3||HETEROSTRUCTURES:3||INSULATOR:3||Andreev reflection:3||electronic transport:3||FISKE:3||superconductor:2||ZnO:2||quantum point contact:2||METAL:2||DYNAMICS:2||interlayer Josephson coupling:2||SUPERCONDUCTORS:2||YBA2CU3O7DELTA:2||LAYER:2||DOTS:2||quantum dot:2||Article:2||TRANSISTORS:2||CARBON NANOTUBES:2||GAP:2||MECHANISM:2||LINE:2||GIANT SHAPIRO STEPS:2||LAYERS:2||electron energy loss spectroscopy:2||physical phenomena:2||scanning electron microscopy:2||HGTE QUANTUMWELLS:2||BI2TE3:2||SPECTROSCOPY:2||PNJUNCTIONS:2||spinpolarized tunneling:2||INTRINSIC JOSEPHSONJUNCTIONS:2||FIELDS:2||positive magnetoresistance:2||dilute magnetic semiconductor:2||magnetic field:2||scanning transmission electron microscopy:2||QUANTUM OSCILLATIONS:2||TRANSPORTPROPERTIES:2||surface pair current:2||MAGNETORESISTANCE:2||NANORIBBONS:2||INSTABILITY:2||ANDREEV REFLECTION:2||microwave irradiation:2||vertical graphene josephson junction:2||BI2SE3:2||CONDUCTIVITY:2||highTc superconductors:2||DIMENSIONAL ELECTRONGAS:2||graphene:2||Topological insulators:2||Josephson coupling Fraunhofer interference pattern:2||FERROMAGNET:2||DEPENDENCE:2||DETECTOR:2||COHERENCE:2||INJECTION:2||GRAPHENE:1||JOSEPHSONJUNCTIONS:1||LAYERED SUPERCONDUCTOR:1||mode splitting:1||BEHAVIOR:1||spinpolarized transport:1||SUPERCONDUCTING TRANSITION:1||microwave response:1||PSEUDOGAP:1||phase coherence:1||TRANSITIONS:1||Long Josephson junction:1||Charge detection:1||collective resonance modes:1||plasma oscillation modes:1||Superconducting proximity effect:1||Iron pnictide superconductor:1||McMillanRowell oscillations:1||ferromagnetic microstructure:1||superradiant state:1||VOLTAGE:1||branch splitting:1||TENSOR:1||INTERCALATION:1||insitu fabrication:1||NDGAO3:1||DISORDERED METALS:1||GAUGE GLASS:1||LOWTEMPERATURE TRANSPORT:1||spontaneous spin polarization model:1||BIAS:1||emission of electromagnetic waves:1||YBA2CU3O7/PRBA2CU3O7 SUPERLATTICES:1||BOHM:1||SHAPIRO STEPS:1||superconductor/ferromagnet interface:1||OXIDE:1||ANDREEVREFLECTION:1||SinFeAsO single crystal:1||COLLECTIVE MOTION:1||ANGULARDEPENDENCE:1||SUPERCONDUCTIVITY:1||BILAYER GRAPHENE:1||PHOTOLUMINESCENT PROPERTIES:1||SUPERCONDUCTING WEAK LINKS:1||intrinsic Josephson junctions geometrical resonance:1||intrinsic Josephson junction:1||MESOSCOPIC SPINVALVE:1||Bi2212 single crystals:1||intrinsic junctions:1||ANDREEV REFLECTIONS:1||normalmetal/superconductor interface:1||IBI2SR2CACU2OY:1||THERMAL FLUCTUATIONS:1||MIXED STATE:1||BI2.15SR1.85CACU2O8+DELTA:1||intrinsic Josephson effects:1||CACUO:1||QUANTUM POINT CONTACTS:1||resonant tunneling state:1||coherence length:1||NANOWIRE:1||GATES:1||Phase line:1||Thermal activation:1||QUANTUMDOT:1||superconducting proximity effect:1||Andreev interferometer:1||WIRE:1||Josephsonvortexflow branches:1||Bi2212 cuprates:1||LATTICE:1||demannetization effect:1||SUPERCONDUCTING MIRRORS:1||GAS:1||VALLEY TRANSPORT:1||ELECTRODES:1||DEPENDENT TRANSPORT:1||BORNOPPENHEIMER APPROXIMATION:1||collective plasma oscillations:1||fluxon resonance steps:1||STACKS:1||COLLECTIVE DYNAMICS:1||PAIRING SYMMETRY:1||MUON SPIN ROTATION:1||DIMENSIONAL CROSSOVER:1||Bi2Sr2CaCu2Oy highTc superconductors:1||heterojunctions:1||nanostructures:1||surfaces and interfaces:1||QUANTUM TRANSPORT:1||MICROJUNCTIONS:1||RESONATORS:1||STATES:1||FIELD:1||FLUCTUATIONS:1||SCATTERING:1||mode splitting of Josephson vortexflow branches:1||2D superconductivity:1||TRANSISTOR:1||ENERGYGAP:1||SUPERLATTICES:1||IRONBASED SUPERCONDUCTORS:1||PHASEDEPENDENT RESISTANCE:1||QUANTUM PHASETRANSITIONS:1||ELECTRICFIELD:1||HIGH MAGNETICFIELDS:1||NANOWIRE HETEROSTRUCTURES:1||ZNO:1||pair breaking.:1||SUPERCONDUCTING PB:1||domain formation:1||FORCE MICROSCOPY:1||RELAXATION:1||PLASMA RESONANCE:1||coupled Josephson junctions:1||COPPEROXIDE SUPERCONDUCTORS:1||CROSSOVER:1||SIMULATIONS:1||LOWTEMPERATURE:1||CONDUCTORS:1||METALINSULATORTRANSITION:1||SEMICONDUCTOR:1||FIELDEFFECT TRANSISTORS:1||ZEROVOLTAGE STATE:1||constanttemperature interlayer tunneling spectroscopy:1||Josephson supercurrent:1||BIPOLAR SUPERCURRENT:1||Interaction between Josephson and pancake vortices:1||flux jump:1||coaxial heterojunction nanorod:1||Natural Josephson coupling:1||BI2SR2CACU2O8+DELTA:1||VORTEX FLOW:1||TC SUPERCONDUCTORS:1||charge imbalance:1||Andreev diffractometer:1||intercalation:1||surface junction:1||Bi2212:1||tunnelling:1||GRAPHITE:1||GROWTH:1||collective transverse plasma modes:1||GAN:1||Macroscopic quantum tunneling:1||Fluctuation conductivity:1||Abovegap conductance jump:1||Josephson vortex motion:1||Intrinsic Josephson junctions:1||LAYERED SUPERCONDUCTORS:1||BI2SR2CACU2O8+Y:1||INTERFACES:1||BREAKDOWN:1||SYSTEMS:1||Anisotropy ratio:1||Josephson vortex:1||spin relaxation in superconductors:1||bibased single crystals:1||MESOSCOPIC PROXIMITY SUPERCONDUCTOR:1||reentrance of conductance:1||interlayer pair tunneling:1||JOSEPHSON:1||DISORDERED 2DIMENSIONAL SUPERCONDUCTORS:1||INDIUM FILMS:1||excited state:1||REGIME:1||triplet superconductivity:1||FILM:1||SCHOTTKY DIODES:1||peakdiphump structure:1||Kondo effect:1||REENTRANCE:1||Graphene:1||CONTACT:1||BERRYS PHASE:1||2DIMENSIONAL SUPERCONDUCTORS:1||Coulomb diamond:1||magnetic domain:1||spin injection:1||RESONANCE:1||plasma excitation modes:1||FLOW:1||OVERDOPED BI2SR2CACU2O8+DELTA:1||hole doping:1||chemical synthesis:1||phase transitions:1||superconductors:1||VORTEXGLASS SUPERCONDUCTIVITY:1||Kondorelated model:1||RADIATION:1||DOT:1||NANOBELTS:1||Complementarity:1||Closedloop AharonovBohm interferometer:1||pair breaking:1||interlayer phase fluctuation:1||MgB2 thin film:1||CONFINEMENT:1||WALLED CARBON NANOTUBES:1||TRANSITION:9||VORTICES:8||STATE:7||intrinsic Josephson junctions:7||SINGLECRYSTALS:7||JUNCTIONS:5||MODES:5||SUPERCURRENT:5||SUPERCONDUCTOR:5||CONDUCTANCE:5||HIGHTEMPERATURE SUPERCONDUCTORS:5||TRANSPORT:5||PHASE:5||FILMS:4||LOCALIZATION:4||SINGLE DIRAC CONE:4||WIRES:4||MAGNETICFIELD:4||STEPS:3||ELECTRONS:3||proximity effect:3||MODEL:3||ARRAYS:3||INTERFERENCE:3||fluxon dynamics:3||HETEROSTRUCTURES:3||INSULATOR:3||Andreev reflection:3||electronic transport:3||FISKE:3||superconductor:2||ZnO:2||quantum point contact:2||METAL:2||DYNAMICS:2||interlayer Josephson coupling:2||SUPERCONDUCTORS:2||YBA2CU3O7DELTA:2||LAYER:2||DOTS:2||quantum dot:2||Article:2||TRANSISTORS:2||CARBON NANOTUBES:2||GAP:2||MECHANISM:2||LINE:2||GIANT SHAPIRO STEPS:2||LAYERS:2||electron energy loss spectroscopy:2||physical phenomena:2||scanning electron microscopy:2||HGTE QUANTUMWELLS:2||BI2TE3:2||SPECTROSCOPY:2||PNJUNCTIONS:2||spinpolarized tunneling:2||INTRINSIC JOSEPHSONJUNCTIONS:2||FIELDS:2||positive magnetoresistance:2||dilute magnetic semiconductor:2||magnetic field:2||scanning transmission electron microscopy:2||QUANTUM OSCILLATIONS:2||TRANSPORTPROPERTIES:2||surface pair current:2||MAGNETORESISTANCE:2||NANORIBBONS:2||INSTABILITY:2||ANDREEV REFLECTION:2||microwave irradiation:2||vertical graphene josephson junction:2||BI2SE3:2||CONDUCTIVITY:2||highTc superconductors:2||DIMENSIONAL ELECTRONGAS:2||graphene:2||Topological insulators:2||Josephson coupling Fraunhofer interference pattern:2||FERROMAGNET:2||DEPENDENCE:2||DETECTOR:2||COHERENCE:2||INJECTION:2||GRAPHENE:1||JOSEPHSONJUNCTIONS:1||LAYERED SUPERCONDUCTOR:1||mode splitting:1||BEHAVIOR:1||spinpolarized transport:1||SUPERCONDUCTING TRANSITION:1||microwave response:1||PSEUDOGAP:1||phase coherence:1||TRANSITIONS:1||Long Josephson junction:1||Charge