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MIN, BYUNG IL (민병일)

Dept of Physics(물리학과)

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electronic structure:15||ELECTRONICSTRUCTURE:11||TRANSITIONMETAL COMPOUNDS:10||METALS:10||photoemission:8||SPECTRA:8||MAGNETORESISTANCE:7||FERROMAGNETISM:7||TRANSPORT:7||TRANSITION:6||FILMS:6||THINFILMS:5||TOTALENERGY CALCULATIONS:5||MAGNETICPROPERTIES:5||SUPERCONDUCTIVITY:5||PR:5||LATTICE:4||STATES:4||SPECTROSCOPY:4||FIELD:4||CRYSTALSTRUCTURE:4||PHOTOEMISSION:4||TEMPERATURE:4||TRANSITIONTEMPERATURE:4||XRAYABSORPTION:4||STATE:4||CU:4||BASISSET:4||XAS:4||CRYSTALS:3||EXCITATIONS:3||MOTTHUBBARD SYSTEMS:3||HIGHENERGY SPIN:3||halfmetal:3||INSULATORS:3||LA2CUO4:3||MODEL:3||FLUCTUATIONS:3||CE:3||double exchange:3||TRANSITIONMETALS:3||RESISTIVITY:3||BORON:3||LA1XCAXMNO3:3||IRON:3||PES:3||ANTIMONIDES:2||MgB2:2||ZR METALLIC GLASSES:2||superconductor:2||CRITICALCURRENT DENSITY:2||CIRCULARDICHROISM:2||SEMICONDUCTORS:2||LOCALIZATION:2||INTRABAND OPTICAL CONDUCTIVITY:2||COLOSSAL MAGNETORESISTANCE:2||OXIDATION:2||EXISTENCE:2||COPPER:2||diboride:2||MAGNESIUMDIBORIDE:2||GAP:2||CE COMPOUNDS:2||CORE POLARIZATION:2||magnetoresistance:2||photoemission spectroscopy:2||electronphonon interaction:2||GETTER:2||PD:2||MAGNETISM:2||FECR2S4:2||SUPERCONDUCTING MGB2:2||WIRES:2||ABSORPTION:2||ENERGY:2||LA1XSRXMNO3:2||CONSTANTS:2||polaron:2||charge ordering:2||SCATTERING:2||XRAY PHOTOEMISSION:2||CeNiSn:2||phase diagram:2||PHOTOELECTRON:2||QUADRUPOLAR:2||perovskitemanganites:2||CO:2||SYSTEMS:2||DOPED ZNO:2||LOWFREQUENCY SOUND:2||LA:2||ELECTRONELECTRON SCATTERING:2||AU:2||DENSITYWAVE INSTABILITY:2||FERMISURFACE:2||hybridization:2||VALENCEBAND SATELLITE:2||SULFUR SPINEL:2||Heusler:2||APPROXIMATION:2||superexchange:2||colossal magnetoresistance:2||ALLOYS:2||DEPENDENCE:2||AG:2||electronic structures:2||AUGERSPECTRA:2||CR:2||PARAMETERS:2||DIFFRACTION:2||SEMICONDUCTORMETAL TRANSITION:1||INTERMEDIATEVALENCE:1||SMB6:1||SRRUO3:1||antiperovskite structure with antipolar nature:1||lowenergy twodimensional phonons:1||anatase TiO2:1||La3S4:1||metalinsulator transitions:1||MNO:1||ELECTRONICSTRUCTURES:1||MAGNETIC CIRCULARDICHROISM:1||Density functional theory:1||CeCo2:1||TOPOLARON CROSSOVER:1||EXCHANGE:1||cuprates:1||high Tc cuprates:1||magnetically ordered materials:1||ZNSE:1||Sr2xKxFeMoO6:1||CDW:1||TeCuO3:1||STRUCTURALPROPERTIES:1||MN:1||screening length:1||amorphous Fe:1||WAVE BASISSET:1||SILICONCARBIDE:1||HIGHPRESSURE:1||electronphonon coupling:1||quenched superconductivity:1||CMR perovskite manganites:1||OXIDE:1||polarons:1||synchrotron radiation:1||FULLERIDES:1||RESONANTPHOTOEMISSION:1||Silicon carbide:1||DFT calculation:1||Hybridized bands:1||GIANT MAGNETORESISTANCE:1||PEROVSKITES:1||Raman spectra:1||EXCHANGE ENHANCEMENT:1||SILICON:1||SR2FEMOO6:1||orbital ordering:1||delafossite:1||TITANIUMDIOXIDE:1||electronic structure of disordered solids:1||YFE2:1||Magnetic polaron:1||NA2TI2SB2O:1||STRONGCOUPLED SUPERCONDUCTORS:1||HEAVYFERMION SYSTEMS:1||firstprinciples calculations:1||MECHANISM:1||UNiSn:1||PHOTONIC BANDGAP:1||SINGLE IMPURITY:1||PHONONSPECTRUM:1||FERMISURFACE TOPOLOGY:1||SUPPRESSION:1||RESONANT PHOTOEMISSION:1||METALDOPED PICENE:1||PHOTOIONIZATION CROSSSECTIONS:1||PHOTOINDUCED FERRIMAGNETIC SYSTEMS:1||LINKAGE ISOMERISM:1||CHARGETRANSFER:1||Bilayer Graphene:1||MAGNETICFIELD:1||SPINWAVES:1||rareearth manganese oxides:1||magnonphonon interaction:1||NACO2O4:1||ENERGYBANDS:1||SELFENERGY:1||GAS:1||Fe0.5Cu0.5Cr2S4:1||scanning photoelectron microscopy (SPEM):1||MAGNETIC PROPERTIES:1||Stoner model:1||AMORPHOUS TRANSITIONMETALS:1||SPINGLASS STATES:1||NI:1||LA3NI2B2N3:1||SOLIDS:1||CEO2:1||BAND THEORY:1||dilute magnetic semiconductor:1||pyrochlore:1||Y1XPRXBA2CU3O7DELTA:1||and electronphonon interactions:1||VIBRATIONS:1||RAY PHOTOEMISSION:1||ALKALI CATION:1||Europium:1||colossal magnetoresistance:1||structural stability:1||ENERGYGAP:1||small polaron:1||DOUBLE EXCHANGE:1||Coulomb correlation:1||magnon:1||phonons:1||ELECTRON FERROMAGNETISM:1||CURIETEMPERATURE:1||ARPES:1||PLANEWAVE METHOD:1||Xray absorption spectroscopy (XAS):1||ROOMTEMPERATURE:1||MONOCHALCOGENIDES:1||HEAT:1||UPDSN:1||MOMENTS:1||XRAY ABSORPTION:1||SEMICONDUCTOR:1||Fermi surface nesting:1||optical phonon:1||disordered system:1||dilute magnetic semiconductors:1||CMR manganites:1||PHONONS:1||LATTICEDYNAMICS:1||OXIDES:1||4fphotoemission:1||permanent magnet:1||pseudogap:1||TRANSPORTPROPERTIES:1||ANTIFERROMAGNET:1||(BI,PB)SRCOO SYSTEM:1||semicore correlation:1||POLARIZATION:1||CRYSTAL:1||spinel:1||Xray magnetic circular dichroism (XMCD):1||magnetocapacitance:1||ANATASE:1||TEMPERATURES:1||Pseudogap:1||INTERFACE:1||SUBSTRATE:1||YNI2B2C:1||SAMARIUM SULFIDE:1||strong swave superconductor:1||DOPED MANGANITE:1||SYMMETRY:1||CENISN:1||resonance mode:1||DISORDERED SYSTEM:1||LITHIUM INTERCALATION:1||CUO2 PLANE:1||SURFACE:1||Delafossite:1||ELECTRICALPROPERTIES:1||NIMNSB:1||PTMNSB:1||ROOMTEMPERATURE FERROMAGNETISM:1||RUBIDIUM MANGANESE HEXACYANOFERRATE:1||COLOSSALMAGNETORESISTANCE:1||FINITE TEMPERATURES:1||LAMNO3:1||FE:1||transitionmetal oxides:1||giant magnetoresistance:1||phonon:1||COPPER OXIDES:1||valence states:1||thermoelectric:1||semiconductor:1||CATION DISTRIBUTION:1||FeCr2S4:1||photoemission spectroscopy (PES):1||METALLIC FERROMAGNETISM:1||GRAPHITE:1||SUSCEPTIBILITY:1||UBE13:1||RCrSb3:1||band JahnTeller:1||Ce3S4:1||TiO2:1||PrBa2Cu3O7delta:1||UNTWINNED PRBA2CU3O7:1||AGNIO2:1||HALFMETALLIC FERROMAGNETS:1||CI:1||Energy gap:1||Photoemission:1||Future applications:1||Photoemission measurements:1||Graphene:1||BANDSTRUCTURE:1||TC:1||superconductivity:1||magnetic semiconductors:1||CMRmanganites:1||thin films:1||spin dynamics:1||highTc superconductors:1||ITINERANTELECTRON FERROMAGNETISM:1||SINGLECRYSTALS:1||CeTe2:1||amorphous magnetic materials:1||EPITAXIAL GRAPHENE:1||LAYERED PNICTIDEOXIDES:1||BOROCARBIDE SUPERCONDUCTORS:1||AUGMENTEDWAVE METHOD:1||METALLIC MAGNET UNISN:1||ORIGIN:1||spectrum rearrangement:1||MEANFIELD THEORY:1||MOLECULEBASED MAGNETS:1||METASTABLE STATE:1||INSULATOR:1||magnetic orderin:1||FCC IRON:1||CeRu2:1||TL2MN2O7:1||isotope effect:1||Perovskitemanganites:1||RECURSION METHOD:1||PERPENDICULAR MAGNETICANISOTROPY:1||quasiparticle spectral density:1||GW:1||MANGANESE FERRITE:1||RESONANCE:1||SeCuO3:1||Optical conductivity:1||MASSLESS DIRAC FERMIONS:1||SCHOTTKYBARRIER:1||electronic structure:15||ELECTRONICSTRUCTURE:11||TRANSITIONMETAL COMPOUNDS:10||METALS:10||photoemission:8||SPECTRA:8||MAGNETORESISTANCE:7||FERROMAGNETISM:7||TRANSPORT:7||TRANSITION:6||FILMS:6||THINFILMS:5||TOTALENERGY CALCULATIONS:5||MAGNETICPROPERTIES:5||SUPERCONDUCTIVITY:5||PR:5||LATTICE:4||STATES:4||SPECTROSCOPY:4||FIELD:4||CRYSTALSTRUCTURE:4||PHOTOEMISSION:4||TEMPERATURE:4||TRANSITIONTEMPERATURE:4||XRAYABSORPTION:4||STATE:4||CU:4||BASISSET:4||XAS:4||CRYSTALS:3||EXCITATIONS:3||MOTTHUBBARD SYSTEMS:3||HIGHENERGY SPIN:3||halfmetal:3||INSULATORS:3||LA2CUO4:3||MODEL:3||FLUCTUATIONS:3||CE:3||double exchange:3||TRANSITIONMETALS:3||RESISTIVITY:3||BORON:3||LA1XCAXMNO3:3||IRON:3||PES:3||ANTIMONIDES:2||MgB2:2||ZR METALLIC GLASSES:2||superconductor:2||CRITICALCURRENT DENSITY:2||CIRCULARDICHROISM:2||SEMICONDUCTORS:2||LOCALIZATION:2||INTRABAND OPTICAL CONDUCTIVITY:2||COLOSSAL MAGNETORESISTANCE:2||OXIDATION:2||EXISTENCE:2||COPPER:2||diboride:2||MAGNESIUMDIBORIDE:2||GAP:2||CE COMPOUNDS:2||CORE POLARIZATION:2||magnetoresistance:2||photoemission spectroscopy:2||electronphonon interaction:2||GETTER:2||PD:2||MAGNETISM:2||FECR2S4:2||SUPERCONDUCTING MGB2:2||WIRES:2||ABSORPTION:2||ENERGY:2||LA1XSRXMNO3:2||CONSTANTS:2||polaron:2||charge ordering:2||SCATTERING:2||XRAY PHOTOEMISSION:2||CeNiSn:2||phase diagram:2||PHOTOELECTRON:2||QUADRUPOLAR:2||perovskitemanganites:2||CO:2||SYSTEMS:2||DOPED ZNO:2||LOWFREQUENCY SOUND:2||LA:2||ELECTRONELECTRON SCATTERING:2||AU:2||DENSITYWAVE INSTABILITY:2||FERMISURFACE:2||hybridization:2||VALENCEBAND SATELLITE:2||SULFUR SPINEL:2||Heusler:2||APPROXIMATION:2||superexchange:2||colossal magnetoresistance:2||ALLOYS:2||DEPENDENCE:2||AG:2||electronic structures:2||AUGERSPECTRA:2||CR:2||PARAMETERS:2||DIFFRACTION:2||SEMICONDUCTORMETAL TRANSITION:1||INTERMEDIATEVALENCE:1||SMB6:1||SRRUO3:1||antiperovskite structure with antipolar nature:1||lowenergy twodimensional phonons:1||anatase TiO2:1||La3S4:1||metalinsulator transitions:1||MNO:1||ELECTRONICSTRUCTURES:1||MAGNETIC CIRCULARDICHROISM:1||Density functional theory:1||CeCo2:1||TOPOLARON CROSSOVER:1||EXCHANGE:1||cuprates:1||high Tc cuprates:1||magnetically ordered materials:1||ZNSE:1||Sr2xKxFeMoO6:1||CDW:1||TeCuO3:1||STRUCTURALPROPERTIES:1||MN:1||screening length:1||amorphous Fe:1||WAVE BASISSET:1||SILICONCARBIDE:1||HIGHPRESSURE:1||electronphonon coupling:1||quenched superconductivity:1||CMR perovskite manganites:1||OXIDE:1||polarons:1||synchrotron radiation:1||FULLERIDES:1||RESONANTPHOTOEMISSION:1||Silicon carbide:1||DFT calculation:1||Hybridized bands:1||GIANT MAGNETORESISTANCE:1||PEROVSKITES:1||Raman spectra:1||EXCHANGE ENHANCEMENT:1||SILICON:1||SR2FEMOO6:1||orbital ordering:1||delafossite:1||TITANIUMDIOXIDE:1||electronic structure of disordered solids:1||YFE2:1||Magnetic polaron:1||NA2TI2SB2O:1||STRONGCOUPLED SUPERCONDUCTORS:1||HEAVYFERMION SYSTEMS:1||firstprinciples calculations:1||MECHANISM:1||UNiSn:1||PHOTONIC BANDGAP:1||SINGLE IMPURITY:1||PHONONSPECTRUM:1||FERMISURFACE TOPOLOGY:1||SUPPRESSION:1||RESONANT PHOTOEMISSION:1||METALDOPED PICENE:1||PHOTOIONIZATION CROSSSECTIONS:1||PHOTOINDUCED FERRIMAGNETIC SYSTEMS:1||LINKAGE ISOMERISM:1||CHARGETRANSFER:1||Bilayer Graphene:1||MAGNETICFIELD:1||SPINWAVES:1||rareearth manganese oxides:1||magnonphonon interaction:1||NACO2O4:1||ENERGYBANDS:1||SELFENERGY:1||GAS:1||Fe0.5Cu0.5Cr2S4:1||scanning photoelectron microscopy (SPEM):1||MAGNETIC PROPERTIES:1||Stoner model:1||AMORPHOUS TRANSITIONMETALS:1||SPINGLASS STATES:1||NI:1||LA3NI2B2N3:1||SOLIDS:1||CEO2:1||BAND THEORY:1||dilute magnetic semiconductor:1||pyrochlore:1||Y1XPRXBA2CU3O7DELTA:1||and electronphonon interactions:1||VIBRATIONS:1||RAY PHOTOEMISSION:1||ALKALI CATION:1||Europium:1||colossal magnetoresistance:1||structural stability:1||ENERGYGAP:1||small polaron:1||DOUBLE EXCHANGE:1||Coulomb correlation:1||magnon:1||phonons:1||ELECTRON FERROMAGNETISM:1||CURIETEMPERATURE:1||ARPES:1||PLANEWAVE METHOD:1||Xray absorption spectroscopy (XAS):1||ROOMTEMPERATURE:1||MONOCHALCOGENIDES:1||HEAT:1||UPDSN:1||MOMENTS:1||XRAY ABSORPTION:1||SEMICONDUCTOR:1||Fermi surface nesting:1||optical phonon:1||disordered system:1||dilute magnetic semiconductors:1||CMR manganites:1||PHONONS:1||LATTICEDYNAMICS:1||OXIDES:1||4fphotoemission:1||permanent magnet:1||pseudogap:1||TRANSPORTPROPERTIES:1||ANTIFERROMAGNET:1||(BI,PB)SRCOO SYSTEM:1||semicore correlation:1||POLARIZATION:1||CRYSTAL:1||spinel:1||Xray magnetic circular dichroism (XMCD):1||magnetocapacitance:1||ANATASE:1||TEMPERATURES:1||Pseudogap:1||INTERFACE:1||SUBSTRATE:1||YNI2B2C:1||SAMARIUM SULFIDE:1||strong swave superconductor:1||DOPED MANGANITE:1||SYMMETRY:1||CENISN:1||resonance mode:1||DISORDERED SYSTEM:1||LITHIUM INTERCALATION:1||CUO2 PLANE:1||SURFACE:1||Delafossite:1||ELECTRICALPROPERTIES:1||NIMNSB:1||PTMNSB:1||ROOMTEMPERATURE FERROMAGNETISM:1||RUBIDIUM MANGANESE HEXACYANOFERRATE:1||COLOSSALMAGNETORESISTANCE:1||FINITE TEMPERATURES:1||LAMNO3:1||FE:1||transitionmetal oxides:1||giant magnetoresistance:1||phonon:1||COPPER OXIDES:1||valence states:1||thermoelectric:1||semiconductor:1||CATION DISTRIBUTION:1||FeCr2S4:1||photoemission spectroscopy (PES):1||METALLIC FERROMAGNETISM:1||GRAPHITE:1||SUSCEPTIBILITY:1||UBE13:1||RCrSb3:1||band JahnTeller:1||Ce3S4:1||TiO2:1||PrBa2Cu3O7delta:1||UNTWINNED PRBA2CU3O7:1||AGNIO2:1||HALFMETALLIC FERROMAGNETS:1||CI:1||Energy gap:1||Photoemission:1||Future applications:1||Photoemission measurements:1||Graphene:1||BANDSTRUCTURE:1||TC:1||superconductivity:1||magnetic semiconductors:1||CMRmanganites:1||thin films:1||spin dynamics:1||highTc superconductors:1||ITINERANTELECTRON FERROMAGNETISM:1||SINGLECRYSTALS:1||CeTe2:1||amorphous magnetic materials:1||EPITAXIAL GRAPHENE:1||LAYERED PNICTIDEOXIDES:1||BOROCARBIDE SUPERCONDUCTORS:1||AUGMENTEDWAVE METHOD:1||METALLIC MAGNET UNISN:1||ORIGIN:1||spectrum rearrangement:1||MEANFIELD THEORY:1||MOLECULEBASED MAGNETS:1||METASTABLE STATE:1||INSULATOR:1||magnetic orderin:1||FCC IRON:1||CeRu2:1||TL2MN2O7:1||isotope effect:1||Perovskitemanganites:1||RECURSION METHOD:1||PERPENDICULAR MAGNETICANISOTROPY:1||quasiparticle spectral density:1||GW:1||MANGANESE FERRITE:1||RESONANCE:1||SeCuO3:1||Optical conductivity:1||MASSLESS DIRAC FERMIONS:1||SCHOTTKYBARRIER:1||electronic structure:15||ELECTRONICSTRUCTURE:11||TRANSITIONMETAL COMPOUNDS:10||METALS:10||photoemission:8||SPECTRA:8||MAGNETORESISTANCE:7||FERROMAGNETISM:7||TRANSPORT:7||TRANSITION:6||FILMS:6||THINFILMS:5||TOTALENERGY CALCULATIONS:5||MAGNETICPROPERTIES:5||SUPERCONDUCTIVITY:5||PR:5||LATTICE:4||STATES:4||SPECTROSCOPY:4||FIELD:4||CRYSTALSTRUCTURE:4||PHOTOEMISSION:4||TEMPERATURE:4||TRANSITIONTEMPERATURE:4||XRAYABSORPTION:4||STATE:4||CU:4||BASISSET:4||XAS:4||CRYSTALS:3||EXCITATIONS:3||MOTTHUBBARD SYSTEMS:3||HIGHENERGY SPIN:3||halfmetal:3||INSULATORS:3||LA2CUO4:3||MODEL:3||FLUCTUATIONS:3||CE:3||double exchange:3||TRANSITIONMETALS:3||RESISTIVITY:3||BORON:3||LA1XCAXMNO3:3||IRON:3||PES:3||ANTIMONIDES:2||MgB2:2||ZR METALLIC GLASSES:2||superconductor:2||CRITICALCURRENT DENSITY:2||CIRCULARDICHROISM:2||SEMICONDUCTORS:2||LOCALIZATION:2||INTRABAND OPTICAL CONDUCTIVITY:2||COLOSSAL MAGNETORESISTANCE:2||OXIDATION:2||EXISTENCE:2||COPPER:2||diboride:2||MAGNESIUMDIBORIDE:2||GAP:2||CE COMPOUNDS:2||CORE POLARIZATION:2||magnetoresistance:2||photoemission spectroscopy:2||electronphonon interaction:2||GETTER:2||PD:2||MAGNETISM:2||FECR2S4:2||SUPERCONDUCTING MGB2:2||WIRES:2||ABSORPTION:2||ENERGY:2||LA1XSRXMNO3:2||CONSTANTS:2||polaron:2||charge ordering:2||SCATTERING:2||XRAY PHOTOEMISSION:2||CeNiSn:2||phase diagram:2||PHOTOELECTRON:2||QUADRUPOLAR:2||perovskitemanganites:2||CO:2||SYSTEMS:2||DOPED ZNO:2||LOWFREQUENCY SOUND:2||LA:2||ELECTRONELECTRON SCATTERING:2||AU:2||DENSITYWAVE INSTABILITY:2||FERMISURFACE:2||hybridization:2||VALENCEBAND SATELLITE:2||SULFUR SPINEL:2||Heusler:2||APPROXIMATION:2||superexchange:2||colossal magnetoresistance:2||ALLOYS:2||DEPENDENCE:2||AG:2||electronic structures:2||AUGERSPECTRA:2||CR:2||PARAMETERS:2||DIFFRACTION:2||SEMICONDUCTORMETAL TRANSITION:1||INTERMEDIATEVALENCE:1||SMB6:1||SRRUO3:1||antiperovskite structure with antipolar nature:1||lowenergy twodimensional phonons:1||anatase TiO2:1||La3S4:1||metalinsulator transitions:1||MNO:1||ELECTRONICSTRUCTURES:1||MAGNETIC CIRCULARDICHROISM:1||Density functional theory:1||CeCo2:1||TOPOLARON CROSSOVER:1||EXCHANGE:1||cuprates:1||high Tc cuprates:1||magnetically ordered materials:1||ZNSE:1||Sr2xKxFeMoO6:1||CDW:1||TeCuO3:1||STRUCTURALPROPERTIES:1||MN:1||screening length:1||amorphous Fe:1||WAVE BASISSET:1||SILICONCARBIDE:1||HIGHPRESSURE:1||electronphonon coupling:1||quenched superconductivity:1||CMR perovskite manganites:1||OXIDE:1||polarons:1||synchrotron radiation:1||FULLERIDES:1||RESONANTPHOTOEMISSION:1||Silicon carbide:1||DFT calculation:1||Hybridized bands:1||GIANT MAGNETORESISTANCE:1||PEROVSKITES:1||Raman spectra:1||EXCHANGE ENHANCEMENT:1||SILICON:1||SR2FEMOO6:1||orbital ordering:1||delafossite:1||TITANIUMDIOXIDE:1||electronic structure of disordered solids:1||YFE2:1||Magnetic polaron:1||NA2TI2SB2O:1||STRONGCOUPLED SUPERCONDUCTORS:1||HEAVYFERMION SYSTEMS:1||firstprinciples calculations:1||MECHANISM:1||UNiSn:1||PHOTONIC BANDGAP:1||SINGLE IMPURITY:1||PHONONSPECTRUM:1||FERMISURFACE TOPOLOGY:1||SUPPRESSION:1||RESONANT PHOTOEMISSION:1||METALDOPED PICENE:1||PHOTOIONIZATION CROSSSECTIONS:1||PHOTOINDUCED FERRIMAGNETIC SYSTEMS:1||LINKAGE ISOMERISM:1||CHARGETRANSFER:1||Bilayer Graphene:1||MAGNETICFIELD:1||SPINWAVES:1||rareearth manganese oxides:1||magnonphonon interaction:1||NACO2O4:1||ENERGYBANDS:1||SELFENERGY:1||GAS:1||Fe0.5Cu0.5Cr2S4:1||scanning photoelectron microscopy (SPEM):1||MAGNETIC PROPERTIES:1||Stoner model:1||AMORPHOUS TRANSITIONMETALS:1||SPINGLASS STATES:1||NI:1||LA3NI2B2N3:1||SOLIDS:1||CEO2:1||BAND THEORY:1||dilute magnetic semiconductor:1||pyrochlore:1||Y1XPRXBA2CU3O7DELTA:1||and electronphonon interactions:1||VIBRATIONS:1||RAY PHOTOEMISSION:1||ALKALI CATION:1||Europium:1||colossal magnetoresistance:1||structural stability:1||ENERGYGAP:1||small polaron:1||DOUBLE EXCHANGE:1||Coulomb correlation:1||magnon:1||phonons:1||ELECTRON FERROMAGNETISM:1||CURIETEMPERATURE:1||ARPES:1||PLANEWAVE METHOD:1||Xray absorption spectroscopy (XAS):1||ROOMTEMPERATURE:1||MONOCHALCOGENIDES:1||HEAT:1||UPDSN:1||MOMENTS:1||XRAY ABSORPTION:1||SEMICONDUCTOR:1||Fermi surface nesting:1||optical phonon:1||disordered system:1||dilute magnetic semiconductors:1||CMR manganites:1||PHONONS:1||LATTICEDYNAMICS:1||OXIDES:1||4fphotoemission:1||permanent magnet:1||pseudogap:1||TRANSPORTPROPERTIES:1||ANTIFERROMAGNET:1||(BI,PB)SRCOO SYSTEM:1||semicore correlation:1||POLARIZATION:1||CRYSTAL:1||spinel:1||Xray magnetic circular dichroism (XMCD):1||magnetocapacitance:1||ANATASE:1||TEMPERATURES:1||Pseudogap:1||INTERFACE:1||SUBSTRATE:1||YNI2B2C:1||SAMARIUM SULFIDE:1||strong swave superconductor:1||DOPED MANGANITE:1||SYMMETRY:1||CENISN:1||resonance mode:1||DISORDERED SYSTEM:1||LITHIUM INTERCALATION:1||CUO2 PLANE:1||SURFACE:1||Delafossite:1||ELECTRICALPROPERTIES:1||NIMNSB:1||PTMNSB:1||ROOMTEMPERATURE FERROMAGNETISM:1||RUBIDIUM MANGANESE HEXACYANOFERRATE:1||COLOSSALMAGNETORESISTANCE:1||FINITE TEMPERATURES:1||LAMNO3:1||FE:1||transitionmetal oxides:1||giant magnetoresistance:1||phonon:1||COPPER OXIDES:1||valence states:1||thermoelectric:1||semiconductor:1||CATION DISTRIBUTION:1||FeCr2S4:1||photoemission spectroscopy (PES):1||METALLIC FERROMAGNETISM:1||GRAPHITE:1||SUSCEPTIBILITY:1||UBE13:1||RCrSb3:1||band JahnTeller:1||Ce3S4:1||TiO2:1||PrBa2Cu3O7delta:1||UNTWINNED PRBA2CU3O7:1||AGNIO2:1||HALFMETALLIC FERROMAGNETS:1||CI:1||Energy gap:1||Photoemission:1||Future applications:1||Photoemission measurements:1||Graphene:1||BANDSTRUCTURE:1||TC:1||superconductivity:1||magnetic semiconductors:1||CMRmanganites:1||thin films:1||spin dynamics:1||highTc superconductors:1||ITINERANTELECTRON FERROMAGNETISM:1||SINGLECRYSTALS:1||CeTe2:1||amorphous magnetic materials:1||EPITAXIAL GRAPHENE:1||LAYERED PNICTIDEOXIDES:1||BOROCARBIDE SUPERCONDUCTORS:1||AUGMENTEDWAVE METHOD:1||METALLIC MAGNET UNISN:1||ORIGIN:1||spectrum rearrangement:1||MEANFIELD THEORY:1||MOLECULEBASED MAGNETS:1||METASTABLE STATE:1||INSULATOR:1||magnetic orderin:1||FCC IRON:1||CeRu2:1||TL2MN2O7:1||isotope effect:1||Perovskitemanganites:1||RECURSION METHOD:1||PERPENDICULAR MAGNETICANISOTROPY:1||quasiparticle spectral density:1||GW:1||MANGANESE FERRITE:1||RESONANCE:1||SeCuO3:1||Optical conductivity:1||MASSLESS DIRAC FERMIONS:1||SCHOTTKYBARRIER:1||electronic structure:15||ELECTRONICSTRUCTURE:11||TRANSITIONMETAL COMPOUNDS:10||METALS:10||photoemission:8||SPECTRA:8||MAGNETORESISTANCE:7||FERROMAGNETISM:7||TRANSPORT:7||TRANSITION:6||FILMS:6||THINFILMS:5||TOTALENERGY CALCULATIONS:5||MAGNETICPROPERTIES:5||SUPERCONDUCTIVITY:5||PR:5||LATTICE:4||STATES:4||SPECTROSCOPY:4||FIELD:4||CRYSTALSTRUCTURE:4||PHOTOEMISSION:4||TEMPERATURE:4||TRANSITIONTEMPERATURE:4||XRAYABSORPTION:4||STATE:4||CU:4||BASISSET:4||XAS:4||CRYSTALS:3||EXCITATIONS:3||MOTTHUBBARD SYSTEMS:3||HIGHENERGY SPIN:3||halfmetal:3||INSULATORS:3||LA2CUO4:3||MODEL:3||FLUCTUATIONS:3||CE:3||double exchange:3||TRANSITIONMETALS:3||RESISTIVITY:3||BORON:3||LA1XCAXMNO3:3||IRON:3||PES:3||ANTIMONIDES:2||MgB2:2||ZR METALLIC GLASSES:2||superconductor:2||CRITICALCURRENT DENSITY:2||CIRCULARDICHROISM:2||SEMICONDUCTORS:2||LOCALIZATION:2||INTRABAND OPTICAL CONDUCTIVITY:2||COLOSSAL MAGNETORESISTANCE:2||OXIDATION:2||EXISTENCE:2||COPPER:2||diboride:2||MAGNESIUMDIBORIDE:2||GAP:2||CE COMPOUNDS:2||CORE POLARIZATION:2||magnetoresistance:2||photoemission spectroscopy:2||electronphonon interaction:2||GETTER:2||PD:2||MAGNETISM:2||FECR2S4:2||SUPERCONDUCTING MGB2:2||WIRES:2||ABSORPTION:2||ENERGY:2||LA1XSRXMNO3:2||CONSTANTS:2||polaron:2||charge ordering:2||SCATTERING:2||XRAY PHOTOEMISSION:2||CeNiSn:2||phase diagram:2||PHOTOELECTRON:2||QUADRUPOLAR:2||perovskitemanganites:2||CO:2||SYSTEMS:2||DOPED ZNO:2||LOWFREQUENCY SOUND:2||LA:2||ELECTRONELECTRON SCATTERING:2||AU:2||DENSITYWAVE INSTABILITY:2||FERMISURFACE:2||hybridization:2||VALENCEBAND SATELLITE:2||SULFUR SPINEL:2||Heusler:2||APPROXIMATION:2||superexchange:2||colossal magnetoresistance:2||ALLOYS:2||DEPENDENCE:2||AG:2||electronic structures:2||AUGERSPECTRA:2||CR:2||PARAMETERS:2||DIFFRACTION:2||SEMICONDUCTORMETAL TRANSITION:1||INTERMEDIATEVALENCE:1||SMB6:1||SRRUO3:1||antiperovskite structure with antipolar nature:1||lowenergy twodimensional phonons:1||anatase TiO2:1||La3S4:1||metalinsulator transitions:1||MNO:1||ELECTRONICSTRUCTURES:1||MAGNETIC CIRCULARDICHROISM:1||Density functional theory:1||CeCo2:1||TOPOLARON CROSSOVER:1||EXCHANGE:1||cuprates:1||high Tc cuprates:1||magnetically ordered materials:1||ZNSE:1||Sr2xKxFeMoO6:1||CDW:1||TeCuO3:1||STRUCTURALPROPERTIES:1||MN:1||screening length:1||amorphous Fe:1||WAVE BASISSET:1||SILICONCARBIDE:1||HIGHPRESSURE:1||electronphonon coupling:1||quenched superconductivity:1||CMR perovskite manganites:1||OXIDE:1||polarons:1||synchrotron radiation:1||FULLERIDES:1||RESONANTPHOTOEMISSION:1||Silicon carbide:1||DFT calculation:1||Hybridized bands:1||GIANT MAGNETORESISTANCE:1||PEROVSKITES:1||Raman spectra:1||EXCHANGE ENHANCEMENT:1||SILICON:1||SR2FEMOO6:1||orbital ordering:1||delafossite:1||TITANIUMDIOXIDE:1||electronic structure of disordered solids:1||YFE2:1||Magnetic polaron:1||NA2TI2SB2O:1||STRONGCOUPLED SUPERCONDUCTORS:1||HEAVYFERMION SYSTEMS:1||firstprinciples calculations:1||MECHANISM:1||UNiSn:1||PHOTONIC BANDGAP:1||SINGLE IMPURITY:1||PHONONSPECTRUM:1||FERMISURFACE TOPOLOGY:1||SUPPRESSION:1||RESONANT PHOTOEMISSION:1||METALDOPED PICENE:1||PHOTOIONIZATION CROSSSECTIONS:1||PHOTOINDUCED FERRIMAGNETIC SYSTEMS:1||LINKAGE ISOMERISM:1||CHARGETRANSFER:1||Bilayer Graphene:1||MAGNETICFIELD:1||SPINWAVES:1||rareearth manganese oxides:1||magnonphonon interaction:1||NACO2O4:1||ENERGYBANDS:1||SELFENERGY:1||GAS:1||Fe0.5Cu0.5Cr2S4:1||scanning photoelectron microscopy (SPEM):1||MAGNETIC PROPERTIES:1||Stoner model:1||AMORPHOUS TRANSITIONMETALS:1||SPINGLASS STATES:1||NI:1||LA3NI2B2N3:1||SOLIDS:1||CEO2:1||BAND THEORY:1||dilute magnetic semiconductor:1||pyrochlore:1||Y1XPRXBA2CU3O7DELTA:1||and electronphonon interactions:1||VIBRATIONS:1||RAY PHOTOEMISSION:1||ALKALI CATION:1||Europium:1||colossal magnetoresistance:1||structural stability:1||ENERGYGAP:1||small polaron:1||DOUBLE EXCHANGE:1||Coulomb correlation:1||magnon:1||phonons:1||ELECTRON FERROMAGNETISM:1||CURIETEMPERATURE:1||ARPES:1||PLANEWAVE METHOD:1||Xray absorption spectroscopy (XAS):1||ROOMTEMPERATURE:1||MONOCHALCOGENIDES:1||HEAT:1||UPDSN:1||MOMENTS:1||XRAY ABSORPTION:1||SEMICONDUCTOR:1||Fermi surface nesting:1||optical phonon:1||disordered system:1||dilute magnetic semiconductors:1||CMR manganites:1||PHONONS:1||LATTICEDYNAMICS:1||OXIDES:1||4fphotoemission:1||permanent magnet:1||pseudogap:1||TRANSPORTPROPERTIES:1||ANTIFERROMAGNET:1||(BI,PB)SRCOO SYSTEM:1||semicore correlation:1||POLARIZATION:1||CRYSTAL:1||spinel:1||Xray magnetic circular dichroism (XMCD):1||magnetocapacitance:1||ANATASE:1||TEMPERATURES:1||Pseudogap:1||INTERFACE:1||SUBSTRATE:1||YNI2B2C:1||SAMARIUM SULFIDE:1||strong swave superconductor:1||DOPED MANGANITE:1||SYMMETRY:1||CENISN:1||resonance mode:1||DISORDERED SYSTEM:1||LITHIUM INTERCALATION:1||CUO2 PLANE:1||SURFACE:1||Delafossite:1||ELECTRICALPROPERTIES:1||NIMNSB:1||PTMNSB:1||ROOMTEMPERATURE FERROMAGNETISM:1||RUBIDIUM MANGANESE HEXACYANOFERRATE:1||COLOSSALMAGNETORESISTANCE:1||FINITE TEMPERATURES:1||LAMNO3:1||FE:1||transitionmetal oxides:1||giant magnetoresistance:1||phonon:1||COPPER OXIDES:1||valence states:1||thermoelectric:1||semiconductor:1||CATION DISTRIBUTION:1||FeCr2S4:1||photoemission spectroscopy (PES):1||METALLIC FERROMAGNETISM:1||GRAPHITE:1||SUSCEPTIBILITY:1||UBE13:1||RCrSb3:1||band JahnTeller:1||Ce3S4:1||TiO2:1||PrBa2Cu3O7delta:1||UNTWINNED PRBA2CU3O7:1||AGNIO2:1||HALFMETALLIC FERROMAGNETS:1||CI:1||Energy gap:1||Photoemission:1||Future applications:1||Photoemission measurements:1||Graphene:1||BANDSTRUCTURE:1||TC:1||superconductivity:1||magnetic semiconductors:1||CMRmanganites:1||thin films:1||spin dynamics:1||highTc superconductors:1||ITINERANTELECTRON FERROMAGNETISM:1||SINGLECRYSTALS:1||CeTe2:1||amorphous magnetic materials:1||EPITAXIAL GRAPHENE:1||LAYERED PNICTIDEOXIDES:1||BOROCARBIDE SUPERCONDUCTORS:1||AUGMENTEDWAVE METHOD:1||METALLIC MAGNET UNISN:1||ORIGIN:1||spectrum rearrangement:1||MEANFIELD THEORY:1||MOLECULEBASED MAGNETS:1||METASTABLE STATE:1||INSULATOR:1||magnetic orderin:1||FCC IRON:1||CeRu2:1||TL2MN2O7:1||isotope effect:1||Perovskitemanganites:1||RECURSION METHOD:1||PERPENDICULAR MAGNETICANISOTROPY:1||quasiparticle spectral density:1||GW:1||MANGANESE FERRITE:1||RESONANCE:1||SeCuO3:1||Optical conductivity:1||MASSLESS DIRAC FERMIONS:1||SCHOTTKYBARRIER:1||electronic structure:15||ELECTRONICSTRUCTURE:11||TRANSITIONMETAL COMPOUNDS:10||METALS:10||photoemission:8||SPECTRA:8||MAGNETORESISTANCE:7||FERROMAGNETISM:7||TRANSPORT:7||TRANSITION:6||FILMS:6||THINFILMS:5||TOTALENERGY CALCULATIONS:5||MAGNETICPROPERTIES:5||SUPERCONDUCTIVITY:5||PR:5||LATTICE:4||STATES:4||SPECTROSCOPY:4||FIELD:4||CRYSTALSTRUCTURE:4||PHOTOEMISSION:4||TEMPERATURE:4||TRANSITIONTEMPERATURE:4||XRAYABSORPTION:4||STATE:4||CU:4||BASISSET:4||XAS:4||CRYSTALS:3||EXCITATIONS:3||MOTTHUBBARD SYSTEMS:3||HIGHENERGY SPIN:3||halfmetal:3||INSULATORS:3||LA2CUO4:3||MODEL:3||FLUCTUATIONS:3||CE:3||double exchange:3||TRANSITIONMETALS:3||RESISTIVITY:3||BORON:3||LA1XCAXMNO3:3||IRON:3||PES:3||ANTIMONIDES:2||MgB2:2||ZR METALLIC GLASSES:2||superconductor:2||CRITICALCURRENT DENSITY:2||CIRCULARDICHROISM:2||SEMICONDUCTORS:2||LOCALIZATION:2||INTRABAND OPTICAL CONDUCTIVITY:2||COLOSSAL MAGNETORESISTANCE:2||OXIDATION:2||EXISTENCE:2||COPPER:2||diboride:2||MAGNESIUMDIBORIDE:2||GAP:2||CE COMPOUNDS:2||CORE POLARIZATION:2||magnetoresistance:2||photoemission spectroscopy:2||electronphonon interaction:2||GETTER:2||PD:2||MAGNETISM:2||FECR2S4:2||SUPERCONDUCTING MGB2:2||WIRES:2||ABSORPTION:2||ENERGY:2||LA1XSRXMNO3:2||CONSTANTS:2||polaron:2||charge ordering:2||SCATTERING:2||XRAY PHOTOEMISSION:2||CeNiSn:2||phase diagram:2||PHOTOELECTRON:2||QUADRUPOLAR:2||perovskitemanganites:2||CO:2||SYSTEMS:2||DOPED ZNO:2||LOWFREQUENCY SOUND:2||LA:2||ELECTRONELECTRON SCATTERING:2||AU:2||DENSITYWAVE INSTABILITY:2||FERMISURFACE:2||hybridization:2||VALENCEBAND SATELLITE:2||SULFUR SPINEL:2||Heusler:2||APPROXIMATION:2||superexchange:2||colossal magnetoresistance:2||ALLOYS:2||DEPENDENCE:2||AG:2||electronic structures:2||AUGERSPECTRA:2||CR:2||PARAMETERS:2||DIFFRACTION:2||SEMICONDUCTORMETAL TRANSITION:1||INTERMEDIATEVALENCE:1||SMB6:1||SRRUO3:1||antiperovskite structure with antipolar nature:1||lowenergy twodimensional phonons:1||anatase TiO2:1||La3S4:1||metalinsulator transitions:1||MNO:1||ELECTRONICSTRUCTURES:1||MAGNETIC CIRCULARDICHROISM:1||Density functional theory:1||CeCo2:1||TOPOLARON CROSSOVER:1||EXCHANGE:1||cuprates:1||high Tc cuprates:1||magnetically ordered materials:1||ZNSE:1||Sr2xKxFeMoO6:1||CDW:1||TeCuO3:1||STRUCTURALPROPERTIES:1||MN:1||screening length:1||amorphous Fe:1||WAVE BASISSET:1||SILICONCARBIDE:1||HIGHPRESSURE:1||electronphonon coupling:1||quenched superconductivity:1||CMR perovskite manganites:1||OXIDE:1||polarons:1||synchrotron radiation:1||FULLERIDES:1||RESONANTPHOTOEMISSION:1||Silicon carbide:1||DFT calculation:1||Hybridized bands:1||GIANT MAGNETORESISTANCE:1||PEROVSKITES:1||Raman spectra:1||EXCHANGE ENHANCEMENT:1||SILICON:1||SR2FEMOO6:1||orbital ordering:1||delafossite:1||TITANIUMDIOXIDE:1||electronic structure of disordered solids:1||YFE2:1||Magnetic polaron:1||NA2TI2SB2O:1||STRONGCOUPLED SUPERCONDUCTORS:1||HEAVYFERMION SYSTEMS:1||firstprinciples calculations:1||MECHANISM:1||UNiSn:1||PHOTONIC BANDGAP:1||SINGLE IMPURITY:1||PHONONSPECTRUM:1||FERMISURFACE TOPOLOGY:1||SUPPRESSION:1||RESONANT PHOTOEMISSION:1||METALDOPED PICENE:1||PHOTOIONIZATION CROSSSECTIONS:1||PHOTOINDUCED FERRIMAGNETIC SYSTEMS:1||LINKAGE ISOMERISM:1||CHARGETRANSFER:1||Bilayer Graphene:1||MAGNETICFIELD:1||SPINWAVES:1||rareearth manganese oxides:1||magnonphonon interaction:1||NACO2O4:1||ENERGYBANDS:1||SELFENERGY:1||GAS:1||Fe0.5Cu0.5Cr2S4:1||scanning photoelectron microscopy (SPEM):1||MAGNETIC PROPERTIES:1||Stoner model:1||AMORPHOUS TRANSITIONMETALS:1||SPINGLASS STATES:1||NI:1||LA3NI2B2N3:1||SOLIDS:1||CEO2:1||BAND THEORY:1||dilute magnetic semiconductor:1||pyrochlore:1||Y1XPRXBA2CU3O7DELTA:1||and electronphonon interactions:1||VIBRATIONS:1||RAY PHOTOEMISSION:1||ALKALI CATION:1||Europium:1||colossal magnetoresistance:1||structural stability:1||ENERGYGAP:1||small polaron:1||DOUBLE EXCHANGE:1||Coulomb correlation:1||magnon:1||phonons:1||ELECTRON FERROMAGNETISM:1||CURIETEMPERATURE:1||ARPES:1||PLANEWAVE METHOD:1||Xray absorption spectroscopy (XAS):1||ROOMTEMPERATURE:1||MONOCHALCOGENIDES:1||HEAT:1||UPDSN:1||MOMENTS:1||XRAY ABSORPTION:1||SEMICONDUCTOR:1||Fermi surface nesting:1||optical phonon:1||disordered system:1||dilute magnetic semiconductors:1||CMR manganites:1||PHONONS:1||LATTICEDYNAMICS:1||OXIDES:1||4fphotoemission:1||permanent magnet:1||pseudogap:1||TRANSPORTPROPERTIES:1||ANTIFERROMAGNET:1||(BI,PB)SRCOO SYSTEM:1||semicore correlation:1||POLARIZATION:1||CRYSTAL:1||spinel:1||Xray magnetic circular dichroism (XMCD):1||magnetocapacitance:1||ANATASE:1||TEMPERATURES:1||Pseudogap:1||INTERFACE:1||SUBSTRATE:1||YNI2B2C:1||SAMARIUM SULFIDE:1||strong swave superconductor:1||DOPED MANGANITE:1||SYMMETRY:1||CENISN:1||resonance mode:1||DISORDERED SYSTEM:1||LITHIUM INTERCALATION:1||CUO2 PLANE:1||SURFACE:1||Delafossite:1||ELECTRICALPROPERTIES:1||NIMNSB:1||PTMNSB:1||ROOMTEMPERATURE FERROMAGNETISM:1||RUBIDIUM MANGANESE HEXACYANOFERRATE:1||COLOSSALMAGNETORESISTANCE:1||FINITE TEMPERATURES:1||LAMNO3:1||FE:1||transitionmetal oxides:1||giant magnetoresistance:1||phonon:1||COPPER OXIDES:1||valence states:1||thermoelectric:1||semiconductor:1||CATION DISTRIBUTION:1||FeCr2S4:1||photoemission spectroscopy (PES):1||METALLIC FERROMAGNETISM:1||GRAPHITE:1||SUSCEPTIBILITY:1||UBE13:1||RCrSb3:1||band JahnTeller:1||Ce3S4:1||TiO2:1||PrBa2Cu3O7delta:1||UNTWINNED PRBA2CU3O7:1||AGNIO2:1||HALFMETALLIC FERROMAGNETS:1||CI:1||Energy gap:1||Photoemission:1||Future applications:1||Photoemission measurements:1||Graphene:1||BANDSTRUCTURE:1||TC:1||superconductivity:1||magnetic semiconductors:1||CMRmanganites:1||thin films:1||spin dynamics:1||highTc superconductors:1||ITINERANTELECTRON FERROMAGNETISM:1||SINGLECRYSTALS:1||CeTe2:1||amorphous magnetic materials:1||EPITAXIAL GRAPHENE:1||LAYERED PNICTIDEOXIDES:1||BOROCARBIDE SUPERCONDUCTORS:1||AUGMENTEDWAVE METHOD:1||METALLIC MAGNET UNISN:1||ORIGIN:1||spectrum rearrangement:1||MEANFIELD THEORY:1||MOLECULEBASED MAGNETS:1||METASTABLE STATE:1||INSULATOR:1||magnetic orderin:1||FCC IRON:1||CeRu2:1||TL2MN2O7:1||isotope effect:1||Perovskitemanganites:1||RECURSION METHOD:1||PERPENDICULAR MAGNETICANISOTROPY:1||quasiparticle spectral density:1||GW:1||MANGANESE FERRITE:1||RESONANCE:1||SeCuO3:1||Optical conductivity:1||MASSLESS DIRAC FERMIONS:1||SCHOTTKYBARRIER:1||electronic structure:15||ELECTRONICSTRUCTURE:11||TRANSITIONMETAL COMPOUNDS:10||METALS:10||photoemission:8||SPECTRA:8||MAGNETORESISTANCE:7||FERROMAGNETISM:7||TRANSPORT:7||TRANSITION:6||FILMS:6||THINFILMS:5||TOTALENERGY CALCULATIONS:5||MAGNETICPROPERTIES:5||SUPERCONDUCTIVITY:5||PR:5||LATTICE:4||STATES:4||SPECTROSCOPY:4||FIELD:4||CRYSTALSTRUCTURE:4||PHOTOEMISSION:4||TEMPERATURE:4||TRANSITIONTEMPERATURE:4||XRAYABSORPTION:4||STATE:4||CU:4||BASISSET:4||XAS:4||CRYSTALS:3||EXCITATIONS:3||MOTTHUBBARD SYSTEMS:3||HIGHENERGY SPIN:3||halfmetal:3||INSULATORS:3||LA2CUO4:3||MODEL:3||FLUCTUATIONS:3||CE:3||double exchange:3||TRANSITIONMETALS:3||RESISTIVITY:3||BORON:3||LA1XCAXMNO3:3||IRON:3||PES:3||ANTIMONIDES:2||MgB2:2||ZR METALLIC GLASSES:2||superconductor:2||CRITICALCURRENT DENSITY:2||CIRCULARDICHROISM:2||SEMICONDUCTORS:2||LOCALIZATION:2||INTRABAND OPTICAL CONDUCTIVITY:2||COLOSSAL MAGNETORESISTANCE:2||OXIDATION:2||EXISTENCE:2||COPPER:2||diboride:2||MAGNESIUMDIBORIDE:2||GAP:2||CE COMPOUNDS:2||CORE POLARIZATION:2||magnetoresistance:2||photoemission spectroscopy:2||electronphonon interaction:2||GETTER:2||PD:2||MAGNETISM:2||FECR2S4:2||SUPERCONDUCTING MGB2:2||WIRES:2||ABSORPTION:2||ENERGY:2||LA1XSRXMNO3:2||CONSTANTS:2||polaron:2||charge ordering:2||SCATTERING:2||XRAY PHOTOEMISSION:2||CeNiSn:2||phase diagram:2||PHOTOELECTRON:2||QUADRUPOLAR:2||perovskitemanganites:2||CO:2||SYSTEMS:2||DOPED ZNO:2||LOWFREQUENCY SOUND:2||LA:2||ELECTRONELECTRON SCATTERING:2||AU:2||DENSITYWAVE INSTABILITY:2||FERMISURFACE:2||hybridization:2||VALENCEBAND SATELLITE:2||SULFUR SPINEL:2||Heusler:2||APPROXIMATION:2||superexchange:2||colossal magnetoresistance:2||ALLOYS:2||DEPENDENCE:2||AG:2||electronic structures:2||AUGERSPECTRA:2||CR:2||PARAMETERS:2||DIFFRACTION:2||SEMICONDUCTORMETAL TRANSITION:1||INTERMEDIATEVALENCE:1||SMB6:1||SRRUO3:1||antiperovskite structure with antipolar nature:1||lowenergy twodimensional phonons:1||anatase TiO2:1||La3S4:1||metalinsulator transitions:1||MNO:1||ELECTRONICSTRUCTURES:1||MAGNETIC CIRCULARDICHROISM:1||Density functional theory:1||CeCo2:1||TOPOLARON CROSSOVER:1||EXCHANGE:1||cuprates:1||high Tc cuprates:1||magnetically ordered materials:1||ZNSE:1||Sr2xKxFeMoO6:1||CDW:1||TeCuO3:1||STRUCTURALPROPERTIES:1||MN:1||screening length:1||amorphous Fe:1||WAVE BASISSET:1||SILICONCARBIDE:1||HIGHPRESSURE:1||electronphonon coupling:1||quenched superconductivity:1||CMR perovskite manganites:1||OXIDE:1||polarons:1||synchrotron radiation:1||FULLERIDES:1||RESONANTPHOTOEMISSION:1||Silicon carbide:1||DFT calculation:1||Hybridized bands:1||GIANT MAGNETORESISTANCE:1||PEROVSKITES:1||Raman spectra:1||EXCHANGE ENHANCEMENT:1||SILICON:1||SR2FEMOO6:1||orbital ordering:1||delafossite:1||TITANIUMDIOXIDE:1||electronic structure of disordered solids:1||YFE2:1||Magnetic polaron:1||NA2TI2SB2O:1||STRONGCOUPLED SUPERCONDUCTORS:1||HEAVYFERMION SYSTEMS:1||firstprinciples calculations:1||MECHANISM:1||UNiSn:1||PHOTONIC BANDGAP:1||SINGLE IMPURITY:1||PHONONSPECTRUM:1||FERMISURFACE TOPOLOGY:1||SUPPRESSION:1||RESONANT PHOTOEMISSION:1||METALDOPED PICENE:1||PHOTOIONIZATION CROSSSECTIONS:1||PHOTOINDUCED FERRIMAGNETIC SYSTEMS:1||LINKAGE ISOMERISM:1||CHARGETRANSFER:1||Bilayer Graphene:1||MAGNETICFIELD:1||SPINWAVES:1||rareearth manganese oxides:1||magnonphonon interaction:1||NACO2O4:1||ENERGYBANDS:1||SELFENERGY:1||GAS:1||Fe0.5Cu0.5Cr2S4:1||scanning photoelectron microscopy (SPEM):1||MAGNETIC PROPERTIES:1||Stoner model:1||AMORPHOUS TRANSITIONMETALS:1||SPINGLASS STATES:1||NI:1||LA3NI2B2N3:1||SOLIDS:1||CEO2:1||BAND THEORY:1||dilute magnetic semiconductor:1||pyrochlore:1||Y1XPRXBA2CU3O7DELTA:1||and electronphonon interactions:1||VIBRATIONS:1||RAY PHOTOEMISSION:1||ALKALI CATION:1||Europium:1||colossal magnetoresistance:1||structural stability:1||ENERGYGAP:1||small polaron:1||DOUBLE EXCHANGE:1||Coulomb correlation:1||magnon:1||phonons:1||ELECTRON FERROMAGNETISM:1||CURIETEMPERATURE:1||ARPES:1||PLANEWAVE METHOD:1||Xray absorption spectroscopy (XAS):1||ROOMTEMPERATURE:1||MONOCHALCOGENIDES:1||HEAT:1||UPDSN:1||MOMENTS:1||XRAY ABSORPTION:1||SEMICONDUCTOR:1||Fermi surface nesting:1||optical phonon:1||disordered system:1||dilute magnetic semiconductors:1||CMR manganites:1||PHONONS:1||LATTICEDYNAMICS:1||OXIDES:1||4fphotoemission:1||permanent magnet:1||pseudogap:1||TRANSPORTPROPERTIES:1||ANTIFERROMAGNET:1||(BI,PB)SRCOO SYSTEM:1||semicore correlation:1||POLARIZATION:1||CRYSTAL:1||spinel:1||Xray magnetic circular dichroism (XMCD):1||magnetocapacitance:1||ANATASE:1||TEMPERATURES:1||Pseudogap:1||INTERFACE:1||SUBSTRATE:1||YNI2B2C:1||SAMARIUM SULFIDE:1||strong swave superconductor:1||DOPED MANGANITE:1||SYMMETRY:1||CENISN:1||resonance mode:1||DISORDERED SYSTEM:1||LITHIUM INTERCALATION:1||CUO2 PLANE:1||SURFACE:1||Delafossite:1||ELECTRICALPROPERTIES:1||NIMNSB:1||PTMNSB:1||ROOMTEMPERATURE FERROMAGNETISM:1||RUBIDIUM MANGANESE HEXACYANOFERRATE:1||COLOSSALMAGNETORESISTANCE:1||FINITE TEMPERATURES:1||LAMNO3:1||FE:1||transitionmetal oxides:1||giant magnetoresistance:1||phonon:1||COPPER OXIDES:1||valence states:1||thermoelectric:1||semiconductor:1||CATION DISTRIBUTION:1||FeCr2S4:1||photoemission spectroscopy (PES):1||METALLIC FERROMAGNETISM:1||GRAPHITE:1||SUSCEPTIBILITY:1||UBE13:1||RCrSb3:1||band JahnTeller:1||Ce3S4:1||TiO2:1||PrBa2Cu3O7delta:1||UNTWINNED PRBA2CU3O7:1||AGNIO2:1||HALFMETALLIC FERROMAGNETS:1||CI:1||Energy gap:1||Photoemission:1||Future applications:1||Photoemission measurements:1||Graphene:1||BANDSTRUCTURE:1||TC:1||superconductivity:1||magnetic semiconductors:1||CMRmanganites:1||thin films:1||spin dynamics:1||highTc superconductors:1||ITINERANTELECTRON FERROMAGNETISM:1||SINGLECRYSTALS:1||CeTe2:1||amorphous magnetic materials:1||EPITAXIAL GRAPHENE:1||LAYERED PNICTIDEOXIDES:1||BOROCARBIDE SUPERCONDUCTORS:1||AUGMENTEDWAVE METHOD:1||METALLIC MAGNET UNISN:1||ORIGIN:1||spectrum rearrangement:1||MEANFIELD THEORY:1||MOLECULEBASED MAGNETS:1||METASTABLE STATE:1||INSULATOR:1||magnetic orderin:1||FCC IRON:1||CeRu2:1||TL2MN2O7:1||isotope effect:1||Perovskitemanganites:1||RECURSION METHOD:1||PERPENDICULAR MAGNETICANISOTROPY:1||quasiparticle spectral density:1||GW:1||MANGANESE FERRITE:1||RESONANCE:1||SeCuO3:1||Optical conductivity:1||MASSLESS DIRAC FERMIONS:1||SCHOTTKYBARRIER:1||electronic structure:15||ELECTRONICSTRUCTURE:11||TRANSITIONMETAL COMPOUNDS:10||METALS:10||photoemission:8||SPECTRA:8||MAGNETORESISTANCE:7||FERROMAGNETISM:7||TRANSPORT:7||TRANSITION:6||FILMS:6||THINFILMS:5||TOTALENERGY CALCULATIONS:5||MAGNETICPROPERTIES:5||SUPERCONDUCTIVITY:5||PR:5||LATTICE:4||STATES:4||SPECTROSCOPY:4||FIELD:4||CRYSTALSTRUCTURE:4||PHOTOEMISSION:4||TEMPERATURE:4||TRANSITIONTEMPERATURE:4||XRAYABSORPTION:4||STATE:4||CU:4||BASISSET:4||XAS:4||CRYSTALS:3||EXCITATIONS:3||MOTTHUBBARD SYSTEMS:3||HIGHENERGY SPIN:3||halfmetal:3||INSULATORS:3||LA2CUO4:3||MODEL:3||FLUCTUATIONS:3||CE:3||double exchange:3||TRANSITIONMETALS:3||RESISTIVITY:3||BORON:3||LA1XCAXMNO3:3||IRON:3||PES:3||ANTIMONIDES:2||MgB2:2||ZR METALLIC GLASSES:2||superconductor:2||CRITICALCURRENT DENSITY:2||CIRCULARDICHROISM:2||SEMICONDUCTORS:2||LOCALIZATION:2||INTRABAND OPTICAL CONDUCTIVITY:2||COLOSSAL MAGNETORESISTANCE:2||OXIDATION:2||EXISTENCE:2||COPPER:2||diboride:2||MAGNESIUMDIBORIDE:2||GAP:2||CE COMPOUNDS:2||CORE POLARIZATION:2||magnetoresistance:2||photoemission spectroscopy:2||electronphonon interaction:2||GETTER:2||PD:2||MAGNETISM:2||FECR2S4:2||SUPERCONDUCTING MGB2:2||WIRES:2||ABSORPTION:2||ENERGY:2||LA1XSRXMNO3:2||CONSTANTS:2||polaron:2||charge ordering:2||SCATTERING:2||XRAY PHOTOEMISSION:2||CeNiSn:2||phase diagram:2||PHOTOELECTRON:2||QUADRUPOLAR:2||perovskitemanganites:2||CO:2||SYSTEMS:2||DOPED ZNO:2||LOWFREQUENCY SOUND:2||LA:2||ELECTRONELECTRON SCATTERING:2||AU:2||DENSITYWAVE INSTABILITY:2||FERMISURFACE:2||hybridization:2||VALENCEBAND SATELLITE:2||SULFUR SPINEL:2||Heusler:2||APPROXIMATION:2||superexchange:2||colossal magnetoresistance:2||ALLOYS:2||DEPENDENCE:2||AG:2||electronic structures:2||AUGERSPECTRA:2||CR:2||PARAMETERS:2||DIFFRACTION:2||SEMICONDUCTORMETAL TRANSITION:1||INTERMEDIATEVALENCE:1||SMB6:1||SRRUO3:1||antiperovskite structure with antipolar nature:1||lowenergy twodimensional phonons:1||anatase TiO2:1||La3S4:1||metalinsulator transitions:1||MNO:1||ELECTRONICSTRUCTURES:1||MAGNETIC CIRCULARDICHROISM:1||Density functional theory:1||CeCo2:1||TOPOLARON CROSSOVER:1||EXCHANGE:1||cuprates:1||high Tc cuprates:1||magnetically ordered materials:1||ZNSE:1||Sr2xKxFeMoO6:1||CDW:1||TeCuO3:1||STRUCTURALPROPERTIES:1||MN:1||screening length:1||amorphous Fe:1||WAVE BASISSET:1||SILICONCARBIDE:1||HIGHPRESSURE:1||electronphonon coupling:1||quenched superconductivity:1||CMR perovskite manganites:1||OXIDE:1||polarons:1||synchrotron radiation:1||FULLERIDES:1||RESONANTPHOTOEMISSION:1||Silicon carbide:1||DFT calculation:1||Hybridized bands:1||GIANT MAGNETORESISTANCE:1||PEROVSKITES:1||Raman spectra:1||EXCHANGE ENHANCEMENT:1||SILICON:1||SR2FEMOO6:1||orbital ordering:1||delafossite:1||TITANIUMDIOXIDE:1||electronic structure of disordered solids:1||YFE2:1||Magnetic polaron:1||NA2TI2SB2O:1||STRONGCOUPLED SUPERCONDUCTORS:1||HEAVYFERMION SYSTEMS:1||firstprinciples calculations:1||MECHANISM:1||UNiSn:1||PHOTONIC BANDGAP:1||SINGLE IMPURITY:1||PHONONSPECTRUM:1||FERMISURFACE TOPOLOGY:1||SUPPRESSION:1||RESONANT PHOTOEMISSION:1||METALDOPED PICENE:1||PHOTOIONIZATION CROSSSECTIONS:1||PHOTOINDUCED FERRIMAGNETIC SYSTEMS:1||LINKAGE ISOMERISM:1||CHARGETRANSFER:1||Bilayer Graphene:1||MAGNETICFIELD:1||SPINWAVES:1||rareearth manganese oxides:1||magnonphonon interaction:1||NACO2O4:1||ENERGYBANDS:1||SELFENERGY:1||GAS:1||Fe0.5Cu0.5Cr2S4:1||scanning photoelectron microscopy (SPEM):1||MAGNETIC PROPERTIES:1||Stoner model:1||AMORPHOUS TRANSITIONMETALS:1||SPINGLASS STATES:1||NI:1||LA3NI2B2N3:1||SOLIDS:1||CEO2:1||BAND THEORY:1||dilute magnetic semiconductor:1||pyrochlore:1||Y1XPRXBA2CU3O7DELTA:1||and electronphonon interactions:1||VIBRATIONS:1||RAY PHOTOEMISSION:1||ALKALI CATION:1||Europium:1||colossal magnetoresistance:1||structural stability:1||ENERGYGAP:1||small polaron:1||DOUBLE EXCHANGE:1||Coulomb correlation:1||magnon:1||phonons:1||ELECTRON FERROMAGNETISM:1||CURIETEMPERATURE:1||ARPES:1||PLANEWAVE METHOD:1||Xray absorption spectroscopy (XAS):1||ROOMTEMPERATURE:1||MONOCHALCOGENIDES:1||HEAT:1||UPDSN:1||MOMENTS:1||XRAY ABSORPTION:1||SEMICONDUCTOR:1||Fermi surface nesting:1||optical phonon:1||disordered system:1||dilute magnetic semiconductors:1||CMR manganites:1||PHONONS:1||LATTICEDYNAMICS:1||OXIDES:1||4fphotoemission:1||permanent magnet:1||pseudogap:1||TRANSPORTPROPERTIES:1||ANTIFERROMAGNET:1||(BI,PB)SRCOO SYSTEM:1||semicore correlation:1||POLARIZATION:1||CRYSTAL:1||spinel:1||Xray magnetic circular dichroism (XMCD):1||magnetocapacitance:1||ANATASE:1||TEMPERATURES:1||Pseudogap:1||INTERFACE:1||SUBSTRATE:1||YNI2B2C:1||SAMARIUM SULFIDE:1||strong swave superconductor:1||DOPED MANGANITE:1||SYMMETRY:1||CENISN:1||resonance mode:1||DISORDERED SYSTEM:1||LITHIUM INTERCALATION:1||CUO2 PLANE:1||SURFACE:1||Delafossite:1||ELECTRICALPROPERTIES:1||NIMNSB:1||PTMNSB:1||ROOMTEMPERATURE FERROMAGNETISM:1||RUBIDIUM MANGANESE HEXACYANOFERRATE:1||COLOSSALMAGNETORESISTANCE:1||FINITE TEMPERATURES:1||LAMNO3:1||FE:1||transitionmetal oxides:1||giant magnetoresistance:1||phonon:1||COPPER OXIDES:1||valence states:1||thermoelectric:1||semiconductor:1||CATION DISTRIBUTION:1||FeCr2S4:1||photoemission spectroscopy (PES):1||METALLIC FERROMAGNETISM:1||GRAPHITE:1||SUSCEPTIBILITY:1||UBE13:1||RCrSb3:1||band JahnTeller:1||Ce3S4:1||TiO2:1||PrBa2Cu3O7delta:1||UNTWINNED PRBA2CU3O7:1||AGNIO2:1||HALFMETALLIC FERROMAGNETS:1||CI:1||Energy gap:1||Photoemission:1||Future applications:1||Photoemission measurements:1||Graphene:1||BANDSTRUCTURE:1||TC:1||superconductivity:1||magnetic semiconductors:1||CMRmanganites:1||thin films:1||spin dynamics:1||highTc superconductors:1||ITINERANTELECTRON FERROMAGNETISM:1||SINGLECRYSTALS:1||CeTe2:1||amorphous magnetic materials:1||EPITAXIAL GRAPHENE:1||LAYERED PNICTIDEOXIDES:1||BOROCARBIDE SUPERCONDUCTORS:1||AUGMENTEDWAVE METHOD:1||METALLIC MAGNET UNISN:1||ORIGIN:1||spectrum rearrangement:1||MEANFIELD THEORY:1||MOLECULEBASED MAGNETS:1||METASTABLE STATE:1||INSULATOR:1||magnetic orderin:1||FCC IRON:1||CeRu2:1||TL2MN2O7:1||isotope effect:1||Perovskitemanganites:1||RECURSION METHOD:1||PERPENDICULAR MAGNETICANISOTROPY:1||quasiparticle spectral density:1||GW:1||MANGANESE FERRITE:1||RESONANCE:1||SeCuO3:1||Optical conductivity:1||MASSLESS DIRAC FERMIONS:1||SCHOTTKYBARRIER:1||electronic structure:15||ELECTRONICSTRUCTURE:11||TRANSITIONMETAL COMPOUNDS:10||METALS:10||photoemission:8||SPECTRA:8||MAGNETORESISTANCE:7||FERROMAGNETISM:7||TRANSPORT:7||TRANSITION:6||FILMS:6||THINFILMS:5||TOTALENERGY CALCULATIONS:5||MAGNETICPROPERTIES:5||SUPERCONDUCTIVITY:5||PR:5||LATTICE:4||STATES:4||SPECTROSCOPY:4||FIELD:4||CRYSTALSTRUCTURE:4||PHOTOEMISSION:4||TEMPERATURE:4||TRANSITIONTEMPERATURE:4||XRAYABSORPTION:4||STATE:4||CU:4||BASISSET:4||XAS:4||CRYSTALS:3||EXCITATIONS:3||MOTTHUBBARD SYSTEMS:3||HIGHENERGY SPIN:3||halfmetal:3||INSULATORS:3||LA2CUO4:3||MODEL:3||FLUCTUATIONS:3||CE:3||double exchange:3||TRANSITIONMETALS:3||RESISTIVITY:3||BORON:3||LA1XCAXMNO3:3||IRON:3||PES:3||ANTIMONIDES:2||MgB2:2||ZR METALLIC GLASSES:2||superconductor:2||CRITICALCURRENT DENSITY:2||CIRCULARDICHROISM:2||SEMICONDUCTORS:2||LOCALIZATION:2||INTRABAND OPTICAL CONDUCTIVITY:2||COLOSSAL MAGNETORESISTANCE:2||OXIDATION:2||EXISTENCE:2||COPPER:2||diboride:2||MAGNESIUMDIBORIDE:2||GAP:2||CE COMPOUNDS:2||CORE POLARIZATION:2||magnetoresistance:2||photoemission spectroscopy:2||electronphonon interaction:2||GETTER:2||PD:2||MAGNETISM:2||FECR2S4:2||SUPERCONDUCTING MGB2:2||WIRES:2||ABSORPTION:2||ENERGY:2||LA1XSRXMNO3:2||CONSTANTS:2||polaron:2||charge ordering:2||SCATTERING:2||XRAY PHOTOEMISSION:2||CeNiSn:2||phase diagram:2||PHOTOELECTRON:2||QUADRUPOLAR:2||perovskitemanganites:2||CO:2||SYSTEMS:2||DOPED ZNO:2||LOWFREQUENCY SOUND:2||LA:2||ELECTRONELECTRON SCATTERING:2||AU:2||DENSITYWAVE INSTABILITY:2||FERMISURFACE:2||hybridization:2||VALENCEBAND SATELLITE:2||SULFUR SPINEL:2||Heusler:2||APPROXIMATION:2||superexchange:2||colossal magnetoresistance:2||ALLOYS:2||DEPENDENCE:2||AG:2||electronic structures:2||AUGERSPECTRA:2||CR:2||PARAMETERS:2||DIFFRACTION:2||SEMICONDUCTORMETAL TRANSITION:1||INTERMEDIATEVALENCE:1||SMB6:1||SRRUO3:1||antiperovskite structure with antipolar nature:1||lowenergy twodimensional phonons:1||anatase TiO2:1||La3S4:1||metalinsulator transitions:1||MNO:1||ELECTRONICSTRUCTURES:1||MAGNETIC CIRCULARDICHROISM:1||Density functional theory:1||CeCo2:1||TOPOLARON CROSSOVER:1||EXCHANGE:1||cuprates:1||high Tc cuprates:1||magnetically ordered materials:1||ZNSE:1||Sr2xKxFeMoO6:1||CDW:1||TeCuO3:1||STRUCTURALPROPERTIES:1||MN:1||screening length:1||amorphous Fe:1||WAVE BASISSET:1||SILICONCARBIDE:1||HIGHPRESSURE:1||electronphonon coupling:1||quenched superconductivity:1||CMR perovskite manganites:1||OXIDE:1||polarons:1||synchrotron radiation:1||FULLERIDES:1||RESONANTPHOTOEMISSION:1||Silicon carbide:1||DFT calculation:1||Hybridized bands:1||GIANT MAGNETORESISTANCE:1||PEROVSKITES:1||Raman spectra:1||EXCHANGE ENHANCEMENT:1||SILICON:1||SR2FEMOO6:1||orbital ordering:1||delafossite:1||TITANIUMDIOXIDE:1||electronic structure of disordered solids:1||YFE2:1||Magnetic polaron:1||NA2TI2SB2O:1||STRONGCOUPLED SUPERCONDUCTORS:1||HEAVYFERMION SYSTEMS:1||firstprinciples calculations:1||MECHANISM:1||UNiSn:1||PHOTONIC BANDGAP:1||SINGLE IMPURITY:1||PHONONSPECTRUM:1||FERMISURFACE TOPOLOGY:1||SUPPRESSION:1||RESONANT PHOTOEMISSION:1||METALDOPED PICENE:1||PHOTOIONIZATION CROSSSECTIONS:1||PHOTOINDUCED FERRIMAGNETIC SYSTEMS:1||LINKAGE ISOMERISM:1||CHARGETRANSFER:1||Bilayer Graphene:1||MAGNETICFIELD:1||SPINWAVES:1||rareearth manganese oxides:1||magnonphonon interaction:1||NACO2O4:1||ENERGYBANDS:1||SELFENERGY:1||GAS:1||Fe0.5Cu0.5Cr2S4:1||scanning photoelectron microscopy (SPEM):1||MAGNETIC PROPERTIES:1||Stoner model:1||AMORPHOUS TRANSITIONMETALS:1||SPINGLASS STATES:1||NI:1||LA3NI2B2N3:1||SOLIDS:1||CEO2:1||BAND THEORY:1||dilute magnetic semiconductor:1||pyrochlore:1||Y1XPRXBA2CU3O7DELTA:1||and electronphonon interactions:1||VIBRATIONS:1||RAY PHOTOEMISSION:1||ALKALI CATION:1||Europium:1||colossal magnetoresistance:1||structural stability:1||ENERGYGAP:1||small polaron:1||DOUBLE EXCHANGE:1||Coulomb correlation:1||magnon:1||phonons:1||ELECTRON FERROMAGNETISM:1||CURIETEMPERATURE:1||ARPES:1||PLANEWAVE METHOD:1||Xray absorption spectroscopy (XAS):1||ROOMTEMPERATURE:1||MONOCHALCOGENIDES:1||HEAT:1||UPDSN:1||MOMENTS:1||XRAY ABSORPTION:1||SEMICONDUCTOR:1||Fermi surface nesting:1||optical phonon:1||disordered system:1||dilute magnetic semiconductors:1||CMR manganites:1||PHONONS:1||LATTICEDYNAMICS:1||OXIDES:1||4fphotoemission:1||permanent magnet:1||pseudogap:1||TRANSPORTPROPERTIES:1||ANTIFERROMAGNET:1||(BI,PB)SRCOO SYSTEM:1||semicore correlation:1||POLARIZATION:1||CRYSTAL:1||spinel:1||Xray magnetic circular dichroism (XMCD):1||magnetocapacitance:1||ANATASE:1||TEMPERATURES:1||Pseudogap:1||INTERFACE:1||SUBSTRATE:1||YNI2B2C:1||SAMARIUM SULFIDE:1||strong swave superconductor:1||DOPED MANGANITE:1||SYMMETRY:1||CENISN:1||resonance mode:1||DISORDERED SYSTEM:1||LITHIUM INTERCALATION:1||CUO2 PLANE:1||SURFACE:1||Delafossite:1||ELECTRICALPROPERTIES:1||NIMNSB:1||PTMNSB:1||ROOMTEMPERATURE FERROMAGNETISM:1||RUBIDIUM MANGANESE HEXACYANOFERRATE:1||COLOSSALMAGNETORESISTANCE:1||FINITE TEMPERATURES:1||LAMNO3:1||FE:1||transitionmetal oxides:1||giant magnetoresistance:1||phonon:1||COPPER OXIDES:1||valence states:1||thermoelectric:1||semiconductor:1||CATION DISTRIBUTION:1||FeCr2S4:1||photoemission spectroscopy (PES):1||METALLIC FERROMAGNETISM:1||GRAPHITE:1||SUSCEPTIBILITY:1||UBE13:1||RCrSb3:1||band JahnTeller:1||Ce3S4:1||TiO2:1||PrBa2Cu3O7delta:1||UNTWINNED PRBA2CU3O7:1||AGNIO2:1||HALFMETALLIC FERROMAGNETS:1||CI:1||Energy gap:1||Photoemission:1||Future applications:1||Photoemission measurements:1||Graphene:1||BANDSTRUCTURE:1||TC:1||superconductivity:1||magnetic semiconductors:1||CMRmanganites:1||thin films:1||spin dynamics:1||highTc superconductors:1||ITINERANTELECTRON FERROMAGNETISM:1||SINGLECRYSTALS:1||CeTe2:1||amorphous magnetic materials:1||EPITAXIAL GRAPHENE:1||LAYERED PNICTIDEOXIDES:1||BOROCARBIDE SUPERCONDUCTORS:1||AUGMENTEDWAVE METHOD:1||METALLIC MAGNET UNISN:1||ORIGIN:1||spectrum rearrangement:1||MEANFIELD THEORY:1||MOLECULEBASED MAGNETS:1||METASTABLE STATE:1||INSULATOR:1||magnetic orderin:1||FCC IRON:1||CeRu2:1||TL2MN2O7:1||isotope effect:1||Perovskitemanganites:1||RECURSION METHOD:1||PERPENDICULAR MAGNETICANISOTROPY:1||quasiparticle spectral density:1||GW:1||MANGANESE FERRITE:1||RESONANCE:1||SeCuO3:1||Optical conductivity:1||MASSLESS DIRAC FERMIONS:1||SCHOTTKYBARRIER:1||electronic structure:15||ELECTRONICSTRUCTURE:11||TRANSITIONMETAL COMPOUNDS:10||METALS:10||photoemission:8||SPECTRA:8||MAGNETORESISTANCE:7||FERROMAGNETISM:7||TRANSPORT:7||TRANSITION:6||FILMS:6||THINFILMS:5||TOTALENERGY CALCULATIONS:5||MAGNETICPROPERTIES:5||SUPERCONDUCTIVITY:5||PR:5||LATTICE:4||STATES:4||SPECTROSCOPY:4||FIELD:4||CRYSTALSTRUCTURE:4||PHOTOEMISSION:4||TEMPERATURE:4||TRANSITIONTEMPERATURE:4||XRAYABSORPTION:4||STATE:4||CU:4||BASISSET:4||XAS:4||CRYSTALS:3||EXCITATIONS:3||MOTTHUBBARD SYSTEMS:3||HIGHENERGY SPIN:3||halfmetal:3||INSULATORS:3||LA2CUO4:3||MODEL:3||FLUCTUATIONS:3||CE:3||double exchange:3||TRANSITIONMETALS:3||RESISTIVITY:3||BORON:3||LA1XCAXMNO3:3||IRON:3||PES:3||ANTIMONIDES:2||MgB2:2||ZR METALLIC GLASSES:2||superconductor:2||CRITICALCURRENT DENSITY:2||CIRCULARDICHROISM:2||SEMICONDUCTORS:2||LOCALIZATION:2||INTRABAND OPTICAL CONDUCTIVITY:2||COLOSSAL MAGNETORESISTANCE:2||OXIDATION:2||EXISTENCE:2||COPPER:2||diboride:2||MAGNESIUMDIBORIDE:2||GAP:2||CE COMPOUNDS:2||CORE POLARIZATION:2||magnetoresistance:2||photoemission spectroscopy:2||electronphonon interaction:2||GETTER:2||PD:2||MAGNETISM:2||FECR2S4:2||SUPERCONDUCTING MGB2:2||WIRES:2||ABSORPTION:2||ENERGY:2||LA1XSRXMNO3:2||CONSTANTS:2||polaron:2||charge ordering:2||SCATTERING:2||XRAY PHOTOEMISSION:2||CeNiSn:2||phase diagram:2||PHOTOELECTRON:2||QUADRUPOLAR:2||perovskitemanganites:2||CO:2||SYSTEMS:2||DOPED ZNO:2||LOWFREQUENCY SOUND:2||LA:2||ELECTRONELECTRON SCATTERING:2||AU:2||DENSITYWAVE INSTABILITY:2||FERMISURFACE:2||hybridization:2||VALENCEBAND SATELLITE:2||SULFUR SPINEL:2||Heusler:2||APPROXIMATION:2||superexchange:2||colossal magnetoresistance:2||ALLOYS:2||DEPENDENCE:2||AG:2||electronic structures:2||AUGERSPECTRA:2||CR:2||PARAMETERS:2||DIFFRACTION:2||SEMICONDUCTORMETAL TRANSITION:1||INTERMEDIATEVALENCE:1||SMB6:1||SRRUO3:1||antiperovskite structure with antipolar nature:1||lowenergy twodimensional phonons:1||anatase TiO2:1||La3S4:1||metalinsulator transitions:1||MNO:1||ELECTRONICSTRUCTURES:1||MAGNETIC CIRCULARDICHROISM:1||Density functional theory:1||CeCo2:1||TOPOLARON CROSSOVER:1||EXCHANGE:1||cuprates:1||high Tc cuprates:1||magnetically ordered materials:1||ZNSE:1||Sr2xKxFeMoO6:1||CDW:1||TeCuO3:1||STRUCTURALPROPERTIES:1||MN:1||screening length:1||amorphous Fe:1||WAVE BASISSET:1||SILICONCARBIDE:1||HIGHPRESSURE:1||electronphonon coupling:1||quenched superconductivity:1||CMR perovskite manganites:1||OXIDE:1||polarons:1||synchrotron radiation:1||FULLERIDES:1||RESONANTPHOTOEMISSION:1||Silicon carbide:1||DFT calculation:1||Hybridized bands:1||GIANT MAGNETORESISTANCE:1||PEROVSKITES:1||Raman spectra:1||EXCHANGE ENHANCEMENT:1||SILICON:1||SR2FEMOO6:1||orbital ordering:1||delafossite:1||TITANIUMDIOXIDE:1||electronic structure of disordered solids:1||YFE2:1||Magnetic polaron:1||NA2TI2SB2O:1||STRONGCOUPLED SUPERCONDUCTORS:1||HEAVYFERMION SYSTEMS:1||firstprinciples calculations:1||MECHANISM:1||UNiSn:1||PHOTONIC BANDGAP:1||SINGLE IMPURITY:1||PHONONSPECTRUM:1||FERMISURFACE TOPOLOGY:1||SUPPRESSION:1||RESONANT PHOTOEMISSION:1||METALDOPED PICENE:1||PHOTOIONIZATION CROSSSECTIONS:1||PHOTOINDUCED FERRIMAGNETIC SYSTEMS:1||LINKAGE ISOMERISM:1||CHARGETRANSFER:1||Bilayer Graphene:1||MAGNETICFIELD:1||SPINWAVES:1||rareearth manganese oxides:1||magnonphonon interaction:1||NACO2O4:1||ENERGYBANDS:1||SELFENERGY:1||GAS:1||Fe0.5Cu0.5Cr2S4:1||scanning photoelectron microscopy (SPEM):1||MAGNETIC PROPERTIES:1||Stoner model:1||AMORPHOUS TRANSITIONMETALS:1||SPINGLASS STATES:1||NI:1||LA3NI2B2N3:1||SOLIDS:1||CEO2:1||BAND THEORY:1||dilute magnetic semiconductor:1||pyrochlore:1||Y1XPRXBA2CU3O7DELTA:1||and electronphonon interactions:1||VIBRATIONS:1||RAY PHOTOEMISSION:1||ALKALI CATION:1||Europium:1||colossal magnetoresistance:1||structural stability:1||ENERGYGAP:1||small polaron:1||DOUBLE EXCHANGE:1||Coulomb correlation:1||magnon:1||phonons:1||ELECTRON FERROMAGNETISM:1||CURIETEMPERATURE:1||ARPES:1||PLANEWAVE METHOD:1||Xray absorption spectroscopy (XAS):1||ROOMTEMPERATURE:1||MONOCHALCOGENIDES:1||HEAT:1||UPDSN:1||MOMENTS:1||XRAY ABSORPTION:1||SEMICONDUCTOR:1||Fermi surface nesting:1||optical phonon:1||disordered system:1||dilute magnetic semiconductors:1||CMR manganites:1||PHONONS:1||LATTICEDYNAMICS:1||OXIDES:1||4fphotoemission:1||permanent magnet:1||pseudogap:1||TRANSPORTPROPERTIES:1||ANTIFERROMAGNET:1||(BI,PB)SRCOO SYSTEM:1||semicore correlation:1||POLARIZATION:1||CRYSTAL:1||spinel:1||Xray magnetic circular dichroism (XMCD):1||magnetocapacitance:1||ANATASE:1||TEMPERATURES:1||Pseudogap:1||INTERFACE:1||SUBSTRATE:1||YNI2B2C:1||SAMARIUM SULFIDE:1||strong swave superconductor:1||DOPED MANGANITE:1||SYMMETRY:1||CENISN:1||resonance mode:1||DISORDERED SYSTEM:1||LITHIUM INTERCALATION:1||CUO2 PLANE:1||SURFACE:1||Delafossite:1||ELECTRICALPROPERTIES:1||NIMNSB:1||PTMNSB:1||ROOMTEMPERATURE FERROMAGNETISM:1||RUBIDIUM MANGANESE HEXACYANOFERRATE:1||COLOSSALMAGNETORESISTANCE:1||FINITE TEMPERATURES:1||LAMNO3:1||FE:1||transitionmetal oxides:1||giant magnetoresistance:1||phonon:1||COPPER OXIDES:1||valence states:1||thermoelectric:1||semiconductor:1||CATION DISTRIBUTION:1||FeCr2S4:1||photoemission spectroscopy (PES):1||METALLIC FERROMAGNETISM:1||GRAPHITE:1||SUSCEPTIBILITY:1||UBE13:1||RCrSb3:1||band JahnTeller:1||Ce3S4:1||TiO2:1||PrBa2Cu3O7delta:1||UNTWINNED PRBA2CU3O7:1||AGNIO2:1||HALFMETALLIC FERROMAGNETS:1||CI:1||Energy gap:1||Photoemission:1||Future applications:1||Photoemission measurements:1||Graphene:1||BANDSTRUCTURE:1||TC:1||superconductivity:1||magnetic semiconductors:1||CMRmanganites:1||thin films:1||spin dynamics:1||highTc superconductors:1||ITINERANTELECTRON FERROMAGNETISM:1||SINGLECRYSTALS:1||CeTe2:1||amorphous magnetic materials:1||EPITAXIAL GRAPHENE:1||LAYERED PNICTIDEOXIDES:1||BOROCARBIDE SUPERCONDUCTORS:1||AUGMENTEDWAVE METHOD:1||METALLIC MAGNET UNISN:1||ORIGIN:1||spectrum rearrangement:1||MEANFIELD THEORY:1||MOLECULEBASED MAGNETS:1||METASTABLE STATE:1||INSULATOR:1||magnetic orderin:1||FCC IRON:1||CeRu2:1||TL2MN2O7:1||isotope effect:1||Perovskitemanganites:1||RECURSION METHOD:1||PERPENDICULAR MAGNETICANISOTROPY:1||quasiparticle spectral density:1||GW:1||MANGANESE FERRITE:1||RESONANCE:1||SeCuO3:1||Optical conductivity:1||MASSLESS DIRAC FERMIONS:1||SCHOTTKYBARRIER:1||electronic structure:15||ELECTRONICSTRUCTURE:11||TRANSITIONMETAL COMPOUNDS:10||METALS:10||photoemission:8||SPECTRA:8||MAGNETORESISTANCE:7||FERROMAGNETISM:7||TRANSPORT:7||TRANSITION:6||FILMS:6||THINFILMS:5||TOTALENERGY CALCULATIONS:5||MAGNETICPROPERTIES:5||SUPERCONDUCTIVITY:5||PR:5||LATTICE:4||STATES:4||SPECTROSCOPY:4||FIELD:4||CRYSTALSTRUCTURE:4||PHOTOEMISSION:4||TEMPERATURE:4||TRANSITIONTEMPERATURE:4||XRAYABSORPTION:4||STATE:4||CU:4||BASISSET:4||XAS:4||CRYSTALS:3||EXCITATIONS:3||MOTTHUBBARD SYSTEMS:3||HIGHENERGY SPIN:3||halfmetal:3||INSULATORS:3||LA2CUO4:3||MODEL:3||FLUCTUATIONS:3||CE:3||double exchange:3||TRANSITIONMETALS:3||RESISTIVITY:3||BORON:3||LA1XCAXMNO3:3||IRON:3||PES:3||ANTIMONIDES:2||MgB2:2||ZR METALLIC GLASSES:2||superconductor:2||CRITICALCURRENT DENSITY:2||CIRCULARDICHROISM:2||SEMICONDUCTORS:2||LOCALIZATION:2||INTRABAND OPTICAL CONDUCTIVITY:2||COLOSSAL MAGNETORESISTANCE:2||OXIDATION:2||EXISTENCE:2||COPPER:2||diboride:2||MAGNESIUMDIBORIDE:2||GAP:2||CE COMPOUNDS:2||CORE POLARIZATION:2||magnetoresistance:2||photoemission spectroscopy:2||electronphonon interaction:2||GETTER:2||PD:2||MAGNETISM:2||FECR2S4:2||SUPERCONDUCTING MGB2:2||WIRES:2||ABSORPTION:2||ENERGY:2||LA1XSRXMNO3:2||CONSTANTS:2||polaron:2||charge ordering:2||SCATTERING:2||XRAY PHOTOEMISSION:2||CeNiSn:2||phase diagram:2||PHOTOELECTRON:2||QUADRUPOLAR:2||perovskitemanganites:2||CO:2||SYSTEMS:2||DOPED ZNO:2||LOWFREQUENCY SOUND:2||LA:2||ELECTRONELECTRON SCATTERING:2||AU:2||DENSITYWAVE INSTABILITY:2||FERMISURFACE:2||hybridization:2||VALENCEBAND SATELLITE:2||SULFUR SPINEL:2||Heusler:2||APPROXIMATION:2||superexchange:2||colossal magnetoresistance:2||ALLOYS:2||DEPENDENCE:2||AG:2||electronic structures:2||AUGERSPECTRA:2||CR:2||PARAMETERS:2||DIFFRACTION:2||SEMICONDUCTORMETAL TRANSITION:1||INTERMEDIATEVALENCE:1||SMB6:1||SRRUO3:1||antiperovskite structure with antipolar nature:1||lowenergy twodimensional phonons:1||anatase TiO2:1||La3S4:1||metalinsulator transitions:1||MNO:1||ELECTRONICSTRUCTURES:1||MAGNETIC CIRCULARDICHROISM:1||Density functional theory:1||CeCo2:1||TOPOLARON CROSSOVER:1||EXCHANGE:1||cuprates:1||high Tc cuprates:1||magnetically ordered materials:1||ZNSE:1||Sr2xKxFeMoO6:1||CDW:1||TeCuO3:1||STRUCTURALPROPERTIES:1||MN:1||screening length:1||amorphous Fe:1||WAVE BASISSET:1||SILICONCARBIDE:1||HIGHPRESSURE:1||electronphonon coupling:1||quenched superconductivity:1||CMR perovskite manganites:1||OXIDE:1||polarons:1||synchrotron radiation:1||FULLERIDES:1||RESONANTPHOTOEMISSION:1||Silicon carbide:1||DFT calculation:1||Hybridized bands:1||GIANT MAGNETORESISTANCE:1||PEROVSKITES:1||Raman spectra:1||EXCHANGE ENHANCEMENT:1||SILICON:1||SR2FEMOO6:1||orbital ordering:1||delafossite:1||TITANIUMDIOXIDE:1||electronic structure of disordered solids:1||YFE2:1||Magnetic polaron:1||NA2TI2SB2O:1||STRONGCOUPLED SUPERCONDUCTORS:1||HEAVYFERMION SYSTEMS:1||firstprinciples calculations:1||MECHANISM:1||UNiSn:1||PHOTONIC BANDGAP:1||SINGLE IMPURITY:1||PHONONSPECTRUM:1||FERMISURFACE TOPOLOGY:1||SUPPRESSION:1||RESONANT PHOTOEMISSION:1||METALDOPED PICENE:1||PHOTOIONIZATION CROSSSECTIONS:1||PHOTOINDUCED FERRIMAGNETIC SYSTEMS:1||LINKAGE ISOMERISM:1||CHARGETRANSFER:1||Bilayer Graphene:1||MAGNETICFIELD:1||SPINWAVES:1||rareearth manganese oxides:1||magnonphonon interaction:1||NACO2O4:1||ENERGYBANDS:1||SELFENERGY:1||GAS:1||Fe0.5Cu0.5Cr2S4:1||scanning photoelectron microscopy (SPEM):1||MAGNETIC PROPERTIES:1||Stoner model:1||AMORPHOUS TRANSITIONMETALS:1||SPINGLASS STATES:1||NI:1||LA3NI2B2N3:1||SOLIDS:1||CEO2:1||BAND THEORY:1||dilute magnetic semiconductor:1||pyrochlore:1||Y1XPRXBA2CU3O7DELTA:1||and electronphonon interactions:1||VIBRATIONS:1||RAY PHOTOEMISSION:1||ALKALI CATION:1||Europium:1||colossal magnetoresistance:1||structural stability:1||ENERGYGAP:1||small polaron:1||DOUBLE EXCHANGE:1||Coulomb correlation:1||magnon:1||phonons:1||ELECTRON FERROMAGNETISM:1||CURIETEMPERATURE:1||ARPES:1||PLANEWAVE METHOD:1||Xray absorption spectroscopy (XAS):1||ROOMTEMPERATURE:1||MONOCHALCOGENIDES:1||HEAT:1||UPDSN:1||MOMENTS:1||XRAY ABSORPTION:1||SEMICONDUCTOR:1||Fermi surface nesting:1||optical phonon:1||disordered system:1||dilute magnetic semiconductors:1||CMR manganites:1||PHONONS:1||LATTICEDYNAMICS:1||OXIDES:1||4fphotoemission:1||permanent magnet:1||pseudogap:1||TRANSPORTPROPERTIES:1||ANTIFERROMAGNET:1||(BI,PB)SRCOO SYSTEM:1||semicore correlation:1||POLARIZATION:1||CRYSTAL:1||spinel:1||Xray magnetic circular dichroism (XMCD):1||magnetocapacitance:1||ANATASE:1||TEMPERATURES:1||Pseudogap:1||INTERFACE:1||SUBSTRATE:1||YNI2B2C:1||SAMARIUM SULFIDE:1||strong swave superconductor:1||DOPED MANGANITE:1||SYMMETRY:1||CENISN:1||resonance mode:1||DISORDERED SYSTEM:1||LITHIUM INTERCALATION:1||CUO2 PLANE:1||SURFACE:1||Delafossite:1||ELECTRICALPROPERTIES:1||NIMNSB:1||PTMNSB:1||ROOMTEMPERATURE FERROMAGNETISM:1||RUBIDIUM MANGANESE HEXACYANOFERRATE:1||COLOSSALMAGNETORESISTANCE:1||FINITE TEMPERATURES:1||LAMNO3:1||FE:1||transitionmetal oxides:1||giant magnetoresistance:1||phonon:1||COPPER OXIDES:1||valence states:1||thermoelectric:1||semiconductor:1||CATION DISTRIBUTION:1||FeCr2S4:1||photoemission spectroscopy (PES):1||METALLIC FERROMAGNETISM:1||GRAPHITE:1||SUSCEPTIBILITY:1||UBE13:1||RCrSb3:1||band JahnTeller:1||Ce3S4:1||TiO2:1||PrBa2Cu3O7delta:1||UNTWINNED PRBA2CU3O7:1||AGNIO2:1||HALFMETALLIC FERROMAGNETS:1||CI:1||Energy gap:1||Photoemission:1||Future applications:1||Photoemission measurements:1||Graphene:1||BANDSTRUCTURE:1||TC:1||superconductivity:1||magnetic semiconductors:1||CMRmanganites:1||thin films:1||spin dynamics:1||highTc superconductors:1||ITINERANTELECTRON FERROMAGNETISM:1||SINGLECRYSTALS:1||CeTe2:1||amorphous magnetic materials:1||EPITAXIAL GRAPHENE:1||LAYERED PNICTIDEOXIDES:1||BOROCARBIDE SUPERCONDUCTORS:1||AUGMENTEDWAVE METHOD:1||METALLIC MAGNET UNISN:1||ORIGIN:1||spectrum rearrangement:1||MEANFIELD THEORY:1||MOLECULEBASED MAGNETS:1||METASTABLE STATE:1||INSULATOR:1||magnetic orderin:1||FCC IRON:1||CeRu2:1||TL2MN2O7:1||isotope effect:1||Perovskitemanganites:1||RECURSION METHOD:1||PERPENDICULAR MAGNETICANISOTROPY:1||quasiparticle spectral density:1||GW:1||MANGANESE FERRITE:1||RESONANCE:1||SeCuO3:1||Optical conductivity:1||MASSLESS DIRAC FERMIONS:1||SCHOTTKYBARRIER:1||electronic structure:15||ELECTRONICSTRUCTURE:11||TRANSITIONMETAL COMPOUNDS:10||METALS:10||photoemission:8||SPECTRA:8||MAGNETORESISTANCE:7||FERROMAGNETISM:7||TRANSPORT:7||TRANSITION:6||FILMS:6||THINFILMS:5||TOTALENERGY CALCULATIONS:5||MAGNETICPROPERTIES:5||SUPERCONDUCTIVITY:5||PR:5||LATTICE:4||STATES:4||SPECTROSCOPY:4||FIELD:4||CRYSTALSTRUCTURE:4||PHOTOEMISSION:4||TEMPERATURE:4||TRANSITIONTEMPERATURE:4||XRAYABSORPTION:4||STATE:4||CU:4||BASISSET:4||XAS:4||CRYSTALS:3||EXCITATIONS:3||MOTTHUBBARD SYSTEMS:3||HIGHENERGY SPIN:3||halfmetal:3||INSULATORS:3||LA2CUO4:3||MODEL:3||FLUCTUATIONS:3||CE:3||double exchange:3||TRANSITIONMETALS:3||RESISTIVITY:3||BORON:3||LA1XCAXMNO3:3||IRON:3||PES:3||ANTIMONIDES:2||MgB2:2||ZR METALLIC GLASSES:2||superconductor:2||CRITICALCURRENT DENSITY:2||CIRCULARDICHROISM:2||SEMICONDUCTORS:2||LOCALIZATION:2||INTRABAND OPTICAL CONDUCTIVITY:2||COLOSSAL MAGNETORESISTANCE:2||OXIDATION:2||EXISTENCE:2||COPPER:2||diboride:2||MAGNESIUMDIBORIDE:2||GAP:2||CE COMPOUNDS:2||CORE POLARIZATION:2||magnetoresistance:2||photoemission spectroscopy:2||electronphonon interaction:2||GETTER:2||PD:2||MAGNETISM:2||FECR2S4:2||SUPERCONDUCTING MGB2:2||WIRES:2||ABSORPTION:2||ENERGY:2||LA1XSRXMNO3:2||CONSTANTS:2||polaron:2||charge ordering:2||SCATTERING:2||XRAY PHOTOEMISSION:2||CeNiSn:2||phase diagram:2||PHOTOELECTRON:2||QUADRUPOLAR:2||perovskitemanganites:2||CO:2||SYSTEMS:2||DOPED ZNO:2||LOWFREQUENCY SOUND:2||LA:2||ELECTRONELECTRON SCATTERING:2||AU:2||DENSITYWAVE INSTABILITY:2||FERMISURFACE:2||hybridization:2||VALENCEBAND SATELLITE:2||SULFUR SPINEL:2||Heusler:2||APPROXIMATION:2||superexchange:2||colossal magnetoresistance:2||ALLOYS:2||DEPENDENCE:2||AG:2||electronic structures:2||AUGERSPECTRA:2||CR:2||PARAMETERS:2||DIFFRACTION:2||SEMICONDUCTORMETAL TRANSITION:1||INTERMEDIATEVALENCE:1||SMB6:1||SRRUO3:1||antiperovskite structure with antipolar nature:1||lowenergy twodimensional phonons:1||anatase TiO2:1||La3S4:1||metalinsulator transitions:1||MNO:1||ELECTRONICSTRUCTURES:1||MAGNETIC CIRCULARDICHROISM:1||Density functional theory:1||CeCo2:1||TOPOLARON CROSSOVER:1||EXCHANGE:1||cuprates:1||high Tc cuprates:1||magnetically ordered materials:1||ZNSE:1||Sr2xKxFeMoO6:1||CDW:1||TeCuO3:1||STRUCTURALPROPERTIES:1||MN:1||screening length:1||amorphous Fe:1||WAVE BASISSET:1||SILICONCARBIDE:1||HIGHPRESSURE:1||electronphonon coupling:1||quenched superconductivity:1||CMR perovskite manganites:1||OXIDE:1||polarons:1||synchrotron radiation:1||FULLERIDES:1||RESONANTPHOTOEMISSION:1||Silicon carbide:1||DFT calculation:1||Hybridized bands:1||GIANT MAGNETORESISTANCE:1||PEROVSKITES:1||Raman spectra:1||EXCHANGE ENHANCEMENT:1||SILICON:1||SR2FEMOO6:1||orbital ordering:1||delafossite:1||TITANIUMDIOXIDE:1||electronic structure of disordered solids:1||YFE2:1||Magnetic polaron:1||NA2TI2SB2O:1||STRONGCOUPLED SUPERCONDUCTORS:1||HEAVYFERMION SYSTEMS:1||firstprinciples calculations:1||MECHANISM:1||UNiSn:1||PHOTONIC BANDGAP:1||SINGLE IMPURITY:1||PHONONSPECTRUM:1||FERMISURFACE TOPOLOGY:1||SUPPRESSION:1||RESONANT PHOTOEMISSION:1||METALDOPED PICENE:1||PHOTOIONIZATION CROSSSECTIONS:1||PHOTOINDUCED FERRIMAGNETIC SYSTEMS:1||LINKAGE ISOMERISM:1||CHARGETRANSFER:1||Bilayer Graphene:1||MAGNETICFIELD:1||SPINWAVES:1||rareearth manganese oxides:1||magnonphonon interaction:1||NACO2O4:1||ENERGYBANDS:1||SELFENERGY:1||GAS:1||Fe0.5Cu0.5Cr2S4:1||scanning photoelectron microscopy (SPEM):1||MAGNETIC PROPERTIES:1||Stoner model:1||AMORPHOUS TRANSITIONMETALS:1||SPINGLASS STATES:1||NI:1||LA3NI2B2N3:1||SOLIDS:1||CEO2:1||BAND THEORY:1||dilute magnetic semiconductor:1||pyrochlore:1||Y1XPRXBA2CU3O7DELTA:1||and electronphonon interactions:1||VIBRATIONS:1||RAY PHOTOEMISSION:1||ALKALI CATION:1||Europium:1||colossal magnetoresistance:1||structural stability:1||ENERGYGAP:1||small polaron:1||DOUBLE EXCHANGE:1||Coulomb correlation:1||magnon:1||phonons:1||ELECTRON FERROMAGNETISM:1||CURIETEMPERATURE:1||ARPES:1||PLANEWAVE METHOD:1||Xray absorption spectroscopy (XAS):1||ROOMTEMPERATURE:1||MONOCHALCOGENIDES:1||HEAT:1||UPDSN:1||MOMENTS:1||XRAY ABSORPTION:1||SEMICONDUCTOR:1||Fermi surface nesting:1||optical phonon:1||disordered system:1||dilute magnetic semiconductors:1||CMR manganites:1||PHONONS:1||LATTICEDYNAMICS:1||OXIDES:1||4fphotoemission:1||permanent magnet:1||pseudogap:1||TRANSPORTPROPERTIES:1||ANTIFERROMAGNET:1||(BI,PB)SRCOO SYSTEM:1||semicore correlation:1||POLARIZATION:1||CRYSTAL:1||spinel:1||Xray magnetic circular dichroism (XMCD):1||magnetocapacitance:1||ANATASE:1||TEMPERATURES:1||Pseudogap:1||INTERFACE:1||SUBSTRATE:1||YNI2B2C:1||SAMARIUM SULFIDE:1||strong swave superconductor:1||DOPED MANGANITE:1||SYMMETRY:1||CENISN:1||resonance mode:1||DISORDERED SYSTEM:1||LITHIUM INTERCALATION:1||CUO2 PLANE:1||SURFACE:1||Delafossite:1||ELECTRICALPROPERTIES:1||NIMNSB:1||PTMNSB:1||ROOMTEMPERATURE FERROMAGNETISM:1||RUBIDIUM MANGANESE HEXACYANOFERRATE:1||COLOSSALMAGNETORESISTANCE:1||FINITE TEMPERATURES:1||LAMNO3:1||FE:1||transitionmetal oxides:1||giant magnetoresistance:1||phonon:1||COPPER OXIDES:1||valence states:1||thermoelectric:1||semiconductor:1||CATION DISTRIBUTION:1||FeCr2S4:1||photoemission spectroscopy (PES):1||METALLIC FERROMAGNETISM:1||GRAPHITE:1||SUSCEPTIBILITY:1||UBE13:1||RCrSb3:1||band JahnTeller:1||Ce3S4:1||TiO2:1||PrBa2Cu3O7delta:1||UNTWINNED PRBA2CU3O7:1||AGNIO2:1||HALFMETALLIC FERROMAGNETS:1||CI:1||Energy gap:1||Photoemission:1||Future applications:1||Photoemission measurements:1||Graphene:1||BANDSTRUCTURE:1||TC:1||superconductivity:1||magnetic semiconductors:1||CMRmanganites:1||thin films:1||spin dynamics:1||highTc superconductors:1||ITINERANTELECTRON FERROMAGNETISM:1||SINGLECRYSTALS:1||CeTe2:1||amorphous magnetic materials:1||EPITAXIAL GRAPHENE:1||LAYERED PNICTIDEOXIDES:1||BOROCARBIDE SUPERCONDUCTORS:1||AUGMENTEDWAVE METHOD:1||METALLIC MAGNET UNISN:1||ORIGIN:1||spectrum rearrangement:1||MEANFIELD THEORY:1||MOLECULEBASED MAGNETS:1||METASTABLE STATE:1||INSULATOR:1||magnetic orderin:1||FCC IRON:1||CeRu2:1||TL2MN2O7:1||isotope effect:1||Perovskitemanganites:1||RECURSION METHOD:1||PERPENDICULAR MAGNETICANISOTROPY:1||quasiparticle spectral density:1||GW:1||MANGANESE FERRITE:1||RESONANCE:1||SeCuO3:1||Optical conductivity:1||MASSLESS DIRAC FERMIONS:1||SCHOTTKYBARRIER:1||electronic structure:15||ELECTRONICSTRUCTURE:11||TRANSITIONMETAL COMPOUNDS:10||METALS:10||photoemission:8||SPECTRA:8||MAGNETORESISTANCE:7||FERROMAGNETISM:7||TRANSPORT:7||TRANSITION:6||FILMS:6||THINFILMS:5||TOTALENERGY CALCULATIONS:5||MAGNETICPROPERTIES:5||SUPERCONDUCTIVITY:5||PR:5||LATTICE:4||STATES:4||SPECTROSCOPY:4||FIELD:4||CRYSTALSTRUCTURE:4||PHOTOEMISSION:4||TEMPERATURE:4||TRANSITIONTEMPERATURE:4||XRAYABSORPTION:4||STATE:4||CU:4||BASISSET:4||XAS:4||CRYSTALS:3||EXCITATIONS:3||MOTTHUBBARD SYSTEMS:3||HIGHENERGY SPIN:3||halfmetal:3||INSULATORS:3||LA2CUO4:3||MODEL:3||FLUCTUATIONS:3||CE:3||double exchange:3||TRANSITIONMETALS:3||RESISTIVITY:3||BORON:3||LA1XCAXMNO3:3||IRON:3||PES:3||ANTIMONIDES:2||MgB2:2||ZR METALLIC GLASSES:2||superconductor:2||CRITICALCURRENT DENSITY:2||CIRCULARDICHROISM:2||SEMICONDUCTORS:2||LOCALIZATION:2||INTRABAND OPTICAL CONDUCTIVITY:2||COLOSSAL MAGNETORESISTANCE:2||OXIDATION:2||EXISTENCE:2||COPPER:2||diboride:2||MAGNESIUMDIBORIDE:2||GAP:2||CE COMPOUNDS:2||CORE POLARIZATION:2||magnetoresistance:2||photoemission spectroscopy:2||electronphonon interaction:2||GETTER:2||PD:2||MAGNETISM:2||FECR2S4:2||SUPERCONDUCTING MGB2:2||WIRES:2||ABSORPTION:2||ENERGY:2||LA1XSRXMNO3:2||CONSTANTS:2||polaron:2||charge ordering:2||SCATTERING:2||XRAY PHOTOEMISSION:2||CeNiSn:2||phase diagram:2||PHOTOELECTRON:2||QUADRUPOLAR:2||perovskitemanganites:2||CO:2||SYSTEMS:2||DOPED ZNO:2||LOWFREQUENCY SOUND:2||LA:2||ELECTRONELECTRON SCATTERING:2||AU:2||DENSITYWAVE INSTABILITY:2||FERMISURFACE:2||hybridization:2||VALENCEBAND SATELLITE:2||SULFUR SPINEL:2||Heusler:2||APPROXIMATION:2||superexchange:2||colossal magnetoresistance:2||ALLOYS:2||DEPENDENCE:2||AG:2||electronic structures:2||AUGERSPECTRA:2||CR:2||PARAMETERS:2||DIFFRACTION:2||SEMICONDUCTORMETAL TRANSITION:1||INTERMEDIATEVALENCE:1||SMB6:1||SRRUO3:1||antiperovskite structure with antipolar nature:1||lowenergy twodimensional phonons:1||anatase TiO2:1||La3S4:1||metalinsulator transitions:1||MNO:1||ELECTRONICSTRUCTURES:1||MAGNETIC CIRCULARDICHROISM:1||Density functional theory:1||CeCo2:1||TOPOLARON CROSSOVER:1||EXCHANGE:1||cuprates:1||high Tc cuprates:1||magnetically ordered materials:1||ZNSE:1||Sr2xKxFeMoO6:1||CDW:1||TeCuO3:1||STRUCTURALPROPERTIES:1||MN:1||screening length:1||amorphous Fe:1||WAVE BASISSET:1||SILICONCARBIDE:1||HIGHPRESSURE:1||electronphonon coupling:1||quenched superconductivity:1||CMR perovskite manganites:1||OXIDE:1||polarons:1||synchrotron radiation:1||FULLERIDES:1||RESONANTPHOTOEMISSION:1||Silicon carbide:1||DFT calculation:1||Hybridized bands:1||GIANT MAGNETORESISTANCE:1||PEROVSKITES:1||Raman spectra:1||EXCHANGE ENHANCEMENT:1||SILICON:1||SR2FEMOO6:1||orbital ordering:1||delafossite:1||TITANIUMDIOXIDE:1||electronic structure of disordered solids:1||YFE2:1||Magnetic polaron:1||NA2TI2SB2O:1||STRONGCOUPLED SUPERCONDUCTORS:1||HEAVYFERMION SYSTEMS:1||firstprinciples calculations:1||MECHANISM:1||UNiSn:1||PHOTONIC BANDGAP:1||SINGLE IMPURITY:1||PHONONSPECTRUM:1||FERMISURFACE TOPOLOGY:1||SUPPRESSION:1||RESONANT PHOTOEMISSION:1||METALDOPED PICENE:1||PHOTOIONIZATION CROSSSECTIONS:1||PHOTOINDUCED FERRIMAGNETIC SYSTEMS:1||LINKAGE ISOMERISM:1||CHARGETRANSFER:1||Bilayer Graphene:1||MAGNETICFIELD:1||SPINWAVES:1||rareearth manganese oxides:1||magnonphonon interaction:1||NACO2O4:1||ENERGYBANDS:1||SELFENERGY:1||GAS:1||Fe0.5Cu0.5Cr2S4:1||scanning photoelectron microscopy (SPEM):1||MAGNETIC PROPERTIES:1||Stoner model:1||AMORPHOUS TRANSITIONMETALS:1||SPINGLASS STATES:1||NI:1||LA3NI2B2N3:1||SOLIDS:1||CEO2:1||BAND THEORY:1||dilute magnetic semiconductor:1||pyrochlore:1||Y1XPRXBA2CU3O7DELTA:1||and electronphonon interactions:1||VIBRATIONS:1||RAY PHOTOEMISSION:1||ALKALI CATION:1||Europium:1||colossal magnetoresistance:1||structural stability:1||ENERGYGAP:1||small polaron:1||DOUBLE EXCHANGE:1||Coulomb correlation:1||magnon:1||phonons:1||ELECTRON FERROMAGNETISM:1||CURIETEMPERATURE:1||ARPES:1||PLANEWAVE METHOD:1||Xray absorption spectroscopy (XAS):1||ROOMTEMPERATURE:1||MONOCHALCOGENIDES:1||HEAT:1||UPDSN:1||MOMENTS:1||XRAY ABSORPTION:1||SEMICONDUCTOR:1||Fermi surface nesting:1||optical phonon:1||disordered system:1||dilute magnetic semiconductors:1||CMR manganites:1||PHONONS:1||LATTICEDYNAMICS:1||OXIDES:1||4fphotoemission:1||permanent magnet:1||pseudogap:1||TRANSPORTPROPERTIES:1||ANTIFERROMAGNET:1||(BI,PB)SRCOO SYSTEM:1||semicore correlation:1||POLARIZATION:1||CRYSTAL:1||spinel:1||Xray magnetic circular dichroism (XMCD):1||magnetocapacitance:1||ANATASE:1||TEMPERATURES:1||Pseudogap:1||INTERFACE:1||SUBSTRATE:1||YNI2B2C:1||SAMARIUM SULFIDE:1||strong swave superconductor:1||DOPED MANGANITE:1||SYMMETRY:1||CENISN:1||resonance mode:1||DISORDERED SYSTEM:1||LITHIUM INTERCALATION:1||CUO2 PLANE:1||SURFACE:1||Delafossite:1||ELECTRICALPROPERTIES:1||NIMNSB:1||PTMNSB:1||ROOMTEMPERATURE FERROMAGNETISM:1||RUBIDIUM MANGANESE HEXACYANOFERRATE:1||COLOSSALMAGNETORESISTANCE:1||FINITE TEMPERATURES:1||LAMNO3:1||FE:1||transitionmetal oxides:1||giant magnetoresistance:1||phonon:1||COPPER OXIDES:1||valence states:1||thermoelectric:1||semiconductor:1||CATION DISTRIBUTION:1||FeCr2S4:1||photoemission spectroscopy (PES):1||METALLIC FERROMAGNETISM:1||GRAPHITE:1||SUSCEPTIBILITY:1||UBE13:1||RCrSb3:1||band JahnTeller:1||Ce3S4:1||TiO2:1||PrBa2Cu3O7delta:1||UNTWINNED PRBA2CU3O7:1||AGNIO2:1||HALFMETALLIC FERROMAGNETS:1||CI:1||Energy gap:1||Photoemission:1||Future applications:1||Photoemission measurements:1||Graphene:1||BANDSTRUCTURE:1||TC:1||superconductivity:1||magnetic semiconductors:1||CMRmanganites:1||thin films:1||spin dynamics:1||highTc superconductors:1||ITINERANTELECTRON FERROMAGNETISM:1||SINGLECRYSTALS:1||CeTe2:1||amorphous magnetic materials:1||EPITAXIAL GRAPHENE:1||LAYERED PNICTIDEOXIDES:1||BOROCARBIDE SUPERCONDUCTORS:1||AUGMENTEDWAVE METHOD:1||METALLIC MAGNET UNISN:1||ORIGIN:1||spectrum rearrangement:1||MEANFIELD THEORY:1||MOLECULEBASED MAGNETS:1||METASTABLE STATE:1||INSULATOR:1||magnetic orderin:1||FCC IRON:1||CeRu2:1||TL2MN2O7:1||isotope effect:1||Perovskitemanganites:1||RECURSION METHOD:1||PERPENDICULAR MAGNETICANISOTROPY:1||quasiparticle spectral density:1||GW:1||MANGANESE FERRITE:1||RESONANCE:1||SeCuO3:1||Optical conductivity:1||MASSLESS DIRAC FERMIONS:1||SCHOTTKYBARRIER:1||electronic structure:15||ELECTRONICSTRUCTURE:11||TRANSITIONMETAL COMPOUNDS:10||METALS:10||photoemission:8||SPECTRA:8||MAGNETORESISTANCE:7||FERROMAGNETISM:7||TRANSPORT:7||TRANSITION:6||FILMS:6||THINFILMS:5||TOTALENERGY CALCULATIONS:5||MAGNETICPROPERTIES:5||SUPERCONDUCTIVITY:5||PR:5||LATTICE:4||STATES:4||SPECTROSCOPY:4||FIELD:4||CRYSTALSTRUCTURE:4||PHOTOEMISSION:4||TEMPERATURE:4||TRANSITIONTEMPERATURE:4||XRAYABSORPTION:4||STATE:4||CU:4||BASISSET:4||XAS:4||CRYSTALS:3||EXCITATIONS:3||MOTTHUBBARD SYSTEMS:3||HIGHENERGY SPIN:3||halfmetal:3||INSULATORS:3||LA2CUO4:3||MODEL:3||FLUCTUATIONS:3||CE:3||double exchange:3||TRANSITIONMETALS:3||RESISTIVITY:3||BORON:3||LA1XCAXMNO3:3||IRON:3||PES:3||ANTIMONIDES:2||MgB2:2||ZR METALLIC GLASSES:2||superconductor:2||CRITICALCURRENT DENSITY:2||CIRCULARDICHROISM:2||SEMICONDUCTORS:2||LOCALIZATION:2||INTRABAND OPTICAL CONDUCTIVITY:2||COLOSSAL MAGNETORESISTANCE:2||OXIDATION:2||EXISTENCE:2||COPPER:2||diboride:2||MAGNESIUMDIBORIDE:2||GAP:2||CE COMPOUNDS:2||CORE POLARIZATION:2||magnetoresistance:2||photoemission spectroscopy:2||electronphonon interaction:2||GETTER:2||PD:2||MAGNETISM:2||FECR2S4:2||SUPERCONDUCTING MGB2:2||WIRES:2||ABSORPTION:2||ENERGY:2||LA1XSRXMNO3:2||CONSTANTS:2||polaron:2||charge ordering:2||SCATTERING:2||XRAY PHOTOEMISSION:2||CeNiSn:2||phase diagram:2||PHOTOELECTRON:2||QUADRUPOLAR:2||perovskitemanganites:2||CO:2||SYSTEMS:2||DOPED ZNO:2||LOWFREQUENCY SOUND:2||LA:2||ELECTRONELECTRON SCATTERING:2||AU:2||DENSITYWAVE INSTABILITY:2||FERMISURFACE:2||hybridization:2||VALENCEBAND SATELLITE:2||SULFUR SPINEL:2||Heusler:2||APPROXIMATION:2||superexchange:2||colossal magnetoresistance:2||ALLOYS:2||DEPENDENCE:2||AG:2||electronic structures:2||AUGERSPECTRA:2||CR:2||PARAMETERS:2||DIFFRACTION:2||SEMICONDUCTORMETAL TRANSITION:1||INTERMEDIATEVALENCE:1||SMB6:1||SRRUO3:1||antiperovskite structure with antipolar nature:1||lowenergy twodimensional phonons:1||anatase TiO2:1||La3S4:1||metalinsulator transitions:1||MNO:1||ELECTRONICSTRUCTURES:1||MAGNETIC CIRCULARDICHROISM:1||Density functional theory:1||CeCo2:1||TOPOLARON CROSSOVER:1||EXCHANGE:1||cuprates:1||high Tc cuprates:1||magnetically ordered materials:1||ZNSE:1||Sr2xKxFeMoO6:1||CDW:1||TeCuO3:1||STRUCTURALPROPERTIES:1||MN:1||screening length:1||amorphous Fe:1||WAVE BASISSET:1||SILICONCARBIDE:1||HIGHPRESSURE:1||electronphonon coupling:1||quenched superconductivity:1||CMR perovskite manganites:1||OXIDE:1||polarons:1||synchrotron radiation:1||FULLERIDES:1||RESONANTPHOTOEMISSION:1||Silicon carbide:1||DFT calculation:1||Hybridized bands:1||GIANT MAGNETORESISTANCE:1||PEROVSKITES:1||Raman spectra:1||EXCHANGE ENHANCEMENT:1||SILICON:1||SR2FEMOO6:1||orbital ordering:1||delafossite:1||TITANIUMDIOXIDE:1||electronic structure of disordered solids:1||YFE2:1||Magnetic polaron:1||NA2TI2SB2O:1||STRONGCOUPLED SUPERCONDUCTORS:1||HEAVYFERMION SYSTEMS:1||firstprinciples calculations:1||MECHANISM:1||UNiSn:1||PHOTONIC BANDGAP:1||SINGLE IMPURITY:1||PHONONSPECTRUM:1||FERMISURFACE TOPOLOGY:1||SUPPRESSION:1||RESONANT PHOTOEMISSION:1||METALDOPED PICENE:1||PHOTOIONIZATION CROSSSECTIONS:1||PHOTOINDUCED FERRIMAGNETIC SYSTEMS:1||LINKAGE ISOMERISM:1||CHARGETRANSFER:1||Bilayer Graphene:1||MAGNETICFIELD:1||SPINWAVES:1||rareearth manganese oxides:1||magnonphonon interaction:1||NACO2O4:1||ENERGYBANDS:1||SELFENERGY:1||GAS:1||Fe0.5Cu0.5Cr2S4:1||scanning photoelectron microscopy (SPEM):1||MAGNETIC PROPERTIES:1||Stoner model:1||AMORPHOUS TRANSITIONMETALS:1||SPINGLASS STATES:1||NI:1||LA3NI2B2N3:1||SOLIDS:1||CEO2:1||BAND THEORY:1||dilute magnetic semiconductor:1||pyrochlore:1||Y1XPRXBA2CU3O7DELTA:1||and electronphonon interactions:1||VIBRATIONS:1||RAY PHOTOEMISSION:1||ALKALI CATION:1||Europium:1||colossal magnetoresistance:1||structural stability:1||ENERGYGAP:1||small polaron:1||DOUBLE EXCHANGE:1||Coulomb correlation:1||magnon:1||phonons:1||ELECTRON FERROMAGNETISM:1||CURIETEMPERATURE:1||ARPES:1||PLANEWAVE METHOD:1||Xray absorption spectroscopy (XAS):1||ROOMTEMPERATURE:1||MONOCHALCOGENIDES:1||HEAT:1||UPDSN:1||MOMENTS:1||XRAY ABSORPTION:1||SEMICONDUCTOR:1||Fermi surface nesting:1||optical phonon:1||disordered system:1||dilute magnetic semiconductors:1||CMR manganites:1||PHONONS:1||LATTICEDYNAMICS:1||OXIDES:1||4fphotoemission:1||permanent magnet:1||pseudogap:1||TRANSPORTPROPERTIES:1||ANTIFERROMAGNET:1||(BI,PB)SRCOO SYSTEM:1||semicore correlation:1||POLARIZATION:1||CRYSTAL:1||spinel:1||Xray magnetic circular dichroism (XMCD):1||magnetocapacitance:1||ANATASE:1||TEMPERATURES:1||Pseudogap:1||INTERFACE:1||SUBSTRATE:1||YNI2B2C:1||SAMARIUM SULFIDE:1||strong swave superconductor:1||DOPED MANGANITE:1||SYMMETRY:1||CENISN:1||resonance mode:1||DISORDERED SYSTEM:1||LITHIUM INTERCALATION:1||CUO2 PLANE:1||SURFACE:1||Delafossite:1||ELECTRICALPROPERTIES:1||NIMNSB:1||PTMNSB:1||ROOMTEMPERATURE FERROMAGNETISM:1||RUBIDIUM MANGANESE HEXACYANOFERRATE:1||COLOSSALMAGNETORESISTANCE:1||FINITE TEMPERATURES:1||LAMNO3:1||FE:1||transitionmetal oxides:1||giant magnetoresistance:1||phonon:1||COPPER OXIDES:1||valence states:1||thermoelectric:1||semiconductor:1||CATION DISTRIBUTION:1||FeCr2S4:1||photoemission spectroscopy (PES):1||METALLIC FERROMAGNETISM:1||GRAPHITE:1||SUSCEPTIBILITY:1||UBE13:1||RCrSb3:1||band JahnTeller:1||Ce3S4:1||TiO2:1||PrBa2Cu3O7delta:1||UNTWINNED PRBA2CU3O7:1||AGNIO2:1||HALFMETALLIC FERROMAGNETS:1||CI:1||Energy gap:1||Photoemission:1||Future applications:1||Photoemission measurements:1||Graphene:1||BANDSTRUCTURE:1||TC:1||superconductivity:1||magnetic semiconductors:1||CMRmanganites:1||thin films:1||spin dynamics:1||highTc superconductors:1||ITINERANTELECTRON FERROMAGNETISM:1||SINGLECRYSTALS:1||CeTe2:1||amorphous magnetic materials:1||EPITAXIAL GRAPHENE:1||LAYERED PNICTIDEOXIDES:1||BOROCARBIDE SUPERCONDUCTORS:1||AUGMENTEDWAVE METHOD:1||METALLIC MAGNET UNISN:1||ORIGIN:1||spectrum rearrangement:1||MEANFIELD THEORY:1||MOLECULEBASED MAGNETS:1||METASTABLE STATE:1||INSULATOR:1||magnetic orderin:1||FCC IRON:1||CeRu2:1||TL2MN2O7:1||isotope effect:1||Perovskitemanganites:1||RECURSION METHOD:1||PERPENDICULAR MAGNETICANISOTROPY:1||quasiparticle spectral density:1||GW:1||MANGANESE FERRITE:1||RESONANCE:1||SeCuO3:1||Optical conductivity:1||MASSLESS DIRAC FERMIONS:1||SCHOTTKYBARRIER:1||electronic structure:15||ELECTRONICSTRUCTURE:11||TRANSITIONMETAL COMPOUNDS:10||METALS:10||photoemission:8||SPECTRA:8||MAGNETORESISTANCE:7||FERROMAGNETISM:7||TRANSPORT:7||TRANSITION:6||FILMS:6||THINFILMS:5||TOTALENERGY CALCULATIONS:5||MAGNETICPROPERTIES:5||SUPERCONDUCTIVITY:5||PR:5||LATTICE:4||STATES:4||SPECTROSCOPY:4||FIELD:4||CRYSTALSTRUCTURE:4||PHOTOEMISSION:4||TEMPERATURE:4||TRANSITIONTEMPERATURE:4||XRAYABSORPTION:4||STATE:4||CU:4||BASISSET:4||XAS:4||CRYSTALS:3||EXCITATIONS:3||MOTTHUBBARD SYSTEMS:3||HIGHENERGY SPIN:3||halfmetal:3||INSULATORS:3||LA2CUO4:3||MODEL:3||FLUCTUATIONS:3||CE:3||double exchange:3||TRANSITIONMETALS:3||RESISTIVITY:3||BORON:3||LA1XCAXMNO3:3||IRON:3||PES:3||ANTIMONIDES:2||MgB2:2||ZR METALLIC GLASSES:2||superconductor:2||CRITICALCURRENT DENSITY:2||CIRCULARDICHROISM:2||SEMICONDUCTORS:2||LOCALIZATION:2||INTRABAND OPTICAL CONDUCTIVITY:2||COLOSSAL MAGNETORESISTANCE:2||OXIDATION:2||EXISTENCE:2||COPPER:2||diboride:2||MAGNESIUMDIBORIDE:2||GAP:2||CE COMPOUNDS:2||CORE POLARIZATION:2||magnetoresistance:2||photoemission spectroscopy:2||electronphonon interaction:2||GETTER:2||PD:2||MAGNETISM:2||FECR2S4:2||SUPERCONDUCTING MGB2:2||WIRES:2||ABSORPTION:2||ENERGY:2||LA1XSRXMNO3:2||CONSTANTS:2||polaron:2||charge ordering:2||SCATTERING:2||XRAY PHOTOEMISSION:2||CeNiSn:2||phase diagram:2||PHOTOELECTRON:2||QUADRUPOLAR:2||perovskitemanganites:2||CO:2||SYSTEMS:2||DOPED ZNO:2||LOWFREQUENCY SOUND:2||LA:2||ELECTRONELECTRON SCATTERING:2||AU:2||DENSITYWAVE INSTABILITY:2||FERMISURFACE:2||hybridization:2||VALENCEBAND SATELLITE:2||SULFUR SPINEL:2||Heusler:2||APPROXIMATION:2||superexchange:2||colossal magnetoresistance:2||ALLOYS:2||DEPENDENCE:2||AG:2||electronic structures:2||AUGERSPECTRA:2||CR:2||PARAMETERS:2||DIFFRACTION:2||SEMICONDUCTORMETAL TRANSITION:1||INTERMEDIATEVALENCE:1||SMB6:1||SRRUO3:1||antiperovskite structure with antipolar nature:1||lowenergy twodimensional phonons:1||anatase TiO2:1||La3S4:1||metalinsulator transitions:1||MNO:1||ELECTRONICSTRUCTURES:1||MAGNETIC CIRCULARDICHROISM:1||Density functional theory:1||CeCo2:1||TOPOLARON CROSSOVER:1||EXCHANGE:1||cuprates:1||high Tc cuprates:1||magnetically ordered materials:1||ZNSE:1||Sr2xKxFeMoO6:1||CDW:1||TeCuO3:1||STRUCTURALPROPERTIES:1||MN:1||screening length:1||amorphous Fe:1||WAVE BASISSET:1||SILICONCARBIDE:1||HIGHPRESSURE:1||electronphonon coupling:1||quenched superconductivity:1||CMR perovskite manganites:1||OXIDE:1||polarons:1||synchrotron radiation:1||FULLERIDES:1||RESONANTPHOTOEMISSION:1||Silicon carbide:1||DFT calculation:1||Hybridized bands:1||GIANT MAGNETORESISTANCE:1||PEROVSKITES:1||Raman spectra:1||EXCHANGE ENHANCEMENT:1||SILICON:1||SR2FEMOO6:1||orbital ordering:1||delafossite:1||TITANIUMDIOXIDE:1||electronic structure of disordered solids:1||YFE2:1||Magnetic polaron:1||NA2TI2SB2O:1||STRONGCOUPLED SUPERCONDUCTORS:1||HEAVYFERMION SYSTEMS:1||firstprinciples calculations:1||MECHANISM:1||UNiSn:1||PHOTONIC BANDGAP:1||SINGLE IMPURITY:1||PHONONSPECTRUM:1||FERMISURFACE TOPOLOGY:1||SUPPRESSION:1||RESONANT PHOTOEMISSION:1||METALDOPED PICENE:1||PHOTOIONIZATION CROSSSECTIONS:1||PHOTOINDUCED FERRIMAGNETIC SYSTEMS:1||LINKAGE ISOMERISM:1||CHARGETRANSFER:1||Bilayer Graphene:1||MAGNETICFIELD:1||SPINWAVES:1||rareearth manganese oxides:1||magnonphonon interaction:1||NACO2O4:1||ENERGYBANDS:1||SELFENERGY:1||GAS:1||Fe0.5Cu0.5Cr2S4:1||scanning photoelectron microscopy (SPEM):1||MAGNETIC PROPERTIES:1||Stoner model:1||AMORPHOUS TRANSITIONMETALS:1||SPINGLASS STATES:1||NI:1||LA3NI2B2N3:1||SOLIDS:1||CEO2:1||BAND THEORY:1||dilute magnetic semiconductor:1||pyrochlore:1||Y1XPRXBA2CU3O7DELTA:1||and electronphonon interactions:1||VIBRATIONS:1||RAY PHOTOEMISSION:1||ALKALI CATION:1||Europium:1||colossal magnetoresistance:1||structural stability:1||ENERGYGAP:1||small polaron:1||DOUBLE EXCHANGE:1||Coulomb correlation:1||magnon:1||phonons:1||ELECTRON FERROMAGNETISM:1||CURIETEMPERATURE:1||ARPES:1||PLANEWAVE METHOD:1||Xray absorption spectroscopy (XAS):1||ROOMTEMPERATURE:1||MONOCHALCOGENIDES:1||HEAT:1||UPDSN:1||MOMENTS:1||XRAY ABSORPTION:1||SEMICONDUCTOR:1||Fermi surface nesting:1||optical phonon:1||disordered system:1||dilute magnetic semiconductors:1||CMR manganites:1||PHONONS:1||LATTICEDYNAMICS:1||OXIDES:1||4fphotoemission:1||permanent magnet:1||pseudogap:1||TRANSPORTPROPERTIES:1||ANTIFERROMAGNET:1||(BI,PB)SRCOO SYSTEM:1||semicore correlation:1||POLARIZATION:1||CRYSTAL:1||spinel:1||Xray magnetic circular dichroism (XMCD):1||magnetocapacitance:1||ANATASE:1||TEMPERATURES:1||Pseudogap:1||INTERFACE:1||SUBSTRATE:1||YNI2B2C:1||SAMARIUM SULFIDE:1||strong swave superconductor:1||DOPED MANGANITE:1||SYMMETRY:1||CENISN:1||resonance mode:1||DISORDERED SYSTEM:1||LITHIUM INTERCALATION:1||CUO2 PLANE:1||SURFACE:1||Delafossite:1||ELECTRICALPROPERTIES:1||NIMNSB:1||PTMNSB:1||ROOMTEMPERATURE FERROMAGNETISM:1||RUBIDIUM MANGANESE HEXACYANOFERRATE:1||COLOSSALMAGNETORESISTANCE:1||FINITE TEMPERATURES:1||LAMNO3:1||FE:1||transitionmetal oxides:1||giant magnetoresistance:1||phonon:1||COPPER OXIDES:1||valence states:1||thermoelectric:1||semiconductor:1||CATION DISTRIBUTION:1||FeCr2S4:1||photoemission spectroscopy (PES):1||METALLIC FERROMAGNETISM:1||GRAPHITE:1||SUSCEPTIBILITY:1||UBE13:1||RCrSb3:1||band JahnTeller:1||Ce3S4:1||TiO2:1||PrBa2Cu3O7delta:1||UNTWINNED PRBA2CU3O7:1||AGNIO2:1||HALFMETALLIC FERROMAGNETS:1||CI:1||Energy gap:1||Photoemission:1||Future applications:1||Photoemission measurements:1||Graphene:1||BANDSTRUCTURE:1||TC:1||superconductivity:1||magnetic semiconductors:1||CMRmanganites:1||thin films:1||spin dynamics:1||highTc superconductors:1||ITINERANTELECTRON FERROMAGNETISM:1||SINGLECRYSTALS:1||CeTe2:1||amorphous magnetic materials:1||EPITAXIAL GRAPHENE:1||LAYERED PNICTIDEOXIDES:1||BOROCARBIDE SUPERCONDUCTORS:1||AUGMENTEDWAVE METHOD:1||METALLIC MAGNET UNISN:1||ORIGIN:1||spectrum rearrangement:1||MEANFIELD THEORY:1||MOLECULEBASED MAGNETS:1||METASTABLE STATE:1||INSULATOR:1||magnetic orderin:1||FCC IRON:1||CeRu2:1||TL2MN2O7:1||isotope effect:1||Perovskitemanganites:1||RECURSION METHOD:1||PERPENDICULAR MAGNETICANISOTROPY:1||quasiparticle spectral density:1||GW:1||MANGANESE FERRITE:1||RESONANCE:1||SeCuO3:1||Optical conductivity:1||MASSLESS DIRAC FERMIONS:1||SCHOTTKYBARRIER:1||electronic structure:15||ELECTRONICSTRUCTURE:11||TRANSITIONMETAL COMPOUNDS:10||METALS:10||photoemission:8||SPECTRA:8||MAGNETORESISTANCE:7||FERROMAGNETISM:7||TRANSPORT:7||TRANSITION:6||FILMS:6||THINFILMS:5||TOTALENERGY CALCULATIONS:5||MAGNETICPROPERTIES:5||SUPERCONDUCTIVITY:5||PR:5||LATTICE:4||STATES:4||SPECTROSCOPY:4||FIELD:4||CRYSTALSTRUCTURE:4||PHOTOEMISSION:4||TEMPERATURE:4||TRANSITIONTEMPERATURE:4||XRAYABSORPTION:4||STATE:4||CU:4||BASISSET:4||XAS:4||CRYSTALS:3||EXCITATIONS:3||MOTTHUBBARD SYSTEMS:3||HIGHENERGY SPIN:3||halfmetal:3||INSULATORS:3||LA2CUO4:3||MODEL:3||FLUCTUATIONS:3||CE:3||double exchange:3||TRANSITIONMETALS:3||RESISTIVITY:3||BORON:3||LA1XCAXMNO3:3||IRON:3||PES:3||ANTIMONIDES:2||MgB2:2||ZR METALLIC GLASSES:2||superconductor:2||CRITICALCURRENT DENSITY:2||CIRCULARDICHROISM:2||SEMICONDUCTORS:2||LOCALIZATION:2||INTRABAND OPTICAL CONDUCTIVITY:2||COLOSSAL MAGNETORESISTANCE:2||OXIDATION:2||EXISTENCE:2||COPPER:2||diboride:2||MAGNESIUMDIBORIDE:2||GAP:2||CE COMPOUNDS:2||CORE POLARIZATION:2||magnetoresistance:2||photoemission spectroscopy:2||electronphonon interaction:2||GETTER:2||PD:2||MAGNETISM:2||FECR2S4:2||SUPERCONDUCTING MGB2:2||WIRES:2||ABSORPTION:2||ENERGY:2||LA1XSRXMNO3:2||CONSTANTS:2||polaron:2||charge ordering:2||SCATTERING:2||XRAY PHOTOEMISSION:2||CeNiSn:2||phase diagram:2||PHOTOELECTRON:2||QUADRUPOLAR:2||perovskitemanganites:2||CO:2||SYSTEMS:2||DOPED ZNO:2||LOWFREQUENCY SOUND:2||LA:2||ELECTRONELECTRON SCATTERING:2||AU:2||DENSITYWAVE INSTABILITY:2||FERMISURFACE:2||hybridization:2||VALENCEBAND SATELLITE:2||SULFUR SPINEL:2||Heusler:2||APPROXIMATION:2||superexchange:2||colossal magnetoresistance:2||ALLOYS:2||DEPENDENCE:2||AG:2||electronic structures:2||AUGERSPECTRA:2||CR:2||PARAMETERS:2||DIFFRACTION:2||SEMICONDUCTORMETAL TRANSITION:1||INTERMEDIATEVALENCE:1||SMB6:1||SRRUO3:1||antiperovskite structure with antipolar nature:1||lowenergy twodimensional phonons:1||anatase TiO2:1||La3S4:1||metalinsulator transitions:1||MNO:1||ELECTRONICSTRUCTURES:1||MAGNETIC CIRCULARDICHROISM:1||Density functional theory:1||CeCo2:1||TOPOLARON CROSSOVER:1||EXCHANGE:1||cuprates:1||high Tc cuprates:1||magnetically ordered materials:1||ZNSE:1||Sr2xKxFeMoO6:1||CDW:1||TeCuO3:1||STRUCTURALPROPERTIES:1||MN:1||screening length:1||amorphous Fe:1||WAVE BASISSET:1||SILICONCARBIDE:1||HIGHPRESSURE:1||electronphonon coupling:1||quenched superconductivity:1||CMR perovskite manganites:1||OXIDE:1||polarons:1||synchrotron radiation:1||FULLERIDES:1||RESONANTPHOTOEMISSION:1||Silicon carbide:1||DFT calculation:1||Hybridized bands:1||GIANT MAGNETORESISTANCE:1||PEROVSKITES:1||Raman spectra:1||EXCHANGE ENHANCEMENT:1||SILICON:1||SR2FEMOO6:1||orbital ordering:1||delafossite:1||TITANIUMDIOXIDE:1||electronic structure of disordered solids:1||YFE2:1||Magnetic polaron:1||NA2TI2SB2O:1||STRONGCOUPLED SUPERCONDUCTORS:1||HEAVYFERMION SYSTEMS:1||firstprinciples calculations:1||MECHANISM:1||UNiSn:1||PHOTONIC BANDGAP:1||SINGLE IMPURITY:1||PHONONSPECTRUM:1||FERMISURFACE TOPOLOGY:1||SUPPRESSION:1||RESONANT PHOTOEMISSION:1||METALDOPED PICENE:1||PHOTOIONIZATION CROSSSECTIONS:1||PHOTOINDUCED FERRIMAGNETIC SYSTEMS:1||LINKAGE ISOMERISM:1||CHARGETRANSFER:1||Bilayer Graphene:1||MAGNETICFIELD:1||SPINWAVES:1||rareearth manganese oxides:1||magnonphonon interaction:1||NACO2O4:1||ENERGYBANDS:1||SELFENERGY:1||GAS:1||Fe0.5Cu0.5Cr2S4:1||scanning photoelectron microscopy (SPEM):1||MAGNETIC PROPERTIES:1||Stoner model:1||AMORPHOUS TRANSITIONMETALS:1||SPINGLASS STATES:1||NI:1||LA3NI2B2N3:1||SOLIDS:1||CEO2:1||BAND THEORY:1||dilute magnetic semiconductor:1||pyrochlore:1||Y1XPRXBA2CU3O7DELTA:1||and electronphonon interactions:1||VIBRATIONS:1||RAY PHOTOEMISSION:1||ALKALI CATION:1||Europium:1||colossal magnetoresistance:1||structural stability:1||ENERGYGAP:1||small polaron:1||DOUBLE EXCHANGE:1||Coulomb correlation:1||magnon:1||phonons:1||ELECTRON FERROMAGNETISM:1||CURIETEMPERATURE:1||ARPES:1||PLANEWAVE METHOD:1||Xray absorption spectroscopy (XAS):1||ROOMTEMPERATURE:1||MONOCHALCOGENIDES:1||HEAT:1||UPDSN:1||MOMENTS:1||XRAY ABSORPTION:1||SEMICONDUCTOR:1||Fermi surface nesting:1||optical phonon:1||disordered system:1||dilute magnetic semiconductors:1||CMR manganites:1||PHONONS:1||LATTICEDYNAMICS:1||OXIDES:1||4fphotoemission:1||permanent magnet:1||pseudogap:1||TRANSPORTPROPERTIES:1||ANTIFERROMAGNET:1||(BI,PB)SRCOO SYSTEM:1||semicore correlation:1||POLARIZATION:1||CRYSTAL:1||spinel:1||Xray magnetic circular dichroism (XMCD):1||magnetocapacitance:1||ANATASE:1||TEMPERATURES:1||Pseudogap:1||INTERFACE:1||SUBSTRATE:1||YNI2B2C:1||SAMARIUM SULFIDE:1||strong swave superconductor:1||DOPED MANGANITE:1||SYMMETRY:1||CENISN:1||resonance mode:1||DISORDERED SYSTEM:1||LITHIUM INTERCALATION:1||CUO2 PLANE:1||SURFACE:1||Delafossite:1||ELECTRICALPROPERTIES:1||NIMNSB:1||PTMNSB:1||ROOMTEMPERATURE FERROMAGNETISM:1||RUBIDIUM MANGANESE HEXACYANOFERRATE:1||COLOSSALMAGNETORESISTANCE:1||FINITE TEMPERATURES:1||LAMNO3:1||FE:1||transitionmetal oxides:1||giant magnetoresistance:1||phonon:1||COPPER OXIDES:1||valence states:1||thermoelectric:1||semiconductor:1||CATION DISTRIBUTION:1||FeCr2S4:1||photoemission spectroscopy (PES):1||METALLIC FERROMAGNETISM:1||GRAPHITE:1||SUSCEPTIBILITY:1||UBE13:1||RCrSb3:1||band JahnTeller:1||Ce3S4:1||TiO2:1||PrBa2Cu3O7delta:1||UNTWINNED PRBA2CU3O7:1||AGNIO2:1||HALFMETALLIC FERROMAGNETS:1||CI:1||Energy gap:1||Photoemission:1||Future applications:1||Photoemission measurements:1||Graphene:1||BANDSTRUCTURE:1||TC:1||superconductivity:1||magnetic semiconductors:1||CMRmanganites:1||thin films:1||spin dynamics:1||highTc superconductors:1||ITINERANTELECTRON FERROMAGNETISM:1||SINGLECRYSTALS:1||CeTe2:1||amorphous magnetic materials:1||EPITAXIAL GRAPHENE:1||LAYERED PNICTIDEOXIDES:1||BOROCARBIDE SUPERCONDUCTORS:1||AUGMENTEDWAVE METHOD:1||METALLIC MAGNET UNISN:1||ORIGIN:1||spectrum rearrangement:1||MEANFIELD THEORY:1||MOLECULEBASED MAGNETS:1||METASTABLE STATE:1||INSULATOR:1||magnetic orderin:1||FCC IRON:1||CeRu2:1||TL2MN2O7:1||isotope effect:1||Perovskitemanganites:1||RECURSION METHOD:1||PERPENDICULAR MAGNETICANISOTROPY:1||quasiparticle spectral density:1||GW:1||MANGANESE FERRITE:1||RESONANCE:1||SeCuO3:1||Optical conductivity:1||MASSLESS DIRAC FERMIONS:1||SCHOTTKYBARRIER:1||electronic structure:15||ELECTRONICSTRUCTURE:11||TRANSITIONMETAL COMPOUNDS:10||METALS:10||photoemission:8||SPECTRA:8||MAGNETORESISTANCE:7||FERROMAGNETISM:7||TRANSPORT:7||TRANSITION:6||FILMS:6||THINFILMS:5||TOTALENERGY CALCULATIONS:5||MAGNETICPROPERTIES:5||SUPERCONDUCTIVITY:5||PR:5||LATTICE:4||STATES:4||SPECTROSCOPY:4||FIELD:4||CRYSTALSTRUCTURE:4||PHOTOEMISSION:4||TEMPERATURE:4||TRANSITIONTEMPERATURE:4||XRAYABSORPTION:4||STATE:4||CU:4||BASISSET:4||XAS:4||CRYSTALS:3||EXCITATIONS:3||MOTTHUBBARD SYSTEMS:3||HIGHENERGY SPIN:3||halfmetal:3||INSULATORS:3||LA2CUO4:3||MODEL:3||FLUCTUATIONS:3||CE:3||double exchange:3||TRANSITIONMETALS:3||RESISTIVITY:3||BORON:3||LA1XCAXMNO3:3||IRON:3||PES:3||ANTIMONIDES:2||MgB2:2||ZR METALLIC GLASSES:2||superconductor:2||CRITICALCURRENT DENSITY:2||CIRCULARDICHROISM:2||SEMICONDUCTORS:2||LOCALIZATION:2||INTRABAND OPTICAL CONDUCTIVITY:2||COLOSSAL MAGNETORESISTANCE:2||OXIDATION:2||EXISTENCE:2||COPPER:2||diboride:2||MAGNESIUMDIBORIDE:2||GAP:2||CE COMPOUNDS:2||CORE POLARIZATION:2||magnetoresistance:2||photoemission spectroscopy:2||electronphonon interaction:2||GETTER:2||PD:2||MAGNETISM:2||FECR2S4:2||SUPERCONDUCTING MGB2:2||WIRES:2||ABSORPTION:2||ENERGY:2||LA1XSRXMNO3:2||CONSTANTS:2||polaron:2||charge ordering:2||SCATTERING:2||XRAY PHOTOEMISSION:2||CeNiSn:2||phase diagram:2||PHOTOELECTRON:2||QUADRUPOLAR:2||perovskitemanganites:2||CO:2||SYSTEMS:2||DOPED ZNO:2||LOWFREQUENCY SOUND:2||LA:2||ELECTRONELECTRON SCATTERING:2||AU:2||DENSITYWAVE INSTABILITY:2||FERMISURFACE:2||hybridization:2||VALENCEBAND SATELLITE:2||SULFUR SPINEL:2||Heusler:2||APPROXIMATION:2||superexchange:2||colossal magnetoresistance:2||ALLOYS:2||DEPENDENCE:2||AG:2||electronic structures:2||AUGERSPECTRA:2||CR:2||PARAMETERS:2||DIFFRACTION:2||SEMICONDUCTORMETAL TRANSITION:1||INTERMEDIATEVALENCE:1||SMB6:1||SRRUO3:1||antiperovskite structure with antipolar nature:1||lowenergy twodimensional phonons:1||anatase TiO2:1||La3S4:1||metalinsulator transitions:1||MNO:1||ELECTRONICSTRUCTURES:1||MAGNETIC CIRCULARDICHROISM:1||Density functional theory:1||CeCo2:1||TOPOLARON CROSSOVER:1||EXCHANGE:1||cuprates:1||high Tc cuprates:1||magnetically ordered materials:1||ZNSE:1||Sr2xKxFeMoO6:1||CDW:1||TeCuO3:1||STRUCTURALPROPERTIES:1||MN:1||screening length:1||amorphous Fe:1||WAVE BASISSET:1||SILICONCARBIDE:1||HIGHPRESSURE:1||electronphonon coupling:1||quenched superconductivity:1||CMR perovskite manganites:1||OXIDE:1||polarons:1||synchrotron radiation:1||FULLERIDES:1||RESONANTPHOTOEMISSION:1||Silicon carbide:1||DFT calculation:1||Hybridized bands:1||GIANT MAGNETORESISTANCE:1||PEROVSKITES:1||Raman spectra:1||EXCHANGE ENHANCEMENT:1||SILICON:1||SR2FEMOO6:1||orbital ordering:1||delafossite:1||TITANIUMDIOXIDE:1||electronic structure of disordered solids:1||YFE2:1||Magnetic polaron:1||NA2TI2SB2O:1||STRONGCOUPLED SUPERCONDUCTORS:1||HEAVYFERMION SYSTEMS:1||firstprinciples calculations:1||MECHANISM:1||UNiSn:1||PHOTONIC BANDGAP:1||SINGLE IMPURITY:1||PHONONSPECTRUM:1||FERMISURFACE TOPOLOGY:1||SUPPRESSION:1||RESONANT PHOTOEMISSION:1||METALDOPED PICENE:1||PHOTOIONIZATION CROSSSECTIONS:1||PHOTOINDUCED FERRIMAGNETIC SYSTEMS:1||LINKAGE ISOMERISM:1||CHARGETRANSFER:1||Bilayer Graphene:1||MAGNETICFIELD:1||SPINWAVES:1||rareearth manganese oxides:1||magnonphonon interaction:1||NACO2O4:1||ENERGYBANDS:1||SELFENERGY:1||GAS:1||Fe0.5Cu0.5Cr2S4:1||scanning photoelectron microscopy (SPEM):1||MAGNETIC PROPERTIES:1||Stoner model:1||AMORPHOUS TRANSITIONMETALS:1||SPINGLASS STATES:1||NI:1||LA3NI2B2N3:1||SOLIDS:1||CEO2:1||BAND THEORY:1||dilute magnetic semiconductor:1||pyrochlore:1||Y1XPRXBA2CU3O7DELTA:1||and electronphonon interactions:1||VIBRATIONS:1||RAY PHOTOEMISSION:1||ALKALI CATION:1||Europium:1||colossal magnetoresistance:1||structural stability:1||ENERGYGAP:1||small polaron:1||DOUBLE EXCHANGE:1||Coulomb correlation:1||magnon:1||phonons:1||ELECTRON FERROMAGNETISM:1||CURIETEMPERATURE:1||ARPES:1||PLANEWAVE METHOD:1||Xray absorption spectroscopy (XAS):1||ROOMTEMPERATURE:1||MONOCHALCOGENIDES:1||HEAT:1||UPDSN:1||MOMENTS:1||XRAY ABSORPTION:1||SEMICONDUCTOR:1||Fermi surface nesting:1||optical phonon:1||disordered system:1||dilute magnetic semiconductors:1||CMR manganites:1||PHONONS:1||LATTICEDYNAMICS:1||OXIDES:1||4fphotoemission:1||permanent magnet:1||pseudogap:1||TRANSPORTPROPERTIES:1||ANTIFERROMAGNET:1||(BI,PB)SRCOO SYSTEM:1||semicore correlation:1||POLARIZATION:1||CRYSTAL:1||spinel:1||Xray magnetic circular dichroism (XMCD):1||magnetocapacitance:1||ANATASE:1||TEMPERATURES:1||Pseudogap:1||INTERFACE:1||SUBSTRATE:1||YNI2B2C:1||SAMARIUM SULFIDE:1||strong swave superconductor:1||DOPED MANGANITE:1||SYMMETRY:1||CENISN:1||resonance mode:1||DISORDERED SYSTEM:1||LITHIUM INTERCALATION:1||CUO2 PLANE:1||SURFACE:1||Delafossite:1||ELECTRICALPROPERTIES:1||NIMNSB:1||PTMNSB:1||ROOMTEMPERATURE FERROMAGNETISM:1||RUBIDIUM MANGANESE HEXACYANOFERRATE:1||COLOSSALMAGNETORESISTANCE:1||FINITE TEMPERATURES:1||LAMNO3:1||FE:1||transitionmetal oxides:1||giant magnetoresistance:1||phonon:1||COPPER OXIDES:1||valence states:1||thermoelectric:1||semiconductor:1||CATION DISTRIBUTION:1||FeCr2S4:1||photoemission spectroscopy (PES):1||METALLIC FERROMAGNETISM:1||GRAPHITE:1||SUSCEPTIBILITY:1||UBE13:1||RCrSb3:1||band JahnTeller:1||Ce3S4:1||TiO2:1||PrBa2Cu3O7delta:1||UNTWINNED PRBA2CU3O7:1||AGNIO2:1||HALFMETALLIC FERROMAGNETS:1||CI:1||Energy gap:1||Photoemission:1||Future applications:1||Photoemission measurements:1||Graphene:1||BANDSTRUCTURE:1||TC:1||superconductivity:1||magnetic semiconductors:1||CMRmanganites:1||thin films:1||spin dynamics:1||highTc superconductors:1||ITINERANTELECTRON FERROMAGNETISM:1||SINGLECRYSTALS:1||CeTe2:1||amorphous magnetic materials:1||EPITAXIAL GRAPHENE:1||LAYERED PNICTIDEOXIDES:1||BOROCARBIDE SUPERCONDUCTORS:1||AUGMENTEDWAVE METHOD:1||METALLIC MAGNET UNISN:1||ORIGIN:1||spectrum rearrangement:1||MEANFIELD THEORY:1||MOLECULEBASED MAGNETS:1||METASTABLE STATE:1||INSULATOR:1||magnetic orderin:1||FCC IRON:1||CeRu2:1||TL2MN2O7:1||isotope effect:1||Perovskitemanganites:1||RECURSION METHOD:1||PERPENDICULAR MAGNETICANISOTROPY:1||quasiparticle spectral density:1||GW:1||MANGANESE FERRITE:1||RESONANCE:1||SeCuO3:1||Optical conductivity:1||MASSLESS DIRAC FERMIONS:1||SCHOTTKYBARRIER:1||electronic structure:15||ELECTRONICSTRUCTURE:11||TRANSITIONMETAL COMPOUNDS:10||METALS:10||photoemission:8||SPECTRA:8||MAGNETORESISTANCE:7||FERROMAGNETISM:7||TRANSPORT:7||TRANSITION:6||FILMS:6||THINFILMS:5||TOTALENERGY CALCULATIONS:5||MAGNETICPROPERTIES:5||SUPERCONDUCTIVITY:5||PR:5||LATTICE:4||STATES:4||SPECTROSCOPY:4||FIELD:4||CRYSTALSTRUCTURE:4||PHOTOEMISSION:4||TEMPERATURE:4||TRANSITIONTEMPERATURE:4||XRAYABSORPTION:4||STATE:4||CU:4||BASISSET:4||XAS:4||CRYSTALS:3||EXCITATIONS:3||MOTTHUBBARD SYSTEMS:3||HIGHENERGY SPIN:3||halfmetal:3||INSULATORS:3||LA2CUO4:3||MODEL:3||FLUCTUATIONS:3||CE:3||double exchange:3||TRANSITIONMETALS:3||RESISTIVITY:3||BORON:3||LA1XCAXMNO3:3||IRON:3||PES:3||ANTIMONIDES:2||MgB2:2||ZR METALLIC GLASSES:2||superconductor:2||CRITICALCURRENT DENSITY:2||CIRCULARDICHROISM:2||SEMICONDUCTORS:2||LOCALIZATION:2||INTRABAND OPTICAL CONDUCTIVITY:2||COLOSSAL MAGNETORESISTANCE:2||OXIDATION:2||EXISTENCE:2||COPPER:2||diboride:2||MAGNESIUMDIBORIDE:2||GAP:2||CE COMPOUNDS:2||CORE POLARIZATION:2||magnetoresistance:2||photoemission spectroscopy:2||electronphonon interaction:2||GETTER:2||PD:2||MAGNETISM:2||FECR2S4:2||SUPERCONDUCTING MGB2:2||WIRES:2||ABSORPTION:2||ENERGY:2||LA1XSRXMNO3:2||CONSTANTS:2||polaron:2||charge ordering:2||SCATTERING:2||XRAY PHOTOEMISSION:2||CeNiSn:2||phase diagram:2||PHOTOELECTRON:2||QUADRUPOLAR:2||perovskitemanganites:2||CO:2||SYSTEMS:2||DOPED ZNO:2||LOWFREQUENCY SOUND:2||LA:2||ELECTRONELECTRON SCATTERING:2||AU:2||DENSITYWAVE INSTABILITY:2||FERMISURFACE:2||hybridization:2||VALENCEBAND SATELLITE:2||SULFUR SPINEL:2||Heusler:2||APPROXIMATION:2||superexchange:2||colossal magnetoresistance:2||ALLOYS:2||DEPENDENCE:2||AG:2||electronic structures:2||AUGERSPECTRA:2||CR:2||PARAMETERS:2||DIFFRACTION:2||SEMICONDUCTORMETAL TRANSITION:1||INTERMEDIATEVALENCE:1||SMB6:1||SRRUO3:1||antiperovskite structure with antipolar nature:1||lowenergy twodimensional phonons:1||anatase TiO2:1||La3S4:1||metalinsulator transitions:1||MNO:1||ELECTRONICSTRUCTURES:1||MAGNETIC CIRCULARDICHROISM:1||Density functional theory:1||CeCo2:1||TOPOLARON CROSSOVER:1||EXCHANGE:1||cuprates:1||high Tc cuprates:1||magnetically ordered materials:1||ZNSE:1||Sr2xKxFeMoO6:1||CDW:1||TeCuO3:1||STRUCTURALPROPERTIES:1||MN:1||screening length:1||amorphous Fe:1||WAVE BASISSET:1||SILICONCARBIDE:1||HIGHPRESSURE:1||electronphonon coupling:1||quenched superconductivity:1||CMR perovskite manganites:1||OXIDE:1||polarons:1||synchrotron radiation:1||FULLERIDES:1||RESONANTPHOTOEMISSION:1||Silicon carbide:1||DFT calculation:1||Hybridized bands:1||GIANT MAGNETORESISTANCE:1||PEROVSKITES:1||Raman spectra:1||EXCHANGE ENHANCEMENT:1||SILICON:1||SR2FEMOO6:1||orbital ordering:1||delafossite:1||TITANIUMDIOXIDE:1||electronic structure of disordered solids:1||YFE2:1||Magnetic polaron:1||NA2TI2SB2O:1||STRONGCOUPLED SUPERCONDUCTORS:1||HEAVYFERMION SYSTEMS:1||firstprinciples calculations:1||MECHANISM:1||UNiSn:1||PHOTONIC BANDGAP:1||SINGLE IMPURITY:1||PHONONSPECTRUM:1||FERMISURFACE TOPOLOGY:1||SUPPRESSION:1||RESONANT PHOTOEMISSION:1||METALDOPED PICENE:1||PHOTOIONIZATION CROSSSECTIONS:1||PHOTOINDUCED FERRIMAGNETIC SYSTEMS:1||LINKAGE ISOMERISM:1||CHARGETRANSFER:1||Bilayer Graphene:1||MAGNETICFIELD:1||SPINWAVES:1||rareearth manganese oxides:1||magnonphonon interaction:1||NACO2O4:1||ENERGYBANDS:1||SELFENERGY:1||GAS:1||Fe0.5Cu0.5Cr2S4:1||scanning photoelectron microscopy (SPEM):1||MAGNETIC PROPERTIES:1||Stoner model:1||AMORPHOUS TRANSITIONMETALS:1||SPINGLASS STATES:1||NI:1||LA3NI2B2N3:1||SOLIDS:1||CEO2:1||BAND THEORY:1||dilute magnetic semiconductor:1||pyrochlore:1||Y1XPRXBA2CU3O7DELTA:1||and electronphonon interactions:1||VIBRATIONS:1||RAY PHOTOEMISSION:1||ALKALI CATION:1||Europium:1||colossal magnetoresistance:1||structural stability:1||ENERGYGAP:1||small polaron:1||DOUBLE EXCHANGE:1||Coulomb correlation:1||magnon:1||phonons:1||ELECTRON FERROMAGNETISM:1||CURIETEMPERATURE:1||ARPES:1||PLANEWAVE METHOD:1||Xray absorption spectroscopy (XAS):1||ROOMTEMPERATURE:1||MONOCHALCOGENIDES:1||HEAT:1||UPDSN:1||MOMENTS:1||XRAY ABSORPTION:1||SEMICONDUCTOR:1||Fermi surface nesting:1||optical phonon:1||disordered system:1||dilute magnetic semiconductors:1||CMR manganites:1||PHONONS:1||LATTICEDYNAMICS:1||OXIDES:1||4fphotoemission:1||permanent magnet:1||pseudogap:1||TRANSPORTPROPERTIES:1||ANTIFERROMAGNET:1||(BI,PB)SRCOO SYSTEM:1||semicore correlation:1||POLARIZATION:1||CRYSTAL:1||spinel:1||Xray magnetic circular dichroism (XMCD):1||magnetocapacitance:1||ANATASE:1||TEMPERATURES:1||Pseudogap:1||INTERFACE:1||SUBSTRATE:1||YNI2B2C:1||SAMARIUM SULFIDE:1||strong swave superconductor:1||DOPED MANGANITE:1||SYMMETRY:1||CENISN:1||resonance mode:1||DISORDERED SYSTEM:1||LITHIUM INTERCALATION:1||CUO2 PLANE:1||SURFACE:1||Delafossite:1||ELECTRICALPROPERTIES:1||NIMNSB:1||PTMNSB:1||ROOMTEMPERATURE FERROMAGNETISM:1||RUBIDIUM MANGANESE HEXACYANOFERRATE:1||COLOSSALMAGNETORESISTANCE:1||FINITE TEMPERATURES:1||LAMNO3:1||FE:1||transitionmetal oxides:1||giant magnetoresistance:1||phonon:1||COPPER OXIDES:1||valence states:1||thermoelectric:1||semiconductor:1||CATION DISTRIBUTION:1||FeCr2S4:1||photoemission spectroscopy (PES):1||METALLIC FERROMAGNETISM:1||GRAPHITE:1||SUSCEPTIBILITY:1||UBE13:1||RCrSb3:1||band JahnTeller:1||Ce3S4:1||TiO2:1||PrBa2Cu3O7delta:1||UNTWINNED PRBA2CU3O7:1||AGNIO2:1||HALFMETALLIC FERROMAGNETS:1||CI:1||Energy gap:1||Photoemission:1||Future applications:1||Photoemission measurements:1||Graphene:1||BANDSTRUCTURE:1||TC:1||superconductivity:1||magnetic semiconductors:1||CMRmanganites:1||thin films:1||spin dynamics:1||highTc superconductors:1||ITINERANTELECTRON FERROMAGNETISM:1||SINGLECRYSTALS:1||CeTe2:1||amorphous magnetic materials:1||EPITAXIAL GRAPHENE:1||LAYERED PNICTIDEOXIDES:1||BOROCARBIDE SUPERCONDUCTORS:1||AUGMENTEDWAVE METHOD:1||METALLIC MAGNET UNISN:1||ORIGIN:1||spectrum rearrangement:1||MEANFIELD THEORY:1||MOLECULEBASED MAGNETS:1||METASTABLE STATE:1||INSULATOR:1||magnetic orderin:1||FCC IRON:1||CeRu2:1||TL2MN2O7:1||isotope effect:1||Perovskitemanganites:1||RECURSION METHOD:1||PERPENDICULAR MAGNETICANISOTROPY:1||quasiparticle spectral density:1||GW:1||MANGANESE FERRITE:1||RESONANCE:1||SeCuO3:1||Optical conductivity:1||MASSLESS DIRAC FERMIONS:1||SCHOTTKYBARRIER:1||electronic structure:15||ELECTRONICSTRUCTURE:11||TRANSITIONMETAL COMPOUNDS:10||METALS:10||photoemission:8||SPECTRA:8||MAGNETORESISTANCE:7||FERROMAGNETISM:7||TRANSPORT:7||TRANSITION:6||FILMS:6||THINFILMS:5||TOTALENERGY CALCULATIONS:5||MAGNETICPROPERTIES:5||SUPERCONDUCTIVITY:5||PR:5||LATTICE:4||STATES:4||SPECTROSCOPY:4||FIELD:4||CRYSTALSTRUCTURE:4||PHOTOEMISSION:4||TEMPERATURE:4||TRANSITIONTEMPERATURE:4||XRAYABSORPTION:4||STATE:4||CU:4||BASISSET:4||XAS:4||CRYSTALS:3||EXCITATIONS:3||MOTTHUBBARD SYSTEMS:3||HIGHENERGY SPIN:3||halfmetal:3||INSULATORS:3||LA2CUO4:3||MODEL:3||FLUCTUATIONS:3||CE:3||double exchange:3||TRANSITIONMETALS:3||RESISTIVITY:3||BORON:3||LA1XCAXMNO3:3||IRON:3||PES:3||ANTIMONIDES:2||MgB2:2||ZR METALLIC GLASSES:2||superconductor:2||CRITICALCURRENT DENSITY:2||CIRCULARDICHROISM:2||SEMICONDUCTORS:2||LOCALIZATION:2||INTRABAND OPTICAL CONDUCTIVITY:2||COLOSSAL MAGNETORESISTANCE:2||OXIDATION:2||EXISTENCE:2||COPPER:2||diboride:2||MAGNESIUMDIBORIDE:2||GAP:2||CE COMPOUNDS:2||CORE POLARIZATION:2||magnetoresistance:2||photoemission spectroscopy:2||electronphonon interaction:2||GETTER:2||PD:2||MAGNETISM:2||FECR2S4:2||SUPERCONDUCTING MGB2:2||WIRES:2||ABSORPTION:2||ENERGY:2||LA1XSRXMNO3:2||CONSTANTS:2||polaron:2||charge ordering:2||SCATTERING:2||XRAY PHOTOEMISSION:2||CeNiSn:2||phase diagram:2||PHOTOELECTRON:2||QUADRUPOLAR:2||perovskitemanganites:2||CO:2||SYSTEMS:2||DOPED ZNO:2||LOWFREQUENCY SOUND:2||LA:2||ELECTRONELECTRON SCATTERING:2||AU:2||DENSITYWAVE INSTABILITY:2||FERMISURFACE:2||hybridization:2||VALENCEBAND SATELLITE:2||SULFUR SPINEL:2||Heusler:2||APPROXIMATION:2||superexchange:2||colossal magnetoresistance:2||ALLOYS:2||DEPENDENCE:2||AG:2||electronic structures:2||AUGERSPECTRA:2||CR:2||PARAMETERS:2||DIFFRACTION:2||SEMICONDUCTORMETAL TRANSITION:1||INTERMEDIATEVALENCE:1||SMB6:1||SRRUO3:1||antiperovskite structure with antipolar nature:1||lowenergy twodimensional phonons:1||anatase TiO2:1||La3S4:1||metalinsulator transitions:1||MNO:1||ELECTRONICSTRUCTURES:1||MAGNETIC CIRCULARDICHROISM:1||Density functional theory:1||CeCo2:1||TOPOLARON CROSSOVER:1||EXCHANGE:1||cuprates:1||high Tc cuprates:1||magnetically ordered materials:1||ZNSE:1||Sr2xKxFeMoO6:1||CDW:1||TeCuO3:1||STRUCTURALPROPERTIES:1||MN:1||screening length:1||amorphous Fe:1||WAVE BASISSET:1||SILICONCARBIDE:1||HIGHPRESSURE:1||electronphonon coupling:1||quenched superconductivity:1||CMR perovskite manganites:1||OXIDE:1||polarons:1||synchrotron radiation:1||FULLERIDES:1||RESONANTPHOTOEMISSION:1||Silicon carbide:1||DFT calculation:1||Hybridized bands:1||GIANT MAGNETORESISTANCE:1||PEROVSKITES:1||Raman spectra:1||EXCHANGE ENHANCEMENT:1||SILICON:1||SR2FEMOO6:1||orbital ordering:1||delafossite:1||TITANIUMDIOXIDE:1||electronic structure of disordered solids:1||YFE2:1||Magnetic polaron:1||NA2TI2SB2O:1||STRONGCOUPLED SUPERCONDUCTORS:1||HEAVYFERMION SYSTEMS:1||firstprinciples calculations:1||MECHANISM:1||UNiSn:1||PHOTONIC BANDGAP:1||SINGLE IMPURITY:1||PHONONSPECTRUM:1||FERMISURFACE TOPOLOGY:1||SUPPRESSION:1||RESONANT PHOTOEMISSION:1||METALDOPED PICENE:1||PHOTOIONIZATION CROSSSECTIONS:1||PHOTOINDUCED FERRIMAGNETIC SYSTEMS:1||LINKAGE ISOMERISM:1||CHARGETRANSFER:1||Bilayer Graphene:1||MAGNETICFIELD:1||SPINWAVES:1||rareearth manganese oxides:1||magnonphonon interaction:1||NACO2O4:1||ENERGYBANDS:1||SELFENERGY:1||GAS:1||Fe0.5Cu0.5Cr2S4:1||scanning photoelectron microscopy (SPEM):1||MAGNETIC PROPERTIES:1||Stoner model:1||AMORPHOUS TRANSITIONMETALS:1||SPINGLASS STATES:1||NI:1||LA3NI2B2N3:1||SOLIDS:1||CEO2:1||BAND THEORY:1||dilute magnetic semiconductor:1||pyrochlore:1||Y1XPRXBA2CU3O7DELTA:1||and electronphonon interactions:1||VIBRATIONS:1||RAY PHOTOEMISSION:1||ALKALI CATION:1||Europium:1||colossal magnetoresistance:1||structural stability:1||ENERGYGAP:1||small polaron:1||DOUBLE EXCHANGE:1||Coulomb correlation:1||magnon:1||phonons:1||ELECTRON FERROMAGNETISM:1||CURIETEMPERATURE:1||ARPES:1||PLANEWAVE METHOD:1||Xray absorption spectroscopy (XAS):1||ROOMTEMPERATURE:1||MONOCHALCOGENIDES:1||HEAT:1||UPDSN:1||MOMENTS:1||XRAY ABSORPTION:1||SEMICONDUCTOR:1||Fermi surface nesting:1||optical phonon:1||disordered system:1||dilute magnetic semiconductors:1||CMR manganites:1||PHONONS:1||LATTICEDYNAMICS:1||OXIDES:1||4fphotoemission:1||permanent magnet:1||pseudogap:1||TRANSPORTPROPERTIES:1||ANTIFERROMAGNET:1||(BI,PB)SRCOO SYSTEM:1||semicore correlation:1||POLARIZATION:1||CRYSTAL:1||spinel:1||Xray magnetic circular dichroism (XMCD):1||magnetocapacitance:1||ANATASE:1||TEMPERATURES:1||Pseudogap:1||INTERFACE:1||SUBSTRATE:1||YNI2B2C:1||SAMARIUM SULFIDE:1||strong swave superconductor:1||DOPED MANGANITE:1||SYMMETRY:1||CENISN:1||resonance mode:1||DISORDERED SYSTEM:1||LITHIUM INTERCALATION:1||CUO2 PLANE:1||SURFACE:1||Delafossite:1||ELECTRICALPROPERTIES:1||NIMNSB:1||PTMNSB:1||ROOMTEMPERATURE FERROMAGNETISM:1||RUBIDIUM MANGANESE HEXACYANOFERRATE:1||COLOSSALMAGNETORESISTANCE:1||FINITE TEMPERATURES:1||LAMNO3:1||FE:1||transitionmetal oxides:1||giant magnetoresistance:1||phonon:1||COPPER OXIDES:1||valence states:1||thermoelectric:1||semiconductor:1||CATION DISTRIBUTION:1||FeCr2S4:1||photoemission spectroscopy (PES):1||METALLIC FERROMAGNETISM:1||GRAPHITE:1||SUSCEPTIBILITY:1||UBE13:1||RCrSb3:1||band JahnTeller:1||Ce3S4:1||TiO2:1||PrBa2Cu3O7delta:1||UNTWINNED PRBA2CU3O7:1||AGNIO2:1||HALFMETALLIC FERROMAGNETS:1||CI:1||Energy gap:1||Photoemission:1||Future applications:1||Photoemission measurements:1||Graphene:1||BANDSTRUCTURE:1||TC:1||superconductivity:1||magnetic semiconductors:1||CMRmanganites:1||thin films:1||spin dynamics:1||highTc superconductors:1||ITINERANTELECTRON FERROMAGNETISM:1||SINGLECRYSTALS:1||CeTe2:1||amorphous magnetic materials:1||EPITAXIAL GRAPHENE:1||LAYERED PNICTIDEOXIDES:1||BOROCARBIDE SUPERCONDUCTORS:1||AUGMENTEDWAVE METHOD:1||METALLIC MAGNET UNISN:1||ORIGIN:1||spectrum rearrangement:1||MEANFIELD THEORY:1||MOLECULEBASED MAGNETS:1||METASTABLE STATE:1||INSULATOR:1||magnetic orderin:1||FCC IRON:1||CeRu2:1||TL2MN2O7:1||isotope effect:1||Perovskitemanganites:1||RECURSION METHOD:1||PERPENDICULAR MAGNETICANISOTROPY:1||quasiparticle spectral density:1||GW:1||MANGANESE FERRITE:1||RESONANCE:1||SeCuO3:1||Optical conductivity:1||MASSLESS DIRAC FERMIONS:1||SCHOTTKYBARRIER:1||electronic structure:15||ELECTRONICSTRUCTURE:11||TRANSITIONMETAL COMPOUNDS:10||METALS:10||photoemission:8||SPECTRA:8||MAGNETORESISTANCE:7||FERROMAGNETISM:7||TRANSPORT:7||TRANSITION:6||FILMS:6||THINFILMS:5||TOTALENERGY CALCULATIONS:5||MAGNETICPROPERTIES:5||SUPERCONDUCTIVITY:5||PR:5||LATTICE:4||STATES:4||SPECTROSCOPY:4||FIELD:4||CRYSTALSTRUCTURE:4||PHOTOEMISSION:4||TEMPERATURE:4||TRANSITIONTEMPERATURE:4||XRAYABSORPTION:4||STATE:4||CU:4||BASISSET:4||XAS:4||CRYSTALS:3||EXCITATIONS:3||MOTTHUBBARD SYSTEMS:3||HIGHENERGY SPIN:3||halfmetal:3||INSULATORS:3||LA2CUO4:3||MODEL:3||FLUCTUATIONS:3||CE:3||double exchange:3||TRANSITIONMETALS:3||RESISTIVITY:3||BORON:3||LA1XCAXMNO3:3||IRON:3||PES:3||ANTIMONIDES:2||MgB2:2||ZR METALLIC GLASSES:2||superconductor:2||CRITICALCURRENT DENSITY:2||CIRCULARDICHROISM:2||SEMICONDUCTORS:2||LOCALIZATION:2||INTRABAND OPTICAL CONDUCTIVITY:2||COLOSSAL MAGNETORESISTANCE:2||OXIDATION:2||EXISTENCE:2||COPPER:2||diboride:2||MAGNESIUMDIBORIDE:2||GAP:2||CE COMPOUNDS:2||CORE POLARIZATION:2||magnetoresistance:2||photoemission spectroscopy:2||electronphonon interaction:2||GETTER:2||PD:2||MAGNETISM:2||FECR2S4:2||SUPERCONDUCTING MGB2:2||WIRES:2||ABSORPTION:2||ENERGY:2||LA1XSRXMNO3:2||CONSTANTS:2||polaron:2||charge ordering:2||SCATTERING:2||XRAY PHOTOEMISSION:2||CeNiSn:2||phase diagram:2||PHOTOELECTRON:2||QUADRUPOLAR:2||perovskitemanganites:2||CO:2||SYSTEMS:2||DOPED ZNO:2||LOWFREQUENCY SOUND:2||LA:2||ELECTRONELECTRON SCATTERING:2||AU:2||DENSITYWAVE INSTABILITY:2||FERMISURFACE:2||hybridization:2||VALENCEBAND SATELLITE:2||SULFUR SPINEL:2||Heusler:2||APPROXIMATION:2||superexchange:2||colossal magnetoresistance:2||ALLOYS:2||DEPENDENCE:2||AG:2||electronic structures:2||AUGERSPECTRA:2||CR:2||PARAMETERS:2||DIFFRACTION:2||SEMICONDUCTORMETAL TRANSITION:1||INTERMEDIATEVALENCE:1||SMB6:1||SRRUO3:1||antiperovskite structure with antipolar nature:1||lowenergy twodimensional phonons:1||anatase TiO2:1||La3S4:1||metalinsulator transitions:1||MNO:1||ELECTRONICSTRUCTURES:1||MAGNETIC CIRCULARDICHROISM:1||Density functional theory:1||CeCo2:1||TOPOLARON CROSSOVER:1||EXCHANGE:1||cuprates:1||high Tc cuprates:1||magnetically ordered materials:1||ZNSE:1||Sr2xKxFeMoO6:1||CDW:1||TeCuO3:1||STRUCTURALPROPERTIES:1||MN:1||screening length:1||amorphous Fe:1||WAVE BASISSET:1||SILICONCARBIDE:1||HIGHPRESSURE:1||electronphonon coupling:1||quenched superconductivity:1||CMR perovskite manganites:1||OXIDE:1||polarons:1||synchrotron radiation:1||FULLERIDES:1||RESONANTPHOTOEMISSION:1||Silicon carbide:1||DFT calculation:1||Hybridized bands:1||GIANT MAGNETORESISTANCE:1||PEROVSKITES:1||Raman spectra:1||EXCHANGE ENHANCEMENT:1||SILICON:1||SR2FEMOO6:1||orbital ordering:1||delafossite:1||TITANIUMDIOXIDE:1||electronic structure of disordered solids:1||YFE2:1||Magnetic polaron:1||NA2TI2SB2O:1||STRONGCOUPLED SUPERCONDUCTORS:1||HEAVYFERMION SYSTEMS:1||firstprinciples calculations:1||MECHANISM:1||UNiSn:1||PHOTONIC BANDGAP:1||SINGLE IMPURITY:1||PHONONSPECTRUM:1||FERMISURFACE TOPOLOGY:1||SUPPRESSION:1||RESONANT PHOTOEMISSION:1||METALDOPED PICENE:1||PHOTOIONIZATION CROSSSECTIONS:1||PHOTOINDUCED FERRIMAGNETIC SYSTEMS:1||LINKAGE ISOMERISM:1||CHARGETRANSFER:1||Bilayer Graphene:1||MAGNETICFIELD:1||SPINWAVES:1||rareearth manganese oxides:1||magnonphonon interaction:1||NACO2O4:1||ENERGYBANDS:1||SELFENERGY:1||GAS:1||Fe0.5Cu0.5Cr2S4:1||scanning photoelectron microscopy (SPEM):1||MAGNETIC PROPERTIES:1||Stoner model:1||AMORPHOUS TRANSITIONMETALS:1||SPINGLASS STATES:1||NI:1||LA3NI2B2N3:1||SOLIDS:1||CEO2:1||BAND THEORY:1||dilute magnetic semiconductor:1||pyrochlore:1||Y1XPRXBA2CU3O7DELTA:1||and electronphonon interactions:1||VIBRATIONS:1||RAY PHOTOEMISSION:1||ALKALI CATION:1||Europium:1||colossal magnetoresistance:1||structural stability:1||ENERGYGAP:1||small polaron:1||DOUBLE EXCHANGE:1||Coulomb correlation:1||magnon:1||phonons:1||ELECTRON FERROMAGNETISM:1||CURIETEMPERATURE:1||ARPES:1||PLANEWAVE METHOD:1||Xray absorption spectroscopy (XAS):1||ROOMTEMPERATURE:1||MONOCHALCOGENIDES:1||HEAT:1||UPDSN:1||MOMENTS:1||XRAY ABSORPTION:1||SEMICONDUCTOR:1||Fermi surface nesting:1||optical phonon:1||disordered system:1||dilute magnetic semiconductors:1||CMR manganites:1||PHONONS:1||LATTICEDYNAMICS:1||OXIDES:1||4fphotoemission:1||permanent magnet:1||pseudogap:1||TRANSPORTPROPERTIES:1||ANTIFERROMAGNET:1||(BI,PB)SRCOO SYSTEM:1||semicore correlation:1||POLARIZATION:1||CRYSTAL:1||spinel:1||Xray magnetic circular dichroism (XMCD):1||magnetocapacitance:1||ANATASE:1||TEMPERATURES:1||Pseudogap:1||INTERFACE:1||SUBSTRATE:1||YNI2B2C:1||SAMARIUM SULFIDE:1||strong swave superconductor:1||DOPED MANGANITE:1||SYMMETRY:1||CENISN:1||resonance mode:1||DISORDERED SYSTEM:1||LITHIUM INTERCALATION:1||CUO2 PLANE:1||SURFACE:1||Delafossite:1||ELECTRICALPROPERTIES:1||NIMNSB:1||PTMNSB:1||ROOMTEMPERATURE FERROMAGNETISM:1||RUBIDIUM MANGANESE HEXACYANOFERRATE:1||COLOSSALMAGNETORESISTANCE:1||FINITE TEMPERATURES:1||LAMNO3:1||FE:1||transitionmetal oxides:1||giant magnetoresistance:1||phonon:1||COPPER OXIDES:1||valence states:1||thermoelectric:1||semiconductor:1||CATION DISTRIBUTION:1||FeCr2S4:1||photoemission spectroscopy (PES):1||METALLIC FERROMAGNETISM:1||GRAPHITE:1||SUSCEPTIBILITY:1||UBE13:1||RCrSb3:1||band JahnTeller:1||Ce3S4:1||TiO2:1||PrBa2Cu3O7delta:1||UNTWINNED PRBA2CU3O7:1||AGNIO2:1||HALFMETALLIC FERROMAGNETS:1||CI:1||Energy gap:1||Photoemission:1||Future applications:1||Photoemission measurements:1||Graphene:1||BANDSTRUCTURE:1||TC:1||superconductivity:1||magnetic semiconductors:1||CMRmanganites:1||thin films:1||spin dynamics:1||highTc superconductors:1||ITINERANTELECTRON FERROMAGNETISM:1||SINGLECRYSTALS:1||CeTe2:1||amorphous magnetic materials:1||EPITAXIAL GRAPHENE:1||LAYERED PNICTIDEOXIDES:1||BOROCARBIDE SUPERCONDUCTORS:1||AUGMENTEDWAVE METHOD:1||METALLIC MAGNET UNISN:1||ORIGIN:1||spectrum rearrangement:1||MEANFIELD THEORY:1||MOLECULEBASED MAGNETS:1||METASTABLE STATE:1||INSULATOR:1||magnetic orderin:1||FCC IRON:1||CeRu2:1||TL2MN2O7:1||isotope effect:1||Perovskitemanganites:1||RECURSION METHOD:1||PERPENDICULAR MAGNETICANISOTROPY:1||quasiparticle spectral density:1||GW:1||MANGANESE FERRITE:1||RESONANCE:1||SeCuO3:1||Optical conductivity:1||MASSLESS DIRAC FERMIONS:1||SCHOTTKYBARRIER:1||electronic structure:15||ELECTRONICSTRUCTURE:11||TRANSITIONMETAL COMPOUNDS:10||METALS:10||photoemission:8||SPECTRA:8||MAGNETORESISTANCE:7||FERROMAGNETISM:7||TRANSPORT:7||TRANSITION:6||FILMS:6||THINFILMS:5||TOTALENERGY CALCULATIONS:5||MAGNETICPROPERTIES:5||SUPERCONDUCTIVITY:5||PR:5||LATTICE:4||STATES:4||SPECTROSCOPY:4||FIELD:4||CRYSTALSTRUCTURE:4||PHOTOEMISSION:4||TEMPERATURE:4||TRANSITIONTEMPERATURE:4||XRAYABSORPTION:4||STATE:4||CU:4||BASISSET:4||XAS:4||CRYSTALS:3||EXCITATIONS:3||MOTTHUBBARD SYSTEMS:3||HIGHENERGY SPIN:3||halfmetal:3||INSULATORS:3||LA2CUO4:3||MODEL:3||FLUCTUATIONS:3||CE:3||double exchange:3||TRANSITIONMETALS:3||RESISTIVITY:3||BORON:3||LA1XCAXMNO3:3||IRON:3||PES:3||ANTIMONIDES:2||MgB2:2||ZR METALLIC GLASSES:2||superconductor:2||CRITICALCURRENT DENSITY:2||CIRCULARDICHROISM:2||SEMICONDUCTORS:2||LOCALIZATION:2||INTRABAND OPTICAL CONDUCTIVITY:2||COLOSSAL MAGNETORESISTANCE:2||OXIDATION:2||EXISTENCE:2||COPPER:2||diboride:2||MAGNESIUMDIBORIDE:2||GAP:2||CE COMPOUNDS:2||CORE POLARIZATION:2||magnetoresistance:2||photoemission spectroscopy:2||electronphonon interaction:2||GETTER:2||PD:2||MAGNETISM:2||FECR2S4:2||SUPERCONDUCTING MGB2:2||WIRES:2||ABSORPTION:2||ENERGY:2||LA1XSRXMNO3:2||CONSTANTS:2||polaron:2||charge ordering:2||SCATTERING:2||XRAY PHOTOEMISSION:2||CeNiSn:2||phase diagram:2||PHOTOELECTRON:2||QUADRUPOLAR:2||perovskitemanganites:2||CO:2||SYSTEMS:2||DOPED ZNO:2||LOWFREQUENCY SOUND:2||LA:2||ELECTRONELECTRON SCATTERING:2||AU:2||DENSITYWAVE INSTABILITY:2||FERMISURFACE:2||hybridization:2||VALENCEBAND SATELLITE:2||SULFUR SPINEL:2||Heusler:2||APPROXIMATION:2||superexchange:2||colossal magnetoresistance:2||ALLOYS:2||DEPENDENCE:2||AG:2||electronic structures:2||AUGERSPECTRA:2||CR:2||PARAMETERS:2||DIFFRACTION:2||SEMICONDUCTORMETAL TRANSITION:1||INTERMEDIATEVALENCE:1||SMB6:1||SRRUO3:1||antiperovskite structure with antipolar nature:1||lowenergy twodimensional phonons:1||anatase TiO2:1||La3S4:1||metalinsulator transitions:1||MNO:1||ELECTRONICSTRUCTURES:1||MAGNETIC CIRCULARDICHROISM:1||Density functional theory:1||CeCo2:1||TOPOLARON CROSSOVER:1||EXCHANGE:1||cuprates:1||high Tc cuprates:1||magnetically ordered materials:1||ZNSE:1||Sr2xKxFeMoO6:1||CDW:1||TeCuO3:1||STRUCTURALPROPERTIES:1||MN:1||screening length:1||amorphous Fe:1||WAVE BASISSET:1||SILICONCARBIDE:1||HIGHPRESSURE:1||electronphonon coupling:1||quenched superconductivity:1||CMR perovskite manganites:1||OXIDE:1||polarons:1||synchrotron radiation:1||FULLERIDES:1||RESONANTPHOTOEMISSION:1||Silicon carbide:1||DFT calculation:1||Hybridized bands:1||GIANT MAGNETORESISTANCE:1||PEROVSKITES:1||Raman spectra:1||EXCHANGE ENHANCEMENT:1||SILICON:1||SR2FEMOO6:1||orbital ordering:1||delafossite:1||TITANIUMDIOXIDE:1||electronic structure of disordered solids:1||YFE2:1||Magnetic polaron:1||NA2TI2SB2O:1||STRONGCOUPLED SUPERCONDUCTORS:1||HEAVYFERMION SYSTEMS:1||firstprinciples calculations:1||MECHANISM:1||UNiSn:1||PHOTONIC BANDGAP:1||SINGLE IMPURITY:1||PHONONSPECTRUM:1||FERMISURFACE TOPOLOGY:1||SUPPRESSION:1||RESONANT PHOTOEMISSION:1||METALDOPED PICENE:1||PHOTOIONIZATION CROSSSECTIONS:1||PHOTOINDUCED FERRIMAGNETIC SYSTEMS:1||LINKAGE ISOMERISM:1||CHARGETRANSFER:1||Bilayer Graphene:1||MAGNETICFIELD:1||SPINWAVES:1||rareearth manganese oxides:1||magnonphonon interaction:1||NACO2O4:1||ENERGYBANDS:1||SELFENERGY:1||GAS:1||Fe0.5Cu0.5Cr2S4:1||scanning photoelectron microscopy (SPEM):1||MAGNETIC PROPERTIES:1||Stoner model:1||AMORPHOUS TRANSITIONMETALS:1||SPINGLASS STATES:1||NI:1||LA3NI2B2N3:1||SOLIDS:1||CEO2:1||BAND THEORY:1||dilute magnetic semiconductor:1||pyrochlore:1||Y1XPRXBA2CU3O7DELTA:1||and electronphonon interactions:1||VIBRATIONS:1||RAY PHOTOEMISSION:1||ALKALI CATION:1||Europium:1||colossal magnetoresistance:1||structural stability:1||ENERGYGAP:1||small polaron:1||DOUBLE EXCHANGE:1||Coulomb correlation:1||magnon:1||phonons:1||ELECTRON FERROMAGNETISM:1||CURIETEMPERATURE:1||ARPES:1||PLANEWAVE METHOD:1||Xray absorption spectroscopy (XAS):1||ROOMTEMPERATURE:1||MONOCHALCOGENIDES:1||HEAT:1||UPDSN:1||MOMENTS:1||XRAY ABSORPTION:1||SEMICONDUCTOR:1||Fermi surface nesting:1||optical phonon:1||disordered system:1||dilute magnetic semiconductors:1||CMR manganites:1||PHONONS:1||LATTICEDYNAMICS:1||OXIDES:1||4fphotoemission:1||permanent magnet:1||pseudogap:1||TRANSPORTPROPERTIES:1||ANTIFERROMAGNET:1||(BI,PB)SRCOO SYSTEM:1||semicore correlation:1||POLARIZATION:1||CRYSTAL:1||spinel:1||Xray magnetic circular dichroism (XMCD):1||magnetocapacitance:1||ANATASE:1||TEMPERATURES:1||Pseudogap:1||INTERFACE:1||SUBSTRATE:1||YNI2B2C:1||SAMARIUM SULFIDE:1||strong swave superconductor:1||DOPED MANGANITE:1||SYMMETRY:1||CENISN:1||resonance mode:1||DISORDERED SYSTEM:1||LITHIUM INTERCALATION:1||CUO2 PLANE:1||SURFACE:1||Delafossite:1||ELECTRICALPROPERTIES:1||NIMNSB:1||PTMNSB:1||ROOMTEMPERATURE FERROMAGNETISM:1||RUBIDIUM MANGANESE HEXACYANOFERRATE:1||COLOSSALMAGNETORESISTANCE:1||FINITE TEMPERATURES:1||LAMNO3:1||FE:1||transitionmetal oxides:1||giant magnetoresistance:1||phonon:1||COPPER OXIDES:1||valence states:1||thermoelectric:1||semiconductor:1||CATION DISTRIBUTION:1||FeCr2S4:1||photoemission spectroscopy (PES):1||METALLIC FERROMAGNETISM:1||GRAPHITE:1||SUSCEPTIBILITY:1||UBE13:1||RCrSb3:1||band JahnTeller:1||Ce3S4:1||TiO2:1||PrBa2Cu3O7delta:1||UNTWINNED PRBA2CU3O7:1||AGNIO2:1||HALFMETALLIC FERROMAGNETS:1||CI:1||Energy gap:1||Photoemission:1||Future applications:1||Photoemission measurements:1||Graphene:1||BANDSTRUCTURE:1||TC:1||superconductivity:1||magnetic semiconductors:1||CMRmanganites:1||thin films:1||spin dynamics:1||highTc superconductors:1||ITINERANTELECTRON FERROMAGNETISM:1||SINGLECRYSTALS:1||CeTe2:1||amorphous magnetic materials:1||EPITAXIAL GRAPHENE:1||LAYERED PNICTIDEOXIDES:1||BOROCARBIDE SUPERCONDUCTORS:1||AUGMENTEDWAVE METHOD:1||METALLIC MAGNET UNISN:1||ORIGIN:1||spectrum rearrangement:1||MEANFIELD THEORY:1||MOLECULEBASED MAGNETS:1||METASTABLE STATE:1||INSULATOR:1||magnetic orderin:1||FCC IRON:1||CeRu2:1||TL2MN2O7:1||isotope effect:1||Perovskitemanganites:1||RECURSION METHOD:1||PERPENDICULAR MAGNETICANISOTROPY:1||quasiparticle spectral density:1||GW:1||MANGANESE FERRITE:1||RESONANCE:1||SeCuO3:1||Optical conductivity:1||MASSLESS DIRAC FERMIONS:1||SCHOTTKYBARRIER:1||electronic structure:15||ELECTRONICSTRUCTURE:11||TRANSITIONMETAL COMPOUNDS:10||METALS:10||photoemission:8||SPECTRA:8||MAGNETORESISTANCE:7||FERROMAGNETISM:7||TRANSPORT:7||TRANSITION:6||FILMS:6||THINFILMS:5||TOTALENERGY CALCULATIONS:5||MAGNETICPROPERTIES:5||SUPERCONDUCTIVITY:5||PR:5||LATTICE:4||STATES:4||SPECTROSCOPY:4||FIELD:4||CRYSTALSTRUCTURE:4||PHOTOEMISSION:4||TEMPERATURE:4||TRANSITIONTEMPERATURE:4||XRAYABSORPTION:4||STATE:4||CU:4||BASISSET:4||XAS:4||CRYSTALS:3||EXCITATIONS:3||MOTTHUBBARD SYSTEMS:3||HIGHENERGY SPIN:3||halfmetal:3||INSULATORS:3||LA2CUO4:3||MODEL:3||FLUCTUATIONS:3||CE:3||double exchange:3||TRANSITIONMETALS:3||RESISTIVITY:3||BORON:3||LA1XCAXMNO3:3||IRON:3||PES:3||ANTIMONIDES:2||MgB2:2||ZR METALLIC GLASSES:2||superconductor:2||CRITICALCURRENT DENSITY:2||CIRCULARDICHROISM:2||SEMICONDUCTORS:2||LOCALIZATION:2||INTRABAND OPTICAL CONDUCTIVITY:2||COLOSSAL MAGNETORESISTANCE:2||OXIDATION:2||EXISTENCE:2||COPPER:2||diboride:2||MAGNESIUMDIBORIDE:2||GAP:2||CE COMPOUNDS:2||CORE POLARIZATION:2||magnetoresistance:2||photoemission spectroscopy:2||electronphonon interaction:2||GETTER:2||PD:2||MAGNETISM:2||FECR2S4:2||SUPERCONDUCTING MGB2:2||WIRES:2||ABSORPTION:2||ENERGY:2||LA1XSRXMNO3:2||CONSTANTS:2||polaron:2||charge ordering:2||SCATTERING:2||XRAY PHOTOEMISSION:2||CeNiSn:2||phase diagram:2||PHOTOELECTRON:2||QUADRUPOLAR:2||perovskitemanganites:2||CO:2||SYSTEMS:2||DOPED ZNO:2||LOWFREQUENCY SOUND:2||LA:2||ELECTRONELECTRON SCATTERING:2||AU:2||DENSITYWAVE INSTABILITY:2||FERMISURFACE:2||hybridization:2||VALENCEBAND SATELLITE:2||SULFUR SPINEL:2||Heusler:2||APPROXIMATION:2||superexchange:2||colossal magnetoresistance:2||ALLOYS:2||DEPENDENCE:2||AG:2||electronic structures:2||AUGERSPECTRA:2||CR:2||PARAMETERS:2||DIFFRACTION:2||SEMICONDUCTORMETAL TRANSITION:1||INTERMEDIATEVALENCE:1||SMB6:1||SRRUO3:1||antiperovskite structure with antipolar nature:1||lowenergy twodimensional phonons:1||anatase TiO2:1||La3S4:1||metalinsulator transitions:1||MNO:1||ELECTRONICSTRUCTURES:1||MAGNETIC CIRCULARDICHROISM:1||Density functional theory:1||CeCo2:1||TOPOLARON CROSSOVER:1||EXCHANGE:1||cuprates:1||high Tc cuprates:1||magnetically ordered materials:1||ZNSE:1||Sr2xKxFeMoO6:1||CDW:1||TeCuO3:1||STRUCTURALPROPERTIES:1||MN:1||screening length:1||amorphous Fe:1||WAVE BASISSET:1||SILICONCARBIDE:1||HIGHPRESSURE:1||electronphonon coupling:1||quenched superconductivity:1||CMR perovskite manganites:1||OXIDE:1||polarons:1||synchrotron radiation:1||FULLERIDES:1||RESONANTPHOTOEMISSION:1||Silicon carbide:1||DFT calculation:1||Hybridized bands:1||GIANT MAGNETORESISTANCE:1||PEROVSKITES:1||Raman spectra:1||EXCHANGE ENHANCEMENT:1||SILICON:1||SR2FEMOO6:1||orbital ordering:1||delafossite:1||TITANIUMDIOXIDE:1||electronic structure of disordered solids:1||YFE2:1||Magnetic polaron:1||NA2TI2SB2O:1||STRONGCOUPLED SUPERCONDUCTORS:1||HEAVYFERMION SYSTEMS:1||firstprinciples calculations:1||MECHANISM:1||UNiSn:1||PHOTONIC BANDGAP:1||SINGLE IMPURITY:1||PHONONSPECTRUM:1||FERMISURFACE TOPOLOGY:1||SUPPRESSION:1||RESONANT PHOTOEMISSION:1||METALDOPED PICENE:1||PHOTOIONIZATION CROSSSECTIONS:1||PHOTOINDUCED FERRIMAGNETIC SYSTEMS:1||LINKAGE ISOMERISM:1||CHARGETRANSFER:1||Bilayer Graphene:1||MAGNETICFIELD:1||SPINWAVES:1||rareearth manganese oxides:1||magnonphonon interaction:1||NACO2O4:1||ENERGYBANDS:1||SELFENERGY:1||GAS:1||Fe0.5Cu0.5Cr2S4:1||scanning photoelectron microscopy (SPEM):1||MAGNETIC PROPERTIES:1||Stoner model:1||AMORPHOUS TRANSITIONMETALS:1||SPINGLASS STATES:1||NI:1||LA3NI2B2N3:1||SOLIDS:1||CEO2:1||BAND THEORY:1||dilute magnetic semiconductor:1||pyrochlore:1||Y1XPRXBA2CU3O7DELTA:1||and electronphonon interactions:1||VIBRATIONS:1||RAY PHOTOEMISSION:1||ALKALI CATION:1||Europium:1||colossal magnetoresistance:1||structural stability:1||ENERGYGAP:1||small polaron:1||DOUBLE EXCHANGE:1||Coulomb correlation:1||magnon:1||phonons:1||ELECTRON FERROMAGNETISM:1||CURIETEMPERATURE:1||ARPES:1||PLANEWAVE METHOD:1||Xray absorption spectroscopy (XAS):1||ROOMTEMPERATURE:1||MONOCHALCOGENIDES:1||HEAT:1||UPDSN:1||MOMENTS:1||XRAY ABSORPTION:1||SEMICONDUCTOR:1||Fermi surface nesting:1||optical phonon:1||disordered system:1||dilute magnetic semiconductors:1||CMR manganites:1||PHONONS:1||LATTICEDYNAMICS:1||OXIDES:1||4fphotoemission:1||permanent magnet:1||pseudogap:1||TRANSPORTPROPERTIES:1||ANTIFERROMAGNET:1||(BI,PB)SRCOO SYSTEM:1||semicore correlation:1||POLARIZATION:1||CRYSTAL:1||spinel:1||Xray