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KIM, DONG EON (김동언)
Dept of Physics(물리학과)
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RADIATION:10||PULSES:8||PHOTOLUMINESCENCE:7||LASER:7||GENERATION:6||NANORODS:6||GROWTH:6||NANOWIRES:5||IMPLANTED GAN:5||SPECTROSCOPY:5||THINFILMS:4||DYNAMICS:4||SILICON:4||EXTREMEULTRAVIOLET:4||AMPLIFICATION:4||PRESSURE:4||PHASE:4||OPTICALPROPERTIES:4||SYSTEM:4||EMISSION:4||FEL:3||N2O:3||FILMS:3||OPTICS:3||SPECTRA:3||FIELD:3||MIRRORS:3||ARRAYS:3||CLUSTERS:3||SIO2:3||IONIZATION:3||VACUUM:3||SCATTERING:3||IONS:2||LUMINESCENCE PROPERTIES:2||ANISOTROPY:2||BEAMS:2||DIFFRACTION:2||DISPERSION:2||chemical vapor deposition (CVD):2||ELECTRONICSTRUCTURE:2||MOSFETS:2||SI3N4:2||DENSITY:2||LIGHT:2||PLASMAS:2||MATTER:2||nanocomposites:2||RAMANSCATTERING:2||NANOPARTICLES:2||OXIDE:2||AMPLIFIED SPONTANEOUS EMISSION:2||NM WAVELENGTH:2||GAIN:2||CARBON NANOTUBES:2||CROSSSECTIONS:2||LIGHTEMITTINGDIODES:2||PULSE:2||CARBON PLASMA:2||TISAPPHIRE LASER:2||Raman scattering:2||ROUTE:2||multilayer:2||CATHODOLUMINESCENCE:2||highresolution transmission electronic microscope (HRTEM):2||DIFFERENCEFREQUENCYGENERATION:2||CRYSTAL:2||laserproduced plasma:2||NANOCABLES:2||photoluminescence:2||MAGNETIC ALLOY SEMICONDUCTORS:2||MOLECULARBEAM EPITAXY:2||EARTHDOPED GAN:2||LASER FIELDS:2||CHIRPEDPULSEAMPLIFICATION:2||ALN:2||GAUSSIANBEAM:2||ASSISTED CATALYTIC GROWTH:2||BLUE:2||NANOSTRUCTURES:2||MAGNETOELECTRONICS:2||MICROSCOPY:2||ELECTROLUMINESCENCE:2||LASERPULSES:2||GaN nanowires:2||GALLIUM NITRIDE NANOWIRES:2||GAMNN:2||NANOTUBES:2||PHYSICS:2||Femtosecond laser:2||parametric oscillators and amplifiers:1||ultrafast lasers:1||VALENCE:1||nanowires:1||DILUTED MAGNETIC SEMICONDUCTOR:1||LUMINESCENCE:1||Density modulation:1||Energy modulation:1||Current enhanced SASE free electron laser:1||Undulator radiation:1||FREEELECTRON LASERS:1||ULTRATHIN FERROMAGNETICFILMS:1||OXIDEFILMS:1||ABLATION:1||COMPONENT:1||METAL:1||innershell excited states:1||Nelike ions:1||TRANSITIONS:1||XUV spectrometer:1||DIAGNOSTICS:1||Xray scattering:1||MO/SI:1||pulsed laser deposition:1||KEV IMPACT ENERGIES:1||vacuum electron acceleration:1||HIGHINTENSITY LASER:1||JUNCTIONS:1||LOWTEMPERATURE GROWTH:1||nanocrystalline materials:1||MOLECULAR PHOTOIONIZATION:1||LOCALIZATION:1||DEUTERIUM CLUSTERS:1||EXPLOSIONS:1||REGENERATIVE AMPLIFIERS:1||RAREGASES:1||THz radiation:1||FREEELECTRON LASER:1||REALTIME OBSERVATION:1||TARGET:1||photoionized plasmas:1||fs Xray laser:1||emission profile:1||HIGHORDER HARMONICS:1||Xray laser:1||atomic transition:1||EXCITATION:1||LASERS:1||PERFORMANCE:1||RELATIVISTIC ELECTRONS:1||BI2O3DOPED ZNO:1||INNERSHELL IONIZATION:1||Laser wakefield:1||FREQUENCY:1||SOLIDSTATE LASERS:1||Linearly polarized:1||THERMIONIC EMISSION:1||PULSE AMPLIFICATION SYSTEM:1||BIB3O6:1||NM:1||NONCOVALENT INTERACTIONS:1||CRYSTALLINE:1||INTENSITY:1||JETS:1||COHERENT:1||LINE:1||ANGULARDISTRIBUTION:1||SILVER IONS:1||magnetic anisotropy:1||DEVICES:1||Auger transitions:1||CosterKronig transitions:1||EFFICIENT:1||ELECTRONIMPACT IONIZATION:1||ULTRASHORTPULSE:1||Nanowire:1||Heterostructure:1||soft Xray reflectivity:1||PLASMA ACCELERATOR:1||ZINCOXIDE NANOWIRES:1||CHEMICALVAPORDEPOSITION:1||Electron acceleration:1||Ionization of gases:1||Delay dependent:1||MULTIPHOTON IONIZATION:1||FRAGMENTATION:1||GASJET:1||ultrafast nonlinear optics:1||CYCLE PULSES:1||KHZ:1||chemical vapor deposition:1||ferromagnetism:1||ABSORPTION:1||TERAHERTZ RADIATION:1||SCIENCE:1||FIELDS:1||ELECTRONS:1||nanomultilayer structures:1||YIELDS:1||AUGER:1||10HZ REPETITION RATE:1||MULTITERAWATT:1||SPECTROGRAPH:1||HIGHHARMONICGENERATION:1||spectroscopy:1||level population:1||PARTICLEACCELERATION:1||OPTICAL FREQUENCYMEASUREMENT:1||NANOWALLS:1||ROOMTEMPERATURE:1||AVERAGE OUTPUT POWER:1||GROUPVELOCITYMISMATCH:1||Impact ionization:1||Dynamics:1||Lasers:1||Collisional process:1||ABOVETHRESHOLD IONIZATION:1||MAINGROUP THERMOCHEMISTRY:1||dilute magnetic semiconductors:1||GACRN:1||SIZE:1||ATTOSECOND:1||Ar cluster:1||Xray astrophysics:1||photoionization:1||irons:1||normal incidence pulsed laser deposition:1||SHELLS:1||Silicon Oxide:1||gaspuff Zpinch:1||Xray:1||soft Xray reflectors:1||ESCAPE:1||ZN2SIO4:1||SILICA:1||Time delay:1||Collisional plasmas:1||MASSSPECTROMETRY:1||NUCLEARFUSION:1||PARAMETRIC AMPLIFICATION:1||LYING ELECTRONIC STATES:1||ADJUSTABLEPARAMETERS:1||MAGNETICPROPERTIES:1||LIQUIDPHASE EPITAXY:1||CEP laser:1||REGION:1||Plasma waveguide:1||AMBIENT GAS:1||DEPOSITION:1||HARMONICGENERATION:1||ENHANCEMENT:1||imaging spectrometer:1||Abel inversion:1||Water window:1||Liquid nitrogen jet:1||CHARGEEXCHANGE:1||NOBEL LECTURE:1||VARISTOR:1||EPITAXY:1||THINDISK LASER:1||HIGHREPETITIONRATE:1||Atom lasers:1||Electronimpact excitation:1||High order harmonics:1||ultrafast technology:1||PEAK POWER:1||CHARGED ALUMINUM CLUSTERS:1||GaN:1||THIN:1||Electron beam:1||INTENSE:1||Hard Xray pulse generation:1||NONLINEAR THOMSON SCATTERING:1||MULTILAYER:1||UVvisible spectrometer:1||ATOMS:1||innershell transitions:1||CORRECTED CONCAVE GRATINGS:1||DISCHARGE:1||LASERPLASMA:1||thin film:1||reflectivity:1||opacity:1||gain:1||smallangle Xray scattering:1||SOFTXRAY:1||ZINCOXIDE:1||CYGNUSX3:1||Betatron oscillation:1||ACCELERATOR:1||STRAINEDLAYER SUPERLATTICES:1||OPTICAL PARAMETRIC AMPLIFICATION:1||PASSIVE MODELOCKING:1||Collision dynamics:1||MUM:1||EXACTEXCHANGE:1||BASISSET:1||APPROXIMATION:1||OXYNITRIDES:1||Beam energy modulation:1||polarization spectroscopy:1||REORIENTATION TRANSITION:1||DEPENDENCE:1||sulfurs:1||BUILDINGBLOCKS:1||RATES:1||OPTICAL PULSES:1||toroidal mirror:1||XRAY LASER:1||CALCIUM:1||radially polarized laser:1||GRAINBOUNDARIES:1||VAPORDEPOSITION:1||Xray generation:1||MAGNETIZATION:1||Electric excitation:1||Laserinduced gas plasmas:1||Qualitative analysis:1||SCHEME:1||RADIATION:10||PULSES:8||PHOTOLUMINESCENCE:7||LASER:7||GENERATION:6||NANORODS:6||GROWTH:6||NANOWIRES:5||IMPLANTED GAN:5||SPECTROSCOPY:5||THINFILMS:4||DYNAMICS:4||SILICON:4||EXTREMEULTRAVIOLET:4||AMPLIFICATION:4||PRESSURE:4||PHASE:4||OPTICALPROPERTIES:4||SYSTEM:4||EMISSION:4||FEL:3||N2O:3||FILMS:3||OPTICS:3||SPECTRA:3||FIELD:3||MIRRORS:3||ARRAYS:3||CLUSTERS:3||SIO2:3||IONIZATION:3||VACUUM:3||SCATTERING:3||IONS:2||LUMINESCENCE PROPERTIES:2||ANISOTROPY:2||BEAMS:2||DIFFRACTION:2||DISPERSION:2||chemical vapor deposition (CVD):2||ELECTRONICSTRUCTURE:2||MOSFETS:2||SI3N4:2||DENSITY:2||LIGHT:2||PLASMAS:2||MATTER:2||nanocomposites:2||RAMANSCATTERING:2||NANOPARTICLES:2||OXIDE:2||AMPLIFIED SPONTANEOUS EMISSION:2||NM WAVELENGTH:2||GAIN:2||CARBON NANOTUBES:2||CROSSSECTIONS:2||LIGHTEMITTINGDIODES:2||PULSE:2||CARBON PLASMA:2||TISAPPHIRE LASER:2||Raman scattering:2||ROUTE:2||multilayer:2||CATHODOLUMINESCENCE:2||highresolution transmission electronic microscope (HRTEM):2||DIFFERENCEFREQUENCYGENERATION:2||CRYSTAL:2||laserproduced plasma:2||NANOCABLES:2||photoluminescence:2||MAGNETIC ALLOY SEMICONDUCTORS:2||MOLECULARBEAM EPITAXY:2||EARTHDOPED GAN:2||LASER FIELDS:2||CHIRPEDPULSEAMPLIFICATION:2||ALN:2||GAUSSIANBEAM:2||ASSISTED CATALYTIC GROWTH:2||BLUE:2||NANOSTRUCTURES:2||MAGNETOELECTRONICS:2||MICROSCOPY:2||ELECTROLUMINESCENCE:2||LASERPULSES:2||GaN nanowires:2||GALLIUM NITRIDE NANOWIRES:2||GAMNN:2||NANOTUBES:2||PHYSICS:2||Femtosecond laser:2||parametric oscillators and amplifiers:1||ultrafast lasers:1||VALENCE:1||nanowires:1||DILUTED MAGNETIC SEMICONDUCTOR:1||LUMINESCENCE:1||Density modulation:1||Energy modulation:1||Current enhanced SASE free electron laser:1||Undulator radiation:1||FREEELECTRON LASERS:1||ULTRATHIN FERROMAGNETICFILMS:1||OXIDEFILMS:1||ABLATION:1||COMPONENT:1||METAL:1||innershell excited states:1||Nelike ions:1||TRANSITIONS:1||XUV spectrometer:1||DIAGNOSTICS:1||Xray scattering:1||MO/SI:1||pulsed laser deposition:1||KEV IMPACT ENERGIES:1||vacuum electron acceleration:1||HIGHINTENSITY LASER:1||JUNCTIONS:1||LOWTEMPERATURE GROWTH:1||nanocrystalline materials:1||MOLECULAR PHOTOIONIZATION:1||LOCALIZATION:1||DEUTERIUM CLUSTERS:1||EXPLOSIONS:1||REGENERATIVE AMPLIFIERS:1||RAREGASES:1||THz radiation:1||FREEELECTRON LASER:1||REALTIME OBSERVATION:1||TARGET:1||photoionized plasmas:1||fs Xray laser:1||emission profile:1||HIGHORDER HARMONICS:1||Xray laser:1||atomic transition:1||EXCITATION:1||LASERS:1||PERFORMANCE:1||RELATIVISTIC ELECTRONS:1||BI2O3DOPED ZNO:1||INNERSHELL IONIZATION:1||Laser wakefield:1||FREQUENCY:1||SOLIDSTATE LASERS:1||Linearly polarized:1||THERMIONIC EMISSION:1||PULSE AMPLIFICATION SYSTEM:1||BIB3O6:1||NM:1||NONCOVALENT INTERACTIONS:1||CRYSTALLINE:1||INTENSITY:1||JETS:1||COHERENT:1||LINE:1||ANGULARDISTRIBUTION:1||SILVER IONS:1||magnetic anisotropy:1||DEVICES:1||Auger transitions:1||CosterKronig transitions:1||EFFICIENT:1||ELECTRONIMPACT IONIZATION:1||ULTRASHORTPULSE:1||Nanowire:1||Heterostructure:1||soft Xray reflectivity:1||PLASMA ACCELERATOR:1||ZINCOXIDE NANOWIRES:1||CHEMICALVAPORDEPOSITION:1||Electron acceleration:1||Ionization of gases:1||Delay dependent:1||MULTIPHOTON IONIZATION:1||FRAGMENTATION:1||GASJET:1||ultrafast nonlinear optics:1||CYCLE PULSES:1||KHZ:1||chemical vapor deposition:1||ferromagnetism:1||ABSORPTION:1||TERAHERTZ RADIATION:1||SCIENCE:1||FIELDS:1||ELECTRONS:1||nanomultilayer structures:1||YIELDS:1||AUGER:1||10HZ REPETITION RATE:1||MULTITERAWATT:1||SPECTROGRAPH:1||HIGHHARMONICGENERATION:1||spectroscopy:1||level population:1||PARTICLEACCELERATION:1||OPTICAL FREQUENCYMEASUREMENT:1||NANOWALLS:1||ROOMTEMPERATURE:1||AVERAGE OUTPUT POWER:1||GROUPVELOCITYMISMATCH:1||Impact ionization:1||Dynamics:1||Lasers:1||Collisional process:1||ABOVETHRESHOLD IONIZATION:1||MAINGROUP THERMOCHEMISTRY:1||dilute magnetic semiconductors:1||GACRN:1||SIZE:1||ATTOSECOND:1||Ar cluster:1||Xray astrophysics:1||photoionization:1||irons:1||normal incidence pulsed laser deposition:1||SHELLS:1||Silicon Oxide:1||gaspuff Zpinch:1||Xray:1||soft Xray reflectors:1||ESCAPE:1||ZN2SIO4:1||SILICA:1||Time delay:1||Collisional plasmas:1||MASSSPECTROMETRY:1||NUCLEARFUSION:1||PARAMETRIC AMPLIFICATION:1||LYING ELECTRONIC STATES:1||ADJUSTABLEPARAMETERS:1||MAGNETICPROPERTIES:1||LIQUIDPHASE EPITAXY:1||CEP laser:1||REGION:1||Plasma waveguide:1||AMBIENT GAS:1||DEPOSITION:1||HARMONICGENERATION:1||ENHANCEMENT:1||imaging spectrometer:1||Abel inversion:1||Water window:1||Liquid nitrogen jet:1||CHARGEEXCHANGE:1||NOBEL LECTURE:1||VARISTOR:1||EPITAXY:1||THINDISK LASER:1||HIGHREPETITIONRATE:1||Atom lasers:1||Electronimpact excitation:1||High order harmonics:1||ultrafast technology:1||PEAK POWER:1||CHARGED ALUMINUM CLUSTERS:1||GaN:1||THIN:1||Electron beam:1||INTENSE:1||Hard Xray pulse generation:1||NONLINEAR THOMSON SCATTERING:1||MULTILAYER:1||UVvisible spectrometer:1||ATOMS:1||innershell transitions:1||CORRECTED CONCAVE GRATINGS:1||DISCHARGE:1||LASERPLASMA:1||thin film:1||reflectivity:1||opacity:1||gain:1||smallangle Xray scattering:1||SOFTXRAY:1||ZINCOXIDE:1||CYGNUSX3:1||Betatron oscillation:1||ACCELERATOR:1||STRAINEDLAYER SUPERLATTICES:1||OPTICAL PARAMETRIC AMPLIFICATION:1||PASSIVE MODELOCKING:1||Collision dynamics:1||MUM:1||EXACTEXCHANGE:1||BASISSET:1||APPROXIMATION:1||OXYNITRIDES:1||Beam energy modulation:1||polarization spectroscopy:1||REORIENTATION TRANSITION:1||DEPENDENCE:1||sulfurs:1||BUILDINGBLOCKS:1||RATES:1||OPTICAL PULSES:1||toroidal mirror:1||XRAY LASER:1||CALCIUM:1||radially polarized laser:1||GRAINBOUNDARIES:1||VAPORDEPOSITION:1||Xray generation:1||MAGNETIZATION:1||Electric excitation:1||Laserinduced gas plasmas:1||Qualitative analysis:1||SCHEME:1||RADIATION:10||PULSES:8||PHOTOLUMINESCENCE:7||LASER:7||GENERATION:6||NANORODS:6||GROWTH:6||NANOWIRES:5||IMPLANTED GAN:5||SPECTROSCOPY:5||THINFILMS:4||DYNAMICS:4||SILICON:4||EXTREMEULTRAVIOLET:4||AMPLIFICATION:4||PRESSURE:4||PHASE:4||OPTICALPROPERTIES:4||SYSTEM:4||EMISSION:4||FEL:3||N2O:3||FILMS:3||OPTICS:3||SPECTRA:3||FIELD:3||MIRRORS:3||ARRAYS:3||CLUSTERS:3||SIO2:3||IONIZATION:3||VACUUM:3||SCATTERING:3||IONS:2||LUMINESCENCE PROPERTIES:2||ANISOTROPY:2||BEAMS:2||DIFFRACTION:2||DISPERSION:2||chemical vapor deposition (CVD):2||ELECTRONICSTRUCTURE:2||MOSFETS:2||SI3N4:2||DENSITY:2||LIGHT:2||PLASMAS:2||MATTER:2||nanocomposites:2||RAMANSCATTERING:2||NANOPARTICLES:2||OXIDE:2||AMPLIFIED SPONTANEOUS EMISSION:2||NM WAVELENGTH:2||GAIN:2||CARBON NANOTUBES:2||CROSSSECTIONS:2||LIGHTEMITTINGDIODES:2||PULSE:2||CARBON PLASMA:2||TISAPPHIRE LASER:2||Raman scattering:2||ROUTE:2||multilayer:2||CATHODOLUMINESCENCE:2||highresolution transmission electronic microscope (HRTEM):2||DIFFERENCEFREQUENCYGENERATION:2||CRYSTAL:2||laserproduced plasma:2||NANOCABLES:2||photoluminescence:2||MAGNETIC ALLOY SEMICONDUCTORS:2||MOLECULARBEAM EPITAXY:2||EARTHDOPED GAN:2||LASER FIELDS:2||CHIRPEDPULSEAMPLIFICATION:2||ALN:2||GAUSSIANBEAM:2||ASSISTED CATALYTIC GROWTH:2||BLUE:2||NANOSTRUCTURES:2||MAGNETOELECTRONICS:2||MICROSCOPY:2||ELECTROLUMINESCENCE:2||LASERPULSES:2||GaN nanowires:2||GALLIUM NITRIDE NANOWIRES:2||GAMNN:2||NANOTUBES:2||PHYSICS:2||Femtosecond laser:2||parametric oscillators and amplifiers:1||ultrafast lasers:1||VALENCE:1||nanowires:1||DILUTED MAGNETIC SEMICONDUCTOR:1||LUMINESCENCE:1||Density modulation:1||Energy modulation:1||Current enhanced SASE free electron laser:1||Undulator radiation:1||FREEELECTRON LASERS:1||ULTRATHIN FERROMAGNETICFILMS:1||OXIDEFILMS:1||ABLATION:1||COMPONENT:1||METAL:1||innershell excited states:1||Nelike ions:1||TRANSITIONS:1||XUV spectrometer:1||DIAGNOSTICS:1||Xray scattering:1||MO/SI:1||pulsed laser deposition:1||KEV IMPACT ENERGIES:1||vacuum electron acceleration:1||HIGHINTENSITY LASER:1||JUNCTIONS:1||LOWTEMPERATURE GROWTH:1||nanocrystalline materials:1||MOLECULAR PHOTOIONIZATION:1||LOCALIZATION:1||DEUTERIUM CLUSTERS:1||EXPLOSIONS:1||REGENERATIVE AMPLIFIERS:1||RAREGASES:1||THz radiation:1||FREEELECTRON LASER:1||REALTIME OBSERVATION:1||TARGET:1||photoionized plasmas:1||fs Xray laser:1||emission profile:1||HIGHORDER HARMONICS:1||Xray laser:1||atomic transition:1||EXCITATION:1||LASERS:1||PERFORMANCE:1||RELATIVISTIC ELECTRONS:1||BI2O3DOPED ZNO:1||INNERSHELL IONIZATION:1||Laser wakefield:1||FREQUENCY:1||SOLIDSTATE LASERS:1||Linearly polarized:1||THERMIONIC EMISSION:1||PULSE AMPLIFICATION SYSTEM:1||BIB3O6:1||NM:1||NONCOVALENT INTERACTIONS:1||CRYSTALLINE:1||INTENSITY:1||JETS:1||COHERENT:1||LINE:1||ANGULARDISTRIBUTION:1||SILVER IONS:1||magnetic anisotropy:1||DEVICES:1||Auger transitions:1||CosterKronig transitions:1||EFFICIENT:1||ELECTRONIMPACT IONIZATION:1||ULTRASHORTPULSE:1||Nanowire:1||Heterostructure:1||soft Xray reflectivity:1||PLASMA ACCELERATOR:1||ZINCOXIDE NANOWIRES:1||CHEMICALVAPORDEPOSITION:1||Electron acceleration:1||Ionization of gases:1||Delay dependent:1||MULTIPHOTON IONIZATION:1||FRAGMENTATION:1||GASJET:1||ultrafast nonlinear optics:1||CYCLE PULSES:1||KHZ:1||chemical vapor deposition:1||ferromagnetism:1||ABSORPTION:1||TERAHERTZ RADIATION:1||SCIENCE:1||FIELDS:1||ELECTRONS:1||nanomultilayer structures:1||YIELDS:1||AUGER:1||10HZ REPETITION RATE:1||MULTITERAWATT:1||SPECTROGRAPH:1||HIGHHARMONICGENERATION:1||spectroscopy:1||level population:1||PARTICLEACCELERATION:1||OPTICAL FREQUENCYMEASUREMENT:1||NANOWALLS:1||ROOMTEMPERATURE:1||AVERAGE OUTPUT POWER:1||GROUPVELOCITYMISMATCH:1||Impact ionization:1||Dynamics:1||Lasers:1||Collisional process:1||ABOVETHRESHOLD IONIZATION:1||MAINGROUP THERMOCHEMISTRY:1||dilute magnetic semiconductors:1||GACRN:1||SIZE:1||ATTOSECOND:1||Ar cluster:1||Xray astrophysics:1||photoionization:1||irons:1||normal incidence pulsed laser deposition:1||SHELLS:1||Silicon Oxide:1||gaspuff Zpinch:1||Xray:1||soft Xray reflectors:1||ESCAPE:1||ZN2SIO4:1||SILICA:1||Time delay:1||Collisional plasmas:1||MASSSPECTROMETRY:1||NUCLEARFUSION:1||PARAMETRIC AMPLIFICATION:1||LYING ELECTRONIC STATES:1||ADJUSTABLEPARAMETERS:1||MAGNETICPROPERTIES:1||LIQUIDPHASE EPITAXY:1||CEP laser:1||REGION:1||Plasma waveguide:1||AMBIENT GAS:1||DEPOSITION:1||HARMONICGENERATION:1||ENHANCEMENT:1||imaging spectrometer:1||Abel inversion:1||Water window:1||Liquid nitrogen jet:1||CHARGEEXCHANGE:1||NOBEL LECTURE:1||VARISTOR:1||EPITAXY:1||THINDISK LASER:1||HIGHREPETITIONRATE:1||Atom lasers:1||Electronimpact excitation:1||High order harmonics:1||ultrafast technology:1||PEAK POWER:1||CHARGED ALUMINUM CLUSTERS:1||GaN:1||THIN:1||Electron beam:1||INTENSE:1||Hard Xray pulse generation:1||NONLINEAR THOMSON SCATTERING:1||MULTILAYER:1||UVvisible spectrometer:1||ATOMS:1||innershell transitions:1||CORRECTED CONCAVE GRATINGS:1||DISCHARGE:1||LASERPLASMA:1||thin film:1||reflectivity:1||opacity:1||gain:1||smallangle Xray scattering:1||SOFTXRAY:1||ZINCOXIDE:1||CYGNUSX3:1||Betatron oscillation:1||ACCELERATOR:1||STRAINEDLAYER SUPERLATTICES:1||OPTICAL PARAMETRIC AMPLIFICATION:1||PASSIVE MODELOCKING:1||Collision dynamics:1||MUM:1||EXACTEXCHANGE:1||BASISSET:1||APPROXIMATION:1||OXYNITRIDES:1||Beam energy modulation:1||polarization spectroscopy:1||REORIENTATION TRANSITION:1||DEPENDENCE:1||sulfurs:1||BUILDINGBLOCKS:1||RATES:1||OPTICAL PULSES:1||toroidal mirror:1||XRAY LASER:1||CALCIUM:1||radially polarized laser:1||GRAINBOUNDARIES:1||VAPORDEPOSITION:1||Xray generation:1||MAGNETIZATION:1||Electric excitation:1||Laserinduced gas plasmas:1||Qualitative analysis:1||SCHEME:1||RADIATION:10||PULSES:8||PHOTOLUMINESCENCE:7||LASER:7||GENERATION:6||NANORODS:6||GROWTH:6||NANOWIRES:5||IMPLANTED GAN:5||SPECTROSCOPY:5||THINFILMS:4||DYNAMICS:4||SILICON:4||EXTREMEULTRAVIOLET:4||AMPLIFICATION:4||PRESSURE:4||PHASE:4||OPTICALPROPERTIES:4||SYSTEM:4||EMISSION:4||FEL:3||N2O:3||FILMS:3||OPTICS:3||SPECTRA:3||FIELD:3||MIRRORS:3||ARRAYS:3||CLUSTERS:3||SIO2:3||IONIZATION:3||VACUUM:3||SCATTERING:3||IONS:2||LUMINESCENCE PROPERTIES:2||ANISOTROPY:2||BEAMS:2||DIFFRACTION:2||DISPERSION:2||chemical vapor deposition (CVD):2||ELECTRONICSTRUCTURE:2||MOSFETS:2||SI3N4:2||DENSITY:2||LIGHT:2||PLASMAS:2||MATTER:2||nanocomposites:2||RAMANSCATTERING:2||NANOPARTICLES:2||OXIDE:2||AMPLIFIED SPONTANEOUS EMISSION:2||NM WAVELENGTH:2||GAIN:2||CARBON NANOTUBES:2||CROSSSECTIONS:2||LIGHTEMITTINGDIODES:2||PULSE:2||CARBON PLASMA:2||TISAPPHIRE LASER:2||Raman scattering:2||ROUTE:2||multilayer:2||CATHODOLUMINESCENCE:2||highresolution transmission electronic microscope (HRTEM):2||DIFFERENCEFREQUENCYGENERATION:2||CRYSTAL:2||laserproduced plasma:2||NANOCABLES:2||photoluminescence:2||MAGNETIC ALLOY SEMICONDUCTORS:2||MOLECULARBEAM EPITAXY:2||EARTHDOPED GAN:2||LASER FIELDS:2||CHIRPEDPULSEAMPLIFICATION:2||ALN:2||GAUSSIANBEAM:2||ASSISTED CATALYTIC GROWTH:2||BLUE:2||NANOSTRUCTURES:2||MAGNETOELECTRONICS:2||MICROSCOPY:2||ELECTROLUMINESCENCE:2||LASERPULSES:2||GaN nanowires:2||GALLIUM NITRIDE NANOWIRES:2||GAMNN:2||NANOTUBES:2||PHYSICS:2||Femtosecond laser:2||parametric oscillators and amplifiers:1||ultrafast lasers:1||VALENCE:1||nanowires:1||DILUTED MAGNETIC SEMICONDUCTOR:1||LUMINESCENCE:1||Density modulation:1||Energy modulation:1||Current enhanced SASE free electron laser:1||Undulator radiation:1||FREEELECTRON LASERS:1||ULTRATHIN FERROMAGNETICFILMS:1||OXIDEFILMS:1||ABLATION:1||COMPONENT:1||METAL:1||innershell excited states:1||Nelike ions:1||TRANSITIONS:1||XUV spectrometer:1||DIAGNOSTICS:1||Xray scattering:1||MO/SI:1||pulsed laser deposition:1||KEV IMPACT ENERGIES:1||vacuum electron acceleration:1||HIGHINTENSITY LASER:1||JUNCTIONS:1||LOWTEMPERATURE GROWTH:1||nanocrystalline materials:1||MOLECULAR PHOTOIONIZATION:1||LOCALIZATION:1||DEUTERIUM CLUSTERS:1||EXPLOSIONS:1||REGENERATIVE AMPLIFIERS:1||RAREGASES:1||THz radiation:1||FREEELECTRON LASER:1||REALTIME OBSERVATION:1||TARGET:1||photoionized plasmas:1||fs Xray laser:1||emission profile:1||HIGHORDER HARMONICS:1||Xray laser:1||atomic transition:1||EXCITATION:1||LASERS:1||PERFORMANCE:1||RELATIVISTIC ELECTRONS:1||BI2O3DOPED ZNO:1||INNERSHELL IONIZATION:1||Laser wakefield:1||FREQUENCY:1||SOLIDSTATE LASERS:1||Linearly polarized:1||THERMIONIC EMISSION:1||PULSE AMPLIFICATION SYSTEM:1||BIB3O6:1||NM:1||NONCOVALENT INTERACTIONS:1||CRYSTALLINE:1||INTENSITY:1||JETS:1||COHERENT:1||LINE:1||ANGULARDISTRIBUTION:1||SILVER IONS:1||magnetic anisotropy:1||DEVICES:1||Auger transitions:1||CosterKronig transitions:1||EFFICIENT:1||ELECTRONIMPACT IONIZATION:1||ULTRASHORTPULSE:1||Nanowire:1||Heterostructure:1||soft Xray reflectivity:1||PLASMA ACCELERATOR:1||ZINCOXIDE NANOWIRES:1||CHEMICALVAPORDEPOSITION:1||Electron acceleration:1||Ionization of gases:1||Delay dependent:1||MULTIPHOTON IONIZATION:1||FRAGMENTATION:1||GASJET:1||ultrafast nonlinear optics:1||CYCLE PULSES:1||KHZ:1||chemical vapor deposition:1||ferromagnetism:1||ABSORPTION:1||TERAHERTZ RADIATION:1||SCIENCE:1||FIELDS:1||ELECTRONS:1||nanomultilayer structures:1||YIELDS:1||AUGER:1||10HZ REPETITION RATE:1||MULTITERAWATT:1||SPECTROGRAPH:1||HIGHHARMONICGENERATION:1||spectroscopy:1||level population:1||PARTICLEACCELERATION:1||OPTICAL FREQUENCYMEASUREMENT:1||NANOWALLS:1||ROOMTEMPERATURE:1||AVERAGE OUTPUT POWER:1||GROUPVELOCITYMISMATCH:1||Impact ionization:1||Dynamics:1||Lasers:1||Collisional process:1||ABOVETHRESHOLD IONIZATION:1||MAINGROUP THERMOCHEMISTRY:1||dilute magnetic semiconductors:1||GACRN:1||SIZE:1||ATTOSECOND:1||Ar cluster:1||Xray astrophysics:1||photoionization:1||irons:1||normal incidence pulsed laser deposition:1||SHELLS:1||Silicon Oxide:1||gaspuff Zpinch:1||Xray:1||soft Xray reflectors:1||ESCAPE:1||ZN2SIO4:1||SILICA:1||Time delay:1||Collisional plasmas:1||MASSSPECTROMETRY:1||NUCLEARFUSION:1||PARAMETRIC AMPLIFICATION:1||LYING ELECTRONIC STATES:1||ADJUSTABLEPARAMETERS:1||MAGNETICPROPERTIES:1||LIQUIDPHASE EPITAXY:1||CEP laser:1||REGION:1||Plasma waveguide:1||AMBIENT GAS:1||DEPOSITION:1||HARMONICGENERATION:1||ENHANCEMENT:1||imaging spectrometer:1||Abel inversion:1||Water window:1||Liquid nitrogen jet:1||CHARGEEXCHANGE:1||NOBEL LECTURE:1||VARISTOR:1||EPITAXY:1||THINDISK LASER:1||HIGHREPETITIONRATE:1||Atom lasers:1||Electronimpact excitation:1||High order harmonics:1||ultrafast technology:1||PEAK POWER:1||CHARGED ALUMINUM CLUSTERS:1||GaN:1||THIN:1||Electron beam:1||INTENSE:1||Hard Xray pulse generation:1||NONLINEAR THOMSON SCATTERING:1||MULTILAYER:1||UVvisible spectrometer:1||ATOMS:1||innershell transitions:1||CORRECTED CONCAVE GRATINGS:1||DISCHARGE:1||LASERPLASMA:1||thin film:1||reflectivity:1||opacity:1||gain:1||smallangle Xray scattering:1||SOFTXRAY:1||ZINCOXIDE:1||CYGNUSX3:1||Betatron oscillation:1||ACCELERATOR:1||STRAINEDLAYER SUPERLATTICES:1||OPTICAL PARAMETRIC AMPLIFICATION:1||PASSIVE MODELOCKING:1||Collision dynamics:1||MUM:1||EXACTEXCHANGE:1||BASISSET:1||APPROXIMATION:1||OXYNITRIDES:1||Beam energy modulation:1||polarization spectroscopy:1||REORIENTATION TRANSITION:1||DEPENDENCE:1||sulfurs:1||BUILDINGBLOCKS:1||RATES:1||OPTICAL PULSES:1||toroidal mirror:1||XRAY LASER:1||CALCIUM:1||radially polarized laser:1||GRAINBOUNDARIES:1||VAPORDEPOSITION:1||Xray generation:1||MAGNETIZATION:1||Electric excitation:1||Laserinduced gas plasmas:1||Qualitative analysis:1||SCHEME:1||RADIATION:10||PULSES:8||PHOTOLUMINESCENCE:7||LASER:7||GENERATION:6||NANORODS:6||GROWTH:6||NANOWIRES:5||IMPLANTED 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SEMICONDUCTORS:2||MOLECULARBEAM EPITAXY:2||EARTHDOPED GAN:2||LASER FIELDS:2||CHIRPEDPULSEAMPLIFICATION:2||ALN:2||GAUSSIANBEAM:2||ASSISTED CATALYTIC GROWTH:2||BLUE:2||NANOSTRUCTURES:2||MAGNETOELECTRONICS:2||MICROSCOPY:2||ELECTROLUMINESCENCE:2||LASERPULSES:2||GaN nanowires:2||GALLIUM NITRIDE NANOWIRES:2||GAMNN:2||NANOTUBES:2||PHYSICS:2||Femtosecond laser:2||parametric oscillators and amplifiers:1||ultrafast lasers:1||VALENCE:1||nanowires:1||DILUTED MAGNETIC SEMICONDUCTOR:1||LUMINESCENCE:1||Density modulation:1||Energy modulation:1||Current enhanced SASE free electron laser:1||Undulator radiation:1||FREEELECTRON LASERS:1||ULTRATHIN FERROMAGNETICFILMS:1||OXIDEFILMS:1||ABLATION:1||COMPONENT:1||METAL:1||innershell excited states:1||Nelike ions:1||TRANSITIONS:1||XUV spectrometer:1||DIAGNOSTICS:1||Xray scattering:1||MO/SI:1||pulsed laser deposition:1||KEV IMPACT ENERGIES:1||vacuum electron acceleration:1||HIGHINTENSITY LASER:1||JUNCTIONS:1||LOWTEMPERATURE GROWTH:1||nanocrystalline materials:1||MOLECULAR PHOTOIONIZATION:1||LOCALIZATION:1||DEUTERIUM CLUSTERS:1||EXPLOSIONS:1||REGENERATIVE AMPLIFIERS:1||RAREGASES:1||THz radiation:1||FREEELECTRON LASER:1||REALTIME OBSERVATION:1||TARGET:1||photoionized plasmas:1||fs Xray laser:1||emission profile:1||HIGHORDER HARMONICS:1||Xray laser:1||atomic transition:1||EXCITATION:1||LASERS:1||PERFORMANCE:1||RELATIVISTIC ELECTRONS:1||BI2O3DOPED ZNO:1||INNERSHELL IONIZATION:1||Laser wakefield:1||FREQUENCY:1||SOLIDSTATE LASERS:1||Linearly polarized:1||THERMIONIC EMISSION:1||PULSE AMPLIFICATION SYSTEM:1||BIB3O6:1||NM:1||NONCOVALENT INTERACTIONS:1||CRYSTALLINE:1||INTENSITY:1||JETS:1||COHERENT:1||LINE:1||ANGULARDISTRIBUTION:1||SILVER IONS:1||magnetic anisotropy:1||DEVICES:1||Auger transitions:1||CosterKronig transitions:1||EFFICIENT:1||ELECTRONIMPACT IONIZATION:1||ULTRASHORTPULSE:1||Nanowire:1||Heterostructure:1||soft Xray reflectivity:1||PLASMA ACCELERATOR:1||ZINCOXIDE NANOWIRES:1||CHEMICALVAPORDEPOSITION:1||Electron acceleration:1||Ionization of gases:1||Delay dependent:1||MULTIPHOTON IONIZATION:1||FRAGMENTATION:1||GASJET:1||ultrafast nonlinear optics:1||CYCLE PULSES:1||KHZ:1||chemical vapor deposition:1||ferromagnetism:1||ABSORPTION:1||TERAHERTZ RADIATION:1||SCIENCE:1||FIELDS:1||ELECTRONS:1||nanomultilayer structures:1||YIELDS:1||AUGER:1||10HZ REPETITION RATE:1||MULTITERAWATT:1||SPECTROGRAPH:1||HIGHHARMONICGENERATION:1||spectroscopy:1||level population:1||PARTICLEACCELERATION:1||OPTICAL FREQUENCYMEASUREMENT:1||NANOWALLS:1||ROOMTEMPERATURE:1||AVERAGE OUTPUT POWER:1||GROUPVELOCITYMISMATCH:1||Impact ionization:1||Dynamics:1||Lasers:1||Collisional process:1||ABOVETHRESHOLD IONIZATION:1||MAINGROUP THERMOCHEMISTRY:1||dilute magnetic semiconductors:1||GACRN:1||SIZE:1||ATTOSECOND:1||Ar cluster:1||Xray astrophysics:1||photoionization:1||irons:1||normal incidence pulsed laser deposition:1||SHELLS:1||Silicon Oxide:1||gaspuff Zpinch:1||Xray:1||soft Xray reflectors:1||ESCAPE:1||ZN2SIO4:1||SILICA:1||Time 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materials:1||MOLECULAR PHOTOIONIZATION:1||LOCALIZATION:1||DEUTERIUM CLUSTERS:1||EXPLOSIONS:1||REGENERATIVE AMPLIFIERS:1||RAREGASES:1||THz radiation:1||FREEELECTRON LASER:1||REALTIME OBSERVATION:1||TARGET:1||photoionized plasmas:1||fs Xray laser:1||emission profile:1||HIGHORDER HARMONICS:1||Xray laser:1||atomic transition:1||EXCITATION:1||LASERS:1||PERFORMANCE:1||RELATIVISTIC ELECTRONS:1||BI2O3DOPED ZNO:1||INNERSHELL IONIZATION:1||Laser wakefield:1||FREQUENCY:1||SOLIDSTATE LASERS:1||Linearly polarized:1||THERMIONIC EMISSION:1||PULSE AMPLIFICATION SYSTEM:1||BIB3O6:1||NM:1||NONCOVALENT INTERACTIONS:1||CRYSTALLINE:1||INTENSITY:1||JETS:1||COHERENT:1||LINE:1||ANGULARDISTRIBUTION:1||SILVER IONS:1||magnetic anisotropy:1||DEVICES:1||Auger transitions:1||CosterKronig transitions:1||EFFICIENT:1||ELECTRONIMPACT IONIZATION:1||ULTRASHORTPULSE:1||Nanowire:1||Heterostructure:1||soft Xray reflectivity:1||PLASMA ACCELERATOR:1||ZINCOXIDE NANOWIRES:1||CHEMICALVAPORDEPOSITION:1||Electron acceleration:1||Ionization of gases:1||Delay dependent:1||MULTIPHOTON IONIZATION:1||FRAGMENTATION:1||GASJET:1||ultrafast nonlinear optics:1||CYCLE PULSES:1||KHZ:1||chemical vapor deposition:1||ferromagnetism:1||ABSORPTION:1||TERAHERTZ RADIATION:1||SCIENCE:1||FIELDS:1||ELECTRONS:1||nanomultilayer structures:1||YIELDS:1||AUGER:1||10HZ REPETITION RATE:1||MULTITERAWATT:1||SPECTROGRAPH:1||HIGHHARMONICGENERATION:1||spectroscopy:1||level population:1||PARTICLEACCELERATION:1||OPTICAL FREQUENCYMEASUREMENT:1||NANOWALLS:1||ROOMTEMPERATURE:1||AVERAGE OUTPUT POWER:1||GROUPVELOCITYMISMATCH:1||Impact ionization:1||Dynamics:1||Lasers:1||Collisional process:1||ABOVETHRESHOLD IONIZATION:1||MAINGROUP THERMOCHEMISTRY:1||dilute magnetic semiconductors:1||GACRN:1||SIZE:1||ATTOSECOND:1||Ar cluster:1||Xray astrophysics:1||photoionization:1||irons:1||normal incidence pulsed laser deposition:1||SHELLS:1||Silicon Oxide:1||gaspuff Zpinch:1||Xray:1||soft Xray reflectors:1||ESCAPE:1||ZN2SIO4:1||SILICA:1||Time delay:1||Collisional plasmas:1||MASSSPECTROMETRY:1||NUCLEARFUSION:1||PARAMETRIC AMPLIFICATION:1||LYING ELECTRONIC STATES:1||ADJUSTABLEPARAMETERS:1||MAGNETICPROPERTIES:1||LIQUIDPHASE EPITAXY:1||CEP laser:1||REGION:1||Plasma waveguide:1||AMBIENT GAS:1||DEPOSITION:1||HARMONICGENERATION:1||ENHANCEMENT:1||imaging spectrometer:1||Abel inversion:1||Water window:1||Liquid nitrogen jet:1||CHARGEEXCHANGE:1||NOBEL LECTURE:1||VARISTOR:1||EPITAXY:1||THINDISK LASER:1||HIGHREPETITIONRATE:1||Atom lasers:1||Electronimpact excitation:1||High order harmonics:1||ultrafast technology:1||PEAK POWER:1||CHARGED ALUMINUM CLUSTERS:1||GaN:1||THIN:1||Electron beam:1||INTENSE:1||Hard Xray pulse generation:1||NONLINEAR THOMSON SCATTERING:1||MULTILAYER:1||UVvisible spectrometer:1||ATOMS:1||innershell transitions:1||CORRECTED CONCAVE GRATINGS:1||DISCHARGE:1||LASERPLASMA:1||thin film:1||reflectivity:1||opacity:1||gain:1||smallangle Xray scattering:1||SOFTXRAY:1||ZINCOXIDE:1||CYGNUSX3:1||Betatron oscillation:1||ACCELERATOR:1||STRAINEDLAYER SUPERLATTICES:1||OPTICAL PARAMETRIC AMPLIFICATION:1||PASSIVE MODELOCKING:1||Collision dynamics:1||MUM:1||EXACTEXCHANGE:1||BASISSET:1||APPROXIMATION:1||OXYNITRIDES:1||Beam energy modulation:1||polarization spectroscopy:1||REORIENTATION TRANSITION:1||DEPENDENCE:1||sulfurs:1||BUILDINGBLOCKS:1||RATES:1||OPTICAL PULSES:1||toroidal mirror:1||XRAY LASER:1||CALCIUM:1||radially polarized laser:1||GRAINBOUNDARIES:1||VAPORDEPOSITION:1||Xray generation:1||MAGNETIZATION:1||Electric excitation:1||Laserinduced gas plasmas:1||Qualitative analysis:1||SCHEME:1||RADIATION:10||PULSES:8||PHOTOLUMINESCENCE:7||LASER:7||GENERATION:6||NANORODS:6||GROWTH:6||NANOWIRES:5||IMPLANTED GAN:5||SPECTROSCOPY:5||THINFILMS:4||DYNAMICS:4||SILICON:4||EXTREMEULTRAVIOLET:4||AMPLIFICATION:4||PRESSURE:4||PHASE:4||OPTICALPROPERTIES:4||SYSTEM:4||EMISSION:4||FEL:3||N2O:3||FILMS:3||OPTICS:3||SPECTRA:3||FIELD:3||MIRRORS:3||ARRAYS:3||CLUSTERS:3||SIO2:3||IONIZATION:3||VACUUM:3||SCATTERING:3||IONS:2||LUMINESCENCE PROPERTIES:2||ANISOTROPY:2||BEAMS:2||DIFFRACTION:2||DISPERSION:2||chemical vapor deposition (CVD):2||ELECTRONICSTRUCTURE:2||MOSFETS:2||SI3N4:2||DENSITY:2||LIGHT:2||PLASMAS:2||MATTER:2||nanocomposites:2||RAMANSCATTERING:2||NANOPARTICLES:2||OXIDE:2||AMPLIFIED SPONTANEOUS EMISSION:2||NM WAVELENGTH:2||GAIN:2||CARBON NANOTUBES:2||CROSSSECTIONS:2||LIGHTEMITTINGDIODES:2||PULSE:2||CARBON PLASMA:2||TISAPPHIRE LASER:2||Raman scattering:2||ROUTE:2||multilayer:2||CATHODOLUMINESCENCE:2||highresolution transmission electronic microscope (HRTEM):2||DIFFERENCEFREQUENCYGENERATION:2||CRYSTAL:2||laserproduced plasma:2||NANOCABLES:2||photoluminescence:2||MAGNETIC ALLOY SEMICONDUCTORS:2||MOLECULARBEAM EPITAXY:2||EARTHDOPED GAN:2||LASER FIELDS:2||CHIRPEDPULSEAMPLIFICATION:2||ALN:2||GAUSSIANBEAM:2||ASSISTED CATALYTIC GROWTH:2||BLUE:2||NANOSTRUCTURES:2||MAGNETOELECTRONICS:2||MICROSCOPY:2||ELECTROLUMINESCENCE:2||LASERPULSES:2||GaN nanowires:2||GALLIUM NITRIDE NANOWIRES:2||GAMNN:2||NANOTUBES:2||PHYSICS:2||Femtosecond laser:2||parametric oscillators and amplifiers:1||ultrafast lasers:1||VALENCE:1||nanowires:1||DILUTED MAGNETIC SEMICONDUCTOR:1||LUMINESCENCE:1||Density modulation:1||Energy modulation:1||Current enhanced SASE free electron laser:1||Undulator radiation:1||FREEELECTRON LASERS:1||ULTRATHIN FERROMAGNETICFILMS:1||OXIDEFILMS:1||ABLATION:1||COMPONENT:1||METAL:1||innershell excited states:1||Nelike ions:1||TRANSITIONS:1||XUV spectrometer:1||DIAGNOSTICS:1||Xray scattering:1||MO/SI:1||pulsed laser deposition:1||KEV IMPACT ENERGIES:1||vacuum electron acceleration:1||HIGHINTENSITY LASER:1||JUNCTIONS:1||LOWTEMPERATURE GROWTH:1||nanocrystalline materials:1||MOLECULAR PHOTOIONIZATION:1||LOCALIZATION:1||DEUTERIUM CLUSTERS:1||EXPLOSIONS:1||REGENERATIVE AMPLIFIERS:1||RAREGASES:1||THz radiation:1||FREEELECTRON LASER:1||REALTIME OBSERVATION:1||TARGET:1||photoionized plasmas:1||fs Xray laser:1||emission profile:1||HIGHORDER HARMONICS:1||Xray laser:1||atomic transition:1||EXCITATION:1||LASERS:1||PERFORMANCE:1||RELATIVISTIC ELECTRONS:1||BI2O3DOPED ZNO:1||INNERSHELL IONIZATION:1||Laser wakefield:1||FREQUENCY:1||SOLIDSTATE LASERS:1||Linearly polarized:1||THERMIONIC EMISSION:1||PULSE AMPLIFICATION SYSTEM:1||BIB3O6:1||NM:1||NONCOVALENT INTERACTIONS:1||CRYSTALLINE:1||INTENSITY:1||JETS:1||COHERENT:1||LINE:1||ANGULARDISTRIBUTION:1||SILVER IONS:1||magnetic anisotropy:1||DEVICES:1||Auger transitions:1||CosterKronig transitions:1||EFFICIENT:1||ELECTRONIMPACT IONIZATION:1||ULTRASHORTPULSE:1||Nanowire:1||Heterostructure:1||soft Xray reflectivity:1||PLASMA ACCELERATOR:1||ZINCOXIDE NANOWIRES:1||CHEMICALVAPORDEPOSITION:1||Electron acceleration:1||Ionization of gases:1||Delay dependent:1||MULTIPHOTON IONIZATION:1||FRAGMENTATION:1||GASJET:1||ultrafast nonlinear optics:1||CYCLE PULSES:1||KHZ:1||chemical vapor deposition:1||ferromagnetism:1||ABSORPTION:1||TERAHERTZ RADIATION:1||SCIENCE:1||FIELDS:1||ELECTRONS:1||nanomultilayer structures:1||YIELDS:1||AUGER:1||10HZ REPETITION RATE:1||MULTITERAWATT:1||SPECTROGRAPH:1||HIGHHARMONICGENERATION:1||spectroscopy:1||level population:1||PARTICLEACCELERATION:1||OPTICAL FREQUENCYMEASUREMENT:1||NANOWALLS:1||ROOMTEMPERATURE:1||AVERAGE OUTPUT POWER:1||GROUPVELOCITYMISMATCH:1||Impact ionization:1||Dynamics:1||Lasers:1||Collisional process:1||ABOVETHRESHOLD IONIZATION:1||MAINGROUP THERMOCHEMISTRY:1||dilute magnetic semiconductors:1||GACRN:1||SIZE:1||ATTOSECOND:1||Ar cluster:1||Xray astrophysics:1||photoionization:1||irons:1||normal incidence pulsed laser deposition:1||SHELLS:1||Silicon Oxide:1||gaspuff Zpinch:1||Xray:1||soft Xray reflectors:1||ESCAPE:1||ZN2SIO4:1||SILICA:1||Time delay:1||Collisional plasmas:1||MASSSPECTROMETRY:1||NUCLEARFUSION:1||PARAMETRIC AMPLIFICATION:1||LYING ELECTRONIC STATES:1||ADJUSTABLEPARAMETERS:1||MAGNETICPROPERTIES:1||LIQUIDPHASE EPITAXY:1||CEP laser:1||REGION:1||Plasma waveguide:1||AMBIENT GAS:1||DEPOSITION:1||HARMONICGENERATION:1||ENHANCEMENT:1||imaging spectrometer:1||Abel inversion:1||Water window:1||Liquid nitrogen jet:1||CHARGEEXCHANGE:1||NOBEL LECTURE:1||VARISTOR:1||EPITAXY:1||THINDISK LASER:1||HIGHREPETITIONRATE:1||Atom lasers:1||Electronimpact excitation:1||High order harmonics:1||ultrafast technology:1||PEAK POWER:1||CHARGED ALUMINUM CLUSTERS:1||GaN:1||THIN:1||Electron beam:1||INTENSE:1||Hard Xray pulse generation:1||NONLINEAR THOMSON SCATTERING:1||MULTILAYER:1||UVvisible spectrometer:1||ATOMS:1||innershell transitions:1||CORRECTED CONCAVE GRATINGS:1||DISCHARGE:1||LASERPLASMA:1||thin film:1||reflectivity:1||opacity:1||gain:1||smallangle Xray scattering:1||SOFTXRAY:1||ZINCOXIDE:1||CYGNUSX3:1||Betatron oscillation:1||ACCELERATOR:1||STRAINEDLAYER SUPERLATTICES:1||OPTICAL PARAMETRIC AMPLIFICATION:1||PASSIVE MODELOCKING:1||Collision dynamics:1||MUM:1||EXACTEXCHANGE:1||BASISSET:1||APPROXIMATION:1||OXYNITRIDES:1||Beam energy modulation:1||polarization spectroscopy:1||REORIENTATION TRANSITION:1||DEPENDENCE:1||sulfurs:1||BUILDINGBLOCKS:1||RATES:1||OPTICAL PULSES:1||toroidal mirror:1||XRAY LASER:1||CALCIUM:1||radially polarized laser:1||GRAINBOUNDARIES:1||VAPORDEPOSITION:1||Xray generation:1||MAGNETIZATION:1||Electric excitation:1||Laserinduced gas plasmas:1||Qualitative analysis:1||SCHEME:1||RADIATION:10||PULSES:8||PHOTOLUMINESCENCE:7||LASER:7||GENERATION:6||NANORODS:6||GROWTH:6||NANOWIRES:5||IMPLANTED 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SEMICONDUCTORS:2||MOLECULARBEAM EPITAXY:2||EARTHDOPED GAN:2||LASER FIELDS:2||CHIRPEDPULSEAMPLIFICATION:2||ALN:2||GAUSSIANBEAM:2||ASSISTED CATALYTIC GROWTH:2||BLUE:2||NANOSTRUCTURES:2||MAGNETOELECTRONICS:2||MICROSCOPY:2||ELECTROLUMINESCENCE:2||LASERPULSES:2||GaN nanowires:2||GALLIUM NITRIDE NANOWIRES:2||GAMNN:2||NANOTUBES:2||PHYSICS:2||Femtosecond laser:2||parametric oscillators and amplifiers:1||ultrafast lasers:1||VALENCE:1||nanowires:1||DILUTED MAGNETIC SEMICONDUCTOR:1||LUMINESCENCE:1||Density modulation:1||Energy modulation:1||Current enhanced SASE free electron laser:1||Undulator radiation:1||FREEELECTRON LASERS:1||ULTRATHIN FERROMAGNETICFILMS:1||OXIDEFILMS:1||ABLATION:1||COMPONENT:1||METAL:1||innershell excited states:1||Nelike ions:1||TRANSITIONS:1||XUV spectrometer:1||DIAGNOSTICS:1||Xray scattering:1||MO/SI:1||pulsed laser deposition:1||KEV IMPACT ENERGIES:1||vacuum electron acceleration:1||HIGHINTENSITY LASER:1||JUNCTIONS:1||LOWTEMPERATURE GROWTH:1||nanocrystalline materials:1||MOLECULAR PHOTOIONIZATION:1||LOCALIZATION:1||DEUTERIUM CLUSTERS:1||EXPLOSIONS:1||REGENERATIVE AMPLIFIERS:1||RAREGASES:1||THz radiation:1||FREEELECTRON LASER:1||REALTIME OBSERVATION:1||TARGET:1||photoionized plasmas:1||fs Xray laser:1||emission profile:1||HIGHORDER HARMONICS:1||Xray laser:1||atomic transition:1||EXCITATION:1||LASERS:1||PERFORMANCE:1||RELATIVISTIC ELECTRONS:1||BI2O3DOPED ZNO:1||INNERSHELL IONIZATION:1||Laser wakefield:1||FREQUENCY:1||SOLIDSTATE LASERS:1||Linearly polarized:1||THERMIONIC EMISSION:1||PULSE AMPLIFICATION SYSTEM:1||BIB3O6:1||NM:1||NONCOVALENT INTERACTIONS:1||CRYSTALLINE:1||INTENSITY:1||JETS:1||COHERENT:1||LINE:1||ANGULARDISTRIBUTION:1||SILVER IONS:1||magnetic anisotropy:1||DEVICES:1||Auger transitions:1||CosterKronig transitions:1||EFFICIENT:1||ELECTRONIMPACT IONIZATION:1||ULTRASHORTPULSE:1||Nanowire:1||Heterostructure:1||soft Xray reflectivity:1||PLASMA ACCELERATOR:1||ZINCOXIDE NANOWIRES:1||CHEMICALVAPORDEPOSITION:1||Electron acceleration:1||Ionization of gases:1||Delay dependent:1||MULTIPHOTON IONIZATION:1||FRAGMENTATION:1||GASJET:1||ultrafast nonlinear optics:1||CYCLE PULSES:1||KHZ:1||chemical vapor deposition:1||ferromagnetism:1||ABSORPTION:1||TERAHERTZ RADIATION:1||SCIENCE:1||FIELDS:1||ELECTRONS:1||nanomultilayer structures:1||YIELDS:1||AUGER:1||10HZ REPETITION RATE:1||MULTITERAWATT:1||SPECTROGRAPH:1||HIGHHARMONICGENERATION:1||spectroscopy:1||level population:1||PARTICLEACCELERATION:1||OPTICAL FREQUENCYMEASUREMENT:1||NANOWALLS:1||ROOMTEMPERATURE:1||AVERAGE OUTPUT POWER:1||GROUPVELOCITYMISMATCH:1||Impact ionization:1||Dynamics:1||Lasers:1||Collisional process:1||ABOVETHRESHOLD IONIZATION:1||MAINGROUP THERMOCHEMISTRY:1||dilute magnetic semiconductors:1||GACRN:1||SIZE:1||ATTOSECOND:1||Ar cluster:1||Xray astrophysics:1||photoionization:1||irons:1||normal incidence pulsed laser deposition:1||SHELLS:1||Silicon Oxide:1||gaspuff Zpinch:1||Xray:1||soft Xray reflectors:1||ESCAPE:1||ZN2SIO4:1||SILICA:1||Time 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materials:1||MOLECULAR PHOTOIONIZATION:1||LOCALIZATION:1||DEUTERIUM CLUSTERS:1||EXPLOSIONS:1||REGENERATIVE AMPLIFIERS:1||RAREGASES:1||THz radiation:1||FREEELECTRON LASER:1||REALTIME OBSERVATION:1||TARGET:1||photoionized plasmas:1||fs Xray laser:1||emission profile:1||HIGHORDER HARMONICS:1||Xray laser:1||atomic transition:1||EXCITATION:1||LASERS:1||PERFORMANCE:1||RELATIVISTIC ELECTRONS:1||BI2O3DOPED ZNO:1||INNERSHELL IONIZATION:1||Laser wakefield:1||FREQUENCY:1||SOLIDSTATE LASERS:1||Linearly polarized:1||THERMIONIC EMISSION:1||PULSE AMPLIFICATION SYSTEM:1||BIB3O6:1||NM:1||NONCOVALENT INTERACTIONS:1||CRYSTALLINE:1||INTENSITY:1||JETS:1||COHERENT:1||LINE:1||ANGULARDISTRIBUTION:1||SILVER IONS:1||magnetic anisotropy:1||DEVICES:1||Auger transitions:1||CosterKronig transitions:1||EFFICIENT:1||ELECTRONIMPACT IONIZATION:1||ULTRASHORTPULSE:1||Nanowire:1||Heterostructure:1||soft Xray reflectivity:1||PLASMA ACCELERATOR:1||ZINCOXIDE NANOWIRES:1||CHEMICALVAPORDEPOSITION:1||Electron acceleration:1||Ionization of gases:1||Delay dependent:1||MULTIPHOTON IONIZATION:1||FRAGMENTATION:1||GASJET:1||ultrafast nonlinear optics:1||CYCLE PULSES:1||KHZ:1||chemical vapor deposition:1||ferromagnetism:1||ABSORPTION:1||TERAHERTZ RADIATION:1||SCIENCE:1||FIELDS:1||ELECTRONS:1||nanomultilayer structures:1||YIELDS:1||AUGER:1||10HZ REPETITION RATE:1||MULTITERAWATT:1||SPECTROGRAPH:1||HIGHHARMONICGENERATION:1||spectroscopy:1||level population:1||PARTICLEACCELERATION:1||OPTICAL FREQUENCYMEASUREMENT:1||NANOWALLS:1||ROOMTEMPERATURE:1||AVERAGE OUTPUT POWER:1||GROUPVELOCITYMISMATCH:1||Impact ionization:1||Dynamics:1||Lasers:1||Collisional process:1||ABOVETHRESHOLD IONIZATION:1||MAINGROUP THERMOCHEMISTRY:1||dilute magnetic semiconductors:1||GACRN:1||SIZE:1||ATTOSECOND:1||Ar cluster:1||Xray astrophysics:1||photoionization:1||irons:1||normal incidence pulsed laser deposition:1||SHELLS:1||Silicon Oxide:1||gaspuff Zpinch:1||Xray:1||soft Xray reflectors:1||ESCAPE:1||ZN2SIO4:1||SILICA:1||Time delay:1||Collisional plasmas:1||MASSSPECTROMETRY:1||NUCLEARFUSION:1||PARAMETRIC AMPLIFICATION:1||LYING ELECTRONIC STATES:1||ADJUSTABLEPARAMETERS:1||MAGNETICPROPERTIES:1||LIQUIDPHASE EPITAXY:1||CEP laser:1||REGION:1||Plasma waveguide:1||AMBIENT GAS:1||DEPOSITION:1||HARMONICGENERATION:1||ENHANCEMENT:1||imaging spectrometer:1||Abel inversion:1||Water window:1||Liquid nitrogen jet:1||CHARGEEXCHANGE:1||NOBEL LECTURE:1||VARISTOR:1||EPITAXY:1||THINDISK LASER:1||HIGHREPETITIONRATE:1||Atom lasers:1||Electronimpact excitation:1||High order harmonics:1||ultrafast technology:1||PEAK POWER:1||CHARGED ALUMINUM CLUSTERS:1||GaN:1||THIN:1||Electron beam:1||INTENSE:1||Hard Xray pulse generation:1||NONLINEAR THOMSON SCATTERING:1||MULTILAYER:1||UVvisible spectrometer:1||ATOMS:1||innershell transitions:1||CORRECTED CONCAVE GRATINGS:1||DISCHARGE:1||LASERPLASMA:1||thin film:1||reflectivity:1||opacity:1||gain:1||smallangle Xray scattering:1||SOFTXRAY:1||ZINCOXIDE:1||CYGNUSX3:1||Betatron oscillation:1||ACCELERATOR:1||STRAINEDLAYER SUPERLATTICES:1||OPTICAL PARAMETRIC AMPLIFICATION:1||PASSIVE MODELOCKING:1||Collision dynamics:1||MUM:1||EXACTEXCHANGE:1||BASISSET:1||APPROXIMATION:1||OXYNITRIDES:1||Beam energy modulation:1||polarization spectroscopy:1||REORIENTATION TRANSITION:1||DEPENDENCE:1||sulfurs:1||BUILDINGBLOCKS:1||RATES:1||OPTICAL PULSES:1||toroidal mirror:1||XRAY LASER:1||CALCIUM:1||radially polarized laser:1||GRAINBOUNDARIES:1||VAPORDEPOSITION:1||Xray generation:1||MAGNETIZATION:1||Electric excitation:1||Laserinduced gas plasmas:1||Qualitative analysis:1||SCHEME:1||RADIATION:10||PULSES:8||PHOTOLUMINESCENCE:7||LASER:7||GENERATION:6||NANORODS:6||GROWTH:6||NANOWIRES:5||IMPLANTED GAN:5||SPECTROSCOPY:5||THINFILMS:4||DYNAMICS:4||SILICON:4||EXTREMEULTRAVIOLET:4||AMPLIFICATION:4||PRESSURE:4||PHASE:4||OPTICALPROPERTIES:4||SYSTEM:4||EMISSION:4||FEL:3||N2O:3||FILMS:3||OPTICS:3||SPECTRA:3||FIELD:3||MIRRORS:3||ARRAYS:3||CLUSTERS:3||SIO2:3||IONIZATION:3||VACUUM:3||SCATTERING:3||IONS:2||LUMINESCENCE PROPERTIES:2||ANISOTROPY:2||BEAMS:2||DIFFRACTION:2||DISPERSION:2||chemical vapor deposition (CVD):2||ELECTRONICSTRUCTURE:2||MOSFETS:2||SI3N4:2||DENSITY:2||LIGHT:2||PLASMAS:2||MATTER:2||nanocomposites:2||RAMANSCATTERING:2||NANOPARTICLES:2||OXIDE:2||AMPLIFIED SPONTANEOUS EMISSION:2||NM WAVELENGTH:2||GAIN:2||CARBON NANOTUBES:2||CROSSSECTIONS:2||LIGHTEMITTINGDIODES:2||PULSE:2||CARBON PLASMA:2||TISAPPHIRE LASER:2||Raman scattering:2||ROUTE:2||multilayer:2||CATHODOLUMINESCENCE:2||highresolution transmission electronic microscope (HRTEM):2||DIFFERENCEFREQUENCYGENERATION:2||CRYSTAL:2||laserproduced plasma:2||NANOCABLES:2||photoluminescence:2||MAGNETIC ALLOY SEMICONDUCTORS:2||MOLECULARBEAM EPITAXY:2||EARTHDOPED GAN:2||LASER FIELDS:2||CHIRPEDPULSEAMPLIFICATION:2||ALN:2||GAUSSIANBEAM:2||ASSISTED CATALYTIC GROWTH:2||BLUE:2||NANOSTRUCTURES:2||MAGNETOELECTRONICS:2||MICROSCOPY:2||ELECTROLUMINESCENCE:2||LASERPULSES:2||GaN nanowires:2||GALLIUM NITRIDE NANOWIRES:2||GAMNN:2||NANOTUBES:2||PHYSICS:2||Femtosecond laser:2||parametric oscillators and amplifiers:1||ultrafast lasers:1||VALENCE:1||nanowires:1||DILUTED MAGNETIC SEMICONDUCTOR:1||LUMINESCENCE:1||Density modulation:1||Energy modulation:1||Current enhanced SASE free electron laser:1||Undulator radiation:1||FREEELECTRON LASERS:1||ULTRATHIN FERROMAGNETICFILMS:1||OXIDEFILMS:1||ABLATION:1||COMPONENT:1||METAL:1||innershell excited states:1||Nelike ions:1||TRANSITIONS:1||XUV spectrometer:1||DIAGNOSTICS:1||Xray scattering:1||MO/SI:1||pulsed laser deposition:1||KEV IMPACT ENERGIES:1||vacuum electron acceleration:1||HIGHINTENSITY LASER:1||JUNCTIONS:1||LOWTEMPERATURE GROWTH:1||nanocrystalline materials:1||MOLECULAR PHOTOIONIZATION:1||LOCALIZATION:1||DEUTERIUM CLUSTERS:1||EXPLOSIONS:1||REGENERATIVE AMPLIFIERS:1||RAREGASES:1||THz radiation:1||FREEELECTRON LASER:1||REALTIME OBSERVATION:1||TARGET:1||photoionized plasmas:1||fs Xray laser:1||emission profile:1||HIGHORDER HARMONICS:1||Xray laser:1||atomic transition:1||EXCITATION:1||LASERS:1||PERFORMANCE:1||RELATIVISTIC ELECTRONS:1||BI2O3DOPED ZNO:1||INNERSHELL IONIZATION:1||Laser wakefield:1||FREQUENCY:1||SOLIDSTATE LASERS:1||Linearly polarized:1||THERMIONIC EMISSION:1||PULSE AMPLIFICATION SYSTEM:1||BIB3O6:1||NM:1||NONCOVALENT INTERACTIONS:1||CRYSTALLINE:1||INTENSITY:1||JETS:1||COHERENT:1||LINE:1||ANGULARDISTRIBUTION:1||SILVER IONS:1||magnetic anisotropy:1||DEVICES:1||Auger transitions:1||CosterKronig transitions:1||EFFICIENT:1||ELECTRONIMPACT IONIZATION:1||ULTRASHORTPULSE:1||Nanowire:1||Heterostructure:1||soft Xray reflectivity:1||PLASMA ACCELERATOR:1||ZINCOXIDE NANOWIRES:1||CHEMICALVAPORDEPOSITION:1||Electron acceleration:1||Ionization of gases:1||Delay dependent:1||MULTIPHOTON IONIZATION:1||FRAGMENTATION:1||GASJET:1||ultrafast nonlinear optics:1||CYCLE PULSES:1||KHZ:1||chemical vapor deposition:1||ferromagnetism:1||ABSORPTION:1||TERAHERTZ RADIATION:1||SCIENCE:1||FIELDS:1||ELECTRONS:1||nanomultilayer structures:1||YIELDS:1||AUGER:1||10HZ REPETITION RATE:1||MULTITERAWATT:1||SPECTROGRAPH:1||HIGHHARMONICGENERATION:1||spectroscopy:1||level population:1||PARTICLEACCELERATION:1||OPTICAL FREQUENCYMEASUREMENT:1||NANOWALLS:1||ROOMTEMPERATURE:1||AVERAGE OUTPUT POWER:1||GROUPVELOCITYMISMATCH:1||Impact ionization:1||Dynamics:1||Lasers:1||Collisional process:1||ABOVETHRESHOLD IONIZATION:1||MAINGROUP THERMOCHEMISTRY:1||dilute magnetic semiconductors:1||GACRN:1||SIZE:1||ATTOSECOND:1||Ar cluster:1||Xray astrophysics:1||photoionization:1||irons:1||normal incidence pulsed laser deposition:1||SHELLS:1||Silicon Oxide:1||gaspuff Zpinch:1||Xray:1||soft Xray reflectors:1||ESCAPE:1||ZN2SIO4:1||SILICA:1||Time delay:1||Collisional plasmas:1||MASSSPECTROMETRY:1||NUCLEARFUSION:1||PARAMETRIC AMPLIFICATION:1||LYING ELECTRONIC STATES:1||ADJUSTABLEPARAMETERS:1||MAGNETICPROPERTIES:1||LIQUIDPHASE EPITAXY:1||CEP laser:1||REGION:1||Plasma waveguide:1||AMBIENT GAS:1||DEPOSITION:1||HARMONICGENERATION:1||ENHANCEMENT:1||imaging spectrometer:1||Abel inversion:1||Water window:1||Liquid nitrogen jet:1||CHARGEEXCHANGE:1||NOBEL LECTURE:1||VARISTOR:1||EPITAXY:1||THINDISK LASER:1||HIGHREPETITIONRATE:1||Atom lasers:1||Electronimpact excitation:1||High order harmonics:1||ultrafast technology:1||PEAK POWER:1||CHARGED ALUMINUM CLUSTERS:1||GaN:1||THIN:1||Electron beam:1||INTENSE:1||Hard Xray pulse generation:1||NONLINEAR THOMSON SCATTERING:1||MULTILAYER:1||UVvisible spectrometer:1||ATOMS:1||innershell transitions:1||CORRECTED CONCAVE GRATINGS:1||DISCHARGE:1||LASERPLASMA:1||thin film:1||reflectivity:1||opacity:1||gain:1||smallangle Xray scattering:1||SOFTXRAY:1||ZINCOXIDE:1||CYGNUSX3:1||Betatron oscillation:1||ACCELERATOR:1||STRAINEDLAYER SUPERLATTICES:1||OPTICAL PARAMETRIC AMPLIFICATION:1||PASSIVE MODELOCKING:1||Collision dynamics:1||MUM:1||EXACTEXCHANGE:1||BASISSET:1||APPROXIMATION:1||OXYNITRIDES:1||Beam energy modulation:1||polarization spectroscopy:1||REORIENTATION TRANSITION:1||DEPENDENCE:1||sulfurs:1||BUILDINGBLOCKS:1||RATES:1||OPTICAL PULSES:1||toroidal mirror:1||XRAY LASER:1||CALCIUM:1||radially polarized laser:1||GRAINBOUNDARIES:1||VAPORDEPOSITION:1||Xray generation:1||MAGNETIZATION:1||Electric excitation:1||Laserinduced gas plasmas:1||Qualitative analysis:1||SCHEME:1||RADIATION:10||PULSES:8||PHOTOLUMINESCENCE:7||LASER:7||GENERATION:6||NANORODS:6||GROWTH:6||NANOWIRES:5||IMPLANTED 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SEMICONDUCTORS:2||MOLECULARBEAM EPITAXY:2||EARTHDOPED GAN:2||LASER FIELDS:2||CHIRPEDPULSEAMPLIFICATION:2||ALN:2||GAUSSIANBEAM:2||ASSISTED CATALYTIC GROWTH:2||BLUE:2||NANOSTRUCTURES:2||MAGNETOELECTRONICS:2||MICROSCOPY:2||ELECTROLUMINESCENCE:2||LASERPULSES:2||GaN nanowires:2||GALLIUM NITRIDE NANOWIRES:2||GAMNN:2||NANOTUBES:2||PHYSICS:2||Femtosecond laser:2||parametric oscillators and amplifiers:1||ultrafast lasers:1||VALENCE:1||nanowires:1||DILUTED MAGNETIC SEMICONDUCTOR:1||LUMINESCENCE:1||Density modulation:1||Energy modulation:1||Current enhanced SASE free electron laser:1||Undulator radiation:1||FREEELECTRON LASERS:1||ULTRATHIN FERROMAGNETICFILMS:1||OXIDEFILMS:1||ABLATION:1||COMPONENT:1||METAL:1||innershell excited states:1||Nelike ions:1||TRANSITIONS:1||XUV spectrometer:1||DIAGNOSTICS:1||Xray scattering:1||MO/SI:1||pulsed laser deposition:1||KEV IMPACT ENERGIES:1||vacuum electron acceleration:1||HIGHINTENSITY LASER:1||JUNCTIONS:1||LOWTEMPERATURE GROWTH:1||nanocrystalline materials:1||MOLECULAR PHOTOIONIZATION:1||LOCALIZATION:1||DEUTERIUM CLUSTERS:1||EXPLOSIONS:1||REGENERATIVE AMPLIFIERS:1||RAREGASES:1||THz radiation:1||FREEELECTRON LASER:1||REALTIME OBSERVATION:1||TARGET:1||photoionized plasmas:1||fs Xray laser:1||emission profile:1||HIGHORDER HARMONICS:1||Xray laser:1||atomic transition:1||EXCITATION:1||LASERS:1||PERFORMANCE:1||RELATIVISTIC ELECTRONS:1||BI2O3DOPED ZNO:1||INNERSHELL IONIZATION:1||Laser wakefield:1||FREQUENCY:1||SOLIDSTATE LASERS:1||Linearly polarized:1||THERMIONIC EMISSION:1||PULSE AMPLIFICATION SYSTEM:1||BIB3O6:1||NM:1||NONCOVALENT INTERACTIONS:1||CRYSTALLINE:1||INTENSITY:1||JETS:1||COHERENT:1||LINE:1||ANGULARDISTRIBUTION:1||SILVER IONS:1||magnetic anisotropy:1||DEVICES:1||Auger transitions:1||CosterKronig transitions:1||EFFICIENT:1||ELECTRONIMPACT IONIZATION:1||ULTRASHORTPULSE:1||Nanowire:1||Heterostructure:1||soft Xray reflectivity:1||PLASMA ACCELERATOR:1||ZINCOXIDE NANOWIRES:1||CHEMICALVAPORDEPOSITION:1||Electron acceleration:1||Ionization of gases:1||Delay dependent:1||MULTIPHOTON IONIZATION:1||FRAGMENTATION:1||GASJET:1||ultrafast nonlinear optics:1||CYCLE PULSES:1||KHZ:1||chemical vapor deposition:1||ferromagnetism:1||ABSORPTION:1||TERAHERTZ RADIATION:1||SCIENCE:1||FIELDS:1||ELECTRONS:1||nanomultilayer structures:1||YIELDS:1||AUGER:1||10HZ REPETITION RATE:1||MULTITERAWATT:1||SPECTROGRAPH:1||HIGHHARMONICGENERATION:1||spectroscopy:1||level population:1||PARTICLEACCELERATION:1||OPTICAL FREQUENCYMEASUREMENT:1||NANOWALLS:1||ROOMTEMPERATURE:1||AVERAGE OUTPUT POWER:1||GROUPVELOCITYMISMATCH:1||Impact ionization:1||Dynamics:1||Lasers:1||Collisional process:1||ABOVETHRESHOLD IONIZATION:1||MAINGROUP THERMOCHEMISTRY:1||dilute magnetic semiconductors:1||GACRN:1||SIZE:1||ATTOSECOND:1||Ar cluster:1||Xray astrophysics:1||photoionization:1||irons:1||normal incidence pulsed laser deposition:1||SHELLS:1||Silicon Oxide:1||gaspuff Zpinch:1||Xray:1||soft Xray reflectors:1||ESCAPE:1||ZN2SIO4:1||SILICA:1||Time 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materials:1||MOLECULAR PHOTOIONIZATION:1||LOCALIZATION:1||DEUTERIUM CLUSTERS:1||EXPLOSIONS:1||REGENERATIVE AMPLIFIERS:1||RAREGASES:1||THz radiation:1||FREEELECTRON LASER:1||REALTIME OBSERVATION:1||TARGET:1||photoionized plasmas:1||fs Xray laser:1||emission profile:1||HIGHORDER HARMONICS:1||Xray laser:1||atomic transition:1||EXCITATION:1||LASERS:1||PERFORMANCE:1||RELATIVISTIC ELECTRONS:1||BI2O3DOPED ZNO:1||INNERSHELL IONIZATION:1||Laser wakefield:1||FREQUENCY:1||SOLIDSTATE LASERS:1||Linearly polarized:1||THERMIONIC EMISSION:1||PULSE AMPLIFICATION SYSTEM:1||BIB3O6:1||NM:1||NONCOVALENT INTERACTIONS:1||CRYSTALLINE:1||INTENSITY:1||JETS:1||COHERENT:1||LINE:1||ANGULARDISTRIBUTION:1||SILVER IONS:1||magnetic anisotropy:1||DEVICES:1||Auger transitions:1||CosterKronig transitions:1||EFFICIENT:1||ELECTRONIMPACT IONIZATION:1||ULTRASHORTPULSE:1||Nanowire:1||Heterostructure:1||soft Xray reflectivity:1||PLASMA ACCELERATOR:1||ZINCOXIDE NANOWIRES:1||CHEMICALVAPORDEPOSITION:1||Electron acceleration:1||Ionization of gases:1||Delay dependent:1||MULTIPHOTON IONIZATION:1||FRAGMENTATION:1||GASJET:1||ultrafast nonlinear optics:1||CYCLE PULSES:1||KHZ:1||chemical vapor deposition:1||ferromagnetism:1||ABSORPTION:1||TERAHERTZ RADIATION:1||SCIENCE:1||FIELDS:1||ELECTRONS:1||nanomultilayer structures:1||YIELDS:1||AUGER:1||10HZ REPETITION RATE:1||MULTITERAWATT:1||SPECTROGRAPH:1||HIGHHARMONICGENERATION:1||spectroscopy:1||level population:1||PARTICLEACCELERATION:1||OPTICAL FREQUENCYMEASUREMENT:1||NANOWALLS:1||ROOMTEMPERATURE:1||AVERAGE OUTPUT POWER:1||GROUPVELOCITYMISMATCH:1||Impact ionization:1||Dynamics:1||Lasers:1||Collisional process:1||ABOVETHRESHOLD IONIZATION:1||MAINGROUP THERMOCHEMISTRY:1||dilute magnetic semiconductors:1||GACRN:1||SIZE:1||ATTOSECOND:1||Ar cluster:1||Xray astrophysics:1||photoionization:1||irons:1||normal incidence pulsed laser deposition:1||SHELLS:1||Silicon Oxide:1||gaspuff Zpinch:1||Xray:1||soft Xray reflectors:1||ESCAPE:1||ZN2SIO4:1||SILICA:1||Time delay:1||Collisional plasmas:1||MASSSPECTROMETRY:1||NUCLEARFUSION:1||PARAMETRIC AMPLIFICATION:1||LYING ELECTRONIC STATES:1||ADJUSTABLEPARAMETERS:1||MAGNETICPROPERTIES:1||LIQUIDPHASE EPITAXY:1||CEP laser:1||REGION:1||Plasma waveguide:1||AMBIENT GAS:1||DEPOSITION:1||HARMONICGENERATION:1||ENHANCEMENT:1||imaging spectrometer:1||Abel inversion:1||Water window:1||Liquid nitrogen jet:1||CHARGEEXCHANGE:1||NOBEL LECTURE:1||VARISTOR:1||EPITAXY:1||THINDISK LASER:1||HIGHREPETITIONRATE:1||Atom lasers:1||Electronimpact excitation:1||High order harmonics:1||ultrafast technology:1||PEAK POWER:1||CHARGED ALUMINUM CLUSTERS:1||GaN:1||THIN:1||Electron beam:1||INTENSE:1||Hard Xray pulse generation:1||NONLINEAR THOMSON SCATTERING:1||MULTILAYER:1||UVvisible spectrometer:1||ATOMS:1||innershell transitions:1||CORRECTED CONCAVE GRATINGS:1||DISCHARGE:1||LASERPLASMA:1||thin film:1||reflectivity:1||opacity:1||gain:1||smallangle Xray scattering:1||SOFTXRAY:1||ZINCOXIDE:1||CYGNUSX3:1||Betatron oscillation:1||ACCELERATOR:1||STRAINEDLAYER SUPERLATTICES:1||OPTICAL PARAMETRIC AMPLIFICATION:1||PASSIVE MODELOCKING:1||Collision dynamics:1||MUM:1||EXACTEXCHANGE:1||BASISSET:1||APPROXIMATION:1||OXYNITRIDES:1||Beam energy modulation:1||polarization spectroscopy:1||REORIENTATION TRANSITION:1||DEPENDENCE:1||sulfurs:1||BUILDINGBLOCKS:1||RATES:1||OPTICAL PULSES:1||toroidal mirror:1||XRAY LASER:1||CALCIUM:1||radially polarized laser:1||GRAINBOUNDARIES:1||VAPORDEPOSITION:1||Xray generation:1||MAGNETIZATION:1||Electric excitation:1||Laserinduced gas plasmas:1||Qualitative analysis:1||SCHEME:1||RADIATION:10||PULSES:8||PHOTOLUMINESCENCE:7||LASER:7||GENERATION:6||NANORODS:6||GROWTH:6||NANOWIRES:5||IMPLANTED GAN:5||SPECTROSCOPY:5||THINFILMS:4||DYNAMICS:4||SILICON:4||EXTREMEULTRAVIOLET:4||AMPLIFICATION:4||PRESSURE:4||PHASE:4||OPTICALPROPERTIES:4||SYSTEM:4||EMISSION:4||FEL:3||N2O:3||FILMS:3||OPTICS:3||SPECTRA:3||FIELD:3||MIRRORS:3||ARRAYS:3||CLUSTERS:3||SIO2:3||IONIZATION:3||VACUUM:3||SCATTERING:3||IONS:2||LUMINESCENCE PROPERTIES:2||ANISOTROPY:2||BEAMS:2||DIFFRACTION:2||DISPERSION:2||chemical vapor deposition (CVD):2||ELECTRONICSTRUCTURE:2||MOSFETS:2||SI3N4:2||DENSITY:2||LIGHT:2||PLASMAS:2||MATTER:2||nanocomposites:2||RAMANSCATTERING:2||NANOPARTICLES:2||OXIDE:2||AMPLIFIED SPONTANEOUS EMISSION:2||NM WAVELENGTH:2||GAIN:2||CARBON NANOTUBES:2||CROSSSECTIONS:2||LIGHTEMITTINGDIODES:2||PULSE:2||CARBON PLASMA:2||TISAPPHIRE LASER:2||Raman scattering:2||ROUTE:2||multilayer:2||CATHODOLUMINESCENCE:2||highresolution transmission electronic microscope (HRTEM):2||DIFFERENCEFREQUENCYGENERATION:2||CRYSTAL:2||laserproduced plasma:2||NANOCABLES:2||photoluminescence:2||MAGNETIC ALLOY SEMICONDUCTORS:2||MOLECULARBEAM EPITAXY:2||EARTHDOPED GAN:2||LASER FIELDS:2||CHIRPEDPULSEAMPLIFICATION:2||ALN:2||GAUSSIANBEAM:2||ASSISTED CATALYTIC GROWTH:2||BLUE:2||NANOSTRUCTURES:2||MAGNETOELECTRONICS:2||MICROSCOPY:2||ELECTROLUMINESCENCE:2||LASERPULSES:2||GaN nanowires:2||GALLIUM NITRIDE NANOWIRES:2||GAMNN:2||NANOTUBES:2||PHYSICS:2||Femtosecond laser:2||parametric oscillators and amplifiers:1||ultrafast lasers:1||VALENCE:1||nanowires:1||DILUTED MAGNETIC SEMICONDUCTOR:1||LUMINESCENCE:1||Density modulation:1||Energy modulation:1||Current enhanced SASE free electron laser:1||Undulator radiation:1||FREEELECTRON LASERS:1||ULTRATHIN FERROMAGNETICFILMS:1||OXIDEFILMS:1||ABLATION:1||COMPONENT:1||METAL:1||innershell excited states:1||Nelike ions:1||TRANSITIONS:1||XUV spectrometer:1||DIAGNOSTICS:1||Xray scattering:1||MO/SI:1||pulsed laser deposition:1||KEV IMPACT ENERGIES:1||vacuum electron acceleration:1||HIGHINTENSITY LASER:1||JUNCTIONS:1||LOWTEMPERATURE GROWTH:1||nanocrystalline materials:1||MOLECULAR PHOTOIONIZATION:1||LOCALIZATION:1||DEUTERIUM CLUSTERS:1||EXPLOSIONS:1||REGENERATIVE AMPLIFIERS:1||RAREGASES:1||THz radiation:1||FREEELECTRON LASER:1||REALTIME OBSERVATION:1||TARGET:1||photoionized plasmas:1||fs Xray laser:1||emission profile:1||HIGHORDER HARMONICS:1||Xray laser:1||atomic transition:1||EXCITATION:1||LASERS:1||PERFORMANCE:1||RELATIVISTIC ELECTRONS:1||BI2O3DOPED ZNO:1||INNERSHELL IONIZATION:1||Laser wakefield:1||FREQUENCY:1||SOLIDSTATE LASERS:1||Linearly polarized:1||THERMIONIC EMISSION:1||PULSE AMPLIFICATION SYSTEM:1||BIB3O6:1||NM:1||NONCOVALENT INTERACTIONS:1||CRYSTALLINE:1||INTENSITY:1||JETS:1||COHERENT:1||LINE:1||ANGULARDISTRIBUTION:1||SILVER IONS:1||magnetic anisotropy:1||DEVICES:1||Auger transitions:1||CosterKronig transitions:1||EFFICIENT:1||ELECTRONIMPACT IONIZATION:1||ULTRASHORTPULSE:1||Nanowire:1||Heterostructure:1||soft Xray reflectivity:1||PLASMA ACCELERATOR:1||ZINCOXIDE NANOWIRES:1||CHEMICALVAPORDEPOSITION:1||Electron acceleration:1||Ionization of gases:1||Delay dependent:1||MULTIPHOTON IONIZATION:1||FRAGMENTATION:1||GASJET:1||ultrafast nonlinear optics:1||CYCLE PULSES:1||KHZ:1||chemical vapor deposition:1||ferromagnetism:1||ABSORPTION:1||TERAHERTZ RADIATION:1||SCIENCE:1||FIELDS:1||ELECTRONS:1||nanomultilayer structures:1||YIELDS:1||AUGER:1||10HZ REPETITION RATE:1||MULTITERAWATT:1||SPECTROGRAPH:1||HIGHHARMONICGENERATION:1||spectroscopy:1||level population:1||PARTICLEACCELERATION:1||OPTICAL FREQUENCYMEASUREMENT:1||NANOWALLS:1||ROOMTEMPERATURE:1||AVERAGE OUTPUT POWER:1||GROUPVELOCITYMISMATCH:1||Impact ionization:1||Dynamics:1||Lasers:1||Collisional process:1||ABOVETHRESHOLD IONIZATION:1||MAINGROUP THERMOCHEMISTRY:1||dilute magnetic semiconductors:1||GACRN:1||SIZE:1||ATTOSECOND:1||Ar cluster:1||Xray astrophysics:1||photoionization:1||irons:1||normal incidence pulsed laser deposition:1||SHELLS:1||Silicon Oxide:1||gaspuff Zpinch:1||Xray:1||soft Xray reflectors:1||ESCAPE:1||ZN2SIO4:1||SILICA:1||Time delay:1||Collisional plasmas:1||MASSSPECTROMETRY:1||NUCLEARFUSION:1||PARAMETRIC AMPLIFICATION:1||LYING ELECTRONIC STATES:1||ADJUSTABLEPARAMETERS:1||MAGNETICPROPERTIES:1||LIQUIDPHASE EPITAXY:1||CEP laser:1||REGION:1||Plasma waveguide:1||AMBIENT GAS:1||DEPOSITION:1||HARMONICGENERATION:1||ENHANCEMENT:1||imaging spectrometer:1||Abel inversion:1||Water window:1||Liquid nitrogen jet:1||CHARGEEXCHANGE:1||NOBEL LECTURE:1||VARISTOR:1||EPITAXY:1||THINDISK LASER:1||HIGHREPETITIONRATE:1||Atom lasers:1||Electronimpact excitation:1||High order harmonics:1||ultrafast technology:1||PEAK POWER:1||CHARGED ALUMINUM CLUSTERS:1||GaN:1||THIN:1||Electron beam:1||INTENSE:1||Hard Xray pulse generation:1||NONLINEAR THOMSON SCATTERING:1||MULTILAYER:1||UVvisible spectrometer:1||ATOMS:1||innershell transitions:1||CORRECTED CONCAVE GRATINGS:1||DISCHARGE:1||LASERPLASMA:1||thin film:1||reflectivity:1||opacity:1||gain:1||smallangle Xray scattering:1||SOFTXRAY:1||ZINCOXIDE:1||CYGNUSX3:1||Betatron oscillation:1||ACCELERATOR:1||STRAINEDLAYER SUPERLATTICES:1||OPTICAL PARAMETRIC AMPLIFICATION:1||PASSIVE MODELOCKING:1||Collision dynamics:1||MUM:1||EXACTEXCHANGE:1||BASISSET:1||APPROXIMATION:1||OXYNITRIDES:1||Beam energy modulation:1||polarization spectroscopy:1||REORIENTATION TRANSITION:1||DEPENDENCE:1||sulfurs:1||BUILDINGBLOCKS:1||RATES:1||OPTICAL PULSES:1||toroidal mirror:1||XRAY LASER:1||CALCIUM:1||radially polarized laser:1||GRAINBOUNDARIES:1||VAPORDEPOSITION:1||Xray generation:1||MAGNETIZATION:1||Electric excitation:1||Laserinduced gas plasmas:1||Qualitative analysis:1||SCHEME:1||RADIATION:10||PULSES:8||PHOTOLUMINESCENCE:7||LASER:7||GENERATION:6||NANORODS:6||GROWTH:6||NANOWIRES:5||IMPLANTED 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SEMICONDUCTORS:2||MOLECULARBEAM EPITAXY:2||EARTHDOPED GAN:2||LASER FIELDS:2||CHIRPEDPULSEAMPLIFICATION:2||ALN:2||GAUSSIANBEAM:2||ASSISTED CATALYTIC GROWTH:2||BLUE:2||NANOSTRUCTURES:2||MAGNETOELECTRONICS:2||MICROSCOPY:2||ELECTROLUMINESCENCE:2||LASERPULSES:2||GaN nanowires:2||GALLIUM NITRIDE NANOWIRES:2||GAMNN:2||NANOTUBES:2||PHYSICS:2||Femtosecond laser:2||parametric oscillators and amplifiers:1||ultrafast lasers:1||VALENCE:1||nanowires:1||DILUTED MAGNETIC SEMICONDUCTOR:1||LUMINESCENCE:1||Density modulation:1||Energy modulation:1||Current enhanced SASE free electron laser:1||Undulator radiation:1||FREEELECTRON LASERS:1||ULTRATHIN FERROMAGNETICFILMS:1||OXIDEFILMS:1||ABLATION:1||COMPONENT:1||METAL:1||innershell excited states:1||Nelike ions:1||TRANSITIONS:1||XUV spectrometer:1||DIAGNOSTICS:1||Xray scattering:1||MO/SI:1||pulsed laser deposition:1||KEV IMPACT ENERGIES:1||vacuum electron acceleration:1||HIGHINTENSITY LASER:1||JUNCTIONS:1||LOWTEMPERATURE GROWTH:1||nanocrystalline materials:1||MOLECULAR PHOTOIONIZATION:1||LOCALIZATION:1||DEUTERIUM CLUSTERS:1||EXPLOSIONS:1||REGENERATIVE AMPLIFIERS:1||RAREGASES:1||THz radiation:1||FREEELECTRON LASER:1||REALTIME OBSERVATION:1||TARGET:1||photoionized plasmas:1||fs Xray laser:1||emission profile:1||HIGHORDER HARMONICS:1||Xray laser:1||atomic transition:1||EXCITATION:1||LASERS:1||PERFORMANCE:1||RELATIVISTIC ELECTRONS:1||BI2O3DOPED ZNO:1||INNERSHELL IONIZATION:1||Laser wakefield:1||FREQUENCY:1||SOLIDSTATE LASERS:1||Linearly polarized:1||THERMIONIC EMISSION:1||PULSE AMPLIFICATION SYSTEM:1||BIB3O6:1||NM:1||NONCOVALENT INTERACTIONS:1||CRYSTALLINE:1||INTENSITY:1||JETS:1||COHERENT:1||LINE:1||ANGULARDISTRIBUTION:1||SILVER IONS:1||magnetic anisotropy:1||DEVICES:1||Auger transitions:1||CosterKronig transitions:1||EFFICIENT:1||ELECTRONIMPACT IONIZATION:1||ULTRASHORTPULSE:1||Nanowire:1||Heterostructure:1||soft Xray reflectivity:1||PLASMA ACCELERATOR:1||ZINCOXIDE NANOWIRES:1||CHEMICALVAPORDEPOSITION:1||Electron acceleration:1||Ionization of gases:1||Delay dependent:1||MULTIPHOTON IONIZATION:1||FRAGMENTATION:1||GASJET:1||ultrafast nonlinear optics:1||CYCLE PULSES:1||KHZ:1||chemical vapor deposition:1||ferromagnetism:1||ABSORPTION:1||TERAHERTZ RADIATION:1||SCIENCE:1||FIELDS:1||ELECTRONS:1||nanomultilayer structures:1||YIELDS:1||AUGER:1||10HZ REPETITION RATE:1||MULTITERAWATT:1||SPECTROGRAPH:1||HIGHHARMONICGENERATION:1||spectroscopy:1||level population:1||PARTICLEACCELERATION:1||OPTICAL FREQUENCYMEASUREMENT:1||NANOWALLS:1||ROOMTEMPERATURE:1||AVERAGE OUTPUT POWER:1||GROUPVELOCITYMISMATCH:1||Impact ionization:1||Dynamics:1||Lasers:1||Collisional process:1||ABOVETHRESHOLD IONIZATION:1||MAINGROUP THERMOCHEMISTRY:1||dilute magnetic semiconductors:1||GACRN:1||SIZE:1||ATTOSECOND:1||Ar cluster:1||Xray astrophysics:1||photoionization:1||irons:1||normal incidence pulsed laser deposition:1||SHELLS:1||Silicon Oxide:1||gaspuff Zpinch:1||Xray:1||soft Xray reflectors:1||ESCAPE:1||ZN2SIO4:1||SILICA:1||Time 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materials:1||MOLECULAR PHOTOIONIZATION:1||LOCALIZATION:1||DEUTERIUM CLUSTERS:1||EXPLOSIONS:1||REGENERATIVE AMPLIFIERS:1||RAREGASES:1||THz radiation:1||FREEELECTRON LASER:1||REALTIME OBSERVATION:1||TARGET:1||photoionized plasmas:1||fs Xray laser:1||emission profile:1||HIGHORDER HARMONICS:1||Xray laser:1||atomic transition:1||EXCITATION:1||LASERS:1||PERFORMANCE:1||RELATIVISTIC ELECTRONS:1||BI2O3DOPED ZNO:1||INNERSHELL IONIZATION:1||Laser wakefield:1||FREQUENCY:1||SOLIDSTATE LASERS:1||Linearly polarized:1||THERMIONIC EMISSION:1||PULSE AMPLIFICATION SYSTEM:1||BIB3O6:1||NM:1||NONCOVALENT INTERACTIONS:1||CRYSTALLINE:1||INTENSITY:1||JETS:1||COHERENT:1||LINE:1||ANGULARDISTRIBUTION:1||SILVER IONS:1||magnetic anisotropy:1||DEVICES:1||Auger transitions:1||CosterKronig transitions:1||EFFICIENT:1||ELECTRONIMPACT IONIZATION:1||ULTRASHORTPULSE:1||Nanowire:1||Heterostructure:1||soft Xray reflectivity:1||PLASMA ACCELERATOR:1||ZINCOXIDE NANOWIRES:1||CHEMICALVAPORDEPOSITION:1||Electron acceleration:1||Ionization of gases:1||Delay dependent:1||MULTIPHOTON IONIZATION:1||FRAGMENTATION:1||GASJET:1||ultrafast nonlinear optics:1||CYCLE PULSES:1||KHZ:1||chemical vapor deposition:1||ferromagnetism:1||ABSORPTION:1||TERAHERTZ RADIATION:1||SCIENCE:1||FIELDS:1||ELECTRONS:1||nanomultilayer structures:1||YIELDS:1||AUGER:1||10HZ REPETITION RATE:1||MULTITERAWATT:1||SPECTROGRAPH:1||HIGHHARMONICGENERATION:1||spectroscopy:1||level population:1||PARTICLEACCELERATION:1||OPTICAL FREQUENCYMEASUREMENT:1||NANOWALLS:1||ROOMTEMPERATURE:1||AVERAGE OUTPUT POWER:1||GROUPVELOCITYMISMATCH:1||Impact ionization:1||Dynamics:1||Lasers:1||Collisional process:1||ABOVETHRESHOLD IONIZATION:1||MAINGROUP THERMOCHEMISTRY:1||dilute magnetic semiconductors:1||GACRN:1||SIZE:1||ATTOSECOND:1||Ar cluster:1||Xray astrophysics:1||photoionization:1||irons:1||normal incidence pulsed laser deposition:1||SHELLS:1||Silicon Oxide:1||gaspuff Zpinch:1||Xray:1||soft Xray reflectors:1||ESCAPE:1||ZN2SIO4:1||SILICA:1||Time delay:1||Collisional plasmas:1||MASSSPECTROMETRY:1||NUCLEARFUSION:1||PARAMETRIC AMPLIFICATION:1||LYING ELECTRONIC STATES:1||ADJUSTABLEPARAMETERS:1||MAGNETICPROPERTIES:1||LIQUIDPHASE EPITAXY:1||CEP laser:1||REGION:1||Plasma waveguide:1||AMBIENT GAS:1||DEPOSITION:1||HARMONICGENERATION:1||ENHANCEMENT:1||imaging spectrometer:1||Abel inversion:1||Water window:1||Liquid nitrogen jet:1||CHARGEEXCHANGE:1||NOBEL LECTURE:1||VARISTOR:1||EPITAXY:1||THINDISK LASER:1||HIGHREPETITIONRATE:1||Atom lasers:1||Electronimpact excitation:1||High order harmonics:1||ultrafast technology:1||PEAK POWER:1||CHARGED ALUMINUM CLUSTERS:1||GaN:1||THIN:1||Electron beam:1||INTENSE:1||Hard Xray pulse generation:1||NONLINEAR THOMSON SCATTERING:1||MULTILAYER:1||UVvisible spectrometer:1||ATOMS:1||innershell transitions:1||CORRECTED CONCAVE GRATINGS:1||DISCHARGE:1||LASERPLASMA:1||thin film:1||reflectivity:1||opacity:1||gain:1||smallangle Xray scattering:1||SOFTXRAY:1||ZINCOXIDE:1||CYGNUSX3:1||Betatron oscillation:1||ACCELERATOR:1||STRAINEDLAYER SUPERLATTICES:1||OPTICAL PARAMETRIC AMPLIFICATION:1||PASSIVE MODELOCKING:1||Collision dynamics:1||MUM:1||EXACTEXCHANGE:1||BASISSET:1||APPROXIMATION:1||OXYNITRIDES:1||Beam energy modulation:1||polarization spectroscopy:1||REORIENTATION TRANSITION:1||DEPENDENCE:1||sulfurs:1||BUILDINGBLOCKS:1||RATES:1||OPTICAL PULSES:1||toroidal mirror:1||XRAY LASER:1||CALCIUM:1||radially polarized laser:1||GRAINBOUNDARIES:1||VAPORDEPOSITION:1||Xray generation:1||MAGNETIZATION:1||Electric excitation:1||Laserinduced gas plasmas:1||Qualitative analysis:1||SCHEME:1||RADIATION:10||PULSES:8||PHOTOLUMINESCENCE:7||LASER:7||GENERATION:6||NANORODS:6||GROWTH:6||NANOWIRES:5||IMPLANTED