detection:1||collective resonance modes:1||plasma oscillation modes:1||Superconducting proximity effect:1||Iron pnictide superconductor:1||McMillanRowell oscillations:1||ferromagnetic microstructure:1||superradiant state:1||VOLTAGE:1||branch splitting:1||TENSOR:1||INTERCALATION:1||insitu fabrication:1||NDGAO3:1||DISORDERED METALS:1||GAUGE GLASS:1||LOWTEMPERATURE TRANSPORT:1||spontaneous spin polarization model:1||BIAS:1||emission of electromagnetic waves:1||YBA2CU3O7/PRBA2CU3O7 SUPERLATTICES:1||BOHM:1||SHAPIRO STEPS:1||superconductor/ferromagnet interface:1||OXIDE:1||ANDREEVREFLECTION:1||SinFeAsO single crystal:1||COLLECTIVE MOTION:1||ANGULARDEPENDENCE:1||SUPERCONDUCTIVITY:1||BILAYER GRAPHENE:1||PHOTOLUMINESCENT PROPERTIES:1||SUPERCONDUCTING WEAK LINKS:1||intrinsic Josephson junctions geometrical resonance:1||intrinsic Josephson junction:1||MESOSCOPIC SPINVALVE:1||Bi2212 single crystals:1||intrinsic junctions:1||ANDREEV REFLECTIONS:1||normalmetal/superconductor interface:1||IBI2SR2CACU2OY:1||THERMAL FLUCTUATIONS:1||MIXED STATE:1||BI2.15SR1.85CACU2O8+DELTA:1||intrinsic Josephson effects:1||CACUO:1||QUANTUM POINT CONTACTS:1||resonant tunneling state:1||coherence length:1||NANOWIRE:1||GATES:1||Phase line:1||Thermal activation:1||QUANTUMDOT:1||superconducting proximity effect:1||Andreev interferometer:1||WIRE:1||Josephsonvortexflow branches:1||Bi2212 cuprates:1||LATTICE:1||demannetization effect:1||SUPERCONDUCTING MIRRORS:1||GAS:1||VALLEY TRANSPORT:1||ELECTRODES:1||DEPENDENT TRANSPORT:1||BORNOPPENHEIMER APPROXIMATION:1||collective plasma oscillations:1||fluxon resonance steps:1||STACKS:1||COLLECTIVE DYNAMICS:1||PAIRING SYMMETRY:1||MUON SPIN ROTATION:1||DIMENSIONAL CROSSOVER:1||Bi2Sr2CaCu2Oy highTc superconductors:1||heterojunctions:1||nanostructures:1||surfaces and interfaces:1||QUANTUM TRANSPORT:1||MICROJUNCTIONS:1||RESONATORS:1||STATES:1||FIELD:1||FLUCTUATIONS:1||SCATTERING:1||mode splitting of Josephson vortexflow branches:1||2D superconductivity:1||TRANSISTOR:1||ENERGYGAP:1||SUPERLATTICES:1||IRONBASED SUPERCONDUCTORS:1||PHASEDEPENDENT RESISTANCE:1||QUANTUM PHASETRANSITIONS:1||ELECTRICFIELD:1||HIGH MAGNETICFIELDS:1||NANOWIRE HETEROSTRUCTURES:1||ZNO:1||pair breaking.:1||SUPERCONDUCTING PB:1||domain formation:1||FORCE MICROSCOPY:1||RELAXATION:1||PLASMA RESONANCE:1||coupled Josephson junctions:1||COPPEROXIDE SUPERCONDUCTORS:1||CROSSOVER:1||SIMULATIONS:1||LOWTEMPERATURE:1||CONDUCTORS:1||METALINSULATORTRANSITION:1||SEMICONDUCTOR:1||FIELDEFFECT TRANSISTORS:1||ZEROVOLTAGE STATE:1||constanttemperature interlayer tunneling spectroscopy:1||Josephson supercurrent:1||BIPOLAR SUPERCURRENT:1||Interaction between Josephson and pancake vortices:1||flux jump:1||coaxial heterojunction nanorod:1||Natural Josephson coupling:1||BI2SR2CACU2O8+DELTA:1||VORTEX FLOW:1||TC SUPERCONDUCTORS:1||charge imbalance:1||Andreev diffractometer:1||intercalation:1||surface junction:1||Bi2212:1||tunnelling:1||GRAPHITE:1||GROWTH:1||collective transverse plasma modes:1||GAN:1||Macroscopic quantum tunneling:1||Fluctuation conductivity:1||Abovegap conductance jump:1||Josephson vortex motion:1||Intrinsic Josephson junctions:1||LAYERED SUPERCONDUCTORS:1||BI2SR2CACU2O8+Y:1||INTERFACES:1||BREAKDOWN:1||SYSTEMS:1||Anisotropy ratio:1||Josephson vortex:1||spin relaxation in superconductors:1||bibased single crystals:1||MESOSCOPIC PROXIMITY SUPERCONDUCTOR:1||reentrance of conductance:1||interlayer pair tunneling:1||JOSEPHSON:1||DISORDERED 2DIMENSIONAL SUPERCONDUCTORS:1||INDIUM FILMS:1||excited state:1||REGIME:1||triplet superconductivity:1||FILM:1||SCHOTTKY DIODES:1||peakdiphump structure:1||Kondo effect:1||REENTRANCE:1||Graphene:1||CONTACT:1||BERRYS PHASE:1||2DIMENSIONAL SUPERCONDUCTORS:1||Coulomb diamond:1||magnetic domain:1||spin injection:1||RESONANCE:1||plasma excitation modes:1||FLOW:1||OVERDOPED BI2SR2CACU2O8+DELTA:1||hole doping:1||chemical synthesis:1||phase transitions:1||superconductors:1||VORTEXGLASS SUPERCONDUCTIVITY:1||Kondorelated model:1||RADIATION:1||DOT:1||NANOBELTS:1||Complementarity:1||Closedloop AharonovBohm interferometer:1||pair breaking:1||interlayer phase fluctuation:1||MgB2 thin film:1||CONFINEMENT:1||WALLED CARBON NANOTUBES:1||TRANSITION:9||VORTICES:8||STATE:7||intrinsic Josephson junctions:7||SINGLECRYSTALS:7||JUNCTIONS:5||MODES:5||SUPERCURRENT:5||SUPERCONDUCTOR:5||CONDUCTANCE:5||HIGHTEMPERATURE SUPERCONDUCTORS:5||TRANSPORT:5||PHASE:5||FILMS:4||LOCALIZATION:4||SINGLE DIRAC CONE:4||WIRES:4||MAGNETICFIELD:4||STEPS:3||ELECTRONS:3||proximity effect:3||MODEL:3||ARRAYS:3||INTERFERENCE:3||fluxon dynamics:3||HETEROSTRUCTURES:3||INSULATOR:3||Andreev reflection:3||electronic transport:3||FISKE:3||superconductor:2||ZnO:2||quantum point contact:2||METAL:2||DYNAMICS:2||interlayer Josephson coupling:2||SUPERCONDUCTORS:2||YBA2CU3O7DELTA:2||LAYER:2||DOTS:2||quantum dot:2||Article:2||TRANSISTORS:2||CARBON NANOTUBES:2||GAP:2||MECHANISM:2||LINE:2||GIANT SHAPIRO STEPS:2||LAYERS:2||electron energy loss spectroscopy:2||physical phenomena:2||scanning electron microscopy:2||HGTE QUANTUMWELLS:2||BI2TE3:2||SPECTROSCOPY:2||PNJUNCTIONS:2||spinpolarized tunneling:2||INTRINSIC JOSEPHSONJUNCTIONS:2||FIELDS:2||positive magnetoresistance:2||dilute magnetic semiconductor:2||magnetic field:2||scanning transmission electron microscopy:2||QUANTUM OSCILLATIONS:2||TRANSPORTPROPERTIES:2||surface pair current:2||MAGNETORESISTANCE:2||NANORIBBONS:2||INSTABILITY:2||ANDREEV REFLECTION:2||microwave irradiation:2||vertical graphene josephson junction:2||BI2SE3:2||CONDUCTIVITY:2||highTc superconductors:2||DIMENSIONAL ELECTRONGAS:2||graphene:2||Topological insulators:2||Josephson coupling Fraunhofer interference pattern:2||FERROMAGNET:2||DEPENDENCE:2||DETECTOR:2||COHERENCE:2||INJECTION:2||GRAPHENE:1||JOSEPHSONJUNCTIONS:1||LAYERED SUPERCONDUCTOR:1||mode splitting:1||BEHAVIOR:1||spinpolarized transport:1||SUPERCONDUCTING TRANSITION:1||microwave response:1||PSEUDOGAP:1||phase coherence:1||TRANSITIONS:1||Long Josephson junction:1||Charge detection:1||collective resonance modes:1||plasma oscillation modes:1||Superconducting proximity effect:1||Iron pnictide superconductor:1||McMillanRowell oscillations:1||ferromagnetic microstructure:1||superradiant state:1||VOLTAGE:1||branch splitting:1||TENSOR:1||INTERCALATION:1||insitu fabrication:1||NDGAO3:1||DISORDERED METALS:1||GAUGE GLASS:1||LOWTEMPERATURE TRANSPORT:1||spontaneous spin polarization model:1||BIAS:1||emission of electromagnetic waves:1||YBA2CU3O7/PRBA2CU3O7 SUPERLATTICES:1||BOHM:1||SHAPIRO STEPS:1||superconductor/ferromagnet interface:1||OXIDE:1||ANDREEVREFLECTION:1||SinFeAsO single crystal:1||COLLECTIVE MOTION:1||ANGULARDEPENDENCE:1||SUPERCONDUCTIVITY:1||BILAYER GRAPHENE:1||PHOTOLUMINESCENT PROPERTIES:1||SUPERCONDUCTING WEAK LINKS:1||intrinsic Josephson junctions geometrical resonance:1||intrinsic Josephson junction:1||MESOSCOPIC SPINVALVE:1||Bi2212 single crystals:1||intrinsic junctions:1||ANDREEV REFLECTIONS:1||normalmetal/superconductor interface:1||IBI2SR2CACU2OY:1||THERMAL FLUCTUATIONS:1||MIXED STATE:1||BI2.15SR1.85CACU2O8+DELTA:1||intrinsic Josephson effects:1||CACUO:1||QUANTUM POINT CONTACTS:1||resonant tunneling state:1||coherence length:1||NANOWIRE:1||GATES:1||Phase line:1||Thermal activation:1||QUANTUMDOT:1||superconducting proximity effect:1||Andreev interferometer:1||WIRE:1||Josephsonvortexflow branches:1||Bi2212 cuprates:1||LATTICE:1||demannetization effect:1||SUPERCONDUCTING