magnetic circular dichroism (XMCD):1||magnetocapacitance:1||ANATASE:1||TEMPERATURES:1||Pseudogap:1||INTERFACE:1||SUBSTRATE:1||YNI2B2C:1||SAMARIUM SULFIDE:1||strong swave superconductor:1||DOPED MANGANITE:1||SYMMETRY:1||CENISN:1||resonance mode:1||DISORDERED SYSTEM:1||LITHIUM INTERCALATION:1||CUO2 PLANE:1||SURFACE:1||Delafossite:1||ELECTRICALPROPERTIES:1||NIMNSB:1||PTMNSB:1||ROOMTEMPERATURE FERROMAGNETISM:1||RUBIDIUM MANGANESE HEXACYANOFERRATE:1||COLOSSALMAGNETORESISTANCE:1||FINITE TEMPERATURES:1||LAMNO3:1||FE:1||transitionmetal oxides:1||giant magnetoresistance:1||phonon:1||COPPER OXIDES:1||valence states:1||thermoelectric:1||semiconductor:1||CATION DISTRIBUTION:1||FeCr2S4:1||photoemission spectroscopy (PES):1||METALLIC FERROMAGNETISM:1||GRAPHITE:1||SUSCEPTIBILITY:1||UBE13:1||RCrSb3:1||band JahnTeller:1||Ce3S4:1||TiO2:1||PrBa2Cu3O7delta:1||UNTWINNED PRBA2CU3O7:1||AGNIO2:1||HALFMETALLIC FERROMAGNETS:1||CI:1||Energy gap:1||Photoemission:1||Future applications:1||Photoemission measurements:1||Graphene:1||BANDSTRUCTURE:1||TC:1||superconductivity:1||magnetic semiconductors:1||CMRmanganites:1||thin films:1||spin dynamics:1||highTc superconductors:1||ITINERANTELECTRON FERROMAGNETISM:1||SINGLECRYSTALS:1||CeTe2:1||amorphous magnetic materials:1||EPITAXIAL GRAPHENE:1||LAYERED PNICTIDEOXIDES:1||BOROCARBIDE SUPERCONDUCTORS:1||AUGMENTEDWAVE METHOD:1||METALLIC MAGNET UNISN:1||ORIGIN:1||spectrum rearrangement:1||MEANFIELD THEORY:1||MOLECULEBASED MAGNETS:1||METASTABLE STATE:1||INSULATOR:1||magnetic orderin:1||FCC IRON:1||CeRu2:1||TL2MN2O7:1||isotope effect:1||Perovskitemanganites:1||RECURSION METHOD:1||PERPENDICULAR MAGNETICANISOTROPY:1||quasiparticle spectral density:1||GW:1||MANGANESE FERRITE:1||RESONANCE:1||SeCuO3:1||Optical conductivity:1||MASSLESS DIRAC FERMIONS:1||SCHOTTKYBARRIER:1||electronic structure:15||ELECTRONICSTRUCTURE:11||TRANSITIONMETAL COMPOUNDS:10||METALS:10||photoemission:8||SPECTRA:8||MAGNETORESISTANCE:7||FERROMAGNETISM:7||TRANSPORT:7||TRANSITION:6||FILMS:6||THINFILMS:5||TOTALENERGY CALCULATIONS:5||MAGNETICPROPERTIES:5||SUPERCONDUCTIVITY:5||PR:5||LATTICE:4||STATES:4||SPECTROSCOPY:4||FIELD:4||CRYSTALSTRUCTURE:4||PHOTOEMISSION:4||TEMPERATURE:4||TRANSITIONTEMPERATURE:4||XRAYABSORPTION:4||STATE:4||CU:4||BASISSET:4||XAS:4||CRYSTALS:3||EXCITATIONS:3||MOTTHUBBARD SYSTEMS:3||HIGHENERGY SPIN:3||halfmetal:3||INSULATORS:3||LA2CUO4:3||MODEL:3||FLUCTUATIONS:3||CE:3||double exchange:3||TRANSITIONMETALS:3||RESISTIVITY:3||BORON:3||LA1XCAXMNO3:3||IRON:3||PES:3||ANTIMONIDES:2||MgB2:2||ZR METALLIC GLASSES:2||superconductor:2||CRITICALCURRENT DENSITY:2||CIRCULARDICHROISM:2||SEMICONDUCTORS:2||LOCALIZATION:2||INTRABAND OPTICAL CONDUCTIVITY:2||COLOSSAL MAGNETORESISTANCE:2||OXIDATION:2||EXISTENCE:2||COPPER:2||diboride:2||MAGNESIUMDIBORIDE:2||GAP:2||CE COMPOUNDS:2||CORE POLARIZATION:2||magnetoresistance:2||photoemission spectroscopy:2||electronphonon interaction:2||GETTER:2||PD:2||MAGNETISM:2||FECR2S4:2||SUPERCONDUCTING MGB2:2||WIRES:2||ABSORPTION:2||ENERGY:2||LA1XSRXMNO3:2||CONSTANTS:2||polaron:2||charge ordering:2||SCATTERING:2||XRAY PHOTOEMISSION:2||CeNiSn:2||phase diagram:2||PHOTOELECTRON:2||QUADRUPOLAR:2||perovskitemanganites:2||CO:2||SYSTEMS:2||DOPED ZNO:2||LOWFREQUENCY SOUND:2||LA:2||ELECTRONELECTRON SCATTERING:2||AU:2||DENSITYWAVE INSTABILITY:2||FERMISURFACE:2||hybridization:2||VALENCEBAND SATELLITE:2||SULFUR SPINEL:2||Heusler:2||APPROXIMATION:2||superexchange:2||colossal magnetoresistance:2||ALLOYS:2||DEPENDENCE:2||AG:2||electronic structures:2||AUGERSPECTRA:2||CR:2||PARAMETERS:2||DIFFRACTION:2||SEMICONDUCTORMETAL TRANSITION:1||INTERMEDIATEVALENCE:1||SMB6:1||SRRUO3:1||antiperovskite structure with antipolar nature:1||lowenergy twodimensional phonons:1||anatase TiO2:1||La3S4:1||metalinsulator transitions:1||MNO:1||ELECTRONICSTRUCTURES:1||MAGNETIC CIRCULARDICHROISM:1||Density functional theory:1||CeCo2:1||TOPOLARON CROSSOVER:1||EXCHANGE:1||cuprates:1||high Tc cuprates:1||magnetically ordered materials:1||ZNSE:1||Sr2xKxFeMoO6:1||CDW:1||TeCuO3:1||STRUCTURALPROPERTIES:1||MN:1||screening length:1||amorphous Fe:1||WAVE BASISSET:1||SILICONCARBIDE:1||HIGHPRESSURE:1||electronphonon coupling:1||quenched superconductivity:1||CMR perovskite manganites:1||OXIDE:1||polarons:1||synchrotron radiation:1||FULLERIDES:1||RESONANTPHOTOEMISSION:1||Silicon carbide:1||DFT calculation:1||Hybridized bands:1||GIANT MAGNETORESISTANCE:1||PEROVSKITES:1||Raman spectra:1||EXCHANGE ENHANCEMENT:1||SILICON:1||SR2FEMOO6:1||orbital ordering:1||delafossite:1||TITANIUMDIOXIDE:1||electronic structure of disordered solids:1||YFE2:1||Magnetic polaron:1||NA2TI2SB2O:1||STRONGCOUPLED SUPERCONDUCTORS:1||HEAVYFERMION SYSTEMS:1||firstprinciples calculations:1||MECHANISM:1||UNiSn:1||PHOTONIC BANDGAP:1||SINGLE IMPURITY:1||PHONONSPECTRUM:1||FERMISURFACE TOPOLOGY:1||SUPPRESSION:1||RESONANT PHOTOEMISSION:1||METALDOPED PICENE:1||PHOTOIONIZATION CROSSSECTIONS:1||PHOTOINDUCED FERRIMAGNETIC SYSTEMS:1||LINKAGE ISOMERISM:1||CHARGETRANSFER:1||Bilayer Graphene:1||MAGNETICFIELD:1||SPINWAVES:1||rareearth manganese oxides:1||magnonphonon interaction:1||NACO2O4:1||ENERGYBANDS:1||SELFENERGY:1||GAS:1||Fe0.5Cu0.5Cr2S4:1||scanning photoelectron microscopy (SPEM):1||MAGNETIC PROPERTIES:1||Stoner model:1||AMORPHOUS TRANSITIONMETALS:1||SPINGLASS STATES:1||NI:1||LA3NI2B2N3:1||SOLIDS:1||CEO2:1||BAND THEORY:1||dilute magnetic semiconductor:1||pyrochlore:1||Y1XPRXBA2CU3O7DELTA:1||and electronphonon interactions:1||VIBRATIONS:1||RAY PHOTOEMISSION:1||ALKALI CATION:1||Europium:1||colossal magnetoresistance:1||structural stability:1||ENERGYGAP:1||small polaron:1||DOUBLE EXCHANGE:1||Coulomb correlation:1||magnon:1||phonons:1||ELECTRON FERROMAGNETISM:1||CURIETEMPERATURE:1||ARPES:1||PLANEWAVE METHOD:1||Xray absorption spectroscopy (XAS):1||ROOMTEMPERATURE:1||MONOCHALCOGENIDES:1||HEAT:1||UPDSN:1||MOMENTS:1||XRAY ABSORPTION:1||SEMICONDUCTOR:1||Fermi surface nesting:1||optical phonon:1||disordered system:1||dilute magnetic semiconductors:1||CMR manganites:1||PHONONS:1||LATTICEDYNAMICS:1||OXIDES:1||4fphotoemission:1||permanent magnet:1||pseudogap:1||TRANSPORTPROPERTIES:1||ANTIFERROMAGNET:1||(BI,PB)SRCOO SYSTEM:1||semicore correlation:1||POLARIZATION:1||CRYSTAL:1||spinel:1||Xray magnetic circular dichroism (XMCD):1||magnetocapacitance:1||ANATASE:1||TEMPERATURES:1||Pseudogap:1||INTERFACE:1||SUBSTRATE:1||YNI2B2C:1||SAMARIUM SULFIDE:1||strong swave superconductor:1||DOPED MANGANITE:1||SYMMETRY:1||CENISN:1||resonance mode:1||DISORDERED SYSTEM:1||LITHIUM INTERCALATION:1||CUO2 PLANE:1||SURFACE:1||Delafossite:1||ELECTRICALPROPERTIES:1||NIMNSB:1||PTMNSB:1||ROOMTEMPERATURE FERROMAGNETISM:1||RUBIDIUM MANGANESE HEXACYANOFERRATE:1||COLOSSALMAGNETORESISTANCE:1||FINITE TEMPERATURES:1||LAMNO3:1||FE:1||transitionmetal oxides:1||giant magnetoresistance:1||phonon:1||COPPER OXIDES:1||valence states:1||thermoelectric:1||semiconductor:1||CATION DISTRIBUTION:1||FeCr2S4:1||photoemission spectroscopy (PES):1||METALLIC FERROMAGNETISM:1||GRAPHITE:1||SUSCEPTIBILITY:1||UBE13:1||RCrSb3:1||band JahnTeller:1||Ce3S4:1||TiO2:1||PrBa2Cu3O7delta:1||UNTWINNED PRBA2CU3O7:1||AGNIO2:1||HALFMETALLIC FERROMAGNETS:1||CI:1||Energy gap:1||Photoemission:1||Future applications:1||Photoemission measurements:1||Graphene:1||BANDSTRUCTURE:1||TC:1||superconductivity:1||magnetic semiconductors:1||CMRmanganites:1||thin films:1||spin dynamics:1||highTc superconductors:1||ITINERANTELECTRON FERROMAGNETISM:1||SINGLECRYSTALS:1||CeTe2:1||amorphous magnetic materials:1||EPITAXIAL GRAPHENE:1||LAYERED PNICTIDEOXIDES:1||BOROCARBIDE SUPERCONDUCTORS:1||AUGMENTEDWAVE METHOD:1||METALLIC MAGNET UNISN:1||ORIGIN:1||spectrum rearrangement:1||MEANFIELD THEORY:1||MOLECULEBASED MAGNETS:1||METASTABLE STATE:1||INSULATOR:1||magnetic orderin:1||FCC IRON:1||CeRu2:1||TL2MN2O7:1||isotope effect:1||Perovskitemanganites:1||RECURSION METHOD:1||PERPENDICULAR MAGNETICANISOTROPY:1||quasiparticle spectral density:1||GW:1||MANGANESE FERRITE:1||RESONANCE:1||SeCuO3:1||Optical conductivity:1||MASSLESS DIRAC FERMIONS:1||SCHOTTKYBARRIER:1||electronic structure:15||ELECTRONICSTRUCTURE:11||TRANSITIONMETAL COMPOUNDS:10||METALS:10||photoemission:8||SPECTRA:8||MAGNETORESISTANCE:7||FERROMAGNETISM:7||TRANSPORT:7||TRANSITION:6||FILMS:6||THINFILMS:5||TOTALENERGY CALCULATIONS:5||MAGNETICPROPERTIES:5||SUPERCONDUCTIVITY:5||PR:5||LATTICE:4||STATES:4||SPECTROSCOPY:4||FIELD:4||CRYSTALSTRUCTURE:4||PHOTOEMISSION:4||TEMPERATURE:4||TRANSITIONTEMPERATURE:4||XRAYABSORPTION:4||STATE:4||CU:4||BASISSET:4||XAS:4||CRYSTALS:3||EXCITATIONS:3||MOTTHUBBARD SYSTEMS:3||HIGHENERGY SPIN:3||halfmetal:3||INSULATORS:3||LA2CUO4:3||MODEL:3||FLUCTUATIONS:3||CE:3||double exchange:3||TRANSITIONMETALS:3||RESISTIVITY:3||BORON:3||LA1XCAXMNO3:3||IRON:3||PES:3||ANTIMONIDES:2||MgB2:2||ZR METALLIC GLASSES:2||superconductor:2||CRITICALCURRENT DENSITY:2||CIRCULARDICHROISM:2||SEMICONDUCTORS:2||LOCALIZATION:2||INTRABAND OPTICAL CONDUCTIVITY:2||COLOSSAL MAGNETORESISTANCE:2||OXIDATION:2||EXISTENCE:2||COPPER:2||diboride:2||MAGNESIUMDIBORIDE:2||GAP:2||CE COMPOUNDS:2||CORE POLARIZATION:2||magnetoresistance:2||photoemission spectroscopy:2||electronphonon interaction:2||GETTER:2||PD:2||MAGNETISM:2||FECR2S4:2||SUPERCONDUCTING MGB2:2||WIRES:2||ABSORPTION:2||ENERGY:2||LA1XSRXMNO3:2||CONSTANTS:2||polaron:2||charge ordering:2||SCATTERING:2||XRAY PHOTOEMISSION:2||CeNiSn:2||phase diagram:2||PHOTOELECTRON:2||QUADRUPOLAR:2||perovskitemanganites:2||CO:2||SYSTEMS:2||DOPED ZNO:2||LOWFREQUENCY SOUND:2||LA:2||ELECTRONELECTRON SCATTERING:2||AU:2||DENSITYWAVE INSTABILITY:2||FERMISURFACE:2||hybridization:2||VALENCEBAND SATELLITE:2||SULFUR SPINEL:2||Heusler:2||APPROXIMATION:2||superexchange:2||colossal magnetoresistance:2||ALLOYS:2||DEPENDENCE:2||AG:2||electronic structures:2||AUGERSPECTRA:2||CR:2||PARAMETERS:2||DIFFRACTION:2||SEMICONDUCTORMETAL TRANSITION:1||INTERMEDIATEVALENCE:1||SMB6:1||SRRUO3:1||antiperovskite structure with antipolar nature:1||lowenergy twodimensional phonons:1||anatase TiO2:1||La3S4:1||metalinsulator transitions:1||MNO:1||ELECTRONICSTRUCTURES:1||MAGNETIC CIRCULARDICHROISM:1||Density functional theory:1||CeCo2:1||TOPOLARON CROSSOVER:1||EXCHANGE:1||cuprates:1||high Tc cuprates:1||magnetically ordered materials:1||ZNSE:1||Sr2xKxFeMoO6:1||CDW:1||TeCuO3:1||STRUCTURALPROPERTIES:1||MN:1||screening length:1||amorphous Fe:1||WAVE BASISSET:1||SILICONCARBIDE:1||HIGHPRESSURE:1||electronphonon coupling:1||quenched superconductivity:1||CMR perovskite manganites:1||OXIDE:1||polarons:1||synchrotron radiation:1||FULLERIDES:1||RESONANTPHOTOEMISSION:1||Silicon carbide:1||DFT calculation:1||Hybridized bands:1||GIANT MAGNETORESISTANCE:1||PEROVSKITES:1||Raman spectra:1||EXCHANGE ENHANCEMENT:1||SILICON:1||SR2FEMOO6:1||orbital ordering:1||delafossite:1||TITANIUMDIOXIDE:1||electronic structure of disordered solids:1||YFE2:1||Magnetic polaron:1||NA2TI2SB2O:1||STRONGCOUPLED SUPERCONDUCTORS:1||HEAVYFERMION SYSTEMS:1||firstprinciples calculations:1||MECHANISM:1||UNiSn:1||PHOTONIC BANDGAP:1||SINGLE IMPURITY:1||PHONONSPECTRUM:1||FERMISURFACE TOPOLOGY:1||SUPPRESSION:1||RESONANT PHOTOEMISSION:1||METALDOPED PICENE:1||PHOTOIONIZATION CROSSSECTIONS:1||PHOTOINDUCED FERRIMAGNETIC SYSTEMS:1||LINKAGE ISOMERISM:1||CHARGETRANSFER:1||Bilayer Graphene:1||MAGNETICFIELD:1||SPINWAVES:1||rareearth manganese oxides:1||magnonphonon interaction:1||NACO2O4:1||ENERGYBANDS:1||SELFENERGY:1||GAS:1||Fe0.5Cu0.5Cr2S4:1||scanning photoelectron microscopy (SPEM):1||MAGNETIC PROPERTIES:1||Stoner model:1||AMORPHOUS TRANSITIONMETALS:1||SPINGLASS STATES:1||NI:1||LA3NI2B2N3:1||SOLIDS:1||CEO2:1||BAND THEORY:1||dilute magnetic semiconductor:1||pyrochlore:1||Y1XPRXBA2CU3O7DELTA:1||and electronphonon interactions:1||VIBRATIONS:1||RAY PHOTOEMISSION:1||ALKALI CATION:1||Europium:1||colossal magnetoresistance:1||structural stability:1||ENERGYGAP:1||small polaron:1||DOUBLE EXCHANGE:1||Coulomb correlation:1||magnon:1||phonons:1||ELECTRON FERROMAGNETISM:1||CURIETEMPERATURE:1||ARPES:1||PLANEWAVE METHOD:1||Xray absorption spectroscopy (XAS):1||ROOMTEMPERATURE:1||MONOCHALCOGENIDES:1||HEAT:1||UPDSN:1||MOMENTS:1||XRAY ABSORPTION:1||SEMICONDUCTOR:1||Fermi surface nesting:1||optical phonon:1||disordered system:1||dilute magnetic semiconductors:1||CMR manganites:1||PHONONS:1||LATTICEDYNAMICS:1||OXIDES:1||4fphotoemission:1||permanent magnet:1||pseudogap:1||TRANSPORTPROPERTIES:1||ANTIFERROMAGNET:1||(BI,PB)SRCOO SYSTEM:1||semicore correlation:1||POLARIZATION:1||CRYSTAL:1||spinel:1||Xray magnetic circular dichroism (XMCD):1||magnetocapacitance:1||ANATASE:1||TEMPERATURES:1||Pseudogap:1||INTERFACE:1||SUBSTRATE:1||YNI2B2C:1||SAMARIUM SULFIDE:1||strong swave superconductor:1||DOPED MANGANITE:1||SYMMETRY:1||CENISN:1||resonance mode:1||DISORDERED SYSTEM:1||LITHIUM INTERCALATION:1||CUO2 PLANE:1||SURFACE:1||Delafossite:1||ELECTRICALPROPERTIES:1||NIMNSB:1||PTMNSB:1||ROOMTEMPERATURE FERROMAGNETISM:1||RUBIDIUM MANGANESE HEXACYANOFERRATE:1||COLOSSALMAGNETORESISTANCE:1||FINITE TEMPERATURES:1||LAMNO3:1||FE:1||transitionmetal oxides:1||giant magnetoresistance:1||phonon:1||COPPER OXIDES:1||valence states:1||thermoelectric:1||semiconductor:1||CATION DISTRIBUTION:1||FeCr2S4:1||photoemission spectroscopy (PES):1||METALLIC FERROMAGNETISM:1||GRAPHITE:1||SUSCEPTIBILITY:1||UBE13:1||RCrSb3:1||band JahnTeller:1||Ce3S4:1||TiO2:1||PrBa2Cu3O7delta:1||UNTWINNED PRBA2CU3O7:1||AGNIO2:1||HALFMETALLIC FERROMAGNETS:1||CI:1||Energy gap:1||Photoemission:1||Future applications:1||Photoemission measurements:1||Graphene:1||BANDSTRUCTURE:1||TC:1||superconductivity:1||magnetic semiconductors:1||CMRmanganites:1||thin films:1||spin dynamics:1||highTc superconductors:1||ITINERANTELECTRON FERROMAGNETISM:1||SINGLECRYSTALS:1||CeTe2:1||amorphous magnetic materials:1||EPITAXIAL GRAPHENE:1||LAYERED PNICTIDEOXIDES:1||BOROCARBIDE SUPERCONDUCTORS:1||AUGMENTEDWAVE METHOD:1||METALLIC MAGNET UNISN:1||ORIGIN:1||spectrum rearrangement:1||MEANFIELD THEORY:1||MOLECULEBASED MAGNETS:1||METASTABLE STATE:1||INSULATOR:1||magnetic orderin:1||FCC IRON:1||CeRu2:1||TL2MN2O7:1||isotope effect:1||Perovskitemanganites:1||RECURSION METHOD:1||PERPENDICULAR MAGNETICANISOTROPY:1||quasiparticle spectral density:1||GW:1||MANGANESE FERRITE:1||RESONANCE:1||SeCuO3:1||Optical conductivity:1||MASSLESS DIRAC FERMIONS:1||SCHOTTKYBARRIER:1||electronic structure:15||ELECTRONICSTRUCTURE:11||TRANSITIONMETAL COMPOUNDS:10||METALS:10||photoemission:8||SPECTRA:8||MAGNETORESISTANCE:7||FERROMAGNETISM:7||TRANSPORT:7||TRANSITION:6||FILMS:6||THINFILMS:5||TOTALENERGY CALCULATIONS:5||MAGNETICPROPERTIES:5||SUPERCONDUCTIVITY:5||PR:5||LATTICE:4||STATES:4||SPECTROSCOPY:4||FIELD:4||CRYSTALSTRUCTURE:4||PHOTOEMISSION:4||TEMPERATURE:4||TRANSITIONTEMPERATURE:4||XRAYABSORPTION:4||STATE:4||CU:4||BASISSET:4||XAS:4||CRYSTALS:3||EXCITATIONS:3||MOTTHUBBARD SYSTEMS:3||HIGHENERGY SPIN:3||halfmetal:3||INSULATORS:3||LA2CUO4:3||MODEL:3||FLUCTUATIONS:3||CE:3||double exchange:3||TRANSITIONMETALS:3||RESISTIVITY:3||BORON:3||LA1XCAXMNO3:3||IRON:3||PES:3||ANTIMONIDES:2||MgB2:2||ZR METALLIC GLASSES:2||superconductor:2||CRITICALCURRENT DENSITY:2||CIRCULARDICHROISM:2||SEMICONDUCTORS:2||LOCALIZATION:2||INTRABAND OPTICAL CONDUCTIVITY:2||COLOSSAL MAGNETORESISTANCE:2||OXIDATION:2||EXISTENCE:2||COPPER:2||diboride:2||MAGNESIUMDIBORIDE:2||GAP:2||CE COMPOUNDS:2||CORE POLARIZATION:2||magnetoresistance:2||photoemission spectroscopy:2||electronphonon interaction:2||GETTER:2||PD:2||MAGNETISM:2||FECR2S4:2||SUPERCONDUCTING MGB2:2||WIRES:2||ABSORPTION:2||ENERGY:2||LA1XSRXMNO3:2||CONSTANTS:2||polaron:2||charge ordering:2||SCATTERING:2||XRAY PHOTOEMISSION:2||CeNiSn:2||phase diagram:2||PHOTOELECTRON:2||QUADRUPOLAR:2||perovskitemanganites:2||CO:2||SYSTEMS:2||DOPED ZNO:2||LOWFREQUENCY SOUND:2||LA:2||ELECTRONELECTRON SCATTERING:2||AU:2||DENSITYWAVE INSTABILITY:2||FERMISURFACE:2||hybridization:2||VALENCEBAND SATELLITE:2||SULFUR SPINEL:2||Heusler:2||APPROXIMATION:2||superexchange:2||colossal magnetoresistance:2||ALLOYS:2||DEPENDENCE:2||AG:2||electronic structures:2||AUGERSPECTRA:2||CR:2||PARAMETERS:2||DIFFRACTION:2||SEMICONDUCTORMETAL TRANSITION:1||INTERMEDIATEVALENCE:1||SMB6:1||SRRUO3:1||antiperovskite structure with antipolar nature:1||lowenergy twodimensional phonons:1||anatase TiO2:1||La3S4:1||metalinsulator transitions:1||MNO:1||ELECTRONICSTRUCTURES:1||MAGNETIC CIRCULARDICHROISM:1||Density functional theory:1||CeCo2:1||TOPOLARON CROSSOVER:1||EXCHANGE:1||cuprates:1||high Tc cuprates:1||magnetically ordered materials:1||ZNSE:1||Sr2xKxFeMoO6:1||CDW:1||TeCuO3:1||STRUCTURALPROPERTIES:1||MN:1||screening length:1||amorphous Fe:1||WAVE BASISSET:1||SILICONCARBIDE:1||HIGHPRESSURE:1||electronphonon coupling:1||quenched superconductivity:1||CMR perovskite manganites:1||OXIDE:1||polarons:1||synchrotron radiation:1||FULLERIDES:1||RESONANTPHOTOEMISSION:1||Silicon carbide:1||DFT calculation:1||Hybridized bands:1||GIANT MAGNETORESISTANCE:1||PEROVSKITES:1||Raman spectra:1||EXCHANGE ENHANCEMENT:1||SILICON:1||SR2FEMOO6:1||orbital ordering:1||delafossite:1||TITANIUMDIOXIDE:1||electronic structure of disordered solids:1||YFE2:1||Magnetic polaron:1||NA2TI2SB2O:1||STRONGCOUPLED SUPERCONDUCTORS:1||HEAVYFERMION SYSTEMS:1||firstprinciples calculations:1||MECHANISM:1||UNiSn:1||PHOTONIC BANDGAP:1||SINGLE IMPURITY:1||PHONONSPECTRUM:1||FERMISURFACE TOPOLOGY:1||SUPPRESSION:1||RESONANT PHOTOEMISSION:1||METALDOPED PICENE:1||PHOTOIONIZATION CROSSSECTIONS:1||PHOTOINDUCED FERRIMAGNETIC SYSTEMS:1||LINKAGE ISOMERISM:1||CHARGETRANSFER:1||Bilayer Graphene:1||MAGNETICFIELD:1||SPINWAVES:1||rareearth manganese oxides:1||magnonphonon interaction:1||NACO2O4:1||ENERGYBANDS:1||SELFENERGY:1||GAS:1||Fe0.5Cu0.5Cr2S4:1||scanning photoelectron microscopy (SPEM):1||MAGNETIC PROPERTIES:1||Stoner model:1||AMORPHOUS TRANSITIONMETALS:1||SPINGLASS STATES:1||NI:1||LA3NI2B2N3:1||SOLIDS:1||CEO2:1||BAND THEORY:1||dilute magnetic semiconductor:1||pyrochlore:1||Y1XPRXBA2CU3O7DELTA:1||and electronphonon interactions:1||VIBRATIONS:1||RAY PHOTOEMISSION:1||ALKALI CATION:1||Europium:1||colossal magnetoresistance:1||structural stability:1||ENERGYGAP:1||small polaron:1||DOUBLE EXCHANGE:1||Coulomb correlation:1||magnon:1||phonons:1||ELECTRON FERROMAGNETISM:1||CURIETEMPERATURE:1||ARPES:1||PLANEWAVE METHOD:1||Xray absorption spectroscopy (XAS):1||ROOMTEMPERATURE:1||MONOCHALCOGENIDES:1||HEAT:1||UPDSN:1||MOMENTS:1||XRAY ABSORPTION:1||SEMICONDUCTOR:1||Fermi surface nesting:1||optical phonon:1||disordered system:1||dilute magnetic semiconductors:1||CMR manganites:1||PHONONS:1||LATTICEDYNAMICS:1||OXIDES:1||4fphotoemission:1||permanent magnet:1||pseudogap:1||TRANSPORTPROPERTIES:1||ANTIFERROMAGNET:1||(BI,PB)SRCOO SYSTEM:1||semicore correlation:1||POLARIZATION:1||CRYSTAL:1||spinel:1||Xray magnetic circular dichroism (XMCD):1||magnetocapacitance:1||ANATASE:1||TEMPERATURES:1||Pseudogap:1||INTERFACE:1||SUBSTRATE:1||YNI2B2C:1||SAMARIUM SULFIDE:1||strong swave superconductor:1||DOPED MANGANITE:1||SYMMETRY:1||CENISN:1||resonance mode:1||DISORDERED SYSTEM:1||LITHIUM INTERCALATION:1||CUO2 PLANE:1||SURFACE:1||Delafossite:1||ELECTRICALPROPERTIES:1||NIMNSB:1||PTMNSB:1||ROOMTEMPERATURE FERROMAGNETISM:1||RUBIDIUM MANGANESE HEXACYANOFERRATE:1||COLOSSALMAGNETORESISTANCE:1||FINITE TEMPERATURES:1||LAMNO3:1||FE:1||transitionmetal oxides:1||giant magnetoresistance:1||phonon:1||COPPER OXIDES:1||valence states:1||thermoelectric:1||semiconductor:1||CATION DISTRIBUTION:1||FeCr2S4:1||photoemission spectroscopy (PES):1||METALLIC FERROMAGNETISM:1||GRAPHITE:1||SUSCEPTIBILITY:1||UBE13:1||RCrSb3:1||band JahnTeller:1||Ce3S4:1||TiO2:1||PrBa2Cu3O7delta:1||UNTWINNED PRBA2CU3O7:1||AGNIO2:1||HALFMETALLIC FERROMAGNETS:1||CI:1||Energy gap:1||Photoemission:1||Future applications:1||Photoemission measurements:1||Graphene:1||BANDSTRUCTURE:1||TC:1||superconductivity:1||magnetic semiconductors:1||CMRmanganites:1||thin films:1||spin dynamics:1||highTc superconductors:1||ITINERANTELECTRON FERROMAGNETISM:1||SINGLECRYSTALS:1||CeTe2:1||amorphous magnetic materials:1||EPITAXIAL GRAPHENE:1||LAYERED PNICTIDEOXIDES:1||BOROCARBIDE SUPERCONDUCTORS:1||AUGMENTEDWAVE METHOD:1||METALLIC MAGNET UNISN:1||ORIGIN:1||spectrum rearrangement:1||MEANFIELD THEORY:1||MOLECULEBASED MAGNETS:1||METASTABLE STATE:1||INSULATOR:1||magnetic orderin:1||FCC IRON:1||CeRu2:1||TL2MN2O7:1||isotope effect:1||Perovskitemanganites:1||RECURSION METHOD:1||PERPENDICULAR MAGNETICANISOTROPY:1||quasiparticle spectral density:1||GW:1||MANGANESE FERRITE:1||RESONANCE:1||SeCuO3:1||Optical conductivity:1||MASSLESS DIRAC FERMIONS:1||SCHOTTKYBARRIER:1||electronic structure:15||ELECTRONICSTRUCTURE:11||TRANSITIONMETAL COMPOUNDS:10||METALS:10||photoemission:8||SPECTRA:8||MAGNETORESISTANCE:7||FERROMAGNETISM:7||TRANSPORT:7||TRANSITION:6||FILMS:6||THINFILMS:5||TOTALENERGY CALCULATIONS:5||MAGNETICPROPERTIES:5||SUPERCONDUCTIVITY:5||PR:5||LATTICE:4||STATES:4||SPECTROSCOPY:4||FIELD:4||CRYSTALSTRUCTURE:4||PHOTOEMISSION:4||TEMPERATURE:4||TRANSITIONTEMPERATURE:4||XRAYABSORPTION:4||STATE:4||CU:4||BASISSET:4||XAS:4||CRYSTALS:3||EXCITATIONS:3||MOTTHUBBARD SYSTEMS:3||HIGHENERGY SPIN:3||halfmetal:3||INSULATORS:3||LA2CUO4:3||MODEL:3||FLUCTUATIONS:3||CE:3||double exchange:3||TRANSITIONMETALS:3||RESISTIVITY:3||BORON:3||LA1XCAXMNO3:3||IRON:3||PES:3||ANTIMONIDES:2||MgB2:2||ZR METALLIC GLASSES:2||superconductor:2||CRITICALCURRENT DENSITY:2||CIRCULARDICHROISM:2||SEMICONDUCTORS:2||LOCALIZATION:2||INTRABAND OPTICAL CONDUCTIVITY:2||COLOSSAL MAGNETORESISTANCE:2||OXIDATION:2||EXISTENCE:2||COPPER:2||diboride:2||MAGNESIUMDIBORIDE:2||GAP:2||CE COMPOUNDS:2||CORE POLARIZATION:2||magnetoresistance:2||photoemission spectroscopy:2||electronphonon interaction:2||GETTER:2||PD:2||MAGNETISM:2||FECR2S4:2||SUPERCONDUCTING MGB2:2||WIRES:2||ABSORPTION:2||ENERGY:2||LA1XSRXMNO3:2||CONSTANTS:2||polaron:2||charge ordering:2||SCATTERING:2||XRAY PHOTOEMISSION:2||CeNiSn:2||phase diagram:2||PHOTOELECTRON:2||QUADRUPOLAR:2||perovskitemanganites:2||CO:2||SYSTEMS:2||DOPED ZNO:2||LOWFREQUENCY SOUND:2||LA:2||ELECTRONELECTRON SCATTERING:2||AU:2||DENSITYWAVE INSTABILITY:2||FERMISURFACE:2||hybridization:2||VALENCEBAND SATELLITE:2||SULFUR SPINEL:2||Heusler:2||APPROXIMATION:2||superexchange:2||colossal magnetoresistance:2||ALLOYS:2||DEPENDENCE:2||AG:2||electronic structures:2||AUGERSPECTRA:2||CR:2||PARAMETERS:2||DIFFRACTION:2||SEMICONDUCTORMETAL TRANSITION:1||INTERMEDIATEVALENCE:1||SMB6:1||SRRUO3:1||antiperovskite structure with antipolar nature:1||lowenergy twodimensional phonons:1||anatase TiO2:1||La3S4:1||metalinsulator transitions:1||MNO:1||ELECTRONICSTRUCTURES:1||MAGNETIC CIRCULARDICHROISM:1||Density functional theory:1||CeCo2:1||TOPOLARON CROSSOVER:1||EXCHANGE:1||cuprates:1||high Tc cuprates:1||magnetically ordered materials:1||ZNSE:1||Sr2xKxFeMoO6:1||CDW:1||TeCuO3:1||STRUCTURALPROPERTIES:1||MN:1||screening length:1||amorphous Fe:1||WAVE BASISSET:1||SILICONCARBIDE:1||HIGHPRESSURE:1||electronphonon coupling:1||quenched superconductivity:1||CMR perovskite manganites:1||OXIDE:1||polarons:1||synchrotron radiation:1||FULLERIDES:1||RESONANTPHOTOEMISSION:1||Silicon carbide:1||DFT calculation:1||Hybridized bands:1||GIANT MAGNETORESISTANCE:1||PEROVSKITES:1||Raman spectra:1||EXCHANGE ENHANCEMENT:1||SILICON:1||SR2FEMOO6:1||orbital ordering:1||delafossite:1||TITANIUMDIOXIDE:1||electronic structure of disordered solids:1||YFE2:1||Magnetic polaron:1||NA2TI2SB2O:1||STRONGCOUPLED SUPERCONDUCTORS:1||HEAVYFERMION SYSTEMS:1||firstprinciples calculations:1||MECHANISM:1||UNiSn:1||PHOTONIC BANDGAP:1||SINGLE IMPURITY:1||PHONONSPECTRUM:1||FERMISURFACE TOPOLOGY:1||SUPPRESSION:1||RESONANT PHOTOEMISSION:1||METALDOPED PICENE:1||PHOTOIONIZATION CROSSSECTIONS:1||PHOTOINDUCED FERRIMAGNETIC SYSTEMS:1||LINKAGE ISOMERISM:1||CHARGETRANSFER:1||Bilayer Graphene:1||MAGNETICFIELD:1||SPINWAVES:1||rareearth manganese oxides:1||magnonphonon interaction:1||NACO2O4:1||ENERGYBANDS:1||SELFENERGY:1||GAS:1||Fe0.5Cu0.5Cr2S4:1||scanning photoelectron microscopy (SPEM):1||MAGNETIC PROPERTIES:1||Stoner model:1||AMORPHOUS TRANSITIONMETALS:1||SPINGLASS STATES:1||NI:1||LA3NI2B2N3:1||SOLIDS:1||CEO2:1||BAND THEORY:1||dilute magnetic semiconductor:1||pyrochlore:1||Y1XPRXBA2CU3O7DELTA:1||and electronphonon interactions:1||VIBRATIONS:1||RAY PHOTOEMISSION:1||ALKALI CATION:1||Europium:1||colossal magnetoresistance:1||structural stability:1||ENERGYGAP:1||small polaron:1||DOUBLE EXCHANGE:1||Coulomb correlation:1||magnon:1||phonons:1||ELECTRON FERROMAGNETISM:1||CURIETEMPERATURE:1||ARPES:1||PLANEWAVE METHOD:1||Xray absorption spectroscopy (XAS):1||ROOMTEMPERATURE:1||MONOCHALCOGENIDES:1||HEAT:1||UPDSN:1||MOMENTS:1||XRAY ABSORPTION:1||SEMICONDUCTOR:1||Fermi surface nesting:1||optical phonon:1||disordered system:1||dilute magnetic semiconductors:1||CMR manganites:1||PHONONS:1||LATTICEDYNAMICS:1||OXIDES:1||4fphotoemission:1||permanent magnet:1||pseudogap:1||TRANSPORTPROPERTIES:1||ANTIFERROMAGNET:1||(BI,PB)SRCOO SYSTEM:1||semicore correlation:1||POLARIZATION:1||CRYSTAL:1||spinel:1||Xray magnetic circular dichroism (XMCD):1||magnetocapacitance:1||ANATASE:1||TEMPERATURES:1||Pseudogap:1||INTERFACE:1||SUBSTRATE:1||YNI2B2C:1||SAMARIUM SULFIDE:1||strong swave superconductor:1||DOPED MANGANITE:1||SYMMETRY:1||CENISN:1||resonance mode:1||DISORDERED SYSTEM:1||LITHIUM INTERCALATION:1||CUO2 PLANE:1||SURFACE:1||Delafossite:1||ELECTRICALPROPERTIES:1||NIMNSB:1||PTMNSB:1||ROOMTEMPERATURE FERROMAGNETISM:1||RUBIDIUM MANGANESE HEXACYANOFERRATE:1||COLOSSALMAGNETORESISTANCE:1||FINITE TEMPERATURES:1||LAMNO3:1||FE:1||transitionmetal oxides:1||giant magnetoresistance:1||phonon:1||COPPER OXIDES:1||valence states:1||thermoelectric:1||semiconductor:1||CATION DISTRIBUTION:1||FeCr2S4:1||photoemission spectroscopy (PES):1||METALLIC FERROMAGNETISM:1||GRAPHITE:1||SUSCEPTIBILITY:1||UBE13:1||RCrSb3:1||band JahnTeller:1||Ce3S4:1||TiO2:1||PrBa2Cu3O7delta:1||UNTWINNED PRBA2CU3O7:1||AGNIO2:1||HALFMETALLIC FERROMAGNETS:1||CI:1||Energy gap:1||Photoemission:1||Future applications:1||Photoemission measurements:1||Graphene:1||BANDSTRUCTURE:1||TC:1||superconductivity:1||magnetic semiconductors:1||CMRmanganites:1||thin films:1||spin dynamics:1||highTc superconductors:1||ITINERANTELECTRON FERROMAGNETISM:1||SINGLECRYSTALS:1||CeTe2:1||amorphous magnetic materials:1||EPITAXIAL GRAPHENE:1||LAYERED PNICTIDEOXIDES:1||BOROCARBIDE SUPERCONDUCTORS:1||AUGMENTEDWAVE METHOD:1||METALLIC MAGNET UNISN:1||ORIGIN:1||spectrum rearrangement:1||MEANFIELD THEORY:1||MOLECULEBASED MAGNETS:1||METASTABLE STATE:1||INSULATOR:1||magnetic orderin:1||FCC IRON:1||CeRu2:1||TL2MN2O7:1||isotope effect:1||Perovskitemanganites:1||RECURSION METHOD:1||PERPENDICULAR MAGNETICANISOTROPY:1||quasiparticle spectral density:1||GW:1||MANGANESE FERRITE:1||RESONANCE:1||SeCuO3:1||Optical conductivity:1||MASSLESS DIRAC FERMIONS:1||SCHOTTKYBARRIER:1||electronic structure:15||ELECTRONICSTRUCTURE:11||TRANSITIONMETAL COMPOUNDS:10||METALS:10||photoemission:8||SPECTRA:8||MAGNETORESISTANCE:7||FERROMAGNETISM:7||TRANSPORT:7||TRANSITION:6||FILMS:6||THINFILMS:5||TOTALENERGY CALCULATIONS:5||MAGNETICPROPERTIES:5||SUPERCONDUCTIVITY:5||PR:5||LATTICE:4||STATES:4||SPECTROSCOPY:4||FIELD:4||CRYSTALSTRUCTURE:4||PHOTOEMISSION:4||TEMPERATURE:4||TRANSITIONTEMPERATURE:4||XRAYABSORPTION:4||STATE:4||CU:4||BASISSET:4||XAS:4||CRYSTALS:3||EXCITATIONS:3||MOTTHUBBARD SYSTEMS:3||HIGHENERGY SPIN:3||halfmetal:3||INSULATORS:3||LA2CUO4:3||MODEL:3||FLUCTUATIONS:3||CE:3||double exchange:3||TRANSITIONMETALS:3||RESISTIVITY:3||BORON:3||LA1XCAXMNO3:3||IRON:3||PES:3||ANTIMONIDES:2||MgB2:2||ZR METALLIC GLASSES:2||superconductor:2||CRITICALCURRENT DENSITY:2||CIRCULARDICHROISM:2||SEMICONDUCTORS:2||LOCALIZATION:2||INTRABAND OPTICAL CONDUCTIVITY:2||COLOSSAL MAGNETORESISTANCE:2||OXIDATION:2||EXISTENCE:2||COPPER:2||diboride:2||MAGNESIUMDIBORIDE:2||GAP:2||CE COMPOUNDS:2||CORE POLARIZATION:2||magnetoresistance:2||photoemission spectroscopy:2||electronphonon interaction:2||GETTER:2||PD:2||MAGNETISM:2||FECR2S4:2||SUPERCONDUCTING MGB2:2||WIRES:2||ABSORPTION:2||ENERGY:2||LA1XSRXMNO3:2||CONSTANTS:2||polaron:2||charge ordering:2||SCATTERING:2||XRAY PHOTOEMISSION:2||CeNiSn:2||phase diagram:2||PHOTOELECTRON:2||QUADRUPOLAR:2||perovskitemanganites:2||CO:2||SYSTEMS:2||DOPED ZNO:2||LOWFREQUENCY SOUND:2||LA:2||ELECTRONELECTRON SCATTERING:2||AU:2||DENSITYWAVE INSTABILITY:2||FERMISURFACE:2||hybridization:2||VALENCEBAND SATELLITE:2||SULFUR SPINEL:2||Heusler:2||APPROXIMATION:2||superexchange:2||colossal magnetoresistance:2||ALLOYS:2||DEPENDENCE:2||AG:2||electronic structures:2||AUGERSPECTRA:2||CR:2||PARAMETERS:2||DIFFRACTION:2||SEMICONDUCTORMETAL TRANSITION:1||INTERMEDIATEVALENCE:1||SMB6:1||SRRUO3:1||antiperovskite structure with antipolar nature:1||lowenergy twodimensional phonons:1||anatase TiO2:1||La3S4:1||metalinsulator transitions:1||MNO:1||ELECTRONICSTRUCTURES:1||MAGNETIC CIRCULARDICHROISM:1||Density functional theory:1||CeCo2:1||TOPOLARON CROSSOVER:1||EXCHANGE:1||cuprates:1||high Tc cuprates:1||magnetically ordered materials:1||ZNSE:1||Sr2xKxFeMoO6:1||CDW:1||TeCuO3:1||STRUCTURALPROPERTIES:1||MN:1||screening length:1||amorphous Fe:1||WAVE BASISSET:1||SILICONCARBIDE:1||HIGHPRESSURE:1||electronphonon coupling:1||quenched superconductivity:1||CMR perovskite manganites:1||OXIDE:1||polarons:1||synchrotron radiation:1||FULLERIDES:1||RESONANTPHOTOEMISSION:1||Silicon carbide:1||DFT calculation:1||Hybridized bands:1||GIANT MAGNETORESISTANCE:1||PEROVSKITES:1||Raman spectra:1||EXCHANGE ENHANCEMENT:1||SILICON:1||SR2FEMOO6:1||orbital ordering:1||delafossite:1||TITANIUMDIOXIDE:1||electronic structure of disordered solids:1||YFE2:1||Magnetic polaron:1||NA2TI2SB2O:1||STRONGCOUPLED SUPERCONDUCTORS:1||HEAVYFERMION SYSTEMS:1||firstprinciples calculations:1||MECHANISM:1||UNiSn:1||PHOTONIC BANDGAP:1||SINGLE IMPURITY:1||PHONONSPECTRUM:1||FERMISURFACE TOPOLOGY:1||SUPPRESSION:1||RESONANT PHOTOEMISSION:1||METALDOPED PICENE:1||PHOTOIONIZATION CROSSSECTIONS:1||PHOTOINDUCED FERRIMAGNETIC SYSTEMS:1||LINKAGE ISOMERISM:1||CHARGETRANSFER:1||Bilayer Graphene:1||MAGNETICFIELD:1||SPINWAVES:1||rareearth manganese oxides:1||magnonphonon interaction:1||NACO2O4:1||ENERGYBANDS:1||SELFENERGY:1||GAS:1||Fe0.5Cu0.5Cr2S4:1||scanning photoelectron microscopy (SPEM):1||MAGNETIC PROPERTIES:1||Stoner model:1||AMORPHOUS TRANSITIONMETALS:1||SPINGLASS STATES:1||NI:1||LA3NI2B2N3:1||SOLIDS:1||CEO2:1||BAND THEORY:1||dilute magnetic semiconductor:1||pyrochlore:1||Y1XPRXBA2CU3O7DELTA:1||and electronphonon interactions:1||VIBRATIONS:1||RAY PHOTOEMISSION:1||ALKALI CATION:1||Europium:1||colossal magnetoresistance:1||structural stability:1||ENERGYGAP:1||small polaron:1||DOUBLE EXCHANGE:1||Coulomb correlation:1||magnon:1||phonons:1||ELECTRON FERROMAGNETISM:1||CURIETEMPERATURE:1||ARPES:1||PLANEWAVE METHOD:1||Xray absorption spectroscopy (XAS):1||ROOMTEMPERATURE:1||MONOCHALCOGENIDES:1||HEAT:1||UPDSN:1||MOMENTS:1||XRAY ABSORPTION:1||SEMICONDUCTOR:1||Fermi surface nesting:1||optical phonon:1||disordered system:1||dilute magnetic semiconductors:1||CMR manganites:1||PHONONS:1||LATTICEDYNAMICS:1||OXIDES:1||4fphotoemission:1||permanent magnet:1||pseudogap:1||TRANSPORTPROPERTIES:1||ANTIFERROMAGNET:1||(BI,PB)SRCOO SYSTEM:1||semicore correlation:1||POLARIZATION:1||CRYSTAL:1||spinel:1||Xray magnetic circular dichroism (XMCD):1||magnetocapacitance:1||ANATASE:1||TEMPERATURES:1||Pseudogap:1||INTERFACE:1||SUBSTRATE:1||YNI2B2C:1||SAMARIUM SULFIDE:1||strong swave superconductor:1||DOPED MANGANITE:1||SYMMETRY:1||CENISN:1||resonance mode:1||DISORDERED SYSTEM:1||LITHIUM INTERCALATION:1||CUO2 PLANE:1||SURFACE:1||Delafossite:1||ELECTRICALPROPERTIES:1||NIMNSB:1||PTMNSB:1||ROOMTEMPERATURE FERROMAGNETISM:1||RUBIDIUM MANGANESE HEXACYANOFERRATE:1||COLOSSALMAGNETORESISTANCE:1||FINITE TEMPERATURES:1||LAMNO3:1||FE:1||transitionmetal oxides:1||giant magnetoresistance:1||phonon:1||COPPER OXIDES:1||valence states:1||thermoelectric:1||semiconductor:1||CATION DISTRIBUTION:1||FeCr2S4:1||photoemission spectroscopy (PES):1||METALLIC FERROMAGNETISM:1||GRAPHITE:1||SUSCEPTIBILITY:1||UBE13:1||RCrSb3:1||band JahnTeller:1||Ce3S4:1||TiO2:1||PrBa2Cu3O7delta:1||UNTWINNED PRBA2CU3O7:1||AGNIO2:1||HALFMETALLIC FERROMAGNETS:1||CI:1||Energy gap:1||Photoemission:1||Future applications:1||Photoemission measurements:1||Graphene:1||BANDSTRUCTURE:1||TC:1||superconductivity:1||magnetic semiconductors:1||CMRmanganites:1||thin films:1||spin dynamics:1||highTc superconductors:1||ITINERANTELECTRON FERROMAGNETISM:1||SINGLECRYSTALS:1||CeTe2:1||amorphous magnetic materials:1||EPITAXIAL GRAPHENE:1||LAYERED PNICTIDEOXIDES:1||BOROCARBIDE SUPERCONDUCTORS:1||AUGMENTEDWAVE METHOD:1||METALLIC MAGNET UNISN:1||ORIGIN:1||spectrum rearrangement:1||MEANFIELD THEORY:1||MOLECULEBASED MAGNETS:1||METASTABLE STATE:1||INSULATOR:1||magnetic orderin:1||FCC IRON:1||CeRu2:1||TL2MN2O7:1||isotope effect:1||Perovskitemanganites:1||RECURSION METHOD:1||PERPENDICULAR MAGNETICANISOTROPY:1||quasiparticle spectral density:1||GW:1||MANGANESE FERRITE:1||RESONANCE:1||SeCuO3:1||Optical conductivity:1||MASSLESS DIRAC FERMIONS:1||SCHOTTKYBARRIER:1||electronic structure:15||ELECTRONICSTRUCTURE:11||TRANSITIONMETAL COMPOUNDS:10||METALS:10||photoemission:8||SPECTRA:8||MAGNETORESISTANCE:7||FERROMAGNETISM:7||TRANSPORT:7||TRANSITION:6||FILMS:6||THINFILMS:5||TOTALENERGY CALCULATIONS:5||MAGNETICPROPERTIES:5||SUPERCONDUCTIVITY:5||PR:5||LATTICE:4||STATES:4||SPECTROSCOPY:4||FIELD:4||CRYSTALSTRUCTURE:4||PHOTOEMISSION:4||TEMPERATURE:4||TRANSITIONTEMPERATURE:4||XRAYABSORPTION:4||STATE:4||CU:4||BASISSET:4||XAS:4||CRYSTALS:3||EXCITATIONS:3||MOTTHUBBARD SYSTEMS:3||HIGHENERGY SPIN:3||halfmetal:3||INSULATORS:3||LA2CUO4:3||MODEL:3||FLUCTUATIONS:3||CE:3||double exchange:3||TRANSITIONMETALS:3||RESISTIVITY:3||BORON:3||LA1XCAXMNO3:3||IRON:3||PES:3||ANTIMONIDES:2||MgB2:2||ZR METALLIC GLASSES:2||superconductor:2||CRITICALCURRENT DENSITY:2||CIRCULARDICHROISM:2||SEMICONDUCTORS:2||LOCALIZATION:2||INTRABAND OPTICAL CONDUCTIVITY:2||COLOSSAL MAGNETORESISTANCE:2||OXIDATION:2||EXISTENCE:2||COPPER:2||diboride:2||MAGNESIUMDIBORIDE:2||GAP:2||CE COMPOUNDS:2||CORE POLARIZATION:2||magnetoresistance:2||photoemission spectroscopy:2||electronphonon interaction:2||GETTER:2||PD:2||MAGNETISM:2||FECR2S4:2||SUPERCONDUCTING MGB2:2||WIRES:2||ABSORPTION:2||ENERGY:2||LA1XSRXMNO3:2||CONSTANTS:2||polaron:2||charge ordering:2||SCATTERING:2||XRAY PHOTOEMISSION:2||CeNiSn:2||phase diagram:2||PHOTOELECTRON:2||QUADRUPOLAR:2||perovskitemanganites:2||CO:2||SYSTEMS:2||DOPED ZNO:2||LOWFREQUENCY SOUND:2||LA:2||ELECTRONELECTRON SCATTERING:2||AU:2||DENSITYWAVE INSTABILITY:2||FERMISURFACE:2||hybridization:2||VALENCEBAND SATELLITE:2||SULFUR SPINEL:2||Heusler:2||APPROXIMATION:2||superexchange:2||colossal magnetoresistance:2||ALLOYS:2||DEPENDENCE:2||AG:2||electronic structures:2||AUGERSPECTRA:2||CR:2||PARAMETERS:2||DIFFRACTION:2||SEMICONDUCTORMETAL TRANSITION:1||INTERMEDIATEVALENCE:1||SMB6:1||SRRUO3:1||antiperovskite structure with antipolar nature:1||lowenergy twodimensional phonons:1||anatase TiO2:1||La3S4:1||metalinsulator transitions:1||MNO:1||ELECTRONICSTRUCTURES:1||MAGNETIC CIRCULARDICHROISM:1||Density functional theory:1||CeCo2:1||TOPOLARON CROSSOVER:1||EXCHANGE:1||cuprates:1||high Tc cuprates:1||magnetically ordered materials:1||ZNSE:1||Sr2xKxFeMoO6:1||CDW:1||TeCuO3:1||STRUCTURALPROPERTIES:1||MN:1||screening length:1||amorphous Fe:1||WAVE BASISSET:1||SILICONCARBIDE:1||HIGHPRESSURE:1||electronphonon coupling:1||quenched superconductivity:1||CMR perovskite manganites:1||OXIDE:1||polarons:1||synchrotron radiation:1||FULLERIDES:1||RESONANTPHOTOEMISSION:1||Silicon carbide:1||DFT calculation:1||Hybridized bands:1||GIANT MAGNETORESISTANCE:1||PEROVSKITES:1||Raman spectra:1||EXCHANGE ENHANCEMENT:1||SILICON:1||SR2FEMOO6:1||orbital ordering:1||delafossite:1||TITANIUMDIOXIDE:1||electronic structure of disordered solids:1||YFE2:1||Magnetic polaron:1||NA2TI2SB2O:1||STRONGCOUPLED SUPERCONDUCTORS:1||HEAVYFERMION SYSTEMS:1||firstprinciples calculations:1||MECHANISM:1||UNiSn:1||PHOTONIC BANDGAP:1||SINGLE IMPURITY:1||PHONONSPECTRUM:1||FERMISURFACE TOPOLOGY:1||SUPPRESSION:1||RESONANT PHOTOEMISSION:1||METALDOPED PICENE:1||PHOTOIONIZATION CROSSSECTIONS:1||PHOTOINDUCED FERRIMAGNETIC SYSTEMS:1||LINKAGE ISOMERISM:1||CHARGETRANSFER:1||Bilayer Graphene:1||MAGNETICFIELD:1||SPINWAVES:1||rareearth manganese oxides:1||magnonphonon interaction:1||NACO2O4:1||ENERGYBANDS:1||SELFENERGY:1||GAS:1||Fe0.5Cu0.5Cr2S4:1||scanning photoelectron microscopy (SPEM):1||MAGNETIC PROPERTIES:1||Stoner model:1||AMORPHOUS TRANSITIONMETALS:1||SPINGLASS STATES:1||NI:1||LA3NI2B2N3:1||SOLIDS:1||CEO2:1||BAND THEORY:1||dilute magnetic semiconductor:1||pyrochlore:1||Y1XPRXBA2CU3O7DELTA:1||and electronphonon interactions:1||VIBRATIONS:1||RAY PHOTOEMISSION:1||ALKALI CATION:1||Europium:1||colossal magnetoresistance:1||structural stability:1||ENERGYGAP:1||small polaron:1||DOUBLE EXCHANGE:1||Coulomb correlation:1||magnon:1||phonons:1||ELECTRON FERROMAGNETISM:1||CURIETEMPERATURE:1||ARPES:1||PLANEWAVE METHOD:1||Xray absorption spectroscopy (XAS):1||ROOMTEMPERATURE:1||MONOCHALCOGENIDES:1||HEAT:1||UPDSN:1||MOMENTS:1||XRAY ABSORPTION:1||SEMICONDUCTOR:1||Fermi surface nesting:1||optical phonon:1||disordered system:1||dilute magnetic semiconductors:1||CMR manganites:1||PHONONS:1||LATTICEDYNAMICS:1||OXIDES:1||4fphotoemission:1||permanent magnet:1||pseudogap:1||TRANSPORTPROPERTIES:1||ANTIFERROMAGNET:1||(BI,PB)SRCOO SYSTEM:1||semicore correlation:1||POLARIZATION:1||CRYSTAL:1||spinel:1||Xray magnetic circular dichroism (XMCD):1||magnetocapacitance:1||ANATASE:1||TEMPERATURES:1||Pseudogap:1||INTERFACE:1||SUBSTRATE:1||YNI2B2C:1||SAMARIUM SULFIDE:1||strong swave superconductor:1||DOPED MANGANITE:1||SYMMETRY:1||CENISN:1||resonance mode:1||DISORDERED SYSTEM:1||LITHIUM INTERCALATION:1||CUO2 PLANE:1||SURFACE:1||Delafossite:1||ELECTRICALPROPERTIES:1||NIMNSB:1||PTMNSB:1||ROOMTEMPERATURE FERROMAGNETISM:1||RUBIDIUM MANGANESE HEXACYANOFERRATE:1||COLOSSALMAGNETORESISTANCE:1||FINITE TEMPERATURES:1||LAMNO3:1||FE:1||transitionmetal oxides:1||giant magnetoresistance:1||phonon:1||COPPER OXIDES:1||valence states:1||thermoelectric:1||semiconductor:1||CATION DISTRIBUTION:1||FeCr2S4:1||photoemission spectroscopy (PES):1||METALLIC FERROMAGNETISM:1||GRAPHITE:1||SUSCEPTIBILITY:1||UBE13:1||RCrSb3:1||band JahnTeller:1||Ce3S4:1||TiO2:1||PrBa2Cu3O7delta:1||UNTWINNED PRBA2CU3O7:1||AGNIO2:1||HALFMETALLIC FERROMAGNETS:1||CI:1||Energy gap:1||Photoemission:1||Future applications:1||Photoemission measurements:1||Graphene:1||BANDSTRUCTURE:1||TC:1||superconductivity:1||magnetic semiconductors:1||CMRmanganites:1||thin films:1||spin dynamics:1||highTc superconductors:1||ITINERANTELECTRON FERROMAGNETISM:1||SINGLECRYSTALS:1||CeTe2:1||amorphous magnetic materials:1||EPITAXIAL GRAPHENE:1||LAYERED PNICTIDEOXIDES:1||BOROCARBIDE SUPERCONDUCTORS:1||AUGMENTEDWAVE METHOD:1||METALLIC MAGNET UNISN:1||ORIGIN:1||spectrum rearrangement:1||MEANFIELD THEORY:1||MOLECULEBASED MAGNETS:1||METASTABLE STATE:1||INSULATOR:1||magnetic orderin:1||FCC IRON:1||CeRu2:1||TL2MN2O7:1||isotope effect:1||Perovskitemanganites:1||RECURSION METHOD:1||PERPENDICULAR MAGNETICANISOTROPY:1||quasiparticle spectral density:1||GW:1||MANGANESE FERRITE:1||RESONANCE:1||SeCuO3:1||Optical conductivity:1||MASSLESS DIRAC FERMIONS:1||SCHOTTKYBARRIER:1||electronic structure:15||ELECTRONICSTRUCTURE:11||TRANSITIONMETAL COMPOUNDS:10||METALS:10||photoemission:8||SPECTRA:8||MAGNETORESISTANCE:7||FERROMAGNETISM:7||TRANSPORT:7||TRANSITION:6||FILMS:6||THINFILMS:5||TOTALENERGY CALCULATIONS:5||MAGNETICPROPERTIES:5||SUPERCONDUCTIVITY:5||PR:5||LATTICE:4||STATES:4||SPECTROSCOPY:4||FIELD:4||CRYSTALSTRUCTURE:4||PHOTOEMISSION:4||TEMPERATURE:4||TRANSITIONTEMPERATURE:4||XRAYABSORPTION:4||STATE:4||CU:4||BASISSET:4||XAS:4||CRYSTALS:3||EXCITATIONS:3||MOTTHUBBARD SYSTEMS:3||HIGHENERGY SPIN:3||halfmetal:3||INSULATORS:3||LA2CUO4:3||MODEL:3||FLUCTUATIONS:3||CE:3||double exchange:3||TRANSITIONMETALS:3||RESISTIVITY:3||BORON:3||LA1XCAXMNO3:3||IRON:3||PES:3||ANTIMONIDES:2||MgB2:2||ZR METALLIC GLASSES:2||superconductor:2||CRITICALCURRENT DENSITY:2||CIRCULARDICHROISM:2||SEMICONDUCTORS:2||LOCALIZATION:2||INTRABAND OPTICAL CONDUCTIVITY:2||COLOSSAL MAGNETORESISTANCE:2||OXIDATION:2||EXISTENCE:2||COPPER:2||diboride:2||MAGNESIUMDIBORIDE:2||GAP:2||CE COMPOUNDS:2||CORE POLARIZATION:2||magnetoresistance:2||photoemission spectroscopy:2||electronphonon interaction:2||GETTER:2||PD:2||MAGNETISM:2||FECR2S4:2||SUPERCONDUCTING MGB2:2||WIRES:2||ABSORPTION:2||ENERGY:2||LA1XSRXMNO3:2||CONSTANTS:2||polaron:2||charge ordering:2||SCATTERING:2||XRAY PHOTOEMISSION:2||CeNiSn:2||phase diagram:2||PHOTOELECTRON:2||QUADRUPOLAR:2||perovskitemanganites:2||CO:2||SYSTEMS:2||DOPED ZNO:2||LOWFREQUENCY SOUND:2||LA:2||ELECTRONELECTRON SCATTERING:2||AU:2||DENSITYWAVE INSTABILITY:2||FERMISURFACE:2||hybridization:2||VALENCEBAND SATELLITE:2||SULFUR SPINEL:2||Heusler:2||APPROXIMATION:2||superexchange:2||colossal magnetoresistance:2||ALLOYS:2||DEPENDENCE:2||AG:2||electronic structures:2||AUGERSPECTRA:2||CR:2||PARAMETERS:2||DIFFRACTION:2||SEMICONDUCTORMETAL TRANSITION:1||INTERMEDIATEVALENCE:1||SMB6:1||SRRUO3:1||antiperovskite structure with antipolar nature:1||lowenergy twodimensional phonons:1||anatase TiO2:1||La3S4:1||metalinsulator transitions:1||MNO:1||ELECTRONICSTRUCTURES:1||MAGNETIC CIRCULARDICHROISM:1||Density functional theory:1||CeCo2:1||TOPOLARON CROSSOVER:1||EXCHANGE:1||cuprates:1||high Tc cuprates:1||magnetically ordered materials:1||ZNSE:1||Sr2xKxFeMoO6:1||CDW:1||TeCuO3:1||STRUCTURALPROPERTIES:1||MN:1||screening length:1||amorphous Fe:1||WAVE BASISSET:1||SILICONCARBIDE:1||HIGHPRESSURE:1||electronphonon coupling:1||quenched superconductivity:1||CMR perovskite manganites:1||OXIDE:1||polarons:1||synchrotron radiation:1||FULLERIDES:1||RESONANTPHOTOEMISSION:1||Silicon carbide:1||DFT calculation:1||Hybridized bands:1||GIANT MAGNETORESISTANCE:1||PEROVSKITES:1||Raman spectra:1||EXCHANGE ENHANCEMENT:1||SILICON:1||SR2FEMOO6:1||orbital ordering:1||delafossite:1||TITANIUMDIOXIDE:1||electronic structure of disordered solids:1||YFE2:1||Magnetic polaron:1||NA2TI2SB2O:1||STRONGCOUPLED SUPERCONDUCTORS:1||HEAVYFERMION SYSTEMS:1||firstprinciples calculations:1||MECHANISM:1||UNiSn:1||PHOTONIC BANDGAP:1||SINGLE IMPURITY:1||PHONONSPECTRUM:1||FERMISURFACE TOPOLOGY:1||SUPPRESSION:1||RESONANT PHOTOEMISSION:1||METALDOPED PICENE:1||PHOTOIONIZATION CROSSSECTIONS:1||PHOTOINDUCED FERRIMAGNETIC SYSTEMS:1||LINKAGE ISOMERISM:1||CHARGETRANSFER:1||Bilayer Graphene:1||MAGNETICFIELD:1||SPINWAVES:1||rareearth manganese oxides:1||magnonphonon interaction:1||NACO2O4:1||ENERGYBANDS:1||SELFENERGY:1||GAS:1||Fe0.5Cu0.5Cr2S4:1||scanning photoelectron microscopy (SPEM):1||MAGNETIC PROPERTIES:1||Stoner model:1||AMORPHOUS TRANSITIONMETALS:1||SPINGLASS STATES:1||NI:1||LA3NI2B2N3:1||SOLIDS:1||CEO2:1||BAND THEORY:1||dilute magnetic semiconductor:1||pyrochlore:1||Y1XPRXBA2CU3O7DELTA:1||and electronphonon interactions:1||VIBRATIONS:1||RAY PHOTOEMISSION:1||ALKALI CATION:1||Europium:1||colossal magnetoresistance:1||structural stability:1||ENERGYGAP:1||small polaron:1||DOUBLE EXCHANGE:1||Coulomb correlation:1||magnon:1||phonons:1||ELECTRON FERROMAGNETISM:1||CURIETEMPERATURE:1||ARPES:1||PLANEWAVE METHOD:1||Xray absorption spectroscopy (XAS):1||ROOMTEMPERATURE:1||MONOCHALCOGENIDES:1||HEAT:1||UPDSN:1||MOMENTS:1||XRAY ABSORPTION:1||SEMICONDUCTOR:1||Fermi surface nesting:1||optical phonon:1||disordered system:1||dilute magnetic semiconductors:1||CMR manganites:1||PHONONS:1||LATTICEDYNAMICS:1||OXIDES:1||4fphotoemission:1||permanent magnet:1||pseudogap:1||TRANSPORTPROPERTIES:1||ANTIFERROMAGNET:1||(BI,PB)SRCOO SYSTEM:1||semicore correlation:1||POLARIZATION:1||CRYSTAL:1||spinel:1||Xray magnetic circular dichroism (XMCD):1||magnetocapacitance:1||ANATASE:1||TEMPERATURES:1||Pseudogap:1||INTERFACE:1||SUBSTRATE:1||YNI2B2C:1||SAMARIUM SULFIDE:1||strong swave superconductor:1||DOPED MANGANITE:1||SYMMETRY:1||CENISN:1||resonance mode:1||DISORDERED SYSTEM:1||LITHIUM INTERCALATION:1||CUO2 PLANE:1||SURFACE:1||Delafossite:1||ELECTRICALPROPERTIES:1||NIMNSB:1||PTMNSB:1||ROOMTEMPERATURE FERROMAGNETISM:1||RUBIDIUM MANGANESE HEXACYANOFERRATE:1||COLOSSALMAGNETORESISTANCE:1||FINITE TEMPERATURES:1||LAMNO3:1||FE:1||transitionmetal oxides:1||giant magnetoresistance:1||phonon:1||COPPER OXIDES:1||valence states:1||thermoelectric:1||semiconductor:1||CATION DISTRIBUTION:1||FeCr2S4:1||photoemission spectroscopy (PES):1||METALLIC FERROMAGNETISM:1||GRAPHITE:1||SUSCEPTIBILITY:1||UBE13:1||RCrSb3:1||band JahnTeller:1||Ce3S4:1||TiO2:1||PrBa2Cu3O7delta:1||UNTWINNED PRBA2CU3O7:1||AGNIO2:1||HALFMETALLIC FERROMAGNETS:1||CI:1||Energy gap:1||Photoemission:1||Future applications:1||Photoemission measurements:1||Graphene:1||BANDSTRUCTURE:1||TC:1||superconductivity:1||magnetic semiconductors:1||CMRmanganites:1||thin films:1||spin dynamics:1||highTc superconductors:1||ITINERANTELECTRON FERROMAGNETISM:1||SINGLECRYSTALS:1||CeTe2:1||amorphous magnetic materials:1||EPITAXIAL GRAPHENE:1||LAYERED PNICTIDEOXIDES:1||BOROCARBIDE SUPERCONDUCTORS:1||AUGMENTEDWAVE METHOD:1||METALLIC MAGNET UNISN:1||ORIGIN:1||spectrum rearrangement:1||MEANFIELD THEORY:1||MOLECULEBASED MAGNETS:1||METASTABLE STATE:1||INSULATOR:1||magnetic orderin:1||FCC IRON:1||CeRu2:1||TL2MN2O7:1||isotope effect:1||Perovskitemanganites:1||RECURSION METHOD:1||PERPENDICULAR MAGNETICANISOTROPY:1||quasiparticle spectral density:1||GW:1||MANGANESE FERRITE:1||RESONANCE:1||SeCuO3:1||Optical conductivity:1||MASSLESS DIRAC FERMIONS:1||SCHOTTKYBARRIER:1||electronic structure:15||ELECTRONICSTRUCTURE:11||TRANSITIONMETAL COMPOUNDS:10||METALS:10||photoemission:8||SPECTRA:8||MAGNETORESISTANCE:7||FERROMAGNETISM:7||TRANSPORT:7||TRANSITION:6||FILMS:6||THINFILMS:5||TOTALENERGY CALCULATIONS:5||MAGNETICPROPERTIES:5||SUPERCONDUCTIVITY:5||PR:5||LATTICE:4||STATES:4||SPECTROSCOPY:4||FIELD:4||CRYSTALSTRUCTURE:4||PHOTOEMISSION:4||TEMPERATURE:4||TRANSITIONTEMPERATURE:4||XRAYABSORPTION:4||STATE:4||CU:4||BASISSET:4||XAS:4||CRYSTALS:3||EXCITATIONS:3||MOTTHUBBARD SYSTEMS:3||HIGHENERGY SPIN:3||halfmetal:3||INSULATORS:3||LA2CUO4:3||MODEL:3||FLUCTUATIONS:3||CE:3||double exchange:3||TRANSITIONMETALS:3||RESISTIVITY:3||BORON:3||LA1XCAXMNO3:3||IRON:3||PES:3||ANTIMONIDES:2||MgB2:2||ZR METALLIC GLASSES:2||superconductor:2||CRITICALCURRENT DENSITY:2||CIRCULARDICHROISM:2||SEMICONDUCTORS:2||LOCALIZATION:2||INTRABAND OPTICAL CONDUCTIVITY:2||COLOSSAL MAGNETORESISTANCE:2||OXIDATION:2||EXISTENCE:2||COPPER:2||diboride:2||MAGNESIUMDIBORIDE:2||GAP:2||CE COMPOUNDS:2||CORE POLARIZATION:2||magnetoresistance:2||photoemission spectroscopy:2||electronphonon interaction:2||GETTER:2||PD:2||MAGNETISM:2||FECR2S4:2||SUPERCONDUCTING MGB2:2||WIRES:2||ABSORPTION:2||ENERGY:2||LA1XSRXMNO3:2||CONSTANTS:2||polaron:2||charge ordering:2||SCATTERING:2||XRAY PHOTOEMISSION:2||CeNiSn:2||phase diagram:2||PHOTOELECTRON:2||QUADRUPOLAR:2||perovskitemanganites:2||CO:2||SYSTEMS:2||DOPED ZNO:2||LOWFREQUENCY SOUND:2||LA:2||ELECTRONELECTRON SCATTERING:2||AU:2||DENSITYWAVE INSTABILITY:2||FERMISURFACE:2||hybridization:2||VALENCEBAND SATELLITE:2||SULFUR SPINEL:2||Heusler:2||APPROXIMATION:2||superexchange:2||colossal magnetoresistance:2||ALLOYS:2||DEPENDENCE:2||AG:2||electronic structures:2||AUGERSPECTRA:2||CR:2||PARAMETERS:2||DIFFRACTION:2||SEMICONDUCTORMETAL TRANSITION:1||INTERMEDIATEVALENCE:1||SMB6:1||SRRUO3:1||antiperovskite structure with antipolar nature:1||lowenergy twodimensional phonons:1||anatase TiO2:1||La3S4:1||metalinsulator transitions:1||MNO:1||ELECTRONICSTRUCTURES:1||MAGNETIC CIRCULARDICHROISM:1||Density functional theory:1||CeCo2:1||TOPOLARON CROSSOVER:1||EXCHANGE:1||cuprates:1||high Tc cuprates:1||magnetically ordered materials:1||ZNSE:1||Sr2xKxFeMoO6:1||CDW:1||TeCuO3:1||STRUCTURALPROPERTIES:1||MN:1||screening length:1||amorphous Fe:1||WAVE BASISSET:1||SILICONCARBIDE:1||HIGHPRESSURE:1||electronphonon coupling:1||quenched superconductivity:1||CMR perovskite manganites:1||OXIDE:1||polarons:1||synchrotron radiation:1||FULLERIDES:1||RESONANTPHOTOEMISSION:1||Silicon carbide:1||DFT calculation:1||Hybridized bands:1||GIANT MAGNETORESISTANCE:1||PEROVSKITES:1||Raman spectra:1||EXCHANGE ENHANCEMENT:1||SILICON:1||SR2FEMOO6:1||orbital ordering:1||delafossite:1||TITANIUMDIOXIDE:1||electronic structure of disordered solids:1||YFE2:1||Magnetic polaron:1||NA2TI2SB2O:1||STRONGCOUPLED SUPERCONDUCTORS:1||HEAVYFERMION SYSTEMS:1||firstprinciples calculations:1||MECHANISM:1||UNiSn:1||PHOTONIC BANDGAP:1||SINGLE IMPURITY:1||PHONONSPECTRUM:1||FERMISURFACE TOPOLOGY:1||SUPPRESSION:1||RESONANT PHOTOEMISSION:1||METALDOPED PICENE:1||PHOTOIONIZATION CROSSSECTIONS:1||PHOTOINDUCED FERRIMAGNETIC SYSTEMS:1||LINKAGE ISOMERISM:1||CHARGETRANSFER:1||Bilayer Graphene:1||MAGNETICFIELD:1||SPINWAVES:1||rareearth manganese oxides:1||magnonphonon interaction:1||NACO2O4:1||ENERGYBANDS:1||SELFENERGY:1||GAS:1||Fe0.5Cu0.5Cr2S4:1||scanning photoelectron microscopy (SPEM):1||MAGNETIC PROPERTIES:1||Stoner model:1||AMORPHOUS TRANSITIONMETALS:1||SPINGLASS STATES:1||NI:1||LA3NI2B2N3:1||SOLIDS:1||CEO2:1||BAND THEORY:1||dilute magnetic semiconductor:1||pyrochlore:1||Y1XPRXBA2CU3O7DELTA:1||and electronphonon interactions:1||VIBRATIONS:1||RAY PHOTOEMISSION:1||ALKALI CATION:1||Europium:1||colossal magnetoresistance:1||structural stability:1||ENERGYGAP:1||small polaron:1||DOUBLE EXCHANGE:1||Coulomb correlation:1||magnon:1||phonons:1||ELECTRON FERROMAGNETISM:1||CURIETEMPERATURE:1||ARPES:1||PLANEWAVE METHOD:1||Xray absorption spectroscopy (XAS):1||ROOMTEMPERATURE:1||MONOCHALCOGENIDES:1||HEAT:1||UPDSN:1||MOMENTS:1||XRAY ABSORPTION:1||SEMICONDUCTOR:1||Fermi surface nesting:1||optical phonon:1||disordered system:1||dilute magnetic semiconductors:1||CMR manganites:1||PHONONS:1||LATTICEDYNAMICS:1||OXIDES:1||4fphotoemission:1||permanent magnet:1||pseudogap:1||TRANSPORTPROPERTIES:1||ANTIFERROMAGNET:1||(BI,PB)SRCOO SYSTEM:1||semicore correlation:1||POLARIZATION:1||CRYSTAL:1||spinel:1||Xray magnetic circular dichroism (XMCD):1||magnetocapacitance:1||ANATASE:1||TEMPERATURES:1||Pseudogap:1||INTERFACE:1||SUBSTRATE:1||YNI2B2C:1||SAMARIUM SULFIDE:1||strong swave superconductor:1||DOPED MANGANITE:1||SYMMETRY:1||CENISN:1||resonance mode:1||DISORDERED SYSTEM:1||LITHIUM INTERCALATION:1||CUO2 PLANE:1||SURFACE:1||Delafossite:1||ELECTRICALPROPERTIES:1||NIMNSB:1||PTMNSB:1||ROOMTEMPERATURE FERROMAGNETISM:1||RUBIDIUM MANGANESE HEXACYANOFERRATE:1||COLOSSALMAGNETORESISTANCE:1||FINITE TEMPERATURES:1||LAMNO3:1||FE:1||transitionmetal oxides:1||giant magnetoresistance:1||phonon:1||COPPER OXIDES:1||valence states:1||thermoelectric:1||semiconductor:1||CATION DISTRIBUTION:1||FeCr2S4:1||photoemission spectroscopy (PES):1||METALLIC FERROMAGNETISM:1||GRAPHITE:1||SUSCEPTIBILITY:1||UBE13:1||RCrSb3:1||band JahnTeller:1||Ce3S4:1||TiO2:1||PrBa2Cu3O7delta:1||UNTWINNED PRBA2CU3O7:1||AGNIO2:1||HALFMETALLIC FERROMAGNETS:1||CI:1||Energy gap:1||Photoemission:1||Future applications:1||Photoemission measurements:1||Graphene:1||BANDSTRUCTURE:1||TC:1||superconductivity:1||magnetic semiconductors:1||CMRmanganites:1||thin films:1||spin dynamics:1||highTc superconductors:1||ITINERANTELECTRON FERROMAGNETISM:1||SINGLECRYSTALS:1||CeTe2:1||amorphous magnetic materials:1||EPITAXIAL GRAPHENE:1||LAYERED PNICTIDEOXIDES:1||BOROCARBIDE SUPERCONDUCTORS:1||AUGMENTEDWAVE METHOD:1||METALLIC MAGNET UNISN:1||ORIGIN:1||spectrum rearrangement:1||MEANFIELD THEORY:1||MOLECULEBASED MAGNETS:1||METASTABLE STATE:1||INSULATOR:1||magnetic orderin:1||FCC IRON:1||CeRu2:1||TL2MN2O7:1||isotope effect:1||Perovskitemanganites:1||RECURSION METHOD:1||PERPENDICULAR MAGNETICANISOTROPY:1||quasiparticle spectral density:1||GW:1||MANGANESE FERRITE:1||RESONANCE:1||SeCuO3:1||Optical conductivity:1||MASSLESS DIRAC FERMIONS:1||SCHOTTKYBARRIER:1||electronic structure:15||ELECTRONICSTRUCTURE:11||TRANSITIONMETAL COMPOUNDS:10||METALS:10||photoemission:8||SPECTRA:8||MAGNETORESISTANCE:7||FERROMAGNETISM:7||TRANSPORT:7||TRANSITION:6||FILMS:6||THINFILMS:5||TOTALENERGY CALCULATIONS:5||MAGNETICPROPERTIES:5||SUPERCONDUCTIVITY:5||PR:5||LATTICE:4||STATES:4||SPECTROSCOPY:4||FIELD:4||CRYSTALSTRUCTURE:4||PHOTOEMISSION:4||TEMPERATURE:4||TRANSITIONTEMPERATURE:4||XRAYABSORPTION:4||STATE:4||CU:4||BASISSET:4||XAS:4||CRYSTALS:3||EXCITATIONS:3||MOTTHUBBARD SYSTEMS:3||HIGHENERGY SPIN:3||halfmetal:3||INSULATORS:3||LA2CUO4:3||MODEL:3||FLUCTUATIONS:3||CE:3||double exchange:3||TRANSITIONMETALS:3||RESISTIVITY:3||BORON:3||LA1XCAXMNO3:3||IRON:3||PES:3||ANTIMONIDES:2||MgB2:2||ZR METALLIC GLASSES:2||superconductor:2||CRITICALCURRENT DENSITY:2||CIRCULARDICHROISM:2||SEMICONDUCTORS:2||LOCALIZATION:2||INTRABAND OPTICAL CONDUCTIVITY:2||COLOSSAL MAGNETORESISTANCE:2||OXIDATION:2||EXISTENCE:2||COPPER:2||diboride:2||MAGNESIUMDIBORIDE:2||GAP:2||CE COMPOUNDS:2||CORE POLARIZATION:2||magnetoresistance:2||photoemission spectroscopy:2||electronphonon interaction:2||GETTER:2||PD:2||MAGNETISM:2||FECR2S4:2||SUPERCONDUCTING MGB2:2||WIRES:2||ABSORPTION:2||ENERGY:2||LA1XSRXMNO3:2||CONSTANTS:2||polaron:2||charge ordering:2||SCATTERING:2||XRAY PHOTOEMISSION:2||CeNiSn:2||phase diagram:2||PHOTOELECTRON:2||QUADRUPOLAR:2||perovskitemanganites:2||CO:2||SYSTEMS:2||DOPED ZNO:2||LOWFREQUENCY SOUND:2||LA:2||ELECTRONELECTRON SCATTERING:2||AU:2||DENSITYWAVE INSTABILITY:2||FERMISURFACE:2||hybridization:2||VALENCEBAND SATELLITE:2||SULFUR SPINEL:2||Heusler:2||APPROXIMATION:2||superexchange:2||colossal magnetoresistance:2||ALLOYS:2||DEPENDENCE:2||AG:2||electronic structures:2||AUGERSPECTRA:2||CR:2||PARAMETERS:2||DIFFRACTION:2||SEMICONDUCTORMETAL TRANSITION:1||INTERMEDIATEVALENCE:1||SMB6:1||SRRUO3:1||antiperovskite structure with antipolar nature:1||lowenergy twodimensional phonons:1||anatase TiO2:1||La3S4:1||metalinsulator transitions:1||MNO:1||ELECTRONICSTRUCTURES:1||MAGNETIC CIRCULARDICHROISM:1||Density functional theory:1||CeCo2:1||TOPOLARON CROSSOVER:1||EXCHANGE:1||cuprates:1||high Tc cuprates:1||magnetically ordered materials:1||ZNSE:1||Sr2xKxFeMoO6:1||CDW:1||TeCuO3:1||STRUCTURALPROPERTIES:1||MN:1||screening length:1||amorphous Fe:1||WAVE BASISSET:1||SILICONCARBIDE:1||HIGHPRESSURE:1||electronphonon coupling:1||quenched superconductivity:1||CMR perovskite manganites:1||OXIDE:1||polarons:1||synchrotron radiation:1||FULLERIDES:1||RESONANTPHOTOEMISSION:1||Silicon carbide:1||DFT calculation:1||Hybridized bands:1||GIANT MAGNETORESISTANCE:1||PEROVSKITES:1||Raman spectra:1||EXCHANGE ENHANCEMENT:1||SILICON:1||SR2FEMOO6:1||orbital ordering:1||delafossite:1||TITANIUMDIOXIDE:1||electronic structure of disordered solids:1||YFE2:1||Magnetic polaron:1||NA2TI2SB2O:1||STRONGCOUPLED SUPERCONDUCTORS:1||HEAVYFERMION SYSTEMS:1||firstprinciples calculations:1||MECHANISM:1||UNiSn:1||PHOTONIC BANDGAP:1||SINGLE IMPURITY:1||PHONONSPECTRUM:1||FERMISURFACE TOPOLOGY:1||SUPPRESSION:1||RESONANT PHOTOEMISSION:1||METALDOPED PICENE:1||PHOTOIONIZATION CROSSSECTIONS:1||PHOTOINDUCED FERRIMAGNETIC SYSTEMS:1||LINKAGE ISOMERISM:1||CHARGETRANSFER:1||Bilayer Graphene:1||MAGNETICFIELD:1||SPINWAVES:1||rareearth manganese oxides:1||magnonphonon interaction:1||NACO2O4:1||ENERGYBANDS:1||SELFENERGY:1||GAS:1||Fe0.5Cu0.5Cr2S4:1||scanning photoelectron microscopy (SPEM):1||MAGNETIC PROPERTIES:1||Stoner model:1||AMORPHOUS TRANSITIONMETALS:1||SPINGLASS STATES:1||NI:1||LA3NI2B2N3:1||SOLIDS:1||CEO2:1||BAND THEORY:1||dilute magnetic semiconductor:1||pyrochlore:1||Y1XPRXBA2CU3O7DELTA:1||and electronphonon interactions:1||VIBRATIONS:1||RAY PHOTOEMISSION:1||ALKALI CATION:1||Europium:1||colossal magnetoresistance:1||structural stability:1||ENERGYGAP:1||small polaron:1||DOUBLE EXCHANGE:1||Coulomb correlation:1||magnon:1||phonons:1||ELECTRON FERROMAGNETISM:1||CURIETEMPERATURE:1||ARPES:1||PLANEWAVE METHOD:1||Xray absorption spectroscopy (XAS):1||ROOMTEMPERATURE:1||MONOCHALCOGENIDES:1||HEAT:1||UPDSN:1||MOMENTS:1||XRAY ABSORPTION:1||SEMICONDUCTOR:1||Fermi surface nesting:1||optical phonon:1||disordered system:1||dilute magnetic semiconductors:1||CMR manganites:1||PHONONS:1||LATTICEDYNAMICS:1||OXIDES:1||4fphotoemission:1||permanent magnet:1||pseudogap:1||TRANSPORTPROPERTIES:1||ANTIFERROMAGNET:1||(BI,PB)SRCOO SYSTEM:1||semicore correlation:1||POLARIZATION:1||CRYSTAL:1||spinel:1||Xray magnetic circular dichroism (XMCD):1||magnetocapacitance:1||ANATASE:1||TEMPERATURES:1||Pseudogap:1||INTERFACE:1||SUBSTRATE:1||YNI2B2C:1||SAMARIUM SULFIDE:1||strong swave superconductor:1||DOPED MANGANITE:1||SYMMETRY:1||CENISN:1||resonance mode:1||DISORDERED SYSTEM:1||LITHIUM INTERCALATION:1||CUO2 PLANE:1||SURFACE:1||Delafossite:1||ELECTRICALPROPERTIES:1||NIMNSB:1||PTMNSB:1||ROOMTEMPERATURE FERROMAGNETISM:1||RUBIDIUM MANGANESE HEXACYANOFERRATE:1||COLOSSALMAGNETORESISTANCE:1||FINITE TEMPERATURES:1||LAMNO3:1||FE:1||transitionmetal oxides:1||giant magnetoresistance:1||phonon:1||COPPER OXIDES:1||valence states:1||thermoelectric:1||semiconductor:1||CATION DISTRIBUTION:1||FeCr2S4:1||photoemission spectroscopy (PES):1||METALLIC FERROMAGNETISM:1||GRAPHITE:1||SUSCEPTIBILITY:1||UBE13:1||RCrSb3:1||band JahnTeller:1||Ce3S4:1||TiO2:1||PrBa2Cu3O7delta:1||UNTWINNED PRBA2CU3O7:1||AGNIO2:1||HALFMETALLIC FERROMAGNETS:1||CI:1||Energy gap:1||Photoemission:1||Future applications:1||Photoemission measurements:1||Graphene:1||BANDSTRUCTURE:1||TC:1||superconductivity:1||magnetic semiconductors:1||CMRmanganites:1||thin films:1||spin dynamics:1||highTc superconductors:1||ITINERANTELECTRON FERROMAGNETISM:1||SINGLECRYSTALS:1||CeTe2:1||amorphous magnetic materials:1||EPITAXIAL GRAPHENE:1||LAYERED PNICTIDEOXIDES:1||BOROCARBIDE SUPERCONDUCTORS:1||AUGMENTEDWAVE METHOD:1||METALLIC MAGNET UNISN:1||ORIGIN:1||spectrum rearrangement:1||MEANFIELD THEORY:1||MOLECULEBASED MAGNETS:1||METASTABLE STATE:1||INSULATOR:1||magnetic orderin:1||FCC IRON:1||CeRu2:1||TL2MN2O7:1||isotope effect:1||Perovskitemanganites:1||RECURSION METHOD:1||PERPENDICULAR MAGNETICANISOTROPY:1||quasiparticle spectral density:1||GW:1||MANGANESE FERRITE:1||RESONANCE:1||SeCuO3:1||Optical conductivity:1||MASSLESS DIRAC FERMIONS:1||SCHOTTKYBARRIER:1||electronic structure:15||ELECTRONICSTRUCTURE:11||TRANSITIONMETAL COMPOUNDS:10||METALS:10||photoemission:8||SPECTRA:8||MAGNETORESISTANCE:7||FERROMAGNETISM:7||TRANSPORT:7||TRANSITION:6||FILMS:6||THINFILMS:5||TOTALENERGY CALCULATIONS:5||MAGNETICPROPERTIES:5||SUPERCONDUCTIVITY:5||PR:5||LATTICE:4||STATES:4||SPECTROSCOPY:4||FIELD:4||CRYSTALSTRUCTURE:4||PHOTOEMISSION:4||TEMPERATURE:4||TRANSITIONTEMPERATURE:4||XRAYABSORPTION:4||STATE:4||CU:4||BASISSET:4||XAS:4||CRYSTALS:3||EXCITATIONS:3||MOTTHUBBARD SYSTEMS:3||HIGHENERGY SPIN:3||halfmetal:3||INSULATORS:3||LA2CUO4:3||MODEL:3||FLUCTUATIONS:3||CE:3||double exchange:3||TRANSITIONMETALS:3||RESISTIVITY:3||BORON:3||LA1XCAXMNO3:3||IRON:3||PES:3||ANTIMONIDES:2||MgB2:2||ZR METALLIC GLASSES:2||superconductor:2||CRITICALCURRENT DENSITY:2||CIRCULARDICHROISM:2||SEMICONDUCTORS:2||LOCALIZATION:2||INTRABAND OPTICAL CONDUCTIVITY:2||COLOSSAL MAGNETORESISTANCE:2||OXIDATION:2||EXISTENCE:2||COPPER:2||diboride:2||MAGNESIUMDIBORIDE:2||GAP:2||CE COMPOUNDS:2||CORE POLARIZATION:2||magnetoresistance:2||photoemission spectroscopy:2||electronphonon interaction:2||GETTER:2||PD:2||MAGNETISM:2||FECR2S4:2||SUPERCONDUCTING MGB2:2||WIRES:2||ABSORPTION:2||ENERGY:2||LA1XSRXMNO3:2||CONSTANTS:2||polaron:2||charge ordering:2||SCATTERING:2||XRAY PHOTOEMISSION:2||CeNiSn:2||phase diagram:2||PHOTOELECTRON:2||QUADRUPOLAR:2||perovskitemanganites:2||CO:2||SYSTEMS:2||DOPED ZNO:2||LOWFREQUENCY SOUND:2||LA:2||ELECTRONELECTRON SCATTERING:2||AU:2||DENSITYWAVE INSTABILITY:2||FERMISURFACE:2||hybridization:2||VALENCEBAND SATELLITE:2||SULFUR SPINEL:2||Heusler:2||APPROXIMATION:2||superexchange:2||colossal magnetoresistance:2||ALLOYS:2||DEPENDENCE:2||AG:2||electronic structures:2||AUGERSPECTRA:2||CR:2||PARAMETERS:2||DIFFRACTION:2||SEMICONDUCTORMETAL TRANSITION:1||INTERMEDIATEVALENCE:1||SMB6:1||SRRUO3:1||antiperovskite structure with antipolar nature:1||lowenergy twodimensional phonons:1||anatase TiO2:1||La3S4:1||metalinsulator transitions:1||MNO:1||ELECTRONICSTRUCTURES:1||MAGNETIC CIRCULARDICHROISM:1||Density functional theory:1||CeCo2:1||TOPOLARON CROSSOVER:1||EXCHANGE:1||cuprates:1||high Tc cuprates:1||magnetically ordered materials:1||ZNSE:1||Sr2xKxFeMoO6:1||CDW:1||TeCuO3:1||STRUCTURALPROPERTIES:1||MN:1||screening length:1||amorphous Fe:1||WAVE BASISSET:1||SILICONCARBIDE:1||HIGHPRESSURE:1||electronphonon coupling:1||quenched superconductivity:1||CMR perovskite manganites:1||OXIDE:1||polarons:1||synchrotron radiation:1||FULLERIDES:1||RESONANTPHOTOEMISSION:1||Silicon carbide:1||DFT calculation:1||Hybridized bands:1||GIANT MAGNETORESISTANCE:1||PEROVSKITES:1||Raman spectra:1||EXCHANGE ENHANCEMENT:1||SILICON:1||SR2FEMOO6:1||orbital ordering:1||delafossite:1||TITANIUMDIOXIDE:1||electronic structure of disordered solids:1||YFE2:1||Magnetic polaron:1||NA2TI2SB2O:1||STRONGCOUPLED SUPERCONDUCTORS:1||HEAVYFERMION SYSTEMS:1||firstprinciples calculations:1||MECHANISM:1||UNiSn:1||PHOTONIC BANDGAP:1||SINGLE IMPURITY:1||PHONONSPECTRUM:1||FERMISURFACE TOPOLOGY:1||SUPPRESSION:1||RESONANT PHOTOEMISSION:1||METALDOPED PICENE:1||PHOTOIONIZATION CROSSSECTIONS:1||PHOTOINDUCED FERRIMAGNETIC SYSTEMS:1||LINKAGE ISOMERISM:1||CHARGETRANSFER:1||Bilayer Graphene:1||MAGNETICFIELD:1||SPINWAVES:1||rareearth manganese oxides:1||magnonphonon interaction:1||NACO2O4:1||ENERGYBANDS:1||SELFENERGY:1||GAS:1||Fe0.5Cu0.5Cr2S4:1||scanning photoelectron microscopy (SPEM):1||MAGNETIC PROPERTIES:1||Stoner model:1||AMORPHOUS TRANSITIONMETALS:1||SPINGLASS STATES:1||NI:1||LA3NI2B2N3:1||SOLIDS:1||CEO2:1||BAND THEORY:1||dilute magnetic semiconductor:1||pyrochlore:1||Y1XPRXBA2CU3O7DELTA:1||and electronphonon interactions:1||VIBRATIONS:1||RAY PHOTOEMISSION:1||ALKALI CATION:1||Europium:1||colossal magnetoresistance:1||structural stability:1||ENERGYGAP:1||small polaron:1||DOUBLE EXCHANGE:1||Coulomb correlation:1||magnon:1||phonons:1||ELECTRON FERROMAGNETISM:1||CURIETEMPERATURE:1||ARPES:1||PLANEWAVE METHOD:1||Xray absorption spectroscopy (XAS):1||ROOMTEMPERATURE:1||MONOCHALCOGENIDES:1||HEAT:1||UPDSN:1||MOMENTS:1||XRAY ABSORPTION:1||SEMICONDUCTOR:1||Fermi surface nesting:1||optical phonon:1||disordered system:1||dilute magnetic semiconductors:1||CMR manganites:1||PHONONS:1||LATTICEDYNAMICS:1||OXIDES:1||4fphotoemission:1||permanent magnet:1||pseudogap:1||TRANSPORTPROPERTIES:1||ANTIFERROMAGNET:1||(BI,PB)SRCOO SYSTEM:1||semicore correlation:1||POLARIZATION:1||CRYSTAL:1||spinel:1||Xray magnetic circular dichroism (XMCD):1||magnetocapacitance:1||ANATASE:1||TEMPERATURES:1||Pseudogap:1||INTERFACE:1||SUBSTRATE:1||YNI2B2C:1||SAMARIUM SULFIDE:1||strong swave superconductor:1||DOPED MANGANITE:1||SYMMETRY:1||CENISN:1||resonance mode:1||DISORDERED SYSTEM:1||LITHIUM INTERCALATION:1||CUO2 PLANE:1||SURFACE:1||Delafossite:1||ELECTRICALPROPERTIES:1||NIMNSB:1||PTMNSB:1||ROOMTEMPERATURE FERROMAGNETISM:1||RUBIDIUM MANGANESE HEXACYANOFERRATE:1||COLOSSALMAGNETORESISTANCE:1||FINITE TEMPERATURES:1||LAMNO3:1||FE:1||transitionmetal oxides:1||giant magnetoresistance:1||phonon:1||COPPER OXIDES:1||valence states:1||thermoelectric:1||semiconductor:1||CATION DISTRIBUTION:1||FeCr2S4:1||photoemission spectroscopy (PES):1||METALLIC FERROMAGNETISM:1||GRAPHITE:1||SUSCEPTIBILITY:1||UBE13:1||RCrSb3:1||band JahnTeller:1||Ce3S4:1||TiO2:1||PrBa2Cu3O7delta:1||UNTWINNED PRBA2CU3O7:1||AGNIO2:1||HALFMETALLIC FERROMAGNETS:1||CI:1||Energy gap:1||Photoemission:1||Future applications:1||Photoemission measurements:1||Graphene:1||BANDSTRUCTURE:1||TC:1||superconductivity:1||magnetic semiconductors:1||CMRmanganites:1||thin films:1||spin dynamics:1||highTc superconductors:1||ITINERANTELECTRON FERROMAGNETISM:1||SINGLECRYSTALS:1||CeTe2:1||amorphous magnetic materials:1||EPITAXIAL GRAPHENE:1||LAYERED PNICTIDEOXIDES:1||BOROCARBIDE SUPERCONDUCTORS:1||AUGMENTEDWAVE METHOD:1||METALLIC MAGNET UNISN:1||ORIGIN:1||spectrum rearrangement:1||MEANFIELD THEORY:1||MOLECULEBASED MAGNETS:1||METASTABLE STATE:1||INSULATOR:1||magnetic orderin:1||FCC IRON:1||CeRu2:1||TL2MN2O7:1||isotope effect:1||Perovskitemanganites:1||RECURSION METHOD:1||PERPENDICULAR MAGNETICANISOTROPY:1||quasiparticle spectral density:1||GW:1||MANGANESE FERRITE:1||RESONANCE:1||SeCuO3:1||Optical conductivity:1||MASSLESS DIRAC FERMIONS:1||SCHOTTKYBARRIER:1||electronic structure:15||ELECTRONICSTRUCTURE:11||TRANSITIONMETAL COMPOUNDS:10||METALS:10||photoemission:8||SPECTRA:8||MAGNETORESISTANCE:7||FERROMAGNETISM:7||TRANSPORT:7||TRANSITION:6||FILMS:6||THINFILMS:5||TOTALENERGY CALCULATIONS:5||MAGNETICPROPERTIES:5||SUPERCONDUCTIVITY:5||PR:5||LATTICE:4||STATES:4||SPECTROSCOPY:4||FIELD:4||CRYSTALSTRUCTURE:4||PHOTOEMISSION:4||TEMPERATURE:4||TRANSITIONTEMPERATURE:4||XRAYABSORPTION:4||STATE:4||CU:4||BASISSET:4||XAS:4||CRYSTALS:3||EXCITATIONS:3||MOTTHUBBARD SYSTEMS:3||HIGHENERGY SPIN:3||halfmetal:3||INSULATORS:3||LA2CUO4:3||MODEL:3||FLUCTUATIONS:3||CE:3||double exchange:3||TRANSITIONMETALS:3||RESISTIVITY:3||BORON:3||LA1XCAXMNO3:3||IRON:3||PES:3||ANTIMONIDES:2||MgB2:2||ZR METALLIC GLASSES:2||superconductor:2||CRITICALCURRENT DENSITY:2||CIRCULARDICHROISM:2||SEMICONDUCTORS:2||LOCALIZATION:2||INTRABAND OPTICAL CONDUCTIVITY:2||COLOSSAL MAGNETORESISTANCE:2||OXIDATION:2||EXISTENCE:2||COPPER:2||diboride:2||MAGNESIUMDIBORIDE:2||GAP:2||CE COMPOUNDS:2||CORE POLARIZATION:2||magnetoresistance:2||photoemission spectroscopy:2||electronphonon interaction:2||GETTER:2||PD:2||MAGNETISM:2||FECR2S4:2||SUPERCONDUCTING MGB2:2||WIRES:2||ABSORPTION:2||ENERGY:2||LA1XSRXMNO3:2||CONSTANTS:2||polaron:2||charge ordering:2||SCATTERING:2||XRAY PHOTOEMISSION:2||CeNiSn:2||phase diagram:2||PHOTOELECTRON:2||QUADRUPOLAR:2||perovskitemanganites:2||CO:2||SYSTEMS:2||DOPED ZNO:2||LOWFREQUENCY SOUND:2||LA:2||ELECTRONELECTRON SCATTERING:2||AU:2||DENSITYWAVE INSTABILITY:2||FERMISURFACE:2||hybridization:2||VALENCEBAND SATELLITE:2||SULFUR SPINEL:2||Heusler:2||APPROXIMATION:2||superexchange:2||colossal magnetoresistance:2||ALLOYS:2||DEPENDENCE:2||AG:2||electronic structures:2||AUGERSPECTRA:2||CR:2||PARAMETERS:2||DIFFRACTION:2||SEMICONDUCTORMETAL TRANSITION:1||INTERMEDIATEVALENCE:1||SMB6:1||SRRUO3:1||antiperovskite structure with antipolar nature:1||lowenergy twodimensional phonons:1||anatase TiO2:1||La3S4:1||metalinsulator transitions:1||MNO:1||ELECTRONICSTRUCTURES:1||MAGNETIC CIRCULARDICHROISM:1||Density functional theory:1||CeCo2:1||TOPOLARON CROSSOVER:1||EXCHANGE:1||cuprates:1||high Tc cuprates:1||magnetically ordered materials:1||ZNSE:1||Sr2xKxFeMoO6:1||CDW:1||TeCuO3:1||STRUCTURALPROPERTIES:1||MN:1||screening length:1||amorphous Fe:1||WAVE BASISSET:1||SILICONCARBIDE:1||HIGHPRESSURE:1||electronphonon coupling:1||quenched superconductivity:1||CMR perovskite manganites:1||OXIDE:1||polarons:1||synchrotron radiation:1||FULLERIDES:1||RESONANTPHOTOEMISSION:1||Silicon carbide:1||DFT calculation:1||Hybridized bands:1||GIANT MAGNETORESISTANCE:1||PEROVSKITES:1||Raman spectra:1||EXCHANGE ENHANCEMENT:1||SILICON:1||SR2FEMOO6:1||orbital ordering:1||delafossite:1||TITANIUMDIOXIDE:1||electronic structure of disordered solids:1||YFE2:1||Magnetic polaron:1||NA2TI2SB2O:1||STRONGCOUPLED SUPERCONDUCTORS:1||HEAVYFERMION SYSTEMS:1||firstprinciples calculations:1||MECHANISM:1||UNiSn:1||PHOTONIC BANDGAP:1||SINGLE IMPURITY:1||PHONONSPECTRUM:1||FERMISURFACE TOPOLOGY:1||SUPPRESSION:1||RESONANT PHOTOEMISSION:1||METALDOPED PICENE:1||PHOTOIONIZATION CROSSSECTIONS:1||PHOTOINDUCED FERRIMAGNETIC SYSTEMS:1||LINKAGE ISOMERISM:1||CHARGETRANSFER:1||Bilayer Graphene:1||MAGNETICFIELD:1||SPINWAVES:1||rareearth manganese oxides:1||magnonphonon interaction:1||NACO2O4:1||ENERGYBANDS:1||SELFENERGY:1||GAS:1||Fe0.5Cu0.5Cr2S4:1||scanning photoelectron microscopy (SPEM):1||MAGNETIC PROPERTIES:1||Stoner model:1||AMORPHOUS TRANSITIONMETALS:1||SPINGLASS STATES:1||NI:1||LA3NI2B2N3:1||SOLIDS:1||CEO2:1||BAND THEORY:1||dilute magnetic semiconductor:1||pyrochlore:1||Y1XPRXBA2CU3O7DELTA:1||and electronphonon interactions:1||VIBRATIONS:1||RAY PHOTOEMISSION:1||ALKALI CATION:1||Europium:1||colossal magnetoresistance:1||structural stability:1||ENERGYGAP:1||small polaron:1||DOUBLE EXCHANGE:1||Coulomb correlation:1||magnon:1||phonons:1||ELECTRON FERROMAGNETISM:1||CURIETEMPERATURE:1||ARPES:1||PLANEWAVE METHOD:1||Xray absorption spectroscopy (XAS):1||ROOMTEMPERATURE:1||MONOCHALCOGENIDES:1||HEAT:1||UPDSN:1||MOMENTS:1||XRAY ABSORPTION:1||SEMICONDUCTOR:1||Fermi surface nesting:1||optical phonon:1||disordered system:1||dilute magnetic semiconductors:1||CMR manganites:1||PHONONS:1||LATTICEDYNAMICS:1||OXIDES:1||4fphotoemission:1||permanent magnet:1||pseudogap:1||TRANSPORTPROPERTIES:1||ANTIFERROMAGNET:1||(BI,PB)SRCOO SYSTEM:1||semicore correlation:1||POLARIZATION:1||CRYSTAL:1||spinel:1||Xray magnetic circular dichroism (XMCD):1||magnetocapacitance:1||ANATASE:1||TEMPERATURES:1||Pseudogap:1||INTERFACE:1||SUBSTRATE:1||YNI2B2C:1||SAMARIUM SULFIDE:1||strong swave superconductor:1||DOPED MANGANITE:1||SYMMETRY:1||CENISN:1||resonance mode:1||DISORDERED SYSTEM:1||LITHIUM INTERCALATION:1||CUO2 PLANE:1||SURFACE:1||Delafossite:1||ELECTRICALPROPERTIES:1||NIMNSB:1||PTMNSB:1||ROOMTEMPERATURE FERROMAGNETISM:1||RUBIDIUM MANGANESE HEXACYANOFERRATE:1||COLOSSALMAGNETORESISTANCE:1||FINITE TEMPERATURES:1||LAMNO3:1||FE:1||transitionmetal oxides:1||giant magnetoresistance:1||phonon:1||COPPER OXIDES:1||valence states:1||thermoelectric:1||semiconductor:1||CATION DISTRIBUTION:1||FeCr2S4:1||photoemission spectroscopy (PES):1||METALLIC FERROMAGNETISM:1||GRAPHITE:1||SUSCEPTIBILITY:1||UBE13:1||RCrSb3:1||band JahnTeller:1||Ce3S4:1||TiO2:1||PrBa2Cu3O7delta:1||UNTWINNED PRBA2CU3O7:1||AGNIO2:1||HALFMETALLIC FERROMAGNETS:1||CI:1||Energy gap:1||Photoemission:1||Future applications:1||Photoemission measurements:1||Graphene:1||BANDSTRUCTURE:1||TC:1||superconductivity:1||magnetic semiconductors:1||CMRmanganites:1||thin films:1||spin dynamics:1||highTc superconductors:1||ITINERANTELECTRON FERROMAGNETISM:1||SINGLECRYSTALS:1||CeTe2:1||amorphous magnetic materials:1||EPITAXIAL GRAPHENE:1||LAYERED PNICTIDEOXIDES:1||BOROCARBIDE SUPERCONDUCTORS:1||AUGMENTEDWAVE METHOD:1||METALLIC MAGNET UNISN:1||ORIGIN:1||spectrum rearrangement:1||MEANFIELD THEORY:1||MOLECULEBASED MAGNETS:1||METASTABLE STATE:1||INSULATOR:1||magnetic orderin:1||FCC IRON:1||CeRu2:1||TL2MN2O7:1||isotope effect:1||Perovskitemanganites:1||RECURSION METHOD:1||PERPENDICULAR MAGNETICANISOTROPY:1||quasiparticle spectral density:1||GW:1||MANGANESE FERRITE:1||RESONANCE:1||SeCuO3:1||Optical conductivity:1||MASSLESS DIRAC FERMIONS:1||SCHOTTKYBARRIER:1||electronic structure:15||ELECTRONICSTRUCTURE:11||TRANSITIONMETAL COMPOUNDS:10||METALS:10||photoemission:8||SPECTRA:8||MAGNETORESISTANCE:7||FERROMAGNETISM:7||TRANSPORT:7||TRANSITION:6||FILMS:6||THINFILMS:5||TOTALENERGY CALCULATIONS:5||MAGNETICPROPERTIES:5||SUPERCONDUCTIVITY:5||PR:5||LATTICE:4||STATES:4||SPECTROSCOPY:4||FIELD:4||CRYSTALSTRUCTURE:4||PHOTOEMISSION:4||TEMPERATURE:4||TRANSITIONTEMPERATURE:4||XRAYABSORPTION:4||STATE:4||CU:4||BASISSET:4||XAS:4||CRYSTALS:3||EXCITATIONS:3||MOTTHUBBARD SYSTEMS:3||HIGHENERGY SPIN:3||halfmetal:3||INSULATORS:3||LA2CUO4:3||MODEL:3||FLUCTUATIONS:3||CE:3||double exchange:3||TRANSITIONMETALS:3||RESISTIVITY:3||BORON:3||LA1XCAXMNO3:3||IRON:3||PES:3||ANTIMONIDES:2||MgB2:2||ZR METALLIC GLASSES:2||superconductor:2||CRITICALCURRENT DENSITY:2||CIRCULARDICHROISM:2||SEMICONDUCTORS:2||LOCALIZATION:2||INTRABAND OPTICAL CONDUCTIVITY:2||COLOSSAL MAGNETORESISTANCE:2||OXIDATION:2||EXISTENCE:2||COPPER:2||diboride:2||MAGNESIUMDIBORIDE:2||GAP:2||CE COMPOUNDS:2||CORE POLARIZATION:2||magnetoresistance:2||photoemission spectroscopy:2||electronphonon interaction:2||GETTER:2||PD:2||MAGNETISM:2||FECR2S4:2||SUPERCONDUCTING MGB2:2||WIRES:2||ABSORPTION:2||ENERGY:2||LA1XSRXMNO3:2||CONSTANTS:2||polaron:2||charge ordering:2||SCATTERING:2||XRAY PHOTOEMISSION:2||CeNiSn:2||phase diagram:2||PHOTOELECTRON:2||QUADRUPOLAR:2||perovskitemanganites:2||CO:2||SYSTEMS:2||DOPED ZNO:2||LOWFREQUENCY SOUND:2||LA:2||ELECTRONELECTRON SCATTERING:2||AU:2||DENSITYWAVE INSTABILITY:2||FERMISURFACE:2||hybridization:2||VALENCEBAND SATELLITE:2||SULFUR SPINEL:2||Heusler:2||APPROXIMATION:2||superexchange:2||colossal magnetoresistance:2||ALLOYS:2||DEPENDENCE:2||AG:2||electronic structures:2||AUGERSPECTRA:2||CR:2||PARAMETERS:2||DIFFRACTION:2||SEMICONDUCTORMETAL TRANSITION:1||INTERMEDIATEVALENCE:1||SMB6:1||SRRUO3:1||antiperovskite structure with antipolar nature:1||lowenergy twodimensional phonons:1||anatase TiO2:1||La3S4:1||metalinsulator transitions:1||MNO:1||ELECTRONICSTRUCTURES:1||MAGNETIC CIRCULARDICHROISM:1||Density functional theory:1||CeCo2:1||TOPOLARON CROSSOVER:1||EXCHANGE:1||cuprates:1||high Tc cuprates:1||magnetically ordered materials:1||ZNSE:1||Sr2xKxFeMoO6:1||CDW:1||TeCuO3:1||STRUCTURALPROPERTIES:1||MN:1||screening length:1||amorphous Fe:1||WAVE BASISSET:1||SILICONCARBIDE:1||HIGHPRESSURE:1||electronphonon coupling:1||quenched superconductivity:1||CMR perovskite manganites:1||OXIDE:1||polarons:1||synchrotron radiation:1||FULLERIDES:1||RESONANTPHOTOEMISSION:1||Silicon carbide:1||DFT calculation:1||Hybridized bands:1||GIANT MAGNETORESISTANCE:1||PEROVSKITES:1||Raman spectra:1||EXCHANGE ENHANCEMENT:1||SILICON:1||SR2FEMOO6:1||orbital ordering:1||delafossite:1||TITANIUMDIOXIDE:1||electronic structure of disordered solids:1||YFE2:1||Magnetic polaron:1||NA2TI2SB2O:1||STRONGCOUPLED SUPERCONDUCTORS:1||HEAVYFERMION SYSTEMS:1||firstprinciples calculations:1||MECHANISM:1||UNiSn:1||PHOTONIC BANDGAP:1||SINGLE IMPURITY:1||PHONONSPECTRUM:1||FERMISURFACE TOPOLOGY:1||SUPPRESSION:1||RESONANT PHOTOEMISSION:1||METALDOPED PICENE:1||PHOTOIONIZATION CROSSSECTIONS:1||PHOTOINDUCED FERRIMAGNETIC SYSTEMS:1||LINKAGE ISOMERISM:1||CHARGETRANSFER:1||Bilayer Graphene:1||MAGNETICFIELD:1||SPINWAVES:1||rareearth manganese oxides:1||magnonphonon interaction:1||NACO2O4:1||ENERGYBANDS:1||SELFENERGY:1||GAS:1||Fe0.5Cu0.5Cr2S4:1||scanning photoelectron microscopy (SPEM):1||MAGNETIC PROPERTIES:1||Stoner model:1||AMORPHOUS TRANSITIONMETALS:1||SPINGLASS STATES:1||NI:1||LA3NI2B2N3:1||SOLIDS:1||CEO2:1||BAND THEORY:1||dilute magnetic semiconductor:1||pyrochlore:1||Y1XPRXBA2CU3O7DELTA:1||and electronphonon interactions:1||VIBRATIONS:1||RAY PHOTOEMISSION:1||ALKALI CATION:1||Europium:1||colossal magnetoresistance:1||structural stability:1||ENERGYGAP:1||small polaron:1||DOUBLE EXCHANGE:1||Coulomb correlation:1||magnon:1||phonons:1||ELECTRON FERROMAGNETISM:1||CURIETEMPERATURE:1||ARPES:1||PLANEWAVE METHOD:1||Xray absorption spectroscopy (XAS):1||ROOMTEMPERATURE:1||MONOCHALCOGENIDES:1||HEAT:1||UPDSN:1||MOMENTS:1||XRAY ABSORPTION:1||SEMICONDUCTOR:1||Fermi surface nesting:1||optical phonon:1||disordered system:1||dilute magnetic semiconductors:1||CMR manganites:1||PHONONS:1||LATTICEDYNAMICS:1||OXIDES:1||4fphotoemission:1||permanent magnet:1||pseudogap:1||TRANSPORTPROPERTIES:1||ANTIFERROMAGNET:1||(BI,PB)SRCOO SYSTEM:1||semicore correlation:1||POLARIZATION:1||CRYSTAL:1||spinel:1||Xray magnetic circular dichroism (XMCD):1||magnetocapacitance:1||ANATASE:1||TEMPERATURES:1||Pseudogap:1||INTERFACE:1||SUBSTRATE:1||YNI2B2C:1||SAMARIUM SULFIDE:1||strong swave superconductor:1||DOPED MANGANITE:1||SYMMETRY:1||CENISN:1||resonance mode:1||DISORDERED SYSTEM:1||LITHIUM INTERCALATION:1||CUO2 PLANE:1||SURFACE:1||Delafossite:1||ELECTRICALPROPERTIES:1||NIMNSB:1||PTMNSB:1||ROOMTEMPERATURE FERROMAGNETISM:1||RUBIDIUM MANGANESE HEXACYANOFERRATE:1||COLOSSALMAGNETORESISTANCE:1||FINITE TEMPERATURES:1||LAMNO3:1||FE:1||transitionmetal oxides:1||giant magnetoresistance:1||phonon:1||COPPER OXIDES:1||valence states:1||thermoelectric:1||semiconductor:1||CATION DISTRIBUTION:1||FeCr2S4:1||photoemission spectroscopy (PES):1||METALLIC FERROMAGNETISM:1||GRAPHITE:1||SUSCEPTIBILITY:1||UBE13:1||RCrSb3:1||band JahnTeller:1||Ce3S4:1||TiO2:1||PrBa2Cu3O7delta:1||UNTWINNED PRBA2CU3O7:1||AGNIO2:1||HALFMETALLIC FERROMAGNETS:1||CI:1||Energy gap:1||Photoemission:1||Future applications:1||Photoemission measurements:1||Graphene:1||BANDSTRUCTURE:1||TC:1||superconductivity:1||magnetic semiconductors:1||CMRmanganites:1||thin films:1||spin dynamics:1||highTc superconductors:1||ITINERANTELECTRON FERROMAGNETISM:1||SINGLECRYSTALS:1||CeTe2:1||amorphous magnetic materials:1||EPITAXIAL GRAPHENE:1||LAYERED PNICTIDEOXIDES:1||BOROCARBIDE SUPERCONDUCTORS:1||AUGMENTEDWAVE METHOD:1||METALLIC MAGNET UNISN:1||ORIGIN:1||spectrum rearrangement:1||MEANFIELD THEORY:1||MOLECULEBASED MAGNETS:1||METASTABLE STATE:1||INSULATOR:1||magnetic orderin:1||FCC IRON:1||CeRu2:1||TL2MN2O7:1||isotope effect:1||Perovskitemanganites:1||RECURSION METHOD:1||PERPENDICULAR MAGNETICANISOTROPY:1||quasiparticle spectral density:1||GW:1||MANGANESE FERRITE:1||RESONANCE:1||SeCuO3:1||Optical conductivity:1||MASSLESS DIRAC FERMIONS:1||SCHOTTKYBARRIER:1||electronic structure:15||ELECTRONICSTRUCTURE:11||TRANSITIONMETAL COMPOUNDS:10||METALS:10||photoemission:8||SPECTRA:8||MAGNETORESISTANCE:7||FERROMAGNETISM:7||TRANSPORT:7||TRANSITION:6||FILMS:6||THINFILMS:5||TOTALENERGY CALCULATIONS:5||MAGNETICPROPERTIES:5||SUPERCONDUCTIVITY:5||PR:5||LATTICE:4||STATES:4||SPECTROSCOPY:4||FIELD:4||CRYSTALSTRUCTURE:4||PHOTOEMISSION:4||TEMPERATURE:4||TRANSITIONTEMPERATURE:4||XRAYABSORPTION:4||STATE:4||CU:4||BASISSET:4||XAS:4||CRYSTALS:3||EXCITATIONS:3||MOTTHUBBARD SYSTEMS:3||HIGHENERGY SPIN:3||halfmetal:3||INSULATORS:3||LA2CUO4:3||MODEL:3||FLUCTUATIONS:3||CE:3||double exchange:3||TRANSITIONMETALS:3||RESISTIVITY:3||BORON:3||LA1XCAXMNO3:3||IRON:3||PES:3||ANTIMONIDES:2||MgB2:2||ZR METALLIC GLASSES:2||superconductor:2||CRITICALCURRENT DENSITY:2||CIRCULARDICHROISM:2||SEMICONDUCTORS:2||LOCALIZATION:2||INTRABAND OPTICAL CONDUCTIVITY:2||COLOSSAL MAGNETORESISTANCE:2||OXIDATION:2||EXISTENCE:2||COPPER:2||diboride:2||MAGNESIUMDIBORIDE:2||GAP:2||CE COMPOUNDS:2||CORE POLARIZATION:2||magnetoresistance:2||photoemission spectroscopy:2||electronphonon interaction:2||GETTER:2||PD:2||MAGNETISM:2||FECR2S4:2||SUPERCONDUCTING MGB2:2||WIRES:2||ABSORPTION:2||ENERGY:2||LA1XSRXMNO3:2||CONSTANTS:2||polaron:2||charge ordering:2||SCATTERING:2||XRAY PHOTOEMISSION:2||CeNiSn:2||phase diagram:2||PHOTOELECTRON:2||QUADRUPOLAR:2||perovskitemanganites:2||CO:2||SYSTEMS:2||DOPED ZNO:2||LOWFREQUENCY SOUND:2||LA:2||ELECTRONELECTRON SCATTERING:2||AU:2||DENSITYWAVE INSTABILITY:2||FERMISURFACE:2||hybridization:2||VALENCEBAND SATELLITE:2||SULFUR SPINEL:2||Heusler:2||APPROXIMATION:2||superexchange:2||colossal magnetoresistance:2||ALLOYS:2||DEPENDENCE:2||AG:2||electronic structures:2||AUGERSPECTRA:2||CR:2||PARAMETERS:2||DIFFRACTION:2||SEMICONDUCTORMETAL TRANSITION:1||INTERMEDIATEVALENCE:1||SMB6:1||SRRUO3:1||antiperovskite structure with antipolar nature:1||lowenergy twodimensional phonons:1||anatase TiO2:1||La3S4:1||metalinsulator transitions:1||MNO:1||ELECTRONICSTRUCTURES:1||MAGNETIC CIRCULARDICHROISM:1||Density functional theory:1||CeCo2:1||TOPOLARON CROSSOVER:1||EXCHANGE:1||cuprates:1||high Tc cuprates:1||magnetically ordered materials:1||ZNSE:1||Sr2xKxFeMoO6:1||CDW:1||TeCuO3:1||STRUCTURALPROPERTIES:1||MN:1||screening length:1||amorphous Fe:1||WAVE BASISSET:1||SILICONCARBIDE:1||HIGHPRESSURE:1||electronphonon coupling:1||quenched superconductivity:1||CMR perovskite manganites:1||OXIDE:1||polarons:1||synchrotron radiation:1||FULLERIDES:1||RESONANTPHOTOEMISSION:1||Silicon carbide:1||DFT calculation:1||Hybridized bands:1||GIANT MAGNETORESISTANCE:1||PEROVSKITES:1||Raman spectra:1||EXCHANGE ENHANCEMENT:1||SILICON:1||SR2FEMOO6:1||orbital ordering:1||delafossite:1||TITANIUMDIOXIDE:1||electronic structure of disordered solids:1||YFE2:1||Magnetic polaron:1||NA2TI2SB2O:1||STRONGCOUPLED SUPERCONDUCTORS:1||HEAVYFERMION SYSTEMS:1||firstprinciples calculations:1||MECHANISM:1||UNiSn:1||PHOTONIC BANDGAP:1||SINGLE IMPURITY:1||PHONONSPECTRUM:1||FERMISURFACE TOPOLOGY:1||SUPPRESSION:1||RESONANT PHOTOEMISSION:1||METALDOPED PICENE:1||PHOTOIONIZATION CROSSSECTIONS:1||PHOTOINDUCED FERRIMAGNETIC SYSTEMS:1||LINKAGE ISOMERISM:1||CHARGETRANSFER:1||Bilayer Graphene:1||MAGNETICFIELD:1||SPINWAVES:1||rareearth manganese oxides:1||magnonphonon interaction:1||NACO2O4:1||ENERGYBANDS:1||SELFENERGY:1||GAS:1||Fe0.5Cu0.5Cr2S4:1||scanning photoelectron microscopy (SPEM):1||MAGNETIC PROPERTIES:1||Stoner model:1||AMORPHOUS TRANSITIONMETALS:1||SPINGLASS STATES:1||NI:1||LA3NI2B2N3:1||SOLIDS:1||CEO2:1||BAND THEORY:1||dilute magnetic semiconductor:1||pyrochlore:1||Y1XPRXBA2CU3O7DELTA:1||and electronphonon interactions:1||VIBRATIONS:1||RAY PHOTOEMISSION:1||ALKALI CATION:1||Europium:1||colossal magnetoresistance:1||structural stability:1||ENERGYGAP:1||small polaron:1||DOUBLE EXCHANGE:1||Coulomb correlation:1||magnon:1||phonons:1||ELECTRON FERROMAGNETISM:1||CURIETEMPERATURE:1||ARPES:1||PLANEWAVE METHOD:1||Xray absorption spectroscopy (XAS):1||ROOMTEMPERATURE:1||MONOCHALCOGENIDES:1||HEAT:1||UPDSN:1||MOMENTS:1||XRAY ABSORPTION:1||SEMICONDUCTOR:1||Fermi surface nesting:1||optical phonon:1||disordered system:1||dilute magnetic semiconductors:1||CMR manganites:1||PHONONS:1||LATTICEDYNAMICS:1||OXIDES:1||4fphotoemission:1||permanent magnet:1||pseudogap:1||TRANSPORTPROPERTIES:1||ANTIFERROMAGNET:1||(BI,PB)SRCOO SYSTEM:1||semicore correlation:1||POLARIZATION:1||CRYSTAL:1||spinel:1||Xray magnetic circular dichroism (XMCD):1||magnetocapacitance:1||ANATASE:1||TEMPERATURES:1||Pseudogap:1||INTERFACE:1||SUBSTRATE:1||YNI2B2C:1||SAMARIUM SULFIDE:1||strong swave superconductor:1||DOPED MANGANITE:1||SYMMETRY:1||CENISN:1||resonance mode:1||DISORDERED SYSTEM:1||LITHIUM INTERCALATION:1||CUO2 PLANE:1||SURFACE:1||Delafossite:1||ELECTRICALPROPERTIES:1||NIMNSB:1||PTMNSB:1||ROOMTEMPERATURE FERROMAGNETISM:1||RUBIDIUM MANGANESE HEXACYANOFERRATE:1||COLOSSALMAGNETORESISTANCE:1||FINITE TEMPERATURES:1||LAMNO3:1||FE:1||transitionmetal oxides:1||giant magnetoresistance:1||phonon:1||COPPER OXIDES:1||valence states:1||thermoelectric:1||semiconductor:1||CATION DISTRIBUTION:1||FeCr2S4:1||photoemission spectroscopy (PES):1||METALLIC FERROMAGNETISM:1||GRAPHITE:1||SUSCEPTIBILITY:1||UBE13:1||RCrSb3:1||band JahnTeller:1||Ce3S4:1||TiO2:1||PrBa2Cu3O7delta:1||UNTWINNED PRBA2CU3O7:1||AGNIO2:1||HALFMETALLIC FERROMAGNETS:1||CI:1||Energy gap:1||Photoemission:1||Future applications:1||Photoemission measurements:1||Graphene:1||BANDSTRUCTURE:1||TC:1||superconductivity:1||magnetic semiconductors:1||CMRmanganites:1||thin films:1||spin dynamics:1||highTc superconductors:1||ITINERANTELECTRON FERROMAGNETISM:1||SINGLECRYSTALS:1||CeTe2:1||amorphous magnetic materials:1||EPITAXIAL GRAPHENE:1||LAYERED PNICTIDEOXIDES:1||BOROCARBIDE SUPERCONDUCTORS:1||AUGMENTEDWAVE METHOD:1||METALLIC MAGNET UNISN:1||ORIGIN:1||spectrum rearrangement:1||MEANFIELD THEORY:1||MOLECULEBASED MAGNETS:1||METASTABLE STATE:1||INSULATOR:1||magnetic orderin:1||FCC IRON:1||CeRu2:1||TL2MN2O7:1||isotope effect:1||Perovskitemanganites:1||RECURSION METHOD:1||PERPENDICULAR MAGNETICANISOTROPY:1||quasiparticle spectral density:1||GW:1||MANGANESE FERRITE:1||RESONANCE:1||SeCuO3:1||Optical conductivity:1||MASSLESS DIRAC FERMIONS:1||SCHOTTKYBARRIER:1||electronic structure:15||ELECTRONICSTRUCTURE:11||TRANSITIONMETAL COMPOUNDS:10||METALS:10||photoemission:8||SPECTRA:8||MAGNETORESISTANCE:7||FERROMAGNETISM:7||TRANSPORT:7||TRANSITION:6||FILMS:6||THINFILMS:5||TOTALENERGY CALCULATIONS:5||MAGNETICPROPERTIES:5||SUPERCONDUCTIVITY:5||PR:5||LATTICE:4||STATES:4||SPECTROSCOPY:4||FIELD:4||CRYSTALSTRUCTURE:4||PHOTOEMISSION:4||TEMPERATURE:4||TRANSITIONTEMPERATURE:4||XRAYABSORPTION:4||STATE:4||CU:4||BASISSET:4||XAS:4||CRYSTALS:3||EXCITATIONS:3||MOTTHUBBARD SYSTEMS:3||HIGHENERGY SPIN:3||halfmetal:3||INSULATORS:3||LA2CUO4:3||MODEL:3||FLUCTUATIONS:3||CE:3||double exchange:3||TRANSITIONMETALS:3||RESISTIVITY:3||BORON:3||LA1XCAXMNO3:3||IRON:3||PES:3||ANTIMONIDES:2||MgB2:2||ZR METALLIC GLASSES:2||superconductor:2||CRITICALCURRENT DENSITY:2||CIRCULARDICHROISM:2||SEMICONDUCTORS:2||LOCALIZATION:2||INTRABAND OPTICAL CONDUCTIVITY:2||COLOSSAL MAGNETORESISTANCE:2||OXIDATION:2||EXISTENCE:2||COPPER:2||diboride:2||MAGNESIUMDIBORIDE:2||GAP:2||CE COMPOUNDS:2||CORE POLARIZATION:2||magnetoresistance:2||photoemission spectroscopy:2||electronphonon interaction:2||GETTER:2||PD:2||MAGNETISM:2||FECR2S4:2||SUPERCONDUCTING MGB2:2||WIRES:2||ABSORPTION:2||ENERGY:2||LA1XSRXMNO3:2||CONSTANTS:2||polaron:2||charge ordering:2||SCATTERING:2||XRAY PHOTOEMISSION:2||CeNiSn:2||phase diagram:2||PHOTOELECTRON:2||QUADRUPOLAR:2||perovskitemanganites:2||CO:2||SYSTEMS:2||DOPED ZNO:2||LOWFREQUENCY SOUND:2||LA:2||ELECTRONELECTRON SCATTERING:2||AU:2||DENSITYWAVE INSTABILITY:2||FERMISURFACE:2||hybridization:2||VALENCEBAND SATELLITE:2||SULFUR SPINEL:2||Heusler:2||APPROXIMATION:2||superexchange:2||colossal magnetoresistance:2||ALLOYS:2||DEPENDENCE:2||AG:2||electronic structures:2||AUGERSPECTRA:2||CR:2||PARAMETERS:2||DIFFRACTION:2||SEMICONDUCTORMETAL TRANSITION:1||INTERMEDIATEVALENCE:1||SMB6:1||SRRUO3:1||antiperovskite structure with antipolar nature:1||lowenergy twodimensional phonons:1||anatase TiO2:1||La3S4:1||metalinsulator transitions:1||MNO:1||ELECTRONICSTRUCTURES:1||MAGNETIC CIRCULARDICHROISM:1||Density functional theory:1||CeCo2:1||TOPOLARON CROSSOVER:1||EXCHANGE:1||cuprates:1||high Tc cuprates:1||magnetically ordered materials:1||ZNSE:1||Sr2xKxFeMoO6:1||CDW:1||TeCuO3:1||STRUCTURALPROPERTIES:1||MN:1||screening length:1||amorphous Fe:1||WAVE BASISSET:1||SILICONCARBIDE:1||HIGHPRESSURE:1||electronphonon coupling:1||quenched superconductivity:1||CMR perovskite manganites:1||OXIDE:1||polarons:1||synchrotron radiation:1||FULLERIDES:1||RESONANTPHOTOEMISSION:1||Silicon carbide:1||DFT calculation:1||Hybridized bands:1||GIANT MAGNETORESISTANCE:1||PEROVSKITES:1||Raman spectra:1||EXCHANGE ENHANCEMENT:1||SILICON:1||SR2FEMOO6:1||orbital ordering:1||delafossite:1||TITANIUMDIOXIDE:1||electronic structure of disordered solids:1||YFE2:1||Magnetic polaron:1||NA2TI2SB2O:1||STRONGCOUPLED SUPERCONDUCTORS:1||HEAVYFERMION SYSTEMS:1||firstprinciples calculations:1||MECHANISM:1||UNiSn:1||PHOTONIC BANDGAP:1||SINGLE IMPURITY:1||PHONONSPECTRUM:1||FERMISURFACE TOPOLOGY:1||SUPPRESSION:1||RESONANT PHOTOEMISSION:1||METALDOPED PICENE:1||PHOTOIONIZATION CROSSSECTIONS:1||PHOTOINDUCED FERRIMAGNETIC SYSTEMS:1||LINKAGE ISOMERISM:1||CHARGETRANSFER:1||Bilayer Graphene:1||MAGNETICFIELD:1||SPINWAVES:1||rareearth manganese oxides:1||magnonphonon interaction:1||NACO2O4:1||ENERGYBANDS:1||SELFENERGY:1||GAS:1||Fe0.5Cu0.5Cr2S4:1||scanning photoelectron microscopy (SPEM):1||MAGNETIC PROPERTIES:1||Stoner model:1||AMORPHOUS TRANSITIONMETALS:1||SPINGLASS STATES:1||NI:1||LA3NI2B2N3:1||SOLIDS:1||CEO2:1||BAND THEORY:1||dilute magnetic semiconductor:1||pyrochlore:1||Y1XPRXBA2CU3O7DELTA:1||and electronphonon interactions:1||VIBRATIONS:1||RAY PHOTOEMISSION:1||ALKALI CATION:1||Europium:1||colossal magnetoresistance:1||structural stability:1||ENERGYGAP:1||small polaron:1||DOUBLE EXCHANGE:1||Coulomb correlation:1||magnon:1||phonons:1||ELECTRON FERROMAGNETISM:1||CURIETEMPERATURE:1||ARPES:1||PLANEWAVE METHOD:1||Xray absorption spectroscopy (XAS):1||ROOMTEMPERATURE:1||MONOCHALCOGENIDES:1||HEAT:1||UPDSN:1||MOMENTS:1||XRAY ABSORPTION:1||SEMICONDUCTOR:1||Fermi surface nesting:1||optical phonon:1||disordered system:1||dilute magnetic semiconductors:1||CMR manganites:1||PHONONS:1||LATTICEDYNAMICS:1||OXIDES:1||4fphotoemission:1||permanent magnet:1||pseudogap:1||TRANSPORTPROPERTIES:1||ANTIFERROMAGNET:1||(BI,PB)SRCOO SYSTEM:1||semicore correlation:1||POLARIZATION:1||CRYSTAL:1||spinel:1||Xray magnetic circular dichroism (XMCD):1||magnetocapacitance:1||ANATASE:1||TEMPERATURES:1||Pseudogap:1||INTERFACE:1||SUBSTRATE:1||YNI2B2C:1||SAMARIUM SULFIDE:1||strong swave superconductor:1||DOPED MANGANITE:1||SYMMETRY:1||CENISN:1||resonance mode:1||DISORDERED SYSTEM:1||LITHIUM INTERCALATION:1||CUO2 PLANE:1||SURFACE:1||Delafossite:1||ELECTRICALPROPERTIES:1||NIMNSB:1||PTMNSB:1||ROOMTEMPERATURE FERROMAGNETISM:1||RUBIDIUM MANGANESE HEXACYANOFERRATE:1||COLOSSALMAGNETORESISTANCE:1||FINITE TEMPERATURES:1||LAMNO3:1||FE:1||transitionmetal oxides:1||giant magnetoresistance:1||phonon:1||COPPER OXIDES:1||valence states:1||thermoelectric:1||semiconductor:1||CATION DISTRIBUTION:1||FeCr2S4:1||photoemission spectroscopy (PES):1||METALLIC FERROMAGNETISM:1||GRAPHITE:1||SUSCEPTIBILITY:1||UBE13:1||RCrSb3:1||band JahnTeller:1||Ce3S4:1||TiO2:1||PrBa2Cu3O7delta:1||UNTWINNED PRBA2CU3O7:1||AGNIO2:1||HALFMETALLIC FERROMAGNETS:1||CI:1||Energy gap:1||Photoemission:1||Future applications:1||Photoemission measurements:1||Graphene:1||BANDSTRUCTURE:1||TC:1||superconductivity:1||magnetic semiconductors:1||CMRmanganites:1||thin films:1||spin dynamics:1||highTc superconductors:1||ITINERANTELECTRON FERROMAGNETISM:1||SINGLECRYSTALS:1||CeTe2:1||amorphous magnetic materials:1||EPITAXIAL GRAPHENE:1||LAYERED PNICTIDEOXIDES:1||BOROCARBIDE SUPERCONDUCTORS:1||AUGMENTEDWAVE METHOD:1||METALLIC MAGNET UNISN:1||ORIGIN:1||spectrum rearrangement:1||MEANFIELD THEORY:1||MOLECULEBASED MAGNETS:1||METASTABLE STATE:1||INSULATOR:1||magnetic orderin:1||FCC IRON:1||CeRu2:1||TL2MN2O7:1||isotope effect:1||Perovskitemanganites:1||RECURSION METHOD:1||PERPENDICULAR MAGNETICANISOTROPY:1||quasiparticle spectral density:1||GW:1||MANGANESE FERRITE:1||RESONANCE:1||SeCuO3:1||Optical conductivity:1||MASSLESS DIRAC FERMIONS:1||SCHOTTKYBARRIER:1||electronic structure:15||ELECTRONICSTRUCTURE:11||TRANSITIONMETAL COMPOUNDS:10||METALS:10||photoemission:8||SPECTRA:8||MAGNETORESISTANCE:7||FERROMAGNETISM:7||TRANSPORT:7||TRANSITION:6||FILMS:6||THINFILMS:5||TOTALENERGY CALCULATIONS:5||MAGNETICPROPERTIES:5||SUPERCONDUCTIVITY:5||PR:5||LATTICE:4||STATES:4||SPECTROSCOPY:4||FIELD:4||CRYSTALSTRUCTURE:4||PHOTOEMISSION:4||TEMPERATURE:4||TRANSITIONTEMPERATURE:4||XRAYABSORPTION:4||STATE:4||CU:4||BASISSET:4||XAS:4||CRYSTALS:3||EXCITATIONS:3||MOTTHUBBARD SYSTEMS:3||HIGHENERGY SPIN:3||halfmetal:3||INSULATORS:3||LA2CUO4:3||MODEL:3||FLUCTUATIONS:3||CE:3||double exchange:3||TRANSITIONMETALS:3||RESISTIVITY:3||BORON:3||LA1XCAXMNO3:3||IRON:3||PES:3||ANTIMONIDES:2||MgB2:2||ZR METALLIC GLASSES:2||superconductor:2||CRITICALCURRENT DENSITY:2||CIRCULARDICHROISM:2||SEMICONDUCTORS:2||LOCALIZATION:2||INTRABAND OPTICAL CONDUCTIVITY:2||COLOSSAL MAGNETORESISTANCE:2||OXIDATION:2||EXISTENCE:2||COPPER:2||diboride:2||MAGNESIUMDIBORIDE:2||GAP:2||CE COMPOUNDS:2||CORE POLARIZATION:2||magnetoresistance:2||photoemission spectroscopy:2||electronphonon interaction:2||GETTER:2||PD:2||MAGNETISM:2||FECR2S4:2||SUPERCONDUCTING MGB2:2||WIRES:2||ABSORPTION:2||ENERGY:2||LA1XSRXMNO3:2||CONSTANTS:2||polaron:2||charge ordering:2||SCATTERING:2||XRAY PHOTOEMISSION:2||CeNiSn:2||phase diagram:2||PHOTOELECTRON:2||QUADRUPOLAR:2||perovskitemanganites:2||CO:2||SYSTEMS:2||DOPED ZNO:2||LOWFREQUENCY SOUND:2||LA:2||ELECTRONELECTRON SCATTERING:2||AU:2||DENSITYWAVE INSTABILITY:2||FERMISURFACE:2||hybridization:2||VALENCEBAND SATELLITE:2||SULFUR SPINEL:2||Heusler:2||APPROXIMATION:2||superexchange:2||colossal magnetoresistance:2||ALLOYS:2||DEPENDENCE:2||AG:2||electronic structures:2||AUGERSPECTRA:2||CR:2||PARAMETERS:2||DIFFRACTION:2||SEMICONDUCTORMETAL TRANSITION:1||INTERMEDIATEVALENCE:1||SMB6:1||SRRUO3:1||antiperovskite structure with antipolar nature:1||lowenergy twodimensional phonons:1||anatase TiO2:1||La3S4:1||metalinsulator transitions:1||MNO:1||ELECTRONICSTRUCTURES:1||MAGNETIC CIRCULARDICHROISM:1||Density functional theory:1||CeCo2:1||TOPOLARON CROSSOVER:1||EXCHANGE:1||cuprates:1||high Tc cuprates:1||magnetically ordered materials:1||ZNSE:1||Sr2xKxFeMoO6:1||CDW:1||TeCuO3:1||STRUCTURALPROPERTIES:1||MN:1||screening length:1||amorphous Fe:1||WAVE BASISSET:1||SILICONCARBIDE:1||HIGHPRESSURE:1||electronphonon coupling:1||quenched superconductivity:1||CMR perovskite manganites:1||OXIDE:1||polarons:1||synchrotron radiation:1||FULLERIDES:1||RESONANTPHOTOEMISSION:1||Silicon carbide:1||DFT calculation:1||Hybridized bands:1||GIANT MAGNETORESISTANCE:1||PEROVSKITES:1||Raman spectra:1||EXCHANGE ENHANCEMENT:1||SILICON:1||SR2FEMOO6:1||orbital ordering:1||delafossite:1||TITANIUMDIOXIDE:1||electronic structure of disordered solids:1||YFE2:1||Magnetic polaron:1||NA2TI2SB2O:1||STRONGCOUPLED SUPERCONDUCTORS:1||HEAVYFERMION SYSTEMS:1||firstprinciples calculations:1||MECHANISM:1||UNiSn:1||PHOTONIC BANDGAP:1||SINGLE IMPURITY:1||PHONONSPECTRUM:1||FERMISURFACE TOPOLOGY:1||SUPPRESSION:1||RESONANT PHOTOEMISSION:1||METALDOPED PICENE:1||PHOTOIONIZATION CROSSSECTIONS:1||PHOTOINDUCED FERRIMAGNETIC SYSTEMS:1||LINKAGE ISOMERISM:1||CHARGETRANSFER:1||Bilayer Graphene:1||MAGNETICFIELD:1||SPINWAVES:1||rareearth manganese oxides:1||magnonphonon interaction:1||NACO2O4:1||ENERGYBANDS:1||SELFENERGY:1||GAS:1||Fe0.5Cu0.5Cr2S4:1||scanning photoelectron microscopy (SPEM):1||MAGNETIC PROPERTIES:1||Stoner model:1||AMORPHOUS TRANSITIONMETALS:1||SPINGLASS STATES:1||NI:1||LA3NI2B2N3:1||SOLIDS:1||CEO2:1||BAND THEORY:1||dilute magnetic semiconductor:1||pyrochlore:1||Y1XPRXBA2CU3O7DELTA:1||and electronphonon interactions:1||VIBRATIONS:1||RAY PHOTOEMISSION:1||ALKALI CATION:1||Europium:1||colossal magnetoresistance:1||structural stability:1||ENERGYGAP:1||small polaron:1||DOUBLE EXCHANGE:1||Coulomb correlation:1||magnon:1||phonons:1||ELECTRON FERROMAGNETISM:1||CURIETEMPERATURE:1||ARPES:1||PLANEWAVE METHOD:1||Xray absorption spectroscopy (XAS):1||ROOMTEMPERATURE:1||MONOCHALCOGENIDES:1||HEAT:1||UPDSN:1||MOMENTS:1||XRAY ABSORPTION:1||SEMICONDUCTOR:1||Fermi surface nesting:1||optical phonon:1||disordered system:1||dilute magnetic semiconductors:1||CMR manganites:1||PHONONS:1||LATTICEDYNAMICS:1||OXIDES:1||4fphotoemission:1||permanent magnet:1||pseudogap:1||TRANSPORTPROPERTIES:1||ANTIFERROMAGNET:1||(BI,PB)SRCOO SYSTEM:1||semicore correlation:1||POLARIZATION:1||CRYSTAL:1||spinel:1||Xray magnetic circular dichroism (XMCD):1||magnetocapacitance:1||ANATASE:1||TEMPERATURES:1||Pseudogap:1||INTERFACE:1||SUBSTRATE:1||YNI2B2C:1||SAMARIUM SULFIDE:1||strong swave superconductor:1||DOPED MANGANITE:1||SYMMETRY:1||CENISN:1||resonance mode:1||DISORDERED SYSTEM:1||LITHIUM INTERCALATION:1||CUO2 PLANE:1||SURFACE:1||Delafossite:1||ELECTRICALPROPERTIES:1||NIMNSB:1||PTMNSB:1||ROOMTEMPERATURE FERROMAGNETISM:1||RUBIDIUM MANGANESE HEXACYANOFERRATE:1||COLOSSALMAGNETORESISTANCE:1||FINITE TEMPERATURES:1||LAMNO3:1||FE:1||transitionmetal oxides:1||giant magnetoresistance:1||phonon:1||COPPER OXIDES:1||valence states:1||thermoelectric:1||semiconductor:1||CATION DISTRIBUTION:1||FeCr2S4:1||photoemission spectroscopy (PES):1||METALLIC FERROMAGNETISM:1||GRAPHITE:1||SUSCEPTIBILITY:1||UBE13:1||RCrSb3:1||band JahnTeller:1||Ce3S4:1||TiO2:1||PrBa2Cu3O7delta:1||UNTWINNED PRBA2CU3O7:1||AGNIO2:1||HALFMETALLIC FERROMAGNETS:1||CI:1||Energy gap:1||Photoemission:1||Future applications:1||Photoemission measurements:1||Graphene:1||BANDSTRUCTURE:1||TC:1||superconductivity:1||magnetic semiconductors:1||CMRmanganites:1||thin films:1||spin dynamics:1||highTc superconductors:1||ITINERANTELECTRON FERROMAGNETISM:1||SINGLECRYSTALS:1||CeTe2:1||amorphous magnetic materials:1||EPITAXIAL GRAPHENE:1||LAYERED PNICTIDEOXIDES:1||BOROCARBIDE SUPERCONDUCTORS:1||AUGMENTEDWAVE METHOD:1||METALLIC MAGNET UNISN:1||ORIGIN:1||spectrum rearrangement:1||MEANFIELD THEORY:1||MOLECULEBASED MAGNETS:1||METASTABLE STATE:1||INSULATOR:1||magnetic orderin:1||FCC IRON:1||CeRu2:1||TL2MN2O7:1||isotope effect:1||Perovskitemanganites:1||RECURSION METHOD:1||PERPENDICULAR MAGNETICANISOTROPY:1||quasiparticle spectral density:1||GW:1||MANGANESE FERRITE:1||RESONANCE:1||SeCuO3:1||Optical conductivity:1||MASSLESS DIRAC FERMIONS:1||SCHOTTKYBARRIER:1||electronic structure:15||ELECTRONICSTRUCTURE:11||TRANSITIONMETAL COMPOUNDS:10||METALS:10||photoemission:8||SPECTRA:8||MAGNETORESISTANCE:7||FERROMAGNETISM:7||TRANSPORT:7||TRANSITION:6||FILMS:6||THINFILMS:5||TOTALENERGY CALCULATIONS:5||MAGNETICPROPERTIES:5||SUPERCONDUCTIVITY:5||PR:5||LATTICE:4||STATES:4||SPECTROSCOPY:4||FIELD:4||CRYSTALSTRUCTURE:4||PHOTOEMISSION:4||TEMPERATURE:4||TRANSITIONTEMPERATURE:4||XRAYABSORPTION:4||STATE:4||CU:4||BASISSET:4||XAS:4||CRYSTALS:3||EXCITATIONS:3||MOTTHUBBARD SYSTEMS:3||HIGHENERGY SPIN:3||halfmetal:3||INSULATORS:3||LA2CUO4:3||MODEL:3||FLUCTUATIONS:3||CE:3||double exchange:3||TRANSITIONMETALS:3||RESISTIVITY:3||BORON:3||LA1XCAXMNO3:3||IRON:3||PES:3||ANTIMONIDES:2||MgB2:2||ZR METALLIC GLASSES:2||superconductor:2||CRITICALCURRENT DENSITY:2||CIRCULARDICHROISM:2||SEMICONDUCTORS:2||LOCALIZATION:2||INTRABAND OPTICAL CONDUCTIVITY:2||COLOSSAL MAGNETORESISTANCE:2||OXIDATION:2||EXISTENCE:2||COPPER:2||diboride:2||MAGNESIUMDIBORIDE:2||GAP:2||CE COMPOUNDS:2||CORE POLARIZATION:2||magnetoresistance:2||photoemission spectroscopy:2||electronphonon interaction:2||GETTER:2||PD:2||MAGNETISM:2||FECR2S4:2||SUPERCONDUCTING MGB2:2||WIRES:2||ABSORPTION:2||ENERGY:2||LA1XSRXMNO3:2||CONSTANTS:2||polaron:2||charge ordering:2||SCATTERING:2||XRAY PHOTOEMISSION:2||CeNiSn:2||phase diagram:2||PHOTOELECTRON:2||QUADRUPOLAR:2||perovskitemanganites:2||CO:2||SYSTEMS:2||DOPED ZNO:2||LOWFREQUENCY SOUND:2||LA:2||ELECTRONELECTRON SCATTERING:2||AU:2||DENSITYWAVE INSTABILITY:2||FERMISURFACE:2||hybridization:2||VALENCEBAND SATELLITE:2||SULFUR SPINEL:2||Heusler:2||APPROXIMATION:2||superexchange:2||colossal magnetoresistance:2||ALLOYS:2||DEPENDENCE:2||AG:2||electronic structures:2||AUGERSPECTRA:2||CR:2||PARAMETERS:2||DIFFRACTION:2||SEMICONDUCTORMETAL TRANSITION:1||INTERMEDIATEVALENCE:1||SMB6:1||SRRUO3:1||antiperovskite structure with antipolar nature:1||lowenergy twodimensional phonons:1||anatase TiO2:1||La3S4:1||metalinsulator transitions:1||MNO:1||ELECTRONICSTRUCTURES:1||MAGNETIC CIRCULARDICHROISM:1||Density functional theory:1||CeCo2:1||TOPOLARON CROSSOVER:1||EXCHANGE:1||cuprates:1||high Tc cuprates:1||magnetically ordered materials:1||ZNSE:1||Sr2xKxFeMoO6:1||CDW:1||TeCuO3:1||STRUCTURALPROPERTIES:1||MN:1||screening length:1||amorphous Fe:1||WAVE BASISSET:1||SILICONCARBIDE:1||HIGHPRESSURE:1||electronphonon coupling:1||quenched superconductivity:1||CMR perovskite manganites:1||OXIDE:1||polarons:1||synchrotron radiation:1||FULLERIDES:1||RESONANTPHOTOEMISSION:1||Silicon carbide:1||DFT calculation:1||Hybridized bands:1||GIANT MAGNETORESISTANCE:1||PEROVSKITES:1||Raman spectra:1||EXCHANGE ENHANCEMENT:1||SILICON:1||SR2FEMOO6:1||orbital ordering:1||delafossite:1||TITANIUMDIOXIDE:1||electronic structure of disordered solids:1||YFE2:1||Magnetic polaron:1||NA2TI2SB2O:1||STRONGCOUPLED SUPERCONDUCTORS:1||HEAVYFERMION SYSTEMS:1||firstprinciples calculations:1||MECHANISM:1||UNiSn:1||PHOTONIC BANDGAP:1||SINGLE IMPURITY:1||PHONONSPECTRUM:1||FERMISURFACE TOPOLOGY:1||SUPPRESSION:1||RESONANT PHOTOEMISSION:1||METALDOPED PICENE:1||PHOTOIONIZATION CROSSSECTIONS:1||PHOTOINDUCED FERRIMAGNETIC SYSTEMS:1||LINKAGE ISOMERISM:1||CHARGETRANSFER:1||Bilayer Graphene:1||MAGNETICFIELD:1||SPINWAVES:1||rareearth manganese oxides:1||magnonphonon interaction:1||NACO2O4:1||ENERGYBANDS:1||SELFENERGY:1||GAS:1||Fe0.5Cu0.5Cr2S4:1||scanning photoelectron microscopy (SPEM):1||MAGNETIC PROPERTIES:1||Stoner model:1||AMORPHOUS TRANSITIONMETALS:1||SPINGLASS STATES:1||NI:1||LA3NI2B2N3:1||SOLIDS:1||CEO2:1||BAND THEORY:1||dilute magnetic semiconductor:1||pyrochlore:1||Y1XPRXBA2CU3O7DELTA:1||and electronphonon interactions:1||VIBRATIONS:1||RAY PHOTOEMISSION:1||ALKALI CATION:1||Europium:1||colossal magnetoresistance:1||structural stability:1||ENERGYGAP:1||small polaron:1||DOUBLE EXCHANGE:1||Coulomb correlation:1||magnon:1||phonons:1||ELECTRON FERROMAGNETISM:1||CURIETEMPERATURE:1||ARPES:1||PLANEWAVE METHOD:1||Xray absorption spectroscopy (XAS):1||ROOMTEMPERATURE:1||MONOCHALCOGENIDES:1||HEAT:1||UPDSN:1||MOMENTS:1||XRAY ABSORPTION:1||SEMICONDUCTOR:1||Fermi surface nesting:1||optical phonon:1||disordered system:1||dilute magnetic semiconductors:1||CMR manganites:1||PHONONS:1||LATTICEDYNAMICS:1||OXIDES:1||4fphotoemission:1||permanent magnet:1||pseudogap:1||TRANSPORTPROPERTIES:1||ANTIFERROMAGNET:1||(BI,PB)SRCOO SYSTEM:1||semicore correlation:1||POLARIZATION:1||CRYSTAL:1||spinel:1||Xray magnetic circular dichroism (XMCD):1||magnetocapacitance:1||ANATASE:1||TEMPERATURES:1||Pseudogap:1||INTERFACE:1||SUBSTRATE:1||YNI2B2C:1||SAMARIUM SULFIDE:1||strong swave superconductor:1||DOPED MANGANITE:1||SYMMETRY:1||CENISN:1||resonance mode:1||DISORDERED SYSTEM:1||LITHIUM INTERCALATION:1||CUO2 PLANE:1||SURFACE:1||Delafossite:1||ELECTRICALPROPERTIES:1||NIMNSB:1||PTMNSB:1||ROOMTEMPERATURE FERROMAGNETISM:1||RUBIDIUM MANGANESE HEXACYANOFERRATE:1||COLOSSALMAGNETORESISTANCE:1||FINITE TEMPERATURES:1||LAMNO3:1||FE:1||transitionmetal oxides:1||giant magnetoresistance:1||phonon:1||COPPER OXIDES:1||valence states:1||thermoelectric:1||semiconductor:1||CATION DISTRIBUTION:1||FeCr2S4:1||photoemission spectroscopy (PES):1||METALLIC FERROMAGNETISM:1||GRAPHITE:1||SUSCEPTIBILITY:1||UBE13:1||RCrSb3:1||band JahnTeller:1||Ce3S4:1||TiO2:1||PrBa2Cu3O7delta:1||UNTWINNED PRBA2CU3O7:1||AGNIO2:1||HALFMETALLIC FERROMAGNETS:1||CI:1||Energy gap:1||Photoemission:1||Future applications:1||Photoemission measurements:1||Graphene:1||BANDSTRUCTURE:1||TC:1||superconductivity:1||magnetic semiconductors:1||CMRmanganites:1||thin films:1||spin dynamics:1||highTc superconductors:1||ITINERANTELECTRON FERROMAGNETISM:1||SINGLECRYSTALS:1||CeTe2:1||amorphous magnetic materials:1||EPITAXIAL GRAPHENE:1||LAYERED PNICTIDEOXIDES:1||BOROCARBIDE SUPERCONDUCTORS:1||AUGMENTEDWAVE METHOD:1||METALLIC MAGNET UNISN:1||ORIGIN:1||spectrum rearrangement:1||MEANFIELD THEORY:1||MOLECULEBASED MAGNETS:1||METASTABLE STATE:1||INSULATOR:1||magnetic orderin:1||FCC IRON:1||CeRu2:1||TL2MN2O7:1||isotope effect:1||Perovskitemanganites:1||RECURSION METHOD:1||PERPENDICULAR MAGNETICANISOTROPY:1||quasiparticle spectral density:1||GW:1||MANGANESE FERRITE:1||RESONANCE:1||SeCuO3:1||Optical conductivity:1||MASSLESS DIRAC FERMIONS:1||SCHOTTKYBARRIER:1||electronic structure:15||ELECTRONICSTRUCTURE:11||TRANSITIONMETAL COMPOUNDS:10||METALS:10||photoemission:8||SPECTRA:8||MAGNETORESISTANCE:7||FERROMAGNETISM:7||TRANSPORT:7||TRANSITION:6||FILMS:6||THINFILMS:5||TOTALENERGY CALCULATIONS:5||MAGNETICPROPERTIES:5||SUPERCONDUCTIVITY:5||PR:5||LATTICE:4||STATES:4||SPECTROSCOPY:4||FIELD:4||CRYSTALSTRUCTURE:4||PHOTOEMISSION:4||TEMPERATURE:4||TRANSITIONTEMPERATURE:4||XRAYABSORPTION:4||STATE:4||CU:4||BASISSET:4||XAS:4||CRYSTALS:3||EXCITATIONS:3||MOTTHUBBARD SYSTEMS:3||HIGHENERGY SPIN:3||halfmetal:3||INSULATORS:3||LA2CUO4:3||MODEL:3||FLUCTUATIONS:3||CE:3||double exchange:3||TRANSITIONMETALS:3||RESISTIVITY:3||BORON:3||LA1XCAXMNO3:3||IRON:3||PES:3||ANTIMONIDES:2||MgB2:2||ZR METALLIC GLASSES:2||superconductor:2||CRITICALCURRENT DENSITY:2||CIRCULARDICHROISM:2||SEMICONDUCTORS:2||LOCALIZATION:2||INTRABAND OPTICAL CONDUCTIVITY:2||COLOSSAL MAGNETORESISTANCE:2||OXIDATION:2||EXISTENCE:2||COPPER:2||diboride:2||MAGNESIUMDIBORIDE:2||GAP:2||CE COMPOUNDS:2||CORE POLARIZATION:2||magnetoresistance:2||photoemission spectroscopy:2||electronphonon interaction:2||GETTER:2||PD:2||MAGNETISM:2||FECR2S4:2||SUPERCONDUCTING MGB2:2||WIRES:2||ABSORPTION:2||ENERGY:2||LA1XSRXMNO3:2||CONSTANTS:2||polaron:2||charge ordering:2||SCATTERING:2||XRAY PHOTOEMISSION:2||CeNiSn:2||phase diagram:2||PHOTOELECTRON:2||QUADRUPOLAR:2||perovskitemanganites:2||CO:2||SYSTEMS:2||DOPED ZNO:2||LOWFREQUENCY SOUND:2||LA:2||ELECTRONELECTRON SCATTERING:2||AU:2||DENSITYWAVE INSTABILITY:2||FERMISURFACE:2||hybridization:2||VALENCEBAND SATELLITE:2||SULFUR SPINEL:2||Heusler:2||APPROXIMATION:2||superexchange:2||colossal magnetoresistance:2||ALLOYS:2||DEPENDENCE:2||AG:2||electronic structures:2||AUGERSPECTRA:2||CR:2||PARAMETERS:2||DIFFRACTION:2||SEMICONDUCTORMETAL TRANSITION:1||INTERMEDIATEVALENCE:1||SMB6:1||SRRUO3:1||antiperovskite structure with antipolar nature:1||lowenergy twodimensional phonons:1||anatase TiO2:1||La3S4:1||metalinsulator transitions:1||MNO:1||ELECTRONICSTRUCTURES:1||MAGNETIC CIRCULARDICHROISM:1||Density functional theory:1||CeCo2:1||TOPOLARON CROSSOVER:1||EXCHANGE:1||cuprates:1||high Tc cuprates:1||magnetically ordered materials:1||ZNSE:1||Sr2xKxFeMoO6:1||CDW:1||TeCuO3:1||STRUCTURALPROPERTIES:1||MN:1||screening length:1||amorphous Fe:1||WAVE BASISSET:1||SILICONCARBIDE:1||HIGHPRESSURE:1||electronphonon coupling:1||quenched superconductivity:1||CMR perovskite manganites:1||OXIDE:1||polarons:1||synchrotron radiation:1||FULLERIDES:1||RESONANTPHOTOEMISSION:1||Silicon carbide:1||DFT calculation:1||Hybridized bands:1||GIANT MAGNETORESISTANCE:1||PEROVSKITES:1||Raman spectra:1||EXCHANGE ENHANCEMENT:1||SILICON:1||SR2FEMOO6:1||orbital ordering:1||delafossite:1||TITANIUMDIOXIDE:1||electronic structure of disordered solids:1||YFE2:1||Magnetic polaron:1||NA2TI2SB2O:1||STRONGCOUPLED SUPERCONDUCTORS:1||HEAVYFERMION SYSTEMS:1||firstprinciples calculations:1||MECHANISM:1||UNiSn:1||PHOTONIC BANDGAP:1||SINGLE IMPURITY:1||PHONONSPECTRUM:1||FERMISURFACE TOPOLOGY:1||SUPPRESSION:1||RESONANT PHOTOEMISSION:1||METALDOPED PICENE:1||PHOTOIONIZATION CROSSSECTIONS:1||PHOTOINDUCED FERRIMAGNETIC SYSTEMS:1||LINKAGE ISOMERISM:1||CHARGETRANSFER:1||Bilayer Graphene:1||MAGNETICFIELD:1||SPINWAVES:1||rareearth manganese oxides:1||magnonphonon interaction:1||NACO2O4:1||ENERGYBANDS:1||SELFENERGY:1||GAS:1||Fe0.5Cu0.5Cr2S4:1||scanning photoelectron microscopy (SPEM):1||MAGNETIC PROPERTIES:1||Stoner model:1||AMORPHOUS TRANSITIONMETALS:1||SPINGLASS STATES:1||NI:1||LA3NI2B2N3:1||SOLIDS:1||CEO2:1||BAND THEORY:1||dilute magnetic semiconductor:1||pyrochlore:1||Y1XPRXBA2CU3O7DELTA:1||and electronphonon interactions:1||VIBRATIONS:1||RAY PHOTOEMISSION:1||ALKALI CATION:1||Europium:1||colossal magnetoresistance:1||structural stability:1||ENERGYGAP:1||small polaron:1||DOUBLE EXCHANGE:1||Coulomb correlation:1||magnon:1||phonons:1||ELECTRON FERROMAGNETISM:1||CURIETEMPERATURE:1||ARPES:1||PLANEWAVE METHOD:1||Xray absorption spectroscopy (XAS):1||ROOMTEMPERATURE:1||MONOCHALCOGENIDES:1||HEAT:1||UPDSN:1||MOMENTS:1||XRAY ABSORPTION:1||SEMICONDUCTOR:1||Fermi surface nesting:1||optical phonon:1||disordered system:1||dilute magnetic semiconductors:1||CMR manganites:1||PHONONS:1||LATTICEDYNAMICS:1||OXIDES:1||4fphotoemission:1||permanent magnet:1||pseudogap:1||TRANSPORTPROPERTIES:1||ANTIFERROMAGNET:1||(BI,PB)SRCOO SYSTEM:1||semicore correlation:1||POLARIZATION:1||CRYSTAL:1||spinel:1||Xray magnetic circular dichroism (XMCD):1||magnetocapacitance:1||ANATASE:1||TEMPERATURES:1||Pseudogap:1||INTERFACE:1||SUBSTRATE:1||YNI2B2C:1||SAMARIUM SULFIDE:1||strong swave superconductor:1||DOPED MANGANITE:1||SYMMETRY:1||CENISN:1||resonance mode:1||DISORDERED SYSTEM:1||LITHIUM INTERCALATION:1||CUO2 PLANE:1||SURFACE:1||Delafossite:1||ELECTRICALPROPERTIES:1||NIMNSB:1||PTMNSB:1||ROOMTEMPERATURE FERROMAGNETISM:1||RUBIDIUM MANGANESE HEXACYANOFERRATE:1||COLOSSALMAGNETORESISTANCE:1||FINITE TEMPERATURES:1||LAMNO3:1||FE:1||transitionmetal oxides:1||giant magnetoresistance:1||phonon:1||COPPER OXIDES:1||valence states:1||thermoelectric:1||semiconductor:1||CATION DISTRIBUTION:1||FeCr2S4:1||photoemission spectroscopy (PES):1||METALLIC FERROMAGNETISM:1||GRAPHITE:1||SUSCEPTIBILITY:1||UBE13:1||RCrSb3:1||band JahnTeller:1||Ce3S4:1||TiO2:1||PrBa2Cu3O7delta:1||UNTWINNED PRBA2CU3O7:1||AGNIO2:1||HALFMETALLIC FERROMAGNETS:1||CI:1||Energy gap:1||Photoemission:1||Future applications:1||Photoemission measurements:1||Graphene:1||BANDSTRUCTURE:1||TC:1||superconductivity:1||magnetic semiconductors:1||CMRmanganites:1||thin films:1||spin dynamics:1||highTc superconductors:1||ITINERANTELECTRON FERROMAGNETISM:1||SINGLECRYSTALS:1||CeTe2:1||amorphous magnetic materials:1||EPITAXIAL GRAPHENE:1||LAYERED PNICTIDEOXIDES:1||BOROCARBIDE SUPERCONDUCTORS:1||AUGMENTEDWAVE METHOD:1||METALLIC MAGNET UNISN:1||ORIGIN:1||spectrum rearrangement:1||MEANFIELD THEORY:1||MOLECULEBASED MAGNETS:1||METASTABLE STATE:1||INSULATOR:1||magnetic orderin:1||FCC IRON:1||CeRu2:1||TL2MN2O7:1||isotope effect:1||Perovskitemanganites:1||RECURSION METHOD:1||PERPENDICULAR MAGNETICANISOTROPY:1||quasiparticle spectral density:1||GW:1||MANGANESE FERRITE:1||RESONANCE:1||SeCuO3:1||Optical conductivity:1||MASSLESS DIRAC FERMIONS:1||SCHOTTKYBARRIER:1||electronic structure:15||ELECTRONICSTRUCTURE:11||TRANSITIONMETAL COMPOUNDS:10||METALS:10||photoemission:8||SPECTRA:8||MAGNETORESISTANCE:7||FERROMAGNETISM:7||TRANSPORT:7||TRANSITION:6||FILMS:6||THINFILMS:5||TOTALENERGY CALCULATIONS:5||MAGNETICPROPERTIES:5||SUPERCONDUCTIVITY:5||PR:5||LATTICE:4||STATES:4||SPECTROSCOPY:4||FIELD:4||CRYSTALSTRUCTURE:4||PHOTOEMISSION:4||TEMPERATURE:4||TRANSITIONTEMPERATURE:4||XRAYABSORPTION:4||STATE:4||CU:4||BASISSET:4||XAS:4||CRYSTALS:3||EXCITATIONS:3||MOTTHUBBARD SYSTEMS:3||HIGHENERGY SPIN:3||halfmetal:3||INSULATORS:3||LA2CUO4:3||MODEL:3||FLUCTUATIONS:3||CE:3||double exchange:3||TRANSITIONMETALS:3||RESISTIVITY:3||BORON:3||LA1XCAXMNO3:3||IRON:3||PES:3||ANTIMONIDES:2||MgB2:2||ZR METALLIC GLASSES:2||superconductor:2||CRITICALCURRENT DENSITY:2||CIRCULARDICHROISM:2||SEMICONDUCTORS:2||LOCALIZATION:2||INTRABAND OPTICAL CONDUCTIVITY:2||COLOSSAL MAGNETORESISTANCE:2||OXIDATION:2||EXISTENCE:2||COPPER:2||diboride:2||MAGNESIUMDIBORIDE:2||GAP:2||CE COMPOUNDS:2||CORE POLARIZATION:2||magnetoresistance:2||photoemission spectroscopy:2||electronphonon interaction:2||GETTER:2||PD:2||MAGNETISM:2||FECR2S4:2||SUPERCONDUCTING MGB2:2||WIRES:2||ABSORPTION:2||ENERGY:2||LA1XSRXMNO3:2||CONSTANTS:2||polaron:2||charge ordering:2||SCATTERING:2||XRAY PHOTOEMISSION:2||CeNiSn:2||phase diagram:2||PHOTOELECTRON:2||QUADRUPOLAR:2||perovskitemanganites:2||CO:2||SYSTEMS:2||DOPED ZNO:2||LOWFREQUENCY SOUND:2||LA:2||ELECTRONELECTRON SCATTERING:2||AU:2||DENSITYWAVE INSTABILITY:2||FERMISURFACE:2||hybridization:2||VALENCEBAND SATELLITE:2||SULFUR SPINEL:2||Heusler:2||APPROXIMATION:2||superexchange:2||colossal magnetoresistance:2||ALLOYS:2||DEPENDENCE:2||AG:2||electronic structures:2||AUGERSPECTRA:2||CR:2||PARAMETERS:2||DIFFRACTION:2||SEMICONDUCTORMETAL TRANSITION:1||INTERMEDIATEVALENCE:1||SMB6:1||SRRUO3:1||antiperovskite structure with antipolar nature:1||lowenergy twodimensional phonons:1||anatase TiO2:1||La3S4:1||metalinsulator transitions:1||MNO:1||ELECTRONICSTRUCTURES:1||MAGNETIC CIRCULARDICHROISM:1||Density functional theory:1||CeCo2:1||TOPOLARON CROSSOVER:1||EXCHANGE:1||cuprates:1||high Tc cuprates:1||magnetically ordered materials:1||ZNSE:1||Sr2xKxFeMoO6:1||CDW:1||TeCuO3:1||STRUCTURALPROPERTIES:1||MN:1||screening length:1||amorphous Fe:1||WAVE BASISSET:1||SILICONCARBIDE:1||HIGHPRESSURE:1||electronphonon coupling:1||quenched superconductivity:1||CMR perovskite manganites:1||OXIDE:1||polarons:1||synchrotron radiation:1||FULLERIDES:1||RESONANTPHOTOEMISSION:1||Silicon carbide:1||DFT calculation:1||Hybridized bands:1||GIANT MAGNETORESISTANCE:1||PEROVSKITES:1||Raman spectra:1||EXCHANGE ENHANCEMENT:1||SILICON:1||SR2FEMOO6:1||orbital ordering:1||delafossite:1||TITANIUMDIOXIDE:1||electronic structure of disordered solids:1||YFE2:1||Magnetic polaron:1||NA2TI2SB2O:1||STRONGCOUPLED SUPERCONDUCTORS:1||HEAVYFERMION SYSTEMS:1||firstprinciples calculations:1||MECHANISM:1||UNiSn:1||PHOTONIC BANDGAP:1||SINGLE IMPURITY:1||PHONONSPECTRUM:1||FERMISURFACE TOPOLOGY:1||SUPPRESSION:1||RESONANT PHOTOEMISSION:1||METALDOPED PICENE:1||PHOTOIONIZATION CROSSSECTIONS:1||PHOTOINDUCED FERRIMAGNETIC SYSTEMS:1||LINKAGE ISOMERISM:1||CHARGETRANSFER:1||Bilayer Graphene:1||MAGNETICFIELD:1||SPINWAVES:1||rareearth manganese oxides:1||magnonphonon interaction:1||NACO2O4:1||ENERGYBANDS:1||SELFENERGY:1||GAS:1||Fe0.5Cu0.5Cr2S4:1||scanning photoelectron microscopy (SPEM):1||MAGNETIC PROPERTIES:1||Stoner model:1||AMORPHOUS TRANSITIONMETALS:1||SPINGLASS STATES:1||NI:1||LA3NI2B2N3:1||SOLIDS:1||CEO2:1||BAND THEORY:1||dilute magnetic semiconductor:1||pyrochlore:1||Y1XPRXBA2CU3O7DELTA:1||and electronphonon interactions:1||VIBRATIONS:1||RAY PHOTOEMISSION:1||ALKALI CATION:1||Europium:1||colossal magnetoresistance:1||structural stability:1||ENERGYGAP:1||small polaron:1||DOUBLE EXCHANGE:1||Coulomb correlation:1||magnon:1||phonons:1||ELECTRON FERROMAGNETISM:1||CURIETEMPERATURE:1||ARPES:1||PLANEWAVE METHOD:1||Xray absorption spectroscopy (XAS):1||ROOMTEMPERATURE:1||MONOCHALCOGENIDES:1||HEAT:1||UPDSN:1||MOMENTS:1||XRAY ABSORPTION:1||SEMICONDUCTOR:1||Fermi surface nesting:1||optical phonon:1||disordered system:1||dilute magnetic semiconductors:1||CMR manganites:1||PHONONS:1||LATTICEDYNAMICS:1||OXIDES:1||4fphotoemission:1||permanent magnet:1||pseudogap:1||TRANSPORTPROPERTIES:1||ANTIFERROMAGNET:1||(BI,PB)SRCOO SYSTEM:1||semicore correlation:1||POLARIZATION:1||CRYSTAL:1||spinel:1||Xray magnetic circular dichroism (XMCD):1||magnetocapacitance:1||ANATASE:1||TEMPERATURES:1||Pseudogap:1||INTERFACE:1||SUBSTRATE:1||YNI2B2C:1||SAMARIUM SULFIDE:1||strong swave superconductor:1||DOPED MANGANITE:1||SYMMETRY:1||CENISN:1||resonance mode:1||DISORDERED SYSTEM:1||LITHIUM INTERCALATION:1||CUO2 PLANE:1||SURFACE:1||Delafossite:1||ELECTRICALPROPERTIES:1||NIMNSB:1||PTMNSB:1||ROOMTEMPERATURE FERROMAGNETISM:1||RUBIDIUM MANGANESE HEXACYANOFERRATE:1||COLOSSALMAGNETORESISTANCE:1||FINITE TEMPERATURES:1||LAMNO3:1||FE:1||transitionmetal oxides:1||giant magnetoresistance:1||phonon:1||COPPER OXIDES:1||valence states:1||thermoelectric:1||semiconductor:1||CATION DISTRIBUTION:1||FeCr2S4:1||photoemission spectroscopy (PES):1||METALLIC FERROMAGNETISM:1||GRAPHITE:1||SUSCEPTIBILITY:1||UBE13:1||RCrSb3:1||band JahnTeller:1||Ce3S4:1||TiO2:1||PrBa2Cu3O7delta:1||UNTWINNED PRBA2CU3O7:1||AGNIO2:1||HALFMETALLIC FERROMAGNETS:1||CI:1||Energy gap:1||Photoemission:1||Future applications:1||Photoemission measurements:1||Graphene:1||BANDSTRUCTURE:1||TC:1||superconductivity:1||magnetic semiconductors:1||CMRmanganites:1||thin films:1||spin dynamics:1||highTc superconductors:1||ITINERANTELECTRON FERROMAGNETISM:1||SINGLECRYSTALS:1||CeTe2:1||amorphous magnetic materials:1||EPITAXIAL GRAPHENE:1||LAYERED PNICTIDEOXIDES:1||BOROCARBIDE SUPERCONDUCTORS:1||AUGMENTEDWAVE METHOD:1||METALLIC MAGNET UNISN:1||ORIGIN:1||spectrum rearrangement:1||MEANFIELD THEORY:1||MOLECULEBASED MAGNETS:1||METASTABLE STATE:1||INSULATOR:1||magnetic orderin:1||FCC IRON:1||CeRu2:1||TL2MN2O7:1||isotope effect:1||Perovskitemanganites:1||RECURSION METHOD:1||PERPENDICULAR MAGNETICANISOTROPY:1||quasiparticle spectral density:1||GW:1||MANGANESE FERRITE:1||RESONANCE:1||SeCuO3:1||Optical conductivity:1||MASSLESS DIRAC FERMIONS:1||SCHOTTKYBARRIER:1||electronic structure:15||ELECTRONICSTRUCTURE:11||TRANSITIONMETAL COMPOUNDS:10||METALS:10||photoemission:8||SPECTRA:8||MAGNETORESISTANCE:7||FERROMAGNETISM:7||TRANSPORT:7||TRANSITION:6||FILMS:6||THINFILMS:5||TOTALENERGY CALCULATIONS:5||MAGNETICPROPERTIES:5||SUPERCONDUCTIVITY:5||PR:5||LATTICE:4||STATES:4||SPECTROSCOPY:4||FIELD:4||CRYSTALSTRUCTURE:4||PHOTOEMISSION:4||TEMPERATURE:4||TRANSITIONTEMPERATURE:4||XRAYABSORPTION:4||STATE:4||CU:4||BASISSET:4||XAS:4||CRYSTALS:3||EXCITATIONS:3||MOTTHUBBARD SYSTEMS:3||HIGHENERGY SPIN:3||halfmetal:3||INSULATORS:3||LA2CUO4:3||MODEL:3||FLUCTUATIONS:3||CE:3||double exchange:3||TRANSITIONMETALS:3||RESISTIVITY:3||BORON:3||LA1XCAXMNO3:3||IRON:3||PES:3||ANTIMONIDES:2||MgB2:2||ZR METALLIC GLASSES:2||superconductor:2||CRITICALCURRENT DENSITY:2||CIRCULARDICHROISM:2||SEMICONDUCTORS:2||LOCALIZATION:2||INTRABAND OPTICAL CONDUCTIVITY:2||COLOSSAL MAGNETORESISTANCE:2||OXIDATION:2||EXISTENCE:2||COPPER:2||diboride:2||MAGNESIUMDIBORIDE:2||GAP:2||CE COMPOUNDS:2||CORE POLARIZATION:2||magnetoresistance:2||photoemission spectroscopy:2||electronphonon interaction:2||GETTER:2||PD:2||MAGNETISM:2||FECR2S4:2||SUPERCONDUCTING MGB2:2||WIRES:2||ABSORPTION:2||ENERGY:2||LA1XSRXMNO3:2||CONSTANTS:2||polaron:2||charge ordering:2||SCATTERING:2||XRAY PHOTOEMISSION:2||CeNiSn:2||phase diagram:2||PHOTOELECTRON:2||QUADRUPOLAR:2||perovskitemanganites:2||CO:2||SYSTEMS:2||DOPED ZNO:2||LOWFREQUENCY SOUND:2||LA:2||ELECTRONELECTRON SCATTERING:2||AU:2||DENSITYWAVE INSTABILITY:2||FERMISURFACE:2||hybridization:2||VALENCEBAND SATELLITE:2||SULFUR SPINEL:2||Heusler:2||APPROXIMATION:2||superexchange:2||colossal magnetoresistance:2||ALLOYS:2||DEPENDENCE:2||AG:2||electronic structures:2||AUGERSPECTRA:2||CR:2||PARAMETERS:2||DIFFRACTION:2||SEMICONDUCTORMETAL TRANSITION:1||INTERMEDIATEVALENCE:1||SMB6:1||SRRUO3:1||antiperovskite structure with antipolar nature:1||lowenergy twodimensional phonons:1||anatase TiO2:1||La3S4:1||metalinsulator transitions:1||MNO:1||ELECTRONICSTRUCTURES:1||MAGNETIC CIRCULARDICHROISM:1||Density functional theory:1||CeCo2:1||TOPOLARON CROSSOVER:1||EXCHANGE:1||cuprates:1||high Tc cuprates:1||magnetically ordered materials:1||ZNSE:1||Sr2xKxFeMoO6:1||CDW:1||TeCuO3:1||STRUCTURALPROPERTIES:1||MN:1||screening length:1||amorphous Fe:1||WAVE BASISSET:1||SILICONCARBIDE:1||HIGHPRESSURE:1||electronphonon coupling:1||quenched superconductivity:1||CMR perovskite manganites:1||OXIDE:1||polarons:1||synchrotron radiation:1||FULLERIDES:1||RESONANTPHOTOEMISSION:1||Silicon carbide:1||DFT calculation:1||Hybridized bands:1||GIANT MAGNETORESISTANCE:1||PEROVSKITES:1||Raman spectra:1||EXCHANGE ENHANCEMENT:1||SILICON:1||SR2FEMOO6:1||orbital ordering:1||delafossite:1||TITANIUMDIOXIDE:1||electronic structure of disordered solids:1||YFE2:1||Magnetic polaron:1||NA2TI2SB2O:1||STRONGCOUPLED SUPERCONDUCTORS:1||HEAVYFERMION SYSTEMS:1||firstprinciples calculations:1||MECHANISM:1||UNiSn:1||PHOTONIC BANDGAP:1||SINGLE IMPURITY:1||PHONONSPECTRUM:1||FERMISURFACE TOPOLOGY:1||SUPPRESSION:1||RESONANT PHOTOEMISSION:1||METALDOPED PICENE:1||PHOTOIONIZATION CROSSSECTIONS:1||PHOTOINDUCED FERRIMAGNETIC SYSTEMS:1||LINKAGE ISOMERISM:1||CHARGETRANSFER:1||Bilayer Graphene:1||MAGNETICFIELD:1||SPINWAVES:1||rareearth manganese oxides:1||magnonphonon interaction:1||NACO2O4:1||ENERGYBANDS:1||SELFENERGY:1||GAS:1||Fe0.5Cu0.5Cr2S4:1||scanning photoelectron microscopy (SPEM):1||MAGNETIC PROPERTIES:1||Stoner model:1||AMORPHOUS TRANSITIONMETALS:1||SPINGLASS STATES:1||NI:1||LA3NI2B2N3:1||SOLIDS:1||CEO2:1||BAND THEORY:1||dilute magnetic semiconductor:1||pyrochlore:1||Y1XPRXBA2CU3O7DELTA:1||and electronphonon interactions:1||VIBRATIONS:1||RAY PHOTOEMISSION:1||ALKALI CATION:1||Europium:1||colossal magnetoresistance:1||structural stability:1||ENERGYGAP:1||small polaron:1||DOUBLE EXCHANGE:1||Coulomb correlation:1||magnon:1||phonons:1||ELECTRON FERROMAGNETISM:1||CURIETEMPERATURE:1||ARPES:1||PLANEWAVE METHOD:1||Xray absorption spectroscopy (XAS):1||ROOMTEMPERATURE:1||MONOCHALCOGENIDES:1||HEAT:1||UPDSN:1||MOMENTS:1||XRAY ABSORPTION:1||SEMICONDUCTOR:1||Fermi surface nesting:1||optical phonon:1||disordered system:1||dilute magnetic semiconductors:1||CMR manganites:1||PHONONS:1||LATTICEDYNAMICS:1||OXIDES:1||4fphotoemission:1||permanent magnet:1||pseudogap:1||TRANSPORTPROPERTIES:1||ANTIFERROMAGNET:1||(BI,PB)SRCOO SYSTEM:1||semicore correlation:1||POLARIZATION:1||CRYSTAL:1||spinel:1||Xray magnetic circular dichroism (XMCD):1||magnetocapacitance:1||ANATASE:1||TEMPERATURES:1||Pseudogap:1||INTERFACE:1||SUBSTRATE:1||YNI2B2C:1||SAMARIUM SULFIDE:1||strong swave superconductor:1||DOPED MANGANITE:1||SYMMETRY:1||CENISN:1||resonance mode:1||DISORDERED SYSTEM:1||LITHIUM INTERCALATION:1||CUO2 PLANE:1||SURFACE:1||Delafossite:1||ELECTRICALPROPERTIES:1||NIMNSB:1||PTMNSB:1||ROOMTEMPERATURE FERROMAGNETISM:1||RUBIDIUM MANGANESE HEXACYANOFERRATE:1||COLOSSALMAGNETORESISTANCE:1||FINITE TEMPERATURES:1||LAMNO3:1||FE:1||transitionmetal oxides:1||giant magnetoresistance:1||phonon:1||COPPER OXIDES:1||valence states:1||thermoelectric:1||semiconductor:1||CATION DISTRIBUTION:1||FeCr2S4:1||photoemission spectroscopy (PES):1||METALLIC FERROMAGNETISM:1||GRAPHITE:1||SUSCEPTIBILITY:1||UBE13:1||RCrSb3:1||band JahnTeller:1||Ce3S4:1||TiO2:1||PrBa2Cu3O7delta:1||UNTWINNED PRBA2CU3O7:1||AGNIO2:1||HALFMETALLIC FERROMAGNETS:1||CI:1||Energy gap:1||Photoemission:1||Future applications:1||Photoemission measurements:1||Graphene:1||BANDSTRUCTURE:1||TC:1||superconductivity:1||magnetic semiconductors:1||CMRmanganites:1||thin films:1||spin dynamics:1||highTc superconductors:1||ITINERANTELECTRON FERROMAGNETISM:1||SINGLECRYSTALS:1||CeTe2:1||amorphous magnetic materials:1||EPITAXIAL GRAPHENE:1||LAYERED PNICTIDEOXIDES:1||BOROCARBIDE SUPERCONDUCTORS:1||AUGMENTEDWAVE METHOD:1||METALLIC MAGNET UNISN:1||ORIGIN:1||spectrum rearrangement:1||MEANFIELD THEORY:1||MOLECULEBASED MAGNETS:1||METASTABLE STATE:1||INSULATOR:1||magnetic orderin:1||FCC IRON:1||CeRu2:1||TL2MN2O7:1||isotope effect:1||Perovskitemanganites:1||RECURSION METHOD:1||PERPENDICULAR MAGNETICANISOTROPY:1||quasiparticle spectral density:1||GW:1||MANGANESE FERRITE:1||RESONANCE:1||SeCuO3:1||Optical conductivity:1||MASSLESS DIRAC FERMIONS:1||SCHOTTKYBARRIER:1||electronic structure:15||ELECTRONICSTRUCTURE:11||TRANSITIONMETAL COMPOUNDS:10||METALS:10||photoemission:8||SPECTRA:8||MAGNETORESISTANCE:7||FERROMAGNETISM:7||TRANSPORT:7||TRANSITION:6||FILMS:6||THINFILMS:5||TOTALENERGY CALCULATIONS:5||MAGNETICPROPERTIES:5||SUPERCONDUCTIVITY:5||PR:5||LATTICE:4||STATES:4||SPECTROSCOPY:4||FIELD:4||CRYSTALSTRUCTURE:4||PHOTOEMISSION:4||TEMPERATURE:4||TRANSITIONTEMPERATURE:4||XRAYABSORPTION:4||STATE:4||CU:4||BASISSET:4||XAS:4||CRYSTALS:3||EXCITATIONS:3||MOTTHUBBARD SYSTEMS:3||HIGHENERGY SPIN:3||halfmetal:3||INSULATORS:3||LA2CUO4:3||MODEL:3||FLUCTUATIONS:3||CE:3||double exchange:3||TRANSITIONMETALS:3||RESISTIVITY:3||BORON:3||LA1XCAXMNO3:3||IRON:3||PES:3||ANTIMONIDES:2||MgB2:2||ZR METALLIC GLASSES:2||superconductor:2||CRITICALCURRENT DENSITY:2||CIRCULARDICHROISM:2||SEMICONDUCTORS:2||LOCALIZATION:2||INTRABAND OPTICAL CONDUCTIVITY:2||COLOSSAL MAGNETORESISTANCE:2||OXIDATION:2||EXISTENCE:2||COPPER:2||diboride:2||MAGNESIUMDIBORIDE:2||GAP:2||CE COMPOUNDS:2||CORE POLARIZATION:2||magnetoresistance:2||photoemission spectroscopy:2||electronphonon interaction:2||GETTER:2||PD:2||MAGNETISM:2||FECR2S4:2||SUPERCONDUCTING MGB2:2||WIRES:2||ABSORPTION:2||ENERGY:2||LA1XSRXMNO3:2||CONSTANTS:2||polaron:2||charge ordering:2||SCATTERING:2||XRAY PHOTOEMISSION:2||CeNiSn:2||phase diagram:2||PHOTOELECTRON:2||QUADRUPOLAR:2||perovskitemanganites:2||CO:2||SYSTEMS:2||DOPED ZNO:2||LOWFREQUENCY SOUND:2||LA:2||ELECTRONELECTRON SCATTERING:2||AU:2||DENSITYWAVE INSTABILITY:2||FERMISURFACE:2||hybridization:2||VALENCEBAND SATELLITE:2||SULFUR SPINEL:2||Heusler:2||APPROXIMATION:2||superexchange:2||colossal magnetoresistance:2||ALLOYS:2||DEPENDENCE:2||AG:2||electronic structures:2||AUGERSPECTRA:2||CR:2||PARAMETERS:2||DIFFRACTION:2||SEMICONDUCTORMETAL TRANSITION:1||INTERMEDIATEVALENCE:1||SMB6:1||SRRUO3:1||antiperovskite structure with antipolar nature:1||lowenergy twodimensional phonons:1||anatase TiO2:1||La3S4:1||metalinsulator transitions:1||MNO:1||ELECTRONICSTRUCTURES:1||MAGNETIC CIRCULARDICHROISM:1||Density functional theory:1||CeCo2:1||TOPOLARON CROSSOVER:1||EXCHANGE:1||cuprates:1||high Tc cuprates:1||magnetically ordered materials:1||ZNSE:1||Sr2xKxFeMoO6:1||CDW:1||TeCuO3:1||STRUCTURALPROPERTIES:1||MN:1||screening length:1||amorphous Fe:1||WAVE BASISSET:1||SILICONCARBIDE:1||HIGHPRESSURE:1||electronphonon coupling:1||quenched superconductivity:1||CMR perovskite manganites:1||OXIDE:1||polarons:1||synchrotron radiation:1||FULLERIDES:1||RESONANTPHOTOEMISSION:1||Silicon carbide:1||DFT calculation:1||Hybridized bands:1||GIANT MAGNETORESISTANCE:1||PEROVSKITES:1||Raman spectra:1||EXCHANGE ENHANCEMENT:1||SILICON:1||SR2FEMOO6:1||orbital ordering:1||delafossite:1||TITANIUMDIOXIDE:1||electronic structure of disordered solids:1||YFE2:1||Magnetic polaron:1||NA2TI2SB2O:1||STRONGCOUPLED SUPERCONDUCTORS:1||HEAVYFERMION SYSTEMS:1||firstprinciples calculations:1||MECHANISM:1||UNiSn:1||PHOTONIC BANDGAP:1||SINGLE IMPURITY:1||PHONONSPECTRUM:1||FERMISURFACE TOPOLOGY:1||SUPPRESSION:1||RESONANT PHOTOEMISSION:1||METALDOPED PICENE:1||PHOTOIONIZATION CROSSSECTIONS:1||PHOTOINDUCED FERRIMAGNETIC SYSTEMS:1||LINKAGE ISOMERISM:1||CHARGETRANSFER:1||Bilayer Graphene:1||MAGNETICFIELD:1||SPINWAVES:1||rareearth manganese oxides:1||magnonphonon interaction:1||NACO2O4:1||ENERGYBANDS:1||SELFENERGY:1||GAS:1||Fe0.5Cu0.5Cr2S4:1||scanning photoelectron microscopy (SPEM):1||MAGNETIC PROPERTIES:1||Stoner model:1||AMORPHOUS TRANSITIONMETALS:1||SPINGLASS STATES:1||NI:1||LA3NI2B2N3:1||SOLIDS:1||CEO2:1||BAND THEORY:1||dilute magnetic semiconductor:1||pyrochlore:1||Y1XPRXBA2CU3O7DELTA:1||and electronphonon interactions:1||VIBRATIONS:1||RAY PHOTOEMISSION:1||ALKALI CATION:1||Europium:1||colossal magnetoresistance:1||structural stability:1||ENERGYGAP:1||small polaron:1||DOUBLE EXCHANGE:1||Coulomb correlation:1||magnon:1||phonons:1||ELECTRON FERROMAGNETISM:1||CURIETEMPERATURE:1||ARPES:1||PLANEWAVE METHOD:1||Xray absorption spectroscopy (XAS):1||ROOMTEMPERATURE:1||MONOCHALCOGENIDES:1||HEAT:1||UPDSN:1||MOMENTS:1||XRAY ABSORPTION:1||SEMICONDUCTOR:1||Fermi surface nesting:1||optical phonon:1||disordered system:1||dilute magnetic semiconductors:1||CMR manganites:1||PHONONS:1||LATTICEDYNAMICS:1||OXIDES:1||4fphotoemission:1||permanent magnet:1||pseudogap:1||TRANSPORTPROPERTIES:1||ANTIFERROMAGNET:1||(BI,PB)SRCOO SYSTEM:1||semicore correlation:1||POLARIZATION:1||CRYSTAL:1||spinel:1||Xray magnetic circular dichroism (XMCD):1||magnetocapacitance:1||ANATASE:1||TEMPERATURES:1||Pseudogap:1||INTERFACE:1||SUBSTRATE:1||YNI2B2C:1||SAMARIUM SULFIDE:1||strong swave superconductor:1||DOPED MANGANITE:1||SYMMETRY:1||CENISN:1||resonance mode:1||DISORDERED SYSTEM:1||LITHIUM INTERCALATION:1||CUO2 PLANE:1||SURFACE:1||Delafossite:1||ELECTRICALPROPERTIES:1||NIMNSB:1||PTMNSB:1||ROOMTEMPERATURE FERROMAGNETISM:1||RUBIDIUM MANGANESE HEXACYANOFERRATE:1||COLOSSALMAGNETORESISTANCE:1||FINITE TEMPERATURES:1||LAMNO3:1||FE:1||transitionmetal oxides:1||giant magnetoresistance:1||phonon:1||COPPER OXIDES:1||valence states:1||thermoelectric:1||semiconductor:1||CATION DISTRIBUTION:1||FeCr2S4:1||photoemission spectroscopy (PES):1||METALLIC FERROMAGNETISM:1||GRAPHITE:1||SUSCEPTIBILITY:1||UBE13:1||RCrSb3:1||band JahnTeller:1||Ce3S4:1||TiO2:1||PrBa2Cu3O7delta:1||UNTWINNED PRBA2CU3O7:1||AGNIO2:1||HALFMETALLIC FERROMAGNETS:1||CI:1||Energy gap:1||Photoemission:1||Future applications:1||Photoemission measurements:1||Graphene:1||BANDSTRUCTURE:1||TC:1||superconductivity:1||magnetic semiconductors:1||CMRmanganites:1||thin films:1||spin dynamics:1||highTc superconductors:1||ITINERANTELECTRON FERROMAGNETISM:1||SINGLECRYSTALS:1||CeTe2:1||amorphous magnetic materials:1||EPITAXIAL GRAPHENE:1||LAYERED PNICTIDEOXIDES:1||BOROCARBIDE SUPERCONDUCTORS:1||AUGMENTEDWAVE METHOD:1||METALLIC MAGNET UNISN:1||ORIGIN:1||spectrum rearrangement:1||MEANFIELD THEORY:1||MOLECULEBASED MAGNETS:1||METASTABLE STATE:1||INSULATOR:1||magnetic orderin:1||FCC IRON:1||CeRu2:1||TL2MN2O7:1||isotope effect:1||Perovskitemanganites:1||RECURSION METHOD:1||PERPENDICULAR MAGNETICANISOTROPY:1||quasiparticle spectral density:1||GW:1||MANGANESE FERRITE:1||RESONANCE:1||SeCuO3:1||Optical conductivity:1||MASSLESS DIRAC FERMIONS:1||SCHOTTKYBARRIER:1||electronic structure:15||ELECTRONICSTRUCTURE:11||TRANSITIONMETAL COMPOUNDS:10||METALS:10||photoemission:8||SPECTRA:8||MAGNETORESISTANCE:7||FERROMAGNETISM:7||TRANSPORT:7||TRANSITION:6||FILMS:6||THINFILMS:5||TOTALENERGY CALCULATIONS:5||MAGNETICPROPERTIES:5||SUPERCONDUCTIVITY:5||PR:5||LATTICE:4||STATES:4||SPECTROSCOPY:4||FIELD:4||CRYSTALSTRUCTURE:4||PHOTOEMISSION:4||TEMPERATURE:4||TRANSITIONTEMPERATURE:4||XRAYABSORPTION:4||STATE:4||CU:4||BASISSET:4||XAS:4||CRYSTALS:3||EXCITATIONS:3||MOTTHUBBARD SYSTEMS:3||HIGHENERGY SPIN:3||halfmetal:3||INSULATORS:3||LA2CUO4:3||MODEL:3||FLUCTUATIONS:3||CE:3||double exchange:3||TRANSITIONMETALS:3||RESISTIVITY:3||BORON:3||LA1XCAXMNO3:3||IRON:3||PES:3||ANTIMONIDES:2||MgB2:2||ZR METALLIC GLASSES:2||superconductor:2||CRITICALCURRENT DENSITY:2||CIRCULARDICHROISM:2||SEMICONDUCTORS:2||LOCALIZATION:2||INTRABAND OPTICAL CONDUCTIVITY:2||COLOSSAL MAGNETORESISTANCE:2||OXIDATION:2||EXISTENCE:2||COPPER:2||diboride:2||MAGNESIUMDIBORIDE:2||GAP:2||CE COMPOUNDS:2||CORE POLARIZATION:2||magnetoresistance:2||photoemission spectroscopy:2||electronphonon interaction:2||GETTER:2||PD:2||MAGNETISM:2||FECR2S4:2||SUPERCONDUCTING MGB2:2||WIRES:2||ABSORPTION:2||ENERGY:2||LA1XSRXMNO3:2||CONSTANTS:2||polaron:2||charge ordering:2||SCATTERING:2||XRAY PHOTOEMISSION:2||CeNiSn:2||phase diagram:2||PHOTOELECTRON:2||QUADRUPOLAR:2||perovskitemanganites:2||CO:2||SYSTEMS:2||DOPED ZNO:2||LOWFREQUENCY SOUND:2||LA:2||ELECTRONELECTRON SCATTERING:2||AU:2||DENSITYWAVE INSTABILITY:2||FERMISURFACE:2||hybridization:2||VALENCEBAND SATELLITE:2||SULFUR SPINEL:2||Heusler:2||APPROXIMATION:2||superexchange:2||colossal magnetoresistance:2||ALLOYS:2||DEPENDENCE:2||AG:2||electronic structures:2||AUGERSPECTRA:2||CR:2||PARAMETERS:2||DIFFRACTION:2||SEMICONDUCTORMETAL TRANSITION:1||INTERMEDIATEVALENCE:1||SMB6:1||SRRUO3:1||antiperovskite structure with antipolar nature:1||lowenergy twodimensional phonons:1||anatase TiO2:1||La3S4:1||metalinsulator transitions:1||MNO:1||ELECTRONICSTRUCTURES:1||MAGNETIC CIRCULARDICHROISM:1||Density functional theory:1||CeCo2:1||TOPOLARON CROSSOVER:1||EXCHANGE:1||cuprates:1||high Tc cuprates:1||magnetically ordered materials:1||ZNSE:1||Sr2xKxFeMoO6:1||CDW:1||TeCuO3:1||STRUCTURALPROPERTIES:1||MN:1||screening length:1||amorphous Fe:1||WAVE BASISSET:1||SILICONCARBIDE:1||HIGHPRESSURE:1||electronphonon coupling:1||quenched superconductivity:1||CMR perovskite manganites:1||OXIDE:1||polarons:1||synchrotron radiation:1||FULLERIDES:1||RESONANTPHOTOEMISSION:1||Silicon carbide:1||DFT calculation:1||Hybridized bands:1||GIANT MAGNETORESISTANCE:1||PEROVSKITES:1||Raman spectra:1||EXCHANGE ENHANCEMENT:1||SILICON:1||SR2FEMOO6:1||orbital ordering:1||delafossite:1||TITANIUMDIOXIDE:1||electronic