GAN:5||SPECTROSCOPY:5||THINFILMS:4||DYNAMICS:4||SILICON:4||EXTREMEULTRAVIOLET:4||AMPLIFICATION:4||PRESSURE:4||PHASE:4||OPTICALPROPERTIES:4||SYSTEM:4||EMISSION:4||FEL:3||N2O:3||FILMS:3||OPTICS:3||SPECTRA:3||FIELD:3||MIRRORS:3||ARRAYS:3||CLUSTERS:3||SIO2:3||IONIZATION:3||VACUUM:3||SCATTERING:3||IONS:2||LUMINESCENCE PROPERTIES:2||ANISOTROPY:2||BEAMS:2||DIFFRACTION:2||DISPERSION:2||chemical vapor deposition (CVD):2||ELECTRONICSTRUCTURE:2||MOSFETS:2||SI3N4:2||DENSITY:2||LIGHT:2||PLASMAS:2||MATTER:2||nanocomposites:2||RAMANSCATTERING:2||NANOPARTICLES:2||OXIDE:2||AMPLIFIED SPONTANEOUS EMISSION:2||NM WAVELENGTH:2||GAIN:2||CARBON NANOTUBES:2||CROSSSECTIONS:2||LIGHTEMITTINGDIODES:2||PULSE:2||CARBON PLASMA:2||TISAPPHIRE LASER:2||Raman scattering:2||ROUTE:2||multilayer:2||CATHODOLUMINESCENCE:2||highresolution transmission electronic microscope (HRTEM):2||DIFFERENCEFREQUENCYGENERATION:2||CRYSTAL:2||laserproduced plasma:2||NANOCABLES:2||photoluminescence:2||MAGNETIC ALLOY SEMICONDUCTORS:2||MOLECULARBEAM EPITAXY:2||EARTHDOPED GAN:2||LASER FIELDS:2||CHIRPEDPULSEAMPLIFICATION:2||ALN:2||GAUSSIANBEAM:2||ASSISTED CATALYTIC GROWTH:2||BLUE:2||NANOSTRUCTURES:2||MAGNETOELECTRONICS:2||MICROSCOPY:2||ELECTROLUMINESCENCE:2||LASERPULSES:2||GaN nanowires:2||GALLIUM NITRIDE NANOWIRES:2||GAMNN:2||NANOTUBES:2||PHYSICS:2||Femtosecond laser:2||parametric oscillators and amplifiers:1||ultrafast lasers:1||VALENCE:1||nanowires:1||DILUTED MAGNETIC SEMICONDUCTOR:1||LUMINESCENCE:1||Density modulation:1||Energy modulation:1||Current enhanced SASE free electron laser:1||Undulator radiation:1||FREEELECTRON LASERS:1||ULTRATHIN FERROMAGNETICFILMS:1||OXIDEFILMS:1||ABLATION:1||COMPONENT:1||METAL:1||innershell excited states:1||Nelike ions:1||TRANSITIONS:1||XUV spectrometer:1||DIAGNOSTICS:1||Xray scattering:1||MO/SI:1||pulsed laser deposition:1||KEV IMPACT ENERGIES:1||vacuum electron acceleration:1||HIGHINTENSITY LASER:1||JUNCTIONS:1||LOWTEMPERATURE GROWTH:1||nanocrystalline materials:1||MOLECULAR PHOTOIONIZATION:1||LOCALIZATION:1||DEUTERIUM CLUSTERS:1||EXPLOSIONS:1||REGENERATIVE AMPLIFIERS:1||RAREGASES:1||THz radiation:1||FREEELECTRON LASER:1||REALTIME OBSERVATION:1||TARGET:1||photoionized plasmas:1||fs Xray laser:1||emission profile:1||HIGHORDER HARMONICS:1||Xray laser:1||atomic transition:1||EXCITATION:1||LASERS:1||PERFORMANCE:1||RELATIVISTIC ELECTRONS:1||BI2O3DOPED ZNO:1||INNERSHELL IONIZATION:1||Laser wakefield:1||FREQUENCY:1||SOLIDSTATE LASERS:1||Linearly polarized:1||THERMIONIC EMISSION:1||PULSE AMPLIFICATION SYSTEM:1||BIB3O6:1||NM:1||NONCOVALENT INTERACTIONS:1||CRYSTALLINE:1||INTENSITY:1||JETS:1||COHERENT:1||LINE:1||ANGULARDISTRIBUTION:1||SILVER IONS:1||magnetic anisotropy:1||DEVICES:1||Auger transitions:1||CosterKronig transitions:1||EFFICIENT:1||ELECTRONIMPACT IONIZATION:1||ULTRASHORTPULSE:1||Nanowire:1||Heterostructure:1||soft Xray reflectivity:1||PLASMA ACCELERATOR:1||ZINCOXIDE NANOWIRES:1||CHEMICALVAPORDEPOSITION:1||Electron acceleration:1||Ionization of gases:1||Delay dependent:1||MULTIPHOTON IONIZATION:1||FRAGMENTATION:1||GASJET:1||ultrafast nonlinear optics:1||CYCLE PULSES:1||KHZ:1||chemical vapor deposition:1||ferromagnetism:1||ABSORPTION:1||TERAHERTZ RADIATION:1||SCIENCE:1||FIELDS:1||ELECTRONS:1||nanomultilayer structures:1||YIELDS:1||AUGER:1||10HZ REPETITION RATE:1||MULTITERAWATT:1||SPECTROGRAPH:1||HIGHHARMONICGENERATION:1||spectroscopy:1||level population:1||PARTICLEACCELERATION:1||OPTICAL FREQUENCYMEASUREMENT:1||NANOWALLS:1||ROOMTEMPERATURE:1||AVERAGE OUTPUT POWER:1||GROUPVELOCITYMISMATCH:1||Impact ionization:1||Dynamics:1||Lasers:1||Collisional process:1||ABOVETHRESHOLD IONIZATION:1||MAINGROUP THERMOCHEMISTRY:1||dilute magnetic semiconductors:1||GACRN:1||SIZE:1||ATTOSECOND:1||Ar cluster:1||Xray astrophysics:1||photoionization:1||irons:1||normal incidence pulsed laser deposition:1||SHELLS:1||Silicon Oxide:1||gaspuff Zpinch:1||Xray:1||soft Xray reflectors:1||ESCAPE:1||ZN2SIO4:1||SILICA:1||Time delay:1||Collisional plasmas:1||MASSSPECTROMETRY:1||NUCLEARFUSION:1||PARAMETRIC AMPLIFICATION:1||LYING ELECTRONIC STATES:1||ADJUSTABLEPARAMETERS:1||MAGNETICPROPERTIES:1||LIQUIDPHASE EPITAXY:1||CEP laser:1||REGION:1||Plasma waveguide:1||AMBIENT GAS:1||DEPOSITION:1||HARMONICGENERATION:1||ENHANCEMENT:1||imaging spectrometer:1||Abel inversion:1||Water window:1||Liquid nitrogen jet:1||CHARGEEXCHANGE:1||NOBEL LECTURE:1||VARISTOR:1||EPITAXY:1||THINDISK LASER:1||HIGHREPETITIONRATE:1||Atom lasers:1||Electronimpact excitation:1||High order harmonics:1||ultrafast technology:1||PEAK POWER:1||CHARGED ALUMINUM CLUSTERS:1||GaN:1||THIN:1||Electron beam:1||INTENSE:1||Hard Xray pulse generation:1||NONLINEAR THOMSON SCATTERING:1||MULTILAYER:1||UVvisible spectrometer:1||ATOMS:1||innershell transitions:1||CORRECTED CONCAVE GRATINGS:1||DISCHARGE:1||LASERPLASMA:1||thin film:1||reflectivity:1||opacity:1||gain:1||smallangle Xray scattering:1||SOFTXRAY:1||ZINCOXIDE:1||CYGNUSX3:1||Betatron oscillation:1||ACCELERATOR:1||STRAINEDLAYER SUPERLATTICES:1||OPTICAL PARAMETRIC AMPLIFICATION:1||PASSIVE MODELOCKING:1||Collision dynamics:1||MUM:1||EXACTEXCHANGE:1||BASISSET:1||APPROXIMATION:1||OXYNITRIDES:1||Beam energy modulation:1||polarization spectroscopy:1||REORIENTATION TRANSITION:1||DEPENDENCE:1||sulfurs:1||BUILDINGBLOCKS:1||RATES:1||OPTICAL PULSES:1||toroidal mirror:1||XRAY LASER:1||CALCIUM:1||radially polarized laser:1||GRAINBOUNDARIES:1||VAPORDEPOSITION:1||Xray generation:1||MAGNETIZATION:1||Electric excitation:1||Laserinduced gas plasmas:1||Qualitative analysis:1||SCHEME:1||RADIATION:10||PULSES:8||PHOTOLUMINESCENCE:7||LASER:7||GENERATION:6||NANORODS:6||GROWTH:6||NANOWIRES:5||IMPLANTED 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SEMICONDUCTORS:2||MOLECULARBEAM EPITAXY:2||EARTHDOPED GAN:2||LASER FIELDS:2||CHIRPEDPULSEAMPLIFICATION:2||ALN:2||GAUSSIANBEAM:2||ASSISTED CATALYTIC GROWTH:2||BLUE:2||NANOSTRUCTURES:2||MAGNETOELECTRONICS:2||MICROSCOPY:2||ELECTROLUMINESCENCE:2||LASERPULSES:2||GaN nanowires:2||GALLIUM NITRIDE NANOWIRES:2||GAMNN:2||NANOTUBES:2||PHYSICS:2||Femtosecond laser:2||parametric oscillators and amplifiers:1||ultrafast lasers:1||VALENCE:1||nanowires:1||DILUTED MAGNETIC SEMICONDUCTOR:1||LUMINESCENCE:1||Density modulation:1||Energy modulation:1||Current enhanced SASE free electron laser:1||Undulator radiation:1||FREEELECTRON LASERS:1||ULTRATHIN FERROMAGNETICFILMS:1||OXIDEFILMS:1||ABLATION:1||COMPONENT:1||METAL:1||innershell excited states:1||Nelike ions:1||TRANSITIONS:1||XUV spectrometer:1||DIAGNOSTICS:1||Xray scattering:1||MO/SI:1||pulsed laser deposition:1||KEV IMPACT ENERGIES:1||vacuum electron acceleration:1||HIGHINTENSITY LASER:1||JUNCTIONS:1||LOWTEMPERATURE GROWTH:1||nanocrystalline materials:1||MOLECULAR PHOTOIONIZATION:1||LOCALIZATION:1||DEUTERIUM CLUSTERS:1||EXPLOSIONS:1||REGENERATIVE AMPLIFIERS:1||RAREGASES:1||THz radiation:1||FREEELECTRON LASER:1||REALTIME OBSERVATION:1||TARGET:1||photoionized plasmas:1||fs Xray laser:1||emission profile:1||HIGHORDER HARMONICS:1||Xray laser:1||atomic transition:1||EXCITATION:1||LASERS:1||PERFORMANCE:1||RELATIVISTIC ELECTRONS:1||BI2O3DOPED ZNO:1||INNERSHELL IONIZATION:1||Laser wakefield:1||FREQUENCY:1||SOLIDSTATE LASERS:1||Linearly polarized:1||THERMIONIC EMISSION:1||PULSE AMPLIFICATION SYSTEM:1||BIB3O6:1||NM:1||NONCOVALENT INTERACTIONS:1||CRYSTALLINE:1||INTENSITY:1||JETS:1||COHERENT:1||LINE:1||ANGULARDISTRIBUTION:1||SILVER IONS:1||magnetic anisotropy:1||DEVICES:1||Auger transitions:1||CosterKronig transitions:1||EFFICIENT:1||ELECTRONIMPACT IONIZATION:1||ULTRASHORTPULSE:1||Nanowire:1||Heterostructure:1||soft Xray reflectivity:1||PLASMA ACCELERATOR:1||ZINCOXIDE NANOWIRES:1||CHEMICALVAPORDEPOSITION:1||Electron acceleration:1||Ionization of gases:1||Delay dependent:1||MULTIPHOTON IONIZATION:1||FRAGMENTATION:1||GASJET:1||ultrafast nonlinear optics:1||CYCLE PULSES:1||KHZ:1||chemical vapor deposition:1||ferromagnetism:1||ABSORPTION:1||TERAHERTZ RADIATION:1||SCIENCE:1||FIELDS:1||ELECTRONS:1||nanomultilayer structures:1||YIELDS:1||AUGER:1||10HZ REPETITION RATE:1||MULTITERAWATT:1||SPECTROGRAPH:1||HIGHHARMONICGENERATION:1||spectroscopy:1||level population:1||PARTICLEACCELERATION:1||OPTICAL FREQUENCYMEASUREMENT:1||NANOWALLS:1||ROOMTEMPERATURE:1||AVERAGE OUTPUT POWER:1||GROUPVELOCITYMISMATCH:1||Impact ionization:1||Dynamics:1||Lasers:1||Collisional process:1||ABOVETHRESHOLD IONIZATION:1||MAINGROUP THERMOCHEMISTRY:1||dilute magnetic semiconductors:1||GACRN:1||SIZE:1||ATTOSECOND:1||Ar cluster:1||Xray astrophysics:1||photoionization:1||irons:1||normal incidence pulsed laser deposition:1||SHELLS:1||Silicon Oxide:1||gaspuff Zpinch:1||Xray:1||soft Xray reflectors:1||ESCAPE:1||ZN2SIO4:1||SILICA:1||Time 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materials:1||MOLECULAR PHOTOIONIZATION:1||LOCALIZATION:1||DEUTERIUM CLUSTERS:1||EXPLOSIONS:1||REGENERATIVE AMPLIFIERS:1||RAREGASES:1||THz radiation:1||FREEELECTRON LASER:1||REALTIME OBSERVATION:1||TARGET:1||photoionized plasmas:1||fs Xray laser:1||emission profile:1||HIGHORDER HARMONICS:1||Xray laser:1||atomic transition:1||EXCITATION:1||LASERS:1||PERFORMANCE:1||RELATIVISTIC ELECTRONS:1||BI2O3DOPED ZNO:1||INNERSHELL IONIZATION:1||Laser wakefield:1||FREQUENCY:1||SOLIDSTATE LASERS:1||Linearly polarized:1||THERMIONIC EMISSION:1||PULSE AMPLIFICATION SYSTEM:1||BIB3O6:1||NM:1||NONCOVALENT INTERACTIONS:1||CRYSTALLINE:1||INTENSITY:1||JETS:1||COHERENT:1||LINE:1||ANGULARDISTRIBUTION:1||SILVER IONS:1||magnetic anisotropy:1||DEVICES:1||Auger transitions:1||CosterKronig transitions:1||EFFICIENT:1||ELECTRONIMPACT IONIZATION:1||ULTRASHORTPULSE:1||Nanowire:1||Heterostructure:1||soft Xray reflectivity:1||PLASMA ACCELERATOR:1||ZINCOXIDE NANOWIRES:1||CHEMICALVAPORDEPOSITION:1||Electron acceleration:1||Ionization of gases:1||Delay dependent:1||MULTIPHOTON IONIZATION:1||FRAGMENTATION:1||GASJET:1||ultrafast nonlinear optics:1||CYCLE PULSES:1||KHZ:1||chemical vapor deposition:1||ferromagnetism:1||ABSORPTION:1||TERAHERTZ RADIATION:1||SCIENCE:1||FIELDS:1||ELECTRONS:1||nanomultilayer structures:1||YIELDS:1||AUGER:1||10HZ REPETITION RATE:1||MULTITERAWATT:1||SPECTROGRAPH:1||HIGHHARMONICGENERATION:1||spectroscopy:1||level population:1||PARTICLEACCELERATION:1||OPTICAL FREQUENCYMEASUREMENT:1||NANOWALLS:1||ROOMTEMPERATURE:1||AVERAGE OUTPUT POWER:1||GROUPVELOCITYMISMATCH:1||Impact ionization:1||Dynamics:1||Lasers:1||Collisional process:1||ABOVETHRESHOLD IONIZATION:1||MAINGROUP THERMOCHEMISTRY:1||dilute magnetic semiconductors:1||GACRN:1||SIZE:1||ATTOSECOND:1||Ar cluster:1||Xray astrophysics:1||photoionization:1||irons:1||normal incidence pulsed laser deposition:1||SHELLS:1||Silicon Oxide:1||gaspuff Zpinch:1||Xray:1||soft Xray reflectors:1||ESCAPE:1||ZN2SIO4:1||SILICA:1||Time delay:1||Collisional plasmas:1||MASSSPECTROMETRY:1||NUCLEARFUSION:1||PARAMETRIC AMPLIFICATION:1||LYING ELECTRONIC STATES:1||ADJUSTABLEPARAMETERS:1||MAGNETICPROPERTIES:1||LIQUIDPHASE EPITAXY:1||CEP laser:1||REGION:1||Plasma waveguide:1||AMBIENT GAS:1||DEPOSITION:1||HARMONICGENERATION:1||ENHANCEMENT:1||imaging spectrometer:1||Abel inversion:1||Water window:1||Liquid nitrogen jet:1||CHARGEEXCHANGE:1||NOBEL LECTURE:1||VARISTOR:1||EPITAXY:1||THINDISK LASER:1||HIGHREPETITIONRATE:1||Atom lasers:1||Electronimpact excitation:1||High order harmonics:1||ultrafast technology:1||PEAK POWER:1||CHARGED ALUMINUM CLUSTERS:1||GaN:1||THIN:1||Electron beam:1||INTENSE:1||Hard Xray pulse generation:1||NONLINEAR THOMSON SCATTERING:1||MULTILAYER:1||UVvisible spectrometer:1||ATOMS:1||innershell transitions:1||CORRECTED CONCAVE GRATINGS:1||DISCHARGE:1||LASERPLASMA:1||thin film:1||reflectivity:1||opacity:1||gain:1||smallangle Xray scattering:1||SOFTXRAY:1||ZINCOXIDE:1||CYGNUSX3:1||Betatron oscillation:1||ACCELERATOR:1||STRAINEDLAYER SUPERLATTICES:1||OPTICAL PARAMETRIC AMPLIFICATION:1||PASSIVE MODELOCKING:1||Collision dynamics:1||MUM:1||EXACTEXCHANGE:1||BASISSET:1||APPROXIMATION:1||OXYNITRIDES:1||Beam energy modulation:1||polarization spectroscopy:1||REORIENTATION TRANSITION:1||DEPENDENCE:1||sulfurs:1||BUILDINGBLOCKS:1||RATES:1||OPTICAL PULSES:1||toroidal mirror:1||XRAY LASER:1||CALCIUM:1||radially polarized laser:1||GRAINBOUNDARIES:1||VAPORDEPOSITION:1||Xray generation:1||MAGNETIZATION:1||Electric excitation:1||Laserinduced gas plasmas:1||Qualitative analysis:1||SCHEME:1||RADIATION:10||PULSES:8||PHOTOLUMINESCENCE:7||LASER:7||GENERATION:6||NANORODS:6||GROWTH:6||NANOWIRES:5||IMPLANTED GAN:5||SPECTROSCOPY:5||THINFILMS:4||DYNAMICS:4||SILICON:4||EXTREMEULTRAVIOLET:4||AMPLIFICATION:4||PRESSURE:4||PHASE:4||OPTICALPROPERTIES:4||SYSTEM:4||EMISSION:4||FEL:3||N2O:3||FILMS:3||OPTICS:3||SPECTRA:3||FIELD:3||MIRRORS:3||ARRAYS:3||CLUSTERS:3||SIO2:3||IONIZATION:3||VACUUM:3||SCATTERING:3||IONS:2||LUMINESCENCE PROPERTIES:2||ANISOTROPY:2||BEAMS:2||DIFFRACTION:2||DISPERSION:2||chemical vapor deposition (CVD):2||ELECTRONICSTRUCTURE:2||MOSFETS:2||SI3N4:2||DENSITY:2||LIGHT:2||PLASMAS:2||MATTER:2||nanocomposites:2||RAMANSCATTERING:2||NANOPARTICLES:2||OXIDE:2||AMPLIFIED SPONTANEOUS EMISSION:2||NM WAVELENGTH:2||GAIN:2||CARBON NANOTUBES:2||CROSSSECTIONS:2||LIGHTEMITTINGDIODES:2||PULSE:2||CARBON PLASMA:2||TISAPPHIRE LASER:2||Raman scattering:2||ROUTE:2||multilayer:2||CATHODOLUMINESCENCE:2||highresolution transmission electronic microscope (HRTEM):2||DIFFERENCEFREQUENCYGENERATION:2||CRYSTAL:2||laserproduced plasma:2||NANOCABLES:2||photoluminescence:2||MAGNETIC ALLOY SEMICONDUCTORS:2||MOLECULARBEAM EPITAXY:2||EARTHDOPED GAN:2||LASER FIELDS:2||CHIRPEDPULSEAMPLIFICATION:2||ALN:2||GAUSSIANBEAM:2||ASSISTED CATALYTIC GROWTH:2||BLUE:2||NANOSTRUCTURES:2||MAGNETOELECTRONICS:2||MICROSCOPY:2||ELECTROLUMINESCENCE:2||LASERPULSES:2||GaN nanowires:2||GALLIUM NITRIDE NANOWIRES:2||GAMNN:2||NANOTUBES:2||PHYSICS:2||Femtosecond laser:2||parametric oscillators and amplifiers:1||ultrafast lasers:1||VALENCE:1||nanowires:1||DILUTED MAGNETIC SEMICONDUCTOR:1||LUMINESCENCE:1||Density modulation:1||Energy modulation:1||Current enhanced SASE free electron laser:1||Undulator radiation:1||FREEELECTRON LASERS:1||ULTRATHIN FERROMAGNETICFILMS:1||OXIDEFILMS:1||ABLATION:1||COMPONENT:1||METAL:1||innershell excited states:1||Nelike ions:1||TRANSITIONS:1||XUV spectrometer:1||DIAGNOSTICS:1||Xray scattering:1||MO/SI:1||pulsed laser deposition:1||KEV IMPACT ENERGIES:1||vacuum electron acceleration:1||HIGHINTENSITY LASER:1||JUNCTIONS:1||LOWTEMPERATURE GROWTH:1||nanocrystalline materials:1||MOLECULAR PHOTOIONIZATION:1||LOCALIZATION:1||DEUTERIUM CLUSTERS:1||EXPLOSIONS:1||REGENERATIVE AMPLIFIERS:1||RAREGASES:1||THz radiation:1||FREEELECTRON LASER:1||REALTIME OBSERVATION:1||TARGET:1||photoionized plasmas:1||fs Xray laser:1||emission profile:1||HIGHORDER HARMONICS:1||Xray laser:1||atomic transition:1||EXCITATION:1||LASERS:1||PERFORMANCE:1||RELATIVISTIC ELECTRONS:1||BI2O3DOPED ZNO:1||INNERSHELL IONIZATION:1||Laser wakefield:1||FREQUENCY:1||SOLIDSTATE LASERS:1||Linearly polarized:1||THERMIONIC EMISSION:1||PULSE AMPLIFICATION SYSTEM:1||BIB3O6:1||NM:1||NONCOVALENT INTERACTIONS:1||CRYSTALLINE:1||INTENSITY:1||JETS:1||COHERENT:1||LINE:1||ANGULARDISTRIBUTION:1||SILVER IONS:1||magnetic anisotropy:1||DEVICES:1||Auger transitions:1||CosterKronig transitions:1||EFFICIENT:1||ELECTRONIMPACT IONIZATION:1||ULTRASHORTPULSE:1||Nanowire:1||Heterostructure:1||soft Xray reflectivity:1||PLASMA ACCELERATOR:1||ZINCOXIDE NANOWIRES:1||CHEMICALVAPORDEPOSITION:1||Electron acceleration:1||Ionization of gases:1||Delay dependent:1||MULTIPHOTON IONIZATION:1||FRAGMENTATION:1||GASJET:1||ultrafast nonlinear optics:1||CYCLE PULSES:1||KHZ:1||chemical vapor deposition:1||ferromagnetism:1||ABSORPTION:1||TERAHERTZ RADIATION:1||SCIENCE:1||FIELDS:1||ELECTRONS:1||nanomultilayer structures:1||YIELDS:1||AUGER:1||10HZ REPETITION RATE:1||MULTITERAWATT:1||SPECTROGRAPH:1||HIGHHARMONICGENERATION:1||spectroscopy:1||level population:1||PARTICLEACCELERATION:1||OPTICAL FREQUENCYMEASUREMENT:1||NANOWALLS:1||ROOMTEMPERATURE:1||AVERAGE OUTPUT POWER:1||GROUPVELOCITYMISMATCH:1||Impact ionization:1||Dynamics:1||Lasers:1||Collisional process:1||ABOVETHRESHOLD IONIZATION:1||MAINGROUP THERMOCHEMISTRY:1||dilute magnetic semiconductors:1||GACRN:1||SIZE:1||ATTOSECOND:1||Ar cluster:1||Xray astrophysics:1||photoionization:1||irons:1||normal incidence pulsed laser deposition:1||SHELLS:1||Silicon Oxide:1||gaspuff Zpinch:1||Xray:1||soft Xray reflectors:1||ESCAPE:1||ZN2SIO4:1||SILICA:1||Time delay:1||Collisional plasmas:1||MASSSPECTROMETRY:1||NUCLEARFUSION:1||PARAMETRIC AMPLIFICATION:1||LYING ELECTRONIC STATES:1||ADJUSTABLEPARAMETERS:1||MAGNETICPROPERTIES:1||LIQUIDPHASE EPITAXY:1||CEP laser:1||REGION:1||Plasma waveguide:1||AMBIENT GAS:1||DEPOSITION:1||HARMONICGENERATION:1||ENHANCEMENT:1||imaging spectrometer:1||Abel inversion:1||Water window:1||Liquid nitrogen jet:1||CHARGEEXCHANGE:1||NOBEL LECTURE:1||VARISTOR:1||EPITAXY:1||THINDISK LASER:1||HIGHREPETITIONRATE:1||Atom lasers:1||Electronimpact excitation:1||High order harmonics:1||ultrafast technology:1||PEAK POWER:1||CHARGED ALUMINUM CLUSTERS:1||GaN:1||THIN:1||Electron beam:1||INTENSE:1||Hard Xray pulse generation:1||NONLINEAR THOMSON SCATTERING:1||MULTILAYER:1||UVvisible spectrometer:1||ATOMS:1||innershell transitions:1||CORRECTED CONCAVE GRATINGS:1||DISCHARGE:1||LASERPLASMA:1||thin film:1||reflectivity:1||opacity:1||gain:1||smallangle Xray scattering:1||SOFTXRAY:1||ZINCOXIDE:1||CYGNUSX3:1||Betatron oscillation:1||ACCELERATOR:1||STRAINEDLAYER SUPERLATTICES:1||OPTICAL PARAMETRIC AMPLIFICATION:1||PASSIVE MODELOCKING:1||Collision dynamics:1||MUM:1||EXACTEXCHANGE:1||BASISSET:1||APPROXIMATION:1||OXYNITRIDES:1||Beam energy modulation:1||polarization spectroscopy:1||REORIENTATION TRANSITION:1||DEPENDENCE:1||sulfurs:1||BUILDINGBLOCKS:1||RATES:1||OPTICAL PULSES:1||toroidal mirror:1||XRAY LASER:1||CALCIUM:1||radially polarized laser:1||GRAINBOUNDARIES:1||VAPORDEPOSITION:1||Xray generation:1||MAGNETIZATION:1||Electric excitation:1||Laserinduced gas plasmas:1||Qualitative analysis:1||SCHEME:1||RADIATION:10||PULSES:8||PHOTOLUMINESCENCE:7||LASER:7||GENERATION:6||NANORODS:6||GROWTH:6||NANOWIRES:5||IMPLANTED 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SEMICONDUCTORS:2||MOLECULARBEAM EPITAXY:2||EARTHDOPED GAN:2||LASER FIELDS:2||CHIRPEDPULSEAMPLIFICATION:2||ALN:2||GAUSSIANBEAM:2||ASSISTED CATALYTIC GROWTH:2||BLUE:2||NANOSTRUCTURES:2||MAGNETOELECTRONICS:2||MICROSCOPY:2||ELECTROLUMINESCENCE:2||LASERPULSES:2||GaN nanowires:2||GALLIUM NITRIDE NANOWIRES:2||GAMNN:2||NANOTUBES:2||PHYSICS:2||Femtosecond laser:2||parametric oscillators and amplifiers:1||ultrafast lasers:1||VALENCE:1||nanowires:1||DILUTED MAGNETIC SEMICONDUCTOR:1||LUMINESCENCE:1||Density modulation:1||Energy modulation:1||Current enhanced SASE free electron laser:1||Undulator radiation:1||FREEELECTRON LASERS:1||ULTRATHIN FERROMAGNETICFILMS:1||OXIDEFILMS:1||ABLATION:1||COMPONENT:1||METAL:1||innershell excited states:1||Nelike ions:1||TRANSITIONS:1||XUV spectrometer:1||DIAGNOSTICS:1||Xray scattering:1||MO/SI:1||pulsed laser deposition:1||KEV IMPACT ENERGIES:1||vacuum electron acceleration:1||HIGHINTENSITY LASER:1||JUNCTIONS:1||LOWTEMPERATURE GROWTH:1||nanocrystalline materials:1||MOLECULAR PHOTOIONIZATION:1||LOCALIZATION:1||DEUTERIUM CLUSTERS:1||EXPLOSIONS:1||REGENERATIVE AMPLIFIERS:1||RAREGASES:1||THz radiation:1||FREEELECTRON LASER:1||REALTIME OBSERVATION:1||TARGET:1||photoionized plasmas:1||fs Xray laser:1||emission profile:1||HIGHORDER HARMONICS:1||Xray laser:1||atomic transition:1||EXCITATION:1||LASERS:1||PERFORMANCE:1||RELATIVISTIC ELECTRONS:1||BI2O3DOPED ZNO:1||INNERSHELL IONIZATION:1||Laser wakefield:1||FREQUENCY:1||SOLIDSTATE LASERS:1||Linearly polarized:1||THERMIONIC EMISSION:1||PULSE AMPLIFICATION SYSTEM:1||BIB3O6:1||NM:1||NONCOVALENT INTERACTIONS:1||CRYSTALLINE:1||INTENSITY:1||JETS:1||COHERENT:1||LINE:1||ANGULARDISTRIBUTION:1||SILVER IONS:1||magnetic anisotropy:1||DEVICES:1||Auger transitions:1||CosterKronig transitions:1||EFFICIENT:1||ELECTRONIMPACT IONIZATION:1||ULTRASHORTPULSE:1||Nanowire:1||Heterostructure:1||soft Xray reflectivity:1||PLASMA ACCELERATOR:1||ZINCOXIDE NANOWIRES:1||CHEMICALVAPORDEPOSITION:1||Electron acceleration:1||Ionization of gases:1||Delay dependent:1||MULTIPHOTON IONIZATION:1||FRAGMENTATION:1||GASJET:1||ultrafast nonlinear optics:1||CYCLE PULSES:1||KHZ:1||chemical vapor deposition:1||ferromagnetism:1||ABSORPTION:1||TERAHERTZ RADIATION:1||SCIENCE:1||FIELDS:1||ELECTRONS:1||nanomultilayer structures:1||YIELDS:1||AUGER:1||10HZ REPETITION RATE:1||MULTITERAWATT:1||SPECTROGRAPH:1||HIGHHARMONICGENERATION:1||spectroscopy:1||level population:1||PARTICLEACCELERATION:1||OPTICAL FREQUENCYMEASUREMENT:1||NANOWALLS:1||ROOMTEMPERATURE:1||AVERAGE OUTPUT POWER:1||GROUPVELOCITYMISMATCH:1||Impact ionization:1||Dynamics:1||Lasers:1||Collisional process:1||ABOVETHRESHOLD IONIZATION:1||MAINGROUP THERMOCHEMISTRY:1||dilute magnetic semiconductors:1||GACRN:1||SIZE:1||ATTOSECOND:1||Ar cluster:1||Xray astrophysics:1||photoionization:1||irons:1||normal incidence pulsed laser deposition:1||SHELLS:1||Silicon Oxide:1||gaspuff Zpinch:1||Xray:1||soft Xray reflectors:1||ESCAPE:1||ZN2SIO4:1||SILICA:1||Time 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materials:1||MOLECULAR PHOTOIONIZATION:1||LOCALIZATION:1||DEUTERIUM CLUSTERS:1||EXPLOSIONS:1||REGENERATIVE AMPLIFIERS:1||RAREGASES:1||THz radiation:1||FREEELECTRON LASER:1||REALTIME OBSERVATION:1||TARGET:1||photoionized plasmas:1||fs Xray laser:1||emission profile:1||HIGHORDER HARMONICS:1||Xray laser:1||atomic transition:1||EXCITATION:1||LASERS:1||PERFORMANCE:1||RELATIVISTIC ELECTRONS:1||BI2O3DOPED ZNO:1||INNERSHELL IONIZATION:1||Laser wakefield:1||FREQUENCY:1||SOLIDSTATE LASERS:1||Linearly polarized:1||THERMIONIC EMISSION:1||PULSE AMPLIFICATION SYSTEM:1||BIB3O6:1||NM:1||NONCOVALENT INTERACTIONS:1||CRYSTALLINE:1||INTENSITY:1||JETS:1||COHERENT:1||LINE:1||ANGULARDISTRIBUTION:1||SILVER IONS:1||magnetic anisotropy:1||DEVICES:1||Auger transitions:1||CosterKronig transitions:1||EFFICIENT:1||ELECTRONIMPACT IONIZATION:1||ULTRASHORTPULSE:1||Nanowire:1||Heterostructure:1||soft Xray reflectivity:1||PLASMA ACCELERATOR:1||ZINCOXIDE NANOWIRES:1||CHEMICALVAPORDEPOSITION:1||Electron acceleration:1||Ionization of gases:1||Delay dependent:1||MULTIPHOTON IONIZATION:1||FRAGMENTATION:1||GASJET:1||ultrafast nonlinear optics:1||CYCLE PULSES:1||KHZ:1||chemical vapor deposition:1||ferromagnetism:1||ABSORPTION:1||TERAHERTZ RADIATION:1||SCIENCE:1||FIELDS:1||ELECTRONS:1||nanomultilayer structures:1||YIELDS:1||AUGER:1||10HZ REPETITION RATE:1||MULTITERAWATT:1||SPECTROGRAPH:1||HIGHHARMONICGENERATION:1||spectroscopy:1||level population:1||PARTICLEACCELERATION:1||OPTICAL FREQUENCYMEASUREMENT:1||NANOWALLS:1||ROOMTEMPERATURE:1||AVERAGE OUTPUT POWER:1||GROUPVELOCITYMISMATCH:1||Impact ionization:1||Dynamics:1||Lasers:1||Collisional process:1||ABOVETHRESHOLD IONIZATION:1||MAINGROUP THERMOCHEMISTRY:1||dilute magnetic semiconductors:1||GACRN:1||SIZE:1||ATTOSECOND:1||Ar cluster:1||Xray astrophysics:1||photoionization:1||irons:1||normal incidence pulsed laser deposition:1||SHELLS:1||Silicon Oxide:1||gaspuff Zpinch:1||Xray:1||soft Xray reflectors:1||ESCAPE:1||ZN2SIO4:1||SILICA:1||Time delay:1||Collisional plasmas:1||MASSSPECTROMETRY:1||NUCLEARFUSION:1||PARAMETRIC AMPLIFICATION:1||LYING ELECTRONIC STATES:1||ADJUSTABLEPARAMETERS:1||MAGNETICPROPERTIES:1||LIQUIDPHASE EPITAXY:1||CEP laser:1||REGION:1||Plasma waveguide:1||AMBIENT GAS:1||DEPOSITION:1||HARMONICGENERATION:1||ENHANCEMENT:1||imaging spectrometer:1||Abel inversion:1||Water window:1||Liquid nitrogen jet:1||CHARGEEXCHANGE:1||NOBEL LECTURE:1||VARISTOR:1||EPITAXY:1||THINDISK LASER:1||HIGHREPETITIONRATE:1||Atom lasers:1||Electronimpact excitation:1||High order harmonics:1||ultrafast technology:1||PEAK POWER:1||CHARGED ALUMINUM CLUSTERS:1||GaN:1||THIN:1||Electron beam:1||INTENSE:1||Hard Xray pulse generation:1||NONLINEAR THOMSON SCATTERING:1||MULTILAYER:1||UVvisible spectrometer:1||ATOMS:1||innershell transitions:1||CORRECTED CONCAVE GRATINGS:1||DISCHARGE:1||LASERPLASMA:1||thin film:1||reflectivity:1||opacity:1||gain:1||smallangle Xray scattering:1||SOFTXRAY:1||ZINCOXIDE:1||CYGNUSX3:1||Betatron oscillation:1||ACCELERATOR:1||STRAINEDLAYER SUPERLATTICES:1||OPTICAL PARAMETRIC AMPLIFICATION:1||PASSIVE MODELOCKING:1||Collision dynamics:1||MUM:1||EXACTEXCHANGE:1||BASISSET:1||APPROXIMATION:1||OXYNITRIDES:1||Beam energy modulation:1||polarization spectroscopy:1||REORIENTATION TRANSITION:1||DEPENDENCE:1||sulfurs:1||BUILDINGBLOCKS:1||RATES:1||OPTICAL PULSES:1||toroidal mirror:1||XRAY LASER:1||CALCIUM:1||radially polarized laser:1||GRAINBOUNDARIES:1||VAPORDEPOSITION:1||Xray generation:1||MAGNETIZATION:1||Electric excitation:1||Laserinduced gas plasmas:1||Qualitative analysis:1||SCHEME:1||RADIATION:10||PULSES:8||PHOTOLUMINESCENCE:7||LASER:7||GENERATION:6||NANORODS:6||GROWTH:6||NANOWIRES:5||IMPLANTED GAN:5||SPECTROSCOPY:5||THINFILMS:4||DYNAMICS:4||SILICON:4||EXTREMEULTRAVIOLET:4||AMPLIFICATION:4||PRESSURE:4||PHASE:4||OPTICALPROPERTIES:4||SYSTEM:4||EMISSION:4||FEL:3||N2O:3||FILMS:3||OPTICS:3||SPECTRA:3||FIELD:3||MIRRORS:3||ARRAYS:3||CLUSTERS:3||SIO2:3||IONIZATION:3||VACUUM:3||SCATTERING:3||IONS:2||LUMINESCENCE PROPERTIES:2||ANISOTROPY:2||BEAMS:2||DIFFRACTION:2||DISPERSION:2||chemical vapor deposition (CVD):2||ELECTRONICSTRUCTURE:2||MOSFETS:2||SI3N4:2||DENSITY:2||LIGHT:2||PLASMAS:2||MATTER:2||nanocomposites:2||RAMANSCATTERING:2||NANOPARTICLES:2||OXIDE:2||AMPLIFIED SPONTANEOUS EMISSION:2||NM WAVELENGTH:2||GAIN:2||CARBON NANOTUBES:2||CROSSSECTIONS:2||LIGHTEMITTINGDIODES:2||PULSE:2||CARBON PLASMA:2||TISAPPHIRE LASER:2||Raman scattering:2||ROUTE:2||multilayer:2||CATHODOLUMINESCENCE:2||highresolution transmission electronic microscope (HRTEM):2||DIFFERENCEFREQUENCYGENERATION:2||CRYSTAL:2||laserproduced plasma:2||NANOCABLES:2||photoluminescence:2||MAGNETIC ALLOY SEMICONDUCTORS:2||MOLECULARBEAM EPITAXY:2||EARTHDOPED GAN:2||LASER FIELDS:2||CHIRPEDPULSEAMPLIFICATION:2||ALN:2||GAUSSIANBEAM:2||ASSISTED CATALYTIC GROWTH:2||BLUE:2||NANOSTRUCTURES:2||MAGNETOELECTRONICS:2||MICROSCOPY:2||ELECTROLUMINESCENCE:2||LASERPULSES:2||GaN nanowires:2||GALLIUM NITRIDE NANOWIRES:2||GAMNN:2||NANOTUBES:2||PHYSICS:2||Femtosecond laser:2||parametric oscillators and amplifiers:1||ultrafast lasers:1||VALENCE:1||nanowires:1||DILUTED MAGNETIC SEMICONDUCTOR:1||LUMINESCENCE:1||Density modulation:1||Energy modulation:1||Current enhanced SASE free electron laser:1||Undulator radiation:1||FREEELECTRON LASERS:1||ULTRATHIN FERROMAGNETICFILMS:1||OXIDEFILMS:1||ABLATION:1||COMPONENT:1||METAL:1||innershell excited states:1||Nelike ions:1||TRANSITIONS:1||XUV spectrometer:1||DIAGNOSTICS:1||Xray scattering:1||MO/SI:1||pulsed laser deposition:1||KEV IMPACT ENERGIES:1||vacuum electron acceleration:1||HIGHINTENSITY LASER:1||JUNCTIONS:1||LOWTEMPERATURE GROWTH:1||nanocrystalline materials:1||MOLECULAR PHOTOIONIZATION:1||LOCALIZATION:1||DEUTERIUM CLUSTERS:1||EXPLOSIONS:1||REGENERATIVE AMPLIFIERS:1||RAREGASES:1||THz radiation:1||FREEELECTRON LASER:1||REALTIME OBSERVATION:1||TARGET:1||photoionized plasmas:1||fs Xray laser:1||emission profile:1||HIGHORDER HARMONICS:1||Xray laser:1||atomic transition:1||EXCITATION:1||LASERS:1||PERFORMANCE:1||RELATIVISTIC ELECTRONS:1||BI2O3DOPED ZNO:1||INNERSHELL IONIZATION:1||Laser wakefield:1||FREQUENCY:1||SOLIDSTATE LASERS:1||Linearly polarized:1||THERMIONIC EMISSION:1||PULSE AMPLIFICATION SYSTEM:1||BIB3O6:1||NM:1||NONCOVALENT INTERACTIONS:1||CRYSTALLINE:1||INTENSITY:1||JETS:1||COHERENT:1||LINE:1||ANGULARDISTRIBUTION:1||SILVER IONS:1||magnetic anisotropy:1||DEVICES:1||Auger transitions:1||CosterKronig transitions:1||EFFICIENT:1||ELECTRONIMPACT IONIZATION:1||ULTRASHORTPULSE:1||Nanowire:1||Heterostructure:1||soft Xray reflectivity:1||PLASMA ACCELERATOR:1||ZINCOXIDE NANOWIRES:1||CHEMICALVAPORDEPOSITION:1||Electron acceleration:1||Ionization of gases:1||Delay dependent:1||MULTIPHOTON IONIZATION:1||FRAGMENTATION:1||GASJET:1||ultrafast nonlinear optics:1||CYCLE PULSES:1||KHZ:1||chemical vapor deposition:1||ferromagnetism:1||ABSORPTION:1||TERAHERTZ RADIATION:1||SCIENCE:1||FIELDS:1||ELECTRONS:1||nanomultilayer structures:1||YIELDS:1||AUGER:1||10HZ REPETITION RATE:1||MULTITERAWATT:1||SPECTROGRAPH:1||HIGHHARMONICGENERATION:1||spectroscopy:1||level population:1||PARTICLEACCELERATION:1||OPTICAL FREQUENCYMEASUREMENT:1||NANOWALLS:1||ROOMTEMPERATURE:1||AVERAGE OUTPUT POWER:1||GROUPVELOCITYMISMATCH:1||Impact ionization:1||Dynamics:1||Lasers:1||Collisional process:1||ABOVETHRESHOLD IONIZATION:1||MAINGROUP THERMOCHEMISTRY:1||dilute magnetic semiconductors:1||GACRN:1||SIZE:1||ATTOSECOND:1||Ar cluster:1||Xray astrophysics:1||photoionization:1||irons:1||normal incidence pulsed laser deposition:1||SHELLS:1||Silicon Oxide:1||gaspuff Zpinch:1||Xray:1||soft Xray reflectors:1||ESCAPE:1||ZN2SIO4:1||SILICA:1||Time delay:1||Collisional plasmas:1||MASSSPECTROMETRY:1||NUCLEARFUSION:1||PARAMETRIC AMPLIFICATION:1||LYING ELECTRONIC STATES:1||ADJUSTABLEPARAMETERS:1||MAGNETICPROPERTIES:1||LIQUIDPHASE EPITAXY:1||CEP laser:1||REGION:1||Plasma waveguide:1||AMBIENT GAS:1||DEPOSITION:1||HARMONICGENERATION:1||ENHANCEMENT:1||imaging spectrometer:1||Abel inversion:1||Water window:1||Liquid nitrogen jet:1||CHARGEEXCHANGE:1||NOBEL LECTURE:1||VARISTOR:1||EPITAXY:1||THINDISK LASER:1||HIGHREPETITIONRATE:1||Atom lasers:1||Electronimpact excitation:1||High order harmonics:1||ultrafast technology:1||PEAK POWER:1||CHARGED ALUMINUM CLUSTERS:1||GaN:1||THIN:1||Electron beam:1||INTENSE:1||Hard Xray pulse generation:1||NONLINEAR THOMSON SCATTERING:1||MULTILAYER:1||UVvisible spectrometer:1||ATOMS:1||innershell transitions:1||CORRECTED CONCAVE GRATINGS:1||DISCHARGE:1||LASERPLASMA:1||thin film:1||reflectivity:1||opacity:1||gain:1||smallangle Xray scattering:1||SOFTXRAY:1||ZINCOXIDE:1||CYGNUSX3:1||Betatron oscillation:1||ACCELERATOR:1||STRAINEDLAYER SUPERLATTICES:1||OPTICAL PARAMETRIC AMPLIFICATION:1||PASSIVE MODELOCKING:1||Collision dynamics:1||MUM:1||EXACTEXCHANGE:1||BASISSET:1||APPROXIMATION:1||OXYNITRIDES:1||Beam energy modulation:1||polarization spectroscopy:1||REORIENTATION TRANSITION:1||DEPENDENCE:1||sulfurs:1||BUILDINGBLOCKS:1||RATES:1||OPTICAL PULSES:1||toroidal mirror:1||XRAY LASER:1||CALCIUM:1||radially polarized laser:1||GRAINBOUNDARIES:1||VAPORDEPOSITION:1||Xray generation:1||MAGNETIZATION:1||Electric excitation:1||Laserinduced gas plasmas:1||Qualitative analysis:1||SCHEME:1||RADIATION:10||PULSES:8||PHOTOLUMINESCENCE:7||LASER:7||GENERATION:6||NANORODS:6||GROWTH:6||NANOWIRES:5||IMPLANTED 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SEMICONDUCTORS:2||MOLECULARBEAM EPITAXY:2||EARTHDOPED GAN:2||LASER FIELDS:2||CHIRPEDPULSEAMPLIFICATION:2||ALN:2||GAUSSIANBEAM:2||ASSISTED CATALYTIC GROWTH:2||BLUE:2||NANOSTRUCTURES:2||MAGNETOELECTRONICS:2||MICROSCOPY:2||ELECTROLUMINESCENCE:2||LASERPULSES:2||GaN nanowires:2||GALLIUM NITRIDE NANOWIRES:2||GAMNN:2||NANOTUBES:2||PHYSICS:2||Femtosecond laser:2||parametric oscillators and amplifiers:1||ultrafast lasers:1||VALENCE:1||nanowires:1||DILUTED MAGNETIC SEMICONDUCTOR:1||LUMINESCENCE:1||Density modulation:1||Energy modulation:1||Current enhanced SASE free electron laser:1||Undulator radiation:1||FREEELECTRON LASERS:1||ULTRATHIN FERROMAGNETICFILMS:1||OXIDEFILMS:1||ABLATION:1||COMPONENT:1||METAL:1||innershell excited states:1||Nelike ions:1||TRANSITIONS:1||XUV spectrometer:1||DIAGNOSTICS:1||Xray scattering:1||MO/SI:1||pulsed laser deposition:1||KEV IMPACT ENERGIES:1||vacuum electron acceleration:1||HIGHINTENSITY LASER:1||JUNCTIONS:1||LOWTEMPERATURE GROWTH:1||nanocrystalline materials:1||MOLECULAR PHOTOIONIZATION:1||LOCALIZATION:1||DEUTERIUM CLUSTERS:1||EXPLOSIONS:1||REGENERATIVE AMPLIFIERS:1||RAREGASES:1||THz radiation:1||FREEELECTRON LASER:1||REALTIME OBSERVATION:1||TARGET:1||photoionized plasmas:1||fs Xray laser:1||emission profile:1||HIGHORDER HARMONICS:1||Xray laser:1||atomic transition:1||EXCITATION:1||LASERS:1||PERFORMANCE:1||RELATIVISTIC ELECTRONS:1||BI2O3DOPED ZNO:1||INNERSHELL IONIZATION:1||Laser wakefield:1||FREQUENCY:1||SOLIDSTATE LASERS:1||Linearly polarized:1||THERMIONIC EMISSION:1||PULSE AMPLIFICATION SYSTEM:1||BIB3O6:1||NM:1||NONCOVALENT INTERACTIONS:1||CRYSTALLINE:1||INTENSITY:1||JETS:1||COHERENT:1||LINE:1||ANGULARDISTRIBUTION:1||SILVER IONS:1||magnetic anisotropy:1||DEVICES:1||Auger transitions:1||CosterKronig transitions:1||EFFICIENT:1||ELECTRONIMPACT IONIZATION:1||ULTRASHORTPULSE:1||Nanowire:1||Heterostructure:1||soft Xray reflectivity:1||PLASMA ACCELERATOR:1||ZINCOXIDE NANOWIRES:1||CHEMICALVAPORDEPOSITION:1||Electron acceleration:1||Ionization of gases:1||Delay dependent:1||MULTIPHOTON IONIZATION:1||FRAGMENTATION:1||GASJET:1||ultrafast nonlinear optics:1||CYCLE PULSES:1||KHZ:1||chemical vapor deposition:1||ferromagnetism:1||ABSORPTION:1||TERAHERTZ RADIATION:1||SCIENCE:1||FIELDS:1||ELECTRONS:1||nanomultilayer structures:1||YIELDS:1||AUGER:1||10HZ REPETITION RATE:1||MULTITERAWATT:1||SPECTROGRAPH:1||HIGHHARMONICGENERATION:1||spectroscopy:1||level population:1||PARTICLEACCELERATION:1||OPTICAL FREQUENCYMEASUREMENT:1||NANOWALLS:1||ROOMTEMPERATURE:1||AVERAGE OUTPUT POWER:1||GROUPVELOCITYMISMATCH:1||Impact ionization:1||Dynamics:1||Lasers:1||Collisional process:1||ABOVETHRESHOLD IONIZATION:1||MAINGROUP THERMOCHEMISTRY:1||dilute magnetic semiconductors:1||GACRN:1||SIZE:1||ATTOSECOND:1||Ar cluster:1||Xray astrophysics:1||photoionization:1||irons:1||normal incidence pulsed laser deposition:1||SHELLS:1||Silicon Oxide:1||gaspuff Zpinch:1||Xray:1||soft Xray reflectors:1||ESCAPE:1||ZN2SIO4:1||SILICA:1||Time 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materials:1||MOLECULAR PHOTOIONIZATION:1||LOCALIZATION:1||DEUTERIUM CLUSTERS:1||EXPLOSIONS:1||REGENERATIVE AMPLIFIERS:1||RAREGASES:1||THz radiation:1||FREEELECTRON LASER:1||REALTIME OBSERVATION:1||TARGET:1||photoionized plasmas:1||fs Xray laser:1||emission profile:1||HIGHORDER HARMONICS:1||Xray laser:1||atomic transition:1||EXCITATION:1||LASERS:1||PERFORMANCE:1||RELATIVISTIC ELECTRONS:1||BI2O3DOPED ZNO:1||INNERSHELL IONIZATION:1||Laser wakefield:1||FREQUENCY:1||SOLIDSTATE LASERS:1||Linearly polarized:1||THERMIONIC EMISSION:1||PULSE AMPLIFICATION SYSTEM:1||BIB3O6:1||NM:1||NONCOVALENT INTERACTIONS:1||CRYSTALLINE:1||INTENSITY:1||JETS:1||COHERENT:1||LINE:1||ANGULARDISTRIBUTION:1||SILVER IONS:1||magnetic anisotropy:1||DEVICES:1||Auger transitions:1||CosterKronig transitions:1||EFFICIENT:1||ELECTRONIMPACT IONIZATION:1||ULTRASHORTPULSE:1||Nanowire:1||Heterostructure:1||soft Xray reflectivity:1||PLASMA ACCELERATOR:1||ZINCOXIDE NANOWIRES:1||CHEMICALVAPORDEPOSITION:1||Electron acceleration:1||Ionization of gases:1||Delay dependent:1||MULTIPHOTON IONIZATION:1||FRAGMENTATION:1||GASJET:1||ultrafast nonlinear optics:1||CYCLE PULSES:1||KHZ:1||chemical vapor deposition:1||ferromagnetism:1||ABSORPTION:1||TERAHERTZ RADIATION:1||SCIENCE:1||FIELDS:1||ELECTRONS:1||nanomultilayer structures:1||YIELDS:1||AUGER:1||10HZ REPETITION RATE:1||MULTITERAWATT:1||SPECTROGRAPH:1||HIGHHARMONICGENERATION:1||spectroscopy:1||level population:1||PARTICLEACCELERATION:1||OPTICAL FREQUENCYMEASUREMENT:1||NANOWALLS:1||ROOMTEMPERATURE:1||AVERAGE OUTPUT POWER:1||GROUPVELOCITYMISMATCH:1||Impact ionization:1||Dynamics:1||Lasers:1||Collisional process:1||ABOVETHRESHOLD IONIZATION:1||MAINGROUP THERMOCHEMISTRY:1||dilute magnetic semiconductors:1||GACRN:1||SIZE:1||ATTOSECOND:1||Ar cluster:1||Xray astrophysics:1||photoionization:1||irons:1||normal incidence pulsed laser deposition:1||SHELLS:1||Silicon Oxide:1||gaspuff Zpinch:1||Xray:1||soft Xray reflectors:1||ESCAPE:1||ZN2SIO4:1||SILICA:1||Time delay:1||Collisional plasmas:1||MASSSPECTROMETRY:1||NUCLEARFUSION:1||PARAMETRIC AMPLIFICATION:1||LYING ELECTRONIC STATES:1||ADJUSTABLEPARAMETERS:1||MAGNETICPROPERTIES:1||LIQUIDPHASE EPITAXY:1||CEP laser:1||REGION:1||Plasma waveguide:1||AMBIENT GAS:1||DEPOSITION:1||HARMONICGENERATION:1||ENHANCEMENT:1||imaging spectrometer:1||Abel inversion:1||Water window:1||Liquid nitrogen jet:1||CHARGEEXCHANGE:1||NOBEL LECTURE:1||VARISTOR:1||EPITAXY:1||THINDISK LASER:1||HIGHREPETITIONRATE:1||Atom lasers:1||Electronimpact excitation:1||High order harmonics:1||ultrafast technology:1||PEAK POWER:1||CHARGED ALUMINUM CLUSTERS:1||GaN:1||THIN:1||Electron beam:1||INTENSE:1||Hard Xray pulse generation:1||NONLINEAR THOMSON SCATTERING:1||MULTILAYER:1||UVvisible spectrometer:1||ATOMS:1||innershell transitions:1||CORRECTED CONCAVE GRATINGS:1||DISCHARGE:1||LASERPLASMA:1||thin film:1||reflectivity:1||opacity:1||gain:1||smallangle Xray scattering:1||SOFTXRAY:1||ZINCOXIDE:1||CYGNUSX3:1||Betatron oscillation:1||ACCELERATOR:1||STRAINEDLAYER SUPERLATTICES:1||OPTICAL PARAMETRIC AMPLIFICATION:1||PASSIVE MODELOCKING:1||Collision dynamics:1||MUM:1||EXACTEXCHANGE:1||BASISSET:1||APPROXIMATION:1||OXYNITRIDES:1||Beam energy modulation:1||polarization spectroscopy:1||REORIENTATION TRANSITION:1||DEPENDENCE:1||sulfurs:1||BUILDINGBLOCKS:1||RATES:1||OPTICAL PULSES:1||toroidal mirror:1||XRAY LASER:1||CALCIUM:1||radially polarized laser:1||GRAINBOUNDARIES:1||VAPORDEPOSITION:1||Xray generation:1||MAGNETIZATION:1||Electric excitation:1||Laserinduced gas plasmas:1||Qualitative analysis:1||SCHEME:1||RADIATION:10||PULSES:8||PHOTOLUMINESCENCE:7||LASER:7||GENERATION:6||NANORODS:6||GROWTH:6||NANOWIRES:5||IMPLANTED GAN:5||SPECTROSCOPY:5||THINFILMS:4||DYNAMICS:4||SILICON:4||EXTREMEULTRAVIOLET:4||AMPLIFICATION:4||PRESSURE:4||PHASE:4||OPTICALPROPERTIES:4||SYSTEM:4||EMISSION:4||FEL:3||N2O:3||FILMS:3||OPTICS:3||SPECTRA:3||FIELD:3||MIRRORS:3||ARRAYS:3||CLUSTERS:3||SIO2:3||IONIZATION:3||VACUUM:3||SCATTERING:3||IONS:2||LUMINESCENCE PROPERTIES:2||ANISOTROPY:2||BEAMS:2||DIFFRACTION:2||DISPERSION:2||chemical vapor deposition (CVD):2||ELECTRONICSTRUCTURE:2||MOSFETS:2||SI3N4:2||DENSITY:2||LIGHT:2||PLASMAS:2||MATTER:2||nanocomposites:2||RAMANSCATTERING:2||NANOPARTICLES:2||OXIDE:2||AMPLIFIED SPONTANEOUS EMISSION:2||NM WAVELENGTH:2||GAIN:2||CARBON NANOTUBES:2||CROSSSECTIONS:2||LIGHTEMITTINGDIODES:2||PULSE:2||CARBON PLASMA:2||TISAPPHIRE LASER:2||Raman scattering:2||ROUTE:2||multilayer:2||CATHODOLUMINESCENCE:2||highresolution transmission electronic microscope (HRTEM):2||DIFFERENCEFREQUENCYGENERATION:2||CRYSTAL:2||laserproduced plasma:2||NANOCABLES:2||photoluminescence:2||MAGNETIC ALLOY SEMICONDUCTORS:2||MOLECULARBEAM EPITAXY:2||EARTHDOPED GAN:2||LASER FIELDS:2||CHIRPEDPULSEAMPLIFICATION:2||ALN:2||GAUSSIANBEAM:2||ASSISTED CATALYTIC GROWTH:2||BLUE:2||NANOSTRUCTURES:2||MAGNETOELECTRONICS:2||MICROSCOPY:2||ELECTROLUMINESCENCE:2||LASERPULSES:2||GaN nanowires:2||GALLIUM NITRIDE NANOWIRES:2||GAMNN:2||NANOTUBES:2||PHYSICS:2||Femtosecond laser:2||parametric oscillators and amplifiers:1||ultrafast lasers:1||VALENCE:1||nanowires:1||DILUTED MAGNETIC SEMICONDUCTOR:1||LUMINESCENCE:1||Density modulation:1||Energy modulation:1||Current enhanced SASE free electron laser:1||Undulator radiation:1||FREEELECTRON LASERS:1||ULTRATHIN FERROMAGNETICFILMS:1||OXIDEFILMS:1||ABLATION:1||COMPONENT:1||METAL:1||innershell excited states:1||Nelike ions:1||TRANSITIONS:1||XUV spectrometer:1||DIAGNOSTICS:1||Xray scattering:1||MO/SI:1||pulsed laser deposition:1||KEV IMPACT ENERGIES:1||vacuum electron acceleration:1||HIGHINTENSITY LASER:1||JUNCTIONS:1||LOWTEMPERATURE GROWTH:1||nanocrystalline materials:1||MOLECULAR PHOTOIONIZATION:1||LOCALIZATION:1||DEUTERIUM CLUSTERS:1||EXPLOSIONS:1||REGENERATIVE AMPLIFIERS:1||RAREGASES:1||THz radiation:1||FREEELECTRON LASER:1||REALTIME OBSERVATION:1||TARGET:1||photoionized plasmas:1||fs Xray laser:1||emission profile:1||HIGHORDER HARMONICS:1||Xray laser:1||atomic transition:1||EXCITATION:1||LASERS:1||PERFORMANCE:1||RELATIVISTIC ELECTRONS:1||BI2O3DOPED ZNO:1||INNERSHELL IONIZATION:1||Laser wakefield:1||FREQUENCY:1||SOLIDSTATE LASERS:1||Linearly polarized:1||THERMIONIC EMISSION:1||PULSE AMPLIFICATION SYSTEM:1||BIB3O6:1||NM:1||NONCOVALENT INTERACTIONS:1||CRYSTALLINE:1||INTENSITY:1||JETS:1||COHERENT:1||LINE:1||ANGULARDISTRIBUTION:1||SILVER IONS:1||magnetic anisotropy:1||DEVICES:1||Auger transitions:1||CosterKronig transitions:1||EFFICIENT:1||ELECTRONIMPACT IONIZATION:1||ULTRASHORTPULSE:1||Nanowire:1||Heterostructure:1||soft Xray reflectivity:1||PLASMA ACCELERATOR:1||ZINCOXIDE NANOWIRES:1||CHEMICALVAPORDEPOSITION:1||Electron acceleration:1||Ionization of gases:1||Delay dependent:1||MULTIPHOTON IONIZATION:1||FRAGMENTATION:1||GASJET:1||ultrafast nonlinear optics:1||CYCLE PULSES:1||KHZ:1||chemical vapor deposition:1||ferromagnetism:1||ABSORPTION:1||TERAHERTZ RADIATION:1||SCIENCE:1||FIELDS:1||ELECTRONS:1||nanomultilayer structures:1||YIELDS:1||AUGER:1||10HZ REPETITION RATE:1||MULTITERAWATT:1||SPECTROGRAPH:1||HIGHHARMONICGENERATION:1||spectroscopy:1||level population:1||PARTICLEACCELERATION:1||OPTICAL FREQUENCYMEASUREMENT:1||NANOWALLS:1||ROOMTEMPERATURE:1||AVERAGE OUTPUT POWER:1||GROUPVELOCITYMISMATCH:1||Impact ionization:1||Dynamics:1||Lasers:1||Collisional process:1||ABOVETHRESHOLD IONIZATION:1||MAINGROUP THERMOCHEMISTRY:1||dilute magnetic semiconductors:1||GACRN:1||SIZE:1||ATTOSECOND:1||Ar cluster:1||Xray astrophysics:1||photoionization:1||irons:1||normal incidence pulsed laser deposition:1||SHELLS:1||Silicon Oxide:1||gaspuff Zpinch:1||Xray:1||soft Xray reflectors:1||ESCAPE:1||ZN2SIO4:1||SILICA:1||Time delay:1||Collisional plasmas:1||MASSSPECTROMETRY:1||NUCLEARFUSION:1||PARAMETRIC AMPLIFICATION:1||LYING ELECTRONIC STATES:1||ADJUSTABLEPARAMETERS:1||MAGNETICPROPERTIES:1||LIQUIDPHASE EPITAXY:1||CEP laser:1||REGION:1||Plasma waveguide:1||AMBIENT GAS:1||DEPOSITION:1||HARMONICGENERATION:1||ENHANCEMENT:1||imaging spectrometer:1||Abel inversion:1||Water window:1||Liquid nitrogen jet:1||CHARGEEXCHANGE:1||NOBEL LECTURE:1||VARISTOR:1||EPITAXY:1||THINDISK LASER:1||HIGHREPETITIONRATE:1||Atom lasers:1||Electronimpact excitation:1||High order harmonics:1||ultrafast technology:1||PEAK POWER:1||CHARGED ALUMINUM CLUSTERS:1||GaN:1||THIN:1||Electron beam:1||INTENSE:1||Hard Xray pulse generation:1||NONLINEAR THOMSON SCATTERING:1||MULTILAYER:1||UVvisible spectrometer:1||ATOMS:1||innershell transitions:1||CORRECTED CONCAVE GRATINGS:1||DISCHARGE:1||LASERPLASMA:1||thin film:1||reflectivity:1||opacity:1||gain:1||smallangle Xray scattering:1||SOFTXRAY:1||ZINCOXIDE:1||CYGNUSX3:1||Betatron oscillation:1||ACCELERATOR:1||STRAINEDLAYER SUPERLATTICES:1||OPTICAL PARAMETRIC AMPLIFICATION:1||PASSIVE MODELOCKING:1||Collision dynamics:1||MUM:1||EXACTEXCHANGE:1||BASISSET:1||APPROXIMATION:1||OXYNITRIDES:1||Beam energy modulation:1||polarization spectroscopy:1||REORIENTATION TRANSITION:1||DEPENDENCE:1||sulfurs:1||BUILDINGBLOCKS:1||RATES:1||OPTICAL PULSES:1||toroidal mirror:1||XRAY LASER:1||CALCIUM:1||radially polarized laser:1||GRAINBOUNDARIES:1||VAPORDEPOSITION:1||Xray generation:1||MAGNETIZATION:1||Electric excitation:1||Laserinduced gas plasmas:1||Qualitative analysis:1||SCHEME:1||RADIATION:10||PULSES:8||PHOTOLUMINESCENCE:7||LASER:7||GENERATION:6||NANORODS:6||GROWTH:6||NANOWIRES:5||IMPLANTED 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SEMICONDUCTORS:2||MOLECULARBEAM EPITAXY:2||EARTHDOPED GAN:2||LASER FIELDS:2||CHIRPEDPULSEAMPLIFICATION:2||ALN:2||GAUSSIANBEAM:2||ASSISTED CATALYTIC GROWTH:2||BLUE:2||NANOSTRUCTURES:2||MAGNETOELECTRONICS:2||MICROSCOPY:2||ELECTROLUMINESCENCE:2||LASERPULSES:2||GaN nanowires:2||GALLIUM NITRIDE NANOWIRES:2||GAMNN:2||NANOTUBES:2||PHYSICS:2||Femtosecond laser:2||parametric oscillators and amplifiers:1||ultrafast lasers:1||VALENCE:1||nanowires:1||DILUTED MAGNETIC SEMICONDUCTOR:1||LUMINESCENCE:1||Density modulation:1||Energy modulation:1||Current enhanced SASE free electron laser:1||Undulator radiation:1||FREEELECTRON LASERS:1||ULTRATHIN FERROMAGNETICFILMS:1||OXIDEFILMS:1||ABLATION:1||COMPONENT:1||METAL:1||innershell excited states:1||Nelike ions:1||TRANSITIONS:1||XUV spectrometer:1||DIAGNOSTICS:1||Xray scattering:1||MO/SI:1||pulsed laser deposition:1||KEV IMPACT ENERGIES:1||vacuum electron acceleration:1||HIGHINTENSITY LASER:1||JUNCTIONS:1||LOWTEMPERATURE GROWTH:1||nanocrystalline materials:1||MOLECULAR PHOTOIONIZATION:1||LOCALIZATION:1||DEUTERIUM CLUSTERS:1||EXPLOSIONS:1||REGENERATIVE AMPLIFIERS:1||RAREGASES:1||THz radiation:1||FREEELECTRON LASER:1||REALTIME OBSERVATION:1||TARGET:1||photoionized plasmas:1||fs Xray laser:1||emission profile:1||HIGHORDER HARMONICS:1||Xray laser:1||atomic transition:1||EXCITATION:1||LASERS:1||PERFORMANCE:1||RELATIVISTIC ELECTRONS:1||BI2O3DOPED ZNO:1||INNERSHELL IONIZATION:1||Laser wakefield:1||FREQUENCY:1||SOLIDSTATE LASERS:1||Linearly polarized:1||THERMIONIC EMISSION:1||PULSE AMPLIFICATION SYSTEM:1||BIB3O6:1||NM:1||NONCOVALENT INTERACTIONS:1||CRYSTALLINE:1||INTENSITY:1||JETS:1||COHERENT:1||LINE:1||ANGULARDISTRIBUTION:1||SILVER IONS:1||magnetic anisotropy:1||DEVICES:1||Auger transitions:1||CosterKronig transitions:1||EFFICIENT:1||ELECTRONIMPACT IONIZATION:1||ULTRASHORTPULSE:1||Nanowire:1||Heterostructure:1||soft Xray reflectivity:1||PLASMA ACCELERATOR:1||ZINCOXIDE NANOWIRES:1||CHEMICALVAPORDEPOSITION:1||Electron acceleration:1||Ionization of gases:1||Delay dependent:1||MULTIPHOTON IONIZATION:1||FRAGMENTATION:1||GASJET:1||ultrafast nonlinear optics:1||CYCLE PULSES:1||KHZ:1||chemical vapor deposition:1||ferromagnetism:1||ABSORPTION:1||TERAHERTZ RADIATION:1||SCIENCE:1||FIELDS:1||ELECTRONS:1||nanomultilayer structures:1||YIELDS:1||AUGER:1||10HZ REPETITION RATE:1||MULTITERAWATT:1||SPECTROGRAPH:1||HIGHHARMONICGENERATION:1||spectroscopy:1||level population:1||PARTICLEACCELERATION:1||OPTICAL FREQUENCYMEASUREMENT:1||NANOWALLS:1||ROOMTEMPERATURE:1||AVERAGE OUTPUT POWER:1||GROUPVELOCITYMISMATCH:1||Impact ionization:1||Dynamics:1||Lasers:1||Collisional process:1||ABOVETHRESHOLD IONIZATION:1||MAINGROUP THERMOCHEMISTRY:1||dilute magnetic semiconductors:1||GACRN:1||SIZE:1||ATTOSECOND:1||Ar cluster:1||Xray astrophysics:1||photoionization:1||irons:1||normal incidence pulsed laser deposition:1||SHELLS:1||Silicon Oxide:1||gaspuff Zpinch:1||Xray:1||soft Xray reflectors:1||ESCAPE:1||ZN2SIO4:1||SILICA:1||Time 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materials:1||MOLECULAR PHOTOIONIZATION:1||LOCALIZATION:1||DEUTERIUM CLUSTERS:1||EXPLOSIONS:1||REGENERATIVE AMPLIFIERS:1||RAREGASES:1||THz radiation:1||FREEELECTRON LASER:1||REALTIME OBSERVATION:1||TARGET:1||photoionized plasmas:1||fs Xray laser:1||emission profile:1||HIGHORDER HARMONICS:1||Xray laser:1||atomic transition:1||EXCITATION:1||LASERS:1||PERFORMANCE:1||RELATIVISTIC ELECTRONS:1||BI2O3DOPED ZNO:1||INNERSHELL IONIZATION:1||Laser wakefield:1||FREQUENCY:1||SOLIDSTATE LASERS:1||Linearly polarized:1||THERMIONIC EMISSION:1||PULSE AMPLIFICATION SYSTEM:1||BIB3O6:1||NM:1||NONCOVALENT INTERACTIONS:1||CRYSTALLINE:1||INTENSITY:1||JETS:1||COHERENT:1||LINE:1||ANGULARDISTRIBUTION:1||SILVER IONS:1||magnetic anisotropy:1||DEVICES:1||Auger transitions:1||CosterKronig transitions:1||EFFICIENT:1||ELECTRONIMPACT IONIZATION:1||ULTRASHORTPULSE:1||Nanowire:1||Heterostructure:1||soft Xray reflectivity:1||PLASMA ACCELERATOR:1||ZINCOXIDE NANOWIRES:1||CHEMICALVAPORDEPOSITION:1||Electron acceleration:1||Ionization of gases:1||Delay dependent:1||MULTIPHOTON IONIZATION:1||FRAGMENTATION:1||GASJET:1||ultrafast nonlinear optics:1||CYCLE PULSES:1||KHZ:1||chemical vapor deposition:1||ferromagnetism:1||ABSORPTION:1||TERAHERTZ RADIATION:1||SCIENCE:1||FIELDS:1||ELECTRONS:1||nanomultilayer structures:1||YIELDS:1||AUGER:1||10HZ REPETITION RATE:1||MULTITERAWATT:1||SPECTROGRAPH:1||HIGHHARMONICGENERATION:1||spectroscopy:1||level population:1||PARTICLEACCELERATION:1||OPTICAL FREQUENCYMEASUREMENT:1||NANOWALLS:1||ROOMTEMPERATURE:1||AVERAGE OUTPUT POWER:1||GROUPVELOCITYMISMATCH:1||Impact ionization:1||Dynamics:1||Lasers:1||Collisional process:1||ABOVETHRESHOLD IONIZATION:1||MAINGROUP THERMOCHEMISTRY:1||dilute magnetic semiconductors:1||GACRN:1||SIZE:1||ATTOSECOND:1||Ar cluster:1||Xray astrophysics:1||photoionization:1||irons:1||normal incidence pulsed laser deposition:1||SHELLS:1||Silicon Oxide:1||gaspuff Zpinch:1||Xray:1||soft Xray reflectors:1||ESCAPE:1||ZN2SIO4:1||SILICA:1||Time delay:1||Collisional plasmas:1||MASSSPECTROMETRY:1||NUCLEARFUSION:1||PARAMETRIC AMPLIFICATION:1||LYING ELECTRONIC STATES:1||ADJUSTABLEPARAMETERS:1||MAGNETICPROPERTIES:1||LIQUIDPHASE EPITAXY:1||CEP laser:1||REGION:1||Plasma waveguide:1||AMBIENT GAS:1||DEPOSITION:1||HARMONICGENERATION:1||ENHANCEMENT:1||imaging spectrometer:1||Abel inversion:1||Water window:1||Liquid nitrogen jet:1||CHARGEEXCHANGE:1||NOBEL LECTURE:1||VARISTOR:1||EPITAXY:1||THINDISK LASER:1||HIGHREPETITIONRATE:1||Atom lasers:1||Electronimpact excitation:1||High order harmonics:1||ultrafast technology:1||PEAK POWER:1||CHARGED ALUMINUM CLUSTERS:1||GaN:1||THIN:1||Electron beam:1||INTENSE:1||Hard Xray pulse generation:1||NONLINEAR THOMSON SCATTERING:1||MULTILAYER:1||UVvisible spectrometer:1||ATOMS:1||innershell transitions:1||CORRECTED CONCAVE GRATINGS:1||DISCHARGE:1||LASERPLASMA:1||thin film:1||reflectivity:1||opacity:1||gain:1||smallangle Xray scattering:1||SOFTXRAY:1||ZINCOXIDE:1||CYGNUSX3:1||Betatron oscillation:1||ACCELERATOR:1||STRAINEDLAYER SUPERLATTICES:1||OPTICAL PARAMETRIC AMPLIFICATION:1||PASSIVE MODELOCKING:1||Collision dynamics:1||MUM:1||EXACTEXCHANGE:1||BASISSET:1||APPROXIMATION:1||OXYNITRIDES:1||Beam energy modulation:1||polarization spectroscopy:1||REORIENTATION TRANSITION:1||DEPENDENCE:1||sulfurs:1||BUILDINGBLOCKS:1||RATES:1||OPTICAL PULSES:1||toroidal mirror:1||XRAY LASER:1||CALCIUM:1||radially polarized laser:1||GRAINBOUNDARIES:1||VAPORDEPOSITION:1||Xray generation:1||MAGNETIZATION:1||Electric excitation:1||Laserinduced gas plasmas:1||Qualitative analysis:1||SCHEME:1||RADIATION:10||PULSES:8||PHOTOLUMINESCENCE:7||LASER:7||GENERATION:6||NANORODS:6||GROWTH:6||NANOWIRES:5||IMPLANTED GAN:5||SPECTROSCOPY:5||THINFILMS:4||DYNAMICS:4||SILICON:4||EXTREMEULTRAVIOLET:4||AMPLIFICATION:4||PRESSURE:4||PHASE:4||OPTICALPROPERTIES:4||SYSTEM:4||EMISSION:4||FEL:3||N2O:3||FILMS:3||OPTICS:3||SPECTRA:3||FIELD:3||MIRRORS:3||ARRAYS:3||CLUSTERS:3||SIO2:3||IONIZATION:3||VACUUM:3||SCATTERING:3||IONS:2||LUMINESCENCE PROPERTIES:2||ANISOTROPY:2||BEAMS:2||DIFFRACTION:2||DISPERSION:2||chemical vapor deposition (CVD):2||ELECTRONICSTRUCTURE:2||MOSFETS:2||SI3N4:2||DENSITY:2||LIGHT:2||PLASMAS:2||MATTER:2||nanocomposites:2||RAMANSCATTERING:2||NANOPARTICLES:2||OXIDE:2||AMPLIFIED SPONTANEOUS EMISSION:2||NM WAVELENGTH:2||GAIN:2||CARBON NANOTUBES:2||CROSSSECTIONS:2||LIGHTEMITTINGDIODES:2||PULSE:2||CARBON PLASMA:2||TISAPPHIRE LASER:2||Raman scattering:2||ROUTE:2||multilayer:2||CATHODOLUMINESCENCE:2||highresolution transmission electronic microscope (HRTEM):2||DIFFERENCEFREQUENCYGENERATION:2||CRYSTAL:2||laserproduced plasma:2||NANOCABLES:2||photoluminescence:2||MAGNETIC ALLOY SEMICONDUCTORS:2||MOLECULARBEAM EPITAXY:2||EARTHDOPED GAN:2||LASER FIELDS:2||CHIRPEDPULSEAMPLIFICATION:2||ALN:2||GAUSSIANBEAM:2||ASSISTED CATALYTIC GROWTH:2||BLUE:2||NANOSTRUCTURES:2||MAGNETOELECTRONICS:2||MICROSCOPY:2||ELECTROLUMINESCENCE:2||LASERPULSES:2||GaN nanowires:2||GALLIUM NITRIDE NANOWIRES:2||GAMNN:2||NANOTUBES:2||PHYSICS:2||Femtosecond laser:2||parametric oscillators and amplifiers:1||ultrafast lasers:1||VALENCE:1||nanowires:1||DILUTED MAGNETIC SEMICONDUCTOR:1||LUMINESCENCE:1||Density modulation:1||Energy modulation:1||Current enhanced SASE free electron laser:1||Undulator radiation:1||FREEELECTRON LASERS:1||ULTRATHIN FERROMAGNETICFILMS:1||OXIDEFILMS:1||ABLATION:1||COMPONENT:1||METAL:1||innershell excited states:1||Nelike ions:1||TRANSITIONS:1||XUV spectrometer:1||DIAGNOSTICS:1||Xray scattering:1||MO/SI:1||pulsed laser deposition:1||KEV IMPACT ENERGIES:1||vacuum electron acceleration:1||HIGHINTENSITY LASER:1||JUNCTIONS:1||LOWTEMPERATURE GROWTH:1||nanocrystalline materials:1||MOLECULAR PHOTOIONIZATION:1||LOCALIZATION:1||DEUTERIUM CLUSTERS:1||EXPLOSIONS:1||REGENERATIVE AMPLIFIERS:1||RAREGASES:1||THz radiation:1||FREEELECTRON LASER:1||REALTIME OBSERVATION:1||TARGET:1||photoionized plasmas:1||fs Xray laser:1||emission profile:1||HIGHORDER HARMONICS:1||Xray laser:1||atomic transition:1||EXCITATION:1||LASERS:1||PERFORMANCE:1||RELATIVISTIC ELECTRONS:1||BI2O3DOPED ZNO:1||INNERSHELL IONIZATION:1||Laser wakefield:1||FREQUENCY:1||SOLIDSTATE LASERS:1||Linearly polarized:1||THERMIONIC EMISSION:1||PULSE AMPLIFICATION SYSTEM:1||BIB3O6:1||NM:1||NONCOVALENT INTERACTIONS:1||CRYSTALLINE:1||INTENSITY:1||JETS:1||COHERENT:1||LINE:1||ANGULARDISTRIBUTION:1||SILVER IONS:1||magnetic anisotropy:1||DEVICES:1||Auger transitions:1||CosterKronig transitions:1||EFFICIENT:1||ELECTRONIMPACT IONIZATION:1||ULTRASHORTPULSE:1||Nanowire:1||Heterostructure:1||soft Xray reflectivity:1||PLASMA ACCELERATOR:1||ZINCOXIDE NANOWIRES:1||CHEMICALVAPORDEPOSITION:1||Electron acceleration:1||Ionization of gases:1||Delay dependent:1||MULTIPHOTON IONIZATION:1||FRAGMENTATION:1||GASJET:1||ultrafast nonlinear optics:1||CYCLE PULSES:1||KHZ:1||chemical vapor deposition:1||ferromagnetism:1||ABSORPTION:1||TERAHERTZ RADIATION:1||SCIENCE:1||FIELDS:1||ELECTRONS:1||nanomultilayer structures:1||YIELDS:1||AUGER:1||10HZ REPETITION RATE:1||MULTITERAWATT:1||SPECTROGRAPH:1||HIGHHARMONICGENERATION:1||spectroscopy:1||level population:1||PARTICLEACCELERATION:1||OPTICAL FREQUENCYMEASUREMENT:1||NANOWALLS:1||ROOMTEMPERATURE:1||AVERAGE OUTPUT POWER:1||GROUPVELOCITYMISMATCH:1||Impact ionization:1||Dynamics:1||Lasers:1||Collisional process:1||ABOVETHRESHOLD IONIZATION:1||MAINGROUP THERMOCHEMISTRY:1||dilute magnetic semiconductors:1||GACRN:1||SIZE:1||ATTOSECOND:1||Ar cluster:1||Xray astrophysics:1||photoionization:1||irons:1||normal incidence pulsed laser deposition:1||SHELLS:1||Silicon Oxide:1||gaspuff Zpinch:1||Xray:1||soft Xray reflectors:1||ESCAPE:1||ZN2SIO4:1||SILICA:1||Time delay:1||Collisional plasmas:1||MASSSPECTROMETRY:1||NUCLEARFUSION:1||PARAMETRIC AMPLIFICATION:1||LYING ELECTRONIC STATES:1||ADJUSTABLEPARAMETERS:1||MAGNETICPROPERTIES:1||LIQUIDPHASE EPITAXY:1||CEP laser:1||REGION:1||Plasma waveguide:1||AMBIENT GAS:1||DEPOSITION:1||HARMONICGENERATION:1||ENHANCEMENT:1||imaging spectrometer:1||Abel inversion:1||Water window:1||Liquid nitrogen jet:1||CHARGEEXCHANGE:1||NOBEL LECTURE:1||VARISTOR:1||EPITAXY:1||THINDISK LASER:1||HIGHREPETITIONRATE:1||Atom lasers:1||Electronimpact excitation:1||High order harmonics:1||ultrafast technology:1||PEAK POWER:1||CHARGED ALUMINUM CLUSTERS:1||GaN:1||THIN:1||Electron beam:1||INTENSE:1||Hard Xray pulse generation:1||NONLINEAR THOMSON SCATTERING:1||MULTILAYER:1||UVvisible spectrometer:1||ATOMS:1||innershell transitions:1||CORRECTED CONCAVE GRATINGS:1||DISCHARGE:1||LASERPLASMA:1||thin film:1||reflectivity:1||opacity:1||gain:1||smallangle Xray scattering:1||SOFTXRAY:1||ZINCOXIDE:1||CYGNUSX3:1||Betatron oscillation:1||ACCELERATOR:1||STRAINEDLAYER SUPERLATTICES:1||OPTICAL PARAMETRIC AMPLIFICATION:1||PASSIVE MODELOCKING:1||Collision dynamics:1||MUM:1||EXACTEXCHANGE:1||BASISSET:1||APPROXIMATION:1||OXYNITRIDES:1||Beam energy modulation:1||polarization spectroscopy:1||REORIENTATION TRANSITION:1||DEPENDENCE:1||sulfurs:1||BUILDINGBLOCKS:1||RATES:1||OPTICAL PULSES:1||toroidal mirror:1||XRAY LASER:1||CALCIUM:1||radially polarized laser:1||GRAINBOUNDARIES:1||VAPORDEPOSITION:1||Xray generation:1||MAGNETIZATION:1||Electric excitation:1||Laserinduced gas plasmas:1||Qualitative analysis:1||SCHEME:1||RADIATION:10||PULSES:8||PHOTOLUMINESCENCE:7||LASER:7||GENERATION:6||NANORODS:6||GROWTH:6||NANOWIRES:5||IMPLANTED 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SEMICONDUCTORS:2||MOLECULARBEAM EPITAXY:2||EARTHDOPED GAN:2||LASER FIELDS:2||CHIRPEDPULSEAMPLIFICATION:2||ALN:2||GAUSSIANBEAM:2||ASSISTED CATALYTIC GROWTH:2||BLUE:2||NANOSTRUCTURES:2||MAGNETOELECTRONICS:2||MICROSCOPY:2||ELECTROLUMINESCENCE:2||LASERPULSES:2||GaN nanowires:2||GALLIUM NITRIDE NANOWIRES:2||GAMNN:2||NANOTUBES:2||PHYSICS:2||Femtosecond laser:2||parametric oscillators and amplifiers:1||ultrafast lasers:1||VALENCE:1||nanowires:1||DILUTED MAGNETIC SEMICONDUCTOR:1||LUMINESCENCE:1||Density modulation:1||Energy modulation:1||Current enhanced SASE free electron laser:1||Undulator radiation:1||FREEELECTRON LASERS:1||ULTRATHIN FERROMAGNETICFILMS:1||OXIDEFILMS:1||ABLATION:1||COMPONENT:1||METAL:1||innershell excited states:1||Nelike ions:1||TRANSITIONS:1||XUV spectrometer:1||DIAGNOSTICS:1||Xray scattering:1||MO/SI:1||pulsed laser deposition:1||KEV IMPACT ENERGIES:1||vacuum electron acceleration:1||HIGHINTENSITY LASER:1||JUNCTIONS:1||LOWTEMPERATURE GROWTH:1||nanocrystalline materials:1||MOLECULAR PHOTOIONIZATION:1||LOCALIZATION:1||DEUTERIUM CLUSTERS:1||EXPLOSIONS:1||REGENERATIVE AMPLIFIERS:1||RAREGASES:1||THz radiation:1||FREEELECTRON LASER:1||REALTIME OBSERVATION:1||TARGET:1||photoionized plasmas:1||fs Xray laser:1||emission profile:1||HIGHORDER HARMONICS:1||Xray laser:1||atomic transition:1||EXCITATION:1||LASERS:1||PERFORMANCE:1||RELATIVISTIC ELECTRONS:1||BI2O3DOPED ZNO:1||INNERSHELL IONIZATION:1||Laser wakefield:1||FREQUENCY:1||SOLIDSTATE LASERS:1||Linearly polarized:1||THERMIONIC EMISSION:1||PULSE AMPLIFICATION SYSTEM:1||BIB3O6:1||NM:1||NONCOVALENT INTERACTIONS:1||CRYSTALLINE:1||INTENSITY:1||JETS:1||COHERENT:1||LINE:1||ANGULARDISTRIBUTION:1||SILVER IONS:1||magnetic anisotropy:1||DEVICES:1||Auger transitions:1||CosterKronig transitions:1||EFFICIENT:1||ELECTRONIMPACT IONIZATION:1||ULTRASHORTPULSE:1||Nanowire:1||Heterostructure:1||soft Xray reflectivity:1||PLASMA ACCELERATOR:1||ZINCOXIDE NANOWIRES:1||CHEMICALVAPORDEPOSITION:1||Electron acceleration:1||Ionization of gases:1||Delay dependent:1||MULTIPHOTON IONIZATION:1||FRAGMENTATION:1||GASJET:1||ultrafast nonlinear optics:1||CYCLE PULSES:1||KHZ:1||chemical vapor deposition:1||ferromagnetism:1||ABSORPTION:1||TERAHERTZ RADIATION:1||SCIENCE:1||FIELDS:1||ELECTRONS:1||nanomultilayer structures:1||YIELDS:1||AUGER:1||10HZ REPETITION RATE:1||MULTITERAWATT:1||SPECTROGRAPH:1||HIGHHARMONICGENERATION:1||spectroscopy:1||level population:1||PARTICLEACCELERATION:1||OPTICAL FREQUENCYMEASUREMENT:1||NANOWALLS:1||ROOMTEMPERATURE:1||AVERAGE OUTPUT POWER:1||GROUPVELOCITYMISMATCH:1||Impact ionization:1||Dynamics:1||Lasers:1||Collisional process:1||ABOVETHRESHOLD IONIZATION:1||MAINGROUP THERMOCHEMISTRY:1||dilute magnetic semiconductors:1||GACRN:1||SIZE:1||ATTOSECOND:1||Ar cluster:1||Xray astrophysics:1||photoionization:1||irons:1||normal incidence pulsed laser deposition:1||SHELLS:1||Silicon Oxide:1||gaspuff Zpinch:1||Xray:1||soft Xray reflectors:1||ESCAPE:1||ZN2SIO4:1||SILICA:1||Time 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materials:1||MOLECULAR PHOTOIONIZATION:1||LOCALIZATION:1||DEUTERIUM CLUSTERS:1||EXPLOSIONS:1||REGENERATIVE AMPLIFIERS:1||RAREGASES:1||THz radiation:1||FREEELECTRON LASER:1||REALTIME OBSERVATION:1||TARGET:1||photoionized plasmas:1||fs Xray laser:1||emission profile:1||HIGHORDER HARMONICS:1||Xray laser:1||atomic transition:1||EXCITATION:1||LASERS:1||PERFORMANCE:1||RELATIVISTIC ELECTRONS:1||BI2O3DOPED ZNO:1||INNERSHELL IONIZATION:1||Laser wakefield:1||FREQUENCY:1||SOLIDSTATE LASERS:1||Linearly polarized:1||THERMIONIC EMISSION:1||PULSE AMPLIFICATION SYSTEM:1||BIB3O6:1||NM:1||NONCOVALENT INTERACTIONS:1||CRYSTALLINE:1||INTENSITY:1||JETS:1||COHERENT:1||LINE:1||ANGULARDISTRIBUTION:1||SILVER IONS:1||magnetic anisotropy:1||DEVICES:1||Auger transitions:1||CosterKronig transitions:1||EFFICIENT:1||ELECTRONIMPACT IONIZATION:1||ULTRASHORTPULSE:1||Nanowire:1||Heterostructure:1||soft Xray reflectivity:1||PLASMA ACCELERATOR:1||ZINCOXIDE NANOWIRES:1||CHEMICALVAPORDEPOSITION:1||Electron acceleration:1||Ionization of gases:1||Delay dependent:1||MULTIPHOTON IONIZATION:1||FRAGMENTATION:1||GASJET:1||ultrafast nonlinear optics:1||CYCLE PULSES:1||KHZ:1||chemical vapor deposition:1||ferromagnetism:1||ABSORPTION:1||TERAHERTZ RADIATION:1||SCIENCE:1||FIELDS:1||ELECTRONS:1||nanomultilayer structures:1||YIELDS:1||AUGER:1||10HZ REPETITION RATE:1||MULTITERAWATT:1||SPECTROGRAPH:1||HIGHHARMONICGENERATION:1||spectroscopy:1||level population:1||PARTICLEACCELERATION:1||OPTICAL FREQUENCYMEASUREMENT:1||NANOWALLS:1||ROOMTEMPERATURE:1||AVERAGE OUTPUT POWER:1||GROUPVELOCITYMISMATCH:1||Impact ionization:1||Dynamics:1||Lasers:1||Collisional process:1||ABOVETHRESHOLD IONIZATION:1||MAINGROUP THERMOCHEMISTRY:1||dilute magnetic semiconductors:1||GACRN:1||SIZE:1||ATTOSECOND:1||Ar cluster:1||Xray astrophysics:1||photoionization:1||irons:1||normal incidence pulsed laser deposition:1||SHELLS:1||Silicon Oxide:1||gaspuff Zpinch:1||Xray:1||soft Xray reflectors:1||ESCAPE:1||ZN2SIO4:1||SILICA:1||Time delay:1||Collisional plasmas:1||MASSSPECTROMETRY:1||NUCLEARFUSION:1||PARAMETRIC AMPLIFICATION:1||LYING ELECTRONIC STATES:1||ADJUSTABLEPARAMETERS:1||MAGNETICPROPERTIES:1||LIQUIDPHASE EPITAXY:1||CEP laser:1||REGION:1||Plasma waveguide:1||AMBIENT GAS:1||DEPOSITION:1||HARMONICGENERATION:1||ENHANCEMENT:1||imaging spectrometer:1||Abel inversion:1||Water window:1||Liquid nitrogen jet:1||CHARGEEXCHANGE:1||NOBEL LECTURE:1||VARISTOR:1||EPITAXY:1||THINDISK LASER:1||HIGHREPETITIONRATE:1||Atom lasers:1||Electronimpact excitation:1||High order harmonics:1||ultrafast technology:1||PEAK POWER:1||CHARGED ALUMINUM CLUSTERS:1||GaN:1||THIN:1||Electron beam:1||INTENSE:1||Hard Xray pulse generation:1||NONLINEAR THOMSON SCATTERING:1||MULTILAYER:1||UVvisible spectrometer:1||ATOMS:1||innershell transitions:1||CORRECTED CONCAVE GRATINGS:1||DISCHARGE:1||LASERPLASMA:1||thin film:1||reflectivity:1||opacity:1||gain:1||smallangle Xray scattering:1||SOFTXRAY:1||ZINCOXIDE:1||CYGNUSX3:1||Betatron oscillation:1||ACCELERATOR:1||STRAINEDLAYER SUPERLATTICES:1||OPTICAL PARAMETRIC AMPLIFICATION:1||PASSIVE MODELOCKING:1||Collision dynamics:1||MUM:1||EXACTEXCHANGE:1||BASISSET:1||APPROXIMATION:1||OXYNITRIDES:1||Beam energy modulation:1||polarization spectroscopy:1||REORIENTATION TRANSITION:1||DEPENDENCE:1||sulfurs:1||BUILDINGBLOCKS:1||RATES:1||OPTICAL PULSES:1||toroidal mirror:1||XRAY LASER:1||CALCIUM:1||radially polarized laser:1||GRAINBOUNDARIES:1||VAPORDEPOSITION:1||Xray generation:1||MAGNETIZATION:1||Electric excitation:1||Laserinduced gas plasmas:1||Qualitative analysis:1||SCHEME:1||RADIATION:10||PULSES:8||PHOTOLUMINESCENCE:7||LASER:7||GENERATION:6||NANORODS:6||GROWTH:6||NANOWIRES:5||IMPLANTED GAN:5||SPECTROSCOPY:5||THINFILMS:4||DYNAMICS:4||SILICON:4||EXTREMEULTRAVIOLET:4||AMPLIFICATION:4||PRESSURE:4||PHASE:4||OPTICALPROPERTIES:4||SYSTEM:4||EMISSION:4||FEL:3||N2O:3||FILMS:3||OPTICS:3||SPECTRA:3||FIELD:3||MIRRORS:3||ARRAYS:3||CLUSTERS:3||SIO2:3||IONIZATION:3||VACUUM:3||SCATTERING:3||IONS:2||LUMINESCENCE PROPERTIES:2||ANISOTROPY:2||BEAMS:2||DIFFRACTION:2||DISPERSION:2||chemical vapor deposition (CVD):2||ELECTRONICSTRUCTURE:2||MOSFETS:2||SI3N4:2||DENSITY:2||LIGHT:2||PLASMAS:2||MATTER:2||nanocomposites:2||RAMANSCATTERING:2||NANOPARTICLES:2||OXIDE:2||AMPLIFIED SPONTANEOUS EMISSION:2||NM WAVELENGTH:2||GAIN:2||CARBON NANOTUBES:2||CROSSSECTIONS:2||LIGHTEMITTINGDIODES:2||PULSE:2||CARBON PLASMA:2||TISAPPHIRE LASER:2||Raman scattering:2||ROUTE:2||multilayer:2||CATHODOLUMINESCENCE:2||highresolution transmission electronic microscope (HRTEM):2||DIFFERENCEFREQUENCYGENERATION:2||CRYSTAL:2||laserproduced plasma:2||NANOCABLES:2||photoluminescence:2||MAGNETIC ALLOY SEMICONDUCTORS:2||MOLECULARBEAM EPITAXY:2||EARTHDOPED GAN:2||LASER FIELDS:2||CHIRPEDPULSEAMPLIFICATION:2||ALN:2||GAUSSIANBEAM:2||ASSISTED CATALYTIC GROWTH:2||BLUE:2||NANOSTRUCTURES:2||MAGNETOELECTRONICS:2||MICROSCOPY:2||ELECTROLUMINESCENCE:2||LASERPULSES:2||GaN nanowires:2||GALLIUM NITRIDE NANOWIRES:2||GAMNN:2||NANOTUBES:2||PHYSICS:2||Femtosecond laser:2||parametric oscillators and amplifiers:1||ultrafast lasers:1||VALENCE:1||nanowires:1||DILUTED MAGNETIC SEMICONDUCTOR:1||LUMINESCENCE:1||Density modulation:1||Energy modulation:1||Current enhanced SASE free electron laser:1||Undulator radiation:1||FREEELECTRON LASERS:1||ULTRATHIN FERROMAGNETICFILMS:1||OXIDEFILMS:1||ABLATION:1||COMPONENT:1||METAL:1||innershell excited states:1||Nelike ions:1||TRANSITIONS:1||XUV spectrometer:1||DIAGNOSTICS:1||Xray scattering:1||MO/SI:1||pulsed laser deposition:1||KEV IMPACT ENERGIES:1||vacuum electron acceleration:1||HIGHINTENSITY LASER:1||JUNCTIONS:1||LOWTEMPERATURE GROWTH:1||nanocrystalline materials:1||MOLECULAR PHOTOIONIZATION:1||LOCALIZATION:1||DEUTERIUM CLUSTERS:1||EXPLOSIONS:1||REGENERATIVE AMPLIFIERS:1||RAREGASES:1||THz radiation:1||FREEELECTRON LASER:1||REALTIME OBSERVATION:1||TARGET:1||photoionized plasmas:1||fs Xray laser:1||emission profile:1||HIGHORDER HARMONICS:1||Xray laser:1||atomic transition:1||EXCITATION:1||LASERS:1||PERFORMANCE:1||RELATIVISTIC ELECTRONS:1||BI2O3DOPED ZNO:1||INNERSHELL IONIZATION:1||Laser wakefield:1||FREQUENCY:1||SOLIDSTATE LASERS:1||Linearly polarized:1||THERMIONIC EMISSION:1||PULSE AMPLIFICATION SYSTEM:1||BIB3O6:1||NM:1||NONCOVALENT INTERACTIONS:1||CRYSTALLINE:1||INTENSITY:1||JETS:1||COHERENT:1||LINE:1||ANGULARDISTRIBUTION:1||SILVER IONS:1||magnetic anisotropy:1||DEVICES:1||Auger transitions:1||CosterKronig transitions:1||EFFICIENT:1||ELECTRONIMPACT IONIZATION:1||ULTRASHORTPULSE:1||Nanowire:1||Heterostructure:1||soft Xray reflectivity:1||PLASMA ACCELERATOR:1||ZINCOXIDE NANOWIRES:1||CHEMICALVAPORDEPOSITION:1||Electron acceleration:1||Ionization of gases:1||Delay dependent:1||MULTIPHOTON IONIZATION:1||FRAGMENTATION:1||GASJET:1||ultrafast nonlinear optics:1||CYCLE PULSES:1||KHZ:1||chemical vapor deposition:1||ferromagnetism:1||ABSORPTION:1||TERAHERTZ RADIATION:1||SCIENCE:1||FIELDS:1||ELECTRONS:1||nanomultilayer structures:1||YIELDS:1||AUGER:1||10HZ REPETITION RATE:1||MULTITERAWATT:1||SPECTROGRAPH:1||HIGHHARMONICGENERATION:1||spectroscopy:1||level population:1||PARTICLEACCELERATION:1||OPTICAL FREQUENCYMEASUREMENT:1||NANOWALLS:1||ROOMTEMPERATURE:1||AVERAGE OUTPUT POWER:1||GROUPVELOCITYMISMATCH:1||Impact ionization:1||Dynamics:1||Lasers:1||Collisional process:1||ABOVETHRESHOLD IONIZATION:1||MAINGROUP THERMOCHEMISTRY:1||dilute magnetic semiconductors:1||GACRN:1||SIZE:1||ATTOSECOND:1||Ar cluster:1||Xray astrophysics:1||photoionization:1||irons:1||normal incidence pulsed laser deposition:1||SHELLS:1||Silicon Oxide:1||gaspuff Zpinch:1||Xray:1||soft Xray reflectors:1||ESCAPE:1||ZN2SIO4:1||SILICA:1||Time delay:1||Collisional plasmas:1||MASSSPECTROMETRY:1||NUCLEARFUSION:1||PARAMETRIC AMPLIFICATION:1||LYING ELECTRONIC STATES:1||ADJUSTABLEPARAMETERS:1||MAGNETICPROPERTIES:1||LIQUIDPHASE EPITAXY:1||CEP laser:1||REGION:1||Plasma waveguide:1||AMBIENT GAS:1||DEPOSITION:1||HARMONICGENERATION:1||ENHANCEMENT:1||imaging spectrometer:1||Abel inversion:1||Water window:1||Liquid nitrogen jet:1||CHARGEEXCHANGE:1||NOBEL LECTURE:1||VARISTOR:1||EPITAXY:1||THINDISK LASER:1||HIGHREPETITIONRATE:1||Atom lasers:1||Electronimpact excitation:1||High order harmonics:1||ultrafast technology:1||PEAK POWER:1||CHARGED ALUMINUM CLUSTERS:1||GaN:1||THIN:1||Electron beam:1||INTENSE:1||Hard Xray pulse generation:1||NONLINEAR THOMSON SCATTERING:1||MULTILAYER:1||UVvisible spectrometer:1||ATOMS:1||innershell transitions:1||CORRECTED CONCAVE GRATINGS:1||DISCHARGE:1||LASERPLASMA:1||thin