MIRRORS:1||GAS:1||VALLEY TRANSPORT:1||ELECTRODES:1||DEPENDENT TRANSPORT:1||BORNOPPENHEIMER APPROXIMATION:1||collective plasma oscillations:1||fluxon resonance steps:1||STACKS:1||COLLECTIVE DYNAMICS:1||PAIRING SYMMETRY:1||MUON SPIN ROTATION:1||DIMENSIONAL CROSSOVER:1||Bi2Sr2CaCu2Oy highTc superconductors:1||heterojunctions:1||nanostructures:1||surfaces and interfaces:1||QUANTUM TRANSPORT:1||MICROJUNCTIONS:1||RESONATORS:1||STATES:1||FIELD:1||FLUCTUATIONS:1||SCATTERING:1||mode splitting of Josephson vortexflow branches:1||2D superconductivity:1||TRANSISTOR:1||ENERGYGAP:1||SUPERLATTICES:1||IRONBASED SUPERCONDUCTORS:1||PHASEDEPENDENT RESISTANCE:1||QUANTUM PHASETRANSITIONS:1||ELECTRICFIELD:1||HIGH MAGNETICFIELDS:1||NANOWIRE HETEROSTRUCTURES:1||ZNO:1||pair breaking.:1||SUPERCONDUCTING PB:1||domain formation:1||FORCE MICROSCOPY:1||RELAXATION:1||PLASMA RESONANCE:1||coupled Josephson junctions:1||COPPEROXIDE SUPERCONDUCTORS:1||CROSSOVER:1||SIMULATIONS:1||LOWTEMPERATURE:1||CONDUCTORS:1||METALINSULATORTRANSITION:1||SEMICONDUCTOR:1||FIELDEFFECT TRANSISTORS:1||ZEROVOLTAGE STATE:1||constanttemperature interlayer tunneling spectroscopy:1||Josephson supercurrent:1||BIPOLAR SUPERCURRENT:1||Interaction between Josephson and pancake vortices:1||flux jump:1||coaxial heterojunction nanorod:1||Natural Josephson coupling:1||BI2SR2CACU2O8+DELTA:1||VORTEX FLOW:1||TC SUPERCONDUCTORS:1||charge imbalance:1||Andreev diffractometer:1||intercalation:1||surface junction:1||Bi2212:1||tunnelling:1||GRAPHITE:1||GROWTH:1||collective transverse plasma modes:1||GAN:1||Macroscopic quantum tunneling:1||Fluctuation conductivity:1||Abovegap conductance jump:1||Josephson vortex motion:1||Intrinsic Josephson junctions:1||LAYERED SUPERCONDUCTORS:1||BI2SR2CACU2O8+Y:1||INTERFACES:1||BREAKDOWN:1||SYSTEMS:1||Anisotropy ratio:1||Josephson vortex:1||spin relaxation in superconductors:1||bibased single crystals:1||MESOSCOPIC PROXIMITY SUPERCONDUCTOR:1||reentrance of conductance:1||interlayer pair tunneling:1||JOSEPHSON:1||DISORDERED 2DIMENSIONAL SUPERCONDUCTORS:1||INDIUM FILMS:1||excited state:1||REGIME:1||triplet superconductivity:1||FILM:1||SCHOTTKY DIODES:1||peakdiphump structure:1||Kondo effect:1||REENTRANCE:1||Graphene:1||CONTACT:1||BERRYS PHASE:1||2DIMENSIONAL SUPERCONDUCTORS:1||Coulomb diamond:1||magnetic domain:1||spin injection:1||RESONANCE:1||plasma excitation modes:1||FLOW:1||OVERDOPED BI2SR2CACU2O8+DELTA:1||hole doping:1||chemical synthesis:1||phase transitions:1||superconductors:1||VORTEXGLASS SUPERCONDUCTIVITY:1||Kondorelated model:1||RADIATION:1||DOT:1||NANOBELTS:1||Complementarity:1||Closedloop AharonovBohm interferometer:1||pair breaking:1||interlayer phase fluctuation:1||MgB2 thin film:1||CONFINEMENT:1||WALLED CARBON NANOTUBES:1||TRANSITION:9||VORTICES:8||STATE:7||intrinsic Josephson junctions:7||SINGLECRYSTALS:7||JUNCTIONS:5||MODES:5||SUPERCURRENT:5||SUPERCONDUCTOR:5||CONDUCTANCE:5||HIGHTEMPERATURE SUPERCONDUCTORS:5||TRANSPORT:5||PHASE:5||FILMS:4||LOCALIZATION:4||SINGLE DIRAC CONE:4||WIRES:4||MAGNETICFIELD:4||STEPS:3||ELECTRONS:3||proximity effect:3||MODEL:3||ARRAYS:3||INTERFERENCE:3||fluxon dynamics:3||HETEROSTRUCTURES:3||INSULATOR:3||Andreev reflection:3||electronic transport:3||FISKE:3||superconductor:2||ZnO:2||quantum point contact:2||METAL:2||DYNAMICS:2||interlayer Josephson coupling:2||SUPERCONDUCTORS:2||YBA2CU3O7DELTA:2||LAYER:2||DOTS:2||quantum dot:2||Article:2||TRANSISTORS:2||CARBON NANOTUBES:2||GAP:2||MECHANISM:2||LINE:2||GIANT SHAPIRO STEPS:2||LAYERS:2||electron energy loss spectroscopy:2||physical phenomena:2||scanning electron microscopy:2||HGTE QUANTUMWELLS:2||BI2TE3:2||SPECTROSCOPY:2||PNJUNCTIONS:2||spinpolarized tunneling:2||INTRINSIC JOSEPHSONJUNCTIONS:2||FIELDS:2||positive magnetoresistance:2||dilute magnetic semiconductor:2||magnetic field:2||scanning transmission electron microscopy:2||QUANTUM OSCILLATIONS:2||TRANSPORTPROPERTIES:2||surface pair current:2||MAGNETORESISTANCE:2||NANORIBBONS:2||INSTABILITY:2||ANDREEV REFLECTION:2||microwave irradiation:2||vertical graphene josephson junction:2||BI2SE3:2||CONDUCTIVITY:2||highTc superconductors:2||DIMENSIONAL ELECTRONGAS:2||graphene:2||Topological insulators:2||Josephson coupling Fraunhofer interference pattern:2||FERROMAGNET:2||DEPENDENCE:2||DETECTOR:2||COHERENCE:2||INJECTION:2||GRAPHENE:1||JOSEPHSONJUNCTIONS:1||LAYERED SUPERCONDUCTOR:1||mode splitting:1||BEHAVIOR:1||spinpolarized transport:1||SUPERCONDUCTING TRANSITION:1||microwave response:1||PSEUDOGAP:1||phase coherence:1||TRANSITIONS:1||Long Josephson junction:1||Charge detection:1||collective resonance modes:1||plasma oscillation modes:1||Superconducting proximity effect:1||Iron pnictide superconductor:1||McMillanRowell oscillations:1||ferromagnetic microstructure:1||superradiant state:1||VOLTAGE:1||branch splitting:1||TENSOR:1||INTERCALATION:1||insitu fabrication:1||NDGAO3:1||DISORDERED METALS:1||GAUGE GLASS:1||LOWTEMPERATURE TRANSPORT:1||spontaneous spin polarization model:1||BIAS:1||emission of electromagnetic waves:1||YBA2CU3O7/PRBA2CU3O7 SUPERLATTICES:1||BOHM:1||SHAPIRO STEPS:1||superconductor/ferromagnet interface:1||OXIDE:1||ANDREEVREFLECTION:1||SinFeAsO single crystal:1||COLLECTIVE MOTION:1||ANGULARDEPENDENCE:1||SUPERCONDUCTIVITY:1||BILAYER GRAPHENE:1||PHOTOLUMINESCENT PROPERTIES:1||SUPERCONDUCTING WEAK LINKS:1||intrinsic Josephson junctions geometrical resonance:1||intrinsic Josephson junction:1||MESOSCOPIC SPINVALVE:1||Bi2212 single crystals:1||intrinsic junctions:1||ANDREEV REFLECTIONS:1||normalmetal/superconductor interface:1||IBI2SR2CACU2OY:1||THERMAL FLUCTUATIONS:1||MIXED STATE:1||BI2.15SR1.85CACU2O8+DELTA:1||intrinsic Josephson effects:1||CACUO:1||QUANTUM POINT CONTACTS:1||resonant tunneling state:1||coherence length:1||NANOWIRE:1||GATES:1||Phase line:1||Thermal activation:1||QUANTUMDOT:1||superconducting proximity effect:1||Andreev interferometer:1||WIRE:1||Josephsonvortexflow branches:1||Bi2212 cuprates:1||LATTICE:1||demannetization effect:1||SUPERCONDUCTING MIRRORS:1||GAS:1||VALLEY TRANSPORT:1||ELECTRODES:1||DEPENDENT TRANSPORT:1||BORNOPPENHEIMER APPROXIMATION:1||collective plasma oscillations:1||fluxon resonance steps:1||STACKS:1||COLLECTIVE DYNAMICS:1||PAIRING SYMMETRY:1||MUON SPIN ROTATION:1||DIMENSIONAL CROSSOVER:1||Bi2Sr2CaCu2Oy highTc superconductors:1||heterojunctions:1||nanostructures:1||surfaces and interfaces:1||QUANTUM TRANSPORT:1||MICROJUNCTIONS:1||RESONATORS:1||STATES:1||FIELD:1||FLUCTUATIONS:1||SCATTERING:1||mode splitting of Josephson vortexflow branches:1||2D superconductivity:1||TRANSISTOR:1||ENERGYGAP:1||SUPERLATTICES:1||IRONBASED SUPERCONDUCTORS:1||PHASEDEPENDENT RESISTANCE:1||QUANTUM PHASETRANSITIONS:1||ELECTRICFIELD:1||HIGH MAGNETICFIELDS:1||NANOWIRE HETEROSTRUCTURES:1||ZNO:1||pair breaking.:1||SUPERCONDUCTING PB:1||domain formation:1||FORCE MICROSCOPY:1||RELAXATION:1||PLASMA RESONANCE:1||coupled Josephson junctions:1||COPPEROXIDE SUPERCONDUCTORS:1||CROSSOVER:1||SIMULATIONS:1||LOWTEMPERATURE:1||CONDUCTORS:1||METALINSULATORTRANSITION:1||SEMICONDUCTOR:1||FIELDEFFECT TRANSISTORS:1||ZEROVOLTAGE STATE:1||constanttemperature interlayer tunneling spectroscopy:1||Josephson supercurrent:1||BIPOLAR SUPERCURRENT:1||Interaction between Josephson and pancake vortices:1||flux jump:1||coaxial heterojunction nanorod:1||Natural Josephson coupling:1||BI2SR2CACU2O8+DELTA:1||VORTEX FLOW:1||TC SUPERCONDUCTORS:1||charge imbalance:1||Andreev