structure of disordered solids:1||YFE2:1||Magnetic polaron:1||NA2TI2SB2O:1||STRONGCOUPLED SUPERCONDUCTORS:1||HEAVYFERMION SYSTEMS:1||firstprinciples calculations:1||MECHANISM:1||UNiSn:1||PHOTONIC BANDGAP:1||SINGLE IMPURITY:1||PHONONSPECTRUM:1||FERMISURFACE TOPOLOGY:1||SUPPRESSION:1||RESONANT PHOTOEMISSION:1||METALDOPED PICENE:1||PHOTOIONIZATION CROSSSECTIONS:1||PHOTOINDUCED FERRIMAGNETIC SYSTEMS:1||LINKAGE ISOMERISM:1||CHARGETRANSFER:1||Bilayer Graphene:1||MAGNETICFIELD:1||SPINWAVES:1||rareearth manganese oxides:1||magnonphonon interaction:1||NACO2O4:1||ENERGYBANDS:1||SELFENERGY:1||GAS:1||Fe0.5Cu0.5Cr2S4:1||scanning photoelectron microscopy (SPEM):1||MAGNETIC PROPERTIES:1||Stoner model:1||AMORPHOUS TRANSITIONMETALS:1||SPINGLASS STATES:1||NI:1||LA3NI2B2N3:1||SOLIDS:1||CEO2:1||BAND THEORY:1||dilute magnetic semiconductor:1||pyrochlore:1||Y1XPRXBA2CU3O7DELTA:1||and electronphonon interactions:1||VIBRATIONS:1||RAY PHOTOEMISSION:1||ALKALI CATION:1||Europium:1||colossal magnetoresistance:1||structural stability:1||ENERGYGAP:1||small polaron:1||DOUBLE EXCHANGE:1||Coulomb correlation:1||magnon:1||phonons:1||ELECTRON FERROMAGNETISM:1||CURIETEMPERATURE:1||ARPES:1||PLANEWAVE METHOD:1||Xray absorption spectroscopy (XAS):1||ROOMTEMPERATURE:1||MONOCHALCOGENIDES:1||HEAT:1||UPDSN:1||MOMENTS:1||XRAY ABSORPTION:1||SEMICONDUCTOR:1||Fermi surface nesting:1||optical phonon:1||disordered system:1||dilute magnetic semiconductors:1||CMR manganites:1||PHONONS:1||LATTICEDYNAMICS:1||OXIDES:1||4fphotoemission:1||permanent magnet:1||pseudogap:1||TRANSPORTPROPERTIES:1||ANTIFERROMAGNET:1||(BI,PB)SRCOO SYSTEM:1||semicore correlation:1||POLARIZATION:1||CRYSTAL:1||spinel:1||Xray magnetic circular dichroism (XMCD):1||magnetocapacitance:1||ANATASE:1||TEMPERATURES:1||Pseudogap:1||INTERFACE:1||SUBSTRATE:1||YNI2B2C:1||SAMARIUM SULFIDE:1||strong swave superconductor:1||DOPED MANGANITE:1||SYMMETRY:1||CENISN:1||resonance mode:1||DISORDERED SYSTEM:1||LITHIUM INTERCALATION:1||CUO2 PLANE:1||SURFACE:1||Delafossite:1||ELECTRICALPROPERTIES:1||NIMNSB:1||PTMNSB:1||ROOMTEMPERATURE FERROMAGNETISM:1||RUBIDIUM MANGANESE HEXACYANOFERRATE:1||COLOSSALMAGNETORESISTANCE:1||FINITE TEMPERATURES:1||LAMNO3:1||FE:1||transitionmetal oxides:1||giant magnetoresistance:1||phonon:1||COPPER OXIDES:1||valence states:1||thermoelectric:1||semiconductor:1||CATION DISTRIBUTION:1||FeCr2S4:1||photoemission spectroscopy (PES):1||METALLIC FERROMAGNETISM:1||GRAPHITE:1||SUSCEPTIBILITY:1||UBE13:1||RCrSb3:1||band JahnTeller:1||Ce3S4:1||TiO2:1||PrBa2Cu3O7delta:1||UNTWINNED PRBA2CU3O7:1||AGNIO2:1||HALFMETALLIC FERROMAGNETS:1||CI:1||Energy gap:1||Photoemission:1||Future applications:1||Photoemission measurements:1||Graphene:1||BANDSTRUCTURE:1||TC:1||superconductivity:1||magnetic semiconductors:1||CMRmanganites:1||thin films:1||spin dynamics:1||highTc superconductors:1||ITINERANTELECTRON FERROMAGNETISM:1||SINGLECRYSTALS:1||CeTe2:1||amorphous magnetic materials:1||EPITAXIAL GRAPHENE:1||LAYERED PNICTIDEOXIDES:1||BOROCARBIDE SUPERCONDUCTORS:1||AUGMENTEDWAVE METHOD:1||METALLIC MAGNET UNISN:1||ORIGIN:1||spectrum rearrangement:1||MEANFIELD THEORY:1||MOLECULEBASED MAGNETS:1||METASTABLE STATE:1||INSULATOR:1||magnetic orderin:1||FCC IRON:1||CeRu2:1||TL2MN2O7:1||isotope effect:1||Perovskitemanganites:1||RECURSION METHOD:1||PERPENDICULAR MAGNETICANISOTROPY:1||quasiparticle spectral density:1||GW:1||MANGANESE FERRITE:1||RESONANCE:1||SeCuO3:1||Optical conductivity:1||MASSLESS DIRAC FERMIONS:1||SCHOTTKYBARRIER:1||electronic structure:15||ELECTRONICSTRUCTURE:11||TRANSITIONMETAL COMPOUNDS:10||METALS:10||photoemission:8||SPECTRA:8||MAGNETORESISTANCE:7||FERROMAGNETISM:7||TRANSPORT:7||TRANSITION:6||FILMS:6||THINFILMS:5||TOTALENERGY CALCULATIONS:5||MAGNETICPROPERTIES:5||SUPERCONDUCTIVITY:5||PR:5||LATTICE:4||STATES:4||SPECTROSCOPY:4||FIELD:4||CRYSTALSTRUCTURE:4||PHOTOEMISSION:4||TEMPERATURE:4||TRANSITIONTEMPERATURE:4||XRAYABSORPTION:4||STATE:4||CU:4||BASISSET:4||XAS:4||CRYSTALS:3||EXCITATIONS:3||MOTTHUBBARD SYSTEMS:3||HIGHENERGY SPIN:3||halfmetal:3||INSULATORS:3||LA2CUO4:3||MODEL:3||FLUCTUATIONS:3||CE:3||double exchange:3||TRANSITIONMETALS:3||RESISTIVITY:3||BORON:3||LA1XCAXMNO3:3||IRON:3||PES:3||ANTIMONIDES:2||MgB2:2||ZR METALLIC GLASSES:2||superconductor:2||CRITICALCURRENT DENSITY:2||CIRCULARDICHROISM:2||SEMICONDUCTORS:2||LOCALIZATION:2||INTRABAND OPTICAL CONDUCTIVITY:2||COLOSSAL MAGNETORESISTANCE:2||OXIDATION:2||EXISTENCE:2||COPPER:2||diboride:2||MAGNESIUMDIBORIDE:2||GAP:2||CE COMPOUNDS:2||CORE POLARIZATION:2||magnetoresistance:2||photoemission spectroscopy:2||electronphonon interaction:2||GETTER:2||PD:2||MAGNETISM:2||FECR2S4:2||SUPERCONDUCTING MGB2:2||WIRES:2||ABSORPTION:2||ENERGY:2||LA1XSRXMNO3:2||CONSTANTS:2||polaron:2||charge ordering:2||SCATTERING:2||XRAY PHOTOEMISSION:2||CeNiSn:2||phase diagram:2||PHOTOELECTRON:2||QUADRUPOLAR:2||perovskitemanganites:2||CO:2||SYSTEMS:2||DOPED ZNO:2||LOWFREQUENCY SOUND:2||LA:2||ELECTRONELECTRON SCATTERING:2||AU:2||DENSITYWAVE INSTABILITY:2||FERMISURFACE:2||hybridization:2||VALENCEBAND SATELLITE:2||SULFUR SPINEL:2||Heusler:2||APPROXIMATION:2||superexchange:2||colossal magnetoresistance:2||ALLOYS:2||DEPENDENCE:2||AG:2||electronic structures:2||AUGERSPECTRA:2||CR:2||PARAMETERS:2||DIFFRACTION:2||SEMICONDUCTORMETAL TRANSITION:1||INTERMEDIATEVALENCE:1||SMB6:1||SRRUO3:1||antiperovskite structure with antipolar nature:1||lowenergy twodimensional phonons:1||anatase TiO2:1||La3S4:1||metalinsulator transitions:1||MNO:1||ELECTRONICSTRUCTURES:1||MAGNETIC CIRCULARDICHROISM:1||Density functional theory:1||CeCo2:1||TOPOLARON CROSSOVER:1||EXCHANGE:1||cuprates:1||high Tc cuprates:1||magnetically ordered materials:1||ZNSE:1||Sr2xKxFeMoO6:1||CDW:1||TeCuO3:1||STRUCTURALPROPERTIES:1||MN:1||screening length:1||amorphous Fe:1||WAVE BASISSET:1||SILICONCARBIDE:1||HIGHPRESSURE:1||electronphonon coupling:1||quenched superconductivity:1||CMR perovskite manganites:1||OXIDE:1||polarons:1||synchrotron radiation:1||FULLERIDES:1||RESONANTPHOTOEMISSION:1||Silicon carbide:1||DFT calculation:1||Hybridized bands:1||GIANT MAGNETORESISTANCE:1||PEROVSKITES:1||Raman spectra:1||EXCHANGE ENHANCEMENT:1||SILICON:1||SR2FEMOO6:1||orbital ordering:1||delafossite:1||TITANIUMDIOXIDE:1||electronic structure of disordered solids:1||YFE2:1||Magnetic polaron:1||NA2TI2SB2O:1||STRONGCOUPLED SUPERCONDUCTORS:1||HEAVYFERMION SYSTEMS:1||firstprinciples calculations:1||MECHANISM:1||UNiSn:1||PHOTONIC BANDGAP:1||SINGLE IMPURITY:1||PHONONSPECTRUM:1||FERMISURFACE TOPOLOGY:1||SUPPRESSION:1||RESONANT PHOTOEMISSION:1||METALDOPED PICENE:1||PHOTOIONIZATION CROSSSECTIONS:1||PHOTOINDUCED FERRIMAGNETIC SYSTEMS:1||LINKAGE ISOMERISM:1||CHARGETRANSFER:1||Bilayer Graphene:1||MAGNETICFIELD:1||SPINWAVES:1||rareearth manganese oxides:1||magnonphonon interaction:1||NACO2O4:1||ENERGYBANDS:1||SELFENERGY:1||GAS:1||Fe0.5Cu0.5Cr2S4:1||scanning photoelectron microscopy (SPEM):1||MAGNETIC PROPERTIES:1||Stoner model:1||AMORPHOUS TRANSITIONMETALS:1||SPINGLASS STATES:1||NI:1||LA3NI2B2N3:1||SOLIDS:1||CEO2:1||BAND THEORY:1||dilute magnetic semiconductor:1||pyrochlore:1||Y1XPRXBA2CU3O7DELTA:1||and electronphonon interactions:1||VIBRATIONS:1||RAY PHOTOEMISSION:1||ALKALI CATION:1||Europium:1||colossal magnetoresistance:1||structural stability:1||ENERGYGAP:1||small polaron:1||DOUBLE EXCHANGE:1||Coulomb correlation:1||magnon:1||phonons:1||ELECTRON FERROMAGNETISM:1||CURIETEMPERATURE:1||ARPES:1||PLANEWAVE METHOD:1||Xray absorption spectroscopy (XAS):1||ROOMTEMPERATURE:1||MONOCHALCOGENIDES:1||HEAT:1||UPDSN:1||MOMENTS:1||XRAY ABSORPTION:1||SEMICONDUCTOR:1||Fermi surface nesting:1||optical phonon:1||disordered system:1||dilute magnetic semiconductors:1||CMR manganites:1||PHONONS:1||LATTICEDYNAMICS:1||OXIDES:1||4fphotoemission:1||permanent magnet:1||pseudogap:1||TRANSPORTPROPERTIES:1||ANTIFERROMAGNET:1||(BI,PB)SRCOO SYSTEM:1||semicore correlation:1||POLARIZATION:1||CRYSTAL:1||spinel:1||Xray magnetic circular dichroism (XMCD):1||magnetocapacitance:1||ANATASE:1||TEMPERATURES:1||Pseudogap:1||INTERFACE:1||SUBSTRATE:1||YNI2B2C:1||SAMARIUM SULFIDE:1||strong swave superconductor:1||DOPED MANGANITE:1||SYMMETRY:1||CENISN:1||resonance mode:1||DISORDERED SYSTEM:1||LITHIUM INTERCALATION:1||CUO2 PLANE:1||SURFACE:1||Delafossite:1||ELECTRICALPROPERTIES:1||NIMNSB:1||PTMNSB:1||ROOMTEMPERATURE FERROMAGNETISM:1||RUBIDIUM MANGANESE HEXACYANOFERRATE:1||COLOSSALMAGNETORESISTANCE:1||FINITE TEMPERATURES:1||LAMNO3:1||FE:1||transitionmetal oxides:1||giant magnetoresistance:1||phonon:1||COPPER OXIDES:1||valence states:1||thermoelectric:1||semiconductor:1||CATION DISTRIBUTION:1||FeCr2S4:1||photoemission spectroscopy (PES):1||METALLIC FERROMAGNETISM:1||GRAPHITE:1||SUSCEPTIBILITY:1||UBE13:1||RCrSb3:1||band JahnTeller:1||Ce3S4:1||TiO2:1||PrBa2Cu3O7delta:1||UNTWINNED PRBA2CU3O7:1||AGNIO2:1||HALFMETALLIC FERROMAGNETS:1||CI:1||Energy gap:1||Photoemission:1||Future applications:1||Photoemission measurements:1||Graphene:1||BANDSTRUCTURE:1||TC:1||superconductivity:1||magnetic semiconductors:1||CMRmanganites:1||thin films:1||spin dynamics:1||highTc superconductors:1||ITINERANTELECTRON FERROMAGNETISM:1||SINGLECRYSTALS:1||CeTe2:1||amorphous magnetic materials:1||EPITAXIAL GRAPHENE:1||LAYERED PNICTIDEOXIDES:1||BOROCARBIDE SUPERCONDUCTORS:1||AUGMENTEDWAVE METHOD:1||METALLIC MAGNET UNISN:1||ORIGIN:1||spectrum rearrangement:1||MEANFIELD THEORY:1||MOLECULEBASED MAGNETS:1||METASTABLE STATE:1||INSULATOR:1||magnetic orderin:1||FCC IRON:1||CeRu2:1||TL2MN2O7:1||isotope effect:1||Perovskitemanganites:1||RECURSION METHOD:1||PERPENDICULAR MAGNETICANISOTROPY:1||quasiparticle spectral density:1||GW:1||MANGANESE FERRITE:1||RESONANCE:1||SeCuO3:1||Optical conductivity:1||MASSLESS DIRAC FERMIONS:1||SCHOTTKYBARRIER:1||electronic structure:15||ELECTRONICSTRUCTURE:11||TRANSITIONMETAL COMPOUNDS:10||METALS:10||photoemission:8||SPECTRA:8||MAGNETORESISTANCE:7||FERROMAGNETISM:7||TRANSPORT:7||TRANSITION:6||FILMS:6||THINFILMS:5||TOTALENERGY CALCULATIONS:5||MAGNETICPROPERTIES:5||SUPERCONDUCTIVITY:5||PR:5||LATTICE:4||STATES:4||SPECTROSCOPY:4||FIELD:4||CRYSTALSTRUCTURE:4||PHOTOEMISSION:4||TEMPERATURE:4||TRANSITIONTEMPERATURE:4||XRAYABSORPTION:4||STATE:4||CU:4||BASISSET:4||XAS:4||CRYSTALS:3||EXCITATIONS:3||MOTTHUBBARD SYSTEMS:3||HIGHENERGY SPIN:3||halfmetal:3||INSULATORS:3||LA2CUO4:3||MODEL:3||FLUCTUATIONS:3||CE:3||double exchange:3||TRANSITIONMETALS:3||RESISTIVITY:3||BORON:3||LA1XCAXMNO3:3||IRON:3||PES:3||ANTIMONIDES:2||MgB2:2||ZR METALLIC GLASSES:2||superconductor:2||CRITICALCURRENT DENSITY:2||CIRCULARDICHROISM:2||SEMICONDUCTORS:2||LOCALIZATION:2||INTRABAND OPTICAL CONDUCTIVITY:2||COLOSSAL MAGNETORESISTANCE:2||OXIDATION:2||EXISTENCE:2||COPPER:2||diboride:2||MAGNESIUMDIBORIDE:2||GAP:2||CE COMPOUNDS:2||CORE POLARIZATION:2||magnetoresistance:2||photoemission spectroscopy:2||electronphonon interaction:2||GETTER:2||PD:2||MAGNETISM:2||FECR2S4:2||SUPERCONDUCTING MGB2:2||WIRES:2||ABSORPTION:2||ENERGY:2||LA1XSRXMNO3:2||CONSTANTS:2||polaron:2||charge ordering:2||SCATTERING:2||XRAY PHOTOEMISSION:2||CeNiSn:2||phase diagram:2||PHOTOELECTRON:2||QUADRUPOLAR:2||perovskitemanganites:2||CO:2||SYSTEMS:2||DOPED ZNO:2||LOWFREQUENCY SOUND:2||LA:2||ELECTRONELECTRON SCATTERING:2||AU:2||DENSITYWAVE INSTABILITY:2||FERMISURFACE:2||hybridization:2||VALENCEBAND SATELLITE:2||SULFUR SPINEL:2||Heusler:2||APPROXIMATION:2||superexchange:2||colossal magnetoresistance:2||ALLOYS:2||DEPENDENCE:2||AG:2||electronic structures:2||AUGERSPECTRA:2||CR:2||PARAMETERS:2||DIFFRACTION:2||SEMICONDUCTORMETAL TRANSITION:1||INTERMEDIATEVALENCE:1||SMB6:1||SRRUO3:1||antiperovskite structure with antipolar nature:1||lowenergy twodimensional phonons:1||anatase TiO2:1||La3S4:1||metalinsulator transitions:1||MNO:1||ELECTRONICSTRUCTURES:1||MAGNETIC CIRCULARDICHROISM:1||Density functional theory:1||CeCo2:1||TOPOLARON CROSSOVER:1||EXCHANGE:1||cuprates:1||high Tc cuprates:1||magnetically ordered materials:1||ZNSE:1||Sr2xKxFeMoO6:1||CDW:1||TeCuO3:1||STRUCTURALPROPERTIES:1||MN:1||screening length:1||amorphous Fe:1||WAVE BASISSET:1||SILICONCARBIDE:1||HIGHPRESSURE:1||electronphonon coupling:1||quenched superconductivity:1||CMR perovskite manganites:1||OXIDE:1||polarons:1||synchrotron radiation:1||FULLERIDES:1||RESONANTPHOTOEMISSION:1||Silicon carbide:1||DFT calculation:1||Hybridized bands:1||GIANT MAGNETORESISTANCE:1||PEROVSKITES:1||Raman spectra:1||EXCHANGE ENHANCEMENT:1||SILICON:1||SR2FEMOO6:1||orbital ordering:1||delafossite:1||TITANIUMDIOXIDE:1||electronic structure of disordered solids:1||YFE2:1||Magnetic polaron:1||NA2TI2SB2O:1||STRONGCOUPLED SUPERCONDUCTORS:1||HEAVYFERMION SYSTEMS:1||firstprinciples calculations:1||MECHANISM:1||UNiSn:1||PHOTONIC BANDGAP:1||SINGLE IMPURITY:1||PHONONSPECTRUM:1||FERMISURFACE TOPOLOGY:1||SUPPRESSION:1||RESONANT PHOTOEMISSION:1||METALDOPED PICENE:1||PHOTOIONIZATION CROSSSECTIONS:1||PHOTOINDUCED FERRIMAGNETIC SYSTEMS:1||LINKAGE ISOMERISM:1||CHARGETRANSFER:1||Bilayer Graphene:1||MAGNETICFIELD:1||SPINWAVES:1||rareearth manganese oxides:1||magnonphonon interaction:1||NACO2O4:1||ENERGYBANDS:1||SELFENERGY:1||GAS:1||Fe0.5Cu0.5Cr2S4:1||scanning photoelectron microscopy (SPEM):1||MAGNETIC PROPERTIES:1||Stoner model:1||AMORPHOUS TRANSITIONMETALS:1||SPINGLASS STATES:1||NI:1||LA3NI2B2N3:1||SOLIDS:1||CEO2:1||BAND THEORY:1||dilute magnetic semiconductor:1||pyrochlore:1||Y1XPRXBA2CU3O7DELTA:1||and electronphonon interactions:1||VIBRATIONS:1||RAY PHOTOEMISSION:1||ALKALI CATION:1||Europium:1||colossal magnetoresistance:1||structural stability:1||ENERGYGAP:1||small polaron:1||DOUBLE EXCHANGE:1||Coulomb correlation:1||magnon:1||phonons:1||ELECTRON FERROMAGNETISM:1||CURIETEMPERATURE:1||ARPES:1||PLANEWAVE METHOD:1||Xray absorption spectroscopy (XAS):1||ROOMTEMPERATURE:1||MONOCHALCOGENIDES:1||HEAT:1||UPDSN:1||MOMENTS:1||XRAY ABSORPTION:1||SEMICONDUCTOR:1||Fermi surface nesting:1||optical phonon:1||disordered system:1||dilute magnetic semiconductors:1||CMR manganites:1||PHONONS:1||LATTICEDYNAMICS:1||OXIDES:1||4fphotoemission:1||permanent magnet:1||pseudogap:1||TRANSPORTPROPERTIES:1||ANTIFERROMAGNET:1||(BI,PB)SRCOO SYSTEM:1||semicore correlation:1||POLARIZATION:1||CRYSTAL:1||spinel:1||Xray magnetic circular dichroism (XMCD):1||magnetocapacitance:1||ANATASE:1||TEMPERATURES:1||Pseudogap:1||INTERFACE:1||SUBSTRATE:1||YNI2B2C:1||SAMARIUM SULFIDE:1||strong swave superconductor:1||DOPED MANGANITE:1||SYMMETRY:1||CENISN:1||resonance mode:1||DISORDERED SYSTEM:1||LITHIUM INTERCALATION:1||CUO2 PLANE:1||SURFACE:1||Delafossite:1||ELECTRICALPROPERTIES:1||NIMNSB:1||PTMNSB:1||ROOMTEMPERATURE FERROMAGNETISM:1||RUBIDIUM MANGANESE HEXACYANOFERRATE:1||COLOSSALMAGNETORESISTANCE:1||FINITE TEMPERATURES:1||LAMNO3:1||FE:1||transitionmetal oxides:1||giant magnetoresistance:1||phonon:1||COPPER OXIDES:1||valence states:1||thermoelectric:1||semiconductor:1||CATION DISTRIBUTION:1||FeCr2S4:1||photoemission spectroscopy (PES):1||METALLIC FERROMAGNETISM:1||GRAPHITE:1||SUSCEPTIBILITY:1||UBE13:1||RCrSb3:1||band JahnTeller:1||Ce3S4:1||TiO2:1||PrBa2Cu3O7delta:1||UNTWINNED PRBA2CU3O7:1||AGNIO2:1||HALFMETALLIC FERROMAGNETS:1||CI:1||Energy gap:1||Photoemission:1||Future applications:1||Photoemission measurements:1||Graphene:1||BANDSTRUCTURE:1||TC:1||superconductivity:1||magnetic semiconductors:1||CMRmanganites:1||thin films:1||spin dynamics:1||highTc superconductors:1||ITINERANTELECTRON FERROMAGNETISM:1||SINGLECRYSTALS:1||CeTe2:1||amorphous magnetic materials:1||EPITAXIAL GRAPHENE:1||LAYERED PNICTIDEOXIDES:1||BOROCARBIDE SUPERCONDUCTORS:1||AUGMENTEDWAVE METHOD:1||METALLIC MAGNET UNISN:1||ORIGIN:1||spectrum rearrangement:1||MEANFIELD THEORY:1||MOLECULEBASED MAGNETS:1||METASTABLE STATE:1||INSULATOR:1||magnetic orderin:1||FCC IRON:1||CeRu2:1||TL2MN2O7:1||isotope effect:1||Perovskitemanganites:1||RECURSION METHOD:1||PERPENDICULAR MAGNETICANISOTROPY:1||quasiparticle spectral density:1||GW:1||MANGANESE FERRITE:1||RESONANCE:1||SeCuO3:1||Optical conductivity:1||MASSLESS DIRAC FERMIONS:1||SCHOTTKYBARRIER:1||electronic structure:15||ELECTRONICSTRUCTURE:11||TRANSITIONMETAL COMPOUNDS:10||METALS:10||photoemission:8||SPECTRA:8||MAGNETORESISTANCE:7||FERROMAGNETISM:7||TRANSPORT:7||TRANSITION:6||FILMS:6||THINFILMS:5||TOTALENERGY CALCULATIONS:5||MAGNETICPROPERTIES:5||SUPERCONDUCTIVITY:5||PR:5||LATTICE:4||STATES:4||SPECTROSCOPY:4||FIELD:4||CRYSTALSTRUCTURE:4||PHOTOEMISSION:4||TEMPERATURE:4||TRANSITIONTEMPERATURE:4||XRAYABSORPTION:4||STATE:4||CU:4||BASISSET:4||XAS:4||CRYSTALS:3||EXCITATIONS:3||MOTTHUBBARD SYSTEMS:3||HIGHENERGY SPIN:3||halfmetal:3||INSULATORS:3||LA2CUO4:3||MODEL:3||FLUCTUATIONS:3||CE:3||double exchange:3||TRANSITIONMETALS:3||RESISTIVITY:3||BORON:3||LA1XCAXMNO3:3||IRON:3||PES:3||ANTIMONIDES:2||MgB2:2||ZR METALLIC GLASSES:2||superconductor:2||CRITICALCURRENT DENSITY:2||CIRCULARDICHROISM:2||SEMICONDUCTORS:2||LOCALIZATION:2||INTRABAND OPTICAL CONDUCTIVITY:2||COLOSSAL MAGNETORESISTANCE:2||OXIDATION:2||EXISTENCE:2||COPPER:2||diboride:2||MAGNESIUMDIBORIDE:2||GAP:2||CE COMPOUNDS:2||CORE POLARIZATION:2||magnetoresistance:2||photoemission spectroscopy:2||electronphonon interaction:2||GETTER:2||PD:2||MAGNETISM:2||FECR2S4:2||SUPERCONDUCTING MGB2:2||WIRES:2||ABSORPTION:2||ENERGY:2||LA1XSRXMNO3:2||CONSTANTS:2||polaron:2||charge ordering:2||SCATTERING:2||XRAY PHOTOEMISSION:2||CeNiSn:2||phase diagram:2||PHOTOELECTRON:2||QUADRUPOLAR:2||perovskitemanganites:2||CO:2||SYSTEMS:2||DOPED ZNO:2||LOWFREQUENCY SOUND:2||LA:2||ELECTRONELECTRON SCATTERING:2||AU:2||DENSITYWAVE INSTABILITY:2||FERMISURFACE:2||hybridization:2||VALENCEBAND SATELLITE:2||SULFUR SPINEL:2||Heusler:2||APPROXIMATION:2||superexchange:2||colossal magnetoresistance:2||ALLOYS:2||DEPENDENCE:2||AG:2||electronic structures:2||AUGERSPECTRA:2||CR:2||PARAMETERS:2||DIFFRACTION:2||SEMICONDUCTORMETAL TRANSITION:1||INTERMEDIATEVALENCE:1||SMB6:1||SRRUO3:1||antiperovskite structure with antipolar nature:1||lowenergy twodimensional phonons:1||anatase TiO2:1||La3S4:1||metalinsulator transitions:1||MNO:1||ELECTRONICSTRUCTURES:1||MAGNETIC CIRCULARDICHROISM:1||Density functional theory:1||CeCo2:1||TOPOLARON CROSSOVER:1||EXCHANGE:1||cuprates:1||high Tc cuprates:1||magnetically ordered materials:1||ZNSE:1||Sr2xKxFeMoO6:1||CDW:1||TeCuO3:1||STRUCTURALPROPERTIES:1||MN:1||screening length:1||amorphous Fe:1||WAVE BASISSET:1||SILICONCARBIDE:1||HIGHPRESSURE:1||electronphonon coupling:1||quenched superconductivity:1||CMR perovskite manganites:1||OXIDE:1||polarons:1||synchrotron radiation:1||FULLERIDES:1||RESONANTPHOTOEMISSION:1||Silicon carbide:1||DFT calculation:1||Hybridized bands:1||GIANT MAGNETORESISTANCE:1||PEROVSKITES:1||Raman spectra:1||EXCHANGE ENHANCEMENT:1||SILICON:1||SR2FEMOO6:1||orbital ordering:1||delafossite:1||TITANIUMDIOXIDE:1||electronic structure of disordered solids:1||YFE2:1||Magnetic polaron:1||NA2TI2SB2O:1||STRONGCOUPLED SUPERCONDUCTORS:1||HEAVYFERMION SYSTEMS:1||firstprinciples calculations:1||MECHANISM:1||UNiSn:1||PHOTONIC BANDGAP:1||SINGLE IMPURITY:1||PHONONSPECTRUM:1||FERMISURFACE TOPOLOGY:1||SUPPRESSION:1||RESONANT PHOTOEMISSION:1||METALDOPED PICENE:1||PHOTOIONIZATION CROSSSECTIONS:1||PHOTOINDUCED FERRIMAGNETIC SYSTEMS:1||LINKAGE ISOMERISM:1||CHARGETRANSFER:1||Bilayer Graphene:1||MAGNETICFIELD:1||SPINWAVES:1||rareearth manganese oxides:1||magnonphonon interaction:1||NACO2O4:1||ENERGYBANDS:1||SELFENERGY:1||GAS:1||Fe0.5Cu0.5Cr2S4:1||scanning photoelectron microscopy (SPEM):1||MAGNETIC PROPERTIES:1||Stoner model:1||AMORPHOUS TRANSITIONMETALS:1||SPINGLASS STATES:1||NI:1||LA3NI2B2N3:1||SOLIDS:1||CEO2:1||BAND THEORY:1||dilute magnetic semiconductor:1||pyrochlore:1||Y1XPRXBA2CU3O7DELTA:1||and electronphonon interactions:1||VIBRATIONS:1||RAY PHOTOEMISSION:1||ALKALI CATION:1||Europium:1||colossal magnetoresistance:1||structural stability:1||ENERGYGAP:1||small polaron:1||DOUBLE EXCHANGE:1||Coulomb correlation:1||magnon:1||phonons:1||ELECTRON FERROMAGNETISM:1||CURIETEMPERATURE:1||ARPES:1||PLANEWAVE METHOD:1||Xray absorption spectroscopy (XAS):1||ROOMTEMPERATURE:1||MONOCHALCOGENIDES:1||HEAT:1||UPDSN:1||MOMENTS:1||XRAY ABSORPTION:1||SEMICONDUCTOR:1||Fermi surface nesting:1||optical phonon:1||disordered system:1||dilute magnetic semiconductors:1||CMR manganites:1||PHONONS:1||LATTICEDYNAMICS:1||OXIDES:1||4fphotoemission:1||permanent magnet:1||pseudogap:1||TRANSPORTPROPERTIES:1||ANTIFERROMAGNET:1||(BI,PB)SRCOO SYSTEM:1||semicore correlation:1||POLARIZATION:1||CRYSTAL:1||spinel:1||Xray magnetic circular dichroism (XMCD):1||magnetocapacitance:1||ANATASE:1||TEMPERATURES:1||Pseudogap:1||INTERFACE:1||SUBSTRATE:1||YNI2B2C:1||SAMARIUM SULFIDE:1||strong swave superconductor:1||DOPED MANGANITE:1||SYMMETRY:1||CENISN:1||resonance mode:1||DISORDERED SYSTEM:1||LITHIUM INTERCALATION:1||CUO2 PLANE:1||SURFACE:1||Delafossite:1||ELECTRICALPROPERTIES:1||NIMNSB:1||PTMNSB:1||ROOMTEMPERATURE FERROMAGNETISM:1||RUBIDIUM MANGANESE HEXACYANOFERRATE:1||COLOSSALMAGNETORESISTANCE:1||FINITE TEMPERATURES:1||LAMNO3:1||FE:1||transitionmetal oxides:1||giant magnetoresistance:1||phonon:1||COPPER OXIDES:1||valence states:1||thermoelectric:1||semiconductor:1||CATION DISTRIBUTION:1||FeCr2S4:1||photoemission spectroscopy (PES):1||METALLIC FERROMAGNETISM:1||GRAPHITE:1||SUSCEPTIBILITY:1||UBE13:1||RCrSb3:1||band JahnTeller:1||Ce3S4:1||TiO2:1||PrBa2Cu3O7delta:1||UNTWINNED PRBA2CU3O7:1||AGNIO2:1||HALFMETALLIC FERROMAGNETS:1||CI:1||Energy gap:1||Photoemission:1||Future applications:1||Photoemission measurements:1||Graphene:1||BANDSTRUCTURE:1||TC:1||superconductivity:1||magnetic semiconductors:1||CMRmanganites:1||thin films:1||spin dynamics:1||highTc superconductors:1||ITINERANTELECTRON FERROMAGNETISM:1||SINGLECRYSTALS:1||CeTe2:1||amorphous magnetic materials:1||EPITAXIAL GRAPHENE:1||LAYERED PNICTIDEOXIDES:1||BOROCARBIDE SUPERCONDUCTORS:1||AUGMENTEDWAVE METHOD:1||METALLIC MAGNET UNISN:1||ORIGIN:1||spectrum rearrangement:1||MEANFIELD THEORY:1||MOLECULEBASED MAGNETS:1||METASTABLE STATE:1||INSULATOR:1||magnetic orderin:1||FCC IRON:1||CeRu2:1||TL2MN2O7:1||isotope effect:1||Perovskitemanganites:1||RECURSION METHOD:1||PERPENDICULAR MAGNETICANISOTROPY:1||quasiparticle spectral density:1||GW:1||MANGANESE FERRITE:1||RESONANCE:1||SeCuO3:1||Optical conductivity:1||MASSLESS DIRAC FERMIONS:1||SCHOTTKYBARRIER:1||electronic structure:15||ELECTRONICSTRUCTURE:11||TRANSITIONMETAL COMPOUNDS:10||METALS:10||photoemission:8||SPECTRA:8||MAGNETORESISTANCE:7||FERROMAGNETISM:7||TRANSPORT:7||TRANSITION:6||FILMS:6||THINFILMS:5||TOTALENERGY CALCULATIONS:5||MAGNETICPROPERTIES:5||SUPERCONDUCTIVITY:5||PR:5||LATTICE:4||STATES:4||SPECTROSCOPY:4||FIELD:4||CRYSTALSTRUCTURE:4||PHOTOEMISSION:4||TEMPERATURE:4||TRANSITIONTEMPERATURE:4||XRAYABSORPTION:4||STATE:4||CU:4||BASISSET:4||XAS:4||CRYSTALS:3||EXCITATIONS:3||MOTTHUBBARD SYSTEMS:3||HIGHENERGY SPIN:3||halfmetal:3||INSULATORS:3||LA2CUO4:3||MODEL:3||FLUCTUATIONS:3||CE:3||double exchange:3||TRANSITIONMETALS:3||RESISTIVITY:3||BORON:3||LA1XCAXMNO3:3||IRON:3||PES:3||ANTIMONIDES:2||MgB2:2||ZR METALLIC GLASSES:2||superconductor:2||CRITICALCURRENT DENSITY:2||CIRCULARDICHROISM:2||SEMICONDUCTORS:2||LOCALIZATION:2||INTRABAND OPTICAL CONDUCTIVITY:2||COLOSSAL MAGNETORESISTANCE:2||OXIDATION:2||EXISTENCE:2||COPPER:2||diboride:2||MAGNESIUMDIBORIDE:2||GAP:2||CE COMPOUNDS:2||CORE POLARIZATION:2||magnetoresistance:2||photoemission spectroscopy:2||electronphonon interaction:2||GETTER:2||PD:2||MAGNETISM:2||FECR2S4:2||SUPERCONDUCTING MGB2:2||WIRES:2||ABSORPTION:2||ENERGY:2||LA1XSRXMNO3:2||CONSTANTS:2||polaron:2||charge ordering:2||SCATTERING:2||XRAY PHOTOEMISSION:2||CeNiSn:2||phase diagram:2||PHOTOELECTRON:2||QUADRUPOLAR:2||perovskitemanganites:2||CO:2||SYSTEMS:2||DOPED ZNO:2||LOWFREQUENCY SOUND:2||LA:2||ELECTRONELECTRON SCATTERING:2||AU:2||DENSITYWAVE INSTABILITY:2||FERMISURFACE:2||hybridization:2||VALENCEBAND SATELLITE:2||SULFUR SPINEL:2||Heusler:2||APPROXIMATION:2||superexchange:2||colossal magnetoresistance:2||ALLOYS:2||DEPENDENCE:2||AG:2||electronic structures:2||AUGERSPECTRA:2||CR:2||PARAMETERS:2||DIFFRACTION:2||SEMICONDUCTORMETAL TRANSITION:1||INTERMEDIATEVALENCE:1||SMB6:1||SRRUO3:1||antiperovskite structure with antipolar nature:1||lowenergy twodimensional phonons:1||anatase TiO2:1||La3S4:1||metalinsulator transitions:1||MNO:1||ELECTRONICSTRUCTURES:1||MAGNETIC CIRCULARDICHROISM:1||Density functional theory:1||CeCo2:1||TOPOLARON CROSSOVER:1||EXCHANGE:1||cuprates:1||high Tc cuprates:1||magnetically ordered materials:1||ZNSE:1||Sr2xKxFeMoO6:1||CDW:1||TeCuO3:1||STRUCTURALPROPERTIES:1||MN:1||screening length:1||amorphous Fe:1||WAVE BASISSET:1||SILICONCARBIDE:1||HIGHPRESSURE:1||electronphonon coupling:1||quenched superconductivity:1||CMR perovskite manganites:1||OXIDE:1||polarons:1||synchrotron radiation:1||FULLERIDES:1||RESONANTPHOTOEMISSION:1||Silicon carbide:1||DFT calculation:1||Hybridized bands:1||GIANT MAGNETORESISTANCE:1||PEROVSKITES:1||Raman spectra:1||EXCHANGE ENHANCEMENT:1||SILICON:1||SR2FEMOO6:1||orbital ordering:1||delafossite:1||TITANIUMDIOXIDE:1||electronic structure of disordered solids:1||YFE2:1||Magnetic polaron:1||NA2TI2SB2O:1||STRONGCOUPLED SUPERCONDUCTORS:1||HEAVYFERMION SYSTEMS:1||firstprinciples calculations:1||MECHANISM:1||UNiSn:1||PHOTONIC BANDGAP:1||SINGLE IMPURITY:1||PHONONSPECTRUM:1||FERMISURFACE TOPOLOGY:1||SUPPRESSION:1||RESONANT PHOTOEMISSION:1||METALDOPED PICENE:1||PHOTOIONIZATION CROSSSECTIONS:1||PHOTOINDUCED FERRIMAGNETIC SYSTEMS:1||LINKAGE ISOMERISM:1||CHARGETRANSFER:1||Bilayer Graphene:1||MAGNETICFIELD:1||SPINWAVES:1||rareearth manganese oxides:1||magnonphonon interaction:1||NACO2O4:1||ENERGYBANDS:1||SELFENERGY:1||GAS:1||Fe0.5Cu0.5Cr2S4:1||scanning photoelectron microscopy (SPEM):1||MAGNETIC PROPERTIES:1||Stoner model:1||AMORPHOUS TRANSITIONMETALS:1||SPINGLASS STATES:1||NI:1||LA3NI2B2N3:1||SOLIDS:1||CEO2:1||BAND THEORY:1||dilute magnetic semiconductor:1||pyrochlore:1||Y1XPRXBA2CU3O7DELTA:1||and electronphonon interactions:1||VIBRATIONS:1||RAY PHOTOEMISSION:1||ALKALI CATION:1||Europium:1||colossal magnetoresistance:1||structural stability:1||ENERGYGAP:1||small polaron:1||DOUBLE EXCHANGE:1||Coulomb correlation:1||magnon:1||phonons:1||ELECTRON FERROMAGNETISM:1||CURIETEMPERATURE:1||ARPES:1||PLANEWAVE METHOD:1||Xray absorption spectroscopy (XAS):1||ROOMTEMPERATURE:1||MONOCHALCOGENIDES:1||HEAT:1||UPDSN:1||MOMENTS:1||XRAY ABSORPTION:1||SEMICONDUCTOR:1||Fermi surface nesting:1||optical phonon:1||disordered system:1||dilute magnetic semiconductors:1||CMR manganites:1||PHONONS:1||LATTICEDYNAMICS:1||OXIDES:1||4fphotoemission:1||permanent magnet:1||pseudogap:1||TRANSPORTPROPERTIES:1||ANTIFERROMAGNET:1||(BI,PB)SRCOO SYSTEM:1||semicore correlation:1||POLARIZATION:1||CRYSTAL:1||spinel:1||Xray magnetic circular dichroism (XMCD):1||magnetocapacitance:1||ANATASE:1||TEMPERATURES:1||Pseudogap:1||INTERFACE:1||SUBSTRATE:1||YNI2B2C:1||SAMARIUM SULFIDE:1||strong swave superconductor:1||DOPED MANGANITE:1||SYMMETRY:1||CENISN:1||resonance mode:1||DISORDERED SYSTEM:1||LITHIUM INTERCALATION:1||CUO2 PLANE:1||SURFACE:1||Delafossite:1||ELECTRICALPROPERTIES:1||NIMNSB:1||PTMNSB:1||ROOMTEMPERATURE FERROMAGNETISM:1||RUBIDIUM MANGANESE HEXACYANOFERRATE:1||COLOSSALMAGNETORESISTANCE:1||FINITE TEMPERATURES:1||LAMNO3:1||FE:1||transitionmetal oxides:1||giant magnetoresistance:1||phonon:1||COPPER OXIDES:1||valence states:1||thermoelectric:1||semiconductor:1||CATION DISTRIBUTION:1||FeCr2S4:1||photoemission spectroscopy (PES):1||METALLIC FERROMAGNETISM:1||GRAPHITE:1||SUSCEPTIBILITY:1||UBE13:1||RCrSb3:1||band JahnTeller:1||Ce3S4:1||TiO2:1||PrBa2Cu3O7delta:1||UNTWINNED PRBA2CU3O7:1||AGNIO2:1||HALFMETALLIC FERROMAGNETS:1||CI:1||Energy gap:1||Photoemission:1||Future applications:1||Photoemission measurements:1||Graphene:1||BANDSTRUCTURE:1||TC:1||superconductivity:1||magnetic semiconductors:1||CMRmanganites:1||thin films:1||spin dynamics:1||highTc superconductors:1||ITINERANTELECTRON FERROMAGNETISM:1||SINGLECRYSTALS:1||CeTe2:1||amorphous magnetic materials:1||EPITAXIAL GRAPHENE:1||LAYERED PNICTIDEOXIDES:1||BOROCARBIDE SUPERCONDUCTORS:1||AUGMENTEDWAVE METHOD:1||METALLIC MAGNET UNISN:1||ORIGIN:1||spectrum rearrangement:1||MEANFIELD THEORY:1||MOLECULEBASED MAGNETS:1||METASTABLE STATE:1||INSULATOR:1||magnetic orderin:1||FCC IRON:1||CeRu2:1||TL2MN2O7:1||isotope effect:1||Perovskitemanganites:1||RECURSION METHOD:1||PERPENDICULAR MAGNETICANISOTROPY:1||quasiparticle spectral density:1||GW:1||MANGANESE FERRITE:1||RESONANCE:1||SeCuO3:1||Optical conductivity:1||MASSLESS DIRAC FERMIONS:1||SCHOTTKYBARRIER:1||electronic structure:15||ELECTRONICSTRUCTURE:11||TRANSITIONMETAL COMPOUNDS:10||METALS:10||photoemission:8||SPECTRA:8||MAGNETORESISTANCE:7||FERROMAGNETISM:7||TRANSPORT:7||TRANSITION:6||FILMS:6||THINFILMS:5||TOTALENERGY CALCULATIONS:5||MAGNETICPROPERTIES:5||SUPERCONDUCTIVITY:5||PR:5||LATTICE:4||STATES:4||SPECTROSCOPY:4||FIELD:4||CRYSTALSTRUCTURE:4||PHOTOEMISSION:4||TEMPERATURE:4||TRANSITIONTEMPERATURE:4||XRAYABSORPTION:4||STATE:4||CU:4||BASISSET:4||XAS:4||CRYSTALS:3||EXCITATIONS:3||MOTTHUBBARD SYSTEMS:3||HIGHENERGY SPIN:3||halfmetal:3||INSULATORS:3||LA2CUO4:3||MODEL:3||FLUCTUATIONS:3||CE:3||double exchange:3||TRANSITIONMETALS:3||RESISTIVITY:3||BORON:3||LA1XCAXMNO3:3||IRON:3||PES:3||ANTIMONIDES:2||MgB2:2||ZR METALLIC GLASSES:2||superconductor:2||CRITICALCURRENT DENSITY:2||CIRCULARDICHROISM:2||SEMICONDUCTORS:2||LOCALIZATION:2||INTRABAND OPTICAL CONDUCTIVITY:2||COLOSSAL MAGNETORESISTANCE:2||OXIDATION:2||EXISTENCE:2||COPPER:2||diboride:2||MAGNESIUMDIBORIDE:2||GAP:2||CE COMPOUNDS:2||CORE POLARIZATION:2||magnetoresistance:2||photoemission spectroscopy:2||electronphonon interaction:2||GETTER:2||PD:2||MAGNETISM:2||FECR2S4:2||SUPERCONDUCTING MGB2:2||WIRES:2||ABSORPTION:2||ENERGY:2||LA1XSRXMNO3:2||CONSTANTS:2||polaron:2||charge ordering:2||SCATTERING:2||XRAY PHOTOEMISSION:2||CeNiSn:2||phase diagram:2||PHOTOELECTRON:2||QUADRUPOLAR:2||perovskitemanganites:2||CO:2||SYSTEMS:2||DOPED ZNO:2||LOWFREQUENCY SOUND:2||LA:2||ELECTRONELECTRON SCATTERING:2||AU:2||DENSITYWAVE INSTABILITY:2||FERMISURFACE:2||hybridization:2||VALENCEBAND SATELLITE:2||SULFUR SPINEL:2||Heusler:2||APPROXIMATION:2||superexchange:2||colossal magnetoresistance:2||ALLOYS:2||DEPENDENCE:2||AG:2||electronic structures:2||AUGERSPECTRA:2||CR:2||PARAMETERS:2||DIFFRACTION:2||SEMICONDUCTORMETAL TRANSITION:1||INTERMEDIATEVALENCE:1||SMB6:1||SRRUO3:1||antiperovskite structure with antipolar nature:1||lowenergy twodimensional phonons:1||anatase TiO2:1||La3S4:1||metalinsulator transitions:1||MNO:1||ELECTRONICSTRUCTURES:1||MAGNETIC CIRCULARDICHROISM:1||Density functional theory:1||CeCo2:1||TOPOLARON CROSSOVER:1||EXCHANGE:1||cuprates:1||high Tc cuprates:1||magnetically ordered materials:1||ZNSE:1||Sr2xKxFeMoO6:1||CDW:1||TeCuO3:1||STRUCTURALPROPERTIES:1||MN:1||screening length:1||amorphous Fe:1||WAVE BASISSET:1||SILICONCARBIDE:1||HIGHPRESSURE:1||electronphonon coupling:1||quenched superconductivity:1||CMR perovskite manganites:1||OXIDE:1||polarons:1||synchrotron radiation:1||FULLERIDES:1||RESONANTPHOTOEMISSION:1||Silicon carbide:1||DFT calculation:1||Hybridized bands:1||GIANT MAGNETORESISTANCE:1||PEROVSKITES:1||Raman spectra:1||EXCHANGE ENHANCEMENT:1||SILICON:1||SR2FEMOO6:1||orbital ordering:1||delafossite:1||TITANIUMDIOXIDE:1||electronic structure of disordered solids:1||YFE2:1||Magnetic polaron:1||NA2TI2SB2O:1||STRONGCOUPLED SUPERCONDUCTORS:1||HEAVYFERMION SYSTEMS:1||firstprinciples calculations:1||MECHANISM:1||UNiSn:1||PHOTONIC BANDGAP:1||SINGLE IMPURITY:1||PHONONSPECTRUM:1||FERMISURFACE TOPOLOGY:1||SUPPRESSION:1||RESONANT PHOTOEMISSION:1||METALDOPED PICENE:1||PHOTOIONIZATION CROSSSECTIONS:1||PHOTOINDUCED FERRIMAGNETIC SYSTEMS:1||LINKAGE ISOMERISM:1||CHARGETRANSFER:1||Bilayer Graphene:1||MAGNETICFIELD:1||SPINWAVES:1||rareearth manganese oxides:1||magnonphonon interaction:1||NACO2O4:1||ENERGYBANDS:1||SELFENERGY:1||GAS:1||Fe0.5Cu0.5Cr2S4:1||scanning photoelectron microscopy (SPEM):1||MAGNETIC PROPERTIES:1||Stoner model:1||AMORPHOUS TRANSITIONMETALS:1||SPINGLASS STATES:1||NI:1||LA3NI2B2N3:1||SOLIDS:1||CEO2:1||BAND THEORY:1||dilute magnetic semiconductor:1||pyrochlore:1||Y1XPRXBA2CU3O7DELTA:1||and electronphonon interactions:1||VIBRATIONS:1||RAY PHOTOEMISSION:1||ALKALI CATION:1||Europium:1||colossal magnetoresistance:1||structural stability:1||ENERGYGAP:1||small polaron:1||DOUBLE EXCHANGE:1||Coulomb correlation:1||magnon:1||phonons:1||ELECTRON FERROMAGNETISM:1||CURIETEMPERATURE:1||ARPES:1||PLANEWAVE METHOD:1||Xray absorption spectroscopy (XAS):1||ROOMTEMPERATURE:1||MONOCHALCOGENIDES:1||HEAT:1||UPDSN:1||MOMENTS:1||XRAY ABSORPTION:1||SEMICONDUCTOR:1||Fermi surface nesting:1||optical phonon:1||disordered system:1||dilute magnetic semiconductors:1||CMR manganites:1||PHONONS:1||LATTICEDYNAMICS:1||OXIDES:1||4fphotoemission:1||permanent magnet:1||pseudogap:1||TRANSPORTPROPERTIES:1||ANTIFERROMAGNET:1||(BI,PB)SRCOO SYSTEM:1||semicore correlation:1||POLARIZATION:1||CRYSTAL:1||spinel:1||Xray magnetic circular dichroism (XMCD):1||magnetocapacitance:1||ANATASE:1||TEMPERATURES:1||Pseudogap:1||INTERFACE:1||SUBSTRATE:1||YNI2B2C:1||SAMARIUM SULFIDE:1||strong swave superconductor:1||DOPED MANGANITE:1||SYMMETRY:1||CENISN:1||resonance mode:1||DISORDERED SYSTEM:1||LITHIUM INTERCALATION:1||CUO2 PLANE:1||SURFACE:1||Delafossite:1||ELECTRICALPROPERTIES:1||NIMNSB:1||PTMNSB:1||ROOMTEMPERATURE FERROMAGNETISM:1||RUBIDIUM MANGANESE HEXACYANOFERRATE:1||COLOSSALMAGNETORESISTANCE:1||FINITE TEMPERATURES:1||LAMNO3:1||FE:1||transitionmetal oxides:1||giant magnetoresistance:1||phonon:1||COPPER OXIDES:1||valence states:1||thermoelectric:1||semiconductor:1||CATION DISTRIBUTION:1||FeCr2S4:1||photoemission spectroscopy (PES):1||METALLIC FERROMAGNETISM:1||GRAPHITE:1||SUSCEPTIBILITY:1||UBE13:1||RCrSb3:1||band JahnTeller:1||Ce3S4:1||TiO2:1||PrBa2Cu3O7delta:1||UNTWINNED PRBA2CU3O7:1||AGNIO2:1||HALFMETALLIC FERROMAGNETS:1||CI:1||Energy gap:1||Photoemission:1||Future applications:1||Photoemission measurements:1||Graphene:1||BANDSTRUCTURE:1||TC:1||superconductivity:1||magnetic semiconductors:1||CMRmanganites:1||thin films:1||spin dynamics:1||highTc superconductors:1||ITINERANTELECTRON FERROMAGNETISM:1||SINGLECRYSTALS:1||CeTe2:1||amorphous magnetic materials:1||EPITAXIAL GRAPHENE:1||LAYERED PNICTIDEOXIDES:1||BOROCARBIDE SUPERCONDUCTORS:1||AUGMENTEDWAVE METHOD:1||METALLIC MAGNET UNISN:1||ORIGIN:1||spectrum rearrangement:1||MEANFIELD THEORY:1||MOLECULEBASED MAGNETS:1||METASTABLE STATE:1||INSULATOR:1||magnetic orderin:1||FCC IRON:1||CeRu2:1||TL2MN2O7:1||isotope effect:1||Perovskitemanganites:1||RECURSION METHOD:1||PERPENDICULAR MAGNETICANISOTROPY:1||quasiparticle spectral density:1||GW:1||MANGANESE FERRITE:1||RESONANCE:1||SeCuO3:1||Optical conductivity:1||MASSLESS DIRAC FERMIONS:1||SCHOTTKYBARRIER:1||electronic structure:15||ELECTRONICSTRUCTURE:11||TRANSITIONMETAL COMPOUNDS:10||METALS:10||photoemission:8||SPECTRA:8||MAGNETORESISTANCE:7||FERROMAGNETISM:7||TRANSPORT:7||TRANSITION:6||FILMS:6||THINFILMS:5||TOTALENERGY CALCULATIONS:5||MAGNETICPROPERTIES:5||SUPERCONDUCTIVITY:5||PR:5||LATTICE:4||STATES:4||SPECTROSCOPY:4||FIELD:4||CRYSTALSTRUCTURE:4||PHOTOEMISSION:4||TEMPERATURE:4||TRANSITIONTEMPERATURE:4||XRAYABSORPTION:4||STATE:4||CU:4||BASISSET:4||XAS:4||CRYSTALS:3||EXCITATIONS:3||MOTTHUBBARD SYSTEMS:3||HIGHENERGY SPIN:3||halfmetal:3||INSULATORS:3||LA2CUO4:3||MODEL:3||FLUCTUATIONS:3||CE:3||double exchange:3||TRANSITIONMETALS:3||RESISTIVITY:3||BORON:3||LA1XCAXMNO3:3||IRON:3||PES:3||ANTIMONIDES:2||MgB2:2||ZR METALLIC GLASSES:2||superconductor:2||CRITICALCURRENT DENSITY:2||CIRCULARDICHROISM:2||SEMICONDUCTORS:2||LOCALIZATION:2||INTRABAND OPTICAL CONDUCTIVITY:2||COLOSSAL MAGNETORESISTANCE:2||OXIDATION:2||EXISTENCE:2||COPPER:2||diboride:2||MAGNESIUMDIBORIDE:2||GAP:2||CE COMPOUNDS:2||CORE POLARIZATION:2||magnetoresistance:2||photoemission spectroscopy:2||electronphonon interaction:2||GETTER:2||PD:2||MAGNETISM:2||FECR2S4:2||SUPERCONDUCTING MGB2:2||WIRES:2||ABSORPTION:2||ENERGY:2||LA1XSRXMNO3:2||CONSTANTS:2||polaron:2||charge ordering:2||SCATTERING:2||XRAY PHOTOEMISSION:2||CeNiSn:2||phase diagram:2||PHOTOELECTRON:2||QUADRUPOLAR:2||perovskitemanganites:2||CO:2||SYSTEMS:2||DOPED ZNO:2||LOWFREQUENCY SOUND:2||LA:2||ELECTRONELECTRON SCATTERING:2||AU:2||DENSITYWAVE INSTABILITY:2||FERMISURFACE:2||hybridization:2||VALENCEBAND SATELLITE:2||SULFUR SPINEL:2||Heusler:2||APPROXIMATION:2||superexchange:2||colossal magnetoresistance:2||ALLOYS:2||DEPENDENCE:2||AG:2||electronic structures:2||AUGERSPECTRA:2||CR:2||PARAMETERS:2||DIFFRACTION:2||SEMICONDUCTORMETAL TRANSITION:1||INTERMEDIATEVALENCE:1||SMB6:1||SRRUO3:1||antiperovskite structure with antipolar nature:1||lowenergy twodimensional phonons:1||anatase TiO2:1||La3S4:1||metalinsulator transitions:1||MNO:1||ELECTRONICSTRUCTURES:1||MAGNETIC CIRCULARDICHROISM:1||Density functional theory:1||CeCo2:1||TOPOLARON CROSSOVER:1||EXCHANGE:1||cuprates:1||high Tc cuprates:1||magnetically ordered materials:1||ZNSE:1||Sr2xKxFeMoO6:1||CDW:1||TeCuO3:1||STRUCTURALPROPERTIES:1||MN:1||screening length:1||amorphous Fe:1||WAVE BASISSET:1||SILICONCARBIDE:1||HIGHPRESSURE:1||electronphonon coupling:1||quenched superconductivity:1||CMR perovskite manganites:1||OXIDE:1||polarons:1||synchrotron radiation:1||FULLERIDES:1||RESONANTPHOTOEMISSION:1||Silicon carbide:1||DFT calculation:1||Hybridized bands:1||GIANT MAGNETORESISTANCE:1||PEROVSKITES:1||Raman spectra:1||EXCHANGE ENHANCEMENT:1||SILICON:1||SR2FEMOO6:1||orbital ordering:1||delafossite:1||TITANIUMDIOXIDE:1||electronic structure of disordered solids:1||YFE2:1||Magnetic polaron:1||NA2TI2SB2O:1||STRONGCOUPLED SUPERCONDUCTORS:1||HEAVYFERMION SYSTEMS:1||firstprinciples calculations:1||MECHANISM:1||UNiSn:1||PHOTONIC BANDGAP:1||SINGLE IMPURITY:1||PHONONSPECTRUM:1||FERMISURFACE TOPOLOGY:1||SUPPRESSION:1||RESONANT PHOTOEMISSION:1||METALDOPED PICENE:1||PHOTOIONIZATION CROSSSECTIONS:1||PHOTOINDUCED FERRIMAGNETIC SYSTEMS:1||LINKAGE ISOMERISM:1||CHARGETRANSFER:1||Bilayer Graphene:1||MAGNETICFIELD:1||SPINWAVES:1||rareearth manganese oxides:1||magnonphonon interaction:1||NACO2O4:1||ENERGYBANDS:1||SELFENERGY:1||GAS:1||Fe0.5Cu0.5Cr2S4:1||scanning photoelectron microscopy (SPEM):1||MAGNETIC PROPERTIES:1||Stoner model:1||AMORPHOUS TRANSITIONMETALS:1||SPINGLASS STATES:1||NI:1||LA3NI2B2N3:1||SOLIDS:1||CEO2:1||BAND THEORY:1||dilute magnetic semiconductor:1||pyrochlore:1||Y1XPRXBA2CU3O7DELTA:1||and electronphonon interactions:1||VIBRATIONS:1||RAY PHOTOEMISSION:1||ALKALI CATION:1||Europium:1||colossal magnetoresistance:1||structural stability:1||ENERGYGAP:1||small polaron:1||DOUBLE EXCHANGE:1||Coulomb correlation:1||magnon:1||phonons:1||ELECTRON FERROMAGNETISM:1||CURIETEMPERATURE:1||ARPES:1||PLANEWAVE METHOD:1||Xray absorption spectroscopy (XAS):1||ROOMTEMPERATURE:1||MONOCHALCOGENIDES:1||HEAT:1||UPDSN:1||MOMENTS:1||XRAY ABSORPTION:1||SEMICONDUCTOR:1||Fermi surface nesting:1||optical phonon:1||disordered system:1||dilute magnetic semiconductors:1||CMR manganites:1||PHONONS:1||LATTICEDYNAMICS:1||OXIDES:1||4fphotoemission:1||permanent magnet:1||pseudogap:1||TRANSPORTPROPERTIES:1||ANTIFERROMAGNET:1||(BI,PB)SRCOO SYSTEM:1||semicore correlation:1||POLARIZATION:1||CRYSTAL:1||spinel:1||Xray magnetic circular dichroism (XMCD):1||magnetocapacitance:1||ANATASE:1||TEMPERATURES:1||Pseudogap:1||INTERFACE:1||SUBSTRATE:1||YNI2B2C:1||SAMARIUM SULFIDE:1||strong swave superconductor:1||DOPED MANGANITE:1||SYMMETRY:1||CENISN:1||resonance mode:1||DISORDERED SYSTEM:1||LITHIUM INTERCALATION:1||CUO2 PLANE:1||SURFACE:1||Delafossite:1||ELECTRICALPROPERTIES:1||NIMNSB:1||PTMNSB:1||ROOMTEMPERATURE FERROMAGNETISM:1||RUBIDIUM MANGANESE HEXACYANOFERRATE:1||COLOSSALMAGNETORESISTANCE:1||FINITE TEMPERATURES:1||LAMNO3:1||FE:1||transitionmetal oxides:1||giant magnetoresistance:1||phonon:1||COPPER OXIDES:1||valence states:1||thermoelectric:1||semiconductor:1||CATION DISTRIBUTION:1||FeCr2S4:1||photoemission spectroscopy (PES):1||METALLIC FERROMAGNETISM:1||GRAPHITE:1||SUSCEPTIBILITY:1||UBE13:1||RCrSb3:1||band JahnTeller:1||Ce3S4:1||TiO2:1||PrBa2Cu3O7delta:1||UNTWINNED PRBA2CU3O7:1||AGNIO2:1||HALFMETALLIC FERROMAGNETS:1||CI:1||Energy gap:1||Photoemission:1||Future applications:1||Photoemission measurements:1||Graphene:1||BANDSTRUCTURE:1||TC:1||superconductivity:1||magnetic semiconductors:1||CMRmanganites:1||thin films:1||spin dynamics:1||highTc superconductors:1||ITINERANTELECTRON FERROMAGNETISM:1||SINGLECRYSTALS:1||CeTe2:1||amorphous magnetic materials:1||EPITAXIAL GRAPHENE:1||LAYERED PNICTIDEOXIDES:1||BOROCARBIDE SUPERCONDUCTORS:1||AUGMENTEDWAVE METHOD:1||METALLIC MAGNET UNISN:1||ORIGIN:1||spectrum rearrangement:1||MEANFIELD THEORY:1||MOLECULEBASED MAGNETS:1||METASTABLE STATE:1||INSULATOR:1||magnetic orderin:1||FCC IRON:1||CeRu2:1||TL2MN2O7:1||isotope effect:1||Perovskitemanganites:1||RECURSION METHOD:1||PERPENDICULAR MAGNETICANISOTROPY:1||quasiparticle spectral density:1||GW:1||MANGANESE FERRITE:1||RESONANCE:1||SeCuO3:1||Optical conductivity:1||MASSLESS DIRAC FERMIONS:1||SCHOTTKYBARRIER:1||electronic structure:15||ELECTRONICSTRUCTURE:11||TRANSITIONMETAL COMPOUNDS:10||METALS:10||photoemission:8||SPECTRA:8||MAGNETORESISTANCE:7||FERROMAGNETISM:7||TRANSPORT:7||TRANSITION:6||FILMS:6||THINFILMS:5||TOTALENERGY CALCULATIONS:5||MAGNETICPROPERTIES:5||SUPERCONDUCTIVITY:5||PR:5||LATTICE:4||STATES:4||SPECTROSCOPY:4||FIELD:4||CRYSTALSTRUCTURE:4||PHOTOEMISSION:4||TEMPERATURE:4||TRANSITIONTEMPERATURE:4||XRAYABSORPTION:4||STATE:4||CU:4||BASISSET:4||XAS:4||CRYSTALS:3||EXCITATIONS:3||MOTTHUBBARD SYSTEMS:3||HIGHENERGY SPIN:3||halfmetal:3||INSULATORS:3||LA2CUO4:3||MODEL:3||FLUCTUATIONS:3||CE:3||double exchange:3||TRANSITIONMETALS:3||RESISTIVITY:3||BORON:3||LA1XCAXMNO3:3||IRON:3||PES:3||ANTIMONIDES:2||MgB2:2||ZR METALLIC GLASSES:2||superconductor:2||CRITICALCURRENT DENSITY:2||CIRCULARDICHROISM:2||SEMICONDUCTORS:2||LOCALIZATION:2||INTRABAND OPTICAL CONDUCTIVITY:2||COLOSSAL MAGNETORESISTANCE:2||OXIDATION:2||EXISTENCE:2||COPPER:2||diboride:2||MAGNESIUMDIBORIDE:2||GAP:2||CE COMPOUNDS:2||CORE POLARIZATION:2||magnetoresistance:2||photoemission spectroscopy:2||electronphonon interaction:2||GETTER:2||PD:2||MAGNETISM:2||FECR2S4:2||SUPERCONDUCTING MGB2:2||WIRES:2||ABSORPTION:2||ENERGY:2||LA1XSRXMNO3:2||CONSTANTS:2||polaron:2||charge ordering:2||SCATTERING:2||XRAY PHOTOEMISSION:2||CeNiSn:2||phase diagram:2||PHOTOELECTRON:2||QUADRUPOLAR:2||perovskitemanganites:2||CO:2||SYSTEMS:2||DOPED ZNO:2||LOWFREQUENCY SOUND:2||LA:2||ELECTRONELECTRON SCATTERING:2||AU:2||DENSITYWAVE INSTABILITY:2||FERMISURFACE:2||hybridization:2||VALENCEBAND SATELLITE:2||SULFUR SPINEL:2||Heusler:2||APPROXIMATION:2||superexchange:2||colossal magnetoresistance:2||ALLOYS:2||DEPENDENCE:2||AG:2||electronic structures:2||AUGERSPECTRA:2||CR:2||PARAMETERS:2||DIFFRACTION:2||SEMICONDUCTORMETAL TRANSITION:1||INTERMEDIATEVALENCE:1||SMB6:1||SRRUO3:1||antiperovskite structure with antipolar nature:1||lowenergy twodimensional phonons:1||anatase TiO2:1||La3S4:1||metalinsulator transitions:1||MNO:1||ELECTRONICSTRUCTURES:1||MAGNETIC CIRCULARDICHROISM:1||Density functional theory:1||CeCo2:1||TOPOLARON CROSSOVER:1||EXCHANGE:1||cuprates:1||high Tc cuprates:1||magnetically ordered materials:1||ZNSE:1||Sr2xKxFeMoO6:1||CDW:1||TeCuO3:1||STRUCTURALPROPERTIES:1||MN:1||screening length:1||amorphous Fe:1||WAVE BASISSET:1||SILICONCARBIDE:1||HIGHPRESSURE:1||electronphonon coupling:1||quenched superconductivity:1||CMR perovskite manganites:1||OXIDE:1||polarons:1||synchrotron radiation:1||FULLERIDES:1||RESONANTPHOTOEMISSION:1||Silicon carbide:1||DFT calculation:1||Hybridized bands:1||GIANT MAGNETORESISTANCE:1||PEROVSKITES:1||Raman spectra:1||EXCHANGE ENHANCEMENT:1||SILICON:1||SR2FEMOO6:1||orbital ordering:1||delafossite:1||TITANIUMDIOXIDE:1||electronic structure of disordered solids:1||YFE2:1||Magnetic polaron:1||NA2TI2SB2O:1||STRONGCOUPLED SUPERCONDUCTORS:1||HEAVYFERMION SYSTEMS:1||firstprinciples calculations:1||MECHANISM:1||UNiSn:1||PHOTONIC BANDGAP:1||SINGLE IMPURITY:1||PHONONSPECTRUM:1||FERMISURFACE TOPOLOGY:1||SUPPRESSION:1||RESONANT PHOTOEMISSION:1||METALDOPED PICENE:1||PHOTOIONIZATION CROSSSECTIONS:1||PHOTOINDUCED FERRIMAGNETIC SYSTEMS:1||LINKAGE ISOMERISM:1||CHARGETRANSFER:1||Bilayer Graphene:1||MAGNETICFIELD:1||SPINWAVES:1||rareearth manganese oxides:1||magnonphonon interaction:1||NACO2O4:1||ENERGYBANDS:1||SELFENERGY:1||GAS:1||Fe0.5Cu0.5Cr2S4:1||scanning photoelectron microscopy (SPEM):1||MAGNETIC PROPERTIES:1||Stoner model:1||AMORPHOUS TRANSITIONMETALS:1||SPINGLASS STATES:1||NI:1||LA3NI2B2N3:1||SOLIDS:1||CEO2:1||BAND THEORY:1||dilute magnetic semiconductor:1||pyrochlore:1||Y1XPRXBA2CU3O7DELTA:1||and electronphonon interactions:1||VIBRATIONS:1||RAY PHOTOEMISSION:1||ALKALI CATION:1||Europium:1||colossal magnetoresistance:1||structural stability:1||ENERGYGAP:1||small polaron:1||DOUBLE EXCHANGE:1||Coulomb correlation:1||magnon:1||phonons:1||ELECTRON FERROMAGNETISM:1||CURIETEMPERATURE:1||ARPES:1||PLANEWAVE METHOD:1||Xray absorption spectroscopy (XAS):1||ROOMTEMPERATURE:1||MONOCHALCOGENIDES:1||HEAT:1||UPDSN:1||MOMENTS:1||XRAY ABSORPTION:1||SEMICONDUCTOR:1||Fermi surface nesting:1||optical phonon:1||disordered system:1||dilute magnetic semiconductors:1||CMR manganites:1||PHONONS:1||LATTICEDYNAMICS:1||OXIDES:1||4fphotoemission:1||permanent magnet:1||pseudogap:1||TRANSPORTPROPERTIES:1||ANTIFERROMAGNET:1||(BI,PB)SRCOO SYSTEM:1||semicore correlation:1||POLARIZATION:1||CRYSTAL:1||spinel:1||Xray magnetic circular dichroism (XMCD):1||magnetocapacitance:1||ANATASE:1||TEMPERATURES:1||Pseudogap:1||INTERFACE:1||SUBSTRATE:1||YNI2B2C:1||SAMARIUM SULFIDE:1||strong swave superconductor:1||DOPED MANGANITE:1||SYMMETRY:1||CENISN:1||resonance mode:1||DISORDERED SYSTEM:1||LITHIUM INTERCALATION:1||CUO2 PLANE:1||SURFACE:1||Delafossite:1||ELECTRICALPROPERTIES:1||NIMNSB:1||PTMNSB:1||ROOMTEMPERATURE FERROMAGNETISM:1||RUBIDIUM MANGANESE HEXACYANOFERRATE:1||COLOSSALMAGNETORESISTANCE:1||FINITE TEMPERATURES:1||LAMNO3:1||FE:1||transitionmetal oxides:1||giant magnetoresistance:1||phonon:1||COPPER OXIDES:1||valence states:1||thermoelectric:1||semiconductor:1||CATION DISTRIBUTION:1||FeCr2S4:1||photoemission spectroscopy (PES):1||METALLIC FERROMAGNETISM:1||GRAPHITE:1||SUSCEPTIBILITY:1||UBE13:1||RCrSb3:1||band JahnTeller:1||Ce3S4:1||TiO2:1||PrBa2Cu3O7delta:1||UNTWINNED PRBA2CU3O7:1||AGNIO2:1||HALFMETALLIC FERROMAGNETS:1||CI:1||Energy gap:1||Photoemission:1||Future applications:1||Photoemission measurements:1||Graphene:1||BANDSTRUCTURE:1||TC:1||superconductivity:1||magnetic semiconductors:1||CMRmanganites:1||thin films:1||spin dynamics:1||highTc superconductors:1||ITINERANTELECTRON FERROMAGNETISM:1||SINGLECRYSTALS:1||CeTe2:1||amorphous magnetic materials:1||EPITAXIAL GRAPHENE:1||LAYERED PNICTIDEOXIDES:1||BOROCARBIDE SUPERCONDUCTORS:1||AUGMENTEDWAVE METHOD:1||METALLIC MAGNET UNISN:1||ORIGIN:1||spectrum rearrangement:1||MEANFIELD THEORY:1||MOLECULEBASED MAGNETS:1||METASTABLE STATE:1||INSULATOR:1||magnetic orderin:1||FCC IRON:1||CeRu2:1||TL2MN2O7:1||isotope effect:1||Perovskitemanganites:1||RECURSION METHOD:1||PERPENDICULAR MAGNETICANISOTROPY:1||quasiparticle spectral density:1||GW:1||MANGANESE FERRITE:1||RESONANCE:1||SeCuO3:1||Optical conductivity:1||MASSLESS DIRAC FERMIONS:1||SCHOTTKYBARRIER:1||electronic structure:15||ELECTRONICSTRUCTURE:11||TRANSITIONMETAL COMPOUNDS:10||METALS:10||photoemission:8||SPECTRA:8||MAGNETORESISTANCE:7||FERROMAGNETISM:7||TRANSPORT:7||TRANSITION:6||FILMS:6||THINFILMS:5||TOTALENERGY CALCULATIONS:5||MAGNETICPROPERTIES:5||SUPERCONDUCTIVITY:5||PR:5||LATTICE:4||STATES:4||SPECTROSCOPY:4||FIELD:4||CRYSTALSTRUCTURE:4||PHOTOEMISSION:4||TEMPERATURE:4||TRANSITIONTEMPERATURE:4||XRAYABSORPTION:4||STATE:4||CU:4||BASISSET:4||XAS:4||CRYSTALS:3||EXCITATIONS:3||MOTTHUBBARD SYSTEMS:3||HIGHENERGY SPIN:3||halfmetal:3||INSULATORS:3||LA2CUO4:3||MODEL:3||FLUCTUATIONS:3||CE:3||double exchange:3||TRANSITIONMETALS:3||RESISTIVITY:3||BORON:3||LA1XCAXMNO3:3||IRON:3||PES:3||ANTIMONIDES:2||MgB2:2||ZR METALLIC GLASSES:2||superconductor:2||CRITICALCURRENT DENSITY:2||CIRCULARDICHROISM:2||SEMICONDUCTORS:2||LOCALIZATION:2||INTRABAND OPTICAL CONDUCTIVITY:2||COLOSSAL MAGNETORESISTANCE:2||OXIDATION:2||EXISTENCE:2||COPPER:2||diboride:2||MAGNESIUMDIBORIDE:2||GAP:2||CE COMPOUNDS:2||CORE POLARIZATION:2||magnetoresistance:2||photoemission spectroscopy:2||electronphonon interaction:2||GETTER:2||PD:2||MAGNETISM:2||FECR2S4:2||SUPERCONDUCTING MGB2:2||WIRES:2||ABSORPTION:2||ENERGY:2||LA1XSRXMNO3:2||CONSTANTS:2||polaron:2||charge ordering:2||SCATTERING:2||XRAY PHOTOEMISSION:2||CeNiSn:2||phase diagram:2||PHOTOELECTRON:2||QUADRUPOLAR:2||perovskitemanganites:2||CO:2||SYSTEMS:2||DOPED ZNO:2||LOWFREQUENCY SOUND:2||LA:2||ELECTRONELECTRON SCATTERING:2||AU:2||DENSITYWAVE INSTABILITY:2||FERMISURFACE:2||hybridization:2||VALENCEBAND SATELLITE:2||SULFUR SPINEL:2||Heusler:2||APPROXIMATION:2||superexchange:2||colossal magnetoresistance:2||ALLOYS:2||DEPENDENCE:2||AG:2||electronic structures:2||AUGERSPECTRA:2||CR:2||PARAMETERS:2||DIFFRACTION:2||SEMICONDUCTORMETAL TRANSITION:1||INTERMEDIATEVALENCE:1||SMB6:1||SRRUO3:1||antiperovskite structure with antipolar nature:1||lowenergy twodimensional phonons:1||anatase TiO2:1||La3S4:1||metalinsulator transitions:1||MNO:1||ELECTRONICSTRUCTURES:1||MAGNETIC CIRCULARDICHROISM:1||Density functional theory:1||CeCo2:1||TOPOLARON CROSSOVER:1||EXCHANGE:1||cuprates:1||high Tc cuprates:1||magnetically ordered materials:1||ZNSE:1||Sr2xKxFeMoO6:1||CDW:1||TeCuO3:1||STRUCTURALPROPERTIES:1||MN:1||screening length:1||amorphous Fe:1||WAVE BASISSET:1||SILICONCARBIDE:1||HIGHPRESSURE:1||electronphonon coupling:1||quenched superconductivity:1||CMR perovskite manganites:1||OXIDE:1||polarons:1||synchrotron radiation:1||FULLERIDES:1||RESONANTPHOTOEMISSION:1||Silicon carbide:1||DFT calculation:1||Hybridized bands:1||GIANT MAGNETORESISTANCE:1||PEROVSKITES:1||Raman spectra:1||EXCHANGE ENHANCEMENT:1||SILICON:1||SR2FEMOO6:1||orbital ordering:1||delafossite:1||TITANIUMDIOXIDE:1||electronic structure of disordered solids:1||YFE2:1||Magnetic polaron:1||NA2TI2SB2O:1||STRONGCOUPLED SUPERCONDUCTORS:1||HEAVYFERMION SYSTEMS:1||firstprinciples calculations:1||MECHANISM:1||UNiSn:1||PHOTONIC BANDGAP:1||SINGLE IMPURITY:1||PHONONSPECTRUM:1||FERMISURFACE TOPOLOGY:1||SUPPRESSION:1||RESONANT PHOTOEMISSION:1||METALDOPED PICENE:1||PHOTOIONIZATION CROSSSECTIONS:1||PHOTOINDUCED FERRIMAGNETIC SYSTEMS:1||LINKAGE ISOMERISM:1||CHARGETRANSFER:1||Bilayer Graphene:1||MAGNETICFIELD:1||SPINWAVES:1||rareearth manganese oxides:1||magnonphonon interaction:1||NACO2O4:1||ENERGYBANDS:1||SELFENERGY:1||GAS:1||Fe0.5Cu0.5Cr2S4:1||scanning photoelectron microscopy (SPEM):1||MAGNETIC PROPERTIES:1||Stoner model:1||AMORPHOUS TRANSITIONMETALS:1||SPINGLASS STATES:1||NI:1||LA3NI2B2N3:1||SOLIDS:1||CEO2:1||BAND THEORY:1||dilute magnetic semiconductor:1||pyrochlore:1||Y1XPRXBA2CU3O7DELTA:1||and electronphonon interactions:1||VIBRATIONS:1||RAY PHOTOEMISSION:1||ALKALI CATION:1||Europium:1||colossal magnetoresistance:1||structural stability:1||ENERGYGAP:1||small polaron:1||DOUBLE EXCHANGE:1||Coulomb correlation:1||magnon:1||phonons:1||ELECTRON FERROMAGNETISM:1||CURIETEMPERATURE:1||ARPES:1||PLANEWAVE METHOD:1||Xray absorption spectroscopy (XAS):1||ROOMTEMPERATURE:1||MONOCHALCOGENIDES:1||HEAT:1||UPDSN:1||MOMENTS:1||XRAY ABSORPTION:1||SEMICONDUCTOR:1||Fermi surface nesting:1||optical phonon:1||disordered system:1||dilute magnetic semiconductors:1||CMR manganites:1||PHONONS:1||LATTICEDYNAMICS:1||OXIDES:1||4fphotoemission:1||permanent magnet:1||pseudogap:1||TRANSPORTPROPERTIES:1||ANTIFERROMAGNET:1||(BI,PB)SRCOO SYSTEM:1||semicore correlation:1||POLARIZATION:1||CRYSTAL:1||spinel:1||Xray magnetic circular dichroism (XMCD):1||magnetocapacitance:1||ANATASE:1||TEMPERATURES:1||Pseudogap:1||INTERFACE:1||SUBSTRATE:1||YNI2B2C:1||SAMARIUM SULFIDE:1||strong swave superconductor:1||DOPED MANGANITE:1||SYMMETRY:1||CENISN:1||resonance mode:1||DISORDERED SYSTEM:1||LITHIUM INTERCALATION:1||CUO2 PLANE:1||SURFACE:1||Delafossite:1||ELECTRICALPROPERTIES:1||NIMNSB:1||PTMNSB:1||ROOMTEMPERATURE FERROMAGNETISM:1||RUBIDIUM MANGANESE HEXACYANOFERRATE:1||COLOSSALMAGNETORESISTANCE:1||FINITE TEMPERATURES:1||LAMNO3:1||FE:1||transitionmetal oxides:1||giant magnetoresistance:1||phonon:1||COPPER OXIDES:1||valence states:1||thermoelectric:1||semiconductor:1||CATION DISTRIBUTION:1||FeCr2S4:1||photoemission spectroscopy (PES):1||METALLIC FERROMAGNETISM:1||GRAPHITE:1||SUSCEPTIBILITY:1||UBE13:1||RCrSb3:1||band JahnTeller:1||Ce3S4:1||TiO2:1||PrBa2Cu3O7delta:1||UNTWINNED PRBA2CU3O7:1||AGNIO2:1||HALFMETALLIC FERROMAGNETS:1||CI:1||Energy gap:1||Photoemission:1||Future applications:1||Photoemission measurements:1||Graphene:1||BANDSTRUCTURE:1||TC:1||superconductivity:1||magnetic semiconductors:1||CMRmanganites:1||thin films:1||spin dynamics:1||highTc superconductors:1||ITINERANTELECTRON FERROMAGNETISM:1||SINGLECRYSTALS:1||CeTe2:1||amorphous magnetic materials:1||EPITAXIAL GRAPHENE:1||LAYERED PNICTIDEOXIDES:1||BOROCARBIDE SUPERCONDUCTORS:1||AUGMENTEDWAVE METHOD:1||METALLIC MAGNET UNISN:1||ORIGIN:1||spectrum rearrangement:1||MEANFIELD THEORY:1||MOLECULEBASED MAGNETS:1||METASTABLE STATE:1||INSULATOR:1||magnetic orderin:1||FCC IRON:1||CeRu2:1||TL2MN2O7:1||isotope effect:1||Perovskitemanganites:1||RECURSION METHOD:1||PERPENDICULAR MAGNETICANISOTROPY:1||quasiparticle spectral density:1||GW:1||MANGANESE FERRITE:1||RESONANCE:1||SeCuO3:1||Optical conductivity:1||MASSLESS DIRAC FERMIONS:1||SCHOTTKYBARRIER:1||electronic structure:15||ELECTRONICSTRUCTURE:11||TRANSITIONMETAL COMPOUNDS:10||METALS:10||photoemission:8||SPECTRA:8||MAGNETORESISTANCE:7||FERROMAGNETISM:7||TRANSPORT:7||TRANSITION:6||FILMS:6||THINFILMS:5||TOTALENERGY CALCULATIONS:5||MAGNETICPROPERTIES:5||SUPERCONDUCTIVITY:5||PR:5||LATTICE:4||STATES:4||SPECTROSCOPY:4||FIELD:4||CRYSTALSTRUCTURE:4||PHOTOEMISSION:4||TEMPERATURE:4||TRANSITIONTEMPERATURE:4||XRAYABSORPTION:4||STATE:4||CU:4||BASISSET:4||XAS:4||CRYSTALS:3||EXCITATIONS:3||MOTTHUBBARD SYSTEMS:3||HIGHENERGY SPIN:3||halfmetal:3||INSULATORS:3||LA2CUO4:3||MODEL:3||FLUCTUATIONS:3||CE:3||double exchange:3||TRANSITIONMETALS:3||RESISTIVITY:3||BORON:3||LA1XCAXMNO3:3||IRON:3||PES:3||ANTIMONIDES:2||MgB2:2||ZR METALLIC GLASSES:2||superconductor:2||CRITICALCURRENT DENSITY:2||CIRCULARDICHROISM:2||SEMICONDUCTORS:2||LOCALIZATION:2||INTRABAND OPTICAL CONDUCTIVITY:2||COLOSSAL MAGNETORESISTANCE:2||OXIDATION:2||EXISTENCE:2||COPPER:2||diboride:2||MAGNESIUMDIBORIDE:2||GAP:2||CE COMPOUNDS:2||CORE POLARIZATION:2||magnetoresistance:2||photoemission spectroscopy:2||electronphonon interaction:2||GETTER:2||PD:2||MAGNETISM:2||FECR2S4:2||SUPERCONDUCTING MGB2:2||WIRES:2||ABSORPTION:2||ENERGY:2||LA1XSRXMNO3:2||CONSTANTS:2||polaron:2||charge ordering:2||SCATTERING:2||XRAY PHOTOEMISSION:2||CeNiSn:2||phase diagram:2||PHOTOELECTRON:2||QUADRUPOLAR:2||perovskitemanganites:2||CO:2||SYSTEMS:2||DOPED ZNO:2||LOWFREQUENCY SOUND:2||LA:2||ELECTRONELECTRON SCATTERING:2||AU:2||DENSITYWAVE INSTABILITY:2||FERMISURFACE:2||hybridization:2||VALENCEBAND SATELLITE:2||SULFUR SPINEL:2||Heusler:2||APPROXIMATION:2||superexchange:2||colossal magnetoresistance:2||ALLOYS:2||DEPENDENCE:2||AG:2||electronic structures:2||AUGERSPECTRA:2||CR:2||PARAMETERS:2||DIFFRACTION:2||SEMICONDUCTORMETAL TRANSITION:1||INTERMEDIATEVALENCE:1||SMB6:1||SRRUO3:1||antiperovskite structure with antipolar nature:1||lowenergy twodimensional phonons:1||anatase TiO2:1||La3S4:1||metalinsulator transitions:1||MNO:1||ELECTRONICSTRUCTURES:1||MAGNETIC CIRCULARDICHROISM:1||Density functional theory:1||CeCo2:1||TOPOLARON CROSSOVER:1||EXCHANGE:1||cuprates:1||high Tc cuprates:1||magnetically ordered materials:1||ZNSE:1||Sr2xKxFeMoO6:1||CDW:1||TeCuO3:1||STRUCTURALPROPERTIES:1||MN:1||screening length:1||amorphous Fe:1||WAVE BASISSET:1||SILICONCARBIDE:1||HIGHPRESSURE:1||electronphonon coupling:1||quenched superconductivity:1||CMR perovskite manganites:1||OXIDE:1||polarons:1||synchrotron radiation:1||FULLERIDES:1||RESONANTPHOTOEMISSION:1||Silicon carbide:1||DFT calculation:1||Hybridized bands:1||GIANT MAGNETORESISTANCE:1||PEROVSKITES:1||Raman spectra:1||EXCHANGE ENHANCEMENT:1||SILICON:1||SR2FEMOO6:1||orbital ordering:1||delafossite:1||TITANIUMDIOXIDE:1||electronic structure of disordered solids:1||YFE2:1||Magnetic polaron:1||NA2TI2SB2O:1||STRONGCOUPLED SUPERCONDUCTORS:1||HEAVYFERMION SYSTEMS:1||firstprinciples calculations:1||MECHANISM:1||UNiSn:1||PHOTONIC BANDGAP:1||SINGLE IMPURITY:1||PHONONSPECTRUM:1||FERMISURFACE TOPOLOGY:1||SUPPRESSION:1||RESONANT PHOTOEMISSION:1||METALDOPED PICENE:1||PHOTOIONIZATION CROSSSECTIONS:1||PHOTOINDUCED FERRIMAGNETIC SYSTEMS:1||LINKAGE ISOMERISM:1||CHARGETRANSFER:1||Bilayer Graphene:1||MAGNETICFIELD:1||SPINWAVES:1||rareearth manganese oxides:1||magnonphonon interaction:1||NACO2O4:1||ENERGYBANDS:1||SELFENERGY:1||GAS:1||Fe0.5Cu0.5Cr2S4:1||scanning photoelectron microscopy (SPEM):1||MAGNETIC PROPERTIES:1||Stoner model:1||AMORPHOUS TRANSITIONMETALS:1||SPINGLASS STATES:1||NI:1||LA3NI2B2N3:1||SOLIDS:1||CEO2:1||BAND THEORY:1||dilute magnetic semiconductor:1||pyrochlore:1||Y1XPRXBA2CU3O7DELTA:1||and electronphonon interactions:1||VIBRATIONS:1||RAY PHOTOEMISSION:1||ALKALI CATION:1||Europium:1||colossal magnetoresistance:1||structural stability:1||ENERGYGAP:1||small polaron:1||DOUBLE EXCHANGE:1||Coulomb correlation:1||magnon:1||phonons:1||ELECTRON FERROMAGNETISM:1||CURIETEMPERATURE:1||ARPES:1||PLANEWAVE METHOD:1||Xray absorption spectroscopy (XAS):1||ROOMTEMPERATURE:1||MONOCHALCOGENIDES:1||HEAT:1||UPDSN:1||MOMENTS:1||XRAY ABSORPTION:1||SEMICONDUCTOR:1||Fermi surface nesting:1||optical phonon:1||disordered system:1||dilute magnetic semiconductors:1||CMR manganites:1||PHONONS:1||LATTICEDYNAMICS:1||OXIDES:1||4fphotoemission:1||permanent magnet:1||pseudogap:1||TRANSPORTPROPERTIES:1||ANTIFERROMAGNET:1||(BI,PB)SRCOO SYSTEM:1||semicore correlation:1||POLARIZATION:1||CRYSTAL:1||spinel:1||Xray magnetic circular dichroism (XMCD):1||magnetocapacitance:1||ANATASE:1||TEMPERATURES:1||Pseudogap:1||INTERFACE:1||SUBSTRATE:1||YNI2B2C:1||SAMARIUM SULFIDE:1||strong swave superconductor:1||DOPED MANGANITE:1||SYMMETRY:1||CENISN:1||resonance mode:1||DISORDERED SYSTEM:1||LITHIUM INTERCALATION:1||CUO2 PLANE:1||SURFACE:1||Delafossite:1||ELECTRICALPROPERTIES:1||NIMNSB:1||PTMNSB:1||ROOMTEMPERATURE FERROMAGNETISM:1||RUBIDIUM MANGANESE HEXACYANOFERRATE:1||COLOSSALMAGNETORESISTANCE:1||FINITE TEMPERATURES:1||LAMNO3:1||FE:1||transitionmetal oxides:1||giant magnetoresistance:1||phonon:1||COPPER OXIDES:1||valence states:1||thermoelectric:1||semiconductor:1||CATION DISTRIBUTION:1||FeCr2S4:1||photoemission spectroscopy (PES):1||METALLIC FERROMAGNETISM:1||GRAPHITE:1||SUSCEPTIBILITY:1||UBE13:1||RCrSb3:1||band JahnTeller:1||Ce3S4:1||TiO2:1||PrBa2Cu3O7delta:1||UNTWINNED PRBA2CU3O7:1||AGNIO2:1||HALFMETALLIC FERROMAGNETS:1||CI:1||Energy gap:1||Photoemission:1||Future applications:1||Photoemission measurements:1||Graphene:1||BANDSTRUCTURE:1||TC:1||superconductivity:1||magnetic semiconductors:1||CMRmanganites:1||thin films:1||spin dynamics:1||highTc superconductors:1||ITINERANTELECTRON FERROMAGNETISM:1||SINGLECRYSTALS:1||CeTe2:1||amorphous magnetic materials:1||EPITAXIAL GRAPHENE:1||LAYERED PNICTIDEOXIDES:1||BOROCARBIDE SUPERCONDUCTORS:1||AUGMENTEDWAVE METHOD:1||METALLIC MAGNET UNISN:1||ORIGIN:1||spectrum rearrangement:1||MEANFIELD THEORY:1||MOLECULEBASED MAGNETS:1||METASTABLE STATE:1||INSULATOR:1||magnetic orderin:1||FCC IRON:1||CeRu2:1||TL2MN2O7:1||isotope effect:1||Perovskitemanganites:1||RECURSION METHOD:1||PERPENDICULAR MAGNETICANISOTROPY:1||quasiparticle spectral density:1||GW:1||MANGANESE FERRITE:1||RESONANCE:1||SeCuO3:1||Optical conductivity:1||MASSLESS DIRAC FERMIONS:1||SCHOTTKYBARRIER:1||electronic structure:15||ELECTRONICSTRUCTURE:11||TRANSITIONMETAL COMPOUNDS:10||METALS:10||photoemission:8||SPECTRA:8||MAGNETORESISTANCE:7||FERROMAGNETISM:7||TRANSPORT:7||TRANSITION:6||FILMS:6||THINFILMS:5||TOTALENERGY CALCULATIONS:5||MAGNETICPROPERTIES:5||SUPERCONDUCTIVITY:5||PR:5||LATTICE:4||STATES:4||SPECTROSCOPY:4||FIELD:4||CRYSTALSTRUCTURE:4||PHOTOEMISSION:4||TEMPERATURE:4||TRANSITIONTEMPERATURE:4||XRAYABSORPTION:4||STATE:4||CU:4||BASISSET:4||XAS:4||CRYSTALS:3||EXCITATIONS:3||MOTTHUBBARD SYSTEMS:3||HIGHENERGY SPIN:3||halfmetal:3||INSULATORS:3||LA2CUO4:3||MODEL:3||FLUCTUATIONS:3||CE:3||double exchange:3||TRANSITIONMETALS:3||RESISTIVITY:3||BORON:3||LA1XCAXMNO3:3||IRON:3||PES:3||ANTIMONIDES:2||MgB2:2||ZR METALLIC GLASSES:2||superconductor:2||CRITICALCURRENT DENSITY:2||CIRCULARDICHROISM:2||SEMICONDUCTORS:2||LOCALIZATION:2||INTRABAND OPTICAL CONDUCTIVITY:2||COLOSSAL MAGNETORESISTANCE:2||OXIDATION:2||EXISTENCE:2||COPPER:2||diboride:2||MAGNESIUMDIBORIDE:2||GAP:2||CE COMPOUNDS:2||CORE POLARIZATION:2||magnetoresistance:2||photoemission spectroscopy:2||electronphonon interaction:2||GETTER:2||PD:2||MAGNETISM:2||FECR2S4:2||SUPERCONDUCTING MGB2:2||WIRES:2||ABSORPTION:2||ENERGY:2||LA1XSRXMNO3:2||CONSTANTS:2||polaron:2||charge ordering:2||SCATTERING:2||XRAY PHOTOEMISSION:2||CeNiSn:2||phase diagram:2||PHOTOELECTRON:2||QUADRUPOLAR:2||perovskitemanganites:2||CO:2||SYSTEMS:2||DOPED ZNO:2||LOWFREQUENCY SOUND:2||LA:2||ELECTRONELECTRON SCATTERING:2||AU:2||DENSITYWAVE INSTABILITY:2||FERMISURFACE:2||hybridization:2||VALENCEBAND SATELLITE:2||SULFUR SPINEL:2||Heusler:2||APPROXIMATION:2||superexchange:2||colossal magnetoresistance:2||ALLOYS:2||DEPENDENCE:2||AG:2||electronic structures:2||AUGERSPECTRA:2||CR:2||PARAMETERS:2||DIFFRACTION:2||SEMICONDUCTORMETAL TRANSITION:1||INTERMEDIATEVALENCE:1||SMB6:1||SRRUO3:1||antiperovskite structure with antipolar nature:1||lowenergy twodimensional phonons:1||anatase TiO2:1||La3S4:1||metalinsulator transitions:1||MNO:1||ELECTRONICSTRUCTURES:1||MAGNETIC CIRCULARDICHROISM:1||Density functional theory:1||CeCo2:1||TOPOLARON CROSSOVER:1||EXCHANGE:1||cuprates:1||high Tc cuprates:1||magnetically ordered materials:1||ZNSE:1||Sr2xKxFeMoO6:1||CDW:1||TeCuO3:1||STRUCTURALPROPERTIES:1||MN:1||screening length:1||amorphous Fe:1||WAVE BASISSET:1||SILICONCARBIDE:1||HIGHPRESSURE:1||electronphonon coupling:1||quenched superconductivity:1||CMR perovskite manganites:1||OXIDE:1||polarons:1||synchrotron radiation:1||FULLERIDES:1||RESONANTPHOTOEMISSION:1||Silicon carbide:1||DFT calculation:1||Hybridized bands:1||GIANT MAGNETORESISTANCE:1||PEROVSKITES:1||Raman spectra:1||EXCHANGE ENHANCEMENT:1||SILICON:1||SR2FEMOO6:1||orbital ordering:1||delafossite:1||TITANIUMDIOXIDE:1||electronic structure of disordered solids:1||YFE2:1||Magnetic polaron:1||NA2TI2SB2O:1||STRONGCOUPLED SUPERCONDUCTORS:1||HEAVYFERMION SYSTEMS:1||firstprinciples calculations:1||MECHANISM:1||UNiSn:1||PHOTONIC BANDGAP:1||SINGLE IMPURITY:1||PHONONSPECTRUM:1||FERMISURFACE TOPOLOGY:1||SUPPRESSION:1||RESONANT PHOTOEMISSION:1||METALDOPED PICENE:1||PHOTOIONIZATION CROSSSECTIONS:1||PHOTOINDUCED FERRIMAGNETIC SYSTEMS:1||LINKAGE ISOMERISM:1||CHARGETRANSFER:1||Bilayer Graphene:1||MAGNETICFIELD:1||SPINWAVES:1||rareearth manganese oxides:1||magnonphonon interaction:1||NACO2O4:1||ENERGYBANDS:1||SELFENERGY:1||GAS:1||Fe0.5Cu0.5Cr2S4:1||scanning photoelectron microscopy (SPEM):1||MAGNETIC PROPERTIES:1||Stoner model:1||AMORPHOUS TRANSITIONMETALS:1||SPINGLASS STATES:1||NI:1||LA3NI2B2N3:1||SOLIDS:1||CEO2:1||BAND THEORY:1||dilute magnetic semiconductor:1||pyrochlore:1||Y1XPRXBA2CU3O7DELTA:1||and electronphonon interactions:1||VIBRATIONS:1||RAY PHOTOEMISSION:1||ALKALI CATION:1||Europium:1||colossal magnetoresistance:1||structural stability:1||ENERGYGAP:1||small polaron:1||DOUBLE EXCHANGE:1||Coulomb correlation:1||magnon:1||phonons:1||ELECTRON FERROMAGNETISM:1||CURIETEMPERATURE:1||ARPES:1||PLANEWAVE METHOD:1||Xray absorption spectroscopy (XAS):1||ROOMTEMPERATURE:1||MONOCHALCOGENIDES:1||HEAT:1||UPDSN:1||MOMENTS:1||XRAY ABSORPTION:1||SEMICONDUCTOR:1||Fermi surface nesting:1||optical phonon:1||disordered system:1||dilute magnetic semiconductors:1||CMR manganites:1||PHONONS:1||LATTICEDYNAMICS:1||OXIDES:1||4fphotoemission:1||permanent magnet:1||pseudogap:1||TRANSPORTPROPERTIES:1||ANTIFERROMAGNET:1||(BI,PB)SRCOO SYSTEM:1||semicore correlation:1||POLARIZATION:1||CRYSTAL:1||spinel:1||Xray magnetic circular dichroism (XMCD):1||magnetocapacitance:1||ANATASE:1||TEMPERATURES:1||Pseudogap:1||INTERFACE:1||SUBSTRATE:1||YNI2B2C:1||SAMARIUM SULFIDE:1||strong swave superconductor:1||DOPED MANGANITE:1||SYMMETRY:1||CENISN:1||resonance mode:1||DISORDERED SYSTEM:1||LITHIUM INTERCALATION:1||CUO2 PLANE:1||SURFACE:1||Delafossite:1||ELECTRICALPROPERTIES:1||NIMNSB:1||PTMNSB:1||ROOMTEMPERATURE FERROMAGNETISM:1||RUBIDIUM MANGANESE HEXACYANOFERRATE:1||COLOSSALMAGNETORESISTANCE:1||FINITE TEMPERATURES:1||LAMNO3:1||FE:1||transitionmetal oxides:1||giant magnetoresistance:1||phonon:1||COPPER OXIDES:1||valence states:1||thermoelectric:1||semiconductor:1||CATION DISTRIBUTION:1||FeCr2S4:1||photoemission spectroscopy (PES):1||METALLIC FERROMAGNETISM:1||GRAPHITE:1||SUSCEPTIBILITY:1||UBE13:1||RCrSb3:1||band JahnTeller:1||Ce3S4:1||TiO2:1||PrBa2Cu3O7delta:1||UNTWINNED PRBA2CU3O7:1||AGNIO2:1||HALFMETALLIC FERROMAGNETS:1||CI:1||Energy gap:1||Photoemission:1||Future applications:1||Photoemission measurements:1||Graphene:1||BANDSTRUCTURE:1||TC:1||superconductivity:1||magnetic semiconductors:1||CMRmanganites:1||thin films:1||spin dynamics:1||highTc superconductors:1||ITINERANTELECTRON FERROMAGNETISM:1||SINGLECRYSTALS:1||CeTe2:1||amorphous magnetic materials:1||EPITAXIAL GRAPHENE:1||LAYERED PNICTIDEOXIDES:1||BOROCARBIDE SUPERCONDUCTORS:1||AUGMENTEDWAVE METHOD:1||METALLIC MAGNET UNISN:1||ORIGIN:1||spectrum rearrangement:1||MEANFIELD THEORY:1||MOLECULEBASED MAGNETS:1||METASTABLE STATE:1||INSULATOR:1||magnetic orderin:1||FCC IRON:1||CeRu2:1||TL2MN2O7:1||isotope effect:1||Perovskitemanganites:1||RECURSION METHOD:1||PERPENDICULAR MAGNETICANISOTROPY:1||quasiparticle spectral density:1||GW:1||MANGANESE FERRITE:1||RESONANCE:1||SeCuO3:1||Optical conductivity:1||MASSLESS DIRAC FERMIONS:1||SCHOTTKYBARRIER:1||electronic structure:15||ELECTRONICSTRUCTURE:11||TRANSITIONMETAL COMPOUNDS:10||METALS:10||photoemission:8||SPECTRA:8||MAGNETORESISTANCE:7||FERROMAGNETISM:7||TRANSPORT:7||TRANSITION:6||FILMS:6||THINFILMS:5||TOTALENERGY CALCULATIONS:5||MAGNETICPROPERTIES:5||SUPERCONDUCTIVITY:5||PR:5||LATTICE:4||STATES:4||SPECTROSCOPY:4||FIELD:4||CRYSTALSTRUCTURE:4||PHOTOEMISSION:4||TEMPERATURE:4||TRANSITIONTEMPERATURE:4||XRAYABSORPTION:4||STATE:4||CU:4||BASISSET:4||XAS:4||CRYSTALS:3||EXCITATIONS:3||MOTTHUBBARD SYSTEMS:3||HIGHENERGY SPIN:3||halfmetal:3||INSULATORS:3||LA2CUO4:3||MODEL:3||FLUCTUATIONS:3||CE:3||double exchange:3||TRANSITIONMETALS:3||RESISTIVITY:3||BORON:3||LA1XCAXMNO3:3||IRON:3||PES:3||ANTIMONIDES:2||MgB2:2||ZR METALLIC GLASSES:2||superconductor:2||CRITICALCURRENT DENSITY:2||CIRCULARDICHROISM:2||SEMICONDUCTORS:2||LOCALIZATION:2||INTRABAND OPTICAL CONDUCTIVITY:2||COLOSSAL MAGNETORESISTANCE:2||OXIDATION:2||EXISTENCE:2||COPPER:2||diboride:2||MAGNESIUMDIBORIDE:2||GAP:2||CE COMPOUNDS:2||CORE POLARIZATION:2||magnetoresistance:2||photoemission spectroscopy:2||electronphonon interaction:2||GETTER:2||PD:2||MAGNETISM:2||FECR2S4:2||SUPERCONDUCTING MGB2:2||WIRES:2||ABSORPTION:2||ENERGY:2||LA1XSRXMNO3:2||CONSTANTS:2||polaron:2||charge ordering:2||SCATTERING:2||XRAY PHOTOEMISSION:2||CeNiSn:2||phase diagram:2||PHOTOELECTRON:2||QUADRUPOLAR:2||perovskitemanganites:2||CO:2||SYSTEMS:2||DOPED ZNO:2||LOWFREQUENCY SOUND:2||LA:2||ELECTRONELECTRON SCATTERING:2||AU:2||DENSITYWAVE INSTABILITY:2||FERMISURFACE:2||hybridization:2||VALENCEBAND SATELLITE:2||SULFUR SPINEL:2||Heusler:2||APPROXIMATION:2||superexchange:2||colossal magnetoresistance:2||ALLOYS:2||DEPENDENCE:2||AG:2||electronic structures:2||AUGERSPECTRA:2||CR:2||PARAMETERS:2||DIFFRACTION:2||SEMICONDUCTORMETAL TRANSITION:1||INTERMEDIATEVALENCE:1||SMB6:1||SRRUO3:1||antiperovskite structure with antipolar nature:1||lowenergy twodimensional phonons:1||anatase TiO2:1||La3S4:1||metalinsulator transitions:1||MNO:1||ELECTRONICSTRUCTURES:1||MAGNETIC CIRCULARDICHROISM:1||Density functional theory:1||CeCo2:1||TOPOLARON CROSSOVER:1||EXCHANGE:1||cuprates:1||high Tc cuprates:1||magnetically ordered materials:1||ZNSE:1||Sr2xKxFeMoO6:1||CDW:1||TeCuO3:1||STRUCTURALPROPERTIES:1||MN:1||screening length:1||amorphous Fe:1||WAVE BASISSET:1||SILICONCARBIDE:1||HIGHPRESSURE:1||electronphonon coupling:1||quenched superconductivity:1||CMR perovskite manganites:1||OXIDE:1||polarons:1||synchrotron radiation:1||FULLERIDES:1||RESONANTPHOTOEMISSION:1||Silicon carbide:1||DFT calculation:1||Hybridized bands:1||GIANT MAGNETORESISTANCE:1||PEROVSKITES:1||Raman spectra:1||EXCHANGE ENHANCEMENT:1||SILICON:1||SR2FEMOO6:1||orbital ordering:1||delafossite:1||TITANIUMDIOXIDE:1||electronic structure of disordered solids:1||YFE2:1||Magnetic polaron:1||NA2TI2SB2O:1||STRONGCOUPLED SUPERCONDUCTORS:1||HEAVYFERMION SYSTEMS:1||firstprinciples calculations:1||MECHANISM:1||UNiSn:1||PHOTONIC BANDGAP:1||SINGLE IMPURITY:1||PHONONSPECTRUM:1||FERMISURFACE TOPOLOGY:1||SUPPRESSION:1||RESONANT PHOTOEMISSION:1||METALDOPED PICENE:1||PHOTOIONIZATION CROSSSECTIONS:1||PHOTOINDUCED FERRIMAGNETIC SYSTEMS:1||LINKAGE ISOMERISM:1||CHARGETRANSFER:1||Bilayer Graphene:1||MAGNETICFIELD:1||SPINWAVES:1||rareearth manganese oxides:1||magnonphonon interaction:1||NACO2O4:1||ENERGYBANDS:1||SELFENERGY:1||GAS:1||Fe0.5Cu0.5Cr2S4:1||scanning photoelectron microscopy (SPEM):1||MAGNETIC PROPERTIES:1||Stoner model:1||AMORPHOUS TRANSITIONMETALS:1||SPINGLASS STATES:1||NI:1||LA3NI2B2N3:1||SOLIDS:1||CEO2:1||BAND THEORY:1||dilute magnetic semiconductor:1||pyrochlore:1||Y1XPRXBA2CU3O7DELTA:1||and electronphonon interactions:1||VIBRATIONS:1||RAY PHOTOEMISSION:1||ALKALI CATION:1||Europium:1||colossal magnetoresistance:1||structural stability:1||ENERGYGAP:1||small polaron:1||DOUBLE EXCHANGE:1||Coulomb correlation:1||magnon:1||phonons:1||ELECTRON FERROMAGNETISM:1||CURIETEMPERATURE:1||ARPES:1||PLANEWAVE METHOD:1||Xray absorption spectroscopy (XAS):1||ROOMTEMPERATURE:1||MONOCHALCOGENIDES:1||HEAT:1||UPDSN:1||MOMENTS:1||XRAY ABSORPTION:1||SEMICONDUCTOR:1||Fermi surface nesting:1||optical phonon:1||disordered system:1||dilute magnetic semiconductors:1||CMR manganites:1||PHONONS:1||LATTICEDYNAMICS:1||OXIDES:1||4fphotoemission:1||permanent magnet:1||pseudogap:1||TRANSPORTPROPERTIES:1||ANTIFERROMAGNET:1||(BI,PB)SRCOO SYSTEM:1||semicore correlation:1||POLARIZATION:1||CRYSTAL:1||spinel:1||Xray magnetic circular dichroism (XMCD):1||magnetocapacitance:1||ANATASE:1||TEMPERATURES:1||Pseudogap:1||INTERFACE:1||SUBSTRATE:1||YNI2B2C:1||SAMARIUM SULFIDE:1||strong swave superconductor:1||DOPED MANGANITE:1||SYMMETRY:1||CENISN:1||resonance mode:1||DISORDERED SYSTEM:1||LITHIUM INTERCALATION:1||CUO2 PLANE:1||SURFACE:1||Delafossite:1||ELECTRICALPROPERTIES:1||NIMNSB:1||PTMNSB:1||ROOMTEMPERATURE FERROMAGNETISM:1||RUBIDIUM MANGANESE HEXACYANOFERRATE:1||COLOSSALMAGNETORESISTANCE:1||FINITE TEMPERATURES:1||LAMNO3:1||FE:1||transitionmetal oxides:1||giant magnetoresistance:1||phonon:1||COPPER OXIDES:1||valence states:1||thermoelectric:1||semiconductor:1||CATION DISTRIBUTION:1||FeCr2S4:1||photoemission spectroscopy (PES):1||METALLIC FERROMAGNETISM:1||GRAPHITE:1||SUSCEPTIBILITY:1||UBE13:1||RCrSb3:1||band JahnTeller:1||Ce3S4:1||TiO2:1||PrBa2Cu3O7delta:1||UNTWINNED PRBA2CU3O7:1||AGNIO2:1||HALFMETALLIC FERROMAGNETS:1||CI:1||Energy gap:1||Photoemission:1||Future applications:1||Photoemission measurements:1||Graphene:1||BANDSTRUCTURE:1||TC:1||superconductivity:1||magnetic semiconductors:1||CMRmanganites:1||thin films:1||spin dynamics:1||highTc superconductors:1||ITINERANTELECTRON FERROMAGNETISM:1||SINGLECRYSTALS:1||CeTe2:1||amorphous magnetic materials:1||EPITAXIAL GRAPHENE:1||LAYERED PNICTIDEOXIDES:1||BOROCARBIDE SUPERCONDUCTORS:1||AUGMENTEDWAVE METHOD:1||METALLIC MAGNET UNISN:1||ORIGIN:1||spectrum rearrangement:1||MEANFIELD THEORY:1||MOLECULEBASED MAGNETS:1||METASTABLE STATE:1||INSULATOR:1||magnetic orderin:1||FCC IRON:1||CeRu2:1||TL2MN2O7:1||isotope effect:1||Perovskitemanganites:1||RECURSION METHOD:1||PERPENDICULAR MAGNETICANISOTROPY:1||quasiparticle spectral density:1||GW:1||MANGANESE FERRITE:1||RESONANCE:1||SeCuO3:1||Optical conductivity:1||MASSLESS DIRAC FERMIONS:1||SCHOTTKYBARRIER:1||electronic structure:15||ELECTRONICSTRUCTURE:11||TRANSITIONMETAL COMPOUNDS:10||METALS:10||photoemission:8||SPECTRA:8||MAGNETORESISTANCE:7||FERROMAGNETISM:7||TRANSPORT:7||TRANSITION:6||FILMS:6||THINFILMS:5||TOTALENERGY CALCULATIONS:5||MAGNETICPROPERTIES:5||SUPERCONDUCTIVITY:5||PR:5||LATTICE:4||STATES:4||SPECTROSCOPY:4||FIELD:4||CRYSTALSTRUCTURE:4||PHOTOEMISSION:4||TEMPERATURE:4||TRANSITIONTEMPERATURE:4||XRAYABSORPTION:4||STATE:4||CU:4||BASISSET:4||XAS:4||CRYSTALS:3||EXCITATIONS:3||MOTTHUBBARD SYSTEMS:3||HIGHENERGY SPIN:3||halfmetal:3||INSULATORS:3||LA2CUO4:3||MODEL:3||FLUCTUATIONS:3||CE:3||double exchange:3||TRANSITIONMETALS:3||RESISTIVITY:3||BORON:3||LA1XCAXMNO3:3||IRON:3||PES:3||ANTIMONIDES:2||MgB2:2||ZR METALLIC GLASSES:2||superconductor:2||CRITICALCURRENT DENSITY:2||CIRCULARDICHROISM:2||SEMICONDUCTORS:2||LOCALIZATION:2||INTRABAND OPTICAL CONDUCTIVITY:2||COLOSSAL MAGNETORESISTANCE:2||OXIDATION:2||EXISTENCE:2||COPPER:2||diboride:2||MAGNESIUMDIBORIDE:2||GAP:2||CE COMPOUNDS:2||CORE POLARIZATION:2||magnetoresistance:2||photoemission spectroscopy:2||electronphonon interaction:2||GETTER:2||PD:2||MAGNETISM:2||FECR2S4:2||SUPERCONDUCTING MGB2:2||WIRES:2||ABSORPTION:2||ENERGY:2||LA1XSRXMNO3:2||CONSTANTS:2||polaron:2||charge ordering:2||SCATTERING:2||XRAY PHOTOEMISSION:2||CeNiSn:2||phase diagram:2||PHOTOELECTRON:2||QUADRUPOLAR:2||perovskitemanganites:2||CO:2||SYSTEMS:2||DOPED ZNO:2||LOWFREQUENCY SOUND:2||LA:2||ELECTRONELECTRON SCATTERING:2||AU:2||DENSITYWAVE INSTABILITY:2||FERMISURFACE:2||hybridization:2||VALENCEBAND SATELLITE:2||SULFUR SPINEL:2||Heusler:2||APPROXIMATION:2||superexchange:2||colossal magnetoresistance:2||ALLOYS:2||DEPENDENCE:2||AG:2||electronic structures:2||AUGERSPECTRA:2||CR:2||PARAMETERS:2||DIFFRACTION:2||SEMICONDUCTORMETAL TRANSITION:1||INTERMEDIATEVALENCE:1||SMB6:1||SRRUO3:1||antiperovskite structure with antipolar nature:1||lowenergy twodimensional phonons:1||anatase TiO2:1||La3S4:1||metalinsulator transitions:1||MNO:1||ELECTRONICSTRUCTURES:1||MAGNETIC CIRCULARDICHROISM:1||Density functional theory:1||CeCo2:1||TOPOLARON CROSSOVER:1||EXCHANGE:1||cuprates:1||high Tc cuprates:1||magnetically ordered materials:1||ZNSE:1||Sr2xKxFeMoO6:1||CDW:1||TeCuO3:1||STRUCTURALPROPERTIES:1||MN:1||screening length:1||amorphous Fe:1||WAVE BASISSET:1||SILICONCARBIDE:1||HIGHPRESSURE:1||electronphonon coupling:1||quenched superconductivity:1||CMR perovskite manganites:1||OXIDE:1||polarons:1||synchrotron radiation:1||FULLERIDES:1||RESONANTPHOTOEMISSION:1||Silicon carbide:1||DFT calculation:1||Hybridized bands:1||GIANT MAGNETORESISTANCE:1||PEROVSKITES:1||Raman spectra:1||EXCHANGE ENHANCEMENT:1||SILICON:1||SR2FEMOO6:1||orbital ordering:1||delafossite:1||TITANIUMDIOXIDE:1||electronic structure of disordered solids:1||YFE2:1||Magnetic polaron:1||NA2TI2SB2O:1||STRONGCOUPLED SUPERCONDUCTORS:1||HEAVYFERMION SYSTEMS:1||firstprinciples calculations:1||MECHANISM:1||UNiSn:1||PHOTONIC BANDGAP:1||SINGLE IMPURITY:1||PHONONSPECTRUM:1||FERMISURFACE TOPOLOGY:1||SUPPRESSION:1||RESONANT PHOTOEMISSION:1||METALDOPED PICENE:1||PHOTOIONIZATION CROSSSECTIONS:1||PHOTOINDUCED FERRIMAGNETIC SYSTEMS:1||LINKAGE ISOMERISM:1||CHARGETRANSFER:1||Bilayer Graphene:1||MAGNETICFIELD:1||SPINWAVES:1||rareearth manganese oxides:1||magnonphonon interaction:1||NACO2O4:1||ENERGYBANDS:1||SELFENERGY:1||GAS:1||Fe0.5Cu0.5Cr2S4:1||scanning photoelectron microscopy (SPEM):1||MAGNETIC PROPERTIES:1||Stoner model:1||AMORPHOUS TRANSITIONMETALS:1||SPINGLASS STATES:1||NI:1||LA3NI2B2N3:1||SOLIDS:1||CEO2:1||BAND THEORY:1||dilute magnetic semiconductor:1||pyrochlore:1||Y1XPRXBA2CU3O7DELTA:1||and electronphonon interactions:1||VIBRATIONS:1||RAY PHOTOEMISSION:1||ALKALI CATION:1||Europium:1||colossal magnetoresistance:1||structural stability:1||ENERGYGAP:1||small polaron:1||DOUBLE EXCHANGE:1||Coulomb correlation:1||magnon:1||phonons:1||ELECTRON FERROMAGNETISM:1||CURIETEMPERATURE:1||ARPES:1||PLANEWAVE METHOD:1||Xray absorption spectroscopy (XAS):1||ROOMTEMPERATURE:1||MONOCHALCOGENIDES:1||HEAT:1||UPDSN:1||MOMENTS:1||XRAY ABSORPTION:1||SEMICONDUCTOR:1||Fermi surface nesting:1||optical phonon:1||disordered system:1||dilute magnetic semiconductors:1||CMR manganites:1||PHONONS:1||LATTICEDYNAMICS:1||OXIDES:1||4fphotoemission:1||permanent magnet:1||pseudogap:1||TRANSPORTPROPERTIES:1||ANTIFERROMAGNET:1||(BI,PB)SRCOO SYSTEM:1||semicore correlation:1||POLARIZATION:1||CRYSTAL:1||spinel:1||Xray magnetic circular dichroism (XMCD):1||magnetocapacitance:1||ANATASE:1||TEMPERATURES:1||Pseudogap:1||INTERFACE:1||SUBSTRATE:1||YNI2B2C:1||SAMARIUM SULFIDE:1||strong swave superconductor:1||DOPED MANGANITE:1||SYMMETRY:1||CENISN:1||resonance mode:1||DISORDERED SYSTEM:1||LITHIUM INTERCALATION:1||CUO2 PLANE:1||SURFACE:1||Delafossite:1||ELECTRICALPROPERTIES:1||NIMNSB:1||PTMNSB:1||ROOMTEMPERATURE FERROMAGNETISM:1||RUBIDIUM MANGANESE HEXACYANOFERRATE:1||COLOSSALMAGNETORESISTANCE:1||FINITE TEMPERATURES:1||LAMNO3:1||FE:1||transitionmetal oxides:1||giant magnetoresistance:1||phonon:1||COPPER OXIDES:1||valence states:1||thermoelectric:1||semiconductor:1||CATION DISTRIBUTION:1||FeCr2S4:1||photoemission spectroscopy (PES):1||METALLIC FERROMAGNETISM:1||GRAPHITE:1||SUSCEPTIBILITY:1||UBE13:1||RCrSb3:1||band JahnTeller:1||Ce3S4:1||TiO2:1||PrBa2Cu3O7delta:1||UNTWINNED PRBA2CU3O7:1||AGNIO2:1||HALFMETALLIC FERROMAGNETS:1||CI:1||Energy gap:1||Photoemission:1||Future applications:1||Photoemission measurements:1||Graphene:1||BANDSTRUCTURE:1||TC:1||superconductivity:1||magnetic semiconductors:1||CMRmanganites:1||thin films:1||spin dynamics:1||highTc superconductors:1||ITINERANTELECTRON FERROMAGNETISM:1||SINGLECRYSTALS:1||CeTe2:1||amorphous magnetic materials:1||EPITAXIAL GRAPHENE:1||LAYERED PNICTIDEOXIDES:1||BOROCARBIDE SUPERCONDUCTORS:1||AUGMENTEDWAVE METHOD:1||METALLIC MAGNET UNISN:1||ORIGIN:1||spectrum rearrangement:1||MEANFIELD THEORY:1||MOLECULEBASED MAGNETS:1||METASTABLE STATE:1||INSULATOR:1||magnetic orderin:1||FCC IRON:1||CeRu2:1||TL2MN2O7:1||isotope effect:1||Perovskitemanganites:1||RECURSION METHOD:1||PERPENDICULAR MAGNETICANISOTROPY:1||quasiparticle spectral density:1||GW:1||MANGANESE FERRITE:1||RESONANCE:1||SeCuO3:1||Optical conductivity:1||MASSLESS DIRAC FERMIONS:1||SCHOTTKYBARRIER:1||electronic structure:15||ELECTRONICSTRUCTURE:11||TRANSITIONMETAL COMPOUNDS:10||METALS:10||photoemission:8||SPECTRA:8||MAGNETORESISTANCE:7||FERROMAGNETISM:7||TRANSPORT:7||TRANSITION:6||FILMS:6||THINFILMS:5||TOTALENERGY CALCULATIONS:5||MAGNETICPROPERTIES:5||SUPERCONDUCTIVITY:5||PR:5||LATTICE:4||STATES:4||SPECTROSCOPY:4||FIELD:4||CRYSTALSTRUCTURE:4||PHOTOEMISSION:4||TEMPERATURE:4||TRANSITIONTEMPERATURE:4||XRAYABSORPTION:4||STATE:4||CU:4||BASISSET:4||XAS:4||CRYSTALS:3||EXCITATIONS:3||MOTTHUBBARD SYSTEMS:3||HIGHENERGY SPIN:3||halfmetal:3||INSULATORS:3||LA2CUO4:3||MODEL:3||FLUCTUATIONS:3||CE:3||double exchange:3||TRANSITIONMETALS:3||RESISTIVITY:3||BORON:3||LA1XCAXMNO3:3||IRON:3||PES:3||ANTIMONIDES:2||MgB2:2||ZR METALLIC GLASSES:2||superconductor:2||CRITICALCURRENT DENSITY:2||CIRCULARDICHROISM:2||SEMICONDUCTORS:2||LOCALIZATION:2||INTRABAND OPTICAL CONDUCTIVITY:2||COLOSSAL MAGNETORESISTANCE:2||OXIDATION:2||EXISTENCE:2||COPPER:2||diboride:2||MAGNESIUMDIBORIDE:2||GAP:2||CE COMPOUNDS:2||CORE POLARIZATION:2||magnetoresistance:2||photoemission spectroscopy:2||electronphonon interaction:2||GETTER:2||PD:2||MAGNETISM:2||FECR2S4:2||SUPERCONDUCTING MGB2:2||WIRES:2||ABSORPTION:2||ENERGY:2||LA1XSRXMNO3:2||CONSTANTS:2||polaron:2||charge ordering:2||SCATTERING:2||XRAY PHOTOEMISSION:2||CeNiSn:2||phase diagram:2||PHOTOELECTRON:2||QUADRUPOLAR:2||perovskitemanganites:2||CO:2||SYSTEMS:2||DOPED ZNO:2||LOWFREQUENCY SOUND:2||LA:2||ELECTRONELECTRON SCATTERING:2||AU:2||DENSITYWAVE INSTABILITY:2||FERMISURFACE:2||hybridization:2||VALENCEBAND SATELLITE:2||SULFUR SPINEL:2||Heusler:2||APPROXIMATION:2||superexchange:2||colossal magnetoresistance:2||ALLOYS:2||DEPENDENCE:2||AG:2||electronic structures:2||AUGERSPECTRA:2||CR:2||PARAMETERS:2||DIFFRACTION:2||SEMICONDUCTORMETAL TRANSITION:1||INTERMEDIATEVALENCE:1||SMB6:1||SRRUO3:1||antiperovskite structure with antipolar nature:1||lowenergy twodimensional phonons:1||anatase TiO2:1||La3S4:1||metalinsulator transitions:1||MNO:1||ELECTRONICSTRUCTURES:1||MAGNETIC CIRCULARDICHROISM:1||Density functional theory:1||CeCo2:1||TOPOLARON CROSSOVER:1||EXCHANGE:1||cuprates:1||high Tc cuprates:1||magnetically ordered materials:1||ZNSE:1||Sr2xKxFeMoO6:1||CDW:1||TeCuO3:1||STRUCTURALPROPERTIES:1||MN:1||screening length:1||amorphous Fe:1||WAVE BASISSET:1||SILICONCARBIDE:1||HIGHPRESSURE:1||electronphonon coupling:1||quenched superconductivity:1||CMR perovskite manganites:1||OXIDE:1||polarons:1||synchrotron radiation:1||FULLERIDES:1||RESONANTPHOTOEMISSION:1||Silicon carbide:1||DFT calculation:1||Hybridized bands:1||GIANT MAGNETORESISTANCE:1||PEROVSKITES:1||Raman spectra:1||EXCHANGE ENHANCEMENT:1||SILICON:1||SR2FEMOO6:1||orbital ordering:1||delafossite:1||TITANIUMDIOXIDE:1||electronic structure of disordered solids:1||YFE2:1||Magnetic polaron:1||NA2TI2SB2O:1||STRONGCOUPLED SUPERCONDUCTORS:1||HEAVYFERMION SYSTEMS:1||firstprinciples calculations:1||MECHANISM:1||UNiSn:1||PHOTONIC BANDGAP:1||SINGLE IMPURITY:1||PHONONSPECTRUM:1||FERMISURFACE TOPOLOGY:1||SUPPRESSION:1||RESONANT PHOTOEMISSION:1||METALDOPED PICENE:1||PHOTOIONIZATION CROSSSECTIONS:1||PHOTOINDUCED FERRIMAGNETIC SYSTEMS:1||LINKAGE ISOMERISM:1||CHARGETRANSFER:1||Bilayer Graphene:1||MAGNETICFIELD:1||SPINWAVES:1||rareearth manganese oxides:1||magnonphonon interaction:1||NACO2O4:1||ENERGYBANDS:1||SELFENERGY:1||GAS:1||Fe0.5Cu0.5Cr2S4:1||scanning photoelectron microscopy (SPEM):1||MAGNETIC PROPERTIES:1||Stoner model:1||AMORPHOUS TRANSITIONMETALS:1||SPINGLASS STATES:1||NI:1||LA3NI2B2N3:1||SOLIDS:1||CEO2:1||BAND THEORY:1||dilute magnetic semiconductor:1||pyrochlore:1||Y1XPRXBA2CU3O7DELTA:1||and electronphonon interactions:1||VIBRATIONS:1||RAY PHOTOEMISSION:1||ALKALI CATION:1||Europium:1||colossal magnetoresistance:1||structural stability:1||ENERGYGAP:1||small polaron:1||DOUBLE EXCHANGE:1||Coulomb correlation:1||magnon:1||phonons:1||ELECTRON FERROMAGNETISM:1||CURIETEMPERATURE:1||ARPES:1||PLANEWAVE METHOD:1||Xray absorption spectroscopy (XAS):1||ROOMTEMPERATURE:1||MONOCHALCOGENIDES:1||HEAT:1||UPDSN:1||MOMENTS:1||XRAY ABSORPTION:1||SEMICONDUCTOR:1||Fermi surface nesting:1||optical phonon:1||disordered system:1||dilute magnetic semiconductors:1||CMR manganites:1||PHONONS:1||LATTICEDYNAMICS:1||OXIDES:1||4fphotoemission:1||permanent magnet:1||pseudogap:1||TRANSPORTPROPERTIES:1||ANTIFERROMAGNET:1||(BI,PB)SRCOO SYSTEM:1||semicore correlation:1||POLARIZATION:1||CRYSTAL:1||spinel:1||Xray magnetic circular dichroism (XMCD):1||magnetocapacitance:1||ANATASE:1||TEMPERATURES:1||Pseudogap:1||INTERFACE:1||SUBSTRATE:1||YNI2B2C:1||SAMARIUM SULFIDE:1||strong swave superconductor:1||DOPED MANGANITE:1||SYMMETRY:1||CENISN:1||resonance mode:1||DISORDERED SYSTEM:1||LITHIUM INTERCALATION:1||CUO2 PLANE:1||SURFACE:1||Delafossite:1||ELECTRICALPROPERTIES:1||NIMNSB:1||PTMNSB:1||ROOMTEMPERATURE FERROMAGNETISM:1||RUBIDIUM MANGANESE HEXACYANOFERRATE:1||COLOSSALMAGNETORESISTANCE:1||FINITE TEMPERATURES:1||LAMNO3:1||FE:1||transitionmetal oxides:1||giant magnetoresistance:1||phonon:1||COPPER OXIDES:1||valence states:1||thermoelectric:1||semiconductor:1||CATION DISTRIBUTION:1||FeCr2S4:1||photoemission spectroscopy (PES):1||METALLIC FERROMAGNETISM:1||GRAPHITE:1||SUSCEPTIBILITY:1||UBE13:1||RCrSb3:1||band JahnTeller:1||Ce3S4:1||TiO2:1||PrBa2Cu3O7delta:1||UNTWINNED PRBA2CU3O7:1||AGNIO2:1||HALFMETALLIC FERROMAGNETS:1||CI:1||Energy gap:1||Photoemission:1||Future applications:1||Photoemission measurements:1||Graphene:1||BANDSTRUCTURE:1||TC:1||superconductivity:1||magnetic semiconductors:1||CMRmanganites:1||thin films:1||spin dynamics:1||highTc superconductors:1||ITINERANTELECTRON FERROMAGNETISM:1||SINGLECRYSTALS:1||CeTe2:1||amorphous magnetic materials:1||EPITAXIAL GRAPHENE:1||LAYERED PNICTIDEOXIDES:1||BOROCARBIDE SUPERCONDUCTORS:1||AUGMENTEDWAVE METHOD:1||METALLIC MAGNET UNISN:1||ORIGIN:1||spectrum rearrangement:1||MEANFIELD THEORY:1||MOLECULEBASED MAGNETS:1||METASTABLE STATE:1||INSULATOR:1||magnetic orderin:1||FCC IRON:1||CeRu2:1||TL2MN2O7:1||isotope effect:1||Perovskitemanganites:1||RECURSION METHOD:1||PERPENDICULAR MAGNETICANISOTROPY:1||quasiparticle spectral density:1||GW:1||MANGANESE FERRITE:1||RESONANCE:1||SeCuO3:1||Optical conductivity:1||MASSLESS DIRAC FERMIONS:1||SCHOTTKYBARRIER:1||electronic structure:15||ELECTRONICSTRUCTURE:11||TRANSITIONMETAL COMPOUNDS:10||METALS:10||photoemission:8||SPECTRA:8||MAGNETORESISTANCE:7||FERROMAGNETISM:7||TRANSPORT:7||TRANSITION:6||FILMS:6||THINFILMS:5||TOTALENERGY CALCULATIONS:5||MAGNETICPROPERTIES:5||SUPERCONDUCTIVITY:5||PR:5||LATTICE:4||STATES:4||SPECTROSCOPY:4||FIELD:4||CRYSTALSTRUCTURE:4||PHOTOEMISSION:4||TEMPERATURE:4||TRANSITIONTEMPERATURE:4||XRAYABSORPTION:4||STATE:4||CU:4||BASISSET:4||XAS:4||CRYSTALS:3||EXCITATIONS:3||MOTTHUBBARD SYSTEMS:3||HIGHENERGY SPIN:3||halfmetal:3||INSULATORS:3||LA2CUO4:3||MODEL:3||FLUCTUATIONS:3||CE:3||double exchange:3||TRANSITIONMETALS:3||RESISTIVITY:3||BORON:3||LA1XCAXMNO3:3||IRON:3||PES:3||ANTIMONIDES:2||MgB2:2||ZR METALLIC GLASSES:2||superconductor:2||CRITICALCURRENT DENSITY:2||CIRCULARDICHROISM:2||SEMICONDUCTORS:2||LOCALIZATION:2||INTRABAND OPTICAL CONDUCTIVITY:2||COLOSSAL MAGNETORESISTANCE:2||OXIDATION:2||EXISTENCE:2||COPPER:2||diboride:2||MAGNESIUMDIBORIDE:2||GAP:2||CE COMPOUNDS:2||CORE POLARIZATION:2||magnetoresistance:2||photoemission spectroscopy:2||electronphonon interaction:2||GETTER:2||PD:2||MAGNETISM:2||FECR2S4:2||SUPERCONDUCTING MGB2:2||WIRES:2||ABSORPTION:2||ENERGY:2||LA1XSRXMNO3:2||CONSTANTS:2||polaron:2||charge ordering:2||SCATTERING:2||XRAY PHOTOEMISSION:2||CeNiSn:2||phase diagram:2||PHOTOELECTRON:2||QUADRUPOLAR:2||perovskitemanganites:2||CO:2||SYSTEMS:2||DOPED ZNO:2||LOWFREQUENCY SOUND:2||LA:2||ELECTRONELECTRON SCATTERING:2||AU:2||DENSITYWAVE INSTABILITY:2||FERMISURFACE:2||hybridization:2||VALENCEBAND SATELLITE:2||SULFUR SPINEL:2||Heusler:2||APPROXIMATION:2||superexchange:2||colossal magnetoresistance:2||ALLOYS:2||DEPENDENCE:2||AG:2||electronic structures:2||AUGERSPECTRA:2||CR:2||PARAMETERS:2||DIFFRACTION:2||SEMICONDUCTORMETAL TRANSITION:1||INTERMEDIATEVALENCE:1||SMB6:1||SRRUO3:1||antiperovskite structure with antipolar nature:1||lowenergy twodimensional phonons:1||anatase TiO2:1||La3S4:1||metalinsulator transitions:1||MNO:1||ELECTRONICSTRUCTURES:1||MAGNETIC CIRCULARDICHROISM:1||Density functional theory:1||CeCo2:1||TOPOLARON CROSSOVER:1||EXCHANGE:1||cuprates:1||high Tc cuprates:1||magnetically ordered materials:1||ZNSE:1||Sr2xKxFeMoO6:1||CDW:1||TeCuO3:1||STRUCTURALPROPERTIES:1||MN:1||screening length:1||amorphous Fe:1||WAVE BASISSET:1||SILICONCARBIDE:1||HIGHPRESSURE:1||electronphonon coupling:1||quenched superconductivity:1||CMR perovskite manganites:1||OXIDE:1||polarons:1||synchrotron radiation:1||FULLERIDES:1||RESONANTPHOTOEMISSION:1||Silicon carbide:1||DFT calculation:1||Hybridized bands:1||GIANT MAGNETORESISTANCE:1||PEROVSKITES:1||Raman spectra:1||EXCHANGE ENHANCEMENT:1||SILICON:1||SR2FEMOO6:1||orbital ordering:1||delafossite:1||TITANIUMDIOXIDE:1||electronic structure of disordered solids:1||YFE2:1||Magnetic polaron:1||NA2TI2SB2O:1||STRONGCOUPLED SUPERCONDUCTORS:1||HEAVYFERMION SYSTEMS:1||firstprinciples calculations:1||MECHANISM:1||UNiSn:1||PHOTONIC BANDGAP:1||SINGLE IMPURITY:1||PHONONSPECTRUM:1||FERMISURFACE TOPOLOGY:1||SUPPRESSION:1||RESONANT PHOTOEMISSION:1||METALDOPED PICENE:1||PHOTOIONIZATION CROSSSECTIONS:1||PHOTOINDUCED FERRIMAGNETIC SYSTEMS:1||LINKAGE ISOMERISM:1||CHARGETRANSFER:1||Bilayer Graphene:1||MAGNETICFIELD:1||SPINWAVES:1||rareearth manganese oxides:1||magnonphonon interaction:1||NACO2O4:1||ENERGYBANDS:1||SELFENERGY:1||GAS:1||Fe0.5Cu0.5Cr2S4:1||scanning photoelectron microscopy (SPEM):1||MAGNETIC PROPERTIES:1||Stoner model:1||AMORPHOUS TRANSITIONMETALS:1||SPINGLASS STATES:1||NI:1||LA3NI2B2N3:1||SOLIDS:1||CEO2:1||BAND THEORY:1||dilute magnetic semiconductor:1||pyrochlore:1||Y1XPRXBA2CU3O7DELTA:1||and electronphonon interactions:1||VIBRATIONS:1||RAY PHOTOEMISSION:1||ALKALI CATION:1||Europium:1||colossal magnetoresistance:1||structural stability:1||ENERGYGAP:1||small polaron:1||DOUBLE EXCHANGE:1||Coulomb correlation:1||magnon:1||phonons:1||ELECTRON FERROMAGNETISM:1||CURIETEMPERATURE:1||ARPES:1||PLANEWAVE METHOD:1||Xray absorption spectroscopy (XAS):1||ROOMTEMPERATURE:1||MONOCHALCOGENIDES:1||HEAT:1||UPDSN:1||MOMENTS:1||XRAY ABSORPTION:1||SEMICONDUCTOR:1||Fermi surface nesting:1||optical phonon:1||disordered system:1||dilute magnetic semiconductors:1||CMR manganites:1||PHONONS:1||LATTICEDYNAMICS:1||OXIDES:1||4fphotoemission:1||permanent magnet:1||pseudogap:1||TRANSPORTPROPERTIES:1||ANTIFERROMAGNET:1||(BI,PB)SRCOO SYSTEM:1||semicore correlation:1||POLARIZATION:1||CRYSTAL:1||spinel:1||Xray magnetic circular dichroism (XMCD):1||magnetocapacitance:1||ANATASE:1||TEMPERATURES:1||Pseudogap:1||INTERFACE:1||SUBSTRATE:1||YNI2B2C:1||SAMARIUM SULFIDE:1||strong swave superconductor:1||DOPED MANGANITE:1||SYMMETRY:1||CENISN:1||resonance mode:1||DISORDERED SYSTEM:1||LITHIUM INTERCALATION:1||CUO2 PLANE:1||SURFACE:1||Delafossite:1||ELECTRICALPROPERTIES:1||NIMNSB:1||PTMNSB:1||ROOMTEMPERATURE FERROMAGNETISM:1||RUBIDIUM MANGANESE HEXACYANOFERRATE:1||COLOSSALMAGNETORESISTANCE:1||FINITE TEMPERATURES:1||LAMNO3:1||FE:1||transitionmetal oxides:1||giant magnetoresistance:1||phonon:1||COPPER OXIDES:1||valence states:1||thermoelectric:1||semiconductor:1||CATION DISTRIBUTION:1||FeCr2S4:1||photoemission spectroscopy (PES):1||METALLIC FERROMAGNETISM:1||GRAPHITE:1||SUSCEPTIBILITY:1||UBE13:1||RCrSb3:1||band JahnTeller:1||Ce3S4:1||TiO2:1||PrBa2Cu3O7delta:1||UNTWINNED PRBA2CU3O7:1||AGNIO2:1||HALFMETALLIC FERROMAGNETS:1||CI:1||Energy gap:1||Photoemission:1||Future applications:1||Photoemission measurements:1||Graphene:1||BANDSTRUCTURE:1||TC:1||superconductivity:1||magnetic semiconductors:1||CMRmanganites:1||thin films:1||spin dynamics:1||highTc superconductors:1||ITINERANTELECTRON FERROMAGNETISM:1||SINGLECRYSTALS:1||CeTe2:1||amorphous magnetic materials:1||EPITAXIAL GRAPHENE:1||LAYERED PNICTIDEOXIDES:1||BOROCARBIDE SUPERCONDUCTORS:1||AUGMENTEDWAVE METHOD:1||METALLIC MAGNET UNISN:1||ORIGIN:1||spectrum rearrangement:1||MEANFIELD THEORY:1||MOLECULEBASED MAGNETS:1||METASTABLE STATE:1||INSULATOR:1||magnetic orderin:1||FCC IRON:1||CeRu2:1||TL2MN2O7:1||isotope effect:1||Perovskitemanganites:1||RECURSION METHOD:1||PERPENDICULAR MAGNETICANISOTROPY:1||quasiparticle spectral density:1||GW:1||MANGANESE FERRITE:1||RESONANCE:1||SeCuO3:1||Optical conductivity:1||MASSLESS DIRAC FERMIONS:1||SCHOTTKYBARRIER:1||electronic structure:15||ELECTRONICSTRUCTURE:11||TRANSITIONMETAL COMPOUNDS:10||METALS:10||photoemission:8||SPECTRA:8||MAGNETORESISTANCE:7||FERROMAGNETISM:7||TRANSPORT:7||TRANSITION:6||FILMS:6||THINFILMS:5||TOTALENERGY CALCULATIONS:5||MAGNETICPROPERTIES:5||SUPERCONDUCTIVITY:5||PR:5||LATTICE:4||STATES:4||SPECTROSCOPY:4||FIELD:4||CRYSTALSTRUCTURE:4||PHOTOEMISSION:4||TEMPERATURE:4||TRANSITIONTEMPERATURE:4||XRAYABSORPTION:4||STATE:4||CU:4||BASISSET:4||XAS:4||CRYSTALS:3||EXCITATIONS:3||MOTTHUBBARD SYSTEMS:3||HIGHENERGY SPIN:3||halfmetal:3||INSULATORS:3||LA2CUO4:3||MODEL:3||FLUCTUATIONS:3||CE:3||double exchange:3||TRANSITIONMETALS:3||RESISTIVITY:3||BORON:3||LA1XCAXMNO3:3||IRON:3||PES:3||ANTIMONIDES:2||MgB2:2||ZR METALLIC GLASSES:2||superconductor:2||CRITICALCURRENT DENSITY:2||CIRCULARDICHROISM:2||SEMICONDUCTORS:2||LOCALIZATION:2||INTRABAND OPTICAL CONDUCTIVITY:2||COLOSSAL MAGNETORESISTANCE:2||OXIDATION:2||EXISTENCE:2||COPPER:2||diboride:2||MAGNESIUMDIBORIDE:2||GAP:2||CE COMPOUNDS:2||CORE POLARIZATION:2||magnetoresistance:2||photoemission spectroscopy:2||electronphonon interaction:2||GETTER:2||PD:2||MAGNETISM:2||FECR2S4:2||SUPERCONDUCTING MGB2:2||WIRES:2||ABSORPTION:2||ENERGY:2||LA1XSRXMNO3:2||CONSTANTS:2||polaron:2||charge ordering:2||SCATTERING:2||XRAY PHOTOEMISSION:2||CeNiSn:2||phase diagram:2||PHOTOELECTRON:2||QUADRUPOLAR:2||perovskitemanganites:2||CO:2||SYSTEMS:2||DOPED ZNO:2||LOWFREQUENCY SOUND:2||LA:2||ELECTRONELECTRON SCATTERING:2||AU:2||DENSITYWAVE INSTABILITY:2||FERMISURFACE:2||hybridization:2||VALENCEBAND SATELLITE:2||SULFUR SPINEL:2||Heusler:2||APPROXIMATION:2||superexchange:2||colossal magnetoresistance:2||ALLOYS:2||DEPENDENCE:2||AG:2||electronic structures:2||AUGERSPECTRA:2||CR:2||PARAMETERS:2||DIFFRACTION:2||SEMICONDUCTORMETAL TRANSITION:1||INTERMEDIATEVALENCE:1||SMB6:1||SRRUO3:1||antiperovskite structure with antipolar nature:1||lowenergy twodimensional phonons:1||anatase TiO2:1||La3S4:1||metalinsulator transitions:1||MNO:1||ELECTRONICSTRUCTURES:1||MAGNETIC CIRCULARDICHROISM:1||Density functional theory:1||CeCo2:1||TOPOLARON CROSSOVER:1||EXCHANGE:1||cuprates:1||high Tc cuprates:1||magnetically ordered materials:1||ZNSE:1||Sr2xKxFeMoO6:1||CDW:1||TeCuO3:1||STRUCTURALPROPERTIES:1||MN:1||screening length:1||amorphous Fe:1||WAVE BASISSET:1||SILICONCARBIDE:1||HIGHPRESSURE:1||electronphonon coupling:1||quenched superconductivity:1||CMR perovskite manganites:1||OXIDE:1||polarons:1||synchrotron radiation:1||FULLERIDES:1||RESONANTPHOTOEMISSION:1||Silicon carbide:1||DFT calculation:1||Hybridized bands:1||GIANT MAGNETORESISTANCE:1||PEROVSKITES:1||Raman spectra:1||EXCHANGE ENHANCEMENT:1||SILICON:1||SR2FEMOO6:1||orbital ordering:1||delafossite:1||TITANIUMDIOXIDE:1||electronic structure of disordered solids:1||YFE2:1||Magnetic polaron:1||NA2TI2SB2O:1||STRONGCOUPLED SUPERCONDUCTORS:1||HEAVYFERMION SYSTEMS:1||firstprinciples calculations:1||MECHANISM:1||UNiSn:1||PHOTONIC BANDGAP:1||SINGLE IMPURITY:1||PHONONSPECTRUM:1||FERMISURFACE TOPOLOGY:1||SUPPRESSION:1||RESONANT PHOTOEMISSION:1||METALDOPED PICENE:1||PHOTOIONIZATION CROSSSECTIONS:1||PHOTOINDUCED FERRIMAGNETIC SYSTEMS:1||LINKAGE ISOMERISM:1||CHARGETRANSFER:1||Bilayer Graphene:1||MAGNETICFIELD:1||SPINWAVES:1||rareearth manganese oxides:1||magnonphonon interaction:1||NACO2O4:1||ENERGYBANDS:1||SELFENERGY:1||GAS:1||Fe0.5Cu0.5Cr2S4:1||scanning photoelectron microscopy (SPEM):1||MAGNETIC PROPERTIES:1||Stoner model:1||AMORPHOUS TRANSITIONMETALS:1||SPINGLASS STATES:1||NI:1||LA3NI2B2N3:1||SOLIDS:1||CEO2:1||BAND THEORY:1||dilute magnetic semiconductor:1||pyrochlore:1||Y1XPRXBA2CU3O7DELTA:1||and electronphonon interactions:1||VIBRATIONS:1||RAY PHOTOEMISSION:1||ALKALI CATION:1||Europium:1||colossal magnetoresistance:1||structural stability:1||ENERGYGAP:1||small polaron:1||DOUBLE EXCHANGE:1||Coulomb correlation:1||magnon:1||phonons:1||ELECTRON FERROMAGNETISM:1||CURIETEMPERATURE:1||ARPES:1||PLANEWAVE METHOD:1||Xray absorption spectroscopy (XAS):1||ROOMTEMPERATURE:1||MONOCHALCOGENIDES:1||HEAT:1||UPDSN:1||MOMENTS:1||XRAY ABSORPTION:1||SEMICONDUCTOR:1||Fermi surface nesting:1||optical phonon:1||disordered system:1||dilute magnetic semiconductors:1||CMR manganites:1||PHONONS:1||LATTICEDYNAMICS:1||OXIDES:1||4fphotoemission:1||permanent magnet:1||pseudogap:1||TRANSPORTPROPERTIES:1||ANTIFERROMAGNET:1||(BI,PB)SRCOO SYSTEM:1||semicore correlation:1||POLARIZATION:1||CRYSTAL:1||spinel:1||Xray magnetic circular dichroism (XMCD):1||magnetocapacitance:1||ANATASE:1||TEMPERATURES:1||Pseudogap:1||INTERFACE:1||SUBSTRATE:1||YNI2B2C:1||SAMARIUM SULFIDE:1||strong swave superconductor:1||DOPED MANGANITE:1||SYMMETRY:1||CENISN:1||resonance mode:1||DISORDERED SYSTEM:1||LITHIUM INTERCALATION:1||CUO2 PLANE:1||SURFACE:1||Delafossite:1||ELECTRICALPROPERTIES:1||NIMNSB:1||PTMNSB:1||ROOMTEMPERATURE FERROMAGNETISM:1||RUBIDIUM MANGANESE HEXACYANOFERRATE:1||COLOSSALMAGNETORESISTANCE:1||FINITE TEMPERATURES:1||LAMNO3:1||FE:1||transitionmetal oxides:1||giant magnetoresistance:1||phonon:1||COPPER OXIDES:1||valence states:1||thermoelectric:1||semiconductor:1||CATION DISTRIBUTION:1||FeCr2S4:1||photoemission spectroscopy (PES):1||METALLIC FERROMAGNETISM:1||GRAPHITE:1||SUSCEPTIBILITY:1||UBE13:1||RCrSb3:1||band JahnTeller:1||Ce3S4:1||TiO2:1||PrBa2Cu3O7delta:1||UNTWINNED PRBA2CU3O7:1||AGNIO2:1||HALFMETALLIC FERROMAGNETS:1||CI:1||Energy gap:1||Photoemission:1||Future applications:1||Photoemission measurements:1||Graphene:1||BANDSTRUCTURE:1||TC:1||superconductivity:1||magnetic semiconductors:1||CMRmanganites:1||thin films:1||spin dynamics:1||highTc superconductors:1||ITINERANTELECTRON FERROMAGNETISM:1||SINGLECRYSTALS:1||CeTe2:1||amorphous magnetic materials:1||EPITAXIAL GRAPHENE:1||LAYERED PNICTIDEOXIDES:1||BOROCARBIDE SUPERCONDUCTORS:1||AUGMENTEDWAVE METHOD:1||METALLIC MAGNET UNISN:1||ORIGIN:1||spectrum rearrangement:1||MEANFIELD THEORY:1||MOLECULEBASED MAGNETS:1||METASTABLE STATE:1||INSULATOR:1||magnetic orderin:1||FCC IRON:1||CeRu2:1||TL2MN2O7:1||isotope effect:1||Perovskitemanganites:1||RECURSION METHOD:1||PERPENDICULAR MAGNETICANISOTROPY:1||quasiparticle spectral density:1||GW:1||MANGANESE FERRITE:1||RESONANCE:1||SeCuO3:1||Optical conductivity:1||MASSLESS DIRAC FERMIONS:1||SCHOTTKYBARRIER:1||electronic structure:15||ELECTRONICSTRUCTURE:11||TRANSITIONMETAL COMPOUNDS:10||METALS:10||photoemission:8||SPECTRA:8||MAGNETORESISTANCE:7||FERROMAGNETISM:7||TRANSPORT:7||TRANSITION:6||FILMS:6||THINFILMS:5||TOTALENERGY CALCULATIONS:5||MAGNETICPROPERTIES:5||SUPERCONDUCTIVITY:5||PR:5||LATTICE:4||STATES:4||SPECTROSCOPY:4||FIELD:4||CRYSTALSTRUCTURE:4||PHOTOEMISSION:4||TEMPERATURE:4||TRANSITIONTEMPERATURE:4||XRAYABSORPTION:4||STATE:4||CU:4||BASISSET:4||XAS:4||CRYSTALS:3||EXCITATIONS:3||MOTTHUBBARD SYSTEMS:3||HIGHENERGY SPIN:3||halfmetal:3||INSULATORS:3||LA2CUO4:3||MODEL:3||FLUCTUATIONS:3||CE:3||double exchange:3||TRANSITIONMETALS:3||RESISTIVITY:3||BORON:3||LA1XCAXMNO3:3||IRON:3||PES:3||ANTIMONIDES:2||MgB2:2||ZR METALLIC GLASSES:2||superconductor:2||CRITICALCURRENT DENSITY:2||CIRCULARDICHROISM:2||SEMICONDUCTORS:2||LOCALIZATION:2||INTRABAND OPTICAL CONDUCTIVITY:2||COLOSSAL MAGNETORESISTANCE:2||OXIDATION:2||EXISTENCE:2||COPPER:2||diboride:2||MAGNESIUMDIBORIDE:2||GAP:2||CE COMPOUNDS:2||CORE POLARIZATION:2||magnetoresistance:2||photoemission spectroscopy:2||electronphonon interaction:2||GETTER:2||PD:2||MAGNETISM:2||FECR2S4:2||SUPERCONDUCTING MGB2:2||WIRES:2||ABSORPTION:2||ENERGY:2||LA1XSRXMNO3:2||CONSTANTS:2||polaron:2||charge ordering:2||SCATTERING:2||XRAY PHOTOEMISSION:2||CeNiSn:2||phase diagram:2||PHOTOELECTRON:2||QUADRUPOLAR:2||perovskitemanganites:2||CO:2||SYSTEMS:2||DOPED ZNO:2||LOWFREQUENCY SOUND:2||LA:2||ELECTRONELECTRON SCATTERING:2||AU:2||DENSITYWAVE INSTABILITY:2||FERMISURFACE:2||hybridization:2||VALENCEBAND SATELLITE:2||SULFUR SPINEL:2||Heusler:2||APPROXIMATION:2||superexchange:2||colossal magnetoresistance:2||ALLOYS:2||DEPENDENCE:2||AG:2||electronic structures:2||AUGERSPECTRA:2||CR:2||PARAMETERS:2||DIFFRACTION:2||SEMICONDUCTORMETAL TRANSITION:1||INTERMEDIATEVALENCE:1||SMB6:1||SRRUO3:1||antiperovskite structure with antipolar nature:1||lowenergy twodimensional phonons:1||anatase TiO2:1||La3S4:1||metalinsulator transitions:1||MNO:1||ELECTRONICSTRUCTURES:1||MAGNETIC CIRCULARDICHROISM:1||Density functional theory:1||CeCo2:1||TOPOLARON CROSSOVER:1||EXCHANGE:1||cuprates:1||high Tc cuprates:1||magnetically ordered materials:1||ZNSE:1||Sr2xKxFeMoO6:1||CDW:1||TeCuO3:1||STRUCTURALPROPERTIES:1||MN:1||screening length:1||amorphous Fe:1||WAVE BASISSET:1||SILICONCARBIDE:1||HIGHPRESSURE:1||electronphonon coupling:1||quenched superconductivity:1||CMR perovskite manganites:1||OXIDE:1||polarons:1||synchrotron radiation:1||FULLERIDES:1||RESONANTPHOTOEMISSION:1||Silicon carbide:1||DFT calculation:1||Hybridized bands:1||GIANT MAGNETORESISTANCE:1||PEROVSKITES:1||Raman spectra:1||EXCHANGE ENHANCEMENT:1||SILICON:1||SR2FEMOO6:1||orbital ordering:1||delafossite:1||TITANIUMDIOXIDE:1||electronic structure of disordered solids:1||YFE2:1||Magnetic polaron:1||NA2TI2SB2O:1||STRONGCOUPLED SUPERCONDUCTORS:1||HEAVYFERMION SYSTEMS:1||firstprinciples calculations:1||MECHANISM:1||UNiSn:1||PHOTONIC BANDGAP:1||SINGLE IMPURITY:1||PHONONSPECTRUM:1||FERMISURFACE TOPOLOGY:1||SUPPRESSION:1||RESONANT PHOTOEMISSION:1||METALDOPED PICENE:1||PHOTOIONIZATION CROSSSECTIONS:1||PHOTOINDUCED FERRIMAGNETIC SYSTEMS:1||LINKAGE ISOMERISM:1||CHARGETRANSFER:1||Bilayer Graphene:1||MAGNETICFIELD:1||SPINWAVES:1||rareearth manganese oxides:1||magnonphonon interaction:1||NACO2O4:1||ENERGYBANDS:1||SELFENERGY:1||GAS:1||Fe0.5Cu0.5Cr2S4:1||scanning photoelectron microscopy (SPEM):1||MAGNETIC PROPERTIES:1||Stoner model:1||AMORPHOUS TRANSITIONMETALS:1||SPINGLASS STATES:1||NI:1||LA3NI2B2N3:1||SOLIDS:1||CEO2:1||BAND THEORY:1||dilute magnetic semiconductor:1||pyrochlore:1||Y1XPRXBA2CU3O7DELTA:1||and electronphonon interactions:1||VIBRATIONS:1||RAY PHOTOEMISSION:1||ALKALI CATION:1||Europium:1||colossal magnetoresistance:1||structural stability:1||ENERGYGAP:1||small polaron:1||DOUBLE EXCHANGE:1||Coulomb correlation:1||magnon:1||phonons:1||ELECTRON FERROMAGNETISM:1||CURIETEMPERATURE:1||ARPES:1||PLANEWAVE METHOD:1||Xray absorption spectroscopy (XAS):1||ROOMTEMPERATURE:1||MONOCHALCOGENIDES:1||HEAT:1||UPDSN:1||MOMENTS:1||XRAY ABSORPTION:1||SEMICONDUCTOR:1||Fermi surface nesting:1||optical phonon:1||disordered system:1||dilute magnetic semiconductors:1||CMR manganites:1||PHONONS:1||LATTICEDYNAMICS:1||OXIDES:1||4fphotoemission:1||permanent magnet:1||pseudogap:1||TRANSPORTPROPERTIES:1||ANTIFERROMAGNET:1||(BI,PB)SRCOO SYSTEM:1||semicore correlation:1||POLARIZATION:1||CRYSTAL:1||spinel:1||Xray magnetic circular dichroism (XMCD):1||magnetocapacitance:1||ANATASE:1||TEMPERATURES:1||Pseudogap:1||INTERFACE:1||SUBSTRATE:1||YNI2B2C:1||SAMARIUM SULFIDE:1||strong swave superconductor:1||DOPED MANGANITE:1||SYMMETRY:1||CENISN:1||resonance mode:1||DISORDERED SYSTEM:1||LITHIUM INTERCALATION:1||CUO2 PLANE:1||SURFACE:1||Delafossite:1||ELECTRICALPROPERTIES:1||NIMNSB:1||PTMNSB:1||ROOMTEMPERATURE FERROMAGNETISM:1||RUBIDIUM MANGANESE HEXACYANOFERRATE:1||COLOSSALMAGNETORESISTANCE:1||FINITE TEMPERATURES:1||LAMNO3:1||FE:1||transitionmetal oxides:1||giant magnetoresistance:1||phonon:1||COPPER OXIDES:1||valence states:1||thermoelectric:1||semiconductor:1||CATION DISTRIBUTION:1||FeCr2S4:1||photoemission spectroscopy (PES):1||METALLIC FERROMAGNETISM:1||GRAPHITE:1||SUSCEPTIBILITY:1||UBE13:1||RCrSb3:1||band JahnTeller:1||Ce3S4:1||TiO2:1||PrBa2Cu3O7delta:1||UNTWINNED PRBA2CU3O7:1||AGNIO2:1||HALFMETALLIC FERROMAGNETS:1||CI:1||Energy gap:1||Photoemission:1||Future applications:1||Photoemission measurements:1||Graphene:1||BANDSTRUCTURE:1||TC:1||superconductivity:1||magnetic semiconductors:1||CMRmanganites:1||thin films:1||spin dynamics:1||highTc superconductors:1||ITINERANTELECTRON FERROMAGNETISM:1||SINGLECRYSTALS:1||CeTe2:1||amorphous magnetic materials:1||EPITAXIAL GRAPHENE:1||LAYERED PNICTIDEOXIDES:1||BOROCARBIDE SUPERCONDUCTORS:1||AUGMENTEDWAVE METHOD:1||METALLIC MAGNET UNISN:1||ORIGIN:1||spectrum rearrangement:1||MEANFIELD THEORY:1||MOLECULEBASED MAGNETS:1||METASTABLE STATE:1||INSULATOR:1||magnetic orderin:1||FCC IRON:1||CeRu2:1||TL2MN2O7:1||isotope effect:1||Perovskitemanganites:1||RECURSION METHOD:1||PERPENDICULAR MAGNETICANISOTROPY:1||quasiparticle spectral density:1||GW:1||MANGANESE FERRITE:1||RESONANCE:1||SeCuO3:1||Optical conductivity:1||MASSLESS DIRAC FERMIONS:1||SCHOTTKYBARRIER:1||electronic structure:15||ELECTRONICSTRUCTURE:11||TRANSITIONMETAL COMPOUNDS:10||METALS:10||photoemission:8||SPECTRA:8||MAGNETORESISTANCE:7||FERROMAGNETISM:7||TRANSPORT:7||TRANSITION:6||FILMS:6||THINFILMS:5||TOTALENERGY CALCULATIONS:5||MAGNETICPROPERTIES:5||SUPERCONDUCTIVITY:5||PR:5||LATTICE:4||STATES:4||SPECTROSCOPY:4||FIELD:4||CRYSTALSTRUCTURE:4||PHOTOEMISSION:4||TEMPERATURE:4||TRANSITIONTEMPERATURE:4||XRAYABSORPTION:4||STATE:4||CU:4||BASISSET:4||XAS:4||CRYSTALS:3||EXCITATIONS:3||MOTTHUBBARD SYSTEMS:3||HIGHENERGY SPIN:3||halfmetal:3||INSULATORS:3||LA2CUO4:3||MODEL:3||FLUCTUATIONS:3||CE:3||double exchange:3||TRANSITIONMETALS:3||RESISTIVITY:3||BORON:3||LA1XCAXMNO3:3||IRON:3||PES:3||ANTIMONIDES:2||MgB2:2||ZR METALLIC GLASSES:2||superconductor:2||CRITICALCURRENT DENSITY:2||CIRCULARDICHROISM:2||SEMICONDUCTORS:2||LOCALIZATION:2||INTRABAND OPTICAL CONDUCTIVITY:2||COLOSSAL MAGNETORESISTANCE:2||OXIDATION:2||EXISTENCE:2||COPPER:2||diboride:2||MAGNESIUMDIBORIDE:2||GAP:2||CE COMPOUNDS:2||CORE POLARIZATION:2||magnetoresistance:2||photoemission spectroscopy:2||electronphonon interaction:2||GETTER:2||PD:2||MAGNETISM:2||FECR2S4:2||SUPERCONDUCTING MGB2:2||WIRES:2||ABSORPTION:2||ENERGY:2||LA1XSRXMNO3:2||CONSTANTS:2||polaron:2||charge ordering:2||SCATTERING:2||XRAY PHOTOEMISSION:2||CeNiSn:2||phase diagram:2||PHOTOELECTRON:2||QUADRUPOLAR:2||perovskitemanganites:2||CO:2||SYSTEMS:2||DOPED ZNO:2||LOWFREQUENCY SOUND:2||LA:2||ELECTRONELECTRON SCATTERING:2||AU:2||DENSITYWAVE INSTABILITY:2||FERMISURFACE:2||hybridization:2||VALENCEBAND SATELLITE:2||SULFUR SPINEL:2||Heusler:2||APPROXIMATION:2||superexchange:2||colossal magnetoresistance:2||ALLOYS:2||DEPENDENCE:2||AG:2||electronic structures:2||AUGERSPECTRA:2||CR:2||PARAMETERS:2||DIFFRACTION:2||SEMICONDUCTORMETAL TRANSITION:1||INTERMEDIATEVALENCE:1||SMB6:1||SRRUO3:1||antiperovskite structure with antipolar nature:1||lowenergy twodimensional phonons:1||anatase TiO2:1||La3S4:1||metalinsulator transitions:1||MNO:1||ELECTRONICSTRUCTURES:1||MAGNETIC CIRCULARDICHROISM:1||Density functional theory:1||CeCo2:1||TOPOLARON CROSSOVER:1||EXCHANGE:1||cuprates:1||high Tc cuprates:1||magnetically ordered materials:1||ZNSE:1||Sr2xKxFeMoO6:1||CDW:1||TeCuO3:1||STRUCTURALPROPERTIES:1||MN:1||screening length:1||amorphous Fe:1||WAVE BASISSET:1||SILICONCARBIDE:1||HIGHPRESSURE:1||electronphonon coupling:1||quenched superconductivity:1||CMR perovskite manganites:1||OXIDE:1||polarons:1||synchrotron radiation:1||FULLERIDES:1||RESONANTPHOTOEMISSION:1||Silicon carbide:1||DFT calculation:1||Hybridized bands:1||GIANT MAGNETORESISTANCE:1||PEROVSKITES:1||Raman spectra:1||EXCHANGE ENHANCEMENT:1||SILICON:1||SR2FEMOO6:1||orbital ordering:1||delafossite:1||TITANIUMDIOXIDE:1||electronic structure of disordered solids:1||YFE2:1||Magnetic polaron:1||NA2TI2SB2O:1||STRONGCOUPLED SUPERCONDUCTORS:1||HEAVYFERMION SYSTEMS:1||firstprinciples calculations:1||MECHANISM:1||UNiSn:1||PHOTONIC BANDGAP:1||SINGLE IMPURITY:1||PHONONSPECTRUM:1||FERMISURFACE TOPOLOGY:1||SUPPRESSION:1||RESONANT PHOTOEMISSION:1||METALDOPED PICENE:1||PHOTOIONIZATION CROSSSECTIONS:1||PHOTOINDUCED FERRIMAGNETIC SYSTEMS:1||LINKAGE ISOMERISM:1||CHARGETRANSFER:1||Bilayer Graphene:1||MAGNETICFIELD:1||SPINWAVES:1||rareearth manganese oxides:1||magnonphonon interaction:1||NACO2O4:1||ENERGYBANDS:1||SELFENERGY:1||GAS:1||Fe0.5Cu0.5Cr2S4:1||scanning photoelectron microscopy (SPEM):1||MAGNETIC PROPERTIES:1||Stoner model:1||AMORPHOUS TRANSITIONMETALS:1||SPINGLASS STATES:1||NI:1||LA3NI2B2N3:1||SOLIDS:1||CEO2:1||BAND THEORY:1||dilute magnetic semiconductor:1||pyrochlore:1||Y1XPRXBA2CU3O7DELTA:1||and electronphonon interactions:1||VIBRATIONS:1||RAY PHOTOEMISSION:1||ALKALI CATION:1||Europium:1||colossal magnetoresistance:1||structural stability:1||ENERGYGAP:1||small polaron:1||DOUBLE EXCHANGE:1||Coulomb correlation:1||magnon:1||phonons:1||ELECTRON FERROMAGNETISM:1||CURIETEMPERATURE:1||ARPES:1||PLANEWAVE METHOD:1||Xray absorption spectroscopy (XAS):1||ROOMTEMPERATURE:1||MONOCHALCOGENIDES:1||HEAT:1||UPDSN:1||MOMENTS:1||XRAY ABSORPTION:1||SEMICONDUCTOR:1||Fermi surface nesting:1||optical phonon:1||disordered system:1||dilute magnetic semiconductors:1||CMR manganites:1||PHONONS:1||LATTICEDYNAMICS:1||OXIDES:1||4fphotoemission:1||permanent magnet:1||pseudogap:1||TRANSPORTPROPERTIES:1||ANTIFERROMAGNET:1||(BI,PB)SRCOO SYSTEM:1||semicore correlation:1||POLARIZATION:1||CRYSTAL:1||spinel:1||Xray magnetic circular dichroism (XMCD):1||magnetocapacitance:1||ANATASE:1||TEMPERATURES:1||Pseudogap:1||INTERFACE:1||SUBSTRATE:1||YNI2B2C:1||SAMARIUM SULFIDE:1||strong swave superconductor:1||DOPED MANGANITE:1||SYMMETRY:1||CENISN:1||resonance mode:1||DISORDERED SYSTEM:1||LITHIUM INTERCALATION:1||CUO2 PLANE:1||SURFACE:1||Delafossite:1||ELECTRICALPROPERTIES:1||NIMNSB:1||PTMNSB:1||ROOMTEMPERATURE FERROMAGNETISM:1||RUBIDIUM MANGANESE HEXACYANOFERRATE:1||COLOSSALMAGNETORESISTANCE:1||FINITE TEMPERATURES:1||LAMNO3:1||FE:1||transitionmetal oxides:1||giant magnetoresistance:1||phonon:1||COPPER OXIDES:1||valence states:1||thermoelectric:1||semiconductor:1||CATION DISTRIBUTION:1||FeCr2S4:1||photoemission spectroscopy (PES):1||METALLIC FERROMAGNETISM:1||GRAPHITE:1||SUSCEPTIBILITY:1||UBE13:1||RCrSb3:1||band JahnTeller:1||Ce3S4:1||TiO2:1||PrBa2Cu3O7delta:1||UNTWINNED PRBA2CU3O7:1||AGNIO2:1||HALFMETALLIC FERROMAGNETS:1||CI:1||Energy gap:1||Photoemission:1||Future applications:1||Photoemission measurements:1||Graphene:1||BANDSTRUCTURE:1||TC:1||superconductivity:1||magnetic semiconductors:1||CMRmanganites:1||thin films:1||spin dynamics:1||highTc superconductors:1||ITINERANTELECTRON FERROMAGNETISM:1||SINGLECRYSTALS:1||CeTe2:1||amorphous magnetic materials:1||EPITAXIAL GRAPHENE:1||LAYERED PNICTIDEOXIDES:1||BOROCARBIDE SUPERCONDUCTORS:1||AUGMENTEDWAVE METHOD:1||METALLIC MAGNET UNISN:1||ORIGIN:1||spectrum rearrangement:1||MEANFIELD THEORY:1||MOLECULEBASED MAGNETS:1||METASTABLE STATE:1||INSULATOR:1||magnetic orderin:1||FCC IRON:1||CeRu2:1||TL2MN2O7:1||isotope effect:1||Perovskitemanganites:1||RECURSION METHOD:1||PERPENDICULAR MAGNETICANISOTROPY:1||quasiparticle spectral density:1||GW:1||MANGANESE FERRITE:1||RESONANCE:1||SeCuO3:1||Optical conductivity:1||MASSLESS DIRAC FERMIONS:1||SCHOTTKYBARRIER:1||electronic structure:15||ELECTRONICSTRUCTURE:11||TRANSITIONMETAL COMPOUNDS:10||METALS:10||photoemission:8||SPECTRA:8||MAGNETORESISTANCE:7||FERROMAGNETISM:7||TRANSPORT:7||TRANSITION:6||FILMS:6||THINFILMS:5||TOTALENERGY CALCULATIONS:5||MAGNETICPROPERTIES:5||SUPERCONDUCTIVITY:5||PR:5||LATTICE:4||STATES:4||SPECTROSCOPY:4||FIELD:4||CRYSTALSTRUCTURE:4||PHOTOEMISSION:4||TEMPERATURE:4||TRANSITIONTEMPERATURE:4||XRAYABSORPTION:4||STATE:4||CU:4||BASISSET:4||XAS:4||CRYSTALS:3||EXCITATIONS:3||MOTTHUBBARD SYSTEMS:3||HIGHENERGY SPIN:3||halfmetal:3||INSULATORS:3||LA2CUO4:3||MODEL:3||FLUCTUATIONS:3||CE:3||double exchange:3||TRANSITIONMETALS:3||RESISTIVITY:3||BORON:3||LA1XCAXMNO3:3||IRON:3||PES:3||ANTIMONIDES:2||MgB2:2||ZR METALLIC GLASSES:2||superconductor:2||CRITICALCURRENT DENSITY:2||CIRCULARDICHROISM:2||SEMICONDUCTORS:2||LOCALIZATION:2||INTRABAND OPTICAL CONDUCTIVITY:2||COLOSSAL MAGNETORESISTANCE:2||OXIDATION:2||EXISTENCE:2||COPPER:2||diboride:2||MAGNESIUMDIBORIDE:2||GAP:2||CE COMPOUNDS:2||CORE POLARIZATION:2||magnetoresistance:2||photoemission spectroscopy:2||electronphonon interaction:2||GETTER:2||PD:2||MAGNETISM:2||FECR2S4:2||SUPERCONDUCTING MGB2:2||WIRES:2||ABSORPTION:2||ENERGY:2||LA1XSRXMNO3:2||CONSTANTS:2||polaron:2||charge ordering:2||SCATTERING:2||XRAY PHOTOEMISSION:2||CeNiSn:2||phase diagram:2||PHOTOELECTRON:2||QUADRUPOLAR:2||perovskitemanganites:2||CO:2||SYSTEMS:2||DOPED ZNO:2||LOWFREQUENCY SOUND:2||LA:2||ELECTRONELECTRON SCATTERING:2||AU:2||DENSITYWAVE INSTABILITY:2||FERMISURFACE:2||hybridization:2||VALENCEBAND SATELLITE:2||SULFUR SPINEL:2||Heusler:2||APPROXIMATION:2||superexchange:2||colossal magnetoresistance:2||ALLOYS:2||DEPENDENCE:2||AG:2||electronic structures:2||AUGERSPECTRA:2||CR:2||PARAMETERS:2||DIFFRACTION:2||SEMICONDUCTORMETAL TRANSITION:1||INTERMEDIATEVALENCE:1||SMB6:1||SRRUO3:1||antiperovskite structure with antipolar nature:1||lowenergy twodimensional phonons:1||anatase TiO2:1||La3S4:1||metalinsulator transitions:1||MNO:1||ELECTRONICSTRUCTURES:1||MAGNETIC CIRCULARDICHROISM:1||Density functional theory:1||CeCo2:1||TOPOLARON CROSSOVER:1||EXCHANGE:1||cuprates:1||high Tc cuprates:1||magnetically ordered materials:1||ZNSE:1||Sr2xKxFeMoO6:1||CDW:1||TeCuO3:1||STRUCTURALPROPERTIES:1||MN:1||screening length:1||amorphous Fe:1||WAVE BASISSET:1||SILICONCARBIDE:1||HIGHPRESSURE:1||electronphonon coupling:1||quenched superconductivity:1||CMR perovskite manganites:1||OXIDE:1||polarons:1||synchrotron radiation:1||FULLERIDES:1||RESONANTPHOTOEMISSION:1||Silicon carbide:1||DFT calculation:1||Hybridized bands:1||GIANT MAGNETORESISTANCE:1||PEROVSKITES:1||Raman spectra:1||EXCHANGE ENHANCEMENT:1||SILICON:1||SR2FEMOO6:1||orbital ordering:1||delafossite:1||TITANIUMDIOXIDE:1||electronic structure of disordered solids:1||YFE2:1||Magnetic polaron:1||NA2TI2SB2O:1||STRONGCOUPLED SUPERCONDUCTORS:1||HEAVYFERMION SYSTEMS:1||firstprinciples calculations:1||MECHANISM:1||UNiSn:1||PHOTONIC BANDGAP:1||SINGLE IMPURITY:1||PHONONSPECTRUM:1||FERMISURFACE TOPOLOGY:1||SUPPRESSION:1||RESONANT PHOTOEMISSION:1||METALDOPED PICENE:1||PHOTOIONIZATION CROSSSECTIONS:1||PHOTOINDUCED FERRIMAGNETIC SYSTEMS:1||LINKAGE ISOMERISM:1||CHARGETRANSFER:1||Bilayer Graphene:1||MAGNETICFIELD:1||SPINWAVES:1||rareearth manganese oxides:1||magnonphonon interaction:1||NACO2O4:1||ENERGYBANDS:1||SELFENERGY:1||GAS:1||Fe0.5Cu0.5Cr2S4:1||scanning photoelectron microscopy (SPEM):1||MAGNETIC PROPERTIES:1||Stoner model:1||AMORPHOUS TRANSITIONMETALS:1||SPINGLASS STATES:1||NI:1||LA3NI2B2N3:1||SOLIDS:1||CEO2:1||BAND THEORY:1||dilute magnetic semiconductor:1||pyrochlore:1||Y1XPRXBA2CU3O7DELTA:1||and electronphonon interactions:1||VIBRATIONS:1||RAY PHOTOEMISSION:1||ALKALI CATION:1||Europium:1||colossal magnetoresistance:1||structural stability:1||ENERGYGAP:1||small polaron:1||DOUBLE EXCHANGE:1||Coulomb correlation:1||magnon:1||phonons:1||ELECTRON FERROMAGNETISM:1||CURIETEMPERATURE:1||ARPES:1||PLANEWAVE METHOD:1||Xray absorption spectroscopy (XAS):1||ROOMTEMPERATURE:1||MONOCHALCOGENIDES:1||HEAT:1||UPDSN:1||MOMENTS:1||XRAY ABSORPTION:1||SEMICONDUCTOR:1||Fermi surface nesting:1||optical phonon:1||disordered system:1||dilute magnetic semiconductors:1||CMR manganites:1||PHONONS:1||LATTICEDYNAMICS:1||OXIDES:1||4fphotoemission:1||permanent magnet:1||pseudogap:1||TRANSPORTPROPERTIES:1||ANTIFERROMAGNET:1||(BI,PB)SRCOO SYSTEM:1||semicore correlation:1||POLARIZATION:1||CRYSTAL:1||spinel:1||Xray magnetic circular dichroism (XMCD):1||magnetocapacitance:1||ANATASE:1||TEMPERATURES:1||Pseudogap:1||INTERFACE:1||SUBSTRATE:1||YNI2B2C:1||SAMARIUM SULFIDE:1||strong swave superconductor:1||DOPED MANGANITE:1||SYMMETRY:1||CENISN:1||resonance mode:1||DISORDERED SYSTEM:1||LITHIUM INTERCALATION:1||CUO2 PLANE:1||SURFACE:1||Delafossite:1||ELECTRICALPROPERTIES:1||NIMNSB:1||PTMNSB:1||ROOMTEMPERATURE FERROMAGNETISM:1||RUBIDIUM MANGANESE HEXACYANOFERRATE:1||COLOSSALMAGNETORESISTANCE:1||FINITE TEMPERATURES:1||LAMNO3:1||FE:1||transitionmetal oxides:1||giant magnetoresistance:1||phonon:1||COPPER OXIDES:1||valence states:1||thermoelectric:1||semiconductor:1||CATION DISTRIBUTION:1||FeCr2S4:1||photoemission spectroscopy (PES):1||METALLIC FERROMAGNETISM:1||GRAPHITE:1||SUSCEPTIBILITY:1||UBE13:1||RCrSb3:1||band JahnTeller:1||Ce3S4:1||TiO2:1||PrBa2Cu3O7delta:1||UNTWINNED PRBA2CU3O7:1||AGNIO2:1||HALFMETALLIC FERROMAGNETS:1||CI:1||Energy gap:1||Photoemission:1||Future applications:1||Photoemission measurements:1||Graphene:1||BANDSTRUCTURE:1||TC:1||superconductivity:1||magnetic semiconductors:1||CMRmanganites:1||thin films:1||spin dynamics:1||highTc superconductors:1||ITINERANTELECTRON FERROMAGNETISM:1||SINGLECRYSTALS:1||CeTe2:1||amorphous magnetic materials:1||EPITAXIAL GRAPHENE:1||LAYERED PNICTIDEOXIDES:1||BOROCARBIDE SUPERCONDUCTORS:1||AUGMENTEDWAVE METHOD:1||METALLIC MAGNET UNISN:1||ORIGIN:1||spectrum rearrangement:1||MEANFIELD THEORY:1||MOLECULEBASED MAGNETS:1||METASTABLE STATE:1||INSULATOR:1||magnetic orderin:1||FCC IRON:1||CeRu2:1||TL2MN2O7:1||isotope effect:1||Perovskitemanganites:1||RECURSION METHOD:1||PERPENDICULAR MAGNETICANISOTROPY:1||quasiparticle spectral density:1||GW:1||MANGANESE FERRITE:1||RESONANCE:1||SeCuO3:1||Optical conductivity:1||MASSLESS DIRAC FERMIONS:1||SCHOTTKYBARRIER:1||electronic structure:15||ELECTRONICSTRUCTURE:11||TRANSITIONMETAL COMPOUNDS:10||METALS:10||photoemission:8||SPECTRA:8||MAGNETORESISTANCE:7||FERROMAGNETISM:7||TRANSPORT:7||TRANSITION:6||FILMS:6||THINFILMS:5||TOTALENERGY CALCULATIONS:5||MAGNETICPROPERTIES:5||SUPERCONDUCTIVITY:5||PR:5||LATTICE:4||STATES:4||SPECTROSCOPY:4||FIELD:4||CRYSTALSTRUCTURE:4||PHOTOEMISSION:4||TEMPERATURE:4||TRANSITIONTEMPERATURE:4||XRAYABSORPTION:4||STATE:4||CU:4||BASISSET:4||XAS:4||CRYSTALS:3||EXCITATIONS:3||MOTTHUBBARD SYSTEMS:3||HIGHENERGY SPIN:3||halfmetal:3||INSULATORS:3||LA2CUO4:3||MODEL:3||FLUCTUATIONS:3||CE:3||double exchange:3||TRANSITIONMETALS:3||RESISTIVITY:3||BORON:3||LA1XCAXMNO3:3||IRON:3||PES:3||ANTIMONIDES:2||MgB2:2||ZR METALLIC GLASSES:2||superconductor:2||CRITICALCURRENT DENSITY:2||CIRCULARDICHROISM:2||SEMICONDUCTORS:2||LOCALIZATION:2||INTRABAND OPTICAL CONDUCTIVITY:2||COLOSSAL MAGNETORESISTANCE:2||OXIDATION:2||EXISTENCE:2||COPPER:2||diboride:2||MAGNESIUMDIBORIDE:2||GAP:2||CE COMPOUNDS:2||CORE POLARIZATION:2||magnetoresistance:2||photoemission spectroscopy:2||electronphonon interaction:2||GETTER:2||PD:2||MAGNETISM:2||FECR2S4:2||SUPERCONDUCTING MGB2:2||WIRES:2||ABSORPTION:2||ENERGY:2||LA1XSRXMNO3:2||CONSTANTS:2||polaron:2||charge ordering:2||SCATTERING:2||XRAY PHOTOEMISSION:2||CeNiSn:2||phase diagram:2||PHOTOELECTRON:2||QUADRUPOLAR:2||perovskitemanganites:2||CO:2||SYSTEMS:2||DOPED ZNO:2||LOWFREQUENCY SOUND:2||LA:2||ELECTRONELECTRON SCATTERING:2||AU:2||DENSITYWAVE INSTABILITY:2||FERMISURFACE:2||hybridization:2||VALENCEBAND SATELLITE:2||SULFUR SPINEL:2||Heusler:2||APPROXIMATION:2||superexchange:2||colossal magnetoresistance:2||ALLOYS:2||DEPENDENCE:2||AG:2||electronic structures:2||AUGERSPECTRA:2||CR:2||PARAMETERS:2||DIFFRACTION:2||SEMICONDUCTORMETAL TRANSITION:1||INTERMEDIATEVALENCE:1||SMB6:1||SRRUO3:1||antiperovskite structure with antipolar nature:1||lowenergy twodimensional phonons:1||anatase TiO2:1||La3S4:1||metalinsulator transitions:1||MNO:1||ELECTRONICSTRUCTURES:1||MAGNETIC CIRCULARDICHROISM:1||Density functional theory:1||CeCo2:1||TOPOLARON CROSSOVER:1||EXCHANGE:1||cuprates:1||high Tc cuprates:1||magnetically ordered materials:1||ZNSE:1||Sr2xKxFeMoO6:1||CDW:1||TeCuO3:1||STRUCTURALPROPERTIES:1||MN:1||screening length:1||amorphous Fe:1||WAVE BASISSET:1||SILICONCARBIDE:1||HIGHPRESSURE:1||electronphonon coupling:1||quenched superconductivity:1||CMR perovskite manganites:1||OXIDE:1||polarons:1||synchrotron radiation:1||FULLERIDES:1||RESONANTPHOTOEMISSION:1||Silicon carbide:1||DFT calculation:1||Hybridized bands:1||GIANT MAGNETORESISTANCE:1||PEROVSKITES:1||Raman spectra:1||EXCHANGE ENHANCEMENT:1||SILICON:1||SR2FEMOO6:1||orbital ordering:1||delafossite:1||TITANIUMDIOXIDE:1||electronic structure of disordered solids:1||YFE2:1||Magnetic polaron:1||NA2TI2SB2O:1||STRONGCOUPLED SUPERCONDUCTORS:1||HEAVYFERMION SYSTEMS:1||firstprinciples calculations:1||MECHANISM:1||UNiSn:1||PHOTONIC BANDGAP:1||SINGLE IMPURITY:1||PHONONSPECTRUM:1||FERMISURFACE TOPOLOGY:1||SUPPRESSION:1||RESONANT PHOTOEMISSION:1||METALDOPED PICENE:1||PHOTOIONIZATION CROSSSECTIONS:1||PHOTOINDUCED FERRIMAGNETIC SYSTEMS:1||LINKAGE ISOMERISM:1||CHARGETRANSFER:1||Bilayer Graphene:1||MAGNETICFIELD:1||SPINWAVES:1||rareearth manganese oxides:1||magnonphonon interaction:1||NACO2O4:1||ENERGYBANDS:1||SELFENERGY:1||GAS:1||Fe0.5Cu0.5Cr2S4:1||scanning photoelectron microscopy (SPEM):1||MAGNETIC PROPERTIES:1||Stoner model:1||AMORPHOUS TRANSITIONMETALS:1||SPINGLASS STATES:1||NI:1||LA3NI2B2N3:1||SOLIDS:1||CEO2:1||BAND THEORY:1||dilute magnetic semiconductor:1||pyrochlore:1||Y1XPRXBA2CU3O7DELTA:1||and electronphonon interactions:1||VIBRATIONS:1||RAY PHOTOEMISSION:1||ALKALI CATION:1||Europium:1||colossal magnetoresistance:1||structural stability:1||ENERGYGAP:1||small polaron:1||DOUBLE EXCHANGE:1||Coulomb correlation:1||magnon:1||phonons:1||ELECTRON FERROMAGNETISM:1||CURIETEMPERATURE:1||ARPES:1||PLANEWAVE METHOD:1||Xray absorption spectroscopy (XAS):1||ROOMTEMPERATURE:1||MONOCHALCOGENIDES:1||HEAT:1||UPDSN:1||MOMENTS:1||XRAY ABSORPTION:1||SEMICONDUCTOR:1||Fermi surface nesting:1||optical phonon:1||disordered system:1||dilute magnetic semiconductors:1||CMR manganites:1||PHONONS:1||LATTICEDYNAMICS:1||OXIDES:1||4fphotoemission:1||permanent magnet:1||pseudogap:1||TRANSPORTPROPERTIES:1||ANTIFERROMAGNET:1||(BI,PB)SRCOO SYSTEM:1||semicore correlation:1||POLARIZATION:1||CRYSTAL:1||spinel:1||Xray magnetic circular dichroism (XMCD):1||magnetocapacitance:1||ANATASE:1||TEMPERATURES:1||Pseudogap:1||INTERFACE:1||SUBSTRATE:1||YNI2B2C:1||SAMARIUM SULFIDE:1||strong swave superconductor:1||DOPED MANGANITE:1||SYMMETRY:1||CENISN:1||resonance mode:1||DISORDERED SYSTEM:1||LITHIUM INTERCALATION:1||CUO2 PLANE:1||SURFACE:1||Delafossite:1||ELECTRICALPROPERTIES:1||NIMNSB:1||PTMNSB:1||ROOMTEMPERATURE FERROMAGNETISM:1||RUBIDIUM MANGANESE HEXACYANOFERRATE:1||COLOSSALMAGNETORESISTANCE:1||FINITE TEMPERATURES:1||LAMNO3:1||FE:1||transitionmetal oxides:1||giant magnetoresistance:1||phonon:1||COPPER OXIDES:1||valence states:1||thermoelectric:1||semiconductor:1||CATION DISTRIBUTION:1||FeCr2S4:1||photoemission spectroscopy (PES):1||METALLIC FERROMAGNETISM:1||GRAPHITE:1||SUSCEPTIBILITY:1||UBE13:1||RCrSb3:1||band JahnTeller:1||Ce3S4:1||TiO2:1||PrBa2Cu3O7delta:1||UNTWINNED PRBA2CU3O7:1||AGNIO2:1||HALFMETALLIC FERROMAGNETS:1||CI:1||Energy gap:1||Photoemission:1||Future applications:1||Photoemission measurements:1||Graphene:1||BANDSTRUCTURE:1||TC:1||superconductivity:1||magnetic semiconductors:1||CMRmanganites:1||thin films:1||spin dynamics:1||highTc superconductors:1||ITINERANTELECTRON FERROMAGNETISM:1||SINGLECRYSTALS:1||CeTe2:1||amorphous magnetic materials:1||EPITAXIAL GRAPHENE:1||LAYERED PNICTIDEOXIDES:1||BOROCARBIDE SUPERCONDUCTORS:1||AUGMENTEDWAVE METHOD:1||METALLIC MAGNET UNISN:1||ORIGIN:1||spectrum rearrangement:1||MEANFIELD THEORY:1||MOLECULEBASED MAGNETS:1||METASTABLE STATE:1||INSULATOR:1||magnetic orderin:1||FCC IRON:1||CeRu2:1||TL2MN2O7:1||isotope effect:1||Perovskitemanganites:1||RECURSION METHOD:1||PERPENDICULAR MAGNETICANISOTROPY:1||quasiparticle spectral density:1||GW:1||MANGANESE FERRITE:1||RESONANCE:1||SeCuO3:1||Optical conductivity:1||MASSLESS DIRAC FERMIONS:1||SCHOTTKYBARRIER:1||electronic structure:15||ELECTRONICSTRUCTURE:11||TRANSITIONMETAL COMPOUNDS:10||METALS:10||photoemission:8||SPECTRA:8||MAGNETORESISTANCE:7||FERROMAGNETISM:7||TRANSPORT:7||TRANSITION:6||FILMS:6||THINFILMS:5||TOTALENERGY CALCULATIONS:5||MAGNETICPROPERTIES:5||SUPERCONDUCTIVITY:5||PR:5||LATTICE:4||STATES:4||SPECTROSCOPY:4||FIELD:4||CRYSTALSTRUCTURE:4||PHOTOEMISSION:4||TEMPERATURE:4||TRANSITIONTEMPERATURE:4||XRAYABSORPTION:4||STATE:4||CU:4||BASISSET:4||XAS:4||CRYSTALS:3||EXCITATIONS:3||MOTTHUBBARD SYSTEMS:3||HIGHENERGY SPIN:3||halfmetal:3||INSULATORS:3||LA2CUO4:3||MODEL:3||FLUCTUATIONS:3||CE:3||double exchange:3||TRANSITIONMETALS:3||RESISTIVITY:3||BORON:3||LA1XCAXMNO3:3||IRON:3||PES:3||ANTIMONIDES:2||MgB2:2||ZR METALLIC GLASSES:2||superconductor:2||CRITICALCURRENT DENSITY:2||CIRCULARDICHROISM:2||SEMICONDUCTORS:2||LOCALIZATION:2||INTRABAND OPTICAL CONDUCTIVITY:2||COLOSSAL MAGNETORESISTANCE:2||OXIDATION:2||EXISTENCE:2||COPPER:2||diboride:2||MAGNESIUMDIBORIDE:2||GAP:2||CE COMPOUNDS:2||CORE POLARIZATION:2||magnetoresistance:2||photoemission spectroscopy:2||electronphonon interaction:2||GETTER:2||PD:2||MAGNETISM:2||FECR2S4:2||SUPERCONDUCTING MGB2:2||WIRES:2||ABSORPTION:2||ENERGY:2||LA1XSRXMNO3:2||CONSTANTS:2||polaron:2||charge ordering:2||SCATTERING:2||XRAY PHOTOEMISSION:2||CeNiSn:2||phase diagram:2||PHOTOELECTRON:2||QUADRUPOLAR:2||perovskitemanganites:2||CO:2||SYSTEMS:2||DOPED ZNO:2||LOWFREQUENCY SOUND:2||LA:2||ELECTRONELECTRON SCATTERING:2||AU:2||DENSITYWAVE INSTABILITY:2||FERMISURFACE:2||hybridization:2||VALENCEBAND SATELLITE:2||SULFUR SPINEL:2||Heusler:2||APPROXIMATION:2||superexchange:2||colossal magnetoresistance:2||ALLOYS:2||DEPENDENCE:2||AG:2||electronic structures:2||AUGERSPECTRA:2||CR:2||PARAMETERS:2||DIFFRACTION:2||SEMICONDUCTORMETAL TRANSITION:1||INTERMEDIATEVALENCE:1||SMB6:1||SRRUO3:1||antiperovskite structure with antipolar nature:1||lowenergy twodimensional phonons:1||anatase TiO2:1||La3S4:1||metalinsulator transitions:1||MNO:1||ELECTRONICSTRUCTURES:1||MAGNETIC CIRCULARDICHROISM:1||Density functional theory:1||CeCo2:1||TOPOLARON CROSSOVER:1||EXCHANGE:1||cuprates:1||high Tc cuprates:1||magnetically ordered materials:1||ZNSE:1||Sr2xKxFeMoO6:1||CDW:1||TeCuO3:1||STRUCTURALPROPERTIES:1||MN:1||screening length:1||amorphous Fe:1||WAVE BASISSET:1||SILICONCARBIDE:1||HIGHPRESSURE:1||electronphonon coupling:1||quenched superconductivity:1||CMR perovskite manganites:1||OXIDE:1||polarons:1||synchrotron radiation:1||FULLERIDES:1||RESONANTPHOTOEMISSION:1||Silicon carbide:1||DFT calculation:1||Hybridized bands:1||GIANT MAGNETORESISTANCE:1||PEROVSKITES:1||Raman spectra:1||EXCHANGE ENHANCEMENT:1||SILICON:1||SR2FEMOO6:1||orbital ordering:1||delafossite:1||TITANIUMDIOXIDE:1||electronic structure of disordered solids:1||YFE2:1||Magnetic polaron:1||NA2TI2SB2O:1||STRONGCOUPLED SUPERCONDUCTORS:1||HEAVYFERMION SYSTEMS:1||firstprinciples calculations:1||MECHANISM:1||UNiSn:1||PHOTONIC BANDGAP:1||SINGLE IMPURITY:1||PHONONSPECTRUM:1||FERMISURFACE TOPOLOGY:1||SUPPRESSION:1||RESONANT PHOTOEMISSION:1||METALDOPED PICENE:1||PHOTOIONIZATION CROSSSECTIONS:1||PHOTOINDUCED FERRIMAGNETIC SYSTEMS:1||LINKAGE ISOMERISM:1||CHARGETRANSFER:1||Bilayer Graphene:1||MAGNETICFIELD:1||SPINWAVES:1||rareearth manganese oxides:1||magnonphonon interaction:1||NACO2O4:1||ENERGYBANDS:1||SELFENERGY:1||GAS:1||Fe0.5Cu0.5Cr2S4:1||scanning photoelectron microscopy (SPEM):1||MAGNETIC PROPERTIES:1||Stoner model:1||AMORPHOUS TRANSITIONMETALS:1||SPINGLASS STATES:1||NI:1||LA3NI2B2N3:1||SOLIDS:1||CEO2:1||BAND THEORY:1||dilute magnetic semiconductor:1||pyrochlore:1||Y1XPRXBA2CU3O7DELTA:1||and electronphonon interactions:1||VIBRATIONS:1||RAY PHOTOEMISSION:1||ALKALI CATION:1||Europium:1||colossal magnetoresistance:1||structural stability:1||ENERGYGAP:1||small polaron:1||DOUBLE EXCHANGE:1||Coulomb correlation:1||magnon:1||phonons:1||ELECTRON FERROMAGNETISM:1||CURIETEMPERATURE:1||ARPES:1||PLANEWAVE METHOD:1||Xray absorption spectroscopy (XAS):1||ROOMTEMPERATURE:1||MONOCHALCOGENIDES:1||HEAT:1||UPDSN:1||MOMENTS:1||XRAY ABSORPTION:1||SEMICONDUCTOR:1||Fermi surface nesting:1||optical phonon:1||disordered system:1||dilute magnetic semiconductors:1||CMR manganites:1||PHONONS:1||LATTICEDYNAMICS:1||OXIDES:1||4fphotoemission:1||permanent magnet:1||pseudogap:1||TRANSPORTPROPERTIES:1||ANTIFERROMAGNET:1||(BI,PB)SRCOO SYSTEM:1||semicore correlation:1||POLARIZATION:1||CRYSTAL:1||spinel:1||Xray magnetic circular dichroism (XMCD):1||magnetocapacitance:1||ANATASE:1||TEMPERATURES:1||Pseudogap:1||INTERFACE:1||SUBSTRATE:1||YNI2B2C:1||SAMARIUM SULFIDE:1||strong swave superconductor:1||DOPED MANGANITE:1||SYMMETRY:1||CENISN:1||resonance mode:1||DISORDERED SYSTEM:1||LITHIUM INTERCALATION:1||CUO2 PLANE:1||SURFACE:1||Delafossite:1||ELECTRICALPROPERTIES:1||NIMNSB:1||PTMNSB:1||ROOMTEMPERATURE FERROMAGNETISM:1||RUBIDIUM MANGANESE HEXACYANOFERRATE:1||COLOSSALMAGNETORESISTANCE:1||FINITE TEMPERATURES:1||LAMNO3:1||FE:1||transitionmetal oxides:1||giant magnetoresistance:1||phonon:1||COPPER OXIDES:1||valence states:1||thermoelectric:1||semiconductor:1||CATION DISTRIBUTION:1||FeCr2S4:1||photoemission spectroscopy (PES):1||METALLIC FERROMAGNETISM:1||GRAPHITE:1||SUSCEPTIBILITY:1||UBE13:1||RCrSb3:1||band JahnTeller:1||Ce3S4:1||TiO2:1||PrBa2Cu3O7delta:1||UNTWINNED PRBA2CU3O7:1||AGNIO2:1||HALFMETALLIC FERROMAGNETS:1||CI:1||Energy gap:1||Photoemission:1||Future applications:1||Photoemission measurements:1||Graphene:1||BANDSTRUCTURE:1||TC:1||superconductivity:1||magnetic semiconductors:1||CMRmanganites:1||thin films:1||spin dynamics:1||highTc superconductors:1||ITINERANTELECTRON FERROMAGNETISM:1||SINGLECRYSTALS:1||CeTe2:1||amorphous magnetic materials:1||EPITAXIAL GRAPHENE:1||LAYERED PNICTIDEOXIDES:1||BOROCARBIDE SUPERCONDUCTORS:1||AUGMENTEDWAVE METHOD:1||METALLIC MAGNET UNISN:1||ORIGIN:1||spectrum rearrangement:1||MEANFIELD THEORY:1||MOLECULEBASED MAGNETS:1||METASTABLE STATE:1||INSULATOR:1||magnetic orderin:1||FCC IRON:1||CeRu2:1||TL2MN2O7:1||isotope effect:1||Perovskitemanganites:1||RECURSION METHOD:1||PERPENDICULAR MAGNETICANISOTROPY:1||quasiparticle spectral density:1||GW:1||MANGANESE FERRITE:1||RESONANCE:1||SeCuO3:1||Optical conductivity:1||MASSLESS DIRAC FERMIONS:1||SCHOTTKYBARRIER:1||electronic structure:15||ELECTRONICSTRUCTURE:11||TRANSITIONMETAL COMPOUNDS:10||METALS:10||photoemission:8||SPECTRA:8||MAGNETORESISTANCE:7||FERROMAGNETISM:7||TRANSPORT:7||TRANSITION:6||FILMS:6||THINFILMS:5||TOTALENERGY CALCULATIONS:5||MAGNETICPROPERTIES:5||SUPERCONDUCTIVITY:5||PR:5||LATTICE:4||STATES:4||SPECTROSCOPY:4||FIELD:4||CRYSTALSTRUCTURE:4||PHOTOEMISSION:4||TEMPERATURE:4||TRANSITIONTEMPERATURE:4||XRAYABSORPTION:4||STATE:4||CU:4||BASISSET:4||XAS:4||CRYSTALS:3||EXCITATIONS:3||MOTTHUBBARD SYSTEMS:3||HIGHENERGY SPIN:3||halfmetal:3||INSULATORS:3||LA2CUO4:3||MODEL:3||FLUCTUATIONS:3||CE:3||double exchange:3||TRANSITIONMETALS:3||RESISTIVITY:3||BORON:3||LA1XCAXMNO3:3||IRON:3||PES:3||ANTIMONIDES:2||MgB2:2||ZR METALLIC GLASSES:2||superconductor:2||CRITICALCURRENT DENSITY:2||CIRCULARDICHROISM:2||SEMICONDUCTORS:2||LOCALIZATION:2||INTRABAND OPTICAL CONDUCTIVITY:2||COLOSSAL MAGNETORESISTANCE:2||OXIDATION:2||EXISTENCE:2||COPPER:2||diboride:2||MAGNESIUMDIBORIDE:2||GAP:2||CE COMPOUNDS:2||CORE POLARIZATION:2||magnetoresistance:2||photoemission