film:1||reflectivity:1||opacity:1||gain:1||smallangle Xray scattering:1||SOFTXRAY:1||ZINCOXIDE:1||CYGNUSX3:1||Betatron oscillation:1||ACCELERATOR:1||STRAINEDLAYER SUPERLATTICES:1||OPTICAL PARAMETRIC AMPLIFICATION:1||PASSIVE MODELOCKING:1||Collision dynamics:1||MUM:1||EXACTEXCHANGE:1||BASISSET:1||APPROXIMATION:1||OXYNITRIDES:1||Beam energy modulation:1||polarization spectroscopy:1||REORIENTATION TRANSITION:1||DEPENDENCE:1||sulfurs:1||BUILDINGBLOCKS:1||RATES:1||OPTICAL PULSES:1||toroidal mirror:1||XRAY LASER:1||CALCIUM:1||radially polarized laser:1||GRAINBOUNDARIES:1||VAPORDEPOSITION:1||Xray generation:1||MAGNETIZATION:1||Electric excitation:1||Laserinduced gas plasmas:1||Qualitative analysis:1||SCHEME:1||RADIATION:10||PULSES:8||PHOTOLUMINESCENCE:7||LASER:7||GENERATION:6||NANORODS:6||GROWTH:6||NANOWIRES:5||IMPLANTED 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SEMICONDUCTORS:2||MOLECULARBEAM EPITAXY:2||EARTHDOPED GAN:2||LASER FIELDS:2||CHIRPEDPULSEAMPLIFICATION:2||ALN:2||GAUSSIANBEAM:2||ASSISTED CATALYTIC GROWTH:2||BLUE:2||NANOSTRUCTURES:2||MAGNETOELECTRONICS:2||MICROSCOPY:2||ELECTROLUMINESCENCE:2||LASERPULSES:2||GaN nanowires:2||GALLIUM NITRIDE NANOWIRES:2||GAMNN:2||NANOTUBES:2||PHYSICS:2||Femtosecond laser:2||parametric oscillators and amplifiers:1||ultrafast lasers:1||VALENCE:1||nanowires:1||DILUTED MAGNETIC SEMICONDUCTOR:1||LUMINESCENCE:1||Density modulation:1||Energy modulation:1||Current enhanced SASE free electron laser:1||Undulator radiation:1||FREEELECTRON LASERS:1||ULTRATHIN FERROMAGNETICFILMS:1||OXIDEFILMS:1||ABLATION:1||COMPONENT:1||METAL:1||innershell excited states:1||Nelike ions:1||TRANSITIONS:1||XUV spectrometer:1||DIAGNOSTICS:1||Xray scattering:1||MO/SI:1||pulsed laser deposition:1||KEV IMPACT ENERGIES:1||vacuum electron acceleration:1||HIGHINTENSITY LASER:1||JUNCTIONS:1||LOWTEMPERATURE GROWTH:1||nanocrystalline materials:1||MOLECULAR PHOTOIONIZATION:1||LOCALIZATION:1||DEUTERIUM CLUSTERS:1||EXPLOSIONS:1||REGENERATIVE AMPLIFIERS:1||RAREGASES:1||THz radiation:1||FREEELECTRON LASER:1||REALTIME OBSERVATION:1||TARGET:1||photoionized plasmas:1||fs Xray laser:1||emission profile:1||HIGHORDER HARMONICS:1||Xray laser:1||atomic transition:1||EXCITATION:1||LASERS:1||PERFORMANCE:1||RELATIVISTIC ELECTRONS:1||BI2O3DOPED ZNO:1||INNERSHELL IONIZATION:1||Laser wakefield:1||FREQUENCY:1||SOLIDSTATE LASERS:1||Linearly polarized:1||THERMIONIC EMISSION:1||PULSE AMPLIFICATION SYSTEM:1||BIB3O6:1||NM:1||NONCOVALENT INTERACTIONS:1||CRYSTALLINE:1||INTENSITY:1||JETS:1||COHERENT:1||LINE:1||ANGULARDISTRIBUTION:1||SILVER IONS:1||magnetic anisotropy:1||DEVICES:1||Auger transitions:1||CosterKronig transitions:1||EFFICIENT:1||ELECTRONIMPACT IONIZATION:1||ULTRASHORTPULSE:1||Nanowire:1||Heterostructure:1||soft Xray reflectivity:1||PLASMA ACCELERATOR:1||ZINCOXIDE NANOWIRES:1||CHEMICALVAPORDEPOSITION:1||Electron acceleration:1||Ionization of gases:1||Delay dependent:1||MULTIPHOTON IONIZATION:1||FRAGMENTATION:1||GASJET:1||ultrafast nonlinear optics:1||CYCLE PULSES:1||KHZ:1||chemical vapor deposition:1||ferromagnetism:1||ABSORPTION:1||TERAHERTZ RADIATION:1||SCIENCE:1||FIELDS:1||ELECTRONS:1||nanomultilayer structures:1||YIELDS:1||AUGER:1||10HZ REPETITION RATE:1||MULTITERAWATT:1||SPECTROGRAPH:1||HIGHHARMONICGENERATION:1||spectroscopy:1||level population:1||PARTICLEACCELERATION:1||OPTICAL FREQUENCYMEASUREMENT:1||NANOWALLS:1||ROOMTEMPERATURE:1||AVERAGE OUTPUT POWER:1||GROUPVELOCITYMISMATCH:1||Impact ionization:1||Dynamics:1||Lasers:1||Collisional process:1||ABOVETHRESHOLD IONIZATION:1||MAINGROUP THERMOCHEMISTRY:1||dilute magnetic semiconductors:1||GACRN:1||SIZE:1||ATTOSECOND:1||Ar cluster:1||Xray astrophysics:1||photoionization:1||irons:1||normal incidence pulsed laser deposition:1||SHELLS:1||Silicon Oxide:1||gaspuff Zpinch:1||Xray:1||soft Xray reflectors:1||ESCAPE:1||ZN2SIO4:1||SILICA:1||Time 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materials:1||MOLECULAR PHOTOIONIZATION:1||LOCALIZATION:1||DEUTERIUM CLUSTERS:1||EXPLOSIONS:1||REGENERATIVE AMPLIFIERS:1||RAREGASES:1||THz radiation:1||FREEELECTRON LASER:1||REALTIME OBSERVATION:1||TARGET:1||photoionized plasmas:1||fs Xray laser:1||emission profile:1||HIGHORDER HARMONICS:1||Xray laser:1||atomic transition:1||EXCITATION:1||LASERS:1||PERFORMANCE:1||RELATIVISTIC ELECTRONS:1||BI2O3DOPED ZNO:1||INNERSHELL IONIZATION:1||Laser wakefield:1||FREQUENCY:1||SOLIDSTATE LASERS:1||Linearly polarized:1||THERMIONIC EMISSION:1||PULSE AMPLIFICATION SYSTEM:1||BIB3O6:1||NM:1||NONCOVALENT INTERACTIONS:1||CRYSTALLINE:1||INTENSITY:1||JETS:1||COHERENT:1||LINE:1||ANGULARDISTRIBUTION:1||SILVER IONS:1||magnetic anisotropy:1||DEVICES:1||Auger transitions:1||CosterKronig transitions:1||EFFICIENT:1||ELECTRONIMPACT IONIZATION:1||ULTRASHORTPULSE:1||Nanowire:1||Heterostructure:1||soft Xray reflectivity:1||PLASMA ACCELERATOR:1||ZINCOXIDE NANOWIRES:1||CHEMICALVAPORDEPOSITION:1||Electron acceleration:1||Ionization of gases:1||Delay dependent:1||MULTIPHOTON IONIZATION:1||FRAGMENTATION:1||GASJET:1||ultrafast nonlinear optics:1||CYCLE PULSES:1||KHZ:1||chemical vapor deposition:1||ferromagnetism:1||ABSORPTION:1||TERAHERTZ RADIATION:1||SCIENCE:1||FIELDS:1||ELECTRONS:1||nanomultilayer structures:1||YIELDS:1||AUGER:1||10HZ REPETITION RATE:1||MULTITERAWATT:1||SPECTROGRAPH:1||HIGHHARMONICGENERATION:1||spectroscopy:1||level population:1||PARTICLEACCELERATION:1||OPTICAL FREQUENCYMEASUREMENT:1||NANOWALLS:1||ROOMTEMPERATURE:1||AVERAGE OUTPUT POWER:1||GROUPVELOCITYMISMATCH:1||Impact ionization:1||Dynamics:1||Lasers:1||Collisional process:1||ABOVETHRESHOLD IONIZATION:1||MAINGROUP THERMOCHEMISTRY:1||dilute magnetic semiconductors:1||GACRN:1||SIZE:1||ATTOSECOND:1||Ar cluster:1||Xray astrophysics:1||photoionization:1||irons:1||normal incidence pulsed laser deposition:1||SHELLS:1||Silicon Oxide:1||gaspuff Zpinch:1||Xray:1||soft Xray reflectors:1||ESCAPE:1||ZN2SIO4:1||SILICA:1||Time delay:1||Collisional plasmas:1||MASSSPECTROMETRY:1||NUCLEARFUSION:1||PARAMETRIC AMPLIFICATION:1||LYING ELECTRONIC STATES:1||ADJUSTABLEPARAMETERS:1||MAGNETICPROPERTIES:1||LIQUIDPHASE EPITAXY:1||CEP laser:1||REGION:1||Plasma waveguide:1||AMBIENT GAS:1||DEPOSITION:1||HARMONICGENERATION:1||ENHANCEMENT:1||imaging spectrometer:1||Abel inversion:1||Water window:1||Liquid nitrogen jet:1||CHARGEEXCHANGE:1||NOBEL LECTURE:1||VARISTOR:1||EPITAXY:1||THINDISK LASER:1||HIGHREPETITIONRATE:1||Atom lasers:1||Electronimpact excitation:1||High order harmonics:1||ultrafast technology:1||PEAK POWER:1||CHARGED ALUMINUM CLUSTERS:1||GaN:1||THIN:1||Electron beam:1||INTENSE:1||Hard Xray pulse generation:1||NONLINEAR THOMSON SCATTERING:1||MULTILAYER:1||UVvisible spectrometer:1||ATOMS:1||innershell transitions:1||CORRECTED CONCAVE GRATINGS:1||DISCHARGE:1||LASERPLASMA:1||thin film:1||reflectivity:1||opacity:1||gain:1||smallangle Xray scattering:1||SOFTXRAY:1||ZINCOXIDE:1||CYGNUSX3:1||Betatron oscillation:1||ACCELERATOR:1||STRAINEDLAYER SUPERLATTICES:1||OPTICAL PARAMETRIC AMPLIFICATION:1||PASSIVE MODELOCKING:1||Collision dynamics:1||MUM:1||EXACTEXCHANGE:1||BASISSET:1||APPROXIMATION:1||OXYNITRIDES:1||Beam energy modulation:1||polarization spectroscopy:1||REORIENTATION TRANSITION:1||DEPENDENCE:1||sulfurs:1||BUILDINGBLOCKS:1||RATES:1||OPTICAL PULSES:1||toroidal mirror:1||XRAY LASER:1||CALCIUM:1||radially polarized laser:1||GRAINBOUNDARIES:1||VAPORDEPOSITION:1||Xray generation:1||MAGNETIZATION:1||Electric excitation:1||Laserinduced gas plasmas:1||Qualitative analysis:1||SCHEME:1||RADIATION:10||PULSES:8||PHOTOLUMINESCENCE:7||LASER:7||GENERATION:6||NANORODS:6||GROWTH:6||NANOWIRES:5||IMPLANTED GAN:5||SPECTROSCOPY:5||THINFILMS:4||DYNAMICS:4||SILICON:4||EXTREMEULTRAVIOLET:4||AMPLIFICATION:4||PRESSURE:4||PHASE:4||OPTICALPROPERTIES:4||SYSTEM:4||EMISSION:4||FEL:3||N2O:3||FILMS:3||OPTICS:3||SPECTRA:3||FIELD:3||MIRRORS:3||ARRAYS:3||CLUSTERS:3||SIO2:3||IONIZATION:3||VACUUM:3||SCATTERING:3||IONS:2||LUMINESCENCE PROPERTIES:2||ANISOTROPY:2||BEAMS:2||DIFFRACTION:2||DISPERSION:2||chemical vapor deposition (CVD):2||ELECTRONICSTRUCTURE:2||MOSFETS:2||SI3N4:2||DENSITY:2||LIGHT:2||PLASMAS:2||MATTER:2||nanocomposites:2||RAMANSCATTERING:2||NANOPARTICLES:2||OXIDE:2||AMPLIFIED SPONTANEOUS EMISSION:2||NM WAVELENGTH:2||GAIN:2||CARBON NANOTUBES:2||CROSSSECTIONS:2||LIGHTEMITTINGDIODES:2||PULSE:2||CARBON PLASMA:2||TISAPPHIRE LASER:2||Raman scattering:2||ROUTE:2||multilayer:2||CATHODOLUMINESCENCE:2||highresolution transmission electronic microscope (HRTEM):2||DIFFERENCEFREQUENCYGENERATION:2||CRYSTAL:2||laserproduced plasma:2||NANOCABLES:2||photoluminescence:2||MAGNETIC ALLOY SEMICONDUCTORS:2||MOLECULARBEAM EPITAXY:2||EARTHDOPED GAN:2||LASER FIELDS:2||CHIRPEDPULSEAMPLIFICATION:2||ALN:2||GAUSSIANBEAM:2||ASSISTED CATALYTIC GROWTH:2||BLUE:2||NANOSTRUCTURES:2||MAGNETOELECTRONICS:2||MICROSCOPY:2||ELECTROLUMINESCENCE:2||LASERPULSES:2||GaN nanowires:2||GALLIUM NITRIDE NANOWIRES:2||GAMNN:2||NANOTUBES:2||PHYSICS:2||Femtosecond laser:2||parametric oscillators and amplifiers:1||ultrafast lasers:1||VALENCE:1||nanowires:1||DILUTED MAGNETIC SEMICONDUCTOR:1||LUMINESCENCE:1||Density modulation:1||Energy modulation:1||Current enhanced SASE free electron laser:1||Undulator radiation:1||FREEELECTRON LASERS:1||ULTRATHIN FERROMAGNETICFILMS:1||OXIDEFILMS:1||ABLATION:1||COMPONENT:1||METAL:1||innershell excited states:1||Nelike ions:1||TRANSITIONS:1||XUV spectrometer:1||DIAGNOSTICS:1||Xray scattering:1||MO/SI:1||pulsed laser deposition:1||KEV IMPACT ENERGIES:1||vacuum electron acceleration:1||HIGHINTENSITY LASER:1||JUNCTIONS:1||LOWTEMPERATURE GROWTH:1||nanocrystalline materials:1||MOLECULAR PHOTOIONIZATION:1||LOCALIZATION:1||DEUTERIUM CLUSTERS:1||EXPLOSIONS:1||REGENERATIVE AMPLIFIERS:1||RAREGASES:1||THz radiation:1||FREEELECTRON LASER:1||REALTIME OBSERVATION:1||TARGET:1||photoionized plasmas:1||fs Xray laser:1||emission profile:1||HIGHORDER HARMONICS:1||Xray laser:1||atomic transition:1||EXCITATION:1||LASERS:1||PERFORMANCE:1||RELATIVISTIC ELECTRONS:1||BI2O3DOPED ZNO:1||INNERSHELL IONIZATION:1||Laser wakefield:1||FREQUENCY:1||SOLIDSTATE LASERS:1||Linearly polarized:1||THERMIONIC EMISSION:1||PULSE AMPLIFICATION SYSTEM:1||BIB3O6:1||NM:1||NONCOVALENT INTERACTIONS:1||CRYSTALLINE:1||INTENSITY:1||JETS:1||COHERENT:1||LINE:1||ANGULARDISTRIBUTION:1||SILVER IONS:1||magnetic anisotropy:1||DEVICES:1||Auger transitions:1||CosterKronig transitions:1||EFFICIENT:1||ELECTRONIMPACT IONIZATION:1||ULTRASHORTPULSE:1||Nanowire:1||Heterostructure:1||soft Xray reflectivity:1||PLASMA ACCELERATOR:1||ZINCOXIDE NANOWIRES:1||CHEMICALVAPORDEPOSITION:1||Electron acceleration:1||Ionization of gases:1||Delay dependent:1||MULTIPHOTON IONIZATION:1||FRAGMENTATION:1||GASJET:1||ultrafast nonlinear optics:1||CYCLE PULSES:1||KHZ:1||chemical vapor deposition:1||ferromagnetism:1||ABSORPTION:1||TERAHERTZ RADIATION:1||SCIENCE:1||FIELDS:1||ELECTRONS:1||nanomultilayer structures:1||YIELDS:1||AUGER:1||10HZ REPETITION RATE:1||MULTITERAWATT:1||SPECTROGRAPH:1||HIGHHARMONICGENERATION:1||spectroscopy:1||level population:1||PARTICLEACCELERATION:1||OPTICAL FREQUENCYMEASUREMENT:1||NANOWALLS:1||ROOMTEMPERATURE:1||AVERAGE OUTPUT POWER:1||GROUPVELOCITYMISMATCH:1||Impact ionization:1||Dynamics:1||Lasers:1||Collisional process:1||ABOVETHRESHOLD IONIZATION:1||MAINGROUP THERMOCHEMISTRY:1||dilute magnetic semiconductors:1||GACRN:1||SIZE:1||ATTOSECOND:1||Ar cluster:1||Xray astrophysics:1||photoionization:1||irons:1||normal incidence pulsed laser deposition:1||SHELLS:1||Silicon Oxide:1||gaspuff Zpinch:1||Xray:1||soft Xray reflectors:1||ESCAPE:1||ZN2SIO4:1||SILICA:1||Time delay:1||Collisional plasmas:1||MASSSPECTROMETRY:1||NUCLEARFUSION:1||PARAMETRIC AMPLIFICATION:1||LYING ELECTRONIC STATES:1||ADJUSTABLEPARAMETERS:1||MAGNETICPROPERTIES:1||LIQUIDPHASE EPITAXY:1||CEP laser:1||REGION:1||Plasma waveguide:1||AMBIENT GAS:1||DEPOSITION:1||HARMONICGENERATION:1||ENHANCEMENT:1||imaging spectrometer:1||Abel inversion:1||Water window:1||Liquid nitrogen jet:1||CHARGEEXCHANGE:1||NOBEL LECTURE:1||VARISTOR:1||EPITAXY:1||THINDISK LASER:1||HIGHREPETITIONRATE:1||Atom lasers:1||Electronimpact excitation:1||High order harmonics:1||ultrafast technology:1||PEAK POWER:1||CHARGED ALUMINUM CLUSTERS:1||GaN:1||THIN:1||Electron beam:1||INTENSE:1||Hard Xray pulse generation:1||NONLINEAR THOMSON SCATTERING:1||MULTILAYER:1||UVvisible spectrometer:1||ATOMS:1||innershell transitions:1||CORRECTED CONCAVE GRATINGS:1||DISCHARGE:1||LASERPLASMA:1||thin film:1||reflectivity:1||opacity:1||gain:1||smallangle Xray scattering:1||SOFTXRAY:1||ZINCOXIDE:1||CYGNUSX3:1||Betatron oscillation:1||ACCELERATOR:1||STRAINEDLAYER SUPERLATTICES:1||OPTICAL PARAMETRIC AMPLIFICATION:1||PASSIVE MODELOCKING:1||Collision dynamics:1||MUM:1||EXACTEXCHANGE:1||BASISSET:1||APPROXIMATION:1||OXYNITRIDES:1||Beam energy modulation:1||polarization spectroscopy:1||REORIENTATION TRANSITION:1||DEPENDENCE:1||sulfurs:1||BUILDINGBLOCKS:1||RATES:1||OPTICAL PULSES:1||toroidal mirror:1||XRAY LASER:1||CALCIUM:1||radially polarized laser:1||GRAINBOUNDARIES:1||VAPORDEPOSITION:1||Xray generation:1||MAGNETIZATION:1||Electric excitation:1||Laserinduced gas plasmas:1||Qualitative analysis:1||SCHEME:1||RADIATION:10||PULSES:8||PHOTOLUMINESCENCE:7||LASER:7||GENERATION:6||NANORODS:6||GROWTH:6||NANOWIRES:5||IMPLANTED 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SEMICONDUCTORS:2||MOLECULARBEAM EPITAXY:2||EARTHDOPED GAN:2||LASER FIELDS:2||CHIRPEDPULSEAMPLIFICATION:2||ALN:2||GAUSSIANBEAM:2||ASSISTED CATALYTIC GROWTH:2||BLUE:2||NANOSTRUCTURES:2||MAGNETOELECTRONICS:2||MICROSCOPY:2||ELECTROLUMINESCENCE:2||LASERPULSES:2||GaN nanowires:2||GALLIUM NITRIDE NANOWIRES:2||GAMNN:2||NANOTUBES:2||PHYSICS:2||Femtosecond laser:2||parametric oscillators and amplifiers:1||ultrafast lasers:1||VALENCE:1||nanowires:1||DILUTED MAGNETIC SEMICONDUCTOR:1||LUMINESCENCE:1||Density modulation:1||Energy modulation:1||Current enhanced SASE free electron laser:1||Undulator radiation:1||FREEELECTRON LASERS:1||ULTRATHIN FERROMAGNETICFILMS:1||OXIDEFILMS:1||ABLATION:1||COMPONENT:1||METAL:1||innershell excited states:1||Nelike ions:1||TRANSITIONS:1||XUV spectrometer:1||DIAGNOSTICS:1||Xray scattering:1||MO/SI:1||pulsed laser deposition:1||KEV IMPACT ENERGIES:1||vacuum electron acceleration:1||HIGHINTENSITY LASER:1||JUNCTIONS:1||LOWTEMPERATURE GROWTH:1||nanocrystalline materials:1||MOLECULAR PHOTOIONIZATION:1||LOCALIZATION:1||DEUTERIUM CLUSTERS:1||EXPLOSIONS:1||REGENERATIVE AMPLIFIERS:1||RAREGASES:1||THz radiation:1||FREEELECTRON LASER:1||REALTIME OBSERVATION:1||TARGET:1||photoionized plasmas:1||fs Xray laser:1||emission profile:1||HIGHORDER HARMONICS:1||Xray laser:1||atomic transition:1||EXCITATION:1||LASERS:1||PERFORMANCE:1||RELATIVISTIC ELECTRONS:1||BI2O3DOPED ZNO:1||INNERSHELL IONIZATION:1||Laser wakefield:1||FREQUENCY:1||SOLIDSTATE LASERS:1||Linearly polarized:1||THERMIONIC EMISSION:1||PULSE AMPLIFICATION SYSTEM:1||BIB3O6:1||NM:1||NONCOVALENT INTERACTIONS:1||CRYSTALLINE:1||INTENSITY:1||JETS:1||COHERENT:1||LINE:1||ANGULARDISTRIBUTION:1||SILVER IONS:1||magnetic anisotropy:1||DEVICES:1||Auger transitions:1||CosterKronig transitions:1||EFFICIENT:1||ELECTRONIMPACT IONIZATION:1||ULTRASHORTPULSE:1||Nanowire:1||Heterostructure:1||soft Xray reflectivity:1||PLASMA ACCELERATOR:1||ZINCOXIDE NANOWIRES:1||CHEMICALVAPORDEPOSITION:1||Electron acceleration:1||Ionization of gases:1||Delay dependent:1||MULTIPHOTON IONIZATION:1||FRAGMENTATION:1||GASJET:1||ultrafast nonlinear optics:1||CYCLE PULSES:1||KHZ:1||chemical vapor deposition:1||ferromagnetism:1||ABSORPTION:1||TERAHERTZ RADIATION:1||SCIENCE:1||FIELDS:1||ELECTRONS:1||nanomultilayer structures:1||YIELDS:1||AUGER:1||10HZ REPETITION RATE:1||MULTITERAWATT:1||SPECTROGRAPH:1||HIGHHARMONICGENERATION:1||spectroscopy:1||level population:1||PARTICLEACCELERATION:1||OPTICAL FREQUENCYMEASUREMENT:1||NANOWALLS:1||ROOMTEMPERATURE:1||AVERAGE OUTPUT POWER:1||GROUPVELOCITYMISMATCH:1||Impact ionization:1||Dynamics:1||Lasers:1||Collisional process:1||ABOVETHRESHOLD IONIZATION:1||MAINGROUP THERMOCHEMISTRY:1||dilute magnetic semiconductors:1||GACRN:1||SIZE:1||ATTOSECOND:1||Ar cluster:1||Xray astrophysics:1||photoionization:1||irons:1||normal incidence pulsed laser deposition:1||SHELLS:1||Silicon Oxide:1||gaspuff Zpinch:1||Xray:1||soft Xray reflectors:1||ESCAPE:1||ZN2SIO4:1||SILICA:1||Time 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materials:1||MOLECULAR PHOTOIONIZATION:1||LOCALIZATION:1||DEUTERIUM CLUSTERS:1||EXPLOSIONS:1||REGENERATIVE AMPLIFIERS:1||RAREGASES:1||THz radiation:1||FREEELECTRON LASER:1||REALTIME OBSERVATION:1||TARGET:1||photoionized plasmas:1||fs Xray laser:1||emission profile:1||HIGHORDER HARMONICS:1||Xray laser:1||atomic transition:1||EXCITATION:1||LASERS:1||PERFORMANCE:1||RELATIVISTIC ELECTRONS:1||BI2O3DOPED ZNO:1||INNERSHELL IONIZATION:1||Laser wakefield:1||FREQUENCY:1||SOLIDSTATE LASERS:1||Linearly polarized:1||THERMIONIC EMISSION:1||PULSE AMPLIFICATION SYSTEM:1||BIB3O6:1||NM:1||NONCOVALENT INTERACTIONS:1||CRYSTALLINE:1||INTENSITY:1||JETS:1||COHERENT:1||LINE:1||ANGULARDISTRIBUTION:1||SILVER IONS:1||magnetic anisotropy:1||DEVICES:1||Auger transitions:1||CosterKronig transitions:1||EFFICIENT:1||ELECTRONIMPACT IONIZATION:1||ULTRASHORTPULSE:1||Nanowire:1||Heterostructure:1||soft Xray reflectivity:1||PLASMA ACCELERATOR:1||ZINCOXIDE NANOWIRES:1||CHEMICALVAPORDEPOSITION:1||Electron acceleration:1||Ionization of gases:1||Delay dependent:1||MULTIPHOTON IONIZATION:1||FRAGMENTATION:1||GASJET:1||ultrafast nonlinear optics:1||CYCLE PULSES:1||KHZ:1||chemical vapor deposition:1||ferromagnetism:1||ABSORPTION:1||TERAHERTZ RADIATION:1||SCIENCE:1||FIELDS:1||ELECTRONS:1||nanomultilayer structures:1||YIELDS:1||AUGER:1||10HZ REPETITION RATE:1||MULTITERAWATT:1||SPECTROGRAPH:1||HIGHHARMONICGENERATION:1||spectroscopy:1||level population:1||PARTICLEACCELERATION:1||OPTICAL FREQUENCYMEASUREMENT:1||NANOWALLS:1||ROOMTEMPERATURE:1||AVERAGE OUTPUT POWER:1||GROUPVELOCITYMISMATCH:1||Impact ionization:1||Dynamics:1||Lasers:1||Collisional process:1||ABOVETHRESHOLD IONIZATION:1||MAINGROUP THERMOCHEMISTRY:1||dilute magnetic semiconductors:1||GACRN:1||SIZE:1||ATTOSECOND:1||Ar cluster:1||Xray astrophysics:1||photoionization:1||irons:1||normal incidence pulsed laser deposition:1||SHELLS:1||Silicon Oxide:1||gaspuff Zpinch:1||Xray:1||soft Xray reflectors:1||ESCAPE:1||ZN2SIO4:1||SILICA:1||Time delay:1||Collisional plasmas:1||MASSSPECTROMETRY:1||NUCLEARFUSION:1||PARAMETRIC AMPLIFICATION:1||LYING ELECTRONIC STATES:1||ADJUSTABLEPARAMETERS:1||MAGNETICPROPERTIES:1||LIQUIDPHASE EPITAXY:1||CEP laser:1||REGION:1||Plasma waveguide:1||AMBIENT GAS:1||DEPOSITION:1||HARMONICGENERATION:1||ENHANCEMENT:1||imaging spectrometer:1||Abel inversion:1||Water window:1||Liquid nitrogen jet:1||CHARGEEXCHANGE:1||NOBEL LECTURE:1||VARISTOR:1||EPITAXY:1||THINDISK LASER:1||HIGHREPETITIONRATE:1||Atom lasers:1||Electronimpact excitation:1||High order harmonics:1||ultrafast technology:1||PEAK POWER:1||CHARGED ALUMINUM CLUSTERS:1||GaN:1||THIN:1||Electron beam:1||INTENSE:1||Hard Xray pulse generation:1||NONLINEAR THOMSON SCATTERING:1||MULTILAYER:1||UVvisible spectrometer:1||ATOMS:1||innershell transitions:1||CORRECTED CONCAVE GRATINGS:1||DISCHARGE:1||LASERPLASMA:1||thin film:1||reflectivity:1||opacity:1||gain:1||smallangle Xray scattering:1||SOFTXRAY:1||ZINCOXIDE:1||CYGNUSX3:1||Betatron oscillation:1||ACCELERATOR:1||STRAINEDLAYER SUPERLATTICES:1||OPTICAL PARAMETRIC AMPLIFICATION:1||PASSIVE MODELOCKING:1||Collision dynamics:1||MUM:1||EXACTEXCHANGE:1||BASISSET:1||APPROXIMATION:1||OXYNITRIDES:1||Beam energy modulation:1||polarization spectroscopy:1||REORIENTATION TRANSITION:1||DEPENDENCE:1||sulfurs:1||BUILDINGBLOCKS:1||RATES:1||OPTICAL PULSES:1||toroidal mirror:1||XRAY LASER:1||CALCIUM:1||radially polarized laser:1||GRAINBOUNDARIES:1||VAPORDEPOSITION:1||Xray generation:1||MAGNETIZATION:1||Electric excitation:1||Laserinduced gas plasmas:1||Qualitative analysis:1||SCHEME:1||RADIATION:10||PULSES:8||PHOTOLUMINESCENCE:7||LASER:7||GENERATION:6||NANORODS:6||GROWTH:6||NANOWIRES:5||IMPLANTED GAN:5||SPECTROSCOPY:5||THINFILMS:4||DYNAMICS:4||SILICON:4||EXTREMEULTRAVIOLET:4||AMPLIFICATION:4||PRESSURE:4||PHASE:4||OPTICALPROPERTIES:4||SYSTEM:4||EMISSION:4||FEL:3||N2O:3||FILMS:3||OPTICS:3||SPECTRA:3||FIELD:3||MIRRORS:3||ARRAYS:3||CLUSTERS:3||SIO2:3||IONIZATION:3||VACUUM:3||SCATTERING:3||IONS:2||LUMINESCENCE PROPERTIES:2||ANISOTROPY:2||BEAMS:2||DIFFRACTION:2||DISPERSION:2||chemical vapor deposition (CVD):2||ELECTRONICSTRUCTURE:2||MOSFETS:2||SI3N4:2||DENSITY:2||LIGHT:2||PLASMAS:2||MATTER:2||nanocomposites:2||RAMANSCATTERING:2||NANOPARTICLES:2||OXIDE:2||AMPLIFIED SPONTANEOUS EMISSION:2||NM WAVELENGTH:2||GAIN:2||CARBON NANOTUBES:2||CROSSSECTIONS:2||LIGHTEMITTINGDIODES:2||PULSE:2||CARBON PLASMA:2||TISAPPHIRE LASER:2||Raman scattering:2||ROUTE:2||multilayer:2||CATHODOLUMINESCENCE:2||highresolution transmission electronic microscope (HRTEM):2||DIFFERENCEFREQUENCYGENERATION:2||CRYSTAL:2||laserproduced plasma:2||NANOCABLES:2||photoluminescence:2||MAGNETIC ALLOY SEMICONDUCTORS:2||MOLECULARBEAM EPITAXY:2||EARTHDOPED GAN:2||LASER FIELDS:2||CHIRPEDPULSEAMPLIFICATION:2||ALN:2||GAUSSIANBEAM:2||ASSISTED CATALYTIC GROWTH:2||BLUE:2||NANOSTRUCTURES:2||MAGNETOELECTRONICS:2||MICROSCOPY:2||ELECTROLUMINESCENCE:2||LASERPULSES:2||GaN nanowires:2||GALLIUM NITRIDE NANOWIRES:2||GAMNN:2||NANOTUBES:2||PHYSICS:2||Femtosecond laser:2||parametric oscillators and amplifiers:1||ultrafast lasers:1||VALENCE:1||nanowires:1||DILUTED MAGNETIC SEMICONDUCTOR:1||LUMINESCENCE:1||Density modulation:1||Energy modulation:1||Current enhanced SASE free electron laser:1||Undulator radiation:1||FREEELECTRON LASERS:1||ULTRATHIN FERROMAGNETICFILMS:1||OXIDEFILMS:1||ABLATION:1||COMPONENT:1||METAL:1||innershell excited states:1||Nelike ions:1||TRANSITIONS:1||XUV spectrometer:1||DIAGNOSTICS:1||Xray scattering:1||MO/SI:1||pulsed laser deposition:1||KEV IMPACT ENERGIES:1||vacuum electron acceleration:1||HIGHINTENSITY LASER:1||JUNCTIONS:1||LOWTEMPERATURE GROWTH:1||nanocrystalline materials:1||MOLECULAR PHOTOIONIZATION:1||LOCALIZATION:1||DEUTERIUM CLUSTERS:1||EXPLOSIONS:1||REGENERATIVE AMPLIFIERS:1||RAREGASES:1||THz radiation:1||FREEELECTRON LASER:1||REALTIME OBSERVATION:1||TARGET:1||photoionized plasmas:1||fs Xray laser:1||emission profile:1||HIGHORDER HARMONICS:1||Xray laser:1||atomic transition:1||EXCITATION:1||LASERS:1||PERFORMANCE:1||RELATIVISTIC ELECTRONS:1||BI2O3DOPED ZNO:1||INNERSHELL IONIZATION:1||Laser wakefield:1||FREQUENCY:1||SOLIDSTATE LASERS:1||Linearly polarized:1||THERMIONIC EMISSION:1||PULSE AMPLIFICATION SYSTEM:1||BIB3O6:1||NM:1||NONCOVALENT INTERACTIONS:1||CRYSTALLINE:1||INTENSITY:1||JETS:1||COHERENT:1||LINE:1||ANGULARDISTRIBUTION:1||SILVER IONS:1||magnetic anisotropy:1||DEVICES:1||Auger transitions:1||CosterKronig transitions:1||EFFICIENT:1||ELECTRONIMPACT IONIZATION:1||ULTRASHORTPULSE:1||Nanowire:1||Heterostructure:1||soft Xray reflectivity:1||PLASMA ACCELERATOR:1||ZINCOXIDE NANOWIRES:1||CHEMICALVAPORDEPOSITION:1||Electron acceleration:1||Ionization of gases:1||Delay dependent:1||MULTIPHOTON IONIZATION:1||FRAGMENTATION:1||GASJET:1||ultrafast nonlinear optics:1||CYCLE PULSES:1||KHZ:1||chemical vapor deposition:1||ferromagnetism:1||ABSORPTION:1||TERAHERTZ RADIATION:1||SCIENCE:1||FIELDS:1||ELECTRONS:1||nanomultilayer structures:1||YIELDS:1||AUGER:1||10HZ REPETITION RATE:1||MULTITERAWATT:1||SPECTROGRAPH:1||HIGHHARMONICGENERATION:1||spectroscopy:1||level population:1||PARTICLEACCELERATION:1||OPTICAL FREQUENCYMEASUREMENT:1||NANOWALLS:1||ROOMTEMPERATURE:1||AVERAGE OUTPUT POWER:1||GROUPVELOCITYMISMATCH:1||Impact ionization:1||Dynamics:1||Lasers:1||Collisional process:1||ABOVETHRESHOLD IONIZATION:1||MAINGROUP THERMOCHEMISTRY:1||dilute magnetic semiconductors:1||GACRN:1||SIZE:1||ATTOSECOND:1||Ar cluster:1||Xray astrophysics:1||photoionization:1||irons:1||normal incidence pulsed laser deposition:1||SHELLS:1||Silicon Oxide:1||gaspuff Zpinch:1||Xray:1||soft Xray reflectors:1||ESCAPE:1||ZN2SIO4:1||SILICA:1||Time delay:1||Collisional plasmas:1||MASSSPECTROMETRY:1||NUCLEARFUSION:1||PARAMETRIC AMPLIFICATION:1||LYING ELECTRONIC STATES:1||ADJUSTABLEPARAMETERS:1||MAGNETICPROPERTIES:1||LIQUIDPHASE EPITAXY:1||CEP laser:1||REGION:1||Plasma waveguide:1||AMBIENT GAS:1||DEPOSITION:1||HARMONICGENERATION:1||ENHANCEMENT:1||imaging spectrometer:1||Abel inversion:1||Water window:1||Liquid nitrogen jet:1||CHARGEEXCHANGE:1||NOBEL LECTURE:1||VARISTOR:1||EPITAXY:1||THINDISK LASER:1||HIGHREPETITIONRATE:1||Atom lasers:1||Electronimpact excitation:1||High order harmonics:1||ultrafast technology:1||PEAK POWER:1||CHARGED ALUMINUM CLUSTERS:1||GaN:1||THIN:1||Electron beam:1||INTENSE:1||Hard Xray pulse generation:1||NONLINEAR THOMSON SCATTERING:1||MULTILAYER:1||UVvisible spectrometer:1||ATOMS:1||innershell transitions:1||CORRECTED CONCAVE GRATINGS:1||DISCHARGE:1||LASERPLASMA:1||thin film:1||reflectivity:1||opacity:1||gain:1||smallangle Xray scattering:1||SOFTXRAY:1||ZINCOXIDE:1||CYGNUSX3:1||Betatron oscillation:1||ACCELERATOR:1||STRAINEDLAYER SUPERLATTICES:1||OPTICAL PARAMETRIC AMPLIFICATION:1||PASSIVE MODELOCKING:1||Collision dynamics:1||MUM:1||EXACTEXCHANGE:1||BASISSET:1||APPROXIMATION:1||OXYNITRIDES:1||Beam energy modulation:1||polarization spectroscopy:1||REORIENTATION TRANSITION:1||DEPENDENCE:1||sulfurs:1||BUILDINGBLOCKS:1||RATES:1||OPTICAL PULSES:1||toroidal mirror:1||XRAY LASER:1||CALCIUM:1||radially polarized laser:1||GRAINBOUNDARIES:1||VAPORDEPOSITION:1||Xray generation:1||MAGNETIZATION:1||Electric excitation:1||Laserinduced gas plasmas:1||Qualitative analysis:1||SCHEME:1||RADIATION:10||PULSES:8||PHOTOLUMINESCENCE:7||LASER:7||GENERATION:6||NANORODS:6||GROWTH:6||NANOWIRES:5||IMPLANTED 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SEMICONDUCTORS:2||MOLECULARBEAM EPITAXY:2||EARTHDOPED GAN:2||LASER FIELDS:2||CHIRPEDPULSEAMPLIFICATION:2||ALN:2||GAUSSIANBEAM:2||ASSISTED CATALYTIC GROWTH:2||BLUE:2||NANOSTRUCTURES:2||MAGNETOELECTRONICS:2||MICROSCOPY:2||ELECTROLUMINESCENCE:2||LASERPULSES:2||GaN nanowires:2||GALLIUM NITRIDE NANOWIRES:2||GAMNN:2||NANOTUBES:2||PHYSICS:2||Femtosecond laser:2||parametric oscillators and amplifiers:1||ultrafast lasers:1||VALENCE:1||nanowires:1||DILUTED MAGNETIC SEMICONDUCTOR:1||LUMINESCENCE:1||Density modulation:1||Energy modulation:1||Current enhanced SASE free electron laser:1||Undulator radiation:1||FREEELECTRON LASERS:1||ULTRATHIN FERROMAGNETICFILMS:1||OXIDEFILMS:1||ABLATION:1||COMPONENT:1||METAL:1||innershell excited states:1||Nelike ions:1||TRANSITIONS:1||XUV spectrometer:1||DIAGNOSTICS:1||Xray scattering:1||MO/SI:1||pulsed laser deposition:1||KEV IMPACT ENERGIES:1||vacuum electron acceleration:1||HIGHINTENSITY LASER:1||JUNCTIONS:1||LOWTEMPERATURE GROWTH:1||nanocrystalline materials:1||MOLECULAR PHOTOIONIZATION:1||LOCALIZATION:1||DEUTERIUM CLUSTERS:1||EXPLOSIONS:1||REGENERATIVE AMPLIFIERS:1||RAREGASES:1||THz radiation:1||FREEELECTRON LASER:1||REALTIME OBSERVATION:1||TARGET:1||photoionized plasmas:1||fs Xray laser:1||emission profile:1||HIGHORDER HARMONICS:1||Xray laser:1||atomic transition:1||EXCITATION:1||LASERS:1||PERFORMANCE:1||RELATIVISTIC ELECTRONS:1||BI2O3DOPED ZNO:1||INNERSHELL IONIZATION:1||Laser wakefield:1||FREQUENCY:1||SOLIDSTATE LASERS:1||Linearly polarized:1||THERMIONIC EMISSION:1||PULSE AMPLIFICATION SYSTEM:1||BIB3O6:1||NM:1||NONCOVALENT INTERACTIONS:1||CRYSTALLINE:1||INTENSITY:1||JETS:1||COHERENT:1||LINE:1||ANGULARDISTRIBUTION:1||SILVER IONS:1||magnetic anisotropy:1||DEVICES:1||Auger transitions:1||CosterKronig transitions:1||EFFICIENT:1||ELECTRONIMPACT IONIZATION:1||ULTRASHORTPULSE:1||Nanowire:1||Heterostructure:1||soft Xray reflectivity:1||PLASMA ACCELERATOR:1||ZINCOXIDE NANOWIRES:1||CHEMICALVAPORDEPOSITION:1||Electron acceleration:1||Ionization of gases:1||Delay dependent:1||MULTIPHOTON IONIZATION:1||FRAGMENTATION:1||GASJET:1||ultrafast nonlinear optics:1||CYCLE PULSES:1||KHZ:1||chemical vapor deposition:1||ferromagnetism:1||ABSORPTION:1||TERAHERTZ RADIATION:1||SCIENCE:1||FIELDS:1||ELECTRONS:1||nanomultilayer structures:1||YIELDS:1||AUGER:1||10HZ REPETITION RATE:1||MULTITERAWATT:1||SPECTROGRAPH:1||HIGHHARMONICGENERATION:1||spectroscopy:1||level population:1||PARTICLEACCELERATION:1||OPTICAL FREQUENCYMEASUREMENT:1||NANOWALLS:1||ROOMTEMPERATURE:1||AVERAGE OUTPUT POWER:1||GROUPVELOCITYMISMATCH:1||Impact ionization:1||Dynamics:1||Lasers:1||Collisional process:1||ABOVETHRESHOLD IONIZATION:1||MAINGROUP THERMOCHEMISTRY:1||dilute magnetic semiconductors:1||GACRN:1||SIZE:1||ATTOSECOND:1||Ar cluster:1||Xray astrophysics:1||photoionization:1||irons:1||normal incidence pulsed laser deposition:1||SHELLS:1||Silicon Oxide:1||gaspuff Zpinch:1||Xray:1||soft Xray reflectors:1||ESCAPE:1||ZN2SIO4:1||SILICA:1||Time 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materials:1||MOLECULAR PHOTOIONIZATION:1||LOCALIZATION:1||DEUTERIUM CLUSTERS:1||EXPLOSIONS:1||REGENERATIVE AMPLIFIERS:1||RAREGASES:1||THz radiation:1||FREEELECTRON LASER:1||REALTIME OBSERVATION:1||TARGET:1||photoionized plasmas:1||fs Xray laser:1||emission profile:1||HIGHORDER HARMONICS:1||Xray laser:1||atomic transition:1||EXCITATION:1||LASERS:1||PERFORMANCE:1||RELATIVISTIC ELECTRONS:1||BI2O3DOPED ZNO:1||INNERSHELL IONIZATION:1||Laser wakefield:1||FREQUENCY:1||SOLIDSTATE LASERS:1||Linearly polarized:1||THERMIONIC EMISSION:1||PULSE AMPLIFICATION SYSTEM:1||BIB3O6:1||NM:1||NONCOVALENT INTERACTIONS:1||CRYSTALLINE:1||INTENSITY:1||JETS:1||COHERENT:1||LINE:1||ANGULARDISTRIBUTION:1||SILVER IONS:1||magnetic anisotropy:1||DEVICES:1||Auger transitions:1||CosterKronig transitions:1||EFFICIENT:1||ELECTRONIMPACT IONIZATION:1||ULTRASHORTPULSE:1||Nanowire:1||Heterostructure:1||soft Xray reflectivity:1||PLASMA ACCELERATOR:1||ZINCOXIDE NANOWIRES:1||CHEMICALVAPORDEPOSITION:1||Electron acceleration:1||Ionization of gases:1||Delay dependent:1||MULTIPHOTON IONIZATION:1||FRAGMENTATION:1||GASJET:1||ultrafast nonlinear optics:1||CYCLE PULSES:1||KHZ:1||chemical vapor deposition:1||ferromagnetism:1||ABSORPTION:1||TERAHERTZ RADIATION:1||SCIENCE:1||FIELDS:1||ELECTRONS:1||nanomultilayer structures:1||YIELDS:1||AUGER:1||10HZ REPETITION RATE:1||MULTITERAWATT:1||SPECTROGRAPH:1||HIGHHARMONICGENERATION:1||spectroscopy:1||level population:1||PARTICLEACCELERATION:1||OPTICAL FREQUENCYMEASUREMENT:1||NANOWALLS:1||ROOMTEMPERATURE:1||AVERAGE OUTPUT POWER:1||GROUPVELOCITYMISMATCH:1||Impact ionization:1||Dynamics:1||Lasers:1||Collisional process:1||ABOVETHRESHOLD IONIZATION:1||MAINGROUP THERMOCHEMISTRY:1||dilute magnetic semiconductors:1||GACRN:1||SIZE:1||ATTOSECOND:1||Ar cluster:1||Xray astrophysics:1||photoionization:1||irons:1||normal incidence pulsed laser deposition:1||SHELLS:1||Silicon Oxide:1||gaspuff Zpinch:1||Xray:1||soft Xray reflectors:1||ESCAPE:1||ZN2SIO4:1||SILICA:1||Time delay:1||Collisional plasmas:1||MASSSPECTROMETRY:1||NUCLEARFUSION:1||PARAMETRIC AMPLIFICATION:1||LYING ELECTRONIC STATES:1||ADJUSTABLEPARAMETERS:1||MAGNETICPROPERTIES:1||LIQUIDPHASE EPITAXY:1||CEP laser:1||REGION:1||Plasma waveguide:1||AMBIENT GAS:1||DEPOSITION:1||HARMONICGENERATION:1||ENHANCEMENT:1||imaging spectrometer:1||Abel inversion:1||Water window:1||Liquid nitrogen jet:1||CHARGEEXCHANGE:1||NOBEL LECTURE:1||VARISTOR:1||EPITAXY:1||THINDISK LASER:1||HIGHREPETITIONRATE:1||Atom lasers:1||Electronimpact excitation:1||High order harmonics:1||ultrafast technology:1||PEAK POWER:1||CHARGED ALUMINUM CLUSTERS:1||GaN:1||THIN:1||Electron beam:1||INTENSE:1||Hard Xray pulse generation:1||NONLINEAR THOMSON SCATTERING:1||MULTILAYER:1||UVvisible spectrometer:1||ATOMS:1||innershell transitions:1||CORRECTED CONCAVE GRATINGS:1||DISCHARGE:1||LASERPLASMA:1||thin film:1||reflectivity:1||opacity:1||gain:1||smallangle Xray scattering:1||SOFTXRAY:1||ZINCOXIDE:1||CYGNUSX3:1||Betatron oscillation:1||ACCELERATOR:1||STRAINEDLAYER SUPERLATTICES:1||OPTICAL PARAMETRIC AMPLIFICATION:1||PASSIVE MODELOCKING:1||Collision dynamics:1||MUM:1||EXACTEXCHANGE:1||BASISSET:1||APPROXIMATION:1||OXYNITRIDES:1||Beam energy modulation:1||polarization spectroscopy:1||REORIENTATION TRANSITION:1||DEPENDENCE:1||sulfurs:1||BUILDINGBLOCKS:1||RATES:1||OPTICAL PULSES:1||toroidal mirror:1||XRAY LASER:1||CALCIUM:1||radially polarized laser:1||GRAINBOUNDARIES:1||VAPORDEPOSITION:1||Xray generation:1||MAGNETIZATION:1||Electric excitation:1||Laserinduced gas plasmas:1||Qualitative analysis:1||SCHEME:1||RADIATION:10||PULSES:8||PHOTOLUMINESCENCE:7||LASER:7||GENERATION:6||NANORODS:6||GROWTH:6||NANOWIRES:5||IMPLANTED GAN:5||SPECTROSCOPY:5||THINFILMS:4||DYNAMICS:4||SILICON:4||EXTREMEULTRAVIOLET:4||AMPLIFICATION:4||PRESSURE:4||PHASE:4||OPTICALPROPERTIES:4||SYSTEM:4||EMISSION:4||FEL:3||N2O:3||FILMS:3||OPTICS:3||SPECTRA:3||FIELD:3||MIRRORS:3||ARRAYS:3||CLUSTERS:3||SIO2:3||IONIZATION:3||VACUUM:3||SCATTERING:3||IONS:2||LUMINESCENCE PROPERTIES:2||ANISOTROPY:2||BEAMS:2||DIFFRACTION:2||DISPERSION:2||chemical vapor deposition (CVD):2||ELECTRONICSTRUCTURE:2||MOSFETS:2||SI3N4:2||DENSITY:2||LIGHT:2||PLASMAS:2||MATTER:2||nanocomposites:2||RAMANSCATTERING:2||NANOPARTICLES:2||OXIDE:2||AMPLIFIED SPONTANEOUS EMISSION:2||NM WAVELENGTH:2||GAIN:2||CARBON NANOTUBES:2||CROSSSECTIONS:2||LIGHTEMITTINGDIODES:2||PULSE:2||CARBON PLASMA:2||TISAPPHIRE LASER:2||Raman scattering:2||ROUTE:2||multilayer:2||CATHODOLUMINESCENCE:2||highresolution transmission electronic microscope (HRTEM):2||DIFFERENCEFREQUENCYGENERATION:2||CRYSTAL:2||laserproduced plasma:2||NANOCABLES:2||photoluminescence:2||MAGNETIC ALLOY SEMICONDUCTORS:2||MOLECULARBEAM EPITAXY:2||EARTHDOPED GAN:2||LASER FIELDS:2||CHIRPEDPULSEAMPLIFICATION:2||ALN:2||GAUSSIANBEAM:2||ASSISTED CATALYTIC GROWTH:2||BLUE:2||NANOSTRUCTURES:2||MAGNETOELECTRONICS:2||MICROSCOPY:2||ELECTROLUMINESCENCE:2||LASERPULSES:2||GaN nanowires:2||GALLIUM NITRIDE NANOWIRES:2||GAMNN:2||NANOTUBES:2||PHYSICS:2||Femtosecond laser:2||parametric oscillators and amplifiers:1||ultrafast lasers:1||VALENCE:1||nanowires:1||DILUTED MAGNETIC SEMICONDUCTOR:1||LUMINESCENCE:1||Density modulation:1||Energy modulation:1||Current enhanced SASE free electron laser:1||Undulator radiation:1||FREEELECTRON LASERS:1||ULTRATHIN FERROMAGNETICFILMS:1||OXIDEFILMS:1||ABLATION:1||COMPONENT:1||METAL:1||innershell excited states:1||Nelike ions:1||TRANSITIONS:1||XUV spectrometer:1||DIAGNOSTICS:1||Xray scattering:1||MO/SI:1||pulsed laser deposition:1||KEV IMPACT ENERGIES:1||vacuum electron acceleration:1||HIGHINTENSITY LASER:1||JUNCTIONS:1||LOWTEMPERATURE GROWTH:1||nanocrystalline materials:1||MOLECULAR PHOTOIONIZATION:1||LOCALIZATION:1||DEUTERIUM CLUSTERS:1||EXPLOSIONS:1||REGENERATIVE AMPLIFIERS:1||RAREGASES:1||THz radiation:1||FREEELECTRON LASER:1||REALTIME OBSERVATION:1||TARGET:1||photoionized plasmas:1||fs Xray laser:1||emission profile:1||HIGHORDER HARMONICS:1||Xray laser:1||atomic transition:1||EXCITATION:1||LASERS:1||PERFORMANCE:1||RELATIVISTIC ELECTRONS:1||BI2O3DOPED ZNO:1||INNERSHELL IONIZATION:1||Laser wakefield:1||FREQUENCY:1||SOLIDSTATE LASERS:1||Linearly polarized:1||THERMIONIC EMISSION:1||PULSE AMPLIFICATION SYSTEM:1||BIB3O6:1||NM:1||NONCOVALENT INTERACTIONS:1||CRYSTALLINE:1||INTENSITY:1||JETS:1||COHERENT:1||LINE:1||ANGULARDISTRIBUTION:1||SILVER IONS:1||magnetic anisotropy:1||DEVICES:1||Auger transitions:1||CosterKronig transitions:1||EFFICIENT:1||ELECTRONIMPACT IONIZATION:1||ULTRASHORTPULSE:1||Nanowire:1||Heterostructure:1||soft Xray reflectivity:1||PLASMA ACCELERATOR:1||ZINCOXIDE NANOWIRES:1||CHEMICALVAPORDEPOSITION:1||Electron acceleration:1||Ionization of gases:1||Delay dependent:1||MULTIPHOTON IONIZATION:1||FRAGMENTATION:1||GASJET:1||ultrafast nonlinear optics:1||CYCLE PULSES:1||KHZ:1||chemical vapor deposition:1||ferromagnetism:1||ABSORPTION:1||TERAHERTZ RADIATION:1||SCIENCE:1||FIELDS:1||ELECTRONS:1||nanomultilayer structures:1||YIELDS:1||AUGER:1||10HZ REPETITION RATE:1||MULTITERAWATT:1||SPECTROGRAPH:1||HIGHHARMONICGENERATION:1||spectroscopy:1||level population:1||PARTICLEACCELERATION:1||OPTICAL FREQUENCYMEASUREMENT:1||NANOWALLS:1||ROOMTEMPERATURE:1||AVERAGE OUTPUT POWER:1||GROUPVELOCITYMISMATCH:1||Impact ionization:1||Dynamics:1||Lasers:1||Collisional process:1||ABOVETHRESHOLD IONIZATION:1||MAINGROUP THERMOCHEMISTRY:1||dilute magnetic semiconductors:1||GACRN:1||SIZE:1||ATTOSECOND:1||Ar cluster:1||Xray astrophysics:1||photoionization:1||irons:1||normal incidence pulsed laser deposition:1||SHELLS:1||Silicon Oxide:1||gaspuff Zpinch:1||Xray:1||soft Xray reflectors:1||ESCAPE:1||ZN2SIO4:1||SILICA:1||Time delay:1||Collisional plasmas:1||MASSSPECTROMETRY:1||NUCLEARFUSION:1||PARAMETRIC AMPLIFICATION:1||LYING ELECTRONIC STATES:1||ADJUSTABLEPARAMETERS:1||MAGNETICPROPERTIES:1||LIQUIDPHASE EPITAXY:1||CEP laser:1||REGION:1||Plasma waveguide:1||AMBIENT GAS:1||DEPOSITION:1||HARMONICGENERATION:1||ENHANCEMENT:1||imaging spectrometer:1||Abel inversion:1||Water window:1||Liquid nitrogen jet:1||CHARGEEXCHANGE:1||NOBEL LECTURE:1||VARISTOR:1||EPITAXY:1||THINDISK LASER:1||HIGHREPETITIONRATE:1||Atom lasers:1||Electronimpact excitation:1||High order harmonics:1||ultrafast technology:1||PEAK POWER:1||CHARGED ALUMINUM CLUSTERS:1||GaN:1||THIN:1||Electron beam:1||INTENSE:1||Hard Xray pulse generation:1||NONLINEAR THOMSON SCATTERING:1||MULTILAYER:1||UVvisible spectrometer:1||ATOMS:1||innershell transitions:1||CORRECTED CONCAVE GRATINGS:1||DISCHARGE:1||LASERPLASMA:1||thin film:1||reflectivity:1||opacity:1||gain:1||smallangle Xray scattering:1||SOFTXRAY:1||ZINCOXIDE:1||CYGNUSX3:1||Betatron oscillation:1||ACCELERATOR:1||STRAINEDLAYER SUPERLATTICES:1||OPTICAL PARAMETRIC AMPLIFICATION:1||PASSIVE MODELOCKING:1||Collision dynamics:1||MUM:1||EXACTEXCHANGE:1||BASISSET:1||APPROXIMATION:1||OXYNITRIDES:1||Beam energy modulation:1||polarization spectroscopy:1||REORIENTATION TRANSITION:1||DEPENDENCE:1||sulfurs:1||BUILDINGBLOCKS:1||RATES:1||OPTICAL PULSES:1||toroidal mirror:1||XRAY LASER:1||CALCIUM:1||radially polarized laser:1||GRAINBOUNDARIES:1||VAPORDEPOSITION:1||Xray generation:1||MAGNETIZATION:1||Electric excitation:1||Laserinduced gas plasmas:1||Qualitative analysis:1||SCHEME:1||RADIATION:10||PULSES:8||PHOTOLUMINESCENCE:7||LASER:7||GENERATION:6||NANORODS:6||GROWTH:6||NANOWIRES:5||IMPLANTED 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SEMICONDUCTORS:2||MOLECULARBEAM EPITAXY:2||EARTHDOPED GAN:2||LASER FIELDS:2||CHIRPEDPULSEAMPLIFICATION:2||ALN:2||GAUSSIANBEAM:2||ASSISTED CATALYTIC GROWTH:2||BLUE:2||NANOSTRUCTURES:2||MAGNETOELECTRONICS:2||MICROSCOPY:2||ELECTROLUMINESCENCE:2||LASERPULSES:2||GaN nanowires:2||GALLIUM NITRIDE NANOWIRES:2||GAMNN:2||NANOTUBES:2||PHYSICS:2||Femtosecond laser:2||parametric oscillators and amplifiers:1||ultrafast lasers:1||VALENCE:1||nanowires:1||DILUTED MAGNETIC SEMICONDUCTOR:1||LUMINESCENCE:1||Density modulation:1||Energy modulation:1||Current enhanced SASE free electron laser:1||Undulator radiation:1||FREEELECTRON LASERS:1||ULTRATHIN FERROMAGNETICFILMS:1||OXIDEFILMS:1||ABLATION:1||COMPONENT:1||METAL:1||innershell excited states:1||Nelike ions:1||TRANSITIONS:1||XUV spectrometer:1||DIAGNOSTICS:1||Xray scattering:1||MO/SI:1||pulsed laser deposition:1||KEV IMPACT ENERGIES:1||vacuum electron acceleration:1||HIGHINTENSITY LASER:1||JUNCTIONS:1||LOWTEMPERATURE GROWTH:1||nanocrystalline materials:1||MOLECULAR PHOTOIONIZATION:1||LOCALIZATION:1||DEUTERIUM CLUSTERS:1||EXPLOSIONS:1||REGENERATIVE AMPLIFIERS:1||RAREGASES:1||THz radiation:1||FREEELECTRON LASER:1||REALTIME OBSERVATION:1||TARGET:1||photoionized plasmas:1||fs Xray laser:1||emission profile:1||HIGHORDER HARMONICS:1||Xray laser:1||atomic transition:1||EXCITATION:1||LASERS:1||PERFORMANCE:1||RELATIVISTIC ELECTRONS:1||BI2O3DOPED ZNO:1||INNERSHELL IONIZATION:1||Laser wakefield:1||FREQUENCY:1||SOLIDSTATE LASERS:1||Linearly polarized:1||THERMIONIC EMISSION:1||PULSE AMPLIFICATION SYSTEM:1||BIB3O6:1||NM:1||NONCOVALENT INTERACTIONS:1||CRYSTALLINE:1||INTENSITY:1||JETS:1||COHERENT:1||LINE:1||ANGULARDISTRIBUTION:1||SILVER IONS:1||magnetic anisotropy:1||DEVICES:1||Auger transitions:1||CosterKronig transitions:1||EFFICIENT:1||ELECTRONIMPACT IONIZATION:1||ULTRASHORTPULSE:1||Nanowire:1||Heterostructure:1||soft Xray reflectivity:1||PLASMA ACCELERATOR:1||ZINCOXIDE NANOWIRES:1||CHEMICALVAPORDEPOSITION:1||Electron acceleration:1||Ionization of gases:1||Delay dependent:1||MULTIPHOTON IONIZATION:1||FRAGMENTATION:1||GASJET:1||ultrafast nonlinear optics:1||CYCLE PULSES:1||KHZ:1||chemical vapor deposition:1||ferromagnetism:1||ABSORPTION:1||TERAHERTZ RADIATION:1||SCIENCE:1||FIELDS:1||ELECTRONS:1||nanomultilayer structures:1||YIELDS:1||AUGER:1||10HZ REPETITION RATE:1||MULTITERAWATT:1||SPECTROGRAPH:1||HIGHHARMONICGENERATION:1||spectroscopy:1||level population:1||PARTICLEACCELERATION:1||OPTICAL FREQUENCYMEASUREMENT:1||NANOWALLS:1||ROOMTEMPERATURE:1||AVERAGE OUTPUT POWER:1||GROUPVELOCITYMISMATCH:1||Impact ionization:1||Dynamics:1||Lasers:1||Collisional process:1||ABOVETHRESHOLD IONIZATION:1||MAINGROUP THERMOCHEMISTRY:1||dilute magnetic semiconductors:1||GACRN:1||SIZE:1||ATTOSECOND:1||Ar cluster:1||Xray astrophysics:1||photoionization:1||irons:1||normal incidence pulsed laser deposition:1||SHELLS:1||Silicon Oxide:1||gaspuff Zpinch:1||Xray:1||soft Xray reflectors:1||ESCAPE:1||ZN2SIO4:1||SILICA:1||Time 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materials:1||MOLECULAR PHOTOIONIZATION:1||LOCALIZATION:1||DEUTERIUM CLUSTERS:1||EXPLOSIONS:1||REGENERATIVE AMPLIFIERS:1||RAREGASES:1||THz radiation:1||FREEELECTRON LASER:1||REALTIME OBSERVATION:1||TARGET:1||photoionized plasmas:1||fs Xray laser:1||emission profile:1||HIGHORDER HARMONICS:1||Xray laser:1||atomic transition:1||EXCITATION:1||LASERS:1||PERFORMANCE:1||RELATIVISTIC ELECTRONS:1||BI2O3DOPED ZNO:1||INNERSHELL IONIZATION:1||Laser wakefield:1||FREQUENCY:1||SOLIDSTATE LASERS:1||Linearly polarized:1||THERMIONIC EMISSION:1||PULSE AMPLIFICATION SYSTEM:1||BIB3O6:1||NM:1||NONCOVALENT INTERACTIONS:1||CRYSTALLINE:1||INTENSITY:1||JETS:1||COHERENT:1||LINE:1||ANGULARDISTRIBUTION:1||SILVER IONS:1||magnetic anisotropy:1||DEVICES:1||Auger transitions:1||CosterKronig transitions:1||EFFICIENT:1||ELECTRONIMPACT IONIZATION:1||ULTRASHORTPULSE:1||Nanowire:1||Heterostructure:1||soft Xray reflectivity:1||PLASMA ACCELERATOR:1||ZINCOXIDE NANOWIRES:1||CHEMICALVAPORDEPOSITION:1||Electron acceleration:1||Ionization of gases:1||Delay dependent:1||MULTIPHOTON IONIZATION:1||FRAGMENTATION:1||GASJET:1||ultrafast nonlinear optics:1||CYCLE PULSES:1||KHZ:1||chemical vapor deposition:1||ferromagnetism:1||ABSORPTION:1||TERAHERTZ RADIATION:1||SCIENCE:1||FIELDS:1||ELECTRONS:1||nanomultilayer structures:1||YIELDS:1||AUGER:1||10HZ REPETITION RATE:1||MULTITERAWATT:1||SPECTROGRAPH:1||HIGHHARMONICGENERATION:1||spectroscopy:1||level population:1||PARTICLEACCELERATION:1||OPTICAL FREQUENCYMEASUREMENT:1||NANOWALLS:1||ROOMTEMPERATURE:1||AVERAGE OUTPUT POWER:1||GROUPVELOCITYMISMATCH:1||Impact ionization:1||Dynamics:1||Lasers:1||Collisional process:1||ABOVETHRESHOLD IONIZATION:1||MAINGROUP THERMOCHEMISTRY:1||dilute magnetic semiconductors:1||GACRN:1||SIZE:1||ATTOSECOND:1||Ar cluster:1||Xray astrophysics:1||photoionization:1||irons:1||normal incidence pulsed laser deposition:1||SHELLS:1||Silicon Oxide:1||gaspuff Zpinch:1||Xray:1||soft Xray reflectors:1||ESCAPE:1||ZN2SIO4:1||SILICA:1||Time delay:1||Collisional plasmas:1||MASSSPECTROMETRY:1||NUCLEARFUSION:1||PARAMETRIC AMPLIFICATION:1||LYING ELECTRONIC STATES:1||ADJUSTABLEPARAMETERS:1||MAGNETICPROPERTIES:1||LIQUIDPHASE EPITAXY:1||CEP laser:1||REGION:1||Plasma waveguide:1||AMBIENT GAS:1||DEPOSITION:1||HARMONICGENERATION:1||ENHANCEMENT:1||imaging spectrometer:1||Abel inversion:1||Water window:1||Liquid nitrogen jet:1||CHARGEEXCHANGE:1||NOBEL LECTURE:1||VARISTOR:1||EPITAXY:1||THINDISK LASER:1||HIGHREPETITIONRATE:1||Atom lasers:1||Electronimpact excitation:1||High order harmonics:1||ultrafast technology:1||PEAK POWER:1||CHARGED ALUMINUM CLUSTERS:1||GaN:1||THIN:1||Electron beam:1||INTENSE:1||Hard Xray pulse generation:1||NONLINEAR THOMSON SCATTERING:1||MULTILAYER:1||UVvisible spectrometer:1||ATOMS:1||innershell transitions:1||CORRECTED CONCAVE GRATINGS:1||DISCHARGE:1||LASERPLASMA:1||thin film:1||reflectivity:1||opacity:1||gain:1||smallangle Xray scattering:1||SOFTXRAY:1||ZINCOXIDE:1||CYGNUSX3:1||Betatron oscillation:1||ACCELERATOR:1||STRAINEDLAYER SUPERLATTICES:1||OPTICAL PARAMETRIC AMPLIFICATION:1||PASSIVE MODELOCKING:1||Collision dynamics:1||MUM:1||EXACTEXCHANGE:1||BASISSET:1||APPROXIMATION:1||OXYNITRIDES:1||Beam energy modulation:1||polarization spectroscopy:1||REORIENTATION TRANSITION:1||DEPENDENCE:1||sulfurs:1||BUILDINGBLOCKS:1||RATES:1||OPTICAL PULSES:1||toroidal mirror:1||XRAY LASER:1||CALCIUM:1||radially polarized laser:1||GRAINBOUNDARIES:1||VAPORDEPOSITION:1||Xray generation:1||MAGNETIZATION:1||Electric excitation:1||Laserinduced gas plasmas:1||Qualitative analysis:1||SCHEME:1||RADIATION:10||PULSES:8||PHOTOLUMINESCENCE:7||LASER:7||GENERATION:6||NANORODS:6||GROWTH:6||NANOWIRES:5||IMPLANTED GAN:5||SPECTROSCOPY:5||THINFILMS:4||DYNAMICS:4||SILICON:4||EXTREMEULTRAVIOLET:4||AMPLIFICATION:4||PRESSURE:4||PHASE:4||OPTICALPROPERTIES:4||SYSTEM:4||EMISSION:4||FEL:3||N2O:3||FILMS:3||OPTICS:3||SPECTRA:3||FIELD:3||MIRRORS:3||ARRAYS:3||CLUSTERS:3||SIO2:3||IONIZATION:3||VACUUM:3||SCATTERING:3||IONS:2||LUMINESCENCE PROPERTIES:2||ANISOTROPY:2||BEAMS:2||DIFFRACTION:2||DISPERSION:2||chemical vapor deposition (CVD):2||ELECTRONICSTRUCTURE:2||MOSFETS:2||SI3N4:2||DENSITY:2||LIGHT:2||PLASMAS:2||MATTER:2||nanocomposites:2||RAMANSCATTERING:2||NANOPARTICLES:2||OXIDE:2||AMPLIFIED SPONTANEOUS EMISSION:2||NM WAVELENGTH:2||GAIN:2||CARBON NANOTUBES:2||CROSSSECTIONS:2||LIGHTEMITTINGDIODES:2||PULSE:2||CARBON PLASMA:2||TISAPPHIRE LASER:2||Raman scattering:2||ROUTE:2||multilayer:2||CATHODOLUMINESCENCE:2||highresolution transmission electronic microscope (HRTEM):2||DIFFERENCEFREQUENCYGENERATION:2||CRYSTAL:2||laserproduced plasma:2||NANOCABLES:2||photoluminescence:2||MAGNETIC ALLOY SEMICONDUCTORS:2||MOLECULARBEAM EPITAXY:2||EARTHDOPED GAN:2||LASER FIELDS:2||CHIRPEDPULSEAMPLIFICATION:2||ALN:2||GAUSSIANBEAM:2||ASSISTED CATALYTIC GROWTH:2||BLUE:2||NANOSTRUCTURES:2||MAGNETOELECTRONICS:2||MICROSCOPY:2||ELECTROLUMINESCENCE:2||LASERPULSES:2||GaN nanowires:2||GALLIUM NITRIDE NANOWIRES:2||GAMNN:2||NANOTUBES:2||PHYSICS:2||Femtosecond laser:2||parametric oscillators and amplifiers:1||ultrafast lasers:1||VALENCE:1||nanowires:1||DILUTED MAGNETIC SEMICONDUCTOR:1||LUMINESCENCE:1||Density modulation:1||Energy modulation:1||Current enhanced SASE free electron laser:1||Undulator radiation:1||FREEELECTRON LASERS:1||ULTRATHIN FERROMAGNETICFILMS:1||OXIDEFILMS:1||ABLATION:1||COMPONENT:1||METAL:1||innershell excited states:1||Nelike ions:1||TRANSITIONS:1||XUV spectrometer:1||DIAGNOSTICS:1||Xray scattering:1||MO/SI:1||pulsed laser deposition:1||KEV IMPACT ENERGIES:1||vacuum electron acceleration:1||HIGHINTENSITY LASER:1||JUNCTIONS:1||LOWTEMPERATURE GROWTH:1||nanocrystalline materials:1||MOLECULAR PHOTOIONIZATION:1||LOCALIZATION:1||DEUTERIUM CLUSTERS:1||EXPLOSIONS:1||REGENERATIVE AMPLIFIERS:1||RAREGASES:1||THz radiation:1||FREEELECTRON LASER:1||REALTIME OBSERVATION:1||TARGET:1||photoionized plasmas:1||fs Xray laser:1||emission profile:1||HIGHORDER HARMONICS:1||Xray laser:1||atomic transition:1||EXCITATION:1||LASERS:1||PERFORMANCE:1||RELATIVISTIC ELECTRONS:1||BI2O3DOPED ZNO:1||INNERSHELL IONIZATION:1||Laser wakefield:1||FREQUENCY:1||SOLIDSTATE LASERS:1||Linearly polarized:1||THERMIONIC EMISSION:1||PULSE AMPLIFICATION SYSTEM:1||BIB3O6:1||NM:1||NONCOVALENT INTERACTIONS:1||CRYSTALLINE:1||INTENSITY:1||JETS:1||COHERENT:1||LINE:1||ANGULARDISTRIBUTION:1||SILVER IONS:1||magnetic anisotropy:1||DEVICES:1||Auger transitions:1||CosterKronig transitions:1||EFFICIENT:1||ELECTRONIMPACT IONIZATION:1||ULTRASHORTPULSE:1||Nanowire:1||Heterostructure:1||soft Xray reflectivity:1||PLASMA ACCELERATOR:1||ZINCOXIDE NANOWIRES:1||CHEMICALVAPORDEPOSITION:1||Electron acceleration:1||Ionization of gases:1||Delay dependent:1||MULTIPHOTON IONIZATION:1||FRAGMENTATION:1||GASJET:1||ultrafast nonlinear optics:1||CYCLE PULSES:1||KHZ:1||chemical vapor deposition:1||ferromagnetism:1||ABSORPTION:1||TERAHERTZ RADIATION:1||SCIENCE:1||FIELDS:1||ELECTRONS:1||nanomultilayer structures:1||YIELDS:1||AUGER:1||10HZ REPETITION RATE:1||MULTITERAWATT:1||SPECTROGRAPH:1||HIGHHARMONICGENERATION:1||spectroscopy:1||level population:1||PARTICLEACCELERATION:1||OPTICAL FREQUENCYMEASUREMENT:1||NANOWALLS:1||ROOMTEMPERATURE:1||AVERAGE OUTPUT POWER:1||GROUPVELOCITYMISMATCH:1||Impact ionization:1||Dynamics:1||Lasers:1||Collisional process:1||ABOVETHRESHOLD IONIZATION:1||MAINGROUP THERMOCHEMISTRY:1||dilute magnetic semiconductors:1||GACRN:1||SIZE:1||ATTOSECOND:1||Ar cluster:1||Xray astrophysics:1||photoionization:1||irons:1||normal incidence pulsed laser deposition:1||SHELLS:1||Silicon Oxide:1||gaspuff Zpinch:1||Xray:1||soft Xray reflectors:1||ESCAPE:1||ZN2SIO4:1||SILICA:1||Time delay:1||Collisional plasmas:1||MASSSPECTROMETRY:1||NUCLEARFUSION:1||PARAMETRIC AMPLIFICATION:1||LYING ELECTRONIC STATES:1||ADJUSTABLEPARAMETERS:1||MAGNETICPROPERTIES:1||LIQUIDPHASE EPITAXY:1||CEP laser:1||REGION:1||Plasma waveguide:1||AMBIENT GAS:1||DEPOSITION:1||HARMONICGENERATION:1||ENHANCEMENT:1||imaging spectrometer:1||Abel inversion:1||Water window:1||Liquid nitrogen jet:1||CHARGEEXCHANGE:1||NOBEL LECTURE:1||VARISTOR:1||EPITAXY:1||THINDISK LASER:1||HIGHREPETITIONRATE:1||Atom lasers:1||Electronimpact excitation:1||High order harmonics:1||ultrafast technology:1||PEAK POWER:1||CHARGED ALUMINUM CLUSTERS:1||GaN:1||THIN:1||Electron beam:1||INTENSE:1||Hard Xray pulse generation:1||NONLINEAR THOMSON SCATTERING:1||MULTILAYER:1||UVvisible spectrometer:1||ATOMS:1||innershell transitions:1||CORRECTED CONCAVE GRATINGS:1||DISCHARGE:1||LASERPLASMA:1||thin film:1||reflectivity:1||opacity:1||gain:1||smallangle Xray scattering:1||SOFTXRAY:1||ZINCOXIDE:1||CYGNUSX3:1||Betatron oscillation:1||ACCELERATOR:1||STRAINEDLAYER SUPERLATTICES:1||OPTICAL PARAMETRIC AMPLIFICATION:1||PASSIVE MODELOCKING:1||Collision dynamics:1||MUM:1||EXACTEXCHANGE:1||BASISSET:1||APPROXIMATION:1||OXYNITRIDES:1||Beam energy modulation:1||polarization spectroscopy:1||REORIENTATION TRANSITION:1||DEPENDENCE:1||sulfurs:1||BUILDINGBLOCKS:1||RATES:1||OPTICAL PULSES:1||toroidal mirror:1||XRAY LASER:1||CALCIUM:1||radially polarized laser:1||GRAINBOUNDARIES:1||VAPORDEPOSITION:1||Xray generation:1||MAGNETIZATION:1||Electric excitation:1||Laserinduced gas plasmas:1||Qualitative analysis:1||SCHEME:1||RADIATION:10||PULSES:8||PHOTOLUMINESCENCE:7||LASER:7||GENERATION:6||NANORODS:6||GROWTH:6||NANOWIRES:5||IMPLANTED 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SEMICONDUCTORS:2||MOLECULARBEAM EPITAXY:2||EARTHDOPED GAN:2||LASER FIELDS:2||CHIRPEDPULSEAMPLIFICATION:2||ALN:2||GAUSSIANBEAM:2||ASSISTED CATALYTIC GROWTH:2||BLUE:2||NANOSTRUCTURES:2||MAGNETOELECTRONICS:2||MICROSCOPY:2||ELECTROLUMINESCENCE:2||LASERPULSES:2||GaN nanowires:2||GALLIUM NITRIDE NANOWIRES:2||GAMNN:2||NANOTUBES:2||PHYSICS:2||Femtosecond laser:2||parametric oscillators and amplifiers:1||ultrafast lasers:1||VALENCE:1||nanowires:1||DILUTED MAGNETIC SEMICONDUCTOR:1||LUMINESCENCE:1||Density modulation:1||Energy modulation:1||Current enhanced SASE free electron laser:1||Undulator radiation:1||FREEELECTRON LASERS:1||ULTRATHIN FERROMAGNETICFILMS:1||OXIDEFILMS:1||ABLATION:1||COMPONENT:1||METAL:1||innershell excited states:1||Nelike ions:1||TRANSITIONS:1||XUV spectrometer:1||DIAGNOSTICS:1||Xray scattering:1||MO/SI:1||pulsed laser deposition:1||KEV IMPACT ENERGIES:1||vacuum electron acceleration:1||HIGHINTENSITY LASER:1||JUNCTIONS:1||LOWTEMPERATURE GROWTH:1||nanocrystalline materials:1||MOLECULAR PHOTOIONIZATION:1||LOCALIZATION:1||DEUTERIUM CLUSTERS:1||EXPLOSIONS:1||REGENERATIVE AMPLIFIERS:1||RAREGASES:1||THz radiation:1||FREEELECTRON LASER:1||REALTIME OBSERVATION:1||TARGET:1||photoionized plasmas:1||fs Xray laser:1||emission profile:1||HIGHORDER HARMONICS:1||Xray laser:1||atomic transition:1||EXCITATION:1||LASERS:1||PERFORMANCE:1||RELATIVISTIC ELECTRONS:1||BI2O3DOPED ZNO:1||INNERSHELL IONIZATION:1||Laser wakefield:1||FREQUENCY:1||SOLIDSTATE LASERS:1||Linearly polarized:1||THERMIONIC EMISSION:1||PULSE AMPLIFICATION SYSTEM:1||BIB3O6:1||NM:1||NONCOVALENT INTERACTIONS:1||CRYSTALLINE:1||INTENSITY:1||JETS:1||COHERENT:1||LINE:1||ANGULARDISTRIBUTION:1||SILVER IONS:1||magnetic anisotropy:1||DEVICES:1||Auger transitions:1||CosterKronig transitions:1||EFFICIENT:1||ELECTRONIMPACT IONIZATION:1||ULTRASHORTPULSE:1||Nanowire:1||Heterostructure:1||soft Xray reflectivity:1||PLASMA ACCELERATOR:1||ZINCOXIDE NANOWIRES:1||CHEMICALVAPORDEPOSITION:1||Electron acceleration:1||Ionization of gases:1||Delay dependent:1||MULTIPHOTON IONIZATION:1||FRAGMENTATION:1||GASJET:1||ultrafast nonlinear optics:1||CYCLE PULSES:1||KHZ:1||chemical vapor deposition:1||ferromagnetism:1||ABSORPTION:1||TERAHERTZ RADIATION:1||SCIENCE:1||FIELDS:1||ELECTRONS:1||nanomultilayer structures:1||YIELDS:1||AUGER:1||10HZ REPETITION RATE:1||MULTITERAWATT:1||SPECTROGRAPH:1||HIGHHARMONICGENERATION:1||spectroscopy:1||level population:1||PARTICLEACCELERATION:1||OPTICAL FREQUENCYMEASUREMENT:1||NANOWALLS:1||ROOMTEMPERATURE:1||AVERAGE OUTPUT POWER:1||GROUPVELOCITYMISMATCH:1||Impact ionization:1||Dynamics:1||Lasers:1||Collisional process:1||ABOVETHRESHOLD IONIZATION:1||MAINGROUP THERMOCHEMISTRY:1||dilute magnetic semiconductors:1||GACRN:1||SIZE:1||ATTOSECOND:1||Ar cluster:1||Xray astrophysics:1||photoionization:1||irons:1||normal incidence pulsed laser deposition:1||SHELLS:1||Silicon Oxide:1||gaspuff Zpinch:1||Xray:1||soft Xray reflectors:1||ESCAPE:1||ZN2SIO4:1||SILICA:1||Time 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materials:1||MOLECULAR PHOTOIONIZATION:1||LOCALIZATION:1||DEUTERIUM CLUSTERS:1||EXPLOSIONS:1||REGENERATIVE AMPLIFIERS:1||RAREGASES:1||THz radiation:1||FREEELECTRON LASER:1||REALTIME OBSERVATION:1||TARGET:1||photoionized plasmas:1||fs Xray laser:1||emission profile:1||HIGHORDER HARMONICS:1||Xray laser:1||atomic transition:1||EXCITATION:1||LASERS:1||PERFORMANCE:1||RELATIVISTIC ELECTRONS:1||BI2O3DOPED ZNO:1||INNERSHELL IONIZATION:1||Laser wakefield:1||FREQUENCY:1||SOLIDSTATE LASERS:1||Linearly polarized:1||THERMIONIC EMISSION:1||PULSE AMPLIFICATION SYSTEM:1||BIB3O6:1||NM:1||NONCOVALENT INTERACTIONS:1||CRYSTALLINE:1||INTENSITY:1||JETS:1||COHERENT:1||LINE:1||ANGULARDISTRIBUTION:1||SILVER IONS:1||magnetic anisotropy:1||DEVICES:1||Auger transitions:1||CosterKronig transitions:1||EFFICIENT:1||ELECTRONIMPACT IONIZATION:1||ULTRASHORTPULSE:1||Nanowire:1||Heterostructure:1||soft Xray reflectivity:1||PLASMA ACCELERATOR:1||ZINCOXIDE NANOWIRES:1||CHEMICALVAPORDEPOSITION:1||Electron acceleration:1||Ionization of gases:1||Delay dependent:1||MULTIPHOTON IONIZATION:1||FRAGMENTATION:1||GASJET:1||ultrafast nonlinear optics:1||CYCLE PULSES:1||KHZ:1||chemical vapor deposition:1||ferromagnetism:1||ABSORPTION:1||TERAHERTZ RADIATION:1||SCIENCE:1||FIELDS:1||ELECTRONS:1||nanomultilayer structures:1||YIELDS:1||AUGER:1||10HZ REPETITION RATE:1||MULTITERAWATT:1||SPECTROGRAPH:1||HIGHHARMONICGENERATION:1||spectroscopy:1||level population:1||PARTICLEACCELERATION:1||OPTICAL FREQUENCYMEASUREMENT:1||NANOWALLS:1||ROOMTEMPERATURE:1||AVERAGE OUTPUT POWER:1||GROUPVELOCITYMISMATCH:1||Impact ionization:1||Dynamics:1||Lasers:1||Collisional process:1||ABOVETHRESHOLD IONIZATION:1||MAINGROUP THERMOCHEMISTRY:1||dilute magnetic semiconductors:1||GACRN:1||SIZE:1||ATTOSECOND:1||Ar cluster:1||Xray astrophysics:1||photoionization:1||irons:1||normal incidence pulsed laser deposition:1||SHELLS:1||Silicon Oxide:1||gaspuff Zpinch:1||Xray:1||soft Xray reflectors:1||ESCAPE:1||ZN2SIO4:1||SILICA:1||Time delay:1||Collisional plasmas:1||MASSSPECTROMETRY:1||NUCLEARFUSION:1||PARAMETRIC AMPLIFICATION:1||LYING ELECTRONIC STATES:1||ADJUSTABLEPARAMETERS:1||MAGNETICPROPERTIES:1||LIQUIDPHASE EPITAXY:1||CEP laser:1||REGION:1||Plasma waveguide:1||AMBIENT GAS:1||DEPOSITION:1||HARMONICGENERATION:1||ENHANCEMENT:1||imaging spectrometer:1||Abel inversion:1||Water window:1||Liquid nitrogen jet:1||CHARGEEXCHANGE:1||NOBEL LECTURE:1||VARISTOR:1||EPITAXY:1||THINDISK LASER:1||HIGHREPETITIONRATE:1||Atom lasers:1||Electronimpact excitation:1||High order harmonics:1||ultrafast technology:1||PEAK POWER:1||CHARGED ALUMINUM CLUSTERS:1||GaN:1||THIN:1||Electron beam:1||INTENSE:1||Hard Xray pulse generation:1||NONLINEAR THOMSON SCATTERING:1||MULTILAYER:1||UVvisible spectrometer:1||ATOMS:1||innershell transitions:1||CORRECTED CONCAVE GRATINGS:1||DISCHARGE:1||LASERPLASMA:1||thin film:1||reflectivity:1||opacity:1||gain:1||smallangle Xray scattering:1||SOFTXRAY:1||ZINCOXIDE:1||CYGNUSX3:1||Betatron oscillation:1||ACCELERATOR:1||STRAINEDLAYER SUPERLATTICES:1||OPTICAL PARAMETRIC AMPLIFICATION:1||PASSIVE MODELOCKING:1||Collision dynamics:1||MUM:1||EXACTEXCHANGE:1||BASISSET:1||APPROXIMATION:1||OXYNITRIDES:1||Beam energy modulation:1||polarization spectroscopy:1||REORIENTATION TRANSITION:1||DEPENDENCE:1||sulfurs:1||BUILDINGBLOCKS:1||RATES:1||OPTICAL PULSES:1||toroidal mirror:1||XRAY LASER:1||CALCIUM:1||radially polarized laser:1||GRAINBOUNDARIES:1||VAPORDEPOSITION:1||Xray generation:1||MAGNETIZATION:1||Electric excitation:1||Laserinduced gas plasmas:1||Qualitative analysis:1||SCHEME:1||RADIATION:10||PULSES:8||PHOTOLUMINESCENCE:7||LASER:7||GENERATION:6||NANORODS:6||GROWTH:6||NANOWIRES:5||IMPLANTED GAN:5||SPECTROSCOPY:5||THINFILMS:4||DYNAMICS:4||SILICON:4||EXTREMEULTRAVIOLET:4||AMPLIFICATION:4||PRESSURE:4||PHASE:4||OPTICALPROPERTIES:4||SYSTEM:4||EMISSION:4||FEL:3||N2O:3||FILMS:3||OPTICS:3||SPECTRA:3||FIELD:3||MIRRORS:3||ARRAYS:3||CLUSTERS:3||SIO2:3||IONIZATION:3||VACUUM:3||SCATTERING:3||IONS:2||LUMINESCENCE PROPERTIES:2||ANISOTROPY:2||BEAMS:2||DIFFRACTION:2||DISPERSION:2||chemical vapor deposition (CVD):2||ELECTRONICSTRUCTURE:2||MOSFETS:2||SI3N4:2||DENSITY:2||LIGHT:2||PLASMAS:2||MATTER:2||nanocomposites:2||RAMANSCATTERING:2||NANOPARTICLES:2||OXIDE:2||AMPLIFIED SPONTANEOUS EMISSION:2||NM WAVELENGTH:2||GAIN:2||CARBON NANOTUBES:2||CROSSSECTIONS:2||LIGHTEMITTINGDIODES:2||PULSE:2||CARBON PLASMA:2||TISAPPHIRE LASER:2||Raman scattering:2||ROUTE:2||multilayer:2||CATHODOLUMINESCENCE:2||highresolution transmission electronic microscope (HRTEM):2||DIFFERENCEFREQUENCYGENERATION:2||CRYSTAL:2||laserproduced plasma:2||NANOCABLES:2||photoluminescence:2||MAGNETIC ALLOY SEMICONDUCTORS:2||MOLECULARBEAM EPITAXY:2||EARTHDOPED GAN:2||LASER FIELDS:2||CHIRPEDPULSEAMPLIFICATION:2||ALN:2||GAUSSIANBEAM:2||ASSISTED CATALYTIC GROWTH:2||BLUE:2||NANOSTRUCTURES:2||MAGNETOELECTRONICS:2||MICROSCOPY:2||ELECTROLUMINESCENCE:2||LASERPULSES:2||GaN nanowires:2||GALLIUM NITRIDE NANOWIRES:2||GAMNN:2||NANOTUBES:2||PHYSICS:2||Femtosecond laser:2||parametric oscillators and amplifiers:1||ultrafast lasers:1||VALENCE:1||nanowires:1||DILUTED MAGNETIC SEMICONDUCTOR:1||LUMINESCENCE:1||Density modulation:1||Energy modulation:1||Current enhanced SASE free electron laser:1||Undulator radiation:1||FREEELECTRON LASERS:1||ULTRATHIN FERROMAGNETICFILMS:1||OXIDEFILMS:1||ABLATION:1||COMPONENT:1||METAL:1||innershell excited states:1||Nelike ions:1||TRANSITIONS:1||XUV spectrometer:1||DIAGNOSTICS:1||Xray scattering:1||MO/SI:1||pulsed laser deposition:1||KEV IMPACT ENERGIES:1||vacuum electron acceleration:1||HIGHINTENSITY LASER:1||JUNCTIONS:1||LOWTEMPERATURE GROWTH:1||nanocrystalline materials:1||MOLECULAR PHOTOIONIZATION:1||LOCALIZATION:1||DEUTERIUM CLUSTERS:1||EXPLOSIONS:1||REGENERATIVE AMPLIFIERS:1||RAREGASES:1||THz radiation:1||FREEELECTRON LASER:1||REALTIME OBSERVATION:1||TARGET:1||photoionized plasmas:1||fs Xray laser:1||emission profile:1||HIGHORDER HARMONICS:1||Xray laser:1||atomic transition:1||EXCITATION:1||LASERS:1||PERFORMANCE:1||RELATIVISTIC ELECTRONS:1||BI2O3DOPED ZNO:1||INNERSHELL IONIZATION:1||Laser wakefield:1||FREQUENCY:1||SOLIDSTATE LASERS:1||Linearly polarized:1||THERMIONIC EMISSION:1||PULSE AMPLIFICATION SYSTEM:1||BIB3O6:1||NM:1||NONCOVALENT INTERACTIONS:1||CRYSTALLINE:1||INTENSITY:1||JETS:1||COHERENT:1||LINE:1||ANGULARDISTRIBUTION:1||SILVER IONS:1||magnetic anisotropy:1||DEVICES:1||Auger transitions:1||CosterKronig transitions:1||EFFICIENT:1||ELECTRONIMPACT IONIZATION:1||ULTRASHORTPULSE:1||Nanowire:1||Heterostructure:1||soft Xray reflectivity:1||PLASMA ACCELERATOR:1||ZINCOXIDE NANOWIRES:1||CHEMICALVAPORDEPOSITION:1||Electron acceleration:1||Ionization of gases:1||Delay dependent:1||MULTIPHOTON IONIZATION:1||FRAGMENTATION:1||GASJET:1||ultrafast nonlinear optics:1||CYCLE PULSES:1||KHZ:1||chemical vapor deposition:1||ferromagnetism:1||ABSORPTION:1||TERAHERTZ RADIATION:1||SCIENCE:1||FIELDS:1||ELECTRONS:1||nanomultilayer structures:1||YIELDS:1||AUGER:1||10HZ REPETITION RATE:1||MULTITERAWATT:1||SPECTROGRAPH:1||HIGHHARMONICGENERATION:1||spectroscopy:1||level population:1||PARTICLEACCELERATION:1||OPTICAL FREQUENCYMEASUREMENT:1||NANOWALLS:1||ROOMTEMPERATURE:1||AVERAGE OUTPUT POWER:1||GROUPVELOCITYMISMATCH:1||Impact ionization:1||Dynamics:1||Lasers:1||Collisional process:1||ABOVETHRESHOLD IONIZATION:1||MAINGROUP THERMOCHEMISTRY:1||dilute magnetic semiconductors:1||GACRN:1||SIZE:1||ATTOSECOND:1||Ar cluster:1||Xray astrophysics:1||photoionization:1||irons:1||normal incidence pulsed laser deposition:1||SHELLS:1||Silicon Oxide:1||gaspuff Zpinch:1||Xray:1||soft Xray reflectors:1||ESCAPE:1||ZN2SIO4:1||SILICA:1||Time delay:1||Collisional plasmas:1||MASSSPECTROMETRY:1||NUCLEARFUSION:1||PARAMETRIC AMPLIFICATION:1||LYING ELECTRONIC STATES:1||ADJUSTABLEPARAMETERS:1||MAGNETICPROPERTIES:1||LIQUIDPHASE EPITAXY:1||CEP laser:1||REGION:1||Plasma waveguide:1||AMBIENT GAS:1||DEPOSITION:1||HARMONICGENERATION:1||ENHANCEMENT:1||imaging spectrometer:1||Abel inversion:1||Water window:1||Liquid nitrogen jet:1||CHARGEEXCHANGE:1||NOBEL LECTURE:1||VARISTOR:1||EPITAXY:1||THINDISK LASER:1||HIGHREPETITIONRATE:1||Atom lasers:1||Electronimpact excitation:1||High order harmonics:1||ultrafast technology:1||PEAK POWER:1||CHARGED ALUMINUM CLUSTERS:1||GaN:1||THIN:1||Electron beam:1||INTENSE:1||Hard Xray pulse generation:1||NONLINEAR THOMSON SCATTERING:1||MULTILAYER:1||UVvisible spectrometer:1||ATOMS:1||innershell transitions:1||CORRECTED CONCAVE GRATINGS:1||DISCHARGE:1||LASERPLASMA:1||thin film:1||reflectivity:1||opacity:1||gain:1||smallangle Xray scattering:1||SOFTXRAY:1||ZINCOXIDE:1||CYGNUSX3:1||Betatron oscillation:1||ACCELERATOR:1||STRAINEDLAYER SUPERLATTICES:1||OPTICAL PARAMETRIC AMPLIFICATION:1||PASSIVE MODELOCKING:1||Collision dynamics:1||MUM:1||EXACTEXCHANGE:1||BASISSET:1||APPROXIMATION:1||OXYNITRIDES:1||Beam energy modulation:1||polarization spectroscopy:1||REORIENTATION TRANSITION:1||DEPENDENCE:1||sulfurs:1||BUILDINGBLOCKS:1||RATES:1||OPTICAL PULSES:1||toroidal mirror:1||XRAY LASER:1||CALCIUM:1||radially polarized laser:1||GRAINBOUNDARIES:1||VAPORDEPOSITION:1||Xray generation:1||MAGNETIZATION:1||Electric excitation:1||Laserinduced gas plasmas:1||Qualitative analysis:1||SCHEME:1||RADIATION:10||PULSES:8||PHOTOLUMINESCENCE:7||LASER:7||GENERATION:6||NANORODS:6||GROWTH:6||NANOWIRES:5||IMPLANTED 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SEMICONDUCTORS:2||MOLECULARBEAM EPITAXY:2||EARTHDOPED GAN:2||LASER FIELDS:2||CHIRPEDPULSEAMPLIFICATION:2||ALN:2||GAUSSIANBEAM:2||ASSISTED CATALYTIC GROWTH:2||BLUE:2||NANOSTRUCTURES:2||MAGNETOELECTRONICS:2||MICROSCOPY:2||ELECTROLUMINESCENCE:2||LASERPULSES:2||GaN nanowires:2||GALLIUM NITRIDE NANOWIRES:2||GAMNN:2||NANOTUBES:2||PHYSICS:2||Femtosecond laser:2||parametric oscillators and amplifiers:1||ultrafast lasers:1||VALENCE:1||nanowires:1||DILUTED MAGNETIC SEMICONDUCTOR:1||LUMINESCENCE:1||Density modulation:1||Energy modulation:1||Current enhanced SASE free electron laser:1||Undulator radiation:1||FREEELECTRON LASERS:1||ULTRATHIN FERROMAGNETICFILMS:1||OXIDEFILMS:1||ABLATION:1||COMPONENT:1||METAL:1||innershell excited states:1||Nelike ions:1||TRANSITIONS:1||XUV spectrometer:1||DIAGNOSTICS:1||Xray scattering:1||MO/SI:1||pulsed laser deposition:1||KEV IMPACT ENERGIES:1||vacuum electron acceleration:1||HIGHINTENSITY LASER:1||JUNCTIONS:1||LOWTEMPERATURE GROWTH:1||nanocrystalline materials:1||MOLECULAR PHOTOIONIZATION:1||LOCALIZATION:1||DEUTERIUM CLUSTERS:1||EXPLOSIONS:1||REGENERATIVE AMPLIFIERS:1||RAREGASES:1||THz radiation:1||FREEELECTRON LASER:1||REALTIME OBSERVATION:1||TARGET:1||photoionized plasmas:1||fs Xray laser:1||emission profile:1||HIGHORDER HARMONICS:1||Xray laser:1||atomic transition:1||EXCITATION:1||LASERS:1||PERFORMANCE:1||RELATIVISTIC ELECTRONS:1||BI2O3DOPED ZNO:1||INNERSHELL IONIZATION:1||Laser wakefield:1||FREQUENCY:1||SOLIDSTATE LASERS:1||Linearly polarized:1||THERMIONIC EMISSION:1||PULSE AMPLIFICATION SYSTEM:1||BIB3O6:1||NM:1||NONCOVALENT INTERACTIONS:1||CRYSTALLINE:1||INTENSITY:1||JETS:1||COHERENT:1||LINE:1||ANGULARDISTRIBUTION:1||SILVER IONS:1||magnetic anisotropy:1||DEVICES:1||Auger transitions:1||CosterKronig transitions:1||EFFICIENT:1||ELECTRONIMPACT IONIZATION:1||ULTRASHORTPULSE:1||Nanowire:1||Heterostructure:1||soft Xray reflectivity:1||PLASMA ACCELERATOR:1||ZINCOXIDE NANOWIRES:1||CHEMICALVAPORDEPOSITION:1||Electron acceleration:1||Ionization of gases:1||Delay dependent:1||MULTIPHOTON IONIZATION:1||FRAGMENTATION:1||GASJET:1||ultrafast nonlinear optics:1||CYCLE PULSES:1||KHZ:1||chemical vapor deposition:1||ferromagnetism:1||ABSORPTION:1||TERAHERTZ RADIATION:1||SCIENCE:1||FIELDS:1||ELECTRONS:1||nanomultilayer structures:1||YIELDS:1||AUGER:1||10HZ REPETITION RATE:1||MULTITERAWATT:1||SPECTROGRAPH:1||HIGHHARMONICGENERATION:1||spectroscopy:1||level population:1||PARTICLEACCELERATION:1||OPTICAL FREQUENCYMEASUREMENT:1||NANOWALLS:1||ROOMTEMPERATURE:1||AVERAGE OUTPUT POWER:1||GROUPVELOCITYMISMATCH:1||Impact ionization:1||Dynamics:1||Lasers:1||Collisional process:1||ABOVETHRESHOLD IONIZATION:1||MAINGROUP THERMOCHEMISTRY:1||dilute magnetic semiconductors:1||GACRN:1||SIZE:1||ATTOSECOND:1||Ar cluster:1||Xray astrophysics:1||photoionization:1||irons:1||normal incidence pulsed laser deposition:1||SHELLS:1||Silicon Oxide:1||gaspuff Zpinch:1||Xray:1||soft Xray reflectors:1||ESCAPE:1||ZN2SIO4:1||SILICA:1||Time 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materials:1||MOLECULAR PHOTOIONIZATION:1||LOCALIZATION:1||DEUTERIUM CLUSTERS:1||EXPLOSIONS:1||REGENERATIVE AMPLIFIERS:1||RAREGASES:1||THz radiation:1||FREEELECTRON LASER:1||REALTIME OBSERVATION:1||TARGET:1||photoionized plasmas:1||fs Xray laser:1||emission profile:1||HIGHORDER HARMONICS:1||Xray laser:1||atomic transition:1||EXCITATION:1||LASERS:1||PERFORMANCE:1||RELATIVISTIC ELECTRONS:1||BI2O3DOPED ZNO:1||INNERSHELL IONIZATION:1||Laser wakefield:1||FREQUENCY:1||SOLIDSTATE LASERS:1||Linearly polarized:1||THERMIONIC EMISSION:1||PULSE AMPLIFICATION SYSTEM:1||BIB3O6:1||NM:1||NONCOVALENT INTERACTIONS:1||CRYSTALLINE:1||INTENSITY:1||JETS:1||COHERENT:1||LINE:1||ANGULARDISTRIBUTION:1||SILVER IONS:1||magnetic anisotropy:1||DEVICES:1||Auger transitions:1||CosterKronig transitions:1||EFFICIENT:1||ELECTRONIMPACT IONIZATION:1||ULTRASHORTPULSE:1||Nanowire:1||Heterostructure:1||soft Xray reflectivity:1||PLASMA