diffractometer:1||intercalation:1||surface junction:1||Bi2212:1||tunnelling:1||GRAPHITE:1||GROWTH:1||collective transverse plasma modes:1||GAN:1||Macroscopic quantum tunneling:1||Fluctuation conductivity:1||Abovegap conductance jump:1||Josephson vortex motion:1||Intrinsic Josephson junctions:1||LAYERED SUPERCONDUCTORS:1||BI2SR2CACU2O8+Y:1||INTERFACES:1||BREAKDOWN:1||SYSTEMS:1||Anisotropy ratio:1||Josephson vortex:1||spin relaxation in superconductors:1||bibased single crystals:1||MESOSCOPIC PROXIMITY SUPERCONDUCTOR:1||reentrance of conductance:1||interlayer pair tunneling:1||JOSEPHSON:1||DISORDERED 2DIMENSIONAL SUPERCONDUCTORS:1||INDIUM FILMS:1||excited state:1||REGIME:1||triplet superconductivity:1||FILM:1||SCHOTTKY DIODES:1||peakdiphump structure:1||Kondo effect:1||REENTRANCE:1||Graphene:1||CONTACT:1||BERRYS PHASE:1||2DIMENSIONAL SUPERCONDUCTORS:1||Coulomb diamond:1||magnetic domain:1||spin injection:1||RESONANCE:1||plasma excitation modes:1||FLOW:1||OVERDOPED BI2SR2CACU2O8+DELTA:1||hole doping:1||chemical synthesis:1||phase transitions:1||superconductors:1||VORTEXGLASS SUPERCONDUCTIVITY:1||Kondorelated model:1||RADIATION:1||DOT:1||NANOBELTS:1||Complementarity:1||Closedloop AharonovBohm interferometer:1||pair breaking:1||interlayer phase fluctuation:1||MgB2 thin film:1||CONFINEMENT:1||WALLED CARBON NANOTUBES:1||TRANSITION:9||VORTICES:8||STATE:7||intrinsic Josephson junctions:7||SINGLECRYSTALS:7||JUNCTIONS:5||MODES:5||SUPERCURRENT:5||SUPERCONDUCTOR:5||CONDUCTANCE:5||HIGHTEMPERATURE SUPERCONDUCTORS:5||TRANSPORT:5||PHASE:5||FILMS:4||LOCALIZATION:4||SINGLE DIRAC CONE:4||WIRES:4||MAGNETICFIELD:4||STEPS:3||ELECTRONS:3||proximity effect:3||MODEL:3||ARRAYS:3||INTERFERENCE:3||fluxon dynamics:3||HETEROSTRUCTURES:3||INSULATOR:3||Andreev reflection:3||electronic transport:3||FISKE:3||superconductor:2||ZnO:2||quantum point contact:2||METAL:2||DYNAMICS:2||interlayer Josephson coupling:2||SUPERCONDUCTORS:2||YBA2CU3O7DELTA:2||LAYER:2||DOTS:2||quantum dot:2||Article:2||TRANSISTORS:2||CARBON NANOTUBES:2||GAP:2||MECHANISM:2||LINE:2||GIANT SHAPIRO STEPS:2||LAYERS:2||electron energy loss spectroscopy:2||physical phenomena:2||scanning electron microscopy:2||HGTE QUANTUMWELLS:2||BI2TE3:2||SPECTROSCOPY:2||PNJUNCTIONS:2||spinpolarized tunneling:2||INTRINSIC JOSEPHSONJUNCTIONS:2||FIELDS:2||positive magnetoresistance:2||dilute magnetic semiconductor:2||magnetic field:2||scanning transmission electron microscopy:2||QUANTUM OSCILLATIONS:2||TRANSPORTPROPERTIES:2||surface pair current:2||MAGNETORESISTANCE:2||NANORIBBONS:2||INSTABILITY:2||ANDREEV REFLECTION:2||microwave irradiation:2||vertical graphene josephson junction:2||BI2SE3:2||CONDUCTIVITY:2||highTc superconductors:2||DIMENSIONAL ELECTRONGAS:2||graphene:2||Topological insulators:2||Josephson coupling Fraunhofer interference pattern:2||FERROMAGNET:2||DEPENDENCE:2||DETECTOR:2||COHERENCE:2||INJECTION:2||GRAPHENE:1||JOSEPHSONJUNCTIONS:1||LAYERED SUPERCONDUCTOR:1||mode splitting:1||BEHAVIOR:1||spinpolarized transport:1||SUPERCONDUCTING TRANSITION:1||microwave response:1||PSEUDOGAP:1||phase coherence:1||TRANSITIONS:1||Long Josephson junction:1||Charge detection:1||collective resonance modes:1||plasma oscillation modes:1||Superconducting proximity effect:1||Iron pnictide superconductor:1||McMillanRowell oscillations:1||ferromagnetic microstructure:1||superradiant state:1||VOLTAGE:1||branch splitting:1||TENSOR:1||INTERCALATION:1||insitu fabrication:1||NDGAO3:1||DISORDERED METALS:1||GAUGE GLASS:1||LOWTEMPERATURE TRANSPORT:1||spontaneous spin polarization model:1||BIAS:1||emission of electromagnetic waves:1||YBA2CU3O7/PRBA2CU3O7 SUPERLATTICES:1||BOHM:1||SHAPIRO STEPS:1||superconductor/ferromagnet interface:1||OXIDE:1||ANDREEVREFLECTION:1||SinFeAsO single crystal:1||COLLECTIVE MOTION:1||ANGULARDEPENDENCE:1||SUPERCONDUCTIVITY:1||BILAYER GRAPHENE:1||PHOTOLUMINESCENT PROPERTIES:1||SUPERCONDUCTING WEAK LINKS:1||intrinsic Josephson junctions geometrical resonance:1||intrinsic Josephson junction:1||MESOSCOPIC SPINVALVE:1||Bi2212 single crystals:1||intrinsic junctions:1||ANDREEV REFLECTIONS:1||normalmetal/superconductor interface:1||IBI2SR2CACU2OY:1||THERMAL FLUCTUATIONS:1||MIXED STATE:1||BI2.15SR1.85CACU2O8+DELTA:1||intrinsic Josephson effects:1||CACUO:1||QUANTUM POINT CONTACTS:1||resonant tunneling state:1||coherence length:1||NANOWIRE:1||GATES:1||Phase line:1||Thermal activation:1||QUANTUMDOT:1||superconducting proximity effect:1||Andreev interferometer:1||WIRE:1||Josephsonvortexflow branches:1||Bi2212 cuprates:1||LATTICE:1||demannetization effect:1||SUPERCONDUCTING MIRRORS:1||GAS:1||VALLEY TRANSPORT:1||ELECTRODES:1||DEPENDENT TRANSPORT:1||BORNOPPENHEIMER APPROXIMATION:1||collective plasma oscillations:1||fluxon resonance steps:1||STACKS:1||COLLECTIVE DYNAMICS:1||PAIRING SYMMETRY:1||MUON SPIN ROTATION:1||DIMENSIONAL CROSSOVER:1||Bi2Sr2CaCu2Oy highTc superconductors:1||heterojunctions:1||nanostructures:1||surfaces and interfaces:1||QUANTUM TRANSPORT:1||MICROJUNCTIONS:1||RESONATORS:1||STATES:1||FIELD:1||FLUCTUATIONS:1||SCATTERING:1||mode splitting of Josephson vortexflow branches:1||2D superconductivity:1||TRANSISTOR:1||ENERGYGAP:1||SUPERLATTICES:1||IRONBASED SUPERCONDUCTORS:1||PHASEDEPENDENT RESISTANCE:1||QUANTUM PHASETRANSITIONS:1||ELECTRICFIELD:1||HIGH MAGNETICFIELDS:1||NANOWIRE HETEROSTRUCTURES:1||ZNO:1||pair breaking.:1||SUPERCONDUCTING PB:1||domain formation:1||FORCE MICROSCOPY:1||RELAXATION:1||PLASMA RESONANCE:1||coupled Josephson junctions:1||COPPEROXIDE SUPERCONDUCTORS:1||CROSSOVER:1||SIMULATIONS:1||LOWTEMPERATURE:1||CONDUCTORS:1||METALINSULATORTRANSITION:1||SEMICONDUCTOR:1||FIELDEFFECT TRANSISTORS:1||ZEROVOLTAGE STATE:1||constanttemperature interlayer tunneling spectroscopy:1||Josephson supercurrent:1||BIPOLAR SUPERCURRENT:1||Interaction between Josephson and pancake vortices:1||flux jump:1||coaxial heterojunction nanorod:1||Natural Josephson coupling:1||BI2SR2CACU2O8+DELTA:1||VORTEX FLOW:1||TC SUPERCONDUCTORS:1||charge imbalance:1||Andreev diffractometer:1||intercalation:1||surface junction:1||Bi2212:1||tunnelling:1||GRAPHITE:1||GROWTH:1||collective transverse plasma modes:1||GAN:1||Macroscopic quantum tunneling:1||Fluctuation conductivity:1||Abovegap conductance jump:1||Josephson vortex motion:1||Intrinsic Josephson junctions:1||LAYERED SUPERCONDUCTORS:1||BI2SR2CACU2O8+Y:1||INTERFACES:1||BREAKDOWN:1||SYSTEMS:1||Anisotropy ratio:1||Josephson vortex:1||spin relaxation in superconductors:1||bibased single crystals:1||MESOSCOPIC PROXIMITY SUPERCONDUCTOR:1||reentrance of conductance:1||interlayer pair tunneling:1||JOSEPHSON:1||DISORDERED 2DIMENSIONAL SUPERCONDUCTORS:1||INDIUM FILMS:1||excited state:1||REGIME:1||triplet superconductivity:1||FILM:1||SCHOTTKY DIODES:1||peakdiphump structure:1||Kondo effect:1||REENTRANCE:1||Graphene:1||CONTACT:1||BERRYS PHASE:1||2DIMENSIONAL SUPERCONDUCTORS:1||Coulomb diamond:1||magnetic domain:1||spin injection:1||RESONANCE:1||plasma excitation modes:1||FLOW:1||OVERDOPED BI2SR2CACU2O8+DELTA:1||hole doping:1||chemical synthesis:1||phase transitions:1||superconductors:1||VORTEXGLASS SUPERCONDUCTIVITY:1||Kondorelated model:1||RADIATION:1||DOT:1||NANOBELTS:1||Complementarity:1||Closedloop AharonovBohm interferometer:1||pair breaking:1||interlayer phase fluctuation:1||MgB2 thin film:1||CONFINEMENT:1||WALLED CARBON NANOTUBES:1||TRANSITION:9||VORTICES:8||STATE:7||intrinsic Josephson