spectroscopy:2||electronphonon interaction:2||GETTER:2||PD:2||MAGNETISM:2||FECR2S4:2||SUPERCONDUCTING MGB2:2||WIRES:2||ABSORPTION:2||ENERGY:2||LA1XSRXMNO3:2||CONSTANTS:2||polaron:2||charge ordering:2||SCATTERING:2||XRAY PHOTOEMISSION:2||CeNiSn:2||phase diagram:2||PHOTOELECTRON:2||QUADRUPOLAR:2||perovskitemanganites:2||CO:2||SYSTEMS:2||DOPED ZNO:2||LOWFREQUENCY SOUND:2||LA:2||ELECTRONELECTRON SCATTERING:2||AU:2||DENSITYWAVE INSTABILITY:2||FERMISURFACE:2||hybridization:2||VALENCEBAND SATELLITE:2||SULFUR SPINEL:2||Heusler:2||APPROXIMATION:2||superexchange:2||colossal magnetoresistance:2||ALLOYS:2||DEPENDENCE:2||AG:2||electronic structures:2||AUGERSPECTRA:2||CR:2||PARAMETERS:2||DIFFRACTION:2||SEMICONDUCTORMETAL TRANSITION:1||INTERMEDIATEVALENCE:1||SMB6:1||SRRUO3:1||antiperovskite structure with antipolar nature:1||lowenergy twodimensional phonons:1||anatase TiO2:1||La3S4:1||metalinsulator transitions:1||MNO:1||ELECTRONICSTRUCTURES:1||MAGNETIC CIRCULARDICHROISM:1||Density functional theory:1||CeCo2:1||TOPOLARON CROSSOVER:1||EXCHANGE:1||cuprates:1||high Tc cuprates:1||magnetically ordered materials:1||ZNSE:1||Sr2xKxFeMoO6:1||CDW:1||TeCuO3:1||STRUCTURALPROPERTIES:1||MN:1||screening length:1||amorphous Fe:1||WAVE BASISSET:1||SILICONCARBIDE:1||HIGHPRESSURE:1||electronphonon coupling:1||quenched superconductivity:1||CMR perovskite manganites:1||OXIDE:1||polarons:1||synchrotron radiation:1||FULLERIDES:1||RESONANTPHOTOEMISSION:1||Silicon carbide:1||DFT calculation:1||Hybridized bands:1||GIANT MAGNETORESISTANCE:1||PEROVSKITES:1||Raman spectra:1||EXCHANGE ENHANCEMENT:1||SILICON:1||SR2FEMOO6:1||orbital ordering:1||delafossite:1||TITANIUMDIOXIDE:1||electronic structure of disordered solids:1||YFE2:1||Magnetic polaron:1||NA2TI2SB2O:1||STRONGCOUPLED SUPERCONDUCTORS:1||HEAVYFERMION SYSTEMS:1||firstprinciples calculations:1||MECHANISM:1||UNiSn:1||PHOTONIC BANDGAP:1||SINGLE IMPURITY:1||PHONONSPECTRUM:1||FERMISURFACE TOPOLOGY:1||SUPPRESSION:1||RESONANT PHOTOEMISSION:1||METALDOPED PICENE:1||PHOTOIONIZATION CROSSSECTIONS:1||PHOTOINDUCED FERRIMAGNETIC SYSTEMS:1||LINKAGE ISOMERISM:1||CHARGETRANSFER:1||Bilayer Graphene:1||MAGNETICFIELD:1||SPINWAVES:1||rareearth manganese oxides:1||magnonphonon interaction:1||NACO2O4:1||ENERGYBANDS:1||SELFENERGY:1||GAS:1||Fe0.5Cu0.5Cr2S4:1||scanning photoelectron microscopy (SPEM):1||MAGNETIC PROPERTIES:1||Stoner model:1||AMORPHOUS TRANSITIONMETALS:1||SPINGLASS STATES:1||NI:1||LA3NI2B2N3:1||SOLIDS:1||CEO2:1||BAND THEORY:1||dilute magnetic semiconductor:1||pyrochlore:1||Y1XPRXBA2CU3O7DELTA:1||and electronphonon interactions:1||VIBRATIONS:1||RAY PHOTOEMISSION:1||ALKALI CATION:1||Europium:1||colossal magnetoresistance:1||structural stability:1||ENERGYGAP:1||small polaron:1||DOUBLE EXCHANGE:1||Coulomb correlation:1||magnon:1||phonons:1||ELECTRON FERROMAGNETISM:1||CURIETEMPERATURE:1||ARPES:1||PLANEWAVE METHOD:1||Xray absorption spectroscopy (XAS):1||ROOMTEMPERATURE:1||MONOCHALCOGENIDES:1||HEAT:1||UPDSN:1||MOMENTS:1||XRAY ABSORPTION:1||SEMICONDUCTOR:1||Fermi surface nesting:1||optical phonon:1||disordered system:1||dilute magnetic semiconductors:1||CMR manganites:1||PHONONS:1||LATTICEDYNAMICS:1||OXIDES:1||4fphotoemission:1||permanent magnet:1||pseudogap:1||TRANSPORTPROPERTIES:1||ANTIFERROMAGNET:1||(BI,PB)SRCOO SYSTEM:1||semicore correlation:1||POLARIZATION:1||CRYSTAL:1||spinel:1||Xray magnetic circular dichroism (XMCD):1||magnetocapacitance:1||ANATASE:1||TEMPERATURES:1||Pseudogap:1||INTERFACE:1||SUBSTRATE:1||YNI2B2C:1||SAMARIUM SULFIDE:1||strong swave superconductor:1||DOPED MANGANITE:1||SYMMETRY:1||CENISN:1||resonance mode:1||DISORDERED SYSTEM:1||LITHIUM INTERCALATION:1||CUO2 PLANE:1||SURFACE:1||Delafossite:1||ELECTRICALPROPERTIES:1||NIMNSB:1||PTMNSB:1||ROOMTEMPERATURE FERROMAGNETISM:1||RUBIDIUM MANGANESE HEXACYANOFERRATE:1||COLOSSALMAGNETORESISTANCE:1||FINITE TEMPERATURES:1||LAMNO3:1||FE:1||transitionmetal oxides:1||giant magnetoresistance:1||phonon:1||COPPER OXIDES:1||valence states:1||thermoelectric:1||semiconductor:1||CATION DISTRIBUTION:1||FeCr2S4:1||photoemission spectroscopy (PES):1||METALLIC FERROMAGNETISM:1||GRAPHITE:1||SUSCEPTIBILITY:1||UBE13:1||RCrSb3:1||band JahnTeller:1||Ce3S4:1||TiO2:1||PrBa2Cu3O7delta:1||UNTWINNED PRBA2CU3O7:1||AGNIO2:1||HALFMETALLIC FERROMAGNETS:1||CI:1||Energy gap:1||Photoemission:1||Future applications:1||Photoemission measurements:1||Graphene:1||BANDSTRUCTURE:1||TC:1||superconductivity:1||magnetic semiconductors:1||CMRmanganites:1||thin films:1||spin dynamics:1||highTc superconductors:1||ITINERANTELECTRON FERROMAGNETISM:1||SINGLECRYSTALS:1||CeTe2:1||amorphous magnetic materials:1||EPITAXIAL GRAPHENE:1||LAYERED PNICTIDEOXIDES:1||BOROCARBIDE SUPERCONDUCTORS:1||AUGMENTEDWAVE METHOD:1||METALLIC MAGNET UNISN:1||ORIGIN:1||spectrum rearrangement:1||MEANFIELD THEORY:1||MOLECULEBASED MAGNETS:1||METASTABLE STATE:1||INSULATOR:1||magnetic orderin:1||FCC IRON:1||CeRu2:1||TL2MN2O7:1||isotope effect:1||Perovskitemanganites:1||RECURSION METHOD:1||PERPENDICULAR MAGNETICANISOTROPY:1||quasiparticle spectral density:1||GW:1||MANGANESE FERRITE:1||RESONANCE:1||SeCuO3:1||Optical conductivity:1||MASSLESS DIRAC FERMIONS:1||SCHOTTKYBARRIER:1||electronic structure:15||ELECTRONICSTRUCTURE:11||TRANSITIONMETAL COMPOUNDS:10||METALS:10||photoemission:8||SPECTRA:8||MAGNETORESISTANCE:7||FERROMAGNETISM:7||TRANSPORT:7||TRANSITION:6||FILMS:6||THINFILMS:5||TOTALENERGY CALCULATIONS:5||MAGNETICPROPERTIES:5||SUPERCONDUCTIVITY:5||PR:5||LATTICE:4||STATES:4||SPECTROSCOPY:4||FIELD:4||CRYSTALSTRUCTURE:4||PHOTOEMISSION:4||TEMPERATURE:4||TRANSITIONTEMPERATURE:4||XRAYABSORPTION:4||STATE:4||CU:4||BASISSET:4||XAS:4||CRYSTALS:3||EXCITATIONS:3||MOTTHUBBARD SYSTEMS:3||HIGHENERGY SPIN:3||halfmetal:3||INSULATORS:3||LA2CUO4:3||MODEL:3||FLUCTUATIONS:3||CE:3||double exchange:3||TRANSITIONMETALS:3||RESISTIVITY:3||BORON:3||LA1XCAXMNO3:3||IRON:3||PES:3||ANTIMONIDES:2||MgB2:2||ZR METALLIC GLASSES:2||superconductor:2||CRITICALCURRENT DENSITY:2||CIRCULARDICHROISM:2||SEMICONDUCTORS:2||LOCALIZATION:2||INTRABAND OPTICAL CONDUCTIVITY:2||COLOSSAL MAGNETORESISTANCE:2||OXIDATION:2||EXISTENCE:2||COPPER:2||diboride:2||MAGNESIUMDIBORIDE:2||GAP:2||CE COMPOUNDS:2||CORE POLARIZATION:2||magnetoresistance:2||photoemission spectroscopy:2||electronphonon interaction:2||GETTER:2||PD:2||MAGNETISM:2||FECR2S4:2||SUPERCONDUCTING MGB2:2||WIRES:2||ABSORPTION:2||ENERGY:2||LA1XSRXMNO3:2||CONSTANTS:2||polaron:2||charge ordering:2||SCATTERING:2||XRAY PHOTOEMISSION:2||CeNiSn:2||phase diagram:2||PHOTOELECTRON:2||QUADRUPOLAR:2||perovskitemanganites:2||CO:2||SYSTEMS:2||DOPED ZNO:2||LOWFREQUENCY SOUND:2||LA:2||ELECTRONELECTRON SCATTERING:2||AU:2||DENSITYWAVE INSTABILITY:2||FERMISURFACE:2||hybridization:2||VALENCEBAND SATELLITE:2||SULFUR SPINEL:2||Heusler:2||APPROXIMATION:2||superexchange:2||colossal magnetoresistance:2||ALLOYS:2||DEPENDENCE:2||AG:2||electronic structures:2||AUGERSPECTRA:2||CR:2||PARAMETERS:2||DIFFRACTION:2||SEMICONDUCTORMETAL TRANSITION:1||INTERMEDIATEVALENCE:1||SMB6:1||SRRUO3:1||antiperovskite structure with antipolar nature:1||lowenergy twodimensional phonons:1||anatase TiO2:1||La3S4:1||metalinsulator transitions:1||MNO:1||ELECTRONICSTRUCTURES:1||MAGNETIC CIRCULARDICHROISM:1||Density functional theory:1||CeCo2:1||TOPOLARON CROSSOVER:1||EXCHANGE:1||cuprates:1||high Tc cuprates:1||magnetically ordered materials:1||ZNSE:1||Sr2xKxFeMoO6:1||CDW:1||TeCuO3:1||STRUCTURALPROPERTIES:1||MN:1||screening length:1||amorphous Fe:1||WAVE BASISSET:1||SILICONCARBIDE:1||HIGHPRESSURE:1||electronphonon coupling:1||quenched superconductivity:1||CMR perovskite manganites:1||OXIDE:1||polarons:1||synchrotron radiation:1||FULLERIDES:1||RESONANTPHOTOEMISSION:1||Silicon carbide:1||DFT calculation:1||Hybridized bands:1||GIANT MAGNETORESISTANCE:1||PEROVSKITES:1||Raman spectra:1||EXCHANGE ENHANCEMENT:1||SILICON:1||SR2FEMOO6:1||orbital ordering:1||delafossite:1||TITANIUMDIOXIDE:1||electronic structure of disordered solids:1||YFE2:1||Magnetic polaron:1||NA2TI2SB2O:1||STRONGCOUPLED SUPERCONDUCTORS:1||HEAVYFERMION SYSTEMS:1||firstprinciples calculations:1||MECHANISM:1||UNiSn:1||PHOTONIC BANDGAP:1||SINGLE IMPURITY:1||PHONONSPECTRUM:1||FERMISURFACE TOPOLOGY:1||SUPPRESSION:1||RESONANT PHOTOEMISSION:1||METALDOPED PICENE:1||PHOTOIONIZATION CROSSSECTIONS:1||PHOTOINDUCED FERRIMAGNETIC SYSTEMS:1||LINKAGE ISOMERISM:1||CHARGETRANSFER:1||Bilayer Graphene:1||MAGNETICFIELD:1||SPINWAVES:1||rareearth manganese oxides:1||magnonphonon interaction:1||NACO2O4:1||ENERGYBANDS:1||SELFENERGY:1||GAS:1||Fe0.5Cu0.5Cr2S4:1||scanning photoelectron microscopy (SPEM):1||MAGNETIC PROPERTIES:1||Stoner model:1||AMORPHOUS TRANSITIONMETALS:1||SPINGLASS STATES:1||NI:1||LA3NI2B2N3:1||SOLIDS:1||CEO2:1||BAND THEORY:1||dilute magnetic semiconductor:1||pyrochlore:1||Y1XPRXBA2CU3O7DELTA:1||and electronphonon interactions:1||VIBRATIONS:1||RAY PHOTOEMISSION:1||ALKALI CATION:1||Europium:1||colossal magnetoresistance:1||structural stability:1||ENERGYGAP:1||small polaron:1||DOUBLE EXCHANGE:1||Coulomb correlation:1||magnon:1||phonons:1||ELECTRON FERROMAGNETISM:1||CURIETEMPERATURE:1||ARPES:1||PLANEWAVE METHOD:1||Xray absorption spectroscopy (XAS):1||ROOMTEMPERATURE:1||MONOCHALCOGENIDES:1||HEAT:1||UPDSN:1||MOMENTS:1||XRAY ABSORPTION:1||SEMICONDUCTOR:1||Fermi surface nesting:1||optical phonon:1||disordered system:1||dilute magnetic semiconductors:1||CMR manganites:1||PHONONS:1||LATTICEDYNAMICS:1||OXIDES:1||4fphotoemission:1||permanent magnet:1||pseudogap:1||TRANSPORTPROPERTIES:1||ANTIFERROMAGNET:1||(BI,PB)SRCOO SYSTEM:1||semicore correlation:1||POLARIZATION:1||CRYSTAL:1||spinel:1||Xray magnetic circular dichroism (XMCD):1||magnetocapacitance:1||ANATASE:1||TEMPERATURES:1||Pseudogap:1||INTERFACE:1||SUBSTRATE:1||YNI2B2C:1||SAMARIUM SULFIDE:1||strong swave superconductor:1||DOPED MANGANITE:1||SYMMETRY:1||CENISN:1||resonance mode:1||DISORDERED SYSTEM:1||LITHIUM INTERCALATION:1||CUO2 PLANE:1||SURFACE:1||Delafossite:1||ELECTRICALPROPERTIES:1||NIMNSB:1||PTMNSB:1||ROOMTEMPERATURE FERROMAGNETISM:1||RUBIDIUM MANGANESE HEXACYANOFERRATE:1||COLOSSALMAGNETORESISTANCE:1||FINITE TEMPERATURES:1||LAMNO3:1||FE:1||transitionmetal oxides:1||giant magnetoresistance:1||phonon:1||COPPER OXIDES:1||valence states:1||thermoelectric:1||semiconductor:1||CATION DISTRIBUTION:1||FeCr2S4:1||photoemission spectroscopy (PES):1||METALLIC FERROMAGNETISM:1||GRAPHITE:1||SUSCEPTIBILITY:1||UBE13:1||RCrSb3:1||band JahnTeller:1||Ce3S4:1||TiO2:1||PrBa2Cu3O7delta:1||UNTWINNED PRBA2CU3O7:1||AGNIO2:1||HALFMETALLIC FERROMAGNETS:1||CI:1||Energy gap:1||Photoemission:1||Future applications:1||Photoemission measurements:1||Graphene:1||BANDSTRUCTURE:1||TC:1||superconductivity:1||magnetic semiconductors:1||CMRmanganites:1||thin films:1||spin dynamics:1||highTc superconductors:1||ITINERANTELECTRON FERROMAGNETISM:1||SINGLECRYSTALS:1||CeTe2:1||amorphous magnetic materials:1||EPITAXIAL GRAPHENE:1||LAYERED PNICTIDEOXIDES:1||BOROCARBIDE SUPERCONDUCTORS:1||AUGMENTEDWAVE METHOD:1||METALLIC MAGNET UNISN:1||ORIGIN:1||spectrum rearrangement:1||MEANFIELD THEORY:1||MOLECULEBASED MAGNETS:1||METASTABLE STATE:1||INSULATOR:1||magnetic orderin:1||FCC IRON:1||CeRu2:1||TL2MN2O7:1||isotope effect:1||Perovskitemanganites:1||RECURSION METHOD:1||PERPENDICULAR MAGNETICANISOTROPY:1||quasiparticle spectral density:1||GW:1||MANGANESE FERRITE:1||RESONANCE:1||SeCuO3:1||Optical conductivity:1||MASSLESS DIRAC FERMIONS:1||SCHOTTKYBARRIER:1||electronic structure:15||ELECTRONICSTRUCTURE:11||TRANSITIONMETAL COMPOUNDS:10||METALS:10||photoemission:8||SPECTRA:8||MAGNETORESISTANCE:7||FERROMAGNETISM:7||TRANSPORT:7||TRANSITION:6||FILMS:6||THINFILMS:5||TOTALENERGY CALCULATIONS:5||MAGNETICPROPERTIES:5||SUPERCONDUCTIVITY:5||PR:5||LATTICE:4||STATES:4||SPECTROSCOPY:4||FIELD:4||CRYSTALSTRUCTURE:4||PHOTOEMISSION:4||TEMPERATURE:4||TRANSITIONTEMPERATURE:4||XRAYABSORPTION:4||STATE:4||CU:4||BASISSET:4||XAS:4||CRYSTALS:3||EXCITATIONS:3||MOTTHUBBARD SYSTEMS:3||HIGHENERGY SPIN:3||halfmetal:3||INSULATORS:3||LA2CUO4:3||MODEL:3||FLUCTUATIONS:3||CE:3||double exchange:3||TRANSITIONMETALS:3||RESISTIVITY:3||BORON:3||LA1XCAXMNO3:3||IRON:3||PES:3||ANTIMONIDES:2||MgB2:2||ZR METALLIC GLASSES:2||superconductor:2||CRITICALCURRENT DENSITY:2||CIRCULARDICHROISM:2||SEMICONDUCTORS:2||LOCALIZATION:2||INTRABAND OPTICAL CONDUCTIVITY:2||COLOSSAL MAGNETORESISTANCE:2||OXIDATION:2||EXISTENCE:2||COPPER:2||diboride:2||MAGNESIUMDIBORIDE:2||GAP:2||CE COMPOUNDS:2||CORE POLARIZATION:2||magnetoresistance:2||photoemission spectroscopy:2||electronphonon interaction:2||GETTER:2||PD:2||MAGNETISM:2||FECR2S4:2||SUPERCONDUCTING MGB2:2||WIRES:2||ABSORPTION:2||ENERGY:2||LA1XSRXMNO3:2||CONSTANTS:2||polaron:2||charge ordering:2||SCATTERING:2||XRAY PHOTOEMISSION:2||CeNiSn:2||phase diagram:2||PHOTOELECTRON:2||QUADRUPOLAR:2||perovskitemanganites:2||CO:2||SYSTEMS:2||DOPED ZNO:2||LOWFREQUENCY SOUND:2||LA:2||ELECTRONELECTRON SCATTERING:2||AU:2||DENSITYWAVE INSTABILITY:2||FERMISURFACE:2||hybridization:2||VALENCEBAND SATELLITE:2||SULFUR SPINEL:2||Heusler:2||APPROXIMATION:2||superexchange:2||colossal magnetoresistance:2||ALLOYS:2||DEPENDENCE:2||AG:2||electronic structures:2||AUGERSPECTRA:2||CR:2||PARAMETERS:2||DIFFRACTION:2||SEMICONDUCTORMETAL TRANSITION:1||INTERMEDIATEVALENCE:1||SMB6:1||SRRUO3:1||antiperovskite structure with antipolar nature:1||lowenergy twodimensional phonons:1||anatase TiO2:1||La3S4:1||metalinsulator transitions:1||MNO:1||ELECTRONICSTRUCTURES:1||MAGNETIC CIRCULARDICHROISM:1||Density functional theory:1||CeCo2:1||TOPOLARON CROSSOVER:1||EXCHANGE:1||cuprates:1||high Tc cuprates:1||magnetically ordered materials:1||ZNSE:1||Sr2xKxFeMoO6:1||CDW:1||TeCuO3:1||STRUCTURALPROPERTIES:1||MN:1||screening length:1||amorphous Fe:1||WAVE BASISSET:1||SILICONCARBIDE:1||HIGHPRESSURE:1||electronphonon coupling:1||quenched superconductivity:1||CMR perovskite manganites:1||OXIDE:1||polarons:1||synchrotron radiation:1||FULLERIDES:1||RESONANTPHOTOEMISSION:1||Silicon carbide:1||DFT calculation:1||Hybridized bands:1||GIANT MAGNETORESISTANCE:1||PEROVSKITES:1||Raman spectra:1||EXCHANGE ENHANCEMENT:1||SILICON:1||SR2FEMOO6:1||orbital ordering:1||delafossite:1||TITANIUMDIOXIDE:1||electronic structure of disordered solids:1||YFE2:1||Magnetic polaron:1||NA2TI2SB2O:1||STRONGCOUPLED SUPERCONDUCTORS:1||HEAVYFERMION SYSTEMS:1||firstprinciples calculations:1||MECHANISM:1||UNiSn:1||PHOTONIC BANDGAP:1||SINGLE IMPURITY:1||PHONONSPECTRUM:1||FERMISURFACE TOPOLOGY:1||SUPPRESSION:1||RESONANT PHOTOEMISSION:1||METALDOPED PICENE:1||PHOTOIONIZATION CROSSSECTIONS:1||PHOTOINDUCED FERRIMAGNETIC SYSTEMS:1||LINKAGE ISOMERISM:1||CHARGETRANSFER:1||Bilayer Graphene:1||MAGNETICFIELD:1||SPINWAVES:1||rareearth manganese oxides:1||magnonphonon interaction:1||NACO2O4:1||ENERGYBANDS:1||SELFENERGY:1||GAS:1||Fe0.5Cu0.5Cr2S4:1||scanning photoelectron microscopy (SPEM):1||MAGNETIC PROPERTIES:1||Stoner model:1||AMORPHOUS TRANSITIONMETALS:1||SPINGLASS STATES:1||NI:1||LA3NI2B2N3:1||SOLIDS:1||CEO2:1||BAND THEORY:1||dilute magnetic semiconductor:1||pyrochlore:1||Y1XPRXBA2CU3O7DELTA:1||and electronphonon interactions:1||VIBRATIONS:1||RAY PHOTOEMISSION:1||ALKALI CATION:1||Europium:1||colossal magnetoresistance:1||structural stability:1||ENERGYGAP:1||small polaron:1||DOUBLE EXCHANGE:1||Coulomb correlation:1||magnon:1||phonons:1||ELECTRON FERROMAGNETISM:1||CURIETEMPERATURE:1||ARPES:1||PLANEWAVE METHOD:1||Xray absorption spectroscopy (XAS):1||ROOMTEMPERATURE:1||MONOCHALCOGENIDES:1||HEAT:1||UPDSN:1||MOMENTS:1||XRAY ABSORPTION:1||SEMICONDUCTOR:1||Fermi surface nesting:1||optical phonon:1||disordered system:1||dilute magnetic semiconductors:1||CMR manganites:1||PHONONS:1||LATTICEDYNAMICS:1||OXIDES:1||4fphotoemission:1||permanent magnet:1||pseudogap:1||TRANSPORTPROPERTIES:1||ANTIFERROMAGNET:1||(BI,PB)SRCOO SYSTEM:1||semicore correlation:1||POLARIZATION:1||CRYSTAL:1||spinel:1||Xray magnetic circular dichroism (XMCD):1||magnetocapacitance:1||ANATASE:1||TEMPERATURES:1||Pseudogap:1||INTERFACE:1||SUBSTRATE:1||YNI2B2C:1||SAMARIUM SULFIDE:1||strong swave superconductor:1||DOPED MANGANITE:1||SYMMETRY:1||CENISN:1||resonance mode:1||DISORDERED SYSTEM:1||LITHIUM INTERCALATION:1||CUO2 PLANE:1||SURFACE:1||Delafossite:1||ELECTRICALPROPERTIES:1||NIMNSB:1||PTMNSB:1||ROOMTEMPERATURE FERROMAGNETISM:1||RUBIDIUM MANGANESE HEXACYANOFERRATE:1||COLOSSALMAGNETORESISTANCE:1||FINITE TEMPERATURES:1||LAMNO3:1||FE:1||transitionmetal oxides:1||giant magnetoresistance:1||phonon:1||COPPER OXIDES:1||valence states:1||thermoelectric:1||semiconductor:1||CATION DISTRIBUTION:1||FeCr2S4:1||photoemission spectroscopy (PES):1||METALLIC FERROMAGNETISM:1||GRAPHITE:1||SUSCEPTIBILITY:1||UBE13:1||RCrSb3:1||band JahnTeller:1||Ce3S4:1||TiO2:1||PrBa2Cu3O7delta:1||UNTWINNED PRBA2CU3O7:1||AGNIO2:1||HALFMETALLIC FERROMAGNETS:1||CI:1||Energy gap:1||Photoemission:1||Future applications:1||Photoemission measurements:1||Graphene:1||BANDSTRUCTURE:1||TC:1||superconductivity:1||magnetic semiconductors:1||CMRmanganites:1||thin films:1||spin dynamics:1||highTc superconductors:1||ITINERANTELECTRON FERROMAGNETISM:1||SINGLECRYSTALS:1||CeTe2:1||amorphous magnetic materials:1||EPITAXIAL GRAPHENE:1||LAYERED PNICTIDEOXIDES:1||BOROCARBIDE SUPERCONDUCTORS:1||AUGMENTEDWAVE METHOD:1||METALLIC MAGNET UNISN:1||ORIGIN:1||spectrum rearrangement:1||MEANFIELD THEORY:1||MOLECULEBASED MAGNETS:1||METASTABLE STATE:1||INSULATOR:1||magnetic orderin:1||FCC IRON:1||CeRu2:1||TL2MN2O7:1||isotope effect:1||Perovskitemanganites:1||RECURSION METHOD:1||PERPENDICULAR MAGNETICANISOTROPY:1||quasiparticle spectral density:1||GW:1||MANGANESE FERRITE:1||RESONANCE:1||SeCuO3:1||Optical conductivity:1||MASSLESS DIRAC FERMIONS:1||SCHOTTKYBARRIER:1||electronic structure:15||ELECTRONICSTRUCTURE:11||TRANSITIONMETAL COMPOUNDS:10||METALS:10||photoemission:8||SPECTRA:8||MAGNETORESISTANCE:7||FERROMAGNETISM:7||TRANSPORT:7||TRANSITION:6||FILMS:6||THINFILMS:5||TOTALENERGY CALCULATIONS:5||MAGNETICPROPERTIES:5||SUPERCONDUCTIVITY:5||PR:5||LATTICE:4||STATES:4||SPECTROSCOPY:4||FIELD:4||CRYSTALSTRUCTURE:4||PHOTOEMISSION:4||TEMPERATURE:4||TRANSITIONTEMPERATURE:4||XRAYABSORPTION:4||STATE:4||CU:4||BASISSET:4||XAS:4||CRYSTALS:3||EXCITATIONS:3||MOTTHUBBARD SYSTEMS:3||HIGHENERGY SPIN:3||halfmetal:3||INSULATORS:3||LA2CUO4:3||MODEL:3||FLUCTUATIONS:3||CE:3||double exchange:3||TRANSITIONMETALS:3||RESISTIVITY:3||BORON:3||LA1XCAXMNO3:3||IRON:3||PES:3||ANTIMONIDES:2||MgB2:2||ZR METALLIC GLASSES:2||superconductor:2||CRITICALCURRENT DENSITY:2||CIRCULARDICHROISM:2||SEMICONDUCTORS:2||LOCALIZATION:2||INTRABAND OPTICAL CONDUCTIVITY:2||COLOSSAL MAGNETORESISTANCE:2||OXIDATION:2||EXISTENCE:2||COPPER:2||diboride:2||MAGNESIUMDIBORIDE:2||GAP:2||CE COMPOUNDS:2||CORE POLARIZATION:2||magnetoresistance:2||photoemission spectroscopy:2||electronphonon interaction:2||GETTER:2||PD:2||MAGNETISM:2||FECR2S4:2||SUPERCONDUCTING MGB2:2||WIRES:2||ABSORPTION:2||ENERGY:2||LA1XSRXMNO3:2||CONSTANTS:2||polaron:2||charge ordering:2||SCATTERING:2||XRAY PHOTOEMISSION:2||CeNiSn:2||phase diagram:2||PHOTOELECTRON:2||QUADRUPOLAR:2||perovskitemanganites:2||CO:2||SYSTEMS:2||DOPED ZNO:2||LOWFREQUENCY SOUND:2||LA:2||ELECTRONELECTRON SCATTERING:2||AU:2||DENSITYWAVE INSTABILITY:2||FERMISURFACE:2||hybridization:2||VALENCEBAND SATELLITE:2||SULFUR SPINEL:2||Heusler:2||APPROXIMATION:2||superexchange:2||colossal magnetoresistance:2||ALLOYS:2||DEPENDENCE:2||AG:2||electronic structures:2||AUGERSPECTRA:2||CR:2||PARAMETERS:2||DIFFRACTION:2||SEMICONDUCTORMETAL TRANSITION:1||INTERMEDIATEVALENCE:1||SMB6:1||SRRUO3:1||antiperovskite structure with antipolar nature:1||lowenergy twodimensional phonons:1||anatase TiO2:1||La3S4:1||metalinsulator transitions:1||MNO:1||ELECTRONICSTRUCTURES:1||MAGNETIC CIRCULARDICHROISM:1||Density functional theory:1||CeCo2:1||TOPOLARON CROSSOVER:1||EXCHANGE:1||cuprates:1||high Tc cuprates:1||magnetically ordered materials:1||ZNSE:1||Sr2xKxFeMoO6:1||CDW:1||TeCuO3:1||STRUCTURALPROPERTIES:1||MN:1||screening length:1||amorphous Fe:1||WAVE BASISSET:1||SILICONCARBIDE:1||HIGHPRESSURE:1||electronphonon coupling:1||quenched superconductivity:1||CMR perovskite manganites:1||OXIDE:1||polarons:1||synchrotron radiation:1||FULLERIDES:1||RESONANTPHOTOEMISSION:1||Silicon carbide:1||DFT calculation:1||Hybridized bands:1||GIANT MAGNETORESISTANCE:1||PEROVSKITES:1||Raman spectra:1||EXCHANGE ENHANCEMENT:1||SILICON:1||SR2FEMOO6:1||orbital ordering:1||delafossite:1||TITANIUMDIOXIDE:1||electronic structure of disordered solids:1||YFE2:1||Magnetic polaron:1||NA2TI2SB2O:1||STRONGCOUPLED SUPERCONDUCTORS:1||HEAVYFERMION SYSTEMS:1||firstprinciples calculations:1||MECHANISM:1||UNiSn:1||PHOTONIC BANDGAP:1||SINGLE IMPURITY:1||PHONONSPECTRUM:1||FERMISURFACE TOPOLOGY:1||SUPPRESSION:1||RESONANT PHOTOEMISSION:1||METALDOPED PICENE:1||PHOTOIONIZATION CROSSSECTIONS:1||PHOTOINDUCED FERRIMAGNETIC SYSTEMS:1||LINKAGE ISOMERISM:1||CHARGETRANSFER:1||Bilayer Graphene:1||MAGNETICFIELD:1||SPINWAVES:1||rareearth manganese oxides:1||magnonphonon interaction:1||NACO2O4:1||ENERGYBANDS:1||SELFENERGY:1||GAS:1||Fe0.5Cu0.5Cr2S4:1||scanning photoelectron microscopy (SPEM):1||MAGNETIC PROPERTIES:1||Stoner model:1||AMORPHOUS TRANSITIONMETALS:1||SPINGLASS STATES:1||NI:1||LA3NI2B2N3:1||SOLIDS:1||CEO2:1||BAND THEORY:1||dilute magnetic semiconductor:1||pyrochlore:1||Y1XPRXBA2CU3O7DELTA:1||and electronphonon interactions:1||VIBRATIONS:1||RAY PHOTOEMISSION:1||ALKALI CATION:1||Europium:1||colossal magnetoresistance:1||structural stability:1||ENERGYGAP:1||small polaron:1||DOUBLE EXCHANGE:1||Coulomb correlation:1||magnon:1||phonons:1||ELECTRON FERROMAGNETISM:1||CURIETEMPERATURE:1||ARPES:1||PLANEWAVE METHOD:1||Xray absorption spectroscopy (XAS):1||ROOMTEMPERATURE:1||MONOCHALCOGENIDES:1||HEAT:1||UPDSN:1||MOMENTS:1||XRAY ABSORPTION:1||SEMICONDUCTOR:1||Fermi surface nesting:1||optical phonon:1||disordered system:1||dilute magnetic semiconductors:1||CMR manganites:1||PHONONS:1||LATTICEDYNAMICS:1||OXIDES:1||4fphotoemission:1||permanent magnet:1||pseudogap:1||TRANSPORTPROPERTIES:1||ANTIFERROMAGNET:1||(BI,PB)SRCOO SYSTEM:1||semicore correlation:1||POLARIZATION:1||CRYSTAL:1||spinel:1||Xray magnetic circular dichroism (XMCD):1||magnetocapacitance:1||ANATASE:1||TEMPERATURES:1||Pseudogap:1||INTERFACE:1||SUBSTRATE:1||YNI2B2C:1||SAMARIUM SULFIDE:1||strong swave superconductor:1||DOPED MANGANITE:1||SYMMETRY:1||CENISN:1||resonance mode:1||DISORDERED SYSTEM:1||LITHIUM INTERCALATION:1||CUO2 PLANE:1||SURFACE:1||Delafossite:1||ELECTRICALPROPERTIES:1||NIMNSB:1||PTMNSB:1||ROOMTEMPERATURE FERROMAGNETISM:1||RUBIDIUM MANGANESE HEXACYANOFERRATE:1||COLOSSALMAGNETORESISTANCE:1||FINITE TEMPERATURES:1||LAMNO3:1||FE:1||transitionmetal oxides:1||giant magnetoresistance:1||phonon:1||COPPER OXIDES:1||valence states:1||thermoelectric:1||semiconductor:1||CATION DISTRIBUTION:1||FeCr2S4:1||photoemission spectroscopy (PES):1||METALLIC FERROMAGNETISM:1||GRAPHITE:1||SUSCEPTIBILITY:1||UBE13:1||RCrSb3:1||band JahnTeller:1||Ce3S4:1||TiO2:1||PrBa2Cu3O7delta:1||UNTWINNED PRBA2CU3O7:1||AGNIO2:1||HALFMETALLIC FERROMAGNETS:1||CI:1||Energy gap:1||Photoemission:1||Future applications:1||Photoemission measurements:1||Graphene:1||BANDSTRUCTURE:1||TC:1||superconductivity:1||magnetic semiconductors:1||CMRmanganites:1||thin films:1||spin dynamics:1||highTc superconductors:1||ITINERANTELECTRON FERROMAGNETISM:1||SINGLECRYSTALS:1||CeTe2:1||amorphous magnetic materials:1||EPITAXIAL GRAPHENE:1||LAYERED PNICTIDEOXIDES:1||BOROCARBIDE SUPERCONDUCTORS:1||AUGMENTEDWAVE METHOD:1||METALLIC MAGNET UNISN:1||ORIGIN:1||spectrum rearrangement:1||MEANFIELD THEORY:1||MOLECULEBASED MAGNETS:1||METASTABLE STATE:1||INSULATOR:1||magnetic orderin:1||FCC IRON:1||CeRu2:1||TL2MN2O7:1||isotope effect:1||Perovskitemanganites:1||RECURSION METHOD:1||PERPENDICULAR MAGNETICANISOTROPY:1||quasiparticle spectral density:1||GW:1||MANGANESE FERRITE:1||RESONANCE:1||SeCuO3:1||Optical conductivity:1||MASSLESS DIRAC FERMIONS:1||SCHOTTKYBARRIER:1||electronic structure:15||ELECTRONICSTRUCTURE:11||TRANSITIONMETAL COMPOUNDS:10||METALS:10||photoemission:8||SPECTRA:8||MAGNETORESISTANCE:7||FERROMAGNETISM:7||TRANSPORT:7||TRANSITION:6||FILMS:6||THINFILMS:5||TOTALENERGY CALCULATIONS:5||MAGNETICPROPERTIES:5||SUPERCONDUCTIVITY:5||PR:5||LATTICE:4||STATES:4||SPECTROSCOPY:4||FIELD:4||CRYSTALSTRUCTURE:4||PHOTOEMISSION:4||TEMPERATURE:4||TRANSITIONTEMPERATURE:4||XRAYABSORPTION:4||STATE:4||CU:4||BASISSET:4||XAS:4||CRYSTALS:3||EXCITATIONS:3||MOTTHUBBARD SYSTEMS:3||HIGHENERGY SPIN:3||halfmetal:3||INSULATORS:3||LA2CUO4:3||MODEL:3||FLUCTUATIONS:3||CE:3||double exchange:3||TRANSITIONMETALS:3||RESISTIVITY:3||BORON:3||LA1XCAXMNO3:3||IRON:3||PES:3||ANTIMONIDES:2||MgB2:2||ZR METALLIC GLASSES:2||superconductor:2||CRITICALCURRENT DENSITY:2||CIRCULARDICHROISM:2||SEMICONDUCTORS:2||LOCALIZATION:2||INTRABAND OPTICAL CONDUCTIVITY:2||COLOSSAL MAGNETORESISTANCE:2||OXIDATION:2||EXISTENCE:2||COPPER:2||diboride:2||MAGNESIUMDIBORIDE:2||GAP:2||CE COMPOUNDS:2||CORE POLARIZATION:2||magnetoresistance:2||photoemission spectroscopy:2||electronphonon interaction:2||GETTER:2||PD:2||MAGNETISM:2||FECR2S4:2||SUPERCONDUCTING MGB2:2||WIRES:2||ABSORPTION:2||ENERGY:2||LA1XSRXMNO3:2||CONSTANTS:2||polaron:2||charge ordering:2||SCATTERING:2||XRAY PHOTOEMISSION:2||CeNiSn:2||phase diagram:2||PHOTOELECTRON:2||QUADRUPOLAR:2||perovskitemanganites:2||CO:2||SYSTEMS:2||DOPED ZNO:2||LOWFREQUENCY SOUND:2||LA:2||ELECTRONELECTRON SCATTERING:2||AU:2||DENSITYWAVE INSTABILITY:2||FERMISURFACE:2||hybridization:2||VALENCEBAND SATELLITE:2||SULFUR SPINEL:2||Heusler:2||APPROXIMATION:2||superexchange:2||colossal magnetoresistance:2||ALLOYS:2||DEPENDENCE:2||AG:2||electronic structures:2||AUGERSPECTRA:2||CR:2||PARAMETERS:2||DIFFRACTION:2||SEMICONDUCTORMETAL TRANSITION:1||INTERMEDIATEVALENCE:1||SMB6:1||SRRUO3:1||antiperovskite structure with antipolar nature:1||lowenergy twodimensional phonons:1||anatase TiO2:1||La3S4:1||metalinsulator transitions:1||MNO:1||ELECTRONICSTRUCTURES:1||MAGNETIC CIRCULARDICHROISM:1||Density functional theory:1||CeCo2:1||TOPOLARON CROSSOVER:1||EXCHANGE:1||cuprates:1||high Tc cuprates:1||magnetically ordered materials:1||ZNSE:1||Sr2xKxFeMoO6:1||CDW:1||TeCuO3:1||STRUCTURALPROPERTIES:1||MN:1||screening length:1||amorphous Fe:1||WAVE BASISSET:1||SILICONCARBIDE:1||HIGHPRESSURE:1||electronphonon coupling:1||quenched superconductivity:1||CMR perovskite manganites:1||OXIDE:1||polarons:1||synchrotron radiation:1||FULLERIDES:1||RESONANTPHOTOEMISSION:1||Silicon carbide:1||DFT calculation:1||Hybridized bands:1||GIANT MAGNETORESISTANCE:1||PEROVSKITES:1||Raman spectra:1||EXCHANGE ENHANCEMENT:1||SILICON:1||SR2FEMOO6:1||orbital ordering:1||delafossite:1||TITANIUMDIOXIDE:1||electronic structure of disordered solids:1||YFE2:1||Magnetic polaron:1||NA2TI2SB2O:1||STRONGCOUPLED SUPERCONDUCTORS:1||HEAVYFERMION SYSTEMS:1||firstprinciples calculations:1||MECHANISM:1||UNiSn:1||PHOTONIC BANDGAP:1||SINGLE IMPURITY:1||PHONONSPECTRUM:1||FERMISURFACE TOPOLOGY:1||SUPPRESSION:1||RESONANT PHOTOEMISSION:1||METALDOPED PICENE:1||PHOTOIONIZATION CROSSSECTIONS:1||PHOTOINDUCED FERRIMAGNETIC SYSTEMS:1||LINKAGE ISOMERISM:1||CHARGETRANSFER:1||Bilayer Graphene:1||MAGNETICFIELD:1||SPINWAVES:1||rareearth manganese oxides:1||magnonphonon interaction:1||NACO2O4:1||ENERGYBANDS:1||SELFENERGY:1||GAS:1||Fe0.5Cu0.5Cr2S4:1||scanning photoelectron microscopy (SPEM):1||MAGNETIC PROPERTIES:1||Stoner model:1||AMORPHOUS TRANSITIONMETALS:1||SPINGLASS STATES:1||NI:1||LA3NI2B2N3:1||SOLIDS:1||CEO2:1||BAND THEORY:1||dilute magnetic semiconductor:1||pyrochlore:1||Y1XPRXBA2CU3O7DELTA:1||and electronphonon interactions:1||VIBRATIONS:1||RAY PHOTOEMISSION:1||ALKALI CATION:1||Europium:1||colossal magnetoresistance:1||structural stability:1||ENERGYGAP:1||small polaron:1||DOUBLE EXCHANGE:1||Coulomb correlation:1||magnon:1||phonons:1||ELECTRON FERROMAGNETISM:1||CURIETEMPERATURE:1||ARPES:1||PLANEWAVE METHOD:1||Xray absorption spectroscopy (XAS):1||ROOMTEMPERATURE:1||MONOCHALCOGENIDES:1||HEAT:1||UPDSN:1||MOMENTS:1||XRAY ABSORPTION:1||SEMICONDUCTOR:1||Fermi surface nesting:1||optical phonon:1||disordered system:1||dilute magnetic semiconductors:1||CMR manganites:1||PHONONS:1||LATTICEDYNAMICS:1||OXIDES:1||4fphotoemission:1||permanent magnet:1||pseudogap:1||TRANSPORTPROPERTIES:1||ANTIFERROMAGNET:1||(BI,PB)SRCOO SYSTEM:1||semicore correlation:1||POLARIZATION:1||CRYSTAL:1||spinel:1||Xray magnetic circular dichroism (XMCD):1||magnetocapacitance:1||ANATASE:1||TEMPERATURES:1||Pseudogap:1||INTERFACE:1||SUBSTRATE:1||YNI2B2C:1||SAMARIUM SULFIDE:1||strong swave superconductor:1||DOPED MANGANITE:1||SYMMETRY:1||CENISN:1||resonance mode:1||DISORDERED SYSTEM:1||LITHIUM INTERCALATION:1||CUO2 PLANE:1||SURFACE:1||Delafossite:1||ELECTRICALPROPERTIES:1||NIMNSB:1||PTMNSB:1||ROOMTEMPERATURE FERROMAGNETISM:1||RUBIDIUM MANGANESE HEXACYANOFERRATE:1||COLOSSALMAGNETORESISTANCE:1||FINITE TEMPERATURES:1||LAMNO3:1||FE:1||transitionmetal oxides:1||giant magnetoresistance:1||phonon:1||COPPER OXIDES:1||valence states:1||thermoelectric:1||semiconductor:1||CATION DISTRIBUTION:1||FeCr2S4:1||photoemission spectroscopy (PES):1||METALLIC FERROMAGNETISM:1||GRAPHITE:1||SUSCEPTIBILITY:1||UBE13:1||RCrSb3:1||band JahnTeller:1||Ce3S4:1||TiO2:1||PrBa2Cu3O7delta:1||UNTWINNED PRBA2CU3O7:1||AGNIO2:1||HALFMETALLIC FERROMAGNETS:1||CI:1||Energy gap:1||Photoemission:1||Future applications:1||Photoemission measurements:1||Graphene:1||BANDSTRUCTURE:1||TC:1||superconductivity:1||magnetic semiconductors:1||CMRmanganites:1||thin films:1||spin dynamics:1||highTc superconductors:1||ITINERANTELECTRON FERROMAGNETISM:1||SINGLECRYSTALS:1||CeTe2:1||amorphous magnetic materials:1||EPITAXIAL GRAPHENE:1||LAYERED PNICTIDEOXIDES:1||BOROCARBIDE SUPERCONDUCTORS:1||AUGMENTEDWAVE METHOD:1||METALLIC MAGNET UNISN:1||ORIGIN:1||spectrum rearrangement:1||MEANFIELD THEORY:1||MOLECULEBASED MAGNETS:1||METASTABLE STATE:1||INSULATOR:1||magnetic orderin:1||FCC IRON:1||CeRu2:1||TL2MN2O7:1||isotope effect:1||Perovskitemanganites:1||RECURSION METHOD:1||PERPENDICULAR MAGNETICANISOTROPY:1||quasiparticle spectral density:1||GW:1||MANGANESE FERRITE:1||RESONANCE:1||SeCuO3:1||Optical conductivity:1||MASSLESS DIRAC FERMIONS:1||SCHOTTKYBARRIER:1||electronic structure:15||ELECTRONICSTRUCTURE:11||TRANSITIONMETAL COMPOUNDS:10||METALS:10||photoemission:8||SPECTRA:8||MAGNETORESISTANCE:7||FERROMAGNETISM:7||TRANSPORT:7||TRANSITION:6||FILMS:6||THINFILMS:5||TOTALENERGY CALCULATIONS:5||MAGNETICPROPERTIES:5||SUPERCONDUCTIVITY:5||PR:5||LATTICE:4||STATES:4||SPECTROSCOPY:4||FIELD:4||CRYSTALSTRUCTURE:4||PHOTOEMISSION:4||TEMPERATURE:4||TRANSITIONTEMPERATURE:4||XRAYABSORPTION:4||STATE:4||CU:4||BASISSET:4||XAS:4||CRYSTALS:3||EXCITATIONS:3||MOTTHUBBARD SYSTEMS:3||HIGHENERGY SPIN:3||halfmetal:3||INSULATORS:3||LA2CUO4:3||MODEL:3||FLUCTUATIONS:3||CE:3||double exchange:3||TRANSITIONMETALS:3||RESISTIVITY:3||BORON:3||LA1XCAXMNO3:3||IRON:3||PES:3||ANTIMONIDES:2||MgB2:2||ZR METALLIC GLASSES:2||superconductor:2||CRITICALCURRENT DENSITY:2||CIRCULARDICHROISM:2||SEMICONDUCTORS:2||LOCALIZATION:2||INTRABAND OPTICAL CONDUCTIVITY:2||COLOSSAL MAGNETORESISTANCE:2||OXIDATION:2||EXISTENCE:2||COPPER:2||diboride:2||MAGNESIUMDIBORIDE:2||GAP:2||CE COMPOUNDS:2||CORE POLARIZATION:2||magnetoresistance:2||photoemission spectroscopy:2||electronphonon interaction:2||GETTER:2||PD:2||MAGNETISM:2||FECR2S4:2||SUPERCONDUCTING MGB2:2||WIRES:2||ABSORPTION:2||ENERGY:2||LA1XSRXMNO3:2||CONSTANTS:2||polaron:2||charge ordering:2||SCATTERING:2||XRAY PHOTOEMISSION:2||CeNiSn:2||phase diagram:2||PHOTOELECTRON:2||QUADRUPOLAR:2||perovskitemanganites:2||CO:2||SYSTEMS:2||DOPED ZNO:2||LOWFREQUENCY SOUND:2||LA:2||ELECTRONELECTRON SCATTERING:2||AU:2||DENSITYWAVE INSTABILITY:2||FERMISURFACE:2||hybridization:2||VALENCEBAND SATELLITE:2||SULFUR SPINEL:2||Heusler:2||APPROXIMATION:2||superexchange:2||colossal magnetoresistance:2||ALLOYS:2||DEPENDENCE:2||AG:2||electronic structures:2||AUGERSPECTRA:2||CR:2||PARAMETERS:2||DIFFRACTION:2||SEMICONDUCTORMETAL TRANSITION:1||INTERMEDIATEVALENCE:1||SMB6:1||SRRUO3:1||antiperovskite structure with antipolar nature:1||lowenergy twodimensional phonons:1||anatase TiO2:1||La3S4:1||metalinsulator transitions:1||MNO:1||ELECTRONICSTRUCTURES:1||MAGNETIC CIRCULARDICHROISM:1||Density functional theory:1||CeCo2:1||TOPOLARON CROSSOVER:1||EXCHANGE:1||cuprates:1||high Tc cuprates:1||magnetically ordered materials:1||ZNSE:1||Sr2xKxFeMoO6:1||CDW:1||TeCuO3:1||STRUCTURALPROPERTIES:1||MN:1||screening length:1||amorphous Fe:1||WAVE BASISSET:1||SILICONCARBIDE:1||HIGHPRESSURE:1||electronphonon coupling:1||quenched superconductivity:1||CMR perovskite manganites:1||OXIDE:1||polarons:1||synchrotron radiation:1||FULLERIDES:1||RESONANTPHOTOEMISSION:1||Silicon carbide:1||DFT calculation:1||Hybridized bands:1||GIANT MAGNETORESISTANCE:1||PEROVSKITES:1||Raman spectra:1||EXCHANGE ENHANCEMENT:1||SILICON:1||SR2FEMOO6:1||orbital ordering:1||delafossite:1||TITANIUMDIOXIDE:1||electronic structure of disordered solids:1||YFE2:1||Magnetic polaron:1||NA2TI2SB2O:1||STRONGCOUPLED SUPERCONDUCTORS:1||HEAVYFERMION SYSTEMS:1||firstprinciples calculations:1||MECHANISM:1||UNiSn:1||PHOTONIC BANDGAP:1||SINGLE IMPURITY:1||PHONONSPECTRUM:1||FERMISURFACE TOPOLOGY:1||SUPPRESSION:1||RESONANT PHOTOEMISSION:1||METALDOPED PICENE:1||PHOTOIONIZATION CROSSSECTIONS:1||PHOTOINDUCED FERRIMAGNETIC SYSTEMS:1||LINKAGE ISOMERISM:1||CHARGETRANSFER:1||Bilayer Graphene:1||MAGNETICFIELD:1||SPINWAVES:1||rareearth manganese oxides:1||magnonphonon interaction:1||NACO2O4:1||ENERGYBANDS:1||SELFENERGY:1||GAS:1||Fe0.5Cu0.5Cr2S4:1||scanning photoelectron microscopy (SPEM):1||MAGNETIC PROPERTIES:1||Stoner model:1||AMORPHOUS TRANSITIONMETALS:1||SPINGLASS STATES:1||NI:1||LA3NI2B2N3:1||SOLIDS:1||CEO2:1||BAND THEORY:1||dilute magnetic semiconductor:1||pyrochlore:1||Y1XPRXBA2CU3O7DELTA:1||and electronphonon interactions:1||VIBRATIONS:1||RAY PHOTOEMISSION:1||ALKALI CATION:1||Europium:1||colossal magnetoresistance:1||structural stability:1||ENERGYGAP:1||small polaron:1||DOUBLE EXCHANGE:1||Coulomb correlation:1||magnon:1||phonons:1||ELECTRON FERROMAGNETISM:1||CURIETEMPERATURE:1||ARPES:1||PLANEWAVE METHOD:1||Xray absorption spectroscopy (XAS):1||ROOMTEMPERATURE:1||MONOCHALCOGENIDES:1||HEAT:1||UPDSN:1||MOMENTS:1||XRAY ABSORPTION:1||SEMICONDUCTOR:1||Fermi surface nesting:1||optical phonon:1||disordered system:1||dilute magnetic semiconductors:1||CMR manganites:1||PHONONS:1||LATTICEDYNAMICS:1||OXIDES:1||4fphotoemission:1||permanent magnet:1||pseudogap:1||TRANSPORTPROPERTIES:1||ANTIFERROMAGNET:1||(BI,PB)SRCOO SYSTEM:1||semicore correlation:1||POLARIZATION:1||CRYSTAL:1||spinel:1||Xray magnetic circular dichroism (XMCD):1||magnetocapacitance:1||ANATASE:1||TEMPERATURES:1||Pseudogap:1||INTERFACE:1||SUBSTRATE:1||YNI2B2C:1||SAMARIUM SULFIDE:1||strong swave superconductor:1||DOPED MANGANITE:1||SYMMETRY:1||CENISN:1||resonance mode:1||DISORDERED SYSTEM:1||LITHIUM INTERCALATION:1||CUO2 PLANE:1||SURFACE:1||Delafossite:1||ELECTRICALPROPERTIES:1||NIMNSB:1||PTMNSB:1||ROOMTEMPERATURE FERROMAGNETISM:1||RUBIDIUM MANGANESE HEXACYANOFERRATE:1||COLOSSALMAGNETORESISTANCE:1||FINITE TEMPERATURES:1||LAMNO3:1||FE:1||transitionmetal oxides:1||giant magnetoresistance:1||phonon:1||COPPER OXIDES:1||valence states:1||thermoelectric:1||semiconductor:1||CATION DISTRIBUTION:1||FeCr2S4:1||photoemission spectroscopy (PES):1||METALLIC FERROMAGNETISM:1||GRAPHITE:1||SUSCEPTIBILITY:1||UBE13:1||RCrSb3:1||band JahnTeller:1||Ce3S4:1||TiO2:1||PrBa2Cu3O7delta:1||UNTWINNED PRBA2CU3O7:1||AGNIO2:1||HALFMETALLIC FERROMAGNETS:1||CI:1||Energy gap:1||Photoemission:1||Future applications:1||Photoemission measurements:1||Graphene:1||BANDSTRUCTURE:1||TC:1||superconductivity:1||magnetic semiconductors:1||CMRmanganites:1||thin films:1||spin dynamics:1||highTc superconductors:1||ITINERANTELECTRON FERROMAGNETISM:1||SINGLECRYSTALS:1||CeTe2:1||amorphous magnetic materials:1||EPITAXIAL GRAPHENE:1||LAYERED PNICTIDEOXIDES:1||BOROCARBIDE SUPERCONDUCTORS:1||AUGMENTEDWAVE METHOD:1||METALLIC MAGNET UNISN:1||ORIGIN:1||spectrum rearrangement:1||MEANFIELD THEORY:1||MOLECULEBASED MAGNETS:1||METASTABLE STATE:1||INSULATOR:1||magnetic orderin:1||FCC IRON:1||CeRu2:1||TL2MN2O7:1||isotope effect:1||Perovskitemanganites:1||RECURSION METHOD:1||PERPENDICULAR MAGNETICANISOTROPY:1||quasiparticle spectral density:1||GW:1||MANGANESE FERRITE:1||RESONANCE:1||SeCuO3:1||Optical conductivity:1||MASSLESS DIRAC FERMIONS:1||SCHOTTKYBARRIER:1||electronic structure:15||ELECTRONICSTRUCTURE:11||TRANSITIONMETAL COMPOUNDS:10||METALS:10||photoemission:8||SPECTRA:8||MAGNETORESISTANCE:7||FERROMAGNETISM:7||TRANSPORT:7||TRANSITION:6||FILMS:6||THINFILMS:5||TOTALENERGY CALCULATIONS:5||MAGNETICPROPERTIES:5||SUPERCONDUCTIVITY:5||PR:5||LATTICE:4||STATES:4||SPECTROSCOPY:4||FIELD:4||CRYSTALSTRUCTURE:4||PHOTOEMISSION:4||TEMPERATURE:4||TRANSITIONTEMPERATURE:4||XRAYABSORPTION:4||STATE:4||CU:4||BASISSET:4||XAS:4||CRYSTALS:3||EXCITATIONS:3||MOTTHUBBARD SYSTEMS:3||HIGHENERGY SPIN:3||halfmetal:3||INSULATORS:3||LA2CUO4:3||MODEL:3||FLUCTUATIONS:3||CE:3||double exchange:3||TRANSITIONMETALS:3||RESISTIVITY:3||BORON:3||LA1XCAXMNO3:3||IRON:3||PES:3||ANTIMONIDES:2||MgB2:2||ZR METALLIC GLASSES:2||superconductor:2||CRITICALCURRENT DENSITY:2||CIRCULARDICHROISM:2||SEMICONDUCTORS:2||LOCALIZATION:2||INTRABAND OPTICAL CONDUCTIVITY:2||COLOSSAL MAGNETORESISTANCE:2||OXIDATION:2||EXISTENCE:2||COPPER:2||diboride:2||MAGNESIUMDIBORIDE:2||GAP:2||CE COMPOUNDS:2||CORE POLARIZATION:2||magnetoresistance:2||photoemission spectroscopy:2||electronphonon interaction:2||GETTER:2||PD:2||MAGNETISM:2||FECR2S4:2||SUPERCONDUCTING MGB2:2||WIRES:2||ABSORPTION:2||ENERGY:2||LA1XSRXMNO3:2||CONSTANTS:2||polaron:2||charge ordering:2||SCATTERING:2||XRAY PHOTOEMISSION:2||CeNiSn:2||phase diagram:2||PHOTOELECTRON:2||QUADRUPOLAR:2||perovskitemanganites:2||CO:2||SYSTEMS:2||DOPED ZNO:2||LOWFREQUENCY SOUND:2||LA:2||ELECTRONELECTRON SCATTERING:2||AU:2||DENSITYWAVE INSTABILITY:2||FERMISURFACE:2||hybridization:2||VALENCEBAND SATELLITE:2||SULFUR SPINEL:2||Heusler:2||APPROXIMATION:2||superexchange:2||colossal magnetoresistance:2||ALLOYS:2||DEPENDENCE:2||AG:2||electronic structures:2||AUGERSPECTRA:2||CR:2||PARAMETERS:2||DIFFRACTION:2||SEMICONDUCTORMETAL TRANSITION:1||INTERMEDIATEVALENCE:1||SMB6:1||SRRUO3:1||antiperovskite structure with antipolar nature:1||lowenergy twodimensional phonons:1||anatase TiO2:1||La3S4:1||metalinsulator transitions:1||MNO:1||ELECTRONICSTRUCTURES:1||MAGNETIC CIRCULARDICHROISM:1||Density functional theory:1||CeCo2:1||TOPOLARON CROSSOVER:1||EXCHANGE:1||cuprates:1||high Tc cuprates:1||magnetically ordered materials:1||ZNSE:1||Sr2xKxFeMoO6:1||CDW:1||TeCuO3:1||STRUCTURALPROPERTIES:1||MN:1||screening length:1||amorphous Fe:1||WAVE BASISSET:1||SILICONCARBIDE:1||HIGHPRESSURE:1||electronphonon coupling:1||quenched superconductivity:1||CMR perovskite manganites:1||OXIDE:1||polarons:1||synchrotron radiation:1||FULLERIDES:1||RESONANTPHOTOEMISSION:1||Silicon carbide:1||DFT calculation:1||Hybridized bands:1||GIANT MAGNETORESISTANCE:1||PEROVSKITES:1||Raman spectra:1||EXCHANGE ENHANCEMENT:1||SILICON:1||SR2FEMOO6:1||orbital ordering:1||delafossite:1||TITANIUMDIOXIDE:1||electronic structure of disordered solids:1||YFE2:1||Magnetic polaron:1||NA2TI2SB2O:1||STRONGCOUPLED SUPERCONDUCTORS:1||HEAVYFERMION SYSTEMS:1||firstprinciples calculations:1||MECHANISM:1||UNiSn:1||PHOTONIC BANDGAP:1||SINGLE IMPURITY:1||PHONONSPECTRUM:1||FERMISURFACE TOPOLOGY:1||SUPPRESSION:1||RESONANT PHOTOEMISSION:1||METALDOPED PICENE:1||PHOTOIONIZATION CROSSSECTIONS:1||PHOTOINDUCED FERRIMAGNETIC SYSTEMS:1||LINKAGE ISOMERISM:1||CHARGETRANSFER:1||Bilayer Graphene:1||MAGNETICFIELD:1||SPINWAVES:1||rareearth manganese oxides:1||magnonphonon interaction:1||NACO2O4:1||ENERGYBANDS:1||SELFENERGY:1||GAS:1||Fe0.5Cu0.5Cr2S4:1||scanning photoelectron microscopy (SPEM):1||MAGNETIC PROPERTIES:1||Stoner model:1||AMORPHOUS TRANSITIONMETALS:1||SPINGLASS STATES:1||NI:1||LA3NI2B2N3:1||SOLIDS:1||CEO2:1||BAND THEORY:1||dilute magnetic semiconductor:1||pyrochlore:1||Y1XPRXBA2CU3O7DELTA:1||and electronphonon interactions:1||VIBRATIONS:1||RAY PHOTOEMISSION:1||ALKALI CATION:1||Europium:1||colossal magnetoresistance:1||structural stability:1||ENERGYGAP:1||small polaron:1||DOUBLE EXCHANGE:1||Coulomb correlation:1||magnon:1||phonons:1||ELECTRON FERROMAGNETISM:1||CURIETEMPERATURE:1||ARPES:1||PLANEWAVE METHOD:1||Xray absorption spectroscopy (XAS):1||ROOMTEMPERATURE:1||MONOCHALCOGENIDES:1||HEAT:1||UPDSN:1||MOMENTS:1||XRAY ABSORPTION:1||SEMICONDUCTOR:1||Fermi surface nesting:1||optical phonon:1||disordered system:1||dilute magnetic semiconductors:1||CMR manganites:1||PHONONS:1||LATTICEDYNAMICS:1||OXIDES:1||4fphotoemission:1||permanent magnet:1||pseudogap:1||TRANSPORTPROPERTIES:1||ANTIFERROMAGNET:1||(BI,PB)SRCOO SYSTEM:1||semicore correlation:1||POLARIZATION:1||CRYSTAL:1||spinel:1||Xray magnetic circular dichroism (XMCD):1||magnetocapacitance:1||ANATASE:1||TEMPERATURES:1||Pseudogap:1||INTERFACE:1||SUBSTRATE:1||YNI2B2C:1||SAMARIUM SULFIDE:1||strong swave superconductor:1||DOPED MANGANITE:1||SYMMETRY:1||CENISN:1||resonance mode:1||DISORDERED SYSTEM:1||LITHIUM INTERCALATION:1||CUO2 PLANE:1||SURFACE:1||Delafossite:1||ELECTRICALPROPERTIES:1||NIMNSB:1||PTMNSB:1||ROOMTEMPERATURE FERROMAGNETISM:1||RUBIDIUM MANGANESE HEXACYANOFERRATE:1||COLOSSALMAGNETORESISTANCE:1||FINITE TEMPERATURES:1||LAMNO3:1||FE:1||transitionmetal oxides:1||giant magnetoresistance:1||phonon:1||COPPER OXIDES:1||valence states:1||thermoelectric:1||semiconductor:1||CATION DISTRIBUTION:1||FeCr2S4:1||photoemission spectroscopy (PES):1||METALLIC FERROMAGNETISM:1||GRAPHITE:1||SUSCEPTIBILITY:1||UBE13:1||RCrSb3:1||band JahnTeller:1||Ce3S4:1||TiO2:1||PrBa2Cu3O7delta:1||UNTWINNED PRBA2CU3O7:1||AGNIO2:1||HALFMETALLIC FERROMAGNETS:1||CI:1||Energy gap:1||Photoemission:1||Future applications:1||Photoemission measurements:1||Graphene:1||BANDSTRUCTURE:1||TC:1||superconductivity:1||magnetic semiconductors:1||CMRmanganites:1||thin films:1||spin dynamics:1||highTc superconductors:1||ITINERANTELECTRON FERROMAGNETISM:1||SINGLECRYSTALS:1||CeTe2:1||amorphous magnetic materials:1||EPITAXIAL GRAPHENE:1||LAYERED PNICTIDEOXIDES:1||BOROCARBIDE SUPERCONDUCTORS:1||AUGMENTEDWAVE METHOD:1||METALLIC MAGNET UNISN:1||ORIGIN:1||spectrum rearrangement:1||MEANFIELD THEORY:1||MOLECULEBASED MAGNETS:1||METASTABLE STATE:1||INSULATOR:1||magnetic orderin:1||FCC IRON:1||CeRu2:1||TL2MN2O7:1||isotope effect:1||Perovskitemanganites:1||RECURSION METHOD:1||PERPENDICULAR MAGNETICANISOTROPY:1||quasiparticle spectral density:1||GW:1||MANGANESE FERRITE:1||RESONANCE:1||SeCuO3:1||Optical conductivity:1||MASSLESS DIRAC FERMIONS:1||SCHOTTKYBARRIER:1||electronic structure:15||ELECTRONICSTRUCTURE:11||TRANSITIONMETAL COMPOUNDS:10||METALS:10||photoemission:8||SPECTRA:8||MAGNETORESISTANCE:7||FERROMAGNETISM:7||TRANSPORT:7||TRANSITION:6||FILMS:6||THINFILMS:5||TOTALENERGY CALCULATIONS:5||MAGNETICPROPERTIES:5||SUPERCONDUCTIVITY:5||PR:5||LATTICE:4||STATES:4||SPECTROSCOPY:4||FIELD:4||CRYSTALSTRUCTURE:4||PHOTOEMISSION:4||TEMPERATURE:4||TRANSITIONTEMPERATURE:4||XRAYABSORPTION:4||STATE:4||CU:4||BASISSET:4||XAS:4||CRYSTALS:3||EXCITATIONS:3||MOTTHUBBARD SYSTEMS:3||HIGHENERGY SPIN:3||halfmetal:3||INSULATORS:3||LA2CUO4:3||MODEL:3||FLUCTUATIONS:3||CE:3||double exchange:3||TRANSITIONMETALS:3||RESISTIVITY:3||BORON:3||LA1XCAXMNO3:3||IRON:3||PES:3||ANTIMONIDES:2||MgB2:2||ZR METALLIC GLASSES:2||superconductor:2||CRITICALCURRENT DENSITY:2||CIRCULARDICHROISM:2||SEMICONDUCTORS:2||LOCALIZATION:2||INTRABAND OPTICAL CONDUCTIVITY:2||COLOSSAL MAGNETORESISTANCE:2||OXIDATION:2||EXISTENCE:2||COPPER:2||diboride:2||MAGNESIUMDIBORIDE:2||GAP:2||CE COMPOUNDS:2||CORE POLARIZATION:2||magnetoresistance:2||photoemission spectroscopy:2||electronphonon interaction:2||GETTER:2||PD:2||MAGNETISM:2||FECR2S4:2||SUPERCONDUCTING MGB2:2||WIRES:2||ABSORPTION:2||ENERGY:2||LA1XSRXMNO3:2||CONSTANTS:2||polaron:2||charge ordering:2||SCATTERING:2||XRAY PHOTOEMISSION:2||CeNiSn:2||phase diagram:2||PHOTOELECTRON:2||QUADRUPOLAR:2||perovskitemanganites:2||CO:2||SYSTEMS:2||DOPED ZNO:2||LOWFREQUENCY SOUND:2||LA:2||ELECTRONELECTRON SCATTERING:2||AU:2||DENSITYWAVE INSTABILITY:2||FERMISURFACE:2||hybridization:2||VALENCEBAND SATELLITE:2||SULFUR SPINEL:2||Heusler:2||APPROXIMATION:2||superexchange:2||colossal magnetoresistance:2||ALLOYS:2||DEPENDENCE:2||AG:2||electronic structures:2||AUGERSPECTRA:2||CR:2||PARAMETERS:2||DIFFRACTION:2||SEMICONDUCTORMETAL TRANSITION:1||INTERMEDIATEVALENCE:1||SMB6:1||SRRUO3:1||antiperovskite structure with antipolar nature:1||lowenergy twodimensional phonons:1||anatase TiO2:1||La3S4:1||metalinsulator transitions:1||MNO:1||ELECTRONICSTRUCTURES:1||MAGNETIC CIRCULARDICHROISM:1||Density functional theory:1||CeCo2:1||TOPOLARON CROSSOVER:1||EXCHANGE:1||cuprates:1||high Tc cuprates:1||magnetically ordered materials:1||ZNSE:1||Sr2xKxFeMoO6:1||CDW:1||TeCuO3:1||STRUCTURALPROPERTIES:1||MN:1||screening length:1||amorphous Fe:1||WAVE BASISSET:1||SILICONCARBIDE:1||HIGHPRESSURE:1||electronphonon coupling:1||quenched superconductivity:1||CMR perovskite manganites:1||OXIDE:1||polarons:1||synchrotron radiation:1||FULLERIDES:1||RESONANTPHOTOEMISSION:1||Silicon carbide:1||DFT calculation:1||Hybridized bands:1||GIANT MAGNETORESISTANCE:1||PEROVSKITES:1||Raman spectra:1||EXCHANGE ENHANCEMENT:1||SILICON:1||SR2FEMOO6:1||orbital ordering:1||delafossite:1||TITANIUMDIOXIDE:1||electronic structure of disordered solids:1||YFE2:1||Magnetic polaron:1||NA2TI2SB2O:1||STRONGCOUPLED SUPERCONDUCTORS:1||HEAVYFERMION SYSTEMS:1||firstprinciples calculations:1||MECHANISM:1||UNiSn:1||PHOTONIC BANDGAP:1||SINGLE IMPURITY:1||PHONONSPECTRUM:1||FERMISURFACE TOPOLOGY:1||SUPPRESSION:1||RESONANT PHOTOEMISSION:1||METALDOPED PICENE:1||PHOTOIONIZATION CROSSSECTIONS:1||PHOTOINDUCED FERRIMAGNETIC SYSTEMS:1||LINKAGE ISOMERISM:1||CHARGETRANSFER:1||Bilayer Graphene:1||MAGNETICFIELD:1||SPINWAVES:1||rareearth manganese oxides:1||magnonphonon interaction:1||NACO2O4:1||ENERGYBANDS:1||SELFENERGY:1||GAS:1||Fe0.5Cu0.5Cr2S4:1||scanning photoelectron microscopy (SPEM):1||MAGNETIC PROPERTIES:1||Stoner model:1||AMORPHOUS TRANSITIONMETALS:1||SPINGLASS STATES:1||NI:1||LA3NI2B2N3:1||SOLIDS:1||CEO2:1||BAND THEORY:1||dilute magnetic semiconductor:1||pyrochlore:1||Y1XPRXBA2CU3O7DELTA:1||and electronphonon interactions:1||VIBRATIONS:1||RAY PHOTOEMISSION:1||ALKALI CATION:1||Europium:1||colossal magnetoresistance:1||structural stability:1||ENERGYGAP:1||small polaron:1||DOUBLE EXCHANGE:1||Coulomb correlation:1||magnon:1||phonons:1||ELECTRON FERROMAGNETISM:1||CURIETEMPERATURE:1||ARPES:1||PLANEWAVE METHOD:1||Xray absorption spectroscopy (XAS):1||ROOMTEMPERATURE:1||MONOCHALCOGENIDES:1||HEAT:1||UPDSN:1||MOMENTS:1||XRAY ABSORPTION:1||SEMICONDUCTOR:1||Fermi surface nesting:1||optical phonon:1||disordered system:1||dilute magnetic semiconductors:1||CMR manganites:1||PHONONS:1||LATTICEDYNAMICS:1||OXIDES:1||4fphotoemission:1||permanent magnet:1||pseudogap:1||TRANSPORTPROPERTIES:1||ANTIFERROMAGNET:1||(BI,PB)SRCOO SYSTEM:1||semicore correlation:1||POLARIZATION:1||CRYSTAL:1||spinel:1||Xray magnetic circular dichroism (XMCD):1||magnetocapacitance:1||ANATASE:1||TEMPERATURES:1||Pseudogap:1||INTERFACE:1||SUBSTRATE:1||YNI2B2C:1||SAMARIUM SULFIDE:1||strong swave superconductor:1||DOPED MANGANITE:1||SYMMETRY:1||CENISN:1||resonance mode:1||DISORDERED SYSTEM:1||LITHIUM INTERCALATION:1||CUO2 PLANE:1||SURFACE:1||Delafossite:1||ELECTRICALPROPERTIES:1||NIMNSB:1||PTMNSB:1||ROOMTEMPERATURE FERROMAGNETISM:1||RUBIDIUM MANGANESE HEXACYANOFERRATE:1||COLOSSALMAGNETORESISTANCE:1||FINITE TEMPERATURES:1||LAMNO3:1||FE:1||transitionmetal oxides:1||giant magnetoresistance:1||phonon:1||COPPER OXIDES:1||valence states:1||thermoelectric:1||semiconductor:1||CATION DISTRIBUTION:1||FeCr2S4:1||photoemission spectroscopy (PES):1||METALLIC FERROMAGNETISM:1||GRAPHITE:1||SUSCEPTIBILITY:1||UBE13:1||RCrSb3:1||band JahnTeller:1||Ce3S4:1||TiO2:1||PrBa2Cu3O7delta:1||UNTWINNED PRBA2CU3O7:1||AGNIO2:1||HALFMETALLIC FERROMAGNETS:1||CI:1||Energy gap:1||Photoemission:1||Future applications:1||Photoemission measurements:1||Graphene:1||BANDSTRUCTURE:1||TC:1||superconductivity:1||magnetic semiconductors:1||CMRmanganites:1||thin films:1||spin dynamics:1||highTc superconductors:1||ITINERANTELECTRON FERROMAGNETISM:1||SINGLECRYSTALS:1||CeTe2:1||amorphous magnetic materials:1||EPITAXIAL GRAPHENE:1||LAYERED PNICTIDEOXIDES:1||BOROCARBIDE SUPERCONDUCTORS:1||AUGMENTEDWAVE METHOD:1||METALLIC MAGNET UNISN:1||ORIGIN:1||spectrum rearrangement:1||MEANFIELD THEORY:1||MOLECULEBASED MAGNETS:1||METASTABLE STATE:1||INSULATOR:1||magnetic orderin:1||FCC IRON:1||CeRu2:1||TL2MN2O7:1||isotope effect:1||Perovskitemanganites:1||RECURSION METHOD:1||PERPENDICULAR MAGNETICANISOTROPY:1||quasiparticle spectral density:1||GW:1||MANGANESE FERRITE:1||RESONANCE:1||SeCuO3:1||Optical conductivity:1||MASSLESS DIRAC FERMIONS:1||SCHOTTKYBARRIER:1||electronic structure:15||ELECTRONICSTRUCTURE:11||TRANSITIONMETAL COMPOUNDS:10||METALS:10||photoemission:8||SPECTRA:8||MAGNETORESISTANCE:7||FERROMAGNETISM:7||TRANSPORT:7||TRANSITION:6||FILMS:6||THINFILMS:5||TOTALENERGY CALCULATIONS:5||MAGNETICPROPERTIES:5||SUPERCONDUCTIVITY:5||PR:5||LATTICE:4||STATES:4||SPECTROSCOPY:4||FIELD:4||CRYSTALSTRUCTURE:4||PHOTOEMISSION:4||TEMPERATURE:4||TRANSITIONTEMPERATURE:4||XRAYABSORPTION:4||STATE:4||CU:4||BASISSET:4||XAS:4||CRYSTALS:3||EXCITATIONS:3||MOTTHUBBARD SYSTEMS:3||HIGHENERGY SPIN:3||halfmetal:3||INSULATORS:3||LA2CUO4:3||MODEL:3||FLUCTUATIONS:3||CE:3||double exchange:3||TRANSITIONMETALS:3||RESISTIVITY:3||BORON:3||LA1XCAXMNO3:3||IRON:3||PES:3||ANTIMONIDES:2||MgB2:2||ZR METALLIC GLASSES:2||superconductor:2||CRITICALCURRENT DENSITY:2||CIRCULARDICHROISM:2||SEMICONDUCTORS:2||LOCALIZATION:2||INTRABAND OPTICAL CONDUCTIVITY:2||COLOSSAL MAGNETORESISTANCE:2||OXIDATION:2||EXISTENCE:2||COPPER:2||diboride:2||MAGNESIUMDIBORIDE:2||GAP:2||CE COMPOUNDS:2||CORE POLARIZATION:2||magnetoresistance:2||photoemission spectroscopy:2||electronphonon interaction:2||GETTER:2||PD:2||MAGNETISM:2||FECR2S4:2||SUPERCONDUCTING MGB2:2||WIRES:2||ABSORPTION:2||ENERGY:2||LA1XSRXMNO3:2||CONSTANTS:2||polaron:2||charge ordering:2||SCATTERING:2||XRAY PHOTOEMISSION:2||CeNiSn:2||phase diagram:2||PHOTOELECTRON:2||QUADRUPOLAR:2||perovskitemanganites:2||CO:2||SYSTEMS:2||DOPED ZNO:2||LOWFREQUENCY SOUND:2||LA:2||ELECTRONELECTRON SCATTERING:2||AU:2||DENSITYWAVE INSTABILITY:2||FERMISURFACE:2||hybridization:2||VALENCEBAND SATELLITE:2||SULFUR SPINEL:2||Heusler:2||APPROXIMATION:2||superexchange:2||colossal magnetoresistance:2||ALLOYS:2||DEPENDENCE:2||AG:2||electronic structures:2||AUGERSPECTRA:2||CR:2||PARAMETERS:2||DIFFRACTION:2||SEMICONDUCTORMETAL TRANSITION:1||INTERMEDIATEVALENCE:1||SMB6:1||SRRUO3:1||antiperovskite structure with antipolar nature:1||lowenergy twodimensional phonons:1||anatase TiO2:1||La3S4:1||metalinsulator transitions:1||MNO:1||ELECTRONICSTRUCTURES:1||MAGNETIC CIRCULARDICHROISM:1||Density functional theory:1||CeCo2:1||TOPOLARON CROSSOVER:1||EXCHANGE:1||cuprates:1||high Tc cuprates:1||magnetically ordered materials:1||ZNSE:1||Sr2xKxFeMoO6:1||CDW:1||TeCuO3:1||STRUCTURALPROPERTIES:1||MN:1||screening length:1||amorphous Fe:1||WAVE BASISSET:1||SILICONCARBIDE:1||HIGHPRESSURE:1||electronphonon coupling:1||quenched superconductivity:1||CMR perovskite manganites:1||OXIDE:1||polarons:1||synchrotron radiation:1||FULLERIDES:1||RESONANTPHOTOEMISSION:1||Silicon carbide:1||DFT calculation:1||Hybridized bands:1||GIANT MAGNETORESISTANCE:1||PEROVSKITES:1||Raman spectra:1||EXCHANGE ENHANCEMENT:1||SILICON:1||SR2FEMOO6:1||orbital ordering:1||delafossite:1||TITANIUMDIOXIDE:1||electronic structure of disordered solids:1||YFE2:1||Magnetic polaron:1||NA2TI2SB2O:1||STRONGCOUPLED SUPERCONDUCTORS:1||HEAVYFERMION SYSTEMS:1||firstprinciples calculations:1||MECHANISM:1||UNiSn:1||PHOTONIC BANDGAP:1||SINGLE IMPURITY:1||PHONONSPECTRUM:1||FERMISURFACE TOPOLOGY:1||SUPPRESSION:1||RESONANT PHOTOEMISSION:1||METALDOPED PICENE:1||PHOTOIONIZATION CROSSSECTIONS:1||PHOTOINDUCED FERRIMAGNETIC SYSTEMS:1||LINKAGE ISOMERISM:1||CHARGETRANSFER:1||Bilayer Graphene:1||MAGNETICFIELD:1||SPINWAVES:1||rareearth manganese oxides:1||magnonphonon interaction:1||NACO2O4:1||ENERGYBANDS:1||SELFENERGY:1||GAS:1||Fe0.5Cu0.5Cr2S4:1||scanning photoelectron microscopy (SPEM):1||MAGNETIC PROPERTIES:1||Stoner model:1||AMORPHOUS TRANSITIONMETALS:1||SPINGLASS STATES:1||NI:1||LA3NI2B2N3:1||SOLIDS:1||CEO2:1||BAND THEORY:1||dilute magnetic semiconductor:1||pyrochlore:1||Y1XPRXBA2CU3O7DELTA:1||and electronphonon interactions:1||VIBRATIONS:1||RAY PHOTOEMISSION:1||ALKALI CATION:1||Europium:1||colossal magnetoresistance:1||structural stability:1||ENERGYGAP:1||small polaron:1||DOUBLE EXCHANGE:1||Coulomb correlation:1||magnon:1||phonons:1||ELECTRON FERROMAGNETISM:1||CURIETEMPERATURE:1||ARPES:1||PLANEWAVE METHOD:1||Xray absorption spectroscopy (XAS):1||ROOMTEMPERATURE:1||MONOCHALCOGENIDES:1||HEAT:1||UPDSN:1||MOMENTS:1||XRAY ABSORPTION:1||SEMICONDUCTOR:1||Fermi surface nesting:1||optical phonon:1||disordered system:1||dilute magnetic semiconductors:1||CMR manganites:1||PHONONS:1||LATTICEDYNAMICS:1||OXIDES:1||4fphotoemission:1||permanent magnet:1||pseudogap:1||TRANSPORTPROPERTIES:1||ANTIFERROMAGNET:1||(BI,PB)SRCOO SYSTEM:1||semicore correlation:1||POLARIZATION:1||CRYSTAL:1||spinel:1||Xray magnetic circular dichroism (XMCD):1||magnetocapacitance:1||ANATASE:1||TEMPERATURES:1||Pseudogap:1||INTERFACE:1||SUBSTRATE:1||YNI2B2C:1||SAMARIUM SULFIDE:1||strong swave superconductor:1||DOPED MANGANITE:1||SYMMETRY:1||CENISN:1||resonance mode:1||DISORDERED SYSTEM:1||LITHIUM INTERCALATION:1||CUO2 PLANE:1||SURFACE:1||Delafossite:1||ELECTRICALPROPERTIES:1||NIMNSB:1||PTMNSB:1||ROOMTEMPERATURE FERROMAGNETISM:1||RUBIDIUM MANGANESE HEXACYANOFERRATE:1||COLOSSALMAGNETORESISTANCE:1||FINITE TEMPERATURES:1||LAMNO3:1||FE:1||transitionmetal oxides:1||giant magnetoresistance:1||phonon:1||COPPER OXIDES:1||valence states:1||thermoelectric:1||semiconductor:1||CATION DISTRIBUTION:1||FeCr2S4:1||photoemission spectroscopy (PES):1||METALLIC FERROMAGNETISM:1||GRAPHITE:1||SUSCEPTIBILITY:1||UBE13:1||RCrSb3:1||band JahnTeller:1||Ce3S4:1||TiO2:1||PrBa2Cu3O7delta:1||UNTWINNED PRBA2CU3O7:1||AGNIO2:1||HALFMETALLIC FERROMAGNETS:1||CI:1||Energy gap:1||Photoemission:1||Future applications:1||Photoemission measurements:1||Graphene:1||BANDSTRUCTURE:1||TC:1||superconductivity:1||magnetic semiconductors:1||CMRmanganites:1||thin films:1||spin dynamics:1||highTc superconductors:1||ITINERANTELECTRON FERROMAGNETISM:1||SINGLECRYSTALS:1||CeTe2:1||amorphous magnetic materials:1||EPITAXIAL GRAPHENE:1||LAYERED PNICTIDEOXIDES:1||BOROCARBIDE SUPERCONDUCTORS:1||AUGMENTEDWAVE METHOD:1||METALLIC MAGNET UNISN:1||ORIGIN:1||spectrum rearrangement:1||MEANFIELD THEORY:1||MOLECULEBASED MAGNETS:1||METASTABLE STATE:1||INSULATOR:1||magnetic orderin:1||FCC IRON:1||CeRu2:1||TL2MN2O7:1||isotope effect:1||Perovskitemanganites:1||RECURSION METHOD:1||PERPENDICULAR MAGNETICANISOTROPY:1||quasiparticle spectral density:1||GW:1||MANGANESE FERRITE:1||RESONANCE:1||SeCuO3:1||Optical conductivity:1||MASSLESS DIRAC FERMIONS:1||SCHOTTKYBARRIER:1||electronic structure:15||ELECTRONICSTRUCTURE:11||TRANSITIONMETAL COMPOUNDS:10||METALS:10||photoemission:8||SPECTRA:8||MAGNETORESISTANCE:7||FERROMAGNETISM:7||TRANSPORT:7||TRANSITION:6||FILMS:6||THINFILMS:5||TOTALENERGY CALCULATIONS:5||MAGNETICPROPERTIES:5||SUPERCONDUCTIVITY:5||PR:5||LATTICE:4||STATES:4||SPECTROSCOPY:4||FIELD:4||CRYSTALSTRUCTURE:4||PHOTOEMISSION:4||TEMPERATURE:4||TRANSITIONTEMPERATURE:4||XRAYABSORPTION:4||STATE:4||CU:4||BASISSET:4||XAS:4||CRYSTALS:3||EXCITATIONS:3||MOTTHUBBARD SYSTEMS:3||HIGHENERGY SPIN:3||halfmetal:3||INSULATORS:3||LA2CUO4:3||MODEL:3||FLUCTUATIONS:3||CE:3||double exchange:3||TRANSITIONMETALS:3||RESISTIVITY:3||BORON:3||LA1XCAXMNO3:3||IRON:3||PES:3||ANTIMONIDES:2||MgB2:2||ZR METALLIC GLASSES:2||superconductor:2||CRITICALCURRENT DENSITY:2||CIRCULARDICHROISM:2||SEMICONDUCTORS:2||LOCALIZATION:2||INTRABAND OPTICAL CONDUCTIVITY:2||COLOSSAL MAGNETORESISTANCE:2||OXIDATION:2||EXISTENCE:2||COPPER:2||diboride:2||MAGNESIUMDIBORIDE:2||GAP:2||CE COMPOUNDS:2||CORE POLARIZATION:2||magnetoresistance:2||photoemission spectroscopy:2||electronphonon interaction:2||GETTER:2||PD:2||MAGNETISM:2||FECR2S4:2||SUPERCONDUCTING MGB2:2||WIRES:2||ABSORPTION:2||ENERGY:2||LA1XSRXMNO3:2||CONSTANTS:2||polaron:2||charge ordering:2||SCATTERING:2||XRAY PHOTOEMISSION:2||CeNiSn:2||phase diagram:2||PHOTOELECTRON:2||QUADRUPOLAR:2||perovskitemanganites:2||CO:2||SYSTEMS:2||DOPED ZNO:2||LOWFREQUENCY SOUND:2||LA:2||ELECTRONELECTRON SCATTERING:2||AU:2||DENSITYWAVE INSTABILITY:2||FERMISURFACE:2||hybridization:2||VALENCEBAND SATELLITE:2||SULFUR SPINEL:2||Heusler:2||APPROXIMATION:2||superexchange:2||colossal magnetoresistance:2||ALLOYS:2||DEPENDENCE:2||AG:2||electronic structures:2||AUGERSPECTRA:2||CR:2||PARAMETERS:2||DIFFRACTION:2||SEMICONDUCTORMETAL TRANSITION:1||INTERMEDIATEVALENCE:1||SMB6:1||SRRUO3:1||antiperovskite structure with antipolar nature:1||lowenergy twodimensional phonons:1||anatase TiO2:1||La3S4:1||metalinsulator transitions:1||MNO:1||ELECTRONICSTRUCTURES:1||MAGNETIC CIRCULARDICHROISM:1||Density functional theory:1||CeCo2:1||TOPOLARON CROSSOVER:1||EXCHANGE:1||cuprates:1||high Tc cuprates:1||magnetically ordered materials:1||ZNSE:1||Sr2xKxFeMoO6:1||CDW:1||TeCuO3:1||STRUCTURALPROPERTIES:1||MN:1||screening length:1||amorphous Fe:1||WAVE BASISSET:1||SILICONCARBIDE:1||HIGHPRESSURE:1||electronphonon coupling:1||quenched superconductivity:1||CMR perovskite manganites:1||OXIDE:1||polarons:1||synchrotron radiation:1||FULLERIDES:1||RESONANTPHOTOEMISSION:1||Silicon carbide:1||DFT calculation:1||Hybridized bands:1||GIANT MAGNETORESISTANCE:1||PEROVSKITES:1||Raman spectra:1||EXCHANGE ENHANCEMENT:1||SILICON:1||SR2FEMOO6:1||orbital ordering:1||delafossite:1||TITANIUMDIOXIDE:1||electronic structure of disordered solids:1||YFE2:1||Magnetic polaron:1||NA2TI2SB2O:1||STRONGCOUPLED SUPERCONDUCTORS:1||HEAVYFERMION SYSTEMS:1||firstprinciples calculations:1||MECHANISM:1||UNiSn:1||PHOTONIC BANDGAP:1||SINGLE IMPURITY:1||PHONONSPECTRUM:1||FERMISURFACE TOPOLOGY:1||SUPPRESSION:1||RESONANT PHOTOEMISSION:1||METALDOPED PICENE:1||PHOTOIONIZATION CROSSSECTIONS:1||PHOTOINDUCED FERRIMAGNETIC SYSTEMS:1||LINKAGE ISOMERISM:1||CHARGETRANSFER:1||Bilayer Graphene:1||MAGNETICFIELD:1||SPINWAVES:1||rareearth manganese oxides:1||magnonphonon interaction:1||NACO2O4:1||ENERGYBANDS:1||SELFENERGY:1||GAS:1||Fe0.5Cu0.5Cr2S4:1||scanning photoelectron microscopy (SPEM):1||MAGNETIC PROPERTIES:1||Stoner model:1||AMORPHOUS TRANSITIONMETALS:1||SPINGLASS STATES:1||NI:1||LA3NI2B2N3:1||SOLIDS:1||CEO2:1||BAND THEORY:1||dilute magnetic semiconductor:1||pyrochlore:1||Y1XPRXBA2CU3O7DELTA:1||and electronphonon interactions:1||VIBRATIONS:1||RAY PHOTOEMISSION:1||ALKALI CATION:1||Europium:1||colossal magnetoresistance:1||structural stability:1||ENERGYGAP:1||small polaron:1||DOUBLE EXCHANGE:1||Coulomb correlation:1||magnon:1||phonons:1||ELECTRON FERROMAGNETISM:1||CURIETEMPERATURE:1||ARPES:1||PLANEWAVE METHOD:1||Xray absorption spectroscopy (XAS):1||ROOMTEMPERATURE:1||MONOCHALCOGENIDES:1||HEAT:1||UPDSN:1||MOMENTS:1||XRAY ABSORPTION:1||SEMICONDUCTOR:1||Fermi surface nesting:1||optical phonon:1||disordered system:1||dilute magnetic semiconductors:1||CMR manganites:1||PHONONS:1||LATTICEDYNAMICS:1||OXIDES:1||4fphotoemission:1||permanent magnet:1||pseudogap:1||TRANSPORTPROPERTIES:1||ANTIFERROMAGNET:1||(BI,PB)SRCOO SYSTEM:1||semicore correlation:1||POLARIZATION:1||CRYSTAL:1||spinel:1||Xray magnetic circular dichroism (XMCD):1||magnetocapacitance:1||ANATASE:1||TEMPERATURES:1||Pseudogap:1||INTERFACE:1||SUBSTRATE:1||YNI2B2C:1||SAMARIUM SULFIDE:1||strong swave superconductor:1||DOPED MANGANITE:1||SYMMETRY:1||CENISN:1||resonance mode:1||DISORDERED SYSTEM:1||LITHIUM INTERCALATION:1||CUO2 PLANE:1||SURFACE:1||Delafossite:1||ELECTRICALPROPERTIES:1||NIMNSB:1||PTMNSB:1||ROOMTEMPERATURE FERROMAGNETISM:1||RUBIDIUM MANGANESE HEXACYANOFERRATE:1||COLOSSALMAGNETORESISTANCE:1||FINITE TEMPERATURES:1||LAMNO3:1||FE:1||transitionmetal oxides:1||giant magnetoresistance:1||phonon:1||COPPER OXIDES:1||valence states:1||thermoelectric:1||semiconductor:1||CATION DISTRIBUTION:1||FeCr2S4:1||photoemission spectroscopy (PES):1||METALLIC FERROMAGNETISM:1||GRAPHITE:1||SUSCEPTIBILITY:1||UBE13:1||RCrSb3:1||band JahnTeller:1||Ce3S4:1||TiO2:1||PrBa2Cu3O7delta:1||UNTWINNED PRBA2CU3O7:1||AGNIO2:1||HALFMETALLIC FERROMAGNETS:1||CI:1||Energy gap:1||Photoemission:1||Future applications:1||Photoemission measurements:1||Graphene:1||BANDSTRUCTURE:1||TC:1||superconductivity:1||magnetic semiconductors:1||CMRmanganites:1||thin films:1||spin dynamics:1||highTc superconductors:1||ITINERANTELECTRON FERROMAGNETISM:1||SINGLECRYSTALS:1||CeTe2:1||amorphous magnetic materials:1||EPITAXIAL GRAPHENE:1||LAYERED PNICTIDEOXIDES:1||BOROCARBIDE SUPERCONDUCTORS:1||AUGMENTEDWAVE METHOD:1||METALLIC MAGNET UNISN:1||ORIGIN:1||spectrum rearrangement:1||MEANFIELD THEORY:1||MOLECULEBASED MAGNETS:1||METASTABLE STATE:1||INSULATOR:1||magnetic orderin:1||FCC IRON:1||CeRu2:1||TL2MN2O7:1||isotope effect:1||Perovskitemanganites:1||RECURSION METHOD:1||PERPENDICULAR MAGNETICANISOTROPY:1||quasiparticle spectral density:1||GW:1||MANGANESE FERRITE:1||RESONANCE:1||SeCuO3:1||Optical conductivity:1||MASSLESS DIRAC FERMIONS:1||SCHOTTKYBARRIER:1||electronic structure:15||ELECTRONICSTRUCTURE:11||TRANSITIONMETAL COMPOUNDS:10||METALS:10||photoemission:8||SPECTRA:8||MAGNETORESISTANCE:7||FERROMAGNETISM:7||TRANSPORT:7||TRANSITION:6||FILMS:6||THINFILMS:5||TOTALENERGY CALCULATIONS:5||MAGNETICPROPERTIES:5||SUPERCONDUCTIVITY:5||PR:5||LATTICE:4||STATES:4||SPECTROSCOPY:4||FIELD:4||CRYSTALSTRUCTURE:4||PHOTOEMISSION:4||TEMPERATURE:4||TRANSITIONTEMPERATURE:4||XRAYABSORPTION:4||STATE:4||CU:4||BASISSET:4||XAS:4||CRYSTALS:3||EXCITATIONS:3||MOTTHUBBARD SYSTEMS:3||HIGHENERGY SPIN:3||halfmetal:3||INSULATORS:3||LA2CUO4:3||MODEL:3||FLUCTUATIONS:3||CE:3||double exchange:3||TRANSITIONMETALS:3||RESISTIVITY:3||BORON:3||LA1XCAXMNO3:3||IRON:3||PES:3||ANTIMONIDES:2||MgB2:2||ZR METALLIC GLASSES:2||superconductor:2||CRITICALCURRENT DENSITY:2||CIRCULARDICHROISM:2||SEMICONDUCTORS:2||LOCALIZATION:2||INTRABAND OPTICAL CONDUCTIVITY:2||COLOSSAL MAGNETORESISTANCE:2||OXIDATION:2||EXISTENCE:2||COPPER:2||diboride:2||MAGNESIUMDIBORIDE:2||GAP:2||CE COMPOUNDS:2||CORE POLARIZATION:2||magnetoresistance:2||photoemission spectroscopy:2||electronphonon interaction:2||GETTER:2||PD:2||MAGNETISM:2||FECR2S4:2||SUPERCONDUCTING MGB2:2||WIRES:2||ABSORPTION:2||ENERGY:2||LA1XSRXMNO3:2||CONSTANTS:2||polaron:2||charge ordering:2||SCATTERING:2||XRAY PHOTOEMISSION:2||CeNiSn:2||phase diagram:2||PHOTOELECTRON:2||QUADRUPOLAR:2||perovskitemanganites:2||CO:2||SYSTEMS:2||DOPED ZNO:2||LOWFREQUENCY SOUND:2||LA:2||ELECTRONELECTRON SCATTERING:2||AU:2||DENSITYWAVE INSTABILITY:2||FERMISURFACE:2||hybridization:2||VALENCEBAND SATELLITE:2||SULFUR SPINEL:2||Heusler:2||APPROXIMATION:2||superexchange:2||colossal magnetoresistance:2||ALLOYS:2||DEPENDENCE:2||AG:2||electronic structures:2||AUGERSPECTRA:2||CR:2||PARAMETERS:2||DIFFRACTION:2||SEMICONDUCTORMETAL TRANSITION:1||INTERMEDIATEVALENCE:1||SMB6:1||SRRUO3:1||antiperovskite structure with antipolar nature:1||lowenergy twodimensional phonons:1||anatase TiO2:1||La3S4:1||metalinsulator transitions:1||MNO:1||ELECTRONICSTRUCTURES:1||MAGNETIC CIRCULARDICHROISM:1||Density functional theory:1||CeCo2:1||TOPOLARON CROSSOVER:1||EXCHANGE:1||cuprates:1||high Tc cuprates:1||magnetically ordered materials:1||ZNSE:1||Sr2xKxFeMoO6:1||CDW:1||TeCuO3:1||STRUCTURALPROPERTIES:1||MN:1||screening length:1||amorphous Fe:1||WAVE BASISSET:1||SILICONCARBIDE:1||HIGHPRESSURE:1||electronphonon coupling:1||quenched superconductivity:1||CMR perovskite manganites:1||OXIDE:1||polarons:1||synchrotron radiation:1||FULLERIDES:1||RESONANTPHOTOEMISSION:1||Silicon carbide:1||DFT calculation:1||Hybridized bands:1||GIANT MAGNETORESISTANCE:1||PEROVSKITES:1||Raman spectra:1||EXCHANGE ENHANCEMENT:1||SILICON:1||SR2FEMOO6:1||orbital ordering:1||delafossite:1||TITANIUMDIOXIDE:1||electronic structure of disordered solids:1||YFE2:1||Magnetic polaron:1||NA2TI2SB2O:1||STRONGCOUPLED SUPERCONDUCTORS:1||HEAVYFERMION SYSTEMS:1||firstprinciples calculations:1||MECHANISM:1||UNiSn:1||PHOTONIC BANDGAP:1||SINGLE IMPURITY:1||PHONONSPECTRUM:1||FERMISURFACE TOPOLOGY:1||SUPPRESSION:1||RESONANT PHOTOEMISSION:1||METALDOPED PICENE:1||PHOTOIONIZATION CROSSSECTIONS:1||PHOTOINDUCED FERRIMAGNETIC SYSTEMS:1||LINKAGE ISOMERISM:1||CHARGETRANSFER:1||Bilayer Graphene:1||MAGNETICFIELD:1||SPINWAVES:1||rareearth manganese oxides:1||magnonphonon interaction:1||NACO2O4:1||ENERGYBANDS:1||SELFENERGY:1||GAS:1||Fe0.5Cu0.5Cr2S4:1||scanning photoelectron microscopy (SPEM):1||MAGNETIC PROPERTIES:1||Stoner model:1||AMORPHOUS TRANSITIONMETALS:1||SPINGLASS STATES:1||NI:1||LA3NI2B2N3:1||SOLIDS:1||CEO2:1||BAND THEORY:1||dilute magnetic semiconductor:1||pyrochlore:1||Y1XPRXBA2CU3O7DELTA:1||and electronphonon interactions:1||VIBRATIONS:1||RAY PHOTOEMISSION:1||ALKALI CATION:1||Europium:1||colossal magnetoresistance:1||structural stability:1||ENERGYGAP:1||small polaron:1||DOUBLE EXCHANGE:1||Coulomb correlation:1||magnon:1||phonons:1||ELECTRON FERROMAGNETISM:1||CURIETEMPERATURE:1||ARPES:1||PLANEWAVE METHOD:1||Xray absorption spectroscopy (XAS):1||ROOMTEMPERATURE:1||MONOCHALCOGENIDES:1||HEAT:1||UPDSN:1||MOMENTS:1||XRAY ABSORPTION:1||SEMICONDUCTOR:1||Fermi surface nesting:1||optical phonon:1||disordered system:1||dilute magnetic semiconductors:1||CMR manganites:1||PHONONS:1||LATTICEDYNAMICS:1||OXIDES:1||4fphotoemission:1||permanent magnet:1||pseudogap:1||TRANSPORTPROPERTIES:1||ANTIFERROMAGNET:1||(BI,PB)SRCOO SYSTEM:1||semicore correlation:1||POLARIZATION:1||CRYSTAL:1||spinel:1||Xray magnetic circular dichroism (XMCD):1||magnetocapacitance:1||ANATASE:1||TEMPERATURES:1||Pseudogap:1||INTERFACE:1||SUBSTRATE:1||YNI2B2C:1||SAMARIUM SULFIDE:1||strong swave superconductor:1||DOPED MANGANITE:1||SYMMETRY:1||CENISN:1||resonance mode:1||DISORDERED SYSTEM:1||LITHIUM INTERCALATION:1||CUO2 PLANE:1||SURFACE:1||Delafossite:1||ELECTRICALPROPERTIES:1||NIMNSB:1||PTMNSB:1||ROOMTEMPERATURE FERROMAGNETISM:1||RUBIDIUM MANGANESE HEXACYANOFERRATE:1||COLOSSALMAGNETORESISTANCE:1||FINITE TEMPERATURES:1||LAMNO3:1||FE:1||transitionmetal oxides:1||giant magnetoresistance:1||phonon:1||COPPER OXIDES:1||valence states:1||thermoelectric:1||semiconductor:1||CATION DISTRIBUTION:1||FeCr2S4:1||photoemission spectroscopy (PES):1||METALLIC FERROMAGNETISM:1||GRAPHITE:1||SUSCEPTIBILITY:1||UBE13:1||RCrSb3:1||band JahnTeller:1||Ce3S4:1||TiO2:1||PrBa2Cu3O7delta:1||UNTWINNED PRBA2CU3O7:1||AGNIO2:1||HALFMETALLIC FERROMAGNETS:1||CI:1||Energy gap:1||Photoemission:1||Future applications:1||Photoemission measurements:1||Graphene:1||BANDSTRUCTURE:1||TC:1||superconductivity:1||magnetic semiconductors:1||CMRmanganites:1||thin films:1||spin dynamics:1||highTc superconductors:1||ITINERANTELECTRON FERROMAGNETISM:1||SINGLECRYSTALS:1||CeTe2:1||amorphous magnetic materials:1||EPITAXIAL GRAPHENE:1||LAYERED PNICTIDEOXIDES:1||BOROCARBIDE SUPERCONDUCTORS:1||AUGMENTEDWAVE METHOD:1||METALLIC MAGNET UNISN:1||ORIGIN:1||spectrum rearrangement:1||MEANFIELD THEORY:1||MOLECULEBASED MAGNETS:1||METASTABLE STATE:1||INSULATOR:1||magnetic orderin:1||FCC IRON:1||CeRu2:1||TL2MN2O7:1||isotope effect:1||Perovskitemanganites:1||RECURSION METHOD:1||PERPENDICULAR MAGNETICANISOTROPY:1||quasiparticle spectral density:1||GW:1||MANGANESE FERRITE:1||RESONANCE:1||SeCuO3:1||Optical conductivity:1||MASSLESS DIRAC FERMIONS:1||SCHOTTKYBARRIER:1||electronic structure:15||ELECTRONICSTRUCTURE:11||TRANSITIONMETAL COMPOUNDS:10||METALS:10||photoemission:8||SPECTRA:8||MAGNETORESISTANCE:7||FERROMAGNETISM:7||TRANSPORT:7||TRANSITION:6||FILMS:6||THINFILMS:5||TOTALENERGY CALCULATIONS:5||MAGNETICPROPERTIES:5||SUPERCONDUCTIVITY:5||PR:5||LATTICE:4||STATES:4||SPECTROSCOPY:4||FIELD:4||CRYSTALSTRUCTURE:4||PHOTOEMISSION:4||TEMPERATURE:4||TRANSITIONTEMPERATURE:4||XRAYABSORPTION:4||STATE:4||CU:4||BASISSET:4||XAS:4||CRYSTALS:3||EXCITATIONS:3||MOTTHUBBARD SYSTEMS:3||HIGHENERGY SPIN:3||halfmetal:3||INSULATORS:3||LA2CUO4:3||MODEL:3||FLUCTUATIONS:3||CE:3||double exchange:3||TRANSITIONMETALS:3||RESISTIVITY:3||BORON:3||LA1XCAXMNO3:3||IRON:3||PES:3||ANTIMONIDES:2||MgB2:2||ZR METALLIC GLASSES:2||superconductor:2||CRITICALCURRENT DENSITY:2||CIRCULARDICHROISM:2||SEMICONDUCTORS:2||LOCALIZATION:2||INTRABAND OPTICAL CONDUCTIVITY:2||COLOSSAL MAGNETORESISTANCE:2||OXIDATION:2||EXISTENCE:2||COPPER:2||diboride:2||MAGNESIUMDIBORIDE:2||GAP:2||CE COMPOUNDS:2||CORE POLARIZATION:2||magnetoresistance:2||photoemission spectroscopy:2||electronphonon interaction:2||GETTER:2||PD:2||MAGNETISM:2||FECR2S4:2||SUPERCONDUCTING MGB2:2||WIRES:2||ABSORPTION:2||ENERGY:2||LA1XSRXMNO3:2||CONSTANTS:2||polaron:2||charge ordering:2||SCATTERING:2||XRAY PHOTOEMISSION:2||CeNiSn:2||phase diagram:2||PHOTOELECTRON:2||QUADRUPOLAR:2||perovskitemanganites:2||CO:2||SYSTEMS:2||DOPED ZNO:2||LOWFREQUENCY SOUND:2||LA:2||ELECTRONELECTRON SCATTERING:2||AU:2||DENSITYWAVE INSTABILITY:2||FERMISURFACE:2||hybridization:2||VALENCEBAND SATELLITE:2||SULFUR SPINEL:2||Heusler:2||APPROXIMATION:2||superexchange:2||colossal magnetoresistance:2||ALLOYS:2||DEPENDENCE:2||AG:2||electronic structures:2||AUGERSPECTRA:2||CR:2||PARAMETERS:2||DIFFRACTION:2||SEMICONDUCTORMETAL TRANSITION:1||INTERMEDIATEVALENCE:1||SMB6:1||SRRUO3:1||antiperovskite structure with antipolar nature:1||lowenergy twodimensional phonons:1||anatase TiO2:1||La3S4:1||metalinsulator transitions:1||MNO:1||ELECTRONICSTRUCTURES:1||MAGNETIC CIRCULARDICHROISM:1||Density functional theory:1||CeCo2:1||TOPOLARON CROSSOVER:1||EXCHANGE:1||cuprates:1||high Tc cuprates:1||magnetically ordered materials:1||ZNSE:1||Sr2xKxFeMoO6:1||CDW:1||TeCuO3:1||STRUCTURALPROPERTIES:1||MN:1||screening length:1||amorphous Fe:1||WAVE BASISSET:1||SILICONCARBIDE:1||HIGHPRESSURE:1||electronphonon coupling:1||quenched superconductivity:1||CMR perovskite manganites:1||OXIDE:1||polarons:1||synchrotron radiation:1||FULLERIDES:1||RESONANTPHOTOEMISSION:1||Silicon carbide:1||DFT calculation:1||Hybridized bands:1||GIANT MAGNETORESISTANCE:1||PEROVSKITES:1||Raman spectra:1||EXCHANGE ENHANCEMENT:1||SILICON:1||SR2FEMOO6:1||orbital ordering:1||delafossite:1||TITANIUMDIOXIDE:1||electronic structure of disordered solids:1||YFE2:1||Magnetic polaron:1||NA2TI2SB2O:1||STRONGCOUPLED SUPERCONDUCTORS:1||HEAVYFERMION SYSTEMS:1||firstprinciples calculations:1||MECHANISM:1||UNiSn:1||PHOTONIC BANDGAP:1||SINGLE IMPURITY:1||PHONONSPECTRUM:1||FERMISURFACE TOPOLOGY:1||SUPPRESSION:1||RESONANT PHOTOEMISSION:1||METALDOPED PICENE:1||PHOTOIONIZATION CROSSSECTIONS:1||PHOTOINDUCED FERRIMAGNETIC SYSTEMS:1||LINKAGE ISOMERISM:1||CHARGETRANSFER:1||Bilayer Graphene:1||MAGNETICFIELD:1||SPINWAVES:1||rareearth manganese oxides:1||magnonphonon interaction:1||NACO2O4:1||ENERGYBANDS:1||SELFENERGY:1||GAS:1||Fe0.5Cu0.5Cr2S4:1||scanning photoelectron microscopy (SPEM):1||MAGNETIC PROPERTIES:1||Stoner model:1||AMORPHOUS TRANSITIONMETALS:1||SPINGLASS STATES:1||NI:1||LA3NI2B2N3:1||SOLIDS:1||CEO2:1||BAND THEORY:1||dilute magnetic semiconductor:1||pyrochlore:1||Y1XPRXBA2CU3O7DELTA:1||and electronphonon interactions:1||VIBRATIONS:1||RAY PHOTOEMISSION:1||ALKALI CATION:1||Europium:1||colossal magnetoresistance:1||structural stability:1||ENERGYGAP:1||small polaron:1||DOUBLE EXCHANGE:1||Coulomb correlation:1||magnon:1||phonons:1||ELECTRON FERROMAGNETISM:1||CURIETEMPERATURE:1||ARPES:1||PLANEWAVE METHOD:1||Xray absorption spectroscopy (XAS):1||ROOMTEMPERATURE:1||MONOCHALCOGENIDES:1||HEAT:1||UPDSN:1||MOMENTS:1||XRAY ABSORPTION:1||SEMICONDUCTOR:1||Fermi surface nesting:1||optical phonon:1||disordered system:1||dilute magnetic semiconductors:1||CMR manganites:1||PHONONS:1||LATTICEDYNAMICS:1||OXIDES:1||4fphotoemission:1||permanent magnet:1||pseudogap:1||TRANSPORTPROPERTIES:1||ANTIFERROMAGNET:1||(BI,PB)SRCOO SYSTEM:1||semicore correlation:1||POLARIZATION:1||CRYSTAL:1||spinel:1||Xray magnetic circular dichroism (XMCD):1||magnetocapacitance:1||ANATASE:1||TEMPERATURES:1||Pseudogap:1||INTERFACE:1||SUBSTRATE:1||YNI2B2C:1||SAMARIUM SULFIDE:1||strong swave superconductor:1||DOPED MANGANITE:1||SYMMETRY:1||CENISN:1||resonance mode:1||DISORDERED SYSTEM:1||LITHIUM INTERCALATION:1||CUO2 PLANE:1||SURFACE:1||Delafossite:1||ELECTRICALPROPERTIES:1||NIMNSB:1||PTMNSB:1||ROOMTEMPERATURE FERROMAGNETISM:1||RUBIDIUM MANGANESE HEXACYANOFERRATE:1||COLOSSALMAGNETORESISTANCE:1||FINITE TEMPERATURES:1||LAMNO3:1||FE:1||transitionmetal oxides:1||giant magnetoresistance:1||phonon:1||COPPER OXIDES:1||valence states:1||thermoelectric:1||semiconductor:1||CATION DISTRIBUTION:1||FeCr2S4:1||photoemission spectroscopy (PES):1||METALLIC FERROMAGNETISM:1||GRAPHITE:1||SUSCEPTIBILITY:1||UBE13:1||RCrSb3:1||band JahnTeller:1||Ce3S4:1||TiO2:1||PrBa2Cu3O7delta:1||UNTWINNED PRBA2CU3O7:1||AGNIO2:1||HALFMETALLIC FERROMAGNETS:1||CI:1||Energy gap:1||Photoemission:1||Future applications:1||Photoemission measurements:1||Graphene:1||BANDSTRUCTURE:1||TC:1||superconductivity:1||magnetic semiconductors:1||CMRmanganites:1||thin films:1||spin dynamics:1||highTc superconductors:1||ITINERANTELECTRON FERROMAGNETISM:1||SINGLECRYSTALS:1||CeTe2:1||amorphous magnetic materials:1||EPITAXIAL GRAPHENE:1||LAYERED PNICTIDEOXIDES:1||BOROCARBIDE SUPERCONDUCTORS:1||AUGMENTEDWAVE METHOD:1||METALLIC MAGNET UNISN:1||ORIGIN:1||spectrum rearrangement:1||MEANFIELD THEORY:1||MOLECULEBASED MAGNETS:1||METASTABLE STATE:1||INSULATOR:1||magnetic orderin:1||FCC IRON:1||CeRu2:1||TL2MN2O7:1||isotope effect:1||Perovskitemanganites:1||RECURSION METHOD:1||PERPENDICULAR MAGNETICANISOTROPY:1||quasiparticle spectral density:1||GW:1||MANGANESE FERRITE:1||RESONANCE:1||SeCuO3:1||Optical conductivity:1||MASSLESS DIRAC FERMIONS:1||SCHOTTKYBARRIER:1||electronic structure:15||ELECTRONICSTRUCTURE:11||TRANSITIONMETAL COMPOUNDS:10||METALS:10||photoemission:8||SPECTRA:8||MAGNETORESISTANCE:7||FERROMAGNETISM:7||TRANSPORT:7||TRANSITION:6||FILMS:6||THINFILMS:5||TOTALENERGY CALCULATIONS:5||MAGNETICPROPERTIES:5||SUPERCONDUCTIVITY:5||PR:5||LATTICE:4||STATES:4||SPECTROSCOPY:4||FIELD:4||CRYSTALSTRUCTURE:4||PHOTOEMISSION:4||TEMPERATURE:4||TRANSITIONTEMPERATURE:4||XRAYABSORPTION:4||STATE:4||CU:4||BASISSET:4||XAS:4||CRYSTALS:3||EXCITATIONS:3||MOTTHUBBARD SYSTEMS:3||HIGHENERGY SPIN:3||halfmetal:3||INSULATORS:3||LA2CUO4:3||MODEL:3||FLUCTUATIONS:3||CE:3||double exchange:3||TRANSITIONMETALS:3||RESISTIVITY:3||BORON:3||LA1XCAXMNO3:3||IRON:3||PES:3||ANTIMONIDES:2||MgB2:2||ZR METALLIC GLASSES:2||superconductor:2||CRITICALCURRENT DENSITY:2||CIRCULARDICHROISM:2||SEMICONDUCTORS:2||LOCALIZATION:2||INTRABAND OPTICAL CONDUCTIVITY:2||COLOSSAL MAGNETORESISTANCE:2||OXIDATION:2||EXISTENCE:2||COPPER:2||diboride:2||MAGNESIUMDIBORIDE:2||GAP:2||CE COMPOUNDS:2||CORE POLARIZATION:2||magnetoresistance:2||photoemission spectroscopy:2||electronphonon interaction:2||GETTER:2||PD:2||MAGNETISM:2||FECR2S4:2||SUPERCONDUCTING MGB2:2||WIRES:2||ABSORPTION:2||ENERGY:2||LA1XSRXMNO3:2||CONSTANTS:2||polaron:2||charge ordering:2||SCATTERING:2||XRAY PHOTOEMISSION:2||CeNiSn:2||phase diagram:2||PHOTOELECTRON:2||QUADRUPOLAR:2||perovskitemanganites:2||CO:2||SYSTEMS:2||DOPED ZNO:2||LOWFREQUENCY SOUND:2||LA:2||ELECTRONELECTRON SCATTERING:2||AU:2||DENSITYWAVE INSTABILITY:2||FERMISURFACE:2||hybridization:2||VALENCEBAND SATELLITE:2||SULFUR SPINEL:2||Heusler:2||APPROXIMATION:2||superexchange:2||colossal magnetoresistance:2||ALLOYS:2||DEPENDENCE:2||AG:2||electronic structures:2||AUGERSPECTRA:2||CR:2||PARAMETERS:2||DIFFRACTION:2||SEMICONDUCTORMETAL TRANSITION:1||INTERMEDIATEVALENCE:1||SMB6:1||SRRUO3:1||antiperovskite structure with antipolar nature:1||lowenergy twodimensional phonons:1||anatase TiO2:1||La3S4:1||metalinsulator transitions:1||MNO:1||ELECTRONICSTRUCTURES:1||MAGNETIC CIRCULARDICHROISM:1||Density functional theory:1||CeCo2:1||TOPOLARON CROSSOVER:1||EXCHANGE:1||cuprates:1||high Tc cuprates:1||magnetically ordered materials:1||ZNSE:1||Sr2xKxFeMoO6:1||CDW:1||TeCuO3:1||STRUCTURALPROPERTIES:1||MN:1||screening length:1||amorphous Fe:1||WAVE BASISSET:1||SILICONCARBIDE:1||HIGHPRESSURE:1||electronphonon coupling:1||quenched superconductivity:1||CMR perovskite manganites:1||OXIDE:1||polarons:1||synchrotron radiation:1||FULLERIDES:1||RESONANTPHOTOEMISSION:1||Silicon carbide:1||DFT calculation:1||Hybridized bands:1||GIANT MAGNETORESISTANCE:1||PEROVSKITES:1||Raman spectra:1||EXCHANGE ENHANCEMENT:1||SILICON:1||SR2FEMOO6:1||orbital ordering:1||delafossite:1||TITANIUMDIOXIDE:1||electronic structure of disordered solids:1||YFE2:1||Magnetic polaron:1||NA2TI2SB2O:1||STRONGCOUPLED SUPERCONDUCTORS:1||HEAVYFERMION SYSTEMS:1||firstprinciples calculations:1||MECHANISM:1||UNiSn:1||PHOTONIC BANDGAP:1||SINGLE IMPURITY:1||PHONONSPECTRUM:1||FERMISURFACE TOPOLOGY:1||SUPPRESSION:1||RESONANT PHOTOEMISSION:1||METALDOPED PICENE:1||PHOTOIONIZATION CROSSSECTIONS:1||PHOTOINDUCED FERRIMAGNETIC SYSTEMS:1||LINKAGE ISOMERISM:1||CHARGETRANSFER:1||Bilayer Graphene:1||MAGNETICFIELD:1||SPINWAVES:1||rareearth manganese oxides:1||magnonphonon interaction:1||NACO2O4:1||ENERGYBANDS:1||SELFENERGY:1||GAS:1||Fe0.5Cu0.5Cr2S4:1||scanning photoelectron microscopy (SPEM):1||MAGNETIC PROPERTIES:1||Stoner model:1||AMORPHOUS TRANSITIONMETALS:1||SPINGLASS STATES:1||NI:1||LA3NI2B2N3:1||SOLIDS:1||CEO2:1||BAND THEORY:1||dilute magnetic semiconductor:1||pyrochlore:1||Y1XPRXBA2CU3O7DELTA:1||and electronphonon interactions:1||VIBRATIONS:1||RAY PHOTOEMISSION:1||ALKALI CATION:1||Europium:1||colossal magnetoresistance:1||structural stability:1||ENERGYGAP:1||small polaron:1||DOUBLE EXCHANGE:1||Coulomb correlation:1||magnon:1||phonons:1||ELECTRON FERROMAGNETISM:1||CURIETEMPERATURE:1||ARPES:1||PLANEWAVE METHOD:1||Xray absorption spectroscopy (XAS):1||ROOMTEMPERATURE:1||MONOCHALCOGENIDES:1||HEAT:1||UPDSN:1||MOMENTS:1||XRAY ABSORPTION:1||SEMICONDUCTOR:1||Fermi surface nesting:1||optical phonon:1||disordered system:1||dilute magnetic semiconductors:1||CMR manganites:1||PHONONS:1||LATTICEDYNAMICS:1||OXIDES:1||4fphotoemission:1||permanent magnet:1||pseudogap:1||TRANSPORTPROPERTIES:1||ANTIFERROMAGNET:1||(BI,PB)SRCOO SYSTEM:1||semicore correlation:1||POLARIZATION:1||CRYSTAL:1||spinel:1||Xray magnetic circular dichroism (XMCD):1||magnetocapacitance:1||ANATASE:1||TEMPERATURES:1||Pseudogap:1||INTERFACE:1||SUBSTRATE:1||YNI2B2C:1||SAMARIUM SULFIDE:1||strong swave superconductor:1||DOPED MANGANITE:1||SYMMETRY:1||CENISN:1||resonance mode:1||DISORDERED SYSTEM:1||LITHIUM INTERCALATION:1||CUO2 PLANE:1||SURFACE:1||Delafossite:1||ELECTRICALPROPERTIES:1||NIMNSB:1||PTMNSB:1||ROOMTEMPERATURE FERROMAGNETISM:1||RUBIDIUM MANGANESE HEXACYANOFERRATE:1||COLOSSALMAGNETORESISTANCE:1||FINITE TEMPERATURES:1||LAMNO3:1||FE:1||transitionmetal oxides:1||giant magnetoresistance:1||phonon:1||COPPER OXIDES:1||valence states:1||thermoelectric:1||semiconductor:1||CATION DISTRIBUTION:1||FeCr2S4:1||photoemission spectroscopy (PES):1||METALLIC FERROMAGNETISM:1||GRAPHITE:1||SUSCEPTIBILITY:1||UBE13:1||RCrSb3:1||band JahnTeller:1||Ce3S4:1||TiO2:1||PrBa2Cu3O7delta:1||UNTWINNED PRBA2CU3O7:1||AGNIO2:1||HALFMETALLIC FERROMAGNETS:1||CI:1||Energy gap:1||Photoemission:1||Future applications:1||Photoemission measurements:1||Graphene:1||BANDSTRUCTURE:1||TC:1||superconductivity:1||magnetic semiconductors:1||CMRmanganites:1||thin films:1||spin dynamics:1||highTc superconductors:1||ITINERANTELECTRON FERROMAGNETISM:1||SINGLECRYSTALS:1||CeTe2:1||amorphous magnetic materials:1||EPITAXIAL GRAPHENE:1||LAYERED PNICTIDEOXIDES:1||BOROCARBIDE SUPERCONDUCTORS:1||AUGMENTEDWAVE METHOD:1||METALLIC MAGNET UNISN:1||ORIGIN:1||spectrum rearrangement:1||MEANFIELD THEORY:1||MOLECULEBASED MAGNETS:1||METASTABLE STATE:1||INSULATOR:1||magnetic orderin:1||FCC IRON:1||CeRu2:1||TL2MN2O7:1||isotope effect:1||Perovskitemanganites:1||RECURSION METHOD:1||PERPENDICULAR MAGNETICANISOTROPY:1||quasiparticle spectral density:1||GW:1||MANGANESE FERRITE:1||RESONANCE:1||SeCuO3:1||Optical conductivity:1||MASSLESS DIRAC FERMIONS:1||SCHOTTKYBARRIER:1||electronic structure:15||ELECTRONICSTRUCTURE:11||TRANSITIONMETAL COMPOUNDS:10||METALS:10||photoemission:8||SPECTRA:8||MAGNETORESISTANCE:7||FERROMAGNETISM:7||TRANSPORT:7||TRANSITION:6||FILMS:6||THINFILMS:5||TOTALENERGY CALCULATIONS:5||MAGNETICPROPERTIES:5||SUPERCONDUCTIVITY:5||PR:5||LATTICE:4||STATES:4||SPECTROSCOPY:4||FIELD:4||CRYSTALSTRUCTURE:4||PHOTOEMISSION:4||TEMPERATURE:4||TRANSITIONTEMPERATURE:4||XRAYABSORPTION:4||STATE:4||CU:4||BASISSET:4||XAS:4||CRYSTALS:3||EXCITATIONS:3||MOTTHUBBARD SYSTEMS:3||HIGHENERGY SPIN:3||halfmetal:3||INSULATORS:3||LA2CUO4:3||MODEL:3||FLUCTUATIONS:3||CE:3||double exchange:3||TRANSITIONMETALS:3||RESISTIVITY:3||BORON:3||LA1XCAXMNO3:3||IRON:3||PES:3||ANTIMONIDES:2||MgB2:2||ZR METALLIC GLASSES:2||superconductor:2||CRITICALCURRENT DENSITY:2||CIRCULARDICHROISM:2||SEMICONDUCTORS:2||LOCALIZATION:2||INTRABAND OPTICAL CONDUCTIVITY:2||COLOSSAL MAGNETORESISTANCE:2||OXIDATION:2||EXISTENCE:2||COPPER:2||diboride:2||MAGNESIUMDIBORIDE:2||GAP:2||CE COMPOUNDS:2||CORE POLARIZATION:2||magnetoresistance:2||photoemission spectroscopy:2||electronphonon interaction:2||GETTER:2||PD:2||MAGNETISM:2||FECR2S4:2||SUPERCONDUCTING MGB2:2||WIRES:2||ABSORPTION:2||ENERGY:2||LA1XSRXMNO3:2||CONSTANTS:2||polaron:2||charge ordering:2||SCATTERING:2||XRAY PHOTOEMISSION:2||CeNiSn:2||phase diagram:2||PHOTOELECTRON:2||QUADRUPOLAR:2||perovskitemanganites:2||CO:2||SYSTEMS:2||DOPED ZNO:2||LOWFREQUENCY SOUND:2||LA:2||ELECTRONELECTRON SCATTERING:2||AU:2||DENSITYWAVE INSTABILITY:2||FERMISURFACE:2||hybridization:2||VALENCEBAND SATELLITE:2||SULFUR SPINEL:2||Heusler:2||APPROXIMATION:2||superexchange:2||colossal magnetoresistance:2||ALLOYS:2||DEPENDENCE:2||AG:2||electronic structures:2||AUGERSPECTRA:2||CR:2||PARAMETERS:2||DIFFRACTION:2||SEMICONDUCTORMETAL TRANSITION:1||INTERMEDIATEVALENCE:1||SMB6:1||SRRUO3:1||antiperovskite structure with antipolar nature:1||lowenergy twodimensional phonons:1||anatase TiO2:1||La3S4:1||metalinsulator transitions:1||MNO:1||ELECTRONICSTRUCTURES:1||MAGNETIC CIRCULARDICHROISM:1||Density functional theory:1||CeCo2:1||TOPOLARON CROSSOVER:1||EXCHANGE:1||cuprates:1||high Tc cuprates:1||magnetically ordered materials:1||ZNSE:1||Sr2xKxFeMoO6:1||CDW:1||TeCuO3:1||STRUCTURALPROPERTIES:1||MN:1||screening length:1||amorphous Fe:1||WAVE BASISSET:1||SILICONCARBIDE:1||HIGHPRESSURE:1||electronphonon coupling:1||quenched superconductivity:1||CMR perovskite manganites:1||OXIDE:1||polarons:1||synchrotron radiation:1||FULLERIDES:1||RESONANTPHOTOEMISSION:1||Silicon carbide:1||DFT calculation:1||Hybridized bands:1||GIANT MAGNETORESISTANCE:1||PEROVSKITES:1||Raman spectra:1||EXCHANGE ENHANCEMENT:1||SILICON:1||SR2FEMOO6:1||orbital ordering:1||delafossite:1||TITANIUMDIOXIDE:1||electronic structure of disordered solids:1||YFE2:1||Magnetic polaron:1||NA2TI2SB2O:1||STRONGCOUPLED SUPERCONDUCTORS:1||HEAVYFERMION SYSTEMS:1||firstprinciples calculations:1||MECHANISM:1||UNiSn:1||PHOTONIC BANDGAP:1||SINGLE IMPURITY:1||PHONONSPECTRUM:1||FERMISURFACE TOPOLOGY:1||SUPPRESSION:1||RESONANT PHOTOEMISSION:1||METALDOPED PICENE:1||PHOTOIONIZATION CROSSSECTIONS:1||PHOTOINDUCED FERRIMAGNETIC SYSTEMS:1||LINKAGE ISOMERISM:1||CHARGETRANSFER:1||Bilayer Graphene:1||MAGNETICFIELD:1||SPINWAVES:1||rareearth manganese oxides:1||magnonphonon interaction:1||NACO2O4:1||ENERGYBANDS:1||SELFENERGY:1||GAS:1||Fe0.5Cu0.5Cr2S4:1||scanning photoelectron microscopy (SPEM):1||MAGNETIC PROPERTIES:1||Stoner model:1||AMORPHOUS TRANSITIONMETALS:1||SPINGLASS STATES:1||NI:1||LA3NI2B2N3:1||SOLIDS:1||CEO2:1||BAND THEORY:1||dilute magnetic semiconductor:1||pyrochlore:1||Y1XPRXBA2CU3O7DELTA:1||and electronphonon interactions:1||VIBRATIONS:1||RAY PHOTOEMISSION:1||ALKALI CATION:1||Europium:1||colossal magnetoresistance:1||structural stability:1||ENERGYGAP:1||small polaron:1||DOUBLE EXCHANGE:1||Coulomb correlation:1||magnon:1||phonons:1||ELECTRON FERROMAGNETISM:1||CURIETEMPERATURE:1||ARPES:1||PLANEWAVE METHOD:1||Xray absorption spectroscopy (XAS):1||ROOMTEMPERATURE:1||MONOCHALCOGENIDES:1||HEAT:1||UPDSN:1||MOMENTS:1||XRAY ABSORPTION:1||SEMICONDUCTOR:1||Fermi surface nesting:1||optical phonon:1||disordered system:1||dilute magnetic semiconductors:1||CMR manganites:1||PHONONS:1||LATTICEDYNAMICS:1||OXIDES:1||4fphotoemission:1||permanent magnet:1||pseudogap:1||TRANSPORTPROPERTIES:1||ANTIFERROMAGNET:1||(BI,PB)SRCOO SYSTEM:1||semicore correlation:1||POLARIZATION:1||CRYSTAL:1||spinel:1||Xray magnetic circular dichroism (XMCD):1||magnetocapacitance:1||ANATASE:1||TEMPERATURES:1||Pseudogap:1||INTERFACE:1||SUBSTRATE:1||YNI2B2C:1||SAMARIUM SULFIDE:1||strong swave superconductor:1||DOPED MANGANITE:1||SYMMETRY:1||CENISN:1||resonance mode:1||DISORDERED SYSTEM:1||LITHIUM INTERCALATION:1||CUO2 PLANE:1||SURFACE:1||Delafossite:1||ELECTRICALPROPERTIES:1||NIMNSB:1||PTMNSB:1||ROOMTEMPERATURE FERROMAGNETISM:1||RUBIDIUM MANGANESE HEXACYANOFERRATE:1||COLOSSALMAGNETORESISTANCE:1||FINITE TEMPERATURES:1||LAMNO3:1||FE:1||transitionmetal oxides:1||giant magnetoresistance:1||phonon:1||COPPER OXIDES:1||valence states:1||thermoelectric:1||semiconductor:1||CATION DISTRIBUTION:1||FeCr2S4:1||photoemission spectroscopy (PES):1||METALLIC FERROMAGNETISM:1||GRAPHITE:1||SUSCEPTIBILITY:1||UBE13:1||RCrSb3:1||band JahnTeller:1||Ce3S4:1||TiO2:1||PrBa2Cu3O7delta:1||UNTWINNED PRBA2CU3O7:1||AGNIO2:1||HALFMETALLIC FERROMAGNETS:1||CI:1||Energy gap:1||Photoemission:1||Future applications:1||Photoemission measurements:1||Graphene:1||BANDSTRUCTURE:1||TC:1||superconductivity:1||magnetic semiconductors:1||CMRmanganites:1||thin films:1||spin dynamics:1||highTc superconductors:1||ITINERANTELECTRON FERROMAGNETISM:1||SINGLECRYSTALS:1||CeTe2:1||amorphous magnetic materials:1||EPITAXIAL GRAPHENE:1||LAYERED PNICTIDEOXIDES:1||BOROCARBIDE SUPERCONDUCTORS:1||AUGMENTEDWAVE METHOD:1||METALLIC MAGNET UNISN:1||ORIGIN:1||spectrum rearrangement:1||MEANFIELD THEORY:1||MOLECULEBASED MAGNETS:1||METASTABLE STATE:1||INSULATOR:1||magnetic orderin:1||FCC IRON:1||CeRu2:1||TL2MN2O7:1||isotope effect:1||Perovskitemanganites:1||RECURSION METHOD:1||PERPENDICULAR MAGNETICANISOTROPY:1||quasiparticle spectral density:1||GW:1||MANGANESE FERRITE:1||RESONANCE:1||SeCuO3:1||Optical conductivity:1||MASSLESS DIRAC FERMIONS:1||SCHOTTKYBARRIER:1||electronic structure:15||ELECTRONICSTRUCTURE:11||TRANSITIONMETAL COMPOUNDS:10||METALS:10||photoemission:8||SPECTRA:8||MAGNETORESISTANCE:7||FERROMAGNETISM:7||TRANSPORT:7||TRANSITION:6||FILMS:6||THINFILMS:5||TOTALENERGY CALCULATIONS:5||MAGNETICPROPERTIES:5||SUPERCONDUCTIVITY:5||PR:5||LATTICE:4||STATES:4||SPECTROSCOPY:4||FIELD:4||CRYSTALSTRUCTURE:4||PHOTOEMISSION:4||TEMPERATURE:4||TRANSITIONTEMPERATURE:4||XRAYABSORPTION:4||STATE:4||CU:4||BASISSET:4||XAS:4||CRYSTALS:3||EXCITATIONS:3||MOTTHUBBARD SYSTEMS:3||HIGHENERGY SPIN:3||halfmetal:3||INSULATORS:3||LA2CUO4:3||MODEL:3||FLUCTUATIONS:3||CE:3||double exchange:3||TRANSITIONMETALS:3||RESISTIVITY:3||BORON:3||LA1XCAXMNO3:3||IRON:3||PES:3||ANTIMONIDES:2||MgB2:2||ZR METALLIC GLASSES:2||superconductor:2||CRITICALCURRENT DENSITY:2||CIRCULARDICHROISM:2||SEMICONDUCTORS:2||LOCALIZATION:2||INTRABAND OPTICAL CONDUCTIVITY:2||COLOSSAL MAGNETORESISTANCE:2||OXIDATION:2||EXISTENCE:2||COPPER:2||diboride:2||MAGNESIUMDIBORIDE:2||GAP:2||CE COMPOUNDS:2||CORE POLARIZATION:2||magnetoresistance:2||photoemission spectroscopy:2||electronphonon interaction:2||GETTER:2||PD:2||MAGNETISM:2||FECR2S4:2||SUPERCONDUCTING MGB2:2||WIRES:2||ABSORPTION:2||ENERGY:2||LA1XSRXMNO3:2||CONSTANTS:2||polaron:2||charge ordering:2||SCATTERING:2||XRAY PHOTOEMISSION:2||CeNiSn:2||phase diagram:2||PHOTOELECTRON:2||QUADRUPOLAR:2||perovskitemanganites:2||CO:2||SYSTEMS:2||DOPED ZNO:2||LOWFREQUENCY SOUND:2||LA:2||ELECTRONELECTRON SCATTERING:2||AU:2||DENSITYWAVE INSTABILITY:2||FERMISURFACE:2||hybridization:2||VALENCEBAND SATELLITE:2||SULFUR SPINEL:2||Heusler:2||APPROXIMATION:2||superexchange:2||colossal magnetoresistance:2||ALLOYS:2||DEPENDENCE:2||AG:2||electronic structures:2||AUGERSPECTRA:2||CR:2||PARAMETERS:2||DIFFRACTION:2||SEMICONDUCTORMETAL TRANSITION:1||INTERMEDIATEVALENCE:1||SMB6:1||SRRUO3:1||antiperovskite structure with antipolar nature:1||lowenergy twodimensional phonons:1||anatase TiO2:1||La3S4:1||metalinsulator transitions:1||MNO:1||ELECTRONICSTRUCTURES:1||MAGNETIC CIRCULARDICHROISM:1||Density functional theory:1||CeCo2:1||TOPOLARON CROSSOVER:1||EXCHANGE:1||cuprates:1||high Tc cuprates:1||magnetically ordered materials:1||ZNSE:1||Sr2xKxFeMoO6:1||CDW:1||TeCuO3:1||STRUCTURALPROPERTIES:1||MN:1||screening length:1||amorphous Fe:1||WAVE BASISSET:1||SILICONCARBIDE:1||HIGHPRESSURE:1||electronphonon coupling:1||quenched superconductivity:1||CMR perovskite manganites:1||OXIDE:1||polarons:1||synchrotron radiation:1||FULLERIDES:1||RESONANTPHOTOEMISSION:1||Silicon carbide:1||DFT calculation:1||Hybridized bands:1||GIANT MAGNETORESISTANCE:1||PEROVSKITES:1||Raman spectra:1||EXCHANGE ENHANCEMENT:1||SILICON:1||SR2FEMOO6:1||orbital ordering:1||delafossite:1||TITANIUMDIOXIDE:1||electronic structure of disordered solids:1||YFE2:1||Magnetic polaron:1||NA2TI2SB2O:1||STRONGCOUPLED SUPERCONDUCTORS:1||HEAVYFERMION SYSTEMS:1||firstprinciples calculations:1||MECHANISM:1||UNiSn:1||PHOTONIC BANDGAP:1||SINGLE IMPURITY:1||PHONONSPECTRUM:1||FERMISURFACE TOPOLOGY:1||SUPPRESSION:1||RESONANT PHOTOEMISSION:1||METALDOPED PICENE:1||PHOTOIONIZATION CROSSSECTIONS:1||PHOTOINDUCED FERRIMAGNETIC SYSTEMS:1||LINKAGE ISOMERISM:1||CHARGETRANSFER:1||Bilayer Graphene:1||MAGNETICFIELD:1||SPINWAVES:1||rareearth manganese oxides:1||magnonphonon interaction:1||NACO2O4:1||ENERGYBANDS:1||SELFENERGY:1||GAS:1||Fe0.5Cu0.5Cr2S4:1||scanning photoelectron microscopy (SPEM):1||MAGNETIC PROPERTIES:1||Stoner model:1||AMORPHOUS TRANSITIONMETALS:1||SPINGLASS STATES:1||NI:1||LA3NI2B2N3:1||SOLIDS:1||CEO2:1||BAND THEORY:1||dilute magnetic semiconductor:1||pyrochlore:1||Y1XPRXBA2CU3O7DELTA:1||and electronphonon interactions:1||VIBRATIONS:1||RAY PHOTOEMISSION:1||ALKALI CATION:1||Europium:1||colossal magnetoresistance:1||structural stability:1||ENERGYGAP:1||small polaron:1||DOUBLE EXCHANGE:1||Coulomb correlation:1||magnon:1||phonons:1||ELECTRON FERROMAGNETISM:1||CURIETEMPERATURE:1||ARPES:1||PLANEWAVE METHOD:1||Xray absorption spectroscopy (XAS):1||ROOMTEMPERATURE:1||MONOCHALCOGENIDES:1||HEAT:1||UPDSN:1||MOMENTS:1||XRAY ABSORPTION:1||SEMICONDUCTOR:1||Fermi surface nesting:1||optical phonon:1||disordered system:1||dilute magnetic semiconductors:1||CMR manganites:1||PHONONS:1||LATTICEDYNAMICS:1||OXIDES:1||4fphotoemission:1||permanent magnet:1||pseudogap:1||TRANSPORTPROPERTIES:1||ANTIFERROMAGNET:1||(BI,PB)SRCOO SYSTEM:1||semicore correlation:1||POLARIZATION:1||CRYSTAL:1||spinel:1||Xray magnetic circular dichroism (XMCD):1||magnetocapacitance:1||ANATASE:1||TEMPERATURES:1||Pseudogap:1||INTERFACE:1||SUBSTRATE:1||YNI2B2C:1||SAMARIUM SULFIDE:1||strong swave superconductor:1||DOPED MANGANITE:1||SYMMETRY:1||CENISN:1||resonance mode:1||DISORDERED SYSTEM:1||LITHIUM INTERCALATION:1||CUO2 PLANE:1||SURFACE:1||Delafossite:1||ELECTRICALPROPERTIES:1||NIMNSB:1||PTMNSB:1||ROOMTEMPERATURE FERROMAGNETISM:1||RUBIDIUM MANGANESE HEXACYANOFERRATE:1||COLOSSALMAGNETORESISTANCE:1||FINITE TEMPERATURES:1||LAMNO3:1||FE:1||transitionmetal oxides:1||giant magnetoresistance:1||phonon:1||COPPER OXIDES:1||valence states:1||thermoelectric:1||semiconductor:1||CATION DISTRIBUTION:1||FeCr2S4:1||photoemission spectroscopy (PES):1||METALLIC FERROMAGNETISM:1||GRAPHITE:1||SUSCEPTIBILITY:1||UBE13:1||RCrSb3:1||band JahnTeller:1||Ce3S4:1||TiO2:1||PrBa2Cu3O7delta:1||UNTWINNED PRBA2CU3O7:1||AGNIO2:1||HALFMETALLIC FERROMAGNETS:1||CI:1||Energy gap:1||Photoemission:1||Future applications:1||Photoemission measurements:1||Graphene:1||BANDSTRUCTURE:1||TC:1||superconductivity:1||magnetic semiconductors:1||CMRmanganites:1||thin films:1||spin dynamics:1||highTc superconductors:1||ITINERANTELECTRON FERROMAGNETISM:1||SINGLECRYSTALS:1||CeTe2:1||amorphous magnetic materials:1||EPITAXIAL GRAPHENE:1||LAYERED PNICTIDEOXIDES:1||BOROCARBIDE SUPERCONDUCTORS:1||AUGMENTEDWAVE METHOD:1||METALLIC MAGNET UNISN:1||ORIGIN:1||spectrum rearrangement:1||MEANFIELD THEORY:1||MOLECULEBASED MAGNETS:1||METASTABLE STATE:1||INSULATOR:1||magnetic orderin:1||FCC IRON:1||CeRu2:1||TL2MN2O7:1||isotope effect:1||Perovskitemanganites:1||RECURSION METHOD:1||PERPENDICULAR MAGNETICANISOTROPY:1||quasiparticle spectral density:1||GW:1||MANGANESE FERRITE:1||RESONANCE:1||SeCuO3:1||Optical conductivity:1||MASSLESS DIRAC FERMIONS:1||SCHOTTKYBARRIER:1||electronic structure:15||ELECTRONICSTRUCTURE:11||TRANSITIONMETAL COMPOUNDS:10||METALS:10||photoemission:8||SPECTRA:8||MAGNETORESISTANCE:7||FERROMAGNETISM:7||TRANSPORT:7||TRANSITION:6||FILMS:6||THINFILMS:5||TOTALENERGY CALCULATIONS:5||MAGNETICPROPERTIES:5||SUPERCONDUCTIVITY:5||PR:5||LATTICE:4||STATES:4||SPECTROSCOPY:4||FIELD:4||CRYSTALSTRUCTURE:4||PHOTOEMISSION:4||TEMPERATURE:4||TRANSITIONTEMPERATURE:4||XRAYABSORPTION:4||STATE:4||CU:4||BASISSET:4||XAS:4||CRYSTALS:3||EXCITATIONS:3||MOTTHUBBARD SYSTEMS:3||HIGHENERGY SPIN:3||halfmetal:3||INSULATORS:3||LA2CUO4:3||MODEL:3||FLUCTUATIONS:3||CE:3||double exchange:3||TRANSITIONMETALS:3||RESISTIVITY:3||BORON:3||LA1XCAXMNO3:3||IRON:3||PES:3||ANTIMONIDES:2||MgB2:2||ZR METALLIC GLASSES:2||superconductor:2||CRITICALCURRENT DENSITY:2||CIRCULARDICHROISM:2||SEMICONDUCTORS:2||LOCALIZATION:2||INTRABAND OPTICAL CONDUCTIVITY:2||COLOSSAL MAGNETORESISTANCE:2||OXIDATION:2||EXISTENCE:2||COPPER:2||diboride:2||MAGNESIUMDIBORIDE:2||GAP:2||CE COMPOUNDS:2||CORE POLARIZATION:2||magnetoresistance:2||photoemission spectroscopy:2||electronphonon interaction:2||GETTER:2||PD:2||MAGNETISM:2||FECR2S4:2||SUPERCONDUCTING MGB2:2||WIRES:2||ABSORPTION:2||ENERGY:2||LA1XSRXMNO3:2||CONSTANTS:2||polaron:2||charge ordering:2||SCATTERING:2||XRAY PHOTOEMISSION:2||CeNiSn:2||phase diagram:2||PHOTOELECTRON:2||QUADRUPOLAR:2||perovskitemanganites:2||CO:2||SYSTEMS:2||DOPED ZNO:2||LOWFREQUENCY SOUND:2||LA:2||ELECTRONELECTRON SCATTERING:2||AU:2||DENSITYWAVE INSTABILITY:2||FERMISURFACE:2||hybridization:2||VALENCEBAND SATELLITE:2||SULFUR SPINEL:2||Heusler:2||APPROXIMATION:2||superexchange:2||colossal magnetoresistance:2||ALLOYS:2||DEPENDENCE:2||AG:2||electronic structures:2||AUGERSPECTRA:2||CR:2||PARAMETERS:2||DIFFRACTION:2||SEMICONDUCTORMETAL TRANSITION:1||INTERMEDIATEVALENCE:1||SMB6:1||SRRUO3:1||antiperovskite structure with antipolar nature:1||lowenergy twodimensional phonons:1||anatase TiO2:1||La3S4:1||metalinsulator transitions:1||MNO:1||ELECTRONICSTRUCTURES:1||MAGNETIC CIRCULARDICHROISM:1||Density functional theory:1||CeCo2:1||TOPOLARON CROSSOVER:1||EXCHANGE:1||cuprates:1||high Tc cuprates:1||magnetically ordered materials:1||ZNSE:1||Sr2xKxFeMoO6:1||CDW:1||TeCuO3:1||STRUCTURALPROPERTIES:1||MN:1||screening length:1||amorphous Fe:1||WAVE BASISSET:1||SILICONCARBIDE:1||HIGHPRESSURE:1||electronphonon coupling:1||quenched superconductivity:1||CMR perovskite manganites:1||OXIDE:1||polarons:1||synchrotron radiation:1||FULLERIDES:1||RESONANTPHOTOEMISSION:1||Silicon carbide:1||DFT calculation:1||Hybridized bands:1||GIANT MAGNETORESISTANCE:1||PEROVSKITES:1||Raman spectra:1||EXCHANGE ENHANCEMENT:1||SILICON:1||SR2FEMOO6:1||orbital ordering:1||delafossite:1||TITANIUMDIOXIDE:1||electronic structure of disordered solids:1||YFE2:1||Magnetic polaron:1||NA2TI2SB2O:1||STRONGCOUPLED SUPERCONDUCTORS:1||HEAVYFERMION SYSTEMS:1||firstprinciples calculations:1||MECHANISM:1||UNiSn:1||PHOTONIC BANDGAP:1||SINGLE IMPURITY:1||PHONONSPECTRUM:1||FERMISURFACE TOPOLOGY:1||SUPPRESSION:1||RESONANT PHOTOEMISSION:1||METALDOPED PICENE:1||PHOTOIONIZATION CROSSSECTIONS:1||PHOTOINDUCED FERRIMAGNETIC SYSTEMS:1||LINKAGE ISOMERISM:1||CHARGETRANSFER:1||Bilayer Graphene:1||MAGNETICFIELD:1||SPINWAVES:1||rareearth manganese oxides:1||magnonphonon interaction:1||NACO2O4:1||ENERGYBANDS:1||SELFENERGY:1||GAS:1||Fe0.5Cu0.5Cr2S4:1||scanning photoelectron microscopy (SPEM):1||MAGNETIC PROPERTIES:1||Stoner model:1||AMORPHOUS TRANSITIONMETALS:1||SPINGLASS STATES:1||NI:1||LA3NI2B2N3:1||SOLIDS:1||CEO2:1||BAND THEORY:1||dilute magnetic semiconductor:1||pyrochlore:1||Y1XPRXBA2CU3O7DELTA:1||and electronphonon interactions:1||VIBRATIONS:1||RAY PHOTOEMISSION:1||ALKALI CATION:1||Europium:1||colossal magnetoresistance:1||structural stability:1||ENERGYGAP:1||small polaron:1||DOUBLE EXCHANGE:1||Coulomb correlation:1||magnon:1||phonons:1||ELECTRON FERROMAGNETISM:1||CURIETEMPERATURE:1||ARPES:1||PLANEWAVE METHOD:1||Xray absorption spectroscopy (XAS):1||ROOMTEMPERATURE:1||MONOCHALCOGENIDES:1||HEAT:1||UPDSN:1||MOMENTS:1||XRAY ABSORPTION:1||SEMICONDUCTOR:1||Fermi surface nesting:1||optical phonon:1||disordered system:1||dilute magnetic semiconductors:1||CMR manganites:1||PHONONS:1||LATTICEDYNAMICS:1||OXIDES:1||4fphotoemission:1||permanent magnet:1||pseudogap:1||TRANSPORTPROPERTIES:1||ANTIFERROMAGNET:1||(BI,PB)SRCOO SYSTEM:1||semicore correlation:1||POLARIZATION:1||CRYSTAL:1||spinel:1||Xray magnetic circular dichroism (XMCD):1||magnetocapacitance:1||ANATASE:1||TEMPERATURES:1||Pseudogap:1||INTERFACE:1||SUBSTRATE:1||YNI2B2C:1||SAMARIUM SULFIDE:1||strong swave superconductor:1||DOPED MANGANITE:1||SYMMETRY:1||CENISN:1||resonance mode:1||DISORDERED SYSTEM:1||LITHIUM INTERCALATION:1||CUO2 PLANE:1||SURFACE:1||Delafossite:1||ELECTRICALPROPERTIES:1||NIMNSB:1||PTMNSB:1||ROOMTEMPERATURE FERROMAGNETISM:1||RUBIDIUM MANGANESE HEXACYANOFERRATE:1||COLOSSALMAGNETORESISTANCE:1||FINITE TEMPERATURES:1||LAMNO3:1||FE:1||transitionmetal oxides:1||giant magnetoresistance:1||phonon:1||COPPER OXIDES:1||valence states:1||thermoelectric:1||semiconductor:1||CATION DISTRIBUTION:1||FeCr2S4:1||photoemission spectroscopy (PES):1||METALLIC FERROMAGNETISM:1||GRAPHITE:1||SUSCEPTIBILITY:1||UBE13:1||RCrSb3:1||band JahnTeller:1||Ce3S4:1||TiO2:1||PrBa2Cu3O7delta:1||UNTWINNED PRBA2CU3O7:1||AGNIO2:1||HALFMETALLIC FERROMAGNETS:1||CI:1||Energy gap:1||Photoemission:1||Future applications:1||Photoemission measurements:1||Graphene:1||BANDSTRUCTURE:1||TC:1||superconductivity:1||magnetic semiconductors:1||CMRmanganites:1||thin films:1||spin dynamics:1||highTc superconductors:1||ITINERANTELECTRON FERROMAGNETISM:1||SINGLECRYSTALS:1||CeTe2:1||amorphous magnetic materials:1||EPITAXIAL GRAPHENE:1||LAYERED PNICTIDEOXIDES:1||BOROCARBIDE SUPERCONDUCTORS:1||AUGMENTEDWAVE METHOD:1||METALLIC MAGNET UNISN:1||ORIGIN:1||spectrum rearrangement:1||MEANFIELD THEORY:1||MOLECULEBASED MAGNETS:1||METASTABLE STATE:1||INSULATOR:1||magnetic orderin:1||FCC IRON:1||CeRu2:1||TL2MN2O7:1||isotope effect:1||Perovskitemanganites:1||RECURSION METHOD:1||PERPENDICULAR MAGNETICANISOTROPY:1||quasiparticle spectral density:1||GW:1||MANGANESE FERRITE:1||RESONANCE:1||SeCuO3:1||Optical conductivity:1||MASSLESS DIRAC FERMIONS:1||SCHOTTKYBARRIER:1||electronic structure:15||ELECTRONICSTRUCTURE:11||TRANSITIONMETAL COMPOUNDS:10||METALS:10||photoemission:8||SPECTRA:8||MAGNETORESISTANCE:7||FERROMAGNETISM:7||TRANSPORT:7||TRANSITION:6||FILMS:6||THINFILMS:5||TOTALENERGY CALCULATIONS:5||MAGNETICPROPERTIES:5||SUPERCONDUCTIVITY:5||PR:5||LATTICE:4||STATES:4||SPECTROSCOPY:4||FIELD:4||CRYSTALSTRUCTURE:4||PHOTOEMISSION:4||TEMPERATURE:4||TRANSITIONTEMPERATURE:4||XRAYABSORPTION:4||STATE:4||CU:4||BASISSET:4||XAS:4||CRYSTALS:3||EXCITATIONS:3||MOTTHUBBARD SYSTEMS:3||HIGHENERGY SPIN:3||halfmetal:3||INSULATORS:3||LA2CUO4:3||MODEL:3||FLUCTUATIONS:3||CE:3||double exchange:3||TRANSITIONMETALS:3||RESISTIVITY:3||BORON:3||LA1XCAXMNO3:3||IRON:3||PES:3||ANTIMONIDES:2||MgB2:2||ZR METALLIC GLASSES:2||superconductor:2||CRITICALCURRENT DENSITY:2||CIRCULARDICHROISM:2||SEMICONDUCTORS:2||LOCALIZATION:2||INTRABAND OPTICAL CONDUCTIVITY:2||COLOSSAL MAGNETORESISTANCE:2||OXIDATION:2||EXISTENCE:2||COPPER:2||diboride:2||MAGNESIUMDIBORIDE:2||GAP:2||CE COMPOUNDS:2||CORE POLARIZATION:2||magnetoresistance:2||photoemission spectroscopy:2||electronphonon interaction:2||GETTER:2||PD:2||MAGNETISM:2||FECR2S4:2||SUPERCONDUCTING MGB2:2||WIRES:2||ABSORPTION:2||ENERGY:2||LA1XSRXMNO3:2||CONSTANTS:2||polaron:2||charge ordering:2||SCATTERING:2||XRAY PHOTOEMISSION:2||CeNiSn:2||phase diagram:2||PHOTOELECTRON:2||QUADRUPOLAR:2||perovskitemanganites:2||CO:2||SYSTEMS:2||DOPED ZNO:2||LOWFREQUENCY SOUND:2||LA:2||ELECTRONELECTRON SCATTERING:2||AU:2||DENSITYWAVE INSTABILITY:2||FERMISURFACE:2||hybridization:2||VALENCEBAND SATELLITE:2||SULFUR SPINEL:2||Heusler:2||APPROXIMATION:2||superexchange:2||colossal magnetoresistance:2||ALLOYS:2||DEPENDENCE:2||AG:2||electronic structures:2||AUGERSPECTRA:2||CR:2||PARAMETERS:2||DIFFRACTION:2||SEMICONDUCTORMETAL TRANSITION:1||INTERMEDIATEVALENCE:1||SMB6:1||SRRUO3:1||antiperovskite structure with antipolar nature:1||lowenergy twodimensional phonons:1||anatase TiO2:1||La3S4:1||metalinsulator transitions:1||MNO:1||ELECTRONICSTRUCTURES:1||MAGNETIC CIRCULARDICHROISM:1||Density functional theory:1||CeCo2:1||TOPOLARON CROSSOVER:1||EXCHANGE:1||cuprates:1||high Tc cuprates:1||magnetically ordered materials:1||ZNSE:1||Sr2xKxFeMoO6:1||CDW:1||TeCuO3:1||STRUCTURALPROPERTIES:1||MN:1||screening length:1||amorphous Fe:1||WAVE BASISSET:1||SILICONCARBIDE:1||HIGHPRESSURE:1||electronphonon coupling:1||quenched superconductivity:1||CMR perovskite manganites:1||OXIDE:1||polarons:1||synchrotron radiation:1||FULLERIDES:1||RESONANTPHOTOEMISSION:1||Silicon carbide:1||DFT calculation:1||Hybridized bands:1||GIANT MAGNETORESISTANCE:1||PEROVSKITES:1||Raman spectra:1||EXCHANGE ENHANCEMENT:1||SILICON:1||SR2FEMOO6:1||orbital ordering:1||delafossite:1||TITANIUMDIOXIDE:1||electronic structure of disordered solids:1||YFE2:1||Magnetic polaron:1||NA2TI2SB2O:1||STRONGCOUPLED SUPERCONDUCTORS:1||HEAVYFERMION SYSTEMS:1||firstprinciples calculations:1||MECHANISM:1||UNiSn:1||PHOTONIC BANDGAP:1||SINGLE IMPURITY:1||PHONONSPECTRUM:1||FERMISURFACE TOPOLOGY:1||SUPPRESSION:1||RESONANT PHOTOEMISSION:1||METALDOPED PICENE:1||PHOTOIONIZATION CROSSSECTIONS:1||PHOTOINDUCED FERRIMAGNETIC SYSTEMS:1||LINKAGE ISOMERISM:1||CHARGETRANSFER:1||Bilayer Graphene:1||MAGNETICFIELD:1||SPINWAVES:1||rareearth manganese oxides:1||magnonphonon interaction:1||NACO2O4:1||ENERGYBANDS:1||SELFENERGY:1||GAS:1||Fe0.5Cu0.5Cr2S4:1||scanning photoelectron microscopy (SPEM):1||MAGNETIC PROPERTIES:1||Stoner model:1||AMORPHOUS TRANSITIONMETALS:1||SPINGLASS STATES:1||NI:1||LA3NI2B2N3:1||SOLIDS:1||CEO2:1||BAND THEORY:1||dilute magnetic semiconductor:1||pyrochlore:1||Y1XPRXBA2CU3O7DELTA:1||and electronphonon interactions:1||VIBRATIONS:1||RAY PHOTOEMISSION:1||ALKALI CATION:1||Europium:1||colossal magnetoresistance:1||structural stability:1||ENERGYGAP:1||small polaron:1||DOUBLE EXCHANGE:1||Coulomb correlation:1||magnon:1||phonons:1||ELECTRON FERROMAGNETISM:1||CURIETEMPERATURE:1||ARPES:1||PLANEWAVE METHOD:1||Xray absorption spectroscopy (XAS):1||ROOMTEMPERATURE:1||MONOCHALCOGENIDES:1||HEAT:1||UPDSN:1||MOMENTS:1||XRAY ABSORPTION:1||SEMICONDUCTOR:1||Fermi surface nesting:1||optical phonon:1||disordered system:1||dilute magnetic semiconductors:1||CMR manganites:1||PHONONS:1||LATTICEDYNAMICS:1||OXIDES:1||4fphotoemission:1||permanent magnet:1||pseudogap:1||TRANSPORTPROPERTIES:1||ANTIFERROMAGNET:1||(BI,PB)SRCOO SYSTEM:1||semicore correlation:1||POLARIZATION:1||CRYSTAL:1||spinel:1||Xray magnetic circular dichroism (XMCD):1||magnetocapacitance:1||ANATASE:1||TEMPERATURES:1||Pseudogap:1||INTERFACE:1||SUBSTRATE:1||YNI2B2C:1||SAMARIUM SULFIDE:1||strong swave superconductor:1||DOPED MANGANITE:1||SYMMETRY:1||CENISN:1||resonance mode:1||DISORDERED SYSTEM:1||LITHIUM INTERCALATION:1||CUO2 PLANE:1||SURFACE:1||Delafossite:1||ELECTRICALPROPERTIES:1||NIMNSB:1||PTMNSB:1||ROOMTEMPERATURE FERROMAGNETISM:1||RUBIDIUM MANGANESE HEXACYANOFERRATE:1||COLOSSALMAGNETORESISTANCE:1||FINITE TEMPERATURES:1||LAMNO3:1||FE:1||transitionmetal oxides:1||giant magnetoresistance:1||phonon:1||COPPER OXIDES:1||valence states:1||thermoelectric:1||semiconductor:1||CATION DISTRIBUTION:1||FeCr2S4:1||photoemission spectroscopy (PES):1||METALLIC FERROMAGNETISM:1||GRAPHITE:1||SUSCEPTIBILITY:1||UBE13:1||RCrSb3:1||band JahnTeller:1||Ce3S4:1||TiO2:1||PrBa2Cu3O7delta:1||UNTWINNED PRBA2CU3O7:1||AGNIO2:1||HALFMETALLIC FERROMAGNETS:1||CI:1||Energy gap:1||Photoemission:1||Future applications:1||Photoemission measurements:1||Graphene:1||BANDSTRUCTURE:1||TC:1||superconductivity:1||magnetic semiconductors:1||CMRmanganites:1||thin films:1||spin dynamics:1||highTc superconductors:1||ITINERANTELECTRON FERROMAGNETISM:1||SINGLECRYSTALS:1||CeTe2:1||amorphous magnetic materials:1||EPITAXIAL GRAPHENE:1||LAYERED PNICTIDEOXIDES:1||BOROCARBIDE SUPERCONDUCTORS:1||AUGMENTEDWAVE METHOD:1||METALLIC MAGNET UNISN:1||ORIGIN:1||spectrum rearrangement:1||MEANFIELD THEORY:1||MOLECULEBASED MAGNETS:1||METASTABLE STATE:1||INSULATOR:1||magnetic orderin:1||FCC IRON:1||CeRu2:1||TL2MN2O7:1||isotope effect:1||Perovskitemanganites:1||RECURSION METHOD:1||PERPENDICULAR MAGNETICANISOTROPY:1||quasiparticle spectral density:1||GW:1||MANGANESE FERRITE:1||RESONANCE:1||SeCuO3:1||Optical conductivity:1||MASSLESS DIRAC FERMIONS:1||SCHOTTKYBARRIER:1||electronic structure:15||ELECTRONICSTRUCTURE:11||TRANSITIONMETAL COMPOUNDS:10||METALS:10||photoemission:8||SPECTRA:8||MAGNETORESISTANCE:7||FERROMAGNETISM:7||TRANSPORT:7||TRANSITION:6||FILMS:6||THINFILMS:5||TOTALENERGY CALCULATIONS:5||MAGNETICPROPERTIES:5||SUPERCONDUCTIVITY:5||PR:5||LATTICE:4||STATES:4||SPECTROSCOPY:4||FIELD:4||CRYSTALSTRUCTURE:4||PHOTOEMISSION:4||TEMPERATURE:4||TRANSITIONTEMPERATURE:4||XRAYABSORPTION:4||STATE:4||CU:4||BASISSET:4||XAS:4||CRYSTALS:3||EXCITATIONS:3||MOTTHUBBARD SYSTEMS:3||HIGHENERGY SPIN:3||halfmetal:3||INSULATORS:3||LA2CUO4:3||MODEL:3||FLUCTUATIONS:3||CE:3||double exchange:3||TRANSITIONMETALS:3||RESISTIVITY:3||BORON:3||LA1XCAXMNO3:3||IRON:3||PES:3||ANTIMONIDES:2||MgB2:2||ZR METALLIC GLASSES:2||superconductor:2||CRITICALCURRENT DENSITY:2||CIRCULARDICHROISM:2||SEMICONDUCTORS:2||LOCALIZATION:2||INTRABAND OPTICAL CONDUCTIVITY:2||COLOSSAL MAGNETORESISTANCE:2||OXIDATION:2||EXISTENCE:2||COPPER:2||diboride:2||MAGNESIUMDIBORIDE:2||GAP:2||CE COMPOUNDS:2||CORE POLARIZATION:2||magnetoresistance:2||photoemission spectroscopy:2||electronphonon interaction:2||GETTER:2||PD:2||MAGNETISM:2||FECR2S4:2||SUPERCONDUCTING MGB2:2||WIRES:2||ABSORPTION:2||ENERGY:2||LA1XSRXMNO3:2||CONSTANTS:2||polaron:2||charge ordering:2||SCATTERING:2||XRAY PHOTOEMISSION:2||CeNiSn:2||phase diagram:2||PHOTOELECTRON:2||QUADRUPOLAR:2||perovskitemanganites:2||CO:2||SYSTEMS:2||DOPED ZNO:2||LOWFREQUENCY SOUND:2||LA:2||ELECTRONELECTRON SCATTERING:2||AU:2||DENSITYWAVE INSTABILITY:2||FERMISURFACE:2||hybridization:2||VALENCEBAND SATELLITE:2||SULFUR SPINEL:2||Heusler:2||APPROXIMATION:2||superexchange:2||colossal magnetoresistance:2||ALLOYS:2||DEPENDENCE:2||AG:2||electronic structures:2||AUGERSPECTRA:2||CR:2||PARAMETERS:2||DIFFRACTION:2||SEMICONDUCTORMETAL TRANSITION:1||INTERMEDIATEVALENCE:1||SMB6:1||SRRUO3:1||antiperovskite structure with antipolar nature:1||lowenergy twodimensional phonons:1||anatase TiO2:1||La3S4:1||metalinsulator transitions:1||MNO:1||ELECTRONICSTRUCTURES:1||MAGNETIC CIRCULARDICHROISM:1||Density functional theory:1||CeCo2:1||TOPOLARON CROSSOVER:1||EXCHANGE:1||cuprates:1||high Tc cuprates:1||magnetically ordered materials:1||ZNSE:1||Sr2xKxFeMoO6:1||CDW:1||TeCuO3:1||STRUCTURALPROPERTIES:1||MN:1||screening length:1||amorphous Fe:1||WAVE BASISSET:1||SILICONCARBIDE:1||HIGHPRESSURE:1||electronphonon coupling:1||quenched superconductivity:1||CMR perovskite manganites:1||OXIDE:1||polarons:1||synchrotron radiation:1||FULLERIDES:1||RESONANTPHOTOEMISSION:1||Silicon carbide:1||DFT calculation:1||Hybridized bands:1||GIANT MAGNETORESISTANCE:1||PEROVSKITES:1||Raman spectra:1||EXCHANGE ENHANCEMENT:1||SILICON:1||SR2FEMOO6:1||orbital ordering:1||delafossite:1||TITANIUMDIOXIDE:1||electronic structure of disordered solids:1||YFE2:1||Magnetic polaron:1||NA2TI2SB2O:1||STRONGCOUPLED SUPERCONDUCTORS:1||HEAVYFERMION SYSTEMS:1||firstprinciples calculations:1||MECHANISM:1||UNiSn:1||PHOTONIC BANDGAP:1||SINGLE IMPURITY:1||PHONONSPECTRUM:1||FERMISURFACE TOPOLOGY:1||SUPPRESSION:1||RESONANT PHOTOEMISSION:1||METALDOPED PICENE:1||PHOTOIONIZATION CROSSSECTIONS:1||PHOTOINDUCED FERRIMAGNETIC SYSTEMS:1||LINKAGE ISOMERISM:1||CHARGETRANSFER:1||Bilayer Graphene:1||MAGNETICFIELD:1||SPINWAVES:1||rareearth manganese oxides:1||magnonphonon interaction:1||NACO2O4:1||ENERGYBANDS:1||SELFENERGY:1||GAS:1||Fe0.5Cu0.5Cr2S4:1||scanning photoelectron microscopy (SPEM):1||MAGNETIC PROPERTIES:1||Stoner model:1||AMORPHOUS TRANSITIONMETALS:1||SPINGLASS STATES:1||NI:1||LA3NI2B2N3:1||SOLIDS:1||CEO2:1||BAND THEORY:1||dilute magnetic semiconductor:1||pyrochlore:1||Y1XPRXBA2CU3O7DELTA:1||and electronphonon interactions:1||VIBRATIONS:1||RAY PHOTOEMISSION:1||ALKALI CATION:1||Europium:1||colossal magnetoresistance:1||structural stability:1||ENERGYGAP:1||small polaron:1||DOUBLE EXCHANGE:1||Coulomb correlation:1||magnon:1||phonons:1||ELECTRON FERROMAGNETISM:1||CURIETEMPERATURE:1||ARPES:1||PLANEWAVE METHOD:1||Xray absorption spectroscopy (XAS):1||ROOMTEMPERATURE:1||MONOCHALCOGENIDES:1||HEAT:1||UPDSN:1||MOMENTS:1||XRAY ABSORPTION:1||SEMICONDUCTOR:1||Fermi surface nesting:1||optical phonon:1||disordered system:1||dilute magnetic semiconductors:1||CMR manganites:1||PHONONS:1||LATTICEDYNAMICS:1||OXIDES:1||4fphotoemission:1||permanent magnet:1||pseudogap:1||TRANSPORTPROPERTIES:1||ANTIFERROMAGNET:1||(BI,PB)SRCOO SYSTEM:1||semicore correlation:1||POLARIZATION:1||CRYSTAL:1||spinel:1||Xray magnetic circular dichroism (XMCD):1||magnetocapacitance:1||ANATASE:1||TEMPERATURES:1||Pseudogap:1||INTERFACE:1||SUBSTRATE:1||YNI2B2C:1||SAMARIUM SULFIDE:1||strong swave superconductor:1||DOPED MANGANITE:1||SYMMETRY:1||CENISN:1||resonance mode:1||DISORDERED SYSTEM:1||LITHIUM INTERCALATION:1||CUO2 PLANE:1||SURFACE:1||Delafossite:1||ELECTRICALPROPERTIES:1||NIMNSB:1||PTMNSB:1||ROOMTEMPERATURE FERROMAGNETISM:1||RUBIDIUM MANGANESE HEXACYANOFERRATE:1||COLOSSALMAGNETORESISTANCE:1||FINITE TEMPERATURES:1||LAMNO3:1||FE:1||transitionmetal oxides:1||giant magnetoresistance:1||phonon:1||COPPER OXIDES:1||valence states:1||thermoelectric:1||semiconductor:1||CATION DISTRIBUTION:1||FeCr2S4:1||photoemission spectroscopy (PES):1||METALLIC FERROMAGNETISM:1||GRAPHITE:1||SUSCEPTIBILITY:1||UBE13:1||RCrSb3:1||band JahnTeller:1||Ce3S4:1||TiO2:1||PrBa2Cu3O7delta:1||UNTWINNED PRBA2CU3O7:1||AGNIO2:1||HALFMETALLIC FERROMAGNETS:1||CI:1||Energy gap:1||Photoemission:1||Future applications:1||Photoemission measurements:1||Graphene:1||BANDSTRUCTURE:1||TC:1||superconductivity:1||magnetic semiconductors:1||CMRmanganites:1||thin films:1||spin dynamics:1||highTc superconductors:1||ITINERANTELECTRON FERROMAGNETISM:1||SINGLECRYSTALS:1||CeTe2:1||amorphous magnetic materials:1||EPITAXIAL GRAPHENE:1||LAYERED PNICTIDEOXIDES:1||BOROCARBIDE SUPERCONDUCTORS:1||AUGMENTEDWAVE METHOD:1||METALLIC MAGNET UNISN:1||ORIGIN:1||spectrum rearrangement:1||MEANFIELD THEORY:1||MOLECULEBASED MAGNETS:1||METASTABLE STATE:1||INSULATOR:1||magnetic orderin:1||FCC IRON:1||CeRu2:1||TL2MN2O7:1||isotope effect:1||Perovskitemanganites:1||RECURSION METHOD:1||PERPENDICULAR MAGNETICANISOTROPY:1||quasiparticle spectral density:1||GW:1||MANGANESE FERRITE:1||RESONANCE:1||SeCuO3:1||Optical conductivity:1||MASSLESS DIRAC FERMIONS:1||SCHOTTKYBARRIER:1||electronic structure:15||ELECTRONICSTRUCTURE:11||TRANSITIONMETAL COMPOUNDS:10||METALS:10||photoemission:8||SPECTRA:8||MAGNETORESISTANCE:7||FERROMAGNETISM:7||TRANSPORT:7||TRANSITION:6||FILMS:6||THINFILMS:5||TOTALENERGY CALCULATIONS:5||MAGNETICPROPERTIES:5||SUPERCONDUCTIVITY:5||PR:5||LATTICE:4||STATES:4||SPECTROSCOPY:4||FIELD:4||CRYSTALSTRUCTURE:4||PHOTOEMISSION:4||TEMPERATURE:4||TRANSITIONTEMPERATURE:4||XRAYABSORPTION:4||STATE:4||CU:4||BASISSET:4||XAS:4||CRYSTALS:3||EXCITATIONS:3||MOTTHUBBARD SYSTEMS:3||HIGHENERGY SPIN:3||halfmetal:3||INSULATORS:3||LA2CUO4:3||MODEL:3||FLUCTUATIONS:3||CE:3||double exchange:3||TRANSITIONMETALS:3||RESISTIVITY:3||BORON:3||LA1XCAXMNO3:3||IRON:3||PES:3||ANTIMONIDES:2||MgB2:2||ZR METALLIC GLASSES:2||superconductor:2||CRITICALCURRENT DENSITY:2||CIRCULARDICHROISM:2||SEMICONDUCTORS:2||LOCALIZATION:2||INTRABAND OPTICAL CONDUCTIVITY:2||COLOSSAL MAGNETORESISTANCE:2||OXIDATION:2||EXISTENCE:2||COPPER:2||diboride:2||MAGNESIUMDIBORIDE:2||GAP:2||CE COMPOUNDS:2||CORE POLARIZATION:2||magnetoresistance:2||photoemission spectroscopy:2||electronphonon interaction:2||GETTER:2||PD:2||MAGNETISM:2||FECR2S4:2||SUPERCONDUCTING MGB2:2||WIRES:2||ABSORPTION:2||ENERGY:2||LA1XSRXMNO3:2||CONSTANTS:2||polaron:2||charge ordering:2||SCATTERING:2||XRAY PHOTOEMISSION:2||CeNiSn:2||phase diagram:2||PHOTOELECTRON:2||QUADRUPOLAR:2||perovskitemanganites:2||CO:2||SYSTEMS:2||DOPED ZNO:2||LOWFREQUENCY SOUND:2||LA:2||ELECTRONELECTRON SCATTERING:2||AU:2||DENSITYWAVE INSTABILITY:2||FERMISURFACE:2||hybridization:2||VALENCEBAND SATELLITE:2||SULFUR SPINEL:2||Heusler:2||APPROXIMATION:2||superexchange:2||colossal magnetoresistance:2||ALLOYS:2||DEPENDENCE:2||AG:2||electronic structures:2||AUGERSPECTRA:2||CR:2||PARAMETERS:2||DIFFRACTION:2||SEMICONDUCTORMETAL TRANSITION:1||INTERMEDIATEVALENCE:1||SMB6:1||SRRUO3:1||antiperovskite structure with antipolar nature:1||lowenergy twodimensional phonons:1||anatase TiO2:1||La3S4:1||metalinsulator transitions:1||MNO:1||ELECTRONICSTRUCTURES:1||MAGNETIC CIRCULARDICHROISM:1||Density functional theory:1||CeCo2:1||TOPOLARON CROSSOVER:1||EXCHANGE:1||cuprates:1||high Tc cuprates:1||magnetically ordered materials:1||ZNSE:1||Sr2xKxFeMoO6:1||CDW:1||TeCuO3:1||STRUCTURALPROPERTIES:1||MN:1||screening length:1||amorphous Fe:1||WAVE BASISSET:1||SILICONCARBIDE:1||HIGHPRESSURE:1||electronphonon coupling:1||quenched superconductivity:1||CMR perovskite manganites:1||OXIDE:1||polarons:1||synchrotron radiation:1||FULLERIDES:1||RESONANTPHOTOEMISSION:1||Silicon carbide:1||DFT calculation:1||Hybridized bands:1||GIANT MAGNETORESISTANCE:1||PEROVSKITES:1||Raman spectra:1||EXCHANGE ENHANCEMENT:1||SILICON:1||SR2FEMOO6:1||orbital ordering:1||delafossite:1||TITANIUMDIOXIDE:1||electronic structure of disordered solids:1||YFE2:1||Magnetic polaron:1||NA2TI2SB2O:1||STRONGCOUPLED SUPERCONDUCTORS:1||HEAVYFERMION SYSTEMS:1||firstprinciples calculations:1||MECHANISM:1||UNiSn:1||PHOTONIC BANDGAP:1||SINGLE IMPURITY:1||PHONONSPECTRUM:1||FERMISURFACE TOPOLOGY:1||SUPPRESSION:1||RESONANT PHOTOEMISSION:1||METALDOPED PICENE:1||PHOTOIONIZATION CROSSSECTIONS:1||PHOTOINDUCED FERRIMAGNETIC SYSTEMS:1||LINKAGE ISOMERISM:1||CHARGETRANSFER:1||Bilayer Graphene:1||MAGNETICFIELD:1||SPINWAVES:1||rareearth manganese oxides:1||magnonphonon interaction:1||NACO2O4:1||ENERGYBANDS:1||SELFENERGY:1||GAS:1||Fe0.5Cu0.5Cr2S4:1||scanning photoelectron microscopy (SPEM):1||MAGNETIC PROPERTIES:1||Stoner model:1||AMORPHOUS TRANSITIONMETALS:1||SPINGLASS STATES:1||NI:1||LA3NI2B2N3:1||SOLIDS:1||CEO2:1||BAND THEORY:1||dilute magnetic semiconductor:1||pyrochlore:1||Y1XPRXBA2CU3O7DELTA:1||and electronphonon interactions:1||VIBRATIONS:1||RAY PHOTOEMISSION:1||ALKALI CATION:1||Europium:1||colossal magnetoresistance:1||structural stability:1||ENERGYGAP:1||small polaron:1||DOUBLE EXCHANGE:1||Coulomb correlation:1||magnon:1||phonons:1||ELECTRON FERROMAGNETISM:1||CURIETEMPERATURE:1||ARPES:1||PLANEWAVE METHOD:1||Xray absorption spectroscopy (XAS):1||ROOMTEMPERATURE:1||MONOCHALCOGENIDES:1||HEAT:1||UPDSN:1||MOMENTS:1||XRAY ABSORPTION:1||SEMICONDUCTOR:1||Fermi surface nesting:1||optical phonon:1||disordered system:1||dilute magnetic semiconductors:1||CMR manganites:1||PHONONS:1||LATTICEDYNAMICS:1||OXIDES:1||4fphotoemission:1||permanent magnet:1||pseudogap:1||TRANSPORTPROPERTIES:1||ANTIFERROMAGNET:1||(BI,PB)SRCOO SYSTEM:1||semicore correlation:1||POLARIZATION:1||CRYSTAL:1||spinel:1||Xray magnetic circular dichroism (XMCD):1||magnetocapacitance:1||ANATASE:1||TEMPERATURES:1||Pseudogap:1||INTERFACE:1||SUBSTRATE:1||YNI2B2C:1||SAMARIUM SULFIDE:1||strong swave superconductor:1||DOPED MANGANITE:1||SYMMETRY:1||CENISN:1||resonance mode:1||DISORDERED SYSTEM:1||LITHIUM INTERCALATION:1||CUO2 PLANE:1||SURFACE:1||Delafossite:1||ELECTRICALPROPERTIES:1||NIMNSB:1||PTMNSB:1||ROOMTEMPERATURE FERROMAGNETISM:1||RUBIDIUM MANGANESE HEXACYANOFERRATE:1||COLOSSALMAGNETORESISTANCE:1||FINITE TEMPERATURES:1||LAMNO3:1||FE:1||transitionmetal oxides:1||giant magnetoresistance:1||phonon:1||COPPER OXIDES:1||valence states:1||thermoelectric:1||semiconductor:1||CATION DISTRIBUTION:1||FeCr2S4:1||photoemission spectroscopy (PES):1||METALLIC FERROMAGNETISM:1||GRAPHITE:1||SUSCEPTIBILITY:1||UBE13:1||RCrSb3:1||band JahnTeller:1||Ce3S4:1||TiO2:1||PrBa2Cu3O7delta:1||UNTWINNED PRBA2CU3O7:1||AGNIO2:1||HALFMETALLIC FERROMAGNETS:1||CI:1||Energy gap:1||Photoemission:1||Future applications:1||Photoemission measurements:1||Graphene:1||BANDSTRUCTURE:1||TC:1||superconductivity:1||magnetic semiconductors:1||CMRmanganites:1||thin films:1||spin dynamics:1||highTc superconductors:1||ITINERANTELECTRON FERROMAGNETISM:1||SINGLECRYSTALS:1||CeTe2:1||amorphous magnetic materials:1||EPITAXIAL GRAPHENE:1||LAYERED PNICTIDEOXIDES:1||BOROCARBIDE SUPERCONDUCTORS:1||AUGMENTEDWAVE METHOD:1||METALLIC MAGNET UNISN:1||ORIGIN:1||spectrum rearrangement:1||MEANFIELD THEORY:1||MOLECULEBASED MAGNETS:1||METASTABLE STATE:1||INSULATOR:1||magnetic orderin:1||FCC IRON:1||CeRu2:1||TL2MN2O7:1||isotope effect:1||Perovskitemanganites:1||RECURSION METHOD:1||PERPENDICULAR MAGNETICANISOTROPY:1||quasiparticle spectral density:1||GW:1||MANGANESE FERRITE:1||RESONANCE:1||SeCuO3:1||Optical conductivity:1||MASSLESS DIRAC FERMIONS:1||SCHOTTKYBARRIER:1||electronic structure:15||ELECTRONICSTRUCTURE:11||TRANSITIONMETAL COMPOUNDS:10||METALS:10||photoemission:8||SPECTRA:8||MAGNETORESISTANCE:7||FERROMAGNETISM:7||TRANSPORT:7||TRANSITION:6||FILMS:6||THINFILMS:5||TOTALENERGY CALCULATIONS:5||MAGNETICPROPERTIES:5||SUPERCONDUCTIVITY:5||PR:5||LATTICE:4||STATES:4||SPECTROSCOPY:4||FIELD:4||CRYSTALSTRUCTURE:4||PHOTOEMISSION:4||TEMPERATURE:4||TRANSITIONTEMPERATURE:4||XRAYABSORPTION:4||STATE:4||CU:4||BASISSET:4||XAS:4||CRYSTALS:3||EXCITATIONS:3||MOTTHUBBARD SYSTEMS:3||HIGHENERGY SPIN:3||halfmetal:3||INSULATORS:3||LA2CUO4:3||MODEL:3||FLUCTUATIONS:3||CE:3||double exchange:3||TRANSITIONMETALS:3||RESISTIVITY:3||BORON:3||LA1XCAXMNO3:3||IRON:3||PES:3||ANTIMONIDES:2||MgB2:2||ZR METALLIC GLASSES:2||superconductor:2||CRITICALCURRENT DENSITY:2||CIRCULARDICHROISM:2||SEMICONDUCTORS:2||LOCALIZATION:2||INTRABAND OPTICAL CONDUCTIVITY:2||COLOSSAL MAGNETORESISTANCE:2||OXIDATION:2||EXISTENCE:2||COPPER:2||diboride:2||MAGNESIUMDIBORIDE:2||GAP:2||CE COMPOUNDS:2||CORE POLARIZATION:2||magnetoresistance:2||photoemission spectroscopy:2||electronphonon interaction:2||GETTER:2||PD:2||MAGNETISM:2||FECR2S4:2||SUPERCONDUCTING MGB2:2||WIRES:2||ABSORPTION:2||ENERGY:2||LA1XSRXMNO3:2||CONSTANTS:2||polaron:2||charge ordering:2||SCATTERING:2||XRAY PHOTOEMISSION:2||CeNiSn:2||phase diagram:2||PHOTOELECTRON:2||QUADRUPOLAR:2||perovskitemanganites:2||CO:2||SYSTEMS:2||DOPED ZNO:2||LOWFREQUENCY SOUND:2||LA:2||ELECTRONELECTRON SCATTERING:2||AU:2||DENSITYWAVE INSTABILITY:2||FERMISURFACE:2||hybridization:2||VALENCEBAND SATELLITE:2||SULFUR SPINEL:2||Heusler:2||APPROXIMATION:2||superexchange:2||colossal magnetoresistance:2||ALLOYS:2||DEPENDENCE:2||AG:2||electronic structures:2||AUGERSPECTRA:2||CR:2||PARAMETERS:2||DIFFRACTION:2||SEMICONDUCTORMETAL TRANSITION:1||INTERMEDIATEVALENCE:1||SMB6:1||SRRUO3:1||antiperovskite structure with antipolar nature:1||lowenergy twodimensional phonons:1||anatase TiO2:1||La3S4:1||metalinsulator transitions:1||MNO:1||ELECTRONICSTRUCTURES:1||MAGNETIC CIRCULARDICHROISM:1||Density functional theory:1||CeCo2:1||TOPOLARON CROSSOVER:1||EXCHANGE:1||cuprates:1||high Tc cuprates:1||magnetically ordered materials:1||ZNSE:1||Sr2xKxFeMoO6:1||CDW:1||TeCuO3:1||STRUCTURALPROPERTIES:1||MN:1||screening length:1||amorphous Fe:1||WAVE BASISSET:1||SILICONCARBIDE:1||HIGHPRESSURE:1||electronphonon coupling:1||quenched superconductivity:1||CMR perovskite manganites:1||OXIDE:1||polarons:1||synchrotron radiation:1||FULLERIDES:1||RESONANTPHOTOEMISSION:1||Silicon carbide:1||DFT calculation:1||Hybridized bands:1||GIANT MAGNETORESISTANCE:1||PEROVSKITES:1||Raman spectra:1||EXCHANGE ENHANCEMENT:1||SILICON:1||SR2FEMOO6:1||orbital ordering:1||delafossite:1||TITANIUMDIOXIDE:1||electronic structure of disordered solids:1||YFE2:1||Magnetic polaron:1||NA2TI2SB2O:1||STRONGCOUPLED SUPERCONDUCTORS:1||HEAVYFERMION SYSTEMS:1||firstprinciples calculations:1||MECHANISM:1||UNiSn:1||PHOTONIC BANDGAP:1||SINGLE IMPURITY:1||PHONONSPECTRUM:1||FERMISURFACE TOPOLOGY:1||SUPPRESSION:1||RESONANT PHOTOEMISSION:1||METALDOPED PICENE:1||PHOTOIONIZATION CROSSSECTIONS:1||PHOTOINDUCED FERRIMAGNETIC SYSTEMS:1||LINKAGE ISOMERISM:1||CHARGETRANSFER:1||Bilayer Graphene:1||MAGNETICFIELD:1||SPINWAVES:1||rareearth manganese oxides:1||magnonphonon interaction:1||NACO2O4:1||ENERGYBANDS:1||SELFENERGY:1||GAS:1||Fe0.5Cu0.5Cr2S4:1||scanning photoelectron microscopy (SPEM):1||MAGNETIC PROPERTIES:1||Stoner model:1||AMORPHOUS TRANSITIONMETALS:1||SPINGLASS STATES:1||NI:1||LA3NI2B2N3:1||SOLIDS:1||CEO2:1||BAND THEORY:1||dilute magnetic semiconductor:1||pyrochlore:1||Y1XPRXBA2CU3O7DELTA:1||and electronphonon interactions:1||VIBRATIONS:1||RAY PHOTOEMISSION:1||ALKALI CATION:1||Europium:1||colossal magnetoresistance:1||structural stability:1||ENERGYGAP:1||small polaron:1||DOUBLE EXCHANGE:1||Coulomb correlation:1||magnon:1||phonons:1||ELECTRON FERROMAGNETISM:1||CURIETEMPERATURE:1||ARPES:1||PLANEWAVE METHOD:1||Xray absorption spectroscopy (XAS):1||ROOMTEMPERATURE:1||MONOCHALCOGENIDES:1||HEAT:1||UPDSN:1||MOMENTS:1||XRAY ABSORPTION:1||SEMICONDUCTOR:1||Fermi surface nesting:1||optical phonon:1||disordered system:1||dilute magnetic semiconductors:1||CMR manganites:1||PHONONS:1||LATTICEDYNAMICS:1||OXIDES:1||4fphotoemission:1||permanent magnet:1||pseudogap:1||TRANSPORTPROPERTIES:1||ANTIFERROMAGNET:1||(BI,PB)SRCOO SYSTEM:1||semicore correlation:1||POLARIZATION:1||CRYSTAL:1||spinel:1||Xray magnetic circular dichroism (XMCD):1||magnetocapacitance:1||ANATASE:1||TEMPERATURES:1||Pseudogap:1||INTERFACE:1||SUBSTRATE:1||YNI2B2C:1||SAMARIUM SULFIDE:1||strong swave superconductor:1||DOPED MANGANITE:1||SYMMETRY:1||CENISN:1||resonance mode:1||DISORDERED SYSTEM:1||LITHIUM INTERCALATION:1||CUO2 PLANE:1||SURFACE:1||Delafossite:1||ELECTRICALPROPERTIES:1||NIMNSB:1||PTMNSB:1||ROOMTEMPERATURE FERROMAGNETISM:1||RUBIDIUM MANGANESE HEXACYANOFERRATE:1||COLOSSALMAGNETORESISTANCE:1||FINITE TEMPERATURES:1||LAMNO3:1||FE:1||transitionmetal oxides:1||giant magnetoresistance:1||phonon:1||COPPER OXIDES:1||valence states:1||thermoelectric:1||semiconductor:1||CATION DISTRIBUTION:1||FeCr2S4:1||photoemission spectroscopy (PES):1||METALLIC FERROMAGNETISM:1||GRAPHITE:1||SUSCEPTIBILITY:1||UBE13:1||RCrSb3:1||band JahnTeller:1||Ce3S4:1||TiO2:1||PrBa2Cu3O7delta:1||UNTWINNED PRBA2CU3O7:1||AGNIO2:1||HALFMETALLIC FERROMAGNETS:1||CI:1||Energy gap:1||Photoemission:1||Future applications:1||Photoemission measurements:1||Graphene:1||BANDSTRUCTURE:1||TC:1||superconductivity:1||magnetic semiconductors:1||CMRmanganites:1||thin films:1||spin dynamics:1||highTc superconductors:1||ITINERANTELECTRON FERROMAGNETISM:1||SINGLECRYSTALS:1||CeTe2:1||amorphous magnetic materials:1||EPITAXIAL GRAPHENE:1||LAYERED PNICTIDEOXIDES:1||BOROCARBIDE SUPERCONDUCTORS:1||AUGMENTEDWAVE METHOD:1||METALLIC MAGNET UNISN:1||ORIGIN:1||spectrum rearrangement:1||MEANFIELD THEORY:1||MOLECULEBASED MAGNETS:1||METASTABLE STATE:1||INSULATOR:1||magnetic orderin:1||FCC IRON:1||CeRu2:1||TL2MN2O7:1||isotope effect:1||Perovskitemanganites:1||RECURSION METHOD:1||PERPENDICULAR MAGNETICANISOTROPY:1||quasiparticle spectral density:1||GW:1||MANGANESE FERRITE:1||RESONANCE:1||SeCuO3:1||Optical conductivity:1||MASSLESS DIRAC FERMIONS:1||SCHOTTKYBARRIER:1||electronic structure:15||ELECTRONICSTRUCTURE:11||TRANSITIONMETAL COMPOUNDS:10||METALS:10||photoemission:8||SPECTRA:8||MAGNETORESISTANCE:7||FERROMAGNETISM:7||TRANSPORT:7||TRANSITION:6||FILMS:6||THINFILMS:5||TOTALENERGY CALCULATIONS:5||MAGNETICPROPERTIES:5||SUPERCONDUCTIVITY:5||PR:5||LATTICE:4||STATES:4||SPECTROSCOPY:4||FIELD:4||CRYSTALSTRUCTURE:4||PHOTOEMISSION:4||TEMPERATURE:4||TRANSITIONTEMPERATURE:4||XRAYABSORPTION:4||STATE:4||CU:4||BASISSET:4||XAS:4||CRYSTALS:3||EXCITATIONS:3||MOTTHUBBARD SYSTEMS:3||HIGHENERGY SPIN:3||halfmetal:3||INSULATORS:3||LA2CUO4:3||MODEL:3||FLUCTUATIONS:3||CE:3||double exchange:3||TRANSITIONMETALS:3||RESISTIVITY:3||BORON:3||LA1XCAXMNO3:3||IRON:3||PES:3||ANTIMONIDES:2||MgB2:2||ZR METALLIC GLASSES:2||superconductor:2||CRITICALCURRENT DENSITY:2||CIRCULARDICHROISM:2||SEMICONDUCTORS:2||LOCALIZATION:2||INTRABAND OPTICAL CONDUCTIVITY:2||COLOSSAL MAGNETORESISTANCE:2||OXIDATION:2||EXISTENCE:2||COPPER:2||diboride:2||MAGNESIUMDIBORIDE:2||GAP:2||CE COMPOUNDS:2||CORE POLARIZATION:2||magnetoresistance:2||photoemission spectroscopy:2||electronphonon interaction:2||GETTER:2||PD:2||MAGNETISM:2||FECR2S4:2||SUPERCONDUCTING MGB2:2||WIRES:2||ABSORPTION:2||ENERGY:2||LA1XSRXMNO3:2||CONSTANTS:2||polaron:2||charge ordering:2||SCATTERING:2||XRAY PHOTOEMISSION:2||CeNiSn:2||phase diagram:2||PHOTOELECTRON:2||QUADRUPOLAR:2||perovskitemanganites:2||CO:2||SYSTEMS:2||DOPED ZNO:2||LOWFREQUENCY SOUND:2||LA:2||ELECTRONELECTRON SCATTERING:2||AU:2||DENSITYWAVE INSTABILITY:2||FERMISURFACE:2||hybridization:2||VALENCEBAND SATELLITE:2||SULFUR SPINEL:2||Heusler:2||APPROXIMATION:2||superexchange:2||colossal magnetoresistance:2||ALLOYS:2||DEPENDENCE:2||AG:2||electronic structures:2||AUGERSPECTRA:2||CR:2||PARAMETERS:2||DIFFRACTION:2||SEMICONDUCTORMETAL TRANSITION:1||INTERMEDIATEVALENCE:1||SMB6:1||SRRUO3:1||antiperovskite structure with antipolar nature:1||lowenergy twodimensional phonons:1||anatase TiO2:1||La3S4:1||metalinsulator transitions:1||MNO:1||ELECTRONICSTRUCTURES:1||MAGNETIC CIRCULARDICHROISM:1||Density functional theory:1||CeCo2:1||TOPOLARON CROSSOVER:1||EXCHANGE:1||cuprates:1||high Tc cuprates:1||magnetically ordered materials:1||ZNSE:1||Sr2xKxFeMoO6:1||CDW:1||TeCuO3:1||STRUCTURALPROPERTIES:1||MN:1||screening length:1||amorphous Fe:1||WAVE BASISSET:1||SILICONCARBIDE:1||HIGHPRESSURE:1||electronphonon coupling:1||quenched superconductivity:1||CMR perovskite manganites:1||OXIDE:1||polarons:1||synchrotron radiation:1||FULLERIDES:1||RESONANTPHOTOEMISSION:1||Silicon carbide:1||DFT calculation:1||Hybridized bands:1||GIANT MAGNETORESISTANCE:1||PEROVSKITES:1||Raman spectra:1||EXCHANGE ENHANCEMENT:1||SILICON:1||SR2FEMOO6:1||orbital ordering:1||delafossite:1||TITANIUMDIOXIDE:1||electronic structure of disordered solids:1||YFE2:1||Magnetic polaron:1||NA2TI2SB2O:1||STRONGCOUPLED SUPERCONDUCTORS:1||HEAVYFERMION SYSTEMS:1||firstprinciples calculations:1||MECHANISM:1||UNiSn:1||PHOTONIC BANDGAP:1||SINGLE IMPURITY:1||PHONONSPECTRUM:1||FERMISURFACE TOPOLOGY:1||SUPPRESSION:1||RESONANT PHOTOEMISSION:1||METALDOPED PICENE:1||PHOTOIONIZATION CROSSSECTIONS:1||PHOTOINDUCED FERRIMAGNETIC SYSTEMS:1||LINKAGE ISOMERISM:1||CHARGETRANSFER:1||Bilayer Graphene:1||MAGNETICFIELD:1||SPINWAVES:1||rareearth manganese oxides:1||magnonphonon interaction:1||NACO2O4:1||ENERGYBANDS:1||SELFENERGY:1||GAS:1||Fe0.5Cu0.5Cr2S4:1||scanning photoelectron microscopy (SPEM):1||MAGNETIC PROPERTIES:1||Stoner model:1||AMORPHOUS TRANSITIONMETALS:1||SPINGLASS STATES:1||NI:1||LA3NI2B2N3:1||SOLIDS:1||CEO2:1||BAND THEORY:1||dilute magnetic semiconductor:1||pyrochlore:1||Y1XPRXBA2CU3O7DELTA:1||and electronphonon interactions:1||VIBRATIONS:1||RAY PHOTOEMISSION:1||ALKALI CATION:1||Europium:1||colossal magnetoresistance:1||structural stability:1||ENERGYGAP:1||small polaron:1||DOUBLE EXCHANGE:1||Coulomb correlation:1||magnon:1||phonons:1||ELECTRON FERROMAGNETISM:1||CURIETEMPERATURE:1||ARPES:1||PLANEWAVE METHOD:1||Xray absorption spectroscopy (XAS):1||ROOMTEMPERATURE:1||MONOCHALCOGENIDES:1||HEAT:1||UPDSN:1||MOMENTS:1||XRAY ABSORPTION:1||SEMICONDUCTOR:1||Fermi surface nesting:1||optical phonon:1||disordered system:1||dilute magnetic semiconductors:1||CMR manganites:1||PHONONS:1||LATTICEDYNAMICS:1||OXIDES:1||4fphotoemission:1||permanent magnet:1||pseudogap:1||TRANSPORTPROPERTIES:1||ANTIFERROMAGNET:1||(BI,PB)SRCOO SYSTEM:1||semicore correlation:1||POLARIZATION:1||CRYSTAL:1||spinel:1||Xray magnetic circular dichroism (XMCD):1||magnetocapacitance:1||ANATASE:1||TEMPERATURES:1||Pseudogap:1||INTERFACE:1||SUBSTRATE:1||YNI2B2C:1||SAMARIUM SULFIDE:1||strong swave superconductor:1||DOPED MANGANITE:1||SYMMETRY:1||CENISN:1||resonance mode:1||DISORDERED SYSTEM:1||LITHIUM INTERCALATION:1||CUO2 PLANE:1||SURFACE:1||Delafossite:1||ELECTRICALPROPERTIES:1||NIMNSB:1||PTMNSB:1||ROOMTEMPERATURE FERROMAGNETISM:1||RUBIDIUM MANGANESE HEXACYANOFERRATE:1||COLOSSALMAGNETORESISTANCE:1||FINITE TEMPERATURES:1||LAMNO3:1||FE:1||transitionmetal oxides:1||giant magnetoresistance:1||phonon:1||COPPER OXIDES:1||valence states:1||thermoelectric:1||semiconductor:1||CATION DISTRIBUTION:1||FeCr2S4:1||photoemission spectroscopy (PES):1||METALLIC FERROMAGNETISM:1||GRAPHITE:1||SUSCEPTIBILITY:1||UBE13:1||RCrSb3:1||band JahnTeller:1||Ce3S4:1||TiO2:1||PrBa2Cu3O7delta:1||UNTWINNED PRBA2CU3O7:1||AGNIO2:1||HALFMETALLIC FERROMAGNETS:1||CI:1||Energy gap:1||Photoemission:1||Future applications:1||Photoemission measurements:1||Graphene:1||BANDSTRUCTURE:1||TC:1||superconductivity:1||magnetic semiconductors:1||CMRmanganites:1||thin films:1||spin dynamics:1||highTc superconductors:1||ITINERANTELECTRON