ACCELERATOR:1||ZINCOXIDE NANOWIRES:1||CHEMICALVAPORDEPOSITION:1||Electron acceleration:1||Ionization of gases:1||Delay dependent:1||MULTIPHOTON IONIZATION:1||FRAGMENTATION:1||GASJET:1||ultrafast nonlinear optics:1||CYCLE PULSES:1||KHZ:1||chemical vapor deposition:1||ferromagnetism:1||ABSORPTION:1||TERAHERTZ RADIATION:1||SCIENCE:1||FIELDS:1||ELECTRONS:1||nanomultilayer structures:1||YIELDS:1||AUGER:1||10HZ REPETITION RATE:1||MULTITERAWATT:1||SPECTROGRAPH:1||HIGHHARMONICGENERATION:1||spectroscopy:1||level population:1||PARTICLEACCELERATION:1||OPTICAL FREQUENCYMEASUREMENT:1||NANOWALLS:1||ROOMTEMPERATURE:1||AVERAGE OUTPUT POWER:1||GROUPVELOCITYMISMATCH:1||Impact ionization:1||Dynamics:1||Lasers:1||Collisional process:1||ABOVETHRESHOLD IONIZATION:1||MAINGROUP THERMOCHEMISTRY:1||dilute magnetic semiconductors:1||GACRN:1||SIZE:1||ATTOSECOND:1||Ar cluster:1||Xray astrophysics:1||photoionization:1||irons:1||normal incidence pulsed laser deposition:1||SHELLS:1||Silicon Oxide:1||gaspuff Zpinch:1||Xray:1||soft Xray reflectors:1||ESCAPE:1||ZN2SIO4:1||SILICA:1||Time delay:1||Collisional plasmas:1||MASSSPECTROMETRY:1||NUCLEARFUSION:1||PARAMETRIC AMPLIFICATION:1||LYING ELECTRONIC STATES:1||ADJUSTABLEPARAMETERS:1||MAGNETICPROPERTIES:1||LIQUIDPHASE EPITAXY:1||CEP laser:1||REGION:1||Plasma waveguide:1||AMBIENT GAS:1||DEPOSITION:1||HARMONICGENERATION:1||ENHANCEMENT:1||imaging spectrometer:1||Abel inversion:1||Water window:1||Liquid nitrogen jet:1||CHARGEEXCHANGE:1||NOBEL LECTURE:1||VARISTOR:1||EPITAXY:1||THINDISK LASER:1||HIGHREPETITIONRATE:1||Atom lasers:1||Electronimpact excitation:1||High order harmonics:1||ultrafast technology:1||PEAK POWER:1||CHARGED ALUMINUM CLUSTERS:1||GaN:1||THIN:1||Electron beam:1||INTENSE:1||Hard Xray pulse generation:1||NONLINEAR THOMSON SCATTERING:1||MULTILAYER:1||UVvisible spectrometer:1||ATOMS:1||innershell transitions:1||CORRECTED CONCAVE GRATINGS:1||DISCHARGE:1||LASERPLASMA:1||thin film:1||reflectivity:1||opacity:1||gain:1||smallangle Xray scattering:1||SOFTXRAY:1||ZINCOXIDE:1||CYGNUSX3:1||Betatron oscillation:1||ACCELERATOR:1||STRAINEDLAYER SUPERLATTICES:1||OPTICAL PARAMETRIC AMPLIFICATION:1||PASSIVE MODELOCKING:1||Collision dynamics:1||MUM:1||EXACTEXCHANGE:1||BASISSET:1||APPROXIMATION:1||OXYNITRIDES:1||Beam energy modulation:1||polarization spectroscopy:1||REORIENTATION TRANSITION:1||DEPENDENCE:1||sulfurs:1||BUILDINGBLOCKS:1||RATES:1||OPTICAL PULSES:1||toroidal mirror:1||XRAY LASER:1||CALCIUM:1||radially polarized laser:1||GRAINBOUNDARIES:1||VAPORDEPOSITION:1||Xray generation:1||MAGNETIZATION:1||Electric excitation:1||Laserinduced gas plasmas:1||Qualitative analysis:1||SCHEME:1||RADIATION:10||PULSES:8||PHOTOLUMINESCENCE:7||LASER:7||GENERATION:6||NANORODS:6||GROWTH:6||NANOWIRES:5||IMPLANTED GAN:5||SPECTROSCOPY:5||THINFILMS:4||DYNAMICS:4||SILICON:4||EXTREMEULTRAVIOLET:4||AMPLIFICATION:4||PRESSURE:4||PHASE:4||OPTICALPROPERTIES:4||SYSTEM:4||EMISSION:4||FEL:3||N2O:3||FILMS:3||OPTICS:3||SPECTRA:3||FIELD:3||MIRRORS:3||ARRAYS:3||CLUSTERS:3||SIO2:3||IONIZATION:3||VACUUM:3||SCATTERING:3||IONS:2||LUMINESCENCE PROPERTIES:2||ANISOTROPY:2||BEAMS:2||DIFFRACTION:2||DISPERSION:2||chemical vapor deposition (CVD):2||ELECTRONICSTRUCTURE:2||MOSFETS:2||SI3N4:2||DENSITY:2||LIGHT:2||PLASMAS:2||MATTER:2||nanocomposites:2||RAMANSCATTERING:2||NANOPARTICLES:2||OXIDE:2||AMPLIFIED SPONTANEOUS EMISSION:2||NM WAVELENGTH:2||GAIN:2||CARBON NANOTUBES:2||CROSSSECTIONS:2||LIGHTEMITTINGDIODES:2||PULSE:2||CARBON PLASMA:2||TISAPPHIRE LASER:2||Raman scattering:2||ROUTE:2||multilayer:2||CATHODOLUMINESCENCE:2||highresolution transmission electronic microscope (HRTEM):2||DIFFERENCEFREQUENCYGENERATION:2||CRYSTAL:2||laserproduced plasma:2||NANOCABLES:2||photoluminescence:2||MAGNETIC ALLOY SEMICONDUCTORS:2||MOLECULARBEAM EPITAXY:2||EARTHDOPED GAN:2||LASER FIELDS:2||CHIRPEDPULSEAMPLIFICATION:2||ALN:2||GAUSSIANBEAM:2||ASSISTED CATALYTIC GROWTH:2||BLUE:2||NANOSTRUCTURES:2||MAGNETOELECTRONICS:2||MICROSCOPY:2||ELECTROLUMINESCENCE:2||LASERPULSES:2||GaN nanowires:2||GALLIUM NITRIDE NANOWIRES:2||GAMNN:2||NANOTUBES:2||PHYSICS:2||Femtosecond laser:2||parametric oscillators and amplifiers:1||ultrafast lasers:1||VALENCE:1||nanowires:1||DILUTED MAGNETIC SEMICONDUCTOR:1||LUMINESCENCE:1||Density modulation:1||Energy modulation:1||Current enhanced SASE free electron laser:1||Undulator radiation:1||FREEELECTRON LASERS:1||ULTRATHIN FERROMAGNETICFILMS:1||OXIDEFILMS:1||ABLATION:1||COMPONENT:1||METAL:1||innershell excited states:1||Nelike ions:1||TRANSITIONS:1||XUV spectrometer:1||DIAGNOSTICS:1||Xray scattering:1||MO/SI:1||pulsed laser deposition:1||KEV IMPACT ENERGIES:1||vacuum electron acceleration:1||HIGHINTENSITY LASER:1||JUNCTIONS:1||LOWTEMPERATURE GROWTH:1||nanocrystalline materials:1||MOLECULAR PHOTOIONIZATION:1||LOCALIZATION:1||DEUTERIUM CLUSTERS:1||EXPLOSIONS:1||REGENERATIVE AMPLIFIERS:1||RAREGASES:1||THz radiation:1||FREEELECTRON LASER:1||REALTIME OBSERVATION:1||TARGET:1||photoionized plasmas:1||fs Xray laser:1||emission profile:1||HIGHORDER HARMONICS:1||Xray laser:1||atomic transition:1||EXCITATION:1||LASERS:1||PERFORMANCE:1||RELATIVISTIC ELECTRONS:1||BI2O3DOPED ZNO:1||INNERSHELL IONIZATION:1||Laser wakefield:1||FREQUENCY:1||SOLIDSTATE LASERS:1||Linearly polarized:1||THERMIONIC EMISSION:1||PULSE AMPLIFICATION SYSTEM:1||BIB3O6:1||NM:1||NONCOVALENT INTERACTIONS:1||CRYSTALLINE:1||INTENSITY:1||JETS:1||COHERENT:1||LINE:1||ANGULARDISTRIBUTION:1||SILVER IONS:1||magnetic anisotropy:1||DEVICES:1||Auger transitions:1||CosterKronig transitions:1||EFFICIENT:1||ELECTRONIMPACT IONIZATION:1||ULTRASHORTPULSE:1||Nanowire:1||Heterostructure:1||soft Xray reflectivity:1||PLASMA ACCELERATOR:1||ZINCOXIDE NANOWIRES:1||CHEMICALVAPORDEPOSITION:1||Electron acceleration:1||Ionization of gases:1||Delay dependent:1||MULTIPHOTON IONIZATION:1||FRAGMENTATION:1||GASJET:1||ultrafast nonlinear optics:1||CYCLE PULSES:1||KHZ:1||chemical vapor deposition:1||ferromagnetism:1||ABSORPTION:1||TERAHERTZ RADIATION:1||SCIENCE:1||FIELDS:1||ELECTRONS:1||nanomultilayer structures:1||YIELDS:1||AUGER:1||10HZ REPETITION RATE:1||MULTITERAWATT:1||SPECTROGRAPH:1||HIGHHARMONICGENERATION:1||spectroscopy:1||level population:1||PARTICLEACCELERATION:1||OPTICAL FREQUENCYMEASUREMENT:1||NANOWALLS:1||ROOMTEMPERATURE:1||AVERAGE OUTPUT POWER:1||GROUPVELOCITYMISMATCH:1||Impact ionization:1||Dynamics:1||Lasers:1||Collisional process:1||ABOVETHRESHOLD IONIZATION:1||MAINGROUP THERMOCHEMISTRY:1||dilute magnetic semiconductors:1||GACRN:1||SIZE:1||ATTOSECOND:1||Ar cluster:1||Xray astrophysics:1||photoionization:1||irons:1||normal incidence pulsed laser deposition:1||SHELLS:1||Silicon Oxide:1||gaspuff Zpinch:1||Xray:1||soft Xray reflectors:1||ESCAPE:1||ZN2SIO4:1||SILICA:1||Time delay:1||Collisional plasmas:1||MASSSPECTROMETRY:1||NUCLEARFUSION:1||PARAMETRIC AMPLIFICATION:1||LYING ELECTRONIC STATES:1||ADJUSTABLEPARAMETERS:1||MAGNETICPROPERTIES:1||LIQUIDPHASE EPITAXY:1||CEP laser:1||REGION:1||Plasma waveguide:1||AMBIENT GAS:1||DEPOSITION:1||HARMONICGENERATION:1||ENHANCEMENT:1||imaging spectrometer:1||Abel inversion:1||Water window:1||Liquid nitrogen jet:1||CHARGEEXCHANGE:1||NOBEL LECTURE:1||VARISTOR:1||EPITAXY:1||THINDISK LASER:1||HIGHREPETITIONRATE:1||Atom lasers:1||Electronimpact excitation:1||High order harmonics:1||ultrafast technology:1||PEAK POWER:1||CHARGED ALUMINUM CLUSTERS:1||GaN:1||THIN:1||Electron beam:1||INTENSE:1||Hard Xray pulse generation:1||NONLINEAR THOMSON SCATTERING:1||MULTILAYER:1||UVvisible spectrometer:1||ATOMS:1||innershell transitions:1||CORRECTED CONCAVE GRATINGS:1||DISCHARGE:1||LASERPLASMA:1||thin film:1||reflectivity:1||opacity:1||gain:1||smallangle Xray scattering:1||SOFTXRAY:1||ZINCOXIDE:1||CYGNUSX3:1||Betatron oscillation:1||ACCELERATOR:1||STRAINEDLAYER SUPERLATTICES:1||OPTICAL PARAMETRIC AMPLIFICATION:1||PASSIVE MODELOCKING:1||Collision dynamics:1||MUM:1||EXACTEXCHANGE:1||BASISSET:1||APPROXIMATION:1||OXYNITRIDES:1||Beam energy modulation:1||polarization spectroscopy:1||REORIENTATION TRANSITION:1||DEPENDENCE:1||sulfurs:1||BUILDINGBLOCKS:1||RATES:1||OPTICAL PULSES:1||toroidal mirror:1||XRAY LASER:1||CALCIUM:1||radially polarized laser:1||GRAINBOUNDARIES:1||VAPORDEPOSITION:1||Xray generation:1||MAGNETIZATION:1||Electric excitation:1||Laserinduced gas plasmas:1||Qualitative analysis:1||SCHEME:1||RADIATION:10||PULSES:8||PHOTOLUMINESCENCE:7||LASER:7||GENERATION:6||NANORODS:6||GROWTH:6||NANOWIRES:5||IMPLANTED 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SEMICONDUCTORS:2||MOLECULARBEAM EPITAXY:2||EARTHDOPED GAN:2||LASER FIELDS:2||CHIRPEDPULSEAMPLIFICATION:2||ALN:2||GAUSSIANBEAM:2||ASSISTED CATALYTIC GROWTH:2||BLUE:2||NANOSTRUCTURES:2||MAGNETOELECTRONICS:2||MICROSCOPY:2||ELECTROLUMINESCENCE:2||LASERPULSES:2||GaN nanowires:2||GALLIUM NITRIDE NANOWIRES:2||GAMNN:2||NANOTUBES:2||PHYSICS:2||Femtosecond laser:2||parametric oscillators and amplifiers:1||ultrafast lasers:1||VALENCE:1||nanowires:1||DILUTED MAGNETIC SEMICONDUCTOR:1||LUMINESCENCE:1||Density modulation:1||Energy modulation:1||Current enhanced SASE free electron laser:1||Undulator radiation:1||FREEELECTRON LASERS:1||ULTRATHIN FERROMAGNETICFILMS:1||OXIDEFILMS:1||ABLATION:1||COMPONENT:1||METAL:1||innershell excited states:1||Nelike ions:1||TRANSITIONS:1||XUV spectrometer:1||DIAGNOSTICS:1||Xray scattering:1||MO/SI:1||pulsed laser deposition:1||KEV IMPACT ENERGIES:1||vacuum electron acceleration:1||HIGHINTENSITY LASER:1||JUNCTIONS:1||LOWTEMPERATURE GROWTH:1||nanocrystalline materials:1||MOLECULAR PHOTOIONIZATION:1||LOCALIZATION:1||DEUTERIUM CLUSTERS:1||EXPLOSIONS:1||REGENERATIVE AMPLIFIERS:1||RAREGASES:1||THz radiation:1||FREEELECTRON LASER:1||REALTIME OBSERVATION:1||TARGET:1||photoionized plasmas:1||fs Xray laser:1||emission profile:1||HIGHORDER HARMONICS:1||Xray laser:1||atomic transition:1||EXCITATION:1||LASERS:1||PERFORMANCE:1||RELATIVISTIC ELECTRONS:1||BI2O3DOPED ZNO:1||INNERSHELL IONIZATION:1||Laser wakefield:1||FREQUENCY:1||SOLIDSTATE LASERS:1||Linearly polarized:1||THERMIONIC EMISSION:1||PULSE AMPLIFICATION SYSTEM:1||BIB3O6:1||NM:1||NONCOVALENT INTERACTIONS:1||CRYSTALLINE:1||INTENSITY:1||JETS:1||COHERENT:1||LINE:1||ANGULARDISTRIBUTION:1||SILVER IONS:1||magnetic anisotropy:1||DEVICES:1||Auger transitions:1||CosterKronig transitions:1||EFFICIENT:1||ELECTRONIMPACT IONIZATION:1||ULTRASHORTPULSE:1||Nanowire:1||Heterostructure:1||soft Xray reflectivity:1||PLASMA ACCELERATOR:1||ZINCOXIDE NANOWIRES:1||CHEMICALVAPORDEPOSITION:1||Electron acceleration:1||Ionization of gases:1||Delay dependent:1||MULTIPHOTON IONIZATION:1||FRAGMENTATION:1||GASJET:1||ultrafast nonlinear optics:1||CYCLE PULSES:1||KHZ:1||chemical vapor deposition:1||ferromagnetism:1||ABSORPTION:1||TERAHERTZ RADIATION:1||SCIENCE:1||FIELDS:1||ELECTRONS:1||nanomultilayer structures:1||YIELDS:1||AUGER:1||10HZ REPETITION RATE:1||MULTITERAWATT:1||SPECTROGRAPH:1||HIGHHARMONICGENERATION:1||spectroscopy:1||level population:1||PARTICLEACCELERATION:1||OPTICAL FREQUENCYMEASUREMENT:1||NANOWALLS:1||ROOMTEMPERATURE:1||AVERAGE OUTPUT POWER:1||GROUPVELOCITYMISMATCH:1||Impact ionization:1||Dynamics:1||Lasers:1||Collisional process:1||ABOVETHRESHOLD IONIZATION:1||MAINGROUP THERMOCHEMISTRY:1||dilute magnetic semiconductors:1||GACRN:1||SIZE:1||ATTOSECOND:1||Ar cluster:1||Xray astrophysics:1||photoionization:1||irons:1||normal incidence pulsed laser deposition:1||SHELLS:1||Silicon Oxide:1||gaspuff Zpinch:1||Xray:1||soft Xray reflectors:1||ESCAPE:1||ZN2SIO4:1||SILICA:1||Time 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materials:1||MOLECULAR PHOTOIONIZATION:1||LOCALIZATION:1||DEUTERIUM CLUSTERS:1||EXPLOSIONS:1||REGENERATIVE AMPLIFIERS:1||RAREGASES:1||THz radiation:1||FREEELECTRON LASER:1||REALTIME OBSERVATION:1||TARGET:1||photoionized plasmas:1||fs Xray laser:1||emission profile:1||HIGHORDER HARMONICS:1||Xray laser:1||atomic transition:1||EXCITATION:1||LASERS:1||PERFORMANCE:1||RELATIVISTIC ELECTRONS:1||BI2O3DOPED ZNO:1||INNERSHELL IONIZATION:1||Laser wakefield:1||FREQUENCY:1||SOLIDSTATE LASERS:1||Linearly polarized:1||THERMIONIC EMISSION:1||PULSE AMPLIFICATION SYSTEM:1||BIB3O6:1||NM:1||NONCOVALENT INTERACTIONS:1||CRYSTALLINE:1||INTENSITY:1||JETS:1||COHERENT:1||LINE:1||ANGULARDISTRIBUTION:1||SILVER IONS:1||magnetic anisotropy:1||DEVICES:1||Auger transitions:1||CosterKronig transitions:1||EFFICIENT:1||ELECTRONIMPACT IONIZATION:1||ULTRASHORTPULSE:1||Nanowire:1||Heterostructure:1||soft Xray reflectivity:1||PLASMA ACCELERATOR:1||ZINCOXIDE NANOWIRES:1||CHEMICALVAPORDEPOSITION:1||Electron acceleration:1||Ionization of gases:1||Delay dependent:1||MULTIPHOTON IONIZATION:1||FRAGMENTATION:1||GASJET:1||ultrafast nonlinear optics:1||CYCLE PULSES:1||KHZ:1||chemical vapor deposition:1||ferromagnetism:1||ABSORPTION:1||TERAHERTZ RADIATION:1||SCIENCE:1||FIELDS:1||ELECTRONS:1||nanomultilayer structures:1||YIELDS:1||AUGER:1||10HZ REPETITION RATE:1||MULTITERAWATT:1||SPECTROGRAPH:1||HIGHHARMONICGENERATION:1||spectroscopy:1||level population:1||PARTICLEACCELERATION:1||OPTICAL FREQUENCYMEASUREMENT:1||NANOWALLS:1||ROOMTEMPERATURE:1||AVERAGE OUTPUT POWER:1||GROUPVELOCITYMISMATCH:1||Impact ionization:1||Dynamics:1||Lasers:1||Collisional process:1||ABOVETHRESHOLD IONIZATION:1||MAINGROUP THERMOCHEMISTRY:1||dilute magnetic semiconductors:1||GACRN:1||SIZE:1||ATTOSECOND:1||Ar cluster:1||Xray astrophysics:1||photoionization:1||irons:1||normal incidence pulsed laser deposition:1||SHELLS:1||Silicon Oxide:1||gaspuff Zpinch:1||Xray:1||soft Xray reflectors:1||ESCAPE:1||ZN2SIO4:1||SILICA:1||Time delay:1||Collisional plasmas:1||MASSSPECTROMETRY:1||NUCLEARFUSION:1||PARAMETRIC AMPLIFICATION:1||LYING ELECTRONIC STATES:1||ADJUSTABLEPARAMETERS:1||MAGNETICPROPERTIES:1||LIQUIDPHASE EPITAXY:1||CEP laser:1||REGION:1||Plasma waveguide:1||AMBIENT GAS:1||DEPOSITION:1||HARMONICGENERATION:1||ENHANCEMENT:1||imaging spectrometer:1||Abel inversion:1||Water window:1||Liquid nitrogen jet:1||CHARGEEXCHANGE:1||NOBEL LECTURE:1||VARISTOR:1||EPITAXY:1||THINDISK LASER:1||HIGHREPETITIONRATE:1||Atom lasers:1||Electronimpact excitation:1||High order harmonics:1||ultrafast technology:1||PEAK POWER:1||CHARGED ALUMINUM CLUSTERS:1||GaN:1||THIN:1||Electron beam:1||INTENSE:1||Hard Xray pulse generation:1||NONLINEAR THOMSON SCATTERING:1||MULTILAYER:1||UVvisible spectrometer:1||ATOMS:1||innershell transitions:1||CORRECTED CONCAVE GRATINGS:1||DISCHARGE:1||LASERPLASMA:1||thin film:1||reflectivity:1||opacity:1||gain:1||smallangle Xray scattering:1||SOFTXRAY:1||ZINCOXIDE:1||CYGNUSX3:1||Betatron oscillation:1||ACCELERATOR:1||STRAINEDLAYER SUPERLATTICES:1||OPTICAL PARAMETRIC AMPLIFICATION:1||PASSIVE MODELOCKING:1||Collision dynamics:1||MUM:1||EXACTEXCHANGE:1||BASISSET:1||APPROXIMATION:1||OXYNITRIDES:1||Beam energy modulation:1||polarization spectroscopy:1||REORIENTATION TRANSITION:1||DEPENDENCE:1||sulfurs:1||BUILDINGBLOCKS:1||RATES:1||OPTICAL PULSES:1||toroidal mirror:1||XRAY LASER:1||CALCIUM:1||radially polarized laser:1||GRAINBOUNDARIES:1||VAPORDEPOSITION:1||Xray generation:1||MAGNETIZATION:1||Electric excitation:1||Laserinduced gas plasmas:1||Qualitative analysis:1||SCHEME:1||RADIATION:10||PULSES:8||PHOTOLUMINESCENCE:7||LASER:7||GENERATION:6||NANORODS:6||GROWTH:6||NANOWIRES:5||IMPLANTED GAN:5||SPECTROSCOPY:5||THINFILMS:4||DYNAMICS:4||SILICON:4||EXTREMEULTRAVIOLET:4||AMPLIFICATION:4||PRESSURE:4||PHASE:4||OPTICALPROPERTIES:4||SYSTEM:4||EMISSION:4||FEL:3||N2O:3||FILMS:3||OPTICS:3||SPECTRA:3||FIELD:3||MIRRORS:3||ARRAYS:3||CLUSTERS:3||SIO2:3||IONIZATION:3||VACUUM:3||SCATTERING:3||IONS:2||LUMINESCENCE PROPERTIES:2||ANISOTROPY:2||BEAMS:2||DIFFRACTION:2||DISPERSION:2||chemical vapor deposition (CVD):2||ELECTRONICSTRUCTURE:2||MOSFETS:2||SI3N4:2||DENSITY:2||LIGHT:2||PLASMAS:2||MATTER:2||nanocomposites:2||RAMANSCATTERING:2||NANOPARTICLES:2||OXIDE:2||AMPLIFIED SPONTANEOUS EMISSION:2||NM WAVELENGTH:2||GAIN:2||CARBON NANOTUBES:2||CROSSSECTIONS:2||LIGHTEMITTINGDIODES:2||PULSE:2||CARBON PLASMA:2||TISAPPHIRE LASER:2||Raman scattering:2||ROUTE:2||multilayer:2||CATHODOLUMINESCENCE:2||highresolution transmission electronic microscope (HRTEM):2||DIFFERENCEFREQUENCYGENERATION:2||CRYSTAL:2||laserproduced plasma:2||NANOCABLES:2||photoluminescence:2||MAGNETIC ALLOY SEMICONDUCTORS:2||MOLECULARBEAM EPITAXY:2||EARTHDOPED GAN:2||LASER FIELDS:2||CHIRPEDPULSEAMPLIFICATION:2||ALN:2||GAUSSIANBEAM:2||ASSISTED CATALYTIC GROWTH:2||BLUE:2||NANOSTRUCTURES:2||MAGNETOELECTRONICS:2||MICROSCOPY:2||ELECTROLUMINESCENCE:2||LASERPULSES:2||GaN nanowires:2||GALLIUM NITRIDE NANOWIRES:2||GAMNN:2||NANOTUBES:2||PHYSICS:2||Femtosecond laser:2||parametric oscillators and amplifiers:1||ultrafast lasers:1||VALENCE:1||nanowires:1||DILUTED MAGNETIC SEMICONDUCTOR:1||LUMINESCENCE:1||Density modulation:1||Energy modulation:1||Current enhanced SASE free electron laser:1||Undulator radiation:1||FREEELECTRON LASERS:1||ULTRATHIN FERROMAGNETICFILMS:1||OXIDEFILMS:1||ABLATION:1||COMPONENT:1||METAL:1||innershell excited states:1||Nelike ions:1||TRANSITIONS:1||XUV spectrometer:1||DIAGNOSTICS:1||Xray scattering:1||MO/SI:1||pulsed laser deposition:1||KEV IMPACT ENERGIES:1||vacuum electron acceleration:1||HIGHINTENSITY LASER:1||JUNCTIONS:1||LOWTEMPERATURE GROWTH:1||nanocrystalline materials:1||MOLECULAR PHOTOIONIZATION:1||LOCALIZATION:1||DEUTERIUM CLUSTERS:1||EXPLOSIONS:1||REGENERATIVE AMPLIFIERS:1||RAREGASES:1||THz radiation:1||FREEELECTRON LASER:1||REALTIME OBSERVATION:1||TARGET:1||photoionized plasmas:1||fs Xray laser:1||emission profile:1||HIGHORDER HARMONICS:1||Xray laser:1||atomic transition:1||EXCITATION:1||LASERS:1||PERFORMANCE:1||RELATIVISTIC ELECTRONS:1||BI2O3DOPED ZNO:1||INNERSHELL IONIZATION:1||Laser wakefield:1||FREQUENCY:1||SOLIDSTATE LASERS:1||Linearly polarized:1||THERMIONIC EMISSION:1||PULSE AMPLIFICATION SYSTEM:1||BIB3O6:1||NM:1||NONCOVALENT INTERACTIONS:1||CRYSTALLINE:1||INTENSITY:1||JETS:1||COHERENT:1||LINE:1||ANGULARDISTRIBUTION:1||SILVER IONS:1||magnetic anisotropy:1||DEVICES:1||Auger transitions:1||CosterKronig transitions:1||EFFICIENT:1||ELECTRONIMPACT IONIZATION:1||ULTRASHORTPULSE:1||Nanowire:1||Heterostructure:1||soft Xray reflectivity:1||PLASMA ACCELERATOR:1||ZINCOXIDE NANOWIRES:1||CHEMICALVAPORDEPOSITION:1||Electron acceleration:1||Ionization of gases:1||Delay dependent:1||MULTIPHOTON IONIZATION:1||FRAGMENTATION:1||GASJET:1||ultrafast nonlinear optics:1||CYCLE PULSES:1||KHZ:1||chemical vapor deposition:1||ferromagnetism:1||ABSORPTION:1||TERAHERTZ RADIATION:1||SCIENCE:1||FIELDS:1||ELECTRONS:1||nanomultilayer structures:1||YIELDS:1||AUGER:1||10HZ REPETITION RATE:1||MULTITERAWATT:1||SPECTROGRAPH:1||HIGHHARMONICGENERATION:1||spectroscopy:1||level population:1||PARTICLEACCELERATION:1||OPTICAL FREQUENCYMEASUREMENT:1||NANOWALLS:1||ROOMTEMPERATURE:1||AVERAGE OUTPUT POWER:1||GROUPVELOCITYMISMATCH:1||Impact ionization:1||Dynamics:1||Lasers:1||Collisional process:1||ABOVETHRESHOLD IONIZATION:1||MAINGROUP THERMOCHEMISTRY:1||dilute magnetic semiconductors:1||GACRN:1||SIZE:1||ATTOSECOND:1||Ar cluster:1||Xray astrophysics:1||photoionization:1||irons:1||normal incidence pulsed laser deposition:1||SHELLS:1||Silicon Oxide:1||gaspuff Zpinch:1||Xray:1||soft Xray reflectors:1||ESCAPE:1||ZN2SIO4:1||SILICA:1||Time delay:1||Collisional plasmas:1||MASSSPECTROMETRY:1||NUCLEARFUSION:1||PARAMETRIC AMPLIFICATION:1||LYING ELECTRONIC STATES:1||ADJUSTABLEPARAMETERS:1||MAGNETICPROPERTIES:1||LIQUIDPHASE EPITAXY:1||CEP laser:1||REGION:1||Plasma waveguide:1||AMBIENT GAS:1||DEPOSITION:1||HARMONICGENERATION:1||ENHANCEMENT:1||imaging spectrometer:1||Abel inversion:1||Water window:1||Liquid nitrogen jet:1||CHARGEEXCHANGE:1||NOBEL LECTURE:1||VARISTOR:1||EPITAXY:1||THINDISK LASER:1||HIGHREPETITIONRATE:1||Atom lasers:1||Electronimpact excitation:1||High order harmonics:1||ultrafast technology:1||PEAK POWER:1||CHARGED ALUMINUM CLUSTERS:1||GaN:1||THIN:1||Electron beam:1||INTENSE:1||Hard Xray pulse generation:1||NONLINEAR THOMSON SCATTERING:1||MULTILAYER:1||UVvisible spectrometer:1||ATOMS:1||innershell transitions:1||CORRECTED CONCAVE GRATINGS:1||DISCHARGE:1||LASERPLASMA:1||thin film:1||reflectivity:1||opacity:1||gain:1||smallangle Xray scattering:1||SOFTXRAY:1||ZINCOXIDE:1||CYGNUSX3:1||Betatron oscillation:1||ACCELERATOR:1||STRAINEDLAYER SUPERLATTICES:1||OPTICAL PARAMETRIC AMPLIFICATION:1||PASSIVE MODELOCKING:1||Collision dynamics:1||MUM:1||EXACTEXCHANGE:1||BASISSET:1||APPROXIMATION:1||OXYNITRIDES:1||Beam energy modulation:1||polarization spectroscopy:1||REORIENTATION TRANSITION:1||DEPENDENCE:1||sulfurs:1||BUILDINGBLOCKS:1||RATES:1||OPTICAL PULSES:1||toroidal mirror:1||XRAY LASER:1||CALCIUM:1||radially polarized laser:1||GRAINBOUNDARIES:1||VAPORDEPOSITION:1||Xray generation:1||MAGNETIZATION:1||Electric excitation:1||Laserinduced gas plasmas:1||Qualitative analysis:1||SCHEME:1||RADIATION:10||PULSES:8||PHOTOLUMINESCENCE:7||LASER:7||GENERATION:6||NANORODS:6||GROWTH:6||NANOWIRES:5||IMPLANTED 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SEMICONDUCTORS:2||MOLECULARBEAM EPITAXY:2||EARTHDOPED GAN:2||LASER FIELDS:2||CHIRPEDPULSEAMPLIFICATION:2||ALN:2||GAUSSIANBEAM:2||ASSISTED CATALYTIC GROWTH:2||BLUE:2||NANOSTRUCTURES:2||MAGNETOELECTRONICS:2||MICROSCOPY:2||ELECTROLUMINESCENCE:2||LASERPULSES:2||GaN nanowires:2||GALLIUM NITRIDE NANOWIRES:2||GAMNN:2||NANOTUBES:2||PHYSICS:2||Femtosecond laser:2||parametric oscillators and amplifiers:1||ultrafast lasers:1||VALENCE:1||nanowires:1||DILUTED MAGNETIC SEMICONDUCTOR:1||LUMINESCENCE:1||Density modulation:1||Energy modulation:1||Current enhanced SASE free electron laser:1||Undulator radiation:1||FREEELECTRON LASERS:1||ULTRATHIN FERROMAGNETICFILMS:1||OXIDEFILMS:1||ABLATION:1||COMPONENT:1||METAL:1||innershell excited states:1||Nelike ions:1||TRANSITIONS:1||XUV spectrometer:1||DIAGNOSTICS:1||Xray scattering:1||MO/SI:1||pulsed laser deposition:1||KEV IMPACT ENERGIES:1||vacuum electron acceleration:1||HIGHINTENSITY LASER:1||JUNCTIONS:1||LOWTEMPERATURE GROWTH:1||nanocrystalline materials:1||MOLECULAR PHOTOIONIZATION:1||LOCALIZATION:1||DEUTERIUM CLUSTERS:1||EXPLOSIONS:1||REGENERATIVE AMPLIFIERS:1||RAREGASES:1||THz radiation:1||FREEELECTRON LASER:1||REALTIME OBSERVATION:1||TARGET:1||photoionized plasmas:1||fs Xray laser:1||emission profile:1||HIGHORDER HARMONICS:1||Xray laser:1||atomic transition:1||EXCITATION:1||LASERS:1||PERFORMANCE:1||RELATIVISTIC ELECTRONS:1||BI2O3DOPED ZNO:1||INNERSHELL IONIZATION:1||Laser wakefield:1||FREQUENCY:1||SOLIDSTATE LASERS:1||Linearly polarized:1||THERMIONIC EMISSION:1||PULSE AMPLIFICATION SYSTEM:1||BIB3O6:1||NM:1||NONCOVALENT INTERACTIONS:1||CRYSTALLINE:1||INTENSITY:1||JETS:1||COHERENT:1||LINE:1||ANGULARDISTRIBUTION:1||SILVER IONS:1||magnetic anisotropy:1||DEVICES:1||Auger transitions:1||CosterKronig transitions:1||EFFICIENT:1||ELECTRONIMPACT IONIZATION:1||ULTRASHORTPULSE:1||Nanowire:1||Heterostructure:1||soft Xray reflectivity:1||PLASMA ACCELERATOR:1||ZINCOXIDE NANOWIRES:1||CHEMICALVAPORDEPOSITION:1||Electron acceleration:1||Ionization of gases:1||Delay dependent:1||MULTIPHOTON IONIZATION:1||FRAGMENTATION:1||GASJET:1||ultrafast nonlinear optics:1||CYCLE PULSES:1||KHZ:1||chemical vapor deposition:1||ferromagnetism:1||ABSORPTION:1||TERAHERTZ RADIATION:1||SCIENCE:1||FIELDS:1||ELECTRONS:1||nanomultilayer structures:1||YIELDS:1||AUGER:1||10HZ REPETITION RATE:1||MULTITERAWATT:1||SPECTROGRAPH:1||HIGHHARMONICGENERATION:1||spectroscopy:1||level population:1||PARTICLEACCELERATION:1||OPTICAL FREQUENCYMEASUREMENT:1||NANOWALLS:1||ROOMTEMPERATURE:1||AVERAGE OUTPUT POWER:1||GROUPVELOCITYMISMATCH:1||Impact ionization:1||Dynamics:1||Lasers:1||Collisional process:1||ABOVETHRESHOLD IONIZATION:1||MAINGROUP THERMOCHEMISTRY:1||dilute magnetic semiconductors:1||GACRN:1||SIZE:1||ATTOSECOND:1||Ar cluster:1||Xray astrophysics:1||photoionization:1||irons:1||normal incidence pulsed laser deposition:1||SHELLS:1||Silicon Oxide:1||gaspuff Zpinch:1||Xray:1||soft Xray reflectors:1||ESCAPE:1||ZN2SIO4:1||SILICA:1||Time 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materials:1||MOLECULAR PHOTOIONIZATION:1||LOCALIZATION:1||DEUTERIUM CLUSTERS:1||EXPLOSIONS:1||REGENERATIVE AMPLIFIERS:1||RAREGASES:1||THz radiation:1||FREEELECTRON LASER:1||REALTIME OBSERVATION:1||TARGET:1||photoionized plasmas:1||fs Xray laser:1||emission profile:1||HIGHORDER HARMONICS:1||Xray laser:1||atomic transition:1||EXCITATION:1||LASERS:1||PERFORMANCE:1||RELATIVISTIC ELECTRONS:1||BI2O3DOPED ZNO:1||INNERSHELL IONIZATION:1||Laser wakefield:1||FREQUENCY:1||SOLIDSTATE LASERS:1||Linearly polarized:1||THERMIONIC EMISSION:1||PULSE AMPLIFICATION SYSTEM:1||BIB3O6:1||NM:1||NONCOVALENT INTERACTIONS:1||CRYSTALLINE:1||INTENSITY:1||JETS:1||COHERENT:1||LINE:1||ANGULARDISTRIBUTION:1||SILVER IONS:1||magnetic anisotropy:1||DEVICES:1||Auger transitions:1||CosterKronig transitions:1||EFFICIENT:1||ELECTRONIMPACT IONIZATION:1||ULTRASHORTPULSE:1||Nanowire:1||Heterostructure:1||soft Xray reflectivity:1||PLASMA ACCELERATOR:1||ZINCOXIDE NANOWIRES:1||CHEMICALVAPORDEPOSITION:1||Electron acceleration:1||Ionization of gases:1||Delay dependent:1||MULTIPHOTON IONIZATION:1||FRAGMENTATION:1||GASJET:1||ultrafast nonlinear optics:1||CYCLE PULSES:1||KHZ:1||chemical vapor deposition:1||ferromagnetism:1||ABSORPTION:1||TERAHERTZ RADIATION:1||SCIENCE:1||FIELDS:1||ELECTRONS:1||nanomultilayer structures:1||YIELDS:1||AUGER:1||10HZ REPETITION RATE:1||MULTITERAWATT:1||SPECTROGRAPH:1||HIGHHARMONICGENERATION:1||spectroscopy:1||level population:1||PARTICLEACCELERATION:1||OPTICAL FREQUENCYMEASUREMENT:1||NANOWALLS:1||ROOMTEMPERATURE:1||AVERAGE OUTPUT POWER:1||GROUPVELOCITYMISMATCH:1||Impact ionization:1||Dynamics:1||Lasers:1||Collisional process:1||ABOVETHRESHOLD IONIZATION:1||MAINGROUP THERMOCHEMISTRY:1||dilute magnetic semiconductors:1||GACRN:1||SIZE:1||ATTOSECOND:1||Ar cluster:1||Xray astrophysics:1||photoionization:1||irons:1||normal incidence pulsed laser deposition:1||SHELLS:1||Silicon Oxide:1||gaspuff Zpinch:1||Xray:1||soft Xray reflectors:1||ESCAPE:1||ZN2SIO4:1||SILICA:1||Time delay:1||Collisional plasmas:1||MASSSPECTROMETRY:1||NUCLEARFUSION:1||PARAMETRIC AMPLIFICATION:1||LYING ELECTRONIC STATES:1||ADJUSTABLEPARAMETERS:1||MAGNETICPROPERTIES:1||LIQUIDPHASE EPITAXY:1||CEP laser:1||REGION:1||Plasma waveguide:1||AMBIENT GAS:1||DEPOSITION:1||HARMONICGENERATION:1||ENHANCEMENT:1||imaging spectrometer:1||Abel inversion:1||Water window:1||Liquid nitrogen jet:1||CHARGEEXCHANGE:1||NOBEL LECTURE:1||VARISTOR:1||EPITAXY:1||THINDISK LASER:1||HIGHREPETITIONRATE:1||Atom lasers:1||Electronimpact excitation:1||High order harmonics:1||ultrafast technology:1||PEAK POWER:1||CHARGED ALUMINUM CLUSTERS:1||GaN:1||THIN:1||Electron beam:1||INTENSE:1||Hard Xray pulse generation:1||NONLINEAR THOMSON SCATTERING:1||MULTILAYER:1||UVvisible spectrometer:1||ATOMS:1||innershell transitions:1||CORRECTED CONCAVE GRATINGS:1||DISCHARGE:1||LASERPLASMA:1||thin film:1||reflectivity:1||opacity:1||gain:1||smallangle Xray scattering:1||SOFTXRAY:1||ZINCOXIDE:1||CYGNUSX3:1||Betatron oscillation:1||ACCELERATOR:1||STRAINEDLAYER SUPERLATTICES:1||OPTICAL PARAMETRIC AMPLIFICATION:1||PASSIVE MODELOCKING:1||Collision dynamics:1||MUM:1||EXACTEXCHANGE:1||BASISSET:1||APPROXIMATION:1||OXYNITRIDES:1||Beam energy modulation:1||polarization spectroscopy:1||REORIENTATION TRANSITION:1||DEPENDENCE:1||sulfurs:1||BUILDINGBLOCKS:1||RATES:1||OPTICAL PULSES:1||toroidal mirror:1||XRAY LASER:1||CALCIUM:1||radially polarized laser:1||GRAINBOUNDARIES:1||VAPORDEPOSITION:1||Xray generation:1||MAGNETIZATION:1||Electric excitation:1||Laserinduced gas plasmas:1||Qualitative analysis:1||SCHEME:1||RADIATION:10||PULSES:8||PHOTOLUMINESCENCE:7||LASER:7||GENERATION:6||NANORODS:6||GROWTH:6||NANOWIRES:5||IMPLANTED GAN:5||SPECTROSCOPY:5||THINFILMS:4||DYNAMICS:4||SILICON:4||EXTREMEULTRAVIOLET:4||AMPLIFICATION:4||PRESSURE:4||PHASE:4||OPTICALPROPERTIES:4||SYSTEM:4||EMISSION:4||FEL:3||N2O:3||FILMS:3||OPTICS:3||SPECTRA:3||FIELD:3||MIRRORS:3||ARRAYS:3||CLUSTERS:3||SIO2:3||IONIZATION:3||VACUUM:3||SCATTERING:3||IONS:2||LUMINESCENCE PROPERTIES:2||ANISOTROPY:2||BEAMS:2||DIFFRACTION:2||DISPERSION:2||chemical vapor deposition (CVD):2||ELECTRONICSTRUCTURE:2||MOSFETS:2||SI3N4:2||DENSITY:2||LIGHT:2||PLASMAS:2||MATTER:2||nanocomposites:2||RAMANSCATTERING:2||NANOPARTICLES:2||OXIDE:2||AMPLIFIED SPONTANEOUS EMISSION:2||NM WAVELENGTH:2||GAIN:2||CARBON NANOTUBES:2||CROSSSECTIONS:2||LIGHTEMITTINGDIODES:2||PULSE:2||CARBON PLASMA:2||TISAPPHIRE LASER:2||Raman scattering:2||ROUTE:2||multilayer:2||CATHODOLUMINESCENCE:2||highresolution transmission electronic microscope (HRTEM):2||DIFFERENCEFREQUENCYGENERATION:2||CRYSTAL:2||laserproduced plasma:2||NANOCABLES:2||photoluminescence:2||MAGNETIC ALLOY SEMICONDUCTORS:2||MOLECULARBEAM EPITAXY:2||EARTHDOPED GAN:2||LASER FIELDS:2||CHIRPEDPULSEAMPLIFICATION:2||ALN:2||GAUSSIANBEAM:2||ASSISTED CATALYTIC GROWTH:2||BLUE:2||NANOSTRUCTURES:2||MAGNETOELECTRONICS:2||MICROSCOPY:2||ELECTROLUMINESCENCE:2||LASERPULSES:2||GaN nanowires:2||GALLIUM NITRIDE NANOWIRES:2||GAMNN:2||NANOTUBES:2||PHYSICS:2||Femtosecond laser:2||parametric oscillators and amplifiers:1||ultrafast lasers:1||VALENCE:1||nanowires:1||DILUTED MAGNETIC SEMICONDUCTOR:1||LUMINESCENCE:1||Density modulation:1||Energy modulation:1||Current enhanced SASE free electron laser:1||Undulator radiation:1||FREEELECTRON LASERS:1||ULTRATHIN FERROMAGNETICFILMS:1||OXIDEFILMS:1||ABLATION:1||COMPONENT:1||METAL:1||innershell excited states:1||Nelike ions:1||TRANSITIONS:1||XUV spectrometer:1||DIAGNOSTICS:1||Xray scattering:1||MO/SI:1||pulsed laser deposition:1||KEV IMPACT ENERGIES:1||vacuum electron acceleration:1||HIGHINTENSITY LASER:1||JUNCTIONS:1||LOWTEMPERATURE GROWTH:1||nanocrystalline materials:1||MOLECULAR PHOTOIONIZATION:1||LOCALIZATION:1||DEUTERIUM CLUSTERS:1||EXPLOSIONS:1||REGENERATIVE AMPLIFIERS:1||RAREGASES:1||THz radiation:1||FREEELECTRON LASER:1||REALTIME OBSERVATION:1||TARGET:1||photoionized plasmas:1||fs Xray laser:1||emission profile:1||HIGHORDER HARMONICS:1||Xray laser:1||atomic transition:1||EXCITATION:1||LASERS:1||PERFORMANCE:1||RELATIVISTIC ELECTRONS:1||BI2O3DOPED ZNO:1||INNERSHELL IONIZATION:1||Laser wakefield:1||FREQUENCY:1||SOLIDSTATE LASERS:1||Linearly polarized:1||THERMIONIC EMISSION:1||PULSE AMPLIFICATION SYSTEM:1||BIB3O6:1||NM:1||NONCOVALENT INTERACTIONS:1||CRYSTALLINE:1||INTENSITY:1||JETS:1||COHERENT:1||LINE:1||ANGULARDISTRIBUTION:1||SILVER IONS:1||magnetic anisotropy:1||DEVICES:1||Auger transitions:1||CosterKronig transitions:1||EFFICIENT:1||ELECTRONIMPACT IONIZATION:1||ULTRASHORTPULSE:1||Nanowire:1||Heterostructure:1||soft Xray reflectivity:1||PLASMA ACCELERATOR:1||ZINCOXIDE NANOWIRES:1||CHEMICALVAPORDEPOSITION:1||Electron acceleration:1||Ionization of gases:1||Delay dependent:1||MULTIPHOTON IONIZATION:1||FRAGMENTATION:1||GASJET:1||ultrafast nonlinear optics:1||CYCLE PULSES:1||KHZ:1||chemical vapor deposition:1||ferromagnetism:1||ABSORPTION:1||TERAHERTZ RADIATION:1||SCIENCE:1||FIELDS:1||ELECTRONS:1||nanomultilayer structures:1||YIELDS:1||AUGER:1||10HZ REPETITION RATE:1||MULTITERAWATT:1||SPECTROGRAPH:1||HIGHHARMONICGENERATION:1||spectroscopy:1||level population:1||PARTICLEACCELERATION:1||OPTICAL FREQUENCYMEASUREMENT:1||NANOWALLS:1||ROOMTEMPERATURE:1||AVERAGE OUTPUT POWER:1||GROUPVELOCITYMISMATCH:1||Impact ionization:1||Dynamics:1||Lasers:1||Collisional process:1||ABOVETHRESHOLD IONIZATION:1||MAINGROUP THERMOCHEMISTRY:1||dilute magnetic semiconductors:1||GACRN:1||SIZE:1||ATTOSECOND:1||Ar cluster:1||Xray astrophysics:1||photoionization:1||irons:1||normal incidence pulsed laser deposition:1||SHELLS:1||Silicon Oxide:1||gaspuff Zpinch:1||Xray:1||soft Xray reflectors:1||ESCAPE:1||ZN2SIO4:1||SILICA:1||Time delay:1||Collisional plasmas:1||MASSSPECTROMETRY:1||NUCLEARFUSION:1||PARAMETRIC AMPLIFICATION:1||LYING ELECTRONIC STATES:1||ADJUSTABLEPARAMETERS:1||MAGNETICPROPERTIES:1||LIQUIDPHASE EPITAXY:1||CEP laser:1||REGION:1||Plasma waveguide:1||AMBIENT GAS:1||DEPOSITION:1||HARMONICGENERATION:1||ENHANCEMENT:1||imaging spectrometer:1||Abel inversion:1||Water window:1||Liquid nitrogen jet:1||CHARGEEXCHANGE:1||NOBEL LECTURE:1||VARISTOR:1||EPITAXY:1||THINDISK LASER:1||HIGHREPETITIONRATE:1||Atom lasers:1||Electronimpact excitation:1||High order harmonics:1||ultrafast technology:1||PEAK POWER:1||CHARGED ALUMINUM CLUSTERS:1||GaN:1||THIN:1||Electron beam:1||INTENSE:1||Hard Xray pulse generation:1||NONLINEAR THOMSON SCATTERING:1||MULTILAYER:1||UVvisible spectrometer:1||ATOMS:1||innershell transitions:1||CORRECTED CONCAVE GRATINGS:1||DISCHARGE:1||LASERPLASMA:1||thin film:1||reflectivity:1||opacity:1||gain:1||smallangle Xray scattering:1||SOFTXRAY:1||ZINCOXIDE:1||CYGNUSX3:1||Betatron oscillation:1||ACCELERATOR:1||STRAINEDLAYER SUPERLATTICES:1||OPTICAL PARAMETRIC AMPLIFICATION:1||PASSIVE MODELOCKING:1||Collision dynamics:1||MUM:1||EXACTEXCHANGE:1||BASISSET:1||APPROXIMATION:1||OXYNITRIDES:1||Beam energy modulation:1||polarization spectroscopy:1||REORIENTATION TRANSITION:1||DEPENDENCE:1||sulfurs:1||BUILDINGBLOCKS:1||RATES:1||OPTICAL PULSES:1||toroidal mirror:1||XRAY LASER:1||CALCIUM:1||radially polarized laser:1||GRAINBOUNDARIES:1||VAPORDEPOSITION:1||Xray generation:1||MAGNETIZATION:1||Electric excitation:1||Laserinduced gas plasmas:1||Qualitative analysis:1||SCHEME:1||RADIATION:10||PULSES:8||PHOTOLUMINESCENCE:7||LASER:7||GENERATION:6||NANORODS:6||GROWTH:6||NANOWIRES:5||IMPLANTED 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SEMICONDUCTORS:2||MOLECULARBEAM EPITAXY:2||EARTHDOPED GAN:2||LASER FIELDS:2||CHIRPEDPULSEAMPLIFICATION:2||ALN:2||GAUSSIANBEAM:2||ASSISTED CATALYTIC GROWTH:2||BLUE:2||NANOSTRUCTURES:2||MAGNETOELECTRONICS:2||MICROSCOPY:2||ELECTROLUMINESCENCE:2||LASERPULSES:2||GaN nanowires:2||GALLIUM NITRIDE NANOWIRES:2||GAMNN:2||NANOTUBES:2||PHYSICS:2||Femtosecond laser:2||parametric oscillators and amplifiers:1||ultrafast lasers:1||VALENCE:1||nanowires:1||DILUTED MAGNETIC SEMICONDUCTOR:1||LUMINESCENCE:1||Density modulation:1||Energy modulation:1||Current enhanced SASE free electron laser:1||Undulator radiation:1||FREEELECTRON LASERS:1||ULTRATHIN FERROMAGNETICFILMS:1||OXIDEFILMS:1||ABLATION:1||COMPONENT:1||METAL:1||innershell excited states:1||Nelike ions:1||TRANSITIONS:1||XUV spectrometer:1||DIAGNOSTICS:1||Xray scattering:1||MO/SI:1||pulsed laser deposition:1||KEV IMPACT ENERGIES:1||vacuum electron acceleration:1||HIGHINTENSITY LASER:1||JUNCTIONS:1||LOWTEMPERATURE GROWTH:1||nanocrystalline materials:1||MOLECULAR PHOTOIONIZATION:1||LOCALIZATION:1||DEUTERIUM CLUSTERS:1||EXPLOSIONS:1||REGENERATIVE AMPLIFIERS:1||RAREGASES:1||THz radiation:1||FREEELECTRON LASER:1||REALTIME OBSERVATION:1||TARGET:1||photoionized plasmas:1||fs Xray laser:1||emission profile:1||HIGHORDER HARMONICS:1||Xray laser:1||atomic transition:1||EXCITATION:1||LASERS:1||PERFORMANCE:1||RELATIVISTIC ELECTRONS:1||BI2O3DOPED ZNO:1||INNERSHELL IONIZATION:1||Laser wakefield:1||FREQUENCY:1||SOLIDSTATE LASERS:1||Linearly polarized:1||THERMIONIC EMISSION:1||PULSE AMPLIFICATION SYSTEM:1||BIB3O6:1||NM:1||NONCOVALENT INTERACTIONS:1||CRYSTALLINE:1||INTENSITY:1||JETS:1||COHERENT:1||LINE:1||ANGULARDISTRIBUTION:1||SILVER IONS:1||magnetic anisotropy:1||DEVICES:1||Auger transitions:1||CosterKronig transitions:1||EFFICIENT:1||ELECTRONIMPACT IONIZATION:1||ULTRASHORTPULSE:1||Nanowire:1||Heterostructure:1||soft Xray reflectivity:1||PLASMA ACCELERATOR:1||ZINCOXIDE NANOWIRES:1||CHEMICALVAPORDEPOSITION:1||Electron acceleration:1||Ionization of gases:1||Delay dependent:1||MULTIPHOTON IONIZATION:1||FRAGMENTATION:1||GASJET:1||ultrafast nonlinear optics:1||CYCLE PULSES:1||KHZ:1||chemical vapor deposition:1||ferromagnetism:1||ABSORPTION:1||TERAHERTZ RADIATION:1||SCIENCE:1||FIELDS:1||ELECTRONS:1||nanomultilayer structures:1||YIELDS:1||AUGER:1||10HZ REPETITION RATE:1||MULTITERAWATT:1||SPECTROGRAPH:1||HIGHHARMONICGENERATION:1||spectroscopy:1||level population:1||PARTICLEACCELERATION:1||OPTICAL FREQUENCYMEASUREMENT:1||NANOWALLS:1||ROOMTEMPERATURE:1||AVERAGE OUTPUT POWER:1||GROUPVELOCITYMISMATCH:1||Impact ionization:1||Dynamics:1||Lasers:1||Collisional process:1||ABOVETHRESHOLD IONIZATION:1||MAINGROUP THERMOCHEMISTRY:1||dilute magnetic semiconductors:1||GACRN:1||SIZE:1||ATTOSECOND:1||Ar cluster:1||Xray astrophysics:1||photoionization:1||irons:1||normal incidence pulsed laser deposition:1||SHELLS:1||Silicon Oxide:1||gaspuff Zpinch:1||Xray:1||soft Xray reflectors:1||ESCAPE:1||ZN2SIO4:1||SILICA:1||Time 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materials:1||MOLECULAR PHOTOIONIZATION:1||LOCALIZATION:1||DEUTERIUM CLUSTERS:1||EXPLOSIONS:1||REGENERATIVE AMPLIFIERS:1||RAREGASES:1||THz radiation:1||FREEELECTRON LASER:1||REALTIME OBSERVATION:1||TARGET:1||photoionized plasmas:1||fs Xray laser:1||emission profile:1||HIGHORDER HARMONICS:1||Xray laser:1||atomic transition:1||EXCITATION:1||LASERS:1||PERFORMANCE:1||RELATIVISTIC ELECTRONS:1||BI2O3DOPED ZNO:1||INNERSHELL IONIZATION:1||Laser wakefield:1||FREQUENCY:1||SOLIDSTATE LASERS:1||Linearly polarized:1||THERMIONIC EMISSION:1||PULSE AMPLIFICATION SYSTEM:1||BIB3O6:1||NM:1||NONCOVALENT INTERACTIONS:1||CRYSTALLINE:1||INTENSITY:1||JETS:1||COHERENT:1||LINE:1||ANGULARDISTRIBUTION:1||SILVER IONS:1||magnetic anisotropy:1||DEVICES:1||Auger transitions:1||CosterKronig transitions:1||EFFICIENT:1||ELECTRONIMPACT IONIZATION:1||ULTRASHORTPULSE:1||Nanowire:1||Heterostructure:1||soft Xray reflectivity:1||PLASMA ACCELERATOR:1||ZINCOXIDE NANOWIRES:1||CHEMICALVAPORDEPOSITION:1||Electron acceleration:1||Ionization of gases:1||Delay dependent:1||MULTIPHOTON IONIZATION:1||FRAGMENTATION:1||GASJET:1||ultrafast nonlinear optics:1||CYCLE PULSES:1||KHZ:1||chemical vapor deposition:1||ferromagnetism:1||ABSORPTION:1||TERAHERTZ RADIATION:1||SCIENCE:1||FIELDS:1||ELECTRONS:1||nanomultilayer structures:1||YIELDS:1||AUGER:1||10HZ REPETITION RATE:1||MULTITERAWATT:1||SPECTROGRAPH:1||HIGHHARMONICGENERATION:1||spectroscopy:1||level population:1||PARTICLEACCELERATION:1||OPTICAL FREQUENCYMEASUREMENT:1||NANOWALLS:1||ROOMTEMPERATURE:1||AVERAGE OUTPUT POWER:1||GROUPVELOCITYMISMATCH:1||Impact ionization:1||Dynamics:1||Lasers:1||Collisional process:1||ABOVETHRESHOLD IONIZATION:1||MAINGROUP THERMOCHEMISTRY:1||dilute magnetic semiconductors:1||GACRN:1||SIZE:1||ATTOSECOND:1||Ar cluster:1||Xray astrophysics:1||photoionization:1||irons:1||normal incidence pulsed laser deposition:1||SHELLS:1||Silicon Oxide:1||gaspuff Zpinch:1||Xray:1||soft Xray reflectors:1||ESCAPE:1||ZN2SIO4:1||SILICA:1||Time delay:1||Collisional plasmas:1||MASSSPECTROMETRY:1||NUCLEARFUSION:1||PARAMETRIC AMPLIFICATION:1||LYING ELECTRONIC STATES:1||ADJUSTABLEPARAMETERS:1||MAGNETICPROPERTIES:1||LIQUIDPHASE EPITAXY:1||CEP laser:1||REGION:1||Plasma waveguide:1||AMBIENT GAS:1||DEPOSITION:1||HARMONICGENERATION:1||ENHANCEMENT:1||imaging spectrometer:1||Abel inversion:1||Water window:1||Liquid nitrogen jet:1||CHARGEEXCHANGE:1||NOBEL LECTURE:1||VARISTOR:1||EPITAXY:1||THINDISK LASER:1||HIGHREPETITIONRATE:1||Atom lasers:1||Electronimpact excitation:1||High order harmonics:1||ultrafast technology:1||PEAK POWER:1||CHARGED ALUMINUM CLUSTERS:1||GaN:1||THIN:1||Electron beam:1||INTENSE:1||Hard Xray pulse generation:1||NONLINEAR THOMSON SCATTERING:1||MULTILAYER:1||UVvisible spectrometer:1||ATOMS:1||innershell transitions:1||CORRECTED CONCAVE GRATINGS:1||DISCHARGE:1||LASERPLASMA:1||thin film:1||reflectivity:1||opacity:1||gain:1||smallangle Xray scattering:1||SOFTXRAY:1||ZINCOXIDE:1||CYGNUSX3:1||Betatron oscillation:1||ACCELERATOR:1||STRAINEDLAYER SUPERLATTICES:1||OPTICAL PARAMETRIC AMPLIFICATION:1||PASSIVE MODELOCKING:1||Collision dynamics:1||MUM:1||EXACTEXCHANGE:1||BASISSET:1||APPROXIMATION:1||OXYNITRIDES:1||Beam energy modulation:1||polarization spectroscopy:1||REORIENTATION TRANSITION:1||DEPENDENCE:1||sulfurs:1||BUILDINGBLOCKS:1||RATES:1||OPTICAL PULSES:1||toroidal mirror:1||XRAY LASER:1||CALCIUM:1||radially polarized laser:1||GRAINBOUNDARIES:1||VAPORDEPOSITION:1||Xray generation:1||MAGNETIZATION:1||Electric excitation:1||Laserinduced gas plasmas:1||Qualitative analysis:1||SCHEME:1||RADIATION:10||PULSES:8||PHOTOLUMINESCENCE:7||LASER:7||GENERATION:6||NANORODS:6||GROWTH:6||NANOWIRES:5||IMPLANTED GAN:5||SPECTROSCOPY:5||THINFILMS:4||DYNAMICS:4||SILICON:4||EXTREMEULTRAVIOLET:4||AMPLIFICATION:4||PRESSURE:4||PHASE:4||OPTICALPROPERTIES:4||SYSTEM:4||EMISSION:4||FEL:3||N2O:3||FILMS:3||OPTICS:3||SPECTRA:3||FIELD:3||MIRRORS:3||ARRAYS:3||CLUSTERS:3||SIO2:3||IONIZATION:3||VACUUM:3||SCATTERING:3||IONS:2||LUMINESCENCE PROPERTIES:2||ANISOTROPY:2||BEAMS:2||DIFFRACTION:2||DISPERSION:2||chemical vapor deposition (CVD):2||ELECTRONICSTRUCTURE:2||MOSFETS:2||SI3N4:2||DENSITY:2||LIGHT:2||PLASMAS:2||MATTER:2||nanocomposites:2||RAMANSCATTERING:2||NANOPARTICLES:2||OXIDE:2||AMPLIFIED SPONTANEOUS EMISSION:2||NM WAVELENGTH:2||GAIN:2||CARBON NANOTUBES:2||CROSSSECTIONS:2||LIGHTEMITTINGDIODES:2||PULSE:2||CARBON PLASMA:2||TISAPPHIRE LASER:2||Raman scattering:2||ROUTE:2||multilayer:2||CATHODOLUMINESCENCE:2||highresolution transmission electronic microscope (HRTEM):2||DIFFERENCEFREQUENCYGENERATION:2||CRYSTAL:2||laserproduced plasma:2||NANOCABLES:2||photoluminescence:2||MAGNETIC ALLOY SEMICONDUCTORS:2||MOLECULARBEAM EPITAXY:2||EARTHDOPED GAN:2||LASER FIELDS:2||CHIRPEDPULSEAMPLIFICATION:2||ALN:2||GAUSSIANBEAM:2||ASSISTED CATALYTIC GROWTH:2||BLUE:2||NANOSTRUCTURES:2||MAGNETOELECTRONICS:2||MICROSCOPY:2||ELECTROLUMINESCENCE:2||LASERPULSES:2||GaN nanowires:2||GALLIUM NITRIDE NANOWIRES:2||GAMNN:2||NANOTUBES:2||PHYSICS:2||Femtosecond laser:2||parametric oscillators and amplifiers:1||ultrafast lasers:1||VALENCE:1||nanowires:1||DILUTED MAGNETIC SEMICONDUCTOR:1||LUMINESCENCE:1||Density modulation:1||Energy modulation:1||Current enhanced SASE free electron laser:1||Undulator radiation:1||FREEELECTRON LASERS:1||ULTRATHIN FERROMAGNETICFILMS:1||OXIDEFILMS:1||ABLATION:1||COMPONENT:1||METAL:1||innershell excited states:1||Nelike ions:1||TRANSITIONS:1||XUV spectrometer:1||DIAGNOSTICS:1||Xray scattering:1||MO/SI:1||pulsed laser deposition:1||KEV IMPACT ENERGIES:1||vacuum electron acceleration:1||HIGHINTENSITY LASER:1||JUNCTIONS:1||LOWTEMPERATURE GROWTH:1||nanocrystalline materials:1||MOLECULAR PHOTOIONIZATION:1||LOCALIZATION:1||DEUTERIUM CLUSTERS:1||EXPLOSIONS:1||REGENERATIVE AMPLIFIERS:1||RAREGASES:1||THz radiation:1||FREEELECTRON LASER:1||REALTIME OBSERVATION:1||TARGET:1||photoionized plasmas:1||fs Xray laser:1||emission profile:1||HIGHORDER HARMONICS:1||Xray laser:1||atomic transition:1||EXCITATION:1||LASERS:1||PERFORMANCE:1||RELATIVISTIC ELECTRONS:1||BI2O3DOPED ZNO:1||INNERSHELL IONIZATION:1||Laser wakefield:1||FREQUENCY:1||SOLIDSTATE LASERS:1||Linearly polarized:1||THERMIONIC EMISSION:1||PULSE AMPLIFICATION SYSTEM:1||BIB3O6:1||NM:1||NONCOVALENT INTERACTIONS:1||CRYSTALLINE:1||INTENSITY:1||JETS:1||COHERENT:1||LINE:1||ANGULARDISTRIBUTION:1||SILVER IONS:1||magnetic anisotropy:1||DEVICES:1||Auger transitions:1||CosterKronig transitions:1||EFFICIENT:1||ELECTRONIMPACT IONIZATION:1||ULTRASHORTPULSE:1||Nanowire:1||Heterostructure:1||soft Xray reflectivity:1||PLASMA ACCELERATOR:1||ZINCOXIDE NANOWIRES:1||CHEMICALVAPORDEPOSITION:1||Electron acceleration:1||Ionization of gases:1||Delay dependent:1||MULTIPHOTON IONIZATION:1||FRAGMENTATION:1||GASJET:1||ultrafast nonlinear optics:1||CYCLE PULSES:1||KHZ:1||chemical vapor deposition:1||ferromagnetism:1||ABSORPTION:1||TERAHERTZ RADIATION:1||SCIENCE:1||FIELDS:1||ELECTRONS:1||nanomultilayer structures:1||YIELDS:1||AUGER:1||10HZ REPETITION RATE:1||MULTITERAWATT:1||SPECTROGRAPH:1||HIGHHARMONICGENERATION:1||spectroscopy:1||level population:1||PARTICLEACCELERATION:1||OPTICAL FREQUENCYMEASUREMENT:1||NANOWALLS:1||ROOMTEMPERATURE:1||AVERAGE OUTPUT POWER:1||GROUPVELOCITYMISMATCH:1||Impact ionization:1||Dynamics:1||Lasers:1||Collisional process:1||ABOVETHRESHOLD IONIZATION:1||MAINGROUP THERMOCHEMISTRY:1||dilute magnetic semiconductors:1||GACRN:1||SIZE:1||ATTOSECOND:1||Ar cluster:1||Xray astrophysics:1||photoionization:1||irons:1||normal incidence pulsed laser deposition:1||SHELLS:1||Silicon Oxide:1||gaspuff Zpinch:1||Xray:1||soft Xray reflectors:1||ESCAPE:1||ZN2SIO4:1||SILICA:1||Time delay:1||Collisional plasmas:1||MASSSPECTROMETRY:1||NUCLEARFUSION:1||PARAMETRIC AMPLIFICATION:1||LYING ELECTRONIC STATES:1||ADJUSTABLEPARAMETERS:1||MAGNETICPROPERTIES:1||LIQUIDPHASE EPITAXY:1||CEP laser:1||REGION:1||Plasma waveguide:1||AMBIENT GAS:1||DEPOSITION:1||HARMONICGENERATION:1||ENHANCEMENT:1||imaging spectrometer:1||Abel inversion:1||Water window:1||Liquid nitrogen jet:1||CHARGEEXCHANGE:1||NOBEL LECTURE:1||VARISTOR:1||EPITAXY:1||THINDISK LASER:1||HIGHREPETITIONRATE:1||Atom lasers:1||Electronimpact excitation:1||High order harmonics:1||ultrafast technology:1||PEAK POWER:1||CHARGED ALUMINUM CLUSTERS:1||GaN:1||THIN:1||Electron beam:1||INTENSE:1||Hard Xray pulse generation:1||NONLINEAR THOMSON SCATTERING:1||MULTILAYER:1||UVvisible spectrometer:1||ATOMS:1||innershell transitions:1||CORRECTED CONCAVE GRATINGS:1||DISCHARGE:1||LASERPLASMA:1||thin film:1||reflectivity:1||opacity:1||gain:1||smallangle Xray scattering:1||SOFTXRAY:1||ZINCOXIDE:1||CYGNUSX3:1||Betatron oscillation:1||ACCELERATOR:1||STRAINEDLAYER SUPERLATTICES:1||OPTICAL PARAMETRIC AMPLIFICATION:1||PASSIVE MODELOCKING:1||Collision dynamics:1||MUM:1||EXACTEXCHANGE:1||BASISSET:1||APPROXIMATION:1||OXYNITRIDES:1||Beam energy modulation:1||polarization spectroscopy:1||REORIENTATION TRANSITION:1||DEPENDENCE:1||sulfurs:1||BUILDINGBLOCKS:1||RATES:1||OPTICAL PULSES:1||toroidal mirror:1||XRAY LASER:1||CALCIUM:1||radially polarized laser:1||GRAINBOUNDARIES:1||VAPORDEPOSITION:1||Xray generation:1||MAGNETIZATION:1||Electric excitation:1||Laserinduced gas plasmas:1||Qualitative analysis:1||SCHEME:1||RADIATION:10||PULSES:8||PHOTOLUMINESCENCE:7||LASER:7||GENERATION:6||NANORODS:6||GROWTH:6||NANOWIRES:5||IMPLANTED 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SEMICONDUCTORS:2||MOLECULARBEAM EPITAXY:2||EARTHDOPED GAN:2||LASER FIELDS:2||CHIRPEDPULSEAMPLIFICATION:2||ALN:2||GAUSSIANBEAM:2||ASSISTED CATALYTIC GROWTH:2||BLUE:2||NANOSTRUCTURES:2||MAGNETOELECTRONICS:2||MICROSCOPY:2||ELECTROLUMINESCENCE:2||LASERPULSES:2||GaN nanowires:2||GALLIUM NITRIDE NANOWIRES:2||GAMNN:2||NANOTUBES:2||PHYSICS:2||Femtosecond laser:2||parametric oscillators and amplifiers:1||ultrafast lasers:1||VALENCE:1||nanowires:1||DILUTED MAGNETIC SEMICONDUCTOR:1||LUMINESCENCE:1||Density modulation:1||Energy modulation:1||Current enhanced SASE free electron laser:1||Undulator radiation:1||FREEELECTRON LASERS:1||ULTRATHIN FERROMAGNETICFILMS:1||OXIDEFILMS:1||ABLATION:1||COMPONENT:1||METAL:1||innershell excited states:1||Nelike ions:1||TRANSITIONS:1||XUV spectrometer:1||DIAGNOSTICS:1||Xray scattering:1||MO/SI:1||pulsed laser deposition:1||KEV IMPACT ENERGIES:1||vacuum electron acceleration:1||HIGHINTENSITY LASER:1||JUNCTIONS:1||LOWTEMPERATURE GROWTH:1||nanocrystalline materials:1||MOLECULAR PHOTOIONIZATION:1||LOCALIZATION:1||DEUTERIUM CLUSTERS:1||EXPLOSIONS:1||REGENERATIVE AMPLIFIERS:1||RAREGASES:1||THz radiation:1||FREEELECTRON LASER:1||REALTIME OBSERVATION:1||TARGET:1||photoionized plasmas:1||fs Xray laser:1||emission profile:1||HIGHORDER HARMONICS:1||Xray laser:1||atomic transition:1||EXCITATION:1||LASERS:1||PERFORMANCE:1||RELATIVISTIC ELECTRONS:1||BI2O3DOPED ZNO:1||INNERSHELL IONIZATION:1||Laser wakefield:1||FREQUENCY:1||SOLIDSTATE LASERS:1||Linearly polarized:1||THERMIONIC EMISSION:1||PULSE AMPLIFICATION SYSTEM:1||BIB3O6:1||NM:1||NONCOVALENT INTERACTIONS:1||CRYSTALLINE:1||INTENSITY:1||JETS:1||COHERENT:1||LINE:1||ANGULARDISTRIBUTION:1||SILVER IONS:1||magnetic anisotropy:1||DEVICES:1||Auger transitions:1||CosterKronig transitions:1||EFFICIENT:1||ELECTRONIMPACT IONIZATION:1||ULTRASHORTPULSE:1||Nanowire:1||Heterostructure:1||soft Xray reflectivity:1||PLASMA ACCELERATOR:1||ZINCOXIDE NANOWIRES:1||CHEMICALVAPORDEPOSITION:1||Electron acceleration:1||Ionization of gases:1||Delay dependent:1||MULTIPHOTON IONIZATION:1||FRAGMENTATION:1||GASJET:1||ultrafast nonlinear optics:1||CYCLE PULSES:1||KHZ:1||chemical vapor deposition:1||ferromagnetism:1||ABSORPTION:1||TERAHERTZ RADIATION:1||SCIENCE:1||FIELDS:1||ELECTRONS:1||nanomultilayer structures:1||YIELDS:1||AUGER:1||10HZ REPETITION RATE:1||MULTITERAWATT:1||SPECTROGRAPH:1||HIGHHARMONICGENERATION:1||spectroscopy:1||level population:1||PARTICLEACCELERATION:1||OPTICAL FREQUENCYMEASUREMENT:1||NANOWALLS:1||ROOMTEMPERATURE:1||AVERAGE OUTPUT POWER:1||GROUPVELOCITYMISMATCH:1||Impact ionization:1||Dynamics:1||Lasers:1||Collisional process:1||ABOVETHRESHOLD IONIZATION:1||MAINGROUP THERMOCHEMISTRY:1||dilute magnetic semiconductors:1||GACRN:1||SIZE:1||ATTOSECOND:1||Ar cluster:1||Xray astrophysics:1||photoionization:1||irons:1||normal incidence pulsed laser deposition:1||SHELLS:1||Silicon Oxide:1||gaspuff Zpinch:1||Xray:1||soft Xray reflectors:1||ESCAPE:1||ZN2SIO4:1||SILICA:1||Time 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materials:1||MOLECULAR PHOTOIONIZATION:1||LOCALIZATION:1||DEUTERIUM CLUSTERS:1||EXPLOSIONS:1||REGENERATIVE AMPLIFIERS:1||RAREGASES:1||THz radiation:1||FREEELECTRON LASER:1||REALTIME OBSERVATION:1||TARGET:1||photoionized plasmas:1||fs Xray laser:1||emission profile:1||HIGHORDER HARMONICS:1||Xray laser:1||atomic transition:1||EXCITATION:1||LASERS:1||PERFORMANCE:1||RELATIVISTIC ELECTRONS:1||BI2O3DOPED ZNO:1||INNERSHELL IONIZATION:1||Laser wakefield:1||FREQUENCY:1||SOLIDSTATE LASERS:1||Linearly polarized:1||THERMIONIC EMISSION:1||PULSE AMPLIFICATION SYSTEM:1||BIB3O6:1||NM:1||NONCOVALENT INTERACTIONS:1||CRYSTALLINE:1||INTENSITY:1||JETS:1||COHERENT:1||LINE:1||ANGULARDISTRIBUTION:1||SILVER IONS:1||magnetic anisotropy:1||DEVICES:1||Auger transitions:1||CosterKronig transitions:1||EFFICIENT:1||ELECTRONIMPACT IONIZATION:1||ULTRASHORTPULSE:1||Nanowire:1||Heterostructure:1||soft Xray reflectivity:1||PLASMA ACCELERATOR:1||ZINCOXIDE NANOWIRES:1||CHEMICALVAPORDEPOSITION:1||Electron acceleration:1||Ionization of gases:1||Delay dependent:1||MULTIPHOTON IONIZATION:1||FRAGMENTATION:1||GASJET:1||ultrafast nonlinear optics:1||CYCLE PULSES:1||KHZ:1||chemical vapor deposition:1||ferromagnetism:1||ABSORPTION:1||TERAHERTZ RADIATION:1||SCIENCE:1||FIELDS:1||ELECTRONS:1||nanomultilayer structures:1||YIELDS:1||AUGER:1||10HZ REPETITION RATE:1||MULTITERAWATT:1||SPECTROGRAPH:1||HIGHHARMONICGENERATION:1||spectroscopy:1||level population:1||PARTICLEACCELERATION:1||OPTICAL FREQUENCYMEASUREMENT:1||NANOWALLS:1||ROOMTEMPERATURE:1||AVERAGE OUTPUT POWER:1||GROUPVELOCITYMISMATCH:1||Impact ionization:1||Dynamics:1||Lasers:1||Collisional process:1||ABOVETHRESHOLD IONIZATION:1||MAINGROUP THERMOCHEMISTRY:1||dilute magnetic semiconductors:1||GACRN:1||SIZE:1||ATTOSECOND:1||Ar cluster:1||Xray astrophysics:1||photoionization:1||irons:1||normal incidence pulsed laser deposition:1||SHELLS:1||Silicon Oxide:1||gaspuff Zpinch:1||Xray:1||soft Xray reflectors:1||ESCAPE:1||ZN2SIO4:1||SILICA:1||Time delay:1||Collisional plasmas:1||MASSSPECTROMETRY:1||NUCLEARFUSION:1||PARAMETRIC AMPLIFICATION:1||LYING ELECTRONIC STATES:1||ADJUSTABLEPARAMETERS:1||MAGNETICPROPERTIES:1||LIQUIDPHASE EPITAXY:1||CEP laser:1||REGION:1||Plasma waveguide:1||AMBIENT GAS:1||DEPOSITION:1||HARMONICGENERATION:1||ENHANCEMENT:1||imaging spectrometer:1||Abel inversion:1||Water window:1||Liquid nitrogen jet:1||CHARGEEXCHANGE:1||NOBEL LECTURE:1||VARISTOR:1||EPITAXY:1||THINDISK LASER:1||HIGHREPETITIONRATE:1||Atom lasers:1||Electronimpact excitation:1||High order harmonics:1||ultrafast technology:1||PEAK POWER:1||CHARGED ALUMINUM CLUSTERS:1||GaN:1||THIN:1||Electron beam:1||INTENSE:1||Hard Xray pulse generation:1||NONLINEAR THOMSON SCATTERING:1||MULTILAYER:1||UVvisible spectrometer:1||ATOMS:1||innershell transitions:1||CORRECTED CONCAVE GRATINGS:1||DISCHARGE:1||LASERPLASMA:1||thin film:1||reflectivity:1||opacity:1||gain:1||smallangle Xray scattering:1||SOFTXRAY:1||ZINCOXIDE:1||CYGNUSX3:1||Betatron oscillation:1||ACCELERATOR:1||STRAINEDLAYER SUPERLATTICES:1||OPTICAL PARAMETRIC AMPLIFICATION:1||PASSIVE MODELOCKING:1||Collision dynamics:1||MUM:1||EXACTEXCHANGE:1||BASISSET:1||APPROXIMATION:1||OXYNITRIDES:1||Beam energy modulation:1||polarization spectroscopy:1||REORIENTATION TRANSITION:1||DEPENDENCE:1||sulfurs:1||BUILDINGBLOCKS:1||RATES:1||OPTICAL PULSES:1||toroidal mirror:1||XRAY LASER:1||CALCIUM:1||radially polarized laser:1||GRAINBOUNDARIES:1||VAPORDEPOSITION:1||Xray generation:1||MAGNETIZATION:1||Electric excitation:1||Laserinduced gas plasmas:1||Qualitative analysis:1||SCHEME:1||RADIATION:10||PULSES:8||PHOTOLUMINESCENCE:7||LASER:7||GENERATION:6||NANORODS:6||GROWTH:6||NANOWIRES:5||IMPLANTED GAN:5||SPECTROSCOPY:5||THINFILMS:4||DYNAMICS:4||SILICON:4||EXTREMEULTRAVIOLET:4||AMPLIFICATION:4||PRESSURE:4||PHASE:4||OPTICALPROPERTIES:4||SYSTEM:4||EMISSION:4||FEL:3||N2O:3||FILMS:3||OPTICS:3||SPECTRA:3||FIELD:3||MIRRORS:3||ARRAYS:3||CLUSTERS:3||SIO2:3||IONIZATION:3||VACUUM:3||SCATTERING:3||IONS:2||LUMINESCENCE PROPERTIES:2||ANISOTROPY:2||BEAMS:2||DIFFRACTION:2||DISPERSION:2||chemical vapor deposition (CVD):2||ELECTRONICSTRUCTURE:2||MOSFETS:2||SI3N4:2||DENSITY:2||LIGHT:2||PLASMAS:2||MATTER:2||nanocomposites:2||RAMANSCATTERING:2||NANOPARTICLES:2||OXIDE:2||AMPLIFIED SPONTANEOUS EMISSION:2||NM WAVELENGTH:2||GAIN:2||CARBON NANOTUBES:2||CROSSSECTIONS:2||LIGHTEMITTINGDIODES:2||PULSE:2||CARBON PLASMA:2||TISAPPHIRE LASER:2||Raman scattering:2||ROUTE:2||multilayer:2||CATHODOLUMINESCENCE:2||highresolution transmission electronic microscope (HRTEM):2||DIFFERENCEFREQUENCYGENERATION:2||CRYSTAL:2||laserproduced plasma:2||NANOCABLES:2||photoluminescence:2||MAGNETIC ALLOY SEMICONDUCTORS:2||MOLECULARBEAM EPITAXY:2||EARTHDOPED GAN:2||LASER FIELDS:2||CHIRPEDPULSEAMPLIFICATION:2||ALN:2||GAUSSIANBEAM:2||ASSISTED CATALYTIC GROWTH:2||BLUE:2||NANOSTRUCTURES:2||MAGNETOELECTRONICS:2||MICROSCOPY:2||ELECTROLUMINESCENCE:2||LASERPULSES:2||GaN nanowires:2||GALLIUM NITRIDE NANOWIRES:2||GAMNN:2||NANOTUBES:2||PHYSICS:2||Femtosecond laser:2||parametric oscillators and amplifiers:1||ultrafast lasers:1||VALENCE:1||nanowires:1||DILUTED MAGNETIC SEMICONDUCTOR:1||LUMINESCENCE:1||Density modulation:1||Energy modulation:1||Current enhanced SASE free electron laser:1||Undulator radiation:1||FREEELECTRON LASERS:1||ULTRATHIN FERROMAGNETICFILMS:1||OXIDEFILMS:1||ABLATION:1||COMPONENT:1||METAL:1||innershell excited states:1||Nelike ions:1||TRANSITIONS:1||XUV spectrometer:1||DIAGNOSTICS:1||Xray scattering:1||MO/SI:1||pulsed laser deposition:1||KEV IMPACT ENERGIES:1||vacuum electron acceleration:1||HIGHINTENSITY LASER:1||JUNCTIONS:1||LOWTEMPERATURE GROWTH:1||nanocrystalline materials:1||MOLECULAR PHOTOIONIZATION:1||LOCALIZATION:1||DEUTERIUM CLUSTERS:1||EXPLOSIONS:1||REGENERATIVE AMPLIFIERS:1||RAREGASES:1||THz radiation:1||FREEELECTRON LASER:1||REALTIME OBSERVATION:1||TARGET:1||photoionized plasmas:1||fs Xray laser:1||emission profile:1||HIGHORDER HARMONICS:1||Xray laser:1||atomic transition:1||EXCITATION:1||LASERS:1||PERFORMANCE:1||RELATIVISTIC ELECTRONS:1||BI2O3DOPED ZNO:1||INNERSHELL IONIZATION:1||Laser wakefield:1||FREQUENCY:1||SOLIDSTATE LASERS:1||Linearly polarized:1||THERMIONIC EMISSION:1||PULSE AMPLIFICATION SYSTEM:1||BIB3O6:1||NM:1||NONCOVALENT INTERACTIONS:1||CRYSTALLINE:1||INTENSITY:1||JETS:1||COHERENT:1||LINE:1||ANGULARDISTRIBUTION:1||SILVER IONS:1||magnetic anisotropy:1||DEVICES:1||Auger transitions:1||CosterKronig transitions:1||EFFICIENT:1||ELECTRONIMPACT IONIZATION:1||ULTRASHORTPULSE:1||Nanowire:1||Heterostructure:1||soft Xray reflectivity:1||PLASMA ACCELERATOR:1||ZINCOXIDE NANOWIRES:1||CHEMICALVAPORDEPOSITION:1||Electron acceleration:1||Ionization of gases:1||Delay dependent:1||MULTIPHOTON IONIZATION:1||FRAGMENTATION:1||GASJET:1||ultrafast nonlinear optics:1||CYCLE PULSES:1||KHZ:1||chemical vapor deposition:1||ferromagnetism:1||ABSORPTION:1||TERAHERTZ RADIATION:1||SCIENCE:1||FIELDS:1||ELECTRONS:1||nanomultilayer structures:1||YIELDS:1||AUGER:1||10HZ REPETITION RATE:1||MULTITERAWATT:1||SPECTROGRAPH:1||HIGHHARMONICGENERATION:1||spectroscopy:1||level population:1||PARTICLEACCELERATION:1||OPTICAL FREQUENCYMEASUREMENT:1||NANOWALLS:1||ROOMTEMPERATURE:1||AVERAGE OUTPUT POWER:1||GROUPVELOCITYMISMATCH:1||Impact ionization:1||Dynamics:1||Lasers:1||Collisional process:1||ABOVETHRESHOLD IONIZATION:1||MAINGROUP THERMOCHEMISTRY:1||dilute magnetic semiconductors:1||GACRN:1||SIZE:1||ATTOSECOND:1||Ar cluster:1||Xray astrophysics:1||photoionization:1||irons:1||normal incidence pulsed laser deposition:1||SHELLS:1||Silicon Oxide:1||gaspuff Zpinch:1||Xray:1||soft Xray reflectors:1||ESCAPE:1||ZN2SIO4:1||SILICA:1||Time delay:1||Collisional plasmas:1||MASSSPECTROMETRY:1||NUCLEARFUSION:1||PARAMETRIC AMPLIFICATION:1||LYING ELECTRONIC STATES:1||ADJUSTABLEPARAMETERS:1||MAGNETICPROPERTIES:1||LIQUIDPHASE EPITAXY:1||CEP laser:1||REGION:1||Plasma waveguide:1||AMBIENT GAS:1||DEPOSITION:1||HARMONICGENERATION:1||ENHANCEMENT:1||imaging spectrometer:1||Abel inversion:1||Water window:1||Liquid nitrogen jet:1||CHARGEEXCHANGE:1||NOBEL LECTURE:1||VARISTOR:1||EPITAXY:1||THINDISK LASER:1||HIGHREPETITIONRATE:1||Atom lasers:1||Electronimpact excitation:1||High order harmonics:1||ultrafast technology:1||PEAK POWER:1||CHARGED ALUMINUM CLUSTERS:1||GaN:1||THIN:1||Electron beam:1||INTENSE:1||Hard Xray pulse generation:1||NONLINEAR THOMSON SCATTERING:1||MULTILAYER:1||UVvisible spectrometer:1||ATOMS:1||innershell transitions:1||CORRECTED CONCAVE GRATINGS:1||DISCHARGE:1||LASERPLASMA:1||thin film:1||reflectivity:1||opacity:1||gain:1||smallangle Xray scattering:1||SOFTXRAY:1||ZINCOXIDE:1||CYGNUSX3:1||Betatron oscillation:1||ACCELERATOR:1||STRAINEDLAYER SUPERLATTICES:1||OPTICAL PARAMETRIC AMPLIFICATION:1||PASSIVE MODELOCKING:1||Collision dynamics:1||MUM:1||EXACTEXCHANGE:1||BASISSET:1||APPROXIMATION:1||OXYNITRIDES:1||Beam energy modulation:1||polarization spectroscopy:1||REORIENTATION TRANSITION:1||DEPENDENCE:1||sulfurs:1||BUILDINGBLOCKS:1||RATES:1||OPTICAL PULSES:1||toroidal mirror:1||XRAY LASER:1||CALCIUM:1||radially polarized laser:1||GRAINBOUNDARIES:1||VAPORDEPOSITION:1||Xray generation:1||MAGNETIZATION:1||Electric excitation:1||Laserinduced gas plasmas:1||Qualitative analysis:1||SCHEME:1||RADIATION:10||PULSES:8||PHOTOLUMINESCENCE:7||LASER:7||GENERATION:6||NANORODS:6||GROWTH:6||NANOWIRES:5||IMPLANTED 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SEMICONDUCTORS:2||MOLECULARBEAM EPITAXY:2||EARTHDOPED GAN:2||LASER FIELDS:2||CHIRPEDPULSEAMPLIFICATION:2||ALN:2||GAUSSIANBEAM:2||ASSISTED CATALYTIC GROWTH:2||BLUE:2||NANOSTRUCTURES:2||MAGNETOELECTRONICS:2||MICROSCOPY:2||ELECTROLUMINESCENCE:2||LASERPULSES:2||GaN nanowires:2||GALLIUM NITRIDE NANOWIRES:2||GAMNN:2||NANOTUBES:2||PHYSICS:2||Femtosecond laser:2||parametric oscillators and amplifiers:1||ultrafast lasers:1||VALENCE:1||nanowires:1||DILUTED MAGNETIC SEMICONDUCTOR:1||LUMINESCENCE:1||Density modulation:1||Energy modulation:1||Current enhanced SASE free electron laser:1||Undulator radiation:1||FREEELECTRON LASERS:1||ULTRATHIN FERROMAGNETICFILMS:1||OXIDEFILMS:1||ABLATION:1||COMPONENT:1||METAL:1||innershell excited states:1||Nelike ions:1||TRANSITIONS:1||XUV spectrometer:1||DIAGNOSTICS:1||Xray scattering:1||MO/SI:1||pulsed laser deposition:1||KEV IMPACT ENERGIES:1||vacuum electron acceleration:1||HIGHINTENSITY LASER:1||JUNCTIONS:1||LOWTEMPERATURE GROWTH:1||nanocrystalline materials:1||MOLECULAR PHOTOIONIZATION:1||LOCALIZATION:1||DEUTERIUM CLUSTERS:1||EXPLOSIONS:1||REGENERATIVE AMPLIFIERS:1||RAREGASES:1||THz radiation:1||FREEELECTRON LASER:1||REALTIME OBSERVATION:1||TARGET:1||photoionized plasmas:1||fs Xray laser:1||emission profile:1||HIGHORDER HARMONICS:1||Xray laser:1||atomic transition:1||EXCITATION:1||LASERS:1||PERFORMANCE:1||RELATIVISTIC ELECTRONS:1||BI2O3DOPED ZNO:1||INNERSHELL IONIZATION:1||Laser wakefield:1||FREQUENCY:1||SOLIDSTATE LASERS:1||Linearly polarized:1||THERMIONIC EMISSION:1||PULSE AMPLIFICATION SYSTEM:1||BIB3O6:1||NM:1||NONCOVALENT INTERACTIONS:1||CRYSTALLINE:1||INTENSITY:1||JETS:1||COHERENT:1||LINE:1||ANGULARDISTRIBUTION:1||SILVER IONS:1||magnetic anisotropy:1||DEVICES:1||Auger transitions:1||CosterKronig transitions:1||EFFICIENT:1||ELECTRONIMPACT IONIZATION:1||ULTRASHORTPULSE:1||Nanowire:1||Heterostructure:1||soft Xray reflectivity:1||PLASMA ACCELERATOR:1||ZINCOXIDE NANOWIRES:1||CHEMICALVAPORDEPOSITION:1||Electron acceleration:1||Ionization of gases:1||Delay dependent:1||MULTIPHOTON IONIZATION:1||FRAGMENTATION:1||GASJET:1||ultrafast nonlinear optics:1||CYCLE PULSES:1||KHZ:1||chemical vapor deposition:1||ferromagnetism:1||ABSORPTION:1||TERAHERTZ RADIATION:1||SCIENCE:1||FIELDS:1||ELECTRONS:1||nanomultilayer structures:1||YIELDS:1||AUGER:1||10HZ REPETITION RATE:1||MULTITERAWATT:1||SPECTROGRAPH:1||HIGHHARMONICGENERATION:1||spectroscopy:1||level population:1||PARTICLEACCELERATION:1||OPTICAL FREQUENCYMEASUREMENT:1||NANOWALLS:1||ROOMTEMPERATURE:1||AVERAGE OUTPUT POWER:1||GROUPVELOCITYMISMATCH:1||Impact ionization:1||Dynamics:1||Lasers:1||Collisional process:1||ABOVETHRESHOLD IONIZATION:1||MAINGROUP THERMOCHEMISTRY:1||dilute magnetic semiconductors:1||GACRN:1||SIZE:1||ATTOSECOND:1||Ar cluster:1||Xray astrophysics:1||photoionization:1||irons:1||normal incidence pulsed laser deposition:1||SHELLS:1||Silicon Oxide:1||gaspuff Zpinch:1||Xray:1||soft Xray reflectors:1||ESCAPE:1||ZN2SIO4:1||SILICA:1||Time 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materials:1||MOLECULAR PHOTOIONIZATION:1||LOCALIZATION:1||DEUTERIUM CLUSTERS:1||EXPLOSIONS:1||REGENERATIVE AMPLIFIERS:1||RAREGASES:1||THz radiation:1||FREEELECTRON LASER:1||REALTIME OBSERVATION:1||TARGET:1||photoionized plasmas:1||fs Xray laser:1||emission profile:1||HIGHORDER HARMONICS:1||Xray laser:1||atomic transition:1||EXCITATION:1||LASERS:1||PERFORMANCE:1||RELATIVISTIC ELECTRONS:1||BI2O3DOPED ZNO:1||INNERSHELL IONIZATION:1||Laser wakefield:1||FREQUENCY:1||SOLIDSTATE LASERS:1||Linearly polarized:1||THERMIONIC EMISSION:1||PULSE AMPLIFICATION SYSTEM:1||BIB3O6:1||NM:1||NONCOVALENT INTERACTIONS:1||CRYSTALLINE:1||INTENSITY:1||JETS:1||COHERENT:1||LINE:1||ANGULARDISTRIBUTION:1||SILVER IONS:1||magnetic anisotropy:1||DEVICES:1||Auger transitions:1||CosterKronig transitions:1||EFFICIENT:1||ELECTRONIMPACT IONIZATION:1||ULTRASHORTPULSE:1||Nanowire:1||Heterostructure:1||soft Xray reflectivity:1||PLASMA ACCELERATOR:1||ZINCOXIDE NANOWIRES:1||CHEMICALVAPORDEPOSITION:1||Electron acceleration:1||Ionization of gases:1||Delay dependent:1||MULTIPHOTON IONIZATION:1||FRAGMENTATION:1||GASJET:1||ultrafast nonlinear optics:1||CYCLE PULSES:1||KHZ:1||chemical vapor deposition:1||ferromagnetism:1||ABSORPTION:1||TERAHERTZ RADIATION:1||SCIENCE:1||FIELDS:1||ELECTRONS:1||nanomultilayer structures:1||YIELDS:1||AUGER:1||10HZ REPETITION RATE:1||MULTITERAWATT:1||SPECTROGRAPH:1||HIGHHARMONICGENERATION:1||spectroscopy:1||level population:1||PARTICLEACCELERATION:1||OPTICAL FREQUENCYMEASUREMENT:1||NANOWALLS:1||ROOMTEMPERATURE:1||AVERAGE OUTPUT POWER:1||GROUPVELOCITYMISMATCH:1||Impact ionization:1||Dynamics:1||Lasers:1||Collisional process:1||ABOVETHRESHOLD IONIZATION:1||MAINGROUP THERMOCHEMISTRY:1||dilute magnetic semiconductors:1||GACRN:1||SIZE:1||ATTOSECOND:1||Ar cluster:1||Xray astrophysics:1||photoionization:1||irons:1||normal incidence pulsed laser deposition:1||SHELLS:1||Silicon Oxide:1||gaspuff Zpinch:1||Xray:1||soft Xray reflectors:1||ESCAPE:1||ZN2SIO4:1||SILICA:1||Time delay:1||Collisional plasmas:1||MASSSPECTROMETRY:1||NUCLEARFUSION:1||PARAMETRIC AMPLIFICATION:1||LYING ELECTRONIC STATES:1||ADJUSTABLEPARAMETERS:1||MAGNETICPROPERTIES:1||LIQUIDPHASE EPITAXY:1||CEP laser:1||REGION:1||Plasma waveguide:1||AMBIENT GAS:1||DEPOSITION:1||HARMONICGENERATION:1||ENHANCEMENT:1||imaging spectrometer:1||Abel inversion:1||Water window:1||Liquid nitrogen jet:1||CHARGEEXCHANGE:1||NOBEL LECTURE:1||VARISTOR:1||EPITAXY:1||THINDISK LASER:1||HIGHREPETITIONRATE:1||Atom lasers:1||Electronimpact excitation:1||High order harmonics:1||ultrafast technology:1||PEAK POWER:1||CHARGED ALUMINUM CLUSTERS:1||GaN:1||THIN:1||Electron beam:1||INTENSE:1||Hard Xray pulse generation:1||NONLINEAR THOMSON SCATTERING:1||MULTILAYER:1||UVvisible spectrometer:1||ATOMS:1||innershell transitions:1||CORRECTED CONCAVE GRATINGS:1||DISCHARGE:1||LASERPLASMA:1||thin film:1||reflectivity:1||opacity:1||gain:1||smallangle Xray scattering:1||SOFTXRAY:1||ZINCOXIDE:1||CYGNUSX3:1||Betatron oscillation:1||ACCELERATOR:1||STRAINEDLAYER SUPERLATTICES:1||OPTICAL PARAMETRIC AMPLIFICATION:1||PASSIVE MODELOCKING:1||Collision dynamics:1||MUM:1||EXACTEXCHANGE:1||BASISSET:1||APPROXIMATION:1||OXYNITRIDES:1||Beam energy modulation:1||polarization spectroscopy:1||REORIENTATION TRANSITION:1||DEPENDENCE:1||sulfurs:1||BUILDINGBLOCKS:1||RATES:1||OPTICAL PULSES:1||toroidal mirror:1||XRAY LASER:1||CALCIUM:1||radially polarized laser:1||GRAINBOUNDARIES:1||VAPORDEPOSITION:1||Xray generation:1||MAGNETIZATION:1||Electric excitation:1||Laserinduced gas plasmas:1||Qualitative analysis:1||SCHEME:1||RADIATION:10||PULSES:8||PHOTOLUMINESCENCE:7||LASER:7||GENERATION:6||NANORODS:6||GROWTH:6||NANOWIRES:5||IMPLANTED GAN:5||SPECTROSCOPY:5||THINFILMS:4||DYNAMICS:4||SILICON:4||EXTREMEULTRAVIOLET:4||AMPLIFICATION:4||PRESSURE:4||PHASE:4||OPTICALPROPERTIES:4||SYSTEM:4||EMISSION:4||FEL:3||N2O:3||FILMS:3||OPTICS:3||SPECTRA:3||FIELD:3||MIRRORS:3||ARRAYS:3||CLUSTERS:3||SIO2:3||IONIZATION:3||VACUUM:3||SCATTERING:3||IONS:2||LUMINESCENCE PROPERTIES:2||ANISOTROPY:2||BEAMS:2||DIFFRACTION:2||DISPERSION:2||chemical vapor deposition (CVD):2||ELECTRONICSTRUCTURE:2||MOSFETS:2||SI3N4:2||DENSITY:2||LIGHT:2||PLASMAS:2||MATTER:2||nanocomposites:2||RAMANSCATTERING:2||NANOPARTICLES:2||OXIDE:2||AMPLIFIED SPONTANEOUS EMISSION:2||NM WAVELENGTH:2||GAIN:2||CARBON NANOTUBES:2||CROSSSECTIONS:2||LIGHTEMITTINGDIODES:2||PULSE:2||CARBON PLASMA:2||TISAPPHIRE LASER:2||Raman scattering:2||ROUTE:2||multilayer:2||CATHODOLUMINESCENCE:2||highresolution transmission electronic microscope (HRTEM):2||DIFFERENCEFREQUENCYGENERATION:2||CRYSTAL:2||laserproduced plasma:2||NANOCABLES:2||photoluminescence:2||MAGNETIC ALLOY SEMICONDUCTORS:2||MOLECULARBEAM EPITAXY:2||EARTHDOPED GAN:2||LASER FIELDS:2||CHIRPEDPULSEAMPLIFICATION:2||ALN:2||GAUSSIANBEAM:2||ASSISTED CATALYTIC GROWTH:2||BLUE:2||NANOSTRUCTURES:2||MAGNETOELECTRONICS:2||MICROSCOPY:2||ELECTROLUMINESCENCE:2||LASERPULSES:2||GaN nanowires:2||GALLIUM NITRIDE NANOWIRES:2||GAMNN:2||NANOTUBES:2||PHYSICS:2||Femtosecond laser:2||parametric oscillators and amplifiers:1||ultrafast lasers:1||VALENCE:1||nanowires:1||DILUTED MAGNETIC SEMICONDUCTOR:1||LUMINESCENCE:1||Density modulation:1||Energy modulation:1||Current enhanced SASE free electron laser:1||Undulator radiation:1||FREEELECTRON LASERS:1||ULTRATHIN FERROMAGNETICFILMS:1||OXIDEFILMS:1||ABLATION:1||COMPONENT:1||METAL:1||innershell excited states:1||Nelike ions:1||TRANSITIONS:1||XUV spectrometer:1||DIAGNOSTICS:1||Xray scattering:1||MO/SI:1||pulsed laser deposition:1||KEV IMPACT ENERGIES:1||vacuum electron acceleration:1||HIGHINTENSITY LASER:1||JUNCTIONS:1||LOWTEMPERATURE GROWTH:1||nanocrystalline materials:1||MOLECULAR PHOTOIONIZATION:1||LOCALIZATION:1||DEUTERIUM