junctions:7||SINGLECRYSTALS:7||JUNCTIONS:5||MODES:5||SUPERCURRENT:5||SUPERCONDUCTOR:5||CONDUCTANCE:5||HIGHTEMPERATURE SUPERCONDUCTORS:5||TRANSPORT:5||PHASE:5||FILMS:4||LOCALIZATION:4||SINGLE DIRAC CONE:4||WIRES:4||MAGNETICFIELD:4||STEPS:3||ELECTRONS:3||proximity effect:3||MODEL:3||ARRAYS:3||INTERFERENCE:3||fluxon dynamics:3||HETEROSTRUCTURES:3||INSULATOR:3||Andreev reflection:3||electronic transport:3||FISKE:3||superconductor:2||ZnO:2||quantum point contact:2||METAL:2||DYNAMICS:2||interlayer Josephson coupling:2||SUPERCONDUCTORS:2||YBA2CU3O7DELTA:2||LAYER:2||DOTS:2||quantum dot:2||Article:2||TRANSISTORS:2||CARBON NANOTUBES:2||GAP:2||MECHANISM:2||LINE:2||GIANT SHAPIRO STEPS:2||LAYERS:2||electron energy loss spectroscopy:2||physical phenomena:2||scanning electron microscopy:2||HGTE QUANTUMWELLS:2||BI2TE3:2||SPECTROSCOPY:2||PNJUNCTIONS:2||spinpolarized tunneling:2||INTRINSIC JOSEPHSONJUNCTIONS:2||FIELDS:2||positive magnetoresistance:2||dilute magnetic semiconductor:2||magnetic field:2||scanning transmission electron microscopy:2||QUANTUM OSCILLATIONS:2||TRANSPORTPROPERTIES:2||surface pair current:2||MAGNETORESISTANCE:2||NANORIBBONS:2||INSTABILITY:2||ANDREEV REFLECTION:2||microwave irradiation:2||vertical graphene josephson junction:2||BI2SE3:2||CONDUCTIVITY:2||highTc superconductors:2||DIMENSIONAL ELECTRONGAS:2||graphene:2||Topological insulators:2||Josephson coupling Fraunhofer interference pattern:2||FERROMAGNET:2||DEPENDENCE:2||DETECTOR:2||COHERENCE:2||INJECTION:2||GRAPHENE:1||JOSEPHSONJUNCTIONS:1||LAYERED SUPERCONDUCTOR:1||mode splitting:1||BEHAVIOR:1||spinpolarized transport:1||SUPERCONDUCTING TRANSITION:1||microwave response:1||PSEUDOGAP:1||phase coherence:1||TRANSITIONS:1||Long Josephson junction:1||Charge detection:1||collective resonance modes:1||plasma oscillation modes:1||Superconducting proximity effect:1||Iron pnictide superconductor:1||McMillanRowell oscillations:1||ferromagnetic microstructure:1||superradiant state:1||VOLTAGE:1||branch splitting:1||TENSOR:1||INTERCALATION:1||insitu fabrication:1||NDGAO3:1||DISORDERED METALS:1||GAUGE GLASS:1||LOWTEMPERATURE TRANSPORT:1||spontaneous spin polarization model:1||BIAS:1||emission of electromagnetic waves:1||YBA2CU3O7/PRBA2CU3O7 SUPERLATTICES:1||BOHM:1||SHAPIRO STEPS:1||superconductor/ferromagnet interface:1||OXIDE:1||ANDREEVREFLECTION:1||SinFeAsO single crystal:1||COLLECTIVE MOTION:1||ANGULARDEPENDENCE:1||SUPERCONDUCTIVITY:1||BILAYER GRAPHENE:1||PHOTOLUMINESCENT PROPERTIES:1||SUPERCONDUCTING WEAK LINKS:1||intrinsic Josephson junctions geometrical resonance:1||intrinsic Josephson junction:1||MESOSCOPIC SPINVALVE:1||Bi2212 single crystals:1||intrinsic junctions:1||ANDREEV REFLECTIONS:1||normalmetal/superconductor interface:1||IBI2SR2CACU2OY:1||THERMAL FLUCTUATIONS:1||MIXED STATE:1||BI2.15SR1.85CACU2O8+DELTA:1||intrinsic Josephson effects:1||CACUO:1||QUANTUM POINT CONTACTS:1||resonant tunneling state:1||coherence length:1||NANOWIRE:1||GATES:1||Phase line:1||Thermal activation:1||QUANTUMDOT:1||superconducting proximity effect:1||Andreev interferometer:1||WIRE:1||Josephsonvortexflow branches:1||Bi2212 cuprates:1||LATTICE:1||demannetization effect:1||SUPERCONDUCTING MIRRORS:1||GAS:1||VALLEY TRANSPORT:1||ELECTRODES:1||DEPENDENT TRANSPORT:1||BORNOPPENHEIMER APPROXIMATION:1||collective plasma oscillations:1||fluxon resonance steps:1||STACKS:1||COLLECTIVE DYNAMICS:1||PAIRING SYMMETRY:1||MUON SPIN ROTATION:1||DIMENSIONAL CROSSOVER:1||Bi2Sr2CaCu2Oy highTc superconductors:1||heterojunctions:1||nanostructures:1||surfaces and interfaces:1||QUANTUM TRANSPORT:1||MICROJUNCTIONS:1||RESONATORS:1||STATES:1||FIELD:1||FLUCTUATIONS:1||SCATTERING:1||mode splitting of Josephson vortexflow branches:1||2D superconductivity:1||TRANSISTOR:1||ENERGYGAP:1||SUPERLATTICES:1||IRONBASED SUPERCONDUCTORS:1||PHASEDEPENDENT RESISTANCE:1||QUANTUM PHASETRANSITIONS:1||ELECTRICFIELD:1||HIGH MAGNETICFIELDS:1||NANOWIRE HETEROSTRUCTURES:1||ZNO:1||pair breaking.:1||SUPERCONDUCTING PB:1||domain formation:1||FORCE MICROSCOPY:1||RELAXATION:1||PLASMA RESONANCE:1||coupled Josephson junctions:1||COPPEROXIDE SUPERCONDUCTORS:1||CROSSOVER:1||SIMULATIONS:1||LOWTEMPERATURE:1||CONDUCTORS:1||METALINSULATORTRANSITION:1||SEMICONDUCTOR:1||FIELDEFFECT TRANSISTORS:1||ZEROVOLTAGE STATE:1||constanttemperature interlayer tunneling spectroscopy:1||Josephson supercurrent:1||BIPOLAR SUPERCURRENT:1||Interaction between Josephson and pancake vortices:1||flux jump:1||coaxial heterojunction nanorod:1||Natural Josephson coupling:1||BI2SR2CACU2O8+DELTA:1||VORTEX FLOW:1||TC SUPERCONDUCTORS:1||charge imbalance:1||Andreev diffractometer:1||intercalation:1||surface junction:1||Bi2212:1||tunnelling:1||GRAPHITE:1||GROWTH:1||collective transverse plasma modes:1||GAN:1||Macroscopic quantum tunneling:1||Fluctuation conductivity:1||Abovegap conductance jump:1||Josephson vortex motion:1||Intrinsic Josephson junctions:1||LAYERED SUPERCONDUCTORS:1||BI2SR2CACU2O8+Y:1||INTERFACES:1||BREAKDOWN:1||SYSTEMS:1||Anisotropy ratio:1||Josephson vortex:1||spin relaxation in superconductors:1||bibased single crystals:1||MESOSCOPIC PROXIMITY SUPERCONDUCTOR:1||reentrance of conductance:1||interlayer pair tunneling:1||JOSEPHSON:1||DISORDERED 2DIMENSIONAL SUPERCONDUCTORS:1||INDIUM FILMS:1||excited state:1||REGIME:1||triplet superconductivity:1||FILM:1||SCHOTTKY DIODES:1||peakdiphump structure:1||Kondo effect:1||REENTRANCE:1||Graphene:1||CONTACT:1||BERRYS PHASE:1||2DIMENSIONAL SUPERCONDUCTORS:1||Coulomb diamond:1||magnetic domain:1||spin injection:1||RESONANCE:1||plasma excitation modes:1||FLOW:1||OVERDOPED BI2SR2CACU2O8+DELTA:1||hole doping:1||chemical synthesis:1||phase transitions:1||superconductors:1||VORTEXGLASS SUPERCONDUCTIVITY:1||Kondorelated model:1||RADIATION:1||DOT:1||NANOBELTS:1||Complementarity:1||Closedloop AharonovBohm interferometer:1||pair breaking:1||interlayer phase fluctuation:1||MgB2 thin film:1||CONFINEMENT:1||WALLED CARBON NANOTUBES:1||TRANSITION:9||VORTICES:8||STATE:7||intrinsic Josephson junctions:7||SINGLECRYSTALS:7||JUNCTIONS:5||MODES:5||SUPERCURRENT:5||SUPERCONDUCTOR:5||CONDUCTANCE:5||HIGHTEMPERATURE SUPERCONDUCTORS:5||TRANSPORT:5||PHASE:5||FILMS:4||LOCALIZATION:4||SINGLE DIRAC CONE:4||WIRES:4||MAGNETICFIELD:4||STEPS:3||ELECTRONS:3||proximity effect:3||MODEL:3||ARRAYS:3||INTERFERENCE:3||fluxon dynamics:3||HETEROSTRUCTURES:3||INSULATOR:3||Andreev reflection:3||electronic transport:3||FISKE:3||superconductor:2||ZnO:2||quantum point contact:2||METAL:2||DYNAMICS:2||interlayer Josephson coupling:2||SUPERCONDUCTORS:2||YBA2CU3O7DELTA:2||LAYER:2||DOTS:2||quantum dot:2||Article:2||TRANSISTORS:2||CARBON NANOTUBES:2||GAP:2||MECHANISM:2||LINE:2||GIANT SHAPIRO STEPS:2||LAYERS:2||electron energy loss spectroscopy:2||physical phenomena:2||scanning electron microscopy:2||HGTE QUANTUMWELLS:2||BI2TE3:2||SPECTROSCOPY:2||PNJUNCTIONS:2||spinpolarized tunneling:2||INTRINSIC JOSEPHSONJUNCTIONS:2||FIELDS:2||positive magnetoresistance:2||dilute magnetic semiconductor:2||magnetic field:2||scanning transmission electron microscopy:2||QUANTUM OSCILLATIONS:2||TRANSPORTPROPERTIES:2||surface pair current:2||MAGNETORESISTANCE:2||NANORIBBONS:2||INSTABILITY:2||ANDREEV REFLECTION:2||microwave irradiation:2||vertical graphene josephson junction:2||BI2SE3:2||CONDUCTIVITY:2||highTc superconductors:2||DIMENSIONAL ELECTRONGAS:2||graphene:2||Topological insulators:2||Josephson coupling Fraunhofer interference