FERROMAGNETISM:1||SINGLECRYSTALS:1||CeTe2:1||amorphous magnetic materials:1||EPITAXIAL GRAPHENE:1||LAYERED PNICTIDEOXIDES:1||BOROCARBIDE SUPERCONDUCTORS:1||AUGMENTEDWAVE METHOD:1||METALLIC MAGNET UNISN:1||ORIGIN:1||spectrum rearrangement:1||MEANFIELD THEORY:1||MOLECULEBASED MAGNETS:1||METASTABLE STATE:1||INSULATOR:1||magnetic orderin:1||FCC IRON:1||CeRu2:1||TL2MN2O7:1||isotope effect:1||Perovskitemanganites:1||RECURSION METHOD:1||PERPENDICULAR MAGNETICANISOTROPY:1||quasiparticle spectral density:1||GW:1||MANGANESE FERRITE:1||RESONANCE:1||SeCuO3:1||Optical conductivity:1||MASSLESS DIRAC FERMIONS:1||SCHOTTKYBARRIER:1||electronic structure:15||ELECTRONICSTRUCTURE:11||TRANSITIONMETAL COMPOUNDS:10||METALS:10||photoemission:8||SPECTRA:8||MAGNETORESISTANCE:7||FERROMAGNETISM:7||TRANSPORT:7||TRANSITION:6||FILMS:6||THINFILMS:5||TOTALENERGY CALCULATIONS:5||MAGNETICPROPERTIES:5||SUPERCONDUCTIVITY:5||PR:5||LATTICE:4||STATES:4||SPECTROSCOPY:4||FIELD:4||CRYSTALSTRUCTURE:4||PHOTOEMISSION:4||TEMPERATURE:4||TRANSITIONTEMPERATURE:4||XRAYABSORPTION:4||STATE:4||CU:4||BASISSET:4||XAS:4||CRYSTALS:3||EXCITATIONS:3||MOTTHUBBARD SYSTEMS:3||HIGHENERGY SPIN:3||halfmetal:3||INSULATORS:3||LA2CUO4:3||MODEL:3||FLUCTUATIONS:3||CE:3||double exchange:3||TRANSITIONMETALS:3||RESISTIVITY:3||BORON:3||LA1XCAXMNO3:3||IRON:3||PES:3||ANTIMONIDES:2||MgB2:2||ZR METALLIC GLASSES:2||superconductor:2||CRITICALCURRENT DENSITY:2||CIRCULARDICHROISM:2||SEMICONDUCTORS:2||LOCALIZATION:2||INTRABAND OPTICAL CONDUCTIVITY:2||COLOSSAL MAGNETORESISTANCE:2||OXIDATION:2||EXISTENCE:2||COPPER:2||diboride:2||MAGNESIUMDIBORIDE:2||GAP:2||CE COMPOUNDS:2||CORE POLARIZATION:2||magnetoresistance:2||photoemission spectroscopy:2||electronphonon interaction:2||GETTER:2||PD:2||MAGNETISM:2||FECR2S4:2||SUPERCONDUCTING MGB2:2||WIRES:2||ABSORPTION:2||ENERGY:2||LA1XSRXMNO3:2||CONSTANTS:2||polaron:2||charge ordering:2||SCATTERING:2||XRAY PHOTOEMISSION:2||CeNiSn:2||phase diagram:2||PHOTOELECTRON:2||QUADRUPOLAR:2||perovskitemanganites:2||CO:2||SYSTEMS:2||DOPED ZNO:2||LOWFREQUENCY SOUND:2||LA:2||ELECTRONELECTRON SCATTERING:2||AU:2||DENSITYWAVE INSTABILITY:2||FERMISURFACE:2||hybridization:2||VALENCEBAND SATELLITE:2||SULFUR SPINEL:2||Heusler:2||APPROXIMATION:2||superexchange:2||colossal magnetoresistance:2||ALLOYS:2||DEPENDENCE:2||AG:2||electronic structures:2||AUGERSPECTRA:2||CR:2||PARAMETERS:2||DIFFRACTION:2||SEMICONDUCTORMETAL TRANSITION:1||INTERMEDIATEVALENCE:1||SMB6:1||SRRUO3:1||antiperovskite structure with antipolar nature:1||lowenergy twodimensional phonons:1||anatase TiO2:1||La3S4:1||metalinsulator transitions:1||MNO:1||ELECTRONICSTRUCTURES:1||MAGNETIC CIRCULARDICHROISM:1||Density functional theory:1||CeCo2:1||TOPOLARON CROSSOVER:1||EXCHANGE:1||cuprates:1||high Tc cuprates:1||magnetically ordered materials:1||ZNSE:1||Sr2xKxFeMoO6:1||CDW:1||TeCuO3:1||STRUCTURALPROPERTIES:1||MN:1||screening length:1||amorphous Fe:1||WAVE BASISSET:1||SILICONCARBIDE:1||HIGHPRESSURE:1||electronphonon coupling:1||quenched superconductivity:1||CMR perovskite manganites:1||OXIDE:1||polarons:1||synchrotron radiation:1||FULLERIDES:1||RESONANTPHOTOEMISSION:1||Silicon carbide:1||DFT calculation:1||Hybridized bands:1||GIANT MAGNETORESISTANCE:1||PEROVSKITES:1||Raman spectra:1||EXCHANGE ENHANCEMENT:1||SILICON:1||SR2FEMOO6:1||orbital ordering:1||delafossite:1||TITANIUMDIOXIDE:1||electronic structure of disordered solids:1||YFE2:1||Magnetic polaron:1||NA2TI2SB2O:1||STRONGCOUPLED SUPERCONDUCTORS:1||HEAVYFERMION SYSTEMS:1||firstprinciples calculations:1||MECHANISM:1||UNiSn:1||PHOTONIC BANDGAP:1||SINGLE IMPURITY:1||PHONONSPECTRUM:1||FERMISURFACE TOPOLOGY:1||SUPPRESSION:1||RESONANT PHOTOEMISSION:1||METALDOPED PICENE:1||PHOTOIONIZATION CROSSSECTIONS:1||PHOTOINDUCED FERRIMAGNETIC SYSTEMS:1||LINKAGE ISOMERISM:1||CHARGETRANSFER:1||Bilayer Graphene:1||MAGNETICFIELD:1||SPINWAVES:1||rareearth manganese oxides:1||magnonphonon interaction:1||NACO2O4:1||ENERGYBANDS:1||SELFENERGY:1||GAS:1||Fe0.5Cu0.5Cr2S4:1||scanning photoelectron microscopy (SPEM):1||MAGNETIC PROPERTIES:1||Stoner model:1||AMORPHOUS TRANSITIONMETALS:1||SPINGLASS STATES:1||NI:1||LA3NI2B2N3:1||SOLIDS:1||CEO2:1||BAND THEORY:1||dilute magnetic semiconductor:1||pyrochlore:1||Y1XPRXBA2CU3O7DELTA:1||and electronphonon interactions:1||VIBRATIONS:1||RAY PHOTOEMISSION:1||ALKALI CATION:1||Europium:1||colossal magnetoresistance:1||structural stability:1||ENERGYGAP:1||small polaron:1||DOUBLE EXCHANGE:1||Coulomb correlation:1||magnon:1||phonons:1||ELECTRON FERROMAGNETISM:1||CURIETEMPERATURE:1||ARPES:1||PLANEWAVE METHOD:1||Xray absorption spectroscopy (XAS):1||ROOMTEMPERATURE:1||MONOCHALCOGENIDES:1||HEAT:1||UPDSN:1||MOMENTS:1||XRAY ABSORPTION:1||SEMICONDUCTOR:1||Fermi surface nesting:1||optical phonon:1||disordered system:1||dilute magnetic semiconductors:1||CMR manganites:1||PHONONS:1||LATTICEDYNAMICS:1||OXIDES:1||4fphotoemission:1||permanent magnet:1||pseudogap:1||TRANSPORTPROPERTIES:1||ANTIFERROMAGNET:1||(BI,PB)SRCOO SYSTEM:1||semicore correlation:1||POLARIZATION:1||CRYSTAL:1||spinel:1||Xray magnetic circular dichroism (XMCD):1||magnetocapacitance:1||ANATASE:1||TEMPERATURES:1||Pseudogap:1||INTERFACE:1||SUBSTRATE:1||YNI2B2C:1||SAMARIUM SULFIDE:1||strong swave superconductor:1||DOPED MANGANITE:1||SYMMETRY:1||CENISN:1||resonance mode:1||DISORDERED SYSTEM:1||LITHIUM INTERCALATION:1||CUO2 PLANE:1||SURFACE:1||Delafossite:1||ELECTRICALPROPERTIES:1||NIMNSB:1||PTMNSB:1||ROOMTEMPERATURE FERROMAGNETISM:1||RUBIDIUM MANGANESE HEXACYANOFERRATE:1||COLOSSALMAGNETORESISTANCE:1||FINITE TEMPERATURES:1||LAMNO3:1||FE:1||transitionmetal oxides:1||giant magnetoresistance:1||phonon:1||COPPER OXIDES:1||valence states:1||thermoelectric:1||semiconductor:1||CATION DISTRIBUTION:1||FeCr2S4:1||photoemission spectroscopy (PES):1||METALLIC FERROMAGNETISM:1||GRAPHITE:1||SUSCEPTIBILITY:1||UBE13:1||RCrSb3:1||band JahnTeller:1||Ce3S4:1||TiO2:1||PrBa2Cu3O7delta:1||UNTWINNED PRBA2CU3O7:1||AGNIO2:1||HALFMETALLIC FERROMAGNETS:1||CI:1||Energy gap:1||Photoemission:1||Future applications:1||Photoemission measurements:1||Graphene:1||BANDSTRUCTURE:1||TC:1||superconductivity:1||magnetic semiconductors:1||CMRmanganites:1||thin films:1||spin dynamics:1||highTc superconductors:1||ITINERANTELECTRON FERROMAGNETISM:1||SINGLECRYSTALS:1||CeTe2:1||amorphous magnetic materials:1||EPITAXIAL GRAPHENE:1||LAYERED PNICTIDEOXIDES:1||BOROCARBIDE SUPERCONDUCTORS:1||AUGMENTEDWAVE METHOD:1||METALLIC MAGNET UNISN:1||ORIGIN:1||spectrum rearrangement:1||MEANFIELD THEORY:1||MOLECULEBASED MAGNETS:1||METASTABLE STATE:1||INSULATOR:1||magnetic orderin:1||FCC IRON:1||CeRu2:1||TL2MN2O7:1||isotope effect:1||Perovskitemanganites:1||RECURSION METHOD:1||PERPENDICULAR MAGNETICANISOTROPY:1||quasiparticle spectral density:1||GW:1||MANGANESE FERRITE:1||RESONANCE:1||SeCuO3:1||Optical conductivity:1||MASSLESS DIRAC FERMIONS:1||SCHOTTKYBARRIER:1||electronic structure:15||ELECTRONICSTRUCTURE:11||TRANSITIONMETAL COMPOUNDS:10||METALS:10||photoemission:8||SPECTRA:8||MAGNETORESISTANCE:7||FERROMAGNETISM:7||TRANSPORT:7||TRANSITION:6||FILMS:6||THINFILMS:5||TOTALENERGY CALCULATIONS:5||MAGNETICPROPERTIES:5||SUPERCONDUCTIVITY:5||PR:5||LATTICE:4||STATES:4||SPECTROSCOPY:4||FIELD:4||CRYSTALSTRUCTURE:4||PHOTOEMISSION:4||TEMPERATURE:4||TRANSITIONTEMPERATURE:4||XRAYABSORPTION:4||STATE:4||CU:4||BASISSET:4||XAS:4||CRYSTALS:3||EXCITATIONS:3||MOTTHUBBARD SYSTEMS:3||HIGHENERGY SPIN:3||halfmetal:3||INSULATORS:3||LA2CUO4:3||MODEL:3||FLUCTUATIONS:3||CE:3||double exchange:3||TRANSITIONMETALS:3||RESISTIVITY:3||BORON:3||LA1XCAXMNO3:3||IRON:3||PES:3||ANTIMONIDES:2||MgB2:2||ZR METALLIC GLASSES:2||superconductor:2||CRITICALCURRENT DENSITY:2||CIRCULARDICHROISM:2||SEMICONDUCTORS:2||LOCALIZATION:2||INTRABAND OPTICAL CONDUCTIVITY:2||COLOSSAL MAGNETORESISTANCE:2||OXIDATION:2||EXISTENCE:2||COPPER:2||diboride:2||MAGNESIUMDIBORIDE:2||GAP:2||CE COMPOUNDS:2||CORE POLARIZATION:2||magnetoresistance:2||photoemission spectroscopy:2||electronphonon interaction:2||GETTER:2||PD:2||MAGNETISM:2||FECR2S4:2||SUPERCONDUCTING MGB2:2||WIRES:2||ABSORPTION:2||ENERGY:2||LA1XSRXMNO3:2||CONSTANTS:2||polaron:2||charge ordering:2||SCATTERING:2||XRAY PHOTOEMISSION:2||CeNiSn:2||phase diagram:2||PHOTOELECTRON:2||QUADRUPOLAR:2||perovskitemanganites:2||CO:2||SYSTEMS:2||DOPED ZNO:2||LOWFREQUENCY SOUND:2||LA:2||ELECTRONELECTRON SCATTERING:2||AU:2||DENSITYWAVE INSTABILITY:2||FERMISURFACE:2||hybridization:2||VALENCEBAND SATELLITE:2||SULFUR SPINEL:2||Heusler:2||APPROXIMATION:2||superexchange:2||colossal magnetoresistance:2||ALLOYS:2||DEPENDENCE:2||AG:2||electronic structures:2||AUGERSPECTRA:2||CR:2||PARAMETERS:2||DIFFRACTION:2||SEMICONDUCTORMETAL TRANSITION:1||INTERMEDIATEVALENCE:1||SMB6:1||SRRUO3:1||antiperovskite structure with antipolar nature:1||lowenergy twodimensional phonons:1||anatase TiO2:1||La3S4:1||metalinsulator transitions:1||MNO:1||ELECTRONICSTRUCTURES:1||MAGNETIC CIRCULARDICHROISM:1||Density functional theory:1||CeCo2:1||TOPOLARON CROSSOVER:1||EXCHANGE:1||cuprates:1||high Tc cuprates:1||magnetically ordered materials:1||ZNSE:1||Sr2xKxFeMoO6:1||CDW:1||TeCuO3:1||STRUCTURALPROPERTIES:1||MN:1||screening length:1||amorphous Fe:1||WAVE BASISSET:1||SILICONCARBIDE:1||HIGHPRESSURE:1||electronphonon coupling:1||quenched superconductivity:1||CMR perovskite manganites:1||OXIDE:1||polarons:1||synchrotron radiation:1||FULLERIDES:1||RESONANTPHOTOEMISSION:1||Silicon carbide:1||DFT calculation:1||Hybridized bands:1||GIANT MAGNETORESISTANCE:1||PEROVSKITES:1||Raman spectra:1||EXCHANGE ENHANCEMENT:1||SILICON:1||SR2FEMOO6:1||orbital ordering:1||delafossite:1||TITANIUMDIOXIDE:1||electronic structure of disordered solids:1||YFE2:1||Magnetic polaron:1||NA2TI2SB2O:1||STRONGCOUPLED SUPERCONDUCTORS:1||HEAVYFERMION SYSTEMS:1||firstprinciples calculations:1||MECHANISM:1||UNiSn:1||PHOTONIC BANDGAP:1||SINGLE IMPURITY:1||PHONONSPECTRUM:1||FERMISURFACE TOPOLOGY:1||SUPPRESSION:1||RESONANT PHOTOEMISSION:1||METALDOPED PICENE:1||PHOTOIONIZATION CROSSSECTIONS:1||PHOTOINDUCED FERRIMAGNETIC SYSTEMS:1||LINKAGE ISOMERISM:1||CHARGETRANSFER:1||Bilayer Graphene:1||MAGNETICFIELD:1||SPINWAVES:1||rareearth manganese oxides:1||magnonphonon interaction:1||NACO2O4:1||ENERGYBANDS:1||SELFENERGY:1||GAS:1||Fe0.5Cu0.5Cr2S4:1||scanning photoelectron microscopy (SPEM):1||MAGNETIC PROPERTIES:1||Stoner model:1||AMORPHOUS TRANSITIONMETALS:1||SPINGLASS STATES:1||NI:1||LA3NI2B2N3:1||SOLIDS:1||CEO2:1||BAND THEORY:1||dilute magnetic semiconductor:1||pyrochlore:1||Y1XPRXBA2CU3O7DELTA:1||and electronphonon interactions:1||VIBRATIONS:1||RAY PHOTOEMISSION:1||ALKALI CATION:1||Europium:1||colossal magnetoresistance:1||structural stability:1||ENERGYGAP:1||small polaron:1||DOUBLE EXCHANGE:1||Coulomb correlation:1||magnon:1||phonons:1||ELECTRON FERROMAGNETISM:1||CURIETEMPERATURE:1||ARPES:1||PLANEWAVE METHOD:1||Xray absorption spectroscopy (XAS):1||ROOMTEMPERATURE:1||MONOCHALCOGENIDES:1||HEAT:1||UPDSN:1||MOMENTS:1||XRAY ABSORPTION:1||SEMICONDUCTOR:1||Fermi surface nesting:1||optical phonon:1||disordered system:1||dilute magnetic semiconductors:1||CMR manganites:1||PHONONS:1||LATTICEDYNAMICS:1||OXIDES:1||4fphotoemission:1||permanent magnet:1||pseudogap:1||TRANSPORTPROPERTIES:1||ANTIFERROMAGNET:1||(BI,PB)SRCOO SYSTEM:1||semicore correlation:1||POLARIZATION:1||CRYSTAL:1||spinel:1||Xray magnetic circular dichroism (XMCD):1||magnetocapacitance:1||ANATASE:1||TEMPERATURES:1||Pseudogap:1||INTERFACE:1||SUBSTRATE:1||YNI2B2C:1||SAMARIUM SULFIDE:1||strong swave superconductor:1||DOPED MANGANITE:1||SYMMETRY:1||CENISN:1||resonance mode:1||DISORDERED SYSTEM:1||LITHIUM INTERCALATION:1||CUO2 PLANE:1||SURFACE:1||Delafossite:1||ELECTRICALPROPERTIES:1||NIMNSB:1||PTMNSB:1||ROOMTEMPERATURE FERROMAGNETISM:1||RUBIDIUM MANGANESE HEXACYANOFERRATE:1||COLOSSALMAGNETORESISTANCE:1||FINITE TEMPERATURES:1||LAMNO3:1||FE:1||transitionmetal oxides:1||giant magnetoresistance:1||phonon:1||COPPER OXIDES:1||valence states:1||thermoelectric:1||semiconductor:1||CATION DISTRIBUTION:1||FeCr2S4:1||photoemission spectroscopy (PES):1||METALLIC FERROMAGNETISM:1||GRAPHITE:1||SUSCEPTIBILITY:1||UBE13:1||RCrSb3:1||band JahnTeller:1||Ce3S4:1||TiO2:1||PrBa2Cu3O7delta:1||UNTWINNED PRBA2CU3O7:1||AGNIO2:1||HALFMETALLIC FERROMAGNETS:1||CI:1||Energy gap:1||Photoemission:1||Future applications:1||Photoemission measurements:1||Graphene:1||BANDSTRUCTURE:1||TC:1||superconductivity:1||magnetic semiconductors:1||CMRmanganites:1||thin films:1||spin dynamics:1||highTc superconductors:1||ITINERANTELECTRON FERROMAGNETISM:1||SINGLECRYSTALS:1||CeTe2:1||amorphous magnetic materials:1||EPITAXIAL GRAPHENE:1||LAYERED PNICTIDEOXIDES:1||BOROCARBIDE SUPERCONDUCTORS:1||AUGMENTEDWAVE METHOD:1||METALLIC MAGNET UNISN:1||ORIGIN:1||spectrum rearrangement:1||MEANFIELD THEORY:1||MOLECULEBASED MAGNETS:1||METASTABLE STATE:1||INSULATOR:1||magnetic orderin:1||FCC IRON:1||CeRu2:1||TL2MN2O7:1||isotope effect:1||Perovskitemanganites:1||RECURSION METHOD:1||PERPENDICULAR MAGNETICANISOTROPY:1||quasiparticle spectral density:1||GW:1||MANGANESE FERRITE:1||RESONANCE:1||SeCuO3:1||Optical conductivity:1||MASSLESS DIRAC FERMIONS:1||SCHOTTKYBARRIER:1||electronic structure:15||ELECTRONICSTRUCTURE:11||TRANSITIONMETAL COMPOUNDS:10||METALS:10||photoemission:8||SPECTRA:8||MAGNETORESISTANCE:7||FERROMAGNETISM:7||TRANSPORT:7||TRANSITION:6||FILMS:6||THINFILMS:5||TOTALENERGY CALCULATIONS:5||MAGNETICPROPERTIES:5||SUPERCONDUCTIVITY:5||PR:5||LATTICE:4||STATES:4||SPECTROSCOPY:4||FIELD:4||CRYSTALSTRUCTURE:4||PHOTOEMISSION:4||TEMPERATURE:4||TRANSITIONTEMPERATURE:4||XRAYABSORPTION:4||STATE:4||CU:4||BASISSET:4||XAS:4||CRYSTALS:3||EXCITATIONS:3||MOTTHUBBARD SYSTEMS:3||HIGHENERGY SPIN:3||halfmetal:3||INSULATORS:3||LA2CUO4:3||MODEL:3||FLUCTUATIONS:3||CE:3||double exchange:3||TRANSITIONMETALS:3||RESISTIVITY:3||BORON:3||LA1XCAXMNO3:3||IRON:3||PES:3||ANTIMONIDES:2||MgB2:2||ZR METALLIC GLASSES:2||superconductor:2||CRITICALCURRENT DENSITY:2||CIRCULARDICHROISM:2||SEMICONDUCTORS:2||LOCALIZATION:2||INTRABAND OPTICAL CONDUCTIVITY:2||COLOSSAL MAGNETORESISTANCE:2||OXIDATION:2||EXISTENCE:2||COPPER:2||diboride:2||MAGNESIUMDIBORIDE:2||GAP:2||CE COMPOUNDS:2||CORE POLARIZATION:2||magnetoresistance:2||photoemission spectroscopy:2||electronphonon interaction:2||GETTER:2||PD:2||MAGNETISM:2||FECR2S4:2||SUPERCONDUCTING MGB2:2||WIRES:2||ABSORPTION:2||ENERGY:2||LA1XSRXMNO3:2||CONSTANTS:2||polaron:2||charge ordering:2||SCATTERING:2||XRAY PHOTOEMISSION:2||CeNiSn:2||phase diagram:2||PHOTOELECTRON:2||QUADRUPOLAR:2||perovskitemanganites:2||CO:2||SYSTEMS:2||DOPED ZNO:2||LOWFREQUENCY SOUND:2||LA:2||ELECTRONELECTRON SCATTERING:2||AU:2||DENSITYWAVE INSTABILITY:2||FERMISURFACE:2||hybridization:2||VALENCEBAND SATELLITE:2||SULFUR SPINEL:2||Heusler:2||APPROXIMATION:2||superexchange:2||colossal magnetoresistance:2||ALLOYS:2||DEPENDENCE:2||AG:2||electronic structures:2||AUGERSPECTRA:2||CR:2||PARAMETERS:2||DIFFRACTION:2||SEMICONDUCTORMETAL TRANSITION:1||INTERMEDIATEVALENCE:1||SMB6:1||SRRUO3:1||antiperovskite structure with antipolar nature:1||lowenergy twodimensional phonons:1||anatase TiO2:1||La3S4:1||metalinsulator transitions:1||MNO:1||ELECTRONICSTRUCTURES:1||MAGNETIC CIRCULARDICHROISM:1||Density functional theory:1||CeCo2:1||TOPOLARON CROSSOVER:1||EXCHANGE:1||cuprates:1||high Tc cuprates:1||magnetically ordered materials:1||ZNSE:1||Sr2xKxFeMoO6:1||CDW:1||TeCuO3:1||STRUCTURALPROPERTIES:1||MN:1||screening length:1||amorphous Fe:1||WAVE BASISSET:1||SILICONCARBIDE:1||HIGHPRESSURE:1||electronphonon coupling:1||quenched superconductivity:1||CMR perovskite manganites:1||OXIDE:1||polarons:1||synchrotron radiation:1||FULLERIDES:1||RESONANTPHOTOEMISSION:1||Silicon carbide:1||DFT calculation:1||Hybridized bands:1||GIANT MAGNETORESISTANCE:1||PEROVSKITES:1||Raman spectra:1||EXCHANGE ENHANCEMENT:1||SILICON:1||SR2FEMOO6:1||orbital ordering:1||delafossite:1||TITANIUMDIOXIDE:1||electronic structure of disordered solids:1||YFE2:1||Magnetic polaron:1||NA2TI2SB2O:1||STRONGCOUPLED SUPERCONDUCTORS:1||HEAVYFERMION SYSTEMS:1||firstprinciples calculations:1||MECHANISM:1||UNiSn:1||PHOTONIC BANDGAP:1||SINGLE IMPURITY:1||PHONONSPECTRUM:1||FERMISURFACE TOPOLOGY:1||SUPPRESSION:1||RESONANT PHOTOEMISSION:1||METALDOPED PICENE:1||PHOTOIONIZATION CROSSSECTIONS:1||PHOTOINDUCED FERRIMAGNETIC SYSTEMS:1||LINKAGE ISOMERISM:1||CHARGETRANSFER:1||Bilayer Graphene:1||MAGNETICFIELD:1||SPINWAVES:1||rareearth manganese oxides:1||magnonphonon interaction:1||NACO2O4:1||ENERGYBANDS:1||SELFENERGY:1||GAS:1||Fe0.5Cu0.5Cr2S4:1||scanning photoelectron microscopy (SPEM):1||MAGNETIC PROPERTIES:1||Stoner model:1||AMORPHOUS TRANSITIONMETALS:1||SPINGLASS STATES:1||NI:1||LA3NI2B2N3:1||SOLIDS:1||CEO2:1||BAND THEORY:1||dilute magnetic semiconductor:1||pyrochlore:1||Y1XPRXBA2CU3O7DELTA:1||and electronphonon interactions:1||VIBRATIONS:1||RAY PHOTOEMISSION:1||ALKALI CATION:1||Europium:1||colossal magnetoresistance:1||structural stability:1||ENERGYGAP:1||small polaron:1||DOUBLE EXCHANGE:1||Coulomb correlation:1||magnon:1||phonons:1||ELECTRON FERROMAGNETISM:1||CURIETEMPERATURE:1||ARPES:1||PLANEWAVE METHOD:1||Xray absorption spectroscopy (XAS):1||ROOMTEMPERATURE:1||MONOCHALCOGENIDES:1||HEAT:1||UPDSN:1||MOMENTS:1||XRAY ABSORPTION:1||SEMICONDUCTOR:1||Fermi surface nesting:1||optical phonon:1||disordered system:1||dilute magnetic semiconductors:1||CMR manganites:1||PHONONS:1||LATTICEDYNAMICS:1||OXIDES:1||4fphotoemission:1||permanent magnet:1||pseudogap:1||TRANSPORTPROPERTIES:1||ANTIFERROMAGNET:1||(BI,PB)SRCOO SYSTEM:1||semicore correlation:1||POLARIZATION:1||CRYSTAL:1||spinel:1||Xray magnetic circular dichroism (XMCD):1||magnetocapacitance:1||ANATASE:1||TEMPERATURES:1||Pseudogap:1||INTERFACE:1||SUBSTRATE:1||YNI2B2C:1||SAMARIUM SULFIDE:1||strong swave superconductor:1||DOPED MANGANITE:1||SYMMETRY:1||CENISN:1||resonance mode:1||DISORDERED SYSTEM:1||LITHIUM INTERCALATION:1||CUO2 PLANE:1||SURFACE:1||Delafossite:1||ELECTRICALPROPERTIES:1||NIMNSB:1||PTMNSB:1||ROOMTEMPERATURE FERROMAGNETISM:1||RUBIDIUM MANGANESE HEXACYANOFERRATE:1||COLOSSALMAGNETORESISTANCE:1||FINITE TEMPERATURES:1||LAMNO3:1||FE:1||transitionmetal oxides:1||giant magnetoresistance:1||phonon:1||COPPER OXIDES:1||valence states:1||thermoelectric:1||semiconductor:1||CATION DISTRIBUTION:1||FeCr2S4:1||photoemission spectroscopy (PES):1||METALLIC FERROMAGNETISM:1||GRAPHITE:1||SUSCEPTIBILITY:1||UBE13:1||RCrSb3:1||band JahnTeller:1||Ce3S4:1||TiO2:1||PrBa2Cu3O7delta:1||UNTWINNED PRBA2CU3O7:1||AGNIO2:1||HALFMETALLIC FERROMAGNETS:1||CI:1||Energy gap:1||Photoemission:1||Future applications:1||Photoemission measurements:1||Graphene:1||BANDSTRUCTURE:1||TC:1||superconductivity:1||magnetic semiconductors:1||CMRmanganites:1||thin films:1||spin dynamics:1||highTc superconductors:1||ITINERANTELECTRON FERROMAGNETISM:1||SINGLECRYSTALS:1||CeTe2:1||amorphous magnetic materials:1||EPITAXIAL GRAPHENE:1||LAYERED PNICTIDEOXIDES:1||BOROCARBIDE SUPERCONDUCTORS:1||AUGMENTEDWAVE METHOD:1||METALLIC MAGNET UNISN:1||ORIGIN:1||spectrum rearrangement:1||MEANFIELD THEORY:1||MOLECULEBASED MAGNETS:1||METASTABLE STATE:1||INSULATOR:1||magnetic orderin:1||FCC IRON:1||CeRu2:1||TL2MN2O7:1||isotope effect:1||Perovskitemanganites:1||RECURSION METHOD:1||PERPENDICULAR MAGNETICANISOTROPY:1||quasiparticle spectral density:1||GW:1||MANGANESE FERRITE:1||RESONANCE:1||SeCuO3:1||Optical conductivity:1||MASSLESS DIRAC FERMIONS:1||SCHOTTKYBARRIER:1||electronic structure:15||ELECTRONICSTRUCTURE:11||TRANSITIONMETAL COMPOUNDS:10||METALS:10||photoemission:8||SPECTRA:8||MAGNETORESISTANCE:7||FERROMAGNETISM:7||TRANSPORT:7||TRANSITION:6||FILMS:6||THINFILMS:5||TOTALENERGY CALCULATIONS:5||MAGNETICPROPERTIES:5||SUPERCONDUCTIVITY:5||PR:5||LATTICE:4||STATES:4||SPECTROSCOPY:4||FIELD:4||CRYSTALSTRUCTURE:4||PHOTOEMISSION:4||TEMPERATURE:4||TRANSITIONTEMPERATURE:4||XRAYABSORPTION:4||STATE:4||CU:4||BASISSET:4||XAS:4||CRYSTALS:3||EXCITATIONS:3||MOTTHUBBARD SYSTEMS:3||HIGHENERGY SPIN:3||halfmetal:3||INSULATORS:3||LA2CUO4:3||MODEL:3||FLUCTUATIONS:3||CE:3||double exchange:3||TRANSITIONMETALS:3||RESISTIVITY:3||BORON:3||LA1XCAXMNO3:3||IRON:3||PES:3||ANTIMONIDES:2||MgB2:2||ZR METALLIC GLASSES:2||superconductor:2||CRITICALCURRENT DENSITY:2||CIRCULARDICHROISM:2||SEMICONDUCTORS:2||LOCALIZATION:2||INTRABAND OPTICAL CONDUCTIVITY:2||COLOSSAL MAGNETORESISTANCE:2||OXIDATION:2||EXISTENCE:2||COPPER:2||diboride:2||MAGNESIUMDIBORIDE:2||GAP:2||CE COMPOUNDS:2||CORE POLARIZATION:2||magnetoresistance:2||photoemission spectroscopy:2||electronphonon interaction:2||GETTER:2||PD:2||MAGNETISM:2||FECR2S4:2||SUPERCONDUCTING MGB2:2||WIRES:2||ABSORPTION:2||ENERGY:2||LA1XSRXMNO3:2||CONSTANTS:2||polaron:2||charge ordering:2||SCATTERING:2||XRAY PHOTOEMISSION:2||CeNiSn:2||phase diagram:2||PHOTOELECTRON:2||QUADRUPOLAR:2||perovskitemanganites:2||CO:2||SYSTEMS:2||DOPED ZNO:2||LOWFREQUENCY SOUND:2||LA:2||ELECTRONELECTRON SCATTERING:2||AU:2||DENSITYWAVE INSTABILITY:2||FERMISURFACE:2||hybridization:2||VALENCEBAND SATELLITE:2||SULFUR SPINEL:2||Heusler:2||APPROXIMATION:2||superexchange:2||colossal magnetoresistance:2||ALLOYS:2||DEPENDENCE:2||AG:2||electronic structures:2||AUGERSPECTRA:2||CR:2||PARAMETERS:2||DIFFRACTION:2||SEMICONDUCTORMETAL TRANSITION:1||INTERMEDIATEVALENCE:1||SMB6:1||SRRUO3:1||antiperovskite structure with antipolar nature:1||lowenergy twodimensional phonons:1||anatase TiO2:1||La3S4:1||metalinsulator transitions:1||MNO:1||ELECTRONICSTRUCTURES:1||MAGNETIC CIRCULARDICHROISM:1||Density functional theory:1||CeCo2:1||TOPOLARON CROSSOVER:1||EXCHANGE:1||cuprates:1||high Tc cuprates:1||magnetically ordered materials:1||ZNSE:1||Sr2xKxFeMoO6:1||CDW:1||TeCuO3:1||STRUCTURALPROPERTIES:1||MN:1||screening length:1||amorphous Fe:1||WAVE BASISSET:1||SILICONCARBIDE:1||HIGHPRESSURE:1||electronphonon coupling:1||quenched superconductivity:1||CMR perovskite manganites:1||OXIDE:1||polarons:1||synchrotron radiation:1||FULLERIDES:1||RESONANTPHOTOEMISSION:1||Silicon carbide:1||DFT calculation:1||Hybridized bands:1||GIANT MAGNETORESISTANCE:1||PEROVSKITES:1||Raman spectra:1||EXCHANGE ENHANCEMENT:1||SILICON:1||SR2FEMOO6:1||orbital ordering:1||delafossite:1||TITANIUMDIOXIDE:1||electronic structure of disordered solids:1||YFE2:1||Magnetic polaron:1||NA2TI2SB2O:1||STRONGCOUPLED SUPERCONDUCTORS:1||HEAVYFERMION SYSTEMS:1||firstprinciples calculations:1||MECHANISM:1||UNiSn:1||PHOTONIC BANDGAP:1||SINGLE IMPURITY:1||PHONONSPECTRUM:1||FERMISURFACE TOPOLOGY:1||SUPPRESSION:1||RESONANT PHOTOEMISSION:1||METALDOPED PICENE:1||PHOTOIONIZATION CROSSSECTIONS:1||PHOTOINDUCED FERRIMAGNETIC SYSTEMS:1||LINKAGE ISOMERISM:1||CHARGETRANSFER:1||Bilayer Graphene:1||MAGNETICFIELD:1||SPINWAVES:1||rareearth manganese oxides:1||magnonphonon interaction:1||NACO2O4:1||ENERGYBANDS:1||SELFENERGY:1||GAS:1||Fe0.5Cu0.5Cr2S4:1||scanning photoelectron microscopy (SPEM):1||MAGNETIC PROPERTIES:1||Stoner model:1||AMORPHOUS TRANSITIONMETALS:1||SPINGLASS STATES:1||NI:1||LA3NI2B2N3:1||SOLIDS:1||CEO2:1||BAND THEORY:1||dilute magnetic semiconductor:1||pyrochlore:1||Y1XPRXBA2CU3O7DELTA:1||and electronphonon interactions:1||VIBRATIONS:1||RAY PHOTOEMISSION:1||ALKALI CATION:1||Europium:1||colossal magnetoresistance:1||structural stability:1||ENERGYGAP:1||small polaron:1||DOUBLE EXCHANGE:1||Coulomb correlation:1||magnon:1||phonons:1||ELECTRON FERROMAGNETISM:1||CURIETEMPERATURE:1||ARPES:1||PLANEWAVE METHOD:1||Xray absorption spectroscopy (XAS):1||ROOMTEMPERATURE:1||MONOCHALCOGENIDES:1||HEAT:1||UPDSN:1||MOMENTS:1||XRAY ABSORPTION:1||SEMICONDUCTOR:1||Fermi surface nesting:1||optical phonon:1||disordered system:1||dilute magnetic semiconductors:1||CMR manganites:1||PHONONS:1||LATTICEDYNAMICS:1||OXIDES:1||4fphotoemission:1||permanent magnet:1||pseudogap:1||TRANSPORTPROPERTIES:1||ANTIFERROMAGNET:1||(BI,PB)SRCOO SYSTEM:1||semicore correlation:1||POLARIZATION:1||CRYSTAL:1||spinel:1||Xray magnetic circular dichroism (XMCD):1||magnetocapacitance:1||ANATASE:1||TEMPERATURES:1||Pseudogap:1||INTERFACE:1||SUBSTRATE:1||YNI2B2C:1||SAMARIUM SULFIDE:1||strong swave superconductor:1||DOPED MANGANITE:1||SYMMETRY:1||CENISN:1||resonance mode:1||DISORDERED SYSTEM:1||LITHIUM INTERCALATION:1||CUO2 PLANE:1||SURFACE:1||Delafossite:1||ELECTRICALPROPERTIES:1||NIMNSB:1||PTMNSB:1||ROOMTEMPERATURE FERROMAGNETISM:1||RUBIDIUM MANGANESE HEXACYANOFERRATE:1||COLOSSALMAGNETORESISTANCE:1||FINITE TEMPERATURES:1||LAMNO3:1||FE:1||transitionmetal oxides:1||giant magnetoresistance:1||phonon:1||COPPER OXIDES:1||valence states:1||thermoelectric:1||semiconductor:1||CATION DISTRIBUTION:1||FeCr2S4:1||photoemission spectroscopy (PES):1||METALLIC FERROMAGNETISM:1||GRAPHITE:1||SUSCEPTIBILITY:1||UBE13:1||RCrSb3:1||band JahnTeller:1||Ce3S4:1||TiO2:1||PrBa2Cu3O7delta:1||UNTWINNED PRBA2CU3O7:1||AGNIO2:1||HALFMETALLIC FERROMAGNETS:1||CI:1||Energy gap:1||Photoemission:1||Future applications:1||Photoemission measurements:1||Graphene:1||BANDSTRUCTURE:1||TC:1||superconductivity:1||magnetic semiconductors:1||CMRmanganites:1||thin films:1||spin dynamics:1||highTc superconductors:1||ITINERANTELECTRON FERROMAGNETISM:1||SINGLECRYSTALS:1||CeTe2:1||amorphous magnetic materials:1||EPITAXIAL GRAPHENE:1||LAYERED PNICTIDEOXIDES:1||BOROCARBIDE SUPERCONDUCTORS:1||AUGMENTEDWAVE METHOD:1||METALLIC MAGNET UNISN:1||ORIGIN:1||spectrum rearrangement:1||MEANFIELD THEORY:1||MOLECULEBASED MAGNETS:1||METASTABLE STATE:1||INSULATOR:1||magnetic orderin:1||FCC IRON:1||CeRu2:1||TL2MN2O7:1||isotope effect:1||Perovskitemanganites:1||RECURSION METHOD:1||PERPENDICULAR MAGNETICANISOTROPY:1||quasiparticle spectral density:1||GW:1||MANGANESE FERRITE:1||RESONANCE:1||SeCuO3:1||Optical conductivity:1||MASSLESS DIRAC FERMIONS:1||SCHOTTKYBARRIER:1||electronic structure:15||ELECTRONICSTRUCTURE:11||TRANSITIONMETAL COMPOUNDS:10||METALS:10||photoemission:8||SPECTRA:8||MAGNETORESISTANCE:7||FERROMAGNETISM:7||TRANSPORT:7||TRANSITION:6||FILMS:6||THINFILMS:5||TOTALENERGY CALCULATIONS:5||MAGNETICPROPERTIES:5||SUPERCONDUCTIVITY:5||PR:5||LATTICE:4||STATES:4||SPECTROSCOPY:4||FIELD:4||CRYSTALSTRUCTURE:4||PHOTOEMISSION:4||TEMPERATURE:4||TRANSITIONTEMPERATURE:4||XRAYABSORPTION:4||STATE:4||CU:4||BASISSET:4||XAS:4||CRYSTALS:3||EXCITATIONS:3||MOTTHUBBARD SYSTEMS:3||HIGHENERGY SPIN:3||halfmetal:3||INSULATORS:3||LA2CUO4:3||MODEL:3||FLUCTUATIONS:3||CE:3||double exchange:3||TRANSITIONMETALS:3||RESISTIVITY:3||BORON:3||LA1XCAXMNO3:3||IRON:3||PES:3||ANTIMONIDES:2||MgB2:2||ZR METALLIC GLASSES:2||superconductor:2||CRITICALCURRENT DENSITY:2||CIRCULARDICHROISM:2||SEMICONDUCTORS:2||LOCALIZATION:2||INTRABAND OPTICAL CONDUCTIVITY:2||COLOSSAL MAGNETORESISTANCE:2||OXIDATION:2||EXISTENCE:2||COPPER:2||diboride:2||MAGNESIUMDIBORIDE:2||GAP:2||CE COMPOUNDS:2||CORE POLARIZATION:2||magnetoresistance:2||photoemission spectroscopy:2||electronphonon interaction:2||GETTER:2||PD:2||MAGNETISM:2||FECR2S4:2||SUPERCONDUCTING MGB2:2||WIRES:2||ABSORPTION:2||ENERGY:2||LA1XSRXMNO3:2||CONSTANTS:2||polaron:2||charge ordering:2||SCATTERING:2||XRAY PHOTOEMISSION:2||CeNiSn:2||phase diagram:2||PHOTOELECTRON:2||QUADRUPOLAR:2||perovskitemanganites:2||CO:2||SYSTEMS:2||DOPED ZNO:2||LOWFREQUENCY SOUND:2||LA:2||ELECTRONELECTRON SCATTERING:2||AU:2||DENSITYWAVE INSTABILITY:2||FERMISURFACE:2||hybridization:2||VALENCEBAND SATELLITE:2||SULFUR SPINEL:2||Heusler:2||APPROXIMATION:2||superexchange:2||colossal magnetoresistance:2||ALLOYS:2||DEPENDENCE:2||AG:2||electronic structures:2||AUGERSPECTRA:2||CR:2||PARAMETERS:2||DIFFRACTION:2||SEMICONDUCTORMETAL TRANSITION:1||INTERMEDIATEVALENCE:1||SMB6:1||SRRUO3:1||antiperovskite structure with antipolar nature:1||lowenergy twodimensional phonons:1||anatase TiO2:1||La3S4:1||metalinsulator transitions:1||MNO:1||ELECTRONICSTRUCTURES:1||MAGNETIC CIRCULARDICHROISM:1||Density functional theory:1||CeCo2:1||TOPOLARON CROSSOVER:1||EXCHANGE:1||cuprates:1||high Tc cuprates:1||magnetically ordered materials:1||ZNSE:1||Sr2xKxFeMoO6:1||CDW:1||TeCuO3:1||STRUCTURALPROPERTIES:1||MN:1||screening length:1||amorphous Fe:1||WAVE BASISSET:1||SILICONCARBIDE:1||HIGHPRESSURE:1||electronphonon coupling:1||quenched superconductivity:1||CMR perovskite manganites:1||OXIDE:1||polarons:1||synchrotron radiation:1||FULLERIDES:1||RESONANTPHOTOEMISSION:1||Silicon carbide:1||DFT calculation:1||Hybridized bands:1||GIANT MAGNETORESISTANCE:1||PEROVSKITES:1||Raman spectra:1||EXCHANGE ENHANCEMENT:1||SILICON:1||SR2FEMOO6:1||orbital ordering:1||delafossite:1||TITANIUMDIOXIDE:1||electronic structure of disordered solids:1||YFE2:1||Magnetic polaron:1||NA2TI2SB2O:1||STRONGCOUPLED SUPERCONDUCTORS:1||HEAVYFERMION SYSTEMS:1||firstprinciples calculations:1||MECHANISM:1||UNiSn:1||PHOTONIC BANDGAP:1||SINGLE IMPURITY:1||PHONONSPECTRUM:1||FERMISURFACE TOPOLOGY:1||SUPPRESSION:1||RESONANT PHOTOEMISSION:1||METALDOPED PICENE:1||PHOTOIONIZATION CROSSSECTIONS:1||PHOTOINDUCED FERRIMAGNETIC SYSTEMS:1||LINKAGE ISOMERISM:1||CHARGETRANSFER:1||Bilayer Graphene:1||MAGNETICFIELD:1||SPINWAVES:1||rareearth manganese oxides:1||magnonphonon interaction:1||NACO2O4:1||ENERGYBANDS:1||SELFENERGY:1||GAS:1||Fe0.5Cu0.5Cr2S4:1||scanning photoelectron microscopy (SPEM):1||MAGNETIC PROPERTIES:1||Stoner model:1||AMORPHOUS TRANSITIONMETALS:1||SPINGLASS STATES:1||NI:1||LA3NI2B2N3:1||SOLIDS:1||CEO2:1||BAND THEORY:1||dilute magnetic semiconductor:1||pyrochlore:1||Y1XPRXBA2CU3O7DELTA:1||and electronphonon interactions:1||VIBRATIONS:1||RAY PHOTOEMISSION:1||ALKALI CATION:1||Europium:1||colossal magnetoresistance:1||structural stability:1||ENERGYGAP:1||small polaron:1||DOUBLE EXCHANGE:1||Coulomb correlation:1||magnon:1||phonons:1||ELECTRON FERROMAGNETISM:1||CURIETEMPERATURE:1||ARPES:1||PLANEWAVE METHOD:1||Xray absorption spectroscopy (XAS):1||ROOMTEMPERATURE:1||MONOCHALCOGENIDES:1||HEAT:1||UPDSN:1||MOMENTS:1||XRAY ABSORPTION:1||SEMICONDUCTOR:1||Fermi surface nesting:1||optical phonon:1||disordered system:1||dilute magnetic semiconductors:1||CMR manganites:1||PHONONS:1||LATTICEDYNAMICS:1||OXIDES:1||4fphotoemission:1||permanent magnet:1||pseudogap:1||TRANSPORTPROPERTIES:1||ANTIFERROMAGNET:1||(BI,PB)SRCOO SYSTEM:1||semicore correlation:1||POLARIZATION:1||CRYSTAL:1||spinel:1||Xray magnetic circular dichroism (XMCD):1||magnetocapacitance:1||ANATASE:1||TEMPERATURES:1||Pseudogap:1||INTERFACE:1||SUBSTRATE:1||YNI2B2C:1||SAMARIUM SULFIDE:1||strong swave superconductor:1||DOPED MANGANITE:1||SYMMETRY:1||CENISN:1||resonance mode:1||DISORDERED SYSTEM:1||LITHIUM INTERCALATION:1||CUO2 PLANE:1||SURFACE:1||Delafossite:1||ELECTRICALPROPERTIES:1||NIMNSB:1||PTMNSB:1||ROOMTEMPERATURE FERROMAGNETISM:1||RUBIDIUM MANGANESE HEXACYANOFERRATE:1||COLOSSALMAGNETORESISTANCE:1||FINITE TEMPERATURES:1||LAMNO3:1||FE:1||transitionmetal oxides:1||giant magnetoresistance:1||phonon:1||COPPER OXIDES:1||valence states:1||thermoelectric:1||semiconductor:1||CATION DISTRIBUTION:1||FeCr2S4:1||photoemission spectroscopy (PES):1||METALLIC FERROMAGNETISM:1||GRAPHITE:1||SUSCEPTIBILITY:1||UBE13:1||RCrSb3:1||band JahnTeller:1||Ce3S4:1||TiO2:1||PrBa2Cu3O7delta:1||UNTWINNED PRBA2CU3O7:1||AGNIO2:1||HALFMETALLIC FERROMAGNETS:1||CI:1||Energy gap:1||Photoemission:1||Future applications:1||Photoemission measurements:1||Graphene:1||BANDSTRUCTURE:1||TC:1||superconductivity:1||magnetic semiconductors:1||CMRmanganites:1||thin films:1||spin dynamics:1||highTc superconductors:1||ITINERANTELECTRON FERROMAGNETISM:1||SINGLECRYSTALS:1||CeTe2:1||amorphous magnetic materials:1||EPITAXIAL GRAPHENE:1||LAYERED PNICTIDEOXIDES:1||BOROCARBIDE SUPERCONDUCTORS:1||AUGMENTEDWAVE METHOD:1||METALLIC MAGNET UNISN:1||ORIGIN:1||spectrum rearrangement:1||MEANFIELD THEORY:1||MOLECULEBASED MAGNETS:1||METASTABLE STATE:1||INSULATOR:1||magnetic orderin:1||FCC IRON:1||CeRu2:1||TL2MN2O7:1||isotope effect:1||Perovskitemanganites:1||RECURSION METHOD:1||PERPENDICULAR MAGNETICANISOTROPY:1||quasiparticle spectral density:1||GW:1||MANGANESE FERRITE:1||RESONANCE:1||SeCuO3:1||Optical conductivity:1||MASSLESS DIRAC FERMIONS:1||SCHOTTKYBARRIER:1||electronic structure:15||ELECTRONICSTRUCTURE:11||TRANSITIONMETAL COMPOUNDS:10||METALS:10||photoemission:8||SPECTRA:8||MAGNETORESISTANCE:7||FERROMAGNETISM:7||TRANSPORT:7||TRANSITION:6||FILMS:6||THINFILMS:5||TOTALENERGY CALCULATIONS:5||MAGNETICPROPERTIES:5||SUPERCONDUCTIVITY:5||PR:5||LATTICE:4||STATES:4||SPECTROSCOPY:4||FIELD:4||CRYSTALSTRUCTURE:4||PHOTOEMISSION:4||TEMPERATURE:4||TRANSITIONTEMPERATURE:4||XRAYABSORPTION:4||STATE:4||CU:4||BASISSET:4||XAS:4||CRYSTALS:3||EXCITATIONS:3||MOTTHUBBARD SYSTEMS:3||HIGHENERGY SPIN:3||halfmetal:3||INSULATORS:3||LA2CUO4:3||MODEL:3||FLUCTUATIONS:3||CE:3||double exchange:3||TRANSITIONMETALS:3||RESISTIVITY:3||BORON:3||LA1XCAXMNO3:3||IRON:3||PES:3||ANTIMONIDES:2||MgB2:2||ZR METALLIC GLASSES:2||superconductor:2||CRITICALCURRENT DENSITY:2||CIRCULARDICHROISM:2||SEMICONDUCTORS:2||LOCALIZATION:2||INTRABAND OPTICAL CONDUCTIVITY:2||COLOSSAL MAGNETORESISTANCE:2||OXIDATION:2||EXISTENCE:2||COPPER:2||diboride:2||MAGNESIUMDIBORIDE:2||GAP:2||CE COMPOUNDS:2||CORE POLARIZATION:2||magnetoresistance:2||photoemission spectroscopy:2||electronphonon interaction:2||GETTER:2||PD:2||MAGNETISM:2||FECR2S4:2||SUPERCONDUCTING MGB2:2||WIRES:2||ABSORPTION:2||ENERGY:2||LA1XSRXMNO3:2||CONSTANTS:2||polaron:2||charge ordering:2||SCATTERING:2||XRAY PHOTOEMISSION:2||CeNiSn:2||phase diagram:2||PHOTOELECTRON:2||QUADRUPOLAR:2||perovskitemanganites:2||CO:2||SYSTEMS:2||DOPED ZNO:2||LOWFREQUENCY SOUND:2||LA:2||ELECTRONELECTRON SCATTERING:2||AU:2||DENSITYWAVE INSTABILITY:2||FERMISURFACE:2||hybridization:2||VALENCEBAND SATELLITE:2||SULFUR SPINEL:2||Heusler:2||APPROXIMATION:2||superexchange:2||colossal magnetoresistance:2||ALLOYS:2||DEPENDENCE:2||AG:2||electronic structures:2||AUGERSPECTRA:2||CR:2||PARAMETERS:2||DIFFRACTION:2||SEMICONDUCTORMETAL TRANSITION:1||INTERMEDIATEVALENCE:1||SMB6:1||SRRUO3:1||antiperovskite structure with antipolar nature:1||lowenergy twodimensional phonons:1||anatase TiO2:1||La3S4:1||metalinsulator transitions:1||MNO:1||ELECTRONICSTRUCTURES:1||MAGNETIC CIRCULARDICHROISM:1||Density functional theory:1||CeCo2:1||TOPOLARON CROSSOVER:1||EXCHANGE:1||cuprates:1||high Tc cuprates:1||magnetically ordered materials:1||ZNSE:1||Sr2xKxFeMoO6:1||CDW:1||TeCuO3:1||STRUCTURALPROPERTIES:1||MN:1||screening length:1||amorphous Fe:1||WAVE BASISSET:1||SILICONCARBIDE:1||HIGHPRESSURE:1||electronphonon coupling:1||quenched superconductivity:1||CMR perovskite manganites:1||OXIDE:1||polarons:1||synchrotron radiation:1||FULLERIDES:1||RESONANTPHOTOEMISSION:1||Silicon carbide:1||DFT calculation:1||Hybridized bands:1||GIANT MAGNETORESISTANCE:1||PEROVSKITES:1||Raman spectra:1||EXCHANGE ENHANCEMENT:1||SILICON:1||SR2FEMOO6:1||orbital ordering:1||delafossite:1||TITANIUMDIOXIDE:1||electronic structure of disordered solids:1||YFE2:1||Magnetic polaron:1||NA2TI2SB2O:1||STRONGCOUPLED SUPERCONDUCTORS:1||HEAVYFERMION SYSTEMS:1||firstprinciples calculations:1||MECHANISM:1||UNiSn:1||PHOTONIC BANDGAP:1||SINGLE IMPURITY:1||PHONONSPECTRUM:1||FERMISURFACE TOPOLOGY:1||SUPPRESSION:1||RESONANT PHOTOEMISSION:1||METALDOPED PICENE:1||PHOTOIONIZATION CROSSSECTIONS:1||PHOTOINDUCED FERRIMAGNETIC SYSTEMS:1||LINKAGE ISOMERISM:1||CHARGETRANSFER:1||Bilayer Graphene:1||MAGNETICFIELD:1||SPINWAVES:1||rareearth manganese oxides:1||magnonphonon interaction:1||NACO2O4:1||ENERGYBANDS:1||SELFENERGY:1||GAS:1||Fe0.5Cu0.5Cr2S4:1||scanning photoelectron microscopy (SPEM):1||MAGNETIC PROPERTIES:1||Stoner model:1||AMORPHOUS TRANSITIONMETALS:1||SPINGLASS STATES:1||NI:1||LA3NI2B2N3:1||SOLIDS:1||CEO2:1||BAND THEORY:1||dilute magnetic semiconductor:1||pyrochlore:1||Y1XPRXBA2CU3O7DELTA:1||and electronphonon interactions:1||VIBRATIONS:1||RAY PHOTOEMISSION:1||ALKALI CATION:1||Europium:1||colossal magnetoresistance:1||structural stability:1||ENERGYGAP:1||small polaron:1||DOUBLE EXCHANGE:1||Coulomb correlation:1||magnon:1||phonons:1||ELECTRON FERROMAGNETISM:1||CURIETEMPERATURE:1||ARPES:1||PLANEWAVE METHOD:1||Xray absorption spectroscopy (XAS):1||ROOMTEMPERATURE:1||MONOCHALCOGENIDES:1||HEAT:1||UPDSN:1||MOMENTS:1||XRAY ABSORPTION:1||SEMICONDUCTOR:1||Fermi surface nesting:1||optical phonon:1||disordered system:1||dilute magnetic semiconductors:1||CMR manganites:1||PHONONS:1||LATTICEDYNAMICS:1||OXIDES:1||4fphotoemission:1||permanent magnet:1||pseudogap:1||TRANSPORTPROPERTIES:1||ANTIFERROMAGNET:1||(BI,PB)SRCOO SYSTEM:1||semicore correlation:1||POLARIZATION:1||CRYSTAL:1||spinel:1||Xray magnetic circular dichroism (XMCD):1||magnetocapacitance:1||ANATASE:1||TEMPERATURES:1||Pseudogap:1||INTERFACE:1||SUBSTRATE:1||YNI2B2C:1||SAMARIUM SULFIDE:1||strong swave superconductor:1||DOPED MANGANITE:1||SYMMETRY:1||CENISN:1||resonance mode:1||DISORDERED SYSTEM:1||LITHIUM INTERCALATION:1||CUO2 PLANE:1||SURFACE:1||Delafossite:1||ELECTRICALPROPERTIES:1||NIMNSB:1||PTMNSB:1||ROOMTEMPERATURE FERROMAGNETISM:1||RUBIDIUM MANGANESE HEXACYANOFERRATE:1||COLOSSALMAGNETORESISTANCE:1||FINITE TEMPERATURES:1||LAMNO3:1||FE:1||transitionmetal oxides:1||giant magnetoresistance:1||phonon:1||COPPER OXIDES:1||valence states:1||thermoelectric:1||semiconductor:1||CATION DISTRIBUTION:1||FeCr2S4:1||photoemission spectroscopy (PES):1||METALLIC FERROMAGNETISM:1||GRAPHITE:1||SUSCEPTIBILITY:1||UBE13:1||RCrSb3:1||band JahnTeller:1||Ce3S4:1||TiO2:1||PrBa2Cu3O7delta:1||UNTWINNED PRBA2CU3O7:1||AGNIO2:1||HALFMETALLIC FERROMAGNETS:1||CI:1||Energy gap:1||Photoemission:1||Future applications:1||Photoemission measurements:1||Graphene:1||BANDSTRUCTURE:1||TC:1||superconductivity:1||magnetic semiconductors:1||CMRmanganites:1||thin films:1||spin dynamics:1||highTc superconductors:1||ITINERANTELECTRON FERROMAGNETISM:1||SINGLECRYSTALS:1||CeTe2:1||amorphous magnetic materials:1||EPITAXIAL GRAPHENE:1||LAYERED PNICTIDEOXIDES:1||BOROCARBIDE SUPERCONDUCTORS:1||AUGMENTEDWAVE METHOD:1||METALLIC MAGNET UNISN:1||ORIGIN:1||spectrum rearrangement:1||MEANFIELD THEORY:1||MOLECULEBASED MAGNETS:1||METASTABLE STATE:1||INSULATOR:1||magnetic orderin:1||FCC IRON:1||CeRu2:1||TL2MN2O7:1||isotope effect:1||Perovskitemanganites:1||RECURSION METHOD:1||PERPENDICULAR MAGNETICANISOTROPY:1||quasiparticle spectral density:1||GW:1||MANGANESE FERRITE:1||RESONANCE:1||SeCuO3:1||Optical conductivity:1||MASSLESS DIRAC FERMIONS:1||SCHOTTKYBARRIER:1||electronic structure:15||ELECTRONICSTRUCTURE:11||TRANSITIONMETAL COMPOUNDS:10||METALS:10||photoemission:8||SPECTRA:8||MAGNETORESISTANCE:7||FERROMAGNETISM:7||TRANSPORT:7||TRANSITION:6||FILMS:6||THINFILMS:5||TOTALENERGY CALCULATIONS:5||MAGNETICPROPERTIES:5||SUPERCONDUCTIVITY:5||PR:5||LATTICE:4||STATES:4||SPECTROSCOPY:4||FIELD:4||CRYSTALSTRUCTURE:4||PHOTOEMISSION:4||TEMPERATURE:4||TRANSITIONTEMPERATURE:4||XRAYABSORPTION:4||STATE:4||CU:4||BASISSET:4||XAS:4||CRYSTALS:3||EXCITATIONS:3||MOTTHUBBARD SYSTEMS:3||HIGHENERGY SPIN:3||halfmetal:3||INSULATORS:3||LA2CUO4:3||MODEL:3||FLUCTUATIONS:3||CE:3||double exchange:3||TRANSITIONMETALS:3||RESISTIVITY:3||BORON:3||LA1XCAXMNO3:3||IRON:3||PES:3||ANTIMONIDES:2||MgB2:2||ZR METALLIC GLASSES:2||superconductor:2||CRITICALCURRENT DENSITY:2||CIRCULARDICHROISM:2||SEMICONDUCTORS:2||LOCALIZATION:2||INTRABAND OPTICAL CONDUCTIVITY:2||COLOSSAL MAGNETORESISTANCE:2||OXIDATION:2||EXISTENCE:2||COPPER:2||diboride:2||MAGNESIUMDIBORIDE:2||GAP:2||CE COMPOUNDS:2||CORE POLARIZATION:2||magnetoresistance:2||photoemission spectroscopy:2||electronphonon interaction:2||GETTER:2||PD:2||MAGNETISM:2||FECR2S4:2||SUPERCONDUCTING MGB2:2||WIRES:2||ABSORPTION:2||ENERGY:2||LA1XSRXMNO3:2||CONSTANTS:2||polaron:2||charge ordering:2||SCATTERING:2||XRAY PHOTOEMISSION:2||CeNiSn:2||phase diagram:2||PHOTOELECTRON:2||QUADRUPOLAR:2||perovskitemanganites:2||CO:2||SYSTEMS:2||DOPED ZNO:2||LOWFREQUENCY SOUND:2||LA:2||ELECTRONELECTRON SCATTERING:2||AU:2||DENSITYWAVE INSTABILITY:2||FERMISURFACE:2||hybridization:2||VALENCEBAND SATELLITE:2||SULFUR SPINEL:2||Heusler:2||APPROXIMATION:2||superexchange:2||colossal magnetoresistance:2||ALLOYS:2||DEPENDENCE:2||AG:2||electronic structures:2||AUGERSPECTRA:2||CR:2||PARAMETERS:2||DIFFRACTION:2||SEMICONDUCTORMETAL TRANSITION:1||INTERMEDIATEVALENCE:1||SMB6:1||SRRUO3:1||antiperovskite structure with antipolar nature:1||lowenergy twodimensional phonons:1||anatase TiO2:1||La3S4:1||metalinsulator transitions:1||MNO:1||ELECTRONICSTRUCTURES:1||MAGNETIC CIRCULARDICHROISM:1||Density functional theory:1||CeCo2:1||TOPOLARON CROSSOVER:1||EXCHANGE:1||cuprates:1||high Tc cuprates:1||magnetically ordered materials:1||ZNSE:1||Sr2xKxFeMoO6:1||CDW:1||TeCuO3:1||STRUCTURALPROPERTIES:1||MN:1||screening length:1||amorphous Fe:1||WAVE BASISSET:1||SILICONCARBIDE:1||HIGHPRESSURE:1||electronphonon coupling:1||quenched superconductivity:1||CMR perovskite manganites:1||OXIDE:1||polarons:1||synchrotron radiation:1||FULLERIDES:1||RESONANTPHOTOEMISSION:1||Silicon carbide:1||DFT calculation:1||Hybridized bands:1||GIANT MAGNETORESISTANCE:1||PEROVSKITES:1||Raman spectra:1||EXCHANGE ENHANCEMENT:1||SILICON:1||SR2FEMOO6:1||orbital ordering:1||delafossite:1||TITANIUMDIOXIDE:1||electronic structure of disordered solids:1||YFE2:1||Magnetic polaron:1||NA2TI2SB2O:1||STRONGCOUPLED SUPERCONDUCTORS:1||HEAVYFERMION SYSTEMS:1||firstprinciples calculations:1||MECHANISM:1||UNiSn:1||PHOTONIC BANDGAP:1||SINGLE IMPURITY:1||PHONONSPECTRUM:1||FERMISURFACE TOPOLOGY:1||SUPPRESSION:1||RESONANT PHOTOEMISSION:1||METALDOPED PICENE:1||PHOTOIONIZATION CROSSSECTIONS:1||PHOTOINDUCED FERRIMAGNETIC SYSTEMS:1||LINKAGE ISOMERISM:1||CHARGETRANSFER:1||Bilayer Graphene:1||MAGNETICFIELD:1||SPINWAVES:1||rareearth manganese oxides:1||magnonphonon interaction:1||NACO2O4:1||ENERGYBANDS:1||SELFENERGY:1||GAS:1||Fe0.5Cu0.5Cr2S4:1||scanning photoelectron microscopy (SPEM):1||MAGNETIC PROPERTIES:1||Stoner model:1||AMORPHOUS TRANSITIONMETALS:1||SPINGLASS STATES:1||NI:1||LA3NI2B2N3:1||SOLIDS:1||CEO2:1||BAND THEORY:1||dilute magnetic semiconductor:1||pyrochlore:1||Y1XPRXBA2CU3O7DELTA:1||and electronphonon interactions:1||VIBRATIONS:1||RAY PHOTOEMISSION:1||ALKALI CATION:1||Europium:1||colossal magnetoresistance:1||structural stability:1||ENERGYGAP:1||small polaron:1||DOUBLE EXCHANGE:1||Coulomb correlation:1||magnon:1||phonons:1||ELECTRON FERROMAGNETISM:1||CURIETEMPERATURE:1||ARPES:1||PLANEWAVE METHOD:1||Xray absorption spectroscopy (XAS):1||ROOMTEMPERATURE:1||MONOCHALCOGENIDES:1||HEAT:1||UPDSN:1||MOMENTS:1||XRAY ABSORPTION:1||SEMICONDUCTOR:1||Fermi surface nesting:1||optical phonon:1||disordered system:1||dilute magnetic semiconductors:1||CMR manganites:1||PHONONS:1||LATTICEDYNAMICS:1||OXIDES:1||4fphotoemission:1||permanent magnet:1||pseudogap:1||TRANSPORTPROPERTIES:1||ANTIFERROMAGNET:1||(BI,PB)SRCOO SYSTEM:1||semicore correlation:1||POLARIZATION:1||CRYSTAL:1||spinel:1||Xray magnetic circular dichroism (XMCD):1||magnetocapacitance:1||ANATASE:1||TEMPERATURES:1||Pseudogap:1||INTERFACE:1||SUBSTRATE:1||YNI2B2C:1||SAMARIUM SULFIDE:1||strong swave superconductor:1||DOPED MANGANITE:1||SYMMETRY:1||CENISN:1||resonance mode:1||DISORDERED SYSTEM:1||LITHIUM INTERCALATION:1||CUO2 PLANE:1||SURFACE:1||Delafossite:1||ELECTRICALPROPERTIES:1||NIMNSB:1||PTMNSB:1||ROOMTEMPERATURE FERROMAGNETISM:1||RUBIDIUM MANGANESE HEXACYANOFERRATE:1||COLOSSALMAGNETORESISTANCE:1||FINITE TEMPERATURES:1||LAMNO3:1||FE:1||transitionmetal oxides:1||giant magnetoresistance:1||phonon:1||COPPER OXIDES:1||valence states:1||thermoelectric:1||semiconductor:1||CATION DISTRIBUTION:1||FeCr2S4:1||photoemission spectroscopy (PES):1||METALLIC FERROMAGNETISM:1||GRAPHITE:1||SUSCEPTIBILITY:1||UBE13:1||RCrSb3:1||band JahnTeller:1||Ce3S4:1||TiO2:1||PrBa2Cu3O7delta:1||UNTWINNED PRBA2CU3O7:1||AGNIO2:1||HALFMETALLIC FERROMAGNETS:1||CI:1||Energy gap:1||Photoemission:1||Future applications:1||Photoemission measurements:1||Graphene:1||BANDSTRUCTURE:1||TC:1||superconductivity:1||magnetic semiconductors:1||CMRmanganites:1||thin films:1||spin dynamics:1||highTc superconductors:1||ITINERANTELECTRON FERROMAGNETISM:1||SINGLECRYSTALS:1||CeTe2:1||amorphous magnetic materials:1||EPITAXIAL GRAPHENE:1||LAYERED PNICTIDEOXIDES:1||BOROCARBIDE SUPERCONDUCTORS:1||AUGMENTEDWAVE METHOD:1||METALLIC MAGNET UNISN:1||ORIGIN:1||spectrum rearrangement:1||MEANFIELD THEORY:1||MOLECULEBASED MAGNETS:1||METASTABLE STATE:1||INSULATOR:1||magnetic orderin:1||FCC IRON:1||CeRu2:1||TL2MN2O7:1||isotope effect:1||Perovskitemanganites:1||RECURSION METHOD:1||PERPENDICULAR MAGNETICANISOTROPY:1||quasiparticle spectral density:1||GW:1||MANGANESE FERRITE:1||RESONANCE:1||SeCuO3:1||Optical conductivity:1||MASSLESS DIRAC FERMIONS:1||SCHOTTKYBARRIER:1||electronic structure:15||ELECTRONICSTRUCTURE:11||TRANSITIONMETAL COMPOUNDS:10||METALS:10||photoemission:8||SPECTRA:8||MAGNETORESISTANCE:7||FERROMAGNETISM:7||TRANSPORT:7||TRANSITION:6||FILMS:6||THINFILMS:5||TOTALENERGY CALCULATIONS:5||MAGNETICPROPERTIES:5||SUPERCONDUCTIVITY:5||PR:5||LATTICE:4||STATES:4||SPECTROSCOPY:4||FIELD:4||CRYSTALSTRUCTURE:4||PHOTOEMISSION:4||TEMPERATURE:4||TRANSITIONTEMPERATURE:4||XRAYABSORPTION:4||STATE:4||CU:4||BASISSET:4||XAS:4||CRYSTALS:3||EXCITATIONS:3||MOTTHUBBARD SYSTEMS:3||HIGHENERGY SPIN:3||halfmetal:3||INSULATORS:3||LA2CUO4:3||MODEL:3||FLUCTUATIONS:3||CE:3||double exchange:3||TRANSITIONMETALS:3||RESISTIVITY:3||BORON:3||LA1XCAXMNO3:3||IRON:3||PES:3||ANTIMONIDES:2||MgB2:2||ZR METALLIC GLASSES:2||superconductor:2||CRITICALCURRENT DENSITY:2||CIRCULARDICHROISM:2||SEMICONDUCTORS:2||LOCALIZATION:2||INTRABAND OPTICAL CONDUCTIVITY:2||COLOSSAL MAGNETORESISTANCE:2||OXIDATION:2||EXISTENCE:2||COPPER:2||diboride:2||MAGNESIUMDIBORIDE:2||GAP:2||CE COMPOUNDS:2||CORE POLARIZATION:2||magnetoresistance:2||photoemission spectroscopy:2||electronphonon interaction:2||GETTER:2||PD:2||MAGNETISM:2||FECR2S4:2||SUPERCONDUCTING MGB2:2||WIRES:2||ABSORPTION:2||ENERGY:2||LA1XSRXMNO3:2||CONSTANTS:2||polaron:2||charge ordering:2||SCATTERING:2||XRAY PHOTOEMISSION:2||CeNiSn:2||phase diagram:2||PHOTOELECTRON:2||QUADRUPOLAR:2||perovskitemanganites:2||CO:2||SYSTEMS:2||DOPED ZNO:2||LOWFREQUENCY SOUND:2||LA:2||ELECTRONELECTRON SCATTERING:2||AU:2||DENSITYWAVE INSTABILITY:2||FERMISURFACE:2||hybridization:2||VALENCEBAND SATELLITE:2||SULFUR SPINEL:2||Heusler:2||APPROXIMATION:2||superexchange:2||colossal magnetoresistance:2||ALLOYS:2||DEPENDENCE:2||AG:2||electronic structures:2||AUGERSPECTRA:2||CR:2||PARAMETERS:2||DIFFRACTION:2||SEMICONDUCTORMETAL TRANSITION:1||INTERMEDIATEVALENCE:1||SMB6:1||SRRUO3:1||antiperovskite structure with antipolar nature:1||lowenergy twodimensional phonons:1||anatase TiO2:1||La3S4:1||metalinsulator transitions:1||MNO:1||ELECTRONICSTRUCTURES:1||MAGNETIC CIRCULARDICHROISM:1||Density functional theory:1||CeCo2:1||TOPOLARON CROSSOVER:1||EXCHANGE:1||cuprates:1||high Tc cuprates:1||magnetically ordered materials:1||ZNSE:1||Sr2xKxFeMoO6:1||CDW:1||TeCuO3:1||STRUCTURALPROPERTIES:1||MN:1||screening length:1||amorphous Fe:1||WAVE BASISSET:1||SILICONCARBIDE:1||HIGHPRESSURE:1||electronphonon coupling:1||quenched superconductivity:1||CMR perovskite manganites:1||OXIDE:1||polarons:1||synchrotron radiation:1||FULLERIDES:1||RESONANTPHOTOEMISSION:1||Silicon carbide:1||DFT calculation:1||Hybridized bands:1||GIANT MAGNETORESISTANCE:1||PEROVSKITES:1||Raman spectra:1||EXCHANGE ENHANCEMENT:1||SILICON:1||SR2FEMOO6:1||orbital ordering:1||delafossite:1||TITANIUMDIOXIDE:1||electronic structure of disordered solids:1||YFE2:1||Magnetic polaron:1||NA2TI2SB2O:1||STRONGCOUPLED SUPERCONDUCTORS:1||HEAVYFERMION SYSTEMS:1||firstprinciples calculations:1||MECHANISM:1||UNiSn:1||PHOTONIC BANDGAP:1||SINGLE IMPURITY:1||PHONONSPECTRUM:1||FERMISURFACE TOPOLOGY:1||SUPPRESSION:1||RESONANT PHOTOEMISSION:1||METALDOPED PICENE:1||PHOTOIONIZATION CROSSSECTIONS:1||PHOTOINDUCED FERRIMAGNETIC SYSTEMS:1||LINKAGE ISOMERISM:1||CHARGETRANSFER:1||Bilayer Graphene:1||MAGNETICFIELD:1||SPINWAVES:1||rareearth manganese oxides:1||magnonphonon interaction:1||NACO2O4:1||ENERGYBANDS:1||SELFENERGY:1||GAS:1||Fe0.5Cu0.5Cr2S4:1||scanning photoelectron microscopy (SPEM):1||MAGNETIC PROPERTIES:1||Stoner model:1||AMORPHOUS TRANSITIONMETALS:1||SPINGLASS STATES:1||NI:1||LA3NI2B2N3:1||SOLIDS:1||CEO2:1||BAND THEORY:1||dilute magnetic semiconductor:1||pyrochlore:1||Y1XPRXBA2CU3O7DELTA:1||and electronphonon interactions:1||VIBRATIONS:1||RAY PHOTOEMISSION:1||ALKALI CATION:1||Europium:1||colossal magnetoresistance:1||structural stability:1||ENERGYGAP:1||small polaron:1||DOUBLE EXCHANGE:1||Coulomb correlation:1||magnon:1||phonons:1||ELECTRON FERROMAGNETISM:1||CURIETEMPERATURE:1||ARPES:1||PLANEWAVE METHOD:1||Xray absorption spectroscopy (XAS):1||ROOMTEMPERATURE:1||MONOCHALCOGENIDES:1||HEAT:1||UPDSN:1||MOMENTS:1||XRAY ABSORPTION:1||SEMICONDUCTOR:1||Fermi surface nesting:1||optical phonon:1||disordered system:1||dilute magnetic semiconductors:1||CMR manganites:1||PHONONS:1||LATTICEDYNAMICS:1||OXIDES:1||4fphotoemission:1||permanent magnet:1||pseudogap:1||TRANSPORTPROPERTIES:1||ANTIFERROMAGNET:1||(BI,PB)SRCOO SYSTEM:1||semicore correlation:1||POLARIZATION:1||CRYSTAL:1||spinel:1||Xray magnetic circular dichroism (XMCD):1||magnetocapacitance:1||ANATASE:1||TEMPERATURES:1||Pseudogap:1||INTERFACE:1||SUBSTRATE:1||YNI2B2C:1||SAMARIUM SULFIDE:1||strong swave superconductor:1||DOPED MANGANITE:1||SYMMETRY:1||CENISN:1||resonance mode:1||DISORDERED SYSTEM:1||LITHIUM INTERCALATION:1||CUO2 PLANE:1||SURFACE:1||Delafossite:1||ELECTRICALPROPERTIES:1||NIMNSB:1||PTMNSB:1||ROOMTEMPERATURE FERROMAGNETISM:1||RUBIDIUM MANGANESE HEXACYANOFERRATE:1||COLOSSALMAGNETORESISTANCE:1||FINITE TEMPERATURES:1||LAMNO3:1||FE:1||transitionmetal oxides:1||giant magnetoresistance:1||phonon:1||COPPER OXIDES:1||valence states:1||thermoelectric:1||semiconductor:1||CATION DISTRIBUTION:1||FeCr2S4:1||photoemission spectroscopy (PES):1||METALLIC FERROMAGNETISM:1||GRAPHITE:1||SUSCEPTIBILITY:1||UBE13:1||RCrSb3:1||band JahnTeller:1||Ce3S4:1||TiO2:1||PrBa2Cu3O7delta:1||UNTWINNED PRBA2CU3O7:1||AGNIO2:1||HALFMETALLIC FERROMAGNETS:1||CI:1||Energy gap:1||Photoemission:1||Future applications:1||Photoemission measurements:1||Graphene:1||BANDSTRUCTURE:1||TC:1||superconductivity:1||magnetic semiconductors:1||CMRmanganites:1||thin films:1||spin dynamics:1||highTc superconductors:1||ITINERANTELECTRON FERROMAGNETISM:1||SINGLECRYSTALS:1||CeTe2:1||amorphous magnetic materials:1||EPITAXIAL GRAPHENE:1||LAYERED PNICTIDEOXIDES:1||BOROCARBIDE SUPERCONDUCTORS:1||AUGMENTEDWAVE METHOD:1||METALLIC MAGNET UNISN:1||ORIGIN:1||spectrum rearrangement:1||MEANFIELD THEORY:1||MOLECULEBASED MAGNETS:1||METASTABLE STATE:1||INSULATOR:1||magnetic orderin:1||FCC IRON:1||CeRu2:1||TL2MN2O7:1||isotope effect:1||Perovskitemanganites:1||RECURSION METHOD:1||PERPENDICULAR MAGNETICANISOTROPY:1||quasiparticle spectral density:1||GW:1||MANGANESE FERRITE:1||RESONANCE:1||SeCuO3:1||Optical conductivity:1||MASSLESS DIRAC FERMIONS:1||SCHOTTKYBARRIER:1||electronic structure:15||ELECTRONICSTRUCTURE:11||TRANSITIONMETAL COMPOUNDS:10||METALS:10||photoemission:8||SPECTRA:8||MAGNETORESISTANCE:7||FERROMAGNETISM:7||TRANSPORT:7||TRANSITION:6||FILMS:6||THINFILMS:5||TOTALENERGY CALCULATIONS:5||MAGNETICPROPERTIES:5||SUPERCONDUCTIVITY:5||PR:5||LATTICE:4||STATES:4||SPECTROSCOPY:4||FIELD:4||CRYSTALSTRUCTURE:4||PHOTOEMISSION:4||TEMPERATURE:4||TRANSITIONTEMPERATURE:4||XRAYABSORPTION:4||STATE:4||CU:4||BASISSET:4||XAS:4||CRYSTALS:3||EXCITATIONS:3||MOTTHUBBARD SYSTEMS:3||HIGHENERGY SPIN:3||halfmetal:3||INSULATORS:3||LA2CUO4:3||MODEL:3||FLUCTUATIONS:3||CE:3||double exchange:3||TRANSITIONMETALS:3||RESISTIVITY:3||BORON:3||LA1XCAXMNO3:3||IRON:3||PES:3||ANTIMONIDES:2||MgB2:2||ZR METALLIC GLASSES:2||superconductor:2||CRITICALCURRENT DENSITY:2||CIRCULARDICHROISM:2||SEMICONDUCTORS:2||LOCALIZATION:2||INTRABAND OPTICAL CONDUCTIVITY:2||COLOSSAL MAGNETORESISTANCE:2||OXIDATION:2||EXISTENCE:2||COPPER:2||diboride:2||MAGNESIUMDIBORIDE:2||GAP:2||CE COMPOUNDS:2||CORE POLARIZATION:2||magnetoresistance:2||photoemission spectroscopy:2||electronphonon interaction:2||GETTER:2||PD:2||MAGNETISM:2||FECR2S4:2||SUPERCONDUCTING MGB2:2||WIRES:2||ABSORPTION:2||ENERGY:2||LA1XSRXMNO3:2||CONSTANTS:2||polaron:2||charge ordering:2||SCATTERING:2||XRAY PHOTOEMISSION:2||CeNiSn:2||phase diagram:2||PHOTOELECTRON:2||QUADRUPOLAR:2||perovskitemanganites:2||CO:2||SYSTEMS:2||DOPED ZNO:2||LOWFREQUENCY SOUND:2||LA:2||ELECTRONELECTRON SCATTERING:2||AU:2||DENSITYWAVE INSTABILITY:2||FERMISURFACE:2||hybridization:2||VALENCEBAND SATELLITE:2||SULFUR SPINEL:2||Heusler:2||APPROXIMATION:2||superexchange:2||colossal magnetoresistance:2||ALLOYS:2||DEPENDENCE:2||AG:2||electronic structures:2||AUGERSPECTRA:2||CR:2||PARAMETERS:2||DIFFRACTION:2||SEMICONDUCTORMETAL TRANSITION:1||INTERMEDIATEVALENCE:1||SMB6:1||SRRUO3:1||antiperovskite structure with antipolar nature:1||lowenergy twodimensional phonons:1||anatase TiO2:1||La3S4:1||metalinsulator transitions:1||MNO:1||ELECTRONICSTRUCTURES:1||MAGNETIC CIRCULARDICHROISM:1||Density functional theory:1||CeCo2:1||TOPOLARON CROSSOVER:1||EXCHANGE:1||cuprates:1||high Tc cuprates:1||magnetically ordered materials:1||ZNSE:1||Sr2xKxFeMoO6:1||CDW:1||TeCuO3:1||STRUCTURALPROPERTIES:1||MN:1||screening length:1||amorphous Fe:1||WAVE BASISSET:1||SILICONCARBIDE:1||HIGHPRESSURE:1||electronphonon coupling:1||quenched superconductivity:1||CMR perovskite manganites:1||OXIDE:1||polarons:1||synchrotron radiation:1||FULLERIDES:1||RESONANTPHOTOEMISSION:1||Silicon carbide:1||DFT calculation:1||Hybridized bands:1||GIANT MAGNETORESISTANCE:1||PEROVSKITES:1||Raman spectra:1||EXCHANGE ENHANCEMENT:1||SILICON:1||SR2FEMOO6:1||orbital ordering:1||delafossite:1||TITANIUMDIOXIDE:1||electronic structure of disordered solids:1||YFE2:1||Magnetic polaron:1||NA2TI2SB2O:1||STRONGCOUPLED SUPERCONDUCTORS:1||HEAVYFERMION SYSTEMS:1||firstprinciples calculations:1||MECHANISM:1||UNiSn:1||PHOTONIC BANDGAP:1||SINGLE IMPURITY:1||PHONONSPECTRUM:1||FERMISURFACE TOPOLOGY:1||SUPPRESSION:1||RESONANT PHOTOEMISSION:1||METALDOPED PICENE:1||PHOTOIONIZATION CROSSSECTIONS:1||PHOTOINDUCED FERRIMAGNETIC SYSTEMS:1||LINKAGE ISOMERISM:1||CHARGETRANSFER:1||Bilayer Graphene:1||MAGNETICFIELD:1||SPINWAVES:1||rareearth manganese oxides:1||magnonphonon interaction:1||NACO2O4:1||ENERGYBANDS:1||SELFENERGY:1||GAS:1||Fe0.5Cu0.5Cr2S4:1||scanning photoelectron microscopy (SPEM):1||MAGNETIC PROPERTIES:1||Stoner model:1||AMORPHOUS TRANSITIONMETALS:1||SPINGLASS STATES:1||NI:1||LA3NI2B2N3:1||SOLIDS:1||CEO2:1||BAND THEORY:1||dilute magnetic semiconductor:1||pyrochlore:1||Y1XPRXBA2CU3O7DELTA:1||and electronphonon interactions:1||VIBRATIONS:1||RAY PHOTOEMISSION:1||ALKALI CATION:1||Europium:1||colossal magnetoresistance:1||structural stability:1||ENERGYGAP:1||small polaron:1||DOUBLE EXCHANGE:1||Coulomb correlation:1||magnon:1||phonons:1||ELECTRON FERROMAGNETISM:1||CURIETEMPERATURE:1||ARPES:1||PLANEWAVE METHOD:1||Xray absorption spectroscopy (XAS):1||ROOMTEMPERATURE:1||MONOCHALCOGENIDES:1||HEAT:1||UPDSN:1||MOMENTS:1||XRAY ABSORPTION:1||SEMICONDUCTOR:1||Fermi surface nesting:1||optical phonon:1||disordered system:1||dilute magnetic semiconductors:1||CMR manganites:1||PHONONS:1||LATTICEDYNAMICS:1||OXIDES:1||4fphotoemission:1||permanent magnet:1||pseudogap:1||TRANSPORTPROPERTIES:1||ANTIFERROMAGNET:1||(BI,PB)SRCOO SYSTEM:1||semicore correlation:1||POLARIZATION:1||CRYSTAL:1||spinel:1||Xray magnetic circular dichroism (XMCD):1||magnetocapacitance:1||ANATASE:1||TEMPERATURES:1||Pseudogap:1||INTERFACE:1||SUBSTRATE:1||YNI2B2C:1||SAMARIUM SULFIDE:1||strong swave superconductor:1||DOPED MANGANITE:1||SYMMETRY:1||CENISN:1||resonance mode:1||DISORDERED SYSTEM:1||LITHIUM INTERCALATION:1||CUO2 PLANE:1||SURFACE:1||Delafossite:1||ELECTRICALPROPERTIES:1||NIMNSB:1||PTMNSB:1||ROOMTEMPERATURE FERROMAGNETISM:1||RUBIDIUM MANGANESE HEXACYANOFERRATE:1||COLOSSALMAGNETORESISTANCE:1||FINITE TEMPERATURES:1||LAMNO3:1||FE:1||transitionmetal oxides:1||giant magnetoresistance:1||phonon:1||COPPER OXIDES:1||valence states:1||thermoelectric:1||semiconductor:1||CATION DISTRIBUTION:1||FeCr2S4:1||photoemission spectroscopy (PES):1||METALLIC FERROMAGNETISM:1||GRAPHITE:1||SUSCEPTIBILITY:1||UBE13:1||RCrSb3:1||band JahnTeller:1||Ce3S4:1||TiO2:1||PrBa2Cu3O7delta:1||UNTWINNED PRBA2CU3O7:1||AGNIO2:1||HALFMETALLIC FERROMAGNETS:1||CI:1||Energy gap:1||Photoemission:1||Future applications:1||Photoemission measurements:1||Graphene:1||BANDSTRUCTURE:1||TC:1||superconductivity:1||magnetic semiconductors:1||CMRmanganites:1||thin films:1||spin dynamics:1||highTc superconductors:1||ITINERANTELECTRON FERROMAGNETISM:1||SINGLECRYSTALS:1||CeTe2:1||amorphous magnetic materials:1||EPITAXIAL GRAPHENE:1||LAYERED PNICTIDEOXIDES:1||BOROCARBIDE SUPERCONDUCTORS:1||AUGMENTEDWAVE METHOD:1||METALLIC MAGNET UNISN:1||ORIGIN:1||spectrum rearrangement:1||MEANFIELD THEORY:1||MOLECULEBASED MAGNETS:1||METASTABLE STATE:1||INSULATOR:1||magnetic orderin:1||FCC IRON:1||CeRu2:1||TL2MN2O7:1||isotope effect:1||Perovskitemanganites:1||RECURSION METHOD:1||PERPENDICULAR MAGNETICANISOTROPY:1||quasiparticle spectral density:1||GW:1||MANGANESE FERRITE:1||RESONANCE:1||SeCuO3:1||Optical conductivity:1||MASSLESS DIRAC FERMIONS:1||SCHOTTKYBARRIER:1||electronic structure:15||ELECTRONICSTRUCTURE:11||TRANSITIONMETAL COMPOUNDS:10||METALS:10||photoemission:8||SPECTRA:8||MAGNETORESISTANCE:7||FERROMAGNETISM:7||TRANSPORT:7||TRANSITION:6||FILMS:6||THINFILMS:5||TOTALENERGY CALCULATIONS:5||MAGNETICPROPERTIES:5||SUPERCONDUCTIVITY:5||PR:5||LATTICE:4||STATES:4||SPECTROSCOPY:4||FIELD:4||CRYSTALSTRUCTURE:4||PHOTOEMISSION:4||TEMPERATURE:4||TRANSITIONTEMPERATURE:4||XRAYABSORPTION:4||STATE:4||CU:4||BASISSET:4||XAS:4||CRYSTALS:3||EXCITATIONS:3||MOTTHUBBARD SYSTEMS:3||HIGHENERGY SPIN:3||halfmetal:3||INSULATORS:3||LA2CUO4:3||MODEL:3||FLUCTUATIONS:3||CE:3||double exchange:3||TRANSITIONMETALS:3||RESISTIVITY:3||BORON:3||LA1XCAXMNO3:3||IRON:3||PES:3||ANTIMONIDES:2||MgB2:2||ZR METALLIC GLASSES:2||superconductor:2||CRITICALCURRENT DENSITY:2||CIRCULARDICHROISM:2||SEMICONDUCTORS:2||LOCALIZATION:2||INTRABAND OPTICAL CONDUCTIVITY:2||COLOSSAL MAGNETORESISTANCE:2||OXIDATION:2||EXISTENCE:2||COPPER:2||diboride:2||MAGNESIUMDIBORIDE:2||GAP:2||CE COMPOUNDS:2||CORE POLARIZATION:2||magnetoresistance:2||photoemission spectroscopy:2||electronphonon interaction:2||GETTER:2||PD:2||MAGNETISM:2||FECR2S4:2||SUPERCONDUCTING MGB2:2||WIRES:2||ABSORPTION:2||ENERGY:2||LA1XSRXMNO3:2||CONSTANTS:2||polaron:2||charge ordering:2||SCATTERING:2||XRAY PHOTOEMISSION:2||CeNiSn:2||phase diagram:2||PHOTOELECTRON:2||QUADRUPOLAR:2||perovskitemanganites:2||CO:2||SYSTEMS:2||DOPED ZNO:2||LOWFREQUENCY SOUND:2||LA:2||ELECTRONELECTRON SCATTERING:2||AU:2||DENSITYWAVE INSTABILITY:2||FERMISURFACE:2||hybridization:2||VALENCEBAND SATELLITE:2||SULFUR SPINEL:2||Heusler:2||APPROXIMATION:2||superexchange:2||colossal magnetoresistance:2||ALLOYS:2||DEPENDENCE:2||AG:2||electronic structures:2||AUGERSPECTRA:2||CR:2||PARAMETERS:2||DIFFRACTION:2||SEMICONDUCTORMETAL TRANSITION:1||INTERMEDIATEVALENCE:1||SMB6:1||SRRUO3:1||antiperovskite structure with antipolar nature:1||lowenergy twodimensional phonons:1||anatase TiO2:1||La3S4:1||metalinsulator transitions:1||MNO:1||ELECTRONICSTRUCTURES:1||MAGNETIC CIRCULARDICHROISM:1||Density functional theory:1||CeCo2:1||TOPOLARON CROSSOVER:1||EXCHANGE:1||cuprates:1||high Tc cuprates:1||magnetically ordered materials:1||ZNSE:1||Sr2xKxFeMoO6:1||CDW:1||TeCuO3:1||STRUCTURALPROPERTIES:1||MN:1||screening length:1||amorphous Fe:1||WAVE BASISSET:1||SILICONCARBIDE:1||HIGHPRESSURE:1||electronphonon coupling:1||quenched superconductivity:1||CMR perovskite manganites:1||OXIDE:1||polarons:1||synchrotron radiation:1||FULLERIDES:1||RESONANTPHOTOEMISSION:1||Silicon carbide:1||DFT calculation:1||Hybridized bands:1||GIANT MAGNETORESISTANCE:1||PEROVSKITES:1||Raman spectra:1||EXCHANGE ENHANCEMENT:1||SILICON:1||SR2FEMOO6:1||orbital ordering:1||delafossite:1||TITANIUMDIOXIDE:1||electronic structure of disordered solids:1||YFE2:1||Magnetic polaron:1||NA2TI2SB2O:1||STRONGCOUPLED SUPERCONDUCTORS:1||HEAVYFERMION SYSTEMS:1||firstprinciples calculations:1||MECHANISM:1||UNiSn:1||PHOTONIC BANDGAP:1||SINGLE IMPURITY:1||PHONONSPECTRUM:1||FERMISURFACE TOPOLOGY:1||SUPPRESSION:1||RESONANT PHOTOEMISSION:1||METALDOPED PICENE:1||PHOTOIONIZATION CROSSSECTIONS:1||PHOTOINDUCED FERRIMAGNETIC SYSTEMS:1||LINKAGE ISOMERISM:1||CHARGETRANSFER:1||Bilayer Graphene:1||MAGNETICFIELD:1||SPINWAVES:1||rareearth manganese oxides:1||magnonphonon interaction:1||NACO2O4:1||ENERGYBANDS:1||SELFENERGY:1||GAS:1||Fe0.5Cu0.5Cr2S4:1||scanning photoelectron microscopy (SPEM):1||MAGNETIC PROPERTIES:1||Stoner model:1||AMORPHOUS TRANSITIONMETALS:1||SPINGLASS STATES:1||NI:1||LA3NI2B2N3:1||SOLIDS:1||CEO2:1||BAND THEORY:1||dilute magnetic semiconductor:1||pyrochlore:1||Y1XPRXBA2CU3O7DELTA:1||and electronphonon interactions:1||VIBRATIONS:1||RAY PHOTOEMISSION:1||ALKALI CATION:1||Europium:1||colossal magnetoresistance:1||structural stability:1||ENERGYGAP:1||small polaron:1||DOUBLE EXCHANGE:1||Coulomb correlation:1||magnon:1||phonons:1||ELECTRON FERROMAGNETISM:1||CURIETEMPERATURE:1||ARPES:1||PLANEWAVE METHOD:1||Xray absorption spectroscopy (XAS):1||ROOMTEMPERATURE:1||MONOCHALCOGENIDES:1||HEAT:1||UPDSN:1||MOMENTS:1||XRAY ABSORPTION:1||SEMICONDUCTOR:1||Fermi surface nesting:1||optical phonon:1||disordered system:1||dilute magnetic semiconductors:1||CMR manganites:1||PHONONS:1||LATTICEDYNAMICS:1||OXIDES:1||4fphotoemission:1||permanent magnet:1||pseudogap:1||TRANSPORTPROPERTIES:1||ANTIFERROMAGNET:1||(BI,PB)SRCOO SYSTEM:1||semicore correlation:1||POLARIZATION:1||CRYSTAL:1||spinel:1||Xray magnetic circular dichroism (XMCD):1||magnetocapacitance:1||ANATASE:1||TEMPERATURES:1||Pseudogap:1||INTERFACE:1||SUBSTRATE:1||YNI2B2C:1||SAMARIUM SULFIDE:1||strong swave superconductor:1||DOPED MANGANITE:1||SYMMETRY:1||CENISN:1||resonance mode:1||DISORDERED SYSTEM:1||LITHIUM INTERCALATION:1||CUO2 PLANE:1||SURFACE:1||Delafossite:1||ELECTRICALPROPERTIES:1||NIMNSB:1||PTMNSB:1||ROOMTEMPERATURE FERROMAGNETISM:1||RUBIDIUM MANGANESE HEXACYANOFERRATE:1||COLOSSALMAGNETORESISTANCE:1||FINITE TEMPERATURES:1||LAMNO3:1||FE:1||transitionmetal oxides:1||giant magnetoresistance:1||phonon:1||COPPER OXIDES:1||valence states:1||thermoelectric:1||semiconductor:1||CATION DISTRIBUTION:1||FeCr2S4:1||photoemission spectroscopy (PES):1||METALLIC FERROMAGNETISM:1||GRAPHITE:1||SUSCEPTIBILITY:1||UBE13:1||RCrSb3:1||band JahnTeller:1||Ce3S4:1||TiO2:1||PrBa2Cu3O7delta:1||UNTWINNED PRBA2CU3O7:1||AGNIO2:1||HALFMETALLIC FERROMAGNETS:1||CI:1||Energy gap:1||Photoemission:1||Future applications:1||Photoemission measurements:1||Graphene:1||BANDSTRUCTURE:1||TC:1||superconductivity:1||magnetic semiconductors:1||CMRmanganites:1||thin films:1||spin dynamics:1||highTc superconductors:1||ITINERANTELECTRON FERROMAGNETISM:1||SINGLECRYSTALS:1||CeTe2:1||amorphous magnetic materials:1||EPITAXIAL GRAPHENE:1||LAYERED PNICTIDEOXIDES:1||BOROCARBIDE SUPERCONDUCTORS:1||AUGMENTEDWAVE METHOD:1||METALLIC MAGNET UNISN:1||ORIGIN:1||spectrum rearrangement:1||MEANFIELD THEORY:1||MOLECULEBASED MAGNETS:1||METASTABLE STATE:1||INSULATOR:1||magnetic orderin:1||FCC IRON:1||CeRu2:1||TL2MN2O7:1||isotope effect:1||Perovskitemanganites:1||RECURSION METHOD:1||PERPENDICULAR MAGNETICANISOTROPY:1||quasiparticle spectral density:1||GW:1||MANGANESE FERRITE:1||RESONANCE:1||SeCuO3:1||Optical conductivity:1||MASSLESS DIRAC FERMIONS:1||SCHOTTKYBARRIER:1||electronic structure:15||ELECTRONICSTRUCTURE:11||TRANSITIONMETAL COMPOUNDS:10||METALS:10||photoemission:8||SPECTRA:8||MAGNETORESISTANCE:7||FERROMAGNETISM:7||TRANSPORT:7||TRANSITION:6||FILMS:6||THINFILMS:5||TOTALENERGY CALCULATIONS:5||MAGNETICPROPERTIES:5||SUPERCONDUCTIVITY:5||PR:5||LATTICE:4||STATES:4||SPECTROSCOPY:4||FIELD:4||CRYSTALSTRUCTURE:4||PHOTOEMISSION:4||TEMPERATURE:4||TRANSITIONTEMPERATURE:4||XRAYABSORPTION:4||STATE:4||CU:4||BASISSET:4||XAS:4||CRYSTALS:3||EXCITATIONS:3||MOTTHUBBARD SYSTEMS:3||HIGHENERGY SPIN:3||halfmetal:3||INSULATORS:3||LA2CUO4:3||MODEL:3||FLUCTUATIONS:3||CE:3||double exchange:3||TRANSITIONMETALS:3||RESISTIVITY:3||BORON:3||LA1XCAXMNO3:3||IRON:3||PES:3||ANTIMONIDES:2||MgB2:2||ZR METALLIC GLASSES:2||superconductor:2||CRITICALCURRENT DENSITY:2||CIRCULARDICHROISM:2||SEMICONDUCTORS:2||LOCALIZATION:2||INTRABAND OPTICAL CONDUCTIVITY:2||COLOSSAL MAGNETORESISTANCE:2||OXIDATION:2||EXISTENCE:2||COPPER:2||diboride:2||MAGNESIUMDIBORIDE:2||GAP:2||CE COMPOUNDS:2||CORE POLARIZATION:2||magnetoresistance:2||photoemission spectroscopy:2||electronphonon interaction:2||GETTER:2||PD:2||MAGNETISM:2||FECR2S4:2||SUPERCONDUCTING MGB2:2||WIRES:2||ABSORPTION:2||ENERGY:2||LA1XSRXMNO3:2||CONSTANTS:2||polaron:2||charge ordering:2||SCATTERING:2||XRAY PHOTOEMISSION:2||CeNiSn:2||phase diagram:2||PHOTOELECTRON:2||QUADRUPOLAR:2||perovskitemanganites:2||CO:2||SYSTEMS:2||DOPED ZNO:2||LOWFREQUENCY SOUND:2||LA:2||ELECTRONELECTRON SCATTERING:2||AU:2||DENSITYWAVE INSTABILITY:2||FERMISURFACE:2||hybridization:2||VALENCEBAND SATELLITE:2||SULFUR SPINEL:2||Heusler:2||APPROXIMATION:2||superexchange:2||colossal magnetoresistance:2||ALLOYS:2||DEPENDENCE:2||AG:2||electronic structures:2||AUGERSPECTRA:2||CR:2||PARAMETERS:2||DIFFRACTION:2||SEMICONDUCTORMETAL TRANSITION:1||INTERMEDIATEVALENCE:1||SMB6:1||SRRUO3:1||antiperovskite structure with antipolar nature:1||lowenergy twodimensional phonons:1||anatase TiO2:1||La3S4:1||metalinsulator transitions:1||MNO:1||ELECTRONICSTRUCTURES:1||MAGNETIC CIRCULARDICHROISM:1||Density functional theory:1||CeCo2:1||TOPOLARON CROSSOVER:1||EXCHANGE:1||cuprates:1||high Tc cuprates:1||magnetically ordered materials:1||ZNSE:1||Sr2xKxFeMoO6:1||CDW:1||TeCuO3:1||STRUCTURALPROPERTIES:1||MN:1||screening length:1||amorphous Fe:1||WAVE BASISSET:1||SILICONCARBIDE:1||HIGHPRESSURE:1||electronphonon coupling:1||quenched superconductivity:1||CMR perovskite manganites:1||OXIDE:1||polarons:1||synchrotron radiation:1||FULLERIDES:1||RESONANTPHOTOEMISSION:1||Silicon carbide:1||DFT calculation:1||Hybridized bands:1||GIANT MAGNETORESISTANCE:1||PEROVSKITES:1||Raman spectra:1||EXCHANGE ENHANCEMENT:1||SILICON:1||SR2FEMOO6:1||orbital ordering:1||delafossite:1||TITANIUMDIOXIDE:1||electronic structure of disordered solids:1||YFE2:1||Magnetic polaron:1||NA2TI2SB2O:1||STRONGCOUPLED SUPERCONDUCTORS:1||HEAVYFERMION SYSTEMS:1||firstprinciples calculations:1||MECHANISM:1||UNiSn:1||PHOTONIC BANDGAP:1||SINGLE IMPURITY:1||PHONONSPECTRUM:1||FERMISURFACE TOPOLOGY:1||SUPPRESSION:1||RESONANT PHOTOEMISSION:1||METALDOPED PICENE:1||PHOTOIONIZATION CROSSSECTIONS:1||PHOTOINDUCED FERRIMAGNETIC SYSTEMS:1||LINKAGE ISOMERISM:1||CHARGETRANSFER:1||Bilayer Graphene:1||MAGNETICFIELD:1||SPINWAVES:1||rareearth manganese oxides:1||magnonphonon interaction:1||NACO2O4:1||ENERGYBANDS:1||SELFENERGY:1||GAS:1||Fe0.5Cu0.5Cr2S4:1||scanning photoelectron microscopy (SPEM):1||MAGNETIC PROPERTIES:1||Stoner model:1||AMORPHOUS TRANSITIONMETALS:1||SPINGLASS STATES:1||NI:1||LA3NI2B2N3:1||SOLIDS:1||CEO2:1||BAND THEORY:1||dilute magnetic semiconductor:1||pyrochlore:1||Y1XPRXBA2CU3O7DELTA:1||and electronphonon interactions:1||VIBRATIONS:1||RAY PHOTOEMISSION:1||ALKALI CATION:1||Europium:1||colossal magnetoresistance:1||structural stability:1||ENERGYGAP:1||small polaron:1||DOUBLE EXCHANGE:1||Coulomb correlation:1||magnon:1||phonons:1||ELECTRON FERROMAGNETISM:1||CURIETEMPERATURE:1||ARPES:1||PLANEWAVE METHOD:1||Xray absorption spectroscopy (XAS):1||ROOMTEMPERATURE:1||MONOCHALCOGENIDES:1||HEAT:1||UPDSN:1||MOMENTS:1||XRAY ABSORPTION:1||SEMICONDUCTOR:1||Fermi surface nesting:1||optical phonon:1||disordered system:1||dilute magnetic semiconductors:1||CMR manganites:1||PHONONS:1||LATTICEDYNAMICS:1||OXIDES:1||4fphotoemission:1||permanent magnet:1||pseudogap:1||TRANSPORTPROPERTIES:1||ANTIFERROMAGNET:1||(BI,PB)SRCOO SYSTEM:1||semicore correlation:1||POLARIZATION:1||CRYSTAL:1||spinel:1||Xray magnetic circular dichroism (XMCD):1||magnetocapacitance:1||ANATASE:1||TEMPERATURES:1||Pseudogap:1||INTERFACE:1||SUBSTRATE:1||YNI2B2C:1||SAMARIUM SULFIDE:1||strong swave superconductor:1||DOPED MANGANITE:1||SYMMETRY:1||CENISN:1||resonance mode:1||DISORDERED SYSTEM:1||LITHIUM INTERCALATION:1||CUO2 PLANE:1||SURFACE:1||Delafossite:1||ELECTRICALPROPERTIES:1||NIMNSB:1||PTMNSB:1||ROOMTEMPERATURE FERROMAGNETISM:1||RUBIDIUM MANGANESE HEXACYANOFERRATE:1||COLOSSALMAGNETORESISTANCE:1||FINITE TEMPERATURES:1||LAMNO3:1||FE:1||transitionmetal oxides:1||giant magnetoresistance:1||phonon:1||COPPER OXIDES:1||valence states:1||thermoelectric:1||semiconductor:1||CATION DISTRIBUTION:1||FeCr2S4:1||photoemission spectroscopy (PES):1||METALLIC FERROMAGNETISM:1||GRAPHITE:1||SUSCEPTIBILITY:1||UBE13:1||RCrSb3:1||band JahnTeller:1||Ce3S4:1||TiO2:1||PrBa2Cu3O7delta:1||UNTWINNED PRBA2CU3O7:1||AGNIO2:1||HALFMETALLIC FERROMAGNETS:1||CI:1||Energy gap:1||Photoemission:1||Future applications:1||Photoemission measurements:1||Graphene:1||BANDSTRUCTURE:1||TC:1||superconductivity:1||magnetic semiconductors:1||CMRmanganites:1||thin films:1||spin dynamics:1||highTc superconductors:1||ITINERANTELECTRON FERROMAGNETISM:1||SINGLECRYSTALS:1||CeTe2:1||amorphous magnetic materials:1||EPITAXIAL GRAPHENE:1||LAYERED PNICTIDEOXIDES:1||BOROCARBIDE SUPERCONDUCTORS:1||AUGMENTEDWAVE METHOD:1||METALLIC MAGNET UNISN:1||ORIGIN:1||spectrum rearrangement:1||MEANFIELD THEORY:1||MOLECULEBASED MAGNETS:1||METASTABLE STATE:1||INSULATOR:1||magnetic orderin:1||FCC IRON:1||CeRu2:1||TL2MN2O7:1||isotope effect:1||Perovskitemanganites:1||RECURSION METHOD:1||PERPENDICULAR MAGNETICANISOTROPY:1||quasiparticle spectral density:1||GW:1||MANGANESE FERRITE:1||RESONANCE:1||SeCuO3:1||Optical conductivity:1||MASSLESS DIRAC FERMIONS:1||SCHOTTKYBARRIER:1||electronic structure:15||ELECTRONICSTRUCTURE:11||TRANSITIONMETAL COMPOUNDS:10||METALS:10||photoemission:8||SPECTRA:8||MAGNETORESISTANCE:7||FERROMAGNETISM:7||TRANSPORT:7||TRANSITION:6||FILMS:6||THINFILMS:5||TOTALENERGY CALCULATIONS:5||MAGNETICPROPERTIES:5||SUPERCONDUCTIVITY:5||PR:5||LATTICE:4||STATES:4||SPECTROSCOPY:4||FIELD:4||CRYSTALSTRUCTURE:4||PHOTOEMISSION:4||TEMPERATURE:4||TRANSITIONTEMPERATURE:4||XRAYABSORPTION:4||STATE:4||CU:4||BASISSET:4||XAS:4||CRYSTALS:3||EXCITATIONS:3||MOTTHUBBARD SYSTEMS:3||HIGHENERGY SPIN:3||halfmetal:3||INSULATORS:3||LA2CUO4:3||MODEL:3||FLUCTUATIONS:3||CE:3||double exchange:3||TRANSITIONMETALS:3||RESISTIVITY:3||BORON:3||LA1XCAXMNO3:3||IRON:3||PES:3||ANTIMONIDES:2||MgB2:2||ZR METALLIC GLASSES:2||superconductor:2||CRITICALCURRENT DENSITY:2||CIRCULARDICHROISM:2||SEMICONDUCTORS:2||LOCALIZATION:2||INTRABAND OPTICAL CONDUCTIVITY:2||COLOSSAL MAGNETORESISTANCE:2||OXIDATION:2||EXISTENCE:2||COPPER:2||diboride:2||MAGNESIUMDIBORIDE:2||GAP:2||CE COMPOUNDS:2||CORE POLARIZATION:2||magnetoresistance:2||photoemission spectroscopy:2||electronphonon interaction:2||GETTER:2||PD:2||MAGNETISM:2||FECR2S4:2||SUPERCONDUCTING MGB2:2||WIRES:2||ABSORPTION:2||ENERGY:2||LA1XSRXMNO3:2||CONSTANTS:2||polaron:2||charge ordering:2||SCATTERING:2||XRAY PHOTOEMISSION:2||CeNiSn:2||phase diagram:2||PHOTOELECTRON:2||QUADRUPOLAR:2||perovskitemanganites:2||CO:2||SYSTEMS:2||DOPED ZNO:2||LOWFREQUENCY SOUND:2||LA:2||ELECTRONELECTRON SCATTERING:2||AU:2||DENSITYWAVE INSTABILITY:2||FERMISURFACE:2||hybridization:2||VALENCEBAND SATELLITE:2||SULFUR SPINEL:2||Heusler:2||APPROXIMATION:2||superexchange:2||colossal magnetoresistance:2||ALLOYS:2||DEPENDENCE:2||AG:2||electronic structures:2||AUGERSPECTRA:2||CR:2||PARAMETERS:2||DIFFRACTION:2||SEMICONDUCTORMETAL TRANSITION:1||INTERMEDIATEVALENCE:1||SMB6:1||SRRUO3:1||antiperovskite structure with antipolar nature:1||lowenergy twodimensional phonons:1||anatase TiO2:1||La3S4:1||metalinsulator transitions:1||MNO:1||ELECTRONICSTRUCTURES:1||MAGNETIC CIRCULARDICHROISM:1||Density functional theory:1||CeCo2:1||TOPOLARON CROSSOVER:1||EXCHANGE:1||cuprates:1||high Tc cuprates:1||magnetically ordered materials:1||ZNSE:1||Sr2xKxFeMoO6:1||CDW:1||TeCuO3:1||STRUCTURALPROPERTIES:1||MN:1||screening length:1||amorphous Fe:1||WAVE BASISSET:1||SILICONCARBIDE:1||HIGHPRESSURE:1||electronphonon coupling:1||quenched superconductivity:1||CMR perovskite manganites:1||OXIDE:1||polarons:1||synchrotron radiation:1||FULLERIDES:1||RESONANTPHOTOEMISSION:1||Silicon carbide:1||DFT calculation:1||Hybridized bands:1||GIANT MAGNETORESISTANCE:1||PEROVSKITES:1||Raman spectra:1||EXCHANGE ENHANCEMENT:1||SILICON:1||SR2FEMOO6:1||orbital ordering:1||delafossite:1||TITANIUMDIOXIDE:1||electronic structure of disordered solids:1||YFE2:1||Magnetic polaron:1||NA2TI2SB2O:1||STRONGCOUPLED SUPERCONDUCTORS:1||HEAVYFERMION SYSTEMS:1||firstprinciples calculations:1||MECHANISM:1||UNiSn:1||PHOTONIC BANDGAP:1||SINGLE IMPURITY:1||PHONONSPECTRUM:1||FERMISURFACE TOPOLOGY:1||SUPPRESSION:1||RESONANT PHOTOEMISSION:1||METALDOPED PICENE:1||PHOTOIONIZATION CROSSSECTIONS:1||PHOTOINDUCED FERRIMAGNETIC SYSTEMS:1||LINKAGE ISOMERISM:1||CHARGETRANSFER:1||Bilayer Graphene:1||MAGNETICFIELD:1||SPINWAVES:1||rareearth manganese oxides:1||magnonphonon interaction:1||NACO2O4:1||ENERGYBANDS:1||SELFENERGY:1||GAS:1||Fe0.5Cu0.5Cr2S4:1||scanning photoelectron microscopy (SPEM):1||MAGNETIC PROPERTIES:1||Stoner model:1||AMORPHOUS TRANSITIONMETALS:1||SPINGLASS STATES:1||NI:1||LA3NI2B2N3:1||SOLIDS:1||CEO2:1||BAND THEORY:1||dilute magnetic semiconductor:1||pyrochlore:1||Y1XPRXBA2CU3O7DELTA:1||and electronphonon interactions:1||VIBRATIONS:1||RAY PHOTOEMISSION:1||ALKALI CATION:1||Europium:1||colossal magnetoresistance:1||structural stability:1||ENERGYGAP:1||small polaron:1||DOUBLE EXCHANGE:1||Coulomb correlation:1||magnon:1||phonons:1||ELECTRON FERROMAGNETISM:1||CURIETEMPERATURE:1||ARPES:1||PLANEWAVE METHOD:1||Xray absorption spectroscopy (XAS):1||ROOMTEMPERATURE:1||MONOCHALCOGENIDES:1||HEAT:1||UPDSN:1||MOMENTS:1||XRAY ABSORPTION:1||SEMICONDUCTOR:1||Fermi surface nesting:1||optical phonon:1||disordered system:1||dilute magnetic semiconductors:1||CMR manganites:1||PHONONS:1||LATTICEDYNAMICS:1||OXIDES:1||4fphotoemission:1||permanent magnet:1||pseudogap:1||TRANSPORTPROPERTIES:1||ANTIFERROMAGNET:1||(BI,PB)SRCOO SYSTEM:1||semicore correlation:1||POLARIZATION:1||CRYSTAL:1||spinel:1||Xray magnetic circular dichroism (XMCD):1||magnetocapacitance:1||ANATASE:1||TEMPERATURES:1||Pseudogap:1||INTERFACE:1||SUBSTRATE:1||YNI2B2C:1||SAMARIUM SULFIDE:1||strong swave superconductor:1||DOPED MANGANITE:1||SYMMETRY:1||CENISN:1||resonance mode:1||DISORDERED SYSTEM:1||LITHIUM INTERCALATION:1||CUO2 PLANE:1||SURFACE:1||Delafossite:1||ELECTRICALPROPERTIES:1||NIMNSB:1||PTMNSB:1||ROOMTEMPERATURE FERROMAGNETISM:1||RUBIDIUM MANGANESE HEXACYANOFERRATE:1||COLOSSALMAGNETORESISTANCE:1||FINITE TEMPERATURES:1||LAMNO3:1||FE:1||transitionmetal oxides:1||giant magnetoresistance:1||phonon:1||COPPER OXIDES:1||valence states:1||thermoelectric:1||semiconductor:1||CATION DISTRIBUTION:1||FeCr2S4:1||photoemission spectroscopy (PES):1||METALLIC FERROMAGNETISM:1||GRAPHITE:1||SUSCEPTIBILITY:1||UBE13:1||RCrSb3:1||band JahnTeller:1||Ce3S4:1||TiO2:1||PrBa2Cu3O7delta:1||UNTWINNED PRBA2CU3O7:1||AGNIO2:1||HALFMETALLIC FERROMAGNETS:1||CI:1||Energy gap:1||Photoemission:1||Future applications:1||Photoemission measurements:1||Graphene:1||BANDSTRUCTURE:1||TC:1||superconductivity:1||magnetic semiconductors:1||CMRmanganites:1||thin films:1||spin dynamics:1||highTc superconductors:1||ITINERANTELECTRON FERROMAGNETISM:1||SINGLECRYSTALS:1||CeTe2:1||amorphous magnetic materials:1||EPITAXIAL GRAPHENE:1||LAYERED PNICTIDEOXIDES:1||BOROCARBIDE SUPERCONDUCTORS:1||AUGMENTEDWAVE METHOD:1||METALLIC MAGNET UNISN:1||ORIGIN:1||spectrum rearrangement:1||MEANFIELD THEORY:1||MOLECULEBASED MAGNETS:1||METASTABLE STATE:1||INSULATOR:1||magnetic orderin:1||FCC IRON:1||CeRu2:1||TL2MN2O7:1||isotope effect:1||Perovskitemanganites:1||RECURSION METHOD:1||PERPENDICULAR MAGNETICANISOTROPY:1||quasiparticle spectral density:1||GW:1||MANGANESE FERRITE:1||RESONANCE:1||SeCuO3:1||Optical conductivity:1||MASSLESS DIRAC FERMIONS:1||SCHOTTKYBARRIER:1||electronic structure:15||ELECTRONICSTRUCTURE:11||TRANSITIONMETAL COMPOUNDS:10||METALS:10||photoemission:8||SPECTRA:8||MAGNETORESISTANCE:7||FERROMAGNETISM:7||TRANSPORT:7||TRANSITION:6||FILMS:6||THINFILMS:5||TOTALENERGY CALCULATIONS:5||MAGNETICPROPERTIES:5||SUPERCONDUCTIVITY:5||PR:5||LATTICE:4||STATES:4||SPECTROSCOPY:4||FIELD:4||CRYSTALSTRUCTURE:4||PHOTOEMISSION:4||TEMPERATURE:4||TRANSITIONTEMPERATURE:4||XRAYABSORPTION:4||STATE:4||CU:4||BASISSET:4||XAS:4||CRYSTALS:3||EXCITATIONS:3||MOTTHUBBARD SYSTEMS:3||HIGHENERGY SPIN:3||halfmetal:3||INSULATORS:3||LA2CUO4:3||MODEL:3||FLUCTUATIONS:3||CE:3||double exchange:3||TRANSITIONMETALS:3||RESISTIVITY:3||BORON:3||LA1XCAXMNO3:3||IRON:3||PES:3||ANTIMONIDES:2||MgB2:2||ZR METALLIC GLASSES:2||superconductor:2||CRITICALCURRENT DENSITY:2||CIRCULARDICHROISM:2||SEMICONDUCTORS:2||LOCALIZATION:2||INTRABAND OPTICAL CONDUCTIVITY:2||COLOSSAL MAGNETORESISTANCE:2||OXIDATION:2||EXISTENCE:2||COPPER:2||diboride:2||MAGNESIUMDIBORIDE:2||GAP:2||CE COMPOUNDS:2||CORE POLARIZATION:2||magnetoresistance:2||photoemission spectroscopy:2||electronphonon interaction:2||GETTER:2||PD:2||MAGNETISM:2||FECR2S4:2||SUPERCONDUCTING MGB2:2||WIRES:2||ABSORPTION:2||ENERGY:2||LA1XSRXMNO3:2||CONSTANTS:2||polaron:2||charge ordering:2||SCATTERING:2||XRAY PHOTOEMISSION:2||CeNiSn:2||phase diagram:2||PHOTOELECTRON:2||QUADRUPOLAR:2||perovskitemanganites:2||CO:2||SYSTEMS:2||DOPED ZNO:2||LOWFREQUENCY SOUND:2||LA:2||ELECTRONELECTRON SCATTERING:2||AU:2||DENSITYWAVE INSTABILITY:2||FERMISURFACE:2||hybridization:2||VALENCEBAND SATELLITE:2||SULFUR SPINEL:2||Heusler:2||APPROXIMATION:2||superexchange:2||colossal magnetoresistance:2||ALLOYS:2||DEPENDENCE:2||AG:2||electronic structures:2||AUGERSPECTRA:2||CR:2||PARAMETERS:2||DIFFRACTION:2||SEMICONDUCTORMETAL TRANSITION:1||INTERMEDIATEVALENCE:1||SMB6:1||SRRUO3:1||antiperovskite structure with antipolar nature:1||lowenergy twodimensional phonons:1||anatase TiO2:1||La3S4:1||metalinsulator transitions:1||MNO:1||ELECTRONICSTRUCTURES:1||MAGNETIC CIRCULARDICHROISM:1||Density functional theory:1||CeCo2:1||TOPOLARON CROSSOVER:1||EXCHANGE:1||cuprates:1||high Tc cuprates:1||magnetically ordered materials:1||ZNSE:1||Sr2xKxFeMoO6:1||CDW:1||TeCuO3:1||STRUCTURALPROPERTIES:1||MN:1||screening length:1||amorphous Fe:1||WAVE BASISSET:1||SILICONCARBIDE:1||HIGHPRESSURE:1||electronphonon coupling:1||quenched superconductivity:1||CMR perovskite manganites:1||OXIDE:1||polarons:1||synchrotron radiation:1||FULLERIDES:1||RESONANTPHOTOEMISSION:1||Silicon carbide:1||DFT calculation:1||Hybridized bands:1||GIANT MAGNETORESISTANCE:1||PEROVSKITES:1||Raman spectra:1||EXCHANGE ENHANCEMENT:1||SILICON:1||SR2FEMOO6:1||orbital ordering:1||delafossite:1||TITANIUMDIOXIDE:1||electronic structure of disordered solids:1||YFE2:1||Magnetic polaron:1||NA2TI2SB2O:1||STRONGCOUPLED SUPERCONDUCTORS:1||HEAVYFERMION SYSTEMS:1||firstprinciples calculations:1||MECHANISM:1||UNiSn:1||PHOTONIC BANDGAP:1||SINGLE IMPURITY:1||PHONONSPECTRUM:1||FERMISURFACE TOPOLOGY:1||SUPPRESSION:1||RESONANT PHOTOEMISSION:1||METALDOPED PICENE:1||PHOTOIONIZATION CROSSSECTIONS:1||PHOTOINDUCED FERRIMAGNETIC SYSTEMS:1||LINKAGE ISOMERISM:1||CHARGETRANSFER:1||Bilayer Graphene:1||MAGNETICFIELD:1||SPINWAVES:1||rareearth manganese oxides:1||magnonphonon interaction:1||NACO2O4:1||ENERGYBANDS:1||SELFENERGY:1||GAS:1||Fe0.5Cu0.5Cr2S4:1||scanning photoelectron microscopy (SPEM):1||MAGNETIC PROPERTIES:1||Stoner model:1||AMORPHOUS TRANSITIONMETALS:1||SPINGLASS STATES:1||NI:1||LA3NI2B2N3:1||SOLIDS:1||CEO2:1||BAND THEORY:1||dilute magnetic semiconductor:1||pyrochlore:1||Y1XPRXBA2CU3O7DELTA:1||and electronphonon interactions:1||VIBRATIONS:1||RAY PHOTOEMISSION:1||ALKALI CATION:1||Europium:1||colossal magnetoresistance:1||structural stability:1||ENERGYGAP:1||small polaron:1||DOUBLE EXCHANGE:1||Coulomb correlation:1||magnon:1||phonons:1||ELECTRON FERROMAGNETISM:1||CURIETEMPERATURE:1||ARPES:1||PLANEWAVE METHOD:1||Xray absorption spectroscopy (XAS):1||ROOMTEMPERATURE:1||MONOCHALCOGENIDES:1||HEAT:1||UPDSN:1||MOMENTS:1||XRAY ABSORPTION:1||SEMICONDUCTOR:1||Fermi surface nesting:1||optical phonon:1||disordered system:1||dilute magnetic semiconductors:1||CMR manganites:1||PHONONS:1||LATTICEDYNAMICS:1||OXIDES:1||4fphotoemission:1||permanent magnet:1||pseudogap:1||TRANSPORTPROPERTIES:1||ANTIFERROMAGNET:1||(BI,PB)SRCOO SYSTEM:1||semicore correlation:1||POLARIZATION:1||CRYSTAL:1||spinel:1||Xray magnetic circular dichroism (XMCD):1||magnetocapacitance:1||ANATASE:1||TEMPERATURES:1||Pseudogap:1||INTERFACE:1||SUBSTRATE:1||YNI2B2C:1||SAMARIUM SULFIDE:1||strong swave superconductor:1||DOPED MANGANITE:1||SYMMETRY:1||CENISN:1||resonance mode:1||DISORDERED SYSTEM:1||LITHIUM INTERCALATION:1||CUO2 PLANE:1||SURFACE:1||Delafossite:1||ELECTRICALPROPERTIES:1||NIMNSB:1||PTMNSB:1||ROOMTEMPERATURE FERROMAGNETISM:1||RUBIDIUM MANGANESE HEXACYANOFERRATE:1||COLOSSALMAGNETORESISTANCE:1||FINITE TEMPERATURES:1||LAMNO3:1||FE:1||transitionmetal oxides:1||giant magnetoresistance:1||phonon:1||COPPER OXIDES:1||valence states:1||thermoelectric:1||semiconductor:1||CATION DISTRIBUTION:1||FeCr2S4:1||photoemission spectroscopy (PES):1||METALLIC FERROMAGNETISM:1||GRAPHITE:1||SUSCEPTIBILITY:1||UBE13:1||RCrSb3:1||band JahnTeller:1||Ce3S4:1||TiO2:1||PrBa2Cu3O7delta:1||UNTWINNED PRBA2CU3O7:1||AGNIO2:1||HALFMETALLIC FERROMAGNETS:1||CI:1||Energy gap:1||Photoemission:1||Future applications:1||Photoemission measurements:1||Graphene:1||BANDSTRUCTURE:1||TC:1||superconductivity:1||magnetic semiconductors:1||CMRmanganites:1||thin films:1||spin dynamics:1||highTc superconductors:1||ITINERANTELECTRON FERROMAGNETISM:1||SINGLECRYSTALS:1||CeTe2:1||amorphous magnetic materials:1||EPITAXIAL GRAPHENE:1||LAYERED PNICTIDEOXIDES:1||BOROCARBIDE SUPERCONDUCTORS:1||AUGMENTEDWAVE METHOD:1||METALLIC MAGNET UNISN:1||ORIGIN:1||spectrum rearrangement:1||MEANFIELD THEORY:1||MOLECULEBASED MAGNETS:1||METASTABLE STATE:1||INSULATOR:1||magnetic orderin:1||FCC IRON:1||CeRu2:1||TL2MN2O7:1||isotope effect:1||Perovskitemanganites:1||RECURSION METHOD:1||PERPENDICULAR MAGNETICANISOTROPY:1||quasiparticle spectral density:1||GW:1||MANGANESE FERRITE:1||RESONANCE:1||SeCuO3:1||Optical conductivity:1||MASSLESS DIRAC FERMIONS:1||SCHOTTKYBARRIER:1||electronic structure:15||ELECTRONICSTRUCTURE:11||TRANSITIONMETAL COMPOUNDS:10||METALS:10||photoemission:8||SPECTRA:8||MAGNETORESISTANCE:7||FERROMAGNETISM:7||TRANSPORT:7||TRANSITION:6||FILMS:6||THINFILMS:5||TOTALENERGY CALCULATIONS:5||MAGNETICPROPERTIES:5||SUPERCONDUCTIVITY:5||PR:5||LATTICE:4||STATES:4||SPECTROSCOPY:4||FIELD:4||CRYSTALSTRUCTURE:4||PHOTOEMISSION:4||TEMPERATURE:4||TRANSITIONTEMPERATURE:4||XRAYABSORPTION:4||STATE:4||CU:4||BASISSET:4||XAS:4||CRYSTALS:3||EXCITATIONS:3||MOTTHUBBARD SYSTEMS:3||HIGHENERGY SPIN:3||halfmetal:3||INSULATORS:3||LA2CUO4:3||MODEL:3||FLUCTUATIONS:3||CE:3||double exchange:3||TRANSITIONMETALS:3||RESISTIVITY:3||BORON:3||LA1XCAXMNO3:3||IRON:3||PES:3||ANTIMONIDES:2||MgB2:2||ZR METALLIC GLASSES:2||superconductor:2||CRITICALCURRENT DENSITY:2||CIRCULARDICHROISM:2||SEMICONDUCTORS:2||LOCALIZATION:2||INTRABAND OPTICAL CONDUCTIVITY:2||COLOSSAL MAGNETORESISTANCE:2||OXIDATION:2||EXISTENCE:2||COPPER:2||diboride:2||MAGNESIUMDIBORIDE:2||GAP:2||CE COMPOUNDS:2||CORE POLARIZATION:2||magnetoresistance:2||photoemission spectroscopy:2||electronphonon interaction:2||GETTER:2||PD:2||MAGNETISM:2||FECR2S4:2||SUPERCONDUCTING MGB2:2||WIRES:2||ABSORPTION:2||ENERGY:2||LA1XSRXMNO3:2||CONSTANTS:2||polaron:2||charge ordering:2||SCATTERING:2||XRAY PHOTOEMISSION:2||CeNiSn:2||phase diagram:2||PHOTOELECTRON:2||QUADRUPOLAR:2||perovskitemanganites:2||CO:2||SYSTEMS:2||DOPED ZNO:2||LOWFREQUENCY SOUND:2||LA:2||ELECTRONELECTRON SCATTERING:2||AU:2||DENSITYWAVE INSTABILITY:2||FERMISURFACE:2||hybridization:2||VALENCEBAND SATELLITE:2||SULFUR SPINEL:2||Heusler:2||APPROXIMATION:2||superexchange:2||colossal magnetoresistance:2||ALLOYS:2||DEPENDENCE:2||AG:2||electronic structures:2||AUGERSPECTRA:2||CR:2||PARAMETERS:2||DIFFRACTION:2||SEMICONDUCTORMETAL TRANSITION:1||INTERMEDIATEVALENCE:1||SMB6:1||SRRUO3:1||antiperovskite structure with antipolar nature:1||lowenergy twodimensional phonons:1||anatase TiO2:1||La3S4:1||metalinsulator transitions:1||MNO:1||ELECTRONICSTRUCTURES:1||MAGNETIC CIRCULARDICHROISM:1||Density functional theory:1||CeCo2:1||TOPOLARON CROSSOVER:1||EXCHANGE:1||cuprates:1||high Tc cuprates:1||magnetically ordered materials:1||ZNSE:1||Sr2xKxFeMoO6:1||CDW:1||TeCuO3:1||STRUCTURALPROPERTIES:1||MN:1||screening length:1||amorphous Fe:1||WAVE BASISSET:1||SILICONCARBIDE:1||HIGHPRESSURE:1||electronphonon coupling:1||quenched superconductivity:1||CMR perovskite manganites:1||OXIDE:1||polarons:1||synchrotron radiation:1||FULLERIDES:1||RESONANTPHOTOEMISSION:1||Silicon carbide:1||DFT calculation:1||Hybridized bands:1||GIANT MAGNETORESISTANCE:1||PEROVSKITES:1||Raman spectra:1||EXCHANGE ENHANCEMENT:1||SILICON:1||SR2FEMOO6:1||orbital ordering:1||delafossite:1||TITANIUMDIOXIDE:1||electronic structure of disordered solids:1||YFE2:1||Magnetic polaron:1||NA2TI2SB2O:1||STRONGCOUPLED SUPERCONDUCTORS:1||HEAVYFERMION SYSTEMS:1||firstprinciples calculations:1||MECHANISM:1||UNiSn:1||PHOTONIC BANDGAP:1||SINGLE IMPURITY:1||PHONONSPECTRUM:1||FERMISURFACE TOPOLOGY:1||SUPPRESSION:1||RESONANT PHOTOEMISSION:1||METALDOPED PICENE:1||PHOTOIONIZATION CROSSSECTIONS:1||PHOTOINDUCED FERRIMAGNETIC SYSTEMS:1||LINKAGE ISOMERISM:1||CHARGETRANSFER:1||Bilayer Graphene:1||MAGNETICFIELD:1||SPINWAVES:1||rareearth manganese oxides:1||magnonphonon interaction:1||NACO2O4:1||ENERGYBANDS:1||SELFENERGY:1||GAS:1||Fe0.5Cu0.5Cr2S4:1||scanning photoelectron microscopy (SPEM):1||MAGNETIC PROPERTIES:1||Stoner model:1||AMORPHOUS TRANSITIONMETALS:1||SPINGLASS STATES:1||NI:1||LA3NI2B2N3:1||SOLIDS:1||CEO2:1||BAND THEORY:1||dilute magnetic semiconductor:1||pyrochlore:1||Y1XPRXBA2CU3O7DELTA:1||and electronphonon interactions:1||VIBRATIONS:1||RAY PHOTOEMISSION:1||ALKALI CATION:1||Europium:1||colossal magnetoresistance:1||structural stability:1||ENERGYGAP:1||small polaron:1||DOUBLE EXCHANGE:1||Coulomb correlation:1||magnon:1||phonons:1||ELECTRON FERROMAGNETISM:1||CURIETEMPERATURE:1||ARPES:1||PLANEWAVE METHOD:1||Xray absorption spectroscopy (XAS):1||ROOMTEMPERATURE:1||MONOCHALCOGENIDES:1||HEAT:1||UPDSN:1||MOMENTS:1||XRAY ABSORPTION:1||SEMICONDUCTOR:1||Fermi surface nesting:1||optical phonon:1||disordered system:1||dilute magnetic semiconductors:1||CMR manganites:1||PHONONS:1||LATTICEDYNAMICS:1||OXIDES:1||4fphotoemission:1||permanent magnet:1||pseudogap:1||TRANSPORTPROPERTIES:1||ANTIFERROMAGNET:1||(BI,PB)SRCOO SYSTEM:1||semicore correlation:1||POLARIZATION:1||CRYSTAL:1||spinel:1||Xray magnetic circular dichroism (XMCD):1||magnetocapacitance:1||ANATASE:1||TEMPERATURES:1||Pseudogap:1||INTERFACE:1||SUBSTRATE:1||YNI2B2C:1||SAMARIUM SULFIDE:1||strong swave superconductor:1||DOPED MANGANITE:1||SYMMETRY:1||CENISN:1||resonance mode:1||DISORDERED SYSTEM:1||LITHIUM INTERCALATION:1||CUO2 PLANE:1||SURFACE:1||Delafossite:1||ELECTRICALPROPERTIES:1||NIMNSB:1||PTMNSB:1||ROOMTEMPERATURE FERROMAGNETISM:1||RUBIDIUM MANGANESE HEXACYANOFERRATE:1||COLOSSALMAGNETORESISTANCE:1||FINITE TEMPERATURES:1||LAMNO3:1||FE:1||transitionmetal oxides:1||giant magnetoresistance:1||phonon:1||COPPER OXIDES:1||valence states:1||thermoelectric:1||semiconductor:1||CATION DISTRIBUTION:1||FeCr2S4:1||photoemission spectroscopy (PES):1||METALLIC FERROMAGNETISM:1||GRAPHITE:1||SUSCEPTIBILITY:1||UBE13:1||RCrSb3:1||band JahnTeller:1||Ce3S4:1||TiO2:1||PrBa2Cu3O7delta:1||UNTWINNED PRBA2CU3O7:1||AGNIO2:1||HALFMETALLIC FERROMAGNETS:1||CI:1||Energy gap:1||Photoemission:1||Future applications:1||Photoemission measurements:1||Graphene:1||BANDSTRUCTURE:1||TC:1||superconductivity:1||magnetic semiconductors:1||CMRmanganites:1||thin films:1||spin dynamics:1||highTc superconductors:1||ITINERANTELECTRON FERROMAGNETISM:1||SINGLECRYSTALS:1||CeTe2:1||amorphous magnetic materials:1||EPITAXIAL GRAPHENE:1||LAYERED PNICTIDEOXIDES:1||BOROCARBIDE SUPERCONDUCTORS:1||AUGMENTEDWAVE METHOD:1||METALLIC MAGNET UNISN:1||ORIGIN:1||spectrum rearrangement:1||MEANFIELD THEORY:1||MOLECULEBASED MAGNETS:1||METASTABLE STATE:1||INSULATOR:1||magnetic orderin:1||FCC IRON:1||CeRu2:1||TL2MN2O7:1||isotope effect:1||Perovskitemanganites:1||RECURSION METHOD:1||PERPENDICULAR MAGNETICANISOTROPY:1||quasiparticle spectral density:1||GW:1||MANGANESE FERRITE:1||RESONANCE:1||SeCuO3:1||Optical conductivity:1||MASSLESS DIRAC FERMIONS:1||SCHOTTKYBARRIER:1||electronic structure:15||ELECTRONICSTRUCTURE:11||TRANSITIONMETAL COMPOUNDS:10||METALS:10||photoemission:8||SPECTRA:8||MAGNETORESISTANCE:7||FERROMAGNETISM:7||TRANSPORT:7||TRANSITION:6||FILMS:6||THINFILMS:5||TOTALENERGY CALCULATIONS:5||MAGNETICPROPERTIES:5||SUPERCONDUCTIVITY:5||PR:5||LATTICE:4||STATES:4||SPECTROSCOPY:4||FIELD:4||CRYSTALSTRUCTURE:4||PHOTOEMISSION:4||TEMPERATURE:4||TRANSITIONTEMPERATURE:4||XRAYABSORPTION:4||STATE:4||CU:4||BASISSET:4||XAS:4||CRYSTALS:3||EXCITATIONS:3||MOTTHUBBARD SYSTEMS:3||HIGHENERGY SPIN:3||halfmetal:3||INSULATORS:3||LA2CUO4:3||MODEL:3||FLUCTUATIONS:3||CE:3||double exchange:3||TRANSITIONMETALS:3||RESISTIVITY:3||BORON:3||LA1XCAXMNO3:3||IRON:3||PES:3||ANTIMONIDES:2||MgB2:2||ZR METALLIC GLASSES:2||superconductor:2||CRITICALCURRENT DENSITY:2||CIRCULARDICHROISM:2||SEMICONDUCTORS:2||LOCALIZATION:2||INTRABAND OPTICAL CONDUCTIVITY:2||COLOSSAL MAGNETORESISTANCE:2||OXIDATION:2||EXISTENCE:2||COPPER:2||diboride:2||MAGNESIUMDIBORIDE:2||GAP:2||CE COMPOUNDS:2||CORE POLARIZATION:2||magnetoresistance:2||photoemission spectroscopy:2||electronphonon interaction:2||GETTER:2||PD:2||MAGNETISM:2||FECR2S4:2||SUPERCONDUCTING MGB2:2||WIRES:2||ABSORPTION:2||ENERGY:2||LA1XSRXMNO3:2||CONSTANTS:2||polaron:2||charge ordering:2||SCATTERING:2||XRAY PHOTOEMISSION:2||CeNiSn:2||phase diagram:2||PHOTOELECTRON:2||QUADRUPOLAR:2||perovskitemanganites:2||CO:2||SYSTEMS:2||DOPED ZNO:2||LOWFREQUENCY SOUND:2||LA:2||ELECTRONELECTRON SCATTERING:2||AU:2||DENSITYWAVE INSTABILITY:2||FERMISURFACE:2||hybridization:2||VALENCEBAND SATELLITE:2||SULFUR SPINEL:2||Heusler:2||APPROXIMATION:2||superexchange:2||colossal magnetoresistance:2||ALLOYS:2||DEPENDENCE:2||AG:2||electronic structures:2||AUGERSPECTRA:2||CR:2||PARAMETERS:2||DIFFRACTION:2||SEMICONDUCTORMETAL TRANSITION:1||INTERMEDIATEVALENCE:1||SMB6:1||SRRUO3:1||antiperovskite structure with antipolar nature:1||lowenergy twodimensional phonons:1||anatase TiO2:1||La3S4:1||metalinsulator transitions:1||MNO:1||ELECTRONICSTRUCTURES:1||MAGNETIC CIRCULARDICHROISM:1||Density functional theory:1||CeCo2:1||TOPOLARON CROSSOVER:1||EXCHANGE:1||cuprates:1||high Tc cuprates:1||magnetically ordered materials:1||ZNSE:1||Sr2xKxFeMoO6:1||CDW:1||TeCuO3:1||STRUCTURALPROPERTIES:1||MN:1||screening length:1||amorphous Fe:1||WAVE BASISSET:1||SILICONCARBIDE:1||HIGHPRESSURE:1||electronphonon coupling:1||quenched superconductivity:1||CMR perovskite manganites:1||OXIDE:1||polarons:1||synchrotron radiation:1||FULLERIDES:1||RESONANTPHOTOEMISSION:1||Silicon carbide:1||DFT calculation:1||Hybridized bands:1||GIANT MAGNETORESISTANCE:1||PEROVSKITES:1||Raman spectra:1||EXCHANGE ENHANCEMENT:1||SILICON:1||SR2FEMOO6:1||orbital ordering:1||delafossite:1||TITANIUMDIOXIDE:1||electronic structure of disordered solids:1||YFE2:1||Magnetic polaron:1||NA2TI2SB2O:1||STRONGCOUPLED SUPERCONDUCTORS:1||HEAVYFERMION SYSTEMS:1||firstprinciples calculations:1||MECHANISM:1||UNiSn:1||PHOTONIC BANDGAP:1||SINGLE IMPURITY:1||PHONONSPECTRUM:1||FERMISURFACE TOPOLOGY:1||SUPPRESSION:1||RESONANT PHOTOEMISSION:1||METALDOPED PICENE:1||PHOTOIONIZATION CROSSSECTIONS:1||PHOTOINDUCED FERRIMAGNETIC SYSTEMS:1||LINKAGE ISOMERISM:1||CHARGETRANSFER:1||Bilayer Graphene:1||MAGNETICFIELD:1||SPINWAVES:1||rareearth manganese oxides:1||magnonphonon interaction:1||NACO2O4:1||ENERGYBANDS:1||SELFENERGY:1||GAS:1||Fe0.5Cu0.5Cr2S4:1||scanning photoelectron microscopy (SPEM):1||MAGNETIC PROPERTIES:1||Stoner model:1||AMORPHOUS TRANSITIONMETALS:1||SPINGLASS STATES:1||NI:1||LA3NI2B2N3:1||SOLIDS:1||CEO2:1||BAND THEORY:1||dilute magnetic semiconductor:1||pyrochlore:1||Y1XPRXBA2CU3O7DELTA:1||and electronphonon interactions:1||VIBRATIONS:1||RAY PHOTOEMISSION:1||ALKALI CATION:1||Europium:1||colossal magnetoresistance:1||structural stability:1||ENERGYGAP:1||small polaron:1||DOUBLE EXCHANGE:1||Coulomb correlation:1||magnon:1||phonons:1||ELECTRON FERROMAGNETISM:1||CURIETEMPERATURE:1||ARPES:1||PLANEWAVE METHOD:1||Xray absorption spectroscopy (XAS):1||ROOMTEMPERATURE:1||MONOCHALCOGENIDES:1||HEAT:1||UPDSN:1||MOMENTS:1||XRAY ABSORPTION:1||SEMICONDUCTOR:1||Fermi surface nesting:1||optical phonon:1||disordered system:1||dilute magnetic semiconductors:1||CMR manganites:1||PHONONS:1||LATTICEDYNAMICS:1||OXIDES:1||4fphotoemission:1||permanent magnet:1||pseudogap:1||TRANSPORTPROPERTIES:1||ANTIFERROMAGNET:1||(BI,PB)SRCOO SYSTEM:1||semicore correlation:1||POLARIZATION:1||CRYSTAL:1||spinel:1||Xray magnetic circular dichroism (XMCD):1||magnetocapacitance:1||ANATASE:1||TEMPERATURES:1||Pseudogap:1||INTERFACE:1||SUBSTRATE:1||YNI2B2C:1||SAMARIUM SULFIDE:1||strong swave superconductor:1||DOPED MANGANITE:1||SYMMETRY:1||CENISN:1||resonance mode:1||DISORDERED SYSTEM:1||LITHIUM INTERCALATION:1||CUO2 PLANE:1||SURFACE:1||Delafossite:1||ELECTRICALPROPERTIES:1||NIMNSB:1||PTMNSB:1||ROOMTEMPERATURE FERROMAGNETISM:1||RUBIDIUM MANGANESE HEXACYANOFERRATE:1||COLOSSALMAGNETORESISTANCE:1||FINITE TEMPERATURES:1||LAMNO3:1||FE:1||transitionmetal oxides:1||giant magnetoresistance:1||phonon:1||COPPER OXIDES:1||valence states:1||thermoelectric:1||semiconductor:1||CATION DISTRIBUTION:1||FeCr2S4:1||photoemission spectroscopy (PES):1||METALLIC FERROMAGNETISM:1||GRAPHITE:1||SUSCEPTIBILITY:1||UBE13:1||RCrSb3:1||band JahnTeller:1||Ce3S4:1||TiO2:1||PrBa2Cu3O7delta:1||UNTWINNED PRBA2CU3O7:1||AGNIO2:1||HALFMETALLIC FERROMAGNETS:1||CI:1||Energy gap:1||Photoemission:1||Future applications:1||Photoemission measurements:1||Graphene:1||BANDSTRUCTURE:1||TC:1||superconductivity:1||magnetic semiconductors:1||CMRmanganites:1||thin films:1||spin dynamics:1||highTc superconductors:1||ITINERANTELECTRON FERROMAGNETISM:1||SINGLECRYSTALS:1||CeTe2:1||amorphous magnetic materials:1||EPITAXIAL GRAPHENE:1||LAYERED PNICTIDEOXIDES:1||BOROCARBIDE SUPERCONDUCTORS:1||AUGMENTEDWAVE METHOD:1||METALLIC MAGNET UNISN:1||ORIGIN:1||spectrum rearrangement:1||MEANFIELD THEORY:1||MOLECULEBASED MAGNETS:1||METASTABLE STATE:1||INSULATOR:1||magnetic orderin:1||FCC IRON:1||CeRu2:1||TL2MN2O7:1||isotope effect:1||Perovskitemanganites:1||RECURSION METHOD:1||PERPENDICULAR MAGNETICANISOTROPY:1||quasiparticle spectral density:1||GW:1||MANGANESE FERRITE:1||RESONANCE:1||SeCuO3:1||Optical conductivity:1||MASSLESS DIRAC FERMIONS:1||SCHOTTKYBARRIER:1||electronic structure:15||ELECTRONICSTRUCTURE:11||TRANSITIONMETAL COMPOUNDS:10||METALS:10||photoemission:8||SPECTRA:8||MAGNETORESISTANCE:7||FERROMAGNETISM:7||TRANSPORT:7||TRANSITION:6||FILMS:6||THINFILMS:5||TOTALENERGY CALCULATIONS:5||MAGNETICPROPERTIES:5||SUPERCONDUCTIVITY:5||PR:5||LATTICE:4||STATES:4||SPECTROSCOPY:4||FIELD:4||CRYSTALSTRUCTURE:4||PHOTOEMISSION:4||TEMPERATURE:4||TRANSITIONTEMPERATURE:4||XRAYABSORPTION:4||STATE:4||CU:4||BASISSET:4||XAS:4||CRYSTALS:3||EXCITATIONS:3||MOTTHUBBARD SYSTEMS:3||HIGHENERGY SPIN:3||halfmetal:3||INSULATORS:3||LA2CUO4:3||MODEL:3||FLUCTUATIONS:3||CE:3||double exchange:3||TRANSITIONMETALS:3||RESISTIVITY:3||BORON:3||LA1XCAXMNO3:3||IRON:3||PES:3||ANTIMONIDES:2||MgB2:2||ZR METALLIC GLASSES:2||superconductor:2||CRITICALCURRENT DENSITY:2||CIRCULARDICHROISM:2||SEMICONDUCTORS:2||LOCALIZATION:2||INTRABAND OPTICAL CONDUCTIVITY:2||COLOSSAL MAGNETORESISTANCE:2||OXIDATION:2||EXISTENCE:2||COPPER:2||diboride:2||MAGNESIUMDIBORIDE:2||GAP:2||CE COMPOUNDS:2||CORE POLARIZATION:2||magnetoresistance:2||photoemission spectroscopy:2||electronphonon interaction:2||GETTER:2||PD:2||MAGNETISM:2||FECR2S4:2||SUPERCONDUCTING MGB2:2||WIRES:2||ABSORPTION:2||ENERGY:2||LA1XSRXMNO3:2||CONSTANTS:2||polaron:2||charge ordering:2||SCATTERING:2||XRAY PHOTOEMISSION:2||CeNiSn:2||phase diagram:2||PHOTOELECTRON:2||QUADRUPOLAR:2||perovskitemanganites:2||CO:2||SYSTEMS:2||DOPED ZNO:2||LOWFREQUENCY SOUND:2||LA:2||ELECTRONELECTRON SCATTERING:2||AU:2||DENSITYWAVE INSTABILITY:2||FERMISURFACE:2||hybridization:2||VALENCEBAND SATELLITE:2||SULFUR SPINEL:2||Heusler:2||APPROXIMATION:2||superexchange:2||colossal magnetoresistance:2||ALLOYS:2||DEPENDENCE:2||AG:2||electronic structures:2||AUGERSPECTRA:2||CR:2||PARAMETERS:2||DIFFRACTION:2||SEMICONDUCTORMETAL TRANSITION:1||INTERMEDIATEVALENCE:1||SMB6:1||SRRUO3:1||antiperovskite structure with antipolar nature:1||lowenergy twodimensional phonons:1||anatase TiO2:1||La3S4:1||metalinsulator transitions:1||MNO:1||ELECTRONICSTRUCTURES:1||MAGNETIC CIRCULARDICHROISM:1||Density functional theory:1||CeCo2:1||TOPOLARON CROSSOVER:1||EXCHANGE:1||cuprates:1||high Tc cuprates:1||magnetically ordered materials:1||ZNSE:1||Sr2xKxFeMoO6:1||CDW:1||TeCuO3:1||STRUCTURALPROPERTIES:1||MN:1||screening length:1||amorphous Fe:1||WAVE BASISSET:1||SILICONCARBIDE:1||HIGHPRESSURE:1||electronphonon coupling:1||quenched superconductivity:1||CMR perovskite manganites:1||OXIDE:1||polarons:1||synchrotron radiation:1||FULLERIDES:1||RESONANTPHOTOEMISSION:1||Silicon carbide:1||DFT calculation:1||Hybridized bands:1||GIANT MAGNETORESISTANCE:1||PEROVSKITES:1||Raman spectra:1||EXCHANGE ENHANCEMENT:1||SILICON:1||SR2FEMOO6:1||orbital ordering:1||delafossite:1||TITANIUMDIOXIDE:1||electronic structure of disordered solids:1||YFE2:1||Magnetic polaron:1||NA2TI2SB2O:1||STRONGCOUPLED SUPERCONDUCTORS:1||HEAVYFERMION SYSTEMS:1||firstprinciples calculations:1||MECHANISM:1||UNiSn:1||PHOTONIC BANDGAP:1||SINGLE IMPURITY:1||PHONONSPECTRUM:1||FERMISURFACE TOPOLOGY:1||SUPPRESSION:1||RESONANT PHOTOEMISSION:1||METALDOPED PICENE:1||PHOTOIONIZATION CROSSSECTIONS:1||PHOTOINDUCED FERRIMAGNETIC SYSTEMS:1||LINKAGE ISOMERISM:1||CHARGETRANSFER:1||Bilayer Graphene:1||MAGNETICFIELD:1||SPINWAVES:1||rareearth manganese oxides:1||magnonphonon interaction:1||NACO2O4:1||ENERGYBANDS:1||SELFENERGY:1||GAS:1||Fe0.5Cu0.5Cr2S4:1||scanning photoelectron microscopy (SPEM):1||MAGNETIC PROPERTIES:1||Stoner model:1||AMORPHOUS TRANSITIONMETALS:1||SPINGLASS STATES:1||NI:1||LA3NI2B2N3:1||SOLIDS:1||CEO2:1||BAND THEORY:1||dilute magnetic semiconductor:1||pyrochlore:1||Y1XPRXBA2CU3O7DELTA:1||and electronphonon interactions:1||VIBRATIONS:1||RAY PHOTOEMISSION:1||ALKALI CATION:1||Europium:1||colossal magnetoresistance:1||structural stability:1||ENERGYGAP:1||small polaron:1||DOUBLE EXCHANGE:1||Coulomb correlation:1||magnon:1||phonons:1||ELECTRON FERROMAGNETISM:1||CURIETEMPERATURE:1||ARPES:1||PLANEWAVE METHOD:1||Xray absorption spectroscopy (XAS):1||ROOMTEMPERATURE:1||MONOCHALCOGENIDES:1||HEAT:1||UPDSN:1||MOMENTS:1||XRAY ABSORPTION:1||SEMICONDUCTOR:1||Fermi surface nesting:1||optical phonon:1||disordered system:1||dilute magnetic semiconductors:1||CMR manganites:1||PHONONS:1||LATTICEDYNAMICS:1||OXIDES:1||4fphotoemission:1||permanent magnet:1||pseudogap:1||TRANSPORTPROPERTIES:1||ANTIFERROMAGNET:1||(BI,PB)SRCOO SYSTEM:1||semicore correlation:1||POLARIZATION:1||CRYSTAL:1||spinel:1||Xray magnetic circular dichroism (XMCD):1||magnetocapacitance:1||ANATASE:1||TEMPERATURES:1||Pseudogap:1||INTERFACE:1||SUBSTRATE:1||YNI2B2C:1||SAMARIUM SULFIDE:1||strong swave superconductor:1||DOPED MANGANITE:1||SYMMETRY:1||CENISN:1||resonance mode:1||DISORDERED SYSTEM:1||LITHIUM INTERCALATION:1||CUO2 PLANE:1||SURFACE:1||Delafossite:1||ELECTRICALPROPERTIES:1||NIMNSB:1||PTMNSB:1||ROOMTEMPERATURE FERROMAGNETISM:1||RUBIDIUM MANGANESE HEXACYANOFERRATE:1||COLOSSALMAGNETORESISTANCE:1||FINITE TEMPERATURES:1||LAMNO3:1||FE:1||transitionmetal oxides:1||giant magnetoresistance:1||phonon:1||COPPER OXIDES:1||valence states:1||thermoelectric:1||semiconductor:1||CATION DISTRIBUTION:1||FeCr2S4:1||photoemission spectroscopy (PES):1||METALLIC FERROMAGNETISM:1||GRAPHITE:1||SUSCEPTIBILITY:1||UBE13:1||RCrSb3:1||band JahnTeller:1||Ce3S4:1||TiO2:1||PrBa2Cu3O7delta:1||UNTWINNED PRBA2CU3O7:1||AGNIO2:1||HALFMETALLIC FERROMAGNETS:1||CI:1||Energy gap:1||Photoemission:1||Future applications:1||Photoemission measurements:1||Graphene:1||BANDSTRUCTURE:1||TC:1||superconductivity:1||magnetic semiconductors:1||CMRmanganites:1||thin films:1||spin dynamics:1||highTc superconductors:1||ITINERANTELECTRON FERROMAGNETISM:1||SINGLECRYSTALS:1||CeTe2:1||amorphous magnetic materials:1||EPITAXIAL GRAPHENE:1||LAYERED PNICTIDEOXIDES:1||BOROCARBIDE SUPERCONDUCTORS:1||AUGMENTEDWAVE METHOD:1||METALLIC MAGNET UNISN:1||ORIGIN:1||spectrum rearrangement:1||MEANFIELD THEORY:1||MOLECULEBASED MAGNETS:1||METASTABLE STATE:1||INSULATOR:1||magnetic orderin:1||FCC IRON:1||CeRu2:1||TL2MN2O7:1||isotope effect:1||Perovskitemanganites:1||RECURSION METHOD:1||PERPENDICULAR MAGNETICANISOTROPY:1||quasiparticle spectral density:1||GW:1||MANGANESE FERRITE:1||RESONANCE:1||SeCuO3:1||Optical conductivity:1||MASSLESS DIRAC FERMIONS:1||SCHOTTKYBARRIER:1||electronic structure:15||ELECTRONICSTRUCTURE:11||TRANSITIONMETAL COMPOUNDS:10||METALS:10||photoemission:8||SPECTRA:8||MAGNETORESISTANCE:7||FERROMAGNETISM:7||TRANSPORT:7||TRANSITION:6||FILMS:6||THINFILMS:5||TOTALENERGY CALCULATIONS:5||MAGNETICPROPERTIES:5||SUPERCONDUCTIVITY:5||PR:5||LATTICE:4||STATES:4||SPECTROSCOPY:4||FIELD:4||CRYSTALSTRUCTURE:4||PHOTOEMISSION:4||TEMPERATURE:4||TRANSITIONTEMPERATURE:4||XRAYABSORPTION:4||STATE:4||CU:4||BASISSET:4||XAS:4||CRYSTALS:3||EXCITATIONS:3||MOTTHUBBARD SYSTEMS:3||HIGHENERGY SPIN:3||halfmetal:3||INSULATORS:3||LA2CUO4:3||MODEL:3||FLUCTUATIONS:3||CE:3||double exchange:3||TRANSITIONMETALS:3||RESISTIVITY:3||BORON:3||LA1XCAXMNO3:3||IRON:3||PES:3||ANTIMONIDES:2||MgB2:2||ZR METALLIC GLASSES:2||superconductor:2||CRITICALCURRENT DENSITY:2||CIRCULARDICHROISM:2||SEMICONDUCTORS:2||LOCALIZATION:2||INTRABAND OPTICAL CONDUCTIVITY:2||COLOSSAL MAGNETORESISTANCE:2||OXIDATION:2||EXISTENCE:2||COPPER:2||diboride:2||MAGNESIUMDIBORIDE:2||GAP:2||CE COMPOUNDS:2||CORE POLARIZATION:2||magnetoresistance:2||photoemission spectroscopy:2||electronphonon interaction:2||GETTER:2||PD:2||MAGNETISM:2||FECR2S4:2||SUPERCONDUCTING MGB2:2||WIRES:2||ABSORPTION:2||ENERGY:2||LA1XSRXMNO3:2||CONSTANTS:2||polaron:2||charge ordering:2||SCATTERING:2||XRAY PHOTOEMISSION:2||CeNiSn:2||phase diagram:2||PHOTOELECTRON:2||QUADRUPOLAR:2||perovskitemanganites:2||CO:2||SYSTEMS:2||DOPED ZNO:2||LOWFREQUENCY SOUND:2||LA:2||ELECTRONELECTRON SCATTERING:2||AU:2||DENSITYWAVE INSTABILITY:2||FERMISURFACE:2||hybridization:2||VALENCEBAND SATELLITE:2||SULFUR SPINEL:2||Heusler:2||APPROXIMATION:2||superexchange:2||colossal magnetoresistance:2||ALLOYS:2||DEPENDENCE:2||AG:2||electronic structures:2||AUGERSPECTRA:2||CR:2||PARAMETERS:2||DIFFRACTION:2||SEMICONDUCTORMETAL TRANSITION:1||INTERMEDIATEVALENCE:1||SMB6:1||SRRUO3:1||antiperovskite structure with antipolar nature:1||lowenergy twodimensional phonons:1||anatase TiO2:1||La3S4:1||metalinsulator transitions:1||MNO:1||ELECTRONICSTRUCTURES:1||MAGNETIC CIRCULARDICHROISM:1||Density functional theory:1||CeCo2:1||TOPOLARON CROSSOVER:1||EXCHANGE:1||cuprates:1||high Tc cuprates:1||magnetically ordered materials:1||ZNSE:1||Sr2xKxFeMoO6:1||CDW:1||TeCuO3:1||STRUCTURALPROPERTIES:1||MN:1||screening length:1||amorphous Fe:1||WAVE BASISSET:1||SILICONCARBIDE:1||HIGHPRESSURE:1||electronphonon coupling:1||quenched superconductivity:1||CMR perovskite manganites:1||OXIDE:1||polarons:1||synchrotron radiation:1||FULLERIDES:1||RESONANTPHOTOEMISSION:1||Silicon carbide:1||DFT calculation:1||Hybridized bands:1||GIANT MAGNETORESISTANCE:1||PEROVSKITES:1||Raman spectra:1||EXCHANGE ENHANCEMENT:1||SILICON:1||SR2FEMOO6:1||orbital ordering:1||delafossite:1||TITANIUMDIOXIDE:1||electronic structure of disordered solids:1||YFE2:1||Magnetic polaron:1||NA2TI2SB2O:1||STRONGCOUPLED SUPERCONDUCTORS:1||HEAVYFERMION SYSTEMS:1||firstprinciples calculations:1||MECHANISM:1||UNiSn:1||PHOTONIC BANDGAP:1||SINGLE IMPURITY:1||PHONONSPECTRUM:1||FERMISURFACE TOPOLOGY:1||SUPPRESSION:1||RESONANT PHOTOEMISSION:1||METALDOPED PICENE:1||PHOTOIONIZATION CROSSSECTIONS:1||PHOTOINDUCED FERRIMAGNETIC SYSTEMS:1||LINKAGE ISOMERISM:1||CHARGETRANSFER:1||Bilayer Graphene:1||MAGNETICFIELD:1||SPINWAVES:1||rareearth manganese oxides:1||magnonphonon interaction:1||NACO2O4:1||ENERGYBANDS:1||SELFENERGY:1||GAS:1||Fe0.5Cu0.5Cr2S4:1||scanning photoelectron microscopy (SPEM):1||MAGNETIC PROPERTIES:1||Stoner model:1||AMORPHOUS TRANSITIONMETALS:1||SPINGLASS STATES:1||NI:1||LA3NI2B2N3:1||SOLIDS:1||CEO2:1||BAND THEORY:1||dilute magnetic semiconductor:1||pyrochlore:1||Y1XPRXBA2CU3O7DELTA:1||and electronphonon interactions:1||VIBRATIONS:1||RAY PHOTOEMISSION:1||ALKALI CATION:1||Europium:1||colossal magnetoresistance:1||structural stability:1||ENERGYGAP:1||small polaron:1||DOUBLE EXCHANGE:1||Coulomb correlation:1||magnon:1||phonons:1||ELECTRON FERROMAGNETISM:1||CURIETEMPERATURE:1||ARPES:1||PLANEWAVE METHOD:1||Xray absorption spectroscopy (XAS):1||ROOMTEMPERATURE:1||MONOCHALCOGENIDES:1||HEAT:1||UPDSN:1||MOMENTS:1||XRAY ABSORPTION:1||SEMICONDUCTOR:1||Fermi surface nesting:1||optical phonon:1||disordered system:1||dilute magnetic semiconductors:1||CMR manganites:1||PHONONS:1||LATTICEDYNAMICS:1||OXIDES:1||4fphotoemission:1||permanent magnet:1||pseudogap:1||TRANSPORTPROPERTIES:1||ANTIFERROMAGNET:1||(BI,PB)SRCOO SYSTEM:1||semicore correlation:1||POLARIZATION:1||CRYSTAL:1||spinel:1||Xray magnetic circular dichroism (XMCD):1||magnetocapacitance:1||ANATASE:1||TEMPERATURES:1||Pseudogap:1||INTERFACE:1||SUBSTRATE:1||YNI2B2C:1||SAMARIUM SULFIDE:1||strong swave superconductor:1||DOPED MANGANITE:1||SYMMETRY:1||CENISN:1||resonance mode:1||DISORDERED SYSTEM:1||LITHIUM INTERCALATION:1||CUO2 PLANE:1||SURFACE:1||Delafossite:1||ELECTRICALPROPERTIES:1||NIMNSB:1||PTMNSB:1||ROOMTEMPERATURE FERROMAGNETISM:1||RUBIDIUM MANGANESE HEXACYANOFERRATE:1||COLOSSALMAGNETORESISTANCE:1||FINITE TEMPERATURES:1||LAMNO3:1||FE:1||transitionmetal oxides:1||giant magnetoresistance:1||phonon:1||COPPER OXIDES:1||valence states:1||thermoelectric:1||semiconductor:1||CATION DISTRIBUTION:1||FeCr2S4:1||photoemission spectroscopy (PES):1||METALLIC FERROMAGNETISM:1||GRAPHITE:1||SUSCEPTIBILITY:1||UBE13:1||RCrSb3:1||band JahnTeller:1||Ce3S4:1||TiO2:1||PrBa2Cu3O7delta:1||UNTWINNED PRBA2CU3O7:1||AGNIO2:1||HALFMETALLIC FERROMAGNETS:1||CI:1||Energy gap:1||Photoemission:1||Future applications:1||Photoemission measurements:1||Graphene:1||BANDSTRUCTURE:1||TC:1||superconductivity:1||magnetic semiconductors:1||CMRmanganites:1||thin films:1||spin dynamics:1||highTc superconductors:1||ITINERANTELECTRON FERROMAGNETISM:1||SINGLECRYSTALS:1||CeTe2:1||amorphous magnetic materials:1||EPITAXIAL GRAPHENE:1||LAYERED PNICTIDEOXIDES:1||BOROCARBIDE SUPERCONDUCTORS:1||AUGMENTEDWAVE METHOD:1||METALLIC MAGNET UNISN:1||ORIGIN:1||spectrum rearrangement:1||MEANFIELD THEORY:1||MOLECULEBASED MAGNETS:1||METASTABLE STATE:1||INSULATOR:1||magnetic orderin:1||FCC IRON:1||CeRu2:1||TL2MN2O7:1||isotope effect:1||Perovskitemanganites:1||RECURSION METHOD:1||PERPENDICULAR MAGNETICANISOTROPY:1||quasiparticle spectral density:1||GW:1||MANGANESE FERRITE:1||RESONANCE:1||SeCuO3:1||Optical conductivity:1||MASSLESS DIRAC FERMIONS:1||SCHOTTKYBARRIER:1||electronic structure:15||ELECTRONICSTRUCTURE:11||TRANSITIONMETAL COMPOUNDS:10||METALS:10||photoemission:8||SPECTRA:8||MAGNETORESISTANCE:7||FERROMAGNETISM:7||TRANSPORT:7||TRANSITION:6||FILMS:6||THINFILMS:5||TOTALENERGY CALCULATIONS:5||MAGNETICPROPERTIES:5||SUPERCONDUCTIVITY:5||PR:5||LATTICE:4||STATES:4||SPECTROSCOPY:4||FIELD:4||CRYSTALSTRUCTURE:4||PHOTOEMISSION:4||TEMPERATURE:4||TRANSITIONTEMPERATURE:4||XRAYABSORPTION:4||STATE:4||CU:4||BASISSET:4||XAS:4||CRYSTALS:3||EXCITATIONS:3||MOTTHUBBARD SYSTEMS:3||HIGHENERGY SPIN:3||halfmetal:3||INSULATORS:3||LA2CUO4:3||MODEL:3||FLUCTUATIONS:3||CE:3||double exchange:3||TRANSITIONMETALS:3||RESISTIVITY:3||BORON:3||LA1XCAXMNO3:3||IRON:3||PES:3||ANTIMONIDES:2||MgB2:2||ZR METALLIC GLASSES:2||superconductor:2||CRITICALCURRENT DENSITY:2||CIRCULARDICHROISM:2||SEMICONDUCTORS:2||LOCALIZATION:2||INTRABAND OPTICAL CONDUCTIVITY:2||COLOSSAL MAGNETORESISTANCE:2||OXIDATION:2||EXISTENCE:2||COPPER:2||diboride:2||MAGNESIUMDIBORIDE:2||GAP:2||CE COMPOUNDS:2||CORE POLARIZATION:2||magnetoresistance:2||photoemission spectroscopy:2||electronphonon interaction:2||GETTER:2||PD:2||MAGNETISM:2||FECR2S4:2||SUPERCONDUCTING MGB2:2||WIRES:2||ABSORPTION:2||ENERGY:2||LA1XSRXMNO3:2||CONSTANTS:2||polaron:2||charge ordering:2||SCATTERING:2||XRAY PHOTOEMISSION:2||CeNiSn:2||phase diagram:2||PHOTOELECTRON:2||QUADRUPOLAR:2||perovskitemanganites:2||CO:2||SYSTEMS:2||DOPED ZNO:2||LOWFREQUENCY SOUND:2||LA:2||ELECTRONELECTRON SCATTERING:2||AU:2||DENSITYWAVE INSTABILITY:2||FERMISURFACE:2||hybridization:2||VALENCEBAND SATELLITE:2||SULFUR SPINEL:2||Heusler:2||APPROXIMATION:2||superexchange:2||colossal magnetoresistance:2||ALLOYS:2||DEPENDENCE:2||AG:2||electronic structures:2||AUGERSPECTRA:2||CR:2||PARAMETERS:2||DIFFRACTION:2||SEMICONDUCTORMETAL TRANSITION:1||INTERMEDIATEVALENCE:1||SMB6:1||SRRUO3:1||antiperovskite structure with antipolar nature:1||lowenergy twodimensional phonons:1||anatase TiO2:1||La3S4:1||metalinsulator transitions:1||MNO:1||ELECTRONICSTRUCTURES:1||MAGNETIC CIRCULARDICHROISM:1||Density functional theory:1||CeCo2:1||TOPOLARON CROSSOVER:1||EXCHANGE:1||cuprates:1||high Tc cuprates:1||magnetically ordered materials:1||ZNSE:1||Sr2xKxFeMoO6:1||CDW:1||TeCuO3:1||STRUCTURALPROPERTIES:1||MN:1||screening length:1||amorphous Fe:1||WAVE BASISSET:1||SILICONCARBIDE:1||HIGHPRESSURE:1||electronphonon coupling:1||quenched superconductivity:1||CMR perovskite manganites:1||OXIDE:1||polarons:1||synchrotron radiation:1||FULLERIDES:1||RESONANTPHOTOEMISSION:1||Silicon carbide:1||DFT calculation:1||Hybridized bands:1||GIANT MAGNETORESISTANCE:1||PEROVSKITES:1||Raman spectra:1||EXCHANGE ENHANCEMENT:1||SILICON:1||SR2FEMOO6:1||orbital ordering:1||delafossite:1||TITANIUMDIOXIDE:1||electronic structure of disordered solids:1||YFE2:1||Magnetic polaron:1||NA2TI2SB2O:1||STRONGCOUPLED SUPERCONDUCTORS:1||HEAVYFERMION SYSTEMS:1||firstprinciples calculations:1||MECHANISM:1||UNiSn:1||PHOTONIC BANDGAP:1||SINGLE IMPURITY:1||PHONONSPECTRUM:1||FERMISURFACE TOPOLOGY:1||SUPPRESSION:1||RESONANT PHOTOEMISSION:1||METALDOPED PICENE:1||PHOTOIONIZATION CROSSSECTIONS:1||PHOTOINDUCED FERRIMAGNETIC SYSTEMS:1||LINKAGE ISOMERISM:1||CHARGETRANSFER:1||Bilayer Graphene:1||MAGNETICFIELD:1||SPINWAVES:1||rareearth manganese oxides:1||magnonphonon interaction:1||NACO2O4:1||ENERGYBANDS:1||SELFENERGY:1||GAS:1||Fe0.5Cu0.5Cr2S4:1||scanning photoelectron microscopy (SPEM):1||MAGNETIC PROPERTIES:1||Stoner model:1||AMORPHOUS TRANSITIONMETALS:1||SPINGLASS STATES:1||NI:1||LA3NI2B2N3:1||SOLIDS:1||CEO2:1||BAND THEORY:1||dilute magnetic semiconductor:1||pyrochlore:1||Y1XPRXBA2CU3O7DELTA:1||and electronphonon interactions:1||VIBRATIONS:1||RAY PHOTOEMISSION:1||ALKALI CATION:1||Europium:1||colossal magnetoresistance:1||structural stability:1||ENERGYGAP:1||small polaron:1||DOUBLE EXCHANGE:1||Coulomb correlation:1||magnon:1||phonons:1||ELECTRON FERROMAGNETISM:1||CURIETEMPERATURE:1||ARPES:1||PLANEWAVE METHOD:1||Xray absorption spectroscopy (XAS):1||ROOMTEMPERATURE:1||MONOCHALCOGENIDES:1||HEAT:1||UPDSN:1||MOMENTS:1||XRAY ABSORPTION:1||SEMICONDUCTOR:1||Fermi surface nesting:1||optical phonon:1||disordered system:1||dilute magnetic semiconductors:1||CMR manganites:1||PHONONS:1||LATTICEDYNAMICS:1||OXIDES:1||4fphotoemission:1||permanent magnet:1||pseudogap:1||TRANSPORTPROPERTIES:1||ANTIFERROMAGNET:1||(BI,PB)SRCOO SYSTEM:1||semicore correlation:1||POLARIZATION:1||CRYSTAL:1||spinel:1||Xray magnetic circular dichroism (XMCD):1||magnetocapacitance:1||ANATASE:1||TEMPERATURES:1||Pseudogap:1||INTERFACE:1||SUBSTRATE:1||YNI2B2C:1||SAMARIUM SULFIDE:1||strong swave superconductor:1||DOPED MANGANITE:1||SYMMETRY:1||CENISN:1||resonance mode:1||DISORDERED SYSTEM:1||LITHIUM INTERCALATION:1||CUO2 PLANE:1||SURFACE:1||Delafossite:1||ELECTRICALPROPERTIES:1||NIMNSB:1||PTMNSB:1||ROOMTEMPERATURE FERROMAGNETISM:1||RUBIDIUM MANGANESE HEXACYANOFERRATE:1||COLOSSALMAGNETORESISTANCE:1||FINITE TEMPERATURES:1||LAMNO3:1||FE:1||transitionmetal oxides:1||giant magnetoresistance:1||phonon:1||COPPER OXIDES:1||valence states:1||thermoelectric:1||semiconductor:1||CATION DISTRIBUTION:1||FeCr2S4:1||photoemission spectroscopy (PES):1||METALLIC FERROMAGNETISM:1||GRAPHITE:1||SUSCEPTIBILITY:1||UBE13:1||RCrSb3:1||band JahnTeller:1||Ce3S4:1||TiO2:1||PrBa2Cu3O7delta:1||UNTWINNED PRBA2CU3O7:1||AGNIO2:1||HALFMETALLIC FERROMAGNETS:1||CI:1||Energy gap:1||Photoemission:1||Future applications:1||Photoemission measurements:1||Graphene:1||BANDSTRUCTURE:1||TC:1||superconductivity:1||magnetic semiconductors:1||CMRmanganites:1||thin films:1||spin dynamics:1||highTc superconductors:1||ITINERANTELECTRON FERROMAGNETISM:1||SINGLECRYSTALS:1||CeTe2:1||amorphous magnetic materials:1||EPITAXIAL GRAPHENE:1||LAYERED PNICTIDEOXIDES:1||BOROCARBIDE SUPERCONDUCTORS:1||AUGMENTEDWAVE METHOD:1||METALLIC MAGNET UNISN:1||ORIGIN:1||spectrum rearrangement:1||MEANFIELD THEORY:1||MOLECULEBASED MAGNETS:1||METASTABLE STATE:1||INSULATOR:1||magnetic orderin:1||FCC IRON:1||CeRu2:1||TL2MN2O7:1||isotope effect:1||Perovskitemanganites:1||RECURSION METHOD:1||PERPENDICULAR MAGNETICANISOTROPY:1||quasiparticle spectral density:1||GW:1||MANGANESE FERRITE:1||RESONANCE:1||SeCuO3:1||Optical conductivity:1||MASSLESS DIRAC FERMIONS:1||SCHOTTKYBARRIER:1||electronic structure:15||ELECTRONICSTRUCTURE:11||TRANSITIONMETAL COMPOUNDS:10||METALS:10||photoemission:8||SPECTRA:8||MAGNETORESISTANCE:7||FERROMAGNETISM:7||TRANSPORT:7||TRANSITION:6||FILMS:6||THINFILMS:5||TOTALENERGY CALCULATIONS:5||MAGNETICPROPERTIES:5||SUPERCONDUCTIVITY:5||PR:5||LATTICE:4||STATES:4||SPECTROSCOPY:4||FIELD:4||CRYSTALSTRUCTURE:4||PHOTOEMISSION:4||TEMPERATURE:4||TRANSITIONTEMPERATURE:4||XRAYABSORPTION:4||STATE:4||CU:4||BASISSET:4||XAS:4||CRYSTALS:3||EXCITATIONS:3||MOTTHUBBARD SYSTEMS:3||HIGHENERGY SPIN:3||halfmetal:3||INSULATORS:3||LA2CUO4:3||MODEL:3||FLUCTUATIONS:3||CE:3||double exchange:3||TRANSITIONMETALS:3||RESISTIVITY:3||BORON:3||LA1XCAXMNO3:3||IRON:3||PES:3||ANTIMONIDES:2||MgB2:2||ZR METALLIC GLASSES:2||superconductor:2||CRITICALCURRENT DENSITY:2||CIRCULARDICHROISM:2||SEMICONDUCTORS:2||LOCALIZATION:2||INTRABAND OPTICAL CONDUCTIVITY:2||COLOSSAL MAGNETORESISTANCE:2||OXIDATION:2||EXISTENCE:2||COPPER:2||diboride:2||MAGNESIUMDIBORIDE:2||GAP:2||CE COMPOUNDS:2||CORE POLARIZATION:2||magnetoresistance:2||photoemission spectroscopy:2||electronphonon interaction:2||GETTER:2||PD:2||MAGNETISM:2||FECR2S4:2||SUPERCONDUCTING MGB2:2||WIRES:2||ABSORPTION:2||ENERGY:2||LA1XSRXMNO3:2||CONSTANTS:2||polaron:2||charge ordering:2||SCATTERING:2||XRAY PHOTOEMISSION:2||CeNiSn:2||phase diagram:2||PHOTOELECTRON:2||QUADRUPOLAR:2||perovskitemanganites:2||CO:2||SYSTEMS:2||DOPED ZNO:2||LOWFREQUENCY SOUND:2||LA:2||ELECTRONELECTRON SCATTERING:2||AU:2||DENSITYWAVE INSTABILITY:2||FERMISURFACE:2||hybridization:2||VALENCEBAND SATELLITE:2||SULFUR SPINEL:2||Heusler:2||APPROXIMATION:2||superexchange:2||colossal magnetoresistance:2||ALLOYS:2||DEPENDENCE:2||AG:2||electronic structures:2||AUGERSPECTRA:2||CR:2||PARAMETERS:2||DIFFRACTION:2||SEMICONDUCTORMETAL TRANSITION:1||INTERMEDIATEVALENCE:1||SMB6:1||SRRUO3:1||antiperovskite structure with antipolar nature:1||lowenergy twodimensional phonons:1||anatase TiO2:1||La3S4:1||metalinsulator transitions:1||MNO:1||ELECTRONICSTRUCTURES:1||MAGNETIC CIRCULARDICHROISM:1||Density functional theory:1||CeCo2:1||TOPOLARON CROSSOVER:1||EXCHANGE:1||cuprates:1||high Tc cuprates:1||magnetically ordered materials:1||ZNSE:1||Sr2xKxFeMoO6:1||CDW:1||TeCuO3:1||STRUCTURALPROPERTIES:1||MN:1||screening length:1||amorphous Fe:1||WAVE BASISSET:1||SILICONCARBIDE:1||HIGHPRESSURE:1||electronphonon coupling:1||quenched superconductivity:1||CMR perovskite manganites:1||OXIDE:1||polarons:1||synchrotron radiation:1||FULLERIDES:1||RESONANTPHOTOEMISSION:1||Silicon carbide:1||DFT calculation:1||Hybridized bands:1||GIANT MAGNETORESISTANCE:1||PEROVSKITES:1||Raman spectra:1||EXCHANGE ENHANCEMENT:1||SILICON:1||SR2FEMOO6:1||orbital ordering:1||delafossite:1||TITANIUMDIOXIDE:1||electronic structure of disordered solids:1||YFE2:1||Magnetic polaron:1||NA2TI2SB2O:1||STRONGCOUPLED SUPERCONDUCTORS:1||HEAVYFERMION SYSTEMS:1||firstprinciples calculations:1||MECHANISM:1||UNiSn:1||PHOTONIC BANDGAP:1||SINGLE IMPURITY:1||PHONONSPECTRUM:1||FERMISURFACE TOPOLOGY:1||SUPPRESSION:1||RESONANT PHOTOEMISSION:1||METALDOPED PICENE:1||PHOTOIONIZATION CROSSSECTIONS:1||PHOTOINDUCED FERRIMAGNETIC SYSTEMS:1||LINKAGE ISOMERISM:1||CHARGETRANSFER:1||Bilayer Graphene:1||MAGNETICFIELD:1||SPINWAVES:1||rareearth manganese oxides:1||magnonphonon interaction:1||NACO2O4:1||ENERGYBANDS:1||SELFENERGY:1||GAS:1||Fe0.5Cu0.5Cr2S4:1||scanning photoelectron microscopy (SPEM):1||MAGNETIC PROPERTIES:1||Stoner model:1||AMORPHOUS TRANSITIONMETALS:1||SPINGLASS STATES:1||NI:1||LA3NI2B2N3:1||SOLIDS:1||CEO2:1||BAND THEORY:1||dilute magnetic semiconductor:1||pyrochlore:1||Y1XPRXBA2CU3O7DELTA:1||and electronphonon interactions:1||VIBRATIONS:1||RAY PHOTOEMISSION:1||ALKALI CATION:1||Europium:1||colossal magnetoresistance:1||structural stability:1||ENERGYGAP:1||small polaron:1||DOUBLE EXCHANGE:1||Coulomb correlation:1||magnon:1||phonons:1||ELECTRON FERROMAGNETISM:1||CURIETEMPERATURE:1||ARPES:1||PLANEWAVE METHOD:1||Xray absorption spectroscopy (XAS):1||ROOMTEMPERATURE:1||MONOCHALCOGENIDES:1||HEAT:1||UPDSN:1||MOMENTS:1||XRAY ABSORPTION:1||SEMICONDUCTOR:1||Fermi surface nesting:1||optical phonon:1||disordered system:1||dilute magnetic semiconductors:1||CMR manganites:1||PHONONS:1||LATTICEDYNAMICS:1||OXIDES:1||4fphotoemission:1||permanent magnet:1||pseudogap:1||TRANSPORTPROPERTIES:1||ANTIFERROMAGNET:1||(BI,PB)SRCOO SYSTEM:1||semicore correlation:1||POLARIZATION:1||CRYSTAL:1||spinel:1||Xray magnetic circular dichroism (XMCD):1||magnetocapacitance:1||ANATASE:1||TEMPERATURES:1||Pseudogap:1||INTERFACE:1||SUBSTRATE:1||YNI2B2C:1||SAMARIUM SULFIDE:1||strong swave superconductor:1||DOPED MANGANITE:1||SYMMETRY:1||CENISN:1||resonance mode:1||DISORDERED SYSTEM:1||LITHIUM INTERCALATION:1||CUO2 PLANE:1||SURFACE:1||Delafossite:1||ELECTRICALPROPERTIES:1||NIMNSB:1||PTMNSB:1||ROOMTEMPERATURE FERROMAGNETISM:1||RUBIDIUM MANGANESE HEXACYANOFERRATE:1||COLOSSALMAGNETORESISTANCE:1||FINITE TEMPERATURES:1||LAMNO3:1||FE:1||transitionmetal oxides:1||giant magnetoresistance:1||phonon:1||COPPER OXIDES:1||valence states:1||thermoelectric:1||semiconductor:1||CATION DISTRIBUTION:1||FeCr2S4:1||photoemission spectroscopy (PES):1||METALLIC FERROMAGNETISM:1||GRAPHITE:1||SUSCEPTIBILITY:1||UBE13:1||RCrSb3:1||band JahnTeller:1||Ce3S4:1||TiO2:1||PrBa2Cu3O7delta:1||UNTWINNED PRBA2CU3O7:1||AGNIO2:1||HALFMETALLIC FERROMAGNETS:1||CI:1||Energy gap:1||Photoemission:1||Future applications:1||Photoemission measurements:1||Graphene:1||BANDSTRUCTURE:1||TC:1||superconductivity:1||magnetic semiconductors:1||CMRmanganites:1||thin films:1||spin dynamics:1||highTc superconductors:1||ITINERANTELECTRON FERROMAGNETISM:1||SINGLECRYSTALS:1||CeTe2:1||amorphous magnetic materials:1||EPITAXIAL GRAPHENE:1||LAYERED PNICTIDEOXIDES:1||BOROCARBIDE SUPERCONDUCTORS:1||AUGMENTEDWAVE METHOD:1||METALLIC MAGNET UNISN:1||ORIGIN:1||spectrum rearrangement:1||MEANFIELD THEORY:1||MOLECULEBASED MAGNETS:1||METASTABLE STATE:1||INSULATOR:1||magnetic orderin:1||FCC IRON:1||CeRu2:1||TL2MN2O7:1||isotope effect:1||Perovskitemanganites:1||RECURSION METHOD:1||PERPENDICULAR MAGNETICANISOTROPY:1||quasiparticle spectral density:1||GW:1||MANGANESE FERRITE:1||RESONANCE:1||SeCuO3:1||Optical conductivity:1||MASSLESS DIRAC FERMIONS:1||SCHOTTKYBARRIER:1||electronic structure:15||ELECTRONICSTRUCTURE:11||TRANSITIONMETAL COMPOUNDS:10||METALS:10||photoemission:8||SPECTRA:8||MAGNETORESISTANCE:7||FERROMAGNETISM:7||TRANSPORT:7||TRANSITION:6||FILMS:6||THINFILMS:5||TOTALENERGY CALCULATIONS:5||MAGNETICPROPERTIES:5||SUPERCONDUCTIVITY:5||PR:5||LATTICE:4||STATES:4||SPECTROSCOPY:4||FIELD:4||CRYSTALSTRUCTURE:4||PHOTOEMISSION:4||TEMPERATURE:4||TRANSITIONTEMPERATURE:4||XRAYABSORPTION:4||STATE:4||CU:4||BASISSET:4||XAS:4||CRYSTALS:3||EXCITATIONS:3||MOTTHUBBARD SYSTEMS:3||HIGHENERGY SPIN:3||halfmetal:3||INSULATORS:3||LA2CUO4:3||MODEL:3||FLUCTUATIONS:3||CE:3||double exchange:3||TRANSITIONMETALS:3||RESISTIVITY:3||BORON:3||LA1XCAXMNO3:3||IRON:3||PES:3||ANTIMONIDES:2||MgB2:2||ZR METALLIC GLASSES:2||superconductor:2||CRITICALCURRENT DENSITY:2||CIRCULARDICHROISM:2||SEMICONDUCTORS:2||LOCALIZATION:2||INTRABAND OPTICAL CONDUCTIVITY:2||COLOSSAL MAGNETORESISTANCE:2||OXIDATION:2||EXISTENCE:2||COPPER:2||diboride:2||MAGNESIUMDIBORIDE:2||GAP:2||CE COMPOUNDS:2||CORE POLARIZATION:2||magnetoresistance:2||photoemission spectroscopy:2||electronphonon interaction:2||GETTER:2||PD:2||MAGNETISM:2||FECR2S4:2||SUPERCONDUCTING MGB2:2||WIRES:2||ABSORPTION:2||ENERGY:2||LA1XSRXMNO3:2||CONSTANTS:2||polaron:2||charge ordering:2||SCATTERING:2||XRAY PHOTOEMISSION:2||CeNiSn:2||phase diagram:2||PHOTOELECTRON:2||QUADRUPOLAR:2||perovskitemanganites:2||CO:2||SYSTEMS:2||DOPED ZNO:2||LOWFREQUENCY SOUND:2||LA:2||ELECTRONELECTRON SCATTERING:2||AU:2||DENSITYWAVE INSTABILITY:2||FERMISURFACE:2||hybridization:2||VALENCEBAND SATELLITE:2||SULFUR SPINEL:2||Heusler:2||APPROXIMATION:2||superexchange:2||colossal magnetoresistance:2||ALLOYS:2||DEPENDENCE:2||AG:2||electronic structures:2||AUGERSPECTRA:2||CR:2||PARAMETERS:2||DIFFRACTION:2||SEMICONDUCTORMETAL TRANSITION:1||INTERMEDIATEVALENCE:1||SMB6:1||SRRUO3:1||antiperovskite structure with antipolar nature:1||lowenergy twodimensional phonons:1||anatase TiO2:1||La3S4:1||metalinsulator transitions:1||MNO:1||ELECTRONICSTRUCTURES:1||MAGNETIC CIRCULARDICHROISM:1||Density functional theory:1||CeCo2:1||TOPOLARON CROSSOVER:1||EXCHANGE:1||cuprates:1||high Tc cuprates:1||magnetically ordered materials:1||ZNSE:1||Sr2xKxFeMoO6:1||CDW:1||TeCuO3:1||STRUCTURALPROPERTIES:1||MN:1||screening length:1||amorphous Fe:1||WAVE BASISSET:1||SILICONCARBIDE:1||HIGHPRESSURE:1||electronphonon coupling:1||quenched superconductivity:1||CMR perovskite manganites:1||OXIDE:1||polarons:1||synchrotron radiation:1||FULLERIDES:1||RESONANTPHOTOEMISSION:1||Silicon carbide:1||DFT calculation:1||Hybridized bands:1||GIANT MAGNETORESISTANCE:1||PEROVSKITES:1||Raman spectra:1||EXCHANGE ENHANCEMENT:1||SILICON:1||SR2FEMOO6:1||orbital ordering:1||delafossite:1||TITANIUMDIOXIDE:1||electronic structure of disordered solids:1||YFE2:1||Magnetic polaron:1||NA2TI2SB2O:1||STRONGCOUPLED SUPERCONDUCTORS:1||HEAVYFERMION SYSTEMS:1||firstprinciples calculations:1||MECHANISM:1||UNiSn:1||PHOTONIC BANDGAP:1||SINGLE IMPURITY:1||PHONONSPECTRUM:1||FERMISURFACE TOPOLOGY:1||SUPPRESSION:1||RESONANT PHOTOEMISSION:1||METALDOPED PICENE:1||PHOTOIONIZATION CROSSSECTIONS:1||PHOTOINDUCED FERRIMAGNETIC SYSTEMS:1||LINKAGE ISOMERISM:1||CHARGETRANSFER:1||Bilayer Graphene:1||MAGNETICFIELD:1||SPINWAVES:1||rareearth manganese oxides:1||magnonphonon interaction:1||NACO2O4:1||ENERGYBANDS:1||SELFENERGY:1||GAS:1||Fe0.5Cu0.5Cr2S4:1||scanning photoelectron microscopy (SPEM):1||MAGNETIC PROPERTIES:1||Stoner model:1||AMORPHOUS TRANSITIONMETALS:1||SPINGLASS STATES:1||NI:1||LA3NI2B2N3:1||SOLIDS:1||CEO2:1||BAND THEORY:1||dilute magnetic semiconductor:1||pyrochlore:1||Y1XPRXBA2CU3O7DELTA:1||and electronphonon interactions:1||VIBRATIONS:1||RAY PHOTOEMISSION:1||ALKALI CATION:1||Europium:1||colossal magnetoresistance:1||structural stability:1||ENERGYGAP:1||small polaron:1||DOUBLE EXCHANGE:1||Coulomb correlation:1||magnon:1||phonons:1||ELECTRON FERROMAGNETISM:1||CURIETEMPERATURE:1||ARPES:1||PLANEWAVE METHOD:1||Xray absorption spectroscopy (XAS):1||ROOMTEMPERATURE:1||MONOCHALCOGENIDES:1||HEAT:1||UPDSN:1||MOMENTS:1||XRAY ABSORPTION:1||SEMICONDUCTOR:1||Fermi surface nesting:1||optical phonon:1||disordered system:1||dilute magnetic semiconductors:1||CMR manganites:1||PHONONS:1||LATTICEDYNAMICS:1||OXIDES:1||4fphotoemission:1||permanent magnet:1||pseudogap:1||TRANSPORTPROPERTIES:1||ANTIFERROMAGNET:1||(BI,PB)SRCOO SYSTEM:1||semicore correlation:1||POLARIZATION:1||CRYSTAL:1||spinel:1||Xray magnetic circular dichroism (XMCD):1||magnetocapacitance:1||ANATASE:1||TEMPERATURES:1||Pseudogap:1||INTERFACE:1||SUBSTRATE:1||YNI2B2C:1||SAMARIUM SULFIDE:1||strong swave superconductor:1||DOPED MANGANITE:1||SYMMETRY:1||CENISN:1||resonance mode:1||DISORDERED SYSTEM:1||LITHIUM INTERCALATION:1||CUO2 PLANE:1||SURFACE:1||Delafossite:1||ELECTRICALPROPERTIES:1||NIMNSB:1||PTMNSB:1||ROOMTEMPERATURE FERROMAGNETISM:1||RUBIDIUM MANGANESE HEXACYANOFERRATE:1||COLOSSALMAGNETORESISTANCE:1||FINITE TEMPERATURES:1||LAMNO3:1||FE:1||transitionmetal oxides:1||giant magnetoresistance:1||phonon:1||COPPER OXIDES:1||valence states:1||thermoelectric:1||semiconductor:1||CATION DISTRIBUTION:1||FeCr2S4:1||photoemission spectroscopy (PES):1||METALLIC FERROMAGNETISM:1||GRAPHITE:1||SUSCEPTIBILITY:1||UBE13:1||RCrSb3:1||band JahnTeller:1||Ce3S4:1||TiO2:1||PrBa2Cu3O7delta:1||UNTWINNED PRBA2CU3O7:1||AGNIO2:1||HALFMETALLIC FERROMAGNETS:1||CI:1||Energy gap:1||Photoemission:1||Future applications:1||Photoemission measurements:1||Graphene:1||BANDSTRUCTURE:1||TC:1||superconductivity:1||magnetic semiconductors:1||CMRmanganites:1||thin films:1||spin dynamics:1||highTc superconductors:1||ITINERANTELECTRON FERROMAGNETISM:1||SINGLECRYSTALS:1||CeTe2:1||amorphous magnetic materials:1||EPITAXIAL GRAPHENE:1||LAYERED PNICTIDEOXIDES:1||BOROCARBIDE SUPERCONDUCTORS:1||AUGMENTEDWAVE METHOD:1||METALLIC MAGNET UNISN:1||ORIGIN:1||spectrum rearrangement:1||MEANFIELD THEORY:1||MOLECULEBASED MAGNETS:1||METASTABLE STATE:1||INSULATOR:1||magnetic orderin:1||FCC IRON:1||CeRu2:1||TL2MN2O7:1||isotope effect:1||Perovskitemanganites:1||RECURSION METHOD:1||PERPENDICULAR MAGNETICANISOTROPY:1||quasiparticle spectral density:1||GW:1||MANGANESE FERRITE:1||RESONANCE:1||SeCuO3:1||Optical conductivity:1||MASSLESS DIRAC FERMIONS:1||SCHOTTKYBARRIER:1||electronic structure:15||ELECTRONICSTRUCTURE:11||TRANSITIONMETAL COMPOUNDS:10||METALS:10||photoemission:8||SPECTRA:8||MAGNETORESISTANCE:7||FERROMAGNETISM:7||TRANSPORT:7||TRANSITION:6||FILMS:6||THINFILMS:5||TOTALENERGY CALCULATIONS:5||MAGNETICPROPERTIES:5||SUPERCONDUCTIVITY:5||PR:5||LATTICE:4||STATES:4||SPECTROSCOPY:4||FIELD:4||CRYSTALSTRUCTURE:4||PHOTOEMISSION:4||TEMPERATURE:4||TRANSITIONTEMPERATURE:4||XRAYABSORPTION:4||STATE:4||CU:4||BASISSET:4||XAS:4||CRYSTALS:3||EXCITATIONS:3||MOTTHUBBARD SYSTEMS:3||HIGHENERGY SPIN:3||halfmetal:3||INSULATORS:3||LA2CUO4:3||MODEL:3||FLUCTUATIONS:3||CE:3||double exchange:3||TRANSITIONMETALS:3||RESISTIVITY:3||BORON:3||LA1XCAXMNO3:3||IRON:3||PES:3||ANTIMONIDES:2||MgB2:2||ZR METALLIC GLASSES:2||superconductor:2||CRITICALCURRENT DENSITY:2||CIRCULARDICHROISM:2||SEMICONDUCTORS:2||LOCALIZATION:2||INTRABAND OPTICAL CONDUCTIVITY:2||COLOSSAL MAGNETORESISTANCE:2||OXIDATION:2||EXISTENCE:2||COPPER:2||diboride:2||MAGNESIUMDIBORIDE:2||GAP:2||CE COMPOUNDS:2||CORE POLARIZATION:2||magnetoresistance:2||photoemission spectroscopy:2||electronphonon interaction:2||GETTER:2||PD:2||MAGNETISM:2||FECR2S4:2||SUPERCONDUCTING MGB2:2||WIRES:2||ABSORPTION:2||ENERGY:2||LA1XSRXMNO3:2||CONSTANTS:2||polaron:2||charge ordering:2||SCATTERING:2||XRAY PHOTOEMISSION:2||CeNiSn:2||phase diagram:2||PHOTOELECTRON:2||QUADRUPOLAR:2||perovskitemanganites:2||CO:2||SYSTEMS:2||DOPED ZNO:2||LOWFREQUENCY SOUND:2||LA:2||ELECTRONELECTRON SCATTERING:2||AU:2||DENSITYWAVE INSTABILITY:2||FERMISURFACE:2||hybridization:2||VALENCEBAND SATELLITE:2||SULFUR SPINEL:2||Heusler:2||APPROXIMATION:2||superexchange:2||colossal magnetoresistance:2||ALLOYS:2||DEPENDENCE:2||AG:2||electronic structures:2||AUGERSPECTRA:2||CR:2||PARAMETERS:2||DIFFRACTION:2||SEMICONDUCTORMETAL TRANSITION:1||INTERMEDIATEVALENCE:1||SMB6:1||SRRUO3:1||antiperovskite structure with antipolar nature:1||lowenergy twodimensional phonons:1||anatase TiO2:1||La3S4:1||metalinsulator transitions:1||MNO:1||ELECTRONICSTRUCTURES:1||MAGNETIC CIRCULARDICHROISM:1||Density functional theory:1||CeCo2:1||TOPOLARON CROSSOVER:1||EXCHANGE:1||cuprates:1||high Tc cuprates:1||magnetically ordered materials:1||ZNSE:1||Sr2xKxFeMoO6:1||CDW:1||TeCuO3:1||STRUCTURALPROPERTIES:1||MN:1||screening length:1||amorphous Fe:1||WAVE BASISSET:1||SILICONCARBIDE:1||HIGHPRESSURE:1||electronphonon coupling:1||quenched superconductivity:1||CMR perovskite manganites:1||OXIDE:1||polarons:1||synchrotron radiation:1||FULLERIDES:1||RESONANTPHOTOEMISSION:1||Silicon carbide:1||DFT calculation:1||Hybridized bands:1||GIANT MAGNETORESISTANCE:1||PEROVSKITES:1||Raman spectra:1||EXCHANGE ENHANCEMENT:1||SILICON:1||SR2FEMOO6:1||orbital ordering:1||delafossite:1||TITANIUMDIOXIDE:1||electronic structure of disordered solids:1||YFE2:1||Magnetic polaron:1||NA2TI2SB2O:1||STRONGCOUPLED SUPERCONDUCTORS:1||HEAVYFERMION SYSTEMS:1||firstprinciples calculations:1||MECHANISM:1||UNiSn:1||PHOTONIC BANDGAP:1||SINGLE IMPURITY:1||PHONONSPECTRUM:1||FERMISURFACE TOPOLOGY:1||SUPPRESSION:1||RESONANT PHOTOEMISSION:1||METALDOPED PICENE:1||PHOTOIONIZATION CROSSSECTIONS:1||PHOTOINDUCED FERRIMAGNETIC SYSTEMS:1||LINKAGE ISOMERISM:1||CHARGETRANSFER:1||Bilayer Graphene:1||MAGNETICFIELD:1||SPINWAVES:1||rareearth manganese oxides:1||magnonphonon interaction:1||NACO2O4:1||ENERGYBANDS:1||SELFENERGY:1||GAS:1||Fe0.5Cu0.5Cr2S4:1||scanning photoelectron microscopy (SPEM):1||MAGNETIC PROPERTIES:1||Stoner model:1||AMORPHOUS TRANSITIONMETALS:1||SPINGLASS STATES:1||NI:1||LA3NI2B2N3:1||SOLIDS:1||CEO2:1||BAND THEORY:1||dilute magnetic semiconductor:1||pyrochlore:1||Y1XPRXBA2CU3O7DELTA:1||and electronphonon interactions:1||VIBRATIONS:1||RAY PHOTOEMISSION:1||ALKALI CATION:1||Europium:1||colossal magnetoresistance:1||structural stability:1||ENERGYGAP:1||small polaron:1||DOUBLE EXCHANGE:1||Coulomb correlation:1||magnon:1||phonons:1||ELECTRON FERROMAGNETISM:1||CURIETEMPERATURE:1||ARPES:1||PLANEWAVE