CLUSTERS:1||EXPLOSIONS:1||REGENERATIVE AMPLIFIERS:1||RAREGASES:1||THz radiation:1||FREEELECTRON LASER:1||REALTIME OBSERVATION:1||TARGET:1||photoionized plasmas:1||fs Xray laser:1||emission profile:1||HIGHORDER HARMONICS:1||Xray laser:1||atomic transition:1||EXCITATION:1||LASERS:1||PERFORMANCE:1||RELATIVISTIC ELECTRONS:1||BI2O3DOPED ZNO:1||INNERSHELL IONIZATION:1||Laser wakefield:1||FREQUENCY:1||SOLIDSTATE LASERS:1||Linearly polarized:1||THERMIONIC EMISSION:1||PULSE AMPLIFICATION SYSTEM:1||BIB3O6:1||NM:1||NONCOVALENT INTERACTIONS:1||CRYSTALLINE:1||INTENSITY:1||JETS:1||COHERENT:1||LINE:1||ANGULARDISTRIBUTION:1||SILVER IONS:1||magnetic anisotropy:1||DEVICES:1||Auger transitions:1||CosterKronig transitions:1||EFFICIENT:1||ELECTRONIMPACT IONIZATION:1||ULTRASHORTPULSE:1||Nanowire:1||Heterostructure:1||soft Xray reflectivity:1||PLASMA ACCELERATOR:1||ZINCOXIDE NANOWIRES:1||CHEMICALVAPORDEPOSITION:1||Electron acceleration:1||Ionization of gases:1||Delay dependent:1||MULTIPHOTON IONIZATION:1||FRAGMENTATION:1||GASJET:1||ultrafast nonlinear optics:1||CYCLE PULSES:1||KHZ:1||chemical vapor deposition:1||ferromagnetism:1||ABSORPTION:1||TERAHERTZ RADIATION:1||SCIENCE:1||FIELDS:1||ELECTRONS:1||nanomultilayer structures:1||YIELDS:1||AUGER:1||10HZ REPETITION RATE:1||MULTITERAWATT:1||SPECTROGRAPH:1||HIGHHARMONICGENERATION:1||spectroscopy:1||level population:1||PARTICLEACCELERATION:1||OPTICAL FREQUENCYMEASUREMENT:1||NANOWALLS:1||ROOMTEMPERATURE:1||AVERAGE OUTPUT POWER:1||GROUPVELOCITYMISMATCH:1||Impact ionization:1||Dynamics:1||Lasers:1||Collisional process:1||ABOVETHRESHOLD IONIZATION:1||MAINGROUP THERMOCHEMISTRY:1||dilute magnetic semiconductors:1||GACRN:1||SIZE:1||ATTOSECOND:1||Ar cluster:1||Xray astrophysics:1||photoionization:1||irons:1||normal incidence pulsed laser deposition:1||SHELLS:1||Silicon Oxide:1||gaspuff Zpinch:1||Xray:1||soft Xray reflectors:1||ESCAPE:1||ZN2SIO4:1||SILICA:1||Time delay:1||Collisional plasmas:1||MASSSPECTROMETRY:1||NUCLEARFUSION:1||PARAMETRIC AMPLIFICATION:1||LYING ELECTRONIC STATES:1||ADJUSTABLEPARAMETERS:1||MAGNETICPROPERTIES:1||LIQUIDPHASE EPITAXY:1||CEP laser:1||REGION:1||Plasma waveguide:1||AMBIENT GAS:1||DEPOSITION:1||HARMONICGENERATION:1||ENHANCEMENT:1||imaging spectrometer:1||Abel inversion:1||Water window:1||Liquid nitrogen jet:1||CHARGEEXCHANGE:1||NOBEL LECTURE:1||VARISTOR:1||EPITAXY:1||THINDISK LASER:1||HIGHREPETITIONRATE:1||Atom lasers:1||Electronimpact excitation:1||High order harmonics:1||ultrafast technology:1||PEAK POWER:1||CHARGED ALUMINUM CLUSTERS:1||GaN:1||THIN:1||Electron beam:1||INTENSE:1||Hard Xray pulse generation:1||NONLINEAR THOMSON SCATTERING:1||MULTILAYER:1||UVvisible spectrometer:1||ATOMS:1||innershell transitions:1||CORRECTED CONCAVE GRATINGS:1||DISCHARGE:1||LASERPLASMA:1||thin film:1||reflectivity:1||opacity:1||gain:1||smallangle Xray scattering:1||SOFTXRAY:1||ZINCOXIDE:1||CYGNUSX3:1||Betatron oscillation:1||ACCELERATOR:1||STRAINEDLAYER SUPERLATTICES:1||OPTICAL PARAMETRIC AMPLIFICATION:1||PASSIVE MODELOCKING:1||Collision dynamics:1||MUM:1||EXACTEXCHANGE:1||BASISSET:1||APPROXIMATION:1||OXYNITRIDES:1||Beam energy modulation:1||polarization spectroscopy:1||REORIENTATION TRANSITION:1||DEPENDENCE:1||sulfurs:1||BUILDINGBLOCKS:1||RATES:1||OPTICAL PULSES:1||toroidal mirror:1||XRAY LASER:1||CALCIUM:1||radially polarized laser:1||GRAINBOUNDARIES:1||VAPORDEPOSITION:1||Xray generation:1||MAGNETIZATION:1||Electric excitation:1||Laserinduced gas plasmas:1||Qualitative analysis:1||SCHEME:1||RADIATION:10||PULSES:8||PHOTOLUMINESCENCE:7||LASER:7||GENERATION:6||NANORODS:6||GROWTH:6||NANOWIRES:5||IMPLANTED 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SEMICONDUCTORS:2||MOLECULARBEAM EPITAXY:2||EARTHDOPED GAN:2||LASER FIELDS:2||CHIRPEDPULSEAMPLIFICATION:2||ALN:2||GAUSSIANBEAM:2||ASSISTED CATALYTIC GROWTH:2||BLUE:2||NANOSTRUCTURES:2||MAGNETOELECTRONICS:2||MICROSCOPY:2||ELECTROLUMINESCENCE:2||LASERPULSES:2||GaN nanowires:2||GALLIUM NITRIDE NANOWIRES:2||GAMNN:2||NANOTUBES:2||PHYSICS:2||Femtosecond laser:2||parametric oscillators and amplifiers:1||ultrafast lasers:1||VALENCE:1||nanowires:1||DILUTED MAGNETIC SEMICONDUCTOR:1||LUMINESCENCE:1||Density modulation:1||Energy modulation:1||Current enhanced SASE free electron laser:1||Undulator radiation:1||FREEELECTRON LASERS:1||ULTRATHIN FERROMAGNETICFILMS:1||OXIDEFILMS:1||ABLATION:1||COMPONENT:1||METAL:1||innershell excited states:1||Nelike ions:1||TRANSITIONS:1||XUV spectrometer:1||DIAGNOSTICS:1||Xray scattering:1||MO/SI:1||pulsed laser deposition:1||KEV IMPACT ENERGIES:1||vacuum electron acceleration:1||HIGHINTENSITY LASER:1||JUNCTIONS:1||LOWTEMPERATURE GROWTH:1||nanocrystalline materials:1||MOLECULAR PHOTOIONIZATION:1||LOCALIZATION:1||DEUTERIUM CLUSTERS:1||EXPLOSIONS:1||REGENERATIVE AMPLIFIERS:1||RAREGASES:1||THz radiation:1||FREEELECTRON LASER:1||REALTIME OBSERVATION:1||TARGET:1||photoionized plasmas:1||fs Xray laser:1||emission profile:1||HIGHORDER HARMONICS:1||Xray laser:1||atomic transition:1||EXCITATION:1||LASERS:1||PERFORMANCE:1||RELATIVISTIC ELECTRONS:1||BI2O3DOPED ZNO:1||INNERSHELL IONIZATION:1||Laser wakefield:1||FREQUENCY:1||SOLIDSTATE LASERS:1||Linearly polarized:1||THERMIONIC EMISSION:1||PULSE AMPLIFICATION SYSTEM:1||BIB3O6:1||NM:1||NONCOVALENT INTERACTIONS:1||CRYSTALLINE:1||INTENSITY:1||JETS:1||COHERENT:1||LINE:1||ANGULARDISTRIBUTION:1||SILVER IONS:1||magnetic anisotropy:1||DEVICES:1||Auger transitions:1||CosterKronig transitions:1||EFFICIENT:1||ELECTRONIMPACT IONIZATION:1||ULTRASHORTPULSE:1||Nanowire:1||Heterostructure:1||soft Xray reflectivity:1||PLASMA ACCELERATOR:1||ZINCOXIDE NANOWIRES:1||CHEMICALVAPORDEPOSITION:1||Electron acceleration:1||Ionization of gases:1||Delay dependent:1||MULTIPHOTON IONIZATION:1||FRAGMENTATION:1||GASJET:1||ultrafast nonlinear optics:1||CYCLE PULSES:1||KHZ:1||chemical vapor deposition:1||ferromagnetism:1||ABSORPTION:1||TERAHERTZ RADIATION:1||SCIENCE:1||FIELDS:1||ELECTRONS:1||nanomultilayer structures:1||YIELDS:1||AUGER:1||10HZ REPETITION RATE:1||MULTITERAWATT:1||SPECTROGRAPH:1||HIGHHARMONICGENERATION:1||spectroscopy:1||level population:1||PARTICLEACCELERATION:1||OPTICAL FREQUENCYMEASUREMENT:1||NANOWALLS:1||ROOMTEMPERATURE:1||AVERAGE OUTPUT POWER:1||GROUPVELOCITYMISMATCH:1||Impact ionization:1||Dynamics:1||Lasers:1||Collisional process:1||ABOVETHRESHOLD IONIZATION:1||MAINGROUP THERMOCHEMISTRY:1||dilute magnetic semiconductors:1||GACRN:1||SIZE:1||ATTOSECOND:1||Ar cluster:1||Xray astrophysics:1||photoionization:1||irons:1||normal incidence pulsed laser deposition:1||SHELLS:1||Silicon Oxide:1||gaspuff Zpinch:1||Xray:1||soft Xray reflectors:1||ESCAPE:1||ZN2SIO4:1||SILICA:1||Time 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materials:1||MOLECULAR PHOTOIONIZATION:1||LOCALIZATION:1||DEUTERIUM CLUSTERS:1||EXPLOSIONS:1||REGENERATIVE AMPLIFIERS:1||RAREGASES:1||THz radiation:1||FREEELECTRON LASER:1||REALTIME OBSERVATION:1||TARGET:1||photoionized plasmas:1||fs Xray laser:1||emission profile:1||HIGHORDER HARMONICS:1||Xray laser:1||atomic transition:1||EXCITATION:1||LASERS:1||PERFORMANCE:1||RELATIVISTIC ELECTRONS:1||BI2O3DOPED ZNO:1||INNERSHELL IONIZATION:1||Laser wakefield:1||FREQUENCY:1||SOLIDSTATE LASERS:1||Linearly polarized:1||THERMIONIC EMISSION:1||PULSE AMPLIFICATION SYSTEM:1||BIB3O6:1||NM:1||NONCOVALENT INTERACTIONS:1||CRYSTALLINE:1||INTENSITY:1||JETS:1||COHERENT:1||LINE:1||ANGULARDISTRIBUTION:1||SILVER IONS:1||magnetic anisotropy:1||DEVICES:1||Auger transitions:1||CosterKronig transitions:1||EFFICIENT:1||ELECTRONIMPACT IONIZATION:1||ULTRASHORTPULSE:1||Nanowire:1||Heterostructure:1||soft Xray reflectivity:1||PLASMA ACCELERATOR:1||ZINCOXIDE NANOWIRES:1||CHEMICALVAPORDEPOSITION:1||Electron acceleration:1||Ionization of gases:1||Delay dependent:1||MULTIPHOTON IONIZATION:1||FRAGMENTATION:1||GASJET:1||ultrafast nonlinear optics:1||CYCLE PULSES:1||KHZ:1||chemical vapor deposition:1||ferromagnetism:1||ABSORPTION:1||TERAHERTZ RADIATION:1||SCIENCE:1||FIELDS:1||ELECTRONS:1||nanomultilayer structures:1||YIELDS:1||AUGER:1||10HZ REPETITION RATE:1||MULTITERAWATT:1||SPECTROGRAPH:1||HIGHHARMONICGENERATION:1||spectroscopy:1||level population:1||PARTICLEACCELERATION:1||OPTICAL FREQUENCYMEASUREMENT:1||NANOWALLS:1||ROOMTEMPERATURE:1||AVERAGE OUTPUT POWER:1||GROUPVELOCITYMISMATCH:1||Impact ionization:1||Dynamics:1||Lasers:1||Collisional process:1||ABOVETHRESHOLD IONIZATION:1||MAINGROUP THERMOCHEMISTRY:1||dilute magnetic semiconductors:1||GACRN:1||SIZE:1||ATTOSECOND:1||Ar cluster:1||Xray astrophysics:1||photoionization:1||irons:1||normal incidence pulsed laser deposition:1||SHELLS:1||Silicon Oxide:1||gaspuff Zpinch:1||Xray:1||soft Xray reflectors:1||ESCAPE:1||ZN2SIO4:1||SILICA:1||Time delay:1||Collisional plasmas:1||MASSSPECTROMETRY:1||NUCLEARFUSION:1||PARAMETRIC AMPLIFICATION:1||LYING ELECTRONIC STATES:1||ADJUSTABLEPARAMETERS:1||MAGNETICPROPERTIES:1||LIQUIDPHASE EPITAXY:1||CEP laser:1||REGION:1||Plasma waveguide:1||AMBIENT GAS:1||DEPOSITION:1||HARMONICGENERATION:1||ENHANCEMENT:1||imaging spectrometer:1||Abel inversion:1||Water window:1||Liquid nitrogen jet:1||CHARGEEXCHANGE:1||NOBEL LECTURE:1||VARISTOR:1||EPITAXY:1||THINDISK LASER:1||HIGHREPETITIONRATE:1||Atom lasers:1||Electronimpact excitation:1||High order harmonics:1||ultrafast technology:1||PEAK POWER:1||CHARGED ALUMINUM CLUSTERS:1||GaN:1||THIN:1||Electron beam:1||INTENSE:1||Hard Xray pulse generation:1||NONLINEAR THOMSON SCATTERING:1||MULTILAYER:1||UVvisible spectrometer:1||ATOMS:1||innershell transitions:1||CORRECTED CONCAVE GRATINGS:1||DISCHARGE:1||LASERPLASMA:1||thin film:1||reflectivity:1||opacity:1||gain:1||smallangle Xray scattering:1||SOFTXRAY:1||ZINCOXIDE:1||CYGNUSX3:1||Betatron oscillation:1||ACCELERATOR:1||STRAINEDLAYER SUPERLATTICES:1||OPTICAL PARAMETRIC AMPLIFICATION:1||PASSIVE MODELOCKING:1||Collision dynamics:1||MUM:1||EXACTEXCHANGE:1||BASISSET:1||APPROXIMATION:1||OXYNITRIDES:1||Beam energy modulation:1||polarization spectroscopy:1||REORIENTATION TRANSITION:1||DEPENDENCE:1||sulfurs:1||BUILDINGBLOCKS:1||RATES:1||OPTICAL PULSES:1||toroidal mirror:1||XRAY LASER:1||CALCIUM:1||radially polarized laser:1||GRAINBOUNDARIES:1||VAPORDEPOSITION:1||Xray generation:1||MAGNETIZATION:1||Electric excitation:1||Laserinduced gas plasmas:1||Qualitative analysis:1||SCHEME:1||RADIATION:10||PULSES:8||PHOTOLUMINESCENCE:7||LASER:7||GENERATION:6||NANORODS:6||GROWTH:6||NANOWIRES:5||IMPLANTED GAN:5||SPECTROSCOPY:5||THINFILMS:4||DYNAMICS:4||SILICON:4||EXTREMEULTRAVIOLET:4||AMPLIFICATION:4||PRESSURE:4||PHASE:4||OPTICALPROPERTIES:4||SYSTEM:4||EMISSION:4||FEL:3||N2O:3||FILMS:3||OPTICS:3||SPECTRA:3||FIELD:3||MIRRORS:3||ARRAYS:3||CLUSTERS:3||SIO2:3||IONIZATION:3||VACUUM:3||SCATTERING:3||IONS:2||LUMINESCENCE PROPERTIES:2||ANISOTROPY:2||BEAMS:2||DIFFRACTION:2||DISPERSION:2||chemical vapor deposition (CVD):2||ELECTRONICSTRUCTURE:2||MOSFETS:2||SI3N4:2||DENSITY:2||LIGHT:2||PLASMAS:2||MATTER:2||nanocomposites:2||RAMANSCATTERING:2||NANOPARTICLES:2||OXIDE:2||AMPLIFIED SPONTANEOUS EMISSION:2||NM WAVELENGTH:2||GAIN:2||CARBON NANOTUBES:2||CROSSSECTIONS:2||LIGHTEMITTINGDIODES:2||PULSE:2||CARBON PLASMA:2||TISAPPHIRE LASER:2||Raman scattering:2||ROUTE:2||multilayer:2||CATHODOLUMINESCENCE:2||highresolution transmission electronic microscope (HRTEM):2||DIFFERENCEFREQUENCYGENERATION:2||CRYSTAL:2||laserproduced plasma:2||NANOCABLES:2||photoluminescence:2||MAGNETIC ALLOY SEMICONDUCTORS:2||MOLECULARBEAM EPITAXY:2||EARTHDOPED GAN:2||LASER FIELDS:2||CHIRPEDPULSEAMPLIFICATION:2||ALN:2||GAUSSIANBEAM:2||ASSISTED CATALYTIC GROWTH:2||BLUE:2||NANOSTRUCTURES:2||MAGNETOELECTRONICS:2||MICROSCOPY:2||ELECTROLUMINESCENCE:2||LASERPULSES:2||GaN nanowires:2||GALLIUM NITRIDE NANOWIRES:2||GAMNN:2||NANOTUBES:2||PHYSICS:2||Femtosecond laser:2||parametric oscillators and amplifiers:1||ultrafast lasers:1||VALENCE:1||nanowires:1||DILUTED MAGNETIC SEMICONDUCTOR:1||LUMINESCENCE:1||Density modulation:1||Energy modulation:1||Current enhanced SASE free electron laser:1||Undulator radiation:1||FREEELECTRON LASERS:1||ULTRATHIN FERROMAGNETICFILMS:1||OXIDEFILMS:1||ABLATION:1||COMPONENT:1||METAL:1||innershell excited states:1||Nelike ions:1||TRANSITIONS:1||XUV spectrometer:1||DIAGNOSTICS:1||Xray scattering:1||MO/SI:1||pulsed laser deposition:1||KEV IMPACT ENERGIES:1||vacuum electron acceleration:1||HIGHINTENSITY LASER:1||JUNCTIONS:1||LOWTEMPERATURE GROWTH:1||nanocrystalline materials:1||MOLECULAR PHOTOIONIZATION:1||LOCALIZATION:1||DEUTERIUM CLUSTERS:1||EXPLOSIONS:1||REGENERATIVE AMPLIFIERS:1||RAREGASES:1||THz radiation:1||FREEELECTRON LASER:1||REALTIME OBSERVATION:1||TARGET:1||photoionized plasmas:1||fs Xray laser:1||emission profile:1||HIGHORDER HARMONICS:1||Xray laser:1||atomic transition:1||EXCITATION:1||LASERS:1||PERFORMANCE:1||RELATIVISTIC ELECTRONS:1||BI2O3DOPED ZNO:1||INNERSHELL IONIZATION:1||Laser wakefield:1||FREQUENCY:1||SOLIDSTATE LASERS:1||Linearly polarized:1||THERMIONIC EMISSION:1||PULSE AMPLIFICATION SYSTEM:1||BIB3O6:1||NM:1||NONCOVALENT INTERACTIONS:1||CRYSTALLINE:1||INTENSITY:1||JETS:1||COHERENT:1||LINE:1||ANGULARDISTRIBUTION:1||SILVER IONS:1||magnetic anisotropy:1||DEVICES:1||Auger transitions:1||CosterKronig transitions:1||EFFICIENT:1||ELECTRONIMPACT IONIZATION:1||ULTRASHORTPULSE:1||Nanowire:1||Heterostructure:1||soft Xray reflectivity:1||PLASMA ACCELERATOR:1||ZINCOXIDE NANOWIRES:1||CHEMICALVAPORDEPOSITION:1||Electron acceleration:1||Ionization of gases:1||Delay dependent:1||MULTIPHOTON IONIZATION:1||FRAGMENTATION:1||GASJET:1||ultrafast nonlinear optics:1||CYCLE PULSES:1||KHZ:1||chemical vapor deposition:1||ferromagnetism:1||ABSORPTION:1||TERAHERTZ RADIATION:1||SCIENCE:1||FIELDS:1||ELECTRONS:1||nanomultilayer structures:1||YIELDS:1||AUGER:1||10HZ REPETITION RATE:1||MULTITERAWATT:1||SPECTROGRAPH:1||HIGHHARMONICGENERATION:1||spectroscopy:1||level population:1||PARTICLEACCELERATION:1||OPTICAL FREQUENCYMEASUREMENT:1||NANOWALLS:1||ROOMTEMPERATURE:1||AVERAGE OUTPUT POWER:1||GROUPVELOCITYMISMATCH:1||Impact ionization:1||Dynamics:1||Lasers:1||Collisional process:1||ABOVETHRESHOLD IONIZATION:1||MAINGROUP THERMOCHEMISTRY:1||dilute magnetic semiconductors:1||GACRN:1||SIZE:1||ATTOSECOND:1||Ar cluster:1||Xray astrophysics:1||photoionization:1||irons:1||normal incidence pulsed laser deposition:1||SHELLS:1||Silicon Oxide:1||gaspuff Zpinch:1||Xray:1||soft Xray reflectors:1||ESCAPE:1||ZN2SIO4:1||SILICA:1||Time delay:1||Collisional plasmas:1||MASSSPECTROMETRY:1||NUCLEARFUSION:1||PARAMETRIC AMPLIFICATION:1||LYING ELECTRONIC STATES:1||ADJUSTABLEPARAMETERS:1||MAGNETICPROPERTIES:1||LIQUIDPHASE EPITAXY:1||CEP laser:1||REGION:1||Plasma waveguide:1||AMBIENT GAS:1||DEPOSITION:1||HARMONICGENERATION:1||ENHANCEMENT:1||imaging spectrometer:1||Abel inversion:1||Water window:1||Liquid nitrogen jet:1||CHARGEEXCHANGE:1||NOBEL LECTURE:1||VARISTOR:1||EPITAXY:1||THINDISK LASER:1||HIGHREPETITIONRATE:1||Atom lasers:1||Electronimpact excitation:1||High order harmonics:1||ultrafast technology:1||PEAK POWER:1||CHARGED ALUMINUM CLUSTERS:1||GaN:1||THIN:1||Electron beam:1||INTENSE:1||Hard Xray pulse generation:1||NONLINEAR THOMSON SCATTERING:1||MULTILAYER:1||UVvisible spectrometer:1||ATOMS:1||innershell transitions:1||CORRECTED CONCAVE GRATINGS:1||DISCHARGE:1||LASERPLASMA:1||thin film:1||reflectivity:1||opacity:1||gain:1||smallangle Xray scattering:1||SOFTXRAY:1||ZINCOXIDE:1||CYGNUSX3:1||Betatron oscillation:1||ACCELERATOR:1||STRAINEDLAYER SUPERLATTICES:1||OPTICAL PARAMETRIC AMPLIFICATION:1||PASSIVE MODELOCKING:1||Collision dynamics:1||MUM:1||EXACTEXCHANGE:1||BASISSET:1||APPROXIMATION:1||OXYNITRIDES:1||Beam energy modulation:1||polarization spectroscopy:1||REORIENTATION TRANSITION:1||DEPENDENCE:1||sulfurs:1||BUILDINGBLOCKS:1||RATES:1||OPTICAL PULSES:1||toroidal mirror:1||XRAY LASER:1||CALCIUM:1||radially polarized laser:1||GRAINBOUNDARIES:1||VAPORDEPOSITION:1||Xray generation:1||MAGNETIZATION:1||Electric excitation:1||Laserinduced gas plasmas:1||Qualitative analysis:1||SCHEME:1||RADIATION:10||PULSES:8||PHOTOLUMINESCENCE:7||LASER:7||GENERATION:6||NANORODS:6||GROWTH:6||NANOWIRES:5||IMPLANTED 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SEMICONDUCTORS:2||MOLECULARBEAM EPITAXY:2||EARTHDOPED GAN:2||LASER FIELDS:2||CHIRPEDPULSEAMPLIFICATION:2||ALN:2||GAUSSIANBEAM:2||ASSISTED CATALYTIC GROWTH:2||BLUE:2||NANOSTRUCTURES:2||MAGNETOELECTRONICS:2||MICROSCOPY:2||ELECTROLUMINESCENCE:2||LASERPULSES:2||GaN nanowires:2||GALLIUM NITRIDE NANOWIRES:2||GAMNN:2||NANOTUBES:2||PHYSICS:2||Femtosecond laser:2||parametric oscillators and amplifiers:1||ultrafast lasers:1||VALENCE:1||nanowires:1||DILUTED MAGNETIC SEMICONDUCTOR:1||LUMINESCENCE:1||Density modulation:1||Energy modulation:1||Current enhanced SASE free electron laser:1||Undulator radiation:1||FREEELECTRON LASERS:1||ULTRATHIN FERROMAGNETICFILMS:1||OXIDEFILMS:1||ABLATION:1||COMPONENT:1||METAL:1||innershell excited states:1||Nelike ions:1||TRANSITIONS:1||XUV spectrometer:1||DIAGNOSTICS:1||Xray scattering:1||MO/SI:1||pulsed laser deposition:1||KEV IMPACT ENERGIES:1||vacuum electron acceleration:1||HIGHINTENSITY LASER:1||JUNCTIONS:1||LOWTEMPERATURE GROWTH:1||nanocrystalline materials:1||MOLECULAR PHOTOIONIZATION:1||LOCALIZATION:1||DEUTERIUM CLUSTERS:1||EXPLOSIONS:1||REGENERATIVE AMPLIFIERS:1||RAREGASES:1||THz radiation:1||FREEELECTRON LASER:1||REALTIME OBSERVATION:1||TARGET:1||photoionized plasmas:1||fs Xray laser:1||emission profile:1||HIGHORDER HARMONICS:1||Xray laser:1||atomic transition:1||EXCITATION:1||LASERS:1||PERFORMANCE:1||RELATIVISTIC ELECTRONS:1||BI2O3DOPED ZNO:1||INNERSHELL IONIZATION:1||Laser wakefield:1||FREQUENCY:1||SOLIDSTATE LASERS:1||Linearly polarized:1||THERMIONIC EMISSION:1||PULSE AMPLIFICATION SYSTEM:1||BIB3O6:1||NM:1||NONCOVALENT INTERACTIONS:1||CRYSTALLINE:1||INTENSITY:1||JETS:1||COHERENT:1||LINE:1||ANGULARDISTRIBUTION:1||SILVER IONS:1||magnetic anisotropy:1||DEVICES:1||Auger transitions:1||CosterKronig transitions:1||EFFICIENT:1||ELECTRONIMPACT IONIZATION:1||ULTRASHORTPULSE:1||Nanowire:1||Heterostructure:1||soft Xray reflectivity:1||PLASMA ACCELERATOR:1||ZINCOXIDE NANOWIRES:1||CHEMICALVAPORDEPOSITION:1||Electron acceleration:1||Ionization of gases:1||Delay dependent:1||MULTIPHOTON IONIZATION:1||FRAGMENTATION:1||GASJET:1||ultrafast nonlinear optics:1||CYCLE PULSES:1||KHZ:1||chemical vapor deposition:1||ferromagnetism:1||ABSORPTION:1||TERAHERTZ RADIATION:1||SCIENCE:1||FIELDS:1||ELECTRONS:1||nanomultilayer structures:1||YIELDS:1||AUGER:1||10HZ REPETITION RATE:1||MULTITERAWATT:1||SPECTROGRAPH:1||HIGHHARMONICGENERATION:1||spectroscopy:1||level population:1||PARTICLEACCELERATION:1||OPTICAL FREQUENCYMEASUREMENT:1||NANOWALLS:1||ROOMTEMPERATURE:1||AVERAGE OUTPUT POWER:1||GROUPVELOCITYMISMATCH:1||Impact ionization:1||Dynamics:1||Lasers:1||Collisional process:1||ABOVETHRESHOLD IONIZATION:1||MAINGROUP THERMOCHEMISTRY:1||dilute magnetic semiconductors:1||GACRN:1||SIZE:1||ATTOSECOND:1||Ar cluster:1||Xray astrophysics:1||photoionization:1||irons:1||normal incidence pulsed laser deposition:1||SHELLS:1||Silicon Oxide:1||gaspuff Zpinch:1||Xray:1||soft Xray reflectors:1||ESCAPE:1||ZN2SIO4:1||SILICA:1||Time 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materials:1||MOLECULAR PHOTOIONIZATION:1||LOCALIZATION:1||DEUTERIUM CLUSTERS:1||EXPLOSIONS:1||REGENERATIVE AMPLIFIERS:1||RAREGASES:1||THz radiation:1||FREEELECTRON LASER:1||REALTIME OBSERVATION:1||TARGET:1||photoionized plasmas:1||fs Xray laser:1||emission profile:1||HIGHORDER HARMONICS:1||Xray laser:1||atomic transition:1||EXCITATION:1||LASERS:1||PERFORMANCE:1||RELATIVISTIC ELECTRONS:1||BI2O3DOPED ZNO:1||INNERSHELL IONIZATION:1||Laser wakefield:1||FREQUENCY:1||SOLIDSTATE LASERS:1||Linearly polarized:1||THERMIONIC EMISSION:1||PULSE AMPLIFICATION SYSTEM:1||BIB3O6:1||NM:1||NONCOVALENT INTERACTIONS:1||CRYSTALLINE:1||INTENSITY:1||JETS:1||COHERENT:1||LINE:1||ANGULARDISTRIBUTION:1||SILVER IONS:1||magnetic anisotropy:1||DEVICES:1||Auger transitions:1||CosterKronig transitions:1||EFFICIENT:1||ELECTRONIMPACT IONIZATION:1||ULTRASHORTPULSE:1||Nanowire:1||Heterostructure:1||soft Xray reflectivity:1||PLASMA ACCELERATOR:1||ZINCOXIDE NANOWIRES:1||CHEMICALVAPORDEPOSITION:1||Electron acceleration:1||Ionization of gases:1||Delay dependent:1||MULTIPHOTON IONIZATION:1||FRAGMENTATION:1||GASJET:1||ultrafast nonlinear optics:1||CYCLE PULSES:1||KHZ:1||chemical vapor deposition:1||ferromagnetism:1||ABSORPTION:1||TERAHERTZ RADIATION:1||SCIENCE:1||FIELDS:1||ELECTRONS:1||nanomultilayer structures:1||YIELDS:1||AUGER:1||10HZ REPETITION RATE:1||MULTITERAWATT:1||SPECTROGRAPH:1||HIGHHARMONICGENERATION:1||spectroscopy:1||level population:1||PARTICLEACCELERATION:1||OPTICAL FREQUENCYMEASUREMENT:1||NANOWALLS:1||ROOMTEMPERATURE:1||AVERAGE OUTPUT POWER:1||GROUPVELOCITYMISMATCH:1||Impact ionization:1||Dynamics:1||Lasers:1||Collisional process:1||ABOVETHRESHOLD IONIZATION:1||MAINGROUP THERMOCHEMISTRY:1||dilute magnetic semiconductors:1||GACRN:1||SIZE:1||ATTOSECOND:1||Ar cluster:1||Xray astrophysics:1||photoionization:1||irons:1||normal incidence pulsed laser deposition:1||SHELLS:1||Silicon Oxide:1||gaspuff Zpinch:1||Xray:1||soft Xray reflectors:1||ESCAPE:1||ZN2SIO4:1||SILICA:1||Time delay:1||Collisional plasmas:1||MASSSPECTROMETRY:1||NUCLEARFUSION:1||PARAMETRIC AMPLIFICATION:1||LYING ELECTRONIC STATES:1||ADJUSTABLEPARAMETERS:1||MAGNETICPROPERTIES:1||LIQUIDPHASE EPITAXY:1||CEP laser:1||REGION:1||Plasma waveguide:1||AMBIENT GAS:1||DEPOSITION:1||HARMONICGENERATION:1||ENHANCEMENT:1||imaging spectrometer:1||Abel inversion:1||Water window:1||Liquid nitrogen jet:1||CHARGEEXCHANGE:1||NOBEL LECTURE:1||VARISTOR:1||EPITAXY:1||THINDISK LASER:1||HIGHREPETITIONRATE:1||Atom lasers:1||Electronimpact excitation:1||High order harmonics:1||ultrafast technology:1||PEAK POWER:1||CHARGED ALUMINUM CLUSTERS:1||GaN:1||THIN:1||Electron beam:1||INTENSE:1||Hard Xray pulse generation:1||NONLINEAR THOMSON SCATTERING:1||MULTILAYER:1||UVvisible spectrometer:1||ATOMS:1||innershell transitions:1||CORRECTED CONCAVE GRATINGS:1||DISCHARGE:1||LASERPLASMA:1||thin film:1||reflectivity:1||opacity:1||gain:1||smallangle Xray scattering:1||SOFTXRAY:1||ZINCOXIDE:1||CYGNUSX3:1||Betatron oscillation:1||ACCELERATOR:1||STRAINEDLAYER SUPERLATTICES:1||OPTICAL PARAMETRIC AMPLIFICATION:1||PASSIVE MODELOCKING:1||Collision dynamics:1||MUM:1||EXACTEXCHANGE:1||BASISSET:1||APPROXIMATION:1||OXYNITRIDES:1||Beam energy modulation:1||polarization spectroscopy:1||REORIENTATION TRANSITION:1||DEPENDENCE:1||sulfurs:1||BUILDINGBLOCKS:1||RATES:1||OPTICAL PULSES:1||toroidal mirror:1||XRAY LASER:1||CALCIUM:1||radially polarized laser:1||GRAINBOUNDARIES:1||VAPORDEPOSITION:1||Xray generation:1||MAGNETIZATION:1||Electric excitation:1||Laserinduced gas plasmas:1||Qualitative analysis:1||SCHEME:1||RADIATION:10||PULSES:8||PHOTOLUMINESCENCE:7||LASER:7||GENERATION:6||NANORODS:6||GROWTH:6||NANOWIRES:5||IMPLANTED GAN:5||SPECTROSCOPY:5||THINFILMS:4||DYNAMICS:4||SILICON:4||EXTREMEULTRAVIOLET:4||AMPLIFICATION:4||PRESSURE:4||PHASE:4||OPTICALPROPERTIES:4||SYSTEM:4||EMISSION:4||FEL:3||N2O:3||FILMS:3||OPTICS:3||SPECTRA:3||FIELD:3||MIRRORS:3||ARRAYS:3||CLUSTERS:3||SIO2:3||IONIZATION:3||VACUUM:3||SCATTERING:3||IONS:2||LUMINESCENCE PROPERTIES:2||ANISOTROPY:2||BEAMS:2||DIFFRACTION:2||DISPERSION:2||chemical vapor deposition (CVD):2||ELECTRONICSTRUCTURE:2||MOSFETS:2||SI3N4:2||DENSITY:2||LIGHT:2||PLASMAS:2||MATTER:2||nanocomposites:2||RAMANSCATTERING:2||NANOPARTICLES:2||OXIDE:2||AMPLIFIED SPONTANEOUS EMISSION:2||NM WAVELENGTH:2||GAIN:2||CARBON NANOTUBES:2||CROSSSECTIONS:2||LIGHTEMITTINGDIODES:2||PULSE:2||CARBON PLASMA:2||TISAPPHIRE LASER:2||Raman scattering:2||ROUTE:2||multilayer:2||CATHODOLUMINESCENCE:2||highresolution transmission electronic microscope (HRTEM):2||DIFFERENCEFREQUENCYGENERATION:2||CRYSTAL:2||laserproduced plasma:2||NANOCABLES:2||photoluminescence:2||MAGNETIC ALLOY SEMICONDUCTORS:2||MOLECULARBEAM EPITAXY:2||EARTHDOPED GAN:2||LASER FIELDS:2||CHIRPEDPULSEAMPLIFICATION:2||ALN:2||GAUSSIANBEAM:2||ASSISTED CATALYTIC GROWTH:2||BLUE:2||NANOSTRUCTURES:2||MAGNETOELECTRONICS:2||MICROSCOPY:2||ELECTROLUMINESCENCE:2||LASERPULSES:2||GaN nanowires:2||GALLIUM NITRIDE NANOWIRES:2||GAMNN:2||NANOTUBES:2||PHYSICS:2||Femtosecond laser:2||parametric oscillators and amplifiers:1||ultrafast lasers:1||VALENCE:1||nanowires:1||DILUTED MAGNETIC SEMICONDUCTOR:1||LUMINESCENCE:1||Density modulation:1||Energy modulation:1||Current enhanced SASE free electron laser:1||Undulator radiation:1||FREEELECTRON LASERS:1||ULTRATHIN FERROMAGNETICFILMS:1||OXIDEFILMS:1||ABLATION:1||COMPONENT:1||METAL:1||innershell excited states:1||Nelike ions:1||TRANSITIONS:1||XUV spectrometer:1||DIAGNOSTICS:1||Xray scattering:1||MO/SI:1||pulsed laser deposition:1||KEV IMPACT ENERGIES:1||vacuum electron acceleration:1||HIGHINTENSITY LASER:1||JUNCTIONS:1||LOWTEMPERATURE GROWTH:1||nanocrystalline materials:1||MOLECULAR PHOTOIONIZATION:1||LOCALIZATION:1||DEUTERIUM CLUSTERS:1||EXPLOSIONS:1||REGENERATIVE AMPLIFIERS:1||RAREGASES:1||THz radiation:1||FREEELECTRON LASER:1||REALTIME OBSERVATION:1||TARGET:1||photoionized plasmas:1||fs Xray laser:1||emission profile:1||HIGHORDER HARMONICS:1||Xray laser:1||atomic transition:1||EXCITATION:1||LASERS:1||PERFORMANCE:1||RELATIVISTIC ELECTRONS:1||BI2O3DOPED ZNO:1||INNERSHELL IONIZATION:1||Laser wakefield:1||FREQUENCY:1||SOLIDSTATE LASERS:1||Linearly polarized:1||THERMIONIC EMISSION:1||PULSE AMPLIFICATION SYSTEM:1||BIB3O6:1||NM:1||NONCOVALENT INTERACTIONS:1||CRYSTALLINE:1||INTENSITY:1||JETS:1||COHERENT:1||LINE:1||ANGULARDISTRIBUTION:1||SILVER IONS:1||magnetic anisotropy:1||DEVICES:1||Auger transitions:1||CosterKronig transitions:1||EFFICIENT:1||ELECTRONIMPACT IONIZATION:1||ULTRASHORTPULSE:1||Nanowire:1||Heterostructure:1||soft Xray reflectivity:1||PLASMA ACCELERATOR:1||ZINCOXIDE NANOWIRES:1||CHEMICALVAPORDEPOSITION:1||Electron acceleration:1||Ionization of gases:1||Delay dependent:1||MULTIPHOTON IONIZATION:1||FRAGMENTATION:1||GASJET:1||ultrafast nonlinear optics:1||CYCLE PULSES:1||KHZ:1||chemical vapor deposition:1||ferromagnetism:1||ABSORPTION:1||TERAHERTZ RADIATION:1||SCIENCE:1||FIELDS:1||ELECTRONS:1||nanomultilayer structures:1||YIELDS:1||AUGER:1||10HZ REPETITION RATE:1||MULTITERAWATT:1||SPECTROGRAPH:1||HIGHHARMONICGENERATION:1||spectroscopy:1||level population:1||PARTICLEACCELERATION:1||OPTICAL FREQUENCYMEASUREMENT:1||NANOWALLS:1||ROOMTEMPERATURE:1||AVERAGE OUTPUT POWER:1||GROUPVELOCITYMISMATCH:1||Impact ionization:1||Dynamics:1||Lasers:1||Collisional process:1||ABOVETHRESHOLD IONIZATION:1||MAINGROUP THERMOCHEMISTRY:1||dilute magnetic semiconductors:1||GACRN:1||SIZE:1||ATTOSECOND:1||Ar cluster:1||Xray astrophysics:1||photoionization:1||irons:1||normal incidence pulsed laser deposition:1||SHELLS:1||Silicon Oxide:1||gaspuff Zpinch:1||Xray:1||soft Xray reflectors:1||ESCAPE:1||ZN2SIO4:1||SILICA:1||Time delay:1||Collisional plasmas:1||MASSSPECTROMETRY:1||NUCLEARFUSION:1||PARAMETRIC AMPLIFICATION:1||LYING ELECTRONIC STATES:1||ADJUSTABLEPARAMETERS:1||MAGNETICPROPERTIES:1||LIQUIDPHASE EPITAXY:1||CEP laser:1||REGION:1||Plasma waveguide:1||AMBIENT GAS:1||DEPOSITION:1||HARMONICGENERATION:1||ENHANCEMENT:1||imaging spectrometer:1||Abel inversion:1||Water window:1||Liquid nitrogen jet:1||CHARGEEXCHANGE:1||NOBEL LECTURE:1||VARISTOR:1||EPITAXY:1||THINDISK LASER:1||HIGHREPETITIONRATE:1||Atom lasers:1||Electronimpact excitation:1||High order harmonics:1||ultrafast technology:1||PEAK POWER:1||CHARGED ALUMINUM CLUSTERS:1||GaN:1||THIN:1||Electron beam:1||INTENSE:1||Hard Xray pulse generation:1||NONLINEAR THOMSON SCATTERING:1||MULTILAYER:1||UVvisible spectrometer:1||ATOMS:1||innershell transitions:1||CORRECTED CONCAVE GRATINGS:1||DISCHARGE:1||LASERPLASMA:1||thin film:1||reflectivity:1||opacity:1||gain:1||smallangle Xray scattering:1||SOFTXRAY:1||ZINCOXIDE:1||CYGNUSX3:1||Betatron oscillation:1||ACCELERATOR:1||STRAINEDLAYER SUPERLATTICES:1||OPTICAL PARAMETRIC AMPLIFICATION:1||PASSIVE MODELOCKING:1||Collision dynamics:1||MUM:1||EXACTEXCHANGE:1||BASISSET:1||APPROXIMATION:1||OXYNITRIDES:1||Beam energy modulation:1||polarization spectroscopy:1||REORIENTATION TRANSITION:1||DEPENDENCE:1||sulfurs:1||BUILDINGBLOCKS:1||RATES:1||OPTICAL PULSES:1||toroidal mirror:1||XRAY LASER:1||CALCIUM:1||radially polarized laser:1||GRAINBOUNDARIES:1||VAPORDEPOSITION:1||Xray generation:1||MAGNETIZATION:1||Electric excitation:1||Laserinduced gas plasmas:1||Qualitative analysis:1||SCHEME:1||RADIATION:10||PULSES:8||PHOTOLUMINESCENCE:7||LASER:7||GENERATION:6||NANORODS:6||GROWTH:6||NANOWIRES:5||IMPLANTED 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SEMICONDUCTORS:2||MOLECULARBEAM EPITAXY:2||EARTHDOPED GAN:2||LASER FIELDS:2||CHIRPEDPULSEAMPLIFICATION:2||ALN:2||GAUSSIANBEAM:2||ASSISTED CATALYTIC GROWTH:2||BLUE:2||NANOSTRUCTURES:2||MAGNETOELECTRONICS:2||MICROSCOPY:2||ELECTROLUMINESCENCE:2||LASERPULSES:2||GaN nanowires:2||GALLIUM NITRIDE NANOWIRES:2||GAMNN:2||NANOTUBES:2||PHYSICS:2||Femtosecond laser:2||parametric oscillators and amplifiers:1||ultrafast lasers:1||VALENCE:1||nanowires:1||DILUTED MAGNETIC SEMICONDUCTOR:1||LUMINESCENCE:1||Density modulation:1||Energy modulation:1||Current enhanced SASE free electron laser:1||Undulator radiation:1||FREEELECTRON LASERS:1||ULTRATHIN FERROMAGNETICFILMS:1||OXIDEFILMS:1||ABLATION:1||COMPONENT:1||METAL:1||innershell excited states:1||Nelike ions:1||TRANSITIONS:1||XUV spectrometer:1||DIAGNOSTICS:1||Xray scattering:1||MO/SI:1||pulsed laser deposition:1||KEV IMPACT ENERGIES:1||vacuum electron acceleration:1||HIGHINTENSITY LASER:1||JUNCTIONS:1||LOWTEMPERATURE GROWTH:1||nanocrystalline materials:1||MOLECULAR PHOTOIONIZATION:1||LOCALIZATION:1||DEUTERIUM CLUSTERS:1||EXPLOSIONS:1||REGENERATIVE AMPLIFIERS:1||RAREGASES:1||THz radiation:1||FREEELECTRON LASER:1||REALTIME OBSERVATION:1||TARGET:1||photoionized plasmas:1||fs Xray laser:1||emission profile:1||HIGHORDER HARMONICS:1||Xray laser:1||atomic transition:1||EXCITATION:1||LASERS:1||PERFORMANCE:1||RELATIVISTIC ELECTRONS:1||BI2O3DOPED ZNO:1||INNERSHELL IONIZATION:1||Laser wakefield:1||FREQUENCY:1||SOLIDSTATE LASERS:1||Linearly polarized:1||THERMIONIC EMISSION:1||PULSE AMPLIFICATION SYSTEM:1||BIB3O6:1||NM:1||NONCOVALENT INTERACTIONS:1||CRYSTALLINE:1||INTENSITY:1||JETS:1||COHERENT:1||LINE:1||ANGULARDISTRIBUTION:1||SILVER IONS:1||magnetic anisotropy:1||DEVICES:1||Auger transitions:1||CosterKronig transitions:1||EFFICIENT:1||ELECTRONIMPACT IONIZATION:1||ULTRASHORTPULSE:1||Nanowire:1||Heterostructure:1||soft Xray reflectivity:1||PLASMA ACCELERATOR:1||ZINCOXIDE NANOWIRES:1||CHEMICALVAPORDEPOSITION:1||Electron acceleration:1||Ionization of gases:1||Delay dependent:1||MULTIPHOTON IONIZATION:1||FRAGMENTATION:1||GASJET:1||ultrafast nonlinear optics:1||CYCLE PULSES:1||KHZ:1||chemical vapor deposition:1||ferromagnetism:1||ABSORPTION:1||TERAHERTZ RADIATION:1||SCIENCE:1||FIELDS:1||ELECTRONS:1||nanomultilayer structures:1||YIELDS:1||AUGER:1||10HZ REPETITION RATE:1||MULTITERAWATT:1||SPECTROGRAPH:1||HIGHHARMONICGENERATION:1||spectroscopy:1||level population:1||PARTICLEACCELERATION:1||OPTICAL FREQUENCYMEASUREMENT:1||NANOWALLS:1||ROOMTEMPERATURE:1||AVERAGE OUTPUT POWER:1||GROUPVELOCITYMISMATCH:1||Impact ionization:1||Dynamics:1||Lasers:1||Collisional process:1||ABOVETHRESHOLD IONIZATION:1||MAINGROUP THERMOCHEMISTRY:1||dilute magnetic semiconductors:1||GACRN:1||SIZE:1||ATTOSECOND:1||Ar cluster:1||Xray astrophysics:1||photoionization:1||irons:1||normal incidence pulsed laser deposition:1||SHELLS:1||Silicon Oxide:1||gaspuff Zpinch:1||Xray:1||soft Xray reflectors:1||ESCAPE:1||ZN2SIO4:1||SILICA:1||Time 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materials:1||MOLECULAR PHOTOIONIZATION:1||LOCALIZATION:1||DEUTERIUM CLUSTERS:1||EXPLOSIONS:1||REGENERATIVE AMPLIFIERS:1||RAREGASES:1||THz radiation:1||FREEELECTRON LASER:1||REALTIME OBSERVATION:1||TARGET:1||photoionized plasmas:1||fs Xray laser:1||emission profile:1||HIGHORDER HARMONICS:1||Xray laser:1||atomic transition:1||EXCITATION:1||LASERS:1||PERFORMANCE:1||RELATIVISTIC ELECTRONS:1||BI2O3DOPED ZNO:1||INNERSHELL IONIZATION:1||Laser wakefield:1||FREQUENCY:1||SOLIDSTATE LASERS:1||Linearly polarized:1||THERMIONIC EMISSION:1||PULSE AMPLIFICATION SYSTEM:1||BIB3O6:1||NM:1||NONCOVALENT INTERACTIONS:1||CRYSTALLINE:1||INTENSITY:1||JETS:1||COHERENT:1||LINE:1||ANGULARDISTRIBUTION:1||SILVER IONS:1||magnetic anisotropy:1||DEVICES:1||Auger transitions:1||CosterKronig transitions:1||EFFICIENT:1||ELECTRONIMPACT IONIZATION:1||ULTRASHORTPULSE:1||Nanowire:1||Heterostructure:1||soft Xray reflectivity:1||PLASMA ACCELERATOR:1||ZINCOXIDE NANOWIRES:1||CHEMICALVAPORDEPOSITION:1||Electron acceleration:1||Ionization of gases:1||Delay dependent:1||MULTIPHOTON IONIZATION:1||FRAGMENTATION:1||GASJET:1||ultrafast nonlinear optics:1||CYCLE PULSES:1||KHZ:1||chemical vapor deposition:1||ferromagnetism:1||ABSORPTION:1||TERAHERTZ RADIATION:1||SCIENCE:1||FIELDS:1||ELECTRONS:1||nanomultilayer structures:1||YIELDS:1||AUGER:1||10HZ REPETITION RATE:1||MULTITERAWATT:1||SPECTROGRAPH:1||HIGHHARMONICGENERATION:1||spectroscopy:1||level population:1||PARTICLEACCELERATION:1||OPTICAL FREQUENCYMEASUREMENT:1||NANOWALLS:1||ROOMTEMPERATURE:1||AVERAGE OUTPUT POWER:1||GROUPVELOCITYMISMATCH:1||Impact ionization:1||Dynamics:1||Lasers:1||Collisional process:1||ABOVETHRESHOLD IONIZATION:1||MAINGROUP THERMOCHEMISTRY:1||dilute magnetic semiconductors:1||GACRN:1||SIZE:1||ATTOSECOND:1||Ar cluster:1||Xray astrophysics:1||photoionization:1||irons:1||normal incidence pulsed laser deposition:1||SHELLS:1||Silicon Oxide:1||gaspuff Zpinch:1||Xray:1||soft Xray reflectors:1||ESCAPE:1||ZN2SIO4:1||SILICA:1||Time delay:1||Collisional plasmas:1||MASSSPECTROMETRY:1||NUCLEARFUSION:1||PARAMETRIC AMPLIFICATION:1||LYING ELECTRONIC STATES:1||ADJUSTABLEPARAMETERS:1||MAGNETICPROPERTIES:1||LIQUIDPHASE EPITAXY:1||CEP laser:1||REGION:1||Plasma waveguide:1||AMBIENT GAS:1||DEPOSITION:1||HARMONICGENERATION:1||ENHANCEMENT:1||imaging spectrometer:1||Abel inversion:1||Water window:1||Liquid nitrogen jet:1||CHARGEEXCHANGE:1||NOBEL LECTURE:1||VARISTOR:1||EPITAXY:1||THINDISK LASER:1||HIGHREPETITIONRATE:1||Atom lasers:1||Electronimpact excitation:1||High order harmonics:1||ultrafast technology:1||PEAK POWER:1||CHARGED ALUMINUM CLUSTERS:1||GaN:1||THIN:1||Electron beam:1||INTENSE:1||Hard Xray pulse generation:1||NONLINEAR THOMSON SCATTERING:1||MULTILAYER:1||UVvisible spectrometer:1||ATOMS:1||innershell transitions:1||CORRECTED CONCAVE GRATINGS:1||DISCHARGE:1||LASERPLASMA:1||thin film:1||reflectivity:1||opacity:1||gain:1||smallangle Xray scattering:1||SOFTXRAY:1||ZINCOXIDE:1||CYGNUSX3:1||Betatron oscillation:1||ACCELERATOR:1||STRAINEDLAYER SUPERLATTICES:1||OPTICAL PARAMETRIC AMPLIFICATION:1||PASSIVE MODELOCKING:1||Collision dynamics:1||MUM:1||EXACTEXCHANGE:1||BASISSET:1||APPROXIMATION:1||OXYNITRIDES:1||Beam energy modulation:1||polarization spectroscopy:1||REORIENTATION TRANSITION:1||DEPENDENCE:1||sulfurs:1||BUILDINGBLOCKS:1||RATES:1||OPTICAL PULSES:1||toroidal mirror:1||XRAY LASER:1||CALCIUM:1||radially polarized laser:1||GRAINBOUNDARIES:1||VAPORDEPOSITION:1||Xray generation:1||MAGNETIZATION:1||Electric excitation:1||Laserinduced gas plasmas:1||Qualitative analysis:1||SCHEME:1||RADIATION:10||PULSES:8||PHOTOLUMINESCENCE:7||LASER:7||GENERATION:6||NANORODS:6||GROWTH:6||NANOWIRES:5||IMPLANTED GAN:5||SPECTROSCOPY:5||THINFILMS:4||DYNAMICS:4||SILICON:4||EXTREMEULTRAVIOLET:4||AMPLIFICATION:4||PRESSURE:4||PHASE:4||OPTICALPROPERTIES:4||SYSTEM:4||EMISSION:4||FEL:3||N2O:3||FILMS:3||OPTICS:3||SPECTRA:3||FIELD:3||MIRRORS:3||ARRAYS:3||CLUSTERS:3||SIO2:3||IONIZATION:3||VACUUM:3||SCATTERING:3||IONS:2||LUMINESCENCE PROPERTIES:2||ANISOTROPY:2||BEAMS:2||DIFFRACTION:2||DISPERSION:2||chemical vapor deposition (CVD):2||ELECTRONICSTRUCTURE:2||MOSFETS:2||SI3N4:2||DENSITY:2||LIGHT:2||PLASMAS:2||MATTER:2||nanocomposites:2||RAMANSCATTERING:2||NANOPARTICLES:2||OXIDE:2||AMPLIFIED SPONTANEOUS EMISSION:2||NM WAVELENGTH:2||GAIN:2||CARBON NANOTUBES:2||CROSSSECTIONS:2||LIGHTEMITTINGDIODES:2||PULSE:2||CARBON PLASMA:2||TISAPPHIRE LASER:2||Raman scattering:2||ROUTE:2||multilayer:2||CATHODOLUMINESCENCE:2||highresolution transmission electronic microscope (HRTEM):2||DIFFERENCEFREQUENCYGENERATION:2||CRYSTAL:2||laserproduced plasma:2||NANOCABLES:2||photoluminescence:2||MAGNETIC ALLOY SEMICONDUCTORS:2||MOLECULARBEAM EPITAXY:2||EARTHDOPED GAN:2||LASER FIELDS:2||CHIRPEDPULSEAMPLIFICATION:2||ALN:2||GAUSSIANBEAM:2||ASSISTED CATALYTIC GROWTH:2||BLUE:2||NANOSTRUCTURES:2||MAGNETOELECTRONICS:2||MICROSCOPY:2||ELECTROLUMINESCENCE:2||LASERPULSES:2||GaN nanowires:2||GALLIUM NITRIDE NANOWIRES:2||GAMNN:2||NANOTUBES:2||PHYSICS:2||Femtosecond laser:2||parametric oscillators and amplifiers:1||ultrafast lasers:1||VALENCE:1||nanowires:1||DILUTED MAGNETIC SEMICONDUCTOR:1||LUMINESCENCE:1||Density modulation:1||Energy modulation:1||Current enhanced SASE free electron laser:1||Undulator radiation:1||FREEELECTRON LASERS:1||ULTRATHIN FERROMAGNETICFILMS:1||OXIDEFILMS:1||ABLATION:1||COMPONENT:1||METAL:1||innershell excited states:1||Nelike ions:1||TRANSITIONS:1||XUV spectrometer:1||DIAGNOSTICS:1||Xray scattering:1||MO/SI:1||pulsed laser deposition:1||KEV IMPACT ENERGIES:1||vacuum electron acceleration:1||HIGHINTENSITY LASER:1||JUNCTIONS:1||LOWTEMPERATURE GROWTH:1||nanocrystalline materials:1||MOLECULAR PHOTOIONIZATION:1||LOCALIZATION:1||DEUTERIUM CLUSTERS:1||EXPLOSIONS:1||REGENERATIVE AMPLIFIERS:1||RAREGASES:1||THz radiation:1||FREEELECTRON LASER:1||REALTIME OBSERVATION:1||TARGET:1||photoionized plasmas:1||fs Xray laser:1||emission profile:1||HIGHORDER HARMONICS:1||Xray laser:1||atomic transition:1||EXCITATION:1||LASERS:1||PERFORMANCE:1||RELATIVISTIC ELECTRONS:1||BI2O3DOPED ZNO:1||INNERSHELL IONIZATION:1||Laser wakefield:1||FREQUENCY:1||SOLIDSTATE LASERS:1||Linearly polarized:1||THERMIONIC EMISSION:1||PULSE AMPLIFICATION SYSTEM:1||BIB3O6:1||NM:1||NONCOVALENT INTERACTIONS:1||CRYSTALLINE:1||INTENSITY:1||JETS:1||COHERENT:1||LINE:1||ANGULARDISTRIBUTION:1||SILVER IONS:1||magnetic anisotropy:1||DEVICES:1||Auger transitions:1||CosterKronig transitions:1||EFFICIENT:1||ELECTRONIMPACT IONIZATION:1||ULTRASHORTPULSE:1||Nanowire:1||Heterostructure:1||soft Xray reflectivity:1||PLASMA ACCELERATOR:1||ZINCOXIDE NANOWIRES:1||CHEMICALVAPORDEPOSITION:1||Electron acceleration:1||Ionization of gases:1||Delay dependent:1||MULTIPHOTON IONIZATION:1||FRAGMENTATION:1||GASJET:1||ultrafast nonlinear optics:1||CYCLE PULSES:1||KHZ:1||chemical vapor deposition:1||ferromagnetism:1||ABSORPTION:1||TERAHERTZ RADIATION:1||SCIENCE:1||FIELDS:1||ELECTRONS:1||nanomultilayer structures:1||YIELDS:1||AUGER:1||10HZ REPETITION RATE:1||MULTITERAWATT:1||SPECTROGRAPH:1||HIGHHARMONICGENERATION:1||spectroscopy:1||level population:1||PARTICLEACCELERATION:1||OPTICAL FREQUENCYMEASUREMENT:1||NANOWALLS:1||ROOMTEMPERATURE:1||AVERAGE OUTPUT POWER:1||GROUPVELOCITYMISMATCH:1||Impact ionization:1||Dynamics:1||Lasers:1||Collisional process:1||ABOVETHRESHOLD IONIZATION:1||MAINGROUP THERMOCHEMISTRY:1||dilute magnetic semiconductors:1||GACRN:1||SIZE:1||ATTOSECOND:1||Ar cluster:1||Xray astrophysics:1||photoionization:1||irons:1||normal incidence pulsed laser deposition:1||SHELLS:1||Silicon Oxide:1||gaspuff Zpinch:1||Xray:1||soft Xray reflectors:1||ESCAPE:1||ZN2SIO4:1||SILICA:1||Time delay:1||Collisional plasmas:1||MASSSPECTROMETRY:1||NUCLEARFUSION:1||PARAMETRIC AMPLIFICATION:1||LYING ELECTRONIC STATES:1||ADJUSTABLEPARAMETERS:1||MAGNETICPROPERTIES:1||LIQUIDPHASE EPITAXY:1||CEP laser:1||REGION:1||Plasma waveguide:1||AMBIENT GAS:1||DEPOSITION:1||HARMONICGENERATION:1||ENHANCEMENT:1||imaging spectrometer:1||Abel inversion:1||Water window:1||Liquid nitrogen jet:1||CHARGEEXCHANGE:1||NOBEL LECTURE:1||VARISTOR:1||EPITAXY:1||THINDISK LASER:1||HIGHREPETITIONRATE:1||Atom lasers:1||Electronimpact excitation:1||High order harmonics:1||ultrafast technology:1||PEAK POWER:1||CHARGED ALUMINUM CLUSTERS:1||GaN:1||THIN:1||Electron beam:1||INTENSE:1||Hard Xray pulse generation:1||NONLINEAR THOMSON SCATTERING:1||MULTILAYER:1||UVvisible spectrometer:1||ATOMS:1||innershell transitions:1||CORRECTED CONCAVE GRATINGS:1||DISCHARGE:1||LASERPLASMA:1||thin film:1||reflectivity:1||opacity:1||gain:1||smallangle Xray scattering:1||SOFTXRAY:1||ZINCOXIDE:1||CYGNUSX3:1||Betatron oscillation:1||ACCELERATOR:1||STRAINEDLAYER SUPERLATTICES:1||OPTICAL PARAMETRIC AMPLIFICATION:1||PASSIVE MODELOCKING:1||Collision dynamics:1||MUM:1||EXACTEXCHANGE:1||BASISSET:1||APPROXIMATION:1||OXYNITRIDES:1||Beam energy modulation:1||polarization spectroscopy:1||REORIENTATION TRANSITION:1||DEPENDENCE:1||sulfurs:1||BUILDINGBLOCKS:1||RATES:1||OPTICAL PULSES:1||toroidal mirror:1||XRAY LASER:1||CALCIUM:1||radially polarized laser:1||GRAINBOUNDARIES:1||VAPORDEPOSITION:1||Xray generation:1||MAGNETIZATION:1||Electric excitation:1||Laserinduced gas plasmas:1||Qualitative analysis:1||SCHEME:1||RADIATION:10||PULSES:8||PHOTOLUMINESCENCE:7||LASER:7||GENERATION:6||NANORODS:6||GROWTH:6||NANOWIRES:5||IMPLANTED 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SEMICONDUCTORS:2||MOLECULARBEAM EPITAXY:2||EARTHDOPED GAN:2||LASER FIELDS:2||CHIRPEDPULSEAMPLIFICATION:2||ALN:2||GAUSSIANBEAM:2||ASSISTED CATALYTIC GROWTH:2||BLUE:2||NANOSTRUCTURES:2||MAGNETOELECTRONICS:2||MICROSCOPY:2||ELECTROLUMINESCENCE:2||LASERPULSES:2||GaN nanowires:2||GALLIUM NITRIDE NANOWIRES:2||GAMNN:2||NANOTUBES:2||PHYSICS:2||Femtosecond laser:2||parametric oscillators and amplifiers:1||ultrafast lasers:1||VALENCE:1||nanowires:1||DILUTED MAGNETIC SEMICONDUCTOR:1||LUMINESCENCE:1||Density modulation:1||Energy modulation:1||Current enhanced SASE free electron laser:1||Undulator radiation:1||FREEELECTRON LASERS:1||ULTRATHIN FERROMAGNETICFILMS:1||OXIDEFILMS:1||ABLATION:1||COMPONENT:1||METAL:1||innershell excited states:1||Nelike ions:1||TRANSITIONS:1||XUV spectrometer:1||DIAGNOSTICS:1||Xray scattering:1||MO/SI:1||pulsed laser deposition:1||KEV IMPACT ENERGIES:1||vacuum electron acceleration:1||HIGHINTENSITY LASER:1||JUNCTIONS:1||LOWTEMPERATURE GROWTH:1||nanocrystalline materials:1||MOLECULAR PHOTOIONIZATION:1||LOCALIZATION:1||DEUTERIUM CLUSTERS:1||EXPLOSIONS:1||REGENERATIVE AMPLIFIERS:1||RAREGASES:1||THz radiation:1||FREEELECTRON LASER:1||REALTIME OBSERVATION:1||TARGET:1||photoionized plasmas:1||fs Xray laser:1||emission profile:1||HIGHORDER HARMONICS:1||Xray laser:1||atomic transition:1||EXCITATION:1||LASERS:1||PERFORMANCE:1||RELATIVISTIC ELECTRONS:1||BI2O3DOPED ZNO:1||INNERSHELL IONIZATION:1||Laser wakefield:1||FREQUENCY:1||SOLIDSTATE LASERS:1||Linearly polarized:1||THERMIONIC EMISSION:1||PULSE AMPLIFICATION SYSTEM:1||BIB3O6:1||NM:1||NONCOVALENT INTERACTIONS:1||CRYSTALLINE:1||INTENSITY:1||JETS:1||COHERENT:1||LINE:1||ANGULARDISTRIBUTION:1||SILVER IONS:1||magnetic anisotropy:1||DEVICES:1||Auger transitions:1||CosterKronig transitions:1||EFFICIENT:1||ELECTRONIMPACT IONIZATION:1||ULTRASHORTPULSE:1||Nanowire:1||Heterostructure:1||soft Xray reflectivity:1||PLASMA ACCELERATOR:1||ZINCOXIDE NANOWIRES:1||CHEMICALVAPORDEPOSITION:1||Electron acceleration:1||Ionization of gases:1||Delay dependent:1||MULTIPHOTON IONIZATION:1||FRAGMENTATION:1||GASJET:1||ultrafast nonlinear optics:1||CYCLE PULSES:1||KHZ:1||chemical vapor deposition:1||ferromagnetism:1||ABSORPTION:1||TERAHERTZ RADIATION:1||SCIENCE:1||FIELDS:1||ELECTRONS:1||nanomultilayer structures:1||YIELDS:1||AUGER:1||10HZ REPETITION RATE:1||MULTITERAWATT:1||SPECTROGRAPH:1||HIGHHARMONICGENERATION:1||spectroscopy:1||level population:1||PARTICLEACCELERATION:1||OPTICAL FREQUENCYMEASUREMENT:1||NANOWALLS:1||ROOMTEMPERATURE:1||AVERAGE OUTPUT POWER:1||GROUPVELOCITYMISMATCH:1||Impact ionization:1||Dynamics:1||Lasers:1||Collisional process:1||ABOVETHRESHOLD IONIZATION:1||MAINGROUP THERMOCHEMISTRY:1||dilute magnetic semiconductors:1||GACRN:1||SIZE:1||ATTOSECOND:1||Ar cluster:1||Xray astrophysics:1||photoionization:1||irons:1||normal incidence pulsed laser deposition:1||SHELLS:1||Silicon Oxide:1||gaspuff Zpinch:1||Xray:1||soft Xray reflectors:1||ESCAPE:1||ZN2SIO4:1||SILICA:1||Time 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materials:1||MOLECULAR PHOTOIONIZATION:1||LOCALIZATION:1||DEUTERIUM CLUSTERS:1||EXPLOSIONS:1||REGENERATIVE AMPLIFIERS:1||RAREGASES:1||THz radiation:1||FREEELECTRON LASER:1||REALTIME OBSERVATION:1||TARGET:1||photoionized plasmas:1||fs Xray laser:1||emission profile:1||HIGHORDER HARMONICS:1||Xray laser:1||atomic transition:1||EXCITATION:1||LASERS:1||PERFORMANCE:1||RELATIVISTIC ELECTRONS:1||BI2O3DOPED ZNO:1||INNERSHELL IONIZATION:1||Laser wakefield:1||FREQUENCY:1||SOLIDSTATE LASERS:1||Linearly polarized:1||THERMIONIC EMISSION:1||PULSE AMPLIFICATION SYSTEM:1||BIB3O6:1||NM:1||NONCOVALENT INTERACTIONS:1||CRYSTALLINE:1||INTENSITY:1||JETS:1||COHERENT:1||LINE:1||ANGULARDISTRIBUTION:1||SILVER IONS:1||magnetic anisotropy:1||DEVICES:1||Auger transitions:1||CosterKronig transitions:1||EFFICIENT:1||ELECTRONIMPACT IONIZATION:1||ULTRASHORTPULSE:1||Nanowire:1||Heterostructure:1||soft Xray reflectivity:1||PLASMA ACCELERATOR:1||ZINCOXIDE NANOWIRES:1||CHEMICALVAPORDEPOSITION:1||Electron acceleration:1||Ionization of gases:1||Delay dependent:1||MULTIPHOTON IONIZATION:1||FRAGMENTATION:1||GASJET:1||ultrafast nonlinear optics:1||CYCLE PULSES:1||KHZ:1||chemical vapor deposition:1||ferromagnetism:1||ABSORPTION:1||TERAHERTZ RADIATION:1||SCIENCE:1||FIELDS:1||ELECTRONS:1||nanomultilayer structures:1||YIELDS:1||AUGER:1||10HZ REPETITION RATE:1||MULTITERAWATT:1||SPECTROGRAPH:1||HIGHHARMONICGENERATION:1||spectroscopy:1||level population:1||PARTICLEACCELERATION:1||OPTICAL FREQUENCYMEASUREMENT:1||NANOWALLS:1||ROOMTEMPERATURE:1||AVERAGE OUTPUT POWER:1||GROUPVELOCITYMISMATCH:1||Impact ionization:1||Dynamics:1||Lasers:1||Collisional process:1||ABOVETHRESHOLD IONIZATION:1||MAINGROUP THERMOCHEMISTRY:1||dilute magnetic semiconductors:1||GACRN:1||SIZE:1||ATTOSECOND:1||Ar cluster:1||Xray astrophysics:1||photoionization:1||irons:1||normal incidence pulsed laser deposition:1||SHELLS:1||Silicon Oxide:1||gaspuff Zpinch:1||Xray:1||soft Xray reflectors:1||ESCAPE:1||ZN2SIO4:1||SILICA:1||Time delay:1||Collisional plasmas:1||MASSSPECTROMETRY:1||NUCLEARFUSION:1||PARAMETRIC AMPLIFICATION:1||LYING ELECTRONIC STATES:1||ADJUSTABLEPARAMETERS:1||MAGNETICPROPERTIES:1||LIQUIDPHASE EPITAXY:1||CEP laser:1||REGION:1||Plasma waveguide:1||AMBIENT GAS:1||DEPOSITION:1||HARMONICGENERATION:1||ENHANCEMENT:1||imaging spectrometer:1||Abel inversion:1||Water window:1||Liquid nitrogen jet:1||CHARGEEXCHANGE:1||NOBEL LECTURE:1||VARISTOR:1||EPITAXY:1||THINDISK LASER:1||HIGHREPETITIONRATE:1||Atom lasers:1||Electronimpact excitation:1||High order harmonics:1||ultrafast technology:1||PEAK POWER:1||CHARGED ALUMINUM CLUSTERS:1||GaN:1||THIN:1||Electron beam:1||INTENSE:1||Hard Xray pulse generation:1||NONLINEAR THOMSON SCATTERING:1||MULTILAYER:1||UVvisible spectrometer:1||ATOMS:1||innershell transitions:1||CORRECTED CONCAVE GRATINGS:1||DISCHARGE:1||LASERPLASMA:1||thin film:1||reflectivity:1||opacity:1||gain:1||smallangle Xray scattering:1||SOFTXRAY:1||ZINCOXIDE:1||CYGNUSX3:1||Betatron oscillation:1||ACCELERATOR:1||STRAINEDLAYER SUPERLATTICES:1||OPTICAL PARAMETRIC AMPLIFICATION:1||PASSIVE MODELOCKING:1||Collision dynamics:1||MUM:1||EXACTEXCHANGE:1||BASISSET:1||APPROXIMATION:1||OXYNITRIDES:1||Beam energy modulation:1||polarization spectroscopy:1||REORIENTATION TRANSITION:1||DEPENDENCE:1||sulfurs:1||BUILDINGBLOCKS:1||RATES:1||OPTICAL PULSES:1||toroidal mirror:1||XRAY LASER:1||CALCIUM:1||radially polarized laser:1||GRAINBOUNDARIES:1||VAPORDEPOSITION:1||Xray generation:1||MAGNETIZATION:1||Electric excitation:1||Laserinduced gas plasmas:1||Qualitative analysis:1||SCHEME:1||RADIATION:10||PULSES:8||PHOTOLUMINESCENCE:7||LASER:7||GENERATION:6||NANORODS:6||GROWTH:6||NANOWIRES:5||IMPLANTED GAN:5||SPECTROSCOPY:5||THINFILMS:4||DYNAMICS:4||SILICON:4||EXTREMEULTRAVIOLET:4||AMPLIFICATION:4||PRESSURE:4||PHASE:4||OPTICALPROPERTIES:4||SYSTEM:4||EMISSION:4||FEL:3||N2O:3||FILMS:3||OPTICS:3||SPECTRA:3||FIELD:3||MIRRORS:3||ARRAYS:3||CLUSTERS:3||SIO2:3||IONIZATION:3||VACUUM:3||SCATTERING:3||IONS:2||LUMINESCENCE PROPERTIES:2||ANISOTROPY:2||BEAMS:2||DIFFRACTION:2||DISPERSION:2||chemical vapor deposition (CVD):2||ELECTRONICSTRUCTURE:2||MOSFETS:2||SI3N4:2||DENSITY:2||LIGHT:2||PLASMAS:2||MATTER:2||nanocomposites:2||RAMANSCATTERING:2||NANOPARTICLES:2||OXIDE:2||AMPLIFIED SPONTANEOUS EMISSION:2||NM WAVELENGTH:2||GAIN:2||CARBON NANOTUBES:2||CROSSSECTIONS:2||LIGHTEMITTINGDIODES:2||PULSE:2||CARBON PLASMA:2||TISAPPHIRE LASER:2||Raman scattering:2||ROUTE:2||multilayer:2||CATHODOLUMINESCENCE:2||highresolution transmission electronic microscope (HRTEM):2||DIFFERENCEFREQUENCYGENERATION:2||CRYSTAL:2||laserproduced plasma:2||NANOCABLES:2||photoluminescence:2||MAGNETIC ALLOY SEMICONDUCTORS:2||MOLECULARBEAM EPITAXY:2||EARTHDOPED GAN:2||LASER FIELDS:2||CHIRPEDPULSEAMPLIFICATION:2||ALN:2||GAUSSIANBEAM:2||ASSISTED CATALYTIC GROWTH:2||BLUE:2||NANOSTRUCTURES:2||MAGNETOELECTRONICS:2||MICROSCOPY:2||ELECTROLUMINESCENCE:2||LASERPULSES:2||GaN nanowires:2||GALLIUM NITRIDE NANOWIRES:2||GAMNN:2||NANOTUBES:2||PHYSICS:2||Femtosecond laser:2||parametric oscillators and amplifiers:1||ultrafast lasers:1||VALENCE:1||nanowires:1||DILUTED MAGNETIC SEMICONDUCTOR:1||LUMINESCENCE:1||Density modulation:1||Energy modulation:1||Current enhanced SASE free electron laser:1||Undulator radiation:1||FREEELECTRON LASERS:1||ULTRATHIN FERROMAGNETICFILMS:1||OXIDEFILMS:1||ABLATION:1||COMPONENT:1||METAL:1||innershell excited states:1||Nelike ions:1||TRANSITIONS:1||XUV spectrometer:1||DIAGNOSTICS:1||Xray scattering:1||MO/SI:1||pulsed laser deposition:1||KEV IMPACT ENERGIES:1||vacuum electron acceleration:1||HIGHINTENSITY LASER:1||JUNCTIONS:1||LOWTEMPERATURE GROWTH:1||nanocrystalline materials:1||MOLECULAR PHOTOIONIZATION:1||LOCALIZATION:1||DEUTERIUM CLUSTERS:1||EXPLOSIONS:1||REGENERATIVE AMPLIFIERS:1||RAREGASES:1||THz radiation:1||FREEELECTRON LASER:1||REALTIME OBSERVATION:1||TARGET:1||photoionized plasmas:1||fs Xray laser:1||emission profile:1||HIGHORDER HARMONICS:1||Xray laser:1||atomic transition:1||EXCITATION:1||LASERS:1||PERFORMANCE:1||RELATIVISTIC ELECTRONS:1||BI2O3DOPED ZNO:1||INNERSHELL IONIZATION:1||Laser wakefield:1||FREQUENCY:1||SOLIDSTATE LASERS:1||Linearly polarized:1||THERMIONIC EMISSION:1||PULSE AMPLIFICATION SYSTEM:1||BIB3O6:1||NM:1||NONCOVALENT INTERACTIONS:1||CRYSTALLINE:1||INTENSITY:1||JETS:1||COHERENT:1||LINE:1||ANGULARDISTRIBUTION:1||SILVER IONS:1||magnetic anisotropy:1||DEVICES:1||Auger transitions:1||CosterKronig transitions:1||EFFICIENT:1||ELECTRONIMPACT IONIZATION:1||ULTRASHORTPULSE:1||Nanowire:1||Heterostructure:1||soft Xray reflectivity:1||PLASMA ACCELERATOR:1||ZINCOXIDE NANOWIRES:1||CHEMICALVAPORDEPOSITION:1||Electron acceleration:1||Ionization of gases:1||Delay dependent:1||MULTIPHOTON IONIZATION:1||FRAGMENTATION:1||GASJET:1||ultrafast nonlinear optics:1||CYCLE PULSES:1||KHZ:1||chemical vapor deposition:1||ferromagnetism:1||ABSORPTION:1||TERAHERTZ RADIATION:1||SCIENCE:1||FIELDS:1||ELECTRONS:1||nanomultilayer structures:1||YIELDS:1||AUGER:1||10HZ REPETITION RATE:1||MULTITERAWATT:1||SPECTROGRAPH:1||HIGHHARMONICGENERATION:1||spectroscopy:1||level population:1||PARTICLEACCELERATION:1||OPTICAL FREQUENCYMEASUREMENT:1||NANOWALLS:1||ROOMTEMPERATURE:1||AVERAGE OUTPUT POWER:1||GROUPVELOCITYMISMATCH:1||Impact ionization:1||Dynamics:1||Lasers:1||Collisional process:1||ABOVETHRESHOLD IONIZATION:1||MAINGROUP THERMOCHEMISTRY:1||dilute magnetic semiconductors:1||GACRN:1||SIZE:1||ATTOSECOND:1||Ar cluster:1||Xray astrophysics:1||photoionization:1||irons:1||normal incidence pulsed laser deposition:1||SHELLS:1||Silicon Oxide:1||gaspuff Zpinch:1||Xray:1||soft Xray reflectors:1||ESCAPE:1||ZN2SIO4:1||SILICA:1||Time delay:1||Collisional plasmas:1||MASSSPECTROMETRY:1||NUCLEARFUSION:1||PARAMETRIC AMPLIFICATION:1||LYING ELECTRONIC STATES:1||ADJUSTABLEPARAMETERS:1||MAGNETICPROPERTIES:1||LIQUIDPHASE EPITAXY:1||CEP laser:1||REGION:1||Plasma waveguide:1||AMBIENT GAS:1||DEPOSITION:1||HARMONICGENERATION:1||ENHANCEMENT:1||imaging spectrometer:1||Abel inversion:1||Water window:1||Liquid nitrogen jet:1||CHARGEEXCHANGE:1||NOBEL LECTURE:1||VARISTOR:1||EPITAXY:1||THINDISK LASER:1||HIGHREPETITIONRATE:1||Atom lasers:1||Electronimpact excitation:1||High order harmonics:1||ultrafast technology:1||PEAK POWER:1||CHARGED ALUMINUM CLUSTERS:1||GaN:1||THIN:1||Electron beam:1||INTENSE:1||Hard Xray pulse generation:1||NONLINEAR THOMSON SCATTERING:1||MULTILAYER:1||UVvisible spectrometer:1||ATOMS:1||innershell transitions:1||CORRECTED CONCAVE GRATINGS:1||DISCHARGE:1||LASERPLASMA:1||thin film:1||reflectivity:1||opacity:1||gain:1||smallangle Xray scattering:1||SOFTXRAY:1||ZINCOXIDE:1||CYGNUSX3:1||Betatron oscillation:1||ACCELERATOR:1||STRAINEDLAYER SUPERLATTICES:1||OPTICAL PARAMETRIC AMPLIFICATION:1||PASSIVE MODELOCKING:1||Collision dynamics:1||MUM:1||EXACTEXCHANGE:1||BASISSET:1||APPROXIMATION:1||OXYNITRIDES:1||Beam energy modulation:1||polarization spectroscopy:1||REORIENTATION TRANSITION:1||DEPENDENCE:1||sulfurs:1||BUILDINGBLOCKS:1||RATES:1||OPTICAL PULSES:1||toroidal mirror:1||XRAY LASER:1||CALCIUM:1||radially polarized laser:1||GRAINBOUNDARIES:1||VAPORDEPOSITION:1||Xray generation:1||MAGNETIZATION:1||Electric excitation:1||Laserinduced gas plasmas:1||Qualitative analysis:1||SCHEME:1||RADIATION:10||PULSES:8||PHOTOLUMINESCENCE:7||LASER:7||GENERATION:6||NANORODS:6||GROWTH:6||NANOWIRES:5||IMPLANTED 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SEMICONDUCTORS:2||MOLECULARBEAM EPITAXY:2||EARTHDOPED GAN:2||LASER FIELDS:2||CHIRPEDPULSEAMPLIFICATION:2||ALN:2||GAUSSIANBEAM:2||ASSISTED CATALYTIC GROWTH:2||BLUE:2||NANOSTRUCTURES:2||MAGNETOELECTRONICS:2||MICROSCOPY:2||ELECTROLUMINESCENCE:2||LASERPULSES:2||GaN nanowires:2||GALLIUM NITRIDE NANOWIRES:2||GAMNN:2||NANOTUBES:2||PHYSICS:2||Femtosecond laser:2||parametric oscillators and amplifiers:1||ultrafast lasers:1||VALENCE:1||nanowires:1||DILUTED MAGNETIC SEMICONDUCTOR:1||LUMINESCENCE:1||Density modulation:1||Energy modulation:1||Current enhanced SASE free electron laser:1||Undulator radiation:1||FREEELECTRON LASERS:1||ULTRATHIN FERROMAGNETICFILMS:1||OXIDEFILMS:1||ABLATION:1||COMPONENT:1||METAL:1||innershell excited states:1||Nelike ions:1||TRANSITIONS:1||XUV spectrometer:1||DIAGNOSTICS:1||Xray scattering:1||MO/SI:1||pulsed laser deposition:1||KEV IMPACT ENERGIES:1||vacuum electron acceleration:1||HIGHINTENSITY LASER:1||JUNCTIONS:1||LOWTEMPERATURE GROWTH:1||nanocrystalline materials:1||MOLECULAR PHOTOIONIZATION:1||LOCALIZATION:1||DEUTERIUM CLUSTERS:1||EXPLOSIONS:1||REGENERATIVE AMPLIFIERS:1||RAREGASES:1||THz radiation:1||FREEELECTRON LASER:1||REALTIME OBSERVATION:1||TARGET:1||photoionized plasmas:1||fs Xray laser:1||emission profile:1||HIGHORDER HARMONICS:1||Xray laser:1||atomic transition:1||EXCITATION:1||LASERS:1||PERFORMANCE:1||RELATIVISTIC ELECTRONS:1||BI2O3DOPED ZNO:1||INNERSHELL IONIZATION:1||Laser wakefield:1||FREQUENCY:1||SOLIDSTATE LASERS:1||Linearly polarized:1||THERMIONIC EMISSION:1||PULSE AMPLIFICATION SYSTEM:1||BIB3O6:1||NM:1||NONCOVALENT INTERACTIONS:1||CRYSTALLINE:1||INTENSITY:1||JETS:1||COHERENT:1||LINE:1||ANGULARDISTRIBUTION:1||SILVER IONS:1||magnetic anisotropy:1||DEVICES:1||Auger transitions:1||CosterKronig transitions:1||EFFICIENT:1||ELECTRONIMPACT IONIZATION:1||ULTRASHORTPULSE:1||Nanowire:1||Heterostructure:1||soft Xray reflectivity:1||PLASMA ACCELERATOR:1||ZINCOXIDE NANOWIRES:1||CHEMICALVAPORDEPOSITION:1||Electron acceleration:1||Ionization of gases:1||Delay dependent:1||MULTIPHOTON IONIZATION:1||FRAGMENTATION:1||GASJET:1||ultrafast nonlinear optics:1||CYCLE PULSES:1||KHZ:1||chemical vapor deposition:1||ferromagnetism:1||ABSORPTION:1||TERAHERTZ RADIATION:1||SCIENCE:1||FIELDS:1||ELECTRONS:1||nanomultilayer structures:1||YIELDS:1||AUGER:1||10HZ REPETITION RATE:1||MULTITERAWATT:1||SPECTROGRAPH:1||HIGHHARMONICGENERATION:1||spectroscopy:1||level population:1||PARTICLEACCELERATION:1||OPTICAL FREQUENCYMEASUREMENT:1||NANOWALLS:1||ROOMTEMPERATURE:1||AVERAGE OUTPUT POWER:1||GROUPVELOCITYMISMATCH:1||Impact ionization:1||Dynamics:1||Lasers:1||Collisional process:1||ABOVETHRESHOLD IONIZATION:1||MAINGROUP THERMOCHEMISTRY:1||dilute magnetic semiconductors:1||GACRN:1||SIZE:1||ATTOSECOND:1||Ar cluster:1||Xray astrophysics:1||photoionization:1||irons:1||normal incidence pulsed laser deposition:1||SHELLS:1||Silicon Oxide:1||gaspuff Zpinch:1||Xray:1||soft Xray reflectors:1||ESCAPE:1||ZN2SIO4:1||SILICA:1||Time 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materials:1||MOLECULAR PHOTOIONIZATION:1||LOCALIZATION:1||DEUTERIUM CLUSTERS:1||EXPLOSIONS:1||REGENERATIVE AMPLIFIERS:1||RAREGASES:1||THz radiation:1||FREEELECTRON LASER:1||REALTIME OBSERVATION:1||TARGET:1||photoionized plasmas:1||fs Xray laser:1||emission profile:1||HIGHORDER HARMONICS:1||Xray laser:1||atomic transition:1||EXCITATION:1||LASERS:1||PERFORMANCE:1||RELATIVISTIC ELECTRONS:1||BI2O3DOPED ZNO:1||INNERSHELL IONIZATION:1||Laser wakefield:1||FREQUENCY:1||SOLIDSTATE LASERS:1||Linearly polarized:1||THERMIONIC EMISSION:1||PULSE AMPLIFICATION SYSTEM:1||BIB3O6:1||NM:1||NONCOVALENT INTERACTIONS:1||CRYSTALLINE:1||INTENSITY:1||JETS:1||COHERENT:1||LINE:1||ANGULARDISTRIBUTION:1||SILVER IONS:1||magnetic anisotropy:1||DEVICES:1||Auger transitions:1||CosterKronig transitions:1||EFFICIENT:1||ELECTRONIMPACT IONIZATION:1||ULTRASHORTPULSE:1||Nanowire:1||Heterostructure:1||soft Xray reflectivity:1||PLASMA ACCELERATOR:1||ZINCOXIDE NANOWIRES:1||CHEMICALVAPORDEPOSITION:1||Electron acceleration:1||Ionization of gases:1||Delay dependent:1||MULTIPHOTON IONIZATION:1||FRAGMENTATION:1||GASJET:1||ultrafast nonlinear optics:1||CYCLE PULSES:1||KHZ:1||chemical vapor deposition:1||ferromagnetism:1||ABSORPTION:1||TERAHERTZ RADIATION:1||SCIENCE:1||FIELDS:1||ELECTRONS:1||nanomultilayer structures:1||YIELDS:1||AUGER:1||10HZ REPETITION RATE:1||MULTITERAWATT:1||SPECTROGRAPH:1||HIGHHARMONICGENERATION:1||spectroscopy:1||level population:1||PARTICLEACCELERATION:1||OPTICAL FREQUENCYMEASUREMENT:1||NANOWALLS:1||ROOMTEMPERATURE:1||AVERAGE OUTPUT POWER:1||GROUPVELOCITYMISMATCH:1||Impact ionization:1||Dynamics:1||Lasers:1||Collisional process:1||ABOVETHRESHOLD IONIZATION:1||MAINGROUP THERMOCHEMISTRY:1||dilute magnetic semiconductors:1||GACRN:1||SIZE:1||ATTOSECOND:1||Ar cluster:1||Xray astrophysics:1||photoionization:1||irons:1||normal incidence pulsed laser deposition:1||SHELLS:1||Silicon Oxide:1||gaspuff Zpinch:1||Xray:1||soft Xray reflectors:1||ESCAPE:1||ZN2SIO4:1||SILICA:1||Time delay:1||Collisional plasmas:1||MASSSPECTROMETRY:1||NUCLEARFUSION:1||PARAMETRIC AMPLIFICATION:1||LYING ELECTRONIC STATES:1||ADJUSTABLEPARAMETERS:1||MAGNETICPROPERTIES:1||LIQUIDPHASE EPITAXY:1||CEP laser:1||REGION:1||Plasma waveguide:1||AMBIENT GAS:1||DEPOSITION:1||HARMONICGENERATION:1||ENHANCEMENT:1||imaging spectrometer:1||Abel inversion:1||Water window:1||Liquid nitrogen jet:1||CHARGEEXCHANGE:1||NOBEL LECTURE:1||VARISTOR:1||EPITAXY:1||THINDISK LASER:1||HIGHREPETITIONRATE:1||Atom lasers:1||Electronimpact excitation:1||High order harmonics:1||ultrafast technology:1||PEAK POWER:1||CHARGED ALUMINUM CLUSTERS:1||GaN:1||THIN:1||Electron beam:1||INTENSE:1||Hard Xray pulse generation:1||NONLINEAR THOMSON SCATTERING:1||MULTILAYER:1||UVvisible spectrometer:1||ATOMS:1||innershell transitions:1||CORRECTED CONCAVE GRATINGS:1||DISCHARGE:1||LASERPLASMA:1||thin film:1||reflectivity:1||opacity:1||gain:1||smallangle Xray scattering:1||SOFTXRAY:1||ZINCOXIDE:1||CYGNUSX3:1||Betatron oscillation:1||ACCELERATOR:1||STRAINEDLAYER SUPERLATTICES:1||OPTICAL PARAMETRIC AMPLIFICATION:1||PASSIVE MODELOCKING:1||Collision dynamics:1||MUM:1||EXACTEXCHANGE:1||BASISSET:1||APPROXIMATION:1||OXYNITRIDES:1||Beam energy modulation:1||polarization spectroscopy:1||REORIENTATION TRANSITION:1||DEPENDENCE:1||sulfurs:1||BUILDINGBLOCKS:1||RATES:1||OPTICAL PULSES:1||toroidal mirror:1||XRAY LASER:1||CALCIUM:1||radially polarized laser:1||GRAINBOUNDARIES:1||VAPORDEPOSITION:1||Xray generation:1||MAGNETIZATION:1||Electric excitation:1||Laserinduced gas plasmas:1||Qualitative analysis:1||SCHEME:1||RADIATION:10||PULSES:8||PHOTOLUMINESCENCE:7||LASER:7||GENERATION:6||NANORODS:6||GROWTH:6||NANOWIRES:5||IMPLANTED GAN:5||SPECTROSCOPY:5||THINFILMS:4||DYNAMICS:4||SILICON:4||EXTREMEULTRAVIOLET:4||AMPLIFICATION:4||PRESSURE:4||PHASE:4||OPTICALPROPERTIES:4||SYSTEM:4||EMISSION:4||FEL:3||N2O:3||FILMS:3||OPTICS:3||SPECTRA:3||FIELD:3||MIRRORS:3||ARRAYS:3||CLUSTERS:3||SIO2:3||IONIZATION:3||VACUUM:3||SCATTERING:3||IONS:2||LUMINESCENCE PROPERTIES:2||ANISOTROPY:2||BEAMS:2||DIFFRACTION:2||DISPERSION:2||chemical vapor deposition (CVD):2||ELECTRONICSTRUCTURE:2||MOSFETS:2||SI3N4:2||DENSITY:2||LIGHT:2||PLASMAS:2||MATTER:2||nanocomposites:2||RAMANSCATTERING:2||NANOPARTICLES:2||OXIDE:2||AMPLIFIED SPONTANEOUS EMISSION:2||NM WAVELENGTH:2||GAIN:2||CARBON NANOTUBES:2||CROSSSECTIONS:2||LIGHTEMITTINGDIODES:2||PULSE:2||CARBON PLASMA:2||TISAPPHIRE LASER:2||Raman scattering:2||ROUTE:2||multilayer:2||CATHODOLUMINESCENCE:2||highresolution transmission electronic microscope (HRTEM):2||DIFFERENCEFREQUENCYGENERATION:2||CRYSTAL:2||laserproduced plasma:2||NANOCABLES:2||photoluminescence:2||MAGNETIC ALLOY SEMICONDUCTORS:2||MOLECULARBEAM EPITAXY:2||EARTHDOPED GAN:2||LASER FIELDS:2||CHIRPEDPULSEAMPLIFICATION:2||ALN:2||GAUSSIANBEAM:2||ASSISTED CATALYTIC GROWTH:2||BLUE:2||NANOSTRUCTURES:2||MAGNETOELECTRONICS:2||MICROSCOPY:2||ELECTROLUMINESCENCE:2||LASERPULSES:2||GaN nanowires:2||GALLIUM NITRIDE NANOWIRES:2||GAMNN:2||NANOTUBES:2||PHYSICS:2||Femtosecond laser:2||parametric oscillators and amplifiers:1||ultrafast lasers:1||VALENCE:1||nanowires:1||DILUTED MAGNETIC SEMICONDUCTOR:1||LUMINESCENCE:1||Density modulation:1||Energy modulation:1||Current enhanced SASE free electron laser:1||Undulator radiation:1||FREEELECTRON LASERS:1||ULTRATHIN FERROMAGNETICFILMS:1||OXIDEFILMS:1||ABLATION:1||COMPONENT:1||METAL:1||innershell excited states:1||Nelike ions:1||TRANSITIONS:1||XUV spectrometer:1||DIAGNOSTICS:1||Xray scattering:1||MO/SI:1||pulsed laser deposition:1||KEV IMPACT ENERGIES:1||vacuum electron acceleration:1||HIGHINTENSITY LASER:1||JUNCTIONS:1||LOWTEMPERATURE GROWTH:1||nanocrystalline materials:1||MOLECULAR PHOTOIONIZATION:1||LOCALIZATION:1||DEUTERIUM CLUSTERS:1||EXPLOSIONS:1||REGENERATIVE AMPLIFIERS:1||RAREGASES:1||THz radiation:1||FREEELECTRON LASER:1||REALTIME OBSERVATION:1||TARGET:1||photoionized plasmas:1||fs Xray laser:1||emission profile:1||HIGHORDER HARMONICS:1||Xray laser:1||atomic transition:1||EXCITATION:1||LASERS:1||PERFORMANCE:1||RELATIVISTIC ELECTRONS:1||BI2O3DOPED ZNO:1||INNERSHELL IONIZATION:1||Laser wakefield:1||FREQUENCY:1||SOLIDSTATE LASERS:1||Linearly polarized:1||THERMIONIC EMISSION:1||PULSE AMPLIFICATION SYSTEM:1||BIB3O6:1||NM:1||NONCOVALENT INTERACTIONS:1||CRYSTALLINE:1||INTENSITY:1||JETS:1||COHERENT:1||LINE:1||ANGULARDISTRIBUTION:1||SILVER IONS:1||magnetic anisotropy:1||DEVICES:1||Auger transitions:1||CosterKronig transitions:1||EFFICIENT:1||ELECTRONIMPACT IONIZATION:1||ULTRASHORTPULSE:1||Nanowire:1||Heterostructure:1||soft Xray reflectivity:1||PLASMA ACCELERATOR:1||ZINCOXIDE NANOWIRES:1||CHEMICALVAPORDEPOSITION:1||Electron acceleration:1||Ionization of gases:1||Delay dependent:1||MULTIPHOTON IONIZATION:1||FRAGMENTATION:1||GASJET:1||ultrafast nonlinear optics:1||CYCLE PULSES:1||KHZ:1||chemical vapor deposition:1||ferromagnetism:1||ABSORPTION:1||TERAHERTZ RADIATION:1||SCIENCE:1||FIELDS:1||ELECTRONS:1||nanomultilayer structures:1||YIELDS:1||AUGER:1||10HZ REPETITION RATE:1||MULTITERAWATT:1||SPECTROGRAPH:1||HIGHHARMONICGENERATION:1||spectroscopy:1||level population:1||PARTICLEACCELERATION:1||OPTICAL FREQUENCYMEASUREMENT:1||NANOWALLS:1||ROOMTEMPERATURE:1||AVERAGE OUTPUT POWER:1||GROUPVELOCITYMISMATCH:1||Impact ionization:1||Dynamics:1||Lasers:1||Collisional process:1||ABOVETHRESHOLD IONIZATION:1||MAINGROUP THERMOCHEMISTRY:1||dilute magnetic semiconductors:1||GACRN:1||SIZE:1||ATTOSECOND:1||Ar cluster:1||Xray astrophysics:1||photoionization:1||irons:1||normal incidence pulsed laser deposition:1||SHELLS:1||Silicon Oxide:1||gaspuff Zpinch:1||Xray:1||soft Xray reflectors:1||ESCAPE:1||ZN2SIO4:1||SILICA:1||Time delay:1||Collisional plasmas:1||MASSSPECTROMETRY:1||NUCLEARFUSION:1||PARAMETRIC AMPLIFICATION:1||LYING ELECTRONIC STATES:1||ADJUSTABLEPARAMETERS:1||MAGNETICPROPERTIES:1||LIQUIDPHASE EPITAXY:1||CEP laser:1||REGION:1||Plasma waveguide:1||AMBIENT GAS:1||DEPOSITION:1||HARMONICGENERATION:1||ENHANCEMENT:1||imaging spectrometer:1||Abel inversion:1||Water window:1||Liquid nitrogen jet:1||CHARGEEXCHANGE:1||NOBEL LECTURE:1||VARISTOR:1||EPITAXY:1||THINDISK LASER:1||HIGHREPETITIONRATE:1||Atom lasers:1||Electronimpact excitation:1||High order harmonics:1||ultrafast technology:1||PEAK POWER:1||CHARGED ALUMINUM CLUSTERS:1||GaN:1||THIN:1||Electron beam:1||INTENSE:1||Hard Xray pulse generation:1||NONLINEAR THOMSON SCATTERING:1||MULTILAYER:1||UVvisible spectrometer:1||ATOMS:1||innershell transitions:1||CORRECTED CONCAVE GRATINGS:1||DISCHARGE:1||LASERPLASMA:1||thin film:1||reflectivity:1||opacity:1||gain:1||smallangle Xray scattering:1||SOFTXRAY:1||ZINCOXIDE:1||CYGNUSX3:1||Betatron oscillation:1||ACCELERATOR:1||STRAINEDLAYER SUPERLATTICES:1||OPTICAL PARAMETRIC AMPLIFICATION:1||PASSIVE MODELOCKING:1||Collision dynamics:1||MUM:1||EXACTEXCHANGE:1||BASISSET:1||APPROXIMATION:1||OXYNITRIDES:1||Beam energy modulation:1||polarization spectroscopy:1||REORIENTATION TRANSITION:1||DEPENDENCE:1||sulfurs:1||BUILDINGBLOCKS:1||RATES:1||OPTICAL PULSES:1||toroidal mirror:1||XRAY LASER:1||CALCIUM:1||radially polarized laser:1||GRAINBOUNDARIES:1||VAPORDEPOSITION:1||Xray generation:1||MAGNETIZATION:1||Electric excitation:1||Laserinduced gas plasmas:1||Qualitative analysis:1||SCHEME:1||RADIATION:10||PULSES:8||PHOTOLUMINESCENCE:7||LASER:7||GENERATION:6||NANORODS:6||GROWTH:6||NANOWIRES:5||IMPLANTED 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SEMICONDUCTORS:2||MOLECULARBEAM EPITAXY:2||EARTHDOPED GAN:2||LASER FIELDS:2||CHIRPEDPULSEAMPLIFICATION:2||ALN:2||GAUSSIANBEAM:2||ASSISTED CATALYTIC GROWTH:2||BLUE:2||NANOSTRUCTURES:2||MAGNETOELECTRONICS:2||MICROSCOPY:2||ELECTROLUMINESCENCE:2||LASERPULSES:2||GaN nanowires:2||GALLIUM NITRIDE NANOWIRES:2||GAMNN:2||NANOTUBES:2||PHYSICS:2||Femtosecond laser:2||parametric oscillators and amplifiers:1||ultrafast lasers:1||VALENCE:1||nanowires:1||DILUTED MAGNETIC SEMICONDUCTOR:1||LUMINESCENCE:1||Density modulation:1||Energy modulation:1||Current enhanced SASE free electron laser:1||Undulator radiation:1||FREEELECTRON LASERS:1||ULTRATHIN FERROMAGNETICFILMS:1||OXIDEFILMS:1||ABLATION:1||COMPONENT:1||METAL:1||innershell excited states:1||Nelike ions:1||TRANSITIONS:1||XUV spectrometer:1||DIAGNOSTICS:1||Xray scattering:1||MO/SI:1||pulsed laser deposition:1||KEV IMPACT ENERGIES:1||vacuum electron acceleration:1||HIGHINTENSITY LASER:1||JUNCTIONS:1||LOWTEMPERATURE GROWTH:1||nanocrystalline materials:1||MOLECULAR PHOTOIONIZATION:1||LOCALIZATION:1||DEUTERIUM CLUSTERS:1||EXPLOSIONS:1||REGENERATIVE AMPLIFIERS:1||RAREGASES:1||THz radiation:1||FREEELECTRON