pattern:2||FERROMAGNET:2||DEPENDENCE:2||DETECTOR:2||COHERENCE:2||INJECTION:2||GRAPHENE:1||JOSEPHSONJUNCTIONS:1||LAYERED SUPERCONDUCTOR:1||mode splitting:1||BEHAVIOR:1||spinpolarized transport:1||SUPERCONDUCTING TRANSITION:1||microwave response:1||PSEUDOGAP:1||phase coherence:1||TRANSITIONS:1||Long Josephson junction:1||Charge detection:1||collective resonance modes:1||plasma oscillation modes:1||Superconducting proximity effect:1||Iron pnictide superconductor:1||McMillanRowell oscillations:1||ferromagnetic microstructure:1||superradiant state:1||VOLTAGE:1||branch splitting:1||TENSOR:1||INTERCALATION:1||insitu fabrication:1||NDGAO3:1||DISORDERED METALS:1||GAUGE GLASS:1||LOWTEMPERATURE TRANSPORT:1||spontaneous spin polarization model:1||BIAS:1||emission of electromagnetic waves:1||YBA2CU3O7/PRBA2CU3O7 SUPERLATTICES:1||BOHM:1||SHAPIRO STEPS:1||superconductor/ferromagnet interface:1||OXIDE:1||ANDREEVREFLECTION:1||SinFeAsO single crystal:1||COLLECTIVE MOTION:1||ANGULARDEPENDENCE:1||SUPERCONDUCTIVITY:1||BILAYER GRAPHENE:1||PHOTOLUMINESCENT PROPERTIES:1||SUPERCONDUCTING WEAK LINKS:1||intrinsic Josephson junctions geometrical resonance:1||intrinsic Josephson junction:1||MESOSCOPIC SPINVALVE:1||Bi2212 single crystals:1||intrinsic junctions:1||ANDREEV REFLECTIONS:1||normalmetal/superconductor interface:1||IBI2SR2CACU2OY:1||THERMAL FLUCTUATIONS:1||MIXED STATE:1||BI2.15SR1.85CACU2O8+DELTA:1||intrinsic Josephson effects:1||CACUO:1||QUANTUM POINT CONTACTS:1||resonant tunneling state:1||coherence length:1||NANOWIRE:1||GATES:1||Phase line:1||Thermal activation:1||QUANTUMDOT:1||superconducting proximity effect:1||Andreev interferometer:1||WIRE:1||Josephsonvortexflow branches:1||Bi2212 cuprates:1||LATTICE:1||demannetization effect:1||SUPERCONDUCTING MIRRORS:1||GAS:1||VALLEY TRANSPORT:1||ELECTRODES:1||DEPENDENT TRANSPORT:1||BORNOPPENHEIMER APPROXIMATION:1||collective plasma oscillations:1||fluxon resonance steps:1||STACKS:1||COLLECTIVE DYNAMICS:1||PAIRING SYMMETRY:1||MUON SPIN ROTATION:1||DIMENSIONAL CROSSOVER:1||Bi2Sr2CaCu2Oy highTc superconductors:1||heterojunctions:1||nanostructures:1||surfaces and interfaces:1||QUANTUM TRANSPORT:1||MICROJUNCTIONS:1||RESONATORS:1||STATES:1||FIELD:1||FLUCTUATIONS:1||SCATTERING:1||mode splitting of Josephson vortexflow branches:1||2D superconductivity:1||TRANSISTOR:1||ENERGYGAP:1||SUPERLATTICES:1||IRONBASED SUPERCONDUCTORS:1||PHASEDEPENDENT RESISTANCE:1||QUANTUM PHASETRANSITIONS:1||ELECTRICFIELD:1||HIGH MAGNETICFIELDS:1||NANOWIRE HETEROSTRUCTURES:1||ZNO:1||pair breaking.:1||SUPERCONDUCTING PB:1||domain formation:1||FORCE MICROSCOPY:1||RELAXATION:1||PLASMA RESONANCE:1||coupled Josephson junctions:1||COPPEROXIDE SUPERCONDUCTORS:1||CROSSOVER:1||SIMULATIONS:1||LOWTEMPERATURE:1||CONDUCTORS:1||METALINSULATORTRANSITION:1||SEMICONDUCTOR:1||FIELDEFFECT TRANSISTORS:1||ZEROVOLTAGE STATE:1||constanttemperature interlayer tunneling spectroscopy:1||Josephson supercurrent:1||BIPOLAR SUPERCURRENT:1||Interaction between Josephson and pancake vortices:1||flux jump:1||coaxial heterojunction nanorod:1||Natural Josephson coupling:1||BI2SR2CACU2O8+DELTA:1||VORTEX FLOW:1||TC SUPERCONDUCTORS:1||charge imbalance:1||Andreev diffractometer:1||intercalation:1||surface junction:1||Bi2212:1||tunnelling:1||GRAPHITE:1||GROWTH:1||collective transverse plasma modes:1||GAN:1||Macroscopic quantum tunneling:1||Fluctuation conductivity:1||Abovegap conductance jump:1||Josephson vortex motion:1||Intrinsic Josephson junctions:1||LAYERED SUPERCONDUCTORS:1||BI2SR2CACU2O8+Y:1||INTERFACES:1||BREAKDOWN:1||SYSTEMS:1||Anisotropy ratio:1||Josephson vortex:1||spin relaxation in superconductors:1||bibased single crystals:1||MESOSCOPIC PROXIMITY SUPERCONDUCTOR:1||reentrance of conductance:1||interlayer pair tunneling:1||JOSEPHSON:1||DISORDERED 2DIMENSIONAL SUPERCONDUCTORS:1||INDIUM FILMS:1||excited state:1||REGIME:1||triplet superconductivity:1||FILM:1||SCHOTTKY DIODES:1||peakdiphump structure:1||Kondo effect:1||REENTRANCE:1||Graphene:1||CONTACT:1||BERRYS PHASE:1||2DIMENSIONAL SUPERCONDUCTORS:1||Coulomb diamond:1||magnetic domain:1||spin injection:1||RESONANCE:1||plasma excitation modes:1||FLOW:1||OVERDOPED BI2SR2CACU2O8+DELTA:1||hole doping:1||chemical synthesis:1||phase transitions:1||superconductors:1||VORTEXGLASS SUPERCONDUCTIVITY:1||Kondorelated model:1||RADIATION:1||DOT:1||NANOBELTS:1||Complementarity:1||Closedloop AharonovBohm interferometer:1||pair breaking:1||interlayer phase fluctuation:1||MgB2 thin film:1||CONFINEMENT:1||WALLED CARBON NANOTUBES:1||TRANSITION:9||VORTICES:8||STATE:7||intrinsic Josephson junctions:7||SINGLECRYSTALS:7||JUNCTIONS:5||MODES:5||SUPERCURRENT:5||SUPERCONDUCTOR:5||CONDUCTANCE:5||HIGHTEMPERATURE SUPERCONDUCTORS:5||TRANSPORT:5||PHASE:5||FILMS:4||LOCALIZATION:4||SINGLE DIRAC CONE:4||WIRES:4||MAGNETICFIELD:4||STEPS:3||ELECTRONS:3||proximity effect:3||MODEL:3||ARRAYS:3||INTERFERENCE:3||fluxon dynamics:3||HETEROSTRUCTURES:3||INSULATOR:3||Andreev reflection:3||electronic transport:3||FISKE:3||superconductor:2||ZnO:2||quantum point contact:2||METAL:2||DYNAMICS:2||interlayer Josephson coupling:2||SUPERCONDUCTORS:2||YBA2CU3O7DELTA:2||LAYER:2||DOTS:2||quantum dot:2||Article:2||TRANSISTORS:2||CARBON NANOTUBES:2||GAP:2||MECHANISM:2||LINE:2||GIANT SHAPIRO STEPS:2||LAYERS:2||electron energy loss spectroscopy:2||physical phenomena:2||scanning electron microscopy:2||HGTE QUANTUMWELLS:2||BI2TE3:2||SPECTROSCOPY:2||PNJUNCTIONS:2||spinpolarized tunneling:2||INTRINSIC JOSEPHSONJUNCTIONS:2||FIELDS:2||positive magnetoresistance:2||dilute magnetic semiconductor:2||magnetic field:2||scanning transmission electron microscopy:2||QUANTUM OSCILLATIONS:2||TRANSPORTPROPERTIES:2||surface pair current:2||MAGNETORESISTANCE:2||NANORIBBONS:2||INSTABILITY:2||ANDREEV REFLECTION:2||microwave irradiation:2||vertical graphene josephson junction:2||BI2SE3:2||CONDUCTIVITY:2||highTc superconductors:2||DIMENSIONAL ELECTRONGAS:2||graphene:2||Topological insulators:2||Josephson coupling Fraunhofer interference pattern:2||FERROMAGNET:2||DEPENDENCE:2||DETECTOR:2||COHERENCE:2||INJECTION:2||GRAPHENE:1||JOSEPHSONJUNCTIONS:1||LAYERED SUPERCONDUCTOR:1||mode splitting:1||BEHAVIOR:1||spinpolarized transport:1||SUPERCONDUCTING TRANSITION:1||microwave response:1||PSEUDOGAP:1||phase coherence:1||TRANSITIONS:1||Long Josephson junction:1||Charge detection:1||collective resonance modes:1||plasma oscillation modes:1||Superconducting proximity effect:1||Iron pnictide superconductor:1||McMillanRowell oscillations:1||ferromagnetic microstructure:1||superradiant state:1||VOLTAGE:1||branch splitting:1||TENSOR:1||INTERCALATION:1||insitu fabrication:1||NDGAO3:1||DISORDERED METALS:1||GAUGE GLASS:1||LOWTEMPERATURE TRANSPORT:1||spontaneous spin polarization model:1||BIAS:1||emission of electromagnetic waves:1||YBA2CU3O7/PRBA2CU3O7 SUPERLATTICES:1||BOHM:1||SHAPIRO STEPS:1||superconductor/ferromagnet interface:1||OXIDE:1||ANDREEVREFLECTION:1||SinFeAsO single crystal:1||COLLECTIVE MOTION:1||ANGULARDEPENDENCE:1||SUPERCONDUCTIVITY:1||BILAYER GRAPHENE:1||PHOTOLUMINESCENT PROPERTIES:1||SUPERCONDUCTING WEAK LINKS:1||intrinsic Josephson junctions geometrical resonance:1||intrinsic Josephson junction:1||MESOSCOPIC SPINVALVE:1||Bi2212 single crystals:1||intrinsic junctions:1||ANDREEV REFLECTIONS:1||normalmetal/superconductor interface:1||IBI2SR2CACU2OY:1||THERMAL FLUCTUATIONS:1||MIXED STATE:1||BI2.15SR1.85CACU2O8+DELTA:1||intrinsic Josephson effects:1||CACUO:1||QUANTUM POINT