METHOD:1||Xray absorption spectroscopy (XAS):1||ROOMTEMPERATURE:1||MONOCHALCOGENIDES:1||HEAT:1||UPDSN:1||MOMENTS:1||XRAY ABSORPTION:1||SEMICONDUCTOR:1||Fermi surface nesting:1||optical phonon:1||disordered system:1||dilute magnetic semiconductors:1||CMR manganites:1||PHONONS:1||LATTICEDYNAMICS:1||OXIDES:1||4fphotoemission:1||permanent magnet:1||pseudogap:1||TRANSPORTPROPERTIES:1||ANTIFERROMAGNET:1||(BI,PB)SRCOO SYSTEM:1||semicore correlation:1||POLARIZATION:1||CRYSTAL:1||spinel:1||Xray magnetic circular dichroism (XMCD):1||magnetocapacitance:1||ANATASE:1||TEMPERATURES:1||Pseudogap:1||INTERFACE:1||SUBSTRATE:1||YNI2B2C:1||SAMARIUM SULFIDE:1||strong swave superconductor:1||DOPED MANGANITE:1||SYMMETRY:1||CENISN:1||resonance mode:1||DISORDERED SYSTEM:1||LITHIUM INTERCALATION:1||CUO2 PLANE:1||SURFACE:1||Delafossite:1||ELECTRICALPROPERTIES:1||NIMNSB:1||PTMNSB:1||ROOMTEMPERATURE FERROMAGNETISM:1||RUBIDIUM MANGANESE HEXACYANOFERRATE:1||COLOSSALMAGNETORESISTANCE:1||FINITE TEMPERATURES:1||LAMNO3:1||FE:1||transitionmetal oxides:1||giant magnetoresistance:1||phonon:1||COPPER OXIDES:1||valence states:1||thermoelectric:1||semiconductor:1||CATION DISTRIBUTION:1||FeCr2S4:1||photoemission spectroscopy (PES):1||METALLIC FERROMAGNETISM:1||GRAPHITE:1||SUSCEPTIBILITY:1||UBE13:1||RCrSb3:1||band JahnTeller:1||Ce3S4:1||TiO2:1||PrBa2Cu3O7delta:1||UNTWINNED PRBA2CU3O7:1||AGNIO2:1||HALFMETALLIC FERROMAGNETS:1||CI:1||Energy gap:1||Photoemission:1||Future applications:1||Photoemission measurements:1||Graphene:1||BANDSTRUCTURE:1||TC:1||superconductivity:1||magnetic semiconductors:1||CMRmanganites:1||thin films:1||spin dynamics:1||highTc superconductors:1||ITINERANTELECTRON FERROMAGNETISM:1||SINGLECRYSTALS:1||CeTe2:1||amorphous magnetic materials:1||EPITAXIAL GRAPHENE:1||LAYERED PNICTIDEOXIDES:1||BOROCARBIDE SUPERCONDUCTORS:1||AUGMENTEDWAVE METHOD:1||METALLIC MAGNET UNISN:1||ORIGIN:1||spectrum rearrangement:1||MEANFIELD THEORY:1||MOLECULEBASED MAGNETS:1||METASTABLE STATE:1||INSULATOR:1||magnetic orderin:1||FCC IRON:1||CeRu2:1||TL2MN2O7:1||isotope effect:1||Perovskitemanganites:1||RECURSION METHOD:1||PERPENDICULAR MAGNETICANISOTROPY:1||quasiparticle spectral density:1||GW:1||MANGANESE FERRITE:1||RESONANCE:1||SeCuO3:1||Optical conductivity:1||MASSLESS DIRAC FERMIONS:1||SCHOTTKYBARRIER:1||electronic structure:15||ELECTRONICSTRUCTURE:11||TRANSITIONMETAL COMPOUNDS:10||METALS:10||photoemission:8||SPECTRA:8||MAGNETORESISTANCE:7||FERROMAGNETISM:7||TRANSPORT:7||TRANSITION:6||FILMS:6||THINFILMS:5||TOTALENERGY CALCULATIONS:5||MAGNETICPROPERTIES:5||SUPERCONDUCTIVITY:5||PR:5||LATTICE:4||STATES:4||SPECTROSCOPY:4||FIELD:4||CRYSTALSTRUCTURE:4||PHOTOEMISSION:4||TEMPERATURE:4||TRANSITIONTEMPERATURE:4||XRAYABSORPTION:4||STATE:4||CU:4||BASISSET:4||XAS:4||CRYSTALS:3||EXCITATIONS:3||MOTTHUBBARD SYSTEMS:3||HIGHENERGY SPIN:3||halfmetal:3||INSULATORS:3||LA2CUO4:3||MODEL:3||FLUCTUATIONS:3||CE:3||double exchange:3||TRANSITIONMETALS:3||RESISTIVITY:3||BORON:3||LA1XCAXMNO3:3||IRON:3||PES:3||ANTIMONIDES:2||MgB2:2||ZR METALLIC GLASSES:2||superconductor:2||CRITICALCURRENT DENSITY:2||CIRCULARDICHROISM:2||SEMICONDUCTORS:2||LOCALIZATION:2||INTRABAND OPTICAL CONDUCTIVITY:2||COLOSSAL MAGNETORESISTANCE:2||OXIDATION:2||EXISTENCE:2||COPPER:2||diboride:2||MAGNESIUMDIBORIDE:2||GAP:2||CE COMPOUNDS:2||CORE POLARIZATION:2||magnetoresistance:2||photoemission spectroscopy:2||electronphonon interaction:2||GETTER:2||PD:2||MAGNETISM:2||FECR2S4:2||SUPERCONDUCTING MGB2:2||WIRES:2||ABSORPTION:2||ENERGY:2||LA1XSRXMNO3:2||CONSTANTS:2||polaron:2||charge ordering:2||SCATTERING:2||XRAY PHOTOEMISSION:2||CeNiSn:2||phase diagram:2||PHOTOELECTRON:2||QUADRUPOLAR:2||perovskitemanganites:2||CO:2||SYSTEMS:2||DOPED ZNO:2||LOWFREQUENCY SOUND:2||LA:2||ELECTRONELECTRON SCATTERING:2||AU:2||DENSITYWAVE INSTABILITY:2||FERMISURFACE:2||hybridization:2||VALENCEBAND SATELLITE:2||SULFUR SPINEL:2||Heusler:2||APPROXIMATION:2||superexchange:2||colossal magnetoresistance:2||ALLOYS:2||DEPENDENCE:2||AG:2||electronic structures:2||AUGERSPECTRA:2||CR:2||PARAMETERS:2||DIFFRACTION:2||SEMICONDUCTORMETAL TRANSITION:1||INTERMEDIATEVALENCE:1||SMB6:1||SRRUO3:1||antiperovskite structure with antipolar nature:1||lowenergy twodimensional phonons:1||anatase TiO2:1||La3S4:1||metalinsulator transitions:1||MNO:1||ELECTRONICSTRUCTURES:1||MAGNETIC CIRCULARDICHROISM:1||Density functional theory:1||CeCo2:1||TOPOLARON CROSSOVER:1||EXCHANGE:1||cuprates:1||high Tc cuprates:1||magnetically ordered materials:1||ZNSE:1||Sr2xKxFeMoO6:1||CDW:1||TeCuO3:1||STRUCTURALPROPERTIES:1||MN:1||screening length:1||amorphous Fe:1||WAVE BASISSET:1||SILICONCARBIDE:1||HIGHPRESSURE:1||electronphonon coupling:1||quenched superconductivity:1||CMR perovskite manganites:1||OXIDE:1||polarons:1||synchrotron radiation:1||FULLERIDES:1||RESONANTPHOTOEMISSION:1||Silicon carbide:1||DFT calculation:1||Hybridized bands:1||GIANT MAGNETORESISTANCE:1||PEROVSKITES:1||Raman spectra:1||EXCHANGE ENHANCEMENT:1||SILICON:1||SR2FEMOO6:1||orbital ordering:1||delafossite:1||TITANIUMDIOXIDE:1||electronic structure of disordered solids:1||YFE2:1||Magnetic polaron:1||NA2TI2SB2O:1||STRONGCOUPLED SUPERCONDUCTORS:1||HEAVYFERMION SYSTEMS:1||firstprinciples calculations:1||MECHANISM:1||UNiSn:1||PHOTONIC BANDGAP:1||SINGLE IMPURITY:1||PHONONSPECTRUM:1||FERMISURFACE TOPOLOGY:1||SUPPRESSION:1||RESONANT PHOTOEMISSION:1||METALDOPED PICENE:1||PHOTOIONIZATION CROSSSECTIONS:1||PHOTOINDUCED FERRIMAGNETIC SYSTEMS:1||LINKAGE ISOMERISM:1||CHARGETRANSFER:1||Bilayer Graphene:1||MAGNETICFIELD:1||SPINWAVES:1||rareearth manganese oxides:1||magnonphonon interaction:1||NACO2O4:1||ENERGYBANDS:1||SELFENERGY:1||GAS:1||Fe0.5Cu0.5Cr2S4:1||scanning photoelectron microscopy (SPEM):1||MAGNETIC PROPERTIES:1||Stoner model:1||AMORPHOUS TRANSITIONMETALS:1||SPINGLASS STATES:1||NI:1||LA3NI2B2N3:1||SOLIDS:1||CEO2:1||BAND THEORY:1||dilute magnetic semiconductor:1||pyrochlore:1||Y1XPRXBA2CU3O7DELTA:1||and electronphonon interactions:1||VIBRATIONS:1||RAY PHOTOEMISSION:1||ALKALI CATION:1||Europium:1||colossal magnetoresistance:1||structural stability:1||ENERGYGAP:1||small polaron:1||DOUBLE EXCHANGE:1||Coulomb correlation:1||magnon:1||phonons:1||ELECTRON FERROMAGNETISM:1||CURIETEMPERATURE:1||ARPES:1||PLANEWAVE METHOD:1||Xray absorption spectroscopy (XAS):1||ROOMTEMPERATURE:1||MONOCHALCOGENIDES:1||HEAT:1||UPDSN:1||MOMENTS:1||XRAY ABSORPTION:1||SEMICONDUCTOR:1||Fermi surface nesting:1||optical phonon:1||disordered system:1||dilute magnetic semiconductors:1||CMR manganites:1||PHONONS:1||LATTICEDYNAMICS:1||OXIDES:1||4fphotoemission:1||permanent magnet:1||pseudogap:1||TRANSPORTPROPERTIES:1||ANTIFERROMAGNET:1||(BI,PB)SRCOO SYSTEM:1||semicore correlation:1||POLARIZATION:1||CRYSTAL:1||spinel:1||Xray magnetic circular dichroism (XMCD):1||magnetocapacitance:1||ANATASE:1||TEMPERATURES:1||Pseudogap:1||INTERFACE:1||SUBSTRATE:1||YNI2B2C:1||SAMARIUM SULFIDE:1||strong swave superconductor:1||DOPED MANGANITE:1||SYMMETRY:1||CENISN:1||resonance mode:1||DISORDERED SYSTEM:1||LITHIUM INTERCALATION:1||CUO2 PLANE:1||SURFACE:1||Delafossite:1||ELECTRICALPROPERTIES:1||NIMNSB:1||PTMNSB:1||ROOMTEMPERATURE FERROMAGNETISM:1||RUBIDIUM MANGANESE HEXACYANOFERRATE:1||COLOSSALMAGNETORESISTANCE:1||FINITE TEMPERATURES:1||LAMNO3:1||FE:1||transitionmetal oxides:1||giant magnetoresistance:1||phonon:1||COPPER OXIDES:1||valence states:1||thermoelectric:1||semiconductor:1||CATION DISTRIBUTION:1||FeCr2S4:1||photoemission spectroscopy (PES):1||METALLIC FERROMAGNETISM:1||GRAPHITE:1||SUSCEPTIBILITY:1||UBE13:1||RCrSb3:1||band JahnTeller:1||Ce3S4:1||TiO2:1||PrBa2Cu3O7delta:1||UNTWINNED PRBA2CU3O7:1||AGNIO2:1||HALFMETALLIC FERROMAGNETS:1||CI:1||Energy gap:1||Photoemission:1||Future applications:1||Photoemission measurements:1||Graphene:1||BANDSTRUCTURE:1||TC:1||superconductivity:1||magnetic semiconductors:1||CMRmanganites:1||thin films:1||spin dynamics:1||highTc superconductors:1||ITINERANTELECTRON FERROMAGNETISM:1||SINGLECRYSTALS:1||CeTe2:1||amorphous magnetic materials:1||EPITAXIAL GRAPHENE:1||LAYERED PNICTIDEOXIDES:1||BOROCARBIDE SUPERCONDUCTORS:1||AUGMENTEDWAVE METHOD:1||METALLIC MAGNET UNISN:1||ORIGIN:1||spectrum rearrangement:1||MEANFIELD THEORY:1||MOLECULEBASED MAGNETS:1||METASTABLE STATE:1||INSULATOR:1||magnetic orderin:1||FCC IRON:1||CeRu2:1||TL2MN2O7:1||isotope effect:1||Perovskitemanganites:1||RECURSION METHOD:1||PERPENDICULAR MAGNETICANISOTROPY:1||quasiparticle spectral density:1||GW:1||MANGANESE FERRITE:1||RESONANCE:1||SeCuO3:1||Optical conductivity:1||MASSLESS DIRAC FERMIONS:1||SCHOTTKYBARRIER:1||electronic structure:15||ELECTRONICSTRUCTURE:11||TRANSITIONMETAL COMPOUNDS:10||METALS:10||photoemission:8||SPECTRA:8||MAGNETORESISTANCE:7||FERROMAGNETISM:7||TRANSPORT:7||TRANSITION:6||FILMS:6||THINFILMS:5||TOTALENERGY CALCULATIONS:5||MAGNETICPROPERTIES:5||SUPERCONDUCTIVITY:5||PR:5||LATTICE:4||STATES:4||SPECTROSCOPY:4||FIELD:4||CRYSTALSTRUCTURE:4||PHOTOEMISSION:4||TEMPERATURE:4||TRANSITIONTEMPERATURE:4||XRAYABSORPTION:4||STATE:4||CU:4||BASISSET:4||XAS:4||CRYSTALS:3||EXCITATIONS:3||MOTTHUBBARD SYSTEMS:3||HIGHENERGY SPIN:3||halfmetal:3||INSULATORS:3||LA2CUO4:3||MODEL:3||FLUCTUATIONS:3||CE:3||double exchange:3||TRANSITIONMETALS:3||RESISTIVITY:3||BORON:3||LA1XCAXMNO3:3||IRON:3||PES:3||ANTIMONIDES:2||MgB2:2||ZR METALLIC GLASSES:2||superconductor:2||CRITICALCURRENT DENSITY:2||CIRCULARDICHROISM:2||SEMICONDUCTORS:2||LOCALIZATION:2||INTRABAND OPTICAL CONDUCTIVITY:2||COLOSSAL MAGNETORESISTANCE:2||OXIDATION:2||EXISTENCE:2||COPPER:2||diboride:2||MAGNESIUMDIBORIDE:2||GAP:2||CE COMPOUNDS:2||CORE POLARIZATION:2||magnetoresistance:2||photoemission spectroscopy:2||electronphonon interaction:2||GETTER:2||PD:2||MAGNETISM:2||FECR2S4:2||SUPERCONDUCTING MGB2:2||WIRES:2||ABSORPTION:2||ENERGY:2||LA1XSRXMNO3:2||CONSTANTS:2||polaron:2||charge ordering:2||SCATTERING:2||XRAY PHOTOEMISSION:2||CeNiSn:2||phase diagram:2||PHOTOELECTRON:2||QUADRUPOLAR:2||perovskitemanganites:2||CO:2||SYSTEMS:2||DOPED ZNO:2||LOWFREQUENCY SOUND:2||LA:2||ELECTRONELECTRON SCATTERING:2||AU:2||DENSITYWAVE INSTABILITY:2||FERMISURFACE:2||hybridization:2||VALENCEBAND SATELLITE:2||SULFUR SPINEL:2||Heusler:2||APPROXIMATION:2||superexchange:2||colossal magnetoresistance:2||ALLOYS:2||DEPENDENCE:2||AG:2||electronic structures:2||AUGERSPECTRA:2||CR:2||PARAMETERS:2||DIFFRACTION:2||SEMICONDUCTORMETAL TRANSITION:1||INTERMEDIATEVALENCE:1||SMB6:1||SRRUO3:1||antiperovskite structure with antipolar nature:1||lowenergy twodimensional phonons:1||anatase TiO2:1||La3S4:1||metalinsulator transitions:1||MNO:1||ELECTRONICSTRUCTURES:1||MAGNETIC CIRCULARDICHROISM:1||Density functional theory:1||CeCo2:1||TOPOLARON CROSSOVER:1||EXCHANGE:1||cuprates:1||high Tc cuprates:1||magnetically ordered materials:1||ZNSE:1||Sr2xKxFeMoO6:1||CDW:1||TeCuO3:1||STRUCTURALPROPERTIES:1||MN:1||screening length:1||amorphous Fe:1||WAVE BASISSET:1||SILICONCARBIDE:1||HIGHPRESSURE:1||electronphonon coupling:1||quenched superconductivity:1||CMR perovskite manganites:1||OXIDE:1||polarons:1||synchrotron radiation:1||FULLERIDES:1||RESONANTPHOTOEMISSION:1||Silicon carbide:1||DFT calculation:1||Hybridized bands:1||GIANT MAGNETORESISTANCE:1||PEROVSKITES:1||Raman spectra:1||EXCHANGE ENHANCEMENT:1||SILICON:1||SR2FEMOO6:1||orbital ordering:1||delafossite:1||TITANIUMDIOXIDE:1||electronic structure of disordered solids:1||YFE2:1||Magnetic polaron:1||NA2TI2SB2O:1||STRONGCOUPLED SUPERCONDUCTORS:1||HEAVYFERMION SYSTEMS:1||firstprinciples calculations:1||MECHANISM:1||UNiSn:1||PHOTONIC BANDGAP:1||SINGLE IMPURITY:1||PHONONSPECTRUM:1||FERMISURFACE TOPOLOGY:1||SUPPRESSION:1||RESONANT PHOTOEMISSION:1||METALDOPED PICENE:1||PHOTOIONIZATION CROSSSECTIONS:1||PHOTOINDUCED FERRIMAGNETIC SYSTEMS:1||LINKAGE ISOMERISM:1||CHARGETRANSFER:1||Bilayer Graphene:1||MAGNETICFIELD:1||SPINWAVES:1||rareearth manganese oxides:1||magnonphonon interaction:1||NACO2O4:1||ENERGYBANDS:1||SELFENERGY:1||GAS:1||Fe0.5Cu0.5Cr2S4:1||scanning photoelectron microscopy (SPEM):1||MAGNETIC PROPERTIES:1||Stoner model:1||AMORPHOUS TRANSITIONMETALS:1||SPINGLASS STATES:1||NI:1||LA3NI2B2N3:1||SOLIDS:1||CEO2:1||BAND THEORY:1||dilute magnetic semiconductor:1||pyrochlore:1||Y1XPRXBA2CU3O7DELTA:1||and electronphonon interactions:1||VIBRATIONS:1||RAY PHOTOEMISSION:1||ALKALI CATION:1||Europium:1||colossal magnetoresistance:1||structural stability:1||ENERGYGAP:1||small polaron:1||DOUBLE EXCHANGE:1||Coulomb correlation:1||magnon:1||phonons:1||ELECTRON FERROMAGNETISM:1||CURIETEMPERATURE:1||ARPES:1||PLANEWAVE METHOD:1||Xray absorption spectroscopy (XAS):1||ROOMTEMPERATURE:1||MONOCHALCOGENIDES:1||HEAT:1||UPDSN:1||MOMENTS:1||XRAY ABSORPTION:1||SEMICONDUCTOR:1||Fermi surface nesting:1||optical phonon:1||disordered system:1||dilute magnetic semiconductors:1||CMR manganites:1||PHONONS:1||LATTICEDYNAMICS:1||OXIDES:1||4fphotoemission:1||permanent magnet:1||pseudogap:1||TRANSPORTPROPERTIES:1||ANTIFERROMAGNET:1||(BI,PB)SRCOO SYSTEM:1||semicore correlation:1||POLARIZATION:1||CRYSTAL:1||spinel:1||Xray magnetic circular dichroism (XMCD):1||magnetocapacitance:1||ANATASE:1||TEMPERATURES:1||Pseudogap:1||INTERFACE:1||SUBSTRATE:1||YNI2B2C:1||SAMARIUM SULFIDE:1||strong swave superconductor:1||DOPED MANGANITE:1||SYMMETRY:1||CENISN:1||resonance mode:1||DISORDERED SYSTEM:1||LITHIUM INTERCALATION:1||CUO2 PLANE:1||SURFACE:1||Delafossite:1||ELECTRICALPROPERTIES:1||NIMNSB:1||PTMNSB:1||ROOMTEMPERATURE FERROMAGNETISM:1||RUBIDIUM MANGANESE HEXACYANOFERRATE:1||COLOSSALMAGNETORESISTANCE:1||FINITE TEMPERATURES:1||LAMNO3:1||FE:1||transitionmetal oxides:1||giant magnetoresistance:1||phonon:1||COPPER OXIDES:1||valence states:1||thermoelectric:1||semiconductor:1||CATION DISTRIBUTION:1||FeCr2S4:1||photoemission spectroscopy (PES):1||METALLIC FERROMAGNETISM:1||GRAPHITE:1||SUSCEPTIBILITY:1||UBE13:1||RCrSb3:1||band JahnTeller:1||Ce3S4:1||TiO2:1||PrBa2Cu3O7delta:1||UNTWINNED PRBA2CU3O7:1||AGNIO2:1||HALFMETALLIC FERROMAGNETS:1||CI:1||Energy gap:1||Photoemission:1||Future applications:1||Photoemission measurements:1||Graphene:1||BANDSTRUCTURE:1||TC:1||superconductivity:1||magnetic semiconductors:1||CMRmanganites:1||thin films:1||spin dynamics:1||highTc superconductors:1||ITINERANTELECTRON FERROMAGNETISM:1||SINGLECRYSTALS:1||CeTe2:1||amorphous magnetic materials:1||EPITAXIAL GRAPHENE:1||LAYERED PNICTIDEOXIDES:1||BOROCARBIDE SUPERCONDUCTORS:1||AUGMENTEDWAVE METHOD:1||METALLIC MAGNET UNISN:1||ORIGIN:1||spectrum rearrangement:1||MEANFIELD THEORY:1||MOLECULEBASED MAGNETS:1||METASTABLE STATE:1||INSULATOR:1||magnetic orderin:1||FCC IRON:1||CeRu2:1||TL2MN2O7:1||isotope effect:1||Perovskitemanganites:1||RECURSION METHOD:1||PERPENDICULAR MAGNETICANISOTROPY:1||quasiparticle spectral density:1||GW:1||MANGANESE FERRITE:1||RESONANCE:1||SeCuO3:1||Optical conductivity:1||MASSLESS DIRAC FERMIONS:1||SCHOTTKYBARRIER:1||electronic structure:15||ELECTRONICSTRUCTURE:11||TRANSITIONMETAL COMPOUNDS:10||METALS:10||photoemission:8||SPECTRA:8||MAGNETORESISTANCE:7||FERROMAGNETISM:7||TRANSPORT:7||TRANSITION:6||FILMS:6||THINFILMS:5||TOTALENERGY CALCULATIONS:5||MAGNETICPROPERTIES:5||SUPERCONDUCTIVITY:5||PR:5||LATTICE:4||STATES:4||SPECTROSCOPY:4||FIELD:4||CRYSTALSTRUCTURE:4||PHOTOEMISSION:4||TEMPERATURE:4||TRANSITIONTEMPERATURE:4||XRAYABSORPTION:4||STATE:4||CU:4||BASISSET:4||XAS:4||CRYSTALS:3||EXCITATIONS:3||MOTTHUBBARD SYSTEMS:3||HIGHENERGY SPIN:3||halfmetal:3||INSULATORS:3||LA2CUO4:3||MODEL:3||FLUCTUATIONS:3||CE:3||double exchange:3||TRANSITIONMETALS:3||RESISTIVITY:3||BORON:3||LA1XCAXMNO3:3||IRON:3||PES:3||ANTIMONIDES:2||MgB2:2||ZR METALLIC GLASSES:2||superconductor:2||CRITICALCURRENT DENSITY:2||CIRCULARDICHROISM:2||SEMICONDUCTORS:2||LOCALIZATION:2||INTRABAND OPTICAL CONDUCTIVITY:2||COLOSSAL MAGNETORESISTANCE:2||OXIDATION:2||EXISTENCE:2||COPPER:2||diboride:2||MAGNESIUMDIBORIDE:2||GAP:2||CE COMPOUNDS:2||CORE POLARIZATION:2||magnetoresistance:2||photoemission spectroscopy:2||electronphonon interaction:2||GETTER:2||PD:2||MAGNETISM:2||FECR2S4:2||SUPERCONDUCTING MGB2:2||WIRES:2||ABSORPTION:2||ENERGY:2||LA1XSRXMNO3:2||CONSTANTS:2||polaron:2||charge ordering:2||SCATTERING:2||XRAY PHOTOEMISSION:2||CeNiSn:2||phase diagram:2||PHOTOELECTRON:2||QUADRUPOLAR:2||perovskitemanganites:2||CO:2||SYSTEMS:2||DOPED ZNO:2||LOWFREQUENCY SOUND:2||LA:2||ELECTRONELECTRON SCATTERING:2||AU:2||DENSITYWAVE INSTABILITY:2||FERMISURFACE:2||hybridization:2||VALENCEBAND SATELLITE:2||SULFUR SPINEL:2||Heusler:2||APPROXIMATION:2||superexchange:2||colossal magnetoresistance:2||ALLOYS:2||DEPENDENCE:2||AG:2||electronic structures:2||AUGERSPECTRA:2||CR:2||PARAMETERS:2||DIFFRACTION:2||SEMICONDUCTORMETAL TRANSITION:1||INTERMEDIATEVALENCE:1||SMB6:1||SRRUO3:1||antiperovskite structure with antipolar nature:1||lowenergy twodimensional phonons:1||anatase TiO2:1||La3S4:1||metalinsulator transitions:1||MNO:1||ELECTRONICSTRUCTURES:1||MAGNETIC CIRCULARDICHROISM:1||Density functional theory:1||CeCo2:1||TOPOLARON CROSSOVER:1||EXCHANGE:1||cuprates:1||high Tc cuprates:1||magnetically ordered materials:1||ZNSE:1||Sr2xKxFeMoO6:1||CDW:1||TeCuO3:1||STRUCTURALPROPERTIES:1||MN:1||screening length:1||amorphous Fe:1||WAVE BASISSET:1||SILICONCARBIDE:1||HIGHPRESSURE:1||electronphonon coupling:1||quenched superconductivity:1||CMR perovskite manganites:1||OXIDE:1||polarons:1||synchrotron radiation:1||FULLERIDES:1||RESONANTPHOTOEMISSION:1||Silicon carbide:1||DFT calculation:1||Hybridized bands:1||GIANT MAGNETORESISTANCE:1||PEROVSKITES:1||Raman spectra:1||EXCHANGE ENHANCEMENT:1||SILICON:1||SR2FEMOO6:1||orbital ordering:1||delafossite:1||TITANIUMDIOXIDE:1||electronic structure of disordered solids:1||YFE2:1||Magnetic polaron:1||NA2TI2SB2O:1||STRONGCOUPLED SUPERCONDUCTORS:1||HEAVYFERMION SYSTEMS:1||firstprinciples calculations:1||MECHANISM:1||UNiSn:1||PHOTONIC BANDGAP:1||SINGLE IMPURITY:1||PHONONSPECTRUM:1||FERMISURFACE TOPOLOGY:1||SUPPRESSION:1||RESONANT PHOTOEMISSION:1||METALDOPED PICENE:1||PHOTOIONIZATION CROSSSECTIONS:1||PHOTOINDUCED FERRIMAGNETIC SYSTEMS:1||LINKAGE ISOMERISM:1||CHARGETRANSFER:1||Bilayer Graphene:1||MAGNETICFIELD:1||SPINWAVES:1||rareearth manganese oxides:1||magnonphonon interaction:1||NACO2O4:1||ENERGYBANDS:1||SELFENERGY:1||GAS:1||Fe0.5Cu0.5Cr2S4:1||scanning photoelectron microscopy (SPEM):1||MAGNETIC PROPERTIES:1||Stoner model:1||AMORPHOUS TRANSITIONMETALS:1||SPINGLASS STATES:1||NI:1||LA3NI2B2N3:1||SOLIDS:1||CEO2:1||BAND THEORY:1||dilute magnetic semiconductor:1||pyrochlore:1||Y1XPRXBA2CU3O7DELTA:1||and electronphonon interactions:1||VIBRATIONS:1||RAY PHOTOEMISSION:1||ALKALI CATION:1||Europium:1||colossal magnetoresistance:1||structural stability:1||ENERGYGAP:1||small polaron:1||DOUBLE EXCHANGE:1||Coulomb correlation:1||magnon:1||phonons:1||ELECTRON FERROMAGNETISM:1||CURIETEMPERATURE:1||ARPES:1||PLANEWAVE METHOD:1||Xray absorption spectroscopy (XAS):1||ROOMTEMPERATURE:1||MONOCHALCOGENIDES:1||HEAT:1||UPDSN:1||MOMENTS:1||XRAY ABSORPTION:1||SEMICONDUCTOR:1||Fermi surface nesting:1||optical phonon:1||disordered system:1||dilute magnetic semiconductors:1||CMR manganites:1||PHONONS:1||LATTICEDYNAMICS:1||OXIDES:1||4fphotoemission:1||permanent magnet:1||pseudogap:1||TRANSPORTPROPERTIES:1||ANTIFERROMAGNET:1||(BI,PB)SRCOO SYSTEM:1||semicore correlation:1||POLARIZATION:1||CRYSTAL:1||spinel:1||Xray magnetic circular dichroism (XMCD):1||magnetocapacitance:1||ANATASE:1||TEMPERATURES:1||Pseudogap:1||INTERFACE:1||SUBSTRATE:1||YNI2B2C:1||SAMARIUM SULFIDE:1||strong swave superconductor:1||DOPED MANGANITE:1||SYMMETRY:1||CENISN:1||resonance mode:1||DISORDERED SYSTEM:1||LITHIUM INTERCALATION:1||CUO2 PLANE:1||SURFACE:1||Delafossite:1||ELECTRICALPROPERTIES:1||NIMNSB:1||PTMNSB:1||ROOMTEMPERATURE FERROMAGNETISM:1||RUBIDIUM MANGANESE HEXACYANOFERRATE:1||COLOSSALMAGNETORESISTANCE:1||FINITE TEMPERATURES:1||LAMNO3:1||FE:1||transitionmetal oxides:1||giant magnetoresistance:1||phonon:1||COPPER OXIDES:1||valence states:1||thermoelectric:1||semiconductor:1||CATION DISTRIBUTION:1||FeCr2S4:1||photoemission spectroscopy (PES):1||METALLIC FERROMAGNETISM:1||GRAPHITE:1||SUSCEPTIBILITY:1||UBE13:1||RCrSb3:1||band JahnTeller:1||Ce3S4:1||TiO2:1||PrBa2Cu3O7delta:1||UNTWINNED PRBA2CU3O7:1||AGNIO2:1||HALFMETALLIC FERROMAGNETS:1||CI:1||Energy gap:1||Photoemission:1||Future applications:1||Photoemission measurements:1||Graphene:1||BANDSTRUCTURE:1||TC:1||superconductivity:1||magnetic semiconductors:1||CMRmanganites:1||thin films:1||spin dynamics:1||highTc superconductors:1||ITINERANTELECTRON FERROMAGNETISM:1||SINGLECRYSTALS:1||CeTe2:1||amorphous magnetic materials:1||EPITAXIAL GRAPHENE:1||LAYERED PNICTIDEOXIDES:1||BOROCARBIDE SUPERCONDUCTORS:1||AUGMENTEDWAVE METHOD:1||METALLIC MAGNET UNISN:1||ORIGIN:1||spectrum rearrangement:1||MEANFIELD THEORY:1||MOLECULEBASED MAGNETS:1||METASTABLE STATE:1||INSULATOR:1||magnetic orderin:1||FCC IRON:1||CeRu2:1||TL2MN2O7:1||isotope effect:1||Perovskitemanganites:1||RECURSION METHOD:1||PERPENDICULAR MAGNETICANISOTROPY:1||quasiparticle spectral density:1||GW:1||MANGANESE FERRITE:1||RESONANCE:1||SeCuO3:1||Optical conductivity:1||MASSLESS DIRAC FERMIONS:1||SCHOTTKYBARRIER:1||electronic structure:15||ELECTRONICSTRUCTURE:11||TRANSITIONMETAL COMPOUNDS:10||METALS:10||photoemission:8||SPECTRA:8||MAGNETORESISTANCE:7||FERROMAGNETISM:7||TRANSPORT:7||TRANSITION:6||FILMS:6||THINFILMS:5||TOTALENERGY CALCULATIONS:5||MAGNETICPROPERTIES:5||SUPERCONDUCTIVITY:5||PR:5||LATTICE:4||STATES:4||SPECTROSCOPY:4||FIELD:4||CRYSTALSTRUCTURE:4||PHOTOEMISSION:4||TEMPERATURE:4||TRANSITIONTEMPERATURE:4||XRAYABSORPTION:4||STATE:4||CU:4||BASISSET:4||XAS:4||CRYSTALS:3||EXCITATIONS:3||MOTTHUBBARD SYSTEMS:3||HIGHENERGY SPIN:3||halfmetal:3||INSULATORS:3||LA2CUO4:3||MODEL:3||FLUCTUATIONS:3||CE:3||double exchange:3||TRANSITIONMETALS:3||RESISTIVITY:3||BORON:3||LA1XCAXMNO3:3||IRON:3||PES:3||ANTIMONIDES:2||MgB2:2||ZR METALLIC GLASSES:2||superconductor:2||CRITICALCURRENT DENSITY:2||CIRCULARDICHROISM:2||SEMICONDUCTORS:2||LOCALIZATION:2||INTRABAND OPTICAL CONDUCTIVITY:2||COLOSSAL MAGNETORESISTANCE:2||OXIDATION:2||EXISTENCE:2||COPPER:2||diboride:2||MAGNESIUMDIBORIDE:2||GAP:2||CE COMPOUNDS:2||CORE POLARIZATION:2||magnetoresistance:2||photoemission spectroscopy:2||electronphonon interaction:2||GETTER:2||PD:2||MAGNETISM:2||FECR2S4:2||SUPERCONDUCTING MGB2:2||WIRES:2||ABSORPTION:2||ENERGY:2||LA1XSRXMNO3:2||CONSTANTS:2||polaron:2||charge ordering:2||SCATTERING:2||XRAY PHOTOEMISSION:2||CeNiSn:2||phase diagram:2||PHOTOELECTRON:2||QUADRUPOLAR:2||perovskitemanganites:2||CO:2||SYSTEMS:2||DOPED ZNO:2||LOWFREQUENCY SOUND:2||LA:2||ELECTRONELECTRON SCATTERING:2||AU:2||DENSITYWAVE INSTABILITY:2||FERMISURFACE:2||hybridization:2||VALENCEBAND SATELLITE:2||SULFUR SPINEL:2||Heusler:2||APPROXIMATION:2||superexchange:2||colossal magnetoresistance:2||ALLOYS:2||DEPENDENCE:2||AG:2||electronic structures:2||AUGERSPECTRA:2||CR:2||PARAMETERS:2||DIFFRACTION:2||SEMICONDUCTORMETAL TRANSITION:1||INTERMEDIATEVALENCE:1||SMB6:1||SRRUO3:1||antiperovskite structure with antipolar nature:1||lowenergy twodimensional phonons:1||anatase TiO2:1||La3S4:1||metalinsulator transitions:1||MNO:1||ELECTRONICSTRUCTURES:1||MAGNETIC CIRCULARDICHROISM:1||Density functional theory:1||CeCo2:1||TOPOLARON CROSSOVER:1||EXCHANGE:1||cuprates:1||high Tc cuprates:1||magnetically ordered materials:1||ZNSE:1||Sr2xKxFeMoO6:1||CDW:1||TeCuO3:1||STRUCTURALPROPERTIES:1||MN:1||screening length:1||amorphous Fe:1||WAVE BASISSET:1||SILICONCARBIDE:1||HIGHPRESSURE:1||electronphonon coupling:1||quenched superconductivity:1||CMR perovskite manganites:1||OXIDE:1||polarons:1||synchrotron radiation:1||FULLERIDES:1||RESONANTPHOTOEMISSION:1||Silicon carbide:1||DFT calculation:1||Hybridized bands:1||GIANT MAGNETORESISTANCE:1||PEROVSKITES:1||Raman spectra:1||EXCHANGE ENHANCEMENT:1||SILICON:1||SR2FEMOO6:1||orbital ordering:1||delafossite:1||TITANIUMDIOXIDE:1||electronic structure of disordered solids:1||YFE2:1||Magnetic polaron:1||NA2TI2SB2O:1||STRONGCOUPLED SUPERCONDUCTORS:1||HEAVYFERMION SYSTEMS:1||firstprinciples calculations:1||MECHANISM:1||UNiSn:1||PHOTONIC BANDGAP:1||SINGLE IMPURITY:1||PHONONSPECTRUM:1||FERMISURFACE TOPOLOGY:1||SUPPRESSION:1||RESONANT PHOTOEMISSION:1||METALDOPED PICENE:1||PHOTOIONIZATION CROSSSECTIONS:1||PHOTOINDUCED FERRIMAGNETIC SYSTEMS:1||LINKAGE ISOMERISM:1||CHARGETRANSFER:1||Bilayer Graphene:1||MAGNETICFIELD:1||SPINWAVES:1||rareearth manganese oxides:1||magnonphonon interaction:1||NACO2O4:1||ENERGYBANDS:1||SELFENERGY:1||GAS:1||Fe0.5Cu0.5Cr2S4:1||scanning photoelectron microscopy (SPEM):1||MAGNETIC PROPERTIES:1||Stoner model:1||AMORPHOUS TRANSITIONMETALS:1||SPINGLASS STATES:1||NI:1||LA3NI2B2N3:1||SOLIDS:1||CEO2:1||BAND THEORY:1||dilute magnetic semiconductor:1||pyrochlore:1||Y1XPRXBA2CU3O7DELTA:1||and electronphonon interactions:1||VIBRATIONS:1||RAY PHOTOEMISSION:1||ALKALI CATION:1||Europium:1||colossal magnetoresistance:1||structural stability:1||ENERGYGAP:1||small polaron:1||DOUBLE EXCHANGE:1||Coulomb correlation:1||magnon:1||phonons:1||ELECTRON FERROMAGNETISM:1||CURIETEMPERATURE:1||ARPES:1||PLANEWAVE METHOD:1||Xray absorption spectroscopy (XAS):1||ROOMTEMPERATURE:1||MONOCHALCOGENIDES:1||HEAT:1||UPDSN:1||MOMENTS:1||XRAY ABSORPTION:1||SEMICONDUCTOR:1||Fermi surface nesting:1||optical phonon:1||disordered system:1||dilute magnetic semiconductors:1||CMR manganites:1||PHONONS:1||LATTICEDYNAMICS:1||OXIDES:1||4fphotoemission:1||permanent magnet:1||pseudogap:1||TRANSPORTPROPERTIES:1||ANTIFERROMAGNET:1||(BI,PB)SRCOO SYSTEM:1||semicore correlation:1||POLARIZATION:1||CRYSTAL:1||spinel:1||Xray magnetic circular dichroism (XMCD):1||magnetocapacitance:1||ANATASE:1||TEMPERATURES:1||Pseudogap:1||INTERFACE:1||SUBSTRATE:1||YNI2B2C:1||SAMARIUM SULFIDE:1||strong swave superconductor:1||DOPED MANGANITE:1||SYMMETRY:1||CENISN:1||resonance mode:1||DISORDERED SYSTEM:1||LITHIUM INTERCALATION:1||CUO2 PLANE:1||SURFACE:1||Delafossite:1||ELECTRICALPROPERTIES:1||NIMNSB:1||PTMNSB:1||ROOMTEMPERATURE FERROMAGNETISM:1||RUBIDIUM MANGANESE HEXACYANOFERRATE:1||COLOSSALMAGNETORESISTANCE:1||FINITE TEMPERATURES:1||LAMNO3:1||FE:1||transitionmetal oxides:1||giant magnetoresistance:1||phonon:1||COPPER OXIDES:1||valence states:1||thermoelectric:1||semiconductor:1||CATION DISTRIBUTION:1||FeCr2S4:1||photoemission spectroscopy (PES):1||METALLIC FERROMAGNETISM:1||GRAPHITE:1||SUSCEPTIBILITY:1||UBE13:1||RCrSb3:1||band JahnTeller:1||Ce3S4:1||TiO2:1||PrBa2Cu3O7delta:1||UNTWINNED PRBA2CU3O7:1||AGNIO2:1||HALFMETALLIC FERROMAGNETS:1||CI:1||Energy gap:1||Photoemission:1||Future applications:1||Photoemission measurements:1||Graphene:1||BANDSTRUCTURE:1||TC:1||superconductivity:1||magnetic semiconductors:1||CMRmanganites:1||thin films:1||spin dynamics:1||highTc superconductors:1||ITINERANTELECTRON FERROMAGNETISM:1||SINGLECRYSTALS:1||CeTe2:1||amorphous magnetic materials:1||EPITAXIAL GRAPHENE:1||LAYERED PNICTIDEOXIDES:1||BOROCARBIDE SUPERCONDUCTORS:1||AUGMENTEDWAVE METHOD:1||METALLIC MAGNET UNISN:1||ORIGIN:1||spectrum rearrangement:1||MEANFIELD THEORY:1||MOLECULEBASED MAGNETS:1||METASTABLE STATE:1||INSULATOR:1||magnetic orderin:1||FCC IRON:1||CeRu2:1||TL2MN2O7:1||isotope effect:1||Perovskitemanganites:1||RECURSION METHOD:1||PERPENDICULAR MAGNETICANISOTROPY:1||quasiparticle spectral density:1||GW:1||MANGANESE FERRITE:1||RESONANCE:1||SeCuO3:1||Optical conductivity:1||MASSLESS DIRAC FERMIONS:1||SCHOTTKYBARRIER:1||electronic structure:15||ELECTRONICSTRUCTURE:11||TRANSITIONMETAL COMPOUNDS:10||METALS:10||photoemission:8||SPECTRA:8||MAGNETORESISTANCE:7||FERROMAGNETISM:7||TRANSPORT:7||TRANSITION:6||FILMS:6||THINFILMS:5||TOTALENERGY CALCULATIONS:5||MAGNETICPROPERTIES:5||SUPERCONDUCTIVITY:5||PR:5||LATTICE:4||STATES:4||SPECTROSCOPY:4||FIELD:4||CRYSTALSTRUCTURE:4||PHOTOEMISSION:4||TEMPERATURE:4||TRANSITIONTEMPERATURE:4||XRAYABSORPTION:4||STATE:4||CU:4||BASISSET:4||XAS:4||CRYSTALS:3||EXCITATIONS:3||MOTTHUBBARD SYSTEMS:3||HIGHENERGY SPIN:3||halfmetal:3||INSULATORS:3||LA2CUO4:3||MODEL:3||FLUCTUATIONS:3||CE:3||double exchange:3||TRANSITIONMETALS:3||RESISTIVITY:3||BORON:3||LA1XCAXMNO3:3||IRON:3||PES:3||ANTIMONIDES:2||MgB2:2||ZR METALLIC GLASSES:2||superconductor:2||CRITICALCURRENT DENSITY:2||CIRCULARDICHROISM:2||SEMICONDUCTORS:2||LOCALIZATION:2||INTRABAND OPTICAL CONDUCTIVITY:2||COLOSSAL MAGNETORESISTANCE:2||OXIDATION:2||EXISTENCE:2||COPPER:2||diboride:2||MAGNESIUMDIBORIDE:2||GAP:2||CE COMPOUNDS:2||CORE POLARIZATION:2||magnetoresistance:2||photoemission spectroscopy:2||electronphonon interaction:2||GETTER:2||PD:2||MAGNETISM:2||FECR2S4:2||SUPERCONDUCTING MGB2:2||WIRES:2||ABSORPTION:2||ENERGY:2||LA1XSRXMNO3:2||CONSTANTS:2||polaron:2||charge ordering:2||SCATTERING:2||XRAY PHOTOEMISSION:2||CeNiSn:2||phase diagram:2||PHOTOELECTRON:2||QUADRUPOLAR:2||perovskitemanganites:2||CO:2||SYSTEMS:2||DOPED ZNO:2||LOWFREQUENCY SOUND:2||LA:2||ELECTRONELECTRON SCATTERING:2||AU:2||DENSITYWAVE INSTABILITY:2||FERMISURFACE:2||hybridization:2||VALENCEBAND SATELLITE:2||SULFUR SPINEL:2||Heusler:2||APPROXIMATION:2||superexchange:2||colossal magnetoresistance:2||ALLOYS:2||DEPENDENCE:2||AG:2||electronic structures:2||AUGERSPECTRA:2||CR:2||PARAMETERS:2||DIFFRACTION:2||SEMICONDUCTORMETAL TRANSITION:1||INTERMEDIATEVALENCE:1||SMB6:1||SRRUO3:1||antiperovskite structure with antipolar nature:1||lowenergy twodimensional phonons:1||anatase TiO2:1||La3S4:1||metalinsulator transitions:1||MNO:1||ELECTRONICSTRUCTURES:1||MAGNETIC CIRCULARDICHROISM:1||Density functional theory:1||CeCo2:1||TOPOLARON CROSSOVER:1||EXCHANGE:1||cuprates:1||high Tc cuprates:1||magnetically ordered materials:1||ZNSE:1||Sr2xKxFeMoO6:1||CDW:1||TeCuO3:1||STRUCTURALPROPERTIES:1||MN:1||screening length:1||amorphous Fe:1||WAVE BASISSET:1||SILICONCARBIDE:1||HIGHPRESSURE:1||electronphonon coupling:1||quenched superconductivity:1||CMR perovskite manganites:1||OXIDE:1||polarons:1||synchrotron radiation:1||FULLERIDES:1||RESONANTPHOTOEMISSION:1||Silicon carbide:1||DFT calculation:1||Hybridized bands:1||GIANT MAGNETORESISTANCE:1||PEROVSKITES:1||Raman spectra:1||EXCHANGE ENHANCEMENT:1||SILICON:1||SR2FEMOO6:1||orbital ordering:1||delafossite:1||TITANIUMDIOXIDE:1||electronic structure of disordered solids:1||YFE2:1||Magnetic polaron:1||NA2TI2SB2O:1||STRONGCOUPLED SUPERCONDUCTORS:1||HEAVYFERMION SYSTEMS:1||firstprinciples calculations:1||MECHANISM:1||UNiSn:1||PHOTONIC BANDGAP:1||SINGLE IMPURITY:1||PHONONSPECTRUM:1||FERMISURFACE TOPOLOGY:1||SUPPRESSION:1||RESONANT PHOTOEMISSION:1||METALDOPED PICENE:1||PHOTOIONIZATION CROSSSECTIONS:1||PHOTOINDUCED FERRIMAGNETIC SYSTEMS:1||LINKAGE ISOMERISM:1||CHARGETRANSFER:1||Bilayer Graphene:1||MAGNETICFIELD:1||SPINWAVES:1||rareearth manganese oxides:1||magnonphonon interaction:1||NACO2O4:1||ENERGYBANDS:1||SELFENERGY:1||GAS:1||Fe0.5Cu0.5Cr2S4:1||scanning photoelectron microscopy (SPEM):1||MAGNETIC PROPERTIES:1||Stoner model:1||AMORPHOUS TRANSITIONMETALS:1||SPINGLASS STATES:1||NI:1||LA3NI2B2N3:1||SOLIDS:1||CEO2:1||BAND THEORY:1||dilute magnetic semiconductor:1||pyrochlore:1||Y1XPRXBA2CU3O7DELTA:1||and electronphonon interactions:1||VIBRATIONS:1||RAY PHOTOEMISSION:1||ALKALI CATION:1||Europium:1||colossal magnetoresistance:1||structural stability:1||ENERGYGAP:1||small polaron:1||DOUBLE EXCHANGE:1||Coulomb correlation:1||magnon:1||phonons:1||ELECTRON FERROMAGNETISM:1||CURIETEMPERATURE:1||ARPES:1||PLANEWAVE METHOD:1||Xray absorption spectroscopy (XAS):1||ROOMTEMPERATURE:1||MONOCHALCOGENIDES:1||HEAT:1||UPDSN:1||MOMENTS:1||XRAY ABSORPTION:1||SEMICONDUCTOR:1||Fermi surface nesting:1||optical phonon:1||disordered system:1||dilute magnetic semiconductors:1||CMR manganites:1||PHONONS:1||LATTICEDYNAMICS:1||OXIDES:1||4fphotoemission:1||permanent magnet:1||pseudogap:1||TRANSPORTPROPERTIES:1||ANTIFERROMAGNET:1||(BI,PB)SRCOO SYSTEM:1||semicore correlation:1||POLARIZATION:1||CRYSTAL:1||spinel:1||Xray magnetic circular dichroism (XMCD):1||magnetocapacitance:1||ANATASE:1||TEMPERATURES:1||Pseudogap:1||INTERFACE:1||SUBSTRATE:1||YNI2B2C:1||SAMARIUM SULFIDE:1||strong swave superconductor:1||DOPED MANGANITE:1||SYMMETRY:1||CENISN:1||resonance mode:1||DISORDERED SYSTEM:1||LITHIUM INTERCALATION:1||CUO2 PLANE:1||SURFACE:1||Delafossite:1||ELECTRICALPROPERTIES:1||NIMNSB:1||PTMNSB:1||ROOMTEMPERATURE FERROMAGNETISM:1||RUBIDIUM MANGANESE HEXACYANOFERRATE:1||COLOSSALMAGNETORESISTANCE:1||FINITE TEMPERATURES:1||LAMNO3:1||FE:1||transitionmetal oxides:1||giant magnetoresistance:1||phonon:1||COPPER OXIDES:1||valence states:1||thermoelectric:1||semiconductor:1||CATION DISTRIBUTION:1||FeCr2S4:1||photoemission spectroscopy (PES):1||METALLIC FERROMAGNETISM:1||GRAPHITE:1||SUSCEPTIBILITY:1||UBE13:1||RCrSb3:1||band JahnTeller:1||Ce3S4:1||TiO2:1||PrBa2Cu3O7delta:1||UNTWINNED PRBA2CU3O7:1||AGNIO2:1||HALFMETALLIC FERROMAGNETS:1||CI:1||Energy gap:1||Photoemission:1||Future applications:1||Photoemission measurements:1||Graphene:1||BANDSTRUCTURE:1||TC:1||superconductivity:1||magnetic semiconductors:1||CMRmanganites:1||thin films:1||spin dynamics:1||highTc superconductors:1||ITINERANTELECTRON FERROMAGNETISM:1||SINGLECRYSTALS:1||CeTe2:1||amorphous magnetic materials:1||EPITAXIAL GRAPHENE:1||LAYERED PNICTIDEOXIDES:1||BOROCARBIDE SUPERCONDUCTORS:1||AUGMENTEDWAVE METHOD:1||METALLIC MAGNET UNISN:1||ORIGIN:1||spectrum rearrangement:1||MEANFIELD THEORY:1||MOLECULEBASED MAGNETS:1||METASTABLE STATE:1||INSULATOR:1||magnetic orderin:1||FCC IRON:1||CeRu2:1||TL2MN2O7:1||isotope effect:1||Perovskitemanganites:1||RECURSION METHOD:1||PERPENDICULAR MAGNETICANISOTROPY:1||quasiparticle spectral density:1||GW:1||MANGANESE FERRITE:1||RESONANCE:1||SeCuO3:1||Optical conductivity:1||MASSLESS DIRAC FERMIONS:1||SCHOTTKYBARRIER:1||electronic structure:15||ELECTRONICSTRUCTURE:11||TRANSITIONMETAL COMPOUNDS:10||METALS:10||photoemission:8||SPECTRA:8||MAGNETORESISTANCE:7||FERROMAGNETISM:7||TRANSPORT:7||TRANSITION:6||FILMS:6||THINFILMS:5||TOTALENERGY CALCULATIONS:5||MAGNETICPROPERTIES:5||SUPERCONDUCTIVITY:5||PR:5||LATTICE:4||STATES:4||SPECTROSCOPY:4||FIELD:4||CRYSTALSTRUCTURE:4||PHOTOEMISSION:4||TEMPERATURE:4||TRANSITIONTEMPERATURE:4||XRAYABSORPTION:4||STATE:4||CU:4||BASISSET:4||XAS:4||CRYSTALS:3||EXCITATIONS:3||MOTTHUBBARD SYSTEMS:3||HIGHENERGY SPIN:3||halfmetal:3||INSULATORS:3||LA2CUO4:3||MODEL:3||FLUCTUATIONS:3||CE:3||double exchange:3||TRANSITIONMETALS:3||RESISTIVITY:3||BORON:3||LA1XCAXMNO3:3||IRON:3||PES:3||ANTIMONIDES:2||MgB2:2||ZR METALLIC GLASSES:2||superconductor:2||CRITICALCURRENT DENSITY:2||CIRCULARDICHROISM:2||SEMICONDUCTORS:2||LOCALIZATION:2||INTRABAND OPTICAL CONDUCTIVITY:2||COLOSSAL MAGNETORESISTANCE:2||OXIDATION:2||EXISTENCE:2||COPPER:2||diboride:2||MAGNESIUMDIBORIDE:2||GAP:2||CE COMPOUNDS:2||CORE POLARIZATION:2||magnetoresistance:2||photoemission spectroscopy:2||electronphonon interaction:2||GETTER:2||PD:2||MAGNETISM:2||FECR2S4:2||SUPERCONDUCTING MGB2:2||WIRES:2||ABSORPTION:2||ENERGY:2||LA1XSRXMNO3:2||CONSTANTS:2||polaron:2||charge ordering:2||SCATTERING:2||XRAY PHOTOEMISSION:2||CeNiSn:2||phase diagram:2||PHOTOELECTRON:2||QUADRUPOLAR:2||perovskitemanganites:2||CO:2||SYSTEMS:2||DOPED ZNO:2||LOWFREQUENCY SOUND:2||LA:2||ELECTRONELECTRON SCATTERING:2||AU:2||DENSITYWAVE INSTABILITY:2||FERMISURFACE:2||hybridization:2||VALENCEBAND SATELLITE:2||SULFUR SPINEL:2||Heusler:2||APPROXIMATION:2||superexchange:2||colossal magnetoresistance:2||ALLOYS:2||DEPENDENCE:2||AG:2||electronic structures:2||AUGERSPECTRA:2||CR:2||PARAMETERS:2||DIFFRACTION:2||SEMICONDUCTORMETAL TRANSITION:1||INTERMEDIATEVALENCE:1||SMB6:1||SRRUO3:1||antiperovskite structure with antipolar nature:1||lowenergy twodimensional phonons:1||anatase TiO2:1||La3S4:1||metalinsulator transitions:1||MNO:1||ELECTRONICSTRUCTURES:1||MAGNETIC CIRCULARDICHROISM:1||Density functional theory:1||CeCo2:1||TOPOLARON CROSSOVER:1||EXCHANGE:1||cuprates:1||high Tc cuprates:1||magnetically ordered materials:1||ZNSE:1||Sr2xKxFeMoO6:1||CDW:1||TeCuO3:1||STRUCTURALPROPERTIES:1||MN:1||screening length:1||amorphous Fe:1||WAVE BASISSET:1||SILICONCARBIDE:1||HIGHPRESSURE:1||electronphonon coupling:1||quenched superconductivity:1||CMR perovskite manganites:1||OXIDE:1||polarons:1||synchrotron radiation:1||FULLERIDES:1||RESONANTPHOTOEMISSION:1||Silicon carbide:1||DFT calculation:1||Hybridized bands:1||GIANT MAGNETORESISTANCE:1||PEROVSKITES:1||Raman spectra:1||EXCHANGE ENHANCEMENT:1||SILICON:1||SR2FEMOO6:1||orbital ordering:1||delafossite:1||TITANIUMDIOXIDE:1||electronic structure of disordered solids:1||YFE2:1||Magnetic polaron:1||NA2TI2SB2O:1||STRONGCOUPLED SUPERCONDUCTORS:1||HEAVYFERMION SYSTEMS:1||firstprinciples calculations:1||MECHANISM:1||UNiSn:1||PHOTONIC BANDGAP:1||SINGLE IMPURITY:1||PHONONSPECTRUM:1||FERMISURFACE TOPOLOGY:1||SUPPRESSION:1||RESONANT PHOTOEMISSION:1||METALDOPED PICENE:1||PHOTOIONIZATION CROSSSECTIONS:1||PHOTOINDUCED FERRIMAGNETIC SYSTEMS:1||LINKAGE ISOMERISM:1||CHARGETRANSFER:1||Bilayer Graphene:1||MAGNETICFIELD:1||SPINWAVES:1||rareearth manganese oxides:1||magnonphonon interaction:1||NACO2O4:1||ENERGYBANDS:1||SELFENERGY:1||GAS:1||Fe0.5Cu0.5Cr2S4:1||scanning photoelectron microscopy (SPEM):1||MAGNETIC PROPERTIES:1||Stoner model:1||AMORPHOUS TRANSITIONMETALS:1||SPINGLASS STATES:1||NI:1||LA3NI2B2N3:1||SOLIDS:1||CEO2:1||BAND THEORY:1||dilute magnetic semiconductor:1||pyrochlore:1||Y1XPRXBA2CU3O7DELTA:1||and electronphonon interactions:1||VIBRATIONS:1||RAY PHOTOEMISSION:1||ALKALI CATION:1||Europium:1||colossal magnetoresistance:1||structural stability:1||ENERGYGAP:1||small polaron:1||DOUBLE EXCHANGE:1||Coulomb correlation:1||magnon:1||phonons:1||ELECTRON FERROMAGNETISM:1||CURIETEMPERATURE:1||ARPES:1||PLANEWAVE METHOD:1||Xray absorption spectroscopy (XAS):1||ROOMTEMPERATURE:1||MONOCHALCOGENIDES:1||HEAT:1||UPDSN:1||MOMENTS:1||XRAY ABSORPTION:1||SEMICONDUCTOR:1||Fermi surface nesting:1||optical phonon:1||disordered system:1||dilute magnetic semiconductors:1||CMR manganites:1||PHONONS:1||LATTICEDYNAMICS:1||OXIDES:1||4fphotoemission:1||permanent magnet:1||pseudogap:1||TRANSPORTPROPERTIES:1||ANTIFERROMAGNET:1||(BI,PB)SRCOO SYSTEM:1||semicore correlation:1||POLARIZATION:1||CRYSTAL:1||spinel:1||Xray magnetic circular dichroism (XMCD):1||magnetocapacitance:1||ANATASE:1||TEMPERATURES:1||Pseudogap:1||INTERFACE:1||SUBSTRATE:1||YNI2B2C:1||SAMARIUM SULFIDE:1||strong swave superconductor:1||DOPED MANGANITE:1||SYMMETRY:1||CENISN:1||resonance mode:1||DISORDERED SYSTEM:1||LITHIUM INTERCALATION:1||CUO2 PLANE:1||SURFACE:1||Delafossite:1||ELECTRICALPROPERTIES:1||NIMNSB:1||PTMNSB:1||ROOMTEMPERATURE FERROMAGNETISM:1||RUBIDIUM MANGANESE HEXACYANOFERRATE:1||COLOSSALMAGNETORESISTANCE:1||FINITE TEMPERATURES:1||LAMNO3:1||FE:1||transitionmetal oxides:1||giant magnetoresistance:1||phonon:1||COPPER OXIDES:1||valence states:1||thermoelectric:1||semiconductor:1||CATION DISTRIBUTION:1||FeCr2S4:1||photoemission spectroscopy (PES):1||METALLIC FERROMAGNETISM:1||GRAPHITE:1||SUSCEPTIBILITY:1||UBE13:1||RCrSb3:1||band JahnTeller:1||Ce3S4:1||TiO2:1||PrBa2Cu3O7delta:1||UNTWINNED PRBA2CU3O7:1||AGNIO2:1||HALFMETALLIC FERROMAGNETS:1||CI:1||Energy gap:1||Photoemission:1||Future applications:1||Photoemission measurements:1||Graphene:1||BANDSTRUCTURE:1||TC:1||superconductivity:1||magnetic semiconductors:1||CMRmanganites:1||thin films:1||spin dynamics:1||highTc superconductors:1||ITINERANTELECTRON FERROMAGNETISM:1||SINGLECRYSTALS:1||CeTe2:1||amorphous magnetic materials:1||EPITAXIAL GRAPHENE:1||LAYERED PNICTIDEOXIDES:1||BOROCARBIDE SUPERCONDUCTORS:1||AUGMENTEDWAVE METHOD:1||METALLIC MAGNET UNISN:1||ORIGIN:1||spectrum rearrangement:1||MEANFIELD THEORY:1||MOLECULEBASED MAGNETS:1||METASTABLE STATE:1||INSULATOR:1||magnetic orderin:1||FCC IRON:1||CeRu2:1||TL2MN2O7:1||isotope effect:1||Perovskitemanganites:1||RECURSION METHOD:1||PERPENDICULAR MAGNETICANISOTROPY:1||quasiparticle spectral density:1||GW:1||MANGANESE FERRITE:1||RESONANCE:1||SeCuO3:1||Optical conductivity:1||MASSLESS DIRAC FERMIONS:1||SCHOTTKYBARRIER:1||electronic structure:15||ELECTRONICSTRUCTURE:11||TRANSITIONMETAL COMPOUNDS:10||METALS:10||photoemission:8||SPECTRA:8||MAGNETORESISTANCE:7||FERROMAGNETISM:7||TRANSPORT:7||TRANSITION:6||FILMS:6||THINFILMS:5||TOTALENERGY CALCULATIONS:5||MAGNETICPROPERTIES:5||SUPERCONDUCTIVITY:5||PR:5||LATTICE:4||STATES:4||SPECTROSCOPY:4||FIELD:4||CRYSTALSTRUCTURE:4||PHOTOEMISSION:4||TEMPERATURE:4||TRANSITIONTEMPERATURE:4||XRAYABSORPTION:4||STATE:4||CU:4||BASISSET:4||XAS:4||CRYSTALS:3||EXCITATIONS:3||MOTTHUBBARD SYSTEMS:3||HIGHENERGY SPIN:3||halfmetal:3||INSULATORS:3||LA2CUO4:3||MODEL:3||FLUCTUATIONS:3||CE:3||double exchange:3||TRANSITIONMETALS:3||RESISTIVITY:3||BORON:3||LA1XCAXMNO3:3||IRON:3||PES:3||ANTIMONIDES:2||MgB2:2||ZR METALLIC GLASSES:2||superconductor:2||CRITICALCURRENT DENSITY:2||CIRCULARDICHROISM:2||SEMICONDUCTORS:2||LOCALIZATION:2||INTRABAND OPTICAL CONDUCTIVITY:2||COLOSSAL MAGNETORESISTANCE:2||OXIDATION:2||EXISTENCE:2||COPPER:2||diboride:2||MAGNESIUMDIBORIDE:2||GAP:2||CE COMPOUNDS:2||CORE POLARIZATION:2||magnetoresistance:2||photoemission spectroscopy:2||electronphonon interaction:2||GETTER:2||PD:2||MAGNETISM:2||FECR2S4:2||SUPERCONDUCTING MGB2:2||WIRES:2||ABSORPTION:2||ENERGY:2||LA1XSRXMNO3:2||CONSTANTS:2||polaron:2||charge ordering:2||SCATTERING:2||XRAY PHOTOEMISSION:2||CeNiSn:2||phase diagram:2||PHOTOELECTRON:2||QUADRUPOLAR:2||perovskitemanganites:2||CO:2||SYSTEMS:2||DOPED ZNO:2||LOWFREQUENCY SOUND:2||LA:2||ELECTRONELECTRON SCATTERING:2||AU:2||DENSITYWAVE INSTABILITY:2||FERMISURFACE:2||hybridization:2||VALENCEBAND SATELLITE:2||SULFUR SPINEL:2||Heusler:2||APPROXIMATION:2||superexchange:2||colossal magnetoresistance:2||ALLOYS:2||DEPENDENCE:2||AG:2||electronic structures:2||AUGERSPECTRA:2||CR:2||PARAMETERS:2||DIFFRACTION:2||SEMICONDUCTORMETAL TRANSITION:1||INTERMEDIATEVALENCE:1||SMB6:1||SRRUO3:1||antiperovskite structure with antipolar nature:1||lowenergy twodimensional phonons:1||anatase TiO2:1||La3S4:1||metalinsulator transitions:1||MNO:1||ELECTRONICSTRUCTURES:1||MAGNETIC CIRCULARDICHROISM:1||Density functional theory:1||CeCo2:1||TOPOLARON CROSSOVER:1||EXCHANGE:1||cuprates:1||high Tc cuprates:1||magnetically ordered materials:1||ZNSE:1||Sr2xKxFeMoO6:1||CDW:1||TeCuO3:1||STRUCTURALPROPERTIES:1||MN:1||screening length:1||amorphous Fe:1||WAVE BASISSET:1||SILICONCARBIDE:1||HIGHPRESSURE:1||electronphonon coupling:1||quenched superconductivity:1||CMR perovskite manganites:1||OXIDE:1||polarons:1||synchrotron radiation:1||FULLERIDES:1||RESONANTPHOTOEMISSION:1||Silicon carbide:1||DFT calculation:1||Hybridized bands:1||GIANT MAGNETORESISTANCE:1||PEROVSKITES:1||Raman spectra:1||EXCHANGE ENHANCEMENT:1||SILICON:1||SR2FEMOO6:1||orbital ordering:1||delafossite:1||TITANIUMDIOXIDE:1||electronic structure of disordered solids:1||YFE2:1||Magnetic polaron:1||NA2TI2SB2O:1||STRONGCOUPLED SUPERCONDUCTORS:1||HEAVYFERMION SYSTEMS:1||firstprinciples calculations:1||MECHANISM:1||UNiSn:1||PHOTONIC BANDGAP:1||SINGLE IMPURITY:1||PHONONSPECTRUM:1||FERMISURFACE TOPOLOGY:1||SUPPRESSION:1||RESONANT PHOTOEMISSION:1||METALDOPED PICENE:1||PHOTOIONIZATION CROSSSECTIONS:1||PHOTOINDUCED FERRIMAGNETIC SYSTEMS:1||LINKAGE ISOMERISM:1||CHARGETRANSFER:1||Bilayer Graphene:1||MAGNETICFIELD:1||SPINWAVES:1||rareearth manganese oxides:1||magnonphonon interaction:1||NACO2O4:1||ENERGYBANDS:1||SELFENERGY:1||GAS:1||Fe0.5Cu0.5Cr2S4:1||scanning photoelectron microscopy (SPEM):1||MAGNETIC PROPERTIES:1||Stoner model:1||AMORPHOUS TRANSITIONMETALS:1||SPINGLASS STATES:1||NI:1||LA3NI2B2N3:1||SOLIDS:1||CEO2:1||BAND THEORY:1||dilute magnetic semiconductor:1||pyrochlore:1||Y1XPRXBA2CU3O7DELTA:1||and electronphonon interactions:1||VIBRATIONS:1||RAY PHOTOEMISSION:1||ALKALI CATION:1||Europium:1||colossal magnetoresistance:1||structural stability:1||ENERGYGAP:1||small polaron:1||DOUBLE EXCHANGE:1||Coulomb correlation:1||magnon:1||phonons:1||ELECTRON FERROMAGNETISM:1||CURIETEMPERATURE:1||ARPES:1||PLANEWAVE METHOD:1||Xray absorption spectroscopy (XAS):1||ROOMTEMPERATURE:1||MONOCHALCOGENIDES:1||HEAT:1||UPDSN:1||MOMENTS:1||XRAY ABSORPTION:1||SEMICONDUCTOR:1||Fermi surface nesting:1||optical phonon:1||disordered system:1||dilute magnetic semiconductors:1||CMR manganites:1||PHONONS:1||LATTICEDYNAMICS:1||OXIDES:1||4fphotoemission:1||permanent magnet:1||pseudogap:1||TRANSPORTPROPERTIES:1||ANTIFERROMAGNET:1||(BI,PB)SRCOO SYSTEM:1||semicore correlation:1||POLARIZATION:1||CRYSTAL:1||spinel:1||Xray magnetic circular dichroism (XMCD):1||magnetocapacitance:1||ANATASE:1||TEMPERATURES:1||Pseudogap:1||INTERFACE:1||SUBSTRATE:1||YNI2B2C:1||SAMARIUM SULFIDE:1||strong swave superconductor:1||DOPED MANGANITE:1||SYMMETRY:1||CENISN:1||resonance mode:1||DISORDERED SYSTEM:1||LITHIUM INTERCALATION:1||CUO2 PLANE:1||SURFACE:1||Delafossite:1||ELECTRICALPROPERTIES:1||NIMNSB:1||PTMNSB:1||ROOMTEMPERATURE FERROMAGNETISM:1||RUBIDIUM MANGANESE HEXACYANOFERRATE:1||COLOSSALMAGNETORESISTANCE:1||FINITE TEMPERATURES:1||LAMNO3:1||FE:1||transitionmetal oxides:1||giant magnetoresistance:1||phonon:1||COPPER OXIDES:1||valence states:1||thermoelectric:1||semiconductor:1||CATION DISTRIBUTION:1||FeCr2S4:1||photoemission spectroscopy (PES):1||METALLIC FERROMAGNETISM:1||GRAPHITE:1||SUSCEPTIBILITY:1||UBE13:1||RCrSb3:1||band JahnTeller:1||Ce3S4:1||TiO2:1||PrBa2Cu3O7delta:1||UNTWINNED PRBA2CU3O7:1||AGNIO2:1||HALFMETALLIC FERROMAGNETS:1||CI:1||Energy gap:1||Photoemission:1||Future applications:1||Photoemission measurements:1||Graphene:1||BANDSTRUCTURE:1||TC:1||superconductivity:1||magnetic semiconductors:1||CMRmanganites:1||thin films:1||spin dynamics:1||highTc superconductors:1||ITINERANTELECTRON FERROMAGNETISM:1||SINGLECRYSTALS:1||CeTe2:1||amorphous magnetic materials:1||EPITAXIAL GRAPHENE:1||LAYERED PNICTIDEOXIDES:1||BOROCARBIDE SUPERCONDUCTORS:1||AUGMENTEDWAVE METHOD:1||METALLIC MAGNET UNISN:1||ORIGIN:1||spectrum rearrangement:1||MEANFIELD THEORY:1||MOLECULEBASED MAGNETS:1||METASTABLE STATE:1||INSULATOR:1||magnetic orderin:1||FCC IRON:1||CeRu2:1||TL2MN2O7:1||isotope effect:1||Perovskitemanganites:1||RECURSION METHOD:1||PERPENDICULAR MAGNETICANISOTROPY:1||quasiparticle spectral density:1||GW:1||MANGANESE FERRITE:1||RESONANCE:1||SeCuO3:1||Optical conductivity:1||MASSLESS DIRAC FERMIONS:1||SCHOTTKYBARRIER:1||electronic structure:15||ELECTRONICSTRUCTURE:11||TRANSITIONMETAL COMPOUNDS:10||METALS:10||photoemission:8||SPECTRA:8||MAGNETORESISTANCE:7||FERROMAGNETISM:7||TRANSPORT:7||TRANSITION:6||FILMS:6||THINFILMS:5||TOTALENERGY CALCULATIONS:5||MAGNETICPROPERTIES:5||SUPERCONDUCTIVITY:5||PR:5||LATTICE:4||STATES:4||SPECTROSCOPY:4||FIELD:4||CRYSTALSTRUCTURE:4||PHOTOEMISSION:4||TEMPERATURE:4||TRANSITIONTEMPERATURE:4||XRAYABSORPTION:4||STATE:4||CU:4||BASISSET:4||XAS:4||CRYSTALS:3||EXCITATIONS:3||MOTTHUBBARD SYSTEMS:3||HIGHENERGY SPIN:3||halfmetal:3||INSULATORS:3||LA2CUO4:3||MODEL:3||FLUCTUATIONS:3||CE:3||double exchange:3||TRANSITIONMETALS:3||RESISTIVITY:3||BORON:3||LA1XCAXMNO3:3||IRON:3||PES:3||ANTIMONIDES:2||MgB2:2||ZR METALLIC GLASSES:2||superconductor:2||CRITICALCURRENT DENSITY:2||CIRCULARDICHROISM:2||SEMICONDUCTORS:2||LOCALIZATION:2||INTRABAND OPTICAL CONDUCTIVITY:2||COLOSSAL MAGNETORESISTANCE:2||OXIDATION:2||EXISTENCE:2||COPPER:2||diboride:2||MAGNESIUMDIBORIDE:2||GAP:2||CE COMPOUNDS:2||CORE POLARIZATION:2||magnetoresistance:2||photoemission spectroscopy:2||electronphonon interaction:2||GETTER:2||PD:2||MAGNETISM:2||FECR2S4:2||SUPERCONDUCTING MGB2:2||WIRES:2||ABSORPTION:2||ENERGY:2||LA1XSRXMNO3:2||CONSTANTS:2||polaron:2||charge ordering:2||SCATTERING:2||XRAY PHOTOEMISSION:2||CeNiSn:2||phase diagram:2||PHOTOELECTRON:2||QUADRUPOLAR:2||perovskitemanganites:2||CO:2||SYSTEMS:2||DOPED ZNO:2||LOWFREQUENCY SOUND:2||LA:2||ELECTRONELECTRON SCATTERING:2||AU:2||DENSITYWAVE INSTABILITY:2||FERMISURFACE:2||hybridization:2||VALENCEBAND SATELLITE:2||SULFUR SPINEL:2||Heusler:2||APPROXIMATION:2||superexchange:2||colossal magnetoresistance:2||ALLOYS:2||DEPENDENCE:2||AG:2||electronic structures:2||AUGERSPECTRA:2||CR:2||PARAMETERS:2||DIFFRACTION:2||SEMICONDUCTORMETAL TRANSITION:1||INTERMEDIATEVALENCE:1||SMB6:1||SRRUO3:1||antiperovskite structure with antipolar nature:1||lowenergy twodimensional phonons:1||anatase TiO2:1||La3S4:1||metalinsulator transitions:1||MNO:1||ELECTRONICSTRUCTURES:1||MAGNETIC CIRCULARDICHROISM:1||Density functional theory:1||CeCo2:1||TOPOLARON CROSSOVER:1||EXCHANGE:1||cuprates:1||high Tc cuprates:1||magnetically ordered materials:1||ZNSE:1||Sr2xKxFeMoO6:1||CDW:1||TeCuO3:1||STRUCTURALPROPERTIES:1||MN:1||screening length:1||amorphous Fe:1||WAVE BASISSET:1||SILICONCARBIDE:1||HIGHPRESSURE:1||electronphonon coupling:1||quenched superconductivity:1||CMR perovskite manganites:1||OXIDE:1||polarons:1||synchrotron radiation:1||FULLERIDES:1||RESONANTPHOTOEMISSION:1||Silicon carbide:1||DFT calculation:1||Hybridized bands:1||GIANT MAGNETORESISTANCE:1||PEROVSKITES:1||Raman spectra:1||EXCHANGE ENHANCEMENT:1||SILICON:1||SR2FEMOO6:1||orbital ordering:1||delafossite:1||TITANIUMDIOXIDE:1||electronic structure of disordered solids:1||YFE2:1||Magnetic polaron:1||NA2TI2SB2O:1||STRONGCOUPLED SUPERCONDUCTORS:1||HEAVYFERMION SYSTEMS:1||firstprinciples calculations:1||MECHANISM:1||UNiSn:1||PHOTONIC BANDGAP:1||SINGLE IMPURITY:1||PHONONSPECTRUM:1||FERMISURFACE TOPOLOGY:1||SUPPRESSION:1||RESONANT PHOTOEMISSION:1||METALDOPED PICENE:1||PHOTOIONIZATION CROSSSECTIONS:1||PHOTOINDUCED FERRIMAGNETIC SYSTEMS:1||LINKAGE ISOMERISM:1||CHARGETRANSFER:1||Bilayer Graphene:1||MAGNETICFIELD:1||SPINWAVES:1||rareearth manganese oxides:1||magnonphonon interaction:1||NACO2O4:1||ENERGYBANDS:1||SELFENERGY:1||GAS:1||Fe0.5Cu0.5Cr2S4:1||scanning photoelectron microscopy (SPEM):1||MAGNETIC PROPERTIES:1||Stoner model:1||AMORPHOUS TRANSITIONMETALS:1||SPINGLASS STATES:1||NI:1||LA3NI2B2N3:1||SOLIDS:1||CEO2:1||BAND THEORY:1||dilute magnetic semiconductor:1||pyrochlore:1||Y1XPRXBA2CU3O7DELTA:1||and electronphonon interactions:1||VIBRATIONS:1||RAY PHOTOEMISSION:1||ALKALI CATION:1||Europium:1||colossal magnetoresistance:1||structural stability:1||ENERGYGAP:1||small polaron:1||DOUBLE EXCHANGE:1||Coulomb correlation:1||magnon:1||phonons:1||ELECTRON FERROMAGNETISM:1||CURIETEMPERATURE:1||ARPES:1||PLANEWAVE METHOD:1||Xray absorption spectroscopy (XAS):1||ROOMTEMPERATURE:1||MONOCHALCOGENIDES:1||HEAT:1||UPDSN:1||MOMENTS:1||XRAY ABSORPTION:1||SEMICONDUCTOR:1||Fermi surface nesting:1||optical phonon:1||disordered system:1||dilute magnetic semiconductors:1||CMR manganites:1||PHONONS:1||LATTICEDYNAMICS:1||OXIDES:1||4fphotoemission:1||permanent magnet:1||pseudogap:1||TRANSPORTPROPERTIES:1||ANTIFERROMAGNET:1||(BI,PB)SRCOO SYSTEM:1||semicore correlation:1||POLARIZATION:1||CRYSTAL:1||spinel:1||Xray magnetic circular dichroism (XMCD):1||magnetocapacitance:1||ANATASE:1||TEMPERATURES:1||Pseudogap:1||INTERFACE:1||SUBSTRATE:1||YNI2B2C:1||SAMARIUM SULFIDE:1||strong swave superconductor:1||DOPED MANGANITE:1||SYMMETRY:1||CENISN:1||resonance mode:1||DISORDERED SYSTEM:1||LITHIUM INTERCALATION:1||CUO2 PLANE:1||SURFACE:1||Delafossite:1||ELECTRICALPROPERTIES:1||NIMNSB:1||PTMNSB:1||ROOMTEMPERATURE FERROMAGNETISM:1||RUBIDIUM MANGANESE HEXACYANOFERRATE:1||COLOSSALMAGNETORESISTANCE:1||FINITE TEMPERATURES:1||LAMNO3:1||FE:1||transitionmetal oxides:1||giant magnetoresistance:1||phonon:1||COPPER OXIDES:1||valence states:1||thermoelectric:1||semiconductor:1||CATION DISTRIBUTION:1||FeCr2S4:1||photoemission spectroscopy (PES):1||METALLIC FERROMAGNETISM:1||GRAPHITE:1||SUSCEPTIBILITY:1||UBE13:1||RCrSb3:1||band JahnTeller:1||Ce3S4:1||TiO2:1||PrBa2Cu3O7delta:1||UNTWINNED PRBA2CU3O7:1||AGNIO2:1||HALFMETALLIC FERROMAGNETS:1||CI:1||Energy gap:1||Photoemission:1||Future applications:1||Photoemission measurements:1||Graphene:1||BANDSTRUCTURE:1||TC:1||superconductivity:1||magnetic semiconductors:1||CMRmanganites:1||thin films:1||spin dynamics:1||highTc superconductors:1||ITINERANTELECTRON FERROMAGNETISM:1||SINGLECRYSTALS:1||CeTe2:1||amorphous magnetic materials:1||EPITAXIAL GRAPHENE:1||LAYERED PNICTIDEOXIDES:1||BOROCARBIDE SUPERCONDUCTORS:1||AUGMENTEDWAVE METHOD:1||METALLIC MAGNET UNISN:1||ORIGIN:1||spectrum rearrangement:1||MEANFIELD THEORY:1||MOLECULEBASED MAGNETS:1||METASTABLE STATE:1||INSULATOR:1||magnetic orderin:1||FCC IRON:1||CeRu2:1||TL2MN2O7:1||isotope effect:1||Perovskitemanganites:1||RECURSION METHOD:1||PERPENDICULAR MAGNETICANISOTROPY:1||quasiparticle spectral density:1||GW:1||MANGANESE FERRITE:1||RESONANCE:1||SeCuO3:1||Optical conductivity:1||MASSLESS DIRAC FERMIONS:1||SCHOTTKYBARRIER:1||electronic structure:15||ELECTRONICSTRUCTURE:11||TRANSITIONMETAL COMPOUNDS:10||METALS:10||photoemission:8||SPECTRA:8||MAGNETORESISTANCE:7||FERROMAGNETISM:7||TRANSPORT:7||TRANSITION:6||FILMS:6||THINFILMS:5||TOTALENERGY CALCULATIONS:5||MAGNETICPROPERTIES:5||SUPERCONDUCTIVITY:5||PR:5||LATTICE:4||STATES:4||SPECTROSCOPY:4||FIELD:4||CRYSTALSTRUCTURE:4||PHOTOEMISSION:4||TEMPERATURE:4||TRANSITIONTEMPERATURE:4||XRAYABSORPTION:4||STATE:4||CU:4||BASISSET:4||XAS:4||CRYSTALS:3||EXCITATIONS:3||MOTTHUBBARD SYSTEMS:3||HIGHENERGY SPIN:3||halfmetal:3||INSULATORS:3||LA2CUO4:3||MODEL:3||FLUCTUATIONS:3||CE:3||double exchange:3||TRANSITIONMETALS:3||RESISTIVITY:3||BORON:3||LA1XCAXMNO3:3||IRON:3||PES:3||ANTIMONIDES:2||MgB2:2||ZR METALLIC GLASSES:2||superconductor:2||CRITICALCURRENT DENSITY:2||CIRCULARDICHROISM:2||SEMICONDUCTORS:2||LOCALIZATION:2||INTRABAND OPTICAL CONDUCTIVITY:2||COLOSSAL MAGNETORESISTANCE:2||OXIDATION:2||EXISTENCE:2||COPPER:2||diboride:2||MAGNESIUMDIBORIDE:2||GAP:2||CE COMPOUNDS:2||CORE POLARIZATION:2||magnetoresistance:2||photoemission spectroscopy:2||electronphonon interaction:2||GETTER:2||PD:2||MAGNETISM:2||FECR2S4:2||SUPERCONDUCTING MGB2:2||WIRES:2||ABSORPTION:2||ENERGY:2||LA1XSRXMNO3:2||CONSTANTS:2||polaron:2||charge ordering:2||SCATTERING:2||XRAY PHOTOEMISSION:2||CeNiSn:2||phase diagram:2||PHOTOELECTRON:2||QUADRUPOLAR:2||perovskitemanganites:2||CO:2||SYSTEMS:2||DOPED ZNO:2||LOWFREQUENCY SOUND:2||LA:2||ELECTRONELECTRON SCATTERING:2||AU:2||DENSITYWAVE INSTABILITY:2||FERMISURFACE:2||hybridization:2||VALENCEBAND SATELLITE:2||SULFUR SPINEL:2||Heusler:2||APPROXIMATION:2||superexchange:2||colossal magnetoresistance:2||ALLOYS:2||DEPENDENCE:2||AG:2||electronic structures:2||AUGERSPECTRA:2||CR:2||PARAMETERS:2||DIFFRACTION:2||SEMICONDUCTORMETAL TRANSITION:1||INTERMEDIATEVALENCE:1||SMB6:1||SRRUO3:1||antiperovskite structure with antipolar nature:1||lowenergy twodimensional phonons:1||anatase TiO2:1||La3S4:1||metalinsulator transitions:1||MNO:1||ELECTRONICSTRUCTURES:1||MAGNETIC CIRCULARDICHROISM:1||Density functional theory:1||CeCo2:1||TOPOLARON CROSSOVER:1||EXCHANGE:1||cuprates:1||high Tc cuprates:1||magnetically ordered materials:1||ZNSE:1||Sr2xKxFeMoO6:1||CDW:1||TeCuO3:1||STRUCTURALPROPERTIES:1||MN:1||screening length:1||amorphous Fe:1||WAVE BASISSET:1||SILICONCARBIDE:1||HIGHPRESSURE:1||electronphonon coupling:1||quenched superconductivity:1||CMR perovskite manganites:1||OXIDE:1||polarons:1||synchrotron radiation:1||FULLERIDES:1||RESONANTPHOTOEMISSION:1||Silicon carbide:1||DFT calculation:1||Hybridized bands:1||GIANT MAGNETORESISTANCE:1||PEROVSKITES:1||Raman spectra:1||EXCHANGE ENHANCEMENT:1||SILICON:1||SR2FEMOO6:1||orbital ordering:1||delafossite:1||TITANIUMDIOXIDE:1||electronic structure of disordered solids:1||YFE2:1||Magnetic polaron:1||NA2TI2SB2O:1||STRONGCOUPLED SUPERCONDUCTORS:1||HEAVYFERMION SYSTEMS:1||firstprinciples calculations:1||MECHANISM:1||UNiSn:1||PHOTONIC BANDGAP:1||SINGLE IMPURITY:1||PHONONSPECTRUM:1||FERMISURFACE TOPOLOGY:1||SUPPRESSION:1||RESONANT PHOTOEMISSION:1||METALDOPED PICENE:1||PHOTOIONIZATION CROSSSECTIONS:1||PHOTOINDUCED FERRIMAGNETIC SYSTEMS:1||LINKAGE ISOMERISM:1||CHARGETRANSFER:1||Bilayer Graphene:1||MAGNETICFIELD:1||SPINWAVES:1||rareearth manganese oxides:1||magnonphonon interaction:1||NACO2O4:1||ENERGYBANDS:1||SELFENERGY:1||GAS:1||Fe0.5Cu0.5Cr2S4:1||scanning photoelectron microscopy (SPEM):1||MAGNETIC PROPERTIES:1||Stoner model:1||AMORPHOUS TRANSITIONMETALS:1||SPINGLASS STATES:1||NI:1||LA3NI2B2N3:1||SOLIDS:1||CEO2:1||BAND THEORY:1||dilute magnetic semiconductor:1||pyrochlore:1||Y1XPRXBA2CU3O7DELTA:1||and electronphonon interactions:1||VIBRATIONS:1||RAY PHOTOEMISSION:1||ALKALI CATION:1||Europium:1||colossal magnetoresistance:1||structural stability:1||ENERGYGAP:1||small polaron:1||DOUBLE EXCHANGE:1||Coulomb correlation:1||magnon:1||phonons:1||ELECTRON FERROMAGNETISM:1||CURIETEMPERATURE:1||ARPES:1||PLANEWAVE METHOD:1||Xray absorption spectroscopy (XAS):1||ROOMTEMPERATURE:1||MONOCHALCOGENIDES:1||HEAT:1||UPDSN:1||MOMENTS:1||XRAY ABSORPTION:1||SEMICONDUCTOR:1||Fermi surface nesting:1||optical phonon:1||disordered system:1||dilute magnetic semiconductors:1||CMR manganites:1||PHONONS:1||LATTICEDYNAMICS:1||OXIDES:1||4fphotoemission:1||permanent magnet:1||pseudogap:1||TRANSPORTPROPERTIES:1||ANTIFERROMAGNET:1||(BI,PB)SRCOO SYSTEM:1||semicore correlation:1||POLARIZATION:1||CRYSTAL:1||spinel:1||Xray magnetic circular dichroism (XMCD):1||magnetocapacitance:1||ANATASE:1||TEMPERATURES:1||Pseudogap:1||INTERFACE:1||SUBSTRATE:1||YNI2B2C:1||SAMARIUM SULFIDE:1||strong swave superconductor:1||DOPED MANGANITE:1||SYMMETRY:1||CENISN:1||resonance mode:1||DISORDERED SYSTEM:1||LITHIUM INTERCALATION:1||CUO2 PLANE:1||SURFACE:1||Delafossite:1||ELECTRICALPROPERTIES:1||NIMNSB:1||PTMNSB:1||ROOMTEMPERATURE FERROMAGNETISM:1||RUBIDIUM MANGANESE HEXACYANOFERRATE:1||COLOSSALMAGNETORESISTANCE:1||FINITE TEMPERATURES:1||LAMNO3:1||FE:1||transitionmetal oxides:1||giant magnetoresistance:1||phonon:1||COPPER OXIDES:1||valence states:1||thermoelectric:1||semiconductor:1||CATION DISTRIBUTION:1||FeCr2S4:1||photoemission spectroscopy (PES):1||METALLIC FERROMAGNETISM:1||GRAPHITE:1||SUSCEPTIBILITY:1||UBE13:1||RCrSb3:1||band JahnTeller:1||Ce3S4:1||TiO2:1||PrBa2Cu3O7delta:1||UNTWINNED PRBA2CU3O7:1||AGNIO2:1||HALFMETALLIC FERROMAGNETS:1||CI:1||Energy gap:1||Photoemission:1||Future applications:1||Photoemission measurements:1||Graphene:1||BANDSTRUCTURE:1||TC:1||superconductivity:1||magnetic semiconductors:1||CMRmanganites:1||thin films:1||spin dynamics:1||highTc superconductors:1||ITINERANTELECTRON FERROMAGNETISM:1||SINGLECRYSTALS:1||CeTe2:1||amorphous magnetic materials:1||EPITAXIAL GRAPHENE:1||LAYERED PNICTIDEOXIDES:1||BOROCARBIDE SUPERCONDUCTORS:1||AUGMENTEDWAVE METHOD:1||METALLIC MAGNET UNISN:1||ORIGIN:1||spectrum rearrangement:1||MEANFIELD THEORY:1||MOLECULEBASED MAGNETS:1||METASTABLE STATE:1||INSULATOR:1||magnetic orderin:1||FCC IRON:1||CeRu2:1||TL2MN2O7:1||isotope effect:1||Perovskitemanganites:1||RECURSION METHOD:1||PERPENDICULAR MAGNETICANISOTROPY:1||quasiparticle spectral density:1||GW:1||MANGANESE FERRITE:1||RESONANCE:1||SeCuO3:1||Optical conductivity:1||MASSLESS DIRAC FERMIONS:1||SCHOTTKYBARRIER:1||electronic structure:15||ELECTRONICSTRUCTURE:11||TRANSITIONMETAL COMPOUNDS:10||METALS:10||photoemission:8||SPECTRA:8||MAGNETORESISTANCE:7||FERROMAGNETISM:7||TRANSPORT:7||TRANSITION:6||FILMS:6||THINFILMS:5||TOTALENERGY CALCULATIONS:5||MAGNETICPROPERTIES:5||SUPERCONDUCTIVITY:5||PR:5||LATTICE:4||STATES:4||SPECTROSCOPY:4||FIELD:4||CRYSTALSTRUCTURE:4||PHOTOEMISSION:4||TEMPERATURE:4||TRANSITIONTEMPERATURE:4||XRAYABSORPTION:4||STATE:4||CU:4||BASISSET:4||XAS:4||CRYSTALS:3||EXCITATIONS:3||MOTTHUBBARD SYSTEMS:3||HIGHENERGY SPIN:3||halfmetal:3||INSULATORS:3||LA2CUO4:3||MODEL:3||FLUCTUATIONS:3||CE:3||double exchange:3||TRANSITIONMETALS:3||RESISTIVITY:3||BORON:3||LA1XCAXMNO3:3||IRON:3||PES:3||ANTIMONIDES:2||MgB2:2||ZR METALLIC GLASSES:2||superconductor:2||CRITICALCURRENT DENSITY:2||CIRCULARDICHROISM:2||SEMICONDUCTORS:2||LOCALIZATION:2||INTRABAND OPTICAL CONDUCTIVITY:2||COLOSSAL MAGNETORESISTANCE:2||OXIDATION:2||EXISTENCE:2||COPPER:2||diboride:2||MAGNESIUMDIBORIDE:2||GAP:2||CE COMPOUNDS:2||CORE POLARIZATION:2||magnetoresistance:2||photoemission spectroscopy:2||electronphonon interaction:2||GETTER:2||PD:2||MAGNETISM:2||FECR2S4:2||SUPERCONDUCTING MGB2:2||WIRES:2||ABSORPTION:2||ENERGY:2||LA1XSRXMNO3:2||CONSTANTS:2||polaron:2||charge ordering:2||SCATTERING:2||XRAY PHOTOEMISSION:2||CeNiSn:2||phase diagram:2||PHOTOELECTRON:2||QUADRUPOLAR:2||perovskitemanganites:2||CO:2||SYSTEMS:2||DOPED ZNO:2||LOWFREQUENCY SOUND:2||LA:2||ELECTRONELECTRON SCATTERING:2||AU:2||DENSITYWAVE INSTABILITY:2||FERMISURFACE:2||hybridization:2||VALENCEBAND SATELLITE:2||SULFUR SPINEL:2||Heusler:2||APPROXIMATION:2||superexchange:2||colossal magnetoresistance:2||ALLOYS:2||DEPENDENCE:2||AG:2||electronic structures:2||AUGERSPECTRA:2||CR:2||PARAMETERS:2||DIFFRACTION:2||SEMICONDUCTORMETAL TRANSITION:1||INTERMEDIATEVALENCE:1||SMB6:1||SRRUO3:1||antiperovskite structure with antipolar nature:1||lowenergy twodimensional phonons:1||anatase TiO2:1||La3S4:1||metalinsulator transitions:1||MNO:1||ELECTRONICSTRUCTURES:1||MAGNETIC CIRCULARDICHROISM:1||Density functional theory:1||CeCo2:1||TOPOLARON CROSSOVER:1||EXCHANGE:1||cuprates:1||high Tc cuprates:1||magnetically ordered materials:1||ZNSE:1||Sr2xKxFeMoO6:1||CDW:1||TeCuO3:1||STRUCTURALPROPERTIES:1||MN:1||screening length:1||amorphous Fe:1||WAVE BASISSET:1||SILICONCARBIDE:1||HIGHPRESSURE:1||electronphonon coupling:1||quenched superconductivity:1||CMR perovskite manganites:1||OXIDE:1||polarons:1||synchrotron radiation:1||FULLERIDES:1||RESONANTPHOTOEMISSION:1||Silicon carbide:1||DFT calculation:1||Hybridized bands:1||GIANT MAGNETORESISTANCE:1||PEROVSKITES:1||Raman spectra:1||EXCHANGE ENHANCEMENT:1||SILICON:1||SR2FEMOO6:1||orbital ordering:1||delafossite:1||TITANIUMDIOXIDE:1||electronic structure of disordered solids:1||YFE2:1||Magnetic polaron:1||NA2TI2SB2O:1||STRONGCOUPLED SUPERCONDUCTORS:1||HEAVYFERMION SYSTEMS:1||firstprinciples calculations:1||MECHANISM:1||UNiSn:1||PHOTONIC BANDGAP:1||SINGLE IMPURITY:1||PHONONSPECTRUM:1||FERMISURFACE TOPOLOGY:1||SUPPRESSION:1||RESONANT PHOTOEMISSION:1||METALDOPED PICENE:1||PHOTOIONIZATION CROSSSECTIONS:1||PHOTOINDUCED FERRIMAGNETIC SYSTEMS:1||LINKAGE ISOMERISM:1||CHARGETRANSFER:1||Bilayer Graphene:1||MAGNETICFIELD:1||SPINWAVES:1||rareearth manganese oxides:1||magnonphonon interaction:1||NACO2O4:1||ENERGYBANDS:1||SELFENERGY:1||GAS:1||Fe0.5Cu0.5Cr2S4:1||scanning photoelectron microscopy (SPEM):1||MAGNETIC PROPERTIES:1||Stoner model:1||AMORPHOUS TRANSITIONMETALS:1||SPINGLASS STATES:1||NI:1||LA3NI2B2N3:1||SOLIDS:1||CEO2:1||BAND THEORY:1||dilute magnetic semiconductor:1||pyrochlore:1||Y1XPRXBA2CU3O7DELTA:1||and electronphonon interactions:1||VIBRATIONS:1||RAY PHOTOEMISSION:1||ALKALI CATION:1||Europium:1||colossal magnetoresistance:1||structural stability:1||ENERGYGAP:1||small polaron:1||DOUBLE EXCHANGE:1||Coulomb correlation:1||magnon:1||phonons:1||ELECTRON FERROMAGNETISM:1||CURIETEMPERATURE:1||ARPES:1||PLANEWAVE METHOD:1||Xray absorption spectroscopy (XAS):1||ROOMTEMPERATURE:1||MONOCHALCOGENIDES:1||HEAT:1||UPDSN:1||MOMENTS:1||XRAY ABSORPTION:1||SEMICONDUCTOR:1||Fermi surface nesting:1||optical phonon:1||disordered system:1||dilute magnetic semiconductors:1||CMR manganites:1||PHONONS:1||LATTICEDYNAMICS:1||OXIDES:1||4fphotoemission:1||permanent magnet:1||pseudogap:1||TRANSPORTPROPERTIES:1||ANTIFERROMAGNET:1||(BI,PB)SRCOO SYSTEM:1||semicore correlation:1||POLARIZATION:1||CRYSTAL:1||spinel:1||Xray magnetic circular dichroism (XMCD):1||magnetocapacitance:1||ANATASE:1||TEMPERATURES:1||Pseudogap:1||INTERFACE:1||SUBSTRATE:1||YNI2B2C:1||SAMARIUM SULFIDE:1||strong swave superconductor:1||DOPED MANGANITE:1||SYMMETRY:1||CENISN:1||resonance mode:1||DISORDERED SYSTEM:1||LITHIUM INTERCALATION:1||CUO2 PLANE:1||SURFACE:1||Delafossite:1||ELECTRICALPROPERTIES:1||NIMNSB:1||PTMNSB:1||ROOMTEMPERATURE FERROMAGNETISM:1||RUBIDIUM MANGANESE HEXACYANOFERRATE:1||COLOSSALMAGNETORESISTANCE:1||FINITE TEMPERATURES:1||LAMNO3:1||FE:1||transitionmetal oxides:1||giant magnetoresistance:1||phonon:1||COPPER OXIDES:1||valence states:1||thermoelectric:1||semiconductor:1||CATION DISTRIBUTION:1||FeCr2S4:1||photoemission spectroscopy (PES):1||METALLIC FERROMAGNETISM:1||GRAPHITE:1||SUSCEPTIBILITY:1||UBE13:1||RCrSb3:1||band JahnTeller:1||Ce3S4:1||TiO2:1||PrBa2Cu3O7delta:1||UNTWINNED PRBA2CU3O7:1||AGNIO2:1||HALFMETALLIC FERROMAGNETS:1||CI:1||Energy gap:1||Photoemission:1||Future applications:1||Photoemission measurements:1||Graphene:1||BANDSTRUCTURE:1||TC:1||superconductivity:1||magnetic semiconductors:1||CMRmanganites:1||thin films:1||spin dynamics:1||highTc superconductors:1||ITINERANTELECTRON FERROMAGNETISM:1||SINGLECRYSTALS:1||CeTe2:1||amorphous magnetic materials:1||EPITAXIAL GRAPHENE:1||LAYERED PNICTIDEOXIDES:1||BOROCARBIDE SUPERCONDUCTORS:1||AUGMENTEDWAVE METHOD:1||METALLIC MAGNET UNISN:1||ORIGIN:1||spectrum rearrangement:1||MEANFIELD THEORY:1||MOLECULEBASED MAGNETS:1||METASTABLE STATE:1||INSULATOR:1||magnetic orderin:1||FCC IRON:1||CeRu2:1||TL2MN2O7:1||isotope effect:1||Perovskitemanganites:1||RECURSION METHOD:1||PERPENDICULAR MAGNETICANISOTROPY:1||quasiparticle spectral density:1||GW:1||MANGANESE FERRITE:1||RESONANCE:1||SeCuO3:1||Optical conductivity:1||MASSLESS DIRAC FERMIONS:1||SCHOTTKYBARRIER:1||electronic structure:15||ELECTRONICSTRUCTURE:11||TRANSITIONMETAL COMPOUNDS:10||METALS:10||photoemission:8||SPECTRA:8||MAGNETORESISTANCE:7||FERROMAGNETISM:7||TRANSPORT:7||TRANSITION:6||FILMS:6||THINFILMS:5||TOTALENERGY CALCULATIONS:5||MAGNETICPROPERTIES:5||SUPERCONDUCTIVITY:5||PR:5||LATTICE:4||STATES:4||SPECTROSCOPY:4||FIELD:4||CRYSTALSTRUCTURE:4||PHOTOEMISSION:4||TEMPERATURE:4||TRANSITIONTEMPERATURE:4||XRAYABSORPTION:4||STATE:4||CU:4||BASISSET:4||XAS:4||CRYSTALS:3||EXCITATIONS:3||MOTTHUBBARD SYSTEMS:3||HIGHENERGY SPIN:3||halfmetal:3||INSULATORS:3||LA2CUO4:3||MODEL:3||FLUCTUATIONS:3||CE:3||double exchange:3||TRANSITIONMETALS:3||RESISTIVITY:3||BORON:3||LA1XCAXMNO3:3||IRON:3||PES:3||ANTIMONIDES:2||MgB2:2||ZR METALLIC GLASSES:2||superconductor:2||CRITICALCURRENT DENSITY:2||CIRCULARDICHROISM:2||SEMICONDUCTORS:2||LOCALIZATION:2||INTRABAND OPTICAL CONDUCTIVITY:2||COLOSSAL MAGNETORESISTANCE:2||OXIDATION:2||EXISTENCE:2||COPPER:2||diboride:2||MAGNESIUMDIBORIDE:2||GAP:2||CE COMPOUNDS:2||CORE POLARIZATION:2||magnetoresistance:2||photoemission spectroscopy:2||electronphonon interaction:2||GETTER:2||PD:2||MAGNETISM:2||FECR2S4:2||SUPERCONDUCTING MGB2:2||WIRES:2||ABSORPTION:2||ENERGY:2||LA1XSRXMNO3:2||CONSTANTS:2||polaron:2||charge ordering:2||SCATTERING:2||XRAY PHOTOEMISSION:2||CeNiSn:2||phase diagram:2||PHOTOELECTRON:2||QUADRUPOLAR:2||perovskitemanganites:2||CO:2||SYSTEMS:2||DOPED ZNO:2||LOWFREQUENCY SOUND:2||LA:2||ELECTRONELECTRON SCATTERING:2||AU:2||DENSITYWAVE INSTABILITY:2||FERMISURFACE:2||hybridization:2||VALENCEBAND SATELLITE:2||SULFUR SPINEL:2||Heusler:2||APPROXIMATION:2||superexchange:2||colossal magnetoresistance:2||ALLOYS:2||DEPENDENCE:2||AG:2||electronic structures:2||AUGERSPECTRA:2||CR:2||PARAMETERS:2||DIFFRACTION:2||SEMICONDUCTORMETAL TRANSITION:1||INTERMEDIATEVALENCE:1||SMB6:1||SRRUO3:1||antiperovskite structure with antipolar nature:1||lowenergy twodimensional phonons:1||anatase TiO2:1||La3S4:1||metalinsulator transitions:1||MNO:1||ELECTRONICSTRUCTURES:1||MAGNETIC CIRCULARDICHROISM:1||Density functional theory:1||CeCo2:1||TOPOLARON CROSSOVER:1||EXCHANGE:1||cuprates:1||high Tc cuprates:1||magnetically ordered materials:1||ZNSE:1||Sr2xKxFeMoO6:1||CDW:1||TeCuO3:1||STRUCTURALPROPERTIES:1||MN:1||screening length:1||amorphous Fe:1||WAVE BASISSET:1||SILICONCARBIDE:1||HIGHPRESSURE:1||electronphonon coupling:1||quenched superconductivity:1||CMR perovskite manganites:1||OXIDE:1||polarons:1||synchrotron radiation:1||FULLERIDES:1||RESONANTPHOTOEMISSION:1||Silicon carbide:1||DFT calculation:1||Hybridized bands:1||GIANT MAGNETORESISTANCE:1||PEROVSKITES:1||Raman spectra:1||EXCHANGE ENHANCEMENT:1||SILICON:1||SR2FEMOO6:1||orbital ordering:1||delafossite:1||TITANIUMDIOXIDE:1||electronic structure of disordered solids:1||YFE2:1||Magnetic polaron:1||NA2TI2SB2O:1||STRONGCOUPLED SUPERCONDUCTORS:1||HEAVYFERMION SYSTEMS:1||firstprinciples calculations:1||MECHANISM:1||UNiSn:1||PHOTONIC BANDGAP:1||SINGLE IMPURITY:1||PHONONSPECTRUM:1||FERMISURFACE TOPOLOGY:1||SUPPRESSION:1||RESONANT PHOTOEMISSION:1||METALDOPED PICENE:1||PHOTOIONIZATION CROSSSECTIONS:1||PHOTOINDUCED FERRIMAGNETIC SYSTEMS:1||LINKAGE ISOMERISM:1||CHARGETRANSFER:1||Bilayer Graphene:1||MAGNETICFIELD:1||SPINWAVES:1||rareearth manganese oxides:1||magnonphonon interaction:1||NACO2O4:1||ENERGYBANDS:1||SELFENERGY:1||GAS:1||Fe0.5Cu0.5Cr2S4:1||scanning photoelectron microscopy (SPEM):1||MAGNETIC PROPERTIES:1||Stoner model:1||AMORPHOUS TRANSITIONMETALS:1||SPINGLASS STATES:1||NI:1||LA3NI2B2N3:1||SOLIDS:1||CEO2:1||BAND THEORY:1||dilute magnetic semiconductor:1||pyrochlore:1||Y1XPRXBA2CU3O7DELTA:1||and electronphonon interactions:1||VIBRATIONS:1||RAY PHOTOEMISSION:1||ALKALI CATION:1||Europium:1||colossal magnetoresistance:1||structural stability:1||ENERGYGAP:1||small polaron:1||DOUBLE EXCHANGE:1||Coulomb correlation:1||magnon:1||phonons:1||ELECTRON FERROMAGNETISM:1||CURIETEMPERATURE:1||ARPES:1||PLANEWAVE METHOD:1||Xray absorption spectroscopy (XAS):1||ROOMTEMPERATURE:1||MONOCHALCOGENIDES:1||HEAT:1||UPDSN:1||MOMENTS:1||XRAY ABSORPTION:1||SEMICONDUCTOR:1||Fermi surface nesting:1||optical phonon:1||disordered system:1||dilute magnetic semiconductors:1||CMR manganites:1||PHONONS:1||LATTICEDYNAMICS:1||OXIDES:1||4fphotoemission:1||permanent magnet:1||pseudogap:1||TRANSPORTPROPERTIES:1||ANTIFERROMAGNET:1||(BI,PB)SRCOO SYSTEM:1||semicore correlation:1||POLARIZATION:1||CRYSTAL:1||spinel:1||Xray magnetic circular dichroism (XMCD):1||magnetocapacitance:1||ANATASE:1||TEMPERATURES:1||Pseudogap:1||INTERFACE:1||SUBSTRATE:1||YNI2B2C:1||SAMARIUM SULFIDE:1||strong swave superconductor:1||DOPED MANGANITE:1||SYMMETRY:1||CENISN:1||resonance mode:1||DISORDERED SYSTEM:1||LITHIUM INTERCALATION:1||CUO2 PLANE:1||SURFACE:1||Delafossite:1||ELECTRICALPROPERTIES:1||NIMNSB:1||PTMNSB:1||ROOMTEMPERATURE FERROMAGNETISM:1||RUBIDIUM MANGANESE HEXACYANOFERRATE:1||COLOSSALMAGNETORESISTANCE:1||FINITE TEMPERATURES:1||LAMNO3:1||FE:1||transitionmetal oxides:1||giant magnetoresistance:1||phonon:1||COPPER OXIDES:1||valence states:1||thermoelectric:1||semiconductor:1||CATION DISTRIBUTION:1||FeCr2S4:1||photoemission spectroscopy (PES):1||METALLIC FERROMAGNETISM:1||GRAPHITE:1||SUSCEPTIBILITY:1||UBE13:1||RCrSb3:1||band JahnTeller:1||Ce3S4:1||TiO2:1||PrBa2Cu3O7delta:1||UNTWINNED PRBA2CU3O7:1||AGNIO2:1||HALFMETALLIC FERROMAGNETS:1||CI:1||Energy gap:1||Photoemission:1||Future applications:1||Photoemission measurements:1||Graphene:1||BANDSTRUCTURE:1||TC:1||superconductivity:1||magnetic semiconductors:1||CMRmanganites:1||thin films:1||spin dynamics:1||highTc superconductors:1||ITINERANTELECTRON FERROMAGNETISM:1||SINGLECRYSTALS:1||CeTe2:1||amorphous magnetic materials:1||EPITAXIAL GRAPHENE:1||LAYERED PNICTIDEOXIDES:1||BOROCARBIDE SUPERCONDUCTORS:1||AUGMENTEDWAVE METHOD:1||METALLIC MAGNET UNISN:1||ORIGIN:1||spectrum rearrangement:1||MEANFIELD THEORY:1||MOLECULEBASED MAGNETS:1||METASTABLE STATE:1||INSULATOR:1||magnetic orderin:1||FCC IRON:1||CeRu2:1||TL2MN2O7:1||isotope effect:1||Perovskitemanganites:1||RECURSION METHOD:1||PERPENDICULAR MAGNETICANISOTROPY:1||quasiparticle spectral density:1||GW:1||MANGANESE FERRITE:1||RESONANCE:1||SeCuO3:1||Optical conductivity:1||MASSLESS DIRAC FERMIONS:1||SCHOTTKYBARRIER:1||electronic structure:15||ELECTRONICSTRUCTURE:11||TRANSITIONMETAL COMPOUNDS:10||METALS:10||photoemission:8||SPECTRA:8||MAGNETORESISTANCE:7||FERROMAGNETISM:7||TRANSPORT:7||TRANSITION:6||FILMS:6||THINFILMS:5||TOTALENERGY CALCULATIONS:5||MAGNETICPROPERTIES:5||SUPERCONDUCTIVITY:5||PR:5||LATTICE:4||STATES:4||SPECTROSCOPY:4||FIELD:4||CRYSTALSTRUCTURE:4||PHOTOEMISSION:4||TEMPERATURE:4||TRANSITIONTEMPERATURE:4||XRAYABSORPTION:4||STATE:4||CU:4||BASISSET:4||XAS:4||CRYSTALS:3||EXCITATIONS:3||MOTTHUBBARD SYSTEMS:3||HIGHENERGY SPIN:3||halfmetal:3||INSULATORS:3||LA2CUO4:3||MODEL:3||FLUCTUATIONS:3||CE:3||double exchange:3||TRANSITIONMETALS:3||RESISTIVITY:3||BORON:3||LA1XCAXMNO3:3||IRON:3||PES:3||ANTIMONIDES:2||MgB2:2||ZR METALLIC GLASSES:2||superconductor:2||CRITICALCURRENT DENSITY:2||CIRCULARDICHROISM:2||SEMICONDUCTORS:2||LOCALIZATION:2||INTRABAND OPTICAL CONDUCTIVITY:2||COLOSSAL MAGNETORESISTANCE:2||OXIDATION:2||EXISTENCE:2||COPPER:2||diboride:2||MAGNESIUMDIBORIDE:2||GAP:2||CE COMPOUNDS:2||CORE POLARIZATION:2||magnetoresistance:2||photoemission spectroscopy:2||electronphonon interaction:2||GETTER:2||PD:2||MAGNETISM:2||FECR2S4:2||SUPERCONDUCTING MGB2:2||WIRES:2||ABSORPTION:2||ENERGY:2||LA1XSRXMNO3:2||CONSTANTS:2||polaron:2||charge ordering:2||SCATTERING:2||XRAY PHOTOEMISSION:2||CeNiSn:2||phase diagram:2||PHOTOELECTRON:2||QUADRUPOLAR:2||perovskitemanganites:2||CO:2||SYSTEMS:2||DOPED ZNO:2||LOWFREQUENCY SOUND:2||LA:2||ELECTRONELECTRON SCATTERING:2||AU:2||DENSITYWAVE INSTABILITY:2||FERMISURFACE:2||hybridization:2||VALENCEBAND SATELLITE:2||SULFUR SPINEL:2||Heusler:2||APPROXIMATION:2||superexchange:2||colossal magnetoresistance:2||ALLOYS:2||DEPENDENCE:2||AG:2||electronic structures:2||AUGERSPECTRA:2||CR:2||PARAMETERS:2||DIFFRACTION:2||SEMICONDUCTORMETAL TRANSITION:1||INTERMEDIATEVALENCE:1||SMB6:1||SRRUO3:1||antiperovskite structure with antipolar nature:1||lowenergy twodimensional phonons:1||anatase TiO2:1||La3S4:1||metalinsulator transitions:1||MNO:1||ELECTRONICSTRUCTURES:1||MAGNETIC CIRCULARDICHROISM:1||Density functional theory:1||CeCo2:1||TOPOLARON CROSSOVER:1||EXCHANGE:1||cuprates:1||high Tc cuprates:1||magnetically ordered materials:1||ZNSE:1||Sr2xKxFeMoO6:1||CDW:1||TeCuO3:1||STRUCTURALPROPERTIES:1||MN:1||screening length:1||amorphous Fe:1||WAVE BASISSET:1||SILICONCARBIDE:1||HIGHPRESSURE:1||electronphonon coupling:1||quenched superconductivity:1||CMR perovskite manganites:1||OXIDE:1||polarons:1||synchrotron radiation:1||FULLERIDES:1||RESONANTPHOTOEMISSION:1||Silicon carbide:1||DFT calculation:1||Hybridized bands:1||GIANT MAGNETORESISTANCE:1||PEROVSKITES:1||Raman spectra:1||EXCHANGE ENHANCEMENT:1||SILICON:1||SR2FEMOO6:1||orbital ordering:1||delafossite:1||TITANIUMDIOXIDE:1||electronic structure of disordered solids:1||YFE2:1||Magnetic polaron:1||NA2TI2SB2O:1||STRONGCOUPLED SUPERCONDUCTORS:1||HEAVYFERMION SYSTEMS:1||firstprinciples calculations:1||MECHANISM:1||UNiSn:1||PHOTONIC BANDGAP:1||SINGLE IMPURITY:1||PHONONSPECTRUM:1||FERMISURFACE TOPOLOGY:1||SUPPRESSION:1||RESONANT PHOTOEMISSION:1||METALDOPED PICENE:1||PHOTOIONIZATION CROSSSECTIONS:1||PHOTOINDUCED FERRIMAGNETIC SYSTEMS:1||LINKAGE ISOMERISM:1||CHARGETRANSFER:1||Bilayer Graphene:1||MAGNETICFIELD:1||SPINWAVES:1||rareearth manganese oxides:1||magnonphonon interaction:1||NACO2O4:1||ENERGYBANDS:1||SELFENERGY:1||GAS:1||Fe0.5Cu0.5Cr2S4:1||scanning photoelectron microscopy (SPEM):1||MAGNETIC PROPERTIES:1||Stoner model:1||AMORPHOUS TRANSITIONMETALS:1||SPINGLASS STATES:1||NI:1||LA3NI2B2N3:1||SOLIDS:1||CEO2:1||BAND THEORY:1||dilute magnetic semiconductor:1||pyrochlore:1||Y1XPRXBA2CU3O7DELTA:1||and electronphonon interactions:1||VIBRATIONS:1||RAY PHOTOEMISSION:1||ALKALI CATION:1||Europium:1||colossal magnetoresistance:1||structural stability:1||ENERGYGAP:1||small polaron:1||DOUBLE EXCHANGE:1||Coulomb correlation:1||magnon:1||phonons:1||ELECTRON FERROMAGNETISM:1||CURIETEMPERATURE:1||ARPES:1||PLANEWAVE METHOD:1||Xray absorption spectroscopy (XAS):1||ROOMTEMPERATURE:1||MONOCHALCOGENIDES:1||HEAT:1||UPDSN:1||MOMENTS:1||XRAY ABSORPTION:1||SEMICONDUCTOR:1||Fermi surface nesting:1||optical phonon:1||disordered system:1||dilute magnetic semiconductors:1||CMR manganites:1||PHONONS:1||LATTICEDYNAMICS:1||OXIDES:1||4fphotoemission:1||permanent magnet:1||pseudogap:1||TRANSPORTPROPERTIES:1||ANTIFERROMAGNET:1||(BI,PB)SRCOO SYSTEM:1||semicore correlation:1||POLARIZATION:1||CRYSTAL:1||spinel:1||Xray magnetic circular dichroism (XMCD):1||magnetocapacitance:1||ANATASE:1||TEMPERATURES:1||Pseudogap:1||INTERFACE:1||SUBSTRATE:1||YNI2B2C:1||SAMARIUM SULFIDE:1||strong swave superconductor:1||DOPED MANGANITE:1||SYMMETRY:1||CENISN:1||resonance mode:1||DISORDERED SYSTEM:1||LITHIUM INTERCALATION:1||CUO2 PLANE:1||SURFACE:1||Delafossite:1||ELECTRICALPROPERTIES:1||NIMNSB:1||PTMNSB:1||ROOMTEMPERATURE FERROMAGNETISM:1||RUBIDIUM MANGANESE HEXACYANOFERRATE:1||COLOSSALMAGNETORESISTANCE:1||FINITE TEMPERATURES:1||LAMNO3:1||FE:1||transitionmetal oxides:1||giant magnetoresistance:1||phonon:1||COPPER OXIDES:1||valence states:1||thermoelectric:1||semiconductor:1||CATION DISTRIBUTION:1||FeCr2S4:1||photoemission spectroscopy (PES):1||METALLIC FERROMAGNETISM:1||GRAPHITE:1||SUSCEPTIBILITY:1||UBE13:1||RCrSb3:1||band JahnTeller:1||Ce3S4:1||TiO2:1||PrBa2Cu3O7delta:1||UNTWINNED PRBA2CU3O7:1||AGNIO2:1||HALFMETALLIC FERROMAGNETS:1||CI:1||Energy gap:1||Photoemission:1||Future applications:1||Photoemission measurements:1||Graphene:1||BANDSTRUCTURE:1||TC:1||superconductivity:1||magnetic semiconductors:1||CMRmanganites:1||thin films:1||spin dynamics:1||highTc superconductors:1||ITINERANTELECTRON FERROMAGNETISM:1||SINGLECRYSTALS:1||CeTe2:1||amorphous magnetic materials:1||EPITAXIAL GRAPHENE:1||LAYERED PNICTIDEOXIDES:1||BOROCARBIDE SUPERCONDUCTORS:1||AUGMENTEDWAVE METHOD:1||METALLIC MAGNET UNISN:1||ORIGIN:1||spectrum rearrangement:1||MEANFIELD THEORY:1||MOLECULEBASED MAGNETS:1||METASTABLE STATE:1||INSULATOR:1||magnetic orderin:1||FCC IRON:1||CeRu2:1||TL2MN2O7:1||isotope effect:1||Perovskitemanganites:1||RECURSION METHOD:1||PERPENDICULAR MAGNETICANISOTROPY:1||quasiparticle spectral density:1||GW:1||MANGANESE FERRITE:1||RESONANCE:1||SeCuO3:1||Optical conductivity:1||MASSLESS DIRAC FERMIONS:1||SCHOTTKYBARRIER:1||electronic structure:15||ELECTRONICSTRUCTURE:11||TRANSITIONMETAL COMPOUNDS:10||METALS:10||photoemission:8||SPECTRA:8||MAGNETORESISTANCE:7||FERROMAGNETISM:7||TRANSPORT:7||TRANSITION:6||FILMS:6||THINFILMS:5||TOTALENERGY CALCULATIONS:5||MAGNETICPROPERTIES:5||SUPERCONDUCTIVITY:5||PR:5||LATTICE:4||STATES:4||SPECTROSCOPY:4||FIELD:4||CRYSTALSTRUCTURE:4||PHOTOEMISSION:4||TEMPERATURE:4||TRANSITIONTEMPERATURE:4||XRAYABSORPTION:4||STATE:4||CU:4||BASISSET:4||XAS:4||CRYSTALS:3||EXCITATIONS:3||MOTTHUBBARD SYSTEMS:3||HIGHENERGY SPIN:3||halfmetal:3||INSULATORS:3||LA2CUO4:3||MODEL:3||FLUCTUATIONS:3||CE:3||double exchange:3||TRANSITIONMETALS:3||RESISTIVITY:3||BORON:3||LA1XCAXMNO3:3||IRON:3||PES:3||ANTIMONIDES:2||MgB2:2||ZR METALLIC GLASSES:2||superconductor:2||CRITICALCURRENT DENSITY:2||CIRCULARDICHROISM:2||SEMICONDUCTORS:2||LOCALIZATION:2||INTRABAND OPTICAL CONDUCTIVITY:2||COLOSSAL MAGNETORESISTANCE:2||OXIDATION:2||EXISTENCE:2||COPPER:2||diboride:2||MAGNESIUMDIBORIDE:2||GAP:2||CE COMPOUNDS:2||CORE POLARIZATION:2||magnetoresistance:2||photoemission spectroscopy:2||electronphonon interaction:2||GETTER:2||PD:2||MAGNETISM:2||FECR2S4:2||SUPERCONDUCTING MGB2:2||WIRES:2||ABSORPTION:2||ENERGY:2||LA1XSRXMNO3:2||CONSTANTS:2||polaron:2||charge ordering:2||SCATTERING:2||XRAY PHOTOEMISSION:2||CeNiSn:2||phase diagram:2||PHOTOELECTRON:2||QUADRUPOLAR:2||perovskitemanganites:2||CO:2||SYSTEMS:2||DOPED ZNO:2||LOWFREQUENCY SOUND:2||LA:2||ELECTRONELECTRON SCATTERING:2||AU:2||DENSITYWAVE INSTABILITY:2||FERMISURFACE:2||hybridization:2||VALENCEBAND SATELLITE:2||SULFUR SPINEL:2||Heusler:2||APPROXIMATION:2||superexchange:2||colossal magnetoresistance:2||ALLOYS:2||DEPENDENCE:2||AG:2||electronic structures:2||AUGERSPECTRA:2||CR:2||PARAMETERS:2||DIFFRACTION:2||SEMICONDUCTORMETAL TRANSITION:1||INTERMEDIATEVALENCE:1||SMB6:1||SRRUO3:1||antiperovskite structure with antipolar nature:1||lowenergy twodimensional phonons:1||anatase TiO2:1||La3S4:1||metalinsulator transitions:1||MNO:1||ELECTRONICSTRUCTURES:1||MAGNETIC CIRCULARDICHROISM:1||Density functional theory:1||CeCo2:1||TOPOLARON CROSSOVER:1||EXCHANGE:1||cuprates:1||high Tc cuprates:1||magnetically ordered materials:1||ZNSE:1||Sr2xKxFeMoO6:1||CDW:1||TeCuO3:1||STRUCTURALPROPERTIES:1||MN:1||screening length:1||amorphous Fe:1||WAVE BASISSET:1||SILICONCARBIDE:1||HIGHPRESSURE:1||electronphonon coupling:1||quenched superconductivity:1||CMR perovskite manganites:1||OXIDE:1||polarons:1||synchrotron radiation:1||FULLERIDES:1||RESONANTPHOTOEMISSION:1||Silicon carbide:1||DFT calculation:1||Hybridized bands:1||GIANT MAGNETORESISTANCE:1||PEROVSKITES:1||Raman spectra:1||EXCHANGE ENHANCEMENT:1||SILICON:1||SR2FEMOO6:1||orbital ordering:1||delafossite:1||TITANIUMDIOXIDE:1||electronic structure of disordered solids:1||YFE2:1||Magnetic polaron:1||NA2TI2SB2O:1||STRONGCOUPLED SUPERCONDUCTORS:1||HEAVYFERMION SYSTEMS:1||firstprinciples calculations:1||MECHANISM:1||UNiSn:1||PHOTONIC BANDGAP:1||SINGLE IMPURITY:1||PHONONSPECTRUM:1||FERMISURFACE TOPOLOGY:1||SUPPRESSION:1||RESONANT PHOTOEMISSION:1||METALDOPED PICENE:1||PHOTOIONIZATION CROSSSECTIONS:1||PHOTOINDUCED FERRIMAGNETIC SYSTEMS:1||LINKAGE ISOMERISM:1||CHARGETRANSFER:1||Bilayer Graphene:1||MAGNETICFIELD:1||SPINWAVES:1||rareearth manganese oxides:1||magnonphonon interaction:1||NACO2O4:1||ENERGYBANDS:1||SELFENERGY:1||GAS:1||Fe0.5Cu0.5Cr2S4:1||scanning photoelectron microscopy (SPEM):1||MAGNETIC PROPERTIES:1||Stoner model:1||AMORPHOUS TRANSITIONMETALS:1||SPINGLASS STATES:1||NI:1||LA3NI2B2N3:1||SOLIDS:1||CEO2:1||BAND THEORY:1||dilute magnetic semiconductor:1||pyrochlore:1||Y1XPRXBA2CU3O7DELTA:1||and electronphonon interactions:1||VIBRATIONS:1||RAY PHOTOEMISSION:1||ALKALI CATION:1||Europium:1||colossal magnetoresistance:1||structural stability:1||ENERGYGAP:1||small polaron:1||DOUBLE EXCHANGE:1||Coulomb correlation:1||magnon:1||phonons:1||ELECTRON FERROMAGNETISM:1||CURIETEMPERATURE:1||ARPES:1||PLANEWAVE METHOD:1||Xray absorption spectroscopy (XAS):1||ROOMTEMPERATURE:1||MONOCHALCOGENIDES:1||HEAT:1||UPDSN:1||MOMENTS:1||XRAY ABSORPTION:1||SEMICONDUCTOR:1||Fermi surface nesting:1||optical phonon:1||disordered system:1||dilute magnetic semiconductors:1||CMR manganites:1||PHONONS:1||LATTICEDYNAMICS:1||OXIDES:1||4fphotoemission:1||permanent magnet:1||pseudogap:1||TRANSPORTPROPERTIES:1||ANTIFERROMAGNET:1||(BI,PB)SRCOO SYSTEM:1||semicore correlation:1||POLARIZATION:1||CRYSTAL:1||spinel:1||Xray magnetic circular dichroism (XMCD):1||magnetocapacitance:1||ANATASE:1||TEMPERATURES:1||Pseudogap:1||INTERFACE:1||SUBSTRATE:1||YNI2B2C:1||SAMARIUM SULFIDE:1||strong swave superconductor:1||DOPED MANGANITE:1||SYMMETRY:1||CENISN:1||resonance mode:1||DISORDERED SYSTEM:1||LITHIUM INTERCALATION:1||CUO2 PLANE:1||SURFACE:1||Delafossite:1||ELECTRICALPROPERTIES:1||NIMNSB:1||PTMNSB:1||ROOMTEMPERATURE FERROMAGNETISM:1||RUBIDIUM MANGANESE HEXACYANOFERRATE:1||COLOSSALMAGNETORESISTANCE:1||FINITE TEMPERATURES:1||LAMNO3:1||FE:1||transitionmetal oxides:1||giant magnetoresistance:1||phonon:1||COPPER OXIDES:1||valence states:1||thermoelectric:1||semiconductor:1||CATION DISTRIBUTION:1||FeCr2S4:1||photoemission spectroscopy (PES):1||METALLIC FERROMAGNETISM:1||GRAPHITE:1||SUSCEPTIBILITY:1||UBE13:1||RCrSb3:1||band JahnTeller:1||Ce3S4:1||TiO2:1||PrBa2Cu3O7delta:1||UNTWINNED PRBA2CU3O7:1||AGNIO2:1||HALFMETALLIC FERROMAGNETS:1||CI:1||Energy gap:1||Photoemission:1||Future applications:1||Photoemission measurements:1||Graphene:1||BANDSTRUCTURE:1||TC:1||superconductivity:1||magnetic semiconductors:1||CMRmanganites:1||thin films:1||spin dynamics:1||highTc superconductors:1||ITINERANTELECTRON FERROMAGNETISM:1||SINGLECRYSTALS:1||CeTe2:1||amorphous magnetic materials:1||EPITAXIAL GRAPHENE:1||LAYERED PNICTIDEOXIDES:1||BOROCARBIDE SUPERCONDUCTORS:1||AUGMENTEDWAVE METHOD:1||METALLIC MAGNET UNISN:1||ORIGIN:1||spectrum rearrangement:1||MEANFIELD THEORY:1||MOLECULEBASED MAGNETS:1||METASTABLE STATE:1||INSULATOR:1||magnetic orderin:1||FCC IRON:1||CeRu2:1||TL2MN2O7:1||isotope effect:1||Perovskitemanganites:1||RECURSION METHOD:1||PERPENDICULAR MAGNETICANISOTROPY:1||quasiparticle spectral density:1||GW:1||MANGANESE FERRITE:1||RESONANCE:1||SeCuO3:1||Optical conductivity:1||MASSLESS DIRAC FERMIONS:1||SCHOTTKYBARRIER:1||electronic structure:15||ELECTRONICSTRUCTURE:11||TRANSITIONMETAL COMPOUNDS:10||METALS:10||photoemission:8||SPECTRA:8||MAGNETORESISTANCE:7||FERROMAGNETISM:7||TRANSPORT:7||TRANSITION:6||FILMS:6||THINFILMS:5||TOTALENERGY CALCULATIONS:5||MAGNETICPROPERTIES:5||SUPERCONDUCTIVITY:5||PR:5||LATTICE:4||STATES:4||SPECTROSCOPY:4||FIELD:4||CRYSTALSTRUCTURE:4||PHOTOEMISSION:4||TEMPERATURE:4||TRANSITIONTEMPERATURE:4||XRAYABSORPTION:4||STATE:4||CU:4||BASISSET:4||XAS:4||CRYSTALS:3||EXCITATIONS:3||MOTTHUBBARD SYSTEMS:3||HIGHENERGY SPIN:3||halfmetal:3||INSULATORS:3||LA2CUO4:3||MODEL:3||FLUCTUATIONS:3||CE:3||double exchange:3||TRANSITIONMETALS:3||RESISTIVITY:3||BORON:3||LA1XCAXMNO3:3||IRON:3||PES:3||ANTIMONIDES:2||MgB2:2||ZR METALLIC GLASSES:2||superconductor:2||CRITICALCURRENT DENSITY:2||CIRCULARDICHROISM:2||SEMICONDUCTORS:2||LOCALIZATION:2||INTRABAND OPTICAL CONDUCTIVITY:2||COLOSSAL MAGNETORESISTANCE:2||OXIDATION:2||EXISTENCE:2||COPPER:2||diboride:2||MAGNESIUMDIBORIDE:2||GAP:2||CE COMPOUNDS:2||CORE POLARIZATION:2||magnetoresistance:2||photoemission spectroscopy:2||electronphonon interaction:2||GETTER:2||PD:2||MAGNETISM:2||FECR2S4:2||SUPERCONDUCTING MGB2:2||WIRES:2||ABSORPTION:2||ENERGY:2||LA1XSRXMNO3:2||CONSTANTS:2||polaron:2||charge ordering:2||SCATTERING:2||XRAY PHOTOEMISSION:2||CeNiSn:2||phase diagram:2||PHOTOELECTRON:2||QUADRUPOLAR:2||perovskitemanganites:2||CO:2||SYSTEMS:2||DOPED ZNO:2||LOWFREQUENCY SOUND:2||LA:2||ELECTRONELECTRON SCATTERING:2||AU:2||DENSITYWAVE INSTABILITY:2||FERMISURFACE:2||hybridization:2||VALENCEBAND SATELLITE:2||SULFUR SPINEL:2||Heusler:2||APPROXIMATION:2||superexchange:2||colossal magnetoresistance:2||ALLOYS:2||DEPENDENCE:2||AG:2||electronic structures:2||AUGERSPECTRA:2||CR:2||PARAMETERS:2||DIFFRACTION:2||SEMICONDUCTORMETAL TRANSITION:1||INTERMEDIATEVALENCE:1||SMB6:1||SRRUO3:1||antiperovskite structure with antipolar nature:1||lowenergy twodimensional phonons:1||anatase TiO2:1||La3S4:1||metalinsulator transitions:1||MNO:1||ELECTRONICSTRUCTURES:1||MAGNETIC CIRCULARDICHROISM:1||Density functional theory:1||CeCo2:1||TOPOLARON CROSSOVER:1||EXCHANGE:1||cuprates:1||high Tc cuprates:1||magnetically ordered materials:1||ZNSE:1||Sr2xKxFeMoO6:1||CDW:1||TeCuO3:1||STRUCTURALPROPERTIES:1||MN:1||screening length:1||amorphous Fe:1||WAVE BASISSET:1||SILICONCARBIDE:1||HIGHPRESSURE:1||electronphonon coupling:1||quenched superconductivity:1||CMR perovskite manganites:1||OXIDE:1||polarons:1||synchrotron radiation:1||FULLERIDES:1||RESONANTPHOTOEMISSION:1||Silicon carbide:1||DFT calculation:1||Hybridized bands:1||GIANT MAGNETORESISTANCE:1||PEROVSKITES:1||Raman spectra:1||EXCHANGE ENHANCEMENT:1||SILICON:1||SR2FEMOO6:1||orbital ordering:1||delafossite:1||TITANIUMDIOXIDE:1||electronic structure of disordered solids:1||YFE2:1||Magnetic polaron:1||NA2TI2SB2O:1||STRONGCOUPLED SUPERCONDUCTORS:1||HEAVYFERMION SYSTEMS:1||firstprinciples calculations:1||MECHANISM:1||UNiSn:1||PHOTONIC BANDGAP:1||SINGLE IMPURITY:1||PHONONSPECTRUM:1||FERMISURFACE TOPOLOGY:1||SUPPRESSION:1||RESONANT PHOTOEMISSION:1||METALDOPED PICENE:1||PHOTOIONIZATION CROSSSECTIONS:1||PHOTOINDUCED FERRIMAGNETIC SYSTEMS:1||LINKAGE ISOMERISM:1||CHARGETRANSFER:1||Bilayer Graphene:1||MAGNETICFIELD:1||SPINWAVES:1||rareearth manganese oxides:1||magnonphonon interaction:1||NACO2O4:1||ENERGYBANDS:1||SELFENERGY:1||GAS:1||Fe0.5Cu0.5Cr2S4:1||scanning photoelectron microscopy (SPEM):1||MAGNETIC PROPERTIES:1||Stoner model:1||AMORPHOUS TRANSITIONMETALS:1||SPINGLASS STATES:1||NI:1||LA3NI2B2N3:1||SOLIDS:1||CEO2:1||BAND THEORY:1||dilute magnetic semiconductor:1||pyrochlore:1||Y1XPRXBA2CU3O7DELTA:1||and electronphonon interactions:1||VIBRATIONS:1||RAY PHOTOEMISSION:1||ALKALI CATION:1||Europium:1||colossal magnetoresistance:1||structural stability:1||ENERGYGAP:1||small polaron:1||DOUBLE EXCHANGE:1||Coulomb correlation:1||magnon:1||phonons:1||ELECTRON FERROMAGNETISM:1||CURIETEMPERATURE:1||ARPES:1||PLANEWAVE METHOD:1||Xray absorption spectroscopy (XAS):1||ROOMTEMPERATURE:1||MONOCHALCOGENIDES:1||HEAT:1||UPDSN:1||MOMENTS:1||XRAY ABSORPTION:1||SEMICONDUCTOR:1||Fermi surface nesting:1||optical phonon:1||disordered system:1||dilute magnetic semiconductors:1||CMR manganites:1||PHONONS:1||LATTICEDYNAMICS:1||OXIDES:1||4fphotoemission:1||permanent magnet:1||pseudogap:1||TRANSPORTPROPERTIES:1||ANTIFERROMAGNET:1||(BI,PB)SRCOO SYSTEM:1||semicore correlation:1||POLARIZATION:1||CRYSTAL:1||spinel:1||Xray magnetic circular dichroism (XMCD):1||magnetocapacitance:1||ANATASE:1||TEMPERATURES:1||Pseudogap:1||INTERFACE:1||SUBSTRATE:1||YNI2B2C:1||SAMARIUM SULFIDE:1||strong swave superconductor:1||DOPED MANGANITE:1||SYMMETRY:1||CENISN:1||resonance mode:1||DISORDERED SYSTEM:1||LITHIUM INTERCALATION:1||CUO2 PLANE:1||SURFACE:1||Delafossite:1||ELECTRICALPROPERTIES:1||NIMNSB:1||PTMNSB:1||ROOMTEMPERATURE FERROMAGNETISM:1||RUBIDIUM MANGANESE HEXACYANOFERRATE:1||COLOSSALMAGNETORESISTANCE:1||FINITE TEMPERATURES:1||LAMNO3:1||FE:1||transitionmetal oxides:1||giant magnetoresistance:1||phonon:1||COPPER OXIDES:1||valence states:1||thermoelectric:1||semiconductor:1||CATION DISTRIBUTION:1||FeCr2S4:1||photoemission spectroscopy (PES):1||METALLIC FERROMAGNETISM:1||GRAPHITE:1||SUSCEPTIBILITY:1||UBE13:1||RCrSb3:1||band JahnTeller:1||Ce3S4:1||TiO2:1||PrBa2Cu3O7delta:1||UNTWINNED PRBA2CU3O7:1||AGNIO2:1||HALFMETALLIC FERROMAGNETS:1||CI:1||Energy gap:1||Photoemission:1||Future applications:1||Photoemission measurements:1||Graphene:1||BANDSTRUCTURE:1||TC:1||superconductivity:1||magnetic semiconductors:1||CMRmanganites:1||thin films:1||spin dynamics:1||highTc superconductors:1||ITINERANTELECTRON FERROMAGNETISM:1||SINGLECRYSTALS:1||CeTe2:1||amorphous magnetic materials:1||EPITAXIAL GRAPHENE:1||LAYERED PNICTIDEOXIDES:1||BOROCARBIDE SUPERCONDUCTORS:1||AUGMENTEDWAVE METHOD:1||METALLIC MAGNET UNISN:1||ORIGIN:1||spectrum rearrangement:1||MEANFIELD THEORY:1||MOLECULEBASED MAGNETS:1||METASTABLE STATE:1||INSULATOR:1||magnetic orderin:1||FCC IRON:1||CeRu2:1||TL2MN2O7:1||isotope effect:1||Perovskitemanganites:1||RECURSION METHOD:1||PERPENDICULAR MAGNETICANISOTROPY:1||quasiparticle spectral density:1||GW:1||MANGANESE FERRITE:1||RESONANCE:1||SeCuO3:1||Optical conductivity:1||MASSLESS DIRAC FERMIONS:1||SCHOTTKYBARRIER:1||electronic structure:15||ELECTRONICSTRUCTURE:11||TRANSITIONMETAL COMPOUNDS:10||METALS:10||photoemission:8||SPECTRA:8||MAGNETORESISTANCE:7||FERROMAGNETISM:7||TRANSPORT:7||TRANSITION:6||FILMS:6||THINFILMS:5||TOTALENERGY CALCULATIONS:5||MAGNETICPROPERTIES:5||SUPERCONDUCTIVITY:5||PR:5||LATTICE:4||STATES:4||SPECTROSCOPY:4||FIELD:4||CRYSTALSTRUCTURE:4||PHOTOEMISSION:4||TEMPERATURE:4||TRANSITIONTEMPERATURE:4||XRAYABSORPTION:4||STATE:4||CU:4||BASISSET:4||XAS:4||CRYSTALS:3||EXCITATIONS:3||MOTTHUBBARD SYSTEMS:3||HIGHENERGY SPIN:3||halfmetal:3||INSULATORS:3||LA2CUO4:3||MODEL:3||FLUCTUATIONS:3||CE:3||double exchange:3||TRANSITIONMETALS:3||RESISTIVITY:3||BORON:3||LA1XCAXMNO3:3||IRON:3||PES:3||ANTIMONIDES:2||MgB2:2||ZR METALLIC GLASSES:2||superconductor:2||CRITICALCURRENT DENSITY:2||CIRCULARDICHROISM:2||SEMICONDUCTORS:2||LOCALIZATION:2||INTRABAND OPTICAL CONDUCTIVITY:2||COLOSSAL MAGNETORESISTANCE:2||OXIDATION:2||EXISTENCE:2||COPPER:2||diboride:2||MAGNESIUMDIBORIDE:2||GAP:2||CE COMPOUNDS:2||CORE POLARIZATION:2||magnetoresistance:2||photoemission spectroscopy:2||electronphonon interaction:2||GETTER:2||PD:2||MAGNETISM:2||FECR2S4:2||SUPERCONDUCTING MGB2:2||WIRES:2||ABSORPTION:2||ENERGY:2||LA1XSRXMNO3:2||CONSTANTS:2||polaron:2||charge ordering:2||SCATTERING:2||XRAY PHOTOEMISSION:2||CeNiSn:2||phase diagram:2||PHOTOELECTRON:2||QUADRUPOLAR:2||perovskitemanganites:2||CO:2||SYSTEMS:2||DOPED ZNO:2||LOWFREQUENCY SOUND:2||LA:2||ELECTRONELECTRON SCATTERING:2||AU:2||DENSITYWAVE INSTABILITY:2||FERMISURFACE:2||hybridization:2||VALENCEBAND SATELLITE:2||SULFUR SPINEL:2||Heusler:2||APPROXIMATION:2||superexchange:2||colossal magnetoresistance:2||ALLOYS:2||DEPENDENCE:2||AG:2||electronic structures:2||AUGERSPECTRA:2||CR:2||PARAMETERS:2||DIFFRACTION:2||SEMICONDUCTORMETAL TRANSITION:1||INTERMEDIATEVALENCE:1||SMB6:1||SRRUO3:1||antiperovskite structure with antipolar nature:1||lowenergy twodimensional phonons:1||anatase TiO2:1||La3S4:1||metalinsulator transitions:1||MNO:1||ELECTRONICSTRUCTURES:1||MAGNETIC CIRCULARDICHROISM:1||Density functional theory:1||CeCo2:1||TOPOLARON CROSSOVER:1||EXCHANGE:1||cuprates:1||high Tc cuprates:1||magnetically ordered materials:1||ZNSE:1||Sr2xKxFeMoO6:1||CDW:1||TeCuO3:1||STRUCTURALPROPERTIES:1||MN:1||screening length:1||amorphous Fe:1||WAVE BASISSET:1||SILICONCARBIDE:1||HIGHPRESSURE:1||electronphonon coupling:1||quenched superconductivity:1||CMR perovskite manganites:1||OXIDE:1||polarons:1||synchrotron radiation:1||FULLERIDES:1||RESONANTPHOTOEMISSION:1||Silicon carbide:1||DFT calculation:1||Hybridized bands:1||GIANT MAGNETORESISTANCE:1||PEROVSKITES:1||Raman spectra:1||EXCHANGE ENHANCEMENT:1||SILICON:1||SR2FEMOO6:1||orbital ordering:1||delafossite:1||TITANIUMDIOXIDE:1||electronic structure of disordered solids:1||YFE2:1||Magnetic polaron:1||NA2TI2SB2O:1||STRONGCOUPLED SUPERCONDUCTORS:1||HEAVYFERMION SYSTEMS:1||firstprinciples calculations:1||MECHANISM:1||UNiSn:1||PHOTONIC BANDGAP:1||SINGLE IMPURITY:1||PHONONSPECTRUM:1||FERMISURFACE TOPOLOGY:1||SUPPRESSION:1||RESONANT PHOTOEMISSION:1||METALDOPED PICENE:1||PHOTOIONIZATION CROSSSECTIONS:1||PHOTOINDUCED FERRIMAGNETIC SYSTEMS:1||LINKAGE ISOMERISM:1||CHARGETRANSFER:1||Bilayer Graphene:1||MAGNETICFIELD:1||SPINWAVES:1||rareearth manganese oxides:1||magnonphonon interaction:1||NACO2O4:1||ENERGYBANDS:1||SELFENERGY:1||GAS:1||Fe0.5Cu0.5Cr2S4:1||scanning photoelectron microscopy (SPEM):1||MAGNETIC PROPERTIES:1||Stoner model:1||AMORPHOUS TRANSITIONMETALS:1||SPINGLASS STATES:1||NI:1||LA3NI2B2N3:1||SOLIDS:1||CEO2:1||BAND THEORY:1||dilute magnetic semiconductor:1||pyrochlore:1||Y1XPRXBA2CU3O7DELTA:1||and electronphonon interactions:1||VIBRATIONS:1||RAY PHOTOEMISSION:1||ALKALI CATION:1||Europium:1||colossal magnetoresistance:1||structural stability:1||ENERGYGAP:1||small polaron:1||DOUBLE EXCHANGE:1||Coulomb correlation:1||magnon:1||phonons:1||ELECTRON FERROMAGNETISM:1||CURIETEMPERATURE:1||ARPES:1||PLANEWAVE METHOD:1||Xray absorption spectroscopy (XAS):1||ROOMTEMPERATURE:1||MONOCHALCOGENIDES:1||HEAT:1||UPDSN:1||MOMENTS:1||XRAY ABSORPTION:1||SEMICONDUCTOR:1||Fermi surface nesting:1||optical phonon:1||disordered system:1||dilute magnetic semiconductors:1||CMR manganites:1||PHONONS:1||LATTICEDYNAMICS:1||OXIDES:1||4fphotoemission:1||permanent magnet:1||pseudogap:1||TRANSPORTPROPERTIES:1||ANTIFERROMAGNET:1||(BI,PB)SRCOO SYSTEM:1||semicore correlation:1||POLARIZATION:1||CRYSTAL:1||spinel:1||Xray magnetic circular dichroism (XMCD):1||magnetocapacitance:1||ANATASE:1||TEMPERATURES:1||Pseudogap:1||INTERFACE:1||SUBSTRATE:1||YNI2B2C:1||SAMARIUM SULFIDE:1||strong swave superconductor:1||DOPED MANGANITE:1||SYMMETRY:1||CENISN:1||resonance mode:1||DISORDERED SYSTEM:1||LITHIUM INTERCALATION:1||CUO2 PLANE:1||SURFACE:1||Delafossite:1||ELECTRICALPROPERTIES:1||NIMNSB:1||PTMNSB:1||ROOMTEMPERATURE FERROMAGNETISM:1||RUBIDIUM MANGANESE HEXACYANOFERRATE:1||COLOSSALMAGNETORESISTANCE:1||FINITE TEMPERATURES:1||LAMNO3:1||FE:1||transitionmetal oxides:1||giant magnetoresistance:1||phonon:1||COPPER OXIDES:1||valence states:1||thermoelectric:1||semiconductor:1||CATION DISTRIBUTION:1||FeCr2S4:1||photoemission spectroscopy (PES):1||METALLIC FERROMAGNETISM:1||GRAPHITE:1||SUSCEPTIBILITY:1||UBE13:1||RCrSb3:1||band JahnTeller:1||Ce3S4:1||TiO2:1||PrBa2Cu3O7delta:1||UNTWINNED PRBA2CU3O7:1||AGNIO2:1||HALFMETALLIC FERROMAGNETS:1||CI:1||Energy gap:1||Photoemission:1||Future applications:1||Photoemission measurements:1||Graphene:1||BANDSTRUCTURE:1||TC:1||superconductivity:1||magnetic semiconductors:1||CMRmanganites:1||thin films:1||spin dynamics:1||highTc superconductors:1||ITINERANTELECTRON FERROMAGNETISM:1||SINGLECRYSTALS:1||CeTe2:1||amorphous magnetic materials:1||EPITAXIAL GRAPHENE:1||LAYERED PNICTIDEOXIDES:1||BOROCARBIDE SUPERCONDUCTORS:1||AUGMENTEDWAVE METHOD:1||METALLIC MAGNET UNISN:1||ORIGIN:1||spectrum rearrangement:1||MEANFIELD THEORY:1||MOLECULEBASED MAGNETS:1||METASTABLE STATE:1||INSULATOR:1||magnetic orderin:1||FCC IRON:1||CeRu2:1||TL2MN2O7:1||isotope effect:1||Perovskitemanganites:1||RECURSION METHOD:1||PERPENDICULAR MAGNETICANISOTROPY:1||quasiparticle spectral density:1||GW:1||MANGANESE FERRITE:1||RESONANCE:1||SeCuO3:1||Optical conductivity:1||MASSLESS DIRAC FERMIONS:1||SCHOTTKYBARRIER:1||electronic structure:15||ELECTRONICSTRUCTURE:11||TRANSITIONMETAL COMPOUNDS:10||METALS:10||photoemission:8||SPECTRA:8||MAGNETORESISTANCE:7||FERROMAGNETISM:7||TRANSPORT:7||TRANSITION:6||FILMS:6||THINFILMS:5||TOTALENERGY CALCULATIONS:5||MAGNETICPROPERTIES:5||SUPERCONDUCTIVITY:5||PR:5||LATTICE:4||STATES:4||SPECTROSCOPY:4||FIELD:4||CRYSTALSTRUCTURE:4||PHOTOEMISSION:4||TEMPERATURE:4||TRANSITIONTEMPERATURE:4||XRAYABSORPTION:4||STATE:4||CU:4||BASISSET:4||XAS:4||CRYSTALS:3||EXCITATIONS:3||MOTTHUBBARD SYSTEMS:3||HIGHENERGY SPIN:3||halfmetal:3||INSULATORS:3||LA2CUO4:3||MODEL:3||FLUCTUATIONS:3||CE:3||double exchange:3||TRANSITIONMETALS:3||RESISTIVITY:3||BORON:3||LA1XCAXMNO3:3||IRON:3||PES:3||ANTIMONIDES:2||MgB2:2||ZR METALLIC GLASSES:2||superconductor:2||CRITICALCURRENT DENSITY:2||CIRCULARDICHROISM:2||SEMICONDUCTORS:2||LOCALIZATION:2||INTRABAND OPTICAL CONDUCTIVITY:2||COLOSSAL MAGNETORESISTANCE:2||OXIDATION:2||EXISTENCE:2||COPPER:2||diboride:2||MAGNESIUMDIBORIDE:2||GAP:2||CE COMPOUNDS:2||CORE POLARIZATION:2||magnetoresistance:2||photoemission spectroscopy:2||electronphonon interaction:2||GETTER:2||PD:2||MAGNETISM:2||FECR2S4:2||SUPERCONDUCTING MGB2:2||WIRES:2||ABSORPTION:2||ENERGY:2||LA1XSRXMNO3:2||CONSTANTS:2||polaron:2||charge ordering:2||SCATTERING:2||XRAY PHOTOEMISSION:2||CeNiSn:2||phase diagram:2||PHOTOELECTRON:2||QUADRUPOLAR:2||perovskitemanganites:2||CO:2||SYSTEMS:2||DOPED ZNO:2||LOWFREQUENCY SOUND:2||LA:2||ELECTRONELECTRON SCATTERING:2||AU:2||DENSITYWAVE INSTABILITY:2||FERMISURFACE:2||hybridization:2||VALENCEBAND SATELLITE:2||SULFUR SPINEL:2||Heusler:2||APPROXIMATION:2||superexchange:2||colossal magnetoresistance:2||ALLOYS:2||DEPENDENCE:2||AG:2||electronic structures:2||AUGERSPECTRA:2||CR:2||PARAMETERS:2||DIFFRACTION:2||SEMICONDUCTORMETAL TRANSITION:1||INTERMEDIATEVALENCE:1||SMB6:1||SRRUO3:1||antiperovskite structure with antipolar nature:1||lowenergy twodimensional phonons:1||anatase TiO2:1||La3S4:1||metalinsulator transitions:1||MNO:1||ELECTRONICSTRUCTURES:1||MAGNETIC CIRCULARDICHROISM:1||Density functional theory:1||CeCo2:1||TOPOLARON CROSSOVER:1||EXCHANGE:1||cuprates:1||high Tc cuprates:1||magnetically ordered materials:1||ZNSE:1||Sr2xKxFeMoO6:1||CDW:1||TeCuO3:1||STRUCTURALPROPERTIES:1||MN:1||screening length:1||amorphous Fe:1||WAVE BASISSET:1||SILICONCARBIDE:1||HIGHPRESSURE:1||electronphonon coupling:1||quenched superconductivity:1||CMR perovskite manganites:1||OXIDE:1||polarons:1||synchrotron radiation:1||FULLERIDES:1||RESONANTPHOTOEMISSION:1||Silicon carbide:1||DFT calculation:1||Hybridized bands:1||GIANT MAGNETORESISTANCE:1||PEROVSKITES:1||Raman spectra:1||EXCHANGE ENHANCEMENT:1||SILICON:1||SR2FEMOO6:1||orbital ordering:1||delafossite:1||TITANIUMDIOXIDE:1||electronic structure of disordered solids:1||YFE2:1||Magnetic polaron:1||NA2TI2SB2O:1||STRONGCOUPLED SUPERCONDUCTORS:1||HEAVYFERMION SYSTEMS:1||firstprinciples calculations:1||MECHANISM:1||UNiSn:1||PHOTONIC BANDGAP:1||SINGLE IMPURITY:1||PHONONSPECTRUM:1||FERMISURFACE TOPOLOGY:1||SUPPRESSION:1||RESONANT PHOTOEMISSION:1||METALDOPED PICENE:1||PHOTOIONIZATION CROSSSECTIONS:1||PHOTOINDUCED FERRIMAGNETIC SYSTEMS:1||LINKAGE ISOMERISM:1||CHARGETRANSFER:1||Bilayer Graphene:1||MAGNETICFIELD:1||SPINWAVES:1||rareearth manganese oxides:1||magnonphonon interaction:1||NACO2O4:1||ENERGYBANDS:1||SELFENERGY:1||GAS:1||Fe0.5Cu0.5Cr2S4:1||scanning photoelectron microscopy (SPEM):1||MAGNETIC PROPERTIES:1||Stoner model:1||AMORPHOUS TRANSITIONMETALS:1||SPINGLASS STATES:1||NI:1||LA3NI2B2N3:1||SOLIDS:1||CEO2:1||BAND THEORY:1||dilute magnetic semiconductor:1||pyrochlore:1||Y1XPRXBA2CU3O7DELTA:1||and electronphonon interactions:1||VIBRATIONS:1||RAY PHOTOEMISSION:1||ALKALI CATION:1||Europium:1||colossal magnetoresistance:1||structural stability:1||ENERGYGAP:1||small polaron:1||DOUBLE EXCHANGE:1||Coulomb correlation:1||magnon:1||phonons:1||ELECTRON FERROMAGNETISM:1||CURIETEMPERATURE:1||ARPES:1||PLANEWAVE METHOD:1||Xray absorption spectroscopy (XAS):1||ROOMTEMPERATURE:1||MONOCHALCOGENIDES:1||HEAT:1||UPDSN:1||MOMENTS:1||XRAY ABSORPTION:1||SEMICONDUCTOR:1||Fermi surface nesting:1||optical phonon:1||disordered system:1||dilute magnetic semiconductors:1||CMR manganites:1||PHONONS:1||LATTICEDYNAMICS:1||OXIDES:1||4fphotoemission:1||permanent magnet:1||pseudogap:1||TRANSPORTPROPERTIES:1||ANTIFERROMAGNET:1||(BI,PB)SRCOO SYSTEM:1||semicore correlation:1||POLARIZATION:1||CRYSTAL:1||spinel:1||Xray magnetic circular dichroism (XMCD):1||magnetocapacitance:1||ANATASE:1||TEMPERATURES:1||Pseudogap:1||INTERFACE:1||SUBSTRATE:1||YNI2B2C:1||SAMARIUM SULFIDE:1||strong swave superconductor:1||DOPED MANGANITE:1||SYMMETRY:1||CENISN:1||resonance mode:1||DISORDERED SYSTEM:1||LITHIUM INTERCALATION:1||CUO2 PLANE:1||SURFACE:1||Delafossite:1||ELECTRICALPROPERTIES:1||NIMNSB:1||PTMNSB:1||ROOMTEMPERATURE FERROMAGNETISM:1||RUBIDIUM MANGANESE HEXACYANOFERRATE:1||COLOSSALMAGNETORESISTANCE:1||FINITE TEMPERATURES:1||LAMNO3:1||FE:1||transitionmetal oxides:1||giant magnetoresistance:1||phonon:1||COPPER OXIDES:1||valence states:1||thermoelectric:1||semiconductor:1||CATION DISTRIBUTION:1||FeCr2S4:1||photoemission spectroscopy (PES):1||METALLIC FERROMAGNETISM:1||GRAPHITE:1||SUSCEPTIBILITY:1||UBE13:1||RCrSb3:1||band JahnTeller:1||Ce3S4:1||TiO2:1||PrBa2Cu3O7delta:1||UNTWINNED PRBA2CU3O7:1||AGNIO2:1||HALFMETALLIC FERROMAGNETS:1||CI:1||Energy gap:1||Photoemission:1||Future applications:1||Photoemission measurements:1||Graphene:1||BANDSTRUCTURE:1||TC:1||superconductivity:1||magnetic semiconductors:1||CMRmanganites:1||thin films:1||spin dynamics:1||highTc superconductors:1||ITINERANTELECTRON FERROMAGNETISM:1||SINGLECRYSTALS:1||CeTe2:1||amorphous magnetic materials:1||EPITAXIAL GRAPHENE:1||LAYERED PNICTIDEOXIDES:1||BOROCARBIDE SUPERCONDUCTORS:1||AUGMENTEDWAVE METHOD:1||METALLIC MAGNET UNISN:1||ORIGIN:1||spectrum rearrangement:1||MEANFIELD THEORY:1||MOLECULEBASED MAGNETS:1||METASTABLE STATE:1||INSULATOR:1||magnetic orderin:1||FCC IRON:1||CeRu2:1||TL2MN2O7:1||isotope effect:1||Perovskitemanganites:1||RECURSION METHOD:1||PERPENDICULAR MAGNETICANISOTROPY:1||quasiparticle spectral density:1||GW:1||MANGANESE FERRITE:1||RESONANCE:1||SeCuO3:1||Optical conductivity:1||MASSLESS DIRAC FERMIONS:1||SCHOTTKYBARRIER:1||electronic structure:15||ELECTRONICSTRUCTURE:11||TRANSITIONMETAL COMPOUNDS:10||METALS:10||photoemission:8||SPECTRA:8||MAGNETORESISTANCE:7||FERROMAGNETISM:7||TRANSPORT:7||TRANSITION:6||FILMS:6||THINFILMS:5||TOTALENERGY CALCULATIONS:5||MAGNETICPROPERTIES:5||SUPERCONDUCTIVITY:5||PR:5||LATTICE:4||STATES:4||SPECTROSCOPY:4||FIELD:4||CRYSTALSTRUCTURE:4||PHOTOEMISSION:4||TEMPERATURE:4||TRANSITIONTEMPERATURE:4||XRAYABSORPTION:4||STATE:4||CU:4||BASISSET:4||XAS:4||CRYSTALS:3||EXCITATIONS:3||MOTTHUBBARD SYSTEMS:3||HIGHENERGY SPIN:3||halfmetal:3||INSULATORS:3||LA2CUO4:3||MODEL:3||FLUCTUATIONS:3||CE:3||double exchange:3||TRANSITIONMETALS:3||RESISTIVITY:3||BORON:3||LA1XCAXMNO3:3||IRON:3||PES:3||ANTIMONIDES:2||MgB2:2||ZR METALLIC GLASSES:2||superconductor:2||CRITICALCURRENT DENSITY:2||CIRCULARDICHROISM:2||SEMICONDUCTORS:2||LOCALIZATION:2||INTRABAND OPTICAL CONDUCTIVITY:2||COLOSSAL MAGNETORESISTANCE:2||OXIDATION:2||EXISTENCE:2||COPPER:2||diboride:2||MAGNESIUMDIBORIDE:2||GAP:2||CE COMPOUNDS:2||CORE POLARIZATION:2||magnetoresistance:2||photoemission spectroscopy:2||electronphonon interaction:2||GETTER:2||PD:2||MAGNETISM:2||FECR2S4:2||SUPERCONDUCTING MGB2:2||WIRES:2||ABSORPTION:2||ENERGY:2||LA1XSRXMNO3:2||CONSTANTS:2||polaron:2||charge ordering:2||SCATTERING:2||XRAY PHOTOEMISSION:2||CeNiSn:2||phase diagram:2||PHOTOELECTRON:2||QUADRUPOLAR:2||perovskitemanganites:2||CO:2||SYSTEMS:2||DOPED ZNO:2||LOWFREQUENCY SOUND:2||LA:2||ELECTRONELECTRON SCATTERING:2||AU:2||DENSITYWAVE INSTABILITY:2||FERMISURFACE:2||hybridization:2||VALENCEBAND SATELLITE:2||SULFUR SPINEL:2||Heusler:2||APPROXIMATION:2||superexchange:2||colossal magnetoresistance:2||ALLOYS:2||DEPENDENCE:2||AG:2||electronic structures:2||AUGERSPECTRA:2||CR:2||PARAMETERS:2||DIFFRACTION:2||SEMICONDUCTORMETAL TRANSITION:1||INTERMEDIATEVALENCE:1||SMB6:1||SRRUO3:1||antiperovskite structure with antipolar nature:1||lowenergy twodimensional phonons:1||anatase TiO2:1||La3S4:1||metalinsulator transitions:1||MNO:1||ELECTRONICSTRUCTURES:1||MAGNETIC CIRCULARDICHROISM:1||Density functional theory:1||CeCo2:1||TOPOLARON CROSSOVER:1||EXCHANGE:1||cuprates:1||high Tc cuprates:1||magnetically ordered materials:1||ZNSE:1||Sr2xKxFeMoO6:1||CDW:1||TeCuO3:1||STRUCTURALPROPERTIES:1||MN:1||screening length:1||amorphous Fe:1||WAVE BASISSET:1||SILICONCARBIDE:1||HIGHPRESSURE:1||electronphonon coupling:1||quenched superconductivity:1||CMR perovskite manganites:1||OXIDE:1||polarons:1||synchrotron radiation:1||FULLERIDES:1||RESONANTPHOTOEMISSION:1||Silicon carbide:1||DFT calculation:1||Hybridized bands:1||GIANT MAGNETORESISTANCE:1||PEROVSKITES:1||Raman spectra:1||EXCHANGE ENHANCEMENT:1||SILICON:1||SR2FEMOO6:1||orbital ordering:1||delafossite:1||TITANIUMDIOXIDE:1||electronic structure of disordered solids:1||YFE2:1||Magnetic polaron:1||NA2TI2SB2O:1||STRONGCOUPLED SUPERCONDUCTORS:1||HEAVYFERMION SYSTEMS:1||firstprinciples calculations:1||MECHANISM:1||UNiSn:1||PHOTONIC BANDGAP:1||SINGLE IMPURITY:1||PHONONSPECTRUM:1||FERMISURFACE TOPOLOGY:1||SUPPRESSION:1||RESONANT PHOTOEMISSION:1||METALDOPED PICENE:1||PHOTOIONIZATION CROSSSECTIONS:1||PHOTOINDUCED FERRIMAGNETIC SYSTEMS:1||LINKAGE ISOMERISM:1||CHARGETRANSFER:1||Bilayer Graphene:1||MAGNETICFIELD:1||SPINWAVES:1||rareearth manganese oxides:1||magnonphonon interaction:1||NACO2O4:1||ENERGYBANDS:1||SELFENERGY:1||GAS:1||Fe0.5Cu0.5Cr2S4:1||scanning photoelectron microscopy (SPEM):1||MAGNETIC PROPERTIES:1||Stoner model:1||AMORPHOUS TRANSITIONMETALS:1||SPINGLASS STATES:1||NI:1||LA3NI2B2N3:1||SOLIDS:1||CEO2:1||BAND THEORY:1||dilute magnetic semiconductor:1||pyrochlore:1||Y1XPRXBA2CU3O7DELTA:1||and electronphonon interactions:1||VIBRATIONS:1||RAY PHOTOEMISSION:1||ALKALI CATION:1||Europium:1||colossal magnetoresistance:1||structural stability:1||ENERGYGAP:1||small polaron:1||DOUBLE EXCHANGE:1||Coulomb correlation:1||magnon:1||phonons:1||ELECTRON FERROMAGNETISM:1||CURIETEMPERATURE:1||ARPES:1||PLANEWAVE METHOD:1||Xray absorption spectroscopy (XAS):1||ROOMTEMPERATURE:1||MONOCHALCOGENIDES:1||HEAT:1||UPDSN:1||MOMENTS:1||XRAY ABSORPTION:1||SEMICONDUCTOR:1||Fermi surface nesting:1||optical phonon:1||disordered system:1||dilute magnetic semiconductors:1||CMR manganites:1||PHONONS:1||LATTICEDYNAMICS:1||OXIDES:1||4fphotoemission:1||permanent magnet:1||pseudogap:1||TRANSPORTPROPERTIES:1||ANTIFERROMAGNET:1||(BI,PB)SRCOO SYSTEM:1||semicore correlation:1||POLARIZATION:1||CRYSTAL:1||spinel:1||Xray magnetic circular dichroism (XMCD):1||magnetocapacitance:1||ANATASE:1||TEMPERATURES:1||Pseudogap:1||INTERFACE:1||SUBSTRATE:1||YNI2B2C:1||SAMARIUM SULFIDE:1||strong swave superconductor:1||DOPED MANGANITE:1||SYMMETRY:1||CENISN:1||resonance mode:1||DISORDERED SYSTEM:1||LITHIUM INTERCALATION:1||CUO2 PLANE:1||SURFACE:1||Delafossite:1||ELECTRICALPROPERTIES:1||NIMNSB:1||PTMNSB:1||ROOMTEMPERATURE FERROMAGNETISM:1||RUBIDIUM MANGANESE HEXACYANOFERRATE:1||COLOSSALMAGNETORESISTANCE:1||FINITE TEMPERATURES:1||LAMNO3:1||FE:1||transitionmetal oxides:1||giant magnetoresistance:1||phonon:1||COPPER OXIDES:1||valence states:1||thermoelectric:1||semiconductor:1||CATION DISTRIBUTION:1||FeCr2S4:1||photoemission spectroscopy (PES):1||METALLIC FERROMAGNETISM:1||GRAPHITE:1||SUSCEPTIBILITY:1||UBE13:1||RCrSb3:1||band JahnTeller:1||Ce3S4:1||TiO2:1||PrBa2Cu3O7delta:1||UNTWINNED PRBA2CU3O7:1||AGNIO2:1||HALFMETALLIC FERROMAGNETS:1||CI:1||Energy gap:1||Photoemission:1||Future applications:1||Photoemission measurements:1||Graphene:1||BANDSTRUCTURE:1||TC:1||superconductivity:1||magnetic semiconductors:1||CMRmanganites:1||thin films:1||spin dynamics:1||highTc superconductors:1||ITINERANTELECTRON FERROMAGNETISM:1||SINGLECRYSTALS:1||CeTe2:1||amorphous magnetic materials:1||EPITAXIAL GRAPHENE:1||LAYERED PNICTIDEOXIDES:1||BOROCARBIDE SUPERCONDUCTORS:1||AUGMENTEDWAVE METHOD:1||METALLIC MAGNET UNISN:1||ORIGIN:1||spectrum rearrangement:1||MEANFIELD THEORY:1||MOLECULEBASED MAGNETS:1||METASTABLE STATE:1||INSULATOR:1||magnetic orderin:1||FCC IRON:1||CeRu2:1||TL2MN2O7:1||isotope effect:1||Perovskitemanganites:1||RECURSION METHOD:1||PERPENDICULAR MAGNETICANISOTROPY:1||quasiparticle spectral density:1||GW:1||MANGANESE FERRITE:1||RESONANCE:1||SeCuO3:1||Optical conductivity:1||MASSLESS DIRAC FERMIONS:1||SCHOTTKYBARRIER:1||electronic structure:15||ELECTRONICSTRUCTURE:11||TRANSITIONMETAL COMPOUNDS:10||METALS:10||photoemission:8||SPECTRA:8||MAGNETORESISTANCE:7||FERROMAGNETISM:7||TRANSPORT:7||TRANSITION:6||FILMS:6||THINFILMS:5||TOTALENERGY CALCULATIONS:5||MAGNETICPROPERTIES:5||SUPERCONDUCTIVITY:5||PR:5||LATTICE:4||STATES:4||SPECTROSCOPY:4||FIELD:4||CRYSTALSTRUCTURE:4||PHOTOEMISSION:4||TEMPERATURE:4||TRANSITIONTEMPERATURE:4||XRAYABSORPTION:4||STATE:4||CU:4||BASISSET:4||XAS:4||CRYSTALS:3||EXCITATIONS:3||MOTTHUBBARD SYSTEMS:3||HIGHENERGY SPIN:3||halfmetal:3||INSULATORS:3||LA2CUO4:3||MODEL:3||FLUCTUATIONS:3||CE:3||double exchange:3||TRANSITIONMETALS:3||RESISTIVITY:3||BORON:3||LA1XCAXMNO3:3||IRON:3||PES:3||ANTIMONIDES:2||MgB2:2||ZR METALLIC GLASSES:2||superconductor:2||CRITICALCURRENT DENSITY:2||CIRCULARDICHROISM:2||SEMICONDUCTORS:2||LOCALIZATION:2||INTRABAND OPTICAL CONDUCTIVITY:2||COLOSSAL MAGNETORESISTANCE:2||OXIDATION:2||EXISTENCE:2||COPPER:2||diboride:2||MAGNESIUMDIBORIDE:2||GAP:2||CE COMPOUNDS:2||CORE POLARIZATION:2||magnetoresistance:2||photoemission spectroscopy:2||electronphonon interaction:2||GETTER:2||PD:2||MAGNETISM:2||FECR2S4:2||SUPERCONDUCTING MGB2:2||WIRES:2||ABSORPTION:2||ENERGY:2||LA1XSRXMNO3:2||CONSTANTS:2||polaron:2||charge ordering:2||SCATTERING:2||XRAY PHOTOEMISSION:2||CeNiSn:2||phase diagram:2||PHOTOELECTRON:2||QUADRUPOLAR:2||perovskitemanganites:2||CO:2||SYSTEMS:2||DOPED ZNO:2||LOWFREQUENCY SOUND:2||LA:2||ELECTRONELECTRON SCATTERING:2||AU:2||DENSITYWAVE INSTABILITY:2||FERMISURFACE:2||hybridization:2||VALENCEBAND SATELLITE:2||SULFUR SPINEL:2||Heusler:2||APPROXIMATION:2||superexchange:2||colossal magnetoresistance:2||ALLOYS:2||DEPENDENCE:2||AG:2||electronic structures:2||AUGERSPECTRA:2||CR:2||PARAMETERS:2||DIFFRACTION:2||SEMICONDUCTORMETAL TRANSITION:1||INTERMEDIATEVALENCE:1||SMB6:1||SRRUO3:1||antiperovskite structure with antipolar nature:1||lowenergy twodimensional phonons:1||anatase TiO2:1||La3S4:1||metalinsulator transitions:1||MNO:1||ELECTRONICSTRUCTURES:1||MAGNETIC CIRCULARDICHROISM:1||Density functional theory:1||CeCo2:1||TOPOLARON CROSSOVER:1||EXCHANGE:1||cuprates:1||high Tc cuprates:1||magnetically ordered materials:1||ZNSE:1||Sr2xKxFeMoO6:1||CDW:1||TeCuO3:1||STRUCTURALPROPERTIES:1||MN:1||screening length:1||amorphous Fe:1||WAVE BASISSET:1||SILICONCARBIDE:1||HIGHPRESSURE:1||electronphonon coupling:1||quenched superconductivity:1||CMR perovskite manganites:1||OXIDE:1||polarons:1||synchrotron radiation:1||FULLERIDES:1||RESONANTPHOTOEMISSION:1||Silicon carbide:1||DFT calculation:1||Hybridized bands:1||GIANT MAGNETORESISTANCE:1||PEROVSKITES:1||Raman spectra:1||EXCHANGE ENHANCEMENT:1||SILICON:1||SR2FEMOO6:1||orbital ordering:1||delafossite:1||TITANIUMDIOXIDE:1||electronic structure of disordered solids:1||YFE2:1||Magnetic polaron:1||NA2TI2SB2O:1||STRONGCOUPLED SUPERCONDUCTORS:1||HEAVYFERMION SYSTEMS:1||firstprinciples calculations:1||MECHANISM:1||UNiSn:1||PHOTONIC BANDGAP:1||SINGLE IMPURITY:1||PHONONSPECTRUM:1||FERMISURFACE TOPOLOGY:1||SUPPRESSION:1||RESONANT PHOTOEMISSION:1||METALDOPED PICENE:1||PHOTOIONIZATION CROSSSECTIONS:1||PHOTOINDUCED FERRIMAGNETIC SYSTEMS:1||LINKAGE ISOMERISM:1||CHARGETRANSFER:1||Bilayer Graphene:1||MAGNETICFIELD:1||SPINWAVES:1||rareearth manganese oxides:1||magnonphonon interaction:1||NACO2O4:1||ENERGYBANDS:1||SELFENERGY:1||GAS:1||Fe0.5Cu0.5Cr2S4:1||scanning photoelectron microscopy (SPEM):1||MAGNETIC PROPERTIES:1||Stoner model:1||AMORPHOUS TRANSITIONMETALS:1||SPINGLASS STATES:1||NI:1||LA3NI2B2N3:1||SOLIDS:1||CEO2:1||BAND THEORY:1||dilute magnetic semiconductor:1||pyrochlore:1||Y1XPRXBA2CU3O7DELTA:1||and electronphonon interactions:1||VIBRATIONS:1||RAY PHOTOEMISSION:1||ALKALI CATION:1||Europium:1||colossal magnetoresistance:1||structural stability:1||ENERGYGAP:1||small polaron:1||DOUBLE EXCHANGE:1||Coulomb correlation:1||magnon:1||phonons:1||ELECTRON FERROMAGNETISM:1||CURIETEMPERATURE:1||ARPES:1||PLANEWAVE METHOD:1||Xray absorption spectroscopy (XAS):1||ROOMTEMPERATURE:1||MONOCHALCOGENIDES:1||HEAT:1||UPDSN:1||MOMENTS:1||XRAY ABSORPTION:1||SEMICONDUCTOR:1||Fermi surface nesting:1||optical phonon:1||disordered system:1||dilute magnetic semiconductors:1||CMR manganites:1||PHONONS:1||LATTICEDYNAMICS:1||OXIDES:1||4fphotoemission:1||permanent magnet:1||pseudogap:1||TRANSPORTPROPERTIES:1||ANTIFERROMAGNET:1||(BI,PB)SRCOO SYSTEM:1||semicore correlation:1||POLARIZATION:1||CRYSTAL:1||spinel:1||Xray magnetic circular dichroism (XMCD):1||magnetocapacitance:1||ANATASE:1||TEMPERATURES:1||Pseudogap:1||INTERFACE:1||SUBSTRATE:1||YNI2B2C:1||SAMARIUM SULFIDE:1||strong swave superconductor:1||DOPED MANGANITE:1||SYMMETRY:1||CENISN:1||resonance mode:1||DISORDERED SYSTEM:1||LITHIUM INTERCALATION:1||CUO2 PLANE:1||SURFACE:1||Delafossite:1||ELECTRICALPROPERTIES:1||NIMNSB:1||PTMNSB:1||ROOMTEMPERATURE FERROMAGNETISM:1||RUBIDIUM MANGANESE HEXACYANOFERRATE:1||COLOSSALMAGNETORESISTANCE:1||FINITE TEMPERATURES:1||LAMNO3:1||FE:1||transitionmetal oxides:1||giant magnetoresistance:1||phonon:1||COPPER OXIDES:1||valence states:1||thermoelectric:1||semiconductor:1||CATION DISTRIBUTION:1||FeCr2S4:1||photoemission spectroscopy (PES):1||METALLIC FERROMAGNETISM:1||GRAPHITE:1||SUSCEPTIBILITY:1||UBE13:1||RCrSb3:1||band JahnTeller:1||Ce3S4:1||TiO2:1||PrBa2Cu3O7delta:1||UNTWINNED PRBA2CU3O7:1||AGNIO2:1||HALFMETALLIC FERROMAGNETS:1||CI:1||Energy gap:1||Photoemission:1||Future applications:1||Photoemission measurements:1||Graphene:1||BANDSTRUCTURE:1||TC:1||superconductivity:1||magnetic semiconductors:1||CMRmanganites:1||thin films:1||spin dynamics:1||highTc superconductors:1||ITINERANTELECTRON FERROMAGNETISM:1||SINGLECRYSTALS:1||CeTe2:1||amorphous magnetic materials:1||EPITAXIAL GRAPHENE:1||LAYERED PNICTIDEOXIDES:1||BOROCARBIDE SUPERCONDUCTORS:1||AUGMENTEDWAVE METHOD:1||METALLIC MAGNET UNISN:1||ORIGIN:1||spectrum rearrangement:1||MEANFIELD THEORY:1||MOLECULEBASED MAGNETS:1||METASTABLE STATE:1||INSULATOR:1||magnetic orderin:1||FCC IRON:1||CeRu2:1||TL2MN2O7:1||isotope effect:1||Perovskitemanganites:1||RECURSION METHOD:1||PERPENDICULAR MAGNETICANISOTROPY:1||quasiparticle spectral density:1||GW:1||MANGANESE FERRITE:1||RESONANCE:1||SeCuO3:1||Optical conductivity:1||MASSLESS DIRAC FERMIONS:1||SCHOTTKYBARRIER:1||electronic structure:15||ELECTRONICSTRUCTURE:11||TRANSITIONMETAL COMPOUNDS:10||METALS:10||photoemission:8||SPECTRA:8||MAGNETORESISTANCE:7||FERROMAGNETISM:7||TRANSPORT:7||TRANSITION:6||FILMS:6||THINFILMS:5||TOTALENERGY CALCULATIONS:5||MAGNETICPROPERTIES:5||SUPERCONDUCTIVITY:5||PR:5||LATTICE:4||STATES:4||SPECTROSCOPY:4||FIELD:4||CRYSTALSTRUCTURE:4||PHOTOEMISSION:4||TEMPERATURE:4||TRANSITIONTEMPERATURE:4||XRAYABSORPTION:4||STATE:4||CU:4||BASISSET:4||XAS:4||CRYSTALS:3||EXCITATIONS:3||MOTTHUBBARD SYSTEMS:3||HIGHENERGY SPIN:3||halfmetal:3||INSULATORS:3||LA2CUO4:3||MODEL:3||FLUCTUATIONS:3||CE:3||double exchange:3||TRANSITIONMETALS:3||RESISTIVITY:3||BORON:3||LA1XCAXMNO3:3||IRON:3||PES:3||ANTIMONIDES:2||MgB2:2||ZR METALLIC GLASSES:2||superconductor:2||CRITICALCURRENT DENSITY:2||CIRCULARDICHROISM:2||SEMICONDUCTORS:2||LOCALIZATION:2||INTRABAND OPTICAL CONDUCTIVITY:2||COLOSSAL MAGNETORESISTANCE:2||OXIDATION:2||EXISTENCE:2||COPPER:2||diboride:2||MAGNESIUMDIBORIDE:2||GAP:2||CE COMPOUNDS:2||CORE POLARIZATION:2||magnetoresistance:2||photoemission spectroscopy:2||electronphonon interaction:2||GETTER:2||PD:2||MAGNETISM:2||FECR2S4:2||SUPERCONDUCTING MGB2:2||WIRES:2||ABSORPTION:2||ENERGY:2||LA1XSRXMNO3:2||CONSTANTS:2||polaron:2||charge ordering:2||SCATTERING:2||XRAY PHOTOEMISSION:2||CeNiSn:2||phase diagram:2||PHOTOELECTRON:2||QUADRUPOLAR:2||perovskitemanganites:2||CO:2||SYSTEMS:2||DOPED ZNO:2||LOWFREQUENCY SOUND:2||LA:2||ELECTRONELECTRON SCATTERING:2||AU:2||DENSITYWAVE INSTABILITY:2||FERMISURFACE:2||hybridization:2||VALENCEBAND SATELLITE:2||SULFUR SPINEL:2||Heusler:2||APPROXIMATION:2||superexchange:2||colossal magnetoresistance:2||ALLOYS:2||DEPENDENCE:2||AG:2||electronic structures:2||AUGERSPECTRA:2||CR:2||PARAMETERS:2||DIFFRACTION:2||SEMICONDUCTORMETAL TRANSITION:1||INTERMEDIATEVALENCE:1||SMB6:1||SRRUO3:1||antiperovskite structure with antipolar nature:1||lowenergy twodimensional phonons:1||anatase TiO2:1||La3S4:1||metalinsulator transitions:1||MNO:1||ELECTRONICSTRUCTURES:1||MAGNETIC CIRCULARDICHROISM:1||Density functional theory:1||CeCo2:1||TOPOLARON CROSSOVER:1||EXCHANGE:1||cuprates:1||high Tc cuprates:1||magnetically ordered materials:1||ZNSE:1||Sr2xKxFeMoO6:1||CDW:1||TeCuO3:1||STRUCTURALPROPERTIES:1||MN:1||screening length:1||amorphous Fe:1||WAVE BASISSET:1||SILICONCARBIDE:1||HIGHPRESSURE:1||electronphonon coupling:1||quenched superconductivity:1||CMR perovskite manganites:1||OXIDE:1||polarons:1||synchrotron radiation:1||FULLERIDES:1||RESONANTPHOTOEMISSION:1||Silicon carbide:1||DFT calculation:1||Hybridized bands:1||GIANT MAGNETORESISTANCE:1||PEROVSKITES:1||Raman spectra:1||EXCHANGE ENHANCEMENT:1||SILICON:1||SR2FEMOO6:1||orbital ordering:1||delafossite:1||TITANIUMDIOXIDE:1||electronic structure of disordered solids:1||YFE2:1||Magnetic polaron:1||NA2TI2SB2O:1||STRONGCOUPLED SUPERCONDUCTORS:1||HEAVYFERMION SYSTEMS:1||firstprinciples calculations:1||MECHANISM:1||UNiSn:1||PHOTONIC BANDGAP:1||SINGLE IMPURITY:1||PHONONSPECTRUM:1||FERMISURFACE TOPOLOGY:1||SUPPRESSION:1||RESONANT PHOTOEMISSION:1||METALDOPED PICENE:1||PHOTOIONIZATION CROSSSECTIONS:1||PHOTOINDUCED FERRIMAGNETIC SYSTEMS:1||LINKAGE ISOMERISM:1||CHARGETRANSFER:1||Bilayer Graphene:1||MAGNETICFIELD:1||SPINWAVES:1||rareearth manganese oxides:1||magnonphonon interaction:1||NACO2O4:1||ENERGYBANDS:1||SELFENERGY:1||GAS:1||Fe0.5Cu0.5Cr2S4:1||scanning photoelectron microscopy (SPEM):1||MAGNETIC PROPERTIES:1||Stoner model:1||AMORPHOUS TRANSITIONMETALS:1||SPINGLASS STATES:1||NI:1||LA3NI2B2N3:1||SOLIDS:1||CEO2:1||BAND THEORY:1||dilute magnetic semiconductor:1||pyrochlore:1||Y1XPRXBA2CU3O7DELTA:1||and electronphonon interactions:1||VIBRATIONS:1||RAY PHOTOEMISSION:1||ALKALI CATION:1||Europium:1||colossal magnetoresistance:1||structural stability:1||ENERGYGAP:1||small polaron:1||DOUBLE EXCHANGE:1||Coulomb correlation:1||magnon:1||phonons:1||ELECTRON FERROMAGNETISM:1||CURIETEMPERATURE:1||ARPES:1||PLANEWAVE METHOD:1||Xray absorption spectroscopy (XAS):1||ROOMTEMPERATURE:1||MONOCHALCOGENIDES:1||HEAT:1||UPDSN:1||MOMENTS:1||XRAY ABSORPTION:1||SEMICONDUCTOR:1||Fermi surface nesting:1||optical phonon:1||disordered system:1||dilute magnetic semiconductors:1||CMR manganites:1||PHONONS:1||LATTICEDYNAMICS:1||OXIDES:1||4fphotoemission:1||permanent magnet:1||pseudogap:1||TRANSPORTPROPERTIES:1||ANTIFERROMAGNET:1||(BI,PB)SRCOO SYSTEM:1||semicore correlation:1||POLARIZATION:1||CRYSTAL:1||spinel:1||Xray magnetic circular dichroism (XMCD):1||magnetocapacitance:1||ANATASE:1||TEMPERATURES:1||Pseudogap:1||INTERFACE:1||SUBSTRATE:1||YNI2B2C:1||SAMARIUM SULFIDE:1||strong swave superconductor:1||DOPED MANGANITE:1||SYMMETRY:1||CENISN:1||resonance mode:1||DISORDERED SYSTEM:1||LITHIUM INTERCALATION:1||CUO2 PLANE:1||SURFACE:1||Delafossite:1||ELECTRICALPROPERTIES:1||NIMNSB:1||PTMNSB:1||ROOMTEMPERATURE FERROMAGNETISM:1||RUBIDIUM MANGANESE HEXACYANOFERRATE:1||COLOSSALMAGNETORESISTANCE:1||FINITE TEMPERATURES:1||LAMNO3:1||FE:1||transitionmetal oxides:1||giant magnetoresistance:1||phonon:1||COPPER OXIDES:1||valence states:1||thermoelectric:1||semiconductor:1||CATION DISTRIBUTION:1||FeCr2S4:1||photoemission spectroscopy (PES):1||METALLIC FERROMAGNETISM:1||GRAPHITE:1||SUSCEPTIBILITY:1||UBE13:1||RCrSb3:1||band JahnTeller:1||Ce3S4:1||TiO2:1||PrBa2Cu3O7delta:1||UNTWINNED PRBA2CU3O7:1||AGNIO2:1||HALFMETALLIC FERROMAGNETS:1||CI:1||Energy gap:1||Photoemission:1||Future applications:1||Photoemission measurements:1||Graphene:1||BANDSTRUCTURE:1||TC:1||superconductivity:1||magnetic semiconductors:1||CMRmanganites:1||thin films:1||spin dynamics:1||highTc superconductors:1||ITINERANTELECTRON FERROMAGNETISM:1||SINGLECRYSTALS:1||CeTe2:1||amorphous magnetic materials:1||EPITAXIAL GRAPHENE:1||LAYERED PNICTIDEOXIDES:1||BOROCARBIDE SUPERCONDUCTORS:1||AUGMENTEDWAVE METHOD:1||METALLIC MAGNET UNISN:1||ORIGIN:1||spectrum rearrangement:1||MEANFIELD THEORY:1||MOLECULEBASED MAGNETS:1||METASTABLE STATE:1||INSULATOR:1||magnetic orderin:1||FCC IRON:1||CeRu2:1||TL2MN2O7:1||isotope effect:1||Perovskitemanganites:1||RECURSION METHOD:1||PERPENDICULAR MAGNETICANISOTROPY:1||quasiparticle spectral density:1||GW:1||MANGANESE FERRITE:1||RESONANCE:1||SeCuO3:1||Optical conductivity:1||MASSLESS DIRAC FERMIONS:1||SCHOTTKYBARRIER:1||electronic structure:15||ELECTRONICSTRUCTURE:11||TRANSITIONMETAL COMPOUNDS:10||METALS:10||photoemission:8||SPECTRA:8||MAGNETORESISTANCE:7||FERROMAGNETISM:7||TRANSPORT:7||TRANSITION:6||FILMS:6||THINFILMS:5||TOTALENERGY CALCULATIONS:5||MAGNETICPROPERTIES:5||SUPERCONDUCTIVITY:5||PR:5||LATTICE:4||STATES:4||SPECTROSCOPY:4||FIELD:4||CRYSTALSTRUCTURE:4||PHOTOEMISSION:4||TEMPERATURE:4||TRANSITIONTEMPERATURE:4||XRAYABSORPTION:4||STATE:4||CU:4||BASISSET:4||XAS:4||CRYSTALS:3||EXCITATIONS:3||MOTTHUBBARD SYSTEMS:3||HIGHENERGY SPIN:3||halfmetal:3||INSULATORS:3||LA2CUO4:3||MODEL:3||FLUCTUATIONS:3||CE:3||double exchange:3||TRANSITIONMETALS:3||RESISTIVITY:3||BORON:3||LA1XCAXMNO3:3||IRON:3||PES:3||ANTIMONIDES:2||MgB2:2||ZR METALLIC GLASSES:2||superconductor:2||CRITICALCURRENT DENSITY:2||CIRCULARDICHROISM:2||SEMICONDUCTORS:2||LOCALIZATION:2||INTRABAND OPTICAL CONDUCTIVITY:2||COLOSSAL MAGNETORESISTANCE:2||OXIDATION:2||EXISTENCE:2||COPPER:2||diboride:2||MAGNESIUMDIBORIDE:2||GAP:2||CE COMPOUNDS:2||CORE POLARIZATION:2||magnetoresistance:2||photoemission spectroscopy:2||electronphonon interaction:2||GETTER:2||PD:2||MAGNETISM:2||FECR2S4:2||SUPERCONDUCTING MGB2:2||WIRES:2||ABSORPTION:2||ENERGY:2||LA1XSRXMNO3:2||CONSTANTS:2||polaron:2||charge ordering:2||SCATTERING:2||XRAY PHOTOEMISSION:2||CeNiSn:2||phase diagram:2||PHOTOELECTRON:2||QUADRUPOLAR:2||perovskitemanganites:2||CO:2||SYSTEMS:2||DOPED ZNO:2||LOWFREQUENCY SOUND:2||LA:2||ELECTRONELECTRON SCATTERING:2||AU:2||DENSITYWAVE INSTABILITY:2||FERMISURFACE:2||hybridization:2||VALENCEBAND SATELLITE:2||SULFUR SPINEL:2||Heusler:2||APPROXIMATION:2||superexchange:2||colossal magnetoresistance:2||ALLOYS:2||DEPENDENCE:2||AG:2||electronic structures:2||AUGERSPECTRA:2||CR:2||PARAMETERS:2||DIFFRACTION:2||SEMICONDUCTORMETAL TRANSITION:1||INTERMEDIATEVALENCE:1||SMB6:1||SRRUO3:1||antiperovskite structure with antipolar nature:1||lowenergy twodimensional phonons:1||anatase TiO2:1||La3S4:1||metalinsulator transitions:1||MNO:1||ELECTRONICSTRUCTURES:1||MAGNETIC CIRCULARDICHROISM:1||Density functional theory:1||CeCo2:1||TOPOLARON CROSSOVER:1||EXCHANGE:1||cuprates:1||high Tc cuprates:1||magnetically ordered materials:1||ZNSE:1||Sr2xKxFeMoO6:1||CDW:1||TeCuO3:1||STRUCTURALPROPERTIES:1||MN:1||screening length:1||amorphous Fe:1||WAVE BASISSET:1||SILICONCARBIDE:1||HIGHPRESSURE:1||electronphonon coupling:1||quenched superconductivity:1||CMR perovskite manganites:1||OXIDE:1||polarons:1||synchrotron radiation:1||FULLERIDES:1||RESONANTPHOTOEMISSION:1||Silicon carbide:1||DFT calculation:1||Hybridized bands:1||GIANT MAGNETORESISTANCE:1||PEROVSKITES:1||Raman spectra:1||EXCHANGE ENHANCEMENT:1||SILICON:1||SR2FEMOO6:1||orbital ordering:1||delafossite:1||TITANIUMDIOXIDE:1||electronic structure of disordered solids:1||YFE2:1||Magnetic polaron:1||NA2TI2SB2O:1||STRONGCOUPLED SUPERCONDUCTORS:1||HEAVYFERMION SYSTEMS:1||firstprinciples calculations:1||MECHANISM:1||UNiSn:1||PHOTONIC BANDGAP:1||SINGLE IMPURITY:1||PHONONSPECTRUM:1||FERMISURFACE TOPOLOGY:1||SUPPRESSION:1||RESONANT PHOTOEMISSION:1||METALDOPED PICENE:1||PHOTOIONIZATION CROSSSECTIONS:1||PHOTOINDUCED FERRIMAGNETIC SYSTEMS:1||LINKAGE ISOMERISM:1||CHARGETRANSFER:1||Bilayer Graphene:1||MAGNETICFIELD:1||SPINWAVES:1||rareearth manganese oxides:1||magnonphonon interaction:1||NACO2O4:1||ENERGYBANDS:1||SELFENERGY:1||GAS:1||Fe0.5Cu0.5Cr2S4:1||scanning photoelectron microscopy (SPEM):1||MAGNETIC PROPERTIES:1||Stoner model:1||AMORPHOUS TRANSITIONMETALS:1||SPINGLASS STATES:1||NI:1||LA3NI2B2N3:1||SOLIDS:1||CEO2:1||BAND THEORY:1||dilute magnetic semiconductor:1||pyrochlore:1||Y1XPRXBA2CU3O7DELTA:1||and electronphonon interactions:1||VIBRATIONS:1||RAY PHOTOEMISSION:1||ALKALI CATION:1||Europium:1||colossal magnetoresistance:1||structural stability:1||ENERGYGAP:1||small polaron:1||DOUBLE EXCHANGE:1||Coulomb correlation:1||magnon:1||phonons:1||ELECTRON FERROMAGNETISM:1||CURIETEMPERATURE:1||ARPES:1||PLANEWAVE METHOD:1||Xray absorption spectroscopy (XAS):1||ROOMTEMPERATURE:1||MONOCHALCOGENIDES:1||HEAT:1||UPDSN:1||MOMENTS:1||XRAY ABSORPTION:1||SEMICONDUCTOR:1||Fermi surface nesting:1||optical phonon:1||disordered system:1||dilute magnetic semiconductors:1||CMR manganites:1||PHONONS:1||LATTICEDYNAMICS:1||OXIDES:1||4fphotoemission:1||permanent magnet:1||pseudogap:1||TRANSPORTPROPERTIES:1||ANTIFERROMAGNET:1||(BI,PB)SRCOO SYSTEM:1||semicore correlation:1||POLARIZATION:1||CRYSTAL:1||spinel:1||Xray magnetic circular dichroism (XMCD):1||magnetocapacitance:1||ANATASE:1||TEMPERATURES:1||Pseudogap:1||INTERFACE:1||SUBSTRATE:1||YNI2B2C:1||SAMARIUM SULFIDE:1||strong swave superconductor:1||DOPED MANGANITE:1||SYMMETRY:1||CENISN:1||resonance mode:1||DISORDERED SYSTEM:1||LITHIUM INTERCALATION:1||CUO2 PLANE:1||SURFACE:1||Delafossite:1||ELECTRICALPROPERTIES:1||NIMNSB:1||PTMNSB:1||ROOMTEMPERATURE FERROMAGNETISM:1||RUBIDIUM MANGANESE HEXACYANOFERRATE:1||COLOSSALMAGNETORESISTANCE:1||FINITE TEMPERATURES:1||LAMNO3:1||FE:1||transitionmetal oxides:1||giant magnetoresistance:1||phonon:1||COPPER OXIDES:1||valence states:1||thermoelectric:1||semiconductor:1||CATION DISTRIBUTION:1||FeCr2S4:1||photoemission spectroscopy (PES):1||METALLIC FERROMAGNETISM:1||GRAPHITE:1||SUSCEPTIBILITY:1||UBE13:1||RCrSb3:1||band JahnTeller:1||Ce3S4:1||TiO2:1||PrBa2Cu3O7delta:1||UNTWINNED PRBA2CU3O7:1||AGNIO2:1||HALFMETALLIC FERROMAGNETS:1||CI:1||Energy gap:1||Photoemission:1||Future applications:1||Photoemission measurements:1||Graphene:1||BANDSTRUCTURE:1||TC:1||superconductivity:1||magnetic semiconductors:1||CMRmanganites:1||thin films:1||spin dynamics:1||highTc superconductors:1||ITINERANTELECTRON FERROMAGNETISM:1||SINGLECRYSTALS:1||CeTe2:1||amorphous magnetic materials:1||EPITAXIAL GRAPHENE:1||LAYERED PNICTIDEOXIDES:1||BOROCARBIDE SUPERCONDUCTORS:1||AUGMENTEDWAVE METHOD:1||METALLIC MAGNET UNISN:1||ORIGIN:1||spectrum rearrangement:1||MEANFIELD THEORY:1||MOLECULEBASED MAGNETS:1||METASTABLE STATE:1||INSULATOR:1||magnetic orderin:1||FCC IRON:1||CeRu2:1||TL2MN2O7:1||isotope effect:1||Perovskitemanganites:1||RECURSION METHOD:1||PERPENDICULAR MAGNETICANISOTROPY:1||quasiparticle spectral density:1||GW:1||MANGANESE FERRITE:1||RESONANCE:1||SeCuO3:1||Optical conductivity:1||MASSLESS DIRAC FERMIONS:1||SCHOTTKYBARRIER:1||electronic structure:15||ELECTRONICSTRUCTURE:11||TRANSITIONMETAL COMPOUNDS:10||METALS:10||photoemission:8||SPECTRA:8||MAGNETORESISTANCE:7||FERROMAGNETISM:7||TRANSPORT:7||TRANSITION:6||FILMS:6||THINFILMS:5||TOTALENERGY CALCULATIONS:5||MAGNETICPROPERTIES:5||SUPERCONDUCTIVITY:5||PR:5||LATTICE:4||STATES:4||SPECTROSCOPY:4||FIELD:4||CRYSTALSTRUCTURE:4||PHOTOEMISSION:4||TEMPERATURE:4||TRANSITIONTEMPERATURE:4||XRAYABSORPTION:4||STATE:4||CU:4||BASISSET:4||XAS:4||CRYSTALS:3||EXCITATIONS:3||MOTTHUBBARD SYSTEMS:3||HIGHENERGY SPIN:3||halfmetal:3||INSULATORS:3||LA2CUO4:3||MODEL:3||FLUCTUATIONS:3||CE:3||double exchange:3||TRANSITIONMETALS:3||RESISTIVITY:3||BORON:3||LA1XCAXMNO3:3||IRON:3||PES:3||ANTIMONIDES:2||MgB2:2||ZR METALLIC GLASSES:2||superconductor:2||CRITICALCURRENT DENSITY:2||CIRCULARDICHROISM:2||SEMICONDUCTORS:2||LOCALIZATION:2||INTRABAND OPTICAL CONDUCTIVITY:2||COLOSSAL MAGNETORESISTANCE:2||OXIDATION:2||EXISTENCE:2||COPPER:2||diboride:2||MAGNESIUMDIBORIDE:2||GAP:2||CE COMPOUNDS:2||CORE POLARIZATION:2||magnetoresistance:2||photoemission spectroscopy:2||electronphonon interaction:2||GETTER:2||PD:2||MAGNETISM:2||FECR2S4:2||SUPERCONDUCTING MGB2:2||WIRES:2||ABSORPTION:2||ENERGY:2||LA1XSRXMNO3:2||CONSTANTS:2||polaron:2||charge ordering:2||SCATTERING:2||XRAY PHOTOEMISSION:2||CeNiSn:2||phase diagram:2||PHOTOELECTRON:2||QUADRUPOLAR:2||perovskitemanganites:2||CO:2||SYSTEMS:2||DOPED ZNO:2||LOWFREQUENCY SOUND:2||LA:2||ELECTRONELECTRON SCATTERING:2||AU:2||DENSITYWAVE INSTABILITY:2||FERMISURFACE:2||hybridization:2||VALENCEBAND SATELLITE:2||SULFUR SPINEL:2||Heusler:2||APPROXIMATION:2||superexchange:2||colossal magnetoresistance:2||ALLOYS:2||DEPENDENCE:2||AG:2||electronic structures:2||AUGERSPECTRA:2||CR:2||PARAMETERS:2||DIFFRACTION:2||SEMICONDUCTORMETAL TRANSITION:1||INTERMEDIATEVALENCE:1||SMB6:1||SRRUO3:1||antiperovskite structure with antipolar nature:1||lowenergy twodimensional phonons:1||anatase TiO2:1||La3S4:1||metalinsulator transitions:1||MNO:1||ELECTRONICSTRUCTURES:1||MAGNETIC CIRCULARDICHROISM:1||Density functional theory:1||CeCo2:1||TOPOLARON CROSSOVER:1||EXCHANGE:1||cuprates:1||high Tc cuprates:1||magnetically ordered materials:1||ZNSE:1||Sr2xKxFeMoO6:1||CDW:1||TeCuO3:1||STRUCTURALPROPERTIES:1||MN:1||screening