LASER:1||REALTIME OBSERVATION:1||TARGET:1||photoionized plasmas:1||fs Xray laser:1||emission profile:1||HIGHORDER HARMONICS:1||Xray laser:1||atomic transition:1||EXCITATION:1||LASERS:1||PERFORMANCE:1||RELATIVISTIC ELECTRONS:1||BI2O3DOPED ZNO:1||INNERSHELL IONIZATION:1||Laser wakefield:1||FREQUENCY:1||SOLIDSTATE LASERS:1||Linearly polarized:1||THERMIONIC EMISSION:1||PULSE AMPLIFICATION SYSTEM:1||BIB3O6:1||NM:1||NONCOVALENT INTERACTIONS:1||CRYSTALLINE:1||INTENSITY:1||JETS:1||COHERENT:1||LINE:1||ANGULARDISTRIBUTION:1||SILVER IONS:1||magnetic anisotropy:1||DEVICES:1||Auger transitions:1||CosterKronig transitions:1||EFFICIENT:1||ELECTRONIMPACT IONIZATION:1||ULTRASHORTPULSE:1||Nanowire:1||Heterostructure:1||soft Xray reflectivity:1||PLASMA ACCELERATOR:1||ZINCOXIDE NANOWIRES:1||CHEMICALVAPORDEPOSITION:1||Electron acceleration:1||Ionization of gases:1||Delay dependent:1||MULTIPHOTON IONIZATION:1||FRAGMENTATION:1||GASJET:1||ultrafast nonlinear optics:1||CYCLE PULSES:1||KHZ:1||chemical vapor deposition:1||ferromagnetism:1||ABSORPTION:1||TERAHERTZ RADIATION:1||SCIENCE:1||FIELDS:1||ELECTRONS:1||nanomultilayer structures:1||YIELDS:1||AUGER:1||10HZ REPETITION RATE:1||MULTITERAWATT:1||SPECTROGRAPH:1||HIGHHARMONICGENERATION:1||spectroscopy:1||level population:1||PARTICLEACCELERATION:1||OPTICAL FREQUENCYMEASUREMENT:1||NANOWALLS:1||ROOMTEMPERATURE:1||AVERAGE OUTPUT POWER:1||GROUPVELOCITYMISMATCH:1||Impact ionization:1||Dynamics:1||Lasers:1||Collisional process:1||ABOVETHRESHOLD IONIZATION:1||MAINGROUP THERMOCHEMISTRY:1||dilute magnetic semiconductors:1||GACRN:1||SIZE:1||ATTOSECOND:1||Ar cluster:1||Xray astrophysics:1||photoionization:1||irons:1||normal incidence pulsed laser deposition:1||SHELLS:1||Silicon Oxide:1||gaspuff Zpinch:1||Xray:1||soft Xray reflectors:1||ESCAPE:1||ZN2SIO4:1||SILICA:1||Time 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materials:1||MOLECULAR PHOTOIONIZATION:1||LOCALIZATION:1||DEUTERIUM CLUSTERS:1||EXPLOSIONS:1||REGENERATIVE AMPLIFIERS:1||RAREGASES:1||THz radiation:1||FREEELECTRON LASER:1||REALTIME OBSERVATION:1||TARGET:1||photoionized plasmas:1||fs Xray laser:1||emission profile:1||HIGHORDER HARMONICS:1||Xray laser:1||atomic transition:1||EXCITATION:1||LASERS:1||PERFORMANCE:1||RELATIVISTIC ELECTRONS:1||BI2O3DOPED ZNO:1||INNERSHELL IONIZATION:1||Laser wakefield:1||FREQUENCY:1||SOLIDSTATE LASERS:1||Linearly polarized:1||THERMIONIC EMISSION:1||PULSE AMPLIFICATION SYSTEM:1||BIB3O6:1||NM:1||NONCOVALENT INTERACTIONS:1||CRYSTALLINE:1||INTENSITY:1||JETS:1||COHERENT:1||LINE:1||ANGULARDISTRIBUTION:1||SILVER IONS:1||magnetic anisotropy:1||DEVICES:1||Auger transitions:1||CosterKronig transitions:1||EFFICIENT:1||ELECTRONIMPACT IONIZATION:1||ULTRASHORTPULSE:1||Nanowire:1||Heterostructure:1||soft Xray reflectivity:1||PLASMA ACCELERATOR:1||ZINCOXIDE NANOWIRES:1||CHEMICALVAPORDEPOSITION:1||Electron acceleration:1||Ionization of gases:1||Delay dependent:1||MULTIPHOTON IONIZATION:1||FRAGMENTATION:1||GASJET:1||ultrafast nonlinear optics:1||CYCLE PULSES:1||KHZ:1||chemical vapor deposition:1||ferromagnetism:1||ABSORPTION:1||TERAHERTZ RADIATION:1||SCIENCE:1||FIELDS:1||ELECTRONS:1||nanomultilayer structures:1||YIELDS:1||AUGER:1||10HZ REPETITION RATE:1||MULTITERAWATT:1||SPECTROGRAPH:1||HIGHHARMONICGENERATION:1||spectroscopy:1||level population:1||PARTICLEACCELERATION:1||OPTICAL FREQUENCYMEASUREMENT:1||NANOWALLS:1||ROOMTEMPERATURE:1||AVERAGE OUTPUT POWER:1||GROUPVELOCITYMISMATCH:1||Impact ionization:1||Dynamics:1||Lasers:1||Collisional process:1||ABOVETHRESHOLD IONIZATION:1||MAINGROUP THERMOCHEMISTRY:1||dilute magnetic semiconductors:1||GACRN:1||SIZE:1||ATTOSECOND:1||Ar cluster:1||Xray astrophysics:1||photoionization:1||irons:1||normal incidence pulsed laser deposition:1||SHELLS:1||Silicon Oxide:1||gaspuff Zpinch:1||Xray:1||soft Xray reflectors:1||ESCAPE:1||ZN2SIO4:1||SILICA:1||Time delay:1||Collisional plasmas:1||MASSSPECTROMETRY:1||NUCLEARFUSION:1||PARAMETRIC AMPLIFICATION:1||LYING ELECTRONIC STATES:1||ADJUSTABLEPARAMETERS:1||MAGNETICPROPERTIES:1||LIQUIDPHASE EPITAXY:1||CEP laser:1||REGION:1||Plasma waveguide:1||AMBIENT GAS:1||DEPOSITION:1||HARMONICGENERATION:1||ENHANCEMENT:1||imaging spectrometer:1||Abel inversion:1||Water window:1||Liquid nitrogen jet:1||CHARGEEXCHANGE:1||NOBEL LECTURE:1||VARISTOR:1||EPITAXY:1||THINDISK LASER:1||HIGHREPETITIONRATE:1||Atom lasers:1||Electronimpact excitation:1||High order harmonics:1||ultrafast technology:1||PEAK POWER:1||CHARGED ALUMINUM CLUSTERS:1||GaN:1||THIN:1||Electron beam:1||INTENSE:1||Hard Xray pulse generation:1||NONLINEAR THOMSON SCATTERING:1||MULTILAYER:1||UVvisible spectrometer:1||ATOMS:1||innershell transitions:1||CORRECTED CONCAVE GRATINGS:1||DISCHARGE:1||LASERPLASMA:1||thin film:1||reflectivity:1||opacity:1||gain:1||smallangle Xray scattering:1||SOFTXRAY:1||ZINCOXIDE:1||CYGNUSX3:1||Betatron oscillation:1||ACCELERATOR:1||STRAINEDLAYER SUPERLATTICES:1||OPTICAL PARAMETRIC AMPLIFICATION:1||PASSIVE MODELOCKING:1||Collision dynamics:1||MUM:1||EXACTEXCHANGE:1||BASISSET:1||APPROXIMATION:1||OXYNITRIDES:1||Beam energy modulation:1||polarization spectroscopy:1||REORIENTATION TRANSITION:1||DEPENDENCE:1||sulfurs:1||BUILDINGBLOCKS:1||RATES:1||OPTICAL PULSES:1||toroidal mirror:1||XRAY LASER:1||CALCIUM:1||radially polarized laser:1||GRAINBOUNDARIES:1||VAPORDEPOSITION:1||Xray generation:1||MAGNETIZATION:1||Electric excitation:1||Laserinduced gas plasmas:1||Qualitative analysis:1||SCHEME:1||RADIATION:10||PULSES:8||PHOTOLUMINESCENCE:7||LASER:7||GENERATION:6||NANORODS:6||GROWTH:6||NANOWIRES:5||IMPLANTED GAN:5||SPECTROSCOPY:5||THINFILMS:4||DYNAMICS:4||SILICON:4||EXTREMEULTRAVIOLET:4||AMPLIFICATION:4||PRESSURE:4||PHASE:4||OPTICALPROPERTIES:4||SYSTEM:4||EMISSION:4||FEL:3||N2O:3||FILMS:3||OPTICS:3||SPECTRA:3||FIELD:3||MIRRORS:3||ARRAYS:3||CLUSTERS:3||SIO2:3||IONIZATION:3||VACUUM:3||SCATTERING:3||IONS:2||LUMINESCENCE PROPERTIES:2||ANISOTROPY:2||BEAMS:2||DIFFRACTION:2||DISPERSION:2||chemical vapor deposition (CVD):2||ELECTRONICSTRUCTURE:2||MOSFETS:2||SI3N4:2||DENSITY:2||LIGHT:2||PLASMAS:2||MATTER:2||nanocomposites:2||RAMANSCATTERING:2||NANOPARTICLES:2||OXIDE:2||AMPLIFIED SPONTANEOUS EMISSION:2||NM WAVELENGTH:2||GAIN:2||CARBON NANOTUBES:2||CROSSSECTIONS:2||LIGHTEMITTINGDIODES:2||PULSE:2||CARBON PLASMA:2||TISAPPHIRE LASER:2||Raman scattering:2||ROUTE:2||multilayer:2||CATHODOLUMINESCENCE:2||highresolution transmission electronic microscope (HRTEM):2||DIFFERENCEFREQUENCYGENERATION:2||CRYSTAL:2||laserproduced plasma:2||NANOCABLES:2||photoluminescence:2||MAGNETIC ALLOY SEMICONDUCTORS:2||MOLECULARBEAM EPITAXY:2||EARTHDOPED GAN:2||LASER FIELDS:2||CHIRPEDPULSEAMPLIFICATION:2||ALN:2||GAUSSIANBEAM:2||ASSISTED CATALYTIC GROWTH:2||BLUE:2||NANOSTRUCTURES:2||MAGNETOELECTRONICS:2||MICROSCOPY:2||ELECTROLUMINESCENCE:2||LASERPULSES:2||GaN nanowires:2||GALLIUM NITRIDE NANOWIRES:2||GAMNN:2||NANOTUBES:2||PHYSICS:2||Femtosecond laser:2||parametric oscillators and amplifiers:1||ultrafast lasers:1||VALENCE:1||nanowires:1||DILUTED MAGNETIC SEMICONDUCTOR:1||LUMINESCENCE:1||Density modulation:1||Energy modulation:1||Current enhanced SASE free electron laser:1||Undulator radiation:1||FREEELECTRON LASERS:1||ULTRATHIN FERROMAGNETICFILMS:1||OXIDEFILMS:1||ABLATION:1||COMPONENT:1||METAL:1||innershell excited states:1||Nelike ions:1||TRANSITIONS:1||XUV spectrometer:1||DIAGNOSTICS:1||Xray scattering:1||MO/SI:1||pulsed laser deposition:1||KEV IMPACT ENERGIES:1||vacuum electron acceleration:1||HIGHINTENSITY LASER:1||JUNCTIONS:1||LOWTEMPERATURE GROWTH:1||nanocrystalline materials:1||MOLECULAR PHOTOIONIZATION:1||LOCALIZATION:1||DEUTERIUM CLUSTERS:1||EXPLOSIONS:1||REGENERATIVE AMPLIFIERS:1||RAREGASES:1||THz radiation:1||FREEELECTRON LASER:1||REALTIME OBSERVATION:1||TARGET:1||photoionized plasmas:1||fs Xray laser:1||emission profile:1||HIGHORDER HARMONICS:1||Xray laser:1||atomic transition:1||EXCITATION:1||LASERS:1||PERFORMANCE:1||RELATIVISTIC ELECTRONS:1||BI2O3DOPED ZNO:1||INNERSHELL IONIZATION:1||Laser wakefield:1||FREQUENCY:1||SOLIDSTATE LASERS:1||Linearly polarized:1||THERMIONIC EMISSION:1||PULSE AMPLIFICATION SYSTEM:1||BIB3O6:1||NM:1||NONCOVALENT INTERACTIONS:1||CRYSTALLINE:1||INTENSITY:1||JETS:1||COHERENT:1||LINE:1||ANGULARDISTRIBUTION:1||SILVER IONS:1||magnetic anisotropy:1||DEVICES:1||Auger transitions:1||CosterKronig transitions:1||EFFICIENT:1||ELECTRONIMPACT IONIZATION:1||ULTRASHORTPULSE:1||Nanowire:1||Heterostructure:1||soft Xray reflectivity:1||PLASMA ACCELERATOR:1||ZINCOXIDE NANOWIRES:1||CHEMICALVAPORDEPOSITION:1||Electron acceleration:1||Ionization of gases:1||Delay dependent:1||MULTIPHOTON IONIZATION:1||FRAGMENTATION:1||GASJET:1||ultrafast nonlinear optics:1||CYCLE PULSES:1||KHZ:1||chemical vapor deposition:1||ferromagnetism:1||ABSORPTION:1||TERAHERTZ RADIATION:1||SCIENCE:1||FIELDS:1||ELECTRONS:1||nanomultilayer structures:1||YIELDS:1||AUGER:1||10HZ REPETITION RATE:1||MULTITERAWATT:1||SPECTROGRAPH:1||HIGHHARMONICGENERATION:1||spectroscopy:1||level population:1||PARTICLEACCELERATION:1||OPTICAL FREQUENCYMEASUREMENT:1||NANOWALLS:1||ROOMTEMPERATURE:1||AVERAGE OUTPUT POWER:1||GROUPVELOCITYMISMATCH:1||Impact ionization:1||Dynamics:1||Lasers:1||Collisional process:1||ABOVETHRESHOLD IONIZATION:1||MAINGROUP THERMOCHEMISTRY:1||dilute magnetic semiconductors:1||GACRN:1||SIZE:1||ATTOSECOND:1||Ar cluster:1||Xray astrophysics:1||photoionization:1||irons:1||normal incidence pulsed laser deposition:1||SHELLS:1||Silicon Oxide:1||gaspuff Zpinch:1||Xray:1||soft Xray reflectors:1||ESCAPE:1||ZN2SIO4:1||SILICA:1||Time delay:1||Collisional plasmas:1||MASSSPECTROMETRY:1||NUCLEARFUSION:1||PARAMETRIC AMPLIFICATION:1||LYING ELECTRONIC STATES:1||ADJUSTABLEPARAMETERS:1||MAGNETICPROPERTIES:1||LIQUIDPHASE EPITAXY:1||CEP laser:1||REGION:1||Plasma waveguide:1||AMBIENT GAS:1||DEPOSITION:1||HARMONICGENERATION:1||ENHANCEMENT:1||imaging spectrometer:1||Abel inversion:1||Water window:1||Liquid nitrogen jet:1||CHARGEEXCHANGE:1||NOBEL LECTURE:1||VARISTOR:1||EPITAXY:1||THINDISK LASER:1||HIGHREPETITIONRATE:1||Atom lasers:1||Electronimpact excitation:1||High order harmonics:1||ultrafast technology:1||PEAK POWER:1||CHARGED ALUMINUM CLUSTERS:1||GaN:1||THIN:1||Electron beam:1||INTENSE:1||Hard Xray pulse generation:1||NONLINEAR THOMSON SCATTERING:1||MULTILAYER:1||UVvisible spectrometer:1||ATOMS:1||innershell transitions:1||CORRECTED CONCAVE GRATINGS:1||DISCHARGE:1||LASERPLASMA:1||thin film:1||reflectivity:1||opacity:1||gain:1||smallangle Xray scattering:1||SOFTXRAY:1||ZINCOXIDE:1||CYGNUSX3:1||Betatron oscillation:1||ACCELERATOR:1||STRAINEDLAYER SUPERLATTICES:1||OPTICAL PARAMETRIC AMPLIFICATION:1||PASSIVE MODELOCKING:1||Collision dynamics:1||MUM:1||EXACTEXCHANGE:1||BASISSET:1||APPROXIMATION:1||OXYNITRIDES:1||Beam energy modulation:1||polarization spectroscopy:1||REORIENTATION TRANSITION:1||DEPENDENCE:1||sulfurs:1||BUILDINGBLOCKS:1||RATES:1||OPTICAL PULSES:1||toroidal mirror:1||XRAY LASER:1||CALCIUM:1||radially polarized laser:1||GRAINBOUNDARIES:1||VAPORDEPOSITION:1||Xray generation:1||MAGNETIZATION:1||Electric excitation:1||Laserinduced gas plasmas:1||Qualitative analysis:1||SCHEME:1||RADIATION:10||PULSES:8||PHOTOLUMINESCENCE:7||LASER:7||GENERATION:6||NANORODS:6||GROWTH:6||NANOWIRES:5||IMPLANTED 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SEMICONDUCTORS:2||MOLECULARBEAM EPITAXY:2||EARTHDOPED GAN:2||LASER FIELDS:2||CHIRPEDPULSEAMPLIFICATION:2||ALN:2||GAUSSIANBEAM:2||ASSISTED CATALYTIC GROWTH:2||BLUE:2||NANOSTRUCTURES:2||MAGNETOELECTRONICS:2||MICROSCOPY:2||ELECTROLUMINESCENCE:2||LASERPULSES:2||GaN nanowires:2||GALLIUM NITRIDE NANOWIRES:2||GAMNN:2||NANOTUBES:2||PHYSICS:2||Femtosecond laser:2||parametric oscillators and amplifiers:1||ultrafast lasers:1||VALENCE:1||nanowires:1||DILUTED MAGNETIC SEMICONDUCTOR:1||LUMINESCENCE:1||Density modulation:1||Energy modulation:1||Current enhanced SASE free electron laser:1||Undulator radiation:1||FREEELECTRON LASERS:1||ULTRATHIN FERROMAGNETICFILMS:1||OXIDEFILMS:1||ABLATION:1||COMPONENT:1||METAL:1||innershell excited states:1||Nelike ions:1||TRANSITIONS:1||XUV spectrometer:1||DIAGNOSTICS:1||Xray scattering:1||MO/SI:1||pulsed laser deposition:1||KEV IMPACT ENERGIES:1||vacuum electron acceleration:1||HIGHINTENSITY LASER:1||JUNCTIONS:1||LOWTEMPERATURE GROWTH:1||nanocrystalline materials:1||MOLECULAR PHOTOIONIZATION:1||LOCALIZATION:1||DEUTERIUM CLUSTERS:1||EXPLOSIONS:1||REGENERATIVE AMPLIFIERS:1||RAREGASES:1||THz radiation:1||FREEELECTRON LASER:1||REALTIME OBSERVATION:1||TARGET:1||photoionized plasmas:1||fs Xray laser:1||emission profile:1||HIGHORDER HARMONICS:1||Xray laser:1||atomic transition:1||EXCITATION:1||LASERS:1||PERFORMANCE:1||RELATIVISTIC ELECTRONS:1||BI2O3DOPED ZNO:1||INNERSHELL IONIZATION:1||Laser wakefield:1||FREQUENCY:1||SOLIDSTATE LASERS:1||Linearly polarized:1||THERMIONIC EMISSION:1||PULSE AMPLIFICATION SYSTEM:1||BIB3O6:1||NM:1||NONCOVALENT INTERACTIONS:1||CRYSTALLINE:1||INTENSITY:1||JETS:1||COHERENT:1||LINE:1||ANGULARDISTRIBUTION:1||SILVER IONS:1||magnetic anisotropy:1||DEVICES:1||Auger transitions:1||CosterKronig transitions:1||EFFICIENT:1||ELECTRONIMPACT IONIZATION:1||ULTRASHORTPULSE:1||Nanowire:1||Heterostructure:1||soft Xray reflectivity:1||PLASMA ACCELERATOR:1||ZINCOXIDE NANOWIRES:1||CHEMICALVAPORDEPOSITION:1||Electron acceleration:1||Ionization of gases:1||Delay dependent:1||MULTIPHOTON IONIZATION:1||FRAGMENTATION:1||GASJET:1||ultrafast nonlinear optics:1||CYCLE PULSES:1||KHZ:1||chemical vapor deposition:1||ferromagnetism:1||ABSORPTION:1||TERAHERTZ RADIATION:1||SCIENCE:1||FIELDS:1||ELECTRONS:1||nanomultilayer structures:1||YIELDS:1||AUGER:1||10HZ REPETITION RATE:1||MULTITERAWATT:1||SPECTROGRAPH:1||HIGHHARMONICGENERATION:1||spectroscopy:1||level population:1||PARTICLEACCELERATION:1||OPTICAL FREQUENCYMEASUREMENT:1||NANOWALLS:1||ROOMTEMPERATURE:1||AVERAGE OUTPUT POWER:1||GROUPVELOCITYMISMATCH:1||Impact ionization:1||Dynamics:1||Lasers:1||Collisional process:1||ABOVETHRESHOLD IONIZATION:1||MAINGROUP THERMOCHEMISTRY:1||dilute magnetic semiconductors:1||GACRN:1||SIZE:1||ATTOSECOND:1||Ar cluster:1||Xray astrophysics:1||photoionization:1||irons:1||normal incidence pulsed laser deposition:1||SHELLS:1||Silicon Oxide:1||gaspuff Zpinch:1||Xray:1||soft Xray reflectors:1||ESCAPE:1||ZN2SIO4:1||SILICA:1||Time 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materials:1||MOLECULAR PHOTOIONIZATION:1||LOCALIZATION:1||DEUTERIUM CLUSTERS:1||EXPLOSIONS:1||REGENERATIVE AMPLIFIERS:1||RAREGASES:1||THz radiation:1||FREEELECTRON LASER:1||REALTIME OBSERVATION:1||TARGET:1||photoionized plasmas:1||fs Xray laser:1||emission profile:1||HIGHORDER HARMONICS:1||Xray laser:1||atomic transition:1||EXCITATION:1||LASERS:1||PERFORMANCE:1||RELATIVISTIC ELECTRONS:1||BI2O3DOPED ZNO:1||INNERSHELL IONIZATION:1||Laser wakefield:1||FREQUENCY:1||SOLIDSTATE LASERS:1||Linearly polarized:1||THERMIONIC EMISSION:1||PULSE AMPLIFICATION SYSTEM:1||BIB3O6:1||NM:1||NONCOVALENT INTERACTIONS:1||CRYSTALLINE:1||INTENSITY:1||JETS:1||COHERENT:1||LINE:1||ANGULARDISTRIBUTION:1||SILVER IONS:1||magnetic anisotropy:1||DEVICES:1||Auger transitions:1||CosterKronig transitions:1||EFFICIENT:1||ELECTRONIMPACT IONIZATION:1||ULTRASHORTPULSE:1||Nanowire:1||Heterostructure:1||soft Xray reflectivity:1||PLASMA ACCELERATOR:1||ZINCOXIDE NANOWIRES:1||CHEMICALVAPORDEPOSITION:1||Electron acceleration:1||Ionization of gases:1||Delay dependent:1||MULTIPHOTON IONIZATION:1||FRAGMENTATION:1||GASJET:1||ultrafast nonlinear optics:1||CYCLE PULSES:1||KHZ:1||chemical vapor deposition:1||ferromagnetism:1||ABSORPTION:1||TERAHERTZ RADIATION:1||SCIENCE:1||FIELDS:1||ELECTRONS:1||nanomultilayer structures:1||YIELDS:1||AUGER:1||10HZ REPETITION RATE:1||MULTITERAWATT:1||SPECTROGRAPH:1||HIGHHARMONICGENERATION:1||spectroscopy:1||level population:1||PARTICLEACCELERATION:1||OPTICAL FREQUENCYMEASUREMENT:1||NANOWALLS:1||ROOMTEMPERATURE:1||AVERAGE OUTPUT POWER:1||GROUPVELOCITYMISMATCH:1||Impact ionization:1||Dynamics:1||Lasers:1||Collisional process:1||ABOVETHRESHOLD IONIZATION:1||MAINGROUP THERMOCHEMISTRY:1||dilute magnetic semiconductors:1||GACRN:1||SIZE:1||ATTOSECOND:1||Ar cluster:1||Xray astrophysics:1||photoionization:1||irons:1||normal incidence pulsed laser deposition:1||SHELLS:1||Silicon Oxide:1||gaspuff Zpinch:1||Xray:1||soft Xray reflectors:1||ESCAPE:1||ZN2SIO4:1||SILICA:1||Time delay:1||Collisional plasmas:1||MASSSPECTROMETRY:1||NUCLEARFUSION:1||PARAMETRIC AMPLIFICATION:1||LYING ELECTRONIC STATES:1||ADJUSTABLEPARAMETERS:1||MAGNETICPROPERTIES:1||LIQUIDPHASE EPITAXY:1||CEP laser:1||REGION:1||Plasma waveguide:1||AMBIENT GAS:1||DEPOSITION:1||HARMONICGENERATION:1||ENHANCEMENT:1||imaging spectrometer:1||Abel inversion:1||Water window:1||Liquid nitrogen jet:1||CHARGEEXCHANGE:1||NOBEL LECTURE:1||VARISTOR:1||EPITAXY:1||THINDISK LASER:1||HIGHREPETITIONRATE:1||Atom lasers:1||Electronimpact excitation:1||High order harmonics:1||ultrafast technology:1||PEAK POWER:1||CHARGED ALUMINUM CLUSTERS:1||GaN:1||THIN:1||Electron beam:1||INTENSE:1||Hard Xray pulse generation:1||NONLINEAR THOMSON SCATTERING:1||MULTILAYER:1||UVvisible spectrometer:1||ATOMS:1||innershell transitions:1||CORRECTED CONCAVE GRATINGS:1||DISCHARGE:1||LASERPLASMA:1||thin film:1||reflectivity:1||opacity:1||gain:1||smallangle Xray scattering:1||SOFTXRAY:1||ZINCOXIDE:1||CYGNUSX3:1||Betatron oscillation:1||ACCELERATOR:1||STRAINEDLAYER SUPERLATTICES:1||OPTICAL PARAMETRIC AMPLIFICATION:1||PASSIVE MODELOCKING:1||Collision dynamics:1||MUM:1||EXACTEXCHANGE:1||BASISSET:1||APPROXIMATION:1||OXYNITRIDES:1||Beam energy modulation:1||polarization spectroscopy:1||REORIENTATION TRANSITION:1||DEPENDENCE:1||sulfurs:1||BUILDINGBLOCKS:1||RATES:1||OPTICAL PULSES:1||toroidal mirror:1||XRAY LASER:1||CALCIUM:1||radially polarized laser:1||GRAINBOUNDARIES:1||VAPORDEPOSITION:1||Xray generation:1||MAGNETIZATION:1||Electric excitation:1||Laserinduced gas plasmas:1||Qualitative analysis:1||SCHEME:1||RADIATION:10||PULSES:8||PHOTOLUMINESCENCE:7||LASER:7||GENERATION:6||NANORODS:6||GROWTH:6||NANOWIRES:5||IMPLANTED GAN:5||SPECTROSCOPY:5||THINFILMS:4||DYNAMICS:4||SILICON:4||EXTREMEULTRAVIOLET:4||AMPLIFICATION:4||PRESSURE:4||PHASE:4||OPTICALPROPERTIES:4||SYSTEM:4||EMISSION:4||FEL:3||N2O:3||FILMS:3||OPTICS:3||SPECTRA:3||FIELD:3||MIRRORS:3||ARRAYS:3||CLUSTERS:3||SIO2:3||IONIZATION:3||VACUUM:3||SCATTERING:3||IONS:2||LUMINESCENCE PROPERTIES:2||ANISOTROPY:2||BEAMS:2||DIFFRACTION:2||DISPERSION:2||chemical vapor deposition (CVD):2||ELECTRONICSTRUCTURE:2||MOSFETS:2||SI3N4:2||DENSITY:2||LIGHT:2||PLASMAS:2||MATTER:2||nanocomposites:2||RAMANSCATTERING:2||NANOPARTICLES:2||OXIDE:2||AMPLIFIED SPONTANEOUS EMISSION:2||NM WAVELENGTH:2||GAIN:2||CARBON NANOTUBES:2||CROSSSECTIONS:2||LIGHTEMITTINGDIODES:2||PULSE:2||CARBON PLASMA:2||TISAPPHIRE LASER:2||Raman scattering:2||ROUTE:2||multilayer:2||CATHODOLUMINESCENCE:2||highresolution transmission electronic microscope (HRTEM):2||DIFFERENCEFREQUENCYGENERATION:2||CRYSTAL:2||laserproduced plasma:2||NANOCABLES:2||photoluminescence:2||MAGNETIC ALLOY SEMICONDUCTORS:2||MOLECULARBEAM EPITAXY:2||EARTHDOPED GAN:2||LASER FIELDS:2||CHIRPEDPULSEAMPLIFICATION:2||ALN:2||GAUSSIANBEAM:2||ASSISTED CATALYTIC GROWTH:2||BLUE:2||NANOSTRUCTURES:2||MAGNETOELECTRONICS:2||MICROSCOPY:2||ELECTROLUMINESCENCE:2||LASERPULSES:2||GaN nanowires:2||GALLIUM NITRIDE NANOWIRES:2||GAMNN:2||NANOTUBES:2||PHYSICS:2||Femtosecond laser:2||parametric oscillators and amplifiers:1||ultrafast lasers:1||VALENCE:1||nanowires:1||DILUTED MAGNETIC SEMICONDUCTOR:1||LUMINESCENCE:1||Density modulation:1||Energy modulation:1||Current enhanced SASE free electron laser:1||Undulator radiation:1||FREEELECTRON LASERS:1||ULTRATHIN FERROMAGNETICFILMS:1||OXIDEFILMS:1||ABLATION:1||COMPONENT:1||METAL:1||innershell excited states:1||Nelike ions:1||TRANSITIONS:1||XUV spectrometer:1||DIAGNOSTICS:1||Xray scattering:1||MO/SI:1||pulsed laser deposition:1||KEV IMPACT ENERGIES:1||vacuum electron acceleration:1||HIGHINTENSITY LASER:1||JUNCTIONS:1||LOWTEMPERATURE GROWTH:1||nanocrystalline materials:1||MOLECULAR PHOTOIONIZATION:1||LOCALIZATION:1||DEUTERIUM CLUSTERS:1||EXPLOSIONS:1||REGENERATIVE AMPLIFIERS:1||RAREGASES:1||THz radiation:1||FREEELECTRON LASER:1||REALTIME OBSERVATION:1||TARGET:1||photoionized plasmas:1||fs Xray laser:1||emission profile:1||HIGHORDER HARMONICS:1||Xray laser:1||atomic transition:1||EXCITATION:1||LASERS:1||PERFORMANCE:1||RELATIVISTIC ELECTRONS:1||BI2O3DOPED ZNO:1||INNERSHELL IONIZATION:1||Laser wakefield:1||FREQUENCY:1||SOLIDSTATE LASERS:1||Linearly polarized:1||THERMIONIC EMISSION:1||PULSE AMPLIFICATION SYSTEM:1||BIB3O6:1||NM:1||NONCOVALENT INTERACTIONS:1||CRYSTALLINE:1||INTENSITY:1||JETS:1||COHERENT:1||LINE:1||ANGULARDISTRIBUTION:1||SILVER IONS:1||magnetic anisotropy:1||DEVICES:1||Auger transitions:1||CosterKronig transitions:1||EFFICIENT:1||ELECTRONIMPACT IONIZATION:1||ULTRASHORTPULSE:1||Nanowire:1||Heterostructure:1||soft Xray reflectivity:1||PLASMA ACCELERATOR:1||ZINCOXIDE NANOWIRES:1||CHEMICALVAPORDEPOSITION:1||Electron acceleration:1||Ionization of gases:1||Delay dependent:1||MULTIPHOTON IONIZATION:1||FRAGMENTATION:1||GASJET:1||ultrafast nonlinear optics:1||CYCLE PULSES:1||KHZ:1||chemical vapor deposition:1||ferromagnetism:1||ABSORPTION:1||TERAHERTZ RADIATION:1||SCIENCE:1||FIELDS:1||ELECTRONS:1||nanomultilayer structures:1||YIELDS:1||AUGER:1||10HZ REPETITION RATE:1||MULTITERAWATT:1||SPECTROGRAPH:1||HIGHHARMONICGENERATION:1||spectroscopy:1||level population:1||PARTICLEACCELERATION:1||OPTICAL FREQUENCYMEASUREMENT:1||NANOWALLS:1||ROOMTEMPERATURE:1||AVERAGE OUTPUT POWER:1||GROUPVELOCITYMISMATCH:1||Impact ionization:1||Dynamics:1||Lasers:1||Collisional process:1||ABOVETHRESHOLD IONIZATION:1||MAINGROUP THERMOCHEMISTRY:1||dilute magnetic semiconductors:1||GACRN:1||SIZE:1||ATTOSECOND:1||Ar cluster:1||Xray astrophysics:1||photoionization:1||irons:1||normal incidence pulsed laser deposition:1||SHELLS:1||Silicon Oxide:1||gaspuff Zpinch:1||Xray:1||soft Xray reflectors:1||ESCAPE:1||ZN2SIO4:1||SILICA:1||Time delay:1||Collisional plasmas:1||MASSSPECTROMETRY:1||NUCLEARFUSION:1||PARAMETRIC AMPLIFICATION:1||LYING ELECTRONIC STATES:1||ADJUSTABLEPARAMETERS:1||MAGNETICPROPERTIES:1||LIQUIDPHASE EPITAXY:1||CEP laser:1||REGION:1||Plasma waveguide:1||AMBIENT GAS:1||DEPOSITION:1||HARMONICGENERATION:1||ENHANCEMENT:1||imaging spectrometer:1||Abel inversion:1||Water window:1||Liquid nitrogen jet:1||CHARGEEXCHANGE:1||NOBEL LECTURE:1||VARISTOR:1||EPITAXY:1||THINDISK LASER:1||HIGHREPETITIONRATE:1||Atom lasers:1||Electronimpact excitation:1||High order harmonics:1||ultrafast technology:1||PEAK POWER:1||CHARGED ALUMINUM CLUSTERS:1||GaN:1||THIN:1||Electron beam:1||INTENSE:1||Hard Xray pulse generation:1||NONLINEAR THOMSON SCATTERING:1||MULTILAYER:1||UVvisible spectrometer:1||ATOMS:1||innershell transitions:1||CORRECTED CONCAVE GRATINGS:1||DISCHARGE:1||LASERPLASMA:1||thin film:1||reflectivity:1||opacity:1||gain:1||smallangle Xray scattering:1||SOFTXRAY:1||ZINCOXIDE:1||CYGNUSX3:1||Betatron oscillation:1||ACCELERATOR:1||STRAINEDLAYER SUPERLATTICES:1||OPTICAL PARAMETRIC AMPLIFICATION:1||PASSIVE MODELOCKING:1||Collision dynamics:1||MUM:1||EXACTEXCHANGE:1||BASISSET:1||APPROXIMATION:1||OXYNITRIDES:1||Beam energy modulation:1||polarization spectroscopy:1||REORIENTATION TRANSITION:1||DEPENDENCE:1||sulfurs:1||BUILDINGBLOCKS:1||RATES:1||OPTICAL PULSES:1||toroidal mirror:1||XRAY LASER:1||CALCIUM:1||radially polarized laser:1||GRAINBOUNDARIES:1||VAPORDEPOSITION:1||Xray generation:1||MAGNETIZATION:1||Electric excitation:1||Laserinduced gas plasmas:1||Qualitative analysis:1||SCHEME:1||RADIATION:10||PULSES:8||PHOTOLUMINESCENCE:7||LASER:7||GENERATION:6||NANORODS:6||GROWTH:6||NANOWIRES:5||IMPLANTED 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SEMICONDUCTORS:2||MOLECULARBEAM EPITAXY:2||EARTHDOPED GAN:2||LASER FIELDS:2||CHIRPEDPULSEAMPLIFICATION:2||ALN:2||GAUSSIANBEAM:2||ASSISTED CATALYTIC GROWTH:2||BLUE:2||NANOSTRUCTURES:2||MAGNETOELECTRONICS:2||MICROSCOPY:2||ELECTROLUMINESCENCE:2||LASERPULSES:2||GaN nanowires:2||GALLIUM NITRIDE NANOWIRES:2||GAMNN:2||NANOTUBES:2||PHYSICS:2||Femtosecond laser:2||parametric oscillators and amplifiers:1||ultrafast lasers:1||VALENCE:1||nanowires:1||DILUTED MAGNETIC SEMICONDUCTOR:1||LUMINESCENCE:1||Density modulation:1||Energy modulation:1||Current enhanced SASE free electron laser:1||Undulator radiation:1||FREEELECTRON LASERS:1||ULTRATHIN FERROMAGNETICFILMS:1||OXIDEFILMS:1||ABLATION:1||COMPONENT:1||METAL:1||innershell excited states:1||Nelike ions:1||TRANSITIONS:1||XUV spectrometer:1||DIAGNOSTICS:1||Xray scattering:1||MO/SI:1||pulsed laser deposition:1||KEV IMPACT ENERGIES:1||vacuum electron acceleration:1||HIGHINTENSITY LASER:1||JUNCTIONS:1||LOWTEMPERATURE GROWTH:1||nanocrystalline materials:1||MOLECULAR PHOTOIONIZATION:1||LOCALIZATION:1||DEUTERIUM CLUSTERS:1||EXPLOSIONS:1||REGENERATIVE AMPLIFIERS:1||RAREGASES:1||THz radiation:1||FREEELECTRON LASER:1||REALTIME OBSERVATION:1||TARGET:1||photoionized plasmas:1||fs Xray laser:1||emission profile:1||HIGHORDER HARMONICS:1||Xray laser:1||atomic transition:1||EXCITATION:1||LASERS:1||PERFORMANCE:1||RELATIVISTIC ELECTRONS:1||BI2O3DOPED ZNO:1||INNERSHELL IONIZATION:1||Laser wakefield:1||FREQUENCY:1||SOLIDSTATE LASERS:1||Linearly polarized:1||THERMIONIC EMISSION:1||PULSE AMPLIFICATION SYSTEM:1||BIB3O6:1||NM:1||NONCOVALENT INTERACTIONS:1||CRYSTALLINE:1||INTENSITY:1||JETS:1||COHERENT:1||LINE:1||ANGULARDISTRIBUTION:1||SILVER IONS:1||magnetic anisotropy:1||DEVICES:1||Auger transitions:1||CosterKronig transitions:1||EFFICIENT:1||ELECTRONIMPACT IONIZATION:1||ULTRASHORTPULSE:1||Nanowire:1||Heterostructure:1||soft Xray reflectivity:1||PLASMA ACCELERATOR:1||ZINCOXIDE NANOWIRES:1||CHEMICALVAPORDEPOSITION:1||Electron acceleration:1||Ionization of gases:1||Delay dependent:1||MULTIPHOTON IONIZATION:1||FRAGMENTATION:1||GASJET:1||ultrafast nonlinear optics:1||CYCLE PULSES:1||KHZ:1||chemical vapor deposition:1||ferromagnetism:1||ABSORPTION:1||TERAHERTZ RADIATION:1||SCIENCE:1||FIELDS:1||ELECTRONS:1||nanomultilayer structures:1||YIELDS:1||AUGER:1||10HZ REPETITION RATE:1||MULTITERAWATT:1||SPECTROGRAPH:1||HIGHHARMONICGENERATION:1||spectroscopy:1||level population:1||PARTICLEACCELERATION:1||OPTICAL FREQUENCYMEASUREMENT:1||NANOWALLS:1||ROOMTEMPERATURE:1||AVERAGE OUTPUT POWER:1||GROUPVELOCITYMISMATCH:1||Impact ionization:1||Dynamics:1||Lasers:1||Collisional process:1||ABOVETHRESHOLD IONIZATION:1||MAINGROUP THERMOCHEMISTRY:1||dilute magnetic semiconductors:1||GACRN:1||SIZE:1||ATTOSECOND:1||Ar cluster:1||Xray astrophysics:1||photoionization:1||irons:1||normal incidence pulsed laser deposition:1||SHELLS:1||Silicon Oxide:1||gaspuff Zpinch:1||Xray:1||soft Xray reflectors:1||ESCAPE:1||ZN2SIO4:1||SILICA:1||Time 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materials:1||MOLECULAR PHOTOIONIZATION:1||LOCALIZATION:1||DEUTERIUM CLUSTERS:1||EXPLOSIONS:1||REGENERATIVE AMPLIFIERS:1||RAREGASES:1||THz radiation:1||FREEELECTRON LASER:1||REALTIME OBSERVATION:1||TARGET:1||photoionized plasmas:1||fs Xray laser:1||emission profile:1||HIGHORDER HARMONICS:1||Xray laser:1||atomic transition:1||EXCITATION:1||LASERS:1||PERFORMANCE:1||RELATIVISTIC ELECTRONS:1||BI2O3DOPED ZNO:1||INNERSHELL IONIZATION:1||Laser wakefield:1||FREQUENCY:1||SOLIDSTATE LASERS:1||Linearly polarized:1||THERMIONIC EMISSION:1||PULSE AMPLIFICATION SYSTEM:1||BIB3O6:1||NM:1||NONCOVALENT INTERACTIONS:1||CRYSTALLINE:1||INTENSITY:1||JETS:1||COHERENT:1||LINE:1||ANGULARDISTRIBUTION:1||SILVER IONS:1||magnetic anisotropy:1||DEVICES:1||Auger transitions:1||CosterKronig transitions:1||EFFICIENT:1||ELECTRONIMPACT IONIZATION:1||ULTRASHORTPULSE:1||Nanowire:1||Heterostructure:1||soft Xray reflectivity:1||PLASMA ACCELERATOR:1||ZINCOXIDE NANOWIRES:1||CHEMICALVAPORDEPOSITION:1||Electron acceleration:1||Ionization of gases:1||Delay dependent:1||MULTIPHOTON IONIZATION:1||FRAGMENTATION:1||GASJET:1||ultrafast nonlinear optics:1||CYCLE PULSES:1||KHZ:1||chemical vapor deposition:1||ferromagnetism:1||ABSORPTION:1||TERAHERTZ RADIATION:1||SCIENCE:1||FIELDS:1||ELECTRONS:1||nanomultilayer structures:1||YIELDS:1||AUGER:1||10HZ REPETITION RATE:1||MULTITERAWATT:1||SPECTROGRAPH:1||HIGHHARMONICGENERATION:1||spectroscopy:1||level population:1||PARTICLEACCELERATION:1||OPTICAL FREQUENCYMEASUREMENT:1||NANOWALLS:1||ROOMTEMPERATURE:1||AVERAGE OUTPUT POWER:1||GROUPVELOCITYMISMATCH:1||Impact ionization:1||Dynamics:1||Lasers:1||Collisional process:1||ABOVETHRESHOLD IONIZATION:1||MAINGROUP THERMOCHEMISTRY:1||dilute magnetic semiconductors:1||GACRN:1||SIZE:1||ATTOSECOND:1||Ar cluster:1||Xray astrophysics:1||photoionization:1||irons:1||normal incidence pulsed laser deposition:1||SHELLS:1||Silicon Oxide:1||gaspuff Zpinch:1||Xray:1||soft Xray reflectors:1||ESCAPE:1||ZN2SIO4:1||SILICA:1||Time delay:1||Collisional plasmas:1||MASSSPECTROMETRY:1||NUCLEARFUSION:1||PARAMETRIC AMPLIFICATION:1||LYING ELECTRONIC STATES:1||ADJUSTABLEPARAMETERS:1||MAGNETICPROPERTIES:1||LIQUIDPHASE EPITAXY:1||CEP laser:1||REGION:1||Plasma waveguide:1||AMBIENT GAS:1||DEPOSITION:1||HARMONICGENERATION:1||ENHANCEMENT:1||imaging spectrometer:1||Abel inversion:1||Water window:1||Liquid nitrogen jet:1||CHARGEEXCHANGE:1||NOBEL LECTURE:1||VARISTOR:1||EPITAXY:1||THINDISK LASER:1||HIGHREPETITIONRATE:1||Atom lasers:1||Electronimpact excitation:1||High order harmonics:1||ultrafast technology:1||PEAK POWER:1||CHARGED ALUMINUM CLUSTERS:1||GaN:1||THIN:1||Electron beam:1||INTENSE:1||Hard Xray pulse generation:1||NONLINEAR THOMSON SCATTERING:1||MULTILAYER:1||UVvisible spectrometer:1||ATOMS:1||innershell transitions:1||CORRECTED CONCAVE GRATINGS:1||DISCHARGE:1||LASERPLASMA:1||thin film:1||reflectivity:1||opacity:1||gain:1||smallangle Xray scattering:1||SOFTXRAY:1||ZINCOXIDE:1||CYGNUSX3:1||Betatron oscillation:1||ACCELERATOR:1||STRAINEDLAYER SUPERLATTICES:1||OPTICAL PARAMETRIC AMPLIFICATION:1||PASSIVE MODELOCKING:1||Collision dynamics:1||MUM:1||EXACTEXCHANGE:1||BASISSET:1||APPROXIMATION:1||OXYNITRIDES:1||Beam energy modulation:1||polarization spectroscopy:1||REORIENTATION TRANSITION:1||DEPENDENCE:1||sulfurs:1||BUILDINGBLOCKS:1||RATES:1||OPTICAL PULSES:1||toroidal mirror:1||XRAY LASER:1||CALCIUM:1||radially polarized laser:1||GRAINBOUNDARIES:1||VAPORDEPOSITION:1||Xray generation:1||MAGNETIZATION:1||Electric excitation:1||Laserinduced gas plasmas:1||Qualitative analysis:1||SCHEME:1||RADIATION:10||PULSES:8||PHOTOLUMINESCENCE:7||LASER:7||GENERATION:6||NANORODS:6||GROWTH:6||NANOWIRES:5||IMPLANTED GAN:5||SPECTROSCOPY:5||THINFILMS:4||DYNAMICS:4||SILICON:4||EXTREMEULTRAVIOLET:4||AMPLIFICATION:4||PRESSURE:4||PHASE:4||OPTICALPROPERTIES:4||SYSTEM:4||EMISSION:4||FEL:3||N2O:3||FILMS:3||OPTICS:3||SPECTRA:3||FIELD:3||MIRRORS:3||ARRAYS:3||CLUSTERS:3||SIO2:3||IONIZATION:3||VACUUM:3||SCATTERING:3||IONS:2||LUMINESCENCE PROPERTIES:2||ANISOTROPY:2||BEAMS:2||DIFFRACTION:2||DISPERSION:2||chemical vapor deposition (CVD):2||ELECTRONICSTRUCTURE:2||MOSFETS:2||SI3N4:2||DENSITY:2||LIGHT:2||PLASMAS:2||MATTER:2||nanocomposites:2||RAMANSCATTERING:2||NANOPARTICLES:2||OXIDE:2||AMPLIFIED SPONTANEOUS EMISSION:2||NM WAVELENGTH:2||GAIN:2||CARBON NANOTUBES:2||CROSSSECTIONS:2||LIGHTEMITTINGDIODES:2||PULSE:2||CARBON PLASMA:2||TISAPPHIRE LASER:2||Raman scattering:2||ROUTE:2||multilayer:2||CATHODOLUMINESCENCE:2||highresolution transmission electronic microscope (HRTEM):2||DIFFERENCEFREQUENCYGENERATION:2||CRYSTAL:2||laserproduced plasma:2||NANOCABLES:2||photoluminescence:2||MAGNETIC ALLOY SEMICONDUCTORS:2||MOLECULARBEAM EPITAXY:2||EARTHDOPED GAN:2||LASER FIELDS:2||CHIRPEDPULSEAMPLIFICATION:2||ALN:2||GAUSSIANBEAM:2||ASSISTED CATALYTIC GROWTH:2||BLUE:2||NANOSTRUCTURES:2||MAGNETOELECTRONICS:2||MICROSCOPY:2||ELECTROLUMINESCENCE:2||LASERPULSES:2||GaN nanowires:2||GALLIUM NITRIDE NANOWIRES:2||GAMNN:2||NANOTUBES:2||PHYSICS:2||Femtosecond laser:2||parametric oscillators and amplifiers:1||ultrafast lasers:1||VALENCE:1||nanowires:1||DILUTED MAGNETIC SEMICONDUCTOR:1||LUMINESCENCE:1||Density modulation:1||Energy modulation:1||Current enhanced SASE free electron laser:1||Undulator radiation:1||FREEELECTRON LASERS:1||ULTRATHIN FERROMAGNETICFILMS:1||OXIDEFILMS:1||ABLATION:1||COMPONENT:1||METAL:1||innershell excited states:1||Nelike ions:1||TRANSITIONS:1||XUV spectrometer:1||DIAGNOSTICS:1||Xray scattering:1||MO/SI:1||pulsed laser deposition:1||KEV IMPACT ENERGIES:1||vacuum electron acceleration:1||HIGHINTENSITY LASER:1||JUNCTIONS:1||LOWTEMPERATURE GROWTH:1||nanocrystalline materials:1||MOLECULAR PHOTOIONIZATION:1||LOCALIZATION:1||DEUTERIUM CLUSTERS:1||EXPLOSIONS:1||REGENERATIVE AMPLIFIERS:1||RAREGASES:1||THz radiation:1||FREEELECTRON LASER:1||REALTIME OBSERVATION:1||TARGET:1||photoionized plasmas:1||fs Xray laser:1||emission profile:1||HIGHORDER HARMONICS:1||Xray laser:1||atomic transition:1||EXCITATION:1||LASERS:1||PERFORMANCE:1||RELATIVISTIC ELECTRONS:1||BI2O3DOPED ZNO:1||INNERSHELL IONIZATION:1||Laser wakefield:1||FREQUENCY:1||SOLIDSTATE LASERS:1||Linearly polarized:1||THERMIONIC EMISSION:1||PULSE AMPLIFICATION SYSTEM:1||BIB3O6:1||NM:1||NONCOVALENT INTERACTIONS:1||CRYSTALLINE:1||INTENSITY:1||JETS:1||COHERENT:1||LINE:1||ANGULARDISTRIBUTION:1||SILVER IONS:1||magnetic anisotropy:1||DEVICES:1||Auger transitions:1||CosterKronig transitions:1||EFFICIENT:1||ELECTRONIMPACT IONIZATION:1||ULTRASHORTPULSE:1||Nanowire:1||Heterostructure:1||soft Xray reflectivity:1||PLASMA ACCELERATOR:1||ZINCOXIDE NANOWIRES:1||CHEMICALVAPORDEPOSITION:1||Electron acceleration:1||Ionization of gases:1||Delay dependent:1||MULTIPHOTON IONIZATION:1||FRAGMENTATION:1||GASJET:1||ultrafast nonlinear optics:1||CYCLE PULSES:1||KHZ:1||chemical vapor deposition:1||ferromagnetism:1||ABSORPTION:1||TERAHERTZ RADIATION:1||SCIENCE:1||FIELDS:1||ELECTRONS:1||nanomultilayer structures:1||YIELDS:1||AUGER:1||10HZ REPETITION RATE:1||MULTITERAWATT:1||SPECTROGRAPH:1||HIGHHARMONICGENERATION:1||spectroscopy:1||level population:1||PARTICLEACCELERATION:1||OPTICAL FREQUENCYMEASUREMENT:1||NANOWALLS:1||ROOMTEMPERATURE:1||AVERAGE OUTPUT POWER:1||GROUPVELOCITYMISMATCH:1||Impact ionization:1||Dynamics:1||Lasers:1||Collisional process:1||ABOVETHRESHOLD IONIZATION:1||MAINGROUP THERMOCHEMISTRY:1||dilute magnetic semiconductors:1||GACRN:1||SIZE:1||ATTOSECOND:1||Ar cluster:1||Xray astrophysics:1||photoionization:1||irons:1||normal incidence pulsed laser deposition:1||SHELLS:1||Silicon Oxide:1||gaspuff Zpinch:1||Xray:1||soft Xray reflectors:1||ESCAPE:1||ZN2SIO4:1||SILICA:1||Time delay:1||Collisional plasmas:1||MASSSPECTROMETRY:1||NUCLEARFUSION:1||PARAMETRIC AMPLIFICATION:1||LYING ELECTRONIC STATES:1||ADJUSTABLEPARAMETERS:1||MAGNETICPROPERTIES:1||LIQUIDPHASE EPITAXY:1||CEP laser:1||REGION:1||Plasma waveguide:1||AMBIENT GAS:1||DEPOSITION:1||HARMONICGENERATION:1||ENHANCEMENT:1||imaging spectrometer:1||Abel inversion:1||Water window:1||Liquid nitrogen jet:1||CHARGEEXCHANGE:1||NOBEL LECTURE:1||VARISTOR:1||EPITAXY:1||THINDISK LASER:1||HIGHREPETITIONRATE:1||Atom lasers:1||Electronimpact excitation:1||High order harmonics:1||ultrafast technology:1||PEAK POWER:1||CHARGED ALUMINUM CLUSTERS:1||GaN:1||THIN:1||Electron beam:1||INTENSE:1||Hard Xray pulse generation:1||NONLINEAR THOMSON SCATTERING:1||MULTILAYER:1||UVvisible spectrometer:1||ATOMS:1||innershell transitions:1||CORRECTED CONCAVE GRATINGS:1||DISCHARGE:1||LASERPLASMA:1||thin film:1||reflectivity:1||opacity:1||gain:1||smallangle Xray scattering:1||SOFTXRAY:1||ZINCOXIDE:1||CYGNUSX3:1||Betatron oscillation:1||ACCELERATOR:1||STRAINEDLAYER SUPERLATTICES:1||OPTICAL PARAMETRIC AMPLIFICATION:1||PASSIVE MODELOCKING:1||Collision dynamics:1||MUM:1||EXACTEXCHANGE:1||BASISSET:1||APPROXIMATION:1||OXYNITRIDES:1||Beam energy modulation:1||polarization spectroscopy:1||REORIENTATION TRANSITION:1||DEPENDENCE:1||sulfurs:1||BUILDINGBLOCKS:1||RATES:1||OPTICAL PULSES:1||toroidal mirror:1||XRAY LASER:1||CALCIUM:1||radially polarized laser:1||GRAINBOUNDARIES:1||VAPORDEPOSITION:1||Xray generation:1||MAGNETIZATION:1||Electric excitation:1||Laserinduced gas plasmas:1||Qualitative analysis:1||SCHEME:1||RADIATION:10||PULSES:8||PHOTOLUMINESCENCE:7||LASER:7||GENERATION:6||NANORODS:6||GROWTH:6||NANOWIRES:5||IMPLANTED 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SEMICONDUCTORS:2||MOLECULARBEAM EPITAXY:2||EARTHDOPED GAN:2||LASER FIELDS:2||CHIRPEDPULSEAMPLIFICATION:2||ALN:2||GAUSSIANBEAM:2||ASSISTED CATALYTIC GROWTH:2||BLUE:2||NANOSTRUCTURES:2||MAGNETOELECTRONICS:2||MICROSCOPY:2||ELECTROLUMINESCENCE:2||LASERPULSES:2||GaN nanowires:2||GALLIUM NITRIDE NANOWIRES:2||GAMNN:2||NANOTUBES:2||PHYSICS:2||Femtosecond laser:2||parametric oscillators and amplifiers:1||ultrafast lasers:1||VALENCE:1||nanowires:1||DILUTED MAGNETIC SEMICONDUCTOR:1||LUMINESCENCE:1||Density modulation:1||Energy modulation:1||Current enhanced SASE free electron laser:1||Undulator radiation:1||FREEELECTRON LASERS:1||ULTRATHIN FERROMAGNETICFILMS:1||OXIDEFILMS:1||ABLATION:1||COMPONENT:1||METAL:1||innershell excited states:1||Nelike ions:1||TRANSITIONS:1||XUV spectrometer:1||DIAGNOSTICS:1||Xray scattering:1||MO/SI:1||pulsed laser deposition:1||KEV IMPACT ENERGIES:1||vacuum electron acceleration:1||HIGHINTENSITY LASER:1||JUNCTIONS:1||LOWTEMPERATURE GROWTH:1||nanocrystalline materials:1||MOLECULAR PHOTOIONIZATION:1||LOCALIZATION:1||DEUTERIUM CLUSTERS:1||EXPLOSIONS:1||REGENERATIVE AMPLIFIERS:1||RAREGASES:1||THz radiation:1||FREEELECTRON LASER:1||REALTIME OBSERVATION:1||TARGET:1||photoionized plasmas:1||fs Xray laser:1||emission profile:1||HIGHORDER HARMONICS:1||Xray laser:1||atomic transition:1||EXCITATION:1||LASERS:1||PERFORMANCE:1||RELATIVISTIC ELECTRONS:1||BI2O3DOPED ZNO:1||INNERSHELL IONIZATION:1||Laser wakefield:1||FREQUENCY:1||SOLIDSTATE LASERS:1||Linearly polarized:1||THERMIONIC EMISSION:1||PULSE AMPLIFICATION SYSTEM:1||BIB3O6:1||NM:1||NONCOVALENT INTERACTIONS:1||CRYSTALLINE:1||INTENSITY:1||JETS:1||COHERENT:1||LINE:1||ANGULARDISTRIBUTION:1||SILVER IONS:1||magnetic anisotropy:1||DEVICES:1||Auger transitions:1||CosterKronig transitions:1||EFFICIENT:1||ELECTRONIMPACT IONIZATION:1||ULTRASHORTPULSE:1||Nanowire:1||Heterostructure:1||soft Xray reflectivity:1||PLASMA ACCELERATOR:1||ZINCOXIDE NANOWIRES:1||CHEMICALVAPORDEPOSITION:1||Electron acceleration:1||Ionization of gases:1||Delay dependent:1||MULTIPHOTON IONIZATION:1||FRAGMENTATION:1||GASJET:1||ultrafast nonlinear optics:1||CYCLE PULSES:1||KHZ:1||chemical vapor deposition:1||ferromagnetism:1||ABSORPTION:1||TERAHERTZ RADIATION:1||SCIENCE:1||FIELDS:1||ELECTRONS:1||nanomultilayer structures:1||YIELDS:1||AUGER:1||10HZ REPETITION RATE:1||MULTITERAWATT:1||SPECTROGRAPH:1||HIGHHARMONICGENERATION:1||spectroscopy:1||level population:1||PARTICLEACCELERATION:1||OPTICAL FREQUENCYMEASUREMENT:1||NANOWALLS:1||ROOMTEMPERATURE:1||AVERAGE OUTPUT POWER:1||GROUPVELOCITYMISMATCH:1||Impact ionization:1||Dynamics:1||Lasers:1||Collisional process:1||ABOVETHRESHOLD IONIZATION:1||MAINGROUP THERMOCHEMISTRY:1||dilute magnetic semiconductors:1||GACRN:1||SIZE:1||ATTOSECOND:1||Ar cluster:1||Xray astrophysics:1||photoionization:1||irons:1||normal incidence pulsed laser deposition:1||SHELLS:1||Silicon Oxide:1||gaspuff Zpinch:1||Xray:1||soft Xray reflectors:1||ESCAPE:1||ZN2SIO4:1||SILICA:1||Time 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materials:1||MOLECULAR PHOTOIONIZATION:1||LOCALIZATION:1||DEUTERIUM CLUSTERS:1||EXPLOSIONS:1||REGENERATIVE AMPLIFIERS:1||RAREGASES:1||THz radiation:1||FREEELECTRON LASER:1||REALTIME OBSERVATION:1||TARGET:1||photoionized plasmas:1||fs Xray laser:1||emission profile:1||HIGHORDER HARMONICS:1||Xray laser:1||atomic transition:1||EXCITATION:1||LASERS:1||PERFORMANCE:1||RELATIVISTIC ELECTRONS:1||BI2O3DOPED ZNO:1||INNERSHELL IONIZATION:1||Laser wakefield:1||FREQUENCY:1||SOLIDSTATE LASERS:1||Linearly polarized:1||THERMIONIC EMISSION:1||PULSE AMPLIFICATION SYSTEM:1||BIB3O6:1||NM:1||NONCOVALENT INTERACTIONS:1||CRYSTALLINE:1||INTENSITY:1||JETS:1||COHERENT:1||LINE:1||ANGULARDISTRIBUTION:1||SILVER IONS:1||magnetic anisotropy:1||DEVICES:1||Auger transitions:1||CosterKronig transitions:1||EFFICIENT:1||ELECTRONIMPACT IONIZATION:1||ULTRASHORTPULSE:1||Nanowire:1||Heterostructure:1||soft Xray reflectivity:1||PLASMA ACCELERATOR:1||ZINCOXIDE NANOWIRES:1||CHEMICALVAPORDEPOSITION:1||Electron acceleration:1||Ionization of gases:1||Delay dependent:1||MULTIPHOTON IONIZATION:1||FRAGMENTATION:1||GASJET:1||ultrafast nonlinear optics:1||CYCLE PULSES:1||KHZ:1||chemical vapor deposition:1||ferromagnetism:1||ABSORPTION:1||TERAHERTZ RADIATION:1||SCIENCE:1||FIELDS:1||ELECTRONS:1||nanomultilayer structures:1||YIELDS:1||AUGER:1||10HZ REPETITION RATE:1||MULTITERAWATT:1||SPECTROGRAPH:1||HIGHHARMONICGENERATION:1||spectroscopy:1||level population:1||PARTICLEACCELERATION:1||OPTICAL FREQUENCYMEASUREMENT:1||NANOWALLS:1||ROOMTEMPERATURE:1||AVERAGE OUTPUT POWER:1||GROUPVELOCITYMISMATCH:1||Impact ionization:1||Dynamics:1||Lasers:1||Collisional process:1||ABOVETHRESHOLD IONIZATION:1||MAINGROUP THERMOCHEMISTRY:1||dilute magnetic semiconductors:1||GACRN:1||SIZE:1||ATTOSECOND:1||Ar cluster:1||Xray astrophysics:1||photoionization:1||irons:1||normal incidence pulsed laser deposition:1||SHELLS:1||Silicon Oxide:1||gaspuff Zpinch:1||Xray:1||soft Xray reflectors:1||ESCAPE:1||ZN2SIO4:1||SILICA:1||Time delay:1||Collisional plasmas:1||MASSSPECTROMETRY:1||NUCLEARFUSION:1||PARAMETRIC AMPLIFICATION:1||LYING ELECTRONIC STATES:1||ADJUSTABLEPARAMETERS:1||MAGNETICPROPERTIES:1||LIQUIDPHASE EPITAXY:1||CEP laser:1||REGION:1||Plasma waveguide:1||AMBIENT GAS:1||DEPOSITION:1||HARMONICGENERATION:1||ENHANCEMENT:1||imaging spectrometer:1||Abel inversion:1||Water window:1||Liquid nitrogen jet:1||CHARGEEXCHANGE:1||NOBEL LECTURE:1||VARISTOR:1||EPITAXY:1||THINDISK LASER:1||HIGHREPETITIONRATE:1||Atom lasers:1||Electronimpact excitation:1||High order harmonics:1||ultrafast technology:1||PEAK POWER:1||CHARGED ALUMINUM CLUSTERS:1||GaN:1||THIN:1||Electron beam:1||INTENSE:1||Hard Xray pulse generation:1||NONLINEAR THOMSON SCATTERING:1||MULTILAYER:1||UVvisible spectrometer:1||ATOMS:1||innershell transitions:1||CORRECTED CONCAVE GRATINGS:1||DISCHARGE:1||LASERPLASMA:1||thin film:1||reflectivity:1||opacity:1||gain:1||smallangle Xray scattering:1||SOFTXRAY:1||ZINCOXIDE:1||CYGNUSX3:1||Betatron oscillation:1||ACCELERATOR:1||STRAINEDLAYER SUPERLATTICES:1||OPTICAL PARAMETRIC AMPLIFICATION:1||PASSIVE MODELOCKING:1||Collision dynamics:1||MUM:1||EXACTEXCHANGE:1||BASISSET:1||APPROXIMATION:1||OXYNITRIDES:1||Beam energy modulation:1||polarization spectroscopy:1||REORIENTATION TRANSITION:1||DEPENDENCE:1||sulfurs:1||BUILDINGBLOCKS:1||RATES:1||OPTICAL PULSES:1||toroidal mirror:1||XRAY LASER:1||CALCIUM:1||radially polarized laser:1||GRAINBOUNDARIES:1||VAPORDEPOSITION:1||Xray generation:1||MAGNETIZATION:1||Electric excitation:1||Laserinduced gas plasmas:1||Qualitative analysis:1||SCHEME:1||RADIATION:10||PULSES:8||PHOTOLUMINESCENCE:7||LASER:7||GENERATION:6||NANORODS:6||GROWTH:6||NANOWIRES:5||IMPLANTED GAN:5||SPECTROSCOPY:5||THINFILMS:4||DYNAMICS:4||SILICON:4||EXTREMEULTRAVIOLET:4||AMPLIFICATION:4||PRESSURE:4||PHASE:4||OPTICALPROPERTIES:4||SYSTEM:4||EMISSION:4||FEL:3||N2O:3||FILMS:3||OPTICS:3||SPECTRA:3||FIELD:3||MIRRORS:3||ARRAYS:3||CLUSTERS:3||SIO2:3||IONIZATION:3||VACUUM:3||SCATTERING:3||IONS:2||LUMINESCENCE PROPERTIES:2||ANISOTROPY:2||BEAMS:2||DIFFRACTION:2||DISPERSION:2||chemical vapor deposition (CVD):2||ELECTRONICSTRUCTURE:2||MOSFETS:2||SI3N4:2||DENSITY:2||LIGHT:2||PLASMAS:2||MATTER:2||nanocomposites:2||RAMANSCATTERING:2||NANOPARTICLES:2||OXIDE:2||AMPLIFIED SPONTANEOUS EMISSION:2||NM WAVELENGTH:2||GAIN:2||CARBON NANOTUBES:2||CROSSSECTIONS:2||LIGHTEMITTINGDIODES:2||PULSE:2||CARBON PLASMA:2||TISAPPHIRE LASER:2||Raman scattering:2||ROUTE:2||multilayer:2||CATHODOLUMINESCENCE:2||highresolution transmission electronic microscope (HRTEM):2||DIFFERENCEFREQUENCYGENERATION:2||CRYSTAL:2||laserproduced plasma:2||NANOCABLES:2||photoluminescence:2||MAGNETIC ALLOY SEMICONDUCTORS:2||MOLECULARBEAM EPITAXY:2||EARTHDOPED GAN:2||LASER FIELDS:2||CHIRPEDPULSEAMPLIFICATION:2||ALN:2||GAUSSIANBEAM:2||ASSISTED CATALYTIC GROWTH:2||BLUE:2||NANOSTRUCTURES:2||MAGNETOELECTRONICS:2||MICROSCOPY:2||ELECTROLUMINESCENCE:2||LASERPULSES:2||GaN nanowires:2||GALLIUM NITRIDE NANOWIRES:2||GAMNN:2||NANOTUBES:2||PHYSICS:2||Femtosecond laser:2||parametric oscillators and amplifiers:1||ultrafast lasers:1||VALENCE:1||nanowires:1||DILUTED MAGNETIC SEMICONDUCTOR:1||LUMINESCENCE:1||Density modulation:1||Energy modulation:1||Current enhanced SASE free electron laser:1||Undulator radiation:1||FREEELECTRON LASERS:1||ULTRATHIN FERROMAGNETICFILMS:1||OXIDEFILMS:1||ABLATION:1||COMPONENT:1||METAL:1||innershell excited states:1||Nelike ions:1||TRANSITIONS:1||XUV spectrometer:1||DIAGNOSTICS:1||Xray scattering:1||MO/SI:1||pulsed laser deposition:1||KEV IMPACT ENERGIES:1||vacuum electron acceleration:1||HIGHINTENSITY LASER:1||JUNCTIONS:1||LOWTEMPERATURE GROWTH:1||nanocrystalline materials:1||MOLECULAR PHOTOIONIZATION:1||LOCALIZATION:1||DEUTERIUM CLUSTERS:1||EXPLOSIONS:1||REGENERATIVE AMPLIFIERS:1||RAREGASES:1||THz radiation:1||FREEELECTRON LASER:1||REALTIME OBSERVATION:1||TARGET:1||photoionized plasmas:1||fs Xray laser:1||emission profile:1||HIGHORDER HARMONICS:1||Xray laser:1||atomic transition:1||EXCITATION:1||LASERS:1||PERFORMANCE:1||RELATIVISTIC ELECTRONS:1||BI2O3DOPED ZNO:1||INNERSHELL IONIZATION:1||Laser wakefield:1||FREQUENCY:1||SOLIDSTATE LASERS:1||Linearly polarized:1||THERMIONIC EMISSION:1||PULSE AMPLIFICATION SYSTEM:1||BIB3O6:1||NM:1||NONCOVALENT INTERACTIONS:1||CRYSTALLINE:1||INTENSITY:1||JETS:1||COHERENT:1||LINE:1||ANGULARDISTRIBUTION:1||SILVER IONS:1||magnetic anisotropy:1||DEVICES:1||Auger transitions:1||CosterKronig transitions:1||EFFICIENT:1||ELECTRONIMPACT IONIZATION:1||ULTRASHORTPULSE:1||Nanowire:1||Heterostructure:1||soft Xray reflectivity:1||PLASMA ACCELERATOR:1||ZINCOXIDE NANOWIRES:1||CHEMICALVAPORDEPOSITION:1||Electron acceleration:1||Ionization of gases:1||Delay dependent:1||MULTIPHOTON IONIZATION:1||FRAGMENTATION:1||GASJET:1||ultrafast nonlinear optics:1||CYCLE PULSES:1||KHZ:1||chemical vapor deposition:1||ferromagnetism:1||ABSORPTION:1||TERAHERTZ RADIATION:1||SCIENCE:1||FIELDS:1||ELECTRONS:1||nanomultilayer structures:1||YIELDS:1||AUGER:1||10HZ REPETITION RATE:1||MULTITERAWATT:1||SPECTROGRAPH:1||HIGHHARMONICGENERATION:1||spectroscopy:1||level population:1||PARTICLEACCELERATION:1||OPTICAL FREQUENCYMEASUREMENT:1||NANOWALLS:1||ROOMTEMPERATURE:1||AVERAGE OUTPUT POWER:1||GROUPVELOCITYMISMATCH:1||Impact ionization:1||Dynamics:1||Lasers:1||Collisional process:1||ABOVETHRESHOLD IONIZATION:1||MAINGROUP THERMOCHEMISTRY:1||dilute magnetic semiconductors:1||GACRN:1||SIZE:1||ATTOSECOND:1||Ar cluster:1||Xray astrophysics:1||photoionization:1||irons:1||normal incidence pulsed laser deposition:1||SHELLS:1||Silicon Oxide:1||gaspuff Zpinch:1||Xray:1||soft Xray reflectors:1||ESCAPE:1||ZN2SIO4:1||SILICA:1||Time delay:1||Collisional plasmas:1||MASSSPECTROMETRY:1||NUCLEARFUSION:1||PARAMETRIC AMPLIFICATION:1||LYING ELECTRONIC STATES:1||ADJUSTABLEPARAMETERS:1||MAGNETICPROPERTIES:1||LIQUIDPHASE EPITAXY:1||CEP laser:1||REGION:1||Plasma waveguide:1||AMBIENT GAS:1||DEPOSITION:1||HARMONICGENERATION:1||ENHANCEMENT:1||imaging spectrometer:1||Abel inversion:1||Water window:1||Liquid nitrogen jet:1||CHARGEEXCHANGE:1||NOBEL LECTURE:1||VARISTOR:1||EPITAXY:1||THINDISK LASER:1||HIGHREPETITIONRATE:1||Atom lasers:1||Electronimpact excitation:1||High order harmonics:1||ultrafast technology:1||PEAK POWER:1||CHARGED ALUMINUM CLUSTERS:1||GaN:1||THIN:1||Electron beam:1||INTENSE:1||Hard Xray pulse generation:1||NONLINEAR THOMSON SCATTERING:1||MULTILAYER:1||UVvisible spectrometer:1||ATOMS:1||innershell transitions:1||CORRECTED CONCAVE GRATINGS:1||DISCHARGE:1||LASERPLASMA:1||thin film:1||reflectivity:1||opacity:1||gain:1||smallangle Xray scattering:1||SOFTXRAY:1||ZINCOXIDE:1||CYGNUSX3:1||Betatron oscillation:1||ACCELERATOR:1||STRAINEDLAYER SUPERLATTICES:1||OPTICAL PARAMETRIC AMPLIFICATION:1||PASSIVE MODELOCKING:1||Collision dynamics:1||MUM:1||EXACTEXCHANGE:1||BASISSET:1||APPROXIMATION:1||OXYNITRIDES:1||Beam energy modulation:1||polarization spectroscopy:1||REORIENTATION TRANSITION:1||DEPENDENCE:1||sulfurs:1||BUILDINGBLOCKS:1||RATES:1||OPTICAL PULSES:1||toroidal mirror:1||XRAY LASER:1||CALCIUM:1||radially polarized laser:1||GRAINBOUNDARIES:1||VAPORDEPOSITION:1||Xray generation:1||MAGNETIZATION:1||Electric excitation:1||Laserinduced gas plasmas:1||Qualitative analysis:1||SCHEME:1||RADIATION:10||PULSES:8||PHOTOLUMINESCENCE:7||LASER:7||GENERATION:6||NANORODS:6||GROWTH:6||NANOWIRES:5||IMPLANTED 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SEMICONDUCTORS:2||MOLECULARBEAM EPITAXY:2||EARTHDOPED GAN:2||LASER FIELDS:2||CHIRPEDPULSEAMPLIFICATION:2||ALN:2||GAUSSIANBEAM:2||ASSISTED CATALYTIC GROWTH:2||BLUE:2||NANOSTRUCTURES:2||MAGNETOELECTRONICS:2||MICROSCOPY:2||ELECTROLUMINESCENCE:2||LASERPULSES:2||GaN nanowires:2||GALLIUM NITRIDE NANOWIRES:2||GAMNN:2||NANOTUBES:2||PHYSICS:2||Femtosecond laser:2||parametric oscillators and amplifiers:1||ultrafast lasers:1||VALENCE:1||nanowires:1||DILUTED MAGNETIC SEMICONDUCTOR:1||LUMINESCENCE:1||Density modulation:1||Energy modulation:1||Current enhanced SASE free electron laser:1||Undulator radiation:1||FREEELECTRON LASERS:1||ULTRATHIN FERROMAGNETICFILMS:1||OXIDEFILMS:1||ABLATION:1||COMPONENT:1||METAL:1||innershell excited states:1||Nelike ions:1||TRANSITIONS:1||XUV spectrometer:1||DIAGNOSTICS:1||Xray scattering:1||MO/SI:1||pulsed laser deposition:1||KEV IMPACT ENERGIES:1||vacuum electron acceleration:1||HIGHINTENSITY LASER:1||JUNCTIONS:1||LOWTEMPERATURE GROWTH:1||nanocrystalline materials:1||MOLECULAR PHOTOIONIZATION:1||LOCALIZATION:1||DEUTERIUM CLUSTERS:1||EXPLOSIONS:1||REGENERATIVE AMPLIFIERS:1||RAREGASES:1||THz radiation:1||FREEELECTRON LASER:1||REALTIME OBSERVATION:1||TARGET:1||photoionized plasmas:1||fs Xray laser:1||emission profile:1||HIGHORDER HARMONICS:1||Xray laser:1||atomic transition:1||EXCITATION:1||LASERS:1||PERFORMANCE:1||RELATIVISTIC ELECTRONS:1||BI2O3DOPED ZNO:1||INNERSHELL IONIZATION:1||Laser wakefield:1||FREQUENCY:1||SOLIDSTATE LASERS:1||Linearly polarized:1||THERMIONIC EMISSION:1||PULSE AMPLIFICATION SYSTEM:1||BIB3O6:1||NM:1||NONCOVALENT INTERACTIONS:1||CRYSTALLINE:1||INTENSITY:1||JETS:1||COHERENT:1||LINE:1||ANGULARDISTRIBUTION:1||SILVER IONS:1||magnetic anisotropy:1||DEVICES:1||Auger transitions:1||CosterKronig transitions:1||EFFICIENT:1||ELECTRONIMPACT IONIZATION:1||ULTRASHORTPULSE:1||Nanowire:1||Heterostructure:1||soft Xray reflectivity:1||PLASMA ACCELERATOR:1||ZINCOXIDE NANOWIRES:1||CHEMICALVAPORDEPOSITION:1||Electron acceleration:1||Ionization of gases:1||Delay dependent:1||MULTIPHOTON IONIZATION:1||FRAGMENTATION:1||GASJET:1||ultrafast nonlinear optics:1||CYCLE PULSES:1||KHZ:1||chemical vapor deposition:1||ferromagnetism:1||ABSORPTION:1||TERAHERTZ RADIATION:1||SCIENCE:1||FIELDS:1||ELECTRONS:1||nanomultilayer structures:1||YIELDS:1||AUGER:1||10HZ REPETITION RATE:1||MULTITERAWATT:1||SPECTROGRAPH:1||HIGHHARMONICGENERATION:1||spectroscopy:1||level population:1||PARTICLEACCELERATION:1||OPTICAL FREQUENCYMEASUREMENT:1||NANOWALLS:1||ROOMTEMPERATURE:1||AVERAGE OUTPUT POWER:1||GROUPVELOCITYMISMATCH:1||Impact ionization:1||Dynamics:1||Lasers:1||Collisional process:1||ABOVETHRESHOLD IONIZATION:1||MAINGROUP THERMOCHEMISTRY:1||dilute magnetic semiconductors:1||GACRN:1||SIZE:1||ATTOSECOND:1||Ar cluster:1||Xray astrophysics:1||photoionization:1||irons:1||normal incidence pulsed laser deposition:1||SHELLS:1||Silicon Oxide:1||gaspuff Zpinch:1||Xray:1||soft Xray reflectors:1||ESCAPE:1||ZN2SIO4:1||SILICA:1||Time 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materials:1||MOLECULAR PHOTOIONIZATION:1||LOCALIZATION:1||DEUTERIUM CLUSTERS:1||EXPLOSIONS:1||REGENERATIVE AMPLIFIERS:1||RAREGASES:1||THz radiation:1||FREEELECTRON LASER:1||REALTIME OBSERVATION:1||TARGET:1||photoionized plasmas:1||fs Xray laser:1||emission profile:1||HIGHORDER HARMONICS:1||Xray laser:1||atomic transition:1||EXCITATION:1||LASERS:1||PERFORMANCE:1||RELATIVISTIC ELECTRONS:1||BI2O3DOPED ZNO:1||INNERSHELL IONIZATION:1||Laser wakefield:1||FREQUENCY:1||SOLIDSTATE LASERS:1||Linearly polarized:1||THERMIONIC EMISSION:1||PULSE AMPLIFICATION SYSTEM:1||BIB3O6:1||NM:1||NONCOVALENT INTERACTIONS:1||CRYSTALLINE:1||INTENSITY:1||JETS:1||COHERENT:1||LINE:1||ANGULARDISTRIBUTION:1||SILVER IONS:1||magnetic anisotropy:1||DEVICES:1||Auger transitions:1||CosterKronig transitions:1||EFFICIENT:1||ELECTRONIMPACT IONIZATION:1||ULTRASHORTPULSE:1||Nanowire:1||Heterostructure:1||soft Xray reflectivity:1||PLASMA ACCELERATOR:1||ZINCOXIDE NANOWIRES:1||CHEMICALVAPORDEPOSITION:1||Electron acceleration:1||Ionization of gases:1||Delay dependent:1||MULTIPHOTON IONIZATION:1||FRAGMENTATION:1||GASJET:1||ultrafast nonlinear optics:1||CYCLE PULSES:1||KHZ:1||chemical vapor deposition:1||ferromagnetism:1||ABSORPTION:1||TERAHERTZ RADIATION:1||SCIENCE:1||FIELDS:1||ELECTRONS:1||nanomultilayer structures:1||YIELDS:1||AUGER:1||10HZ REPETITION RATE:1||MULTITERAWATT:1||SPECTROGRAPH:1||HIGHHARMONICGENERATION:1||spectroscopy:1||level population:1||PARTICLEACCELERATION:1||OPTICAL FREQUENCYMEASUREMENT:1||NANOWALLS:1||ROOMTEMPERATURE:1||AVERAGE OUTPUT POWER:1||GROUPVELOCITYMISMATCH:1||Impact ionization:1||Dynamics:1||Lasers:1||Collisional process:1||ABOVETHRESHOLD IONIZATION:1||MAINGROUP THERMOCHEMISTRY:1||dilute magnetic semiconductors:1||GACRN:1||SIZE:1||ATTOSECOND:1||Ar cluster:1||Xray astrophysics:1||photoionization:1||irons:1||normal incidence pulsed laser deposition:1||SHELLS:1||Silicon Oxide:1||gaspuff Zpinch:1||Xray:1||soft Xray reflectors:1||ESCAPE:1||ZN2SIO4:1||SILICA:1||Time delay:1||Collisional plasmas:1||MASSSPECTROMETRY:1||NUCLEARFUSION:1||PARAMETRIC AMPLIFICATION:1||LYING ELECTRONIC STATES:1||ADJUSTABLEPARAMETERS:1||MAGNETICPROPERTIES:1||LIQUIDPHASE EPITAXY:1||CEP laser:1||REGION:1||Plasma waveguide:1||AMBIENT GAS:1||DEPOSITION:1||HARMONICGENERATION:1||ENHANCEMENT:1||imaging spectrometer:1||Abel inversion:1||Water window:1||Liquid nitrogen jet:1||CHARGEEXCHANGE:1||NOBEL LECTURE:1||VARISTOR:1||EPITAXY:1||THINDISK LASER:1||HIGHREPETITIONRATE:1||Atom lasers:1||Electronimpact excitation:1||High order harmonics:1||ultrafast technology:1||PEAK POWER:1||CHARGED ALUMINUM CLUSTERS:1||GaN:1||THIN:1||Electron beam:1||INTENSE:1||Hard Xray pulse generation:1||NONLINEAR THOMSON SCATTERING:1||MULTILAYER:1||UVvisible spectrometer:1||ATOMS:1||innershell transitions:1||CORRECTED CONCAVE GRATINGS:1||DISCHARGE:1||LASERPLASMA:1||thin film:1||reflectivity:1||opacity:1||gain:1||smallangle Xray scattering:1||SOFTXRAY:1||ZINCOXIDE:1||CYGNUSX3:1||Betatron oscillation:1||ACCELERATOR:1||STRAINEDLAYER SUPERLATTICES:1||OPTICAL PARAMETRIC AMPLIFICATION:1||PASSIVE MODELOCKING:1||Collision dynamics:1||MUM:1||EXACTEXCHANGE:1||BASISSET:1||APPROXIMATION:1||OXYNITRIDES:1||Beam energy modulation:1||polarization spectroscopy:1||REORIENTATION TRANSITION:1||DEPENDENCE:1||sulfurs:1||BUILDINGBLOCKS:1||RATES:1||OPTICAL PULSES:1||toroidal mirror:1||XRAY LASER:1||CALCIUM:1||radially polarized laser:1||GRAINBOUNDARIES:1||VAPORDEPOSITION:1||Xray generation:1||MAGNETIZATION:1||Electric excitation:1||Laserinduced gas plasmas:1||Qualitative analysis:1||SCHEME:1||RADIATION:10||PULSES:8||PHOTOLUMINESCENCE:7||LASER:7||GENERATION:6||NANORODS:6||GROWTH:6||NANOWIRES:5||IMPLANTED GAN:5||SPECTROSCOPY:5||THINFILMS:4||DYNAMICS:4||SILICON:4||EXTREMEULTRAVIOLET:4||AMPLIFICATION:4||PRESSURE:4||PHASE:4||OPTICALPROPERTIES:4||SYSTEM:4||EMISSION:4||FEL:3||N2O:3||FILMS:3||OPTICS:3||SPECTRA:3||FIELD:3||MIRRORS:3||ARRAYS:3||CLUSTERS:3||SIO2:3||IONIZATION:3||VACUUM:3||SCATTERING:3||IONS:2||LUMINESCENCE PROPERTIES:2||ANISOTROPY:2||BEAMS:2||DIFFRACTION:2||DISPERSION:2||chemical vapor deposition (CVD):2||ELECTRONICSTRUCTURE:2||MOSFETS:2||SI3N4:2||DENSITY:2||LIGHT:2||PLASMAS:2||MATTER:2||nanocomposites:2||RAMANSCATTERING:2||NANOPARTICLES:2||OXIDE:2||AMPLIFIED SPONTANEOUS EMISSION:2||NM WAVELENGTH:2||GAIN:2||CARBON NANOTUBES:2||CROSSSECTIONS:2||LIGHTEMITTINGDIODES:2||PULSE:2||CARBON PLASMA:2||TISAPPHIRE LASER:2||Raman scattering:2||ROUTE:2||multilayer:2||CATHODOLUMINESCENCE:2||highresolution transmission electronic microscope (HRTEM):2||DIFFERENCEFREQUENCYGENERATION:2||CRYSTAL:2||laserproduced plasma:2||NANOCABLES:2||photoluminescence:2||MAGNETIC ALLOY SEMICONDUCTORS:2||MOLECULARBEAM EPITAXY:2||EARTHDOPED GAN:2||LASER FIELDS:2||CHIRPEDPULSEAMPLIFICATION:2||ALN:2||GAUSSIANBEAM:2||ASSISTED CATALYTIC GROWTH:2||BLUE:2||NANOSTRUCTURES:2||MAGNETOELECTRONICS:2||MICROSCOPY:2||ELECTROLUMINESCENCE:2||LASERPULSES:2||GaN nanowires:2||GALLIUM NITRIDE NANOWIRES:2||GAMNN:2||NANOTUBES:2||PHYSICS:2||Femtosecond laser:2||parametric oscillators and amplifiers:1||ultrafast lasers:1||VALENCE:1||nanowires:1||DILUTED MAGNETIC SEMICONDUCTOR:1||LUMINESCENCE:1||Density modulation:1||Energy modulation:1||Current enhanced SASE free electron laser:1||Undulator radiation:1||FREEELECTRON LASERS:1||ULTRATHIN FERROMAGNETICFILMS:1||OXIDEFILMS:1||ABLATION:1||COMPONENT:1||METAL:1||innershell excited states:1||Nelike ions:1||TRANSITIONS:1||XUV spectrometer:1||DIAGNOSTICS:1||Xray scattering:1||MO/SI:1||pulsed laser deposition:1||KEV IMPACT ENERGIES:1||vacuum electron acceleration:1||HIGHINTENSITY LASER:1||JUNCTIONS:1||LOWTEMPERATURE GROWTH:1||nanocrystalline materials:1||MOLECULAR PHOTOIONIZATION:1||LOCALIZATION:1||DEUTERIUM CLUSTERS:1||EXPLOSIONS:1||REGENERATIVE AMPLIFIERS:1||RAREGASES:1||THz radiation:1||FREEELECTRON LASER:1||REALTIME OBSERVATION:1||TARGET:1||photoionized plasmas:1||fs Xray laser:1||emission profile:1||HIGHORDER HARMONICS:1||Xray laser:1||atomic transition:1||EXCITATION:1||LASERS:1||PERFORMANCE:1||RELATIVISTIC ELECTRONS:1||BI2O3DOPED ZNO:1||INNERSHELL IONIZATION:1||Laser wakefield:1||FREQUENCY:1||SOLIDSTATE LASERS:1||Linearly polarized:1||THERMIONIC EMISSION:1||PULSE AMPLIFICATION SYSTEM:1||BIB3O6:1||NM:1||NONCOVALENT INTERACTIONS:1||CRYSTALLINE:1||INTENSITY:1||JETS:1||COHERENT:1||LINE:1||ANGULARDISTRIBUTION:1||SILVER IONS:1||magnetic anisotropy:1||DEVICES:1||Auger transitions:1||CosterKronig transitions:1||EFFICIENT:1||ELECTRONIMPACT IONIZATION:1||ULTRASHORTPULSE:1||Nanowire:1||Heterostructure:1||soft Xray reflectivity:1||PLASMA ACCELERATOR:1||ZINCOXIDE NANOWIRES:1||CHEMICALVAPORDEPOSITION:1||Electron acceleration:1||Ionization of gases:1||Delay dependent:1||MULTIPHOTON IONIZATION:1||FRAGMENTATION:1||GASJET:1||ultrafast nonlinear optics:1||CYCLE PULSES:1||KHZ:1||chemical vapor deposition:1||ferromagnetism:1||ABSORPTION:1||TERAHERTZ RADIATION:1||SCIENCE:1||FIELDS:1||ELECTRONS:1||nanomultilayer structures:1||YIELDS:1||AUGER:1||10HZ REPETITION RATE:1||MULTITERAWATT:1||SPECTROGRAPH:1||HIGHHARMONICGENERATION:1||spectroscopy:1||level population:1||PARTICLEACCELERATION:1||OPTICAL FREQUENCYMEASUREMENT:1||NANOWALLS:1||ROOMTEMPERATURE:1||AVERAGE OUTPUT POWER:1||GROUPVELOCITYMISMATCH:1||Impact ionization:1||Dynamics:1||Lasers:1||Collisional process:1||ABOVETHRESHOLD IONIZATION:1||MAINGROUP THERMOCHEMISTRY:1||dilute magnetic semiconductors:1||GACRN:1||SIZE:1||ATTOSECOND:1||Ar cluster:1||Xray astrophysics:1||photoionization:1||irons:1||normal incidence pulsed laser deposition:1||SHELLS:1||Silicon Oxide:1||gaspuff Zpinch:1||Xray:1||soft Xray reflectors:1||ESCAPE:1||ZN2SIO4:1||SILICA:1||Time delay:1||Collisional plasmas:1||MASSSPECTROMETRY:1||NUCLEARFUSION:1||PARAMETRIC AMPLIFICATION:1||LYING ELECTRONIC STATES:1||ADJUSTABLEPARAMETERS:1||MAGNETICPROPERTIES:1||LIQUIDPHASE EPITAXY:1||CEP laser:1||REGION:1||Plasma waveguide:1||AMBIENT GAS:1||DEPOSITION:1||HARMONICGENERATION:1||ENHANCEMENT:1||imaging spectrometer:1||Abel inversion:1||Water window:1||Liquid nitrogen jet:1||CHARGEEXCHANGE:1||NOBEL LECTURE:1||VARISTOR:1||EPITAXY:1||THINDISK LASER:1||HIGHREPETITIONRATE:1||Atom lasers:1||Electronimpact excitation:1||High order harmonics:1||ultrafast technology:1||PEAK POWER:1||CHARGED ALUMINUM CLUSTERS:1||GaN:1||THIN:1||Electron beam:1||INTENSE:1||Hard Xray pulse generation:1||NONLINEAR THOMSON SCATTERING:1||MULTILAYER:1||UVvisible spectrometer:1||ATOMS:1||innershell transitions:1||CORRECTED CONCAVE GRATINGS:1||DISCHARGE:1||LASERPLASMA:1||thin film:1||reflectivity:1||opacity:1||gain:1||smallangle Xray scattering:1||SOFTXRAY:1||ZINCOXIDE:1||CYGNUSX3:1||Betatron oscillation:1||ACCELERATOR:1||STRAINEDLAYER SUPERLATTICES:1||OPTICAL PARAMETRIC AMPLIFICATION:1||PASSIVE MODELOCKING:1||Collision dynamics:1||MUM:1||EXACTEXCHANGE:1||BASISSET:1||APPROXIMATION:1||OXYNITRIDES:1||Beam energy modulation:1||polarization spectroscopy:1||REORIENTATION TRANSITION:1||DEPENDENCE:1||sulfurs:1||BUILDINGBLOCKS:1||RATES:1||OPTICAL PULSES:1||toroidal mirror:1||XRAY LASER:1||CALCIUM:1||radially polarized laser:1||GRAINBOUNDARIES:1||VAPORDEPOSITION:1||Xray generation:1||MAGNETIZATION:1||Electric excitation:1||Laserinduced gas plasmas:1||Qualitative analysis:1||SCHEME:1||RADIATION:10||PULSES:8||PHOTOLUMINESCENCE:7||LASER:7||GENERATION:6||NANORODS:6||GROWTH:6||NANOWIRES:5||IMPLANTED 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SEMICONDUCTORS:2||MOLECULARBEAM EPITAXY:2||EARTHDOPED GAN:2||LASER FIELDS:2||CHIRPEDPULSEAMPLIFICATION:2||ALN:2||GAUSSIANBEAM:2||ASSISTED CATALYTIC GROWTH:2||BLUE:2||NANOSTRUCTURES:2||MAGNETOELECTRONICS:2||MICROSCOPY:2||ELECTROLUMINESCENCE:2||LASERPULSES:2||GaN nanowires:2||GALLIUM NITRIDE NANOWIRES:2||GAMNN:2||NANOTUBES:2||PHYSICS:2||Femtosecond laser:2||parametric oscillators and amplifiers:1||ultrafast lasers:1||VALENCE:1||nanowires:1||DILUTED MAGNETIC SEMICONDUCTOR:1||LUMINESCENCE:1||Density modulation:1||Energy modulation:1||Current enhanced SASE free electron laser:1||Undulator radiation:1||FREEELECTRON LASERS:1||ULTRATHIN FERROMAGNETICFILMS:1||OXIDEFILMS:1||ABLATION:1||COMPONENT:1||METAL:1||innershell excited states:1||Nelike ions:1||TRANSITIONS:1||XUV spectrometer:1||DIAGNOSTICS:1||Xray scattering:1||MO/SI:1||pulsed laser deposition:1||KEV IMPACT ENERGIES:1||vacuum electron acceleration:1||HIGHINTENSITY LASER:1||JUNCTIONS:1||LOWTEMPERATURE GROWTH:1||nanocrystalline materials:1||MOLECULAR PHOTOIONIZATION:1||LOCALIZATION:1||DEUTERIUM CLUSTERS:1||EXPLOSIONS:1||REGENERATIVE AMPLIFIERS:1||RAREGASES:1||THz radiation:1||FREEELECTRON LASER:1||REALTIME OBSERVATION:1||TARGET:1||photoionized plasmas:1||fs Xray laser:1||emission profile:1||HIGHORDER HARMONICS:1||Xray laser:1||atomic transition:1||EXCITATION:1||LASERS:1||PERFORMANCE:1||RELATIVISTIC ELECTRONS:1||BI2O3DOPED ZNO:1||INNERSHELL IONIZATION:1||Laser wakefield:1||FREQUENCY:1||SOLIDSTATE LASERS:1||Linearly polarized:1||THERMIONIC EMISSION:1||PULSE AMPLIFICATION SYSTEM:1||BIB3O6:1||NM:1||NONCOVALENT INTERACTIONS:1||CRYSTALLINE:1||INTENSITY:1||JETS:1||COHERENT:1||LINE:1||ANGULARDISTRIBUTION:1||SILVER IONS:1||magnetic anisotropy:1||DEVICES:1||Auger transitions:1||CosterKronig transitions:1||EFFICIENT:1||ELECTRONIMPACT IONIZATION:1||ULTRASHORTPULSE:1||Nanowire:1||Heterostructure:1||soft Xray reflectivity:1||PLASMA ACCELERATOR:1||ZINCOXIDE NANOWIRES:1||CHEMICALVAPORDEPOSITION:1||Electron acceleration:1||Ionization of gases:1||Delay dependent:1||MULTIPHOTON IONIZATION:1||FRAGMENTATION:1||GASJET:1||ultrafast nonlinear optics:1||CYCLE PULSES:1||KHZ:1||chemical vapor deposition:1||ferromagnetism:1||ABSORPTION:1||TERAHERTZ RADIATION:1||SCIENCE:1||FIELDS:1||ELECTRONS:1||nanomultilayer structures:1||YIELDS:1||AUGER:1||10HZ REPETITION RATE:1||MULTITERAWATT:1||SPECTROGRAPH:1||HIGHHARMONICGENERATION:1||spectroscopy:1||level population:1||PARTICLEACCELERATION:1||OPTICAL FREQUENCYMEASUREMENT:1||NANOWALLS:1||ROOMTEMPERATURE:1||AVERAGE OUTPUT POWER:1||GROUPVELOCITYMISMATCH:1||Impact ionization:1||Dynamics:1||Lasers:1||Collisional process:1||ABOVETHRESHOLD IONIZATION:1||MAINGROUP THERMOCHEMISTRY:1||dilute magnetic semiconductors:1||GACRN:1||SIZE:1||ATTOSECOND:1||Ar cluster:1||Xray astrophysics:1||photoionization:1||irons:1||normal incidence pulsed laser deposition:1||SHELLS:1||Silicon Oxide:1||gaspuff Zpinch:1||Xray:1||soft Xray reflectors:1||ESCAPE:1||ZN2SIO4:1||SILICA:1||Time 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materials:1||MOLECULAR PHOTOIONIZATION:1||LOCALIZATION:1||DEUTERIUM CLUSTERS:1||EXPLOSIONS:1||REGENERATIVE AMPLIFIERS:1||RAREGASES:1||THz radiation:1||FREEELECTRON LASER:1||REALTIME OBSERVATION:1||TARGET:1||photoionized plasmas:1||fs Xray laser:1||emission profile:1||HIGHORDER HARMONICS:1||Xray laser:1||atomic transition:1||EXCITATION:1||LASERS:1||PERFORMANCE:1||RELATIVISTIC ELECTRONS:1||BI2O3DOPED ZNO:1||INNERSHELL IONIZATION:1||Laser wakefield:1||FREQUENCY:1||SOLIDSTATE LASERS:1||Linearly polarized:1||THERMIONIC EMISSION:1||PULSE AMPLIFICATION SYSTEM:1||BIB3O6:1||NM:1||NONCOVALENT INTERACTIONS:1||CRYSTALLINE:1||INTENSITY:1||JETS:1||COHERENT:1||LINE:1||ANGULARDISTRIBUTION:1||SILVER IONS:1||magnetic anisotropy:1||DEVICES:1||Auger transitions:1||CosterKronig transitions:1||EFFICIENT:1||ELECTRONIMPACT IONIZATION:1||ULTRASHORTPULSE:1||Nanowire:1||Heterostructure:1||soft Xray reflectivity:1||PLASMA ACCELERATOR:1||ZINCOXIDE NANOWIRES:1||CHEMICALVAPORDEPOSITION:1||Electron acceleration:1||Ionization of gases:1||Delay dependent:1||MULTIPHOTON IONIZATION:1||FRAGMENTATION:1||GASJET:1||ultrafast nonlinear optics:1||CYCLE PULSES:1||KHZ:1||chemical vapor deposition:1||ferromagnetism:1||ABSORPTION:1||TERAHERTZ RADIATION:1||SCIENCE:1||FIELDS:1||ELECTRONS:1||nanomultilayer structures:1||YIELDS:1||AUGER:1||10HZ REPETITION RATE:1||MULTITERAWATT:1||SPECTROGRAPH:1||HIGHHARMONICGENERATION:1||spectroscopy:1||level population:1||PARTICLEACCELERATION:1||OPTICAL FREQUENCYMEASUREMENT:1||NANOWALLS:1||ROOMTEMPERATURE:1||AVERAGE OUTPUT POWER:1||GROUPVELOCITYMISMATCH:1||Impact ionization:1||Dynamics:1||Lasers:1||Collisional process:1||ABOVETHRESHOLD IONIZATION:1||MAINGROUP THERMOCHEMISTRY:1||dilute magnetic semiconductors:1||GACRN:1||SIZE:1||ATTOSECOND:1||Ar cluster:1||Xray astrophysics:1||photoionization:1||irons:1||normal incidence pulsed laser deposition:1||SHELLS:1||Silicon Oxide:1||gaspuff Zpinch:1||Xray:1||soft Xray reflectors:1||ESCAPE:1||ZN2SIO4:1||SILICA:1||Time delay:1||Collisional plasmas:1||MASSSPECTROMETRY:1||NUCLEARFUSION:1||PARAMETRIC AMPLIFICATION:1||LYING ELECTRONIC STATES:1||ADJUSTABLEPARAMETERS:1||MAGNETICPROPERTIES:1||LIQUIDPHASE EPITAXY:1||CEP laser:1||REGION:1||Plasma waveguide:1||AMBIENT GAS:1||DEPOSITION:1||HARMONICGENERATION:1||ENHANCEMENT:1||imaging spectrometer:1||Abel inversion:1||Water window:1||Liquid nitrogen jet:1||CHARGEEXCHANGE:1||NOBEL LECTURE:1||VARISTOR:1||EPITAXY:1||THINDISK LASER:1||HIGHREPETITIONRATE:1||Atom lasers:1||Electronimpact excitation:1||High order harmonics:1||ultrafast technology:1||PEAK POWER:1||CHARGED ALUMINUM CLUSTERS:1||GaN:1||THIN:1||Electron beam:1||INTENSE:1||Hard Xray pulse generation:1||NONLINEAR THOMSON SCATTERING:1||MULTILAYER:1||UVvisible spectrometer:1||ATOMS:1||innershell transitions:1||CORRECTED CONCAVE GRATINGS:1||DISCHARGE:1||LASERPLASMA:1||thin film:1||reflectivity:1||opacity:1||gain:1||smallangle Xray