CONTACTS:1||resonant tunneling state:1||coherence length:1||NANOWIRE:1||GATES:1||Phase line:1||Thermal activation:1||QUANTUMDOT:1||superconducting proximity effect:1||Andreev interferometer:1||WIRE:1||Josephsonvortexflow branches:1||Bi2212 cuprates:1||LATTICE:1||demannetization effect:1||SUPERCONDUCTING MIRRORS:1||GAS:1||VALLEY TRANSPORT:1||ELECTRODES:1||DEPENDENT TRANSPORT:1||BORNOPPENHEIMER APPROXIMATION:1||collective plasma oscillations:1||fluxon resonance steps:1||STACKS:1||COLLECTIVE DYNAMICS:1||PAIRING SYMMETRY:1||MUON SPIN ROTATION:1||DIMENSIONAL CROSSOVER:1||Bi2Sr2CaCu2Oy highTc superconductors:1||heterojunctions:1||nanostructures:1||surfaces and interfaces:1||QUANTUM TRANSPORT:1||MICROJUNCTIONS:1||RESONATORS:1||STATES:1||FIELD:1||FLUCTUATIONS:1||SCATTERING:1||mode splitting of Josephson vortexflow branches:1||2D superconductivity:1||TRANSISTOR:1||ENERGYGAP:1||SUPERLATTICES:1||IRONBASED SUPERCONDUCTORS:1||PHASEDEPENDENT RESISTANCE:1||QUANTUM PHASETRANSITIONS:1||ELECTRICFIELD:1||HIGH MAGNETICFIELDS:1||NANOWIRE HETEROSTRUCTURES:1||ZNO:1||pair breaking.:1||SUPERCONDUCTING PB:1||domain formation:1||FORCE MICROSCOPY:1||RELAXATION:1||PLASMA RESONANCE:1||coupled Josephson junctions:1||COPPEROXIDE SUPERCONDUCTORS:1||CROSSOVER:1||SIMULATIONS:1||LOWTEMPERATURE:1||CONDUCTORS:1||METALINSULATORTRANSITION:1||SEMICONDUCTOR:1||FIELDEFFECT TRANSISTORS:1||ZEROVOLTAGE STATE:1||constanttemperature interlayer tunneling spectroscopy:1||Josephson supercurrent:1||BIPOLAR SUPERCURRENT:1||Interaction between Josephson and pancake vortices:1||flux jump:1||coaxial heterojunction nanorod:1||Natural Josephson coupling:1||BI2SR2CACU2O8+DELTA:1||VORTEX FLOW:1||TC SUPERCONDUCTORS:1||charge imbalance:1||Andreev diffractometer:1||intercalation:1||surface junction:1||Bi2212:1||tunnelling:1||GRAPHITE:1||GROWTH:1||collective transverse plasma modes:1||GAN:1||Macroscopic quantum tunneling:1||Fluctuation conductivity:1||Abovegap conductance jump:1||Josephson vortex motion:1||Intrinsic Josephson junctions:1||LAYERED SUPERCONDUCTORS:1||BI2SR2CACU2O8+Y:1||INTERFACES:1||BREAKDOWN:1||SYSTEMS:1||Anisotropy ratio:1||Josephson vortex:1||spin relaxation in superconductors:1||bibased single crystals:1||MESOSCOPIC PROXIMITY SUPERCONDUCTOR:1||reentrance of conductance:1||interlayer pair tunneling:1||JOSEPHSON:1||DISORDERED 2DIMENSIONAL SUPERCONDUCTORS:1||INDIUM FILMS:1||excited state:1||REGIME:1||triplet superconductivity:1||FILM:1||SCHOTTKY DIODES:1||peakdiphump structure:1||Kondo effect:1||REENTRANCE:1||Graphene:1||CONTACT:1||BERRYS PHASE:1||2DIMENSIONAL SUPERCONDUCTORS:1||Coulomb diamond:1||magnetic domain:1||spin injection:1||RESONANCE:1||plasma excitation modes:1||FLOW:1||OVERDOPED BI2SR2CACU2O8+DELTA:1||hole doping:1||chemical synthesis:1||phase transitions:1||superconductors:1||VORTEXGLASS SUPERCONDUCTIVITY:1||Kondorelated model:1||RADIATION:1||DOT:1||NANOBELTS:1||Complementarity:1||Closedloop AharonovBohm interferometer:1||pair breaking:1||interlayer phase fluctuation:1||MgB2 thin film:1||CONFINEMENT:1||WALLED CARBON NANOTUBES:1||TRANSITION:9||VORTICES:8||STATE:7||intrinsic Josephson junctions:7||SINGLECRYSTALS:7||JUNCTIONS:5||MODES:5||SUPERCURRENT:5||SUPERCONDUCTOR:5||CONDUCTANCE:5||HIGHTEMPERATURE SUPERCONDUCTORS:5||TRANSPORT:5||PHASE:5||FILMS:4||LOCALIZATION:4||SINGLE DIRAC CONE:4||WIRES:4||MAGNETICFIELD:4||STEPS:3||ELECTRONS:3||proximity effect:3||MODEL:3||ARRAYS:3||INTERFERENCE:3||fluxon dynamics:3||HETEROSTRUCTURES:3||INSULATOR:3||Andreev reflection:3||electronic transport:3||FISKE:3||superconductor:2||ZnO:2||quantum point contact:2||METAL:2||DYNAMICS:2||interlayer Josephson coupling:2||SUPERCONDUCTORS:2||YBA2CU3O7DELTA:2||LAYER:2||DOTS:2||quantum dot:2||Article:2||TRANSISTORS:2||CARBON NANOTUBES:2||GAP:2||MECHANISM:2||LINE:2||GIANT SHAPIRO STEPS:2||LAYERS:2||electron energy loss spectroscopy:2||physical phenomena:2||scanning electron microscopy:2||HGTE QUANTUMWELLS:2||BI2TE3:2||SPECTROSCOPY:2||PNJUNCTIONS:2||spinpolarized tunneling:2||INTRINSIC JOSEPHSONJUNCTIONS:2||FIELDS:2||positive magnetoresistance:2||dilute magnetic semiconductor:2||magnetic field:2||scanning transmission electron microscopy:2||QUANTUM OSCILLATIONS:2||TRANSPORTPROPERTIES:2||surface pair current:2||MAGNETORESISTANCE:2||NANORIBBONS:2||INSTABILITY:2||ANDREEV REFLECTION:2||microwave irradiation:2||vertical graphene josephson junction:2||BI2SE3:2||CONDUCTIVITY:2||highTc superconductors:2||DIMENSIONAL ELECTRONGAS:2||graphene:2||Topological insulators:2||Josephson coupling Fraunhofer interference pattern:2||FERROMAGNET:2||DEPENDENCE:2||DETECTOR:2||COHERENCE:2||INJECTION:2||GRAPHENE:1||JOSEPHSONJUNCTIONS:1||LAYERED SUPERCONDUCTOR:1||mode splitting:1||BEHAVIOR:1||spinpolarized transport:1||SUPERCONDUCTING TRANSITION:1||microwave response:1||PSEUDOGAP:1||phase coherence:1||TRANSITIONS:1||Long Josephson junction:1||Charge detection:1||collective resonance modes:1||plasma oscillation modes:1||Superconducting proximity effect:1||Iron pnictide superconductor:1||McMillanRowell oscillations:1||ferromagnetic microstructure:1||superradiant state:1||VOLTAGE:1||branch splitting:1||TENSOR:1||INTERCALATION:1||insitu fabrication:1||NDGAO3:1||DISORDERED METALS:1||GAUGE GLASS:1||LOWTEMPERATURE TRANSPORT:1||spontaneous spin polarization model:1||BIAS:1||emission of electromagnetic waves:1||YBA2CU3O7/PRBA2CU3O7 SUPERLATTICES:1||BOHM:1||SHAPIRO STEPS:1||superconductor/ferromagnet interface:1||OXIDE:1||ANDREEVREFLECTION:1||SinFeAsO single crystal:1||COLLECTIVE MOTION:1||ANGULARDEPENDENCE:1||SUPERCONDUCTIVITY:1||BILAYER GRAPHENE:1||PHOTOLUMINESCENT PROPERTIES:1||SUPERCONDUCTING WEAK LINKS:1||intrinsic Josephson junctions geometrical resonance:1||intrinsic Josephson junction:1||MESOSCOPIC SPINVALVE:1||Bi2212 single crystals:1||intrinsic junctions:1||ANDREEV REFLECTIONS:1||normalmetal/superconductor interface:1||IBI2SR2CACU2OY:1||THERMAL FLUCTUATIONS:1||MIXED STATE:1||BI2.15SR1.85CACU2O8+DELTA:1||intrinsic Josephson effects:1||CACUO:1||QUANTUM POINT CONTACTS:1||resonant tunneling state:1||coherence length:1||NANOWIRE:1||GATES:1||Phase line:1||Thermal activation:1||QUANTUMDOT:1||superconducting proximity effect:1||Andreev interferometer:1||WIRE:1||Josephsonvortexflow branches:1||Bi2212 cuprates:1||LATTICE:1||demannetization effect:1||SUPERCONDUCTING MIRRORS:1||GAS:1||VALLEY TRANSPORT:1||ELECTRODES:1||DEPENDENT TRANSPORT:1||BORNOPPENHEIMER APPROXIMATION:1||collective plasma oscillations:1||fluxon resonance steps:1||STACKS:1||COLLECTIVE DYNAMICS:1||PAIRING SYMMETRY:1||MUON SPIN ROTATION:1||DIMENSIONAL CROSSOVER:1||Bi2Sr2CaCu2Oy highTc superconductors:1||heterojunctions:1||nanostructures:1||surfaces and interfaces:1||QUANTUM TRANSPORT:1||MICROJUNCTIONS:1||RESONATORS:1||STATES:1||FIELD:1||FLUCTUATIONS:1||SCATTERING:1||mode splitting of Josephson vortexflow branches:1||2D superconductivity:1||TRANSISTOR:1||ENERGYGAP:1||SUPERLATTICES:1||IRONBASED SUPERCONDUCTORS:1||PHASEDEPENDENT RESISTANCE:1||QUANTUM PHASETRANSITIONS:1||ELECTRICFIELD:1||HIGH MAGNETICFIELDS:1||NANOWIRE HETEROSTRUCTURES:1||ZNO:1||pair breaking.:1||SUPERCONDUCTING PB:1||domain formation:1||FORCE MICROSCOPY:1||RELAXATION:1||PLASMA RESONANCE:1||coupled Josephson junctions:1||COPPEROXIDE SUPERCONDUCTORS:1||CROSSOVER:1||SIMULATIONS:1||LOWTEMPERATURE:1||CONDUCTORS:1||METALINSULATORTRANSITION:1||SEMICONDUCTOR:1||FIELDEFFECT TRANSISTORS:1||ZEROVOLTAGE STATE:1||constanttemperature interlayer tunneling