length:1||amorphous Fe:1||WAVE BASISSET:1||SILICONCARBIDE:1||HIGHPRESSURE:1||electronphonon coupling:1||quenched superconductivity:1||CMR perovskite manganites:1||OXIDE:1||polarons:1||synchrotron radiation:1||FULLERIDES:1||RESONANTPHOTOEMISSION:1||Silicon carbide:1||DFT calculation:1||Hybridized bands:1||GIANT MAGNETORESISTANCE:1||PEROVSKITES:1||Raman spectra:1||EXCHANGE ENHANCEMENT:1||SILICON:1||SR2FEMOO6:1||orbital ordering:1||delafossite:1||TITANIUMDIOXIDE:1||electronic structure of disordered solids:1||YFE2:1||Magnetic polaron:1||NA2TI2SB2O:1||STRONGCOUPLED SUPERCONDUCTORS:1||HEAVYFERMION SYSTEMS:1||firstprinciples calculations:1||MECHANISM:1||UNiSn:1||PHOTONIC BANDGAP:1||SINGLE IMPURITY:1||PHONONSPECTRUM:1||FERMISURFACE TOPOLOGY:1||SUPPRESSION:1||RESONANT PHOTOEMISSION:1||METALDOPED PICENE:1||PHOTOIONIZATION CROSSSECTIONS:1||PHOTOINDUCED FERRIMAGNETIC SYSTEMS:1||LINKAGE ISOMERISM:1||CHARGETRANSFER:1||Bilayer Graphene:1||MAGNETICFIELD:1||SPINWAVES:1||rareearth manganese oxides:1||magnonphonon interaction:1||NACO2O4:1||ENERGYBANDS:1||SELFENERGY:1||GAS:1||Fe0.5Cu0.5Cr2S4:1||scanning photoelectron microscopy (SPEM):1||MAGNETIC PROPERTIES:1||Stoner model:1||AMORPHOUS TRANSITIONMETALS:1||SPINGLASS STATES:1||NI:1||LA3NI2B2N3:1||SOLIDS:1||CEO2:1||BAND THEORY:1||dilute magnetic semiconductor:1||pyrochlore:1||Y1XPRXBA2CU3O7DELTA:1||and electronphonon interactions:1||VIBRATIONS:1||RAY PHOTOEMISSION:1||ALKALI CATION:1||Europium:1||colossal magnetoresistance:1||structural stability:1||ENERGYGAP:1||small polaron:1||DOUBLE EXCHANGE:1||Coulomb correlation:1||magnon:1||phonons:1||ELECTRON FERROMAGNETISM:1||CURIETEMPERATURE:1||ARPES:1||PLANEWAVE METHOD:1||Xray absorption spectroscopy (XAS):1||ROOMTEMPERATURE:1||MONOCHALCOGENIDES:1||HEAT:1||UPDSN:1||MOMENTS:1||XRAY ABSORPTION:1||SEMICONDUCTOR:1||Fermi surface nesting:1||optical phonon:1||disordered system:1||dilute magnetic semiconductors:1||CMR manganites:1||PHONONS:1||LATTICEDYNAMICS:1||OXIDES:1||4fphotoemission:1||permanent magnet:1||pseudogap:1||TRANSPORTPROPERTIES:1||ANTIFERROMAGNET:1||(BI,PB)SRCOO SYSTEM:1||semicore correlation:1||POLARIZATION:1||CRYSTAL:1||spinel:1||Xray magnetic circular dichroism (XMCD):1||magnetocapacitance:1||ANATASE:1||TEMPERATURES:1||Pseudogap:1||INTERFACE:1||SUBSTRATE:1||YNI2B2C:1||SAMARIUM SULFIDE:1||strong swave superconductor:1||DOPED MANGANITE:1||SYMMETRY:1||CENISN:1||resonance mode:1||DISORDERED SYSTEM:1||LITHIUM INTERCALATION:1||CUO2 PLANE:1||SURFACE:1||Delafossite:1||ELECTRICALPROPERTIES:1||NIMNSB:1||PTMNSB:1||ROOMTEMPERATURE FERROMAGNETISM:1||RUBIDIUM MANGANESE HEXACYANOFERRATE:1||COLOSSALMAGNETORESISTANCE:1||FINITE TEMPERATURES:1||LAMNO3:1||FE:1||transitionmetal oxides:1||giant magnetoresistance:1||phonon:1||COPPER OXIDES:1||valence states:1||thermoelectric:1||semiconductor:1||CATION DISTRIBUTION:1||FeCr2S4:1||photoemission spectroscopy (PES):1||METALLIC FERROMAGNETISM:1||GRAPHITE:1||SUSCEPTIBILITY:1||UBE13:1||RCrSb3:1||band JahnTeller:1||Ce3S4:1||TiO2:1||PrBa2Cu3O7delta:1||UNTWINNED PRBA2CU3O7:1||AGNIO2:1||HALFMETALLIC FERROMAGNETS:1||CI:1||Energy gap:1||Photoemission:1||Future applications:1||Photoemission measurements:1||Graphene:1||BANDSTRUCTURE:1||TC:1||superconductivity:1||magnetic semiconductors:1||CMRmanganites:1||thin films:1||spin dynamics:1||highTc superconductors:1||ITINERANTELECTRON FERROMAGNETISM:1||SINGLECRYSTALS:1||CeTe2:1||amorphous magnetic materials:1||EPITAXIAL GRAPHENE:1||LAYERED PNICTIDEOXIDES:1||BOROCARBIDE SUPERCONDUCTORS:1||AUGMENTEDWAVE METHOD:1||METALLIC MAGNET UNISN:1||ORIGIN:1||spectrum rearrangement:1||MEANFIELD THEORY:1||MOLECULEBASED MAGNETS:1||METASTABLE STATE:1||INSULATOR:1||magnetic orderin:1||FCC IRON:1||CeRu2:1||TL2MN2O7:1||isotope effect:1||Perovskitemanganites:1||RECURSION METHOD:1||PERPENDICULAR MAGNETICANISOTROPY:1||quasiparticle spectral density:1||GW:1||MANGANESE FERRITE:1||RESONANCE:1||SeCuO3:1||Optical conductivity:1||MASSLESS DIRAC FERMIONS:1||SCHOTTKYBARRIER:1||electronic structure:15||ELECTRONICSTRUCTURE:11||TRANSITIONMETAL COMPOUNDS:10||METALS:10||photoemission:8||SPECTRA:8||MAGNETORESISTANCE:7||FERROMAGNETISM:7||TRANSPORT:7||TRANSITION:6||FILMS:6||THINFILMS:5||TOTALENERGY CALCULATIONS:5||MAGNETICPROPERTIES:5||SUPERCONDUCTIVITY:5||PR:5||LATTICE:4||STATES:4||SPECTROSCOPY:4||FIELD:4||CRYSTALSTRUCTURE:4||PHOTOEMISSION:4||TEMPERATURE:4||TRANSITIONTEMPERATURE:4||XRAYABSORPTION:4||STATE:4||CU:4||BASISSET:4||XAS:4||CRYSTALS:3||EXCITATIONS:3||MOTTHUBBARD SYSTEMS:3||HIGHENERGY SPIN:3||halfmetal:3||INSULATORS:3||LA2CUO4:3||MODEL:3||FLUCTUATIONS:3||CE:3||double exchange:3||TRANSITIONMETALS:3||RESISTIVITY:3||BORON:3||LA1XCAXMNO3:3||IRON:3||PES:3||ANTIMONIDES:2||MgB2:2||ZR METALLIC GLASSES:2||superconductor:2||CRITICALCURRENT DENSITY:2||CIRCULARDICHROISM:2||SEMICONDUCTORS:2||LOCALIZATION:2||INTRABAND OPTICAL CONDUCTIVITY:2||COLOSSAL MAGNETORESISTANCE:2||OXIDATION:2||EXISTENCE:2||COPPER:2||diboride:2||MAGNESIUMDIBORIDE:2||GAP:2||CE COMPOUNDS:2||CORE POLARIZATION:2||magnetoresistance:2||photoemission spectroscopy:2||electronphonon interaction:2||GETTER:2||PD:2||MAGNETISM:2||FECR2S4:2||SUPERCONDUCTING MGB2:2||WIRES:2||ABSORPTION:2||ENERGY:2||LA1XSRXMNO3:2||CONSTANTS:2||polaron:2||charge ordering:2||SCATTERING:2||XRAY PHOTOEMISSION:2||CeNiSn:2||phase diagram:2||PHOTOELECTRON:2||QUADRUPOLAR:2||perovskitemanganites:2||CO:2||SYSTEMS:2||DOPED ZNO:2||LOWFREQUENCY SOUND:2||LA:2||ELECTRONELECTRON SCATTERING:2||AU:2||DENSITYWAVE INSTABILITY:2||FERMISURFACE:2||hybridization:2||VALENCEBAND SATELLITE:2||SULFUR SPINEL:2||Heusler:2||APPROXIMATION:2||superexchange:2||colossal magnetoresistance:2||ALLOYS:2||DEPENDENCE:2||AG:2||electronic structures:2||AUGERSPECTRA:2||CR:2||PARAMETERS:2||DIFFRACTION:2||SEMICONDUCTORMETAL TRANSITION:1||INTERMEDIATEVALENCE:1||SMB6:1||SRRUO3:1||antiperovskite structure with antipolar nature:1||lowenergy twodimensional phonons:1||anatase TiO2:1||La3S4:1||metalinsulator transitions:1||MNO:1||ELECTRONICSTRUCTURES:1||MAGNETIC CIRCULARDICHROISM:1||Density functional theory:1||CeCo2:1||TOPOLARON CROSSOVER:1||EXCHANGE:1||cuprates:1||high Tc cuprates:1||magnetically ordered materials:1||ZNSE:1||Sr2xKxFeMoO6:1||CDW:1||TeCuO3:1||STRUCTURALPROPERTIES:1||MN:1||screening length:1||amorphous Fe:1||WAVE BASISSET:1||SILICONCARBIDE:1||HIGHPRESSURE:1||electronphonon coupling:1||quenched superconductivity:1||CMR perovskite manganites:1||OXIDE:1||polarons:1||synchrotron radiation:1||FULLERIDES:1||RESONANTPHOTOEMISSION:1||Silicon carbide:1||DFT calculation:1||Hybridized bands:1||GIANT MAGNETORESISTANCE:1||PEROVSKITES:1||Raman spectra:1||EXCHANGE ENHANCEMENT:1||SILICON:1||SR2FEMOO6:1||orbital ordering:1||delafossite:1||TITANIUMDIOXIDE:1||electronic structure of disordered solids:1||YFE2:1||Magnetic polaron:1||NA2TI2SB2O:1||STRONGCOUPLED SUPERCONDUCTORS:1||HEAVYFERMION SYSTEMS:1||firstprinciples calculations:1||MECHANISM:1||UNiSn:1||PHOTONIC BANDGAP:1||SINGLE IMPURITY:1||PHONONSPECTRUM:1||FERMISURFACE TOPOLOGY:1||SUPPRESSION:1||RESONANT PHOTOEMISSION:1||METALDOPED PICENE:1||PHOTOIONIZATION CROSSSECTIONS:1||PHOTOINDUCED FERRIMAGNETIC SYSTEMS:1||LINKAGE ISOMERISM:1||CHARGETRANSFER:1||Bilayer Graphene:1||MAGNETICFIELD:1||SPINWAVES:1||rareearth manganese oxides:1||magnonphonon interaction:1||NACO2O4:1||ENERGYBANDS:1||SELFENERGY:1||GAS:1||Fe0.5Cu0.5Cr2S4:1||scanning photoelectron microscopy (SPEM):1||MAGNETIC PROPERTIES:1||Stoner model:1||AMORPHOUS TRANSITIONMETALS:1||SPINGLASS STATES:1||NI:1||LA3NI2B2N3:1||SOLIDS:1||CEO2:1||BAND THEORY:1||dilute magnetic semiconductor:1||pyrochlore:1||Y1XPRXBA2CU3O7DELTA:1||and electronphonon interactions:1||VIBRATIONS:1||RAY PHOTOEMISSION:1||ALKALI CATION:1||Europium:1||colossal magnetoresistance:1||structural stability:1||ENERGYGAP:1||small polaron:1||DOUBLE EXCHANGE:1||Coulomb correlation:1||magnon:1||phonons:1||ELECTRON FERROMAGNETISM:1||CURIETEMPERATURE:1||ARPES:1||PLANEWAVE METHOD:1||Xray absorption spectroscopy (XAS):1||ROOMTEMPERATURE:1||MONOCHALCOGENIDES:1||HEAT:1||UPDSN:1||MOMENTS:1||XRAY ABSORPTION:1||SEMICONDUCTOR:1||Fermi surface nesting:1||optical phonon:1||disordered system:1||dilute magnetic semiconductors:1||CMR manganites:1||PHONONS:1||LATTICEDYNAMICS:1||OXIDES:1||4fphotoemission:1||permanent magnet:1||pseudogap:1||TRANSPORTPROPERTIES:1||ANTIFERROMAGNET:1||(BI,PB)SRCOO SYSTEM:1||semicore correlation:1||POLARIZATION:1||CRYSTAL:1||spinel:1||Xray magnetic circular dichroism (XMCD):1||magnetocapacitance:1||ANATASE:1||TEMPERATURES:1||Pseudogap:1||INTERFACE:1||SUBSTRATE:1||YNI2B2C:1||SAMARIUM SULFIDE:1||strong swave superconductor:1||DOPED MANGANITE:1||SYMMETRY:1||CENISN:1||resonance mode:1||DISORDERED SYSTEM:1||LITHIUM INTERCALATION:1||CUO2 PLANE:1||SURFACE:1||Delafossite:1||ELECTRICALPROPERTIES:1||NIMNSB:1||PTMNSB:1||ROOMTEMPERATURE FERROMAGNETISM:1||RUBIDIUM MANGANESE HEXACYANOFERRATE:1||COLOSSALMAGNETORESISTANCE:1||FINITE TEMPERATURES:1||LAMNO3:1||FE:1||transitionmetal oxides:1||giant magnetoresistance:1||phonon:1||COPPER OXIDES:1||valence states:1||thermoelectric:1||semiconductor:1||CATION DISTRIBUTION:1||FeCr2S4:1||photoemission spectroscopy (PES):1||METALLIC FERROMAGNETISM:1||GRAPHITE:1||SUSCEPTIBILITY:1||UBE13:1||RCrSb3:1||band JahnTeller:1||Ce3S4:1||TiO2:1||PrBa2Cu3O7delta:1||UNTWINNED PRBA2CU3O7:1||AGNIO2:1||HALFMETALLIC FERROMAGNETS:1||CI:1||Energy gap:1||Photoemission:1||Future applications:1||Photoemission measurements:1||Graphene:1||BANDSTRUCTURE:1||TC:1||superconductivity:1||magnetic semiconductors:1||CMRmanganites:1||thin films:1||spin dynamics:1||highTc superconductors:1||ITINERANTELECTRON FERROMAGNETISM:1||SINGLECRYSTALS:1||CeTe2:1||amorphous magnetic materials:1||EPITAXIAL GRAPHENE:1||LAYERED PNICTIDEOXIDES:1||BOROCARBIDE SUPERCONDUCTORS:1||AUGMENTEDWAVE METHOD:1||METALLIC MAGNET UNISN:1||ORIGIN:1||spectrum rearrangement:1||MEANFIELD THEORY:1||MOLECULEBASED MAGNETS:1||METASTABLE STATE:1||INSULATOR:1||magnetic orderin:1||FCC IRON:1||CeRu2:1||TL2MN2O7:1||isotope effect:1||Perovskitemanganites:1||RECURSION METHOD:1||PERPENDICULAR MAGNETICANISOTROPY:1||quasiparticle spectral density:1||GW:1||MANGANESE FERRITE:1||RESONANCE:1||SeCuO3:1||Optical conductivity:1||MASSLESS DIRAC FERMIONS:1||SCHOTTKYBARRIER:1||electronic structure:15||ELECTRONICSTRUCTURE:11||TRANSITIONMETAL COMPOUNDS:10||METALS:10||photoemission:8||SPECTRA:8||MAGNETORESISTANCE:7||FERROMAGNETISM:7||TRANSPORT:7||TRANSITION:6||FILMS:6||THINFILMS:5||TOTALENERGY CALCULATIONS:5||MAGNETICPROPERTIES:5||SUPERCONDUCTIVITY:5||PR:5||LATTICE:4||STATES:4||SPECTROSCOPY:4||FIELD:4||CRYSTALSTRUCTURE:4||PHOTOEMISSION:4||TEMPERATURE:4||TRANSITIONTEMPERATURE:4||XRAYABSORPTION:4||STATE:4||CU:4||BASISSET:4||XAS:4||CRYSTALS:3||EXCITATIONS:3||MOTTHUBBARD SYSTEMS:3||HIGHENERGY SPIN:3||halfmetal:3||INSULATORS:3||LA2CUO4:3||MODEL:3||FLUCTUATIONS:3||CE:3||double exchange:3||TRANSITIONMETALS:3||RESISTIVITY:3||BORON:3||LA1XCAXMNO3:3||IRON:3||PES:3||ANTIMONIDES:2||MgB2:2||ZR METALLIC GLASSES:2||superconductor:2||CRITICALCURRENT DENSITY:2||CIRCULARDICHROISM:2||SEMICONDUCTORS:2||LOCALIZATION:2||INTRABAND OPTICAL CONDUCTIVITY:2||COLOSSAL MAGNETORESISTANCE:2||OXIDATION:2||EXISTENCE:2||COPPER:2||diboride:2||MAGNESIUMDIBORIDE:2||GAP:2||CE COMPOUNDS:2||CORE POLARIZATION:2||magnetoresistance:2||photoemission spectroscopy:2||electronphonon interaction:2||GETTER:2||PD:2||MAGNETISM:2||FECR2S4:2||SUPERCONDUCTING MGB2:2||WIRES:2||ABSORPTION:2||ENERGY:2||LA1XSRXMNO3:2||CONSTANTS:2||polaron:2||charge ordering:2||SCATTERING:2||XRAY PHOTOEMISSION:2||CeNiSn:2||phase diagram:2||PHOTOELECTRON:2||QUADRUPOLAR:2||perovskitemanganites:2||CO:2||SYSTEMS:2||DOPED ZNO:2||LOWFREQUENCY SOUND:2||LA:2||ELECTRONELECTRON SCATTERING:2||AU:2||DENSITYWAVE INSTABILITY:2||FERMISURFACE:2||hybridization:2||VALENCEBAND SATELLITE:2||SULFUR SPINEL:2||Heusler:2||APPROXIMATION:2||superexchange:2||colossal magnetoresistance:2||ALLOYS:2||DEPENDENCE:2||AG:2||electronic structures:2||AUGERSPECTRA:2||CR:2||PARAMETERS:2||DIFFRACTION:2||SEMICONDUCTORMETAL TRANSITION:1||INTERMEDIATEVALENCE:1||SMB6:1||SRRUO3:1||antiperovskite structure with antipolar nature:1||lowenergy twodimensional phonons:1||anatase TiO2:1||La3S4:1||metalinsulator transitions:1||MNO:1||ELECTRONICSTRUCTURES:1||MAGNETIC CIRCULARDICHROISM:1||Density functional theory:1||CeCo2:1||TOPOLARON CROSSOVER:1||EXCHANGE:1||cuprates:1||high Tc cuprates:1||magnetically ordered materials:1||ZNSE:1||Sr2xKxFeMoO6:1||CDW:1||TeCuO3:1||STRUCTURALPROPERTIES:1||MN:1||screening length:1||amorphous Fe:1||WAVE BASISSET:1||SILICONCARBIDE:1||HIGHPRESSURE:1||electronphonon coupling:1||quenched superconductivity:1||CMR perovskite manganites:1||OXIDE:1||polarons:1||synchrotron radiation:1||FULLERIDES:1||RESONANTPHOTOEMISSION:1||Silicon carbide:1||DFT calculation:1||Hybridized bands:1||GIANT MAGNETORESISTANCE:1||PEROVSKITES:1||Raman spectra:1||EXCHANGE ENHANCEMENT:1||SILICON:1||SR2FEMOO6:1||orbital ordering:1||delafossite:1||TITANIUMDIOXIDE:1||electronic structure of disordered solids:1||YFE2:1||Magnetic polaron:1||NA2TI2SB2O:1||STRONGCOUPLED SUPERCONDUCTORS:1||HEAVYFERMION SYSTEMS:1||firstprinciples calculations:1||MECHANISM:1||UNiSn:1||PHOTONIC BANDGAP:1||SINGLE IMPURITY:1||PHONONSPECTRUM:1||FERMISURFACE TOPOLOGY:1||SUPPRESSION:1||RESONANT PHOTOEMISSION:1||METALDOPED PICENE:1||PHOTOIONIZATION CROSSSECTIONS:1||PHOTOINDUCED FERRIMAGNETIC SYSTEMS:1||LINKAGE ISOMERISM:1||CHARGETRANSFER:1||Bilayer Graphene:1||MAGNETICFIELD:1||SPINWAVES:1||rareearth manganese oxides:1||magnonphonon interaction:1||NACO2O4:1||ENERGYBANDS:1||SELFENERGY:1||GAS:1||Fe0.5Cu0.5Cr2S4:1||scanning photoelectron microscopy (SPEM):1||MAGNETIC PROPERTIES:1||Stoner model:1||AMORPHOUS TRANSITIONMETALS:1||SPINGLASS STATES:1||NI:1||LA3NI2B2N3:1||SOLIDS:1||CEO2:1||BAND THEORY:1||dilute magnetic semiconductor:1||pyrochlore:1||Y1XPRXBA2CU3O7DELTA:1||and electronphonon interactions:1||VIBRATIONS:1||RAY PHOTOEMISSION:1||ALKALI CATION:1||Europium:1||colossal magnetoresistance:1||structural stability:1||ENERGYGAP:1||small polaron:1||DOUBLE EXCHANGE:1||Coulomb correlation:1||magnon:1||phonons:1||ELECTRON FERROMAGNETISM:1||CURIETEMPERATURE:1||ARPES:1||PLANEWAVE METHOD:1||Xray absorption spectroscopy (XAS):1||ROOMTEMPERATURE:1||MONOCHALCOGENIDES:1||HEAT:1||UPDSN:1||MOMENTS:1||XRAY ABSORPTION:1||SEMICONDUCTOR:1||Fermi surface nesting:1||optical phonon:1||disordered system:1||dilute magnetic semiconductors:1||CMR manganites:1||PHONONS:1||LATTICEDYNAMICS:1||OXIDES:1||4fphotoemission:1||permanent magnet:1||pseudogap:1||TRANSPORTPROPERTIES:1||ANTIFERROMAGNET:1||(BI,PB)SRCOO SYSTEM:1||semicore correlation:1||POLARIZATION:1||CRYSTAL:1||spinel:1||Xray magnetic circular dichroism (XMCD):1||magnetocapacitance:1||ANATASE:1||TEMPERATURES:1||Pseudogap:1||INTERFACE:1||SUBSTRATE:1||YNI2B2C:1||SAMARIUM SULFIDE:1||strong swave superconductor:1||DOPED MANGANITE:1||SYMMETRY:1||CENISN:1||resonance mode:1||DISORDERED SYSTEM:1||LITHIUM INTERCALATION:1||CUO2 PLANE:1||SURFACE:1||Delafossite:1||ELECTRICALPROPERTIES:1||NIMNSB:1||PTMNSB:1||ROOMTEMPERATURE FERROMAGNETISM:1||RUBIDIUM MANGANESE HEXACYANOFERRATE:1||COLOSSALMAGNETORESISTANCE:1||FINITE TEMPERATURES:1||LAMNO3:1||FE:1||transitionmetal oxides:1||giant magnetoresistance:1||phonon:1||COPPER OXIDES:1||valence states:1||thermoelectric:1||semiconductor:1||CATION DISTRIBUTION:1||FeCr2S4:1||photoemission spectroscopy (PES):1||METALLIC FERROMAGNETISM:1||GRAPHITE:1||SUSCEPTIBILITY:1||UBE13:1||RCrSb3:1||band JahnTeller:1||Ce3S4:1||TiO2:1||PrBa2Cu3O7delta:1||UNTWINNED PRBA2CU3O7:1||AGNIO2:1||HALFMETALLIC FERROMAGNETS:1||CI:1||Energy gap:1||Photoemission:1||Future applications:1||Photoemission measurements:1||Graphene:1||BANDSTRUCTURE:1||TC:1||superconductivity:1||magnetic semiconductors:1||CMRmanganites:1||thin films:1||spin dynamics:1||highTc superconductors:1||ITINERANTELECTRON FERROMAGNETISM:1||SINGLECRYSTALS:1||CeTe2:1||amorphous magnetic materials:1||EPITAXIAL GRAPHENE:1||LAYERED PNICTIDEOXIDES:1||BOROCARBIDE SUPERCONDUCTORS:1||AUGMENTEDWAVE METHOD:1||METALLIC MAGNET UNISN:1||ORIGIN:1||spectrum rearrangement:1||MEANFIELD THEORY:1||MOLECULEBASED MAGNETS:1||METASTABLE STATE:1||INSULATOR:1||magnetic orderin:1||FCC IRON:1||CeRu2:1||TL2MN2O7:1||isotope effect:1||Perovskitemanganites:1||RECURSION METHOD:1||PERPENDICULAR MAGNETICANISOTROPY:1||quasiparticle spectral density:1||GW:1||MANGANESE FERRITE:1||RESONANCE:1||SeCuO3:1||Optical conductivity:1||MASSLESS DIRAC FERMIONS:1||SCHOTTKYBARRIER:1||electronic structure:15||ELECTRONICSTRUCTURE:11||TRANSITIONMETAL COMPOUNDS:10||METALS:10||photoemission:8||SPECTRA:8||MAGNETORESISTANCE:7||FERROMAGNETISM:7||TRANSPORT:7||TRANSITION:6||FILMS:6||THINFILMS:5||TOTALENERGY CALCULATIONS:5||MAGNETICPROPERTIES:5||SUPERCONDUCTIVITY:5||PR:5||LATTICE:4||STATES:4||SPECTROSCOPY:4||FIELD:4||CRYSTALSTRUCTURE:4||PHOTOEMISSION:4||TEMPERATURE:4||TRANSITIONTEMPERATURE:4||XRAYABSORPTION:4||STATE:4||CU:4||BASISSET:4||XAS:4||CRYSTALS:3||EXCITATIONS:3||MOTTHUBBARD SYSTEMS:3||HIGHENERGY SPIN:3||halfmetal:3||INSULATORS:3||LA2CUO4:3||MODEL:3||FLUCTUATIONS:3||CE:3||double exchange:3||TRANSITIONMETALS:3||RESISTIVITY:3||BORON:3||LA1XCAXMNO3:3||IRON:3||PES:3||ANTIMONIDES:2||MgB2:2||ZR METALLIC GLASSES:2||superconductor:2||CRITICALCURRENT DENSITY:2||CIRCULARDICHROISM:2||SEMICONDUCTORS:2||LOCALIZATION:2||INTRABAND OPTICAL CONDUCTIVITY:2||COLOSSAL MAGNETORESISTANCE:2||OXIDATION:2||EXISTENCE:2||COPPER:2||diboride:2||MAGNESIUMDIBORIDE:2||GAP:2||CE COMPOUNDS:2||CORE POLARIZATION:2||magnetoresistance:2||photoemission spectroscopy:2||electronphonon interaction:2||GETTER:2||PD:2||MAGNETISM:2||FECR2S4:2||SUPERCONDUCTING MGB2:2||WIRES:2||ABSORPTION:2||ENERGY:2||LA1XSRXMNO3:2||CONSTANTS:2||polaron:2||charge ordering:2||SCATTERING:2||XRAY PHOTOEMISSION:2||CeNiSn:2||phase diagram:2||PHOTOELECTRON:2||QUADRUPOLAR:2||perovskitemanganites:2||CO:2||SYSTEMS:2||DOPED ZNO:2||LOWFREQUENCY SOUND:2||LA:2||ELECTRONELECTRON SCATTERING:2||AU:2||DENSITYWAVE INSTABILITY:2||FERMISURFACE:2||hybridization:2||VALENCEBAND SATELLITE:2||SULFUR SPINEL:2||Heusler:2||APPROXIMATION:2||superexchange:2||colossal magnetoresistance:2||ALLOYS:2||DEPENDENCE:2||AG:2||electronic structures:2||AUGERSPECTRA:2||CR:2||PARAMETERS:2||DIFFRACTION:2||SEMICONDUCTORMETAL TRANSITION:1||INTERMEDIATEVALENCE:1||SMB6:1||SRRUO3:1||antiperovskite structure with antipolar nature:1||lowenergy twodimensional phonons:1||anatase TiO2:1||La3S4:1||metalinsulator transitions:1||MNO:1||ELECTRONICSTRUCTURES:1||MAGNETIC CIRCULARDICHROISM:1||Density functional theory:1||CeCo2:1||TOPOLARON CROSSOVER:1||EXCHANGE:1||cuprates:1||high Tc cuprates:1||magnetically ordered materials:1||ZNSE:1||Sr2xKxFeMoO6:1||CDW:1||TeCuO3:1||STRUCTURALPROPERTIES:1||MN:1||screening length:1||amorphous Fe:1||WAVE BASISSET:1||SILICONCARBIDE:1||HIGHPRESSURE:1||electronphonon coupling:1||quenched superconductivity:1||CMR perovskite manganites:1||OXIDE:1||polarons:1||synchrotron radiation:1||FULLERIDES:1||RESONANTPHOTOEMISSION:1||Silicon carbide:1||DFT calculation:1||Hybridized bands:1||GIANT MAGNETORESISTANCE:1||PEROVSKITES:1||Raman spectra:1||EXCHANGE ENHANCEMENT:1||SILICON:1||SR2FEMOO6:1||orbital ordering:1||delafossite:1||TITANIUMDIOXIDE:1||electronic structure of disordered solids:1||YFE2:1||Magnetic polaron:1||NA2TI2SB2O:1||STRONGCOUPLED SUPERCONDUCTORS:1||HEAVYFERMION SYSTEMS:1||firstprinciples calculations:1||MECHANISM:1||UNiSn:1||PHOTONIC BANDGAP:1||SINGLE IMPURITY:1||PHONONSPECTRUM:1||FERMISURFACE TOPOLOGY:1||SUPPRESSION:1||RESONANT PHOTOEMISSION:1||METALDOPED PICENE:1||PHOTOIONIZATION CROSSSECTIONS:1||PHOTOINDUCED FERRIMAGNETIC SYSTEMS:1||LINKAGE ISOMERISM:1||CHARGETRANSFER:1||Bilayer Graphene:1||MAGNETICFIELD:1||SPINWAVES:1||rareearth manganese oxides:1||magnonphonon interaction:1||NACO2O4:1||ENERGYBANDS:1||SELFENERGY:1||GAS:1||Fe0.5Cu0.5Cr2S4:1||scanning photoelectron microscopy (SPEM):1||MAGNETIC PROPERTIES:1||Stoner model:1||AMORPHOUS TRANSITIONMETALS:1||SPINGLASS STATES:1||NI:1||LA3NI2B2N3:1||SOLIDS:1||CEO2:1||BAND THEORY:1||dilute magnetic semiconductor:1||pyrochlore:1||Y1XPRXBA2CU3O7DELTA:1||and electronphonon interactions:1||VIBRATIONS:1||RAY PHOTOEMISSION:1||ALKALI CATION:1||Europium:1||colossal magnetoresistance:1||structural stability:1||ENERGYGAP:1||small polaron:1||DOUBLE EXCHANGE:1||Coulomb correlation:1||magnon:1||phonons:1||ELECTRON FERROMAGNETISM:1||CURIETEMPERATURE:1||ARPES:1||PLANEWAVE METHOD:1||Xray absorption spectroscopy (XAS):1||ROOMTEMPERATURE:1||MONOCHALCOGENIDES:1||HEAT:1||UPDSN:1||MOMENTS:1||XRAY ABSORPTION:1||SEMICONDUCTOR:1||Fermi surface nesting:1||optical phonon:1||disordered system:1||dilute magnetic semiconductors:1||CMR manganites:1||PHONONS:1||LATTICEDYNAMICS:1||OXIDES:1||4fphotoemission:1||permanent magnet:1||pseudogap:1||TRANSPORTPROPERTIES:1||ANTIFERROMAGNET:1||(BI,PB)SRCOO SYSTEM:1||semicore correlation:1||POLARIZATION:1||CRYSTAL:1||spinel:1||Xray magnetic circular dichroism (XMCD):1||magnetocapacitance:1||ANATASE:1||TEMPERATURES:1||Pseudogap:1||INTERFACE:1||SUBSTRATE:1||YNI2B2C:1||SAMARIUM SULFIDE:1||strong swave superconductor:1||DOPED MANGANITE:1||SYMMETRY:1||CENISN:1||resonance mode:1||DISORDERED SYSTEM:1||LITHIUM INTERCALATION:1||CUO2 PLANE:1||SURFACE:1||Delafossite:1||ELECTRICALPROPERTIES:1||NIMNSB:1||PTMNSB:1||ROOMTEMPERATURE FERROMAGNETISM:1||RUBIDIUM MANGANESE HEXACYANOFERRATE:1||COLOSSALMAGNETORESISTANCE:1||FINITE TEMPERATURES:1||LAMNO3:1||FE:1||transitionmetal oxides:1||giant magnetoresistance:1||phonon:1||COPPER OXIDES:1||valence states:1||thermoelectric:1||semiconductor:1||CATION DISTRIBUTION:1||FeCr2S4:1||photoemission spectroscopy (PES):1||METALLIC FERROMAGNETISM:1||GRAPHITE:1||SUSCEPTIBILITY:1||UBE13:1||RCrSb3:1||band JahnTeller:1||Ce3S4:1||TiO2:1||PrBa2Cu3O7delta:1||UNTWINNED PRBA2CU3O7:1||AGNIO2:1||HALFMETALLIC FERROMAGNETS:1||CI:1||Energy gap:1||Photoemission:1||Future applications:1||Photoemission measurements:1||Graphene:1||BANDSTRUCTURE:1||TC:1||superconductivity:1||magnetic semiconductors:1||CMRmanganites:1||thin films:1||spin dynamics:1||highTc superconductors:1||ITINERANTELECTRON FERROMAGNETISM:1||SINGLECRYSTALS:1||CeTe2:1||amorphous magnetic materials:1||EPITAXIAL GRAPHENE:1||LAYERED PNICTIDEOXIDES:1||BOROCARBIDE SUPERCONDUCTORS:1||AUGMENTEDWAVE METHOD:1||METALLIC MAGNET UNISN:1||ORIGIN:1||spectrum rearrangement:1||MEANFIELD THEORY:1||MOLECULEBASED MAGNETS:1||METASTABLE STATE:1||INSULATOR:1||magnetic orderin:1||FCC IRON:1||CeRu2:1||TL2MN2O7:1||isotope effect:1||Perovskitemanganites:1||RECURSION METHOD:1||PERPENDICULAR MAGNETICANISOTROPY:1||quasiparticle spectral density:1||GW:1||MANGANESE FERRITE:1||RESONANCE:1||SeCuO3:1||Optical conductivity:1||MASSLESS DIRAC FERMIONS:1||SCHOTTKYBARRIER:1||electronic structure:15||ELECTRONICSTRUCTURE:11||TRANSITIONMETAL COMPOUNDS:10||METALS:10||photoemission:8||SPECTRA:8||MAGNETORESISTANCE:7||FERROMAGNETISM:7||TRANSPORT:7||TRANSITION:6||FILMS:6||THINFILMS:5||TOTALENERGY CALCULATIONS:5||MAGNETICPROPERTIES:5||SUPERCONDUCTIVITY:5||PR:5||LATTICE:4||STATES:4||SPECTROSCOPY:4||FIELD:4||CRYSTALSTRUCTURE:4||PHOTOEMISSION:4||TEMPERATURE:4||TRANSITIONTEMPERATURE:4||XRAYABSORPTION:4||STATE:4||CU:4||BASISSET:4||XAS:4||CRYSTALS:3||EXCITATIONS:3||MOTTHUBBARD SYSTEMS:3||HIGHENERGY SPIN:3||halfmetal:3||INSULATORS:3||LA2CUO4:3||MODEL:3||FLUCTUATIONS:3||CE:3||double exchange:3||TRANSITIONMETALS:3||RESISTIVITY:3||BORON:3||LA1XCAXMNO3:3||IRON:3||PES:3||ANTIMONIDES:2||MgB2:2||ZR METALLIC GLASSES:2||superconductor:2||CRITICALCURRENT DENSITY:2||CIRCULARDICHROISM:2||SEMICONDUCTORS:2||LOCALIZATION:2||INTRABAND OPTICAL CONDUCTIVITY:2||COLOSSAL MAGNETORESISTANCE:2||OXIDATION:2||EXISTENCE:2||COPPER:2||diboride:2||MAGNESIUMDIBORIDE:2||GAP:2||CE COMPOUNDS:2||CORE POLARIZATION:2||magnetoresistance:2||photoemission spectroscopy:2||electronphonon interaction:2||GETTER:2||PD:2||MAGNETISM:2||FECR2S4:2||SUPERCONDUCTING MGB2:2||WIRES:2||ABSORPTION:2||ENERGY:2||LA1XSRXMNO3:2||CONSTANTS:2||polaron:2||charge ordering:2||SCATTERING:2||XRAY PHOTOEMISSION:2||CeNiSn:2||phase diagram:2||PHOTOELECTRON:2||QUADRUPOLAR:2||perovskitemanganites:2||CO:2||SYSTEMS:2||DOPED ZNO:2||LOWFREQUENCY SOUND:2||LA:2||ELECTRONELECTRON SCATTERING:2||AU:2||DENSITYWAVE INSTABILITY:2||FERMISURFACE:2||hybridization:2||VALENCEBAND SATELLITE:2||SULFUR SPINEL:2||Heusler:2||APPROXIMATION:2||superexchange:2||colossal magnetoresistance:2||ALLOYS:2||DEPENDENCE:2||AG:2||electronic structures:2||AUGERSPECTRA:2||CR:2||PARAMETERS:2||DIFFRACTION:2||SEMICONDUCTORMETAL TRANSITION:1||INTERMEDIATEVALENCE:1||SMB6:1||SRRUO3:1||antiperovskite structure with antipolar nature:1||lowenergy twodimensional phonons:1||anatase TiO2:1||La3S4:1||metalinsulator transitions:1||MNO:1||ELECTRONICSTRUCTURES:1||MAGNETIC CIRCULARDICHROISM:1||Density functional theory:1||CeCo2:1||TOPOLARON CROSSOVER:1||EXCHANGE:1||cuprates:1||high Tc cuprates:1||magnetically ordered materials:1||ZNSE:1||Sr2xKxFeMoO6:1||CDW:1||TeCuO3:1||STRUCTURALPROPERTIES:1||MN:1||screening length:1||amorphous Fe:1||WAVE BASISSET:1||SILICONCARBIDE:1||HIGHPRESSURE:1||electronphonon coupling:1||quenched superconductivity:1||CMR perovskite manganites:1||OXIDE:1||polarons:1||synchrotron radiation:1||FULLERIDES:1||RESONANTPHOTOEMISSION:1||Silicon carbide:1||DFT calculation:1||Hybridized bands:1||GIANT MAGNETORESISTANCE:1||PEROVSKITES:1||Raman spectra:1||EXCHANGE ENHANCEMENT:1||SILICON:1||SR2FEMOO6:1||orbital ordering:1||delafossite:1||TITANIUMDIOXIDE:1||electronic structure of disordered solids:1||YFE2:1||Magnetic polaron:1||NA2TI2SB2O:1||STRONGCOUPLED SUPERCONDUCTORS:1||HEAVYFERMION SYSTEMS:1||firstprinciples calculations:1||MECHANISM:1||UNiSn:1||PHOTONIC BANDGAP:1||SINGLE IMPURITY:1||PHONONSPECTRUM:1||FERMISURFACE TOPOLOGY:1||SUPPRESSION:1||RESONANT PHOTOEMISSION:1||METALDOPED PICENE:1||PHOTOIONIZATION CROSSSECTIONS:1||PHOTOINDUCED FERRIMAGNETIC SYSTEMS:1||LINKAGE ISOMERISM:1||CHARGETRANSFER:1||Bilayer Graphene:1||MAGNETICFIELD:1||SPINWAVES:1||rareearth manganese oxides:1||magnonphonon interaction:1||NACO2O4:1||ENERGYBANDS:1||SELFENERGY:1||GAS:1||Fe0.5Cu0.5Cr2S4:1||scanning photoelectron microscopy (SPEM):1||MAGNETIC PROPERTIES:1||Stoner model:1||AMORPHOUS TRANSITIONMETALS:1||SPINGLASS STATES:1||NI:1||LA3NI2B2N3:1||SOLIDS:1||CEO2:1||BAND THEORY:1||dilute magnetic semiconductor:1||pyrochlore:1||Y1XPRXBA2CU3O7DELTA:1||and electronphonon interactions:1||VIBRATIONS:1||RAY PHOTOEMISSION:1||ALKALI CATION:1||Europium:1||colossal magnetoresistance:1||structural stability:1||ENERGYGAP:1||small polaron:1||DOUBLE EXCHANGE:1||Coulomb correlation:1||magnon:1||phonons:1||ELECTRON FERROMAGNETISM:1||CURIETEMPERATURE:1||ARPES:1||PLANEWAVE METHOD:1||Xray absorption spectroscopy (XAS):1||ROOMTEMPERATURE:1||MONOCHALCOGENIDES:1||HEAT:1||UPDSN:1||MOMENTS:1||XRAY ABSORPTION:1||SEMICONDUCTOR:1||Fermi surface nesting:1||optical phonon:1||disordered system:1||dilute magnetic semiconductors:1||CMR manganites:1||PHONONS:1||LATTICEDYNAMICS:1||OXIDES:1||4fphotoemission:1||permanent magnet:1||pseudogap:1||TRANSPORTPROPERTIES:1||ANTIFERROMAGNET:1||(BI,PB)SRCOO SYSTEM:1||semicore correlation:1||POLARIZATION:1||CRYSTAL:1||spinel:1||Xray magnetic circular dichroism (XMCD):1||magnetocapacitance:1||ANATASE:1||TEMPERATURES:1||Pseudogap:1||INTERFACE:1||SUBSTRATE:1||YNI2B2C:1||SAMARIUM SULFIDE:1||strong swave superconductor:1||DOPED MANGANITE:1||SYMMETRY:1||CENISN:1||resonance mode:1||DISORDERED SYSTEM:1||LITHIUM INTERCALATION:1||CUO2 PLANE:1||SURFACE:1||Delafossite:1||ELECTRICALPROPERTIES:1||NIMNSB:1||PTMNSB:1||ROOMTEMPERATURE FERROMAGNETISM:1||RUBIDIUM MANGANESE HEXACYANOFERRATE:1||COLOSSALMAGNETORESISTANCE:1||FINITE TEMPERATURES:1||LAMNO3:1||FE:1||transitionmetal oxides:1||giant magnetoresistance:1||phonon:1||COPPER OXIDES:1||valence states:1||thermoelectric:1||semiconductor:1||CATION DISTRIBUTION:1||FeCr2S4:1||photoemission spectroscopy (PES):1||METALLIC FERROMAGNETISM:1||GRAPHITE:1||SUSCEPTIBILITY:1||UBE13:1||RCrSb3:1||band JahnTeller:1||Ce3S4:1||TiO2:1||PrBa2Cu3O7delta:1||UNTWINNED PRBA2CU3O7:1||AGNIO2:1||HALFMETALLIC FERROMAGNETS:1||CI:1||Energy gap:1||Photoemission:1||Future applications:1||Photoemission measurements:1||Graphene:1||BANDSTRUCTURE:1||TC:1||superconductivity:1||magnetic semiconductors:1||CMRmanganites:1||thin films:1||spin dynamics:1||highTc superconductors:1||ITINERANTELECTRON FERROMAGNETISM:1||SINGLECRYSTALS:1||CeTe2:1||amorphous magnetic materials:1||EPITAXIAL GRAPHENE:1||LAYERED PNICTIDEOXIDES:1||BOROCARBIDE SUPERCONDUCTORS:1||AUGMENTEDWAVE METHOD:1||METALLIC MAGNET UNISN:1||ORIGIN:1||spectrum rearrangement:1||MEANFIELD THEORY:1||MOLECULEBASED MAGNETS:1||METASTABLE STATE:1||INSULATOR:1||magnetic orderin:1||FCC IRON:1||CeRu2:1||TL2MN2O7:1||isotope effect:1||Perovskitemanganites:1||RECURSION METHOD:1||PERPENDICULAR MAGNETICANISOTROPY:1||quasiparticle spectral density:1||GW:1||MANGANESE FERRITE:1||RESONANCE:1||SeCuO3:1||Optical conductivity:1||MASSLESS DIRAC FERMIONS:1||SCHOTTKYBARRIER:1||electronic structure:15||ELECTRONICSTRUCTURE:11||TRANSITIONMETAL COMPOUNDS:10||METALS:10||photoemission:8||SPECTRA:8||MAGNETORESISTANCE:7||FERROMAGNETISM:7||TRANSPORT:7||TRANSITION:6||FILMS:6||THINFILMS:5||TOTALENERGY CALCULATIONS:5||MAGNETICPROPERTIES:5||SUPERCONDUCTIVITY:5||PR:5||LATTICE:4||STATES:4||SPECTROSCOPY:4||FIELD:4||CRYSTALSTRUCTURE:4||PHOTOEMISSION:4||TEMPERATURE:4||TRANSITIONTEMPERATURE:4||XRAYABSORPTION:4||STATE:4||CU:4||BASISSET:4||XAS:4||CRYSTALS:3||EXCITATIONS:3||MOTTHUBBARD SYSTEMS:3||HIGHENERGY SPIN:3||halfmetal:3||INSULATORS:3||LA2CUO4:3||MODEL:3||FLUCTUATIONS:3||CE:3||double exchange:3||TRANSITIONMETALS:3||RESISTIVITY:3||BORON:3||LA1XCAXMNO3:3||IRON:3||PES:3||ANTIMONIDES:2||MgB2:2||ZR METALLIC GLASSES:2||superconductor:2||CRITICALCURRENT DENSITY:2||CIRCULARDICHROISM:2||SEMICONDUCTORS:2||LOCALIZATION:2||INTRABAND OPTICAL CONDUCTIVITY:2||COLOSSAL MAGNETORESISTANCE:2||OXIDATION:2||EXISTENCE:2||COPPER:2||diboride:2||MAGNESIUMDIBORIDE:2||GAP:2||CE COMPOUNDS:2||CORE POLARIZATION:2||magnetoresistance:2||photoemission spectroscopy:2||electronphonon interaction:2||GETTER:2||PD:2||MAGNETISM:2||FECR2S4:2||SUPERCONDUCTING MGB2:2||WIRES:2||ABSORPTION:2||ENERGY:2||LA1XSRXMNO3:2||CONSTANTS:2||polaron:2||charge ordering:2||SCATTERING:2||XRAY PHOTOEMISSION:2||CeNiSn:2||phase diagram:2||PHOTOELECTRON:2||QUADRUPOLAR:2||perovskitemanganites:2||CO:2||SYSTEMS:2||DOPED ZNO:2||LOWFREQUENCY SOUND:2||LA:2||ELECTRONELECTRON SCATTERING:2||AU:2||DENSITYWAVE INSTABILITY:2||FERMISURFACE:2||hybridization:2||VALENCEBAND SATELLITE:2||SULFUR SPINEL:2||Heusler:2||APPROXIMATION:2||superexchange:2||colossal magnetoresistance:2||ALLOYS:2||DEPENDENCE:2||AG:2||electronic structures:2||AUGERSPECTRA:2||CR:2||PARAMETERS:2||DIFFRACTION:2||SEMICONDUCTORMETAL TRANSITION:1||INTERMEDIATEVALENCE:1||SMB6:1||SRRUO3:1||antiperovskite structure with antipolar nature:1||lowenergy twodimensional phonons:1||anatase TiO2:1||La3S4:1||metalinsulator transitions:1||MNO:1||ELECTRONICSTRUCTURES:1||MAGNETIC CIRCULARDICHROISM:1||Density functional theory:1||CeCo2:1||TOPOLARON CROSSOVER:1||EXCHANGE:1||cuprates:1||high Tc cuprates:1||magnetically ordered materials:1||ZNSE:1||Sr2xKxFeMoO6:1||CDW:1||TeCuO3:1||STRUCTURALPROPERTIES:1||MN:1||screening length:1||amorphous Fe:1||WAVE BASISSET:1||SILICONCARBIDE:1||HIGHPRESSURE:1||electronphonon coupling:1||quenched superconductivity:1||CMR perovskite manganites:1||OXIDE:1||polarons:1||synchrotron radiation:1||FULLERIDES:1||RESONANTPHOTOEMISSION:1||Silicon carbide:1||DFT calculation:1||Hybridized bands:1||GIANT MAGNETORESISTANCE:1||PEROVSKITES:1||Raman spectra:1||EXCHANGE ENHANCEMENT:1||SILICON:1||SR2FEMOO6:1||orbital ordering:1||delafossite:1||TITANIUMDIOXIDE:1||electronic structure of disordered solids:1||YFE2:1||Magnetic polaron:1||NA2TI2SB2O:1||STRONGCOUPLED SUPERCONDUCTORS:1||HEAVYFERMION SYSTEMS:1||firstprinciples calculations:1||MECHANISM:1||UNiSn:1||PHOTONIC BANDGAP:1||SINGLE IMPURITY:1||PHONONSPECTRUM:1||FERMISURFACE TOPOLOGY:1||SUPPRESSION:1||RESONANT PHOTOEMISSION:1||METALDOPED PICENE:1||PHOTOIONIZATION CROSSSECTIONS:1||PHOTOINDUCED FERRIMAGNETIC SYSTEMS:1||LINKAGE ISOMERISM:1||CHARGETRANSFER:1||Bilayer Graphene:1||MAGNETICFIELD:1||SPINWAVES:1||rareearth manganese oxides:1||magnonphonon interaction:1||NACO2O4:1||ENERGYBANDS:1||SELFENERGY:1||GAS:1||Fe0.5Cu0.5Cr2S4:1||scanning photoelectron microscopy (SPEM):1||MAGNETIC PROPERTIES:1||Stoner model:1||AMORPHOUS TRANSITIONMETALS:1||SPINGLASS STATES:1||NI:1||LA3NI2B2N3:1||SOLIDS:1||CEO2:1||BAND THEORY:1||dilute magnetic semiconductor:1||pyrochlore:1||Y1XPRXBA2CU3O7DELTA:1||and electronphonon interactions:1||VIBRATIONS:1||RAY PHOTOEMISSION:1||ALKALI CATION:1||Europium:1||colossal magnetoresistance:1||structural stability:1||ENERGYGAP:1||small polaron:1||DOUBLE EXCHANGE:1||Coulomb correlation:1||magnon:1||phonons:1||ELECTRON FERROMAGNETISM:1||CURIETEMPERATURE:1||ARPES:1||PLANEWAVE METHOD:1||Xray absorption spectroscopy (XAS):1||ROOMTEMPERATURE:1||MONOCHALCOGENIDES:1||HEAT:1||UPDSN:1||MOMENTS:1||XRAY ABSORPTION:1||SEMICONDUCTOR:1||Fermi surface nesting:1||optical phonon:1||disordered system:1||dilute magnetic semiconductors:1||CMR manganites:1||PHONONS:1||LATTICEDYNAMICS:1||OXIDES:1||4fphotoemission:1||permanent magnet:1||pseudogap:1||TRANSPORTPROPERTIES:1||ANTIFERROMAGNET:1||(BI,PB)SRCOO SYSTEM:1||semicore correlation:1||POLARIZATION:1||CRYSTAL:1||spinel:1||Xray magnetic circular dichroism (XMCD):1||magnetocapacitance:1||ANATASE:1||TEMPERATURES:1||Pseudogap:1||INTERFACE:1||SUBSTRATE:1||YNI2B2C:1||SAMARIUM SULFIDE:1||strong swave superconductor:1||DOPED MANGANITE:1||SYMMETRY:1||CENISN:1||resonance mode:1||DISORDERED SYSTEM:1||LITHIUM INTERCALATION:1||CUO2 PLANE:1||SURFACE:1||Delafossite:1||ELECTRICALPROPERTIES:1||NIMNSB:1||PTMNSB:1||ROOMTEMPERATURE FERROMAGNETISM:1||RUBIDIUM MANGANESE HEXACYANOFERRATE:1||COLOSSALMAGNETORESISTANCE:1||FINITE TEMPERATURES:1||LAMNO3:1||FE:1||transitionmetal oxides:1||giant magnetoresistance:1||phonon:1||COPPER OXIDES:1||valence states:1||thermoelectric:1||semiconductor:1||CATION DISTRIBUTION:1||FeCr2S4:1||photoemission spectroscopy (PES):1||METALLIC FERROMAGNETISM:1||GRAPHITE:1||SUSCEPTIBILITY:1||UBE13:1||RCrSb3:1||band JahnTeller:1||Ce3S4:1||TiO2:1||PrBa2Cu3O7delta:1||UNTWINNED PRBA2CU3O7:1||AGNIO2:1||HALFMETALLIC FERROMAGNETS:1||CI:1||Energy gap:1||Photoemission:1||Future applications:1||Photoemission measurements:1||Graphene:1||BANDSTRUCTURE:1||TC:1||superconductivity:1||magnetic semiconductors:1||CMRmanganites:1||thin films:1||spin dynamics:1||highTc superconductors:1||ITINERANTELECTRON FERROMAGNETISM:1||SINGLECRYSTALS:1||CeTe2:1||amorphous magnetic materials:1||EPITAXIAL GRAPHENE:1||LAYERED PNICTIDEOXIDES:1||BOROCARBIDE SUPERCONDUCTORS:1||AUGMENTEDWAVE METHOD:1||METALLIC MAGNET UNISN:1||ORIGIN:1||spectrum rearrangement:1||MEANFIELD THEORY:1||MOLECULEBASED MAGNETS:1||METASTABLE STATE:1||INSULATOR:1||magnetic orderin:1||FCC IRON:1||CeRu2:1||TL2MN2O7:1||isotope effect:1||Perovskitemanganites:1||RECURSION METHOD:1||PERPENDICULAR MAGNETICANISOTROPY:1||quasiparticle spectral density:1||GW:1||MANGANESE FERRITE:1||RESONANCE:1||SeCuO3:1||Optical conductivity:1||MASSLESS DIRAC FERMIONS:1||SCHOTTKYBARRIER:1||electronic structure:15||ELECTRONICSTRUCTURE:11||TRANSITIONMETAL COMPOUNDS:10||METALS:10||photoemission:8||SPECTRA:8||MAGNETORESISTANCE:7||FERROMAGNETISM:7||TRANSPORT:7||TRANSITION:6||FILMS:6||THINFILMS:5||TOTALENERGY CALCULATIONS:5||MAGNETICPROPERTIES:5||SUPERCONDUCTIVITY:5||PR:5||LATTICE:4||STATES:4||SPECTROSCOPY:4||FIELD:4||CRYSTALSTRUCTURE:4||PHOTOEMISSION:4||TEMPERATURE:4||TRANSITIONTEMPERATURE:4||XRAYABSORPTION:4||STATE:4||CU:4||BASISSET:4||XAS:4||CRYSTALS:3||EXCITATIONS:3||MOTTHUBBARD SYSTEMS:3||HIGHENERGY SPIN:3||halfmetal:3||INSULATORS:3||LA2CUO4:3||MODEL:3||FLUCTUATIONS:3||CE:3||double exchange:3||TRANSITIONMETALS:3||RESISTIVITY:3||BORON:3||LA1XCAXMNO3:3||IRON:3||PES:3||ANTIMONIDES:2||MgB2:2||ZR METALLIC GLASSES:2||superconductor:2||CRITICALCURRENT DENSITY:2||CIRCULARDICHROISM:2||SEMICONDUCTORS:2||LOCALIZATION:2||INTRABAND OPTICAL CONDUCTIVITY:2||COLOSSAL MAGNETORESISTANCE:2||OXIDATION:2||EXISTENCE:2||COPPER:2||diboride:2||MAGNESIUMDIBORIDE:2||GAP:2||CE COMPOUNDS:2||CORE POLARIZATION:2||magnetoresistance:2||photoemission spectroscopy:2||electronphonon interaction:2||GETTER:2||PD:2||MAGNETISM:2||FECR2S4:2||SUPERCONDUCTING MGB2:2||WIRES:2||ABSORPTION:2||ENERGY:2||LA1XSRXMNO3:2||CONSTANTS:2||polaron:2||charge ordering:2||SCATTERING:2||XRAY PHOTOEMISSION:2||CeNiSn:2||phase diagram:2||PHOTOELECTRON:2||QUADRUPOLAR:2||perovskitemanganites:2||CO:2||SYSTEMS:2||DOPED ZNO:2||LOWFREQUENCY SOUND:2||LA:2||ELECTRONELECTRON SCATTERING:2||AU:2||DENSITYWAVE INSTABILITY:2||FERMISURFACE:2||hybridization:2||VALENCEBAND SATELLITE:2||SULFUR SPINEL:2||Heusler:2||APPROXIMATION:2||superexchange:2||colossal magnetoresistance:2||ALLOYS:2||DEPENDENCE:2||AG:2||electronic structures:2||AUGERSPECTRA:2||CR:2||PARAMETERS:2||DIFFRACTION:2||SEMICONDUCTORMETAL TRANSITION:1||INTERMEDIATEVALENCE:1||SMB6:1||SRRUO3:1||antiperovskite structure with antipolar nature:1||lowenergy twodimensional phonons:1||anatase TiO2:1||La3S4:1||metalinsulator transitions:1||MNO:1||ELECTRONICSTRUCTURES:1||MAGNETIC CIRCULARDICHROISM:1||Density functional theory:1||CeCo2:1||TOPOLARON CROSSOVER:1||EXCHANGE:1||cuprates:1||high Tc cuprates:1||magnetically ordered materials:1||ZNSE:1||Sr2xKxFeMoO6:1||CDW:1||TeCuO3:1||STRUCTURALPROPERTIES:1||MN:1||screening length:1||amorphous Fe:1||WAVE BASISSET:1||SILICONCARBIDE:1||HIGHPRESSURE:1||electronphonon coupling:1||quenched superconductivity:1||CMR perovskite manganites:1||OXIDE:1||polarons:1||synchrotron radiation:1||FULLERIDES:1||RESONANTPHOTOEMISSION:1||Silicon carbide:1||DFT calculation:1||Hybridized bands:1||GIANT MAGNETORESISTANCE:1||PEROVSKITES:1||Raman spectra:1||EXCHANGE ENHANCEMENT:1||SILICON:1||SR2FEMOO6:1||orbital ordering:1||delafossite:1||TITANIUMDIOXIDE:1||electronic structure of disordered solids:1||YFE2:1||Magnetic polaron:1||NA2TI2SB2O:1||STRONGCOUPLED SUPERCONDUCTORS:1||HEAVYFERMION SYSTEMS:1||firstprinciples calculations:1||MECHANISM:1||UNiSn:1||PHOTONIC BANDGAP:1||SINGLE IMPURITY:1||PHONONSPECTRUM:1||FERMISURFACE TOPOLOGY:1||SUPPRESSION:1||RESONANT PHOTOEMISSION:1||METALDOPED PICENE:1||PHOTOIONIZATION CROSSSECTIONS:1||PHOTOINDUCED FERRIMAGNETIC SYSTEMS:1||LINKAGE ISOMERISM:1||CHARGETRANSFER:1||Bilayer Graphene:1||MAGNETICFIELD:1||SPINWAVES:1||rareearth manganese oxides:1||magnonphonon interaction:1||NACO2O4:1||ENERGYBANDS:1||SELFENERGY:1||GAS:1||Fe0.5Cu0.5Cr2S4:1||scanning photoelectron microscopy (SPEM):1||MAGNETIC PROPERTIES:1||Stoner model:1||AMORPHOUS TRANSITIONMETALS:1||SPINGLASS STATES:1||NI:1||LA3NI2B2N3:1||SOLIDS:1||CEO2:1||BAND THEORY:1||dilute magnetic semiconductor:1||pyrochlore:1||Y1XPRXBA2CU3O7DELTA:1||and electronphonon interactions:1||VIBRATIONS:1||RAY PHOTOEMISSION:1||ALKALI CATION:1||Europium:1||colossal magnetoresistance:1||structural stability:1||ENERGYGAP:1||small polaron:1||DOUBLE EXCHANGE:1||Coulomb correlation:1||magnon:1||phonons:1||ELECTRON FERROMAGNETISM:1||CURIETEMPERATURE:1||ARPES:1||PLANEWAVE METHOD:1||Xray absorption spectroscopy (XAS):1||ROOMTEMPERATURE:1||MONOCHALCOGENIDES:1||HEAT:1||UPDSN:1||MOMENTS:1||XRAY ABSORPTION:1||SEMICONDUCTOR:1||Fermi surface nesting:1||optical phonon:1||disordered system:1||dilute magnetic semiconductors:1||CMR manganites:1||PHONONS:1||LATTICEDYNAMICS:1||OXIDES:1||4fphotoemission:1||permanent magnet:1||pseudogap:1||TRANSPORTPROPERTIES:1||ANTIFERROMAGNET:1||(BI,PB)SRCOO SYSTEM:1||semicore correlation:1||POLARIZATION:1||CRYSTAL:1||spinel:1||Xray magnetic circular dichroism (XMCD):1||magnetocapacitance:1||ANATASE:1||TEMPERATURES:1||Pseudogap:1||INTERFACE:1||SUBSTRATE:1||YNI2B2C:1||SAMARIUM SULFIDE:1||strong swave superconductor:1||DOPED MANGANITE:1||SYMMETRY:1||CENISN:1||resonance mode:1||DISORDERED SYSTEM:1||LITHIUM INTERCALATION:1||CUO2 PLANE:1||SURFACE:1||Delafossite:1||ELECTRICALPROPERTIES:1||NIMNSB:1||PTMNSB:1||ROOMTEMPERATURE FERROMAGNETISM:1||RUBIDIUM MANGANESE HEXACYANOFERRATE:1||COLOSSALMAGNETORESISTANCE:1||FINITE TEMPERATURES:1||LAMNO3:1||FE:1||transitionmetal oxides:1||giant magnetoresistance:1||phonon:1||COPPER OXIDES:1||valence states:1||thermoelectric:1||semiconductor:1||CATION DISTRIBUTION:1||FeCr2S4:1||photoemission spectroscopy (PES):1||METALLIC FERROMAGNETISM:1||GRAPHITE:1||SUSCEPTIBILITY:1||UBE13:1||RCrSb3:1||band JahnTeller:1||Ce3S4:1||TiO2:1||PrBa2Cu3O7delta:1||UNTWINNED PRBA2CU3O7:1||AGNIO2:1||HALFMETALLIC FERROMAGNETS:1||CI:1||Energy gap:1||Photoemission:1||Future applications:1||Photoemission measurements:1||Graphene:1||BANDSTRUCTURE:1||TC:1||superconductivity:1||magnetic semiconductors:1||CMRmanganites:1||thin films:1||spin dynamics:1||highTc superconductors:1||ITINERANTELECTRON FERROMAGNETISM:1||SINGLECRYSTALS:1||CeTe2:1||amorphous magnetic materials:1||EPITAXIAL GRAPHENE:1||LAYERED PNICTIDEOXIDES:1||BOROCARBIDE SUPERCONDUCTORS:1||AUGMENTEDWAVE METHOD:1||METALLIC MAGNET UNISN:1||ORIGIN:1||spectrum rearrangement:1||MEANFIELD THEORY:1||MOLECULEBASED MAGNETS:1||METASTABLE STATE:1||INSULATOR:1||magnetic orderin:1||FCC IRON:1||CeRu2:1||TL2MN2O7:1||isotope effect:1||Perovskitemanganites:1||RECURSION METHOD:1||PERPENDICULAR MAGNETICANISOTROPY:1||quasiparticle spectral density:1||GW:1||MANGANESE FERRITE:1||RESONANCE:1||SeCuO3:1||Optical conductivity:1||MASSLESS DIRAC FERMIONS:1||SCHOTTKYBARRIER:1||electronic structure:15||ELECTRONICSTRUCTURE:11||TRANSITIONMETAL COMPOUNDS:10||METALS:10||photoemission:8||SPECTRA:8||MAGNETORESISTANCE:7||FERROMAGNETISM:7||TRANSPORT:7||TRANSITION:6||FILMS:6||THINFILMS:5||TOTALENERGY CALCULATIONS:5||MAGNETICPROPERTIES:5||SUPERCONDUCTIVITY:5||PR:5||LATTICE:4||STATES:4||SPECTROSCOPY:4||FIELD:4||CRYSTALSTRUCTURE:4||PHOTOEMISSION:4||TEMPERATURE:4||TRANSITIONTEMPERATURE:4||XRAYABSORPTION:4||STATE:4||CU:4||BASISSET:4||XAS:4||CRYSTALS:3||EXCITATIONS:3||MOTTHUBBARD SYSTEMS:3||HIGHENERGY SPIN:3||halfmetal:3||INSULATORS:3||LA2CUO4:3||MODEL:3||FLUCTUATIONS:3||CE:3||double exchange:3||TRANSITIONMETALS:3||RESISTIVITY:3||BORON:3||LA1XCAXMNO3:3||IRON:3||PES:3||ANTIMONIDES:2||MgB2:2||ZR METALLIC GLASSES:2||superconductor:2||CRITICALCURRENT DENSITY:2||CIRCULARDICHROISM:2||SEMICONDUCTORS:2||LOCALIZATION:2||INTRABAND OPTICAL CONDUCTIVITY:2||COLOSSAL MAGNETORESISTANCE:2||OXIDATION:2||EXISTENCE:2||COPPER:2||diboride:2||MAGNESIUMDIBORIDE:2||GAP:2||CE COMPOUNDS:2||CORE POLARIZATION:2||magnetoresistance:2||photoemission spectroscopy:2||electronphonon interaction:2||GETTER:2||PD:2||MAGNETISM:2||FECR2S4:2||SUPERCONDUCTING MGB2:2||WIRES:2||ABSORPTION:2||ENERGY:2||LA1XSRXMNO3:2||CONSTANTS:2||polaron:2||charge ordering:2||SCATTERING:2||XRAY PHOTOEMISSION:2||CeNiSn:2||phase diagram:2||PHOTOELECTRON:2||QUADRUPOLAR:2||perovskitemanganites:2||CO:2||SYSTEMS:2||DOPED ZNO:2||LOWFREQUENCY SOUND:2||LA:2||ELECTRONELECTRON SCATTERING:2||AU:2||DENSITYWAVE INSTABILITY:2||FERMISURFACE:2||hybridization:2||VALENCEBAND SATELLITE:2||SULFUR SPINEL:2||Heusler:2||APPROXIMATION:2||superexchange:2||colossal magnetoresistance:2||ALLOYS:2||DEPENDENCE:2||AG:2||electronic structures:2||AUGERSPECTRA:2||CR:2||PARAMETERS:2||DIFFRACTION:2||SEMICONDUCTORMETAL TRANSITION:1||INTERMEDIATEVALENCE:1||SMB6:1||SRRUO3:1||antiperovskite structure with antipolar nature:1||lowenergy twodimensional phonons:1||anatase TiO2:1||La3S4:1||metalinsulator transitions:1||MNO:1||ELECTRONICSTRUCTURES:1||MAGNETIC CIRCULARDICHROISM:1||Density functional theory:1||CeCo2:1||TOPOLARON CROSSOVER:1||EXCHANGE:1||cuprates:1||high Tc cuprates:1||magnetically ordered materials:1||ZNSE:1||Sr2xKxFeMoO6:1||CDW:1||TeCuO3:1||STRUCTURALPROPERTIES:1||MN:1||screening length:1||amorphous Fe:1||WAVE BASISSET:1||SILICONCARBIDE:1||HIGHPRESSURE:1||electronphonon coupling:1||quenched superconductivity:1||CMR perovskite manganites:1||OXIDE:1||polarons:1||synchrotron radiation:1||FULLERIDES:1||RESONANTPHOTOEMISSION:1||Silicon carbide:1||DFT calculation:1||Hybridized bands:1||GIANT MAGNETORESISTANCE:1||PEROVSKITES:1||Raman spectra:1||EXCHANGE ENHANCEMENT:1||SILICON:1||SR2FEMOO6:1||orbital ordering:1||delafossite:1||TITANIUMDIOXIDE:1||electronic structure of disordered solids:1||YFE2:1||Magnetic polaron:1||NA2TI2SB2O:1||STRONGCOUPLED SUPERCONDUCTORS:1||HEAVYFERMION SYSTEMS:1||firstprinciples calculations:1||MECHANISM:1||UNiSn:1||PHOTONIC BANDGAP:1||SINGLE IMPURITY:1||PHONONSPECTRUM:1||FERMISURFACE TOPOLOGY:1||SUPPRESSION:1||RESONANT PHOTOEMISSION:1||METALDOPED PICENE:1||PHOTOIONIZATION CROSSSECTIONS:1||PHOTOINDUCED FERRIMAGNETIC SYSTEMS:1||LINKAGE ISOMERISM:1||CHARGETRANSFER:1||Bilayer Graphene:1||MAGNETICFIELD:1||SPINWAVES:1||rareearth manganese oxides:1||magnonphonon interaction:1||NACO2O4:1||ENERGYBANDS:1||SELFENERGY:1||GAS:1||Fe0.5Cu0.5Cr2S4:1||scanning photoelectron microscopy (SPEM):1||MAGNETIC PROPERTIES:1||Stoner model:1||AMORPHOUS TRANSITIONMETALS:1||SPINGLASS STATES:1||NI:1||LA3NI2B2N3:1||SOLIDS:1||CEO2:1||BAND THEORY:1||dilute magnetic semiconductor:1||pyrochlore:1||Y1XPRXBA2CU3O7DELTA:1||and electronphonon interactions:1||VIBRATIONS:1||RAY PHOTOEMISSION:1||ALKALI CATION:1||Europium:1||colossal magnetoresistance:1||structural stability:1||ENERGYGAP:1||small polaron:1||DOUBLE EXCHANGE:1||Coulomb correlation:1||magnon:1||phonons:1||ELECTRON FERROMAGNETISM:1||CURIETEMPERATURE:1||ARPES:1||PLANEWAVE METHOD:1||Xray absorption spectroscopy (XAS):1||ROOMTEMPERATURE:1||MONOCHALCOGENIDES:1||HEAT:1||UPDSN:1||MOMENTS:1||XRAY ABSORPTION:1||SEMICONDUCTOR:1||Fermi surface nesting:1||optical phonon:1||disordered system:1||dilute magnetic semiconductors:1||CMR manganites:1||PHONONS:1||LATTICEDYNAMICS:1||OXIDES:1||4fphotoemission:1||permanent magnet:1||pseudogap:1||TRANSPORTPROPERTIES:1||ANTIFERROMAGNET:1||(BI,PB)SRCOO SYSTEM:1||semicore correlation:1||POLARIZATION:1||CRYSTAL:1||spinel:1||Xray magnetic circular dichroism (XMCD):1||magnetocapacitance:1||ANATASE:1||TEMPERATURES:1||Pseudogap:1||INTERFACE:1||SUBSTRATE:1||YNI2B2C:1||SAMARIUM SULFIDE:1||strong swave superconductor:1||DOPED MANGANITE:1||SYMMETRY:1||CENISN:1||resonance mode:1||DISORDERED SYSTEM:1||LITHIUM INTERCALATION:1||CUO2 PLANE:1||SURFACE:1||Delafossite:1||ELECTRICALPROPERTIES:1||NIMNSB:1||PTMNSB:1||ROOMTEMPERATURE FERROMAGNETISM:1||RUBIDIUM MANGANESE HEXACYANOFERRATE:1||COLOSSALMAGNETORESISTANCE:1||FINITE TEMPERATURES:1||LAMNO3:1||FE:1||transitionmetal oxides:1||giant magnetoresistance:1||phonon:1||COPPER OXIDES:1||valence states:1||thermoelectric:1||semiconductor:1||CATION DISTRIBUTION:1||FeCr2S4:1||photoemission spectroscopy (PES):1||METALLIC FERROMAGNETISM:1||GRAPHITE:1||SUSCEPTIBILITY:1||UBE13:1||RCrSb3:1||band JahnTeller:1||Ce3S4:1||TiO2:1||PrBa2Cu3O7delta:1||UNTWINNED PRBA2CU3O7:1||AGNIO2:1||HALFMETALLIC FERROMAGNETS:1||CI:1||Energy gap:1||Photoemission:1||Future applications:1||Photoemission measurements:1||Graphene:1||BANDSTRUCTURE:1||TC:1||superconductivity:1||magnetic semiconductors:1||CMRmanganites:1||thin films:1||spin dynamics:1||highTc superconductors:1||ITINERANTELECTRON FERROMAGNETISM:1||SINGLECRYSTALS:1||CeTe2:1||amorphous magnetic materials:1||EPITAXIAL GRAPHENE:1||LAYERED PNICTIDEOXIDES:1||BOROCARBIDE SUPERCONDUCTORS:1||AUGMENTEDWAVE METHOD:1||METALLIC MAGNET UNISN:1||ORIGIN:1||spectrum rearrangement:1||MEANFIELD THEORY:1||MOLECULEBASED MAGNETS:1||METASTABLE STATE:1||INSULATOR:1||magnetic orderin:1||FCC IRON:1||CeRu2:1||TL2MN2O7:1||isotope effect:1||Perovskitemanganites:1||RECURSION METHOD:1||PERPENDICULAR MAGNETICANISOTROPY:1||quasiparticle spectral density:1||GW:1||MANGANESE FERRITE:1||RESONANCE:1||SeCuO3:1||Optical conductivity:1||MASSLESS DIRAC FERMIONS:1||SCHOTTKYBARRIER:1||electronic structure:15||ELECTRONICSTRUCTURE:11||TRANSITIONMETAL COMPOUNDS:10||METALS:10||photoemission:8||SPECTRA:8||MAGNETORESISTANCE:7||FERROMAGNETISM:7||TRANSPORT:7||TRANSITION:6||FILMS:6||THINFILMS:5||TOTALENERGY CALCULATIONS:5||MAGNETICPROPERTIES:5||SUPERCONDUCTIVITY:5||PR:5||LATTICE:4||STATES:4||SPECTROSCOPY:4||FIELD:4||CRYSTALSTRUCTURE:4||PHOTOEMISSION:4||TEMPERATURE:4||TRANSITIONTEMPERATURE:4||XRAYABSORPTION:4||STATE:4||CU:4||BASISSET:4||XAS:4||CRYSTALS:3||EXCITATIONS:3||MOTTHUBBARD SYSTEMS:3||HIGHENERGY SPIN:3||halfmetal:3||INSULATORS:3||LA2CUO4:3||MODEL:3||FLUCTUATIONS:3||CE:3||double exchange:3||TRANSITIONMETALS:3||RESISTIVITY:3||BORON:3||LA1XCAXMNO3:3||IRON:3||PES:3||ANTIMONIDES:2||MgB2:2||ZR METALLIC GLASSES:2||superconductor:2||CRITICALCURRENT DENSITY:2||CIRCULARDICHROISM:2||SEMICONDUCTORS:2||LOCALIZATION:2||INTRABAND OPTICAL CONDUCTIVITY:2||COLOSSAL MAGNETORESISTANCE:2||OXIDATION:2||EXISTENCE:2||COPPER:2||diboride:2||MAGNESIUMDIBORIDE:2||GAP:2||CE COMPOUNDS:2||CORE POLARIZATION:2||magnetoresistance:2||photoemission spectroscopy:2||electronphonon interaction:2||GETTER:2||PD:2||MAGNETISM:2||FECR2S4:2||SUPERCONDUCTING MGB2:2||WIRES:2||ABSORPTION:2||ENERGY:2||LA1XSRXMNO3:2||CONSTANTS:2||polaron:2||charge ordering:2||SCATTERING:2||XRAY PHOTOEMISSION:2||CeNiSn:2||phase diagram:2||PHOTOELECTRON:2||QUADRUPOLAR:2||perovskitemanganites:2||CO:2||SYSTEMS:2||DOPED ZNO:2||LOWFREQUENCY SOUND:2||LA:2||ELECTRONELECTRON SCATTERING:2||AU:2||DENSITYWAVE INSTABILITY:2||FERMISURFACE:2||hybridization:2||VALENCEBAND SATELLITE:2||SULFUR SPINEL:2||Heusler:2||APPROXIMATION:2||superexchange:2||colossal magnetoresistance:2||ALLOYS:2||DEPENDENCE:2||AG:2||electronic structures:2||AUGERSPECTRA:2||CR:2||PARAMETERS:2||DIFFRACTION:2||SEMICONDUCTORMETAL TRANSITION:1||INTERMEDIATEVALENCE:1||SMB6:1||SRRUO3:1||antiperovskite structure with antipolar nature:1||lowenergy twodimensional phonons:1||anatase TiO2:1||La3S4:1||metalinsulator transitions:1||MNO:1||ELECTRONICSTRUCTURES:1||MAGNETIC CIRCULARDICHROISM:1||Density functional theory:1||CeCo2:1||TOPOLARON CROSSOVER:1||EXCHANGE:1||cuprates:1||high Tc cuprates:1||magnetically ordered materials:1||ZNSE:1||Sr2xKxFeMoO6:1||CDW:1||TeCuO3:1||STRUCTURALPROPERTIES:1||MN:1||screening length:1||amorphous Fe:1||WAVE BASISSET:1||SILICONCARBIDE:1||HIGHPRESSURE:1||electronphonon coupling:1||quenched superconductivity:1||CMR perovskite manganites:1||OXIDE:1||polarons:1||synchrotron radiation:1||FULLERIDES:1||RESONANTPHOTOEMISSION:1||Silicon carbide:1||DFT calculation:1||Hybridized bands:1||GIANT MAGNETORESISTANCE:1||PEROVSKITES:1||Raman spectra:1||EXCHANGE ENHANCEMENT:1||SILICON:1||SR2FEMOO6:1||orbital ordering:1||delafossite:1||TITANIUMDIOXIDE:1||electronic structure of disordered solids:1||YFE2:1||Magnetic polaron:1||NA2TI2SB2O:1||STRONGCOUPLED SUPERCONDUCTORS:1||HEAVYFERMION SYSTEMS:1||firstprinciples calculations:1||MECHANISM:1||UNiSn:1||PHOTONIC BANDGAP:1||SINGLE IMPURITY:1||PHONONSPECTRUM:1||FERMISURFACE TOPOLOGY:1||SUPPRESSION:1||RESONANT PHOTOEMISSION:1||METALDOPED PICENE:1||PHOTOIONIZATION CROSSSECTIONS:1||PHOTOINDUCED FERRIMAGNETIC SYSTEMS:1||LINKAGE ISOMERISM:1||CHARGETRANSFER:1||Bilayer Graphene:1||MAGNETICFIELD:1||SPINWAVES:1||rareearth manganese oxides:1||magnonphonon interaction:1||NACO2O4:1||ENERGYBANDS:1||SELFENERGY:1||GAS:1||Fe0.5Cu0.5Cr2S4:1||scanning photoelectron microscopy (SPEM):1||MAGNETIC PROPERTIES:1||Stoner model:1||AMORPHOUS TRANSITIONMETALS:1||SPINGLASS STATES:1||NI:1||LA3NI2B2N3:1||SOLIDS:1||CEO2:1||BAND THEORY:1||dilute magnetic semiconductor:1||pyrochlore:1||Y1XPRXBA2CU3O7DELTA:1||and electronphonon interactions:1||VIBRATIONS:1||RAY PHOTOEMISSION:1||ALKALI CATION:1||Europium:1||colossal magnetoresistance:1||structural stability:1||ENERGYGAP:1||small polaron:1||DOUBLE EXCHANGE:1||Coulomb correlation:1||magnon:1||phonons:1||ELECTRON FERROMAGNETISM:1||CURIETEMPERATURE:1||ARPES:1||PLANEWAVE METHOD:1||Xray absorption spectroscopy (XAS):1||ROOMTEMPERATURE:1||MONOCHALCOGENIDES:1||HEAT:1||UPDSN:1||MOMENTS:1||XRAY ABSORPTION:1||SEMICONDUCTOR:1||Fermi surface nesting:1||optical phonon:1||disordered system:1||dilute magnetic semiconductors:1||CMR manganites:1||PHONONS:1||LATTICEDYNAMICS:1||OXIDES:1||4fphotoemission:1||permanent magnet:1||pseudogap:1||TRANSPORTPROPERTIES:1||ANTIFERROMAGNET:1||(BI,PB)SRCOO SYSTEM:1||semicore correlation:1||POLARIZATION:1||CRYSTAL:1||spinel:1||Xray magnetic circular dichroism (XMCD):1||magnetocapacitance:1||ANATASE:1||TEMPERATURES:1||Pseudogap:1||INTERFACE:1||SUBSTRATE:1||YNI2B2C:1||SAMARIUM SULFIDE:1||strong swave superconductor:1||DOPED MANGANITE:1||SYMMETRY:1||CENISN:1||resonance mode:1||DISORDERED SYSTEM:1||LITHIUM INTERCALATION:1||CUO2 PLANE:1||SURFACE:1||Delafossite:1||ELECTRICALPROPERTIES:1||NIMNSB:1||PTMNSB:1||ROOMTEMPERATURE FERROMAGNETISM:1||RUBIDIUM MANGANESE HEXACYANOFERRATE:1||COLOSSALMAGNETORESISTANCE:1||FINITE TEMPERATURES:1||LAMNO3:1||FE:1||transitionmetal oxides:1||giant magnetoresistance:1||phonon:1||COPPER OXIDES:1||valence states:1||thermoelectric:1||semiconductor:1||CATION DISTRIBUTION:1||FeCr2S4:1||photoemission spectroscopy (PES):1||METALLIC FERROMAGNETISM:1||GRAPHITE:1||SUSCEPTIBILITY:1||UBE13:1||RCrSb3:1||band JahnTeller:1||Ce3S4:1||TiO2:1||PrBa2Cu3O7delta:1||UNTWINNED PRBA2CU3O7:1||AGNIO2:1||HALFMETALLIC FERROMAGNETS:1||CI:1||Energy gap:1||Photoemission:1||Future applications:1||Photoemission measurements:1||Graphene:1||BANDSTRUCTURE:1||TC:1||superconductivity:1||magnetic semiconductors:1||CMRmanganites:1||thin films:1||spin dynamics:1||highTc superconductors:1||ITINERANTELECTRON FERROMAGNETISM:1||SINGLECRYSTALS:1||CeTe2:1||amorphous magnetic materials:1||EPITAXIAL GRAPHENE:1||LAYERED PNICTIDEOXIDES:1||BOROCARBIDE SUPERCONDUCTORS:1||AUGMENTEDWAVE METHOD:1||METALLIC MAGNET UNISN:1||ORIGIN:1||spectrum rearrangement:1||MEANFIELD THEORY:1||MOLECULEBASED MAGNETS:1||METASTABLE STATE:1||INSULATOR:1||magnetic orderin:1||FCC IRON:1||CeRu2:1||TL2MN2O7:1||isotope effect:1||Perovskitemanganites:1||RECURSION METHOD:1||PERPENDICULAR MAGNETICANISOTROPY:1||quasiparticle spectral density:1||GW:1||MANGANESE FERRITE:1||RESONANCE:1||SeCuO3:1||Optical conductivity:1||MASSLESS DIRAC FERMIONS:1||SCHOTTKYBARRIER:1||electronic structure:15||ELECTRONICSTRUCTURE:11||TRANSITIONMETAL COMPOUNDS:10||METALS:10||photoemission:8||SPECTRA:8||MAGNETORESISTANCE:7||FERROMAGNETISM:7||TRANSPORT:7||TRANSITION:6||FILMS:6||THINFILMS:5||TOTALENERGY CALCULATIONS:5||MAGNETICPROPERTIES:5||SUPERCONDUCTIVITY:5||PR:5||LATTICE:4||STATES:4||SPECTROSCOPY:4||FIELD:4||CRYSTALSTRUCTURE:4||PHOTOEMISSION:4||TEMPERATURE:4||TRANSITIONTEMPERATURE:4||XRAYABSORPTION:4||STATE:4||CU:4||BASISSET:4||XAS:4||CRYSTALS:3||EXCITATIONS:3||MOTTHUBBARD SYSTEMS:3||HIGHENERGY SPIN:3||halfmetal:3||INSULATORS:3||LA2CUO4:3||MODEL:3||FLUCTUATIONS:3||CE:3||double exchange:3||TRANSITIONMETALS:3||RESISTIVITY:3||BORON:3||LA1XCAXMNO3:3||IRON:3||PES:3||ANTIMONIDES:2||MgB2:2||ZR METALLIC GLASSES:2||superconductor:2||CRITICALCURRENT DENSITY:2||CIRCULARDICHROISM:2||SEMICONDUCTORS:2||LOCALIZATION:2||INTRABAND OPTICAL CONDUCTIVITY:2||COLOSSAL MAGNETORESISTANCE:2||OXIDATION:2||EXISTENCE:2||COPPER:2||diboride:2||MAGNESIUMDIBORIDE:2||GAP:2||CE COMPOUNDS:2||CORE POLARIZATION:2||magnetoresistance:2||photoemission spectroscopy:2||electronphonon interaction:2||GETTER:2||PD:2||MAGNETISM:2||FECR2S4:2||SUPERCONDUCTING MGB2:2||WIRES:2||ABSORPTION:2||ENERGY:2||LA1XSRXMNO3:2||CONSTANTS:2||polaron:2||charge ordering:2||SCATTERING:2||XRAY PHOTOEMISSION:2||CeNiSn:2||phase diagram:2||PHOTOELECTRON:2||QUADRUPOLAR:2||perovskitemanganites:2||CO:2||SYSTEMS:2||DOPED ZNO:2||LOWFREQUENCY SOUND:2||LA:2||ELECTRONELECTRON SCATTERING:2||AU:2||DENSITYWAVE INSTABILITY:2||FERMISURFACE:2||hybridization:2||VALENCEBAND SATELLITE:2||SULFUR SPINEL:2||Heusler:2||APPROXIMATION:2||superexchange:2||colossal magnetoresistance:2||ALLOYS:2||DEPENDENCE:2||AG:2||electronic structures:2||AUGERSPECTRA:2||CR:2||PARAMETERS:2||DIFFRACTION:2||SEMICONDUCTORMETAL TRANSITION:1||INTERMEDIATEVALENCE:1||SMB6:1||SRRUO3:1||antiperovskite structure with antipolar nature:1||lowenergy twodimensional phonons:1||anatase TiO2:1||La3S4:1||metalinsulator transitions:1||MNO:1||ELECTRONICSTRUCTURES:1||MAGNETIC CIRCULARDICHROISM:1||Density functional theory:1||CeCo2:1||TOPOLARON CROSSOVER:1||EXCHANGE:1||cuprates:1||high Tc cuprates:1||magnetically ordered materials:1||ZNSE:1||Sr2xKxFeMoO6:1||CDW:1||TeCuO3:1||STRUCTURALPROPERTIES:1||MN:1||screening length:1||amorphous Fe:1||WAVE BASISSET:1||SILICONCARBIDE:1||HIGHPRESSURE:1||electronphonon coupling:1||quenched superconductivity:1||CMR perovskite manganites:1||OXIDE:1||polarons:1||synchrotron radiation:1||FULLERIDES:1||RESONANTPHOTOEMISSION:1||Silicon carbide:1||DFT calculation:1||Hybridized bands:1||GIANT MAGNETORESISTANCE:1||PEROVSKITES:1||Raman spectra:1||EXCHANGE ENHANCEMENT:1||SILICON:1||SR2FEMOO6:1||orbital ordering:1||delafossite:1||TITANIUMDIOXIDE:1||electronic structure of disordered solids:1||YFE2:1||Magnetic polaron:1||NA2TI2SB2O:1||STRONGCOUPLED SUPERCONDUCTORS:1||HEAVYFERMION SYSTEMS:1||firstprinciples calculations:1||MECHANISM:1||UNiSn:1||PHOTONIC BANDGAP:1||SINGLE IMPURITY:1||PHONONSPECTRUM:1||FERMISURFACE TOPOLOGY:1||SUPPRESSION:1||RESONANT PHOTOEMISSION:1||METALDOPED PICENE:1||PHOTOIONIZATION CROSSSECTIONS:1||PHOTOINDUCED FERRIMAGNETIC SYSTEMS:1||LINKAGE ISOMERISM:1||CHARGETRANSFER:1||Bilayer Graphene:1||MAGNETICFIELD:1||SPINWAVES:1||rareearth manganese oxides:1||magnonphonon interaction:1||NACO2O4:1||ENERGYBANDS:1||SELFENERGY:1||GAS:1||Fe0.5Cu0.5Cr2S4:1||scanning photoelectron microscopy (SPEM):1||MAGNETIC PROPERTIES:1||Stoner model:1||AMORPHOUS TRANSITIONMETALS:1||SPINGLASS STATES:1||NI:1||LA3NI2B2N3:1||SOLIDS:1||CEO2:1||BAND THEORY:1||dilute magnetic semiconductor:1||pyrochlore:1||Y1XPRXBA2CU3O7DELTA:1||and electronphonon interactions:1||VIBRATIONS:1||RAY PHOTOEMISSION:1||ALKALI CATION:1||Europium:1||colossal magnetoresistance:1||structural stability:1||ENERGYGAP:1||small polaron:1||DOUBLE EXCHANGE:1||Coulomb correlation:1||magnon:1||phonons:1||ELECTRON FERROMAGNETISM:1||CURIETEMPERATURE:1||ARPES:1||PLANEWAVE METHOD:1||Xray absorption spectroscopy (XAS):1||ROOMTEMPERATURE:1||MONOCHALCOGENIDES:1||HEAT:1||UPDSN:1||MOMENTS:1||XRAY ABSORPTION:1||SEMICONDUCTOR:1||Fermi surface nesting:1||optical phonon:1||disordered system:1||dilute magnetic semiconductors:1||CMR manganites:1||PHONONS:1||LATTICEDYNAMICS:1||OXIDES:1||4fphotoemission:1||permanent magnet:1||pseudogap:1||TRANSPORTPROPERTIES:1||ANTIFERROMAGNET:1||(BI,PB)SRCOO SYSTEM:1||semicore correlation:1||POLARIZATION:1||CRYSTAL:1||spinel:1||Xray magnetic circular dichroism (XMCD):1||magnetocapacitance:1||ANATASE:1||TEMPERATURES:1||Pseudogap:1||INTERFACE:1||SUBSTRATE:1||YNI2B2C:1||SAMARIUM SULFIDE:1||strong swave superconductor:1||DOPED MANGANITE:1||SYMMETRY:1||CENISN:1||resonance mode:1||DISORDERED SYSTEM:1||LITHIUM INTERCALATION:1||CUO2 PLANE:1||SURFACE:1||Delafossite:1||ELECTRICALPROPERTIES:1||NIMNSB:1||PTMNSB:1||ROOMTEMPERATURE FERROMAGNETISM:1||RUBIDIUM MANGANESE HEXACYANOFERRATE:1||COLOSSALMAGNETORESISTANCE:1||FINITE TEMPERATURES:1||LAMNO3:1||FE:1||transitionmetal oxides:1||giant magnetoresistance:1||phonon:1||COPPER OXIDES:1||valence states:1||thermoelectric:1||semiconductor:1||CATION DISTRIBUTION:1||FeCr2S4:1||photoemission spectroscopy (PES):1||METALLIC FERROMAGNETISM:1||GRAPHITE:1||SUSCEPTIBILITY:1||UBE13:1||RCrSb3:1||band JahnTeller:1||Ce3S4:1||TiO2:1||PrBa2Cu3O7delta:1||UNTWINNED PRBA2CU3O7:1||AGNIO2:1||HALFMETALLIC FERROMAGNETS:1||CI:1||Energy gap:1||Photoemission:1||Future applications:1||Photoemission measurements:1||Graphene:1||BANDSTRUCTURE:1||TC:1||superconductivity:1||magnetic semiconductors:1||CMRmanganites:1||thin films:1||spin dynamics:1||highTc superconductors:1||ITINERANTELECTRON FERROMAGNETISM:1||SINGLECRYSTALS:1||CeTe2:1||amorphous magnetic materials:1||EPITAXIAL GRAPHENE:1||LAYERED PNICTIDEOXIDES:1||BOROCARBIDE SUPERCONDUCTORS:1||AUGMENTEDWAVE METHOD:1||METALLIC MAGNET UNISN:1||ORIGIN:1||spectrum rearrangement:1||MEANFIELD THEORY:1||MOLECULEBASED MAGNETS:1||METASTABLE STATE:1||INSULATOR:1||magnetic orderin:1||FCC IRON:1||CeRu2:1||TL2MN2O7:1||isotope effect:1||Perovskitemanganites:1||RECURSION METHOD:1||PERPENDICULAR MAGNETICANISOTROPY:1||quasiparticle spectral density:1||GW:1||MANGANESE FERRITE:1||RESONANCE:1||SeCuO3:1||Optical conductivity:1||MASSLESS DIRAC FERMIONS:1||SCHOTTKYBARRIER:1||electronic structure:15||ELECTRONICSTRUCTURE:11||TRANSITIONMETAL COMPOUNDS:10||METALS:10||photoemission:8||SPECTRA:8||MAGNETORESISTANCE:7||FERROMAGNETISM:7||TRANSPORT:7||TRANSITION:6||FILMS:6||THINFILMS:5||TOTALENERGY CALCULATIONS:5||MAGNETICPROPERTIES:5||SUPERCONDUCTIVITY:5||PR:5||LATTICE:4||STATES:4||SPECTROSCOPY:4||FIELD:4||CRYSTALSTRUCTURE:4||PHOTOEMISSION:4||TEMPERATURE:4||TRANSITIONTEMPERATURE:4||XRAYABSORPTION:4||STATE:4||CU:4||BASISSET:4||XAS:4||CRYSTALS:3||EXCITATIONS:3||MOTTHUBBARD SYSTEMS:3||HIGHENERGY SPIN:3||halfmetal:3||INSULATORS:3||LA2CUO4:3||MODEL:3||FLUCTUATIONS:3||CE:3||double exchange:3||TRANSITIONMETALS:3||RESISTIVITY:3||BORON:3||LA1XCAXMNO3:3||IRON:3||PES:3||ANTIMONIDES:2||MgB2:2||ZR METALLIC GLASSES:2||superconductor:2||CRITICALCURRENT DENSITY:2||CIRCULARDICHROISM:2||SEMICONDUCTORS:2||LOCALIZATION:2||INTRABAND OPTICAL CONDUCTIVITY:2||COLOSSAL MAGNETORESISTANCE:2||OXIDATION:2||EXISTENCE:2||COPPER:2||diboride:2||MAGNESIUMDIBORIDE:2||GAP:2||CE COMPOUNDS:2||CORE POLARIZATION:2||magnetoresistance:2||photoemission spectroscopy:2||electronphonon interaction:2||GETTER:2||PD:2||MAGNETISM:2||FECR2S4:2||SUPERCONDUCTING MGB2:2||WIRES:2||ABSORPTION:2||ENERGY:2||LA1XSRXMNO3:2||CONSTANTS:2||polaron:2||charge ordering:2||SCATTERING:2||XRAY PHOTOEMISSION:2||CeNiSn:2||phase diagram:2||PHOTOELECTRON:2||QUADRUPOLAR:2||perovskitemanganites:2||CO:2||SYSTEMS:2||DOPED ZNO:2||LOWFREQUENCY SOUND:2||LA:2||ELECTRONELECTRON SCATTERING:2||AU:2||DENSITYWAVE INSTABILITY:2||FERMISURFACE:2||hybridization:2||VALENCEBAND SATELLITE:2||SULFUR SPINEL:2||Heusler:2||APPROXIMATION:2||superexchange:2||colossal magnetoresistance:2||ALLOYS:2||DEPENDENCE:2||AG:2||electronic structures:2||AUGERSPECTRA:2||CR:2||PARAMETERS:2||DIFFRACTION:2||SEMICONDUCTORMETAL TRANSITION:1||INTERMEDIATEVALENCE:1||SMB6:1||SRRUO3:1||antiperovskite structure with antipolar nature:1||lowenergy twodimensional phonons:1||anatase TiO2:1||La3S4:1||metalinsulator transitions:1||MNO:1||ELECTRONICSTRUCTURES:1||MAGNETIC CIRCULARDICHROISM:1||Density functional theory:1||CeCo2:1||TOPOLARON CROSSOVER:1||EXCHANGE:1||cuprates:1||high Tc cuprates:1||magnetically ordered materials:1||ZNSE:1||Sr2xKxFeMoO6:1||CDW:1||TeCuO3:1||STRUCTURALPROPERTIES:1||MN:1||screening length:1||amorphous Fe:1||WAVE BASISSET:1||SILICONCARBIDE:1||HIGHPRESSURE:1||electronphonon coupling:1||quenched superconductivity:1||CMR perovskite manganites:1||OXIDE:1||polarons:1||synchrotron radiation:1||FULLERIDES:1||RESONANTPHOTOEMISSION:1||Silicon carbide:1||DFT calculation:1||Hybridized bands:1||GIANT MAGNETORESISTANCE:1||PEROVSKITES:1||Raman spectra:1||EXCHANGE ENHANCEMENT:1||SILICON:1||SR2FEMOO6:1||orbital ordering:1||delafossite:1||TITANIUMDIOXIDE:1||electronic structure of disordered solids:1||YFE2:1||Magnetic polaron:1||NA2TI2SB2O:1||STRONGCOUPLED SUPERCONDUCTORS:1||HEAVYFERMION SYSTEMS:1||firstprinciples calculations:1||MECHANISM:1||UNiSn:1||PHOTONIC BANDGAP:1||SINGLE IMPURITY:1||PHONONSPECTRUM:1||FERMISURFACE TOPOLOGY:1||SUPPRESSION:1||RESONANT PHOTOEMISSION:1||METALDOPED PICENE:1||PHOTOIONIZATION CROSSSECTIONS:1||PHOTOINDUCED FERRIMAGNETIC SYSTEMS:1||LINKAGE ISOMERISM:1||CHARGETRANSFER:1||Bilayer Graphene:1||MAGNETICFIELD:1||SPINWAVES:1||rareearth manganese oxides:1||magnonphonon interaction:1||NACO2O4:1||ENERGYBANDS:1||SELFENERGY:1||GAS:1||Fe0.5Cu0.5Cr2S4:1||scanning photoelectron microscopy (SPEM):1||MAGNETIC PROPERTIES:1||Stoner model:1||AMORPHOUS TRANSITIONMETALS:1||SPINGLASS STATES:1||NI:1||LA3NI2B2N3:1||SOLIDS:1||CEO2:1||BAND THEORY:1||dilute magnetic semiconductor:1||pyrochlore:1||Y1XPRXBA2CU3O7DELTA:1||and electronphonon interactions:1||VIBRATIONS:1||RAY PHOTOEMISSION:1||ALKALI CATION:1||Europium:1||colossal magnetoresistance:1||structural stability:1||ENERGYGAP:1||small polaron:1||DOUBLE EXCHANGE:1||Coulomb correlation:1||magnon:1||phonons:1||ELECTRON FERROMAGNETISM:1||CURIETEMPERATURE:1||ARPES:1||PLANEWAVE METHOD:1||Xray absorption spectroscopy (XAS):1||ROOMTEMPERATURE:1||MONOCHALCOGENIDES:1||HEAT:1||UPDSN:1||MOMENTS:1||XRAY ABSORPTION:1||SEMICONDUCTOR:1||Fermi surface nesting:1||optical phonon:1||disordered system:1||dilute magnetic semiconductors:1||CMR manganites:1||PHONONS:1||LATTICEDYNAMICS:1||OXIDES:1||4fphotoemission:1||permanent magnet:1||pseudogap:1||TRANSPORTPROPERTIES:1||ANTIFERROMAGNET:1||(BI,PB)SRCOO SYSTEM:1||semicore correlation:1||POLARIZATION:1||CRYSTAL:1||spinel:1||Xray magnetic circular dichroism (XMCD):1||magnetocapacitance:1||ANATASE:1||TEMPERATURES:1||Pseudogap:1||INTERFACE:1||SUBSTRATE:1||YNI2B2C:1||SAMARIUM SULFIDE:1||strong swave superconductor:1||DOPED MANGANITE:1||SYMMETRY:1||CENISN:1||resonance mode:1||DISORDERED SYSTEM:1||LITHIUM INTERCALATION:1||CUO2 PLANE:1||SURFACE:1||Delafossite:1||ELECTRICALPROPERTIES:1||NIMNSB:1||PTMNSB:1||ROOMTEMPERATURE FERROMAGNETISM:1||RUBIDIUM MANGANESE HEXACYANOFERRATE:1||COLOSSALMAGNETORESISTANCE:1||FINITE TEMPERATURES:1||LAMNO3:1||FE:1||transitionmetal oxides:1||giant magnetoresistance:1||phonon:1||COPPER OXIDES:1||valence states:1||thermoelectric:1||semiconductor:1||CATION DISTRIBUTION:1||FeCr2S4:1||photoemission spectroscopy (PES):1||METALLIC FERROMAGNETISM:1||GRAPHITE:1||SUSCEPTIBILITY:1||UBE13:1||RCrSb3:1||band JahnTeller:1||Ce3S4:1||TiO2:1||PrBa2Cu3O7delta:1||UNTWINNED PRBA2CU3O7:1||AGNIO2:1||HALFMETALLIC FERROMAGNETS:1||CI:1||Energy gap:1||Photoemission:1||Future applications:1||Photoemission measurements:1||Graphene:1||BANDSTRUCTURE:1||TC:1||superconductivity:1||magnetic semiconductors:1||CMRmanganites:1||thin films:1||spin dynamics:1||highTc superconductors:1||ITINERANTELECTRON FERROMAGNETISM:1||SINGLECRYSTALS:1||CeTe2:1||amorphous magnetic materials:1||EPITAXIAL GRAPHENE:1||LAYERED PNICTIDEOXIDES:1||BOROCARBIDE SUPERCONDUCTORS:1||AUGMENTEDWAVE METHOD:1||METALLIC MAGNET UNISN:1||ORIGIN:1||spectrum rearrangement:1||MEANFIELD THEORY:1||MOLECULEBASED MAGNETS:1||METASTABLE STATE:1||INSULATOR:1||magnetic orderin:1||FCC IRON:1||CeRu2:1||TL2MN2O7:1||isotope effect:1||Perovskitemanganites:1||RECURSION METHOD:1||PERPENDICULAR MAGNETICANISOTROPY:1||quasiparticle spectral density:1||GW:1||MANGANESE FERRITE:1||RESONANCE:1||SeCuO3:1||Optical conductivity:1||MASSLESS DIRAC FERMIONS:1||SCHOTTKYBARRIER:1||electronic structure:15||ELECTRONICSTRUCTURE:11||TRANSITIONMETAL COMPOUNDS:10||METALS:10||photoemission:8||SPECTRA:8||MAGNETORESISTANCE:7||FERROMAGNETISM:7||TRANSPORT:7||TRANSITION:6||FILMS:6||THINFILMS:5||TOTALENERGY CALCULATIONS:5||MAGNETICPROPERTIES:5||SUPERCONDUCTIVITY:5||PR:5||LATTICE:4||STATES:4||SPECTROSCOPY:4||FIELD:4||CRYSTALSTRUCTURE:4||PHOTOEMISSION:4||TEMPERATURE:4||TRANSITIONTEMPERATURE:4||XRAYABSORPTION:4||STATE:4||CU:4||BASISSET:4||XAS:4||CRYSTALS:3||EXCITATIONS:3||MOTTHUBBARD SYSTEMS:3||HIGHENERGY SPIN:3||halfmetal:3||INSULATORS:3||LA2CUO4:3||MODEL:3||FLUCTUATIONS:3||CE:3||double exchange:3||TRANSITIONMETALS:3||RESISTIVITY:3||BORON:3||LA1XCAXMNO3:3||IRON:3||PES:3||ANTIMONIDES:2||MgB2:2||ZR METALLIC GLASSES:2||superconductor:2||CRITICALCURRENT DENSITY:2||CIRCULARDICHROISM:2||SEMICONDUCTORS:2||LOCALIZATION:2||INTRABAND OPTICAL CONDUCTIVITY:2||COLOSSAL MAGNETORESISTANCE:2||OXIDATION:2||EXISTENCE:2||COPPER:2||diboride:2||MAGNESIUMDIBORIDE:2||GAP:2||CE COMPOUNDS:2||CORE POLARIZATION:2||magnetoresistance:2||photoemission spectroscopy:2||electronphonon interaction:2||GETTER:2||PD:2||MAGNETISM:2||FECR2S4:2||SUPERCONDUCTING MGB2:2||WIRES:2||ABSORPTION:2||ENERGY:2||LA1XSRXMNO3:2||CONSTANTS:2||polaron:2||charge ordering:2||SCATTERING:2||XRAY PHOTOEMISSION:2||CeNiSn:2||phase diagram:2||PHOTOELECTRON:2||QUADRUPOLAR:2||perovskitemanganites:2||CO:2||SYSTEMS:2||DOPED ZNO:2||LOWFREQUENCY SOUND:2||LA:2||ELECTRONELECTRON SCATTERING:2||AU:2||DENSITYWAVE INSTABILITY:2||FERMISURFACE:2||hybridization:2||VALENCEBAND SATELLITE:2||SULFUR SPINEL:2||Heusler:2||APPROXIMATION:2||superexchange:2||colossal magnetoresistance:2||ALLOYS:2||DEPENDENCE:2||AG:2||electronic structures:2||AUGERSPECTRA:2||CR:2||PARAMETERS:2||DIFFRACTION:2||SEMICONDUCTORMETAL TRANSITION:1||INTERMEDIATEVALENCE:1||SMB6:1||SRRUO3:1||antiperovskite structure with antipolar nature:1||lowenergy twodimensional phonons:1||anatase TiO2:1||La3S4:1||metalinsulator transitions:1||MNO:1||ELECTRONICSTRUCTURES:1||MAGNETIC CIRCULARDICHROISM:1||Density functional theory:1||CeCo2:1||TOPOLARON CROSSOVER:1||EXCHANGE:1||cuprates:1||high Tc cuprates:1||magnetically ordered materials:1||ZNSE:1||Sr2xKxFeMoO6:1||CDW:1||TeCuO3:1||STRUCTURALPROPERTIES:1||MN:1||screening length:1||amorphous Fe:1||WAVE BASISSET:1||SILICONCARBIDE:1||HIGHPRESSURE:1||electronphonon coupling:1||quenched superconductivity:1||CMR perovskite manganites:1||OXIDE:1||polarons:1||synchrotron radiation:1||FULLERIDES:1||RESONANTPHOTOEMISSION:1||Silicon carbide:1||DFT calculation:1||Hybridized bands:1||GIANT MAGNETORESISTANCE:1||PEROVSKITES:1||Raman spectra:1||EXCHANGE ENHANCEMENT:1||SILICON:1||SR2FEMOO6:1||orbital ordering:1||delafossite:1||TITANIUMDIOXIDE:1||electronic structure of disordered solids:1||YFE2:1||Magnetic polaron:1||NA2TI2SB2O:1||STRONGCOUPLED SUPERCONDUCTORS:1||HEAVYFERMION SYSTEMS:1||firstprinciples calculations:1||MECHANISM:1||UNiSn:1||PHOTONIC BANDGAP:1||SINGLE IMPURITY:1||PHONONSPECTRUM:1||FERMISURFACE TOPOLOGY:1||SUPPRESSION:1||RESONANT PHOTOEMISSION:1||METALDOPED PICENE:1||PHOTOIONIZATION CROSSSECTIONS:1||PHOTOINDUCED FERRIMAGNETIC SYSTEMS:1||LINKAGE ISOMERISM:1||CHARGETRANSFER:1||Bilayer Graphene:1||MAGNETICFIELD:1||SPINWAVES:1||rareearth manganese oxides:1||magnonphonon interaction:1||NACO2O4:1||ENERGYBANDS:1||SELFENERGY:1||GAS:1||Fe0.5Cu0.5Cr2S4:1||scanning photoelectron microscopy (SPEM):1||MAGNETIC PROPERTIES:1||Stoner model:1||AMORPHOUS TRANSITIONMETALS:1||SPINGLASS STATES:1||NI:1||LA3NI2B2N3:1||SOLIDS:1||CEO2:1||BAND THEORY:1||dilute magnetic semiconductor:1||pyrochlore:1||Y1XPRXBA2CU3O7DELTA:1||and electronphonon interactions:1||VIBRATIONS:1||RAY PHOTOEMISSION:1||ALKALI CATION:1||Europium:1||colossal magnetoresistance:1||structural stability:1||ENERGYGAP:1||small polaron:1||DOUBLE EXCHANGE:1||Coulomb correlation:1||magnon:1||phonons:1||ELECTRON FERROMAGNETISM:1||CURIETEMPERATURE:1||ARPES:1||PLANEWAVE METHOD:1||Xray absorption spectroscopy (XAS):1||ROOMTEMPERATURE:1||MONOCHALCOGENIDES:1||HEAT:1||UPDSN:1||MOMENTS:1||XRAY ABSORPTION:1||SEMICONDUCTOR:1||Fermi surface nesting:1||optical phonon:1||disordered system:1||dilute magnetic semiconductors:1||CMR manganites:1||PHONONS:1||LATTICEDYNAMICS:1||OXIDES:1||4fphotoemission:1||permanent magnet:1||pseudogap:1||TRANSPORTPROPERTIES:1||ANTIFERROMAGNET:1||(BI,PB)SRCOO SYSTEM:1||semicore correlation:1||POLARIZATION:1||CRYSTAL:1||spinel:1||Xray magnetic circular dichroism (XMCD):1||magnetocapacitance:1||ANATASE:1||TEMPERATURES:1||Pseudogap:1||INTERFACE:1||SUBSTRATE:1||YNI2B2C:1||SAMARIUM SULFIDE:1||strong swave superconductor:1||DOPED MANGANITE:1||SYMMETRY:1||CENISN:1||resonance mode:1||DISORDERED SYSTEM:1||LITHIUM INTERCALATION:1||CUO2 PLANE:1||SURFACE:1||Delafossite:1||ELECTRICALPROPERTIES:1||NIMNSB:1||PTMNSB:1||ROOMTEMPERATURE FERROMAGNETISM:1||RUBIDIUM MANGANESE HEXACYANOFERRATE:1||COLOSSALMAGNETORESISTANCE:1||FINITE TEMPERATURES:1||LAMNO3:1||FE:1||transitionmetal oxides:1||giant magnetoresistance:1||phonon:1||COPPER OXIDES:1||valence states:1||thermoelectric:1||semiconductor:1||CATION DISTRIBUTION:1||FeCr2S4:1||photoemission spectroscopy (PES):1||METALLIC FERROMAGNETISM:1||GRAPHITE:1||SUSCEPTIBILITY:1||UBE13:1||RCrSb3:1||band JahnTeller:1||Ce3S4:1||TiO2:1||PrBa2Cu3O7delta:1||UNTWINNED PRBA2CU3O7:1||AGNIO2:1||HALFMETALLIC FERROMAGNETS:1||CI:1||Energy gap:1||Photoemission:1||Future applications:1||Photoemission measurements:1||Graphene:1||BANDSTRUCTURE:1||TC:1||superconductivity:1||magnetic semiconductors:1||CMRmanganites:1||thin films:1||spin dynamics:1||highTc superconductors:1||ITINERANTELECTRON FERROMAGNETISM:1||SINGLECRYSTALS:1||CeTe2:1||amorphous magnetic materials:1||EPITAXIAL GRAPHENE:1||LAYERED PNICTIDEOXIDES:1||BOROCARBIDE SUPERCONDUCTORS:1||AUGMENTEDWAVE METHOD:1||METALLIC MAGNET UNISN:1||ORIGIN:1||spectrum rearrangement:1||MEANFIELD THEORY:1||MOLECULEBASED MAGNETS:1||METASTABLE STATE:1||INSULATOR:1||magnetic orderin:1||FCC IRON:1||CeRu2:1||TL2MN2O7:1||isotope effect:1||Perovskitemanganites:1||RECURSION METHOD:1||PERPENDICULAR MAGNETICANISOTROPY:1||quasiparticle spectral density:1||GW:1||MANGANESE FERRITE:1||RESONANCE:1||SeCuO3:1||Optical conductivity:1||MASSLESS DIRAC FERMIONS:1||SCHOTTKYBARRIER:1||electronic structure:15||ELECTRONICSTRUCTURE:11||TRANSITIONMETAL COMPOUNDS:10||METALS:10||photoemission:8||SPECTRA:8||MAGNETORESISTANCE:7||FERROMAGNETISM:7||TRANSPORT:7||TRANSITION:6||FILMS:6||THINFILMS:5||TOTALENERGY CALCULATIONS:5||MAGNETICPROPERTIES:5||SUPERCONDUCTIVITY:5||PR:5||LATTICE:4||STATES:4||SPECTROSCOPY:4||FIELD:4||CRYSTALSTRUCTURE:4||PHOTOEMISSION:4||TEMPERATURE:4||TRANSITIONTEMPERATURE:4||XRAYABSORPTION:4||STATE:4||CU:4||BASISSET:4||XAS:4||CRYSTALS:3||EXCITATIONS:3||MOTTHUBBARD SYSTEMS:3||HIGHENERGY SPIN:3||halfmetal:3||INSULATORS:3||LA2CUO4:3||MODEL:3||FLUCTUATIONS:3||CE:3||double exchange:3||TRANSITIONMETALS:3||RESISTIVITY:3||BORON:3||LA1XCAXMNO3:3||IRON:3||PES:3||ANTIMONIDES:2||MgB2:2||ZR METALLIC GLASSES:2||superconductor:2||CRITICALCURRENT DENSITY:2||CIRCULARDICHROISM:2||SEMICONDUCTORS:2||LOCALIZATION:2||INTRABAND OPTICAL CONDUCTIVITY:2||COLOSSAL MAGNETORESISTANCE:2||OXIDATION:2||EXISTENCE:2||COPPER:2||diboride:2||MAGNESIUMDIBORIDE:2||GAP:2||CE COMPOUNDS:2||CORE POLARIZATION:2||magnetoresistance:2||photoemission spectroscopy:2||electronphonon interaction:2||GETTER:2||PD:2||MAGNETISM:2||FECR2S4:2||SUPERCONDUCTING MGB2:2||WIRES:2||ABSORPTION:2||ENERGY:2||LA1XSRXMNO3:2||CONSTANTS:2||polaron:2||charge ordering:2||SCATTERING:2||XRAY PHOTOEMISSION:2||CeNiSn:2||phase diagram:2||PHOTOELECTRON:2||QUADRUPOLAR:2||perovskitemanganites:2||CO:2||SYSTEMS:2||DOPED ZNO:2||LOWFREQUENCY SOUND:2||LA:2||ELECTRONELECTRON SCATTERING:2||AU:2||DENSITYWAVE INSTABILITY:2||FERMISURFACE:2||hybridization:2||VALENCEBAND SATELLITE:2||SULFUR SPINEL:2||Heusler:2||APPROXIMATION:2||superexchange:2||colossal magnetoresistance:2||ALLOYS:2||DEPENDENCE:2||AG:2||electronic structures:2||AUGERSPECTRA:2||CR:2||PARAMETERS:2||DIFFRACTION:2||SEMICONDUCTORMETAL TRANSITION:1||INTERMEDIATEVALENCE:1||SMB6:1||SRRUO3:1||antiperovskite structure with antipolar nature:1||lowenergy twodimensional phonons:1||anatase TiO2:1||La3S4:1||metalinsulator transitions:1||MNO:1||ELECTRONICSTRUCTURES:1||MAGNETIC CIRCULARDICHROISM:1||Density functional theory:1||CeCo2:1||TOPOLARON CROSSOVER:1||EXCHANGE:1||cuprates:1||high Tc cuprates:1||magnetically ordered materials:1||ZNSE:1||Sr2xKxFeMoO6:1||CDW:1||TeCuO3:1||STRUCTURALPROPERTIES:1||MN:1||screening length:1||amorphous Fe:1||WAVE BASISSET:1||SILICONCARBIDE:1||HIGHPRESSURE:1||electronphonon coupling:1||quenched superconductivity:1||CMR perovskite manganites:1||OXIDE:1||polarons:1||synchrotron radiation:1||FULLERIDES:1||RESONANTPHOTOEMISSION:1||Silicon carbide:1||DFT calculation:1||Hybridized bands:1||GIANT MAGNETORESISTANCE:1||PEROVSKITES:1||Raman spectra:1||EXCHANGE ENHANCEMENT:1||SILICON:1||SR2FEMOO6:1||orbital ordering:1||delafossite:1||TITANIUMDIOXIDE:1||electronic structure of disordered solids:1||YFE2:1||Magnetic polaron:1||NA2TI2SB2O:1||STRONGCOUPLED SUPERCONDUCTORS:1||HEAVYFERMION SYSTEMS:1||firstprinciples calculations:1||MECHANISM:1||UNiSn:1||PHOTONIC BANDGAP:1||SINGLE IMPURITY:1||PHONONSPECTRUM:1||FERMISURFACE TOPOLOGY:1||SUPPRESSION:1||RESONANT PHOTOEMISSION:1||METALDOPED PICENE:1||PHOTOIONIZATION CROSSSECTIONS:1||PHOTOINDUCED FERRIMAGNETIC SYSTEMS:1||LINKAGE ISOMERISM:1||CHARGETRANSFER:1||Bilayer Graphene:1||MAGNETICFIELD:1||SPINWAVES:1||rareearth manganese oxides:1||magnonphonon interaction:1||NACO2O4:1||ENERGYBANDS:1||SELFENERGY:1||GAS:1||Fe0.5Cu0.5Cr2S4:1||scanning photoelectron microscopy (SPEM):1||MAGNETIC PROPERTIES:1||Stoner model:1||AMORPHOUS TRANSITIONMETALS:1||SPINGLASS STATES:1||NI:1||LA3NI2B2N3:1||SOLIDS:1||CEO2:1||BAND THEORY:1||dilute magnetic semiconductor:1||pyrochlore:1||Y1XPRXBA2CU3O7DELTA:1||and electronphonon interactions:1||VIBRATIONS:1||RAY PHOTOEMISSION:1||ALKALI CATION:1||Europium:1||colossal magnetoresistance:1||structural stability:1||ENERGYGAP:1||small polaron:1||DOUBLE EXCHANGE:1||Coulomb correlation:1||magnon:1||phonons:1||ELECTRON FERROMAGNETISM:1||CURIETEMPERATURE:1||ARPES:1||PLANEWAVE METHOD:1||Xray absorption spectroscopy (XAS):1||ROOMTEMPERATURE:1||MONOCHALCOGENIDES:1||HEAT:1||UPDSN:1||MOMENTS:1||XRAY ABSORPTION:1||SEMICONDUCTOR:1||Fermi surface nesting:1||optical phonon:1||disordered system:1||dilute magnetic semiconductors:1||CMR manganites:1||PHONONS:1||LATTICEDYNAMICS:1||OXIDES:1||4fphotoemission:1||permanent magnet:1||pseudogap:1||TRANSPORTPROPERTIES:1||ANTIFERROMAGNET:1||(BI,PB)SRCOO SYSTEM:1||semicore correlation:1||POLARIZATION:1||CRYSTAL:1||spinel:1||Xray magnetic circular dichroism (XMCD):1||magnetocapacitance:1||ANATASE:1||TEMPERATURES:1||Pseudogap:1||INTERFACE:1||SUBSTRATE:1||YNI2B2C:1||SAMARIUM SULFIDE:1||strong swave superconductor:1||DOPED MANGANITE:1||SYMMETRY:1||CENISN:1||resonance mode:1||DISORDERED SYSTEM:1||LITHIUM INTERCALATION:1||CUO2 PLANE:1||SURFACE:1||Delafossite:1||ELECTRICALPROPERTIES:1||NIMNSB:1||PTMNSB:1||ROOMTEMPERATURE FERROMAGNETISM:1||RUBIDIUM MANGANESE HEXACYANOFERRATE:1||COLOSSALMAGNETORESISTANCE:1||FINITE TEMPERATURES:1||LAMNO3:1||FE:1||transitionmetal oxides:1||giant magnetoresistance:1||phonon:1||COPPER OXIDES:1||valence states:1||thermoelectric:1||semiconductor:1||CATION DISTRIBUTION:1||FeCr2S4:1||photoemission spectroscopy (PES):1||METALLIC FERROMAGNETISM:1||GRAPHITE:1||SUSCEPTIBILITY:1||UBE13:1||RCrSb3:1||band JahnTeller:1||Ce3S4:1||TiO2:1||PrBa2Cu3O7delta:1||UNTWINNED PRBA2CU3O7:1||AGNIO2:1||HALFMETALLIC FERROMAGNETS:1||CI:1||Energy gap:1||Photoemission:1||Future applications:1||Photoemission measurements:1||Graphene:1||BANDSTRUCTURE:1||TC:1||superconductivity:1||magnetic semiconductors:1||CMRmanganites:1||thin films:1||spin dynamics:1||highTc superconductors:1||ITINERANTELECTRON FERROMAGNETISM:1||SINGLECRYSTALS:1||CeTe2:1||amorphous magnetic materials:1||EPITAXIAL GRAPHENE:1||LAYERED PNICTIDEOXIDES:1||BOROCARBIDE SUPERCONDUCTORS:1||AUGMENTEDWAVE METHOD:1||METALLIC MAGNET UNISN:1||ORIGIN:1||spectrum rearrangement:1||MEANFIELD THEORY:1||MOLECULEBASED MAGNETS:1||METASTABLE STATE:1||INSULATOR:1||magnetic orderin:1||FCC IRON:1||CeRu2:1||TL2MN2O7:1||isotope effect:1||Perovskitemanganites:1||RECURSION METHOD:1||PERPENDICULAR MAGNETICANISOTROPY:1||quasiparticle spectral density:1||GW:1||MANGANESE FERRITE:1||RESONANCE:1||SeCuO3:1||Optical conductivity:1||MASSLESS DIRAC FERMIONS:1||SCHOTTKYBARRIER:1||electronic structure:15||ELECTRONICSTRUCTURE:11||TRANSITIONMETAL COMPOUNDS:10||METALS:10||photoemission:8||SPECTRA:8||MAGNETORESISTANCE:7||FERROMAGNETISM:7||TRANSPORT:7||TRANSITION:6||FILMS:6||THINFILMS:5||TOTALENERGY CALCULATIONS:5||MAGNETICPROPERTIES:5||SUPERCONDUCTIVITY:5||PR:5||LATTICE:4||STATES:4||SPECTROSCOPY:4||FIELD:4||CRYSTALSTRUCTURE:4||PHOTOEMISSION:4||TEMPERATURE:4||TRANSITIONTEMPERATURE:4||XRAYABSORPTION:4||STATE:4||CU:4||BASISSET:4||XAS:4||CRYSTALS:3||EXCITATIONS:3||MOTTHUBBARD SYSTEMS:3||HIGHENERGY SPIN:3||halfmetal:3||INSULATORS:3||LA2CUO4:3||MODEL:3||FLUCTUATIONS:3||CE:3||double exchange:3||TRANSITIONMETALS:3||RESISTIVITY:3||BORON:3||LA1XCAXMNO3:3||IRON:3||PES:3||ANTIMONIDES:2||MgB2:2||ZR METALLIC GLASSES:2||superconductor:2||CRITICALCURRENT DENSITY:2||CIRCULARDICHROISM:2||SEMICONDUCTORS:2||LOCALIZATION:2||INTRABAND OPTICAL CONDUCTIVITY:2||COLOSSAL MAGNETORESISTANCE:2||OXIDATION:2||EXISTENCE:2||COPPER:2||diboride:2||MAGNESIUMDIBORIDE:2||GAP:2||CE COMPOUNDS:2||CORE POLARIZATION:2||magnetoresistance:2||photoemission spectroscopy:2||electronphonon interaction:2||GETTER:2||PD:2||MAGNETISM:2||FECR2S4:2||SUPERCONDUCTING MGB2:2||WIRES:2||ABSORPTION:2||ENERGY:2||LA1XSRXMNO3:2||CONSTANTS:2||polaron:2||charge ordering:2||SCATTERING:2||XRAY PHOTOEMISSION:2||CeNiSn:2||phase diagram:2||PHOTOELECTRON:2||QUADRUPOLAR:2||perovskitemanganites:2||CO:2||SYSTEMS:2||DOPED ZNO:2||LOWFREQUENCY SOUND:2||LA:2||ELECTRONELECTRON SCATTERING:2||AU:2||DENSITYWAVE INSTABILITY:2||FERMISURFACE:2||hybridization:2||VALENCEBAND SATELLITE:2||SULFUR SPINEL:2||Heusler:2||APPROXIMATION:2||superexchange:2||colossal magnetoresistance:2||ALLOYS:2||DEPENDENCE:2||AG:2||electronic structures:2||AUGERSPECTRA:2||CR:2||PARAMETERS:2||DIFFRACTION:2||SEMICONDUCTORMETAL TRANSITION:1||INTERMEDIATEVALENCE:1||SMB6:1||SRRUO3:1||antiperovskite structure with antipolar nature:1||lowenergy twodimensional phonons:1||anatase TiO2:1||La3S4:1||metalinsulator transitions:1||MNO:1||ELECTRONICSTRUCTURES:1||MAGNETIC CIRCULARDICHROISM:1||Density functional theory:1||CeCo2:1||TOPOLARON CROSSOVER:1||EXCHANGE:1||cuprates:1||high Tc cuprates:1||magnetically ordered materials:1||ZNSE:1||Sr2xKxFeMoO6:1||CDW:1||TeCuO3:1||STRUCTURALPROPERTIES:1||MN:1||screening length:1||amorphous Fe:1||WAVE BASISSET:1||SILICONCARBIDE:1||HIGHPRESSURE:1||electronphonon coupling:1||quenched superconductivity:1||CMR perovskite manganites:1||OXIDE:1||polarons:1||synchrotron radiation:1||FULLERIDES:1||RESONANTPHOTOEMISSION:1||Silicon carbide:1||DFT calculation:1||Hybridized bands:1||GIANT MAGNETORESISTANCE:1||PEROVSKITES:1||Raman spectra:1||EXCHANGE ENHANCEMENT:1||SILICON:1||SR2FEMOO6:1||orbital ordering:1||delafossite:1||TITANIUMDIOXIDE:1||electronic structure of disordered solids:1||YFE2:1||Magnetic polaron:1||NA2TI2SB2O:1||STRONGCOUPLED SUPERCONDUCTORS:1||HEAVYFERMION SYSTEMS:1||firstprinciples calculations:1||MECHANISM:1||UNiSn:1||PHOTONIC BANDGAP:1||SINGLE IMPURITY:1||PHONONSPECTRUM:1||FERMISURFACE TOPOLOGY:1||SUPPRESSION:1||RESONANT PHOTOEMISSION:1||METALDOPED PICENE:1||PHOTOIONIZATION CROSSSECTIONS:1||PHOTOINDUCED FERRIMAGNETIC SYSTEMS:1||LINKAGE ISOMERISM:1||CHARGETRANSFER:1||Bilayer Graphene:1||MAGNETICFIELD:1||SPINWAVES:1||rareearth manganese oxides:1||magnonphonon interaction:1||NACO2O4:1||ENERGYBANDS:1||SELFENERGY:1||GAS:1||Fe0.5Cu0.5Cr2S4:1||scanning photoelectron microscopy (SPEM):1||MAGNETIC PROPERTIES:1||Stoner model:1||AMORPHOUS TRANSITIONMETALS:1||SPINGLASS STATES:1||NI:1||LA3NI2B2N3:1||SOLIDS:1||CEO2:1||BAND THEORY:1||dilute magnetic semiconductor:1||pyrochlore:1||Y1XPRXBA2CU3O7DELTA:1||and electronphonon interactions:1||VIBRATIONS:1||RAY PHOTOEMISSION:1||ALKALI CATION:1||Europium:1||colossal magnetoresistance:1||structural stability:1||ENERGYGAP:1||small polaron:1||DOUBLE EXCHANGE:1||Coulomb correlation:1||magnon:1||phonons:1||ELECTRON FERROMAGNETISM:1||CURIETEMPERATURE:1||ARPES:1||PLANEWAVE METHOD:1||Xray absorption spectroscopy (XAS):1||ROOMTEMPERATURE:1||MONOCHALCOGENIDES:1||HEAT:1||UPDSN:1||MOMENTS:1||XRAY ABSORPTION:1||SEMICONDUCTOR:1||Fermi surface nesting:1||optical phonon:1||disordered system:1||dilute magnetic semiconductors:1||CMR manganites:1||PHONONS:1||LATTICEDYNAMICS:1||OXIDES:1||4fphotoemission:1||permanent magnet:1||pseudogap:1||TRANSPORTPROPERTIES:1||ANTIFERROMAGNET:1||(BI,PB)SRCOO SYSTEM:1||semicore correlation:1||POLARIZATION:1||CRYSTAL:1||spinel:1||Xray magnetic circular dichroism (XMCD):1||magnetocapacitance:1||ANATASE:1||TEMPERATURES:1||Pseudogap:1||INTERFACE:1||SUBSTRATE:1||YNI2B2C:1||SAMARIUM SULFIDE:1||strong swave superconductor:1||DOPED MANGANITE:1||SYMMETRY:1||CENISN:1||resonance mode:1||DISORDERED SYSTEM:1||LITHIUM INTERCALATION:1||CUO2 PLANE:1||SURFACE:1||Delafossite:1||ELECTRICALPROPERTIES:1||NIMNSB:1||PTMNSB:1||ROOMTEMPERATURE FERROMAGNETISM:1||RUBIDIUM MANGANESE HEXACYANOFERRATE:1||COLOSSALMAGNETORESISTANCE:1||FINITE TEMPERATURES:1||LAMNO3:1||FE:1||transitionmetal oxides:1||giant magnetoresistance:1||phonon:1||COPPER OXIDES:1||valence states:1||thermoelectric:1||semiconductor:1||CATION DISTRIBUTION:1||FeCr2S4:1||photoemission spectroscopy (PES):1||METALLIC FERROMAGNETISM:1||GRAPHITE:1||SUSCEPTIBILITY:1||UBE13:1||RCrSb3:1||band JahnTeller:1||Ce3S4:1||TiO2:1||PrBa2Cu3O7delta:1||UNTWINNED PRBA2CU3O7:1||AGNIO2:1||HALFMETALLIC FERROMAGNETS:1||CI:1||Energy gap:1||Photoemission:1||Future applications:1||Photoemission measurements:1||Graphene:1||BANDSTRUCTURE:1||TC:1||superconductivity:1||magnetic semiconductors:1||CMRmanganites:1||thin films:1||spin dynamics:1||highTc superconductors:1||ITINERANTELECTRON FERROMAGNETISM:1||SINGLECRYSTALS:1||CeTe2:1||amorphous magnetic materials:1||EPITAXIAL GRAPHENE:1||LAYERED PNICTIDEOXIDES:1||BOROCARBIDE SUPERCONDUCTORS:1||AUGMENTEDWAVE METHOD:1||METALLIC MAGNET UNISN:1||ORIGIN:1||spectrum rearrangement:1||MEANFIELD THEORY:1||MOLECULEBASED MAGNETS:1||METASTABLE STATE:1||INSULATOR:1||magnetic orderin:1||FCC IRON:1||CeRu2:1||TL2MN2O7:1||isotope effect:1||Perovskitemanganites:1||RECURSION METHOD:1||PERPENDICULAR MAGNETICANISOTROPY:1||quasiparticle spectral density:1||GW:1||MANGANESE FERRITE:1||RESONANCE:1||SeCuO3:1||Optical conductivity:1||MASSLESS DIRAC FERMIONS:1||SCHOTTKYBARRIER:1||electronic structure:15||ELECTRONICSTRUCTURE:11||TRANSITIONMETAL COMPOUNDS:10||METALS:10||photoemission:8||SPECTRA:8||MAGNETORESISTANCE:7||FERROMAGNETISM:7||TRANSPORT:7||TRANSITION:6||FILMS:6||THINFILMS:5||TOTALENERGY CALCULATIONS:5||MAGNETICPROPERTIES:5||SUPERCONDUCTIVITY:5||PR:5||LATTICE:4||STATES:4||SPECTROSCOPY:4||FIELD:4||CRYSTALSTRUCTURE:4||PHOTOEMISSION:4||TEMPERATURE:4||TRANSITIONTEMPERATURE:4||XRAYABSORPTION:4||STATE:4||CU:4||BASISSET:4||XAS:4||CRYSTALS:3||EXCITATIONS:3||MOTTHUBBARD SYSTEMS:3||HIGHENERGY SPIN:3||halfmetal:3||INSULATORS:3||LA2CUO4:3||MODEL:3||FLUCTUATIONS:3||CE:3||double exchange:3||TRANSITIONMETALS:3||RESISTIVITY:3||BORON:3||LA1XCAXMNO3:3||IRON:3||PES:3||ANTIMONIDES:2||MgB2:2||ZR METALLIC GLASSES:2||superconductor:2||CRITICALCURRENT DENSITY:2||CIRCULARDICHROISM:2||SEMICONDUCTORS:2||LOCALIZATION:2||INTRABAND OPTICAL CONDUCTIVITY:2||COLOSSAL MAGNETORESISTANCE:2||OXIDATION:2||EXISTENCE:2||COPPER:2||diboride:2||MAGNESIUMDIBORIDE:2||GAP:2||CE COMPOUNDS:2||CORE POLARIZATION:2||magnetoresistance:2||photoemission spectroscopy:2||electronphonon interaction:2||GETTER:2||PD:2||MAGNETISM:2||FECR2S4:2||SUPERCONDUCTING MGB2:2||WIRES:2||ABSORPTION:2||ENERGY:2||LA1XSRXMNO3:2||CONSTANTS:2||polaron:2||charge ordering:2||SCATTERING:2||XRAY PHOTOEMISSION:2||CeNiSn:2||phase diagram:2||PHOTOELECTRON:2||QUADRUPOLAR:2||perovskitemanganites:2||CO:2||SYSTEMS:2||DOPED ZNO:2||LOWFREQUENCY SOUND:2||LA:2||ELECTRONELECTRON SCATTERING:2||AU:2||DENSITYWAVE INSTABILITY:2||FERMISURFACE:2||hybridization:2||VALENCEBAND SATELLITE:2||SULFUR SPINEL:2||Heusler:2||APPROXIMATION:2||superexchange:2||colossal magnetoresistance:2||ALLOYS:2||DEPENDENCE:2||AG:2||electronic structures:2||AUGERSPECTRA:2||CR:2||PARAMETERS:2||DIFFRACTION:2||SEMICONDUCTORMETAL TRANSITION:1||INTERMEDIATEVALENCE:1||SMB6:1||SRRUO3:1||antiperovskite structure with antipolar nature:1||lowenergy twodimensional phonons:1||anatase TiO2:1||La3S4:1||metalinsulator transitions:1||MNO:1||ELECTRONICSTRUCTURES:1||MAGNETIC CIRCULARDICHROISM:1||Density functional theory:1||CeCo2:1||TOPOLARON CROSSOVER:1||EXCHANGE:1||cuprates:1||high Tc cuprates:1||magnetically ordered materials:1||ZNSE:1||Sr2xKxFeMoO6:1||CDW:1||TeCuO3:1||STRUCTURALPROPERTIES:1||MN:1||screening length:1||amorphous Fe:1||WAVE BASISSET:1||SILICONCARBIDE:1||HIGHPRESSURE:1||electronphonon coupling:1||quenched superconductivity:1||CMR perovskite manganites:1||OXIDE:1||polarons:1||synchrotron radiation:1||FULLERIDES:1||RESONANTPHOTOEMISSION:1||Silicon carbide:1||DFT calculation:1||Hybridized bands:1||GIANT MAGNETORESISTANCE:1||PEROVSKITES:1||Raman spectra:1||EXCHANGE ENHANCEMENT:1||SILICON:1||SR2FEMOO6:1||orbital ordering:1||delafossite:1||TITANIUMDIOXIDE:1||electronic structure of disordered solids:1||YFE2:1||Magnetic polaron:1||NA2TI2SB2O:1||STRONGCOUPLED SUPERCONDUCTORS:1||HEAVYFERMION SYSTEMS:1||firstprinciples calculations:1||MECHANISM:1||UNiSn:1||PHOTONIC BANDGAP:1||SINGLE IMPURITY:1||PHONONSPECTRUM:1||FERMISURFACE TOPOLOGY:1||SUPPRESSION:1||RESONANT PHOTOEMISSION:1||METALDOPED PICENE:1||PHOTOIONIZATION CROSSSECTIONS:1||PHOTOINDUCED FERRIMAGNETIC SYSTEMS:1||LINKAGE ISOMERISM:1||CHARGETRANSFER:1||Bilayer Graphene:1||MAGNETICFIELD:1||SPINWAVES:1||rareearth manganese oxides:1||magnonphonon interaction:1||NACO2O4:1||ENERGYBANDS:1||SELFENERGY:1||GAS:1||Fe0.5Cu0.5Cr2S4:1||scanning photoelectron microscopy (SPEM):1||MAGNETIC PROPERTIES:1||Stoner model:1||AMORPHOUS TRANSITIONMETALS:1||SPINGLASS STATES:1||NI:1||LA3NI2B2N3:1||SOLIDS:1||CEO2:1||BAND THEORY:1||dilute magnetic semiconductor:1||pyrochlore:1||Y1XPRXBA2CU3O7DELTA:1||and electronphonon interactions:1||VIBRATIONS:1||RAY PHOTOEMISSION:1||ALKALI CATION:1||Europium:1||colossal magnetoresistance:1||structural stability:1||ENERGYGAP:1||small polaron:1||DOUBLE EXCHANGE:1||Coulomb correlation:1||magnon:1||phonons:1||ELECTRON FERROMAGNETISM:1||CURIETEMPERATURE:1||ARPES:1||PLANEWAVE METHOD:1||Xray absorption spectroscopy (XAS):1||ROOMTEMPERATURE:1||MONOCHALCOGENIDES:1||HEAT:1||UPDSN:1||MOMENTS:1||XRAY ABSORPTION:1||SEMICONDUCTOR:1||Fermi surface nesting:1||optical phonon:1||disordered system:1||dilute magnetic semiconductors:1||CMR manganites:1||PHONONS:1||LATTICEDYNAMICS:1||OXIDES:1||4fphotoemission:1||permanent magnet:1||pseudogap:1||TRANSPORTPROPERTIES:1||ANTIFERROMAGNET:1||(BI,PB)SRCOO SYSTEM:1||semicore correlation:1||POLARIZATION:1||CRYSTAL:1||spinel:1||Xray magnetic circular dichroism (XMCD):1||magnetocapacitance:1||ANATASE:1||TEMPERATURES:1||Pseudogap:1||INTERFACE:1||SUBSTRATE:1||YNI2B2C:1||SAMARIUM SULFIDE:1||strong swave superconductor:1||DOPED MANGANITE:1||SYMMETRY:1||CENISN:1||resonance mode:1||DISORDERED SYSTEM:1||LITHIUM INTERCALATION:1||CUO2 PLANE:1||SURFACE:1||Delafossite:1||ELECTRICALPROPERTIES:1||NIMNSB:1||PTMNSB:1||ROOMTEMPERATURE FERROMAGNETISM:1||RUBIDIUM MANGANESE HEXACYANOFERRATE:1||COLOSSALMAGNETORESISTANCE:1||FINITE TEMPERATURES:1||LAMNO3:1||FE:1||transitionmetal oxides:1||giant magnetoresistance:1||phonon:1||COPPER OXIDES:1||valence states:1||thermoelectric:1||semiconductor:1||CATION DISTRIBUTION:1||FeCr2S4:1||photoemission spectroscopy (PES):1||METALLIC FERROMAGNETISM:1||GRAPHITE:1||SUSCEPTIBILITY:1||UBE13:1||RCrSb3:1||band JahnTeller:1||Ce3S4:1||TiO2:1||PrBa2Cu3O7delta:1||UNTWINNED PRBA2CU3O7:1||AGNIO2:1||HALFMETALLIC FERROMAGNETS:1||CI:1||Energy gap:1||Photoemission:1||Future applications:1||Photoemission measurements:1||Graphene:1||BANDSTRUCTURE:1||TC:1||superconductivity:1||magnetic semiconductors:1||CMRmanganites:1||thin films:1||spin dynamics:1||highTc superconductors:1||ITINERANTELECTRON FERROMAGNETISM:1||SINGLECRYSTALS:1||CeTe2:1||amorphous magnetic materials:1||EPITAXIAL GRAPHENE:1||LAYERED PNICTIDEOXIDES:1||BOROCARBIDE SUPERCONDUCTORS:1||AUGMENTEDWAVE METHOD:1||METALLIC MAGNET UNISN:1||ORIGIN:1||spectrum rearrangement:1||MEANFIELD THEORY:1||MOLECULEBASED MAGNETS:1||METASTABLE STATE:1||INSULATOR:1||magnetic orderin:1||FCC IRON:1||CeRu2:1||TL2MN2O7:1||isotope effect:1||Perovskitemanganites:1||RECURSION METHOD:1||PERPENDICULAR MAGNETICANISOTROPY:1||quasiparticle spectral density:1||GW:1||MANGANESE FERRITE:1||RESONANCE:1||SeCuO3:1||Optical conductivity:1||MASSLESS DIRAC FERMIONS:1||SCHOTTKYBARRIER:1||electronic structure:15||ELECTRONICSTRUCTURE:11||TRANSITIONMETAL COMPOUNDS:10||METALS:10||photoemission:8||SPECTRA:8||MAGNETORESISTANCE:7||FERROMAGNETISM:7||TRANSPORT:7||TRANSITION:6||FILMS:6||THINFILMS:5||TOTALENERGY CALCULATIONS:5||MAGNETICPROPERTIES:5||SUPERCONDUCTIVITY:5||PR:5||LATTICE:4||STATES:4||SPECTROSCOPY:4||FIELD:4||CRYSTALSTRUCTURE:4||PHOTOEMISSION:4||TEMPERATURE:4||TRANSITIONTEMPERATURE:4||XRAYABSORPTION:4||STATE:4||CU:4||BASISSET:4||XAS:4||CRYSTALS:3||EXCITATIONS:3||MOTTHUBBARD SYSTEMS:3||HIGHENERGY SPIN:3||halfmetal:3||INSULATORS:3||LA2CUO4:3||MODEL:3||FLUCTUATIONS:3||CE:3||double exchange:3||TRANSITIONMETALS:3||RESISTIVITY:3||BORON:3||LA1XCAXMNO3:3||IRON:3||PES:3||ANTIMONIDES:2||MgB2:2||ZR METALLIC GLASSES:2||superconductor:2||CRITICALCURRENT DENSITY:2||CIRCULARDICHROISM:2||SEMICONDUCTORS:2||LOCALIZATION:2||INTRABAND OPTICAL CONDUCTIVITY:2||COLOSSAL MAGNETORESISTANCE:2||OXIDATION:2||EXISTENCE:2||COPPER:2||diboride:2||MAGNESIUMDIBORIDE:2||GAP:2||CE COMPOUNDS:2||CORE POLARIZATION:2||magnetoresistance:2||photoemission spectroscopy:2||electronphonon interaction:2||GETTER:2||PD:2||MAGNETISM:2||FECR2S4:2||SUPERCONDUCTING MGB2:2||WIRES:2||ABSORPTION:2||ENERGY:2||LA1XSRXMNO3:2||CONSTANTS:2||polaron:2||charge ordering:2||SCATTERING:2||XRAY PHOTOEMISSION:2||CeNiSn:2||phase diagram:2||PHOTOELECTRON:2||QUADRUPOLAR:2||perovskitemanganites:2||CO:2||SYSTEMS:2||DOPED ZNO:2||LOWFREQUENCY SOUND:2||LA:2||ELECTRONELECTRON SCATTERING:2||AU:2||DENSITYWAVE INSTABILITY:2||FERMISURFACE:2||hybridization:2||VALENCEBAND SATELLITE:2||SULFUR SPINEL:2||Heusler:2||APPROXIMATION:2||superexchange:2||colossal magnetoresistance:2||ALLOYS:2||DEPENDENCE:2||AG:2||electronic structures:2||AUGERSPECTRA:2||CR:2||PARAMETERS:2||DIFFRACTION:2||SEMICONDUCTORMETAL TRANSITION:1||INTERMEDIATEVALENCE:1||SMB6:1||SRRUO3:1||antiperovskite structure with antipolar nature:1||lowenergy twodimensional phonons:1||anatase TiO2:1||La3S4:1||metalinsulator transitions:1||MNO:1||ELECTRONICSTRUCTURES:1||MAGNETIC CIRCULARDICHROISM:1||Density functional theory:1||CeCo2:1||TOPOLARON CROSSOVER:1||EXCHANGE:1||cuprates:1||high Tc cuprates:1||magnetically ordered materials:1||ZNSE:1||Sr2xKxFeMoO6:1||CDW:1||TeCuO3:1||STRUCTURALPROPERTIES:1||MN:1||screening length:1||amorphous Fe:1||WAVE BASISSET:1||SILICONCARBIDE:1||HIGHPRESSURE:1||electronphonon coupling:1||quenched superconductivity:1||CMR perovskite manganites:1||OXIDE:1||polarons:1||synchrotron radiation:1||FULLERIDES:1||RESONANTPHOTOEMISSION:1||Silicon carbide:1||DFT calculation:1||Hybridized bands:1||GIANT MAGNETORESISTANCE:1||PEROVSKITES:1||Raman spectra:1||EXCHANGE ENHANCEMENT:1||SILICON:1||SR2FEMOO6:1||orbital ordering:1||delafossite:1||TITANIUMDIOXIDE:1||electronic structure of disordered solids:1||YFE2:1||Magnetic polaron:1||NA2TI2SB2O:1||STRONGCOUPLED SUPERCONDUCTORS:1||HEAVYFERMION SYSTEMS:1||firstprinciples calculations:1||MECHANISM:1||UNiSn:1||PHOTONIC BANDGAP:1||SINGLE IMPURITY:1||PHONONSPECTRUM:1||FERMISURFACE TOPOLOGY:1||SUPPRESSION:1||RESONANT PHOTOEMISSION:1||METALDOPED PICENE:1||PHOTOIONIZATION CROSSSECTIONS:1||PHOTOINDUCED FERRIMAGNETIC SYSTEMS:1||LINKAGE ISOMERISM:1||CHARGETRANSFER:1||Bilayer Graphene:1||MAGNETICFIELD:1||SPINWAVES:1||rareearth manganese oxides:1||magnonphonon interaction:1||NACO2O4:1||ENERGYBANDS:1||SELFENERGY:1||GAS:1||Fe0.5Cu0.5Cr2S4:1||scanning photoelectron microscopy (SPEM):1||MAGNETIC PROPERTIES:1||Stoner model:1||AMORPHOUS TRANSITIONMETALS:1||SPINGLASS STATES:1||NI:1||LA3NI2B2N3:1||SOLIDS:1||CEO2:1||BAND THEORY:1||dilute magnetic semiconductor:1||pyrochlore:1||Y1XPRXBA2CU3O7DELTA:1||and electronphonon interactions:1||VIBRATIONS:1||RAY PHOTOEMISSION:1||ALKALI CATION:1||Europium:1||colossal magnetoresistance:1||structural stability:1||ENERGYGAP:1||small polaron:1||DOUBLE EXCHANGE:1||Coulomb correlation:1||magnon:1||phonons:1||ELECTRON FERROMAGNETISM:1||CURIETEMPERATURE:1||ARPES:1||PLANEWAVE METHOD:1||Xray absorption spectroscopy (XAS):1||ROOMTEMPERATURE:1||MONOCHALCOGENIDES:1||HEAT:1||UPDSN:1||MOMENTS:1||XRAY ABSORPTION:1||SEMICONDUCTOR:1||Fermi surface nesting:1||optical phonon:1||disordered system:1||dilute magnetic semiconductors:1||CMR manganites:1||PHONONS:1||LATTICEDYNAMICS:1||OXIDES:1||4fphotoemission:1||permanent magnet:1||pseudogap:1||TRANSPORTPROPERTIES:1||ANTIFERROMAGNET:1||(BI,PB)SRCOO SYSTEM:1||semicore correlation:1||POLARIZATION:1||CRYSTAL:1||spinel:1||Xray magnetic circular dichroism (XMCD):1||magnetocapacitance:1||ANATASE:1||TEMPERATURES:1||Pseudogap:1||INTERFACE:1||SUBSTRATE:1||YNI2B2C:1||SAMARIUM SULFIDE:1||strong swave superconductor:1||DOPED MANGANITE:1||SYMMETRY:1||CENISN:1||resonance mode:1||DISORDERED SYSTEM:1||LITHIUM INTERCALATION:1||CUO2 PLANE:1||SURFACE:1||Delafossite:1||ELECTRICALPROPERTIES:1||NIMNSB:1||PTMNSB:1||ROOMTEMPERATURE FERROMAGNETISM:1||RUBIDIUM MANGANESE HEXACYANOFERRATE:1||COLOSSALMAGNETORESISTANCE:1||FINITE TEMPERATURES:1||LAMNO3:1||FE:1||transitionmetal oxides:1||giant magnetoresistance:1||phonon:1||COPPER OXIDES:1||valence states:1||thermoelectric:1||semiconductor:1||CATION DISTRIBUTION:1||FeCr2S4:1||photoemission spectroscopy (PES):1||METALLIC FERROMAGNETISM:1||GRAPHITE:1||SUSCEPTIBILITY:1||UBE13:1||RCrSb3:1||band JahnTeller:1||Ce3S4:1||TiO2:1||PrBa2Cu3O7delta:1||UNTWINNED PRBA2CU3O7:1||AGNIO2:1||HALFMETALLIC FERROMAGNETS:1||CI:1||Energy gap:1||Photoemission:1||Future applications:1||Photoemission measurements:1||Graphene:1||BANDSTRUCTURE:1||TC:1||superconductivity:1||magnetic semiconductors:1||CMRmanganites:1||thin films:1||spin dynamics:1||highTc superconductors:1||ITINERANTELECTRON FERROMAGNETISM:1||SINGLECRYSTALS:1||CeTe2:1||amorphous magnetic materials:1||EPITAXIAL GRAPHENE:1||LAYERED PNICTIDEOXIDES:1||BOROCARBIDE SUPERCONDUCTORS:1||AUGMENTEDWAVE METHOD:1||METALLIC MAGNET UNISN:1||ORIGIN:1||spectrum rearrangement:1||MEANFIELD THEORY:1||MOLECULEBASED MAGNETS:1||METASTABLE STATE:1||INSULATOR:1||magnetic orderin:1||FCC IRON:1||CeRu2:1||TL2MN2O7:1||isotope effect:1||Perovskitemanganites:1||RECURSION METHOD:1||PERPENDICULAR MAGNETICANISOTROPY:1||quasiparticle spectral density:1||GW:1||MANGANESE FERRITE:1||RESONANCE:1||SeCuO3:1||Optical conductivity:1||MASSLESS DIRAC FERMIONS:1||SCHOTTKYBARRIER:1||electronic structure:15||ELECTRONICSTRUCTURE:11||TRANSITIONMETAL COMPOUNDS:10||METALS:10||photoemission:8||SPECTRA:8||MAGNETORESISTANCE:7||FERROMAGNETISM:7||TRANSPORT:7||TRANSITION:6||FILMS:6||THINFILMS:5||TOTALENERGY CALCULATIONS:5||MAGNETICPROPERTIES:5||SUPERCONDUCTIVITY:5||PR:5||LATTICE:4||STATES:4||SPECTROSCOPY:4||FIELD:4||CRYSTALSTRUCTURE:4||PHOTOEMISSION:4||TEMPERATURE:4||TRANSITIONTEMPERATURE:4||XRAYABSORPTION:4||STATE:4||CU:4||BASISSET:4||XAS:4||CRYSTALS:3||EXCITATIONS:3||MOTTHUBBARD SYSTEMS:3||HIGHENERGY SPIN:3||halfmetal:3||INSULATORS:3||LA2CUO4:3||MODEL:3||FLUCTUATIONS:3||CE:3||double exchange:3||TRANSITIONMETALS:3||RESISTIVITY:3||BORON:3||LA1XCAXMNO3:3||IRON:3||PES:3||ANTIMONIDES:2||MgB2:2||ZR METALLIC GLASSES:2||superconductor:2||CRITICALCURRENT DENSITY:2||CIRCULARDICHROISM:2||SEMICONDUCTORS:2||LOCALIZATION:2||INTRABAND OPTICAL CONDUCTIVITY:2||COLOSSAL MAGNETORESISTANCE:2||OXIDATION:2||EXISTENCE:2||COPPER:2||diboride:2||MAGNESIUMDIBORIDE:2||GAP:2||CE COMPOUNDS:2||CORE POLARIZATION:2||magnetoresistance:2||photoemission spectroscopy:2||electronphonon interaction:2||GETTER:2||PD:2||MAGNETISM:2||FECR2S4:2||SUPERCONDUCTING MGB2:2||WIRES:2||ABSORPTION:2||ENERGY:2||LA1XSRXMNO3:2||CONSTANTS:2||polaron:2||charge ordering:2||SCATTERING:2||XRAY PHOTOEMISSION:2||CeNiSn:2||phase diagram:2||PHOTOELECTRON:2||QUADRUPOLAR:2||perovskitemanganites:2||CO:2||SYSTEMS:2||DOPED ZNO:2||LOWFREQUENCY SOUND:2||LA:2||ELECTRONELECTRON SCATTERING:2||AU:2||DENSITYWAVE INSTABILITY:2||FERMISURFACE:2||hybridization:2||VALENCEBAND SATELLITE:2||SULFUR SPINEL:2||Heusler:2||APPROXIMATION:2||superexchange:2||colossal magnetoresistance:2||ALLOYS:2||DEPENDENCE:2||AG:2||electronic structures:2||AUGERSPECTRA:2||CR:2||PARAMETERS:2||DIFFRACTION:2||SEMICONDUCTORMETAL TRANSITION:1||INTERMEDIATEVALENCE:1||SMB6:1||SRRUO3:1||antiperovskite structure with antipolar nature:1||lowenergy twodimensional phonons:1||anatase TiO2:1||La3S4:1||metalinsulator transitions:1||MNO:1||ELECTRONICSTRUCTURES:1||MAGNETIC CIRCULARDICHROISM:1||Density functional theory:1||CeCo2:1||TOPOLARON CROSSOVER:1||EXCHANGE:1||cuprates:1||high Tc cuprates:1||magnetically ordered materials:1||ZNSE:1||Sr2xKxFeMoO6:1||CDW:1||TeCuO3:1||STRUCTURALPROPERTIES:1||MN:1||screening length:1||amorphous Fe:1||WAVE BASISSET:1||SILICONCARBIDE:1||HIGHPRESSURE:1||electronphonon coupling:1||quenched superconductivity:1||CMR perovskite manganites:1||OXIDE:1||polarons:1||synchrotron radiation:1||FULLERIDES:1||RESONANTPHOTOEMISSION:1||Silicon carbide:1||DFT calculation:1||Hybridized bands:1||GIANT MAGNETORESISTANCE:1||PEROVSKITES:1||Raman spectra:1||EXCHANGE ENHANCEMENT:1||SILICON:1||SR2FEMOO6:1||orbital ordering:1||delafossite:1||TITANIUMDIOXIDE:1||electronic structure of disordered solids:1||YFE2:1||Magnetic polaron:1||NA2TI2SB2O:1||STRONGCOUPLED SUPERCONDUCTORS:1||HEAVYFERMION SYSTEMS:1||firstprinciples calculations:1||MECHANISM:1||UNiSn:1||PHOTONIC BANDGAP:1||SINGLE IMPURITY:1||PHONONSPECTRUM:1||FERMISURFACE TOPOLOGY:1||SUPPRESSION:1||RESONANT PHOTOEMISSION:1||METALDOPED PICENE:1||PHOTOIONIZATION CROSSSECTIONS:1||PHOTOINDUCED FERRIMAGNETIC SYSTEMS:1||LINKAGE ISOMERISM:1||CHARGETRANSFER:1||Bilayer Graphene:1||MAGNETICFIELD:1||SPINWAVES:1||rareearth manganese oxides:1||magnonphonon interaction:1||NACO2O4:1||ENERGYBANDS:1||SELFENERGY:1||GAS:1||Fe0.5Cu0.5Cr2S4:1||scanning photoelectron microscopy (SPEM):1||MAGNETIC PROPERTIES:1||Stoner model:1||AMORPHOUS TRANSITIONMETALS:1||SPINGLASS STATES:1||NI:1||LA3NI2B2N3:1||SOLIDS:1||CEO2:1||BAND THEORY:1||dilute magnetic semiconductor:1||pyrochlore:1||Y1XPRXBA2CU3O7DELTA:1||and electronphonon interactions:1||VIBRATIONS:1||RAY PHOTOEMISSION:1||ALKALI CATION:1||Europium:1||colossal magnetoresistance:1||structural stability:1||ENERGYGAP:1||small polaron:1||DOUBLE EXCHANGE:1||Coulomb correlation:1||magnon:1||phonons:1||ELECTRON FERROMAGNETISM:1||CURIETEMPERATURE:1||ARPES:1||PLANEWAVE METHOD:1||Xray absorption spectroscopy (XAS):1||ROOMTEMPERATURE:1||MONOCHALCOGENIDES:1||HEAT:1||UPDSN:1||MOMENTS:1||XRAY ABSORPTION:1||SEMICONDUCTOR:1||Fermi surface nesting:1||optical phonon:1||disordered system:1||dilute magnetic semiconductors:1||CMR manganites:1||PHONONS:1||LATTICEDYNAMICS:1||OXIDES:1||4fphotoemission:1||permanent magnet:1||pseudogap:1||TRANSPORTPROPERTIES:1||ANTIFERROMAGNET:1||(BI,PB)SRCOO SYSTEM:1||semicore correlation:1||POLARIZATION:1||CRYSTAL:1||spinel:1||Xray magnetic circular dichroism (XMCD):1||magnetocapacitance:1||ANATASE:1||TEMPERATURES:1||Pseudogap:1||INTERFACE:1||SUBSTRATE:1||YNI2B2C:1||SAMARIUM SULFIDE:1||strong swave superconductor:1||DOPED MANGANITE:1||SYMMETRY:1||CENISN:1||resonance mode:1||DISORDERED SYSTEM:1||LITHIUM INTERCALATION:1||CUO2 PLANE:1||SURFACE:1||Delafossite:1||ELECTRICALPROPERTIES:1||NIMNSB:1||PTMNSB:1||ROOMTEMPERATURE FERROMAGNETISM:1||RUBIDIUM MANGANESE HEXACYANOFERRATE:1||COLOSSALMAGNETORESISTANCE:1||FINITE TEMPERATURES:1||LAMNO3:1||FE:1||transitionmetal oxides:1||giant magnetoresistance:1||phonon:1||COPPER OXIDES:1||valence states:1||thermoelectric:1||semiconductor:1||CATION DISTRIBUTION:1||FeCr2S4:1||photoemission spectroscopy (PES):1||METALLIC FERROMAGNETISM:1||GRAPHITE:1||SUSCEPTIBILITY:1||UBE13:1||RCrSb3:1||band JahnTeller:1||Ce3S4:1||TiO2:1||PrBa2Cu3O7delta:1||UNTWINNED PRBA2CU3O7:1||AGNIO2:1||HALFMETALLIC FERROMAGNETS:1||CI:1||Energy gap:1||Photoemission:1||Future applications:1||Photoemission measurements:1||Graphene:1||BANDSTRUCTURE:1||TC:1||superconductivity:1||magnetic semiconductors:1||CMRmanganites:1||thin films:1||spin dynamics:1||highTc superconductors:1||ITINERANTELECTRON FERROMAGNETISM:1||SINGLECRYSTALS:1||CeTe2:1||amorphous magnetic materials:1||EPITAXIAL GRAPHENE:1||LAYERED PNICTIDEOXIDES:1||BOROCARBIDE SUPERCONDUCTORS:1||AUGMENTEDWAVE METHOD:1||METALLIC MAGNET UNISN:1||ORIGIN:1||spectrum rearrangement:1||MEANFIELD THEORY:1||MOLECULEBASED MAGNETS:1||METASTABLE STATE:1||INSULATOR:1||magnetic orderin:1||FCC IRON:1||CeRu2:1||TL2MN2O7:1||isotope effect:1||Perovskitemanganites:1||RECURSION METHOD:1||PERPENDICULAR MAGNETICANISOTROPY:1||quasiparticle spectral density:1||GW:1||MANGANESE FERRITE:1||RESONANCE:1||SeCuO3:1||Optical conductivity:1||MASSLESS DIRAC FERMIONS:1||SCHOTTKYBARRIER:1||electronic structure:15||ELECTRONICSTRUCTURE:11||TRANSITIONMETAL COMPOUNDS:10||METALS:10||photoemission:8||SPECTRA:8||MAGNETORESISTANCE:7||FERROMAGNETISM:7||TRANSPORT:7||TRANSITION:6||FILMS:6||THINFILMS:5||TOTALENERGY CALCULATIONS:5||MAGNETICPROPERTIES:5||SUPERCONDUCTIVITY:5||PR:5||LATTICE:4||STATES:4||SPECTROSCOPY:4||FIELD:4||CRYSTALSTRUCTURE:4||PHOTOEMISSION:4||TEMPERATURE:4||TRANSITIONTEMPERATURE:4||XRAYABSORPTION:4||STATE:4||CU:4||BASISSET:4||XAS:4||CRYSTALS:3||EXCITATIONS:3||MOTTHUBBARD SYSTEMS:3||HIGHENERGY SPIN:3||halfmetal:3||INSULATORS:3||LA2CUO4:3||MODEL:3||FLUCTUATIONS:3||CE:3||double exchange:3||TRANSITIONMETALS:3||RESISTIVITY:3||BORON:3||LA1XCAXMNO3:3||IRON:3||PES:3||ANTIMONIDES:2||MgB2:2||ZR METALLIC GLASSES:2||superconductor:2||CRITICALCURRENT DENSITY:2||CIRCULARDICHROISM:2||SEMICONDUCTORS:2||LOCALIZATION:2||INTRABAND OPTICAL CONDUCTIVITY:2||COLOSSAL MAGNETORESISTANCE:2||OXIDATION:2||EXISTENCE:2||COPPER:2||diboride:2||MAGNESIUMDIBORIDE:2||GAP:2||CE COMPOUNDS:2||CORE POLARIZATION:2||magnetoresistance:2||photoemission spectroscopy:2||electronphonon interaction:2||GETTER:2||PD:2||MAGNETISM:2||FECR2S4:2||SUPERCONDUCTING MGB2:2||WIRES:2||ABSORPTION:2||ENERGY:2||LA1XSRXMNO3:2||CONSTANTS:2||polaron:2||charge ordering:2||SCATTERING:2||XRAY PHOTOEMISSION:2||CeNiSn:2||phase diagram:2||PHOTOELECTRON:2||QUADRUPOLAR:2||perovskitemanganites:2||CO:2||SYSTEMS:2||DOPED ZNO:2||LOWFREQUENCY SOUND:2||LA:2||ELECTRONELECTRON SCATTERING:2||AU:2||DENSITYWAVE INSTABILITY:2||FERMISURFACE:2||hybridization:2||VALENCEBAND SATELLITE:2||SULFUR SPINEL:2||Heusler:2||APPROXIMATION:2||superexchange:2||colossal magnetoresistance:2||ALLOYS:2||DEPENDENCE:2||AG:2||electronic structures:2||AUGERSPECTRA:2||CR:2||PARAMETERS:2||DIFFRACTION:2||SEMICONDUCTORMETAL TRANSITION:1||INTERMEDIATEVALENCE:1||SMB6:1||SRRUO3:1||antiperovskite structure with antipolar nature:1||lowenergy twodimensional phonons:1||anatase TiO2:1||La3S4:1||metalinsulator transitions:1||MNO:1||ELECTRONICSTRUCTURES:1||MAGNETIC CIRCULARDICHROISM:1||Density functional theory:1||CeCo2:1||TOPOLARON CROSSOVER:1||EXCHANGE:1||cuprates:1||high Tc cuprates:1||magnetically ordered materials:1||ZNSE:1||Sr2xKxFeMoO6:1||CDW:1||TeCuO3:1||STRUCTURALPROPERTIES:1||MN:1||screening length:1||amorphous Fe:1||WAVE BASISSET:1||SILICONCARBIDE:1||HIGHPRESSURE:1||electronphonon coupling:1||quenched superconductivity:1||CMR perovskite manganites:1||OXIDE:1||polarons:1||synchrotron radiation:1||FULLERIDES:1||RESONANTPHOTOEMISSION:1||Silicon carbide:1||DFT calculation:1||Hybridized bands:1||GIANT MAGNETORESISTANCE:1||PEROVSKITES:1||Raman spectra:1||EXCHANGE ENHANCEMENT:1||SILICON:1||SR2FEMOO6:1||orbital ordering:1||delafossite:1||TITANIUMDIOXIDE:1||electronic structure of disordered solids:1||YFE2:1||Magnetic polaron:1||NA2TI2SB2O:1||STRONGCOUPLED SUPERCONDUCTORS:1||HEAVYFERMION SYSTEMS:1||firstprinciples calculations:1||MECHANISM:1||UNiSn:1||PHOTONIC BANDGAP:1||SINGLE IMPURITY:1||PHONONSPECTRUM:1||FERMISURFACE TOPOLOGY:1||SUPPRESSION:1||RESONANT PHOTOEMISSION:1||METALDOPED PICENE:1||PHOTOIONIZATION CROSSSECTIONS:1||PHOTOINDUCED FERRIMAGNETIC SYSTEMS:1||LINKAGE ISOMERISM:1||CHARGETRANSFER:1||Bilayer Graphene:1||MAGNETICFIELD:1||SPINWAVES:1||rareearth manganese oxides:1||magnonphonon interaction:1||NACO2O4:1||ENERGYBANDS:1||SELFENERGY:1||GAS:1||Fe0.5Cu0.5Cr2S4:1||scanning photoelectron microscopy (SPEM):1||MAGNETIC PROPERTIES:1||Stoner model:1||AMORPHOUS TRANSITIONMETALS:1||SPINGLASS STATES:1||NI:1||LA3NI2B2N3:1||SOLIDS:1||CEO2:1||BAND THEORY:1||dilute magnetic semiconductor:1||pyrochlore:1||Y1XPRXBA2CU3O7DELTA:1||and electronphonon interactions:1||VIBRATIONS:1||RAY PHOTOEMISSION:1||ALKALI CATION:1||Europium:1||colossal magnetoresistance:1||structural stability:1||ENERGYGAP:1||small polaron:1||DOUBLE EXCHANGE:1||Coulomb correlation:1||magnon:1||phonons:1||ELECTRON FERROMAGNETISM:1||CURIETEMPERATURE:1||ARPES:1||PLANEWAVE METHOD:1||Xray absorption spectroscopy (XAS):1||ROOMTEMPERATURE:1||MONOCHALCOGENIDES:1||HEAT:1||UPDSN:1||MOMENTS:1||XRAY ABSORPTION:1||SEMICONDUCTOR:1||Fermi surface nesting:1||optical phonon:1||disordered system:1||dilute magnetic semiconductors:1||CMR manganites:1||PHONONS:1||LATTICEDYNAMICS:1||OXIDES:1||4fphotoemission:1||permanent magnet:1||pseudogap:1||TRANSPORTPROPERTIES:1||ANTIFERROMAGNET:1||(BI,PB)SRCOO SYSTEM:1||semicore correlation:1||POLARIZATION:1||CRYSTAL:1||spinel:1||Xray magnetic circular dichroism (XMCD):1||magnetocapacitance:1||ANATASE:1||TEMPERATURES:1||Pseudogap:1||INTERFACE:1||SUBSTRATE:1||YNI2B2C:1||SAMARIUM SULFIDE:1||strong swave superconductor:1||DOPED MANGANITE:1||SYMMETRY:1||CENISN:1||resonance mode:1||DISORDERED SYSTEM:1||LITHIUM INTERCALATION:1||CUO2 PLANE:1||SURFACE:1||Delafossite:1||ELECTRICALPROPERTIES:1||NIMNSB:1||PTMNSB:1||ROOMTEMPERATURE FERROMAGNETISM:1||RUBIDIUM MANGANESE HEXACYANOFERRATE:1||COLOSSALMAGNETORESISTANCE:1||FINITE TEMPERATURES:1||LAMNO3:1||FE:1||transitionmetal oxides:1||giant magnetoresistance:1||phonon:1||COPPER OXIDES:1||valence states:1||thermoelectric:1||semiconductor:1||CATION DISTRIBUTION:1||FeCr2S4:1||photoemission spectroscopy (PES):1||METALLIC FERROMAGNETISM:1||GRAPHITE:1||SUSCEPTIBILITY:1||UBE13:1||RCrSb3:1||band JahnTeller:1||Ce3S4:1||TiO2:1||PrBa2Cu3O7delta:1||UNTWINNED PRBA2CU3O7:1||AGNIO2:1||HALFMETALLIC FERROMAGNETS:1||CI:1||Energy gap:1||Photoemission:1||Future applications:1||Photoemission measurements:1||Graphene:1||BANDSTRUCTURE:1||TC:1||superconductivity:1||magnetic semiconductors:1||CMRmanganites:1||thin films:1||spin dynamics:1||highTc superconductors:1||ITINERANTELECTRON FERROMAGNETISM:1||SINGLECRYSTALS:1||CeTe2:1||amorphous magnetic materials:1||EPITAXIAL GRAPHENE:1||LAYERED PNICTIDEOXIDES:1||BOROCARBIDE SUPERCONDUCTORS:1||AUGMENTEDWAVE METHOD:1||METALLIC MAGNET UNISN:1||ORIGIN:1||spectrum rearrangement:1||MEANFIELD THEORY:1||MOLECULEBASED MAGNETS:1||METASTABLE STATE:1||INSULATOR:1||magnetic orderin:1||FCC IRON:1||CeRu2:1||TL2MN2O7:1||isotope effect:1||Perovskitemanganites:1||RECURSION METHOD:1||PERPENDICULAR MAGNETICANISOTROPY:1||quasiparticle spectral density:1||GW:1||MANGANESE FERRITE:1||RESONANCE:1||SeCuO3:1||Optical conductivity:1||MASSLESS DIRAC FERMIONS:1||SCHOTTKYBARRIER:1||electronic structure:15||ELECTRONICSTRUCTURE:11||TRANSITIONMETAL COMPOUNDS:10||METALS:10||photoemission:8||SPECTRA:8||MAGNETORESISTANCE:7||FERROMAGNETISM:7||TRANSPORT:7||TRANSITION:6||FILMS:6||THINFILMS:5||TOTALENERGY CALCULATIONS:5||MAGNETICPROPERTIES:5||SUPERCONDUCTIVITY:5||PR:5||LATTICE:4||STATES:4||SPECTROSCOPY:4||FIELD:4||CRYSTALSTRUCTURE:4||PHOTOEMISSION:4||TEMPERATURE:4||TRANSITIONTEMPERATURE:4||XRAYABSORPTION:4||STATE:4||CU:4||BASISSET:4||XAS:4||CRYSTALS:3||EXCITATIONS:3||MOTTHUBBARD SYSTEMS:3||HIGHENERGY SPIN:3||halfmetal:3||INSULATORS:3||LA2CUO4:3||MODEL:3||FLUCTUATIONS:3||CE:3||double exchange:3||TRANSITIONMETALS:3||RESISTIVITY:3||BORON:3||LA1XCAXMNO3:3||IRON:3||PES:3||ANTIMONIDES:2||MgB2:2||ZR METALLIC GLASSES:2||superconductor:2||CRITICALCURRENT DENSITY:2||CIRCULARDICHROISM:2||SEMICONDUCTORS:2||LOCALIZATION:2||INTRABAND OPTICAL CONDUCTIVITY:2||COLOSSAL MAGNETORESISTANCE:2||OXIDATION:2||EXISTENCE:2||COPPER:2||diboride:2||MAGNESIUMDIBORIDE:2||GAP:2||CE COMPOUNDS:2||CORE POLARIZATION:2||magnetoresistance:2||photoemission spectroscopy:2||electronphonon interaction:2||GETTER:2||PD:2||MAGNETISM:2||FECR2S4:2||SUPERCONDUCTING MGB2:2||WIRES:2||ABSORPTION:2||ENERGY:2||LA1XSRXMNO3:2||CONSTANTS:2||polaron:2||charge ordering:2||SCATTERING:2||XRAY PHOTOEMISSION:2||CeNiSn:2||phase diagram:2||PHOTOELECTRON:2||QUADRUPOLAR:2||perovskitemanganites:2||CO:2||SYSTEMS:2||DOPED ZNO:2||LOWFREQUENCY SOUND:2||LA:2||ELECTRONELECTRON SCATTERING:2||AU:2||DENSITYWAVE INSTABILITY:2||FERMISURFACE:2||hybridization:2||VALENCEBAND SATELLITE:2||SULFUR SPINEL:2||Heusler:2||APPROXIMATION:2||superexchange:2||colossal magnetoresistance:2||ALLOYS:2||DEPENDENCE:2||AG:2||electronic structures:2||AUGERSPECTRA:2||CR:2||PARAMETERS:2||DIFFRACTION:2||SEMICONDUCTORMETAL TRANSITION:1||INTERMEDIATEVALENCE:1||SMB6:1||SRRUO3:1||antiperovskite structure with antipolar nature:1||lowenergy twodimensional phonons:1||anatase TiO2:1||La3S4:1||metalinsulator transitions:1||MNO:1||ELECTRONICSTRUCTURES:1||MAGNETIC CIRCULARDICHROISM:1||Density functional theory:1||CeCo2:1||TOPOLARON CROSSOVER:1||EXCHANGE:1||cuprates:1||high Tc cuprates:1||magnetically ordered materials:1||ZNSE:1||Sr2xKxFeMoO6:1||CDW:1||TeCuO3:1||STRUCTURALPROPERTIES:1||MN:1||screening length:1||amorphous Fe:1||WAVE BASISSET:1||SILICONCARBIDE:1||HIGHPRESSURE:1||electronphonon coupling:1||quenched superconductivity:1||CMR perovskite manganites:1||OXIDE:1||polarons:1||synchrotron radiation:1||FULLERIDES:1||RESONANTPHOTOEMISSION:1||Silicon carbide:1||DFT calculation:1||Hybridized bands:1||GIANT MAGNETORESISTANCE:1||PEROVSKITES:1||Raman spectra:1||EXCHANGE ENHANCEMENT:1||SILICON:1||SR2FEMOO6:1||orbital ordering:1||delafossite:1||TITANIUMDIOXIDE:1||electronic structure of disordered solids:1||YFE2:1||Magnetic polaron:1||NA2TI2SB2O:1||STRONGCOUPLED SUPERCONDUCTORS:1||HEAVYFERMION SYSTEMS:1||firstprinciples calculations:1||MECHANISM:1||UNiSn:1||PHOTONIC BANDGAP:1||SINGLE IMPURITY:1||PHONONSPECTRUM:1||FERMISURFACE TOPOLOGY:1||SUPPRESSION:1||RESONANT PHOTOEMISSION:1||METALDOPED PICENE:1||PHOTOIONIZATION CROSSSECTIONS:1||PHOTOINDUCED FERRIMAGNETIC SYSTEMS:1||LINKAGE ISOMERISM:1||CHARGETRANSFER:1||Bilayer Graphene:1||MAGNETICFIELD:1||SPINWAVES:1||rareearth manganese oxides:1||magnonphonon interaction:1||NACO2O4:1||ENERGYBANDS:1||SELFENERGY:1||GAS:1||Fe0.5Cu0.5Cr2S4:1||scanning photoelectron microscopy (SPEM):1||MAGNETIC PROPERTIES:1||Stoner model:1||AMORPHOUS TRANSITIONMETALS:1||SPINGLASS STATES:1||NI:1||LA3NI2B2N3:1||SOLIDS:1||CEO2:1||BAND THEORY:1||dilute magnetic semiconductor:1||pyrochlore:1||Y1XPRXBA2CU3O7DELTA:1||and electronphonon interactions:1||VIBRATIONS:1||RAY PHOTOEMISSION:1||ALKALI CATION:1||Europium:1||colossal magnetoresistance:1||structural stability:1||ENERGYGAP:1||small polaron:1||DOUBLE EXCHANGE:1||Coulomb correlation:1||magnon:1||phonons:1||ELECTRON FERROMAGNETISM:1||CURIETEMPERATURE:1||ARPES:1||PLANEWAVE METHOD:1||Xray absorption spectroscopy (XAS):1||ROOMTEMPERATURE:1||MONOCHALCOGENIDES:1||HEAT:1||UPDSN:1||MOMENTS:1||XRAY ABSORPTION:1||SEMICONDUCTOR:1||Fermi surface nesting:1||optical phonon:1||disordered system:1||dilute magnetic semiconductors:1||CMR manganites:1||PHONONS:1||LATTICEDYNAMICS:1||OXIDES:1||4fphotoemission:1||permanent magnet:1||pseudogap:1||TRANSPORTPROPERTIES:1||ANTIFERROMAGNET:1||(BI,PB)SRCOO SYSTEM:1||semicore correlation:1||POLARIZATION:1||CRYSTAL:1||spinel:1||Xray magnetic circular dichroism (XMCD):1||magnetocapacitance:1||ANATASE:1||TEMPERATURES:1||Pseudogap:1||INTERFACE:1||SUBSTRATE:1||YNI2B2C:1||SAMARIUM SULFIDE:1||strong swave superconductor:1||DOPED MANGANITE:1||SYMMETRY:1||CENISN:1||resonance mode:1||DISORDERED SYSTEM:1||LITHIUM INTERCALATION:1||CUO2 PLANE:1||SURFACE:1||Delafossite:1||ELECTRICALPROPERTIES:1||NIMNSB:1||PTMNSB:1||ROOMTEMPERATURE FERROMAGNETISM:1||RUBIDIUM MANGANESE HEXACYANOFERRATE:1||COLOSSALMAGNETORESISTANCE:1||FINITE TEMPERATURES:1||LAMNO3:1||FE:1||transitionmetal oxides:1||giant magnetoresistance:1||phonon:1||COPPER OXIDES:1||valence states:1||thermoelectric:1||semiconductor:1||CATION DISTRIBUTION:1||FeCr2S4:1||photoemission spectroscopy (PES):1||METALLIC FERROMAGNETISM:1||GRAPHITE:1||SUSCEPTIBILITY:1||UBE13:1||RCrSb3:1||band JahnTeller:1||Ce3S4:1||TiO2:1||PrBa2Cu3O7delta:1||UNTWINNED PRBA2CU3O7:1||AGNIO2:1||HALFMETALLIC FERROMAGNETS:1||CI:1||Energy gap:1||Photoemission:1||Future applications:1||Photoemission measurements:1||Graphene:1||BANDSTRUCTURE:1||TC:1||superconductivity:1||magnetic semiconductors:1||CMRmanganites:1||thin films:1||spin dynamics:1||highTc superconductors:1||ITINERANTELECTRON FERROMAGNETISM:1||SINGLECRYSTALS:1||CeTe2:1||amorphous magnetic materials:1||EPITAXIAL GRAPHENE:1||LAYERED PNICTIDEOXIDES:1||BOROCARBIDE SUPERCONDUCTORS:1||AUGMENTEDWAVE METHOD:1||METALLIC MAGNET UNISN:1||ORIGIN:1||spectrum rearrangement:1||MEANFIELD THEORY:1||MOLECULEBASED MAGNETS:1||METASTABLE STATE:1||INSULATOR:1||magnetic orderin:1||FCC IRON:1||CeRu2:1||TL2MN2O7:1||isotope effect:1||Perovskitemanganites:1||RECURSION METHOD:1||PERPENDICULAR MAGNETICANISOTROPY:1||quasiparticle spectral density:1||GW:1||MANGANESE FERRITE:1||RESONANCE:1||SeCuO3:1||Optical conductivity:1||MASSLESS DIRAC FERMIONS:1||SCHOTTKYBARRIER:1||electronic structure:15||ELECTRONICSTRUCTURE:11||TRANSITIONMETAL COMPOUNDS:10||METALS:10||photoemission:8||SPECTRA:8||MAGNETORESISTANCE:7||FERROMAGNETISM:7||TRANSPORT:7||TRANSITION:6||FILMS:6||THINFILMS:5||TOTALENERGY CALCULATIONS:5||MAGNETICPROPERTIES:5||SUPERCONDUCTIVITY:5||PR:5||LATTICE:4||STATES:4||SPECTROSCOPY:4||FIELD:4||CRYSTALSTRUCTURE:4||PHOTOEMISSION:4||TEMPERATURE:4||TRANSITIONTEMPERATURE:4||XRAYABSORPTION:4||STATE:4||CU:4||BASISSET:4||XAS:4||CRYSTALS:3||EXCITATIONS:3||MOTTHUBBARD SYSTEMS:3||HIGHENERGY SPIN:3||halfmetal:3||INSULATORS:3||LA2CUO4:3||MODEL:3||FLUCTUATIONS:3||CE:3||double exchange:3||TRANSITIONMETALS:3||RESISTIVITY:3||BORON:3||LA1XCAXMNO3:3||IRON:3||PES:3||ANTIMONIDES:2||MgB2:2||ZR METALLIC GLASSES:2||superconductor:2||CRITICALCURRENT DENSITY:2||CIRCULARDICHROISM:2||SEMICONDUCTORS:2||LOCALIZATION:2||INTRABAND OPTICAL CONDUCTIVITY:2||COLOSSAL MAGNETORESISTANCE:2||OXIDATION:2||EXISTENCE:2||COPPER:2||diboride:2||MAGNESIUMDIBORIDE:2||GAP:2||CE COMPOUNDS:2||CORE POLARIZATION:2||magnetoresistance:2||photoemission spectroscopy:2||electronphonon interaction:2||GETTER:2||PD:2||MAGNETISM:2||FECR2S4:2||SUPERCONDUCTING MGB2:2||WIRES:2||ABSORPTION:2||ENERGY:2||LA1XSRXMNO3:2||CONSTANTS:2||polaron:2||charge ordering:2||SCATTERING:2||XRAY PHOTOEMISSION:2||CeNiSn:2||phase diagram:2||PHOTOELECTRON:2||QUADRUPOLAR:2||perovskitemanganites:2||CO:2||SYSTEMS:2||DOPED ZNO:2||LOWFREQUENCY SOUND:2||LA:2||ELECTRONELECTRON SCATTERING:2||AU:2||DENSITYWAVE INSTABILITY:2||FERMISURFACE:2||hybridization:2||VALENCEBAND SATELLITE:2||SULFUR SPINEL:2||Heusler:2||APPROXIMATION:2||superexchange:2||colossal magnetoresistance:2||ALLOYS:2||DEPENDENCE:2||AG:2||electronic structures:2||AUGERSPECTRA:2||CR:2||PARAMETERS:2||DIFFRACTION:2||SEMICONDUCTORMETAL TRANSITION:1||INTERMEDIATEVALENCE:1||SMB6:1||SRRUO3:1||antiperovskite structure with antipolar nature:1||lowenergy twodimensional phonons:1||anatase TiO2:1||La3S4:1||metalinsulator transitions:1||MNO:1||ELECTRONICSTRUCTURES:1||MAGNETIC CIRCULARDICHROISM:1||Density functional theory:1||CeCo2:1||TOPOLARON CROSSOVER:1||EXCHANGE:1||cuprates:1||high Tc cuprates:1||magnetically ordered materials:1||ZNSE:1||Sr2xKxFeMoO6:1||CDW:1||TeCuO3:1||STRUCTURALPROPERTIES:1||MN:1||screening length:1||amorphous Fe:1||WAVE BASISSET:1||SILICONCARBIDE:1||HIGHPRESSURE:1||electronphonon coupling:1||quenched superconductivity:1||CMR perovskite manganites:1||OXIDE:1||polarons:1||synchrotron radiation:1||FULLERIDES:1||RESONANTPHOTOEMISSION:1||Silicon carbide:1||DFT calculation:1||Hybridized bands:1||GIANT MAGNETORESISTANCE:1||PEROVSKITES:1||Raman spectra:1||EXCHANGE ENHANCEMENT:1||SILICON:1||SR2FEMOO6:1||orbital ordering:1||delafossite:1||TITANIUMDIOXIDE:1||electronic structure of disordered solids:1||YFE2:1||Magnetic polaron:1||NA2TI2SB2O:1||STRONGCOUPLED SUPERCONDUCTORS:1||HEAVYFERMION SYSTEMS:1||firstprinciples calculations:1||MECHANISM:1||UNiSn:1||PHOTONIC BANDGAP:1||SINGLE IMPURITY:1||PHONONSPECTRUM:1||FERMISURFACE TOPOLOGY:1||SUPPRESSION:1||RESONANT PHOTOEMISSION:1||METALDOPED PICENE:1||PHOTOIONIZATION CROSSSECTIONS:1||PHOTOINDUCED FERRIMAGNETIC SYSTEMS:1||LINKAGE ISOMERISM:1||CHARGETRANSFER:1||Bilayer Graphene:1||MAGNETICFIELD:1||SPINWAVES:1||rareearth manganese oxides:1||magnonphonon interaction:1||NACO2O4:1||ENERGYBANDS:1||SELFENERGY:1||GAS:1||Fe0.5Cu0.5Cr2S4:1||scanning photoelectron microscopy (SPEM):1||MAGNETIC PROPERTIES:1||Stoner model:1||AMORPHOUS TRANSITIONMETALS:1||SPINGLASS STATES:1||NI:1||LA3NI2B2N3:1||SOLIDS:1||CEO2:1||BAND THEORY:1||dilute magnetic semiconductor:1||pyrochlore:1||Y1XPRXBA2CU3O7DELTA:1||and electronphonon interactions:1||VIBRATIONS:1||RAY PHOTOEMISSION:1||ALKALI CATION:1||Europium:1||colossal magnetoresistance:1||structural stability:1||ENERGYGAP:1||small polaron:1||DOUBLE EXCHANGE:1||Coulomb correlation:1||magnon:1||phonons:1||ELECTRON FERROMAGNETISM:1||CURIETEMPERATURE:1||ARPES:1||PLANEWAVE METHOD:1||Xray absorption spectroscopy (XAS):1||ROOMTEMPERATURE:1||MONOCHALCOGENIDES:1||HEAT:1||UPDSN:1||MOMENTS:1||XRAY ABSORPTION:1||SEMICONDUCTOR:1||Fermi surface nesting:1||optical phonon:1||disordered system:1||dilute magnetic semiconductors:1||CMR manganites:1||PHONONS:1||LATTICEDYNAMICS:1||OXIDES:1||4fphotoemission:1||permanent magnet:1||pseudogap:1||TRANSPORTPROPERTIES:1||ANTIFERROMAGNET:1||(BI,PB)SRCOO SYSTEM:1||semicore correlation:1||POLARIZATION:1||CRYSTAL:1||spinel:1||Xray magnetic circular dichroism (XMCD):1||magnetocapacitance:1||ANATASE:1||TEMPERATURES:1||Pseudogap:1||INTERFACE:1||SUBSTRATE:1||YNI2B2C:1||SAMARIUM SULFIDE:1||strong swave superconductor:1||DOPED MANGANITE:1||SYMMETRY:1||CENISN:1||resonance mode:1||DISORDERED SYSTEM:1||LITHIUM INTERCALATION:1||CUO2 PLANE:1||SURFACE:1||Delafossite:1||ELECTRICALPROPERTIES:1||NIMNSB:1||PTMNSB:1||ROOMTEMPERATURE FERROMAGNETISM:1||RUBIDIUM MANGANESE HEXACYANOFERRATE:1||COLOSSALMAGNETORESISTANCE:1||FINITE TEMPERATURES:1||LAMNO3:1||FE:1||transitionmetal oxides:1||giant magnetoresistance:1||phonon:1||COPPER OXIDES:1||valence states:1||thermoelectric:1||semiconductor:1||CATION DISTRIBUTION:1||FeCr2S4:1||photoemission spectroscopy (PES):1||METALLIC FERROMAGNETISM:1||GRAPHITE:1||SUSCEPTIBILITY:1||UBE13:1||RCrSb3:1||band JahnTeller:1||Ce3S4:1||TiO2:1||PrBa2Cu3O7delta:1||UNTWINNED PRBA2CU3O7:1||AGNIO2:1||HALFMETALLIC FERROMAGNETS:1||CI:1||Energy gap:1||Photoemission:1||Future applications:1||Photoemission measurements:1||Graphene:1||BANDSTRUCTURE:1||TC:1||superconductivity:1||magnetic semiconductors:1||CMRmanganites:1||thin films:1||spin dynamics:1||highTc superconductors:1||ITINERANTELECTRON FERROMAGNETISM:1||SINGLECRYSTALS:1||CeTe2:1||amorphous magnetic materials:1||EPITAXIAL GRAPHENE:1||LAYERED PNICTIDEOXIDES:1||BOROCARBIDE SUPERCONDUCTORS:1||AUGMENTEDWAVE METHOD:1||METALLIC MAGNET UNISN:1||ORIGIN:1||spectrum rearrangement:1||MEANFIELD THEORY:1||MOLECULEBASED MAGNETS:1||METASTABLE STATE:1||INSULATOR:1||magnetic orderin:1||FCC IRON:1||CeRu2:1||TL2MN2O7:1||isotope effect:1||Perovskitemanganites:1||RECURSION METHOD:1||PERPENDICULAR MAGNETICANISOTROPY:1||quasiparticle spectral density:1||GW:1||MANGANESE FERRITE:1||RESONANCE:1||SeCuO3:1||Optical conductivity:1||MASSLESS DIRAC FERMIONS:1||SCHOTTKYBARRIER:1||electronic structure:15||ELECTRONICSTRUCTURE:11||TRANSITIONMETAL COMPOUNDS:10||METALS:10||photoemission:8||SPECTRA:8||MAGNETORESISTANCE:7||FERROMAGNETISM:7||TRANSPORT:7||TRANSITION:6||FILMS:6||THINFILMS:5||TOTALENERGY CALCULATIONS:5||MAGNETICPROPERTIES:5||SUPERCONDUCTIVITY:5||PR:5||LATTICE:4||STATES:4||SPECTROSCOPY:4||FIELD:4||CRYSTALSTRUCTURE:4||PHOTOEMISSION:4||TEMPERATURE:4||TRANSITIONTEMPERATURE:4||XRAYABSORPTION:4||STATE:4||CU:4||BASISSET:4||XAS:4||CRYSTALS:3||EXCITATIONS:3||MOTTHUBBARD SYSTEMS:3||HIGHENERGY SPIN:3||halfmetal:3||INSULATORS:3||LA2CUO4:3||MODEL:3||FLUCTUATIONS:3||CE:3||double exchange:3||TRANSITIONMETALS:3||RESISTIVITY:3||BORON:3||LA1XCAXMNO3:3||IRON:3||PES:3||ANTIMONIDES:2||MgB2:2||ZR METALLIC GLASSES:2||superconductor:2||CRITICALCURRENT DENSITY:2||CIRCULARDICHROISM:2||SEMICONDUCTORS:2||LOCALIZATION:2||INTRABAND OPTICAL CONDUCTIVITY:2||COLOSSAL MAGNETORESISTANCE:2||OXIDATION:2||EXISTENCE:2||COPPER:2||diboride:2||MAGNESIUMDIBORIDE:2||GAP:2||CE COMPOUNDS:2||CORE POLARIZATION:2||magnetoresistance:2||photoemission spectroscopy:2||electronphonon interaction:2||GETTER:2||PD:2||MAGNETISM:2||FECR2S4:2||SUPERCONDUCTING MGB2:2||WIRES:2||ABSORPTION:2||ENERGY:2||LA1XSRXMNO3:2||CONSTANTS:2||polaron:2||charge ordering:2||SCATTERING:2||XRAY PHOTOEMISSION:2||CeNiSn:2||phase diagram:2||PHOTOELECTRON:2||QUADRUPOLAR:2||perovskitemanganites:2||CO:2||SYSTEMS:2||DOPED ZNO:2||LOWFREQUENCY SOUND:2||LA:2||ELECTRONELECTRON SCATTERING:2||AU:2||DENSITYWAVE INSTABILITY:2||FERMISURFACE:2||hybridization:2||VALENCEBAND SATELLITE:2||SULFUR SPINEL:2||Heusler:2||APPROXIMATION:2||superexchange:2||colossal magnetoresistance:2||ALLOYS:2||DEPENDENCE:2||AG:2||electronic structures:2||AUGERSPECTRA:2||CR:2||PARAMETERS:2||DIFFRACTION:2||SEMICONDUCTORMETAL TRANSITION:1||INTERMEDIATEVALENCE:1||SMB6:1||SRRUO3:1||antiperovskite structure with antipolar nature:1||lowenergy twodimensional phonons:1||anatase TiO2:1||La3S4:1||metalinsulator transitions:1||MNO:1||ELECTRONICSTRUCTURES:1||MAGNETIC CIRCULARDICHROISM:1||Density functional theory:1||CeCo2:1||TOPOLARON CROSSOVER:1||EXCHANGE:1||cuprates:1||high Tc cuprates:1||magnetically ordered materials:1||ZNSE:1||Sr2xKxFeMoO6:1||CDW:1||TeCuO3:1||STRUCTURALPROPERTIES:1||MN:1||screening length:1||amorphous Fe:1||WAVE BASISSET:1||SILICONCARBIDE:1||HIGHPRESSURE:1||electronphonon coupling:1||quenched superconductivity:1||CMR perovskite manganites:1||OXIDE:1||polarons:1||synchrotron radiation:1||FULLERIDES:1||RESONANTPHOTOEMISSION:1||Silicon carbide:1||DFT calculation:1||Hybridized bands:1||GIANT MAGNETORESISTANCE:1||PEROVSKITES:1||Raman spectra:1||EXCHANGE ENHANCEMENT:1||SILICON:1||SR2FEMOO6:1||orbital ordering:1||delafossite:1||TITANIUMDIOXIDE:1||electronic structure of disordered solids:1||YFE2:1||Magnetic polaron:1||NA2TI2SB2O:1||STRONGCOUPLED SUPERCONDUCTORS:1||HEAVYFERMION SYSTEMS:1||firstprinciples calculations:1||MECHANISM:1||UNiSn:1||PHOTONIC BANDGAP:1||SINGLE IMPURITY:1||PHONONSPECTRUM:1||FERMISURFACE TOPOLOGY:1||SUPPRESSION:1||RESONANT PHOTOEMISSION:1||METALDOPED PICENE:1||PHOTOIONIZATION CROSSSECTIONS:1||PHOTOINDUCED FERRIMAGNETIC SYSTEMS:1||LINKAGE ISOMERISM:1||CHARGETRANSFER:1||Bilayer Graphene:1||MAGNETICFIELD:1||SPINWAVES:1||rareearth manganese oxides:1||magnonphonon interaction:1||NACO2O4:1||ENERGYBANDS:1||SELFENERGY:1||GAS:1||Fe0.5Cu0.5Cr2S4:1||scanning photoelectron microscopy (SPEM):1||MAGNETIC PROPERTIES:1||Stoner model:1||AMORPHOUS TRANSITIONMETALS:1||SPINGLASS STATES:1||NI:1||LA3NI2B2N3:1||SOLIDS:1||CEO2:1||BAND THEORY:1||dilute magnetic semiconductor:1||pyrochlore:1||Y1XPRXBA2CU3O7DELTA:1||and electronphonon interactions:1||VIBRATIONS:1||RAY PHOTOEMISSION:1||ALKALI CATION:1||Europium:1||colossal magnetoresistance:1||structural stability:1||ENERGYGAP:1||small polaron:1||DOUBLE EXCHANGE:1||Coulomb correlation:1||magnon:1||phonons:1||ELECTRON FERROMAGNETISM:1||CURIETEMPERATURE:1||ARPES:1||PLANEWAVE METHOD:1||Xray absorption spectroscopy (XAS):1||ROOMTEMPERATURE:1||MONOCHALCOGENIDES:1||HEAT:1||UPDSN:1||MOMENTS:1||XRAY ABSORPTION:1||SEMICONDUCTOR:1||Fermi surface nesting:1||optical phonon:1||disordered system:1||dilute magnetic semiconductors:1||CMR manganites:1||PHONONS:1||LATTICEDYNAMICS:1||OXIDES:1||4fphotoemission:1||permanent magnet:1||pseudogap:1||TRANSPORTPROPERTIES:1||ANTIFERROMAGNET:1||(BI,PB)SRCOO SYSTEM:1||semicore correlation:1||POLARIZATION:1||CRYSTAL:1||spinel:1||Xray magnetic circular dichroism (XMCD):1||magnetocapacitance:1||ANATASE:1||TEMPERATURES:1||Pseudogap:1||INTERFACE:1||SUBSTRATE:1||YNI2B2C:1||SAMARIUM SULFIDE:1||strong swave superconductor:1||DOPED MANGANITE:1||SYMMETRY:1||CENISN:1||resonance mode:1||DISORDERED SYSTEM:1||LITHIUM INTERCALATION:1||CUO2 PLANE:1||SURFACE:1||Delafossite:1||ELECTRICALPROPERTIES:1||NIMNSB:1||PTMNSB:1||ROOMTEMPERATURE FERROMAGNETISM:1||RUBIDIUM MANGANESE HEXACYANOFERRATE:1||COLOSSALMAGNETORESISTANCE:1||FINITE TEMPERATURES:1||LAMNO3:1||FE:1||transitionmetal oxides:1||giant magnetoresistance:1||phonon:1||COPPER OXIDES:1||valence states:1||thermoelectric:1||semiconductor:1||CATION DISTRIBUTION:1||FeCr2S4:1||photoemission spectroscopy (PES):1||METALLIC FERROMAGNETISM:1||GRAPHITE:1||SUSCEPTIBILITY:1||UBE13:1||RCrSb3:1||band JahnTeller:1||Ce3S4:1||TiO2:1||PrBa2Cu3O7delta:1||UNTWINNED PRBA2CU3O7:1||AGNIO2:1||HALFMETALLIC FERROMAGNETS:1||CI:1||Energy gap:1||Photoemission:1||Future applications:1||Photoemission measurements:1||Graphene:1||BANDSTRUCTURE:1||TC:1||superconductivity:1||magnetic semiconductors:1||CMRmanganites:1||thin films:1||spin dynamics:1||highTc superconductors:1||ITINERANTELECTRON FERROMAGNETISM:1||SINGLECRYSTALS:1||CeTe2:1||amorphous magnetic materials:1||EPITAXIAL GRAPHENE:1||LAYERED PNICTIDEOXIDES:1||BOROCARBIDE SUPERCONDUCTORS:1||AUGMENTEDWAVE METHOD:1||METALLIC MAGNET UNISN:1||ORIGIN:1||spectrum rearrangement:1||MEANFIELD THEORY:1||MOLECULEBASED MAGNETS:1||METASTABLE STATE:1||INSULATOR:1||magnetic orderin:1||FCC IRON:1||CeRu2:1||TL2MN2O7:1||isotope effect:1||Perovskitemanganites:1||RECURSION METHOD:1||PERPENDICULAR MAGNETICANISOTROPY:1||quasiparticle spectral density:1||GW:1||MANGANESE FERRITE:1||RESONANCE:1||SeCuO3:1||Optical conductivity:1||MASSLESS DIRAC FERMIONS:1||SCHOTTKYBARRIER:1||electronic structure:15||ELECTRONICSTRUCTURE:11||TRANSITIONMETAL COMPOUNDS:10||METALS:10||photoemission:8||SPECTRA:8||MAGNETORESISTANCE:7||FERROMAGNETISM:7||TRANSPORT:7||TRANSITION:6||FILMS:6||THINFILMS:5||TOTALENERGY CALCULATIONS:5||MAGNETICPROPERTIES:5||SUPERCONDUCTIVITY:5||PR:5||LATTICE:4||STATES:4||SPECTROSCOPY:4||FIELD:4||CRYSTALSTRUCTURE:4||PHOTOEMISSION:4||TEMPERATURE:4||TRANSITIONTEMPERATURE:4||XRAYABSORPTION:4||STATE:4||CU:4||BASISSET:4||XAS:4||CRYSTALS:3||EXCITATIONS:3||MOTTHUBBARD SYSTEMS:3||HIGHENERGY