scattering:1||SOFTXRAY:1||ZINCOXIDE:1||CYGNUSX3:1||Betatron oscillation:1||ACCELERATOR:1||STRAINEDLAYER SUPERLATTICES:1||OPTICAL PARAMETRIC AMPLIFICATION:1||PASSIVE MODELOCKING:1||Collision dynamics:1||MUM:1||EXACTEXCHANGE:1||BASISSET:1||APPROXIMATION:1||OXYNITRIDES:1||Beam energy modulation:1||polarization spectroscopy:1||REORIENTATION TRANSITION:1||DEPENDENCE:1||sulfurs:1||BUILDINGBLOCKS:1||RATES:1||OPTICAL PULSES:1||toroidal mirror:1||XRAY LASER:1||CALCIUM:1||radially polarized laser:1||GRAINBOUNDARIES:1||VAPORDEPOSITION:1||Xray generation:1||MAGNETIZATION:1||Electric excitation:1||Laserinduced gas plasmas:1||Qualitative analysis:1||SCHEME:1||RADIATION:10||PULSES:8||PHOTOLUMINESCENCE:7||LASER:7||GENERATION:6||NANORODS:6||GROWTH:6||NANOWIRES:5||IMPLANTED GAN:5||SPECTROSCOPY:5||THINFILMS:4||DYNAMICS:4||SILICON:4||EXTREMEULTRAVIOLET:4||AMPLIFICATION:4||PRESSURE:4||PHASE:4||OPTICALPROPERTIES:4||SYSTEM:4||EMISSION:4||FEL:3||N2O:3||FILMS:3||OPTICS:3||SPECTRA:3||FIELD:3||MIRRORS:3||ARRAYS:3||CLUSTERS:3||SIO2:3||IONIZATION:3||VACUUM:3||SCATTERING:3||IONS:2||LUMINESCENCE PROPERTIES:2||ANISOTROPY:2||BEAMS:2||DIFFRACTION:2||DISPERSION:2||chemical vapor deposition (CVD):2||ELECTRONICSTRUCTURE:2||MOSFETS:2||SI3N4:2||DENSITY:2||LIGHT:2||PLASMAS:2||MATTER:2||nanocomposites:2||RAMANSCATTERING:2||NANOPARTICLES:2||OXIDE:2||AMPLIFIED SPONTANEOUS EMISSION:2||NM WAVELENGTH:2||GAIN:2||CARBON NANOTUBES:2||CROSSSECTIONS:2||LIGHTEMITTINGDIODES:2||PULSE:2||CARBON PLASMA:2||TISAPPHIRE LASER:2||Raman scattering:2||ROUTE:2||multilayer:2||CATHODOLUMINESCENCE:2||highresolution transmission electronic microscope (HRTEM):2||DIFFERENCEFREQUENCYGENERATION:2||CRYSTAL:2||laserproduced plasma:2||NANOCABLES:2||photoluminescence:2||MAGNETIC ALLOY SEMICONDUCTORS:2||MOLECULARBEAM EPITAXY:2||EARTHDOPED GAN:2||LASER FIELDS:2||CHIRPEDPULSEAMPLIFICATION:2||ALN:2||GAUSSIANBEAM:2||ASSISTED CATALYTIC GROWTH:2||BLUE:2||NANOSTRUCTURES:2||MAGNETOELECTRONICS:2||MICROSCOPY:2||ELECTROLUMINESCENCE:2||LASERPULSES:2||GaN nanowires:2||GALLIUM NITRIDE NANOWIRES:2||GAMNN:2||NANOTUBES:2||PHYSICS:2||Femtosecond laser:2||parametric oscillators and amplifiers:1||ultrafast lasers:1||VALENCE:1||nanowires:1||DILUTED MAGNETIC SEMICONDUCTOR:1||LUMINESCENCE:1||Density modulation:1||Energy modulation:1||Current enhanced SASE free electron laser:1||Undulator radiation:1||FREEELECTRON LASERS:1||ULTRATHIN FERROMAGNETICFILMS:1||OXIDEFILMS:1||ABLATION:1||COMPONENT:1||METAL:1||innershell excited states:1||Nelike ions:1||TRANSITIONS:1||XUV spectrometer:1||DIAGNOSTICS:1||Xray scattering:1||MO/SI:1||pulsed laser deposition:1||KEV IMPACT ENERGIES:1||vacuum electron acceleration:1||HIGHINTENSITY LASER:1||JUNCTIONS:1||LOWTEMPERATURE GROWTH:1||nanocrystalline materials:1||MOLECULAR PHOTOIONIZATION:1||LOCALIZATION:1||DEUTERIUM CLUSTERS:1||EXPLOSIONS:1||REGENERATIVE AMPLIFIERS:1||RAREGASES:1||THz radiation:1||FREEELECTRON LASER:1||REALTIME OBSERVATION:1||TARGET:1||photoionized plasmas:1||fs Xray laser:1||emission profile:1||HIGHORDER HARMONICS:1||Xray laser:1||atomic transition:1||EXCITATION:1||LASERS:1||PERFORMANCE:1||RELATIVISTIC ELECTRONS:1||BI2O3DOPED ZNO:1||INNERSHELL IONIZATION:1||Laser wakefield:1||FREQUENCY:1||SOLIDSTATE LASERS:1||Linearly polarized:1||THERMIONIC EMISSION:1||PULSE AMPLIFICATION SYSTEM:1||BIB3O6:1||NM:1||NONCOVALENT INTERACTIONS:1||CRYSTALLINE:1||INTENSITY:1||JETS:1||COHERENT:1||LINE:1||ANGULARDISTRIBUTION:1||SILVER IONS:1||magnetic anisotropy:1||DEVICES:1||Auger transitions:1||CosterKronig transitions:1||EFFICIENT:1||ELECTRONIMPACT IONIZATION:1||ULTRASHORTPULSE:1||Nanowire:1||Heterostructure:1||soft Xray reflectivity:1||PLASMA ACCELERATOR:1||ZINCOXIDE NANOWIRES:1||CHEMICALVAPORDEPOSITION:1||Electron acceleration:1||Ionization of gases:1||Delay dependent:1||MULTIPHOTON IONIZATION:1||FRAGMENTATION:1||GASJET:1||ultrafast nonlinear optics:1||CYCLE PULSES:1||KHZ:1||chemical vapor deposition:1||ferromagnetism:1||ABSORPTION:1||TERAHERTZ RADIATION:1||SCIENCE:1||FIELDS:1||ELECTRONS:1||nanomultilayer structures:1||YIELDS:1||AUGER:1||10HZ REPETITION RATE:1||MULTITERAWATT:1||SPECTROGRAPH:1||HIGHHARMONICGENERATION:1||spectroscopy:1||level population:1||PARTICLEACCELERATION:1||OPTICAL FREQUENCYMEASUREMENT:1||NANOWALLS:1||ROOMTEMPERATURE:1||AVERAGE OUTPUT POWER:1||GROUPVELOCITYMISMATCH:1||Impact ionization:1||Dynamics:1||Lasers:1||Collisional process:1||ABOVETHRESHOLD IONIZATION:1||MAINGROUP THERMOCHEMISTRY:1||dilute magnetic semiconductors:1||GACRN:1||SIZE:1||ATTOSECOND:1||Ar cluster:1||Xray astrophysics:1||photoionization:1||irons:1||normal incidence pulsed laser deposition:1||SHELLS:1||Silicon Oxide:1||gaspuff Zpinch:1||Xray:1||soft Xray reflectors:1||ESCAPE:1||ZN2SIO4:1||SILICA:1||Time delay:1||Collisional plasmas:1||MASSSPECTROMETRY:1||NUCLEARFUSION:1||PARAMETRIC AMPLIFICATION:1||LYING ELECTRONIC STATES:1||ADJUSTABLEPARAMETERS:1||MAGNETICPROPERTIES:1||LIQUIDPHASE EPITAXY:1||CEP laser:1||REGION:1||Plasma waveguide:1||AMBIENT GAS:1||DEPOSITION:1||HARMONICGENERATION:1||ENHANCEMENT:1||imaging spectrometer:1||Abel inversion:1||Water window:1||Liquid nitrogen jet:1||CHARGEEXCHANGE:1||NOBEL LECTURE:1||VARISTOR:1||EPITAXY:1||THINDISK LASER:1||HIGHREPETITIONRATE:1||Atom lasers:1||Electronimpact excitation:1||High order harmonics:1||ultrafast technology:1||PEAK POWER:1||CHARGED ALUMINUM CLUSTERS:1||GaN:1||THIN:1||Electron beam:1||INTENSE:1||Hard Xray pulse generation:1||NONLINEAR THOMSON SCATTERING:1||MULTILAYER:1||UVvisible spectrometer:1||ATOMS:1||innershell transitions:1||CORRECTED CONCAVE GRATINGS:1||DISCHARGE:1||LASERPLASMA:1||thin film:1||reflectivity:1||opacity:1||gain:1||smallangle Xray scattering:1||SOFTXRAY:1||ZINCOXIDE:1||CYGNUSX3:1||Betatron oscillation:1||ACCELERATOR:1||STRAINEDLAYER SUPERLATTICES:1||OPTICAL PARAMETRIC AMPLIFICATION:1||PASSIVE MODELOCKING:1||Collision dynamics:1||MUM:1||EXACTEXCHANGE:1||BASISSET:1||APPROXIMATION:1||OXYNITRIDES:1||Beam energy modulation:1||polarization spectroscopy:1||REORIENTATION TRANSITION:1||DEPENDENCE:1||sulfurs:1||BUILDINGBLOCKS:1||RATES:1||OPTICAL PULSES:1||toroidal mirror:1||XRAY LASER:1||CALCIUM:1||radially polarized laser:1||GRAINBOUNDARIES:1||VAPORDEPOSITION:1||Xray generation:1||MAGNETIZATION:1||Electric excitation:1||Laserinduced gas plasmas:1||Qualitative analysis:1||SCHEME:1||RADIATION:10||PULSES:8||PHOTOLUMINESCENCE:7||LASER:7||GENERATION:6||NANORODS:6||GROWTH:6||NANOWIRES:5||IMPLANTED 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SEMICONDUCTORS:2||MOLECULARBEAM EPITAXY:2||EARTHDOPED GAN:2||LASER FIELDS:2||CHIRPEDPULSEAMPLIFICATION:2||ALN:2||GAUSSIANBEAM:2||ASSISTED CATALYTIC GROWTH:2||BLUE:2||NANOSTRUCTURES:2||MAGNETOELECTRONICS:2||MICROSCOPY:2||ELECTROLUMINESCENCE:2||LASERPULSES:2||GaN nanowires:2||GALLIUM NITRIDE NANOWIRES:2||GAMNN:2||NANOTUBES:2||PHYSICS:2||Femtosecond laser:2||parametric oscillators and amplifiers:1||ultrafast lasers:1||VALENCE:1||nanowires:1||DILUTED MAGNETIC SEMICONDUCTOR:1||LUMINESCENCE:1||Density modulation:1||Energy modulation:1||Current enhanced SASE free electron laser:1||Undulator radiation:1||FREEELECTRON LASERS:1||ULTRATHIN FERROMAGNETICFILMS:1||OXIDEFILMS:1||ABLATION:1||COMPONENT:1||METAL:1||innershell excited states:1||Nelike ions:1||TRANSITIONS:1||XUV spectrometer:1||DIAGNOSTICS:1||Xray scattering:1||MO/SI:1||pulsed laser deposition:1||KEV IMPACT ENERGIES:1||vacuum electron acceleration:1||HIGHINTENSITY LASER:1||JUNCTIONS:1||LOWTEMPERATURE GROWTH:1||nanocrystalline materials:1||MOLECULAR PHOTOIONIZATION:1||LOCALIZATION:1||DEUTERIUM CLUSTERS:1||EXPLOSIONS:1||REGENERATIVE AMPLIFIERS:1||RAREGASES:1||THz radiation:1||FREEELECTRON LASER:1||REALTIME OBSERVATION:1||TARGET:1||photoionized plasmas:1||fs Xray laser:1||emission profile:1||HIGHORDER HARMONICS:1||Xray laser:1||atomic transition:1||EXCITATION:1||LASERS:1||PERFORMANCE:1||RELATIVISTIC ELECTRONS:1||BI2O3DOPED ZNO:1||INNERSHELL IONIZATION:1||Laser wakefield:1||FREQUENCY:1||SOLIDSTATE LASERS:1||Linearly polarized:1||THERMIONIC EMISSION:1||PULSE AMPLIFICATION SYSTEM:1||BIB3O6:1||NM:1||NONCOVALENT INTERACTIONS:1||CRYSTALLINE:1||INTENSITY:1||JETS:1||COHERENT:1||LINE:1||ANGULARDISTRIBUTION:1||SILVER IONS:1||magnetic anisotropy:1||DEVICES:1||Auger transitions:1||CosterKronig transitions:1||EFFICIENT:1||ELECTRONIMPACT IONIZATION:1||ULTRASHORTPULSE:1||Nanowire:1||Heterostructure:1||soft Xray reflectivity:1||PLASMA ACCELERATOR:1||ZINCOXIDE NANOWIRES:1||CHEMICALVAPORDEPOSITION:1||Electron acceleration:1||Ionization of gases:1||Delay dependent:1||MULTIPHOTON IONIZATION:1||FRAGMENTATION:1||GASJET:1||ultrafast nonlinear optics:1||CYCLE PULSES:1||KHZ:1||chemical vapor deposition:1||ferromagnetism:1||ABSORPTION:1||TERAHERTZ RADIATION:1||SCIENCE:1||FIELDS:1||ELECTRONS:1||nanomultilayer structures:1||YIELDS:1||AUGER:1||10HZ REPETITION RATE:1||MULTITERAWATT:1||SPECTROGRAPH:1||HIGHHARMONICGENERATION:1||spectroscopy:1||level population:1||PARTICLEACCELERATION:1||OPTICAL FREQUENCYMEASUREMENT:1||NANOWALLS:1||ROOMTEMPERATURE:1||AVERAGE OUTPUT POWER:1||GROUPVELOCITYMISMATCH:1||Impact ionization:1||Dynamics:1||Lasers:1||Collisional process:1||ABOVETHRESHOLD IONIZATION:1||MAINGROUP THERMOCHEMISTRY:1||dilute magnetic semiconductors:1||GACRN:1||SIZE:1||ATTOSECOND:1||Ar cluster:1||Xray astrophysics:1||photoionization:1||irons:1||normal incidence pulsed laser deposition:1||SHELLS:1||Silicon Oxide:1||gaspuff Zpinch:1||Xray:1||soft Xray reflectors:1||ESCAPE:1||ZN2SIO4:1||SILICA:1||Time 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materials:1||MOLECULAR PHOTOIONIZATION:1||LOCALIZATION:1||DEUTERIUM CLUSTERS:1||EXPLOSIONS:1||REGENERATIVE AMPLIFIERS:1||RAREGASES:1||THz radiation:1||FREEELECTRON LASER:1||REALTIME OBSERVATION:1||TARGET:1||photoionized plasmas:1||fs Xray laser:1||emission profile:1||HIGHORDER HARMONICS:1||Xray laser:1||atomic transition:1||EXCITATION:1||LASERS:1||PERFORMANCE:1||RELATIVISTIC ELECTRONS:1||BI2O3DOPED ZNO:1||INNERSHELL IONIZATION:1||Laser wakefield:1||FREQUENCY:1||SOLIDSTATE LASERS:1||Linearly polarized:1||THERMIONIC EMISSION:1||PULSE AMPLIFICATION SYSTEM:1||BIB3O6:1||NM:1||NONCOVALENT INTERACTIONS:1||CRYSTALLINE:1||INTENSITY:1||JETS:1||COHERENT:1||LINE:1||ANGULARDISTRIBUTION:1||SILVER IONS:1||magnetic anisotropy:1||DEVICES:1||Auger transitions:1||CosterKronig transitions:1||EFFICIENT:1||ELECTRONIMPACT IONIZATION:1||ULTRASHORTPULSE:1||Nanowire:1||Heterostructure:1||soft Xray reflectivity:1||PLASMA ACCELERATOR:1||ZINCOXIDE NANOWIRES:1||CHEMICALVAPORDEPOSITION:1||Electron acceleration:1||Ionization of gases:1||Delay dependent:1||MULTIPHOTON IONIZATION:1||FRAGMENTATION:1||GASJET:1||ultrafast nonlinear optics:1||CYCLE PULSES:1||KHZ:1||chemical vapor deposition:1||ferromagnetism:1||ABSORPTION:1||TERAHERTZ RADIATION:1||SCIENCE:1||FIELDS:1||ELECTRONS:1||nanomultilayer structures:1||YIELDS:1||AUGER:1||10HZ REPETITION RATE:1||MULTITERAWATT:1||SPECTROGRAPH:1||HIGHHARMONICGENERATION:1||spectroscopy:1||level population:1||PARTICLEACCELERATION:1||OPTICAL FREQUENCYMEASUREMENT:1||NANOWALLS:1||ROOMTEMPERATURE:1||AVERAGE OUTPUT POWER:1||GROUPVELOCITYMISMATCH:1||Impact ionization:1||Dynamics:1||Lasers:1||Collisional process:1||ABOVETHRESHOLD IONIZATION:1||MAINGROUP THERMOCHEMISTRY:1||dilute magnetic semiconductors:1||GACRN:1||SIZE:1||ATTOSECOND:1||Ar cluster:1||Xray astrophysics:1||photoionization:1||irons:1||normal incidence pulsed laser deposition:1||SHELLS:1||Silicon Oxide:1||gaspuff Zpinch:1||Xray:1||soft Xray reflectors:1||ESCAPE:1||ZN2SIO4:1||SILICA:1||Time delay:1||Collisional plasmas:1||MASSSPECTROMETRY:1||NUCLEARFUSION:1||PARAMETRIC AMPLIFICATION:1||LYING ELECTRONIC STATES:1||ADJUSTABLEPARAMETERS:1||MAGNETICPROPERTIES:1||LIQUIDPHASE EPITAXY:1||CEP laser:1||REGION:1||Plasma waveguide:1||AMBIENT GAS:1||DEPOSITION:1||HARMONICGENERATION:1||ENHANCEMENT:1||imaging spectrometer:1||Abel inversion:1||Water window:1||Liquid nitrogen jet:1||CHARGEEXCHANGE:1||NOBEL LECTURE:1||VARISTOR:1||EPITAXY:1||THINDISK LASER:1||HIGHREPETITIONRATE:1||Atom lasers:1||Electronimpact excitation:1||High order harmonics:1||ultrafast technology:1||PEAK POWER:1||CHARGED ALUMINUM CLUSTERS:1||GaN:1||THIN:1||Electron beam:1||INTENSE:1||Hard Xray pulse generation:1||NONLINEAR THOMSON SCATTERING:1||MULTILAYER:1||UVvisible spectrometer:1||ATOMS:1||innershell transitions:1||CORRECTED CONCAVE GRATINGS:1||DISCHARGE:1||LASERPLASMA:1||thin film:1||reflectivity:1||opacity:1||gain:1||smallangle Xray scattering:1||SOFTXRAY:1||ZINCOXIDE:1||CYGNUSX3:1||Betatron oscillation:1||ACCELERATOR:1||STRAINEDLAYER SUPERLATTICES:1||OPTICAL PARAMETRIC AMPLIFICATION:1||PASSIVE MODELOCKING:1||Collision dynamics:1||MUM:1||EXACTEXCHANGE:1||BASISSET:1||APPROXIMATION:1||OXYNITRIDES:1||Beam energy modulation:1||polarization spectroscopy:1||REORIENTATION TRANSITION:1||DEPENDENCE:1||sulfurs:1||BUILDINGBLOCKS:1||RATES:1||OPTICAL PULSES:1||toroidal mirror:1||XRAY LASER:1||CALCIUM:1||radially polarized laser:1||GRAINBOUNDARIES:1||VAPORDEPOSITION:1||Xray generation:1||MAGNETIZATION:1||Electric excitation:1||Laserinduced gas plasmas:1||Qualitative analysis:1||SCHEME:1||RADIATION:10||PULSES:8||PHOTOLUMINESCENCE:7||LASER:7||GENERATION:6||NANORODS:6||GROWTH:6||NANOWIRES:5||IMPLANTED GAN:5||SPECTROSCOPY:5||THINFILMS:4||DYNAMICS:4||SILICON:4||EXTREMEULTRAVIOLET:4||AMPLIFICATION:4||PRESSURE:4||PHASE:4||OPTICALPROPERTIES:4||SYSTEM:4||EMISSION:4||FEL:3||N2O:3||FILMS:3||OPTICS:3||SPECTRA:3||FIELD:3||MIRRORS:3||ARRAYS:3||CLUSTERS:3||SIO2:3||IONIZATION:3||VACUUM:3||SCATTERING:3||IONS:2||LUMINESCENCE PROPERTIES:2||ANISOTROPY:2||BEAMS:2||DIFFRACTION:2||DISPERSION:2||chemical vapor deposition (CVD):2||ELECTRONICSTRUCTURE:2||MOSFETS:2||SI3N4:2||DENSITY:2||LIGHT:2||PLASMAS:2||MATTER:2||nanocomposites:2||RAMANSCATTERING:2||NANOPARTICLES:2||OXIDE:2||AMPLIFIED SPONTANEOUS EMISSION:2||NM WAVELENGTH:2||GAIN:2||CARBON NANOTUBES:2||CROSSSECTIONS:2||LIGHTEMITTINGDIODES:2||PULSE:2||CARBON PLASMA:2||TISAPPHIRE LASER:2||Raman scattering:2||ROUTE:2||multilayer:2||CATHODOLUMINESCENCE:2||highresolution transmission electronic microscope (HRTEM):2||DIFFERENCEFREQUENCYGENERATION:2||CRYSTAL:2||laserproduced plasma:2||NANOCABLES:2||photoluminescence:2||MAGNETIC ALLOY SEMICONDUCTORS:2||MOLECULARBEAM EPITAXY:2||EARTHDOPED GAN:2||LASER FIELDS:2||CHIRPEDPULSEAMPLIFICATION:2||ALN:2||GAUSSIANBEAM:2||ASSISTED CATALYTIC GROWTH:2||BLUE:2||NANOSTRUCTURES:2||MAGNETOELECTRONICS:2||MICROSCOPY:2||ELECTROLUMINESCENCE:2||LASERPULSES:2||GaN nanowires:2||GALLIUM NITRIDE NANOWIRES:2||GAMNN:2||NANOTUBES:2||PHYSICS:2||Femtosecond laser:2||parametric oscillators and amplifiers:1||ultrafast lasers:1||VALENCE:1||nanowires:1||DILUTED MAGNETIC SEMICONDUCTOR:1||LUMINESCENCE:1||Density modulation:1||Energy modulation:1||Current enhanced SASE free electron laser:1||Undulator radiation:1||FREEELECTRON LASERS:1||ULTRATHIN FERROMAGNETICFILMS:1||OXIDEFILMS:1||ABLATION:1||COMPONENT:1||METAL:1||innershell excited states:1||Nelike ions:1||TRANSITIONS:1||XUV spectrometer:1||DIAGNOSTICS:1||Xray scattering:1||MO/SI:1||pulsed laser deposition:1||KEV IMPACT ENERGIES:1||vacuum electron acceleration:1||HIGHINTENSITY LASER:1||JUNCTIONS:1||LOWTEMPERATURE GROWTH:1||nanocrystalline materials:1||MOLECULAR PHOTOIONIZATION:1||LOCALIZATION:1||DEUTERIUM CLUSTERS:1||EXPLOSIONS:1||REGENERATIVE AMPLIFIERS:1||RAREGASES:1||THz radiation:1||FREEELECTRON LASER:1||REALTIME OBSERVATION:1||TARGET:1||photoionized plasmas:1||fs Xray laser:1||emission profile:1||HIGHORDER HARMONICS:1||Xray laser:1||atomic transition:1||EXCITATION:1||LASERS:1||PERFORMANCE:1||RELATIVISTIC ELECTRONS:1||BI2O3DOPED ZNO:1||INNERSHELL IONIZATION:1||Laser wakefield:1||FREQUENCY:1||SOLIDSTATE LASERS:1||Linearly polarized:1||THERMIONIC EMISSION:1||PULSE AMPLIFICATION SYSTEM:1||BIB3O6:1||NM:1||NONCOVALENT INTERACTIONS:1||CRYSTALLINE:1||INTENSITY:1||JETS:1||COHERENT:1||LINE:1||ANGULARDISTRIBUTION:1||SILVER IONS:1||magnetic anisotropy:1||DEVICES:1||Auger transitions:1||CosterKronig transitions:1||EFFICIENT:1||ELECTRONIMPACT IONIZATION:1||ULTRASHORTPULSE:1||Nanowire:1||Heterostructure:1||soft Xray reflectivity:1||PLASMA ACCELERATOR:1||ZINCOXIDE NANOWIRES:1||CHEMICALVAPORDEPOSITION:1||Electron acceleration:1||Ionization of gases:1||Delay dependent:1||MULTIPHOTON IONIZATION:1||FRAGMENTATION:1||GASJET:1||ultrafast nonlinear optics:1||CYCLE PULSES:1||KHZ:1||chemical vapor deposition:1||ferromagnetism:1||ABSORPTION:1||TERAHERTZ RADIATION:1||SCIENCE:1||FIELDS:1||ELECTRONS:1||nanomultilayer structures:1||YIELDS:1||AUGER:1||10HZ REPETITION RATE:1||MULTITERAWATT:1||SPECTROGRAPH:1||HIGHHARMONICGENERATION:1||spectroscopy:1||level population:1||PARTICLEACCELERATION:1||OPTICAL FREQUENCYMEASUREMENT:1||NANOWALLS:1||ROOMTEMPERATURE:1||AVERAGE OUTPUT POWER:1||GROUPVELOCITYMISMATCH:1||Impact ionization:1||Dynamics:1||Lasers:1||Collisional process:1||ABOVETHRESHOLD IONIZATION:1||MAINGROUP THERMOCHEMISTRY:1||dilute magnetic semiconductors:1||GACRN:1||SIZE:1||ATTOSECOND:1||Ar cluster:1||Xray astrophysics:1||photoionization:1||irons:1||normal incidence pulsed laser deposition:1||SHELLS:1||Silicon Oxide:1||gaspuff Zpinch:1||Xray:1||soft Xray reflectors:1||ESCAPE:1||ZN2SIO4:1||SILICA:1||Time delay:1||Collisional plasmas:1||MASSSPECTROMETRY:1||NUCLEARFUSION:1||PARAMETRIC AMPLIFICATION:1||LYING ELECTRONIC STATES:1||ADJUSTABLEPARAMETERS:1||MAGNETICPROPERTIES:1||LIQUIDPHASE EPITAXY:1||CEP laser:1||REGION:1||Plasma waveguide:1||AMBIENT GAS:1||DEPOSITION:1||HARMONICGENERATION:1||ENHANCEMENT:1||imaging spectrometer:1||Abel inversion:1||Water window:1||Liquid nitrogen jet:1||CHARGEEXCHANGE:1||NOBEL LECTURE:1||VARISTOR:1||EPITAXY:1||THINDISK LASER:1||HIGHREPETITIONRATE:1||Atom lasers:1||Electronimpact excitation:1||High order harmonics:1||ultrafast technology:1||PEAK POWER:1||CHARGED ALUMINUM CLUSTERS:1||GaN:1||THIN:1||Electron beam:1||INTENSE:1||Hard Xray pulse generation:1||NONLINEAR THOMSON SCATTERING:1||MULTILAYER:1||UVvisible spectrometer:1||ATOMS:1||innershell transitions:1||CORRECTED CONCAVE GRATINGS:1||DISCHARGE:1||LASERPLASMA:1||thin film:1||reflectivity:1||opacity:1||gain:1||smallangle Xray scattering:1||SOFTXRAY:1||ZINCOXIDE:1||CYGNUSX3:1||Betatron oscillation:1||ACCELERATOR:1||STRAINEDLAYER SUPERLATTICES:1||OPTICAL PARAMETRIC AMPLIFICATION:1||PASSIVE MODELOCKING:1||Collision dynamics:1||MUM:1||EXACTEXCHANGE:1||BASISSET:1||APPROXIMATION:1||OXYNITRIDES:1||Beam energy modulation:1||polarization spectroscopy:1||REORIENTATION TRANSITION:1||DEPENDENCE:1||sulfurs:1||BUILDINGBLOCKS:1||RATES:1||OPTICAL PULSES:1||toroidal mirror:1||XRAY LASER:1||CALCIUM:1||radially polarized laser:1||GRAINBOUNDARIES:1||VAPORDEPOSITION:1||Xray generation:1||MAGNETIZATION:1||Electric excitation:1||Laserinduced gas plasmas:1||Qualitative analysis:1||SCHEME:1||RADIATION:10||PULSES:8||PHOTOLUMINESCENCE:7||LASER:7||GENERATION:6||NANORODS:6||GROWTH:6||NANOWIRES:5||IMPLANTED 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SEMICONDUCTORS:2||MOLECULARBEAM EPITAXY:2||EARTHDOPED GAN:2||LASER FIELDS:2||CHIRPEDPULSEAMPLIFICATION:2||ALN:2||GAUSSIANBEAM:2||ASSISTED CATALYTIC GROWTH:2||BLUE:2||NANOSTRUCTURES:2||MAGNETOELECTRONICS:2||MICROSCOPY:2||ELECTROLUMINESCENCE:2||LASERPULSES:2||GaN nanowires:2||GALLIUM NITRIDE NANOWIRES:2||GAMNN:2||NANOTUBES:2||PHYSICS:2||Femtosecond laser:2||parametric oscillators and amplifiers:1||ultrafast lasers:1||VALENCE:1||nanowires:1||DILUTED MAGNETIC SEMICONDUCTOR:1||LUMINESCENCE:1||Density modulation:1||Energy modulation:1||Current enhanced SASE free electron laser:1||Undulator radiation:1||FREEELECTRON LASERS:1||ULTRATHIN FERROMAGNETICFILMS:1||OXIDEFILMS:1||ABLATION:1||COMPONENT:1||METAL:1||innershell excited states:1||Nelike ions:1||TRANSITIONS:1||XUV spectrometer:1||DIAGNOSTICS:1||Xray scattering:1||MO/SI:1||pulsed laser deposition:1||KEV IMPACT ENERGIES:1||vacuum electron acceleration:1||HIGHINTENSITY LASER:1||JUNCTIONS:1||LOWTEMPERATURE GROWTH:1||nanocrystalline materials:1||MOLECULAR PHOTOIONIZATION:1||LOCALIZATION:1||DEUTERIUM CLUSTERS:1||EXPLOSIONS:1||REGENERATIVE AMPLIFIERS:1||RAREGASES:1||THz radiation:1||FREEELECTRON LASER:1||REALTIME OBSERVATION:1||TARGET:1||photoionized plasmas:1||fs Xray laser:1||emission profile:1||HIGHORDER HARMONICS:1||Xray laser:1||atomic transition:1||EXCITATION:1||LASERS:1||PERFORMANCE:1||RELATIVISTIC ELECTRONS:1||BI2O3DOPED ZNO:1||INNERSHELL IONIZATION:1||Laser wakefield:1||FREQUENCY:1||SOLIDSTATE LASERS:1||Linearly polarized:1||THERMIONIC EMISSION:1||PULSE AMPLIFICATION SYSTEM:1||BIB3O6:1||NM:1||NONCOVALENT INTERACTIONS:1||CRYSTALLINE:1||INTENSITY:1||JETS:1||COHERENT:1||LINE:1||ANGULARDISTRIBUTION:1||SILVER IONS:1||magnetic anisotropy:1||DEVICES:1||Auger transitions:1||CosterKronig transitions:1||EFFICIENT:1||ELECTRONIMPACT IONIZATION:1||ULTRASHORTPULSE:1||Nanowire:1||Heterostructure:1||soft Xray reflectivity:1||PLASMA ACCELERATOR:1||ZINCOXIDE NANOWIRES:1||CHEMICALVAPORDEPOSITION:1||Electron acceleration:1||Ionization of gases:1||Delay dependent:1||MULTIPHOTON IONIZATION:1||FRAGMENTATION:1||GASJET:1||ultrafast nonlinear optics:1||CYCLE PULSES:1||KHZ:1||chemical vapor deposition:1||ferromagnetism:1||ABSORPTION:1||TERAHERTZ RADIATION:1||SCIENCE:1||FIELDS:1||ELECTRONS:1||nanomultilayer structures:1||YIELDS:1||AUGER:1||10HZ REPETITION RATE:1||MULTITERAWATT:1||SPECTROGRAPH:1||HIGHHARMONICGENERATION:1||spectroscopy:1||level population:1||PARTICLEACCELERATION:1||OPTICAL FREQUENCYMEASUREMENT:1||NANOWALLS:1||ROOMTEMPERATURE:1||AVERAGE OUTPUT POWER:1||GROUPVELOCITYMISMATCH:1||Impact ionization:1||Dynamics:1||Lasers:1||Collisional process:1||ABOVETHRESHOLD IONIZATION:1||MAINGROUP THERMOCHEMISTRY:1||dilute magnetic semiconductors:1||GACRN:1||SIZE:1||ATTOSECOND:1||Ar cluster:1||Xray astrophysics:1||photoionization:1||irons:1||normal incidence pulsed laser deposition:1||SHELLS:1||Silicon Oxide:1||gaspuff Zpinch:1||Xray:1||soft Xray reflectors:1||ESCAPE:1||ZN2SIO4:1||SILICA:1||Time 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materials:1||MOLECULAR PHOTOIONIZATION:1||LOCALIZATION:1||DEUTERIUM CLUSTERS:1||EXPLOSIONS:1||REGENERATIVE AMPLIFIERS:1||RAREGASES:1||THz radiation:1||FREEELECTRON LASER:1||REALTIME OBSERVATION:1||TARGET:1||photoionized plasmas:1||fs Xray laser:1||emission profile:1||HIGHORDER HARMONICS:1||Xray laser:1||atomic transition:1||EXCITATION:1||LASERS:1||PERFORMANCE:1||RELATIVISTIC ELECTRONS:1||BI2O3DOPED ZNO:1||INNERSHELL IONIZATION:1||Laser wakefield:1||FREQUENCY:1||SOLIDSTATE LASERS:1||Linearly polarized:1||THERMIONIC EMISSION:1||PULSE AMPLIFICATION SYSTEM:1||BIB3O6:1||NM:1||NONCOVALENT INTERACTIONS:1||CRYSTALLINE:1||INTENSITY:1||JETS:1||COHERENT:1||LINE:1||ANGULARDISTRIBUTION:1||SILVER IONS:1||magnetic anisotropy:1||DEVICES:1||Auger transitions:1||CosterKronig transitions:1||EFFICIENT:1||ELECTRONIMPACT IONIZATION:1||ULTRASHORTPULSE:1||Nanowire:1||Heterostructure:1||soft Xray reflectivity:1||PLASMA ACCELERATOR:1||ZINCOXIDE NANOWIRES:1||CHEMICALVAPORDEPOSITION:1||Electron acceleration:1||Ionization of gases:1||Delay dependent:1||MULTIPHOTON IONIZATION:1||FRAGMENTATION:1||GASJET:1||ultrafast nonlinear optics:1||CYCLE PULSES:1||KHZ:1||chemical vapor deposition:1||ferromagnetism:1||ABSORPTION:1||TERAHERTZ RADIATION:1||SCIENCE:1||FIELDS:1||ELECTRONS:1||nanomultilayer structures:1||YIELDS:1||AUGER:1||10HZ REPETITION RATE:1||MULTITERAWATT:1||SPECTROGRAPH:1||HIGHHARMONICGENERATION:1||spectroscopy:1||level population:1||PARTICLEACCELERATION:1||OPTICAL FREQUENCYMEASUREMENT:1||NANOWALLS:1||ROOMTEMPERATURE:1||AVERAGE OUTPUT POWER:1||GROUPVELOCITYMISMATCH:1||Impact ionization:1||Dynamics:1||Lasers:1||Collisional process:1||ABOVETHRESHOLD IONIZATION:1||MAINGROUP THERMOCHEMISTRY:1||dilute magnetic semiconductors:1||GACRN:1||SIZE:1||ATTOSECOND:1||Ar cluster:1||Xray astrophysics:1||photoionization:1||irons:1||normal incidence pulsed laser deposition:1||SHELLS:1||Silicon Oxide:1||gaspuff Zpinch:1||Xray:1||soft Xray reflectors:1||ESCAPE:1||ZN2SIO4:1||SILICA:1||Time delay:1||Collisional plasmas:1||MASSSPECTROMETRY:1||NUCLEARFUSION:1||PARAMETRIC AMPLIFICATION:1||LYING ELECTRONIC STATES:1||ADJUSTABLEPARAMETERS:1||MAGNETICPROPERTIES:1||LIQUIDPHASE EPITAXY:1||CEP laser:1||REGION:1||Plasma waveguide:1||AMBIENT GAS:1||DEPOSITION:1||HARMONICGENERATION:1||ENHANCEMENT:1||imaging spectrometer:1||Abel inversion:1||Water window:1||Liquid nitrogen jet:1||CHARGEEXCHANGE:1||NOBEL LECTURE:1||VARISTOR:1||EPITAXY:1||THINDISK LASER:1||HIGHREPETITIONRATE:1||Atom lasers:1||Electronimpact excitation:1||High order harmonics:1||ultrafast technology:1||PEAK POWER:1||CHARGED ALUMINUM CLUSTERS:1||GaN:1||THIN:1||Electron beam:1||INTENSE:1||Hard Xray pulse generation:1||NONLINEAR THOMSON SCATTERING:1||MULTILAYER:1||UVvisible spectrometer:1||ATOMS:1||innershell transitions:1||CORRECTED CONCAVE GRATINGS:1||DISCHARGE:1||LASERPLASMA:1||thin film:1||reflectivity:1||opacity:1||gain:1||smallangle Xray scattering:1||SOFTXRAY:1||ZINCOXIDE:1||CYGNUSX3:1||Betatron oscillation:1||ACCELERATOR:1||STRAINEDLAYER SUPERLATTICES:1||OPTICAL PARAMETRIC AMPLIFICATION:1||PASSIVE MODELOCKING:1||Collision dynamics:1||MUM:1||EXACTEXCHANGE:1||BASISSET:1||APPROXIMATION:1||OXYNITRIDES:1||Beam energy modulation:1||polarization spectroscopy:1||REORIENTATION TRANSITION:1||DEPENDENCE:1||sulfurs:1||BUILDINGBLOCKS:1||RATES:1||OPTICAL PULSES:1||toroidal mirror:1||XRAY LASER:1||CALCIUM:1||radially polarized laser:1||GRAINBOUNDARIES:1||VAPORDEPOSITION:1||Xray generation:1||MAGNETIZATION:1||Electric excitation:1||Laserinduced gas plasmas:1||Qualitative analysis:1||SCHEME:1||RADIATION:10||PULSES:8||PHOTOLUMINESCENCE:7||LASER:7||GENERATION:6||NANORODS:6||GROWTH:6||NANOWIRES:5||IMPLANTED GAN:5||SPECTROSCOPY:5||THINFILMS:4||DYNAMICS:4||SILICON:4||EXTREMEULTRAVIOLET:4||AMPLIFICATION:4||PRESSURE:4||PHASE:4||OPTICALPROPERTIES:4||SYSTEM:4||EMISSION:4||FEL:3||N2O:3||FILMS:3||OPTICS:3||SPECTRA:3||FIELD:3||MIRRORS:3||ARRAYS:3||CLUSTERS:3||SIO2:3||IONIZATION:3||VACUUM:3||SCATTERING:3||IONS:2||LUMINESCENCE PROPERTIES:2||ANISOTROPY:2||BEAMS:2||DIFFRACTION:2||DISPERSION:2||chemical vapor deposition (CVD):2||ELECTRONICSTRUCTURE:2||MOSFETS:2||SI3N4:2||DENSITY:2||LIGHT:2||PLASMAS:2||MATTER:2||nanocomposites:2||RAMANSCATTERING:2||NANOPARTICLES:2||OXIDE:2||AMPLIFIED SPONTANEOUS EMISSION:2||NM WAVELENGTH:2||GAIN:2||CARBON NANOTUBES:2||CROSSSECTIONS:2||LIGHTEMITTINGDIODES:2||PULSE:2||CARBON PLASMA:2||TISAPPHIRE LASER:2||Raman scattering:2||ROUTE:2||multilayer:2||CATHODOLUMINESCENCE:2||highresolution transmission electronic microscope (HRTEM):2||DIFFERENCEFREQUENCYGENERATION:2||CRYSTAL:2||laserproduced plasma:2||NANOCABLES:2||photoluminescence:2||MAGNETIC ALLOY SEMICONDUCTORS:2||MOLECULARBEAM EPITAXY:2||EARTHDOPED GAN:2||LASER FIELDS:2||CHIRPEDPULSEAMPLIFICATION:2||ALN:2||GAUSSIANBEAM:2||ASSISTED CATALYTIC GROWTH:2||BLUE:2||NANOSTRUCTURES:2||MAGNETOELECTRONICS:2||MICROSCOPY:2||ELECTROLUMINESCENCE:2||LASERPULSES:2||GaN nanowires:2||GALLIUM NITRIDE NANOWIRES:2||GAMNN:2||NANOTUBES:2||PHYSICS:2||Femtosecond laser:2||parametric oscillators and amplifiers:1||ultrafast lasers:1||VALENCE:1||nanowires:1||DILUTED MAGNETIC SEMICONDUCTOR:1||LUMINESCENCE:1||Density modulation:1||Energy modulation:1||Current enhanced SASE free electron laser:1||Undulator radiation:1||FREEELECTRON LASERS:1||ULTRATHIN FERROMAGNETICFILMS:1||OXIDEFILMS:1||ABLATION:1||COMPONENT:1||METAL:1||innershell excited states:1||Nelike ions:1||TRANSITIONS:1||XUV spectrometer:1||DIAGNOSTICS:1||Xray scattering:1||MO/SI:1||pulsed laser deposition:1||KEV IMPACT ENERGIES:1||vacuum electron acceleration:1||HIGHINTENSITY LASER:1||JUNCTIONS:1||LOWTEMPERATURE GROWTH:1||nanocrystalline materials:1||MOLECULAR PHOTOIONIZATION:1||LOCALIZATION:1||DEUTERIUM CLUSTERS:1||EXPLOSIONS:1||REGENERATIVE AMPLIFIERS:1||RAREGASES:1||THz radiation:1||FREEELECTRON LASER:1||REALTIME OBSERVATION:1||TARGET:1||photoionized plasmas:1||fs Xray laser:1||emission profile:1||HIGHORDER HARMONICS:1||Xray laser:1||atomic transition:1||EXCITATION:1||LASERS:1||PERFORMANCE:1||RELATIVISTIC ELECTRONS:1||BI2O3DOPED ZNO:1||INNERSHELL IONIZATION:1||Laser wakefield:1||FREQUENCY:1||SOLIDSTATE LASERS:1||Linearly polarized:1||THERMIONIC EMISSION:1||PULSE AMPLIFICATION SYSTEM:1||BIB3O6:1||NM:1||NONCOVALENT INTERACTIONS:1||CRYSTALLINE:1||INTENSITY:1||JETS:1||COHERENT:1||LINE:1||ANGULARDISTRIBUTION:1||SILVER IONS:1||magnetic anisotropy:1||DEVICES:1||Auger transitions:1||CosterKronig transitions:1||EFFICIENT:1||ELECTRONIMPACT IONIZATION:1||ULTRASHORTPULSE:1||Nanowire:1||Heterostructure:1||soft Xray reflectivity:1||PLASMA ACCELERATOR:1||ZINCOXIDE NANOWIRES:1||CHEMICALVAPORDEPOSITION:1||Electron acceleration:1||Ionization of gases:1||Delay dependent:1||MULTIPHOTON IONIZATION:1||FRAGMENTATION:1||GASJET:1||ultrafast nonlinear optics:1||CYCLE PULSES:1||KHZ:1||chemical vapor deposition:1||ferromagnetism:1||ABSORPTION:1||TERAHERTZ RADIATION:1||SCIENCE:1||FIELDS:1||ELECTRONS:1||nanomultilayer structures:1||YIELDS:1||AUGER:1||10HZ REPETITION RATE:1||MULTITERAWATT:1||SPECTROGRAPH:1||HIGHHARMONICGENERATION:1||spectroscopy:1||level population:1||PARTICLEACCELERATION:1||OPTICAL FREQUENCYMEASUREMENT:1||NANOWALLS:1||ROOMTEMPERATURE:1||AVERAGE OUTPUT POWER:1||GROUPVELOCITYMISMATCH:1||Impact ionization:1||Dynamics:1||Lasers:1||Collisional process:1||ABOVETHRESHOLD IONIZATION:1||MAINGROUP THERMOCHEMISTRY:1||dilute magnetic semiconductors:1||GACRN:1||SIZE:1||ATTOSECOND:1||Ar cluster:1||Xray astrophysics:1||photoionization:1||irons:1||normal incidence pulsed laser deposition:1||SHELLS:1||Silicon Oxide:1||gaspuff Zpinch:1||Xray:1||soft Xray reflectors:1||ESCAPE:1||ZN2SIO4:1||SILICA:1||Time delay:1||Collisional plasmas:1||MASSSPECTROMETRY:1||NUCLEARFUSION:1||PARAMETRIC AMPLIFICATION:1||LYING ELECTRONIC STATES:1||ADJUSTABLEPARAMETERS:1||MAGNETICPROPERTIES:1||LIQUIDPHASE EPITAXY:1||CEP laser:1||REGION:1||Plasma waveguide:1||AMBIENT GAS:1||DEPOSITION:1||HARMONICGENERATION:1||ENHANCEMENT:1||imaging spectrometer:1||Abel inversion:1||Water window:1||Liquid nitrogen jet:1||CHARGEEXCHANGE:1||NOBEL LECTURE:1||VARISTOR:1||EPITAXY:1||THINDISK LASER:1||HIGHREPETITIONRATE:1||Atom lasers:1||Electronimpact excitation:1||High order harmonics:1||ultrafast technology:1||PEAK POWER:1||CHARGED ALUMINUM CLUSTERS:1||GaN:1||THIN:1||Electron beam:1||INTENSE:1||Hard Xray pulse generation:1||NONLINEAR THOMSON SCATTERING:1||MULTILAYER:1||UVvisible spectrometer:1||ATOMS:1||innershell transitions:1||CORRECTED CONCAVE GRATINGS:1||DISCHARGE:1||LASERPLASMA:1||thin film:1||reflectivity:1||opacity:1||gain:1||smallangle Xray scattering:1||SOFTXRAY:1||ZINCOXIDE:1||CYGNUSX3:1||Betatron oscillation:1||ACCELERATOR:1||STRAINEDLAYER SUPERLATTICES:1||OPTICAL PARAMETRIC AMPLIFICATION:1||PASSIVE MODELOCKING:1||Collision dynamics:1||MUM:1||EXACTEXCHANGE:1||BASISSET:1||APPROXIMATION:1||OXYNITRIDES:1||Beam energy modulation:1||polarization spectroscopy:1||REORIENTATION TRANSITION:1||DEPENDENCE:1||sulfurs:1||BUILDINGBLOCKS:1||RATES:1||OPTICAL PULSES:1||toroidal mirror:1||XRAY LASER:1||CALCIUM:1||radially polarized laser:1||GRAINBOUNDARIES:1||VAPORDEPOSITION:1||Xray generation:1||MAGNETIZATION:1||Electric excitation:1||Laserinduced gas plasmas:1||Qualitative analysis:1||SCHEME:1||RADIATION:10||PULSES:8||PHOTOLUMINESCENCE:7||LASER:7||GENERATION:6||NANORODS:6||GROWTH:6||NANOWIRES:5||IMPLANTED 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SEMICONDUCTORS:2||MOLECULARBEAM EPITAXY:2||EARTHDOPED GAN:2||LASER FIELDS:2||CHIRPEDPULSEAMPLIFICATION:2||ALN:2||GAUSSIANBEAM:2||ASSISTED CATALYTIC GROWTH:2||BLUE:2||NANOSTRUCTURES:2||MAGNETOELECTRONICS:2||MICROSCOPY:2||ELECTROLUMINESCENCE:2||LASERPULSES:2||GaN nanowires:2||GALLIUM NITRIDE NANOWIRES:2||GAMNN:2||NANOTUBES:2||PHYSICS:2||Femtosecond laser:2||parametric oscillators and amplifiers:1||ultrafast lasers:1||VALENCE:1||nanowires:1||DILUTED MAGNETIC SEMICONDUCTOR:1||LUMINESCENCE:1||Density modulation:1||Energy modulation:1||Current enhanced SASE free electron laser:1||Undulator radiation:1||FREEELECTRON LASERS:1||ULTRATHIN FERROMAGNETICFILMS:1||OXIDEFILMS:1||ABLATION:1||COMPONENT:1||METAL:1||innershell excited states:1||Nelike ions:1||TRANSITIONS:1||XUV spectrometer:1||DIAGNOSTICS:1||Xray scattering:1||MO/SI:1||pulsed laser deposition:1||KEV IMPACT ENERGIES:1||vacuum electron acceleration:1||HIGHINTENSITY LASER:1||JUNCTIONS:1||LOWTEMPERATURE GROWTH:1||nanocrystalline materials:1||MOLECULAR PHOTOIONIZATION:1||LOCALIZATION:1||DEUTERIUM CLUSTERS:1||EXPLOSIONS:1||REGENERATIVE AMPLIFIERS:1||RAREGASES:1||THz radiation:1||FREEELECTRON LASER:1||REALTIME OBSERVATION:1||TARGET:1||photoionized plasmas:1||fs Xray laser:1||emission profile:1||HIGHORDER HARMONICS:1||Xray laser:1||atomic transition:1||EXCITATION:1||LASERS:1||PERFORMANCE:1||RELATIVISTIC ELECTRONS:1||BI2O3DOPED ZNO:1||INNERSHELL IONIZATION:1||Laser wakefield:1||FREQUENCY:1||SOLIDSTATE LASERS:1||Linearly polarized:1||THERMIONIC EMISSION:1||PULSE AMPLIFICATION SYSTEM:1||BIB3O6:1||NM:1||NONCOVALENT INTERACTIONS:1||CRYSTALLINE:1||INTENSITY:1||JETS:1||COHERENT:1||LINE:1||ANGULARDISTRIBUTION:1||SILVER IONS:1||magnetic anisotropy:1||DEVICES:1||Auger transitions:1||CosterKronig transitions:1||EFFICIENT:1||ELECTRONIMPACT IONIZATION:1||ULTRASHORTPULSE:1||Nanowire:1||Heterostructure:1||soft Xray reflectivity:1||PLASMA ACCELERATOR:1||ZINCOXIDE NANOWIRES:1||CHEMICALVAPORDEPOSITION:1||Electron acceleration:1||Ionization of gases:1||Delay dependent:1||MULTIPHOTON IONIZATION:1||FRAGMENTATION:1||GASJET:1||ultrafast nonlinear optics:1||CYCLE PULSES:1||KHZ:1||chemical vapor deposition:1||ferromagnetism:1||ABSORPTION:1||TERAHERTZ RADIATION:1||SCIENCE:1||FIELDS:1||ELECTRONS:1||nanomultilayer structures:1||YIELDS:1||AUGER:1||10HZ REPETITION RATE:1||MULTITERAWATT:1||SPECTROGRAPH:1||HIGHHARMONICGENERATION:1||spectroscopy:1||level population:1||PARTICLEACCELERATION:1||OPTICAL FREQUENCYMEASUREMENT:1||NANOWALLS:1||ROOMTEMPERATURE:1||AVERAGE OUTPUT POWER:1||GROUPVELOCITYMISMATCH:1||Impact ionization:1||Dynamics:1||Lasers:1||Collisional process:1||ABOVETHRESHOLD IONIZATION:1||MAINGROUP THERMOCHEMISTRY:1||dilute magnetic semiconductors:1||GACRN:1||SIZE:1||ATTOSECOND:1||Ar cluster:1||Xray astrophysics:1||photoionization:1||irons:1||normal incidence pulsed laser deposition:1||SHELLS:1||Silicon Oxide:1||gaspuff Zpinch:1||Xray:1||soft Xray reflectors:1||ESCAPE:1||ZN2SIO4:1||SILICA:1||Time 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materials:1||MOLECULAR PHOTOIONIZATION:1||LOCALIZATION:1||DEUTERIUM CLUSTERS:1||EXPLOSIONS:1||REGENERATIVE AMPLIFIERS:1||RAREGASES:1||THz radiation:1||FREEELECTRON LASER:1||REALTIME OBSERVATION:1||TARGET:1||photoionized plasmas:1||fs Xray laser:1||emission profile:1||HIGHORDER HARMONICS:1||Xray laser:1||atomic transition:1||EXCITATION:1||LASERS:1||PERFORMANCE:1||RELATIVISTIC ELECTRONS:1||BI2O3DOPED ZNO:1||INNERSHELL IONIZATION:1||Laser wakefield:1||FREQUENCY:1||SOLIDSTATE LASERS:1||Linearly polarized:1||THERMIONIC EMISSION:1||PULSE AMPLIFICATION SYSTEM:1||BIB3O6:1||NM:1||NONCOVALENT INTERACTIONS:1||CRYSTALLINE:1||INTENSITY:1||JETS:1||COHERENT:1||LINE:1||ANGULARDISTRIBUTION:1||SILVER IONS:1||magnetic anisotropy:1||DEVICES:1||Auger transitions:1||CosterKronig transitions:1||EFFICIENT:1||ELECTRONIMPACT IONIZATION:1||ULTRASHORTPULSE:1||Nanowire:1||Heterostructure:1||soft Xray reflectivity:1||PLASMA ACCELERATOR:1||ZINCOXIDE NANOWIRES:1||CHEMICALVAPORDEPOSITION:1||Electron acceleration:1||Ionization of gases:1||Delay dependent:1||MULTIPHOTON IONIZATION:1||FRAGMENTATION:1||GASJET:1||ultrafast nonlinear optics:1||CYCLE PULSES:1||KHZ:1||chemical vapor deposition:1||ferromagnetism:1||ABSORPTION:1||TERAHERTZ RADIATION:1||SCIENCE:1||FIELDS:1||ELECTRONS:1||nanomultilayer structures:1||YIELDS:1||AUGER:1||10HZ REPETITION RATE:1||MULTITERAWATT:1||SPECTROGRAPH:1||HIGHHARMONICGENERATION:1||spectroscopy:1||level population:1||PARTICLEACCELERATION:1||OPTICAL FREQUENCYMEASUREMENT:1||NANOWALLS:1||ROOMTEMPERATURE:1||AVERAGE OUTPUT POWER:1||GROUPVELOCITYMISMATCH:1||Impact ionization:1||Dynamics:1||Lasers:1||Collisional process:1||ABOVETHRESHOLD IONIZATION:1||MAINGROUP THERMOCHEMISTRY:1||dilute magnetic semiconductors:1||GACRN:1||SIZE:1||ATTOSECOND:1||Ar cluster:1||Xray astrophysics:1||photoionization:1||irons:1||normal incidence pulsed laser deposition:1||SHELLS:1||Silicon Oxide:1||gaspuff Zpinch:1||Xray:1||soft Xray reflectors:1||ESCAPE:1||ZN2SIO4:1||SILICA:1||Time delay:1||Collisional plasmas:1||MASSSPECTROMETRY:1||NUCLEARFUSION:1||PARAMETRIC AMPLIFICATION:1||LYING ELECTRONIC STATES:1||ADJUSTABLEPARAMETERS:1||MAGNETICPROPERTIES:1||LIQUIDPHASE EPITAXY:1||CEP laser:1||REGION:1||Plasma waveguide:1||AMBIENT GAS:1||DEPOSITION:1||HARMONICGENERATION:1||ENHANCEMENT:1||imaging spectrometer:1||Abel inversion:1||Water window:1||Liquid nitrogen jet:1||CHARGEEXCHANGE:1||NOBEL LECTURE:1||VARISTOR:1||EPITAXY:1||THINDISK LASER:1||HIGHREPETITIONRATE:1||Atom lasers:1||Electronimpact excitation:1||High order harmonics:1||ultrafast technology:1||PEAK POWER:1||CHARGED ALUMINUM CLUSTERS:1||GaN:1||THIN:1||Electron beam:1||INTENSE:1||Hard Xray pulse generation:1||NONLINEAR THOMSON SCATTERING:1||MULTILAYER:1||UVvisible spectrometer:1||ATOMS:1||innershell transitions:1||CORRECTED CONCAVE GRATINGS:1||DISCHARGE:1||LASERPLASMA:1||thin film:1||reflectivity:1||opacity:1||gain:1||smallangle Xray scattering:1||SOFTXRAY:1||ZINCOXIDE:1||CYGNUSX3:1||Betatron oscillation:1||ACCELERATOR:1||STRAINEDLAYER SUPERLATTICES:1||OPTICAL PARAMETRIC AMPLIFICATION:1||PASSIVE MODELOCKING:1||Collision dynamics:1||MUM:1||EXACTEXCHANGE:1||BASISSET:1||APPROXIMATION:1||OXYNITRIDES:1||Beam energy modulation:1||polarization spectroscopy:1||REORIENTATION TRANSITION:1||DEPENDENCE:1||sulfurs:1||BUILDINGBLOCKS:1||RATES:1||OPTICAL PULSES:1||toroidal mirror:1||XRAY LASER:1||CALCIUM:1||radially polarized laser:1||GRAINBOUNDARIES:1||VAPORDEPOSITION:1||Xray generation:1||MAGNETIZATION:1||Electric excitation:1||Laserinduced gas plasmas:1||Qualitative analysis:1||SCHEME:1||RADIATION:10||PULSES:8||PHOTOLUMINESCENCE:7||LASER:7||GENERATION:6||NANORODS:6||GROWTH:6||NANOWIRES:5||IMPLANTED GAN:5||SPECTROSCOPY:5||THINFILMS:4||DYNAMICS:4||SILICON:4||EXTREMEULTRAVIOLET:4||AMPLIFICATION:4||PRESSURE:4||PHASE:4||OPTICALPROPERTIES:4||SYSTEM:4||EMISSION:4||FEL:3||N2O:3||FILMS:3||OPTICS:3||SPECTRA:3||FIELD:3||MIRRORS:3||ARRAYS:3||CLUSTERS:3||SIO2:3||IONIZATION:3||VACUUM:3||SCATTERING:3||IONS:2||LUMINESCENCE PROPERTIES:2||ANISOTROPY:2||BEAMS:2||DIFFRACTION:2||DISPERSION:2||chemical vapor deposition (CVD):2||ELECTRONICSTRUCTURE:2||MOSFETS:2||SI3N4:2||DENSITY:2||LIGHT:2||PLASMAS:2||MATTER:2||nanocomposites:2||RAMANSCATTERING:2||NANOPARTICLES:2||OXIDE:2||AMPLIFIED SPONTANEOUS EMISSION:2||NM WAVELENGTH:2||GAIN:2||CARBON NANOTUBES:2||CROSSSECTIONS:2||LIGHTEMITTINGDIODES:2||PULSE:2||CARBON PLASMA:2||TISAPPHIRE LASER:2||Raman scattering:2||ROUTE:2||multilayer:2||CATHODOLUMINESCENCE:2||highresolution transmission electronic microscope (HRTEM):2||DIFFERENCEFREQUENCYGENERATION:2||CRYSTAL:2||laserproduced plasma:2||NANOCABLES:2||photoluminescence:2||MAGNETIC ALLOY SEMICONDUCTORS:2||MOLECULARBEAM EPITAXY:2||EARTHDOPED GAN:2||LASER FIELDS:2||CHIRPEDPULSEAMPLIFICATION:2||ALN:2||GAUSSIANBEAM:2||ASSISTED CATALYTIC GROWTH:2||BLUE:2||NANOSTRUCTURES:2||MAGNETOELECTRONICS:2||MICROSCOPY:2||ELECTROLUMINESCENCE:2||LASERPULSES:2||GaN nanowires:2||GALLIUM NITRIDE NANOWIRES:2||GAMNN:2||NANOTUBES:2||PHYSICS:2||Femtosecond laser:2||parametric oscillators and amplifiers:1||ultrafast lasers:1||VALENCE:1||nanowires:1||DILUTED MAGNETIC SEMICONDUCTOR:1||LUMINESCENCE:1||Density modulation:1||Energy modulation:1||Current enhanced SASE free electron laser:1||Undulator radiation:1||FREEELECTRON LASERS:1||ULTRATHIN FERROMAGNETICFILMS:1||OXIDEFILMS:1||ABLATION:1||COMPONENT:1||METAL:1||innershell excited states:1||Nelike ions:1||TRANSITIONS:1||XUV spectrometer:1||DIAGNOSTICS:1||Xray scattering:1||MO/SI:1||pulsed laser deposition:1||KEV IMPACT ENERGIES:1||vacuum electron acceleration:1||HIGHINTENSITY LASER:1||JUNCTIONS:1||LOWTEMPERATURE GROWTH:1||nanocrystalline materials:1||MOLECULAR PHOTOIONIZATION:1||LOCALIZATION:1||DEUTERIUM CLUSTERS:1||EXPLOSIONS:1||REGENERATIVE AMPLIFIERS:1||RAREGASES:1||THz radiation:1||FREEELECTRON LASER:1||REALTIME OBSERVATION:1||TARGET:1||photoionized plasmas:1||fs Xray laser:1||emission profile:1||HIGHORDER HARMONICS:1||Xray laser:1||atomic transition:1||EXCITATION:1||LASERS:1||PERFORMANCE:1||RELATIVISTIC ELECTRONS:1||BI2O3DOPED ZNO:1||INNERSHELL IONIZATION:1||Laser wakefield:1||FREQUENCY:1||SOLIDSTATE LASERS:1||Linearly polarized:1||THERMIONIC EMISSION:1||PULSE AMPLIFICATION SYSTEM:1||BIB3O6:1||NM:1||NONCOVALENT INTERACTIONS:1||CRYSTALLINE:1||INTENSITY:1||JETS:1||COHERENT:1||LINE:1||ANGULARDISTRIBUTION:1||SILVER IONS:1||magnetic anisotropy:1||DEVICES:1||Auger transitions:1||CosterKronig transitions:1||EFFICIENT:1||ELECTRONIMPACT IONIZATION:1||ULTRASHORTPULSE:1||Nanowire:1||Heterostructure:1||soft Xray reflectivity:1||PLASMA ACCELERATOR:1||ZINCOXIDE NANOWIRES:1||CHEMICALVAPORDEPOSITION:1||Electron acceleration:1||Ionization of gases:1||Delay dependent:1||MULTIPHOTON IONIZATION:1||FRAGMENTATION:1||GASJET:1||ultrafast nonlinear optics:1||CYCLE PULSES:1||KHZ:1||chemical vapor deposition:1||ferromagnetism:1||ABSORPTION:1||TERAHERTZ RADIATION:1||SCIENCE:1||FIELDS:1||ELECTRONS:1||nanomultilayer structures:1||YIELDS:1||AUGER:1||10HZ REPETITION RATE:1||MULTITERAWATT:1||SPECTROGRAPH:1||HIGHHARMONICGENERATION:1||spectroscopy:1||level population:1||PARTICLEACCELERATION:1||OPTICAL FREQUENCYMEASUREMENT:1||NANOWALLS:1||ROOMTEMPERATURE:1||AVERAGE OUTPUT POWER:1||GROUPVELOCITYMISMATCH:1||Impact ionization:1||Dynamics:1||Lasers:1||Collisional process:1||ABOVETHRESHOLD IONIZATION:1||MAINGROUP THERMOCHEMISTRY:1||dilute magnetic semiconductors:1||GACRN:1||SIZE:1||ATTOSECOND:1||Ar cluster:1||Xray astrophysics:1||photoionization:1||irons:1||normal incidence pulsed laser deposition:1||SHELLS:1||Silicon Oxide:1||gaspuff Zpinch:1||Xray:1||soft Xray reflectors:1||ESCAPE:1||ZN2SIO4:1||SILICA:1||Time delay:1||Collisional plasmas:1||MASSSPECTROMETRY:1||NUCLEARFUSION:1||PARAMETRIC AMPLIFICATION:1||LYING ELECTRONIC STATES:1||ADJUSTABLEPARAMETERS:1||MAGNETICPROPERTIES:1||LIQUIDPHASE EPITAXY:1||CEP laser:1||REGION:1||Plasma waveguide:1||AMBIENT GAS:1||DEPOSITION:1||HARMONICGENERATION:1||ENHANCEMENT:1||imaging spectrometer:1||Abel inversion:1||Water window:1||Liquid nitrogen jet:1||CHARGEEXCHANGE:1||NOBEL LECTURE:1||VARISTOR:1||EPITAXY:1||THINDISK LASER:1||HIGHREPETITIONRATE:1||Atom lasers:1||Electronimpact excitation:1||High order harmonics:1||ultrafast technology:1||PEAK POWER:1||CHARGED ALUMINUM CLUSTERS:1||GaN:1||THIN:1||Electron beam:1||INTENSE:1||Hard Xray pulse generation:1||NONLINEAR THOMSON SCATTERING:1||MULTILAYER:1||UVvisible spectrometer:1||ATOMS:1||innershell transitions:1||CORRECTED CONCAVE GRATINGS:1||DISCHARGE:1||LASERPLASMA:1||thin film:1||reflectivity:1||opacity:1||gain:1||smallangle Xray scattering:1||SOFTXRAY:1||ZINCOXIDE:1||CYGNUSX3:1||Betatron oscillation:1||ACCELERATOR:1||STRAINEDLAYER SUPERLATTICES:1||OPTICAL PARAMETRIC AMPLIFICATION:1||PASSIVE MODELOCKING:1||Collision dynamics:1||MUM:1||EXACTEXCHANGE:1||BASISSET:1||APPROXIMATION:1||OXYNITRIDES:1||Beam energy modulation:1||polarization spectroscopy:1||REORIENTATION TRANSITION:1||DEPENDENCE:1||sulfurs:1||BUILDINGBLOCKS:1||RATES:1||OPTICAL PULSES:1||toroidal mirror:1||XRAY LASER:1||CALCIUM:1||radially polarized laser:1||GRAINBOUNDARIES:1||VAPORDEPOSITION:1||Xray generation:1||MAGNETIZATION:1||Electric excitation:1||Laserinduced gas plasmas:1||Qualitative analysis:1||SCHEME:1||RADIATION:10||PULSES:8||PHOTOLUMINESCENCE:7||LASER:7||GENERATION:6||NANORODS:6||GROWTH:6||NANOWIRES:5||IMPLANTED 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SEMICONDUCTORS:2||MOLECULARBEAM EPITAXY:2||EARTHDOPED GAN:2||LASER FIELDS:2||CHIRPEDPULSEAMPLIFICATION:2||ALN:2||GAUSSIANBEAM:2||ASSISTED CATALYTIC GROWTH:2||BLUE:2||NANOSTRUCTURES:2||MAGNETOELECTRONICS:2||MICROSCOPY:2||ELECTROLUMINESCENCE:2||LASERPULSES:2||GaN nanowires:2||GALLIUM NITRIDE NANOWIRES:2||GAMNN:2||NANOTUBES:2||PHYSICS:2||Femtosecond laser:2||parametric oscillators and amplifiers:1||ultrafast lasers:1||VALENCE:1||nanowires:1||DILUTED MAGNETIC SEMICONDUCTOR:1||LUMINESCENCE:1||Density modulation:1||Energy modulation:1||Current enhanced SASE free electron laser:1||Undulator radiation:1||FREEELECTRON LASERS:1||ULTRATHIN FERROMAGNETICFILMS:1||OXIDEFILMS:1||ABLATION:1||COMPONENT:1||METAL:1||innershell excited states:1||Nelike ions:1||TRANSITIONS:1||XUV spectrometer:1||DIAGNOSTICS:1||Xray scattering:1||MO/SI:1||pulsed laser deposition:1||KEV IMPACT ENERGIES:1||vacuum electron acceleration:1||HIGHINTENSITY LASER:1||JUNCTIONS:1||LOWTEMPERATURE GROWTH:1||nanocrystalline materials:1||MOLECULAR PHOTOIONIZATION:1||LOCALIZATION:1||DEUTERIUM CLUSTERS:1||EXPLOSIONS:1||REGENERATIVE AMPLIFIERS:1||RAREGASES:1||THz radiation:1||FREEELECTRON LASER:1||REALTIME OBSERVATION:1||TARGET:1||photoionized plasmas:1||fs Xray laser:1||emission profile:1||HIGHORDER HARMONICS:1||Xray laser:1||atomic transition:1||EXCITATION:1||LASERS:1||PERFORMANCE:1||RELATIVISTIC ELECTRONS:1||BI2O3DOPED ZNO:1||INNERSHELL IONIZATION:1||Laser wakefield:1||FREQUENCY:1||SOLIDSTATE LASERS:1||Linearly polarized:1||THERMIONIC EMISSION:1||PULSE AMPLIFICATION SYSTEM:1||BIB3O6:1||NM:1||NONCOVALENT INTERACTIONS:1||CRYSTALLINE:1||INTENSITY:1||JETS:1||COHERENT:1||LINE:1||ANGULARDISTRIBUTION:1||SILVER IONS:1||magnetic anisotropy:1||DEVICES:1||Auger transitions:1||CosterKronig transitions:1||EFFICIENT:1||ELECTRONIMPACT IONIZATION:1||ULTRASHORTPULSE:1||Nanowire:1||Heterostructure:1||soft Xray reflectivity:1||PLASMA ACCELERATOR:1||ZINCOXIDE NANOWIRES:1||CHEMICALVAPORDEPOSITION:1||Electron acceleration:1||Ionization of gases:1||Delay dependent:1||MULTIPHOTON IONIZATION:1||FRAGMENTATION:1||GASJET:1||ultrafast nonlinear optics:1||CYCLE PULSES:1||KHZ:1||chemical vapor deposition:1||ferromagnetism:1||ABSORPTION:1||TERAHERTZ RADIATION:1||SCIENCE:1||FIELDS:1||ELECTRONS:1||nanomultilayer structures:1||YIELDS:1||AUGER:1||10HZ REPETITION RATE:1||MULTITERAWATT:1||SPECTROGRAPH:1||HIGHHARMONICGENERATION:1||spectroscopy:1||level population:1||PARTICLEACCELERATION:1||OPTICAL FREQUENCYMEASUREMENT:1||NANOWALLS:1||ROOMTEMPERATURE:1||AVERAGE OUTPUT POWER:1||GROUPVELOCITYMISMATCH:1||Impact ionization:1||Dynamics:1||Lasers:1||Collisional process:1||ABOVETHRESHOLD IONIZATION:1||MAINGROUP THERMOCHEMISTRY:1||dilute magnetic semiconductors:1||GACRN:1||SIZE:1||ATTOSECOND:1||Ar cluster:1||Xray astrophysics:1||photoionization:1||irons:1||normal incidence pulsed laser deposition:1||SHELLS:1||Silicon Oxide:1||gaspuff Zpinch:1||Xray:1||soft Xray reflectors:1||ESCAPE:1||ZN2SIO4:1||SILICA:1||Time 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materials:1||MOLECULAR PHOTOIONIZATION:1||LOCALIZATION:1||DEUTERIUM CLUSTERS:1||EXPLOSIONS:1||REGENERATIVE AMPLIFIERS:1||RAREGASES:1||THz radiation:1||FREEELECTRON LASER:1||REALTIME OBSERVATION:1||TARGET:1||photoionized plasmas:1||fs Xray laser:1||emission profile:1||HIGHORDER HARMONICS:1||Xray laser:1||atomic transition:1||EXCITATION:1||LASERS:1||PERFORMANCE:1||RELATIVISTIC ELECTRONS:1||BI2O3DOPED ZNO:1||INNERSHELL IONIZATION:1||Laser wakefield:1||FREQUENCY:1||SOLIDSTATE LASERS:1||Linearly polarized:1||THERMIONIC EMISSION:1||PULSE AMPLIFICATION SYSTEM:1||BIB3O6:1||NM:1||NONCOVALENT INTERACTIONS:1||CRYSTALLINE:1||INTENSITY:1||JETS:1||COHERENT:1||LINE:1||ANGULARDISTRIBUTION:1||SILVER IONS:1||magnetic anisotropy:1||DEVICES:1||Auger transitions:1||CosterKronig transitions:1||EFFICIENT:1||ELECTRONIMPACT IONIZATION:1||ULTRASHORTPULSE:1||Nanowire:1||Heterostructure:1||soft Xray reflectivity:1||PLASMA ACCELERATOR:1||ZINCOXIDE NANOWIRES:1||CHEMICALVAPORDEPOSITION:1||Electron acceleration:1||Ionization of gases:1||Delay dependent:1||MULTIPHOTON IONIZATION:1||FRAGMENTATION:1||GASJET:1||ultrafast nonlinear optics:1||CYCLE PULSES:1||KHZ:1||chemical vapor deposition:1||ferromagnetism:1||ABSORPTION:1||TERAHERTZ RADIATION:1||SCIENCE:1||FIELDS:1||ELECTRONS:1||nanomultilayer structures:1||YIELDS:1||AUGER:1||10HZ REPETITION RATE:1||MULTITERAWATT:1||SPECTROGRAPH:1||HIGHHARMONICGENERATION:1||spectroscopy:1||level population:1||PARTICLEACCELERATION:1||OPTICAL FREQUENCYMEASUREMENT:1||NANOWALLS:1||ROOMTEMPERATURE:1||AVERAGE OUTPUT POWER:1||GROUPVELOCITYMISMATCH:1||Impact ionization:1||Dynamics:1||Lasers:1||Collisional process:1||ABOVETHRESHOLD IONIZATION:1||MAINGROUP THERMOCHEMISTRY:1||dilute magnetic semiconductors:1||GACRN:1||SIZE:1||ATTOSECOND:1||Ar cluster:1||Xray astrophysics:1||photoionization:1||irons:1||normal incidence pulsed laser deposition:1||SHELLS:1||Silicon Oxide:1||gaspuff Zpinch:1||Xray:1||soft Xray reflectors:1||ESCAPE:1||ZN2SIO4:1||SILICA:1||Time delay:1||Collisional plasmas:1||MASSSPECTROMETRY:1||NUCLEARFUSION:1||PARAMETRIC AMPLIFICATION:1||LYING ELECTRONIC STATES:1||ADJUSTABLEPARAMETERS:1||MAGNETICPROPERTIES:1||LIQUIDPHASE EPITAXY:1||CEP laser:1||REGION:1||Plasma waveguide:1||AMBIENT GAS:1||DEPOSITION:1||HARMONICGENERATION:1||ENHANCEMENT:1||imaging spectrometer:1||Abel inversion:1||Water window:1||Liquid nitrogen jet:1||CHARGEEXCHANGE:1||NOBEL LECTURE:1||VARISTOR:1||EPITAXY:1||THINDISK LASER:1||HIGHREPETITIONRATE:1||Atom lasers:1||Electronimpact excitation:1||High order harmonics:1||ultrafast technology:1||PEAK POWER:1||CHARGED ALUMINUM CLUSTERS:1||GaN:1||THIN:1||Electron beam:1||INTENSE:1||Hard Xray pulse generation:1||NONLINEAR THOMSON SCATTERING:1||MULTILAYER:1||UVvisible spectrometer:1||ATOMS:1||innershell transitions:1||CORRECTED CONCAVE GRATINGS:1||DISCHARGE:1||LASERPLASMA:1||thin film:1||reflectivity:1||opacity:1||gain:1||smallangle Xray scattering:1||SOFTXRAY:1||ZINCOXIDE:1||CYGNUSX3:1||Betatron oscillation:1||ACCELERATOR:1||STRAINEDLAYER SUPERLATTICES:1||OPTICAL PARAMETRIC AMPLIFICATION:1||PASSIVE MODELOCKING:1||Collision dynamics:1||MUM:1||EXACTEXCHANGE:1||BASISSET:1||APPROXIMATION:1||OXYNITRIDES:1||Beam energy modulation:1||polarization spectroscopy:1||REORIENTATION TRANSITION:1||DEPENDENCE:1||sulfurs:1||BUILDINGBLOCKS:1||RATES:1||OPTICAL PULSES:1||toroidal mirror:1||XRAY LASER:1||CALCIUM:1||radially polarized laser:1||GRAINBOUNDARIES:1||VAPORDEPOSITION:1||Xray generation:1||MAGNETIZATION:1||Electric excitation:1||Laserinduced gas plasmas:1||Qualitative analysis:1||SCHEME:1||RADIATION:10||PULSES:8||PHOTOLUMINESCENCE:7||LASER:7||GENERATION:6||NANORODS:6||GROWTH:6||NANOWIRES:5||IMPLANTED GAN:5||SPECTROSCOPY:5||THINFILMS:4||DYNAMICS:4||SILICON:4||EXTREMEULTRAVIOLET:4||AMPLIFICATION:4||PRESSURE:4||PHASE:4||OPTICALPROPERTIES:4||SYSTEM:4||EMISSION:4||FEL:3||N2O:3||FILMS:3||OPTICS:3||SPECTRA:3||FIELD:3||MIRRORS:3||ARRAYS:3||CLUSTERS:3||SIO2:3||IONIZATION:3||VACUUM:3||SCATTERING:3||IONS:2||LUMINESCENCE PROPERTIES:2||ANISOTROPY:2||BEAMS:2||DIFFRACTION:2||DISPERSION:2||chemical vapor deposition (CVD):2||ELECTRONICSTRUCTURE:2||MOSFETS:2||SI3N4:2||DENSITY:2||LIGHT:2||PLASMAS:2||MATTER:2||nanocomposites:2||RAMANSCATTERING:2||NANOPARTICLES:2||OXIDE:2||AMPLIFIED SPONTANEOUS EMISSION:2||NM WAVELENGTH:2||GAIN:2||CARBON NANOTUBES:2||CROSSSECTIONS:2||LIGHTEMITTINGDIODES:2||PULSE:2||CARBON PLASMA:2||TISAPPHIRE LASER:2||Raman scattering:2||ROUTE:2||multilayer:2||CATHODOLUMINESCENCE:2||highresolution transmission electronic microscope (HRTEM):2||DIFFERENCEFREQUENCYGENERATION:2||CRYSTAL:2||laserproduced plasma:2||NANOCABLES:2||photoluminescence:2||MAGNETIC ALLOY SEMICONDUCTORS:2||MOLECULARBEAM EPITAXY:2||EARTHDOPED GAN:2||LASER FIELDS:2||CHIRPEDPULSEAMPLIFICATION:2||ALN:2||GAUSSIANBEAM:2||ASSISTED CATALYTIC GROWTH:2||BLUE:2||NANOSTRUCTURES:2||MAGNETOELECTRONICS:2||MICROSCOPY:2||ELECTROLUMINESCENCE:2||LASERPULSES:2||GaN nanowires:2||GALLIUM NITRIDE NANOWIRES:2||GAMNN:2||NANOTUBES:2||PHYSICS:2||Femtosecond laser:2||parametric oscillators and amplifiers:1||ultrafast lasers:1||VALENCE:1||nanowires:1||DILUTED MAGNETIC SEMICONDUCTOR:1||LUMINESCENCE:1||Density modulation:1||Energy modulation:1||Current enhanced SASE free electron laser:1||Undulator radiation:1||FREEELECTRON LASERS:1||ULTRATHIN FERROMAGNETICFILMS:1||OXIDEFILMS:1||ABLATION:1||COMPONENT:1||METAL:1||innershell excited states:1||Nelike ions:1||TRANSITIONS:1||XUV spectrometer:1||DIAGNOSTICS:1||Xray scattering:1||MO/SI:1||pulsed laser deposition:1||KEV IMPACT ENERGIES:1||vacuum electron acceleration:1||HIGHINTENSITY LASER:1||JUNCTIONS:1||LOWTEMPERATURE GROWTH:1||nanocrystalline materials:1||MOLECULAR PHOTOIONIZATION:1||LOCALIZATION:1||DEUTERIUM CLUSTERS:1||EXPLOSIONS:1||REGENERATIVE AMPLIFIERS:1||RAREGASES:1||THz radiation:1||FREEELECTRON LASER:1||REALTIME OBSERVATION:1||TARGET:1||photoionized plasmas:1||fs Xray laser:1||emission profile:1||HIGHORDER HARMONICS:1||Xray laser:1||atomic transition:1||EXCITATION:1||LASERS:1||PERFORMANCE:1||RELATIVISTIC ELECTRONS:1||BI2O3DOPED ZNO:1||INNERSHELL IONIZATION:1||Laser wakefield:1||FREQUENCY:1||SOLIDSTATE LASERS:1||Linearly polarized:1||THERMIONIC EMISSION:1||PULSE AMPLIFICATION SYSTEM:1||BIB3O6:1||NM:1||NONCOVALENT INTERACTIONS:1||CRYSTALLINE:1||INTENSITY:1||JETS:1||COHERENT:1||LINE:1||ANGULARDISTRIBUTION:1||SILVER IONS:1||magnetic anisotropy:1||DEVICES:1||Auger transitions:1||CosterKronig transitions:1||EFFICIENT:1||ELECTRONIMPACT IONIZATION:1||ULTRASHORTPULSE:1||Nanowire:1||Heterostructure:1||soft Xray reflectivity:1||PLASMA ACCELERATOR:1||ZINCOXIDE NANOWIRES:1||CHEMICALVAPORDEPOSITION:1||Electron acceleration:1||Ionization of gases:1||Delay dependent:1||MULTIPHOTON IONIZATION:1||FRAGMENTATION:1||GASJET:1||ultrafast nonlinear optics:1||CYCLE PULSES:1||KHZ:1||chemical vapor deposition:1||ferromagnetism:1||ABSORPTION:1||TERAHERTZ RADIATION:1||SCIENCE:1||FIELDS:1||ELECTRONS:1||nanomultilayer structures:1||YIELDS:1||AUGER:1||10HZ REPETITION RATE:1||MULTITERAWATT:1||SPECTROGRAPH:1||HIGHHARMONICGENERATION:1||spectroscopy:1||level population:1||PARTICLEACCELERATION:1||OPTICAL FREQUENCYMEASUREMENT:1||NANOWALLS:1||ROOMTEMPERATURE:1||AVERAGE OUTPUT POWER:1||GROUPVELOCITYMISMATCH:1||Impact ionization:1||Dynamics:1||Lasers:1||Collisional process:1||ABOVETHRESHOLD IONIZATION:1||MAINGROUP THERMOCHEMISTRY:1||dilute magnetic semiconductors:1||GACRN:1||SIZE:1||ATTOSECOND:1||Ar cluster:1||Xray astrophysics:1||photoionization:1||irons:1||normal incidence pulsed laser deposition:1||SHELLS:1||Silicon Oxide:1||gaspuff Zpinch:1||Xray:1||soft Xray reflectors:1||ESCAPE:1||ZN2SIO4:1||SILICA:1||Time delay:1||Collisional plasmas:1||MASSSPECTROMETRY:1||NUCLEARFUSION:1||PARAMETRIC AMPLIFICATION:1||LYING ELECTRONIC STATES:1||ADJUSTABLEPARAMETERS:1||MAGNETICPROPERTIES:1||LIQUIDPHASE EPITAXY:1||CEP laser:1||REGION:1||Plasma waveguide:1||AMBIENT GAS:1||DEPOSITION:1||HARMONICGENERATION:1||ENHANCEMENT:1||imaging spectrometer:1||Abel inversion:1||Water window:1||Liquid nitrogen jet:1||CHARGEEXCHANGE:1||NOBEL LECTURE:1||VARISTOR:1||EPITAXY:1||THINDISK LASER:1||HIGHREPETITIONRATE:1||Atom lasers:1||Electronimpact excitation:1||High order harmonics:1||ultrafast technology:1||PEAK POWER:1||CHARGED ALUMINUM CLUSTERS:1||GaN:1||THIN:1||Electron beam:1||INTENSE:1||Hard Xray pulse generation:1||NONLINEAR THOMSON SCATTERING:1||MULTILAYER:1||UVvisible spectrometer:1||ATOMS:1||innershell transitions:1||CORRECTED CONCAVE GRATINGS:1||DISCHARGE:1||LASERPLASMA:1||thin film:1||reflectivity:1||opacity:1||gain:1||smallangle Xray scattering:1||SOFTXRAY:1||ZINCOXIDE:1||CYGNUSX3:1||Betatron oscillation:1||ACCELERATOR:1||STRAINEDLAYER SUPERLATTICES:1||OPTICAL PARAMETRIC AMPLIFICATION:1||PASSIVE MODELOCKING:1||Collision dynamics:1||MUM:1||EXACTEXCHANGE:1||BASISSET:1||APPROXIMATION:1||OXYNITRIDES:1||Beam energy modulation:1||polarization spectroscopy:1||REORIENTATION TRANSITION:1||DEPENDENCE:1||sulfurs:1||BUILDINGBLOCKS:1||RATES:1||OPTICAL PULSES:1||toroidal mirror:1||XRAY LASER:1||CALCIUM:1||radially polarized laser:1||GRAINBOUNDARIES:1||VAPORDEPOSITION:1||Xray generation:1||MAGNETIZATION:1||Electric excitation:1||Laserinduced gas plasmas:1||Qualitative analysis:1||SCHEME:1||RADIATION:10||PULSES:8||PHOTOLUMINESCENCE:7||LASER:7||GENERATION:6||NANORODS:6||GROWTH:6||NANOWIRES:5||IMPLANTED 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SEMICONDUCTORS:2||MOLECULARBEAM EPITAXY:2||EARTHDOPED GAN:2||LASER FIELDS:2||CHIRPEDPULSEAMPLIFICATION:2||ALN:2||GAUSSIANBEAM:2||ASSISTED CATALYTIC GROWTH:2||BLUE:2||NANOSTRUCTURES:2||MAGNETOELECTRONICS:2||MICROSCOPY:2||ELECTROLUMINESCENCE:2||LASERPULSES:2||GaN nanowires:2||GALLIUM NITRIDE NANOWIRES:2||GAMNN:2||NANOTUBES:2||PHYSICS:2||Femtosecond laser:2||parametric oscillators and amplifiers:1||ultrafast lasers:1||VALENCE:1||nanowires:1||DILUTED MAGNETIC SEMICONDUCTOR:1||LUMINESCENCE:1||Density modulation:1||Energy modulation:1||Current enhanced SASE free electron laser:1||Undulator radiation:1||FREEELECTRON LASERS:1||ULTRATHIN FERROMAGNETICFILMS:1||OXIDEFILMS:1||ABLATION:1||COMPONENT:1||METAL:1||innershell excited states:1||Nelike ions:1||TRANSITIONS:1||XUV spectrometer:1||DIAGNOSTICS:1||Xray scattering:1||MO/SI:1||pulsed laser deposition:1||KEV IMPACT ENERGIES:1||vacuum electron acceleration:1||HIGHINTENSITY LASER:1||JUNCTIONS:1||LOWTEMPERATURE GROWTH:1||nanocrystalline materials:1||MOLECULAR PHOTOIONIZATION:1||LOCALIZATION:1||DEUTERIUM CLUSTERS:1||EXPLOSIONS:1||REGENERATIVE AMPLIFIERS:1||RAREGASES:1||THz radiation:1||FREEELECTRON LASER:1||REALTIME OBSERVATION:1||TARGET:1||photoionized plasmas:1||fs Xray laser:1||emission profile:1||HIGHORDER HARMONICS:1||Xray laser:1||atomic transition:1||EXCITATION:1||LASERS:1||PERFORMANCE:1||RELATIVISTIC ELECTRONS:1||BI2O3DOPED ZNO:1||INNERSHELL IONIZATION:1||Laser wakefield:1||FREQUENCY:1||SOLIDSTATE LASERS:1||Linearly polarized:1||THERMIONIC EMISSION:1||PULSE AMPLIFICATION SYSTEM:1||BIB3O6:1||NM:1||NONCOVALENT INTERACTIONS:1||CRYSTALLINE:1||INTENSITY:1||JETS:1||COHERENT:1||LINE:1||ANGULARDISTRIBUTION:1||SILVER IONS:1||magnetic anisotropy:1||DEVICES:1||Auger transitions:1||CosterKronig transitions:1||EFFICIENT:1||ELECTRONIMPACT IONIZATION:1||ULTRASHORTPULSE:1||Nanowire:1||Heterostructure:1||soft Xray reflectivity:1||PLASMA ACCELERATOR:1||ZINCOXIDE NANOWIRES:1||CHEMICALVAPORDEPOSITION:1||Electron acceleration:1||Ionization of gases:1||Delay dependent:1||MULTIPHOTON IONIZATION:1||FRAGMENTATION:1||GASJET:1||ultrafast nonlinear optics:1||CYCLE PULSES:1||KHZ:1||chemical vapor deposition:1||ferromagnetism:1||ABSORPTION:1||TERAHERTZ RADIATION:1||SCIENCE:1||FIELDS:1||ELECTRONS:1||nanomultilayer structures:1||YIELDS:1||AUGER:1||10HZ REPETITION RATE:1||MULTITERAWATT:1||SPECTROGRAPH:1||HIGHHARMONICGENERATION:1||spectroscopy:1||level population:1||PARTICLEACCELERATION:1||OPTICAL FREQUENCYMEASUREMENT:1||NANOWALLS:1||ROOMTEMPERATURE:1||AVERAGE OUTPUT POWER:1||GROUPVELOCITYMISMATCH:1||Impact ionization:1||Dynamics:1||Lasers:1||Collisional process:1||ABOVETHRESHOLD IONIZATION:1||MAINGROUP THERMOCHEMISTRY:1||dilute magnetic semiconductors:1||GACRN:1||SIZE:1||ATTOSECOND:1||Ar cluster:1||Xray astrophysics:1||photoionization:1||irons:1||normal incidence pulsed laser deposition:1||SHELLS:1||Silicon Oxide:1||gaspuff Zpinch:1||Xray:1||soft Xray reflectors:1||ESCAPE:1||ZN2SIO4:1||SILICA:1||Time 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materials:1||MOLECULAR PHOTOIONIZATION:1||LOCALIZATION:1||DEUTERIUM CLUSTERS:1||EXPLOSIONS:1||REGENERATIVE AMPLIFIERS:1||RAREGASES:1||THz radiation:1||FREEELECTRON LASER:1||REALTIME OBSERVATION:1||TARGET:1||photoionized plasmas:1||fs Xray laser:1||emission profile:1||HIGHORDER HARMONICS:1||Xray laser:1||atomic transition:1||EXCITATION:1||LASERS:1||PERFORMANCE:1||RELATIVISTIC ELECTRONS:1||BI2O3DOPED ZNO:1||INNERSHELL IONIZATION:1||Laser wakefield:1||FREQUENCY:1||SOLIDSTATE LASERS:1||Linearly polarized:1||THERMIONIC EMISSION:1||PULSE AMPLIFICATION SYSTEM:1||BIB3O6:1||NM:1||NONCOVALENT INTERACTIONS:1||CRYSTALLINE:1||INTENSITY:1||JETS:1||COHERENT:1||LINE:1||ANGULARDISTRIBUTION:1||SILVER IONS:1||magnetic anisotropy:1||DEVICES:1||Auger transitions:1||CosterKronig transitions:1||EFFICIENT:1||ELECTRONIMPACT IONIZATION:1||ULTRASHORTPULSE:1||Nanowire:1||Heterostructure:1||soft Xray reflectivity:1||PLASMA ACCELERATOR:1||ZINCOXIDE NANOWIRES:1||CHEMICALVAPORDEPOSITION:1||Electron acceleration:1||Ionization of gases:1||Delay dependent:1||MULTIPHOTON IONIZATION:1||FRAGMENTATION:1||GASJET:1||ultrafast nonlinear optics:1||CYCLE PULSES:1||KHZ:1||chemical vapor deposition:1||ferromagnetism:1||ABSORPTION:1||TERAHERTZ RADIATION:1||SCIENCE:1||FIELDS:1||ELECTRONS:1||nanomultilayer structures:1||YIELDS:1||AUGER:1||10HZ REPETITION RATE:1||MULTITERAWATT:1||SPECTROGRAPH:1||HIGHHARMONICGENERATION:1||spectroscopy:1||level population:1||PARTICLEACCELERATION:1||OPTICAL FREQUENCYMEASUREMENT:1||NANOWALLS:1||ROOMTEMPERATURE:1||AVERAGE OUTPUT POWER:1||GROUPVELOCITYMISMATCH:1||Impact ionization:1||Dynamics:1||Lasers:1||Collisional process:1||ABOVETHRESHOLD IONIZATION:1||MAINGROUP THERMOCHEMISTRY:1||dilute magnetic semiconductors:1||GACRN:1||SIZE:1||ATTOSECOND:1||Ar cluster:1||Xray astrophysics:1||photoionization:1||irons:1||normal incidence pulsed laser deposition:1||SHELLS:1||Silicon Oxide:1||gaspuff Zpinch:1||Xray:1||soft Xray reflectors:1||ESCAPE:1||ZN2SIO4:1||SILICA:1||Time delay:1||Collisional plasmas:1||MASSSPECTROMETRY:1||NUCLEARFUSION:1||PARAMETRIC AMPLIFICATION:1||LYING ELECTRONIC STATES:1||ADJUSTABLEPARAMETERS:1||MAGNETICPROPERTIES:1||LIQUIDPHASE EPITAXY:1||CEP laser:1||REGION:1||Plasma waveguide:1||AMBIENT GAS:1||DEPOSITION:1||HARMONICGENERATION:1||ENHANCEMENT:1||imaging spectrometer:1||Abel inversion:1||Water window:1||Liquid nitrogen jet:1||CHARGEEXCHANGE:1||NOBEL LECTURE:1||VARISTOR:1||EPITAXY:1||THINDISK LASER:1||HIGHREPETITIONRATE:1||Atom lasers:1||Electronimpact excitation:1||High order harmonics:1||ultrafast technology:1||PEAK POWER:1||CHARGED ALUMINUM CLUSTERS:1||GaN:1||THIN:1||Electron beam:1||INTENSE:1||Hard Xray pulse generation:1||NONLINEAR THOMSON SCATTERING:1||MULTILAYER:1||UVvisible spectrometer:1||ATOMS:1||innershell transitions:1||CORRECTED CONCAVE GRATINGS:1||DISCHARGE:1||LASERPLASMA:1||thin film:1||reflectivity:1||opacity:1||gain:1||smallangle Xray scattering:1||SOFTXRAY:1||ZINCOXIDE:1||CYGNUSX3:1||Betatron oscillation:1||ACCELERATOR:1||STRAINEDLAYER SUPERLATTICES:1||OPTICAL PARAMETRIC AMPLIFICATION:1||PASSIVE MODELOCKING:1||Collision dynamics:1||MUM:1||EXACTEXCHANGE:1||BASISSET:1||APPROXIMATION:1||OXYNITRIDES:1||Beam energy modulation:1||polarization spectroscopy:1||REORIENTATION TRANSITION:1||DEPENDENCE:1||sulfurs:1||BUILDINGBLOCKS:1||RATES:1||OPTICAL PULSES:1||toroidal mirror:1||XRAY LASER:1||CALCIUM:1||radially polarized laser:1||GRAINBOUNDARIES:1||VAPORDEPOSITION:1||Xray generation:1||MAGNETIZATION:1||Electric excitation:1||Laserinduced gas plasmas:1||Qualitative analysis:1||SCHEME:1||RADIATION:10||PULSES:8||PHOTOLUMINESCENCE:7||LASER:7||GENERATION:6||NANORODS:6||GROWTH:6||NANOWIRES:5||IMPLANTED GAN:5||SPECTROSCOPY:5||THINFILMS:4||DYNAMICS:4||SILICON:4||EXTREMEULTRAVIOLET:4||AMPLIFICATION:4||PRESSURE:4||PHASE:4||OPTICALPROPERTIES:4||SYSTEM:4||EMISSION:4||FEL:3||N2O:3||FILMS:3||OPTICS:3||SPECTRA:3||FIELD:3||MIRRORS:3||ARRAYS:3||CLUSTERS:3||SIO2:3||IONIZATION:3||VACUUM:3||SCATTERING:3||IONS:2||LUMINESCENCE PROPERTIES:2||ANISOTROPY:2||BEAMS:2||DIFFRACTION:2||DISPERSION:2||chemical vapor deposition (CVD):2||ELECTRONICSTRUCTURE:2||MOSFETS:2||SI3N4:2||DENSITY:2||LIGHT:2||PLASMAS:2||MATTER:2||nanocomposites:2||RAMANSCATTERING:2||NANOPARTICLES:2||OXIDE:2||AMPLIFIED SPONTANEOUS EMISSION:2||NM WAVELENGTH:2||GAIN:2||CARBON NANOTUBES:2||CROSSSECTIONS:2||LIGHTEMITTINGDIODES:2||PULSE:2||CARBON PLASMA:2||TISAPPHIRE LASER:2||Raman scattering:2||ROUTE:2||multilayer:2||CATHODOLUMINESCENCE:2||highresolution transmission electronic microscope (HRTEM):2||DIFFERENCEFREQUENCYGENERATION:2||CRYSTAL:2||laserproduced plasma:2||NANOCABLES:2||photoluminescence:2||MAGNETIC ALLOY SEMICONDUCTORS:2||MOLECULARBEAM EPITAXY:2||EARTHDOPED GAN:2||LASER FIELDS:2||CHIRPEDPULSEAMPLIFICATION:2||ALN:2||GAUSSIANBEAM:2||ASSISTED CATALYTIC GROWTH:2||BLUE:2||NANOSTRUCTURES:2||MAGNETOELECTRONICS:2||MICROSCOPY:2||ELECTROLUMINESCENCE:2||LASERPULSES:2||GaN nanowires:2||GALLIUM NITRIDE NANOWIRES:2||GAMNN:2||NANOTUBES:2||PHYSICS:2||Femtosecond laser:2||parametric oscillators and amplifiers:1||ultrafast lasers:1||VALENCE:1||nanowires:1||DILUTED MAGNETIC SEMICONDUCTOR:1||LUMINESCENCE:1||Density modulation:1||Energy modulation:1||Current enhanced SASE free electron laser:1||Undulator radiation:1||FREEELECTRON LASERS:1||ULTRATHIN FERROMAGNETICFILMS:1||OXIDEFILMS:1||ABLATION:1||COMPONENT:1||METAL:1||innershell excited states:1||Nelike ions:1||TRANSITIONS:1||XUV spectrometer:1||DIAGNOSTICS:1||Xray scattering:1||MO/SI:1||pulsed laser deposition:1||KEV IMPACT ENERGIES:1||vacuum electron acceleration:1||HIGHINTENSITY LASER:1||JUNCTIONS:1||LOWTEMPERATURE GROWTH:1||nanocrystalline materials:1||MOLECULAR PHOTOIONIZATION:1||LOCALIZATION:1||DEUTERIUM CLUSTERS:1||EXPLOSIONS:1||REGENERATIVE AMPLIFIERS:1||RAREGASES:1||THz radiation:1||FREEELECTRON LASER:1||REALTIME OBSERVATION:1||TARGET:1||photoionized plasmas:1||fs Xray laser:1||emission profile:1||HIGHORDER HARMONICS:1||Xray laser:1||atomic transition:1||EXCITATION:1||LASERS:1||PERFORMANCE:1||RELATIVISTIC ELECTRONS:1||BI2O3DOPED ZNO:1||INNERSHELL IONIZATION:1||Laser wakefield:1||FREQUENCY:1||SOLIDSTATE LASERS:1||Linearly polarized:1||THERMIONIC EMISSION:1||PULSE AMPLIFICATION SYSTEM:1||BIB3O6:1||NM:1||NONCOVALENT INTERACTIONS:1||CRYSTALLINE:1||INTENSITY:1||JETS:1||COHERENT:1||LINE:1||ANGULARDISTRIBUTION:1||SILVER IONS:1||magnetic anisotropy:1||DEVICES:1||Auger transitions:1||CosterKronig transitions:1||EFFICIENT:1||ELECTRONIMPACT IONIZATION:1||ULTRASHORTPULSE:1||Nanowire:1||Heterostructure:1||soft Xray reflectivity:1||PLASMA ACCELERATOR:1||ZINCOXIDE NANOWIRES:1||CHEMICALVAPORDEPOSITION:1||Electron acceleration:1||Ionization of gases:1||Delay dependent:1||MULTIPHOTON IONIZATION:1||FRAGMENTATION:1||GASJET:1||ultrafast nonlinear optics:1||CYCLE PULSES:1||KHZ:1||chemical vapor deposition:1||ferromagnetism:1||ABSORPTION:1||TERAHERTZ RADIATION:1||SCIENCE:1||FIELDS:1||ELECTRONS:1||nanomultilayer structures:1||YIELDS:1||AUGER:1||10HZ REPETITION RATE:1||MULTITERAWATT:1||SPECTROGRAPH:1||HIGHHARMONICGENERATION:1||spectroscopy:1||level population:1||PARTICLEACCELERATION:1||OPTICAL FREQUENCYMEASUREMENT:1||NANOWALLS:1||ROOMTEMPERATURE:1||AVERAGE OUTPUT POWER:1||GROUPVELOCITYMISMATCH:1||Impact ionization:1||Dynamics:1||Lasers:1||Collisional process:1||ABOVETHRESHOLD IONIZATION:1||MAINGROUP THERMOCHEMISTRY:1||dilute magnetic semiconductors:1||GACRN:1||SIZE:1||ATTOSECOND:1||Ar cluster:1||Xray astrophysics:1||photoionization:1||irons:1||normal incidence pulsed laser deposition:1||SHELLS:1||Silicon Oxide:1||gaspuff Zpinch:1||Xray:1||soft Xray reflectors:1||ESCAPE:1||ZN2SIO4:1||SILICA:1||Time delay:1||Collisional plasmas:1||MASSSPECTROMETRY:1||NUCLEARFUSION:1||PARAMETRIC AMPLIFICATION:1||LYING