spectroscopy:1||Josephson supercurrent:1||BIPOLAR SUPERCURRENT:1||Interaction between Josephson and pancake vortices:1||flux jump:1||coaxial heterojunction nanorod:1||Natural Josephson coupling:1||BI2SR2CACU2O8+DELTA:1||VORTEX FLOW:1||TC SUPERCONDUCTORS:1||charge imbalance:1||Andreev diffractometer:1||intercalation:1||surface junction:1||Bi2212:1||tunnelling:1||GRAPHITE:1||GROWTH:1||collective transverse plasma modes:1||GAN:1||Macroscopic quantum tunneling:1||Fluctuation conductivity:1||Abovegap conductance jump:1||Josephson vortex motion:1||Intrinsic Josephson junctions:1||LAYERED SUPERCONDUCTORS:1||BI2SR2CACU2O8+Y:1||INTERFACES:1||BREAKDOWN:1||SYSTEMS:1||Anisotropy ratio:1||Josephson vortex:1||spin relaxation in superconductors:1||bibased single crystals:1||MESOSCOPIC PROXIMITY SUPERCONDUCTOR:1||reentrance of conductance:1||interlayer pair tunneling:1||JOSEPHSON:1||DISORDERED 2DIMENSIONAL SUPERCONDUCTORS:1||INDIUM FILMS:1||excited state:1||REGIME:1||triplet superconductivity:1||FILM:1||SCHOTTKY DIODES:1||peakdiphump structure:1||Kondo effect:1||REENTRANCE:1||Graphene:1||CONTACT:1||BERRYS PHASE:1||2DIMENSIONAL SUPERCONDUCTORS:1||Coulomb diamond:1||magnetic domain:1||spin injection:1||RESONANCE:1||plasma excitation modes:1||FLOW:1||OVERDOPED BI2SR2CACU2O8+DELTA:1||hole doping:1||chemical synthesis:1||phase transitions:1||superconductors:1||VORTEXGLASS SUPERCONDUCTIVITY:1||Kondorelated model:1||RADIATION:1||DOT:1||NANOBELTS:1||Complementarity:1||Closedloop AharonovBohm interferometer:1||pair breaking:1||interlayer phase fluctuation:1||MgB2 thin film:1||CONFINEMENT:1||WALLED CARBON NANOTUBES:1||TRANSITION:9||VORTICES:8||STATE:7||intrinsic Josephson junctions:7||SINGLECRYSTALS:7||JUNCTIONS:5||MODES:5||SUPERCURRENT:5||SUPERCONDUCTOR:5||CONDUCTANCE:5||HIGHTEMPERATURE SUPERCONDUCTORS:5||TRANSPORT:5||PHASE:5||FILMS:4||LOCALIZATION:4||SINGLE DIRAC CONE:4||WIRES:4||MAGNETICFIELD:4||STEPS:3||ELECTRONS:3||proximity effect:3||MODEL:3||ARRAYS:3||INTERFERENCE:3||fluxon dynamics:3||HETEROSTRUCTURES:3||INSULATOR:3||Andreev reflection:3||electronic transport:3||FISKE:3||superconductor:2||ZnO:2||quantum point contact:2||METAL:2||DYNAMICS:2||interlayer Josephson coupling:2||SUPERCONDUCTORS:2||YBA2CU3O7DELTA:2||LAYER:2||DOTS:2||quantum dot:2||Article:2||TRANSISTORS:2||CARBON NANOTUBES:2||GAP:2||MECHANISM:2||LINE:2||GIANT SHAPIRO STEPS:2||LAYERS:2||electron energy loss spectroscopy:2||physical phenomena:2||scanning electron microscopy:2||HGTE QUANTUMWELLS:2||BI2TE3:2||SPECTROSCOPY:2||PNJUNCTIONS:2||spinpolarized tunneling:2||INTRINSIC JOSEPHSONJUNCTIONS:2||FIELDS:2||positive magnetoresistance:2||dilute magnetic semiconductor:2||magnetic field:2||scanning transmission electron microscopy:2||QUANTUM OSCILLATIONS:2||TRANSPORTPROPERTIES:2||surface pair current:2||MAGNETORESISTANCE:2||NANORIBBONS:2||INSTABILITY:2||ANDREEV REFLECTION:2||microwave irradiation:2||vertical graphene josephson junction:2||BI2SE3:2||CONDUCTIVITY:2||highTc superconductors:2||DIMENSIONAL ELECTRONGAS:2||graphene:2||Topological insulators:2||Josephson coupling Fraunhofer interference pattern:2||FERROMAGNET:2||DEPENDENCE:2||DETECTOR:2||COHERENCE:2||INJECTION:2||GRAPHENE:1||JOSEPHSONJUNCTIONS:1||LAYERED SUPERCONDUCTOR:1||mode splitting:1||BEHAVIOR:1||spinpolarized transport:1||SUPERCONDUCTING TRANSITION:1||microwave response:1||PSEUDOGAP:1||phase coherence:1||TRANSITIONS:1||Long Josephson junction:1||Charge detection:1||collective resonance modes:1||plasma oscillation modes:1||Superconducting proximity effect:1||Iron pnictide superconductor:1||McMillanRowell oscillations:1||ferromagnetic microstructure:1||superradiant state:1||VOLTAGE:1||branch splitting:1||TENSOR:1||INTERCALATION:1||insitu fabrication:1||NDGAO3:1||DISORDERED METALS:1||GAUGE GLASS:1||LOWTEMPERATURE TRANSPORT:1||spontaneous spin polarization model:1||BIAS:1||emission of electromagnetic waves:1||YBA2CU3O7/PRBA2CU3O7 SUPERLATTICES:1||BOHM:1||SHAPIRO STEPS:1||superconductor/ferromagnet interface:1||OXIDE:1||ANDREEVREFLECTION:1||SinFeAsO single crystal:1||COLLECTIVE MOTION:1||ANGULARDEPENDENCE:1||SUPERCONDUCTIVITY:1||BILAYER GRAPHENE:1||PHOTOLUMINESCENT PROPERTIES:1||SUPERCONDUCTING WEAK LINKS:1||intrinsic Josephson junctions geometrical resonance:1||intrinsic Josephson junction:1||MESOSCOPIC SPINVALVE:1||Bi2212 single crystals:1||intrinsic junctions:1||ANDREEV REFLECTIONS:1||normalmetal/superconductor interface:1||IBI2SR2CACU2OY:1||THERMAL FLUCTUATIONS:1||MIXED STATE:1||BI2.15SR1.85CACU2O8+DELTA:1||intrinsic Josephson effects:1||CACUO:1||QUANTUM POINT CONTACTS:1||resonant tunneling state:1||coherence length:1||NANOWIRE:1||GATES:1||Phase line:1||Thermal activation:1||QUANTUMDOT:1||superconducting proximity effect:1||Andreev interferometer:1||WIRE:1||Josephsonvortexflow branches:1||Bi2212 cuprates:1||LATTICE:1||demannetization effect:1||SUPERCONDUCTING MIRRORS:1||GAS:1||VALLEY TRANSPORT:1||ELECTRODES:1||DEPENDENT TRANSPORT:1||BORNOPPENHEIMER APPROXIMATION:1||collective plasma oscillations:1||fluxon resonance steps:1||STACKS:1||COLLECTIVE DYNAMICS:1||PAIRING SYMMETRY:1||MUON SPIN ROTATION:1||DIMENSIONAL CROSSOVER:1||Bi2Sr2CaCu2Oy highTc superconductors:1||heterojunctions:1||nanostructures:1||surfaces and interfaces:1||QUANTUM TRANSPORT:1||MICROJUNCTIONS:1||RESONATORS:1||STATES:1||FIELD:1||FLUCTUATIONS:1||SCATTERING:1||mode splitting of Josephson vortexflow branches:1||2D superconductivity:1||TRANSISTOR:1||ENERGYGAP:1||SUPERLATTICES:1||IRONBASED SUPERCONDUCTORS:1||PHASEDEPENDENT RESISTANCE:1||QUANTUM PHASETRANSITIONS:1||ELECTRICFIELD:1||HIGH MAGNETICFIELDS:1||NANOWIRE HETEROSTRUCTURES:1||ZNO:1||pair breaking.:1||SUPERCONDUCTING PB:1||domain formation:1||FORCE MICROSCOPY:1||RELAXATION:1||PLASMA RESONANCE:1||coupled Josephson junctions:1||COPPEROXIDE SUPERCONDUCTORS:1||CROSSOVER:1||SIMULATIONS:1||LOWTEMPERATURE:1||CONDUCTORS:1||METALINSULATORTRANSITION:1||SEMICONDUCTOR:1||FIELDEFFECT TRANSISTORS:1||ZEROVOLTAGE STATE:1||constanttemperature interlayer tunneling spectroscopy:1||Josephson supercurrent:1||BIPOLAR SUPERCURRENT:1||Interaction between Josephson and pancake vortices:1||flux jump:1||coaxial heterojunction nanorod:1||Natural Josephson coupling:1||BI2SR2CACU2O8+DELTA:1||VORTEX FLOW:1||TC SUPERCONDUCTORS:1||charge imbalance:1||Andreev diffractometer:1||intercalation:1||surface junction:1||Bi2212:1||tunnelling:1||GRAPHITE:1||GROWTH:1||collective transverse plasma modes:1||GAN:1||Macroscopic quantum tunneling:1||Fluctuation conductivity:1||Abovegap conductance jump:1||Josephson vortex motion:1||Intrinsic Josephson junctions:1||LAYERED SUPERCONDUCTORS:1||BI2SR2CACU2O8+Y:1||INTERFACES:1||BREAKDOWN:1||SYSTEMS:1||Anisotropy ratio:1||Josephson vortex:1||spin relaxation in superconductors:1||bibased single crystals:1||MESOSCOPIC PROXIMITY SUPERCONDUCTOR:1||reentrance of conductance:1||interlayer pair tunneling:1||JOSEPHSON:1||DISORDERED 2DIMENSIONAL SUPERCONDUCTORS:1||INDIUM FILMS:1||excited state:1||REGIME:1||triplet superconductivity:1||FILM:1||SCHOTTKY DIODES:1||peakdiphump structure:1||Kondo effect:1||REENTRANCE:1||Graphene:1||CONTACT:1||BERRYS PHASE:1||2DIMENSIONAL SUPERCONDUCTORS:1||Coulomb diamond:1||magnetic domain:1||spin injection:1||RESONANCE:1||plasma excitation modes:1||FLOW:1||OVERDOPED BI2SR2CACU2O8+DELTA:1||hole doping:1||chemical synthesis:1||phase transitions:1||superconductors:1||VORTEXGLASS SUPERCONDUCTIVITY:1||Kondorelated model:1|