SPIN:3||halfmetal:3||INSULATORS:3||LA2CUO4:3||MODEL:3||FLUCTUATIONS:3||CE:3||double exchange:3||TRANSITIONMETALS:3||RESISTIVITY:3||BORON:3||LA1XCAXMNO3:3||IRON:3||PES:3||ANTIMONIDES:2||MgB2:2||ZR METALLIC GLASSES:2||superconductor:2||CRITICALCURRENT DENSITY:2||CIRCULARDICHROISM:2||SEMICONDUCTORS:2||LOCALIZATION:2||INTRABAND OPTICAL CONDUCTIVITY:2||COLOSSAL MAGNETORESISTANCE:2||OXIDATION:2||EXISTENCE:2||COPPER:2||diboride:2||MAGNESIUMDIBORIDE:2||GAP:2||CE COMPOUNDS:2||CORE POLARIZATION:2||magnetoresistance:2||photoemission spectroscopy:2||electronphonon interaction:2||GETTER:2||PD:2||MAGNETISM:2||FECR2S4:2||SUPERCONDUCTING MGB2:2||WIRES:2||ABSORPTION:2||ENERGY:2||LA1XSRXMNO3:2||CONSTANTS:2||polaron:2||charge ordering:2||SCATTERING:2||XRAY PHOTOEMISSION:2||CeNiSn:2||phase diagram:2||PHOTOELECTRON:2||QUADRUPOLAR:2||perovskitemanganites:2||CO:2||SYSTEMS:2||DOPED ZNO:2||LOWFREQUENCY SOUND:2||LA:2||ELECTRONELECTRON SCATTERING:2||AU:2||DENSITYWAVE INSTABILITY:2||FERMISURFACE:2||hybridization:2||VALENCEBAND SATELLITE:2||SULFUR SPINEL:2||Heusler:2||APPROXIMATION:2||superexchange:2||colossal magnetoresistance:2||ALLOYS:2||DEPENDENCE:2||AG:2||electronic structures:2||AUGERSPECTRA:2||CR:2||PARAMETERS:2||DIFFRACTION:2||SEMICONDUCTORMETAL TRANSITION:1||INTERMEDIATEVALENCE:1||SMB6:1||SRRUO3:1||antiperovskite structure with antipolar nature:1||lowenergy twodimensional phonons:1||anatase TiO2:1||La3S4:1||metalinsulator transitions:1||MNO:1||ELECTRONICSTRUCTURES:1||MAGNETIC CIRCULARDICHROISM:1||Density functional theory:1||CeCo2:1||TOPOLARON CROSSOVER:1||EXCHANGE:1||cuprates:1||high Tc cuprates:1||magnetically ordered materials:1||ZNSE:1||Sr2xKxFeMoO6:1||CDW:1||TeCuO3:1||STRUCTURALPROPERTIES:1||MN:1||screening length:1||amorphous Fe:1||WAVE BASISSET:1||SILICONCARBIDE:1||HIGHPRESSURE:1||electronphonon coupling:1||quenched superconductivity:1||CMR perovskite manganites:1||OXIDE:1||polarons:1||synchrotron radiation:1||FULLERIDES:1||RESONANTPHOTOEMISSION:1||Silicon carbide:1||DFT calculation:1||Hybridized bands:1||GIANT MAGNETORESISTANCE:1||PEROVSKITES:1||Raman spectra:1||EXCHANGE ENHANCEMENT:1||SILICON:1||SR2FEMOO6:1||orbital ordering:1||delafossite:1||TITANIUMDIOXIDE:1||electronic structure of disordered solids:1||YFE2:1||Magnetic polaron:1||NA2TI2SB2O:1||STRONGCOUPLED SUPERCONDUCTORS:1||HEAVYFERMION SYSTEMS:1||firstprinciples calculations:1||MECHANISM:1||UNiSn:1||PHOTONIC BANDGAP:1||SINGLE IMPURITY:1||PHONONSPECTRUM:1||FERMISURFACE TOPOLOGY:1||SUPPRESSION:1||RESONANT PHOTOEMISSION:1||METALDOPED PICENE:1||PHOTOIONIZATION CROSSSECTIONS:1||PHOTOINDUCED FERRIMAGNETIC SYSTEMS:1||LINKAGE ISOMERISM:1||CHARGETRANSFER:1||Bilayer Graphene:1||MAGNETICFIELD:1||SPINWAVES:1||rareearth manganese oxides:1||magnonphonon interaction:1||NACO2O4:1||ENERGYBANDS:1||SELFENERGY:1||GAS:1||Fe0.5Cu0.5Cr2S4:1||scanning photoelectron microscopy (SPEM):1||MAGNETIC PROPERTIES:1||Stoner model:1||AMORPHOUS TRANSITIONMETALS:1||SPINGLASS STATES:1||NI:1||LA3NI2B2N3:1||SOLIDS:1||CEO2:1||BAND THEORY:1||dilute magnetic semiconductor:1||pyrochlore:1||Y1XPRXBA2CU3O7DELTA:1||and electronphonon interactions:1||VIBRATIONS:1||RAY PHOTOEMISSION:1||ALKALI CATION:1||Europium:1||colossal magnetoresistance:1||structural stability:1||ENERGYGAP:1||small polaron:1||DOUBLE EXCHANGE:1||Coulomb correlation:1||magnon:1||phonons:1||ELECTRON FERROMAGNETISM:1||CURIETEMPERATURE:1||ARPES:1||PLANEWAVE METHOD:1||Xray absorption spectroscopy (XAS):1||ROOMTEMPERATURE:1||MONOCHALCOGENIDES:1||HEAT:1||UPDSN:1||MOMENTS:1||XRAY ABSORPTION:1||SEMICONDUCTOR:1||Fermi surface nesting:1||optical phonon:1||disordered system:1||dilute magnetic semiconductors:1||CMR manganites:1||PHONONS:1||LATTICEDYNAMICS:1||OXIDES:1||4fphotoemission:1||permanent magnet:1||pseudogap:1||TRANSPORTPROPERTIES:1||ANTIFERROMAGNET:1||(BI,PB)SRCOO SYSTEM:1||semicore correlation:1||POLARIZATION:1||CRYSTAL:1||spinel:1||Xray magnetic circular dichroism (XMCD):1||magnetocapacitance:1||ANATASE:1||TEMPERATURES:1||Pseudogap:1||INTERFACE:1||SUBSTRATE:1||YNI2B2C:1||SAMARIUM SULFIDE:1||strong swave superconductor:1||DOPED MANGANITE:1||SYMMETRY:1||CENISN:1||resonance mode:1||DISORDERED SYSTEM:1||LITHIUM INTERCALATION:1||CUO2 PLANE:1||SURFACE:1||Delafossite:1||ELECTRICALPROPERTIES:1||NIMNSB:1||PTMNSB:1||ROOMTEMPERATURE FERROMAGNETISM:1||RUBIDIUM MANGANESE HEXACYANOFERRATE:1||COLOSSALMAGNETORESISTANCE:1||FINITE TEMPERATURES:1||LAMNO3:1||FE:1||transitionmetal oxides:1||giant magnetoresistance:1||phonon:1||COPPER OXIDES:1||valence states:1||thermoelectric:1||semiconductor:1||CATION DISTRIBUTION:1||FeCr2S4:1||photoemission spectroscopy (PES):1||METALLIC FERROMAGNETISM:1||GRAPHITE:1||SUSCEPTIBILITY:1||UBE13:1||RCrSb3:1||band JahnTeller:1||Ce3S4:1||TiO2:1||PrBa2Cu3O7delta:1||UNTWINNED PRBA2CU3O7:1||AGNIO2:1||HALFMETALLIC FERROMAGNETS:1||CI:1||Energy gap:1||Photoemission:1||Future applications:1||Photoemission measurements:1||Graphene:1||BANDSTRUCTURE:1||TC:1||superconductivity:1||magnetic semiconductors:1||CMRmanganites:1||thin films:1||spin dynamics:1||highTc superconductors:1||ITINERANTELECTRON FERROMAGNETISM:1||SINGLECRYSTALS:1||CeTe2:1||amorphous magnetic materials:1||EPITAXIAL GRAPHENE:1||LAYERED PNICTIDEOXIDES:1||BOROCARBIDE SUPERCONDUCTORS:1||AUGMENTEDWAVE METHOD:1||METALLIC MAGNET UNISN:1||ORIGIN:1||spectrum rearrangement:1||MEANFIELD THEORY:1||MOLECULEBASED MAGNETS:1||METASTABLE STATE:1||INSULATOR:1||magnetic orderin:1||FCC IRON:1||CeRu2:1||TL2MN2O7:1||isotope effect:1||Perovskitemanganites:1||RECURSION METHOD:1||PERPENDICULAR MAGNETICANISOTROPY:1||quasiparticle spectral density:1||GW:1||MANGANESE FERRITE:1||RESONANCE:1||SeCuO3:1||Optical conductivity:1||MASSLESS DIRAC FERMIONS:1||SCHOTTKYBARRIER:1||electronic structure:15||ELECTRONICSTRUCTURE:11||TRANSITIONMETAL COMPOUNDS:10||METALS:10||photoemission:8||SPECTRA:8||MAGNETORESISTANCE:7||FERROMAGNETISM:7||TRANSPORT:7||TRANSITION:6||FILMS:6||THINFILMS:5||TOTALENERGY CALCULATIONS:5||MAGNETICPROPERTIES:5||SUPERCONDUCTIVITY:5||PR:5||LATTICE:4||STATES:4||SPECTROSCOPY:4||FIELD:4||CRYSTALSTRUCTURE:4||PHOTOEMISSION:4||TEMPERATURE:4||TRANSITIONTEMPERATURE:4||XRAYABSORPTION:4||STATE:4||CU:4||BASISSET:4||XAS:4||CRYSTALS:3||EXCITATIONS:3||MOTTHUBBARD SYSTEMS:3||HIGHENERGY SPIN:3||halfmetal:3||INSULATORS:3||LA2CUO4:3||MODEL:3||FLUCTUATIONS:3||CE:3||double exchange:3||TRANSITIONMETALS:3||RESISTIVITY:3||BORON:3||LA1XCAXMNO3:3||IRON:3||PES:3||ANTIMONIDES:2||MgB2:2||ZR METALLIC GLASSES:2||superconductor:2||CRITICALCURRENT DENSITY:2||CIRCULARDICHROISM:2||SEMICONDUCTORS:2||LOCALIZATION:2||INTRABAND OPTICAL CONDUCTIVITY:2||COLOSSAL MAGNETORESISTANCE:2||OXIDATION:2||EXISTENCE:2||COPPER:2||diboride:2||MAGNESIUMDIBORIDE:2||GAP:2||CE COMPOUNDS:2||CORE POLARIZATION:2||magnetoresistance:2||photoemission spectroscopy:2||electronphonon interaction:2||GETTER:2||PD:2||MAGNETISM:2||FECR2S4:2||SUPERCONDUCTING MGB2:2||WIRES:2||ABSORPTION:2||ENERGY:2||LA1XSRXMNO3:2||CONSTANTS:2||polaron:2||charge ordering:2||SCATTERING:2||XRAY PHOTOEMISSION:2||CeNiSn:2||phase diagram:2||PHOTOELECTRON:2||QUADRUPOLAR:2||perovskitemanganites:2||CO:2||SYSTEMS:2||DOPED ZNO:2||LOWFREQUENCY SOUND:2||LA:2||ELECTRONELECTRON SCATTERING:2||AU:2||DENSITYWAVE INSTABILITY:2||FERMISURFACE:2||hybridization:2||VALENCEBAND SATELLITE:2||SULFUR SPINEL:2||Heusler:2||APPROXIMATION:2||superexchange:2||colossal magnetoresistance:2||ALLOYS:2||DEPENDENCE:2||AG:2||electronic structures:2||AUGERSPECTRA:2||CR:2||PARAMETERS:2||DIFFRACTION:2||SEMICONDUCTORMETAL TRANSITION:1||INTERMEDIATEVALENCE:1||SMB6:1||SRRUO3:1||antiperovskite structure with antipolar nature:1||lowenergy twodimensional phonons:1||anatase TiO2:1||La3S4:1||metalinsulator transitions:1||MNO:1||ELECTRONICSTRUCTURES:1||MAGNETIC CIRCULARDICHROISM:1||Density functional theory:1||CeCo2:1||TOPOLARON CROSSOVER:1||EXCHANGE:1||cuprates:1||high Tc cuprates:1||magnetically ordered materials:1||ZNSE:1||Sr2xKxFeMoO6:1||CDW:1||TeCuO3:1||STRUCTURALPROPERTIES:1||MN:1||screening length:1||amorphous Fe:1||WAVE BASISSET:1||SILICONCARBIDE:1||HIGHPRESSURE:1||electronphonon coupling:1||quenched superconductivity:1||CMR perovskite manganites:1||OXIDE:1||polarons:1||synchrotron radiation:1||FULLERIDES:1||RESONANTPHOTOEMISSION:1||Silicon carbide:1||DFT calculation:1||Hybridized bands:1||GIANT MAGNETORESISTANCE:1||PEROVSKITES:1||Raman spectra:1||EXCHANGE ENHANCEMENT:1||SILICON:1||SR2FEMOO6:1||orbital ordering:1||delafossite:1||TITANIUMDIOXIDE:1||electronic structure of disordered solids:1||YFE2:1||Magnetic polaron:1||NA2TI2SB2O:1||STRONGCOUPLED SUPERCONDUCTORS:1||HEAVYFERMION SYSTEMS:1||firstprinciples calculations:1||MECHANISM:1||UNiSn:1||PHOTONIC BANDGAP:1||SINGLE IMPURITY:1||PHONONSPECTRUM:1||FERMISURFACE TOPOLOGY:1||SUPPRESSION:1||RESONANT PHOTOEMISSION:1||METALDOPED PICENE:1||PHOTOIONIZATION CROSSSECTIONS:1||PHOTOINDUCED FERRIMAGNETIC SYSTEMS:1||LINKAGE ISOMERISM:1||CHARGETRANSFER:1||Bilayer Graphene:1||MAGNETICFIELD:1||SPINWAVES:1||rareearth manganese oxides:1||magnonphonon interaction:1||NACO2O4:1||ENERGYBANDS:1||SELFENERGY:1||GAS:1||Fe0.5Cu0.5Cr2S4:1||scanning photoelectron microscopy (SPEM):1||MAGNETIC PROPERTIES:1||Stoner model:1||AMORPHOUS TRANSITIONMETALS:1||SPINGLASS STATES:1||NI:1||LA3NI2B2N3:1||SOLIDS:1||CEO2:1||BAND THEORY:1||dilute magnetic semiconductor:1||pyrochlore:1||Y1XPRXBA2CU3O7DELTA:1||and electronphonon interactions:1||VIBRATIONS:1||RAY PHOTOEMISSION:1||ALKALI CATION:1||Europium:1||colossal magnetoresistance:1||structural stability:1||ENERGYGAP:1||small polaron:1||DOUBLE EXCHANGE:1||Coulomb correlation:1||magnon:1||phonons:1||ELECTRON FERROMAGNETISM:1||CURIETEMPERATURE:1||ARPES:1||PLANEWAVE METHOD:1||Xray absorption spectroscopy (XAS):1||ROOMTEMPERATURE:1||MONOCHALCOGENIDES:1||HEAT:1||UPDSN:1||MOMENTS:1||XRAY ABSORPTION:1||SEMICONDUCTOR:1||Fermi surface nesting:1||optical phonon:1||disordered system:1||dilute magnetic semiconductors:1||CMR manganites:1||PHONONS:1||LATTICEDYNAMICS:1||OXIDES:1||4fphotoemission:1||permanent magnet:1||pseudogap:1||TRANSPORTPROPERTIES:1||ANTIFERROMAGNET:1||(BI,PB)SRCOO SYSTEM:1||semicore correlation:1||POLARIZATION:1||CRYSTAL:1||spinel:1||Xray magnetic circular dichroism (XMCD):1||magnetocapacitance:1||ANATASE:1||TEMPERATURES:1||Pseudogap:1||INTERFACE:1||SUBSTRATE:1||YNI2B2C:1||SAMARIUM SULFIDE:1||strong swave superconductor:1||DOPED MANGANITE:1||SYMMETRY:1||CENISN:1||resonance mode:1||DISORDERED SYSTEM:1||LITHIUM INTERCALATION:1||CUO2 PLANE:1||SURFACE:1||Delafossite:1||ELECTRICALPROPERTIES:1||NIMNSB:1||PTMNSB:1||ROOMTEMPERATURE FERROMAGNETISM:1||RUBIDIUM MANGANESE HEXACYANOFERRATE:1||COLOSSALMAGNETORESISTANCE:1||FINITE TEMPERATURES:1||LAMNO3:1||FE:1||transitionmetal oxides:1||giant magnetoresistance:1||phonon:1||COPPER OXIDES:1||valence states:1||thermoelectric:1||semiconductor:1||CATION DISTRIBUTION:1||FeCr2S4:1||photoemission spectroscopy (PES):1||METALLIC FERROMAGNETISM:1||GRAPHITE:1||SUSCEPTIBILITY:1||UBE13:1||RCrSb3:1||band JahnTeller:1||Ce3S4:1||TiO2:1||PrBa2Cu3O7delta:1||UNTWINNED PRBA2CU3O7:1||AGNIO2:1||HALFMETALLIC FERROMAGNETS:1||CI:1||Energy gap:1||Photoemission:1||Future applications:1||Photoemission measurements:1||Graphene:1||BANDSTRUCTURE:1||TC:1||superconductivity:1||magnetic semiconductors:1||CMRmanganites:1||thin films:1||spin dynamics:1||highTc superconductors:1||ITINERANTELECTRON FERROMAGNETISM:1||SINGLECRYSTALS:1||CeTe2:1||amorphous magnetic materials:1||EPITAXIAL GRAPHENE:1||LAYERED PNICTIDEOXIDES:1||BOROCARBIDE SUPERCONDUCTORS:1||AUGMENTEDWAVE METHOD:1||METALLIC MAGNET UNISN:1||ORIGIN:1||spectrum rearrangement:1||MEANFIELD THEORY:1||MOLECULEBASED MAGNETS:1||METASTABLE STATE:1||INSULATOR:1||magnetic orderin:1||FCC IRON:1||CeRu2:1||TL2MN2O7:1||isotope effect:1||Perovskitemanganites:1||RECURSION METHOD:1||PERPENDICULAR MAGNETICANISOTROPY:1||quasiparticle spectral density:1||GW:1||MANGANESE FERRITE:1||RESONANCE:1||SeCuO3:1||Optical conductivity:1||MASSLESS DIRAC FERMIONS:1||SCHOTTKYBARRIER:1||electronic structure:15||ELECTRONICSTRUCTURE:11||TRANSITIONMETAL COMPOUNDS:10||METALS:10||photoemission:8||SPECTRA:8||MAGNETORESISTANCE:7||FERROMAGNETISM:7||TRANSPORT:7||TRANSITION:6||FILMS:6||THINFILMS:5||TOTALENERGY CALCULATIONS:5||MAGNETICPROPERTIES:5||SUPERCONDUCTIVITY:5||PR:5||LATTICE:4||STATES:4||SPECTROSCOPY:4||FIELD:4||CRYSTALSTRUCTURE:4||PHOTOEMISSION:4||TEMPERATURE:4||TRANSITIONTEMPERATURE:4||XRAYABSORPTION:4||STATE:4||CU:4||BASISSET:4||XAS:4||CRYSTALS:3||EXCITATIONS:3||MOTTHUBBARD SYSTEMS:3||HIGHENERGY SPIN:3||halfmetal:3||INSULATORS:3||LA2CUO4:3||MODEL:3||FLUCTUATIONS:3||CE:3||double exchange:3||TRANSITIONMETALS:3||RESISTIVITY:3||BORON:3||LA1XCAXMNO3:3||IRON:3||PES:3||ANTIMONIDES:2||MgB2:2||ZR METALLIC GLASSES:2||superconductor:2||CRITICALCURRENT DENSITY:2||CIRCULARDICHROISM:2||SEMICONDUCTORS:2||LOCALIZATION:2||INTRABAND OPTICAL CONDUCTIVITY:2||COLOSSAL MAGNETORESISTANCE:2||OXIDATION:2||EXISTENCE:2||COPPER:2||diboride:2||MAGNESIUMDIBORIDE:2||GAP:2||CE COMPOUNDS:2||CORE POLARIZATION:2||magnetoresistance:2||photoemission spectroscopy:2||electronphonon interaction:2||GETTER:2||PD:2||MAGNETISM:2||FECR2S4:2||SUPERCONDUCTING MGB2:2||WIRES:2||ABSORPTION:2||ENERGY:2||LA1XSRXMNO3:2||CONSTANTS:2||polaron:2||charge ordering:2||SCATTERING:2||XRAY PHOTOEMISSION:2||CeNiSn:2||phase diagram:2||PHOTOELECTRON:2||QUADRUPOLAR:2||perovskitemanganites:2||CO:2||SYSTEMS:2||DOPED ZNO:2||LOWFREQUENCY SOUND:2||LA:2||ELECTRONELECTRON SCATTERING:2||AU:2||DENSITYWAVE INSTABILITY:2||FERMISURFACE:2||hybridization:2||VALENCEBAND SATELLITE:2||SULFUR SPINEL:2||Heusler:2||APPROXIMATION:2||superexchange:2||colossal magnetoresistance:2||ALLOYS:2||DEPENDENCE:2||AG:2||electronic structures:2||AUGERSPECTRA:2||CR:2||PARAMETERS:2||DIFFRACTION:2||SEMICONDUCTORMETAL TRANSITION:1||INTERMEDIATEVALENCE:1||SMB6:1||SRRUO3:1||antiperovskite structure with antipolar nature:1||lowenergy twodimensional phonons:1||anatase TiO2:1||La3S4:1||metalinsulator transitions:1||MNO:1||ELECTRONICSTRUCTURES:1||MAGNETIC CIRCULARDICHROISM:1||Density functional theory:1||CeCo2:1||TOPOLARON CROSSOVER:1||EXCHANGE:1||cuprates:1||high Tc cuprates:1||magnetically ordered materials:1||ZNSE:1||Sr2xKxFeMoO6:1||CDW:1||TeCuO3:1||STRUCTURALPROPERTIES:1||MN:1||screening length:1||amorphous Fe:1||WAVE BASISSET:1||SILICONCARBIDE:1||HIGHPRESSURE:1||electronphonon coupling:1||quenched superconductivity:1||CMR perovskite manganites:1||OXIDE:1||polarons:1||synchrotron radiation:1||FULLERIDES:1||RESONANTPHOTOEMISSION:1||Silicon carbide:1||DFT calculation:1||Hybridized bands:1||GIANT MAGNETORESISTANCE:1||PEROVSKITES:1||Raman spectra:1||EXCHANGE ENHANCEMENT:1||SILICON:1||SR2FEMOO6:1||orbital ordering:1||delafossite:1||TITANIUMDIOXIDE:1||electronic structure of disordered solids:1||YFE2:1||Magnetic polaron:1||NA2TI2SB2O:1||STRONGCOUPLED SUPERCONDUCTORS:1||HEAVYFERMION SYSTEMS:1||firstprinciples calculations:1||MECHANISM:1||UNiSn:1||PHOTONIC BANDGAP:1||SINGLE IMPURITY:1||PHONONSPECTRUM:1||FERMISURFACE TOPOLOGY:1||SUPPRESSION:1||RESONANT PHOTOEMISSION:1||METALDOPED PICENE:1||PHOTOIONIZATION CROSSSECTIONS:1||PHOTOINDUCED FERRIMAGNETIC SYSTEMS:1||LINKAGE ISOMERISM:1||CHARGETRANSFER:1||Bilayer Graphene:1||MAGNETICFIELD:1||SPINWAVES:1||rareearth manganese oxides:1||magnonphonon interaction:1||NACO2O4:1||ENERGYBANDS:1||SELFENERGY:1||GAS:1||Fe0.5Cu0.5Cr2S4:1||scanning photoelectron microscopy (SPEM):1||MAGNETIC PROPERTIES:1||Stoner model:1||AMORPHOUS TRANSITIONMETALS:1||SPINGLASS STATES:1||NI:1||LA3NI2B2N3:1||SOLIDS:1||CEO2:1||BAND THEORY:1||dilute magnetic semiconductor:1||pyrochlore:1||Y1XPRXBA2CU3O7DELTA:1||and electronphonon interactions:1||VIBRATIONS:1||RAY PHOTOEMISSION:1||ALKALI CATION:1||Europium:1||colossal magnetoresistance:1||structural stability:1||ENERGYGAP:1||small polaron:1||DOUBLE EXCHANGE:1||Coulomb correlation:1||magnon:1||phonons:1||ELECTRON FERROMAGNETISM:1||CURIETEMPERATURE:1||ARPES:1||PLANEWAVE METHOD:1||Xray absorption spectroscopy (XAS):1||ROOMTEMPERATURE:1||MONOCHALCOGENIDES:1||HEAT:1||UPDSN:1||MOMENTS:1||XRAY ABSORPTION:1||SEMICONDUCTOR:1||Fermi surface nesting:1||optical phonon:1||disordered system:1||dilute magnetic semiconductors:1||CMR manganites:1||PHONONS:1||LATTICEDYNAMICS:1||OXIDES:1||4fphotoemission:1||permanent magnet:1||pseudogap:1||TRANSPORTPROPERTIES:1||ANTIFERROMAGNET:1||(BI,PB)SRCOO SYSTEM:1||semicore correlation:1||POLARIZATION:1||CRYSTAL:1||spinel:1||Xray magnetic circular dichroism (XMCD):1||magnetocapacitance:1||ANATASE:1||TEMPERATURES:1||Pseudogap:1||INTERFACE:1||SUBSTRATE:1||YNI2B2C:1||SAMARIUM SULFIDE:1||strong swave superconductor:1||DOPED MANGANITE:1||SYMMETRY:1||CENISN:1||resonance mode:1||DISORDERED SYSTEM:1||LITHIUM INTERCALATION:1||CUO2 PLANE:1||SURFACE:1||Delafossite:1||ELECTRICALPROPERTIES:1||NIMNSB:1||PTMNSB:1||ROOMTEMPERATURE FERROMAGNETISM:1||RUBIDIUM MANGANESE HEXACYANOFERRATE:1||COLOSSALMAGNETORESISTANCE:1||FINITE TEMPERATURES:1||LAMNO3:1||FE:1||transitionmetal oxides:1||giant magnetoresistance:1||phonon:1||COPPER OXIDES:1||valence states:1||thermoelectric:1||semiconductor:1||CATION DISTRIBUTION:1||FeCr2S4:1||photoemission spectroscopy (PES):1||METALLIC FERROMAGNETISM:1||GRAPHITE:1||SUSCEPTIBILITY:1||UBE13:1||RCrSb3:1||band JahnTeller:1||Ce3S4:1||TiO2:1||PrBa2Cu3O7delta:1||UNTWINNED PRBA2CU3O7:1||AGNIO2:1||HALFMETALLIC FERROMAGNETS:1||CI:1||Energy gap:1||Photoemission:1||Future applications:1||Photoemission measurements:1||Graphene:1||BANDSTRUCTURE:1||TC:1||superconductivity:1||magnetic semiconductors:1||CMRmanganites:1||thin films:1||spin dynamics:1||highTc superconductors:1||ITINERANTELECTRON FERROMAGNETISM:1||SINGLECRYSTALS:1||CeTe2:1||amorphous magnetic materials:1||EPITAXIAL GRAPHENE:1||LAYERED PNICTIDEOXIDES:1||BOROCARBIDE SUPERCONDUCTORS:1||AUGMENTEDWAVE METHOD:1||METALLIC MAGNET UNISN:1||ORIGIN:1||spectrum rearrangement:1||MEANFIELD THEORY:1||MOLECULEBASED MAGNETS:1||METASTABLE STATE:1||INSULATOR:1||magnetic orderin:1||FCC IRON:1||CeRu2:1||TL2MN2O7:1||isotope effect:1||Perovskitemanganites:1||RECURSION METHOD:1||PERPENDICULAR MAGNETICANISOTROPY:1||quasiparticle spectral density:1||GW:1||MANGANESE FERRITE:1||RESONANCE:1||SeCuO3:1||Optical conductivity:1||MASSLESS DIRAC FERMIONS:1||SCHOTTKYBARRIER:1||electronic structure:15||ELECTRONICSTRUCTURE:11||TRANSITIONMETAL COMPOUNDS:10||METALS:10||photoemission:8||SPECTRA:8||MAGNETORESISTANCE:7||FERROMAGNETISM:7||TRANSPORT:7||TRANSITION:6||FILMS:6||THINFILMS:5||TOTALENERGY CALCULATIONS:5||MAGNETICPROPERTIES:5||SUPERCONDUCTIVITY:5||PR:5||LATTICE:4||STATES:4||SPECTROSCOPY:4||FIELD:4||CRYSTALSTRUCTURE:4||PHOTOEMISSION:4||TEMPERATURE:4||TRANSITIONTEMPERATURE:4||XRAYABSORPTION:4||STATE:4||CU:4||BASISSET:4||XAS:4||CRYSTALS:3||EXCITATIONS:3||MOTTHUBBARD SYSTEMS:3||HIGHENERGY SPIN:3||halfmetal:3||INSULATORS:3||LA2CUO4:3||MODEL:3||FLUCTUATIONS:3||CE:3||double exchange:3||TRANSITIONMETALS:3||RESISTIVITY:3||BORON:3||LA1XCAXMNO3:3||IRON:3||PES:3||ANTIMONIDES:2||MgB2:2||ZR METALLIC GLASSES:2||superconductor:2||CRITICALCURRENT DENSITY:2||CIRCULARDICHROISM:2||SEMICONDUCTORS:2||LOCALIZATION:2||INTRABAND OPTICAL CONDUCTIVITY:2||COLOSSAL MAGNETORESISTANCE:2||OXIDATION:2||EXISTENCE:2||COPPER:2||diboride:2||MAGNESIUMDIBORIDE:2||GAP:2||CE COMPOUNDS:2||CORE POLARIZATION:2||magnetoresistance:2||photoemission spectroscopy:2||electronphonon interaction:2||GETTER:2||PD:2||MAGNETISM:2||FECR2S4:2||SUPERCONDUCTING MGB2:2||WIRES:2||ABSORPTION:2||ENERGY:2||LA1XSRXMNO3:2||CONSTANTS:2||polaron:2||charge ordering:2||SCATTERING:2||XRAY PHOTOEMISSION:2||CeNiSn:2||phase diagram:2||PHOTOELECTRON:2||QUADRUPOLAR:2||perovskitemanganites:2||CO:2||SYSTEMS:2||DOPED ZNO:2||LOWFREQUENCY SOUND:2||LA:2||ELECTRONELECTRON SCATTERING:2||AU:2||DENSITYWAVE INSTABILITY:2||FERMISURFACE:2||hybridization:2||VALENCEBAND SATELLITE:2||SULFUR SPINEL:2||Heusler:2||APPROXIMATION:2||superexchange:2||colossal magnetoresistance:2||ALLOYS:2||DEPENDENCE:2||AG:2||electronic structures:2||AUGERSPECTRA:2||CR:2||PARAMETERS:2||DIFFRACTION:2||SEMICONDUCTORMETAL TRANSITION:1||INTERMEDIATEVALENCE:1||SMB6:1||SRRUO3:1||antiperovskite structure with antipolar nature:1||lowenergy twodimensional phonons:1||anatase TiO2:1||La3S4:1||metalinsulator transitions:1||MNO:1||ELECTRONICSTRUCTURES:1||MAGNETIC CIRCULARDICHROISM:1||Density functional theory:1||CeCo2:1||TOPOLARON CROSSOVER:1||EXCHANGE:1||cuprates:1||high Tc cuprates:1||magnetically ordered materials:1||ZNSE:1||Sr2xKxFeMoO6:1||CDW:1||TeCuO3:1||STRUCTURALPROPERTIES:1||MN:1||screening length:1||amorphous Fe:1||WAVE BASISSET:1||SILICONCARBIDE:1||HIGHPRESSURE:1||electronphonon coupling:1||quenched superconductivity:1||CMR perovskite manganites:1||OXIDE:1||polarons:1||synchrotron radiation:1||FULLERIDES:1||RESONANTPHOTOEMISSION:1||Silicon carbide:1||DFT calculation:1||Hybridized bands:1||GIANT MAGNETORESISTANCE:1||PEROVSKITES:1||Raman spectra:1||EXCHANGE ENHANCEMENT:1||SILICON:1||SR2FEMOO6:1||orbital ordering:1||delafossite:1||TITANIUMDIOXIDE:1||electronic structure of disordered solids:1||YFE2:1||Magnetic polaron:1||NA2TI2SB2O:1||STRONGCOUPLED SUPERCONDUCTORS:1||HEAVYFERMION SYSTEMS:1||firstprinciples calculations:1||MECHANISM:1||UNiSn:1||PHOTONIC BANDGAP:1||SINGLE IMPURITY:1||PHONONSPECTRUM:1||FERMISURFACE TOPOLOGY:1||SUPPRESSION:1||RESONANT PHOTOEMISSION:1||METALDOPED PICENE:1||PHOTOIONIZATION CROSSSECTIONS:1||PHOTOINDUCED FERRIMAGNETIC SYSTEMS:1||LINKAGE ISOMERISM:1||CHARGETRANSFER:1||Bilayer Graphene:1||MAGNETICFIELD:1||SPINWAVES:1||rareearth manganese oxides:1||magnonphonon interaction:1||NACO2O4:1||ENERGYBANDS:1||SELFENERGY:1||GAS:1||Fe0.5Cu0.5Cr2S4:1||scanning photoelectron microscopy (SPEM):1||MAGNETIC PROPERTIES:1||Stoner model:1||AMORPHOUS TRANSITIONMETALS:1||SPINGLASS STATES:1||NI:1||LA3NI2B2N3:1||SOLIDS:1||CEO2:1||BAND THEORY:1||dilute magnetic semiconductor:1||pyrochlore:1||Y1XPRXBA2CU3O7DELTA:1||and electronphonon interactions:1||VIBRATIONS:1||RAY PHOTOEMISSION:1||ALKALI CATION:1||Europium:1||colossal magnetoresistance:1||structural stability:1||ENERGYGAP:1||small polaron:1||DOUBLE EXCHANGE:1||Coulomb correlation:1||magnon:1||phonons:1||ELECTRON FERROMAGNETISM:1||CURIETEMPERATURE:1||ARPES:1||PLANEWAVE METHOD:1||Xray absorption spectroscopy (XAS):1||ROOMTEMPERATURE:1||MONOCHALCOGENIDES:1||HEAT:1||UPDSN:1||MOMENTS:1||XRAY ABSORPTION:1||SEMICONDUCTOR:1||Fermi surface nesting:1||optical phonon:1||disordered system:1||dilute magnetic semiconductors:1||CMR manganites:1||PHONONS:1||LATTICEDYNAMICS:1||OXIDES:1||4fphotoemission:1||permanent magnet:1||pseudogap:1||TRANSPORTPROPERTIES:1||ANTIFERROMAGNET:1||(BI,PB)SRCOO SYSTEM:1||semicore correlation:1||POLARIZATION:1||CRYSTAL:1||spinel:1||Xray magnetic circular dichroism (XMCD):1||magnetocapacitance:1||ANATASE:1||TEMPERATURES:1||Pseudogap:1||INTERFACE:1||SUBSTRATE:1||YNI2B2C:1||SAMARIUM SULFIDE:1||strong swave superconductor:1||DOPED MANGANITE:1||SYMMETRY:1||CENISN:1||resonance mode:1||DISORDERED SYSTEM:1||LITHIUM INTERCALATION:1||CUO2 PLANE:1||SURFACE:1||Delafossite:1||ELECTRICALPROPERTIES:1||NIMNSB:1||PTMNSB:1||ROOMTEMPERATURE FERROMAGNETISM:1||RUBIDIUM MANGANESE HEXACYANOFERRATE:1||COLOSSALMAGNETORESISTANCE:1||FINITE TEMPERATURES:1||LAMNO3:1||FE:1||transitionmetal oxides:1||giant magnetoresistance:1||phonon:1||COPPER OXIDES:1||valence states:1||thermoelectric:1||semiconductor:1||CATION DISTRIBUTION:1||FeCr2S4:1||photoemission spectroscopy (PES):1||METALLIC FERROMAGNETISM:1||GRAPHITE:1||SUSCEPTIBILITY:1||UBE13:1||RCrSb3:1||band JahnTeller:1||Ce3S4:1||TiO2:1||PrBa2Cu3O7delta:1||UNTWINNED PRBA2CU3O7:1||AGNIO2:1||HALFMETALLIC FERROMAGNETS:1||CI:1||Energy gap:1||Photoemission:1||Future applications:1||Photoemission measurements:1||Graphene:1||BANDSTRUCTURE:1||TC:1||superconductivity:1||magnetic semiconductors:1||CMRmanganites:1||thin films:1||spin dynamics:1||highTc superconductors:1||ITINERANTELECTRON FERROMAGNETISM:1||SINGLECRYSTALS:1||CeTe2:1||amorphous magnetic materials:1||EPITAXIAL GRAPHENE:1||LAYERED PNICTIDEOXIDES:1||BOROCARBIDE SUPERCONDUCTORS:1||AUGMENTEDWAVE METHOD:1||METALLIC MAGNET UNISN:1||ORIGIN:1||spectrum rearrangement:1||MEANFIELD THEORY:1||MOLECULEBASED MAGNETS:1||METASTABLE STATE:1||INSULATOR:1||magnetic orderin:1||FCC IRON:1||CeRu2:1||TL2MN2O7:1||isotope effect:1||Perovskitemanganites:1||RECURSION METHOD:1||PERPENDICULAR MAGNETICANISOTROPY:1||quasiparticle spectral density:1||GW:1||MANGANESE FERRITE:1||RESONANCE:1||SeCuO3:1||Optical conductivity:1||MASSLESS DIRAC FERMIONS:1||SCHOTTKYBARRIER:1||electronic structure:15||ELECTRONICSTRUCTURE:11||TRANSITIONMETAL COMPOUNDS:10||METALS:10||photoemission:8||SPECTRA:8||MAGNETORESISTANCE:7||FERROMAGNETISM:7||TRANSPORT:7||TRANSITION:6||FILMS:6||THINFILMS:5||TOTALENERGY CALCULATIONS:5||MAGNETICPROPERTIES:5||SUPERCONDUCTIVITY:5||PR:5||LATTICE:4||STATES:4||SPECTROSCOPY:4||FIELD:4||CRYSTALSTRUCTURE:4||PHOTOEMISSION:4||TEMPERATURE:4||TRANSITIONTEMPERATURE:4||XRAYABSORPTION:4||STATE:4||CU:4||BASISSET:4||XAS:4||CRYSTALS:3||EXCITATIONS:3||MOTTHUBBARD SYSTEMS:3||HIGHENERGY SPIN:3||halfmetal:3||INSULATORS:3||LA2CUO4:3||MODEL:3||FLUCTUATIONS:3||CE:3||double exchange:3||TRANSITIONMETALS:3||RESISTIVITY:3||BORON:3||LA1XCAXMNO3:3||IRON:3||PES:3||ANTIMONIDES:2||MgB2:2||ZR METALLIC GLASSES:2||superconductor:2||CRITICALCURRENT DENSITY:2||CIRCULARDICHROISM:2||SEMICONDUCTORS:2||LOCALIZATION:2||INTRABAND OPTICAL CONDUCTIVITY:2||COLOSSAL MAGNETORESISTANCE:2||OXIDATION:2||EXISTENCE:2||COPPER:2||diboride:2||MAGNESIUMDIBORIDE:2||GAP:2||CE COMPOUNDS:2||CORE POLARIZATION:2||magnetoresistance:2||photoemission spectroscopy:2||electronphonon interaction:2||GETTER:2||PD:2||MAGNETISM:2||FECR2S4:2||SUPERCONDUCTING MGB2:2||WIRES:2||ABSORPTION:2||ENERGY:2||LA1XSRXMNO3:2||CONSTANTS:2||polaron:2||charge ordering:2||SCATTERING:2||XRAY PHOTOEMISSION:2||CeNiSn:2||phase diagram:2||PHOTOELECTRON:2||QUADRUPOLAR:2||perovskitemanganites:2||CO:2||SYSTEMS:2||DOPED ZNO:2||LOWFREQUENCY SOUND:2||LA:2||ELECTRONELECTRON SCATTERING:2||AU:2||DENSITYWAVE INSTABILITY:2||FERMISURFACE:2||hybridization:2||VALENCEBAND SATELLITE:2||SULFUR SPINEL:2||Heusler:2||APPROXIMATION:2||superexchange:2||colossal magnetoresistance:2||ALLOYS:2||DEPENDENCE:2||AG:2||electronic structures:2||AUGERSPECTRA:2||CR:2||PARAMETERS:2||DIFFRACTION:2||SEMICONDUCTORMETAL TRANSITION:1||INTERMEDIATEVALENCE:1||SMB6:1||SRRUO3:1||antiperovskite structure with antipolar nature:1||lowenergy twodimensional phonons:1||anatase TiO2:1||La3S4:1||metalinsulator transitions:1||MNO:1||ELECTRONICSTRUCTURES:1||MAGNETIC CIRCULARDICHROISM:1||Density functional theory:1||CeCo2:1||TOPOLARON CROSSOVER:1||EXCHANGE:1||cuprates:1||high Tc cuprates:1||magnetically ordered materials:1||ZNSE:1||Sr2xKxFeMoO6:1||CDW:1||TeCuO3:1||STRUCTURALPROPERTIES:1||MN:1||screening length:1||amorphous Fe:1||WAVE BASISSET:1||SILICONCARBIDE:1||HIGHPRESSURE:1||electronphonon coupling:1||quenched superconductivity:1||CMR perovskite manganites:1||OXIDE:1||polarons:1||synchrotron radiation:1||FULLERIDES:1||RESONANTPHOTOEMISSION:1||Silicon carbide:1||DFT calculation:1||Hybridized bands:1||GIANT MAGNETORESISTANCE:1||PEROVSKITES:1||Raman spectra:1||EXCHANGE ENHANCEMENT:1||SILICON:1||SR2FEMOO6:1||orbital ordering:1||delafossite:1||TITANIUMDIOXIDE:1||electronic structure of disordered solids:1||YFE2:1||Magnetic polaron:1||NA2TI2SB2O:1||STRONGCOUPLED SUPERCONDUCTORS:1||HEAVYFERMION SYSTEMS:1||firstprinciples calculations:1||MECHANISM:1||UNiSn:1||PHOTONIC BANDGAP:1||SINGLE IMPURITY:1||PHONONSPECTRUM:1||FERMISURFACE TOPOLOGY:1||SUPPRESSION:1||RESONANT PHOTOEMISSION:1||METALDOPED PICENE:1||PHOTOIONIZATION CROSSSECTIONS:1||PHOTOINDUCED FERRIMAGNETIC SYSTEMS:1||LINKAGE ISOMERISM:1||CHARGETRANSFER:1||Bilayer Graphene:1||MAGNETICFIELD:1||SPINWAVES:1||rareearth manganese oxides:1||magnonphonon interaction:1||NACO2O4:1||ENERGYBANDS:1||SELFENERGY:1||GAS:1||Fe0.5Cu0.5Cr2S4:1||scanning photoelectron microscopy (SPEM):1||MAGNETIC PROPERTIES:1||Stoner model:1||AMORPHOUS TRANSITIONMETALS:1||SPINGLASS STATES:1||NI:1||LA3NI2B2N3:1||SOLIDS:1||CEO2:1||BAND THEORY:1||dilute magnetic semiconductor:1||pyrochlore:1||Y1XPRXBA2CU3O7DELTA:1||and electronphonon interactions:1||VIBRATIONS:1||RAY PHOTOEMISSION:1||ALKALI CATION:1||Europium:1||colossal magnetoresistance:1||structural stability:1||ENERGYGAP:1||small polaron:1||DOUBLE EXCHANGE:1||Coulomb correlation:1||magnon:1||phonons:1||ELECTRON FERROMAGNETISM:1||CURIETEMPERATURE:1||ARPES:1||PLANEWAVE METHOD:1||Xray absorption spectroscopy (XAS):1||ROOMTEMPERATURE:1||MONOCHALCOGENIDES:1||HEAT:1||UPDSN:1||MOMENTS:1||XRAY ABSORPTION:1||SEMICONDUCTOR:1||Fermi surface nesting:1||optical phonon:1||disordered system:1||dilute magnetic semiconductors:1||CMR manganites:1||PHONONS:1||LATTICEDYNAMICS:1||OXIDES:1||4fphotoemission:1||permanent magnet:1||pseudogap:1||TRANSPORTPROPERTIES:1||ANTIFERROMAGNET:1||(BI,PB)SRCOO SYSTEM:1||semicore correlation:1||POLARIZATION:1||CRYSTAL:1||spinel:1||Xray magnetic circular dichroism (XMCD):1||magnetocapacitance:1||ANATASE:1||TEMPERATURES:1||Pseudogap:1||INTERFACE:1||SUBSTRATE:1||YNI2B2C:1||SAMARIUM SULFIDE:1||strong swave superconductor:1||DOPED MANGANITE:1||SYMMETRY:1||CENISN:1||resonance mode:1||DISORDERED SYSTEM:1||LITHIUM INTERCALATION:1||CUO2 PLANE:1||SURFACE:1||Delafossite:1||ELECTRICALPROPERTIES:1||NIMNSB:1||PTMNSB:1||ROOMTEMPERATURE FERROMAGNETISM:1||RUBIDIUM MANGANESE HEXACYANOFERRATE:1||COLOSSALMAGNETORESISTANCE:1||FINITE TEMPERATURES:1||LAMNO3:1||FE:1||transitionmetal oxides:1||giant magnetoresistance:1||phonon:1||COPPER OXIDES:1||valence states:1||thermoelectric:1||semiconductor:1||CATION DISTRIBUTION:1||FeCr2S4:1||photoemission spectroscopy (PES):1||METALLIC FERROMAGNETISM:1||GRAPHITE:1||SUSCEPTIBILITY:1||UBE13:1||RCrSb3:1||band JahnTeller:1||Ce3S4:1||TiO2:1||PrBa2Cu3O7delta:1||UNTWINNED PRBA2CU3O7:1||AGNIO2:1||HALFMETALLIC FERROMAGNETS:1||CI:1||Energy gap:1||Photoemission:1||Future applications:1||Photoemission measurements:1||Graphene:1||BANDSTRUCTURE:1||TC:1||superconductivity:1||magnetic semiconductors:1||CMRmanganites:1||thin films:1||spin dynamics:1||highTc superconductors:1||ITINERANTELECTRON FERROMAGNETISM:1||SINGLECRYSTALS:1||CeTe2:1||amorphous magnetic materials:1||EPITAXIAL GRAPHENE:1||LAYERED PNICTIDEOXIDES:1||BOROCARBIDE SUPERCONDUCTORS:1||AUGMENTEDWAVE METHOD:1||METALLIC MAGNET UNISN:1||ORIGIN:1||spectrum rearrangement:1||MEANFIELD THEORY:1||MOLECULEBASED MAGNETS:1||METASTABLE STATE:1||INSULATOR:1||magnetic orderin:1||FCC IRON:1||CeRu2:1||TL2MN2O7:1||isotope effect:1||Perovskitemanganites:1||RECURSION METHOD:1||PERPENDICULAR MAGNETICANISOTROPY:1||quasiparticle spectral density:1||GW:1||MANGANESE FERRITE:1||RESONANCE:1||SeCuO3:1||Optical conductivity:1||MASSLESS DIRAC FERMIONS:1||SCHOTTKYBARRIER:1||electronic structure:15||ELECTRONICSTRUCTURE:11||TRANSITIONMETAL COMPOUNDS:10||METALS:10||photoemission:8||SPECTRA:8||MAGNETORESISTANCE:7||FERROMAGNETISM:7||TRANSPORT:7||TRANSITION:6||FILMS:6||THINFILMS:5||TOTALENERGY CALCULATIONS:5||MAGNETICPROPERTIES:5||SUPERCONDUCTIVITY:5||PR:5||LATTICE:4||STATES:4||SPECTROSCOPY:4||FIELD:4||CRYSTALSTRUCTURE:4||PHOTOEMISSION:4||TEMPERATURE:4||TRANSITIONTEMPERATURE:4||XRAYABSORPTION:4||STATE:4||CU:4||BASISSET:4||XAS:4||CRYSTALS:3||EXCITATIONS:3||MOTTHUBBARD SYSTEMS:3||HIGHENERGY SPIN:3||halfmetal:3||INSULATORS:3||LA2CUO4:3||MODEL:3||FLUCTUATIONS:3||CE:3||double exchange:3||TRANSITIONMETALS:3||RESISTIVITY:3||BORON:3||LA1XCAXMNO3:3||IRON:3||PES:3||ANTIMONIDES:2||MgB2:2||ZR METALLIC GLASSES:2||superconductor:2||CRITICALCURRENT DENSITY:2||CIRCULARDICHROISM:2||SEMICONDUCTORS:2||LOCALIZATION:2||INTRABAND OPTICAL CONDUCTIVITY:2||COLOSSAL MAGNETORESISTANCE:2||OXIDATION:2||EXISTENCE:2||COPPER:2||diboride:2||MAGNESIUMDIBORIDE:2||GAP:2||CE COMPOUNDS:2||CORE POLARIZATION:2||magnetoresistance:2||photoemission spectroscopy:2||electronphonon interaction:2||GETTER:2||PD:2||MAGNETISM:2||FECR2S4:2||SUPERCONDUCTING MGB2:2||WIRES:2||ABSORPTION:2||ENERGY:2||LA1XSRXMNO3:2||CONSTANTS:2||polaron:2||charge ordering:2||SCATTERING:2||XRAY PHOTOEMISSION:2||CeNiSn:2||phase diagram:2||PHOTOELECTRON:2||QUADRUPOLAR:2||perovskitemanganites:2||CO:2||SYSTEMS:2||DOPED ZNO:2||LOWFREQUENCY SOUND:2||LA:2||ELECTRONELECTRON SCATTERING:2||AU:2||DENSITYWAVE INSTABILITY:2||FERMISURFACE:2||hybridization:2||VALENCEBAND SATELLITE:2||SULFUR SPINEL:2||Heusler:2||APPROXIMATION:2||superexchange:2||colossal magnetoresistance:2||ALLOYS:2||DEPENDENCE:2||AG:2||electronic structures:2||AUGERSPECTRA:2||CR:2||PARAMETERS:2||DIFFRACTION:2||SEMICONDUCTORMETAL TRANSITION:1||INTERMEDIATEVALENCE:1||SMB6:1||SRRUO3:1||antiperovskite structure with antipolar nature:1||lowenergy twodimensional phonons:1||anatase TiO2:1||La3S4:1||metalinsulator transitions:1||MNO:1||ELECTRONICSTRUCTURES:1||MAGNETIC CIRCULARDICHROISM:1||Density functional theory:1||CeCo2:1||TOPOLARON CROSSOVER:1||EXCHANGE:1||cuprates:1||high Tc cuprates:1||magnetically ordered materials:1||ZNSE:1||Sr2xKxFeMoO6:1||CDW:1||TeCuO3:1||STRUCTURALPROPERTIES:1||MN:1||screening length:1||amorphous Fe:1||WAVE BASISSET:1||SILICONCARBIDE:1||HIGHPRESSURE:1||electronphonon coupling:1||quenched superconductivity:1||CMR perovskite manganites:1||OXIDE:1||polarons:1||synchrotron radiation:1||FULLERIDES:1||RESONANTPHOTOEMISSION:1||Silicon carbide:1||DFT calculation:1||Hybridized bands:1||GIANT MAGNETORESISTANCE:1||PEROVSKITES:1||Raman spectra:1||EXCHANGE ENHANCEMENT:1||SILICON:1||SR2FEMOO6:1||orbital ordering:1||delafossite:1||TITANIUMDIOXIDE:1||electronic structure of disordered solids:1||YFE2:1||Magnetic polaron:1||NA2TI2SB2O:1||STRONGCOUPLED SUPERCONDUCTORS:1||HEAVYFERMION SYSTEMS:1||firstprinciples calculations:1||MECHANISM:1||UNiSn:1||PHOTONIC BANDGAP:1||SINGLE IMPURITY:1||PHONONSPECTRUM:1||FERMISURFACE TOPOLOGY:1||SUPPRESSION:1||RESONANT PHOTOEMISSION:1||METALDOPED PICENE:1||PHOTOIONIZATION CROSSSECTIONS:1||PHOTOINDUCED FERRIMAGNETIC SYSTEMS:1||LINKAGE ISOMERISM:1||CHARGETRANSFER:1||Bilayer Graphene:1||MAGNETICFIELD:1||SPINWAVES:1||rareearth manganese oxides:1||magnonphonon interaction:1||NACO2O4:1||ENERGYBANDS:1||SELFENERGY:1||GAS:1||Fe0.5Cu0.5Cr2S4:1||scanning photoelectron microscopy (SPEM):1||MAGNETIC PROPERTIES:1||Stoner model:1||AMORPHOUS TRANSITIONMETALS:1||SPINGLASS STATES:1||NI:1||LA3NI2B2N3:1||SOLIDS:1||CEO2:1||BAND THEORY:1||dilute magnetic semiconductor:1||pyrochlore:1||Y1XPRXBA2CU3O7DELTA:1||and electronphonon interactions:1||VIBRATIONS:1||RAY PHOTOEMISSION:1||ALKALI CATION:1||Europium:1||colossal magnetoresistance:1||structural stability:1||ENERGYGAP:1||small polaron:1||DOUBLE EXCHANGE:1||Coulomb correlation:1||magnon:1||phonons:1||ELECTRON FERROMAGNETISM:1||CURIETEMPERATURE:1||ARPES:1||PLANEWAVE METHOD:1||Xray absorption spectroscopy (XAS):1||ROOMTEMPERATURE:1||MONOCHALCOGENIDES:1||HEAT:1||UPDSN:1||MOMENTS:1||XRAY ABSORPTION:1||SEMICONDUCTOR:1||Fermi surface nesting:1||optical phonon:1||disordered system:1||dilute magnetic semiconductors:1||CMR manganites:1||PHONONS:1||LATTICEDYNAMICS:1||OXIDES:1||4fphotoemission:1||permanent magnet:1||pseudogap:1||TRANSPORTPROPERTIES:1||ANTIFERROMAGNET:1||(BI,PB)SRCOO SYSTEM:1||semicore correlation:1||POLARIZATION:1||CRYSTAL:1||spinel:1||Xray magnetic circular dichroism (XMCD):1||magnetocapacitance:1||ANATASE:1||TEMPERATURES:1||Pseudogap:1||INTERFACE:1||SUBSTRATE:1||YNI2B2C:1||SAMARIUM SULFIDE:1||strong swave superconductor:1||DOPED MANGANITE:1||SYMMETRY:1||CENISN:1||resonance mode:1||DISORDERED SYSTEM:1||LITHIUM INTERCALATION:1||CUO2 PLANE:1||SURFACE:1||Delafossite:1||ELECTRICALPROPERTIES:1||NIMNSB:1||PTMNSB:1||ROOMTEMPERATURE FERROMAGNETISM:1||RUBIDIUM MANGANESE HEXACYANOFERRATE:1||COLOSSALMAGNETORESISTANCE:1||FINITE TEMPERATURES:1||LAMNO3:1||FE:1||transitionmetal oxides:1||giant magnetoresistance:1||phonon:1||COPPER OXIDES:1||valence states:1||thermoelectric:1||semiconductor:1||CATION DISTRIBUTION:1||FeCr2S4:1||photoemission spectroscopy (PES):1||METALLIC FERROMAGNETISM:1||GRAPHITE:1||SUSCEPTIBILITY:1||UBE13:1||RCrSb3:1||band JahnTeller:1||Ce3S4:1||TiO2:1||PrBa2Cu3O7delta:1||UNTWINNED PRBA2CU3O7:1||AGNIO2:1||HALFMETALLIC FERROMAGNETS:1||CI:1||Energy gap:1||Photoemission:1||Future applications:1||Photoemission measurements:1||Graphene:1||BANDSTRUCTURE:1||TC:1||superconductivity:1||magnetic semiconductors:1||CMRmanganites:1||thin films:1||spin dynamics:1||highTc superconductors:1||ITINERANTELECTRON FERROMAGNETISM:1||SINGLECRYSTALS:1||CeTe2:1||amorphous magnetic materials:1||EPITAXIAL GRAPHENE:1||LAYERED PNICTIDEOXIDES:1||BOROCARBIDE SUPERCONDUCTORS:1||AUGMENTEDWAVE METHOD:1||METALLIC MAGNET UNISN:1||ORIGIN:1||spectrum rearrangement:1||MEANFIELD THEORY:1||MOLECULEBASED MAGNETS:1||METASTABLE STATE:1||INSULATOR:1||magnetic orderin:1||FCC IRON:1||CeRu2:1||TL2MN2O7:1||isotope effect:1||Perovskitemanganites:1||RECURSION METHOD:1||PERPENDICULAR MAGNETICANISOTROPY:1||quasiparticle spectral density:1||GW:1||MANGANESE FERRITE:1||RESONANCE:1||SeCuO3:1||Optical conductivity:1||MASSLESS DIRAC FERMIONS:1||SCHOTTKYBARRIER:1||electronic structure:15||ELECTRONICSTRUCTURE:11||TRANSITIONMETAL COMPOUNDS:10||METALS:10||photoemission:8||SPECTRA:8||MAGNETORESISTANCE:7||FERROMAGNETISM:7||TRANSPORT:7||TRANSITION:6||FILMS:6||THINFILMS:5||TOTALENERGY CALCULATIONS:5||MAGNETICPROPERTIES:5||SUPERCONDUCTIVITY:5||PR:5||LATTICE:4||STATES:4||SPECTROSCOPY:4||FIELD:4||CRYSTALSTRUCTURE:4||PHOTOEMISSION:4||TEMPERATURE:4||TRANSITIONTEMPERATURE:4||XRAYABSORPTION:4||STATE:4||CU:4||BASISSET:4||XAS:4||CRYSTALS:3||EXCITATIONS:3||MOTTHUBBARD SYSTEMS:3||HIGHENERGY SPIN:3||halfmetal:3||INSULATORS:3||LA2CUO4:3||MODEL:3||FLUCTUATIONS:3||CE:3||double exchange:3||TRANSITIONMETALS:3||RESISTIVITY:3||BORON:3||LA1XCAXMNO3:3||IRON:3||PES:3||ANTIMONIDES:2||MgB2:2||ZR METALLIC GLASSES:2||superconductor:2||CRITICALCURRENT DENSITY:2||CIRCULARDICHROISM:2||SEMICONDUCTORS:2||LOCALIZATION:2||INTRABAND OPTICAL CONDUCTIVITY:2||COLOSSAL MAGNETORESISTANCE:2||OXIDATION:2||EXISTENCE:2||COPPER:2||diboride:2||MAGNESIUMDIBORIDE:2||GAP:2||CE COMPOUNDS:2||CORE POLARIZATION:2||magnetoresistance:2||photoemission spectroscopy:2||electronphonon interaction:2||GETTER:2||PD:2||MAGNETISM:2||FECR2S4:2||SUPERCONDUCTING MGB2:2||WIRES:2||ABSORPTION:2||ENERGY:2||LA1XSRXMNO3:2||CONSTANTS:2||polaron:2||charge ordering:2||SCATTERING:2||XRAY PHOTOEMISSION:2||CeNiSn:2||phase diagram:2||PHOTOELECTRON:2||QUADRUPOLAR:2||perovskitemanganites:2||CO:2||SYSTEMS:2||DOPED ZNO:2||LOWFREQUENCY SOUND:2||LA:2||ELECTRONELECTRON SCATTERING:2||AU:2||DENSITYWAVE INSTABILITY:2||FERMISURFACE:2||hybridization:2||VALENCEBAND SATELLITE:2||SULFUR SPINEL:2||Heusler:2||APPROXIMATION:2||superexchange:2||colossal magnetoresistance:2||ALLOYS:2||DEPENDENCE:2||AG:2||electronic structures:2||AUGERSPECTRA:2||CR:2||PARAMETERS:2||DIFFRACTION:2||SEMICONDUCTORMETAL TRANSITION:1||INTERMEDIATEVALENCE:1||SMB6:1||SRRUO3:1||antiperovskite structure with antipolar nature:1||lowenergy twodimensional phonons:1||anatase TiO2:1||La3S4:1||metalinsulator transitions:1||MNO:1||ELECTRONICSTRUCTURES:1||MAGNETIC CIRCULARDICHROISM:1||Density functional theory:1||CeCo2:1||TOPOLARON CROSSOVER:1||EXCHANGE:1||cuprates:1||high Tc cuprates:1||magnetically ordered materials:1||ZNSE:1||Sr2xKxFeMoO6:1||CDW:1||TeCuO3:1||STRUCTURALPROPERTIES:1||MN:1||screening length:1||amorphous Fe:1||WAVE BASISSET:1||SILICONCARBIDE:1||HIGHPRESSURE:1||electronphonon coupling:1||quenched superconductivity:1||CMR perovskite manganites:1||OXIDE:1||polarons:1||synchrotron radiation:1||FULLERIDES:1||RESONANTPHOTOEMISSION:1||Silicon carbide:1||DFT calculation:1||Hybridized bands:1||GIANT MAGNETORESISTANCE:1||PEROVSKITES:1||Raman spectra:1||EXCHANGE ENHANCEMENT:1||SILICON:1||SR2FEMOO6:1||orbital ordering:1||delafossite:1||TITANIUMDIOXIDE:1||electronic structure of disordered solids:1||YFE2:1||Magnetic polaron:1||NA2TI2SB2O:1||STRONGCOUPLED SUPERCONDUCTORS:1||HEAVYFERMION SYSTEMS:1||firstprinciples calculations:1||MECHANISM:1||UNiSn:1||PHOTONIC BANDGAP:1||SINGLE IMPURITY:1||PHONONSPECTRUM:1||FERMISURFACE TOPOLOGY:1||SUPPRESSION:1||RESONANT PHOTOEMISSION:1||METALDOPED PICENE:1||PHOTOIONIZATION CROSSSECTIONS:1||PHOTOINDUCED FERRIMAGNETIC SYSTEMS:1||LINKAGE ISOMERISM:1||CHARGETRANSFER:1||Bilayer Graphene:1||MAGNETICFIELD:1||SPINWAVES:1||rareearth manganese oxides:1||magnonphonon interaction:1||NACO2O4:1||ENERGYBANDS:1||SELFENERGY:1||GAS:1||Fe0.5Cu0.5Cr2S4:1||scanning photoelectron microscopy (SPEM):1||MAGNETIC PROPERTIES:1||Stoner model:1||AMORPHOUS TRANSITIONMETALS:1||SPINGLASS STATES:1||NI:1||LA3NI2B2N3:1||SOLIDS:1||CEO2:1||BAND THEORY:1||dilute magnetic semiconductor:1||pyrochlore:1||Y1XPRXBA2CU3O7DELTA:1||and electronphonon interactions:1||VIBRATIONS:1||RAY PHOTOEMISSION:1||ALKALI CATION:1||Europium:1||colossal magnetoresistance:1||structural stability:1||ENERGYGAP:1||small polaron:1||DOUBLE EXCHANGE:1||Coulomb correlation:1||magnon:1||phonons:1||ELECTRON FERROMAGNETISM:1||CURIETEMPERATURE:1||ARPES:1||PLANEWAVE METHOD:1||Xray absorption spectroscopy (XAS):1||ROOMTEMPERATURE:1||MONOCHALCOGENIDES:1||HEAT:1||UPDSN:1||MOMENTS:1||XRAY ABSORPTION:1||SEMICONDUCTOR:1||Fermi surface nesting:1||optical phonon:1||disordered system:1||dilute magnetic semiconductors:1||CMR manganites:1||PHONONS:1||LATTICEDYNAMICS:1||OXIDES:1||4fphotoemission:1||permanent magnet:1||pseudogap:1||TRANSPORTPROPERTIES:1||ANTIFERROMAGNET:1||(BI,PB)SRCOO SYSTEM:1||semicore correlation:1||POLARIZATION:1||CRYSTAL:1||spinel:1||Xray magnetic circular dichroism (XMCD):1||magnetocapacitance:1||ANATASE:1||TEMPERATURES:1||Pseudogap:1||INTERFACE:1||SUBSTRATE:1||YNI2B2C:1||SAMARIUM SULFIDE:1||strong swave superconductor:1||DOPED MANGANITE:1||SYMMETRY:1||CENISN:1||resonance mode:1||DISORDERED SYSTEM:1||LITHIUM INTERCALATION:1||CUO2 PLANE:1||SURFACE:1||Delafossite:1||ELECTRICALPROPERTIES:1||NIMNSB:1||PTMNSB:1||ROOMTEMPERATURE FERROMAGNETISM:1||RUBIDIUM MANGANESE HEXACYANOFERRATE:1||COLOSSALMAGNETORESISTANCE:1||FINITE TEMPERATURES:1||LAMNO3:1||FE:1||transitionmetal oxides:1||giant magnetoresistance:1||phonon:1||COPPER OXIDES:1||valence states:1||thermoelectric:1||semiconductor:1||CATION DISTRIBUTION:1||FeCr2S4:1||photoemission spectroscopy (PES):1||METALLIC FERROMAGNETISM:1||GRAPHITE:1||SUSCEPTIBILITY:1||UBE13:1||RCrSb3:1||band JahnTeller:1||Ce3S4:1||TiO2:1||PrBa2Cu3O7delta:1||UNTWINNED PRBA2CU3O7:1||AGNIO2:1||HALFMETALLIC FERROMAGNETS:1||CI:1||Energy gap:1||Photoemission:1||Future applications:1||Photoemission measurements:1||Graphene:1||BANDSTRUCTURE:1||TC:1||superconductivity:1||magnetic semiconductors:1||CMRmanganites:1||thin films:1||spin dynamics:1||highTc superconductors:1||ITINERANTELECTRON FERROMAGNETISM:1||SINGLECRYSTALS:1||CeTe2:1||amorphous magnetic materials:1||EPITAXIAL GRAPHENE:1||LAYERED PNICTIDEOXIDES:1||BOROCARBIDE SUPERCONDUCTORS:1||AUGMENTEDWAVE METHOD:1||METALLIC MAGNET UNISN:1||ORIGIN:1||spectrum rearrangement:1||MEANFIELD THEORY:1||MOLECULEBASED MAGNETS:1||METASTABLE STATE:1||INSULATOR:1||magnetic orderin:1||FCC IRON:1||CeRu2:1||TL2MN2O7:1||isotope effect:1||Perovskitemanganites:1||RECURSION METHOD:1||PERPENDICULAR MAGNETICANISOTROPY:1||quasiparticle spectral density:1||GW:1||MANGANESE FERRITE:1||RESONANCE:1||SeCuO3:1||Optical conductivity:1||MASSLESS DIRAC FERMIONS:1||SCHOTTKYBARRIER:1||electronic structure:15||ELECTRONICSTRUCTURE:11||TRANSITIONMETAL COMPOUNDS:10||METALS:10||photoemission:8||SPECTRA:8||MAGNETORESISTANCE:7||FERROMAGNETISM:7||TRANSPORT:7||TRANSITION:6||FILMS:6||THINFILMS:5||TOTALENERGY CALCULATIONS:5||MAGNETICPROPERTIES:5||SUPERCONDUCTIVITY:5||PR:5||LATTICE:4||STATES:4||SPECTROSCOPY:4||FIELD:4||CRYSTALSTRUCTURE:4||PHOTOEMISSION:4||TEMPERATURE:4||TRANSITIONTEMPERATURE:4||XRAYABSORPTION:4||STATE:4||CU:4||BASISSET:4||XAS:4||CRYSTALS:3||EXCITATIONS:3||MOTTHUBBARD SYSTEMS:3||HIGHENERGY SPIN:3||halfmetal:3||INSULATORS:3||LA2CUO4:3||MODEL:3||FLUCTUATIONS:3||CE:3||double exchange:3||TRANSITIONMETALS:3||RESISTIVITY:3||BORON:3||LA1XCAXMNO3:3||IRON:3||PES:3||ANTIMONIDES:2||MgB2:2||ZR METALLIC GLASSES:2||superconductor:2||CRITICALCURRENT DENSITY:2||CIRCULARDICHROISM:2||SEMICONDUCTORS:2||LOCALIZATION:2||INTRABAND OPTICAL CONDUCTIVITY:2||COLOSSAL MAGNETORESISTANCE:2||OXIDATION:2||EXISTENCE:2||COPPER:2||diboride:2||MAGNESIUMDIBORIDE:2||GAP:2||CE COMPOUNDS:2||CORE POLARIZATION:2||magnetoresistance:2||photoemission spectroscopy:2||electronphonon interaction:2||GETTER:2||PD:2||MAGNETISM:2||FECR2S4:2||SUPERCONDUCTING MGB2:2||WIRES:2||ABSORPTION:2||ENERGY:2||LA1XSRXMNO3:2||CONSTANTS:2||polaron:2||charge ordering:2||SCATTERING:2||XRAY PHOTOEMISSION:2||CeNiSn:2||phase diagram:2||PHOTOELECTRON:2||QUADRUPOLAR:2||perovskitemanganites:2||CO:2||SYSTEMS:2||DOPED ZNO:2||LOWFREQUENCY SOUND:2||LA:2||ELECTRONELECTRON SCATTERING:2||AU:2||DENSITYWAVE INSTABILITY:2||FERMISURFACE:2||hybridization:2||VALENCEBAND SATELLITE:2||SULFUR SPINEL:2||Heusler:2||APPROXIMATION:2||superexchange:2||colossal magnetoresistance:2||ALLOYS:2||DEPENDENCE:2||AG:2||electronic structures:2||AUGERSPECTRA:2||CR:2||PARAMETERS:2||DIFFRACTION:2||SEMICONDUCTORMETAL TRANSITION:1||INTERMEDIATEVALENCE:1||SMB6:1||SRRUO3:1||antiperovskite structure with antipolar nature:1||lowenergy twodimensional phonons:1||anatase TiO2:1||La3S4:1||metalinsulator transitions:1||MNO:1||ELECTRONICSTRUCTURES:1||MAGNETIC CIRCULARDICHROISM:1||Density functional theory:1||CeCo2:1||TOPOLARON CROSSOVER:1||EXCHANGE:1||cuprates:1||high Tc cuprates:1||magnetically ordered materials:1||ZNSE:1||Sr2xKxFeMoO6:1||CDW:1||TeCuO3:1||STRUCTURALPROPERTIES:1||MN:1||screening length:1||amorphous Fe:1||WAVE BASISSET:1||SILICONCARBIDE:1||HIGHPRESSURE:1||electronphonon coupling:1||quenched superconductivity:1||CMR perovskite manganites:1||OXIDE:1||polarons:1||synchrotron radiation:1||FULLERIDES:1||RESONANTPHOTOEMISSION:1||Silicon carbide:1||DFT calculation:1||Hybridized bands:1||GIANT MAGNETORESISTANCE:1||PEROVSKITES:1||Raman spectra:1||EXCHANGE ENHANCEMENT:1||SILICON:1||SR2FEMOO6:1||orbital ordering:1||delafossite:1||TITANIUMDIOXIDE:1||electronic structure of disordered solids:1||YFE2:1||Magnetic polaron:1||NA2TI2SB2O:1||STRONGCOUPLED SUPERCONDUCTORS:1||HEAVYFERMION SYSTEMS:1||firstprinciples calculations:1||MECHANISM:1||UNiSn:1||PHOTONIC BANDGAP:1||SINGLE IMPURITY:1||PHONONSPECTRUM:1||FERMISURFACE TOPOLOGY:1||SUPPRESSION:1||RESONANT PHOTOEMISSION:1||METALDOPED PICENE:1||PHOTOIONIZATION CROSSSECTIONS:1||PHOTOINDUCED FERRIMAGNETIC SYSTEMS:1||LINKAGE ISOMERISM:1||CHARGETRANSFER:1||Bilayer Graphene:1||MAGNETICFIELD:1||SPINWAVES:1||rareearth manganese oxides:1||magnonphonon interaction:1||NACO2O4:1||ENERGYBANDS:1||SELFENERGY:1||GAS:1||Fe0.5Cu0.5Cr2S4:1||scanning photoelectron microscopy (SPEM):1||MAGNETIC PROPERTIES:1||Stoner model:1||AMORPHOUS TRANSITIONMETALS:1||SPINGLASS STATES:1||NI:1||LA3NI2B2N3:1||SOLIDS:1||CEO2:1||BAND THEORY:1||dilute magnetic semiconductor:1||pyrochlore:1||Y1XPRXBA2CU3O7DELTA:1||and electronphonon interactions:1||VIBRATIONS:1||RAY PHOTOEMISSION:1||ALKALI CATION:1||Europium:1||colossal magnetoresistance:1||structural stability:1||ENERGYGAP:1||small polaron:1||DOUBLE EXCHANGE:1||Coulomb correlation:1||magnon:1||phonons:1||ELECTRON FERROMAGNETISM:1||CURIETEMPERATURE:1||ARPES:1||PLANEWAVE METHOD:1||Xray absorption spectroscopy (XAS):1||ROOMTEMPERATURE:1||MONOCHALCOGENIDES:1||HEAT:1||UPDSN:1||MOMENTS:1||XRAY ABSORPTION:1||SEMICONDUCTOR:1||Fermi surface nesting:1||optical phonon:1||disordered system:1||dilute magnetic semiconductors:1||CMR manganites:1||PHONONS:1||LATTICEDYNAMICS:1||OXIDES:1||4fphotoemission:1||permanent magnet:1||pseudogap:1||TRANSPORTPROPERTIES:1||ANTIFERROMAGNET:1||(BI,PB)SRCOO SYSTEM:1||semicore correlation:1||POLARIZATION:1||CRYSTAL:1||spinel:1||Xray magnetic circular dichroism (XMCD):1||magnetocapacitance:1||ANATASE:1||TEMPERATURES:1||Pseudogap:1||INTERFACE:1||SUBSTRATE:1||YNI2B2C:1||SAMARIUM SULFIDE:1||strong swave superconductor:1||DOPED MANGANITE:1||SYMMETRY:1||CENISN:1||resonance mode:1||DISORDERED SYSTEM:1||LITHIUM INTERCALATION:1||CUO2 PLANE:1||SURFACE:1||Delafossite:1||ELECTRICALPROPERTIES:1||NIMNSB:1||PTMNSB:1||ROOMTEMPERATURE FERROMAGNETISM:1||RUBIDIUM MANGANESE HEXACYANOFERRATE:1||COLOSSALMAGNETORESISTANCE:1||FINITE TEMPERATURES:1||LAMNO3:1||FE:1||transitionmetal oxides:1||giant magnetoresistance:1||phonon:1||COPPER OXIDES:1||valence states:1||thermoelectric:1||semiconductor:1||CATION DISTRIBUTION:1||FeCr2S4:1||photoemission spectroscopy (PES):1||METALLIC FERROMAGNETISM:1||GRAPHITE:1||SUSCEPTIBILITY:1||UBE13:1||RCrSb3:1||band JahnTeller:1||Ce3S4:1||TiO2:1||PrBa2Cu3O7delta:1||UNTWINNED PRBA2CU3O7:1||AGNIO2:1||HALFMETALLIC FERROMAGNETS:1||CI:1||Energy gap:1||Photoemission:1||Future applications:1||Photoemission measurements:1||Graphene:1||BANDSTRUCTURE:1||TC:1||superconductivity:1||magnetic semiconductors:1||CMRmanganites:1||thin films:1||spin dynamics:1||highTc superconductors:1||ITINERANTELECTRON FERROMAGNETISM:1||SINGLECRYSTALS:1||CeTe2:1||amorphous magnetic materials:1||EPITAXIAL GRAPHENE:1||LAYERED PNICTIDEOXIDES:1||BOROCARBIDE SUPERCONDUCTORS:1||AUGMENTEDWAVE METHOD:1||METALLIC MAGNET UNISN:1||ORIGIN:1||spectrum rearrangement:1||MEANFIELD THEORY:1||MOLECULEBASED MAGNETS:1||METASTABLE STATE:1||INSULATOR:1||magnetic orderin:1||FCC IRON:1||CeRu2:1||TL2MN2O7:1||isotope effect:1||Perovskitemanganites:1||RECURSION METHOD:1||PERPENDICULAR MAGNETICANISOTROPY:1||quasiparticle spectral density:1||GW:1||MANGANESE FERRITE:1||RESONANCE:1||SeCuO3:1||Optical conductivity:1||MASSLESS DIRAC FERMIONS:1||SCHOTTKYBARRIER:1||electronic structure:15||ELECTRONICSTRUCTURE:11||TRANSITIONMETAL COMPOUNDS:10||METALS:10||photoemission:8||SPECTRA:8||MAGNETORESISTANCE:7||FERROMAGNETISM:7||TRANSPORT:7||TRANSITION:6||FILMS:6||THINFILMS:5||TOTALENERGY CALCULATIONS:5||MAGNETICPROPERTIES:5||SUPERCONDUCTIVITY:5||PR:5||LATTICE:4||STATES:4||SPECTROSCOPY:4||FIELD:4||CRYSTALSTRUCTURE:4||PHOTOEMISSION:4||TEMPERATURE:4||TRANSITIONTEMPERATURE:4||XRAYABSORPTION:4||STATE:4||CU:4||BASISSET:4||XAS:4||CRYSTALS:3||EXCITATIONS:3||MOTTHUBBARD SYSTEMS:3||HIGHENERGY SPIN:3||halfmetal:3||INSULATORS:3||LA2CUO4:3||MODEL:3||FLUCTUATIONS:3||CE:3||double exchange:3||TRANSITIONMETALS:3||RESISTIVITY:3||BORON:3||LA1XCAXMNO3:3||IRON:3||PES:3||ANTIMONIDES:2||MgB2:2||ZR METALLIC GLASSES:2||superconductor:2||CRITICALCURRENT DENSITY:2||CIRCULARDICHROISM:2||SEMICONDUCTORS:2||LOCALIZATION:2||INTRABAND OPTICAL CONDUCTIVITY:2||COLOSSAL MAGNETORESISTANCE:2||OXIDATION:2||EXISTENCE:2||COPPER:2||diboride:2||MAGNESIUMDIBORIDE:2||GAP:2||CE COMPOUNDS:2||CORE POLARIZATION:2||magnetoresistance:2||photoemission spectroscopy:2||electronphonon interaction:2||GETTER:2||PD:2||MAGNETISM:2||FECR2S4:2||SUPERCONDUCTING MGB2:2||WIRES:2||ABSORPTION:2||ENERGY:2||LA1XSRXMNO3:2||CONSTANTS:2||polaron:2||charge ordering:2||SCATTERING:2||XRAY PHOTOEMISSION:2||CeNiSn:2||phase diagram:2||PHOTOELECTRON:2||QUADRUPOLAR:2||perovskitemanganites:2||CO:2||SYSTEMS:2||DOPED ZNO:2||LOWFREQUENCY SOUND:2||LA:2||ELECTRONELECTRON SCATTERING:2||AU:2||DENSITYWAVE INSTABILITY:2||FERMISURFACE:2||hybridization:2||VALENCEBAND SATELLITE:2||SULFUR SPINEL:2||Heusler:2||APPROXIMATION:2||superexchange:2||colossal magnetoresistance:2||ALLOYS:2||DEPENDENCE:2||AG:2||electronic structures:2||AUGERSPECTRA:2||CR:2||PARAMETERS:2||DIFFRACTION:2||SEMICONDUCTORMETAL TRANSITION:1||INTERMEDIATEVALENCE:1||SMB6:1||SRRUO3:1||antiperovskite structure with antipolar nature:1||lowenergy twodimensional phonons:1||anatase TiO2:1||La3S4:1||metalinsulator transitions:1||MNO:1||ELECTRONICSTRUCTURES:1||MAGNETIC CIRCULARDICHROISM:1||Density functional theory:1||CeCo2:1||TOPOLARON CROSSOVER:1||EXCHANGE:1||cuprates:1||high Tc cuprates:1||magnetically ordered materials:1||ZNSE:1||Sr2xKxFeMoO6:1||CDW:1||TeCuO3:1||STRUCTURALPROPERTIES:1||MN:1||screening length:1||amorphous Fe:1||WAVE BASISSET:1||SILICONCARBIDE:1||HIGHPRESSURE:1||electronphonon coupling:1||quenched superconductivity:1||CMR perovskite manganites:1||OXIDE:1||polarons:1||synchrotron radiation:1||FULLERIDES:1||RESONANTPHOTOEMISSION:1||Silicon carbide:1||DFT calculation:1||Hybridized bands:1||GIANT MAGNETORESISTANCE:1||PEROVSKITES:1||Raman spectra:1||EXCHANGE ENHANCEMENT:1||SILICON:1||SR2FEMOO6:1||orbital ordering:1||delafossite:1||TITANIUMDIOXIDE:1||electronic structure of disordered solids:1||YFE2:1||Magnetic polaron:1||NA2TI2SB2O:1||STRONGCOUPLED SUPERCONDUCTORS:1||HEAVYFERMION SYSTEMS:1||firstprinciples calculations:1||MECHANISM:1||UNiSn:1||PHOTONIC BANDGAP:1||SINGLE IMPURITY:1||PHONONSPECTRUM:1||FERMISURFACE TOPOLOGY:1||SUPPRESSION:1||RESONANT PHOTOEMISSION:1||METALDOPED PICENE:1||PHOTOIONIZATION CROSSSECTIONS:1||PHOTOINDUCED FERRIMAGNETIC SYSTEMS:1||LINKAGE ISOMERISM:1||CHARGETRANSFER:1||Bilayer Graphene:1||MAGNETICFIELD:1||SPINWAVES:1||rareearth manganese oxides:1||magnonphonon interaction:1||NACO2O4:1||ENERGYBANDS:1||SELFENERGY:1||GAS:1||Fe0.5Cu0.5Cr2S4:1||scanning photoelectron microscopy (SPEM):1||MAGNETIC PROPERTIES:1||Stoner model:1||AMORPHOUS TRANSITIONMETALS:1||SPINGLASS STATES:1||NI:1||LA3NI2B2N3:1||SOLIDS:1||CEO2:1||BAND THEORY:1||dilute magnetic semiconductor:1||pyrochlore:1||Y1XPRXBA2CU3O7DELTA:1||and electronphonon interactions:1||VIBRATIONS:1||RAY PHOTOEMISSION:1||ALKALI CATION:1||Europium:1||colossal magnetoresistance:1||structural stability:1||ENERGYGAP:1||small polaron:1||DOUBLE EXCHANGE:1||Coulomb correlation:1||magnon:1||phonons:1||ELECTRON FERROMAGNETISM:1||CURIETEMPERATURE:1||ARPES:1||PLANEWAVE METHOD:1||Xray absorption spectroscopy (XAS):1||ROOMTEMPERATURE:1||MONOCHALCOGENIDES:1||HEAT:1||UPDSN:1||MOMENTS:1||XRAY ABSORPTION:1||SEMICONDUCTOR:1||Fermi surface nesting:1||optical phonon:1||disordered system:1||dilute magnetic semiconductors:1||CMR manganites:1||PHONONS:1||LATTICEDYNAMICS:1||OXIDES:1||4fphotoemission:1||permanent magnet:1||pseudogap:1||TRANSPORTPROPERTIES:1||ANTIFERROMAGNET:1||(BI,PB)SRCOO SYSTEM:1||semicore correlation:1||POLARIZATION:1||CRYSTAL:1||spinel:1||Xray magnetic circular dichroism (XMCD):1||magnetocapacitance:1||ANATASE:1||TEMPERATURES:1||Pseudogap:1||INTERFACE:1||SUBSTRATE:1||YNI2B2C:1||SAMARIUM SULFIDE:1||strong swave superconductor:1||DOPED MANGANITE:1||SYMMETRY:1||CENISN:1||resonance mode:1||DISORDERED SYSTEM:1||LITHIUM INTERCALATION:1||CUO2 PLANE:1||SURFACE:1||Delafossite:1||ELECTRICALPROPERTIES:1||NIMNSB:1||PTMNSB:1||ROOMTEMPERATURE FERROMAGNETISM:1||RUBIDIUM MANGANESE HEXACYANOFERRATE:1||COLOSSALMAGNETORESISTANCE:1||FINITE TEMPERATURES:1||LAMNO3:1||FE:1||transitionmetal oxides:1||giant magnetoresistance:1||phonon:1||COPPER OXIDES:1||valence states:1||thermoelectric:1||semiconductor:1||CATION DISTRIBUTION:1||FeCr2S4:1||photoemission spectroscopy (PES):1||METALLIC FERROMAGNETISM:1||GRAPHITE:1||SUSCEPTIBILITY:1||UBE13:1||RCrSb3:1||band JahnTeller:1||Ce3S4:1||TiO2:1||PrBa2Cu3O7delta:1||UNTWINNED PRBA2CU3O7:1||AGNIO2:1||HALFMETALLIC FERROMAGNETS:1||CI:1||Energy gap:1||Photoemission:1||Future applications:1||Photoemission measurements:1||Graphene:1||BANDSTRUCTURE:1||TC:1||superconductivity:1||magnetic semiconductors:1||CMRmanganites:1||thin films:1||spin dynamics:1||highTc superconductors:1||ITINERANTELECTRON FERROMAGNETISM:1||SINGLECRYSTALS:1||CeTe2:1||amorphous magnetic materials:1||EPITAXIAL GRAPHENE:1||LAYERED PNICTIDEOXIDES:1||BOROCARBIDE SUPERCONDUCTORS:1||AUGMENTEDWAVE METHOD:1||METALLIC MAGNET UNISN:1||ORIGIN:1||spectrum rearrangement:1||MEANFIELD THEORY:1||MOLECULEBASED MAGNETS:1||METASTABLE STATE:1||INSULATOR:1||magnetic orderin:1||FCC IRON:1||CeRu2:1||TL2MN2O7:1||isotope effect:1||Perovskitemanganites:1||RECURSION METHOD:1||PERPENDICULAR MAGNETICANISOTROPY:1||quasiparticle spectral density:1||GW:1||MANGANESE FERRITE:1||RESONANCE:1||SeCuO3:1||Optical conductivity:1||MASSLESS DIRAC FERMIONS:1||SCHOTTKYBARRIER:1||electronic structure:15||ELECTRONICSTRUCTURE:11||TRANSITIONMETAL COMPOUNDS:10||METALS:10||photoemission:8||SPECTRA:8||MAGNETORESISTANCE:7||FERROMAGNETISM:7||TRANSPORT:7||TRANSITION:6||FILMS:6||THINFILMS:5||TOTALENERGY CALCULATIONS:5||MAGNETICPROPERTIES:5||SUPERCONDUCTIVITY:5||PR:5||LATTICE:4||STATES:4||SPECTROSCOPY:4||FIELD:4||CRYSTALSTRUCTURE:4||PHOTOEMISSION:4||TEMPERATURE:4||TRANSITIONTEMPERATURE:4||XRAYABSORPTION:4||STATE:4||CU:4||BASISSET:4||XAS:4||CRYSTALS:3||EXCITATIONS:3||MOTTHUBBARD SYSTEMS:3||HIGHENERGY SPIN:3||halfmetal:3||INSULATORS:3||LA2CUO4:3||MODEL:3||FLUCTUATIONS:3||CE:3||double exchange:3||TRANSITIONMETALS:3||RESISTIVITY:3||BORON:3||LA1XCAXMNO3:3||IRON:3||PES:3||ANTIMONIDES:2||MgB2:2||ZR METALLIC GLASSES:2||superconductor:2||CRITICALCURRENT DENSITY:2||CIRCULARDICHROISM:2||SEMICONDUCTORS:2||LOCALIZATION:2||INTRABAND OPTICAL CONDUCTIVITY:2||COLOSSAL MAGNETORESISTANCE:2||OXIDATION:2||EXISTENCE:2||COPPER:2||diboride:2||MAGNESIUMDIBORIDE:2||GAP:2||CE COMPOUNDS:2||CORE POLARIZATION:2||magnetoresistance:2||photoemission spectroscopy:2||electronphonon interaction:2||GETTER:2||PD:2||MAGNETISM:2||FECR2S4:2||SUPERCONDUCTING MGB2:2||WIRES:2||ABSORPTION:2||ENERGY:2||LA1XSRXMNO3:2||CONSTANTS:2||polaron:2||charge ordering:2||SCATTERING:2||XRAY PHOTOEMISSION:2||CeNiSn:2||phase diagram:2||PHOTOELECTRON:2||QUADRUPOLAR:2||perovskitemanganites:2||CO:2||SYSTEMS:2||DOPED ZNO:2||LOWFREQUENCY SOUND:2||LA:2||ELECTRONELECTRON SCATTERING:2||AU:2||DENSITYWAVE INSTABILITY:2||FERMISURFACE:2||hybridization:2||VALENCEBAND SATELLITE:2||SULFUR SPINEL:2||Heusler:2||APPROXIMATION:2||superexchange:2||colossal magnetoresistance:2||ALLOYS:2||DEPENDENCE:2||AG:2||electronic structures:2||AUGERSPECTRA:2||CR:2||PARAMETERS:2||DIFFRACTION:2||SEMICONDUCTORMETAL TRANSITION:1||INTERMEDIATEVALENCE:1||SMB6:1||SRRUO3:1||antiperovskite structure with antipolar nature:1||lowenergy twodimensional phonons:1||anatase TiO2:1||La3S4:1||metalinsulator transitions:1||MNO:1||ELECTRONICSTRUCTURES:1||MAGNETIC CIRCULARDICHROISM:1||Density functional theory:1||CeCo2:1||TOPOLARON CROSSOVER:1||EXCHANGE:1||cuprates:1||high Tc cuprates:1||magnetically ordered materials:1||ZNSE:1||Sr2xKxFeMoO6:1||CDW:1||TeCuO3:1||STRUCTURALPROPERTIES:1||MN:1||screening length:1||amorphous Fe:1||WAVE BASISSET:1||SILICONCARBIDE:1||HIGHPRESSURE:1||electronphonon coupling:1||quenched superconductivity:1||CMR perovskite manganites:1||OXIDE:1||polarons:1||synchrotron radiation:1||FULLERIDES:1||RESONANTPHOTOEMISSION:1||Silicon carbide:1||DFT calculation:1||Hybridized bands:1||GIANT MAGNETORESISTANCE:1||PEROVSKITES:1||Raman spectra:1||EXCHANGE ENHANCEMENT:1||SILICON:1||SR2FEMOO6:1||orbital ordering:1||delafossite:1||TITANIUMDIOXIDE:1||electronic structure of disordered solids:1||YFE2:1||Magnetic polaron:1||NA2TI2SB2O:1||STRONGCOUPLED SUPERCONDUCTORS:1||HEAVYFERMION SYSTEMS:1||firstprinciples calculations:1||MECHANISM:1||UNiSn:1||PHOTONIC BANDGAP:1||SINGLE IMPURITY:1||PHONONSPECTRUM:1||FERMISURFACE TOPOLOGY:1||SUPPRESSION:1||RESONANT PHOTOEMISSION:1||METALDOPED PICENE:1||PHOTOIONIZATION CROSSSECTIONS:1||PHOTOINDUCED FERRIMAGNETIC SYSTEMS:1||LINKAGE ISOMERISM:1||CHARGETRANSFER:1||Bilayer Graphene:1||MAGNETICFIELD:1||SPINWAVES:1||rareearth manganese oxides:1||magnonphonon interaction:1||NACO2O4:1||ENERGYBANDS:1||SELFENERGY:1||GAS:1||Fe0.5Cu0.5Cr2S4:1||scanning photoelectron microscopy (SPEM):1||MAGNETIC PROPERTIES:1||Stoner model:1||AMORPHOUS TRANSITIONMETALS:1||SPINGLASS STATES:1||NI:1||LA3NI2B2N3:1||SOLIDS:1||CEO2:1||BAND THEORY:1||dilute magnetic semiconductor:1||pyrochlore:1||Y1XPRXBA2CU3O7DELTA:1||and electronphonon interactions:1||VIBRATIONS:1||RAY PHOTOEMISSION:1||ALKALI CATION:1||Europium:1||colossal magnetoresistance:1||structural stability:1||ENERGYGAP:1||small polaron:1||DOUBLE EXCHANGE:1||Coulomb correlation:1||magnon:1||phonons:1||ELECTRON FERROMAGNETISM:1||CURIETEMPERATURE:1||ARPES:1||PLANEWAVE METHOD:1||Xray absorption spectroscopy (XAS):1||ROOMTEMPERATURE:1||MONOCHALCOGENIDES:1||HEAT:1||UPDSN:1||MOMENTS:1||XRAY ABSORPTION:1||SEMICONDUCTOR:1||Fermi surface nesting:1||optical phonon:1||disordered system:1||dilute magnetic semiconductors:1||CMR manganites:1||PHONONS:1||LATTICEDYNAMICS:1||OXIDES:1||4fphotoemission:1||permanent magnet:1||pseudogap:1||TRANSPORTPROPERTIES:1||ANTIFERROMAGNET:1||(BI,PB)SRCOO SYSTEM:1||semicore correlation:1||POLARIZATION:1||CRYSTAL:1||spinel:1||Xray magnetic circular dichroism (XMCD):1||magnetocapacitance:1||ANATASE:1||TEMPERATURES:1||Pseudogap:1||INTERFACE:1||SUBSTRATE:1||YNI2B2C:1||SAMARIUM SULFIDE:1||strong swave superconductor:1||DOPED MANGANITE:1||SYMMETRY:1||CENISN:1||resonance mode:1||DISORDERED SYSTEM:1||LITHIUM INTERCALATION:1||CUO2 PLANE:1||SURFACE:1||Delafossite:1||ELECTRICALPROPERTIES:1||NIMNSB:1||PTMNSB:1||ROOMTEMPERATURE FERROMAGNETISM:1||RUBIDIUM MANGANESE HEXACYANOFERRATE:1||COLOSSALMAGNETORESISTANCE:1||FINITE TEMPERATURES:1||LAMNO3:1||FE:1||transitionmetal oxides:1||giant magnetoresistance:1||phonon:1||COPPER OXIDES:1||valence states:1||thermoelectric:1||semiconductor:1||CATION DISTRIBUTION:1||FeCr2S4:1||photoemission spectroscopy (PES):1||METALLIC FERROMAGNETISM:1||GRAPHITE:1||SUSCEPTIBILITY:1||UBE13:1||RCrSb3:1||band JahnTeller:1||Ce3S4:1||TiO2:1||PrBa2Cu3O7delta:1||UNTWINNED PRBA2CU3O7:1||AGNIO2:1||HALFMETALLIC FERROMAGNETS:1||CI:1||Energy gap:1||Photoemission:1||Future applications:1||Photoemission measurements:1||Graphene:1||BANDSTRUCTURE:1||TC:1||superconductivity:1||magnetic semiconductors:1||CMRmanganites:1||thin films:1||spin dynamics:1||highTc superconductors:1||ITINERANTELECTRON FERROMAGNETISM:1||SINGLECRYSTALS:1||CeTe2:1||amorphous magnetic materials:1||EPITAXIAL GRAPHENE:1||LAYERED PNICTIDEOXIDES:1||BOROCARBIDE SUPERCONDUCTORS:1||AUGMENTEDWAVE METHOD:1||METALLIC MAGNET UNISN:1||ORIGIN:1||spectrum rearrangement:1||MEANFIELD THEORY:1||MOLECULEBASED MAGNETS:1||METASTABLE STATE:1||INSULATOR:1||magnetic orderin:1||FCC IRON:1||CeRu2:1||TL2MN2O7:1||isotope effect:1||Perovskitemanganites:1||RECURSION METHOD:1||PERPENDICULAR MAGNETICANISOTROPY:1||quasiparticle spectral density:1||GW:1||MANGANESE FERRITE:1||RESONANCE:1||SeCuO3:1||Optical conductivity:1||MASSLESS DIRAC FERMIONS:1||SCHOTTKYBARRIER:1||electronic structure:15||ELECTRONICSTRUCTURE:11||TRANSITIONMETAL COMPOUNDS:10||METALS:10||photoemission:8||SPECTRA:8||MAGNETORESISTANCE:7||FERROMAGNETISM:7||TRANSPORT:7||TRANSITION:6||FILMS:6||THINFILMS:5||TOTALENERGY CALCULATIONS:5||MAGNETICPROPERTIES:5||SUPERCONDUCTIVITY:5||PR:5||LATTICE:4||STATES:4||SPECTROSCOPY:4||FIELD:4||CRYSTALSTRUCTURE:4||PHOTOEMISSION:4||TEMPERATURE:4||TRANSITIONTEMPERATURE:4||XRAYABSORPTION:4||STATE:4||CU:4||BASISSET:4||XAS:4||CRYSTALS:3||EXCITATIONS:3||MOTTHUBBARD SYSTEMS:3||HIGHENERGY SPIN:3||halfmetal:3||INSULATORS:3||LA2CUO4:3||MODEL:3||FLUCTUATIONS:3||CE:3||double exchange:3||TRANSITIONMETALS:3||RESISTIVITY:3||BORON:3||LA1XCAXMNO3:3||IRON:3||PES:3||ANTIMONIDES:2||MgB2:2||ZR METALLIC GLASSES:2||superconductor:2||CRITICALCURRENT DENSITY:2||CIRCULARDICHROISM:2||SEMICONDUCTORS:2||LOCALIZATION:2||INTRABAND OPTICAL CONDUCTIVITY:2||COLOSSAL MAGNETORESISTANCE:2||OXIDATION:2||EXISTENCE:2||COPPER:2||diboride:2||MAGNESIUMDIBORIDE:2||GAP:2||CE COMPOUNDS:2||CORE POLARIZATION:2||magnetoresistance:2||photoemission spectroscopy:2||electronphonon interaction:2||GETTER:2||PD:2||MAGNETISM:2||FECR2S4:2||SUPERCONDUCTING MGB2:2||WIRES:2||ABSORPTION:2||ENERGY:2||LA1XSRXMNO3:2||CONSTANTS:2||polaron:2||charge ordering:2||SCATTERING:2||XRAY PHOTOEMISSION:2||CeNiSn:2||phase diagram:2||PHOTOELECTRON:2||QUADRUPOLAR:2||perovskitemanganites:2||CO:2||SYSTEMS:2||DOPED ZNO:2||LOWFREQUENCY SOUND:2||LA:2||ELECTRONELECTRON SCATTERING:2||AU:2||DENSITYWAVE INSTABILITY:2||FERMISURFACE:2||hybridization:2||VALENCEBAND SATELLITE:2||SULFUR SPINEL:2||Heusler:2||APPROXIMATION:2||superexchange:2||colossal magnetoresistance:2||ALLOYS:2||DEPENDENCE:2||AG:2||electronic structures:2||AUGERSPECTRA:2||CR:2||PARAMETERS:2||DIFFRACTION:2||SEMICONDUCTORMETAL TRANSITION:1||INTERMEDIATEVALENCE:1||SMB6:1||SRRUO3:1||antiperovskite structure with antipolar nature:1||lowenergy twodimensional phonons:1||anatase TiO2:1||La3S4:1||metalinsulator transitions:1||MNO:1||ELECTRONICSTRUCTURES:1||MAGNETIC CIRCULARDICHROISM:1||Density functional theory:1||CeCo2:1||TOPOLARON CROSSOVER:1||EXCHANGE:1||cuprates:1||high Tc cuprates:1||magnetically ordered materials:1||ZNSE:1||Sr2xKxFeMoO6:1||CDW:1||TeCuO3:1||STRUCTURALPROPERTIES:1||MN:1||screening length:1||amorphous Fe:1||WAVE BASISSET:1||SILICONCARBIDE:1||HIGHPRESSURE:1||electronphonon coupling:1||quenched superconductivity:1||CMR perovskite manganites:1||OXIDE:1||polarons:1||synchrotron radiation:1||FULLERIDES:1||RESONANTPHOTOEMISSION:1||Silicon carbide:1||DFT calculation:1||Hybridized bands:1||GIANT MAGNETORESISTANCE:1||PEROVSKITES:1||Raman spectra:1||EXCHANGE ENHANCEMENT:1||SILICON:1||SR2FEMOO6:1||orbital ordering:1||delafossite:1||TITANIUMDIOXIDE:1||electronic structure of disordered solids:1||YFE2:1||Magnetic polaron:1||NA2TI2SB2O:1||STRONGCOUPLED SUPERCONDUCTORS:1||HEAVYFERMION SYSTEMS:1||firstprinciples calculations:1||MECHANISM:1||UNiSn:1||PHOTONIC BANDGAP:1||SINGLE IMPURITY:1||PHONONSPECTRUM:1||FERMISURFACE TOPOLOGY:1||SUPPRESSION:1||RESONANT PHOTOEMISSION:1||METALDOPED PICENE:1||PHOTOIONIZATION CROSSSECTIONS:1||PHOTOINDUCED FERRIMAGNETIC SYSTEMS:1||LINKAGE ISOMERISM:1||CHARGETRANSFER:1||Bilayer Graphene:1||MAGNETICFIELD:1||SPINWAVES:1||rareearth manganese oxides:1||magnonphonon interaction:1||NACO2O4:1||ENERGYBANDS:1||SELFENERGY:1||GAS:1||Fe0.5Cu0.5Cr2S4:1||scanning photoelectron microscopy (SPEM):1||MAGNETIC PROPERTIES:1||Stoner model:1||AMORPHOUS TRANSITIONMETALS:1||SPINGLASS STATES:1||NI:1||LA3NI2B2N3:1||SOLIDS:1||CEO2:1||BAND THEORY:1||dilute magnetic semiconductor:1||pyrochlore:1||Y1XPRXBA2CU3O7DELTA:1||and electronphonon interactions:1||VIBRATIONS:1||RAY PHOTOEMISSION:1||ALKALI CATION:1||Europium:1||colossal magnetoresistance:1||structural stability:1||ENERGYGAP:1||small polaron:1||DOUBLE EXCHANGE:1||Coulomb correlation:1||magnon:1||phonons:1||ELECTRON FERROMAGNETISM:1||CURIETEMPERATURE:1||ARPES:1||PLANEWAVE METHOD:1||Xray absorption spectroscopy (XAS):1||ROOMTEMPERATURE:1||MONOCHALCOGENIDES:1||HEAT:1||UPDSN:1||MOMENTS:1||XRAY ABSORPTION:1||SEMICONDUCTOR:1||Fermi surface nesting:1||optical phonon:1||disordered system:1||dilute magnetic semiconductors:1||CMR manganites:1||PHONONS:1||LATTICEDYNAMICS:1||OXIDES:1||4fphotoemission:1||permanent magnet:1||pseudogap:1||TRANSPORTPROPERTIES:1||ANTIFERROMAGNET:1||(BI,PB)SRCOO SYSTEM:1||semicore correlation:1||POLARIZATION:1||CRYSTAL:1||spinel:1||Xray magnetic circular dichroism (XMCD):1||magnetocapacitance:1||ANATASE:1||TEMPERATURES:1||Pseudogap:1||INTERFACE:1||SUBSTRATE:1||YNI2B2C:1||SAMARIUM SULFIDE:1||strong swave superconductor:1||DOPED MANGANITE:1||SYMMETRY:1||CENISN:1||resonance mode:1||DISORDERED SYSTEM:1||LITHIUM INTERCALATION:1||CUO2 PLANE:1||SURFACE:1||Delafossite:1||ELECTRICALPROPERTIES:1||NIMNSB:1||PTMNSB:1||ROOMTEMPERATURE FERROMAGNETISM:1||RUBIDIUM MANGANESE HEXACYANOFERRATE:1||COLOSSALMAGNETORESISTANCE:1||FINITE TEMPERATURES:1||LAMNO3:1||FE:1||transitionmetal oxides:1||giant magnetoresistance:1||phonon:1||COPPER OXIDES:1||valence states:1||thermoelectric:1||semiconductor:1||CATION DISTRIBUTION:1||FeCr2S4:1||photoemission spectroscopy (PES):1||METALLIC FERROMAGNETISM:1||GRAPHITE:1||SUSCEPTIBILITY:1||UBE13:1||RCrSb3:1||band JahnTeller:1||Ce3S4:1||TiO2:1||PrBa2Cu3O7delta:1||UNTWINNED PRBA2CU3O7:1||AGNIO2:1||HALFMETALLIC FERROMAGNETS:1||CI:1||Energy gap:1||Photoemission:1||Future applications:1||Photoemission measurements:1||Graphene:1||BANDSTRUCTURE:1||TC:1||superconductivity:1||magnetic semiconductors:1||CMRmanganites:1||thin films:1||spin dynamics:1||highTc superconductors:1||ITINERANTELECTRON FERROMAGNETISM:1||SINGLECRYSTALS:1||CeTe2:1||amorphous magnetic materials:1||EPITAXIAL GRAPHENE:1||LAYERED PNICTIDEOXIDES:1||BOROCARBIDE SUPERCONDUCTORS:1||AUGMENTEDWAVE METHOD:1||METALLIC MAGNET UNISN:1||ORIGIN:1||spectrum rearrangement:1||MEANFIELD THEORY:1||MOLECULEBASED MAGNETS:1||METASTABLE STATE:1||INSULATOR:1||magnetic orderin:1||FCC IRON:1||CeRu2:1||TL2MN2O7:1||isotope effect:1||Perovskitemanganites:1||RECURSION METHOD:1||PERPENDICULAR MAGNETICANISOTROPY:1||quasiparticle spectral density:1||GW:1||MANGANESE FERRITE:1||RESONANCE:1||SeCuO3:1||Optical conductivity:1||MASSLESS DIRAC FERMIONS:1||SCHOTTKYBARRIER:1||electronic structure:15||ELECTRONICSTRUCTURE:11||TRANSITIONMETAL COMPOUNDS:10||METALS:10||photoemission:8||SPECTRA:8||MAGNETORESISTANCE:7||FERROMAGNETISM:7||TRANSPORT:7||TRANSITION:6||FILMS:6||THINFILMS:5||TOTALENERGY CALCULATIONS:5||MAGNETICPROPERTIES:5||SUPERCONDUCTIVITY:5||PR:5||LATTICE:4||STATES:4||SPECTROSCOPY:4||FIELD:4||CRYSTALSTRUCTURE:4||PHOTOEMISSION:4||TEMPERATURE:4||TRANSITIONTEMPERATURE:4||XRAYABSORPTION:4||STATE:4||CU:4||BASISSET:4||XAS:4||CRYSTALS:3||EXCITATIONS:3||MOTTHUBBARD SYSTEMS:3||HIGHENERGY SPIN:3||halfmetal:3||INSULATORS:3||LA2CUO4:3||MODEL:3||FLUCTUATIONS:3||CE:3||double exchange:3||TRANSITIONMETALS:3||RESISTIVITY:3||BORON:3||LA1XCAXMNO3:3||IRON:3||PES:3||ANTIMONIDES:2||MgB2:2||ZR METALLIC GLASSES:2||superconductor:2||CRITICALCURRENT DENSITY:2||CIRCULARDICHROISM:2||SEMICONDUCTORS:2||LOCALIZATION:2||INTRABAND OPTICAL CONDUCTIVITY:2||COLOSSAL MAGNETORESISTANCE:2||OXIDATION:2||EXISTENCE:2||COPPER:2||diboride:2||MAGNESIUMDIBORIDE:2||GAP:2||CE COMPOUNDS:2||CORE POLARIZATION:2||magnetoresistance:2||photoemission spectroscopy:2||electronphonon interaction:2||GETTER:2||PD:2||MAGNETISM:2||FECR2S4:2||SUPERCONDUCTING MGB2:2||WIRES:2||ABSORPTION:2||ENERGY:2||LA1XSRXMNO3:2||CONSTANTS:2||polaron:2||charge ordering:2||SCATTERING:2||XRAY PHOTOEMISSION:2||CeNiSn:2||phase diagram:2||PHOTOELECTRON:2||QUADRUPOLAR:2||perovskitemanganites:2||CO:2||SYSTEMS:2||DOPED ZNO:2||LOWFREQUENCY SOUND:2||LA:2||ELECTRONELECTRON SCATTERING:2||AU:2||DENSITYWAVE INSTABILITY:2||FERMISURFACE:2||hybridization:2||VALENCEBAND SATELLITE:2||SULFUR SPINEL:2||Heusler:2||APPROXIMATION:2||superexchange:2||colossal magnetoresistance:2||ALLOYS:2||DEPENDENCE:2||AG:2||electronic structures:2||AUGERSPECTRA:2||CR:2||PARAMETERS:2||DIFFRACTION:2||SEMICONDUCTORMETAL TRANSITION:1||INTERMEDIATEVALENCE:1||SMB6:1||SRRUO3:1||antiperovskite structure with antipolar nature:1||lowenergy twodimensional phonons:1||anatase TiO2:1||La3S4:1||metalinsulator transitions:1||MNO:1||ELECTRONICSTRUCTURES:1||MAGNETIC CIRCULARDICHROISM:1||Density functional theory:1||CeCo2:1||TOPOLARON CROSSOVER:1||EXCHANGE:1||cuprates:1||high Tc cuprates:1||magnetically ordered materials:1||ZNSE:1||Sr2xKxFeMoO6:1||CDW:1||TeCuO3:1||STRUCTURALPROPERTIES:1||MN:1||screening length:1||amorphous Fe:1||WAVE BASISSET:1||SILICONCARBIDE:1||HIGHPRESSURE:1||electronphonon coupling:1||quenched superconductivity:1||CMR perovskite manganites:1||OXIDE:1||polarons:1||synchrotron radiation:1||FULLERIDES:1||RESONANTPHOTOEMISSION:1||Silicon carbide:1||DFT calculation:1||Hybridized bands:1||GIANT MAGNETORESISTANCE:1||PEROVSKITES:1||Raman spectra:1||EXCHANGE ENHANCEMENT:1||SILICON:1||SR2FEMOO6:1||orbital ordering:1||delafossite:1||TITANIUMDIOXIDE:1||electronic structure of disordered solids:1||YFE2:1||Magnetic polaron:1||NA2TI2SB2O:1||STRONGCOUPLED SUPERCONDUCTORS:1||HEAVYFERMION SYSTEMS:1||firstprinciples calculations:1||MECHANISM:1||UNiSn:1||PHOTONIC BANDGAP:1||SINGLE IMPURITY:1||PHONONSPECTRUM:1||FERMISURFACE TOPOLOGY:1||SUPPRESSION:1||RESONANT PHOTOEMISSION:1||METALDOPED PICENE:1||PHOTOIONIZATION CROSSSECTIONS:1||PHOTOINDUCED FERRIMAGNETIC SYSTEMS:1||LINKAGE ISOMERISM:1||CHARGETRANSFER:1||Bilayer Graphene:1||MAGNETICFIELD:1||SPINWAVES:1||rareearth manganese oxides:1||magnonphonon interaction:1||NACO2O4:1||ENERGYBANDS:1||SELFENERGY:1||GAS:1||Fe0.5Cu0.5Cr2S4:1||scanning photoelectron microscopy (SPEM):1||MAGNETIC PROPERTIES:1||Stoner model:1||AMORPHOUS TRANSITIONMETALS:1||SPINGLASS STATES:1||NI:1||LA3NI2B2N3:1||SOLIDS:1||CEO2:1||BAND THEORY:1||dilute magnetic semiconductor:1||pyrochlore:1||Y1XPRXBA2CU3O7DELTA:1||and electronphonon interactions:1||VIBRATIONS:1||RAY PHOTOEMISSION:1||ALKALI CATION:1||Europium:1||colossal magnetoresistance:1||structural stability:1||ENERGYGAP:1||small polaron:1||DOUBLE EXCHANGE:1||Coulomb correlation:1||magnon:1||phonons:1||ELECTRON FERROMAGNETISM:1||CURIETEMPERATURE:1||ARPES:1||PLANEWAVE METHOD:1||Xray absorption spectroscopy (XAS):1||ROOMTEMPERATURE:1||MONOCHALCOGENIDES:1||HEAT:1||UPDSN:1||MOMENTS:1||XRAY ABSORPTION:1||SEMICONDUCTOR:1||Fermi surface nesting:1||optical phonon:1||disordered system:1||dilute magnetic semiconductors:1||CMR manganites:1||PHONONS:1||LATTICEDYNAMICS:1||OXIDES:1||4fphotoemission:1||permanent magnet:1||pseudogap:1||TRANSPORTPROPERTIES:1||ANTIFERROMAGNET:1||(BI,PB)SRCOO SYSTEM:1||semicore correlation:1||POLARIZATION:1||CRYSTAL:1||spinel:1||Xray magnetic circular dichroism (XMCD):1||magnetocapacitance:1||ANATASE:1||TEMPERATURES:1||Pseudogap:1||INTERFACE:1||SUBSTRATE:1||YNI2B2C:1||SAMARIUM SULFIDE:1||strong swave superconductor:1||DOPED MANGANITE:1||SYMMETRY:1||CENISN:1||resonance mode:1||DISORDERED SYSTEM:1||LITHIUM INTERCALATION:1||CUO2 PLANE:1||SURFACE:1||Delafossite:1||ELECTRICALPROPERTIES:1||NIMNSB:1||PTMNSB:1||ROOMTEMPERATURE FERROMAGNETISM:1||RUBIDIUM MANGANESE HEXACYANOFERRATE:1||COLOSSALMAGNETORESISTANCE:1||FINITE TEMPERATURES:1||LAMNO3:1||FE:1||transitionmetal oxides:1||giant magnetoresistance:1||phonon:1||COPPER OXIDES:1||valence states:1||thermoelectric:1||semiconductor:1||CATION DISTRIBUTION:1||FeCr2S4:1||photoemission spectroscopy (PES):1||METALLIC FERROMAGNETISM:1||GRAPHITE:1||SUSCEPTIBILITY:1||UBE13:1||RCrSb3:1||band JahnTeller:1||Ce3S4:1||TiO2:1||PrBa2Cu3O7delta:1||UNTWINNED PRBA2CU3O7:1||AGNIO2:1||HALFMETALLIC FERROMAGNETS:1||CI:1||Energy gap:1||Photoemission:1||Future applications:1||Photoemission measurements:1||Graphene:1||BANDSTRUCTURE:1||TC:1||superconductivity:1||magnetic semiconductors:1||CMRmanganites:1||thin films:1||spin dynamics:1||highTc superconductors:1||ITINERANTELECTRON FERROMAGNETISM:1||SINGLECRYSTALS:1||CeTe2:1||amorphous magnetic materials:1||EPITAXIAL GRAPHENE:1||LAYERED PNICTIDEOXIDES:1||BOROCARBIDE SUPERCONDUCTORS:1||AUGMENTEDWAVE METHOD:1||METALLIC MAGNET UNISN:1||ORIGIN:1||spectrum rearrangement:1||MEANFIELD THEORY:1||MOLECULEBASED MAGNETS:1||METASTABLE STATE:1||INSULATOR:1||magnetic orderin:1||FCC IRON:1||CeRu2:1||TL2MN2O7:1||isotope effect:1||Perovskitemanganites:1||RECURSION METHOD:1||PERPENDICULAR MAGNETICANISOTROPY:1||quasiparticle spectral density:1||GW:1||MANGANESE FERRITE:1||RESONANCE:1||SeCuO3:1||Optical conductivity:1||MASSLESS DIRAC FERMIONS:1||SCHOTTKYBARRIER:1||electronic structure:15||ELECTRONICSTRUCTURE:11||TRANSITIONMETAL COMPOUNDS:10||METALS:10||photoemission:8||SPECTRA:8||MAGNETORESISTANCE:7||FERROMAGNETISM:7||TRANSPORT:7||TRANSITION:6||FILMS:6||THINFILMS:5||TOTALENERGY CALCULATIONS:5||MAGNETICPROPERTIES:5||SUPERCONDUCTIVITY:5||PR:5||LATTICE:4||STATES:4||SPECTROSCOPY:4||FIELD:4||CRYSTALSTRUCTURE:4||PHOTOEMISSION:4||TEMPERATURE:4||TRANSITIONTEMPERATURE:4||XRAYABSORPTION:4||STATE:4||CU:4||BASISSET:4||XAS:4||CRYSTALS:3||EXCITATIONS:3||MOTTHUBBARD SYSTEMS:3||HIGHENERGY SPIN:3||halfmetal:3||INSULATORS:3||LA2CUO4:3||MODEL:3||FLUCTUATIONS:3||CE:3||double exchange:3||TRANSITIONMETALS:3||RESISTIVITY:3||BORON:3||LA1XCAXMNO3:3||IRON:3||PES:3||ANTIMONIDES:2||MgB2:2||ZR METALLIC GLASSES:2||superconductor:2||CRITICALCURRENT DENSITY:2||CIRCULARDICHROISM:2||SEMICONDUCTORS:2||LOCALIZATION:2||INTRABAND OPTICAL CONDUCTIVITY:2||COLOSSAL MAGNETORESISTANCE:2||OXIDATION:2||EXISTENCE:2||COPPER:2||diboride:2||MAGNESIUMDIBORIDE:2||GAP:2||CE COMPOUNDS:2||CORE POLARIZATION:2||magnetoresistance:2||photoemission spectroscopy:2||electronphonon interaction:2||GETTER:2||PD:2||MAGNETISM:2||FECR2S4:2||SUPERCONDUCTING MGB2:2||WIRES:2||ABSORPTION:2||ENERGY:2||LA1XSRXMNO3:2||CONSTANTS:2||polaron:2||charge ordering:2||SCATTERING:2||XRAY PHOTOEMISSION:2||CeNiSn:2||phase diagram:2||PHOTOELECTRON:2||QUADRUPOLAR:2||perovskitemanganites:2||CO:2||SYSTEMS:2||DOPED ZNO:2||LOWFREQUENCY SOUND:2||LA:2||ELECTRONELECTRON SCATTERING:2||AU:2||DENSITYWAVE INSTABILITY:2||FERMISURFACE:2||hybridization:2||VALENCEBAND SATELLITE:2||SULFUR SPINEL:2||Heusler:2||APPROXIMATION:2||superexchange:2||colossal magnetoresistance:2||ALLOYS:2||DEPENDENCE:2||AG:2||electronic structures:2||AUGERSPECTRA:2||CR:2||PARAMETERS:2||DIFFRACTION:2||SEMICONDUCTORMETAL TRANSITION:1||INTERMEDIATEVALENCE:1||SMB6:1||SRRUO3:1||antiperovskite structure with antipolar nature:1||lowenergy twodimensional phonons:1||anatase TiO2:1||La3S4:1||metalinsulator transitions:1||MNO:1||ELECTRONICSTRUCTURES:1||MAGNETIC CIRCULARDICHROISM:1||Density functional theory:1||CeCo2:1||TOPOLARON CROSSOVER:1||EXCHANGE:1||cuprates:1||high Tc cuprates:1||magnetically ordered materials:1||ZNSE:1||Sr2xKxFeMoO6:1||CDW:1||TeCuO3:1||STRUCTURALPROPERTIES:1||MN:1||screening length:1||amorphous Fe:1||WAVE BASISSET:1||SILICONCARBIDE:1||HIGHPRESSURE:1||electronphonon coupling:1||quenched superconductivity:1||CMR perovskite manganites:1||OXIDE:1||polarons:1||synchrotron radiation:1||FULLERIDES:1||RESONANTPHOTOEMISSION:1||Silicon carbide:1||DFT calculation:1||Hybridized bands:1||GIANT MAGNETORESISTANCE:1||PEROVSKITES:1||Raman spectra:1||EXCHANGE ENHANCEMENT:1||SILICON:1||SR2FEMOO6:1||orbital ordering:1||delafossite:1||TITANIUMDIOXIDE:1||electronic structure of disordered solids:1||YFE2:1||Magnetic polaron:1||NA2TI2SB2O:1||STRONGCOUPLED SUPERCONDUCTORS:1||HEAVYFERMION SYSTEMS:1||firstprinciples calculations:1||MECHANISM:1||UNiSn:1||PHOTONIC BANDGAP:1||SINGLE IMPURITY:1||PHONONSPECTRUM:1||FERMISURFACE TOPOLOGY:1||SUPPRESSION:1||RESONANT PHOTOEMISSION:1||METALDOPED PICENE:1||PHOTOIONIZATION CROSSSECTIONS:1||PHOTOINDUCED FERRIMAGNETIC SYSTEMS:1||LINKAGE ISOMERISM:1||CHARGETRANSFER:1||Bilayer Graphene:1||MAGNETICFIELD:1||SPINWAVES:1||rareearth manganese oxides:1||magnonphonon interaction:1||NACO2O4:1||ENERGYBANDS:1||SELFENERGY:1||GAS:1||Fe0.5Cu0.5Cr2S4:1||scanning photoelectron microscopy (SPEM):1||MAGNETIC PROPERTIES:1||Stoner model:1||AMORPHOUS TRANSITIONMETALS:1||SPINGLASS STATES:1||NI:1||LA3NI2B2N3:1||SOLIDS:1||CEO2:1||BAND THEORY:1||dilute magnetic semiconductor:1||pyrochlore:1||Y1XPRXBA2CU3O7DELTA:1||and electronphonon interactions:1||VIBRATIONS:1||RAY PHOTOEMISSION:1||ALKALI CATION:1||Europium:1||colossal magnetoresistance:1||structural stability:1||ENERGYGAP:1||small polaron:1||DOUBLE EXCHANGE:1||Coulomb correlation:1||magnon:1||phonons:1||ELECTRON FERROMAGNETISM:1||CURIETEMPERATURE:1||ARPES:1||PLANEWAVE METHOD:1||Xray absorption spectroscopy (XAS):1||ROOMTEMPERATURE:1||MONOCHALCOGENIDES:1||HEAT:1||UPDSN:1||MOMENTS:1||XRAY ABSORPTION:1||SEMICONDUCTOR:1||Fermi surface nesting:1||optical phonon:1||disordered system:1||dilute magnetic semiconductors:1||CMR manganites:1||PHONONS:1||LATTICEDYNAMICS:1||OXIDES:1||4fphotoemission:1||permanent magnet:1||pseudogap:1||TRANSPORTPROPERTIES:1||ANTIFERROMAGNET:1||(BI,PB)SRCOO SYSTEM:1||semicore correlation:1||POLARIZATION:1||CRYSTAL:1||spinel:1||Xray magnetic circular dichroism (XMCD):1||magnetocapacitance:1||ANATASE:1||TEMPERATURES:1||Pseudogap:1||INTERFACE:1||SUBSTRATE:1||YNI2B2C:1||SAMARIUM SULFIDE:1||strong swave superconductor:1||DOPED MANGANITE:1||SYMMETRY:1||CENISN:1||resonance mode:1||DISORDERED SYSTEM:1||LITHIUM INTERCALATION:1||CUO2 PLANE:1||SURFACE:1||Delafossite:1||ELECTRICALPROPERTIES:1||NIMNSB:1||PTMNSB:1||ROOMTEMPERATURE FERROMAGNETISM:1||RUBIDIUM MANGANESE HEXACYANOFERRATE:1||COLOSSALMAGNETORESISTANCE:1||FINITE TEMPERATURES:1||LAMNO3:1||FE:1||transitionmetal oxides:1||giant magnetoresistance:1||phonon:1||COPPER OXIDES:1||valence states:1||thermoelectric:1||semiconductor:1||CATION DISTRIBUTION:1||FeCr2S4:1||photoemission spectroscopy (PES):1||METALLIC FERROMAGNETISM:1||GRAPHITE:1||SUSCEPTIBILITY:1||UBE13:1||RCrSb3:1||band JahnTeller:1||Ce3S4:1||TiO2:1||PrBa2Cu3O7delta:1||UNTWINNED PRBA2CU3O7:1||AGNIO2:1||HALFMETALLIC FERROMAGNETS:1||CI:1||Energy gap:1||Photoemission:1||Future applications:1||Photoemission measurements:1||Graphene:1||BANDSTRUCTURE:1||TC:1||superconductivity:1||magnetic semiconductors:1||CMRmanganites:1||thin films:1||spin dynamics:1||highTc superconductors:1||ITINERANTELECTRON FERROMAGNETISM:1||SINGLECRYSTALS:1||CeTe2:1||amorphous magnetic materials:1||EPITAXIAL GRAPHENE:1||LAYERED PNICTIDEOXIDES:1||BOROCARBIDE SUPERCONDUCTORS:1||AUGMENTEDWAVE METHOD:1||METALLIC MAGNET UNISN:1||ORIGIN:1||spectrum rearrangement:1||MEANFIELD THEORY:1||MOLECULEBASED MAGNETS:1||METASTABLE STATE:1||INSULATOR:1||magnetic orderin:1||FCC IRON:1||CeRu2:1||TL2MN2O7:1||isotope effect:1||Perovskitemanganites:1||RECURSION METHOD:1||PERPENDICULAR MAGNETICANISOTROPY:1||quasiparticle spectral density:1||GW:1||MANGANESE FERRITE:1||RESONANCE:1||SeCuO3:1||Optical conductivity:1||MASSLESS DIRAC FERMIONS:1||SCHOTTKYBARRIER:1||electronic structure:15||ELECTRONICSTRUCTURE:11||TRANSITIONMETAL COMPOUNDS:10||METALS:10||photoemission:8||SPECTRA:8||MAGNETORESISTANCE:7||FERROMAGNETISM:7||TRANSPORT:7||TRANSITION:6||FILMS:6||THINFILMS:5||TOTALENERGY CALCULATIONS:5||MAGNETICPROPERTIES:5||SUPERCONDUCTIVITY:5||PR:5||LATTICE:4||STATES:4||SPECTROSCOPY:4||FIELD:4||CRYSTALSTRUCTURE:4||PHOTOEMISSION:4||TEMPERATURE:4||TRANSITIONTEMPERATURE:4||XRAYABSORPTION:4||STATE:4||CU:4||BASISSET:4||XAS:4||CRYSTALS:3||EXCITATIONS:3||MOTTHUBBARD SYSTEMS:3||HIGHENERGY SPIN:3||halfmetal:3||INSULATORS:3||LA2CUO4:3||MODEL:3||FLUCTUATIONS:3||CE:3||double exchange:3||TRANSITIONMETALS:3||RESISTIVITY:3||BORON:3||LA1XCAXMNO3:3||IRON:3||PES:3||ANTIMONIDES:2||MgB2:2||ZR METALLIC GLASSES:2||superconductor:2||CRITICALCURRENT DENSITY:2||CIRCULARDICHROISM:2||SEMICONDUCTORS:2||LOCALIZATION:2||INTRABAND OPTICAL CONDUCTIVITY:2||COLOSSAL MAGNETORESISTANCE:2||OXIDATION:2||EXISTENCE:2||COPPER:2||diboride:2||MAGNESIUMDIBORIDE:2||GAP:2||CE COMPOUNDS:2||CORE POLARIZATION:2||magnetoresistance:2||photoemission spectroscopy:2||electronphonon interaction:2||GETTER:2||PD:2||MAGNETISM:2||FECR2S4:2||SUPERCONDUCTING MGB2:2||WIRES:2||ABSORPTION:2||ENERGY:2||LA1XSRXMNO3:2||CONSTANTS:2||polaron:2||charge ordering:2||SCATTERING:2||XRAY PHOTOEMISSION:2||CeNiSn:2||phase diagram:2||PHOTOELECTRON:2||QUADRUPOLAR:2||perovskitemanganites:2||CO:2||SYSTEMS:2||DOPED ZNO:2||LOWFREQUENCY SOUND:2||LA:2||ELECTRONELECTRON SCATTERING:2||AU:2||DENSITYWAVE INSTABILITY:2||FERMISURFACE:2||hybridization:2||VALENCEBAND SATELLITE:2||SULFUR SPINEL:2||Heusler:2||APPROXIMATION:2||superexchange:2||colossal magnetoresistance:2||ALLOYS:2||DEPENDENCE:2||AG:2||electronic structures:2||AUGERSPECTRA:2||CR:2||PARAMETERS:2||DIFFRACTION:2||SEMICONDUCTORMETAL TRANSITION:1||INTERMEDIATEVALENCE:1||SMB6:1||SRRUO3:1||antiperovskite structure with antipolar nature:1||lowenergy twodimensional phonons:1||anatase TiO2:1||La3S4:1||metalinsulator transitions:1||MNO:1||ELECTRONICSTRUCTURES:1||MAGNETIC CIRCULARDICHROISM:1||Density functional theory:1||CeCo2:1||TOPOLARON CROSSOVER:1||EXCHANGE:1||cuprates:1||high Tc cuprates:1||magnetically ordered materials:1||ZNSE:1||Sr2xKxFeMoO6:1||CDW:1||TeCuO3:1||STRUCTURALPROPERTIES:1||MN:1||screening length:1||amorphous Fe:1||WAVE BASISSET:1||SILICONCARBIDE:1||HIGHPRESSURE:1||electronphonon coupling:1||quenched superconductivity:1||CMR perovskite manganites:1||OXIDE:1||polarons:1||synchrotron radiation:1||FULLERIDES:1||RESONANTPHOTOEMISSION:1||Silicon carbide:1||DFT calculation:1||Hybridized bands:1||GIANT MAGNETORESISTANCE:1||PEROVSKITES:1||Raman spectra:1||EXCHANGE ENHANCEMENT:1||SILICON:1||SR2FEMOO6:1||orbital ordering:1||delafossite:1||TITANIUMDIOXIDE:1||electronic structure of disordered solids:1||YFE2:1||Magnetic polaron:1||NA2TI2SB2O:1||STRONGCOUPLED SUPERCONDUCTORS:1||HEAVYFERMION SYSTEMS:1||firstprinciples calculations:1||MECHANISM:1||UNiSn:1||PHOTONIC BANDGAP:1||SINGLE IMPURITY:1||PHONONSPECTRUM:1||FERMISURFACE TOPOLOGY:1||SUPPRESSION:1||RESONANT PHOTOEMISSION:1||METALDOPED PICENE:1||PHOTOIONIZATION CROSSSECTIONS:1||PHOTOINDUCED FERRIMAGNETIC SYSTEMS:1||LINKAGE ISOMERISM:1||CHARGETRANSFER:1||Bilayer Graphene:1||MAGNETICFIELD:1||SPINWAVES:1||rareearth manganese oxides:1||magnonphonon interaction:1||NACO2O4:1||ENERGYBANDS:1||SELFENERGY:1||GAS:1||Fe0.5Cu0.5Cr2S4:1||scanning photoelectron microscopy (SPEM):1||MAGNETIC PROPERTIES:1||Stoner model:1||AMORPHOUS TRANSITIONMETALS:1||SPINGLASS STATES:1||NI:1||LA3NI2B2N3:1||SOLIDS:1||CEO2:1||BAND THEORY:1||dilute magnetic semiconductor:1||pyrochlore:1||Y1XPRXBA2CU3O7DELTA:1||and electronphonon interactions:1||VIBRATIONS:1||RAY PHOTOEMISSION:1||ALKALI CATION:1||Europium:1||colossal magnetoresistance:1||structural stability:1||ENERGYGAP:1||small polaron:1||DOUBLE EXCHANGE:1||Coulomb correlation:1||magnon:1||phonons:1||ELECTRON FERROMAGNETISM:1||CURIETEMPERATURE:1||ARPES:1||PLANEWAVE METHOD:1||Xray absorption spectroscopy (XAS):1||ROOMTEMPERATURE:1||MONOCHALCOGENIDES:1||HEAT:1||UPDSN:1||MOMENTS:1||XRAY ABSORPTION:1||SEMICONDUCTOR:1||Fermi surface nesting:1||optical phonon:1||disordered system:1||dilute magnetic semiconductors:1||CMR manganites:1||PHONONS:1||LATTICEDYNAMICS:1||OXIDES:1||4fphotoemission:1||permanent magnet:1||pseudogap:1||TRANSPORTPROPERTIES:1||ANTIFERROMAGNET:1||(BI,PB)SRCOO SYSTEM:1||semicore correlation:1||POLARIZATION:1||CRYSTAL:1||spinel:1||Xray magnetic circular dichroism (XMCD):1||magnetocapacitance:1||ANATASE:1||TEMPERATURES:1||Pseudogap:1||INTERFACE:1||SUBSTRATE:1||YNI2B2C:1||SAMARIUM SULFIDE:1||strong swave superconductor:1||DOPED MANGANITE:1||SYMMETRY:1||CENISN:1||resonance mode:1||DISORDERED SYSTEM:1||LITHIUM INTERCALATION:1||CUO2 PLANE:1||SURFACE:1||Delafossite:1||ELECTRICALPROPERTIES:1||NIMNSB:1||PTMNSB:1||ROOMTEMPERATURE FERROMAGNETISM:1||RUBIDIUM MANGANESE HEXACYANOFERRATE:1||COLOSSALMAGNETORESISTANCE:1||FINITE TEMPERATURES:1||LAMNO3:1||FE:1||transitionmetal oxides:1||giant magnetoresistance:1||phonon:1||COPPER OXIDES:1||valence states:1||thermoelectric:1||semiconductor:1||CATION DISTRIBUTION:1||FeCr2S4:1||photoemission spectroscopy (PES):1||METALLIC FERROMAGNETISM:1||GRAPHITE:1||SUSCEPTIBILITY:1||UBE13:1||RCrSb3:1||band JahnTeller:1||Ce3S4:1||TiO2:1||PrBa2Cu3O7delta:1||UNTWINNED PRBA2CU3O7:1||AGNIO2:1||HALFMETALLIC FERROMAGNETS:1||CI:1||Energy gap:1||Photoemission:1||Future applications:1||Photoemission measurements:1||Graphene:1||BANDSTRUCTURE:1||TC:1||superconductivity:1||magnetic semiconductors:1||CMRmanganites:1||thin films:1||spin dynamics:1||highTc superconductors:1||ITINERANTELECTRON FERROMAGNETISM:1||SINGLECRYSTALS:1||CeTe2:1||amorphous magnetic materials:1||EPITAXIAL GRAPHENE:1||LAYERED PNICTIDEOXIDES:1||BOROCARBIDE SUPERCONDUCTORS:1||AUGMENTEDWAVE METHOD:1||METALLIC MAGNET UNISN:1||ORIGIN:1||spectrum rearrangement:1||MEANFIELD THEORY:1||MOLECULEBASED MAGNETS:1||METASTABLE STATE:1||INSULATOR:1||magnetic orderin:1||FCC IRON:1||CeRu2:1||TL2MN2O7:1||isotope effect:1||Perovskitemanganites:1||RECURSION METHOD:1||PERPENDICULAR MAGNETICANISOTROPY:1||quasiparticle spectral density:1||GW:1||MANGANESE FERRITE:1||RESONANCE:1||SeCuO3:1||Optical conductivity:1||MASSLESS DIRAC FERMIONS:1||SCHOTTKYBARRIER:1||electronic structure:15||ELECTRONICSTRUCTURE:11||TRANSITIONMETAL COMPOUNDS:10||METALS:10||photoemission:8||SPECTRA:8||MAGNETORESISTANCE:7||FERROMAGNETISM:7||TRANSPORT:7||TRANSITION:6||FILMS:6||THINFILMS:5||TOTALENERGY CALCULATIONS:5||MAGNETICPROPERTIES:5||SUPERCONDUCTIVITY:5||PR:5||LATTICE:4||STATES:4||SPECTROSCOPY:4||FIELD:4||CRYSTALSTRUCTURE:4||PHOTOEMISSION:4||TEMPERATURE:4||TRANSITIONTEMPERATURE:4||XRAYABSORPTION:4||STATE:4||CU:4||BASISSET:4||XAS:4||CRYSTALS:3||EXCITATIONS:3||MOTTHUBBARD SYSTEMS:3||HIGHENERGY SPIN:3||halfmetal:3||INSULATORS:3||LA2CUO4:3||MODEL:3||FLUCTUATIONS:3||CE:3||double exchange:3||TRANSITIONMETALS:3||RESISTIVITY:3||BORON:3||LA1XCAXMNO3:3||IRON:3||PES:3||ANTIMONIDES:2||MgB2:2||ZR METALLIC GLASSES:2||superconductor:2||CRITICALCURRENT DENSITY:2||CIRCULARDICHROISM:2||SEMICONDUCTORS:2||LOCALIZATION:2||INTRABAND OPTICAL CONDUCTIVITY:2||COLOSSAL MAGNETORESISTANCE:2||OXIDATION:2||EXISTENCE:2||COPPER:2||diboride:2||MAGNESIUMDIBORIDE:2||GAP:2||CE COMPOUNDS:2||CORE POLARIZATION:2||magnetoresistance:2||photoemission spectroscopy:2||electronphonon interaction:2||GETTER:2||PD:2||MAGNETISM:2||FECR2S4:2||SUPERCONDUCTING MGB2:2||WIRES:2||ABSORPTION:2||ENERGY:2||LA1XSRXMNO3:2||CONSTANTS:2||polaron:2||charge ordering:2||SCATTERING:2||XRAY PHOTOEMISSION:2||CeNiSn:2||phase diagram:2||PHOTOELECTRON:2||QUADRUPOLAR:2||perovskitemanganites:2||CO:2||SYSTEMS:2||DOPED ZNO:2||LOWFREQUENCY SOUND:2||LA:2||ELECTRONELECTRON SCATTERING:2||AU:2||DENSITYWAVE INSTABILITY:2||FERMISURFACE:2||hybridization:2||VALENCEBAND SATELLITE:2||SULFUR SPINEL:2||Heusler:2||APPROXIMATION:2||superexchange:2||colossal magnetoresistance:2||ALLOYS:2||DEPENDENCE:2||AG:2||electronic structures:2||AUGERSPECTRA:2||CR:2||PARAMETERS:2||DIFFRACTION:2||SEMICONDUCTORMETAL TRANSITION:1||INTERMEDIATEVALENCE:1||SMB6:1||SRRUO3:1||antiperovskite structure with antipolar nature:1||lowenergy twodimensional phonons:1||anatase TiO2:1||La3S4:1||metalinsulator transitions:1||MNO:1||ELECTRONICSTRUCTURES:1||MAGNETIC CIRCULARDICHROISM:1||Density functional theory:1||CeCo2:1||TOPOLARON CROSSOVER:1||EXCHANGE:1||cuprates:1||high Tc cuprates:1||magnetically ordered materials:1||ZNSE:1||Sr2xKxFeMoO6:1||CDW:1||TeCuO3:1||STRUCTURALPROPERTIES:1||MN:1||screening length:1||amorphous Fe:1||WAVE BASISSET:1||SILICONCARBIDE:1||HIGHPRESSURE:1||electronphonon coupling:1||quenched superconductivity:1||CMR perovskite manganites:1||OXIDE:1||polarons:1||synchrotron radiation:1||FULLERIDES:1||RESONANTPHOTOEMISSION:1||Silicon carbide:1||DFT calculation:1||Hybridized bands:1||GIANT MAGNETORESISTANCE:1||PEROVSKITES:1||Raman spectra:1||EXCHANGE ENHANCEMENT:1||SILICON:1||SR2FEMOO6:1||orbital ordering:1||delafossite:1||TITANIUMDIOXIDE:1||electronic structure of disordered solids:1||YFE2:1||Magnetic polaron:1||NA2TI2SB2O:1||STRONGCOUPLED SUPERCONDUCTORS:1||HEAVYFERMION SYSTEMS:1||firstprinciples calculations:1||MECHANISM:1||UNiSn:1||PHOTONIC BANDGAP:1||SINGLE IMPURITY:1||PHONONSPECTRUM:1||FERMISURFACE TOPOLOGY:1||SUPPRESSION:1||RESONANT PHOTOEMISSION:1||METALDOPED PICENE:1||PHOTOIONIZATION CROSSSECTIONS:1||PHOTOINDUCED FERRIMAGNETIC SYSTEMS:1||LINKAGE ISOMERISM:1||CHARGETRANSFER:1||Bilayer Graphene:1||MAGNETICFIELD:1||SPINWAVES:1||rareearth manganese oxides:1||magnonphonon interaction:1||NACO2O4:1||ENERGYBANDS:1||SELFENERGY:1||GAS:1||Fe0.5Cu0.5Cr2S4:1||scanning photoelectron microscopy (SPEM):1||MAGNETIC PROPERTIES:1||Stoner model:1||AMORPHOUS TRANSITIONMETALS:1||SPINGLASS STATES:1||NI:1||LA3NI2B2N3:1||SOLIDS:1||CEO2:1||BAND THEORY:1||dilute magnetic semiconductor:1||pyrochlore:1||Y1XPRXBA2CU3O7DELTA:1||and electronphonon interactions:1||VIBRATIONS:1||RAY PHOTOEMISSION:1||ALKALI CATION:1||Europium:1||colossal magnetoresistance:1||structural stability:1||ENERGYGAP:1||small polaron:1||DOUBLE EXCHANGE:1||Coulomb correlation:1||magnon:1||phonons:1||ELECTRON FERROMAGNETISM:1||CURIETEMPERATURE:1||ARPES:1||PLANEWAVE METHOD:1||Xray absorption spectroscopy (XAS):1||ROOMTEMPERATURE:1||MONOCHALCOGENIDES:1||HEAT:1||UPDSN:1||MOMENTS:1||XRAY ABSORPTION:1||SEMICONDUCTOR:1||Fermi surface nesting:1||optical phonon:1||disordered system:1||dilute magnetic semiconductors:1||CMR manganites:1||PHONONS:1||LATTICEDYNAMICS:1||OXIDES:1||4fphotoemission:1||permanent magnet:1||pseudogap:1||TRANSPORTPROPERTIES:1||ANTIFERROMAGNET:1||(BI,PB)SRCOO SYSTEM:1||semicore correlation:1||POLARIZATION:1||CRYSTAL:1||spinel:1||Xray magnetic circular dichroism (XMCD):1||magnetocapacitance:1||ANATASE:1||TEMPERATURES:1||Pseudogap:1||INTERFACE:1||SUBSTRATE:1||YNI2B2C:1||SAMARIUM SULFIDE:1||strong swave superconductor:1||DOPED MANGANITE:1||SYMMETRY:1||CENISN:1||resonance mode:1||DISORDERED SYSTEM:1||LITHIUM INTERCALATION:1||CUO2 PLANE:1||SURFACE:1||Delafossite:1||ELECTRICALPROPERTIES:1||NIMNSB:1||PTMNSB:1||ROOMTEMPERATURE FERROMAGNETISM:1||RUBIDIUM MANGANESE HEXACYANOFERRATE:1||COLOSSALMAGNETORESISTANCE:1||FINITE TEMPERATURES:1||LAMNO3:1||FE:1||transitionmetal oxides:1||giant magnetoresistance:1||phonon:1||COPPER OXIDES:1||valence states:1||thermoelectric:1||semiconductor:1||CATION DISTRIBUTION:1||FeCr2S4:1||photoemission spectroscopy (PES):1||METALLIC FERROMAGNETISM:1||GRAPHITE:1||SUSCEPTIBILITY:1||UBE13:1||RCrSb3:1||band JahnTeller:1||Ce3S4:1||TiO2:1||PrBa2Cu3O7delta:1||UNTWINNED PRBA2CU3O7:1||AGNIO2:1||HALFMETALLIC FERROMAGNETS:1||CI:1||Energy gap:1||Photoemission:1||Future applications:1||Photoemission measurements:1||Graphene:1||BANDSTRUCTURE:1||TC:1||superconductivity:1||magnetic semiconductors:1||CMRmanganites:1||thin films:1||spin dynamics:1||highTc superconductors:1||ITINERANTELECTRON FERROMAGNETISM:1||SINGLECRYSTALS:1||CeTe2:1||amorphous magnetic materials:1||EPITAXIAL GRAPHENE:1||LAYERED PNICTIDEOXIDES:1||BOROCARBIDE SUPERCONDUCTORS:1||AUGMENTEDWAVE METHOD:1||METALLIC MAGNET UNISN:1||ORIGIN:1||spectrum rearrangement:1||MEANFIELD THEORY:1||MOLECULEBASED MAGNETS:1||METASTABLE STATE:1||INSULATOR:1||magnetic orderin:1||FCC IRON:1||CeRu2:1||TL2MN2O7:1||isotope effect:1||Perovskitemanganites:1||RECURSION METHOD:1||PERPENDICULAR MAGNETICANISOTROPY:1||quasiparticle spectral density:1||GW:1||MANGANESE FERRITE:1||RESONANCE:1||SeCuO3:1||Optical conductivity:1||MASSLESS DIRAC FERMIONS:1||SCHOTTKYBARRIER:1||electronic structure:15||ELECTRONICSTRUCTURE:11||TRANSITIONMETAL COMPOUNDS:10||METALS:10||photoemission:8||SPECTRA:8||MAGNETORESISTANCE:7||FERROMAGNETISM:7||TRANSPORT:7||TRANSITION:6||FILMS:6||THINFILMS:5||TOTALENERGY CALCULATIONS:5||MAGNETICPROPERTIES:5||SUPERCONDUCTIVITY:5||PR:5||LATTICE:4||STATES:4||SPECTROSCOPY:4||FIELD:4||CRYSTALSTRUCTURE:4||PHOTOEMISSION:4||TEMPERATURE:4||TRANSITIONTEMPERATURE:4||XRAYABSORPTION:4||STATE:4||CU:4||BASISSET:4||XAS:4||CRYSTALS:3||EXCITATIONS:3||MOTTHUBBARD SYSTEMS:3||HIGHENERGY SPIN:3||halfmetal:3||INSULATORS:3||LA2CUO4:3||MODEL:3||FLUCTUATIONS:3||CE:3||double exchange:3||TRANSITIONMETALS:3||RESISTIVITY:3||BORON:3||LA1XCAXMNO3:3||IRON:3||PES:3||ANTIMONIDES:2||MgB2:2||ZR METALLIC GLASSES:2||superconductor:2||CRITICALCURRENT DENSITY:2||CIRCULARDICHROISM:2||SEMICONDUCTORS:2||LOCALIZATION:2||INTRABAND OPTICAL CONDUCTIVITY:2||COLOSSAL MAGNETORESISTANCE:2||OXIDATION:2||EXISTENCE:2||COPPER:2||diboride:2||MAGNESIUMDIBORIDE:2||GAP:2||CE COMPOUNDS:2||CORE POLARIZATION:2||magnetoresistance:2||photoemission spectroscopy:2||electronphonon interaction:2||GETTER:2||PD:2||MAGNETISM:2||FECR2S4:2||SUPERCONDUCTING MGB2:2||WIRES:2||ABSORPTION:2||ENERGY:2||LA1XSRXMNO3:2||CONSTANTS:2||polaron:2||charge ordering:2||SCATTERING:2||XRAY PHOTOEMISSION:2||CeNiSn:2||phase diagram:2||PHOTOELECTRON:2||QUADRUPOLAR:2||perovskitemanganites:2||CO:2||SYSTEMS:2||DOPED ZNO:2||LOWFREQUENCY SOUND:2||LA:2||ELECTRONELECTRON SCATTERING:2||AU:2||DENSITYWAVE INSTABILITY:2||FERMISURFACE:2||hybridization:2||VALENCEBAND SATELLITE:2||SULFUR SPINEL:2||Heusler:2||APPROXIMATION:2||superexchange:2||colossal magnetoresistance:2||ALLOYS:2||DEPENDENCE:2||AG:2||electronic structures:2||AUGERSPECTRA:2||CR:2||PARAMETERS:2||DIFFRACTION:2||SEMICONDUCTORMETAL TRANSITION:1||INTERMEDIATEVALENCE:1||SMB6:1||SRRUO3:1||antiperovskite structure with antipolar nature:1||lowenergy twodimensional phonons:1||anatase TiO2:1||La3S4:1||metalinsulator transitions:1||MNO:1||ELECTRONICSTRUCTURES:1||MAGNETIC CIRCULARDICHROISM:1||Density functional theory:1||CeCo2:1||TOPOLARON CROSSOVER:1||EXCHANGE:1||cuprates:1||high Tc cuprates:1||magnetically ordered materials:1||ZNSE:1||Sr2xKxFeMoO6:1||CDW:1||TeCuO3:1||STRUCTURALPROPERTIES:1||MN:1||screening length:1||amorphous Fe:1||WAVE BASISSET:1||SILICONCARBIDE:1||HIGHPRESSURE:1||electronphonon coupling:1||quenched superconductivity:1||CMR perovskite manganites:1||OXIDE:1||polarons:1||synchrotron radiation:1||FULLERIDES:1||RESONANTPHOTOEMISSION:1||Silicon carbide:1||DFT calculation:1||Hybridized bands:1||GIANT MAGNETORESISTANCE:1||PEROVSKITES:1||Raman spectra:1||EXCHANGE ENHANCEMENT:1||SILICON:1||SR2FEMOO6:1||orbital ordering:1||delafossite:1||TITANIUMDIOXIDE:1||electronic structure of disordered solids:1||YFE2:1||Magnetic polaron:1||NA2TI2SB2O:1||STRONGCOUPLED SUPERCONDUCTORS:1||HEAVYFERMION SYSTEMS:1||firstprinciples calculations:1||MECHANISM:1||UNiSn:1||PHOTONIC BANDGAP:1||SINGLE IMPURITY:1||PHONONSPECTRUM:1||FERMISURFACE TOPOLOGY:1||SUPPRESSION:1||RESONANT PHOTOEMISSION:1||METALDOPED PICENE:1||PHOTOIONIZATION CROSSSECTIONS:1||PHOTOINDUCED FERRIMAGNETIC SYSTEMS:1||LINKAGE ISOMERISM:1||CHARGETRANSFER:1||Bilayer Graphene:1||MAGNETICFIELD:1||SPINWAVES:1||rareearth manganese oxides:1||magnonphonon interaction:1||NACO2O4:1||ENERGYBANDS:1||SELFENERGY:1||GAS:1||Fe0.5Cu0.5Cr2S4:1||scanning photoelectron microscopy (SPEM):1||MAGNETIC PROPERTIES:1||Stoner model:1||AMORPHOUS TRANSITIONMETALS:1||SPINGLASS STATES:1||NI:1||LA3NI2B2N3:1||SOLIDS:1||CEO2:1||BAND THEORY:1||dilute magnetic semiconductor:1||pyrochlore:1||Y1XPRXBA2CU3O7DELTA:1||and electronphonon interactions:1||VIBRATIONS:1||RAY PHOTOEMISSION:1||ALKALI CATION:1||Europium:1||colossal magnetoresistance:1||structural stability:1||ENERGYGAP:1||small polaron:1||DOUBLE EXCHANGE:1||Coulomb correlation:1||magnon:1||phonons:1||ELECTRON FERROMAGNETISM:1||CURIETEMPERATURE:1||ARPES:1||PLANEWAVE METHOD:1||Xray absorption spectroscopy (XAS):1||ROOMTEMPERATURE:1||MONOCHALCOGENIDES:1||HEAT:1||UPDSN:1||MOMENTS:1||XRAY ABSORPTION:1||SEMICONDUCTOR:1||Fermi surface nesting:1||optical phonon:1||disordered system:1||dilute magnetic semiconductors:1||CMR manganites:1||PHONONS:1||LATTICEDYNAMICS:1||OXIDES:1||4fphotoemission:1||permanent magnet:1||pseudogap:1||TRANSPORTPROPERTIES:1||ANTIFERROMAGNET:1||(BI,PB)SRCOO SYSTEM:1||semicore correlation:1||POLARIZATION:1||CRYSTAL:1||spinel:1||Xray magnetic circular dichroism (XMCD):1||magnetocapacitance:1||ANATASE:1||TEMPERATURES:1||Pseudogap:1||INTERFACE:1||SUBSTRATE:1||YNI2B2C:1||SAMARIUM SULFIDE:1||strong swave superconductor:1||DOPED MANGANITE:1||SYMMETRY:1||CENISN:1||resonance mode:1||DISORDERED SYSTEM:1||LITHIUM INTERCALATION:1||CUO2 PLANE:1||SURFACE:1||Delafossite:1||ELECTRICALPROPERTIES:1||NIMNSB:1||PTMNSB:1||ROOMTEMPERATURE FERROMAGNETISM:1||RUBIDIUM MANGANESE HEXACYANOFERRATE:1||COLOSSALMAGNETORESISTANCE:1||FINITE TEMPERATURES:1||LAMNO3:1||FE:1||transitionmetal oxides:1||giant magnetoresistance:1||phonon:1||COPPER OXIDES:1||valence states:1||thermoelectric:1||semiconductor:1||CATION DISTRIBUTION:1||FeCr2S4:1||photoemission spectroscopy (PES):1||METALLIC FERROMAGNETISM:1||GRAPHITE:1||SUSCEPTIBILITY:1||UBE13:1||RCrSb3:1||band JahnTeller:1||Ce3S4:1||TiO2:1||PrBa2Cu3O7delta:1||UNTWINNED PRBA2CU3O7:1||AGNIO2:1||HALFMETALLIC FERROMAGNETS:1||CI:1||Energy gap:1||Photoemission:1||Future applications:1||Photoemission measurements:1||Graphene:1||BANDSTRUCTURE:1||TC:1||superconductivity:1||magnetic semiconductors:1||CMRmanganites:1||thin films:1||spin dynamics:1||highTc superconductors:1||ITINERANTELECTRON FERROMAGNETISM:1||SINGLECRYSTALS:1||CeTe2:1||amorphous magnetic materials:1||EPITAXIAL GRAPHENE:1||LAYERED PNICTIDEOXIDES:1||BOROCARBIDE SUPERCONDUCTORS:1||AUGMENTEDWAVE METHOD:1||METALLIC MAGNET UNISN:1||ORIGIN:1||spectrum rearrangement:1||MEANFIELD THEORY:1||MOLECULEBASED MAGNETS:1||METASTABLE STATE:1||INSULATOR:1||magnetic orderin:1||FCC IRON:1||CeRu2:1||TL2MN2O7:1||isotope effect:1||Perovskitemanganites:1||RECURSION METHOD:1||PERPENDICULAR MAGNETICANISOTROPY:1||quasiparticle spectral density:1||GW:1||MANGANESE FERRITE:1||RESONANCE:1||SeCuO3:1||Optical conductivity:1||MASSLESS DIRAC FERMIONS:1||SCHOTTKYBARRIER:1||electronic structure:15||ELECTRONICSTRUCTURE:11||TRANSITIONMETAL COMPOUNDS:10||METALS:10||photoemission:8||SPECTRA:8||MAGNETORESISTANCE:7||FERROMAGNETISM:7||TRANSPORT:7||TRANSITION:6||FILMS:6||THINFILMS:5||TOTALENERGY CALCULATIONS:5||MAGNETICPROPERTIES:5||SUPERCONDUCTIVITY:5||PR:5||LATTICE:4||STATES:4||SPECTROSCOPY:4||FIELD:4||CRYSTALSTRUCTURE:4||PHOTOEMISSION:4||TEMPERATURE:4||TRANSITIONTEMPERATURE:4||XRAYABSORPTION:4||STATE:4||CU:4||BASISSET:4||XAS:4||CRYSTALS:3||EXCITATIONS:3||MOTTHUBBARD SYSTEMS:3||HIGHENERGY SPIN:3||halfmetal:3||INSULATORS:3||LA2CUO4:3||MODEL:3||FLUCTUATIONS:3||CE:3||double exchange:3||TRANSITIONMETALS:3||RESISTIVITY:3||BORON:3||LA1XCAXMNO3:3||IRON:3||PES:3||ANTIMONIDES:2||MgB2:2||ZR METALLIC GLASSES:2||superconductor:2||CRITICALCURRENT DENSITY:2||CIRCULARDICHROISM:2||SEMICONDUCTORS:2||LOCALIZATION:2||INTRABAND OPTICAL CONDUCTIVITY:2||COLOSSAL MAGNETORESISTANCE:2||OXIDATION:2||EXISTENCE:2||COPPER:2||diboride:2||MAGNESIUMDIBORIDE:2||GAP:2||CE COMPOUNDS:2||CORE POLARIZATION:2||magnetoresistance:2||photoemission spectroscopy:2||electronphonon interaction:2||GETTER:2||PD:2||MAGNETISM:2||FECR2S4:2||SUPERCONDUCTING MGB2:2||WIRES:2||ABSORPTION:2||ENERGY:2||LA1XSRXMNO3:2||CONSTANTS:2||polaron:2||charge ordering:2||SCATTERING:2||XRAY PHOTOEMISSION:2||CeNiSn:2||phase diagram:2||PHOTOELECTRON:2||QUADRUPOLAR:2||perovskitemanganites:2||CO:2||SYSTEMS:2||DOPED ZNO:2||LOWFREQUENCY SOUND:2||LA:2||ELECTRONELECTRON SCATTERING:2||AU:2||DENSITYWAVE INSTABILITY:2||FERMISURFACE:2||hybridization:2||VALENCEBAND SATELLITE:2||SULFUR SPINEL:2||Heusler:2||APPROXIMATION:2||superexchange:2||colossal magnetoresistance:2||ALLOYS:2||DEPENDENCE:2||AG:2||electronic structures:2||AUGERSPECTRA:2||CR:2||PARAMETERS:2||DIFFRACTION:2||SEMICONDUCTORMETAL TRANSITION:1||INTERMEDIATEVALENCE:1||SMB6:1||SRRUO3:1||antiperovskite structure with antipolar nature:1||lowenergy twodimensional phonons:1||anatase TiO2:1||La3S4:1||metalinsulator transitions:1||MNO:1||ELECTRONICSTRUCTURES:1||MAGNETIC CIRCULARDICHROISM:1||Density functional theory:1||CeCo2:1||TOPOLARON CROSSOVER:1||EXCHANGE:1||cuprates:1||high Tc cuprates:1||magnetically ordered materials:1||ZNSE:1||Sr2xKxFeMoO6:1||CDW:1||TeCuO3:1||STRUCTURALPROPERTIES:1||MN:1||screening length:1||amorphous Fe:1||WAVE BASISSET:1||SILICONCARBIDE:1||HIGHPRESSURE:1||electronphonon coupling:1||quenched superconductivity:1||CMR perovskite manganites:1||OXIDE:1||polarons:1||synchrotron radiation:1||FULLERIDES:1||RESONANTPHOTOEMISSION:1||Silicon carbide:1||DFT calculation:1||Hybridized bands:1||GIANT MAGNETORESISTANCE:1||PEROVSKITES:1||Raman spectra:1||EXCHANGE ENHANCEMENT:1||SILICON:1||SR2FEMOO6:1||orbital ordering:1||delafossite:1||TITANIUMDIOXIDE:1||electronic structure of disordered solids:1||YFE2:1||Magnetic polaron:1||NA2TI2SB2O:1||STRONGCOUPLED SUPERCONDUCTORS:1||HEAVYFERMION SYSTEMS:1||firstprinciples calculations:1||MECHANISM:1||UNiSn:1||PHOTONIC BANDGAP:1||SINGLE IMPURITY:1||PHONONSPECTRUM:1||FERMISURFACE TOPOLOGY:1||SUPPRESSION:1||RESONANT PHOTOEMISSION:1||METALDOPED PICENE:1||PHOTOIONIZATION CROSSSECTIONS:1||PHOTOINDUCED FERRIMAGNETIC SYSTEMS:1||LINKAGE ISOMERISM:1||CHARGETRANSFER:1||Bilayer Graphene:1||MAGNETICFIELD:1||SPINWAVES:1||rareearth manganese oxides:1||magnonphonon interaction:1||NACO2O4:1||ENERGYBANDS:1||SELFENERGY:1||GAS:1||Fe0.5Cu0.5Cr2S4:1||scanning photoelectron microscopy (SPEM):1||MAGNETIC PROPERTIES:1||Stoner model:1||AMORPHOUS TRANSITIONMETALS:1||SPINGLASS STATES:1||NI:1||LA3NI2B2N3:1||SOLIDS:1||CEO2:1||BAND THEORY:1||dilute magnetic semiconductor:1||pyrochlore:1||Y1XPRXBA2CU3O7DELTA:1||and electronphonon interactions:1||VIBRATIONS:1||RAY PHOTOEMISSION:1||ALKALI CATION:1||Europium:1||colossal magnetoresistance:1||structural stability:1||ENERGYGAP:1||small polaron:1||DOUBLE EXCHANGE:1||Coulomb correlation:1||magnon:1||phonons:1||ELECTRON FERROMAGNETISM:1||CURIETEMPERATURE:1||ARPES:1||PLANEWAVE METHOD:1||Xray absorption spectroscopy (XAS):1||ROOMTEMPERATURE:1||MONOCHALCOGENIDES:1||HEAT:1||UPDSN:1||MOMENTS:1||XRAY ABSORPTION:1||SEMICONDUCTOR:1||Fermi surface nesting:1||optical phonon:1||disordered system:1||dilute magnetic semiconductors:1||CMR manganites:1||PHONONS:1||LATTICEDYNAMICS:1||OXIDES:1||4fphotoemission:1||permanent magnet:1||pseudogap:1||TRANSPORTPROPERTIES:1||ANTIFERROMAGNET:1||(BI,PB)SRCOO SYSTEM:1||semicore correlation:1||POLARIZATION:1||CRYSTAL:1||spinel:1||Xray magnetic circular dichroism (XMCD):1||magnetocapacitance:1||ANATASE:1||TEMPERATURES:1||Pseudogap:1||INTERFACE:1||SUBSTRATE:1||YNI2B2C:1||SAMARIUM SULFIDE:1||strong swave superconductor:1||DOPED MANGANITE:1||SYMMETRY:1||CENISN:1||resonance mode:1||DISORDERED SYSTEM:1||LITHIUM INTERCALATION:1||CUO2 PLANE:1||SURFACE:1||Delafossite:1||ELECTRICALPROPERTIES:1||NIMNSB:1||PTMNSB:1||ROOMTEMPERATURE FERROMAGNETISM:1||RUBIDIUM MANGANESE HEXACYANOFERRATE:1||COLOSSALMAGNETORESISTANCE:1||FINITE TEMPERATURES:1||LAMNO3:1||FE:1||transitionmetal oxides:1||giant magnetoresistance:1||phonon:1||COPPER OXIDES:1||valence states:1||thermoelectric:1||semiconductor:1||CATION DISTRIBUTION:1||FeCr2S4:1||photoemission spectroscopy (PES):1||METALLIC FERROMAGNETISM:1||GRAPHITE:1||SUSCEPTIBILITY:1||UBE13:1||RCrSb3:1||band JahnTeller:1||Ce3S4:1||TiO2:1||PrBa2Cu3O7delta:1||UNTWINNED PRBA2CU3O7:1||AGNIO2:1||HALFMETALLIC FERROMAGNETS:1||CI:1||Energy gap:1||Photoemission:1||Future applications:1||Photoemission measurements:1||Graphene:1||BANDSTRUCTURE:1||TC:1||superconductivity:1||magnetic semiconductors:1||CMRmanganites:1||thin films:1||spin dynamics:1||highTc superconductors:1||ITINERANTELECTRON FERROMAGNETISM:1||SINGLECRYSTALS:1||CeTe2:1||amorphous magnetic materials:1||EPITAXIAL GRAPHENE:1||LAYERED PNICTIDEOXIDES:1||BOROCARBIDE SUPERCONDUCTORS:1||AUGMENTEDWAVE METHOD:1||METALLIC MAGNET UNISN:1||ORIGIN:1||spectrum rearrangement:1||MEANFIELD THEORY:1||MOLECULEBASED MAGNETS:1||METASTABLE STATE:1||INSULATOR:1||magnetic orderin:1||FCC IRON:1||CeRu2:1||TL2MN2O7:1||isotope effect:1||Perovskitemanganites:1||RECURSION METHOD:1||PERPENDICULAR MAGNETICANISOTROPY:1||quasiparticle spectral density:1||GW:1||MANGANESE FERRITE:1||RESONANCE:1||SeCuO3:1||Optical conductivity:1||MASSLESS DIRAC FERMIONS:1||SCHOTTKYBARRIER:1||electronic structure:15||ELECTRONICSTRUCTURE:11||TRANSITIONMETAL COMPOUNDS:10||METALS:10||photoemission:8||SPECTRA:8||MAGNETORESISTANCE:7||FERROMAGNETISM:7||TRANSPORT:7||TRANSITION:6||FILMS:6||THINFILMS:5||TOTALENERGY CALCULATIONS:5||MAGNETICPROPERTIES:5||SUPERCONDUCTIVITY:5||PR:5||LATTICE:4||STATES:4||SPECTROSCOPY:4||FIELD:4||CRYSTALSTRUCTURE:4||PHOTOEMISSION:4||TEMPERATURE:4||TRANSITIONTEMPERATURE:4||XRAYABSORPTION:4||STATE:4||CU:4||BASISSET:4||XAS:4||CRYSTALS:3||EXCITATIONS:3||MOTTHUBBARD SYSTEMS:3||HIGHENERGY SPIN:3||halfmetal:3||INSULATORS:3||LA2CUO4:3||MODEL:3||FLUCTUATIONS:3||CE:3||double exchange:3||TRANSITIONMETALS:3||RESISTIVITY:3||BORON:3||LA1XCAXMNO3:3||IRON:3||PES:3||ANTIMONIDES:2||MgB2:2||ZR METALLIC GLASSES:2||superconductor:2||CRITICALCURRENT DENSITY:2||CIRCULARDICHROISM:2||SEMICONDUCTORS:2||LOCALIZATION:2||INTRABAND OPTICAL CONDUCTIVITY:2||COLOSSAL MAGNETORESISTANCE:2||OXIDATION:2||EXISTENCE:2||COPPER:2||diboride:2||MAGNESIUMDIBORIDE:2||GAP:2||CE COMPOUNDS:2||CORE POLARIZATION:2||magnetoresistance:2||photoemission spectroscopy:2||electronphonon interaction:2||GETTER:2||PD:2||MAGNETISM:2||FECR2S4:2||SUPERCONDUCTING MGB2:2||WIRES:2||ABSORPTION:2||ENERGY:2||LA1XSRXMNO3:2||CONSTANTS:2||polaron:2||charge ordering:2||SCATTERING:2||XRAY PHOTOEMISSION:2||CeNiSn:2||phase diagram:2||PHOTOELECTRON:2||QUADRUPOLAR:2||perovskitemanganites:2||CO:2||SYSTEMS:2||DOPED ZNO:2||LOWFREQUENCY SOUND:2||LA:2||ELECTRONELECTRON SCATTERING:2||AU:2||DENSITYWAVE INSTABILITY:2||FERMISURFACE:2||hybridization:2||VALENCEBAND SATELLITE:2||SULFUR SPINEL:2||Heusler:2||APPROXIMATION:2||superexchange:2||colossal magnetoresistance:2||ALLOYS:2||DEPENDENCE:2||AG:2||electronic structures:2||AUGERSPECTRA:2||CR:2||PARAMETERS:2||DIFFRACTION:2||SEMICONDUCTORMETAL TRANSITION:1||INTERMEDIATEVALENCE:1||SMB6:1||SRRUO3:1||antiperovskite structure with antipolar nature:1||lowenergy twodimensional phonons:1||anatase TiO2:1||La3S4:1||metalinsulator transitions:1||MNO:1||ELECTRONICSTRUCTURES:1||MAGNETIC CIRCULARDICHROISM:1||Density functional theory:1||CeCo2:1||TOPOLARON CROSSOVER:1||EXCHANGE:1||cuprates:1||high Tc cuprates:1||magnetically ordered materials:1||ZNSE:1||Sr2xKxFeMoO6:1||CDW:1||TeCuO3:1||STRUCTURALPROPERTIES:1||MN:1||screening length:1||amorphous Fe:1||WAVE BASISSET:1||SILICONCARBIDE:1||HIGHPRESSURE:1||electronphonon coupling:1||quenched superconductivity:1||CMR perovskite manganites:1||OXIDE:1||polarons:1||synchrotron radiation:1||FULLERIDES:1||RESONANTPHOTOEMISSION:1||Silicon carbide:1||DFT calculation:1||Hybridized bands:1||GIANT MAGNETORESISTANCE:1||PEROVSKITES:1||Raman spectra:1||EXCHANGE ENHANCEMENT:1||SILICON:1||SR2FEMOO6:1||orbital ordering:1||delafossite:1||TITANIUMDIOXIDE:1||electronic structure of disordered solids:1||YFE2:1||Magnetic polaron:1||NA2TI2SB2O:1||STRONGCOUPLED SUPERCONDUCTORS:1||HEAVYFERMION SYSTEMS:1||firstprinciples calculations:1||MECHANISM:1||UNiSn:1||PHOTONIC BANDGAP:1||SINGLE IMPURITY:1||PHONONSPECTRUM:1||FERMISURFACE TOPOLOGY:1||SUPPRESSION:1||RESONANT PHOTOEMISSION:1||METALDOPED PICENE:1||PHOTOIONIZATION CROSSSECTIONS:1||PHOTOINDUCED FERRIMAGNETIC SYSTEMS:1||LINKAGE ISOMERISM:1||CHARGETRANSFER:1||Bilayer Graphene:1||MAGNETICFIELD:1||SPINWAVES:1||rareearth manganese oxides:1||magnonphonon interaction:1||NACO2O4:1||ENERGYBANDS:1||SELFENERGY:1||GAS:1||Fe0.5Cu0.5Cr2S4:1||scanning photoelectron microscopy (SPEM):1||MAGNETIC PROPERTIES:1||Stoner model:1||AMORPHOUS TRANSITIONMETALS:1||SPINGLASS STATES:1||NI:1||LA3NI2B2N3:1||SOLIDS:1||CEO2:1||BAND THEORY:1||dilute magnetic semiconductor:1||pyrochlore:1||Y1XPRXBA2CU3O7DELTA:1||and electronphonon interactions:1||VIBRATIONS:1||RAY PHOTOEMISSION:1||ALKALI CATION:1||Europium:1||colossal magnetoresistance:1||structural stability:1||ENERGYGAP:1||small polaron:1||DOUBLE EXCHANGE:1||Coulomb correlation:1||magnon:1||phonons:1||ELECTRON FERROMAGNETISM:1||CURIETEMPERATURE:1||ARPES:1||PLANEWAVE METHOD:1||Xray absorption spectroscopy (XAS):1||ROOMTEMPERATURE:1||MONOCHALCOGENIDES:1||HEAT:1||UPDSN:1||MOMENTS:1||XRAY ABSORPTION:1||SEMICONDUCTOR:1||Fermi surface nesting:1||optical phonon:1||disordered system:1||dilute magnetic semiconductors:1||CMR manganites:1||PHONONS:1||LATTICEDYNAMICS:1||OXIDES:1||4fphotoemission:1||permanent magnet:1||pseudogap:1||TRANSPORTPROPERTIES:1||ANTIFERROMAGNET:1||(BI,PB)SRCOO SYSTEM:1||semicore correlation:1||POLARIZATION:1||CRYSTAL:1||spinel:1||Xray magnetic circular dichroism (XMCD):1||magnetocapacitance:1||ANATASE:1||TEMPERATURES:1||Pseudogap:1||INTERFACE:1||SUBSTRATE:1||YNI2B2C:1||SAMARIUM SULFIDE:1||strong swave superconductor:1||DOPED MANGANITE:1||SYMMETRY:1||CENISN:1||resonance mode:1||DISORDERED SYSTEM:1||LITHIUM INTERCALATION:1||CUO2 PLANE:1||SURFACE:1||Delafossite:1||ELECTRICALPROPERTIES:1||NIMNSB:1||PTMNSB:1||ROOMTEMPERATURE FERROMAGNETISM:1||RUBIDIUM MANGANESE HEXACYANOFERRATE:1||COLOSSALMAGNETORESISTANCE:1||FINITE TEMPERATURES:1||LAMNO3:1||FE:1||transitionmetal oxides:1||giant magnetoresistance:1||phonon:1||COPPER OXIDES:1||valence states:1||thermoelectric:1||semiconductor:1||CATION DISTRIBUTION:1||FeCr2S4:1||photoemission spectroscopy (PES):1||METALLIC FERROMAGNETISM:1||GRAPHITE:1||SUSCEPTIBILITY:1||UBE13:1||RCrSb3:1||band JahnTeller:1||Ce3S4:1||TiO2:1||PrBa2Cu3O7delta:1||UNTWINNED PRBA2CU3O7:1||AGNIO2:1||HALFMETALLIC FERROMAGNETS:1||CI:1||Energy gap:1||Photoemission:1||Future applications:1||Photoemission measurements:1||Graphene:1||BANDSTRUCTURE:1||TC:1||superconductivity:1||magnetic semiconductors:1||CMRmanganites:1||thin films:1||spin dynamics:1||highTc superconductors:1||ITINERANTELECTRON FERROMAGNETISM:1||SINGLECRYSTALS:1||CeTe2:1||amorphous magnetic materials:1||EPITAXIAL GRAPHENE:1||LAYERED PNICTIDEOXIDES:1||BOROCARBIDE SUPERCONDUCTORS:1||AUGMENTEDWAVE METHOD:1||METALLIC MAGNET UNISN:1||ORIGIN:1||spectrum rearrangement:1||MEANFIELD THEORY:1||MOLECULEBASED MAGNETS:1||METASTABLE STATE:1||INSULATOR:1||magnetic orderin:1||FCC IRON:1||CeRu2:1||TL2MN2O7:1||isotope effect:1||Perovskitemanganites:1||RECURSION METHOD:1||PERPENDICULAR MAGNETICANISOTROPY:1||quasiparticle spectral density:1||GW:1||MANGANESE FERRITE:1||RESONANCE:1||SeCuO3:1||Optical conductivity:1||MASSLESS DIRAC FERMIONS:1||SCHOTTKYBARRIER:1||electronic structure:15||ELECTRONICSTRUCTURE:11||TRANSITIONMETAL COMPOUNDS:10||METALS:10||photoemission:8||SPECTRA:8||MAGNETORESISTANCE:7||FERROMAGNETISM:7||TRANSPORT:7||TRANSITION:6||FILMS:6||THINFILMS:5||TOTALENERGY CALCULATIONS:5||MAGNETICPROPERTIES:5||SUPERCONDUCTIVITY:5||PR:5||LATTICE:4||STATES:4||SPECTROSCOPY:4||FIELD:4||CRYSTALSTRUCTURE:4||PHOTOEMISSION:4||TEMPERATURE:4||TRANSITIONTEMPERATURE:4||XRAYABSORPTION:4||STATE:4||CU:4||BASISSET:4||XAS:4||CRYSTALS:3||EXCITATIONS:3||MOTTHUBBARD SYSTEMS:3||HIGHENERGY SPIN:3||halfmetal:3||INSULATORS:3||LA2CUO4:3||MODEL:3||FLUCTUATIONS:3||CE:3||double exchange:3||TRANSITIONMETALS:3||RESISTIVITY:3||BORON:3||LA1XCAXMNO3:3||IRON:3||PES:3||ANTIMONIDES:2||MgB2:2||ZR METALLIC GLASSES:2||superconductor:2||CRITICALCURRENT DENSITY:2||CIRCULARDICHROISM:2||SEMICONDUCTORS:2||LOCALIZATION:2||INTRABAND OPTICAL CONDUCTIVITY:2||COLOSSAL MAGNETORESISTANCE:2||OXIDATION:2||EXISTENCE:2||COPPER:2||diboride:2||MAGNESIUMDIBORIDE:2||GAP:2||CE COMPOUNDS:2||CORE POLARIZATION:2||magnetoresistance:2||photoemission spectroscopy:2||electronphonon interaction:2||GETTER:2||PD:2||MAGNETISM:2||FECR2S4:2||SUPERCONDUCTING MGB2:2||WIRES:2||ABSORPTION:2||ENERGY:2||LA1XSRXMNO3:2||CONSTANTS:2||polaron:2||charge ordering:2||SCATTERING:2||XRAY PHOTOEMISSION:2||CeNiSn:2||phase diagram:2||PHOTOELECTRON:2||QUADRUPOLAR:2||perovskitemanganites:2||CO:2||SYSTEMS:2||DOPED ZNO:2||LOWFREQUENCY SOUND:2||LA:2||ELECTRONELECTRON SCATTERING:2||AU:2||DENSITYWAVE INSTABILITY:2||FERMISURFACE:2||hybridization:2||VALENCEBAND SATELLITE:2||SULFUR SPINEL:2||Heusler:2||APPROXIMATION:2||superexchange:2||colossal magnetoresistance:2||ALLOYS:2||DEPENDENCE:2||AG:2||electronic structures:2||AUGERSPECTRA:2||CR:2||PARAMETERS:2||DIFFRACTION:2||SEMICONDUCTORMETAL TRANSITION:1||INTERMEDIATEVALENCE:1||SMB6:1||SRRUO3:1||antiperovskite structure with antipolar nature:1||lowenergy twodimensional phonons:1||anatase TiO2:1||La3S4:1||metalinsulator transitions:1||MNO:1||ELECTRONICSTRUCTURES:1||MAGNETIC CIRCULARDICHROISM:1||Density functional theory:1||CeCo2:1||TOPOLARON CROSSOVER:1||EXCHANGE:1||cuprates:1||high Tc cuprates:1||magnetically ordered materials:1||ZNSE:1||Sr2xKxFeMoO6:1||CDW:1||TeCuO3:1||STRUCTURALPROPERTIES:1||MN:1||screening length:1||amorphous Fe:1||WAVE BASISSET:1||SILICONCARBIDE:1||HIGHPRESSURE:1||electronphonon coupling:1||quenched superconductivity:1||CMR perovskite manganites:1||OXIDE:1||polarons:1||synchrotron radiation:1||FULLERIDES:1||RESONANTPHOTOEMISSION:1||Silicon carbide:1||DFT calculation:1||Hybridized bands:1||GIANT MAGNETORESISTANCE:1||PEROVSKITES:1||Raman spectra:1||EXCHANGE ENHANCEMENT:1||SILICON:1||SR2FEMOO6:1||orbital ordering:1||delafossite:1||TITANIUMDIOXIDE:1||electronic structure of disordered solids:1||YFE2:1||Magnetic polaron:1||NA2TI2SB2O:1||STRONGCOUPLED SUPERCONDUCTORS:1||HEAVYFERMION SYSTEMS:1||firstprinciples calculations:1||MECHANISM:1||UNiSn:1||PHOTONIC BANDGAP:1||SINGLE IMPURITY:1||PHONONSPECTRUM:1||FERMISURFACE TOPOLOGY:1||SUPPRESSION:1||RESONANT PHOTOEMISSION:1||METALDOPED PICENE:1||PHOTOIONIZATION CROSSSECTIONS:1||PHOTOINDUCED FERRIMAGNETIC SYSTEMS:1||LINKAGE ISOMERISM:1||CHARGETRANSFER:1||Bilayer Graphene:1||MAGNETICFIELD:1||SPINWAVES:1||rareearth manganese oxides:1||magnonphonon interaction:1||NACO2O4:1||ENERGYBANDS:1||SELFENERGY:1||GAS:1||Fe0.5Cu0.5Cr2S4:1||scanning photoelectron microscopy (SPEM):1||MAGNETIC PROPERTIES:1||Stoner model:1||AMORPHOUS TRANSITIONMETALS:1||SPINGLASS STATES:1||NI:1||LA3NI2B2N3:1||SOLIDS:1||CEO2:1||BAND THEORY:1||dilute magnetic semiconductor:1||pyrochlore:1||Y1XPRXBA2CU3O7DELTA:1||and electronphonon interactions:1||VIBRATIONS:1||RAY PHOTOEMISSION:1||ALKALI CATION:1||Europium:1||colossal magnetoresistance:1||structural stability:1||ENERGYGAP:1||small polaron:1||DOUBLE EXCHANGE:1||Coulomb correlation:1||magnon:1||phonons:1||ELECTRON FERROMAGNETISM:1||CURIETEMPERATURE:1||ARPES:1||PLANEWAVE METHOD:1||Xray absorption spectroscopy (XAS):1||ROOMTEMPERATURE:1||MONOCHALCOGENIDES:1||HEAT:1||UPDSN:1||MOMENTS:1||XRAY ABSORPTION:1||SEMICONDUCTOR:1||Fermi surface nesting:1||optical phonon:1||disordered system:1||dilute magnetic semiconductors:1||CMR manganites:1||PHONONS:1||LATTICEDYNAMICS:1||OXIDES:1||4fphotoemission:1||permanent magnet:1||pseudogap:1||TRANSPORTPROPERTIES:1||ANTIFERROMAGNET:1||(BI,PB)SRCOO SYSTEM:1||semicore correlation:1||POLARIZATION:1||CRYSTAL:1||spinel:1||Xray magnetic circular dichroism (XMCD):1||magnetocapacitance:1||ANATASE:1||TEMPERATURES:1||Pseudogap:1||INTERFACE:1||SUBSTRATE:1||YNI2B2C:1||SAMARIUM SULFIDE:1||strong swave superconductor:1||DOPED MANGANITE:1||SYMMETRY:1||CENISN:1||resonance mode:1||DISORDERED SYSTEM:1||LITHIUM INTERCALATION:1||CUO2 PLANE:1||SURFACE:1||Delafossite:1||ELECTRICALPROPERTIES:1||NIMNSB:1||PTMNSB:1||ROOMTEMPERATURE FERROMAGNETISM:1||RUBIDIUM MANGANESE HEXACYANOFERRATE:1||COLOSSALMAGNETORESISTANCE:1||FINITE TEMPERATURES:1||LAMNO3:1||FE:1||transitionmetal oxides:1||giant magnetoresistance:1||phonon:1||COPPER OXIDES:1||valence states:1||thermoelectric:1||semiconductor:1||CATION DISTRIBUTION:1||FeCr2S4:1||photoemission spectroscopy (PES):1||METALLIC FERROMAGNETISM:1||GRAPHITE:1||SUSCEPTIBILITY:1||UBE13:1||RCrSb3:1||band JahnTeller:1||Ce3S4:1||TiO2:1||PrBa2Cu3O7delta:1||UNTWINNED PRBA2CU3O7:1||AGNIO2:1||HALFMETALLIC FERROMAGNETS:1||CI:1||Energy gap:1||Photoemission:1||Future applications:1||Photoemission measurements:1||Graphene:1||BANDSTRUCTURE:1||TC:1||superconductivity:1||magnetic semiconductors:1||CMRmanganites:1||thin films:1||spin dynamics:1||highTc superconductors:1||ITINERANTELECTRON FERROMAGNETISM:1||SINGLECRYSTALS:1||CeTe2:1||amorphous magnetic materials:1||EPITAXIAL GRAPHENE:1||LAYERED PNICTIDEOXIDES:1||BOROCARBIDE SUPERCONDUCTORS:1||AUGMENTEDWAVE METHOD:1||METALLIC MAGNET UNISN:1||ORIGIN:1||spectrum rearrangement:1||MEANFIELD THEORY:1||MOLECULEBASED MAGNETS:1||METASTABLE STATE:1||INSULATOR:1||magnetic orderin:1||FCC IRON:1||CeRu2:1||TL2MN2O7:1||isotope effect:1||Perovskitemanganites:1||RECURSION METHOD:1||PERPENDICULAR MAGNETICANISOTROPY:1||quasiparticle spectral density:1||GW:1||MANGANESE FERRITE:1||RESONANCE:1||SeCuO3:1||Optical conductivity:1||MASSLESS DIRAC FERMIONS:1||SCHOTTKYBARRIER:1||electronic structure:15||ELECTRONICSTRUCTURE:11||TRANSITIONMETAL COMPOUNDS:10||METALS:10||photoemission:8||SPECTRA:8||MAGNETORESISTANCE:7||FERROMAGNETISM:7||TRANSPORT:7||TRANSITION:6||FILMS:6||THINFILMS:5||TOTALENERGY CALCULATIONS:5||MAGNETICPROPERTIES:5||SUPERCONDUCTIVITY:5||PR:5||LATTICE:4||STATES:4||SPECTROSCOPY:4||FIELD:4||CRYSTALSTRUCTURE:4||PHOTOEMISSION:4||TEMPERATURE:4||TRANSITIONTEMPERATURE:4||XRAYABSORPTION:4||STATE:4||CU:4||BASISSET:4||XAS:4||CRYSTALS:3||EXCITATIONS:3||MOTTHUBBARD SYSTEMS:3||HIGHENERGY SPIN:3||halfmetal:3||INSULATORS:3||LA2CUO4:3||MODEL:3||FLUCTUATIONS:3||CE:3||double exchange:3||TRANSITIONMETALS:3||RESISTIVITY:3||BORON:3||LA1XCAXMNO3:3||IRON:3||PES:3||ANTIMONIDES:2||MgB2:2||ZR METALLIC GLASSES:2||superconductor:2||CRITICALCURRENT DENSITY:2||CIRCULARDICHROISM:2||SEMICONDUCTORS:2||LOCALIZATION:2||INTRABAND OPTICAL CONDUCTIVITY:2||COLOSSAL MAGNETORESISTANCE:2||OXIDATION:2||EXISTENCE:2||COPPER:2||diboride:2||MAGNESIUMDIBORIDE:2||GAP:2||CE COMPOUNDS:2||CORE POLARIZATION:2||magnetoresistance:2||photoemission spectroscopy:2||electronphonon interaction:2||GETTER:2||PD:2||MAGNETISM:2||FECR2S4:2||SUPERCONDUCTING MGB2:2||WIRES:2||ABSORPTION:2||ENERGY:2||LA1XSRXMNO3:2||CONSTANTS:2||polaron:2||charge ordering:2||SCATTERING:2||XRAY PHOTOEMISSION:2||CeNiSn:2||phase diagram:2||PHOTOELECTRON:2||QUADRUPOLAR:2||perovskitemanganites:2||CO:2||SYSTEMS:2||DOPED ZNO:2||LOWFREQUENCY SOUND:2||LA:2||ELECTRONELECTRON SCATTERING:2||AU:2||DENSITYWAVE INSTABILITY:2||FERMISURFACE:2||hybridization:2||VALENCEBAND SATELLITE:2||SULFUR SPINEL:2||Heusler:2||APPROXIMATION:2||superexchange:2||colossal magnetoresistance:2||ALLOYS:2||DEPENDENCE:2||AG:2||electronic structures:2||AUGERSPECTRA:2||CR:2||PARAMETERS:2||DIFFRACTION:2||SEMICONDUCTORMETAL TRANSITION:1||INTERMEDIATEVALENCE:1||SMB6:1||SRRUO3:1||antiperovskite structure with antipolar nature:1||lowenergy twodimensional phonons:1||anatase TiO2:1||La3S4:1||metalinsulator transitions:1||MNO:1||ELECTRONICSTRUCTURES:1||MAGNETIC CIRCULARDICHROISM:1||Density functional theory:1||CeCo2:1||TOPOLARON CROSSOVER:1||EXCHANGE:1||cuprates:1||high Tc cuprates:1||magnetically ordered materials:1||ZNSE:1||Sr2xKxFeMoO6:1||CDW:1||TeCuO3:1||STRUCTURALPROPERTIES:1||MN:1||screening length:1||amorphous Fe:1||WAVE BASISSET:1||SILICONCARBIDE:1||HIGHPRESSURE:1||electronphonon coupling:1||quenched superconductivity:1||CMR perovskite manganites:1||OXIDE:1||polarons:1||synchrotron radiation:1||FULLERIDES:1||RESONANTPHOTOEMISSION:1||Silicon carbide:1||DFT calculation:1||Hybridized bands:1||GIANT MAGNETORESISTANCE:1||PEROVSKITES:1||Raman spectra:1||EXCHANGE ENHANCEMENT:1||SILICON:1||SR2FEMOO6:1||orbital ordering:1||delafossite:1||TITANIUMDIOXIDE:1||electronic structure of disordered solids:1||YFE2:1||Magnetic polaron:1||NA2TI2SB2O:1||STRONGCOUPLED SUPERCONDUCTORS:1||HEAVYFERMION SYSTEMS:1||firstprinciples calculations:1||MECHANISM:1||UNiSn:1||PHOTONIC BANDGAP:1||SINGLE IMPURITY:1||PHONONSPECTRUM:1||FERMISURFACE TOPOLOGY:1||SUPPRESSION:1||RESONANT PHOTOEMISSION:1||METALDOPED PICENE:1||PHOTOIONIZATION CROSSSECTIONS:1||PHOTOINDUCED FERRIMAGNETIC SYSTEMS:1||LINKAGE ISOMERISM:1||CHARGETRANSFER:1||Bilayer Graphene:1||MAGNETICFIELD:1||SPINWAVES:1||rareearth manganese oxides:1||magnonphonon interaction:1||NACO2O4:1||ENERGYBANDS:1||SELFENERGY:1||GAS:1||Fe0.5Cu0.5Cr2S4:1||scanning photoelectron microscopy (SPEM):1||MAGNETIC PROPERTIES:1||Stoner model:1||AMORPHOUS TRANSITIONMETALS:1||SPINGLASS STATES:1||NI:1||LA3NI2B2N3:1||SOLIDS:1||CEO2:1||BAND THEORY:1||dilute magnetic semiconductor:1||pyrochlore:1||Y1XPRXBA2CU3O7DELTA:1||and electronphonon interactions:1||VIBRATIONS:1||RAY PHOTOEMISSION:1||ALKALI CATION:1||Europium:1||colossal magnetoresistance:1||structural stability:1||ENERGYGAP:1||small polaron:1||DOUBLE EXCHANGE:1||Coulomb correlation:1||magnon:1||phonons:1||ELECTRON FERROMAGNETISM:1||CURIETEMPERATURE:1||ARPES:1||PLANEWAVE METHOD:1||Xray absorption spectroscopy (XAS):1||ROOMTEMPERATURE:1||MONOCHALCOGENIDES:1||HEAT:1||UPDSN:1||MOMENTS:1||XRAY ABSORPTION:1||SEMICONDUCTOR:1||Fermi surface nesting:1||optical phonon:1||disordered system:1||dilute magnetic semiconductors:1||CMR manganites:1||PHONONS:1||LATTICEDYNAMICS:1||OXIDES:1||4fphotoemission:1||permanent magnet:1||pseudogap:1||TRANSPORTPROPERTIES:1||ANTIFERROMAGNET:1||(BI,PB)SRCOO SYSTEM:1||semicore correlation:1||POLARIZATION:1||CRYSTAL:1||spinel:1||Xray magnetic circular dichroism (XMCD):1||magnetocapacitance:1||ANATASE:1||TEMPERATURES:1||Pseudogap:1||INTERFACE:1||SUBSTRATE:1||YNI2B2C:1||SAMARIUM SULFIDE:1||strong swave superconductor:1||DOPED MANGANITE:1||SYMMETRY:1||CENISN:1||resonance mode:1||DISORDERED SYSTEM:1||LITHIUM INTERCALATION:1||CUO2 PLANE:1||SURFACE:1||Delafossite:1||ELECTRICALPROPERTIES:1||NIMNSB:1||PTMNSB:1||ROOMTEMPERATURE FERROMAGNETISM:1||RUBIDIUM MANGANESE HEXACYANOFERRATE:1||COLOSSALMAGNETORESISTANCE:1||FINITE TEMPERATURES:1||LAMNO3:1||FE:1||transitionmetal oxides:1||giant magnetoresistance:1||phonon:1||COPPER OXIDES:1||valence states:1||thermoelectric:1||semiconductor:1||CATION DISTRIBUTION:1||FeCr2S4:1||photoemission spectroscopy (PES):1||METALLIC FERROMAGNETISM:1||GRAPHITE:1||SUSCEPTIBILITY:1||UBE13:1||RCrSb3:1||band JahnTeller:1||Ce3S4:1||TiO2:1||PrBa2Cu3O7delta:1||UNTWINNED PRBA2CU3O7:1||AGNIO2:1||HALFMETALLIC FERROMAGNETS:1||CI:1||Energy gap:1||Photoemission:1||Future applications:1||Photoemission measurements:1||Graphene:1||BANDSTRUCTURE:1||TC:1||superconductivity:1||magnetic semiconductors:1||CMRmanganites:1||thin films:1||spin dynamics:1||highTc superconductors:1||ITINERANTELECTRON FERROMAGNETISM:1||SINGLECRYSTALS:1||CeTe2:1||amorphous magnetic materials:1||EPITAXIAL GRAPHENE:1||LAYERED PNICTIDEOXIDES:1||BOROCARBIDE SUPERCONDUCTORS:1||AUGMENTEDWAVE METHOD:1||METALLIC MAGNET UNISN:1||ORIGIN:1||spectrum rearrangement:1||MEANFIELD THEORY:1||MOLECULEBASED MAGNETS:1||METASTABLE STATE:1||INSULATOR:1||magnetic orderin:1||FCC IRON:1||CeRu2:1||TL2MN2O7:1||isotope effect:1||Perovskitemanganites:1||RECURSION METHOD:1||PERPENDICULAR MAGNETICANISOTROPY:1||quasiparticle spectral density:1||GW:1||MANGANESE FERRITE:1||RESONANCE:1||SeCuO3:1||Optical conductivity:1||MASSLESS DIRAC FERMIONS:1||SCHOTTKYBARRIER:1||electronic structure:15||ELECTRONICSTRUCTURE:11||TRANSITIONMETAL COMPOUNDS:10||METALS:10||photoemission:8||SPECTRA:8||MAGNETORESISTANCE:7||FERROMAGNETISM:7||TRANSPORT:7||TRANSITION:6||FILMS:6||THINFILMS:5||TOTALENERGY CALCULATIONS:5||MAGNETICPROPERTIES:5||SUPERCONDUCTIVITY:5||PR:5||LATTICE:4||STATES:4||SPECTROSCOPY:4||FIELD:4||CRYSTALSTRUCTURE:4||PHOTOEMISSION:4||TEMPERATURE:4||TRANSITIONTEMPERATURE:4||XRAYABSORPTION:4||STATE:4||CU:4||BASISSET:4||XAS:4||CRYSTALS:3||EXCITATIONS:3||MOTTHUBBARD SYSTEMS:3||HIGHENERGY SPIN:3||halfmetal:3||INSULATORS:3||LA2CUO4:3||MODEL:3||FLUCTUATIONS:3||CE:3||double exchange:3||TRANSITIONMETALS:3||RESISTIVITY:3||BORON:3||LA1XCAXMNO3:3||IRON:3||PES:3||ANTIMONIDES:2||MgB2:2||ZR METALLIC GLASSES:2||superconductor:2||CRITICALCURRENT DENSITY:2||CIRCULARDICHROISM:2||SEMICONDUCTORS:2||LOCALIZATION:2||INTRABAND OPTICAL CONDUCTIVITY:2||COLOSSAL MAGNETORESISTANCE:2||OXIDATION:2||EXISTENCE:2||COPPER:2||diboride:2||MAGNESIUMDIBORIDE:2||GAP:2||CE COMPOUNDS:2||CORE POLARIZATION:2||magnetoresistance:2||photoemission spectroscopy:2||electronphonon interaction:2||GETTER:2||PD:2||MAGNETISM:2||FECR2S4:2||SUPERCONDUCTING MGB2:2||WIRES:2||ABSORPTION:2||ENERGY:2||LA1XSRXMNO3:2||CONSTANTS:2||polaron:2||charge ordering:2||SCATTERING:2||XRAY PHOTOEMISSION:2||CeNiSn:2||phase diagram:2||PHOTOELECTRON:2||QUADRUPOLAR:2||perovskitemanganites:2||CO:2||SYSTEMS:2||DOPED ZNO:2||LOWFREQUENCY SOUND:2||LA:2||ELECTRONELECTRON SCATTERING:2||AU:2||DENSITYWAVE INSTABILITY:2||FERMISURFACE:2||hybridization:2||VALENCEBAND SATELLITE:2||SULFUR SPINEL:2||Heusler:2||APPROXIMATION:2||superexchange:2||colossal magnetoresistance:2||ALLOYS:2||DEPENDENCE:2||AG:2||electronic structures:2||AUGERSPECTRA:2||CR:2||PARAMETERS:2||DIFFRACTION:2||SEMICONDUCTORMETAL TRANSITION:1||INTERMEDIATEVALENCE:1||SMB6:1||SRRUO3:1||antiperovskite structure with antipolar nature:1||lowenergy twodimensional phonons:1||anatase TiO2:1||La3S4:1||metalinsulator transitions:1||MNO:1||ELECTRONICSTRUCTURES:1||MAGNETIC CIRCULARDICHROISM:1||Density functional theory:1||CeCo2:1||TOPOLARON CROSSOVER:1||EXCHANGE:1||cuprates:1||high Tc cuprates:1||magnetically ordered materials:1||ZNSE:1||Sr2xKxFeMoO6:1||CDW:1||TeCuO3:1||STRUCTURALPROPERTIES:1||MN:1||screening length:1||amorphous Fe:1||WAVE BASISSET:1||SILICONCARBIDE:1||HIGHPRESSURE:1||electronphonon coupling:1||quenched superconductivity:1||CMR perovskite manganites:1||OXIDE:1||polarons:1||synchrotron radiation:1||FULLERIDES:1||RESONANTPHOTOEMISSION:1||Silicon carbide:1||DFT calculation:1||Hybridized bands:1||GIANT MAGNETORESISTANCE:1||PEROVSKITES:1||Raman spectra:1||EXCHANGE ENHANCEMENT:1||SILICON:1||SR2FEMOO6:1||orbital ordering:1||delafossite:1||TITANIUMDIOXIDE:1||electronic structure of disordered solids:1||YFE2:1||Magnetic polaron:1||NA2TI2SB2O:1||STRONGCOUPLED SUPERCONDUCTORS:1||HEAVYFERMION SYSTEMS:1||firstprinciples calculations:1||MECHANISM:1||UNiSn:1||PHOTONIC BANDGAP:1||SINGLE IMPURITY:1||PHONONSPECTRUM:1||FERMISURFACE TOPOLOGY:1||SUPPRESSION:1||RESONANT PHOTOEMISSION:1||METALDOPED PICENE:1||PHOTOIONIZATION CROSSSECTIONS:1||PHOTOINDUCED FERRIMAGNETIC SYSTEMS:1||LINKAGE ISOMERISM:1||CHARGETRANSFER:1||Bilayer Graphene:1||MAGNETICFIELD:1||SPINWAVES:1||rareearth manganese oxides:1||magnonphonon interaction:1||NACO2O4:1||ENERGYBANDS:1||SELFENERGY:1||GAS:1||Fe0.5Cu0.5Cr2S4:1||scanning photoelectron microscopy (SPEM):1||MAGNETIC PROPERTIES:1||Stoner model:1||AMORPHOUS TRANSITIONMETALS:1||SPINGLASS STATES:1||NI:1||LA3NI2B2N3:1||SOLIDS:1||CEO2:1||BAND THEORY:1||dilute magnetic semiconductor:1||pyrochlore:1||Y1XPRXBA2CU3O7DELTA:1||and electronphonon interactions:1||VIBRATIONS:1||RAY PHOTOEMISSION:1||ALKALI CATION:1||Europium:1||colossal magnetoresistance:1||structural stability:1||ENERGYGAP:1||small polaron:1||DOUBLE EXCHANGE:1||Coulomb correlation:1||magnon:1||phonons:1||ELECTRON FERROMAGNETISM:1||CURIETEMPERATURE:1||ARPES:1||PLANEWAVE METHOD:1||Xray absorption spectroscopy (XAS):1||ROOMTEMPERATURE:1||MONOCHALCOGENIDES:1||HEAT:1||UPDSN:1||MOMENTS:1||XRAY ABSORPTION:1||SEMICONDUCTOR:1||Fermi surface nesting:1||optical phonon:1||disordered system:1||dilute magnetic semiconductors:1||CMR manganites:1||PHONONS:1||LATTICEDYNAMICS:1||OXIDES:1||4fphotoemission:1||permanent magnet:1||pseudogap:1||TRANSPORTPROPERTIES:1||ANTIFERROMAGNET:1||(BI,PB)SRCOO SYSTEM:1||semicore correlation:1||POLARIZATION:1||CRYSTAL:1||spinel:1||Xray magnetic circular dichroism (XMCD):1||magnetocapacitance:1||ANATASE:1||TEMPERATURES:1||Pseudogap:1||INTERFACE:1||SUBSTRATE:1||YNI2B2C:1||SAMARIUM SULFIDE:1||strong swave superconductor:1||DOPED MANGANITE:1||SYMMETRY:1||CENISN:1||resonance mode:1||DISORDERED SYSTEM:1||LITHIUM INTERCALATION:1||CUO2 PLANE:1||SURFACE:1||Delafossite:1||ELECTRICALPROPERTIES:1||NIMNSB:1||PTMNSB:1||ROOMTEMPERATURE FERROMAGNETISM:1||RUBIDIUM MANGANESE HEXACYANOFERRATE:1||COLOSSALMAGNETORESISTANCE:1||FINITE TEMPERATURES:1||LAMNO3:1||FE:1||transitionmetal oxides:1||giant magnetoresistance:1||phonon:1||COPPER OXIDES:1||valence states:1||thermoelectric:1||semiconductor:1||CATION DISTRIBUTION:1||FeCr2S4:1||photoem