ELECTRONIC STATES:1||ADJUSTABLEPARAMETERS:1||MAGNETICPROPERTIES:1||LIQUIDPHASE EPITAXY:1||CEP laser:1||REGION:1||Plasma waveguide:1||AMBIENT GAS:1||DEPOSITION:1||HARMONICGENERATION:1||ENHANCEMENT:1||imaging spectrometer:1||Abel inversion:1||Water window:1||Liquid nitrogen jet:1||CHARGEEXCHANGE:1||NOBEL LECTURE:1||VARISTOR:1||EPITAXY:1||THINDISK LASER:1||HIGHREPETITIONRATE:1||Atom lasers:1||Electronimpact excitation:1||High order harmonics:1||ultrafast technology:1||PEAK POWER:1||CHARGED ALUMINUM CLUSTERS:1||GaN:1||THIN:1||Electron beam:1||INTENSE:1||Hard Xray pulse generation:1||NONLINEAR THOMSON SCATTERING:1||MULTILAYER:1||UVvisible spectrometer:1||ATOMS:1||innershell transitions:1||CORRECTED CONCAVE GRATINGS:1||DISCHARGE:1||LASERPLASMA:1||thin film:1||reflectivity:1||opacity:1||gain:1||smallangle Xray scattering:1||SOFTXRAY:1||ZINCOXIDE:1||CYGNUSX3:1||Betatron oscillation:1||ACCELERATOR:1||STRAINEDLAYER SUPERLATTICES:1||OPTICAL PARAMETRIC AMPLIFICATION:1||PASSIVE MODELOCKING:1||Collision dynamics:1||MUM:1||EXACTEXCHANGE:1||BASISSET:1||APPROXIMATION:1||OXYNITRIDES:1||Beam energy modulation:1||polarization spectroscopy:1||REORIENTATION TRANSITION:1||DEPENDENCE:1||sulfurs:1||BUILDINGBLOCKS:1||RATES:1||OPTICAL PULSES:1||toroidal mirror:1||XRAY LASER:1||CALCIUM:1||radially polarized laser:1||GRAINBOUNDARIES:1||VAPORDEPOSITION:1||Xray generation:1||MAGNETIZATION:1||Electric excitation:1||Laserinduced gas plasmas:1||Qualitative analysis:1||SCHEME:1||RADIATION:10||PULSES:8||PHOTOLUMINESCENCE:7||LASER:7||GENERATION:6||NANORODS:6||GROWTH:6||NANOWIRES:5||IMPLANTED 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SEMICONDUCTORS:2||MOLECULARBEAM EPITAXY:2||EARTHDOPED GAN:2||LASER FIELDS:2||CHIRPEDPULSEAMPLIFICATION:2||ALN:2||GAUSSIANBEAM:2||ASSISTED CATALYTIC GROWTH:2||BLUE:2||NANOSTRUCTURES:2||MAGNETOELECTRONICS:2||MICROSCOPY:2||ELECTROLUMINESCENCE:2||LASERPULSES:2||GaN nanowires:2||GALLIUM NITRIDE NANOWIRES:2||GAMNN:2||NANOTUBES:2||PHYSICS:2||Femtosecond laser:2||parametric oscillators and amplifiers:1||ultrafast lasers:1||VALENCE:1||nanowires:1||DILUTED MAGNETIC SEMICONDUCTOR:1||LUMINESCENCE:1||Density modulation:1||Energy modulation:1||Current enhanced SASE free electron laser:1||Undulator radiation:1||FREEELECTRON LASERS:1||ULTRATHIN FERROMAGNETICFILMS:1||OXIDEFILMS:1||ABLATION:1||COMPONENT:1||METAL:1||innershell excited states:1||Nelike ions:1||TRANSITIONS:1||XUV spectrometer:1||DIAGNOSTICS:1||Xray scattering:1||MO/SI:1||pulsed laser deposition:1||KEV IMPACT ENERGIES:1||vacuum electron acceleration:1||HIGHINTENSITY LASER:1||JUNCTIONS:1||LOWTEMPERATURE GROWTH:1||nanocrystalline materials:1||MOLECULAR PHOTOIONIZATION:1||LOCALIZATION:1||DEUTERIUM CLUSTERS:1||EXPLOSIONS:1||REGENERATIVE AMPLIFIERS:1||RAREGASES:1||THz radiation:1||FREEELECTRON LASER:1||REALTIME OBSERVATION:1||TARGET:1||photoionized plasmas:1||fs Xray laser:1||emission profile:1||HIGHORDER HARMONICS:1||Xray laser:1||atomic transition:1||EXCITATION:1||LASERS:1||PERFORMANCE:1||RELATIVISTIC ELECTRONS:1||BI2O3DOPED ZNO:1||INNERSHELL IONIZATION:1||Laser wakefield:1||FREQUENCY:1||SOLIDSTATE LASERS:1||Linearly polarized:1||THERMIONIC EMISSION:1||PULSE AMPLIFICATION SYSTEM:1||BIB3O6:1||NM:1||NONCOVALENT INTERACTIONS:1||CRYSTALLINE:1||INTENSITY:1||JETS:1||COHERENT:1||LINE:1||ANGULARDISTRIBUTION:1||SILVER IONS:1||magnetic anisotropy:1||DEVICES:1||Auger transitions:1||CosterKronig transitions:1||EFFICIENT:1||ELECTRONIMPACT IONIZATION:1||ULTRASHORTPULSE:1||Nanowire:1||Heterostructure:1||soft Xray reflectivity:1||PLASMA ACCELERATOR:1||ZINCOXIDE NANOWIRES:1||CHEMICALVAPORDEPOSITION:1||Electron acceleration:1||Ionization of gases:1||Delay dependent:1||MULTIPHOTON IONIZATION:1||FRAGMENTATION:1||GASJET:1||ultrafast nonlinear optics:1||CYCLE PULSES:1||KHZ:1||chemical vapor deposition:1||ferromagnetism:1||ABSORPTION:1||TERAHERTZ RADIATION:1||SCIENCE:1||FIELDS:1||ELECTRONS:1||nanomultilayer structures:1||YIELDS:1||AUGER:1||10HZ REPETITION RATE:1||MULTITERAWATT:1||SPECTROGRAPH:1||HIGHHARMONICGENERATION:1||spectroscopy:1||level population:1||PARTICLEACCELERATION:1||OPTICAL FREQUENCYMEASUREMENT:1||NANOWALLS:1||ROOMTEMPERATURE:1||AVERAGE OUTPUT POWER:1||GROUPVELOCITYMISMATCH:1||Impact ionization:1||Dynamics:1||Lasers:1||Collisional process:1||ABOVETHRESHOLD IONIZATION:1||MAINGROUP THERMOCHEMISTRY:1||dilute magnetic semiconductors:1||GACRN:1||SIZE:1||ATTOSECOND:1||Ar cluster:1||Xray astrophysics:1||photoionization:1||irons:1||normal incidence pulsed laser deposition:1||SHELLS:1||Silicon Oxide:1||gaspuff Zpinch:1||Xray:1||soft Xray reflectors:1||ESCAPE:1||ZN2SIO4:1||SILICA:1||Time 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materials:1||MOLECULAR PHOTOIONIZATION:1||LOCALIZATION:1||DEUTERIUM CLUSTERS:1||EXPLOSIONS:1||REGENERATIVE AMPLIFIERS:1||RAREGASES:1||THz radiation:1||FREEELECTRON LASER:1||REALTIME OBSERVATION:1||TARGET:1||photoionized plasmas:1||fs Xray laser:1||emission profile:1||HIGHORDER HARMONICS:1||Xray laser:1||atomic transition:1||EXCITATION:1||LASERS:1||PERFORMANCE:1||RELATIVISTIC ELECTRONS:1||BI2O3DOPED ZNO:1||INNERSHELL IONIZATION:1||Laser wakefield:1||FREQUENCY:1||SOLIDSTATE LASERS:1||Linearly polarized:1||THERMIONIC EMISSION:1||PULSE AMPLIFICATION SYSTEM:1||BIB3O6:1||NM:1||NONCOVALENT INTERACTIONS:1||CRYSTALLINE:1||INTENSITY:1||JETS:1||COHERENT:1||LINE:1||ANGULARDISTRIBUTION:1||SILVER IONS:1||magnetic anisotropy:1||DEVICES:1||Auger transitions:1||CosterKronig transitions:1||EFFICIENT:1||ELECTRONIMPACT IONIZATION:1||ULTRASHORTPULSE:1||Nanowire:1||Heterostructure:1||soft Xray reflectivity:1||PLASMA ACCELERATOR:1||ZINCOXIDE NANOWIRES:1||CHEMICALVAPORDEPOSITION:1||Electron acceleration:1||Ionization of gases:1||Delay dependent:1||MULTIPHOTON IONIZATION:1||FRAGMENTATION:1||GASJET:1||ultrafast nonlinear optics:1||CYCLE PULSES:1||KHZ:1||chemical vapor deposition:1||ferromagnetism:1||ABSORPTION:1||TERAHERTZ RADIATION:1||SCIENCE:1||FIELDS:1||ELECTRONS:1||nanomultilayer structures:1||YIELDS:1||AUGER:1||10HZ REPETITION RATE:1||MULTITERAWATT:1||SPECTROGRAPH:1||HIGHHARMONICGENERATION:1||spectroscopy:1||level population:1||PARTICLEACCELERATION:1||OPTICAL FREQUENCYMEASUREMENT:1||NANOWALLS:1||ROOMTEMPERATURE:1||AVERAGE OUTPUT POWER:1||GROUPVELOCITYMISMATCH:1||Impact ionization:1||Dynamics:1||Lasers:1||Collisional process:1||ABOVETHRESHOLD IONIZATION:1||MAINGROUP THERMOCHEMISTRY:1||dilute magnetic semiconductors:1||GACRN:1||SIZE:1||ATTOSECOND:1||Ar cluster:1||Xray astrophysics:1||photoionization:1||irons:1||normal incidence pulsed laser deposition:1||SHELLS:1||Silicon Oxide:1||gaspuff Zpinch:1||Xray:1||soft Xray reflectors:1||ESCAPE:1||ZN2SIO4:1||SILICA:1||Time delay:1||Collisional plasmas:1||MASSSPECTROMETRY:1||NUCLEARFUSION:1||PARAMETRIC AMPLIFICATION:1||LYING ELECTRONIC STATES:1||ADJUSTABLEPARAMETERS:1||MAGNETICPROPERTIES:1||LIQUIDPHASE EPITAXY:1||CEP laser:1||REGION:1||Plasma waveguide:1||AMBIENT GAS:1||DEPOSITION:1||HARMONICGENERATION:1||ENHANCEMENT:1||imaging spectrometer:1||Abel inversion:1||Water window:1||Liquid nitrogen jet:1||CHARGEEXCHANGE:1||NOBEL LECTURE:1||VARISTOR:1||EPITAXY:1||THINDISK LASER:1||HIGHREPETITIONRATE:1||Atom lasers:1||Electronimpact excitation:1||High order harmonics:1||ultrafast technology:1||PEAK POWER:1||CHARGED ALUMINUM CLUSTERS:1||GaN:1||THIN:1||Electron beam:1||INTENSE:1||Hard Xray pulse generation:1||NONLINEAR THOMSON SCATTERING:1||MULTILAYER:1||UVvisible spectrometer:1||ATOMS:1||innershell transitions:1||CORRECTED CONCAVE GRATINGS:1||DISCHARGE:1||LASERPLASMA:1||thin film:1||reflectivity:1||opacity:1||gain:1||smallangle Xray scattering:1||SOFTXRAY:1||ZINCOXIDE:1||CYGNUSX3:1||Betatron oscillation:1||ACCELERATOR:1||STRAINEDLAYER SUPERLATTICES:1||OPTICAL PARAMETRIC AMPLIFICATION:1||PASSIVE MODELOCKING:1||Collision dynamics:1||MUM:1||EXACTEXCHANGE:1||BASISSET:1||APPROXIMATION:1||OXYNITRIDES:1||Beam energy modulation:1||polarization spectroscopy:1||REORIENTATION TRANSITION:1||DEPENDENCE:1||sulfurs:1||BUILDINGBLOCKS:1||RATES:1||OPTICAL PULSES:1||toroidal mirror:1||XRAY LASER:1||CALCIUM:1||radially polarized laser:1||GRAINBOUNDARIES:1||VAPORDEPOSITION:1||Xray generation:1||MAGNETIZATION:1||Electric excitation:1||Laserinduced gas plasmas:1||Qualitative analysis:1||SCHEME:1||RADIATION:10||PULSES:8||PHOTOLUMINESCENCE:7||LASER:7||GENERATION:6||NANORODS:6||GROWTH:6||NANOWIRES:5||IMPLANTED GAN:5||SPECTROSCOPY:5||THINFILMS:4||DYNAMICS:4||SILICON:4||EXTREMEULTRAVIOLET:4||AMPLIFICATION:4||PRESSURE:4||PHASE:4||OPTICALPROPERTIES:4||SYSTEM:4||EMISSION:4||FEL:3||N2O:3||FILMS:3||OPTICS:3||SPECTRA:3||FIELD:3||MIRRORS:3||ARRAYS:3||CLUSTERS:3||SIO2:3||IONIZATION:3||VACUUM:3||SCATTERING:3||IONS:2||LUMINESCENCE PROPERTIES:2||ANISOTROPY:2||BEAMS:2||DIFFRACTION:2||DISPERSION:2||chemical vapor deposition (CVD):2||ELECTRONICSTRUCTURE:2||MOSFETS:2||SI3N4:2||DENSITY:2||LIGHT:2||PLASMAS:2||MATTER:2||nanocomposites:2||RAMANSCATTERING:2||NANOPARTICLES:2||OXIDE:2||AMPLIFIED SPONTANEOUS EMISSION:2||NM WAVELENGTH:2||GAIN:2||CARBON NANOTUBES:2||CROSSSECTIONS:2||LIGHTEMITTINGDIODES:2||PULSE:2||CARBON PLASMA:2||TISAPPHIRE LASER:2||Raman scattering:2||ROUTE:2||multilayer:2||CATHODOLUMINESCENCE:2||highresolution transmission electronic microscope (HRTEM):2||DIFFERENCEFREQUENCYGENERATION:2||CRYSTAL:2||laserproduced plasma:2||NANOCABLES:2||photoluminescence:2||MAGNETIC ALLOY SEMICONDUCTORS:2||MOLECULARBEAM EPITAXY:2||EARTHDOPED GAN:2||LASER FIELDS:2||CHIRPEDPULSEAMPLIFICATION:2||ALN:2||GAUSSIANBEAM:2||ASSISTED CATALYTIC GROWTH:2||BLUE:2||NANOSTRUCTURES:2||MAGNETOELECTRONICS:2||MICROSCOPY:2||ELECTROLUMINESCENCE:2||LASERPULSES:2||GaN nanowires:2||GALLIUM NITRIDE NANOWIRES:2||GAMNN:2||NANOTUBES:2||PHYSICS:2||Femtosecond laser:2||parametric oscillators and amplifiers:1||ultrafast lasers:1||VALENCE:1||nanowires:1||DILUTED MAGNETIC SEMICONDUCTOR:1||LUMINESCENCE:1||Density modulation:1||Energy modulation:1||Current enhanced SASE free electron laser:1||Undulator radiation:1||FREEELECTRON LASERS:1||ULTRATHIN FERROMAGNETICFILMS:1||OXIDEFILMS:1||ABLATION:1||COMPONENT:1||METAL:1||innershell excited states:1||Nelike ions:1||TRANSITIONS:1||XUV spectrometer:1||DIAGNOSTICS:1||Xray scattering:1||MO/SI:1||pulsed laser deposition:1||KEV IMPACT ENERGIES:1||vacuum electron acceleration:1||HIGHINTENSITY LASER:1||JUNCTIONS:1||LOWTEMPERATURE GROWTH:1||nanocrystalline materials:1||MOLECULAR PHOTOIONIZATION:1||LOCALIZATION:1||DEUTERIUM CLUSTERS:1||EXPLOSIONS:1||REGENERATIVE AMPLIFIERS:1||RAREGASES:1||THz radiation:1||FREEELECTRON LASER:1||REALTIME OBSERVATION:1||TARGET:1||photoionized plasmas:1||fs Xray laser:1||emission profile:1||HIGHORDER HARMONICS:1||Xray laser:1||atomic transition:1||EXCITATION:1||LASERS:1||PERFORMANCE:1||RELATIVISTIC ELECTRONS:1||BI2O3DOPED ZNO:1||INNERSHELL IONIZATION:1||Laser wakefield:1||FREQUENCY:1||SOLIDSTATE LASERS:1||Linearly polarized:1||THERMIONIC EMISSION:1||PULSE AMPLIFICATION SYSTEM:1||BIB3O6:1||NM:1||NONCOVALENT INTERACTIONS:1||CRYSTALLINE:1||INTENSITY:1||JETS:1||COHERENT:1||LINE:1||ANGULARDISTRIBUTION:1||SILVER IONS:1||magnetic anisotropy:1||DEVICES:1||Auger transitions:1||CosterKronig transitions:1||EFFICIENT:1||ELECTRONIMPACT IONIZATION:1||ULTRASHORTPULSE:1||Nanowire:1||Heterostructure:1||soft Xray reflectivity:1||PLASMA ACCELERATOR:1||ZINCOXIDE NANOWIRES:1||CHEMICALVAPORDEPOSITION:1||Electron acceleration:1||Ionization of gases:1||Delay dependent:1||MULTIPHOTON IONIZATION:1||FRAGMENTATION:1||GASJET:1||ultrafast nonlinear optics:1||CYCLE PULSES:1||KHZ:1||chemical vapor deposition:1||ferromagnetism:1||ABSORPTION:1||TERAHERTZ RADIATION:1||SCIENCE:1||FIELDS:1||ELECTRONS:1||nanomultilayer structures:1||YIELDS:1||AUGER:1||10HZ REPETITION RATE:1||MULTITERAWATT:1||SPECTROGRAPH:1||HIGHHARMONICGENERATION:1||spectroscopy:1||level population:1||PARTICLEACCELERATION:1||OPTICAL FREQUENCYMEASUREMENT:1||NANOWALLS:1||ROOMTEMPERATURE:1||AVERAGE OUTPUT POWER:1||GROUPVELOCITYMISMATCH:1||Impact ionization:1||Dynamics:1||Lasers:1||Collisional process:1||ABOVETHRESHOLD IONIZATION:1||MAINGROUP THERMOCHEMISTRY:1||dilute magnetic semiconductors:1||GACRN:1||SIZE:1||ATTOSECOND:1||Ar cluster:1||Xray astrophysics:1||photoionization:1||irons:1||normal incidence pulsed laser deposition:1||SHELLS:1||Silicon Oxide:1||gaspuff Zpinch:1||Xray:1||soft Xray reflectors:1||ESCAPE:1||ZN2SIO4:1||SILICA:1||Time delay:1||Collisional plasmas:1||MASSSPECTROMETRY:1||NUCLEARFUSION:1||PARAMETRIC AMPLIFICATION:1||LYING ELECTRONIC STATES:1||ADJUSTABLEPARAMETERS:1||MAGNETICPROPERTIES:1||LIQUIDPHASE EPITAXY:1||CEP laser:1||REGION:1||Plasma waveguide:1||AMBIENT GAS:1||DEPOSITION:1||HARMONICGENERATION:1||ENHANCEMENT:1||imaging spectrometer:1||Abel inversion:1||Water window:1||Liquid nitrogen jet:1||CHARGEEXCHANGE:1||NOBEL LECTURE:1||VARISTOR:1||EPITAXY:1||THINDISK LASER:1||HIGHREPETITIONRATE:1||Atom lasers:1||Electronimpact excitation:1||High order harmonics:1||ultrafast technology:1||PEAK POWER:1||CHARGED ALUMINUM CLUSTERS:1||GaN:1||THIN:1||Electron beam:1||INTENSE:1||Hard Xray pulse generation:1||NONLINEAR THOMSON SCATTERING:1||MULTILAYER:1||UVvisible spectrometer:1||ATOMS:1||innershell transitions:1||CORRECTED CONCAVE GRATINGS:1||DISCHARGE:1||LASERPLASMA:1||thin film:1||reflectivity:1||opacity:1||gain:1||smallangle Xray scattering:1||SOFTXRAY:1||ZINCOXIDE:1||CYGNUSX3:1||Betatron oscillation:1||ACCELERATOR:1||STRAINEDLAYER SUPERLATTICES:1||OPTICAL PARAMETRIC AMPLIFICATION:1||PASSIVE MODELOCKING:1||Collision dynamics:1||MUM:1||EXACTEXCHANGE:1||BASISSET:1||APPROXIMATION:1||OXYNITRIDES:1||Beam energy modulation:1||polarization spectroscopy:1||REORIENTATION TRANSITION:1||DEPENDENCE:1||sulfurs:1||BUILDINGBLOCKS:1||RATES:1||OPTICAL PULSES:1||toroidal mirror:1||XRAY LASER:1||CALCIUM:1||radially polarized laser:1||GRAINBOUNDARIES:1||VAPORDEPOSITION:1||Xray generation:1||MAGNETIZATION:1||Electric excitation:1||Laserinduced gas plasmas:1||Qualitative analysis:1||SCHEME:1||RADIATION:10||PULSES:8||PHOTOLUMINESCENCE:7||LASER:7||GENERATION:6||NANORODS:6||GROWTH:6||NANOWIRES:5||IMPLANTED 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SEMICONDUCTORS:2||MOLECULARBEAM EPITAXY:2||EARTHDOPED GAN:2||LASER FIELDS:2||CHIRPEDPULSEAMPLIFICATION:2||ALN:2||GAUSSIANBEAM:2||ASSISTED CATALYTIC GROWTH:2||BLUE:2||NANOSTRUCTURES:2||MAGNETOELECTRONICS:2||MICROSCOPY:2||ELECTROLUMINESCENCE:2||LASERPULSES:2||GaN nanowires:2||GALLIUM NITRIDE NANOWIRES:2||GAMNN:2||NANOTUBES:2||PHYSICS:2||Femtosecond laser:2||parametric oscillators and amplifiers:1||ultrafast lasers:1||VALENCE:1||nanowires:1||DILUTED MAGNETIC SEMICONDUCTOR:1||LUMINESCENCE:1||Density modulation:1||Energy modulation:1||Current enhanced SASE free electron laser:1||Undulator radiation:1||FREEELECTRON LASERS:1||ULTRATHIN FERROMAGNETICFILMS:1||OXIDEFILMS:1||ABLATION:1||COMPONENT:1||METAL:1||innershell excited states:1||Nelike ions:1||TRANSITIONS:1||XUV spectrometer:1||DIAGNOSTICS:1||Xray scattering:1||MO/SI:1||pulsed laser deposition:1||KEV IMPACT ENERGIES:1||vacuum electron acceleration:1||HIGHINTENSITY LASER:1||JUNCTIONS:1||LOWTEMPERATURE GROWTH:1||nanocrystalline materials:1||MOLECULAR PHOTOIONIZATION:1||LOCALIZATION:1||DEUTERIUM CLUSTERS:1||EXPLOSIONS:1||REGENERATIVE AMPLIFIERS:1||RAREGASES:1||THz radiation:1||FREEELECTRON LASER:1||REALTIME OBSERVATION:1||TARGET:1||photoionized plasmas:1||fs Xray laser:1||emission profile:1||HIGHORDER HARMONICS:1||Xray laser:1||atomic transition:1||EXCITATION:1||LASERS:1||PERFORMANCE:1||RELATIVISTIC ELECTRONS:1||BI2O3DOPED ZNO:1||INNERSHELL IONIZATION:1||Laser wakefield:1||FREQUENCY:1||SOLIDSTATE LASERS:1||Linearly polarized:1||THERMIONIC EMISSION:1||PULSE AMPLIFICATION SYSTEM:1||BIB3O6:1||NM:1||NONCOVALENT INTERACTIONS:1||CRYSTALLINE:1||INTENSITY:1||JETS:1||COHERENT:1||LINE:1||ANGULARDISTRIBUTION:1||SILVER IONS:1||magnetic anisotropy:1||DEVICES:1||Auger transitions:1||CosterKronig transitions:1||EFFICIENT:1||ELECTRONIMPACT IONIZATION:1||ULTRASHORTPULSE:1||Nanowire:1||Heterostructure:1||soft Xray reflectivity:1||PLASMA ACCELERATOR:1||ZINCOXIDE NANOWIRES:1||CHEMICALVAPORDEPOSITION:1||Electron acceleration:1||Ionization of gases:1||Delay dependent:1||MULTIPHOTON IONIZATION:1||FRAGMENTATION:1||GASJET:1||ultrafast nonlinear optics:1||CYCLE PULSES:1||KHZ:1||chemical vapor deposition:1||ferromagnetism:1||ABSORPTION:1||TERAHERTZ RADIATION:1||SCIENCE:1||FIELDS:1||ELECTRONS:1||nanomultilayer structures:1||YIELDS:1||AUGER:1||10HZ REPETITION RATE:1||MULTITERAWATT:1||SPECTROGRAPH:1||HIGHHARMONICGENERATION:1||spectroscopy:1||level population:1||PARTICLEACCELERATION:1||OPTICAL FREQUENCYMEASUREMENT:1||NANOWALLS:1||ROOMTEMPERATURE:1||AVERAGE OUTPUT POWER:1||GROUPVELOCITYMISMATCH:1||Impact ionization:1||Dynamics:1||Lasers:1||Collisional process:1||ABOVETHRESHOLD IONIZATION:1||MAINGROUP THERMOCHEMISTRY:1||dilute magnetic semiconductors:1||GACRN:1||SIZE:1||ATTOSECOND:1||Ar cluster:1||Xray astrophysics:1||photoionization:1||irons:1||normal incidence pulsed laser deposition:1||SHELLS:1||Silicon Oxide:1||gaspuff Zpinch:1||Xray:1||soft Xray reflectors:1||ESCAPE:1||ZN2SIO4:1||SILICA:1||Time 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materials:1||MOLECULAR PHOTOIONIZATION:1||LOCALIZATION:1||DEUTERIUM CLUSTERS:1||EXPLOSIONS:1||REGENERATIVE AMPLIFIERS:1||RAREGASES:1||THz radiation:1||FREEELECTRON LASER:1||REALTIME OBSERVATION:1||TARGET:1||photoionized plasmas:1||fs Xray laser:1||emission profile:1||HIGHORDER HARMONICS:1||Xray laser:1||atomic transition:1||EXCITATION:1||LASERS:1||PERFORMANCE:1||RELATIVISTIC ELECTRONS:1||BI2O3DOPED ZNO:1||INNERSHELL IONIZATION:1||Laser wakefield:1||FREQUENCY:1||SOLIDSTATE LASERS:1||Linearly polarized:1||THERMIONIC EMISSION:1||PULSE AMPLIFICATION SYSTEM:1||BIB3O6:1||NM:1||NONCOVALENT INTERACTIONS:1||CRYSTALLINE:1||INTENSITY:1||JETS:1||COHERENT:1||LINE:1||ANGULARDISTRIBUTION:1||SILVER IONS:1||magnetic anisotropy:1||DEVICES:1||Auger transitions:1||CosterKronig transitions:1||EFFICIENT:1||ELECTRONIMPACT IONIZATION:1||ULTRASHORTPULSE:1||Nanowire:1||Heterostructure:1||soft Xray reflectivity:1||PLASMA ACCELERATOR:1||ZINCOXIDE NANOWIRES:1||CHEMICALVAPORDEPOSITION:1||Electron acceleration:1||Ionization of gases:1||Delay dependent:1||MULTIPHOTON IONIZATION:1||FRAGMENTATION:1||GASJET:1||ultrafast nonlinear optics:1||CYCLE PULSES:1||KHZ:1||chemical vapor deposition:1||ferromagnetism:1||ABSORPTION:1||TERAHERTZ RADIATION:1||SCIENCE:1||FIELDS:1||ELECTRONS:1||nanomultilayer structures:1||YIELDS:1||AUGER:1||10HZ REPETITION RATE:1||MULTITERAWATT:1||SPECTROGRAPH:1||HIGHHARMONICGENERATION:1||spectroscopy:1||level population:1||PARTICLEACCELERATION:1||OPTICAL FREQUENCYMEASUREMENT:1||NANOWALLS:1||ROOMTEMPERATURE:1||AVERAGE OUTPUT POWER:1||GROUPVELOCITYMISMATCH:1||Impact ionization:1||Dynamics:1||Lasers:1||Collisional process:1||ABOVETHRESHOLD IONIZATION:1||MAINGROUP THERMOCHEMISTRY:1||dilute magnetic semiconductors:1||GACRN:1||SIZE:1||ATTOSECOND:1||Ar cluster:1||Xray astrophysics:1||photoionization:1||irons:1||normal incidence pulsed laser deposition:1||SHELLS:1||Silicon Oxide:1||gaspuff Zpinch:1||Xray:1||soft Xray reflectors:1||ESCAPE:1||ZN2SIO4:1||SILICA:1||Time delay:1||Collisional plasmas:1||MASSSPECTROMETRY:1||NUCLEARFUSION:1||PARAMETRIC AMPLIFICATION:1||LYING ELECTRONIC STATES:1||ADJUSTABLEPARAMETERS:1||MAGNETICPROPERTIES:1||LIQUIDPHASE EPITAXY:1||CEP laser:1||REGION:1||Plasma waveguide:1||AMBIENT GAS:1||DEPOSITION:1||HARMONICGENERATION:1||ENHANCEMENT:1||imaging spectrometer:1||Abel inversion:1||Water window:1||Liquid nitrogen jet:1||CHARGEEXCHANGE:1||NOBEL LECTURE:1||VARISTOR:1||EPITAXY:1||THINDISK LASER:1||HIGHREPETITIONRATE:1||Atom lasers:1||Electronimpact excitation:1||High order harmonics:1||ultrafast technology:1||PEAK POWER:1||CHARGED ALUMINUM CLUSTERS:1||GaN:1||THIN:1||Electron beam:1||INTENSE:1||Hard Xray pulse generation:1||NONLINEAR THOMSON SCATTERING:1||MULTILAYER:1||UVvisible spectrometer:1||ATOMS:1||innershell transitions:1||CORRECTED CONCAVE GRATINGS:1||DISCHARGE:1||LASERPLASMA:1||thin film:1||reflectivity:1||opacity:1||gain:1||smallangle Xray scattering:1||SOFTXRAY:1||ZINCOXIDE:1||CYGNUSX3:1||Betatron oscillation:1||ACCELERATOR:1||STRAINEDLAYER SUPERLATTICES:1||OPTICAL PARAMETRIC AMPLIFICATION:1||PASSIVE MODELOCKING:1||Collision dynamics:1||MUM:1||EXACTEXCHANGE:1||BASISSET:1||APPROXIMATION:1||OXYNITRIDES:1||Beam energy modulation:1||polarization spectroscopy:1||REORIENTATION TRANSITION:1||DEPENDENCE:1||sulfurs:1||BUILDINGBLOCKS:1||RATES:1||OPTICAL PULSES:1||toroidal mirror:1||XRAY LASER:1||CALCIUM:1||radially polarized laser:1||GRAINBOUNDARIES:1||VAPORDEPOSITION:1||Xray generation:1||MAGNETIZATION:1||Electric excitation:1||Laserinduced gas plasmas:1||Qualitative analysis:1||SCHEME:1||RADIATION:10||PULSES:8||PHOTOLUMINESCENCE:7||LASER:7||GENERATION:6||NANORODS:6||GROWTH:6||NANOWIRES:5||IMPLANTED GAN:5||SPECTROSCOPY:5||THINFILMS:4||DYNAMICS:4||SILICON:4||EXTREMEULTRAVIOLET:4||AMPLIFICATION:4||PRESSURE:4||PHASE:4||OPTICALPROPERTIES:4||SYSTEM:4||EMISSION:4||FEL:3||N2O:3||FILMS:3||OPTICS:3||SPECTRA:3||FIELD:3||MIRRORS:3||ARRAYS:3||CLUSTERS:3||SIO2:3||IONIZATION:3||VACUUM:3||SCATTERING:3||IONS:2||LUMINESCENCE PROPERTIES:2||ANISOTROPY:2||BEAMS:2||DIFFRACTION:2||DISPERSION:2||chemical vapor deposition (CVD):2||ELECTRONICSTRUCTURE:2||MOSFETS:2||SI3N4:2||DENSITY:2||LIGHT:2||PLASMAS:2||MATTER:2||nanocomposites:2||RAMANSCATTERING:2||NANOPARTICLES:2||OXIDE:2||AMPLIFIED SPONTANEOUS EMISSION:2||NM WAVELENGTH:2||GAIN:2||CARBON NANOTUBES:2||CROSSSECTIONS:2||LIGHTEMITTINGDIODES:2||PULSE:2||CARBON PLASMA:2||TISAPPHIRE LASER:2||Raman scattering:2||ROUTE:2||multilayer:2||CATHODOLUMINESCENCE:2||highresolution transmission electronic microscope (HRTEM):2||DIFFERENCEFREQUENCYGENERATION:2||CRYSTAL:2||laserproduced plasma:2||NANOCABLES:2||photoluminescence:2||MAGNETIC ALLOY SEMICONDUCTORS:2||MOLECULARBEAM EPITAXY:2||EARTHDOPED GAN:2||LASER FIELDS:2||CHIRPEDPULSEAMPLIFICATION:2||ALN:2||GAUSSIANBEAM:2||ASSISTED CATALYTIC GROWTH:2||BLUE:2||NANOSTRUCTURES:2||MAGNETOELECTRONICS:2||MICROSCOPY:2||ELECTROLUMINESCENCE:2||LASERPULSES:2||GaN nanowires:2||GALLIUM NITRIDE NANOWIRES:2||GAMNN:2||NANOTUBES:2||PHYSICS:2||Femtosecond laser:2||parametric oscillators and amplifiers:1||ultrafast lasers:1||VALENCE:1||nanowires:1||DILUTED MAGNETIC SEMICONDUCTOR:1||LUMINESCENCE:1||Density modulation:1||Energy modulation:1||Current enhanced SASE free electron laser:1||Undulator radiation:1||FREEELECTRON LASERS:1||ULTRATHIN FERROMAGNETICFILMS:1||OXIDEFILMS:1||ABLATION:1||COMPONENT:1||METAL:1||innershell excited states:1||Nelike ions:1||TRANSITIONS:1||XUV spectrometer:1||DIAGNOSTICS:1||Xray scattering:1||MO/SI:1||pulsed laser deposition:1||KEV IMPACT ENERGIES:1||vacuum electron acceleration:1||HIGHINTENSITY LASER:1||JUNCTIONS:1||LOWTEMPERATURE GROWTH:1||nanocrystalline materials:1||MOLECULAR PHOTOIONIZATION:1||LOCALIZATION:1||DEUTERIUM CLUSTERS:1||EXPLOSIONS:1||REGENERATIVE AMPLIFIERS:1||RAREGASES:1||THz radiation:1||FREEELECTRON LASER:1||REALTIME OBSERVATION:1||TARGET:1||photoionized plasmas:1||fs Xray laser:1||emission profile:1||HIGHORDER HARMONICS:1||Xray laser:1||atomic transition:1||EXCITATION:1||LASERS:1||PERFORMANCE:1||RELATIVISTIC ELECTRONS:1||BI2O3DOPED ZNO:1||INNERSHELL IONIZATION:1||Laser wakefield:1||FREQUENCY:1||SOLIDSTATE LASERS:1||Linearly polarized:1||THERMIONIC EMISSION:1||PULSE AMPLIFICATION SYSTEM:1||BIB3O6:1||NM:1||NONCOVALENT INTERACTIONS:1||CRYSTALLINE:1||INTENSITY:1||JETS:1||COHERENT:1||LINE:1||ANGULARDISTRIBUTION:1||SILVER IONS:1||magnetic anisotropy:1||DEVICES:1||Auger transitions:1||CosterKronig transitions:1||EFFICIENT:1||ELECTRONIMPACT IONIZATION:1||ULTRASHORTPULSE:1||Nanowire:1||Heterostructure:1||soft Xray reflectivity:1||PLASMA ACCELERATOR:1||ZINCOXIDE NANOWIRES:1||CHEMICALVAPORDEPOSITION:1||Electron acceleration:1||Ionization of gases:1||Delay dependent:1||MULTIPHOTON IONIZATION:1||FRAGMENTATION:1||GASJET:1||ultrafast nonlinear optics:1||CYCLE PULSES:1||KHZ:1||chemical vapor deposition:1||ferromagnetism:1||ABSORPTION:1||TERAHERTZ RADIATION:1||SCIENCE:1||FIELDS:1||ELECTRONS:1||nanomultilayer structures:1||YIELDS:1||AUGER:1||10HZ REPETITION RATE:1||MULTITERAWATT:1||SPECTROGRAPH:1||HIGHHARMONICGENERATION:1||spectroscopy:1||level population:1||PARTICLEACCELERATION:1||OPTICAL FREQUENCYMEASUREMENT:1||NANOWALLS:1||ROOMTEMPERATURE:1||AVERAGE OUTPUT POWER:1||GROUPVELOCITYMISMATCH:1||Impact ionization:1||Dynamics:1||Lasers:1||Collisional process:1||ABOVETHRESHOLD IONIZATION:1||MAINGROUP THERMOCHEMISTRY:1||dilute magnetic semiconductors:1||GACRN:1||SIZE:1||ATTOSECOND:1||Ar cluster:1||Xray astrophysics:1||photoionization:1||irons:1||normal incidence pulsed laser deposition:1||SHELLS:1||Silicon Oxide:1||gaspuff Zpinch:1||Xray:1||soft Xray reflectors:1||ESCAPE:1||ZN2SIO4:1||SILICA:1||Time delay:1||Collisional plasmas:1||MASSSPECTROMETRY:1||NUCLEARFUSION:1||PARAMETRIC AMPLIFICATION:1||LYING ELECTRONIC STATES:1||ADJUSTABLEPARAMETERS:1||MAGNETICPROPERTIES:1||LIQUIDPHASE EPITAXY:1||CEP laser:1||REGION:1||Plasma waveguide:1||AMBIENT GAS:1||DEPOSITION:1||HARMONICGENERATION:1||ENHANCEMENT:1||imaging spectrometer:1||Abel inversion:1||Water window:1||Liquid nitrogen jet:1||CHARGEEXCHANGE:1||NOBEL LECTURE:1||VARISTOR:1||EPITAXY:1||THINDISK LASER:1||HIGHREPETITIONRATE:1||Atom lasers:1||Electronimpact excitation:1||High order harmonics:1||ultrafast technology:1||PEAK POWER:1||CHARGED ALUMINUM CLUSTERS:1||GaN:1||THIN:1||Electron beam:1||INTENSE:1||Hard Xray pulse generation:1||NONLINEAR THOMSON SCATTERING:1||MULTILAYER:1||UVvisible spectrometer:1||ATOMS:1||innershell transitions:1||CORRECTED CONCAVE GRATINGS:1||DISCHARGE:1||LASERPLASMA:1||thin film:1||reflectivity:1||opacity:1||gain:1||smallangle Xray scattering:1||SOFTXRAY:1||ZINCOXIDE:1||CYGNUSX3:1||Betatron oscillation:1||ACCELERATOR:1||STRAINEDLAYER SUPERLATTICES:1||OPTICAL PARAMETRIC AMPLIFICATION:1||PASSIVE MODELOCKING:1||Collision dynamics:1||MUM:1||EXACTEXCHANGE:1||BASISSET:1||APPROXIMATION:1||OXYNITRIDES:1||Beam energy modulation:1||polarization spectroscopy:1||REORIENTATION TRANSITION:1||DEPENDENCE:1||sulfurs:1||BUILDINGBLOCKS:1||RATES:1||OPTICAL PULSES:1||toroidal mirror:1||XRAY LASER:1||CALCIUM:1||radially polarized laser:1||GRAINBOUNDARIES:1||VAPORDEPOSITION:1||Xray generation:1||MAGNETIZATION:1||Electric excitation:1||Laserinduced gas plasmas:1||Qualitative analysis:1||SCHEME:1||RADIATION:10||PULSES:8||PHOTOLUMINESCENCE:7||LASER:7||GENERATION:6||NANORODS:6||GROWTH:6||NANOWIRES:5||IMPLANTED 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SEMICONDUCTORS:2||MOLECULARBEAM EPITAXY:2||EARTHDOPED GAN:2||LASER FIELDS:2||CHIRPEDPULSEAMPLIFICATION:2||ALN:2||GAUSSIANBEAM:2||ASSISTED CATALYTIC GROWTH:2||BLUE:2||NANOSTRUCTURES:2||MAGNETOELECTRONICS:2||MICROSCOPY:2||ELECTROLUMINESCENCE:2||LASERPULSES:2||GaN nanowires:2||GALLIUM NITRIDE NANOWIRES:2||GAMNN:2||NANOTUBES:2||PHYSICS:2||Femtosecond laser:2||parametric oscillators and amplifiers:1||ultrafast lasers:1||VALENCE:1||nanowires:1||DILUTED MAGNETIC SEMICONDUCTOR:1||LUMINESCENCE:1||Density modulation:1||Energy modulation:1||Current enhanced SASE free electron laser:1||Undulator radiation:1||FREEELECTRON LASERS:1||ULTRATHIN FERROMAGNETICFILMS:1||OXIDEFILMS:1||ABLATION:1||COMPONENT:1||METAL:1||innershell excited states:1||Nelike ions:1||TRANSITIONS:1||XUV spectrometer:1||DIAGNOSTICS:1||Xray scattering:1||MO/SI:1||pulsed laser deposition:1||KEV IMPACT ENERGIES:1||vacuum electron acceleration:1||HIGHINTENSITY LASER:1||JUNCTIONS:1||LOWTEMPERATURE GROWTH:1||nanocrystalline materials:1||MOLECULAR PHOTOIONIZATION:1||LOCALIZATION:1||DEUTERIUM CLUSTERS:1||EXPLOSIONS:1||REGENERATIVE AMPLIFIERS:1||RAREGASES:1||THz radiation:1||FREEELECTRON LASER:1||REALTIME OBSERVATION:1||TARGET:1||photoionized plasmas:1||fs Xray laser:1||emission profile:1||HIGHORDER HARMONICS:1||Xray laser:1||atomic transition:1||EXCITATION:1||LASERS:1||PERFORMANCE:1||RELATIVISTIC ELECTRONS:1||BI2O3DOPED ZNO:1||INNERSHELL IONIZATION:1||Laser wakefield:1||FREQUENCY:1||SOLIDSTATE LASERS:1||Linearly polarized:1||THERMIONIC EMISSION:1||PULSE AMPLIFICATION SYSTEM:1||BIB3O6:1||NM:1||NONCOVALENT INTERACTIONS:1||CRYSTALLINE:1||INTENSITY:1||JETS:1||COHERENT:1||LINE:1||ANGULARDISTRIBUTION:1||SILVER IONS:1||magnetic anisotropy:1||DEVICES:1||Auger transitions:1||CosterKronig transitions:1||EFFICIENT:1||ELECTRONIMPACT IONIZATION:1||ULTRASHORTPULSE:1||Nanowire:1||Heterostructure:1||soft Xray reflectivity:1||PLASMA ACCELERATOR:1||ZINCOXIDE NANOWIRES:1||CHEMICALVAPORDEPOSITION:1||Electron acceleration:1||Ionization of gases:1||Delay dependent:1||MULTIPHOTON IONIZATION:1||FRAGMENTATION:1||GASJET:1||ultrafast nonlinear optics:1||CYCLE PULSES:1||KHZ:1||chemical vapor deposition:1||ferromagnetism:1||ABSORPTION:1||TERAHERTZ RADIATION:1||SCIENCE:1||FIELDS:1||ELECTRONS:1||nanomultilayer structures:1||YIELDS:1||AUGER:1||10HZ REPETITION RATE:1||MULTITERAWATT:1||SPECTROGRAPH:1||HIGHHARMONICGENERATION:1||spectroscopy:1||level population:1||PARTICLEACCELERATION:1||OPTICAL FREQUENCYMEASUREMENT:1||NANOWALLS:1||ROOMTEMPERATURE:1||AVERAGE OUTPUT POWER:1||GROUPVELOCITYMISMATCH:1||Impact ionization:1||Dynamics:1||Lasers:1||Collisional process:1||ABOVETHRESHOLD IONIZATION:1||MAINGROUP THERMOCHEMISTRY:1||dilute magnetic semiconductors:1||GACRN:1||SIZE:1||ATTOSECOND:1||Ar cluster:1||Xray astrophysics:1||photoionization:1||irons:1||normal incidence pulsed laser deposition:1||SHELLS:1||Silicon Oxide:1||gaspuff Zpinch:1||Xray:1||soft Xray reflectors:1||ESCAPE:1||ZN2SIO4:1||SILICA:1||Time 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materials:1||MOLECULAR PHOTOIONIZATION:1||LOCALIZATION:1||DEUTERIUM CLUSTERS:1||EXPLOSIONS:1||REGENERATIVE AMPLIFIERS:1||RAREGASES:1||THz radiation:1||FREEELECTRON LASER:1||REALTIME OBSERVATION:1||TARGET:1||photoionized plasmas:1||fs Xray laser:1||emission profile:1||HIGHORDER HARMONICS:1||Xray laser:1||atomic transition:1||EXCITATION:1||LASERS:1||PERFORMANCE:1||RELATIVISTIC ELECTRONS:1||BI2O3DOPED ZNO:1||INNERSHELL IONIZATION:1||Laser wakefield:1||FREQUENCY:1||SOLIDSTATE LASERS:1||Linearly polarized:1||THERMIONIC EMISSION:1||PULSE AMPLIFICATION SYSTEM:1||BIB3O6:1||NM:1||NONCOVALENT INTERACTIONS:1||CRYSTALLINE:1||INTENSITY:1||JETS:1||COHERENT:1||LINE:1||ANGULARDISTRIBUTION:1||SILVER IONS:1||magnetic anisotropy:1||DEVICES:1||Auger transitions:1||CosterKronig transitions:1||EFFICIENT:1||ELECTRONIMPACT IONIZATION:1||ULTRASHORTPULSE:1||Nanowire:1||Heterostructure:1||soft Xray reflectivity:1||PLASMA ACCELERATOR:1||ZINCOXIDE NANOWIRES:1||CHEMICALVAPORDEPOSITION:1||Electron acceleration:1||Ionization of gases:1||Delay dependent:1||MULTIPHOTON IONIZATION:1||FRAGMENTATION:1||GASJET:1||ultrafast nonlinear optics:1||CYCLE PULSES:1||KHZ:1||chemical vapor deposition:1||ferromagnetism:1||ABSORPTION:1||TERAHERTZ RADIATION:1||SCIENCE:1||FIELDS:1||ELECTRONS:1||nanomultilayer structures:1||YIELDS:1||AUGER:1||10HZ REPETITION RATE:1||MULTITERAWATT:1||SPECTROGRAPH:1||HIGHHARMONICGENERATION:1||spectroscopy:1||level population:1||PARTICLEACCELERATION:1||OPTICAL FREQUENCYMEASUREMENT:1||NANOWALLS:1||ROOMTEMPERATURE:1||AVERAGE OUTPUT POWER:1||GROUPVELOCITYMISMATCH:1||Impact ionization:1||Dynamics:1||Lasers:1||Collisional process:1||ABOVETHRESHOLD IONIZATION:1||MAINGROUP THERMOCHEMISTRY:1||dilute magnetic semiconductors:1||GACRN:1||SIZE:1||ATTOSECOND:1||Ar cluster:1||Xray astrophysics:1||photoionization:1||irons:1||normal incidence pulsed laser deposition:1||SHELLS:1||Silicon Oxide:1||gaspuff Zpinch:1||Xray:1||soft Xray reflectors:1||ESCAPE:1||ZN2SIO4:1||SILICA:1||Time delay:1||Collisional plasmas:1||MASSSPECTROMETRY:1||NUCLEARFUSION:1||PARAMETRIC AMPLIFICATION:1||LYING ELECTRONIC STATES:1||ADJUSTABLEPARAMETERS:1||MAGNETICPROPERTIES:1||LIQUIDPHASE EPITAXY:1||CEP laser:1||REGION:1||Plasma waveguide:1||AMBIENT GAS:1||DEPOSITION:1||HARMONICGENERATION:1||ENHANCEMENT:1||imaging spectrometer:1||Abel inversion:1||Water window:1||Liquid nitrogen jet:1||CHARGEEXCHANGE:1||NOBEL LECTURE:1||VARISTOR:1||EPITAXY:1||THINDISK LASER:1||HIGHREPETITIONRATE:1||Atom lasers:1||Electronimpact excitation:1||High order harmonics:1||ultrafast technology:1||PEAK POWER:1||CHARGED ALUMINUM CLUSTERS:1||GaN:1||THIN:1||Electron beam:1||INTENSE:1||Hard Xray pulse generation:1||NONLINEAR THOMSON SCATTERING:1||MULTILAYER:1||UVvisible spectrometer:1||ATOMS:1||innershell transitions:1||CORRECTED CONCAVE GRATINGS:1||DISCHARGE:1||LASERPLASMA:1||thin film:1||reflectivity:1||opacity:1||gain:1||smallangle Xray scattering:1||SOFTXRAY:1||ZINCOXIDE:1||CYGNUSX3:1||Betatron oscillation:1||ACCELERATOR:1||STRAINEDLAYER SUPERLATTICES:1||OPTICAL PARAMETRIC AMPLIFICATION:1||PASSIVE MODELOCKING:1||Collision dynamics:1||MUM:1||EXACTEXCHANGE:1||BASISSET:1||APPROXIMATION:1||OXYNITRIDES:1||Beam energy modulation:1||polarization spectroscopy:1||REORIENTATION TRANSITION:1||DEPENDENCE:1||sulfurs:1||BUILDINGBLOCKS:1||RATES:1||OPTICAL PULSES:1||toroidal mirror:1||XRAY LASER:1||CALCIUM:1||radially polarized laser:1||GRAINBOUNDARIES:1||VAPORDEPOSITION:1||Xray generation:1||MAGNETIZATION:1||Electric excitation:1||Laserinduced gas plasmas:1||Qualitative analysis:1||SCHEME:1||RADIATION:10||PULSES:8||PHOTOLUMINESCENCE:7||LASER:7||GENERATION:6||NANORODS:6||GROWTH:6||NANOWIRES:5||IMPLANTED GAN:5||SPECTROSCOPY:5||THINFILMS:4||DYNAMICS:4||SILICON:4||EXTREMEULTRAVIOLET:4||AMPLIFICATION:4||PRESSURE:4||PHASE:4||OPTICALPROPERTIES:4||SYSTEM:4||EMISSION:4||FEL:3||N2O:3||FILMS:3||OPTICS:3||SPECTRA:3||FIELD:3||MIRRORS:3||ARRAYS:3||CLUSTERS:3||SIO2:3||IONIZATION:3||VACUUM:3||SCATTERING:3||IONS:2||LUMINESCENCE PROPERTIES:2||ANISOTROPY:2||BEAMS:2||DIFFRACTION:2||DISPERSION:2||chemical vapor deposition (CVD):2||ELECTRONICSTRUCTURE:2||MOSFETS:2||SI3N4:2||DENSITY:2||LIGHT:2||PLASMAS:2||MATTER:2||nanocomposites:2||RAMANSCATTERING:2||NANOPARTICLES:2||OXIDE:2||AMPLIFIED SPONTANEOUS EMISSION:2||NM WAVELENGTH:2||GAIN:2||CARBON NANOTUBES:2||CROSSSECTIONS:2||LIGHTEMITTINGDIODES:2||PULSE:2||CARBON PLASMA:2||TISAPPHIRE LASER:2||Raman scattering:2||ROUTE:2||multilayer:2||CATHODOLUMINESCENCE:2||highresolution transmission electronic microscope (HRTEM):2||DIFFERENCEFREQUENCYGENERATION:2||CRYSTAL:2||laserproduced plasma:2||NANOCABLES:2||photoluminescence:2||MAGNETIC ALLOY SEMICONDUCTORS:2||MOLECULARBEAM EPITAXY:2||EARTHDOPED GAN:2||LASER FIELDS:2||CHIRPEDPULSEAMPLIFICATION:2||ALN:2||GAUSSIANBEAM:2||ASSISTED CATALYTIC GROWTH:2||BLUE:2||NANOSTRUCTURES:2||MAGNETOELECTRONICS:2||MICROSCOPY:2||ELECTROLUMINESCENCE:2||LASERPULSES:2||GaN nanowires:2||GALLIUM NITRIDE NANOWIRES:2||GAMNN:2||NANOTUBES:2||PHYSICS:2||Femtosecond laser:2||parametric oscillators and amplifiers:1||ultrafast lasers:1||VALENCE:1||nanowires:1||DILUTED MAGNETIC SEMICONDUCTOR:1||LUMINESCENCE:1||Density modulation:1||Energy modulation:1||Current enhanced SASE free electron laser:1||Undulator radiation:1||FREEELECTRON LASERS:1||ULTRATHIN FERROMAGNETICFILMS:1||OXIDEFILMS:1||ABLATION:1||COMPONENT:1||METAL:1||innershell excited states:1||Nelike ions:1||TRANSITIONS:1||XUV spectrometer:1||DIAGNOSTICS:1||Xray scattering:1||MO/SI:1||pulsed laser deposition:1||KEV IMPACT ENERGIES:1||vacuum electron acceleration:1||HIGHINTENSITY LASER:1||JUNCTIONS:1||LOWTEMPERATURE GROWTH:1||nanocrystalline materials:1||MOLECULAR PHOTOIONIZATION:1||LOCALIZATION:1||DEUTERIUM CLUSTERS:1||EXPLOSIONS:1||REGENERATIVE AMPLIFIERS:1||RAREGASES:1||THz radiation:1||FREEELECTRON LASER:1||REALTIME OBSERVATION:1||TARGET:1||photoionized plasmas:1||fs Xray laser:1||emission profile:1||HIGHORDER HARMONICS:1||Xray laser:1||atomic transition:1||EXCITATION:1||LASERS:1||PERFORMANCE:1||RELATIVISTIC ELECTRONS:1||BI2O3DOPED ZNO:1||INNERSHELL IONIZATION:1||Laser wakefield:1||FREQUENCY:1||SOLIDSTATE LASERS:1||Linearly polarized:1||THERMIONIC EMISSION:1||PULSE AMPLIFICATION SYSTEM:1||BIB3O6:1||NM:1||NONCOVALENT INTERACTIONS:1||CRYSTALLINE:1||INTENSITY:1||JETS:1||COHERENT:1||LINE:1||ANGULARDISTRIBUTION:1||SILVER IONS:1||magnetic anisotropy:1||DEVICES:1||Auger transitions:1||CosterKronig transitions:1||EFFICIENT:1||ELECTRONIMPACT IONIZATION:1||ULTRASHORTPULSE:1||Nanowire:1||Heterostructure:1||soft Xray reflectivity:1||PLASMA ACCELERATOR:1||ZINCOXIDE NANOWIRES:1||CHEMICALVAPORDEPOSITION:1||Electron acceleration:1||Ionization of gases:1||Delay dependent:1||MULTIPHOTON IONIZATION:1||FRAGMENTATION:1||GASJET:1||ultrafast nonlinear optics:1||CYCLE PULSES:1||KHZ:1||chemical vapor deposition:1||ferromagnetism:1||ABSORPTION:1||TERAHERTZ RADIATION:1||SCIENCE:1||FIELDS:1||ELECTRONS:1||nanomultilayer structures:1||YIELDS:1||AUGER:1||10HZ REPETITION RATE:1||MULTITERAWATT:1||SPECTROGRAPH:1||HIGHHARMONICGENERATION:1||spectroscopy:1||level population:1||PARTICLEACCELERATION:1||OPTICAL FREQUENCYMEASUREMENT:1||NANOWALLS:1||ROOMTEMPERATURE:1||AVERAGE OUTPUT POWER:1||GROUPVELOCITYMISMATCH:1||Impact ionization:1||Dynamics:1||Lasers:1||Collisional process:1||ABOVETHRESHOLD IONIZATION:1||MAINGROUP THERMOCHEMISTRY:1||dilute magnetic semiconductors:1||GACRN:1||SIZE:1||ATTOSECOND:1||Ar cluster:1||Xray astrophysics:1||photoionization:1||irons:1||normal incidence pulsed laser deposition:1||SHELLS:1||Silicon Oxide:1||gaspuff Zpinch:1||Xray:1||soft Xray reflectors:1||ESCAPE:1||ZN2SIO4:1||SILICA:1||Time delay:1||Collisional plasmas:1||MASSSPECTROMETRY:1||NUCLEARFUSION:1||PARAMETRIC AMPLIFICATION:1||LYING ELECTRONIC STATES:1||ADJUSTABLEPARAMETERS:1||MAGNETICPROPERTIES:1||LIQUIDPHASE EPITAXY:1||CEP laser:1||REGION:1||Plasma waveguide:1||AMBIENT GAS:1||DEPOSITION:1||HARMONICGENERATION:1||ENHANCEMENT:1||imaging spectrometer:1||Abel inversion:1||Water window:1||Liquid nitrogen jet:1||CHARGEEXCHANGE:1||NOBEL LECTURE:1||VARISTOR:1||EPITAXY:1||THINDISK LASER:1||HIGHREPETITIONRATE:1||Atom lasers:1||Electronimpact excitation:1||High order harmonics:1||ultrafast technology:1||PEAK POWER:1||CHARGED ALUMINUM CLUSTERS:1||GaN:1||THIN:1||Electron beam:1||INTENSE:1||Hard Xray pulse generation:1||NONLINEAR THOMSON SCATTERING:1||MULTILAYER:1||UVvisible spectrometer:1||ATOMS:1||innershell transitions:1||CORRECTED CONCAVE GRATINGS:1||DISCHARGE:1||LASERPLASMA:1||thin film:1||reflectivity:1||opacity:1||gain:1||smallangle Xray scattering:1||SOFTXRAY:1||ZINCOXIDE:1||CYGNUSX3:1||Betatron oscillation:1||ACCELERATOR:1||STRAINEDLAYER SUPERLATTICES:1||OPTICAL PARAMETRIC AMPLIFICATION:1||PASSIVE MODELOCKING:1||Collision dynamics:1||MUM:1||EXACTEXCHANGE:1||BASISSET:1||APPROXIMATION:1||OXYNITRIDES:1||Beam energy modulation:1||polarization spectroscopy:1||REORIENTATION TRANSITION:1||DEPENDENCE:1||sulfurs:1||BUILDINGBLOCKS:1||RATES:1||OPTICAL PULSES:1||toroidal mirror:1||XRAY LASER:1||CALCIUM:1||radially polarized laser:1||GRAINBOUNDARIES:1||VAPORDEPOSITION:1||Xray generation:1||MAGNETIZATION:1||Electric excitation:1||Laserinduced gas plasmas:1||Qualitative analysis:1||SCHEME:1||RADIATION:10||PULSES:8||PHOTOLUMINESCENCE:7||LASER:7||GENERATION:6||NANORODS:6||GROWTH:6||NANOWIRES:5||IMPLANTED 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SEMICONDUCTORS:2||MOLECULARBEAM EPITAXY:2||EARTHDOPED GAN:2||LASER FIELDS:2||CHIRPEDPULSEAMPLIFICATION:2||ALN:2||GAUSSIANBEAM:2||ASSISTED CATALYTIC GROWTH:2||BLUE:2||NANOSTRUCTURES:2||MAGNETOELECTRONICS:2||MICROSCOPY:2||ELECTROLUMINESCENCE:2||LASERPULSES:2||GaN nanowires:2||GALLIUM NITRIDE NANOWIRES:2||GAMNN:2||NANOTUBES:2||PHYSICS:2||Femtosecond laser:2||parametric oscillators and amplifiers:1||ultrafast lasers:1||VALENCE:1||nanowires:1||DILUTED MAGNETIC SEMICONDUCTOR:1||LUMINESCENCE:1||Density modulation:1||Energy modulation:1||Current enhanced SASE free electron laser:1||Undulator radiation:1||FREEELECTRON LASERS:1||ULTRATHIN FERROMAGNETICFILMS:1||OXIDEFILMS:1||ABLATION:1||COMPONENT:1||METAL:1||innershell excited states:1||Nelike ions:1||TRANSITIONS:1||XUV spectrometer:1||DIAGNOSTICS:1||Xray scattering:1||MO/SI:1||pulsed laser deposition:1||KEV IMPACT ENERGIES:1||vacuum electron acceleration:1||HIGHINTENSITY LASER:1||JUNCTIONS:1||LOWTEMPERATURE GROWTH:1||nanocrystalline materials:1||MOLECULAR PHOTOIONIZATION:1||LOCALIZATION:1||DEUTERIUM CLUSTERS:1||EXPLOSIONS:1||REGENERATIVE AMPLIFIERS:1||RAREGASES:1||THz radiation:1||FREEELECTRON LASER:1||REALTIME OBSERVATION:1||TARGET:1||photoionized plasmas:1||fs Xray laser:1||emission profile:1||HIGHORDER HARMONICS:1||Xray laser:1||atomic transition:1||EXCITATION:1||LASERS:1||PERFORMANCE:1||RELATIVISTIC ELECTRONS:1||BI2O3DOPED ZNO:1||INNERSHELL IONIZATION:1||Laser wakefield:1||FREQUENCY:1||SOLIDSTATE LASERS:1||Linearly polarized:1||THERMIONIC EMISSION:1||PULSE AMPLIFICATION SYSTEM:1||BIB3O6:1||NM:1||NONCOVALENT INTERACTIONS:1||CRYSTALLINE:1||INTENSITY:1||JETS:1||COHERENT:1||LINE:1||ANGULARDISTRIBUTION:1||SILVER IONS:1||magnetic anisotropy:1||DEVICES:1||Auger transitions:1||CosterKronig transitions:1||EFFICIENT:1||ELECTRONIMPACT IONIZATION:1||ULTRASHORTPULSE:1||Nanowire:1||Heterostructure:1||soft Xray reflectivity:1||PLASMA ACCELERATOR:1||ZINCOXIDE NANOWIRES:1||CHEMICALVAPORDEPOSITION:1||Electron acceleration:1||Ionization of gases:1||Delay dependent:1||MULTIPHOTON IONIZATION:1||FRAGMENTATION:1||GASJET:1||ultrafast nonlinear optics:1||CYCLE PULSES:1||KHZ:1||chemical vapor deposition:1||ferromagnetism:1||ABSORPTION:1||TERAHERTZ RADIATION:1||SCIENCE:1||FIELDS:1||ELECTRONS:1||nanomultilayer structures:1||YIELDS:1||AUGER:1||10HZ REPETITION RATE:1||MULTITERAWATT:1||SPECTROGRAPH:1||HIGHHARMONICGENERATION:1||spectroscopy:1||level population:1||PARTICLEACCELERATION:1||OPTICAL FREQUENCYMEASUREMENT:1||NANOWALLS:1||ROOMTEMPERATURE:1||AVERAGE OUTPUT POWER:1||GROUPVELOCITYMISMATCH:1||Impact ionization:1||Dynamics:1||Lasers:1||Collisional process:1||ABOVETHRESHOLD IONIZATION:1||MAINGROUP THERMOCHEMISTRY:1||dilute magnetic semiconductors:1||GACRN:1||SIZE:1||ATTOSECOND:1||Ar cluster:1||Xray astrophysics:1||photoionization:1||irons:1||normal incidence pulsed laser deposition:1||SHELLS:1||Silicon Oxide:1||gaspuff Zpinch:1||Xray:1||soft Xray reflectors:1||ESCAPE:1||ZN2SIO4:1||SILICA:1||Time 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materials:1||MOLECULAR PHOTOIONIZATION:1||LOCALIZATION:1||DEUTERIUM CLUSTERS:1||EXPLOSIONS:1||REGENERATIVE AMPLIFIERS:1||RAREGASES:1||THz radiation:1||FREEELECTRON LASER:1||REALTIME OBSERVATION:1||TARGET:1||photoionized plasmas:1||fs Xray laser:1||emission profile:1||HIGHORDER HARMONICS:1||Xray laser:1||atomic transition:1||EXCITATION:1||LASERS:1||PERFORMANCE:1||RELATIVISTIC ELECTRONS:1||BI2O3DOPED ZNO:1||INNERSHELL IONIZATION:1||Laser wakefield:1||FREQUENCY:1||SOLIDSTATE LASERS:1||Linearly polarized:1||THERMIONIC EMISSION:1||PULSE AMPLIFICATION SYSTEM:1||BIB3O6:1||NM:1||NONCOVALENT INTERACTIONS:1||CRYSTALLINE:1||INTENSITY:1||JETS:1||COHERENT:1||LINE:1||ANGULARDISTRIBUTION:1||SILVER IONS:1||magnetic anisotropy:1||DEVICES:1||Auger transitions:1||CosterKronig transitions:1||EFFICIENT:1||ELECTRONIMPACT IONIZATION:1||ULTRASHORTPULSE:1||Nanowire:1||Heterostructure:1||soft Xray reflectivity:1||PLASMA ACCELERATOR:1||ZINCOXIDE NANOWIRES:1||CHEMICALVAPORDEPOSITION:1||Electron acceleration:1||Ionization of gases:1||Delay dependent:1||MULTIPHOTON IONIZATION:1||FRAGMENTATION:1||GASJET:1||ultrafast nonlinear optics:1||CYCLE PULSES:1||KHZ:1||chemical vapor deposition:1||ferromagnetism:1||ABSORPTION:1||TERAHERTZ RADIATION:1||SCIENCE:1||FIELDS:1||ELECTRONS:1||nanomultilayer structures:1||YIELDS:1||AUGER:1||10HZ REPETITION RATE:1||MULTITERAWATT:1||SPECTROGRAPH:1||HIGHHARMONICGENERATION:1||spectroscopy:1||level population:1||PARTICLEACCELERATION:1||OPTICAL FREQUENCYMEASUREMENT:1||NANOWALLS:1||ROOMTEMPERATURE:1||AVERAGE OUTPUT POWER:1||GROUPVELOCITYMISMATCH:1||Impact ionization:1||Dynamics:1||Lasers:1||Collisional process:1||ABOVETHRESHOLD IONIZATION:1||MAINGROUP THERMOCHEMISTRY:1||dilute magnetic semiconductors:1||GACRN:1||SIZE:1||ATTOSECOND:1||Ar cluster:1||Xray astrophysics:1||photoionization:1||irons:1||normal incidence pulsed laser deposition:1||SHELLS:1||Silicon Oxide:1||gaspuff Zpinch:1||Xray:1||soft Xray reflectors:1||ESCAPE:1||ZN2SIO4:1||SILICA:1||Time delay:1||Collisional plasmas:1||MASSSPECTROMETRY:1||NUCLEARFUSION:1||PARAMETRIC AMPLIFICATION:1||LYING ELECTRONIC STATES:1||ADJUSTABLEPARAMETERS:1||MAGNETICPROPERTIES:1||LIQUIDPHASE EPITAXY:1||CEP laser:1||REGION:1||Plasma waveguide:1||AMBIENT GAS:1||DEPOSITION:1||HARMONICGENERATION:1||ENHANCEMENT:1||imaging spectrometer:1||Abel inversion:1||Water window:1||Liquid nitrogen jet:1||CHARGEEXCHANGE:1||NOBEL LECTURE:1||VARISTOR:1||EPITAXY:1||THINDISK LASER:1||HIGHREPETITIONRATE:1||Atom lasers:1||Electronimpact excitation:1||High order harmonics:1||ultrafast technology:1||PEAK POWER:1||CHARGED ALUMINUM CLUSTERS:1||GaN:1||THIN:1||Electron beam:1||INTENSE:1||Hard Xray pulse generation:1||NONLINEAR THOMSON SCATTERING:1||MULTILAYER:1||UVvisible spectrometer:1||ATOMS:1||innershell transitions:1||CORRECTED CONCAVE GRATINGS:1||DISCHARGE:1||LASERPLASMA:1||thin film:1||reflectivity:1||opacity:1||gain:1||smallangle Xray scattering:1||SOFTXRAY:1||ZINCOXIDE:1||CYGNUSX3:1||Betatron oscillation:1||ACCELERATOR:1||STRAINEDLAYER SUPERLATTICES:1||OPTICAL PARAMETRIC AMPLIFICATION:1||PASSIVE MODELOCKING:1||Collision dynamics:1||MUM:1||EXACTEXCHANGE:1||BASISSET:1||APPROXIMATION:1||OXYNITRIDES:1||Beam energy modulation:1||polarization spectroscopy:1||REORIENTATION TRANSITION:1||DEPENDENCE:1||sulfurs:1||BUILDINGBLOCKS:1||RATES:1||OPTICAL PULSES:1||toroidal mirror:1||XRAY LASER:1||CALCIUM:1||radially polarized laser:1||GRAINBOUNDARIES:1||VAPORDEPOSITION:1||Xray generation:1||MAGNETIZATION:1||Electric excitation:1||Laserinduced gas plasmas:1||Qualitative analysis:1||SCHEME:1||RADIATION:10||PULSES:8||PHOTOLUMINESCENCE:7||LASER:7||GENERATION:6||NANORODS:6||GROWTH:6||NANOWIRES:5||IMPLANTED GAN:5||SPECTROSCOPY:5||THINFILMS:4||DYNAMICS:4||SILICON:4||EXTREMEULTRAVIOLET:4||AMPLIFICATION:4||PRESSURE:4||PHASE:4||OPTICALPROPERTIES:4||SYSTEM:4||EMISSION:4||FEL:3||N2O:3||FILMS:3||OPTICS:3||SPECTRA:3||FIELD:3||MIRRORS:3||ARRAYS:3||CLUSTERS:3||SIO2:3||IONIZATION:3||VACUUM:3||SCATTERING:3||IONS:2||LUMINESCENCE PROPERTIES:2||ANISOTROPY:2||BEAMS:2||DIFFRACTION:2||DISPERSION:2||chemical vapor deposition (CVD):2||ELECTRONICSTRUCTURE:2||MOSFETS:2||SI3N4:2||DENSITY:2||LIGHT:2||PLASMAS:2||MATTER:2||nanocomposites:2||RAMANSCATTERING:2||NANOPARTICLES:2||OXIDE:2||AMPLIFIED SPONTANEOUS EMISSION:2||NM WAVELENGTH:2||GAIN:2||CARBON NANOTUBES:2||CROSSSECTIONS:2||LIGHTEMITTINGDIODES:2||PULSE:2||CARBON PLASMA:2||TISAPPHIRE LASER:2||Raman scattering:2||ROUTE:2||multilayer:2||CATHODOLUMINESCENCE:2||highresolution transmission electronic microscope (HRTEM):2||DIFFERENCEFREQUENCYGENERATION:2||CRYSTAL:2||laserproduced plasma:2||NANOCABLES:2||photoluminescence:2||MAGNETIC ALLOY SEMICONDUCTORS:2||MOLECULARBEAM EPITAXY:2||EARTHDOPED GAN:2||LASER FIELDS:2||CHIRPEDPULSEAMPLIFICATION:2||ALN:2||GAUSSIANBEAM:2||ASSISTED CATALYTIC GROWTH:2||BLUE:2||NANOSTRUCTURES:2||MAGNETOELECTRONICS:2||MICROSCOPY:2||ELECTROLUMINESCENCE:2||LASERPULSES:2||GaN nanowires:2||GALLIUM NITRIDE NANOWIRES:2||GAMNN:2||NANOTUBES:2||PHYSICS:2||Femtosecond laser:2||parametric oscillators and amplifiers:1||ultrafast lasers:1||VALENCE:1||nanowires:1||DILUTED MAGNETIC SEMICONDUCTOR:1||LUMINESCENCE:1||Density modulation:1||Energy modulation:1||Current enhanced SASE free electron laser:1||Undulator radiation:1||FREEELECTRON LASERS:1||ULTRATHIN FERROMAGNETICFILMS:1||OXIDEFILMS:1||ABLATION:1||COMPONENT:1||METAL:1||innershell excited states:1||Nelike ions:1||TRANSITIONS:1||XUV spectrometer:1||DIAGNOSTICS:1||Xray scattering:1||MO/SI:1||pulsed laser deposition:1||KEV IMPACT ENERGIES:1||vacuum electron acceleration:1||HIGHINTENSITY LASER:1||JUNCTIONS:1||LOWTEMPERATURE GROWTH:1||nanocrystalline materials:1||MOLECULAR PHOTOIONIZATION:1||LOCALIZATION:1||DEUTERIUM CLUSTERS:1||EXPLOSIONS:1||REGENERATIVE AMPLIFIERS:1||RAREGASES:1||THz radiation:1||FREEELECTRON LASER:1||REALTIME OBSERVATION:1||TARGET:1||photoionized plasmas:1||fs Xray laser:1||emission profile:1||HIGHORDER HARMONICS:1||Xray laser:1||atomic transition:1||EXCITATION:1||LASERS:1||PERFORMANCE:1||RELATIVISTIC ELECTRONS:1||BI2O3DOPED ZNO:1||INNERSHELL IONIZATION:1||Laser wakefield:1||FREQUENCY:1||SOLIDSTATE LASERS:1||Linearly polarized:1||THERMIONIC EMISSION:1||PULSE AMPLIFICATION SYSTEM:1||BIB3O6:1||NM:1||NONCOVALENT INTERACTIONS:1||CRYSTALLINE:1||INTENSITY:1||JETS:1||COHERENT:1||LINE:1||ANGULARDISTRIBUTION:1||SILVER IONS:1||magnetic anisotropy:1||DEVICES:1||Auger transitions:1||CosterKronig transitions:1||EFFICIENT:1||ELECTRONIMPACT IONIZATION:1||ULTRASHORTPULSE:1||Nanowire:1||Heterostructure:1||soft Xray reflectivity:1||PLASMA ACCELERATOR:1||ZINCOXIDE NANOWIRES:1||CHEMICALVAPORDEPOSITION:1||Electron acceleration:1||Ionization of gases:1||Delay dependent:1||MULTIPHOTON IONIZATION:1||FRAGMENTATION:1||GASJET:1||ultrafast nonlinear optics:1||CYCLE PULSES:1||KHZ:1||chemical vapor deposition:1||ferromagnetism:1||ABSORPTION:1||TERAHERTZ RADIATION:1||SCIENCE:1||FIELDS:1||ELECTRONS:1||nanomultilayer structures:1||YIELDS:1||AUGER:1||10HZ REPETITION RATE:1||MULTITERAWATT:1||SPECTROGRAPH:1||HIGHHARMONICGENERATION:1||spectroscopy:1||level population:1||PARTICLEACCELERATION:1||OPTICAL FREQUENCYMEASUREMENT:1||NANOWALLS:1||ROOMTEMPERATURE:1||AVERAGE OUTPUT POWER:1||GROUPVELOCITYMISMATCH:1||Impact ionization:1||Dynamics:1||Lasers:1||Collisional process:1||ABOVETHRESHOLD IONIZATION:1||MAINGROUP THERMOCHEMISTRY:1||dilute magnetic semiconductors:1||GACRN:1||SIZE:1||ATTOSECOND:1||Ar cluster:1||Xray astrophysics:1||photoionization:1||irons:1||normal incidence pulsed laser deposition:1||SHELLS:1||Silicon Oxide:1||gaspuff Zpinch:1||Xray:1||soft Xray reflectors:1||ESCAPE:1||ZN2SIO4:1||SILICA:1||Time delay:1||Collisional plasmas:1||MASSSPECTROMETRY:1||NUCLEARFUSION:1||PARAMETRIC AMPLIFICATION:1||LYING ELECTRONIC STATES:1||ADJUSTABLEPARAMETERS:1||MAGNETICPROPERTIES:1||LIQUIDPHASE EPITAXY:1||CEP laser:1||REGION:1||Plasma waveguide:1||AMBIENT GAS:1||DEPOSITION:1||HARMONICGENERATION:1||ENHANCEMENT:1||imaging spectrometer:1||Abel inversion:1||Water window:1||Liquid nitrogen jet:1||CHARGEEXCHANGE:1||NOBEL LECTURE:1||VARISTOR:1||EPITAXY:1||THINDISK LASER:1||HIGHREPETITIONRATE:1||Atom lasers:1||Electronimpact excitation:1||High order harmonics:1||ultrafast technology:1||PEAK POWER:1||CHARGED ALUMINUM CLUSTERS:1||GaN:1||THIN:1||Electron beam:1||INTENSE:1||Hard Xray pulse generation:1||NONLINEAR THOMSON SCATTERING:1||MULTILAYER:1||UVvisible spectrometer:1||ATOMS:1||innershell transitions:1||CORRECTED CONCAVE GRATINGS:1||DISCHARGE:1||LASERPLASMA:1||thin film:1||reflectivity:1||opacity:1||gain:1||smallangle Xray scattering:1||SOFTXRAY:1||ZINCOXIDE:1||CYGNUSX3:1||Betatron oscillation:1||ACCELERATOR:1||STRAINEDLAYER SUPERLATTICES:1||OPTICAL PARAMETRIC AMPLIFICATION:1||PASSIVE MODELOCKING:1||Collision dynamics:1||MUM:1||EXACTEXCHANGE:1||BASISSET:1||APPROXIMATION:1||OXYNITRIDES:1||Beam energy modulation:1||polarization spectroscopy:1||REORIENTATION TRANSITION:1||DEPENDENCE:1||sulfurs:1||BUILDINGBLOCKS:1||RATES:1||OPTICAL PULSES:1||toroidal mirror:1||XRAY LASER:1||CALCIUM:1||radially polarized laser:1||GRAINBOUNDARIES:1||VAPORDEPOSITION:1||Xray generation:1||MAGNETIZATION:1||Electric excitation:1||Laserinduced gas plasmas:1||Qualitative analysis:1||SCHEME:1||RADIATION:10||PULSES:8||PHOTOLUMINESCENCE:7||LASER:7||GENERATION:6||NANORODS:6||GROWTH:6||NANOWIRES:5||IMPLANTED 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SEMICONDUCTORS:2||MOLECULARBEAM EPITAXY:2||EARTHDOPED GAN:2||LASER FIELDS:2||CHIRPEDPULSEAMPLIFICATION:2||ALN:2||GAUSSIANBEAM:2||ASSISTED CATALYTIC GROWTH:2||BLUE:2||NANOSTRUCTURES:2||MAGNETOELECTRONICS:2||MICROSCOPY:2||ELECTROLUMINESCENCE:2||LASERPULSES:2||GaN nanowires:2||GALLIUM NITRIDE NANOWIRES:2||GAMNN:2||NANOTUBES:2||PHYSICS:2||Femtosecond laser:2||parametric oscillators and amplifiers:1||ultrafast lasers:1||VALENCE:1||nanowires:1||DILUTED MAGNETIC SEMICONDUCTOR:1||LUMINESCENCE:1||Density modulation:1||Energy modulation:1||Current enhanced SASE free electron laser:1||Undulator radiation:1||FREEELECTRON LASERS:1||ULTRATHIN FERROMAGNETICFILMS:1||OXIDEFILMS:1||ABLATION:1||COMPONENT:1||METAL:1||innershell excited states:1||Nelike ions:1||TRANSITIONS:1||XUV spectrometer:1||DIAGNOSTICS:1||Xray scattering:1||MO/SI:1||pulsed laser deposition:1||KEV IMPACT ENERGIES:1||vacuum electron acceleration:1||HIGHINTENSITY LASER:1||JUNCTIONS:1||LOWTEMPERATURE GROWTH:1||nanocrystalline materials:1||MOLECULAR PHOTOIONIZATION:1||LOCALIZATION:1||DEUTERIUM CLUSTERS:1||EXPLOSIONS:1||REGENERATIVE AMPLIFIERS:1||RAREGASES:1||THz radiation:1||FREEELECTRON LASER:1||REALTIME OBSERVATION:1||TARGET:1||photoionized plasmas:1||fs Xray laser:1||emission profile:1||HIGHORDER HARMONICS:1||Xray laser:1||atomic transition:1||EXCITATION:1||LASERS:1||PERFORMANCE:1||RELATIVISTIC ELECTRONS:1||BI2O3DOPED ZNO:1||INNERSHELL IONIZATION:1||Laser wakefield:1||FREQUENCY:1||SOLIDSTATE LASERS:1||Linearly polarized:1||THERMIONIC EMISSION:1||PULSE AMPLIFICATION SYSTEM:1||BIB3O6:1||NM:1||NONCOVALENT INTERACTIONS:1||CRYSTALLINE:1||INTENSITY:1||JETS:1||COHERENT:1||LINE:1||ANGULARDISTRIBUTION:1||SILVER IONS:1||magnetic anisotropy:1||DEVICES:1||Auger transitions:1||CosterKronig transitions:1||EFFICIENT:1||ELECTRONIMPACT IONIZATION:1||ULTRASHORTPULSE:1||Nanowire:1||Heterostructure:1||soft Xray reflectivity:1||PLASMA ACCELERATOR:1||ZINCOXIDE NANOWIRES:1||CHEMICALVAPORDEPOSITION:1||Electron acceleration:1||Ionization of gases:1||Delay dependent:1||MULTIPHOTON IONIZATION:1||FRAGMENTATION:1||GASJET:1||ultrafast nonlinear optics:1||CYCLE PULSES:1||KHZ:1||chemical vapor deposition:1||ferromagnetism:1||ABSORPTION:1||TERAHERTZ RADIATION:1||SCIENCE:1||FIELDS:1||ELECTRONS:1||nanomultilayer structures:1||YIELDS:1||AUGER:1||10HZ REPETITION RATE:1||MULTITERAWATT:1||SPECTROGRAPH:1||HIGHHARMONICGENERATION:1||spectroscopy:1||level population:1||PARTICLEACCELERATION:1||OPTICAL FREQUENCYMEASUREMENT:1||NANOWALLS:1||ROOMTEMPERATURE:1||AVERAGE OUTPUT POWER:1||GROUPVELOCITYMISMATCH:1||Impact ionization:1||Dynamics:1||Lasers:1||Collisional process:1||ABOVETHRESHOLD IONIZATION:1||MAINGROUP THERMOCHEMISTRY:1||dilute magnetic semiconductors:1||GACRN:1||SIZE:1||ATTOSECOND:1||Ar cluster:1||Xray astrophysics:1||photoionization:1||irons:1||normal incidence pulsed laser deposition:1||SHELLS:1||Silicon Oxide:1||gaspuff Zpinch:1||Xray:1||soft Xray reflectors:1||ESCAPE:1||ZN2SIO4:1||SILICA:1||Time 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materials:1||MOLECULAR PHOTOIONIZATION:1||LOCALIZATION:1||DEUTERIUM CLUSTERS:1||EXPLOSIONS:1||REGENERATIVE AMPLIFIERS:1||RAREGASES:1||THz radiation:1||FREEELECTRON LASER:1||REALTIME OBSERVATION:1||TARGET:1||photoionized plasmas:1||fs Xray laser:1||emission profile:1||HIGHORDER HARMONICS:1||Xray laser:1||atomic transition:1||EXCITATION:1||LASERS:1||PERFORMANCE:1||RELATIVISTIC ELECTRONS:1||BI2O3DOPED ZNO:1||INNERSHELL IONIZATION:1||Laser wakefield:1||FREQUENCY:1||SOLIDSTATE LASERS:1||Linearly polarized:1||THERMIONIC EMISSION:1||PULSE AMPLIFICATION SYSTEM:1||BIB3O6:1||NM:1||NONCOVALENT INTERACTIONS:1||CRYSTALLINE:1||INTENSITY:1||JETS:1||COHERENT:1||LINE:1||ANGULARDISTRIBUTION:1||SILVER IONS:1||magnetic anisotropy:1||DEVICES:1||Auger transitions:1||CosterKronig transitions:1||EFFICIENT:1||ELECTRONIMPACT IONIZATION:1||ULTRASHORTPULSE:1||Nanowire:1||Heterostructure:1||soft Xray reflectivity:1||PLASMA ACCELERATOR:1||ZINCOXIDE NANOWIRES:1||CHEMICALVAPORDEPOSITION:1||Electron acceleration:1||Ionization of gases:1||Delay dependent:1||MULTIPHOTON IONIZATION:1||FRAGMENTATION:1||GASJET:1||ultrafast nonlinear optics:1||CYCLE PULSES:1||KHZ:1||chemical vapor deposition:1||ferromagnetism:1||ABSORPTION:1||TERAHERTZ RADIATION:1||SCIENCE:1||FIELDS:1||ELECTRONS:1||nanomultilayer structures:1||YIELDS:1||AUGER:1||10HZ REPETITION RATE:1||MULTITERAWATT:1||SPECTROGRAPH:1||HIGHHARMONICGENERATION:1||spectroscopy:1||level population:1||PARTICLEACCELERATION:1||OPTICAL FREQUENCYMEASUREMENT:1||NANOWALLS:1||ROOMTEMPERATURE:1||AVERAGE OUTPUT POWER:1||GROUPVELOCITYMISMATCH:1||Impact ionization:1||Dynamics:1||Lasers:1||Collisional process:1||ABOVETHRESHOLD IONIZATION:1||MAINGROUP THERMOCHEMISTRY:1||dilute magnetic semiconductors:1||GACRN:1||SIZE:1||ATTOSECOND:1||Ar cluster:1||Xray astrophysics:1||photoionization:1||irons:1||normal incidence pulsed laser deposition:1||SHELLS:1||Silicon Oxide:1||gaspuff Zpinch:1||Xray:1||soft Xray reflectors:1||ESCAPE:1||ZN2SIO4:1||SILICA:1||Time delay:1||Collisional plasmas:1||MASSSPECTROMETRY:1||NUCLEARFUSION:1||PARAMETRIC AMPLIFICATION:1||LYING ELECTRONIC STATES:1||ADJUSTABLEPARAMETERS:1||MAGNETICPROPERTIES:1||LIQUIDPHASE EPITAXY:1||CEP laser:1||REGION:1||Plasma waveguide:1||AMBIENT GAS:1||DEPOSITION:1||HARMONICGENERATION:1||ENHANCEMENT:1||imaging spectrometer:1||Abel inversion:1||Water window:1||Liquid nitrogen jet:1||CHARGEEXCHANGE:1||NOBEL LECTURE:1||VARISTOR:1||EPITAXY:1||THINDISK LASER:1||HIGHREPETITIONRATE:1||Atom lasers:1||Electronimpact excitation:1||High order harmonics:1||ultrafast technology:1||PEAK POWER:1||CHARGED ALUMINUM CLUSTERS:1||GaN:1||THIN:1||Electron beam:1||INTENSE:1||Hard Xray pulse generation:1||NONLINEAR THOMSON SCATTERING:1||MULTILAYER:1||UVvisible spectrometer:1||ATOMS:1||innershell transitions:1||CORRECTED CONCAVE GRATINGS:1||DISCHARGE:1||LASERPLASMA:1||thin film:1||reflectivity:1||opacity:1||gain:1||smallangle Xray scattering:1||SOFTXRAY:1||ZINCOXIDE:1||CYGNUSX3:1||Betatron oscillation:1||ACCELERATOR:1||STRAINEDLAYER SUPERLATTICES:1||OPTICAL PARAMETRIC AMPLIFICATION:1||PASSIVE MODELOCKING:1||Collision dynamics:1||MUM:1||EXACTEXCHANGE:1||BASISSET:1||APPROXIMATION:1||OXYNITRIDES:1||Beam energy modulation:1||polarization spectroscopy:1||REORIENTATION TRANSITION:1||DEPENDENCE:1||sulfurs:1||BUILDINGBLOCKS:1||RATES:1||OPTICAL PULSES:1||toroidal mirror:1||XRAY LASER:1||CALCIUM:1||radially polarized laser:1||GRAINBOUNDARIES:1||VAPORDEPOSITION:1||Xray generation:1||MAGNETIZATION:1||Electric excitation:1||Laserinduced gas plasmas:1||Qualitative analysis:1||SCHEME:1||RADIATION:10||PULSES:8||PHOTOLUMINESCENCE:7||LASER:7||GENERATION:6||NANORODS:6||GROWTH:6||NANOWIRES:5||IMPLANTED GAN:5||SPECTROSCOPY:5||THINFILMS:4||DYNAMICS:4||SILICON:4||EXTREMEULTRAVIOLET:4||AMPLIFICATION:4||PRESSURE:4||PHASE:4||OPTICALPROPERTIES:4||SYSTEM:4||EMISSION:4||FEL:3||N2O:3||FILMS:3||OPTICS:3||SPECTRA:3||FIELD:3||MIRRORS:3||ARRAYS:3||CLUSTERS:3||SIO2:3||IONIZATION:3||VACUUM:3||SCATTERING:3||IONS:2||LUMINESCENCE PROPERTIES:2||ANISOTROPY:2||BEAMS:2||DIFFRACTION:2||DISPERSION:2||chemical vapor deposition (CVD):2||ELECTRONICSTRUCTURE:2||MOSFETS:2||SI3N4:2||DENSITY:2||LIGHT:2||PLASMAS:2||MATTER:2||nanocomposites:2||RAMANSCATTERING:2||NANOPARTICLES:2||OXIDE:2||AMPLIFIED SPONTANEOUS EMISSION:2||NM WAVELENGTH:2||GAIN:2||CARBON NANOTUBES:2||CROSSSECTIONS:2||LIGHTEMITTINGDIODES:2||PULSE:2||CARBON PLASMA:2||TISAPPHIRE LASER:2||Raman scattering:2||ROUTE:2||multilayer:2||CATHODOLUMINESCENCE:2||highresolution transmission electronic microscope (HRTEM):2||DIFFERENCEFREQUENCYGENERATION:2||CRYSTAL:2||laserproduced plasma:2||NANOCABLES:2||photoluminescence:2||MAGNETIC ALLOY SEMICONDUCTORS:2||MOLECULARBEAM EPITAXY:2||EARTHDOPED GAN:2||LASER FIELDS:2||CHIRPEDPULSEAMPLIFICATION:2||ALN:2||GAUSSIANBEAM:2||ASSISTED CATALYTIC GROWTH:2||BLUE:2||NANOSTRUCTURES:2||MAGNETOELECTRONICS:2||MICROSCOPY:2||ELECTROLUMINESCENCE:2||LASERPULSES:2||GaN nanowires:2||GALLIUM NITRIDE NANOWIRES:2||GAMNN:2||NANOTUBES:2||PHYSICS:2||Femtosecond laser:2||parametric oscillators and amplifiers:1||ultrafast lasers:1||VALENCE:1||nanowires:1||DILUTED MAGNETIC SEMICONDUCTOR:1||LUMINESCENCE:1||Density modulation:1||Energy modulation:1||Current enhanced SASE free electron laser:1||Undulator radiation:1||FREEELECTRON LASERS:1||ULTRATHIN FERROMAGNETICFILMS:1||OXIDEFILMS:1||ABLATION:1||COMPONENT:1||METAL:1||innershell excited states:1||Nelike ions:1||TRANSITIONS:1||XUV spectrometer:1||DIAGNOSTICS:1||Xray scattering:1||MO/SI:1||pulsed laser deposition:1||KEV IMPACT ENERGIES:1||vacuum electron acceleration:1||HIGHINTENSITY LASER:1||JUNCTIONS:1||LOWTEMPERATURE GROWTH:1||nanocrystalline materials:1||MOLECULAR PHOTOIONIZATION:1||LOCALIZATION:1||DEUTERIUM CLUSTERS:1||EXPLOSIONS:1||REGENERATIVE AMPLIFIERS:1||RAREGASES:1||THz radiation:1||FREEELECTRON LASER:1||REALTIME OBSERVATION:1||TARGET:1||photoionized plasmas:1||fs Xray laser:1||emission profile:1||HIGHORDER HARMONICS:1||Xray laser:1||atomic transition:1||EXCITATION:1||LASERS:1||PERFORMANCE:1||RELATIVISTIC ELECTRONS:1||BI2O3DOPED ZNO:1||INNERSHELL IONIZATION:1||Laser wakefield:1||FREQUENCY:1||SOLIDSTATE LASERS:1||Linearly polarized:1||THERMIONIC EMISSION:1||PULSE AMPLIFICATION SYSTEM:1||BIB3O6:1||NM:1||NONCOVALENT INTERACTIONS:1||CRYSTALLINE:1||INTENSITY:1||JETS:1||COHERENT:1||LINE:1||ANGULARDISTRIBUTION:1||SILVER IONS:1||magnetic anisotropy:1||DEVICES:1||Auger transitions:1||CosterKronig transitions:1||EFFICIENT:1||ELECTRONIMPACT IONIZATION:1||ULTRASHORTPULSE:1||Nanowire:1||Heterostructure:1||soft Xray reflectivity:1||PLASMA ACCELERATOR:1||ZINCOXIDE NANOWIRES:1||CHEMICALVAPORDEPOSITION:1||Electron acceleration:1||Ionization of gases:1||Delay dependent:1||MULTIPHOTON IONIZATION:1||FRAGMENTATION:1||GASJET:1||ultrafast nonlinear optics:1||CYCLE PULSES:1||KHZ:1||chemical vapor deposition:1||ferromagnetism:1||ABSORPTION:1||TERAHERTZ RADIATION:1||SCIENCE:1||FIELDS:1||ELECTRONS:1||nanomultilayer structures:1||YIELDS:1||AUGER:1||10HZ REPETITION RATE:1||MULTITERAWATT:1||SPECTROGRAPH:1||HIGHHARMONICGENERATION:1||spectroscopy:1||level population:1||PARTICLEACCELERATION:1||OPTICAL FREQUENCYMEASUREMENT:1||NANOWALLS:1||ROOMTEMPERATURE:1||AVERAGE OUTPUT POWER:1||GROUPVELOCITYMISMATCH:1||Impact ionization:1||Dynamics:1||Lasers:1||Collisional process:1||ABOVETHRESHOLD IONIZATION:1||MAINGROUP THERMOCHEMISTRY:1||dilute magnetic semiconductors:1||GACRN:1||SIZE:1||ATTOSECOND:1||Ar cluster:1||Xray astrophysics:1||photoionization:1||irons:1||normal incidence pulsed laser deposition:1||SHELLS:1||Silicon Oxide:1||gaspuff Zpinch:1||Xray:1||soft Xray reflectors:1||ESCAPE:1||ZN2SIO4:1||SILICA:1||Time delay:1||Collisional plasmas:1||MASSSPECTROMETRY:1||NUCLEARFUSION:1||PARAMETRIC AMPLIFICATION:1||LYING ELECTRONIC STATES:1||ADJUSTABLEPARAMETERS:1||MAGNETICPROPERTIES:1||LIQUIDPHASE EPITAXY:1||CEP laser:1||REGION:1||Plasma waveguide:1||AMBIENT GAS:1||DEPOSITION:1||HARMONICGENERATION:1||ENHANCEMENT:1||imaging spectrometer:1||Abel inversion:1||Water window:1||Liquid nitrogen jet:1||CHARGEEXCHANGE:1||NOBEL LECTURE:1||VARISTOR:1||EPITAXY:1||THINDISK LASER:1||HIGHREPETITIONRATE:1||Atom lasers:1||Electronimpact excitation:1||High order harmonics:1||ultrafast technology:1||PEAK POWER:1||CHARGED ALUMINUM CLUSTERS:1||GaN:1||THIN:1||Electron beam:1||INTENSE:1||Hard Xray pulse generation:1||NONLINEAR THOMSON SCATTERING:1||MULTILAYER:1||UVvisible spectrometer:1||ATOMS:1||innershell transitions:1||CORRECTED CONCAVE GRATINGS:1||DISCHARGE:1||LASERPLASMA:1||thin film:1||reflectivity:1||opacity:1||gain:1||smallangle Xray scattering:1||SOFTXRAY:1||ZINCOXIDE:1||CYGNUSX3:1||Betatron oscillation:1||ACCELERATOR:1||STRAINEDLAYER SUPERLATTICES:1||OPTICAL PARAMETRIC AMPLIFICATION:1||PASSIVE MODELOCKING:1||Collision dynamics:1||MUM:1||EXACTEXCHANGE:1||BASISSET:1||APPROXIMATION:1||OXYNITRIDES:1||Beam energy modulation:1||polarization spectroscopy:1||REORIENTATION TRANSITION:1||DEPENDENCE:1||sulfurs:1||BUILDINGBLOCKS:1||RATES:1||OPTICAL PULSES:1||toroidal mirror:1||XRAY LASER:1||CALCIUM:1||radially polarized laser:1||GRAINBOUNDARIES:1||VAPORDEPOSITION:1||Xray generation:1||MAGNETIZATION:1||Electric excitation:1||Laserinduced gas plasmas:1||Qualitative analysis:1||SCHEME:1||RADIATION:10||PULSES:8||PHOTOLUMINESCENCE:7||LASER:7||GENERATION:6||NANORODS:6||GROWTH:6||NANOWIRES:5||IMPLANTED 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SEMICONDUCTORS:2||MOLECULARBEAM EPITAXY:2||EARTHDOPED GAN:2||LASER FIELDS:2||CHIRPEDPULSEAMPLIFICATION:2||ALN:2||GAUSSIANBEAM:2||ASSISTED CATALYTIC GROWTH:2||BLUE:2||NANOSTRUCTURES:2||MAGNETOELECTRONICS:2||MICROSCOPY:2||ELECTROLUMINESCENCE:2||LASERPULSES:2||GaN nanowires:2||GALLIUM NITRIDE NANOWIRES:2||GAMNN:2||NANOTUBES:2||PHYSICS:2||Femtosecond laser:2||parametric oscillators and amplifiers:1||ultrafast lasers:1||VALENCE:1||nanowires:1||DILUTED MAGNETIC SEMICONDUCTOR:1||LUMINESCENCE:1||Density modulation:1||Energy modulation:1||Current enhanced SASE free electron laser:1||Undulator radiation:1||FREEELECTRON LASERS:1||ULTRATHIN FERROMAGNETICFILMS:1||OXIDEFILMS:1||ABLATION:1||COMPONENT:1||METAL:1||innershell excited states:1||Nelike ions:1||TRANSITIONS:1||XUV spectrometer:1||DIAGNOSTICS:1||Xray scattering:1||MO/SI:1||pulsed laser deposition:1||KEV IMPACT ENERGIES:1||vacuum electron acceleration:1||HIGHINTENSITY LASER:1||JUNCTIONS:1||LOWTEMPERATURE GROWTH:1||nanocrystalline materials:1||MOLECULAR PHOTOIONIZATION:1||LOCALIZATION:1||DEUTERIUM CLUSTERS:1||EXPLOSIONS:1||REGENERATIVE AMPLIFIERS:1||RAREGASES:1||THz radiation:1||FREEELECTRON LASER:1||REALTIME OBSERVATION:1||TARGET:1||photoionized plasmas:1||fs Xray laser:1||emission profile:1||HIGHORDER HARMONICS:1||Xray laser:1||atomic transition:1||EXCITATION:1||LASERS:1||PERFORMANCE:1||RELATIVISTIC ELECTRONS:1||BI2O3DOPED ZNO:1||INNERSHELL IONIZATION:1||Laser wakefield:1||FREQUENCY:1||SOLIDSTATE LASERS:1||Linearly polarized:1||THERMIONIC EMISSION:1||PULSE AMPLIFICATION SYSTEM:1||BIB3O6:1||NM:1||NONCOVALENT INTERACTIONS:1||CRYSTALLINE:1||INTENSITY:1||JETS:1||COHERENT:1||LINE:1||ANGULARDISTRIBUTION:1||SILVER IONS:1||magnetic anisotropy:1||DEVICES:1||Auger transitions:1||CosterKronig transitions:1||EFFICIENT:1||ELECTRONIMPACT IONIZATION:1||ULTRASHORTPULSE:1||Nanowire:1||Heterostructure:1||soft Xray reflectivity:1||PLASMA ACCELERATOR:1||ZINCOXIDE NANOWIRES:1||CHEMICALVAPORDEPOSITION:1||Electron acceleration:1||Ionization of gases:1||Delay dependent:1||MULTIPHOTON IONIZATION:1||FRAGMENTATION:1||GASJET:1||ultrafast nonlinear optics:1||CYCLE PULSES:1||KHZ:1||chemical vapor deposition:1||ferromagnetism:1||ABSORPTION:1||TERAHERTZ RADIATION:1||SCIENCE:1||FIELDS:1||ELECTRONS:1||nanomultilayer structures:1||YIELDS:1||AUGER:1||10HZ REPETITION RATE:1||MULTITERAWATT:1||SPECTROGRAPH:1||HIGHHARMONICGENERATION:1||spectroscopy:1||level population:1||PARTICLEACCELERATION:1||OPTICAL FREQUENCYMEASUREMENT:1||NANOWALLS:1||ROOMTEMPERATURE:1||AVERAGE OUTPUT POWER:1||GROUPVELOCITYMISMATCH:1||Impact ionization:1||Dynamics:1||Lasers:1||Collisional process:1||ABOVETHRESHOLD IONIZATION:1||MAINGROUP THERMOCHEMISTRY:1||dilute magnetic semiconductors:1||GACRN:1||SIZE:1||ATTOSECOND:1||Ar cluster:1||Xray astrophysics:1||photoionization:1||irons:1||normal incidence pulsed laser deposition:1||SHELLS:1||Silicon Oxide:1||gaspuff Zpinch:1||Xray:1||soft Xray reflectors:1||ESCAPE:1||ZN2SIO4:1||SILICA:1||Time 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materials:1||MOLECULAR PHOTOIONIZATION:1||LOCALIZATION:1||DEUTERIUM CLUSTERS:1||EXPLOSIONS:1||REGENERATIVE AMPLIFIERS:1||RAREGASES:1||THz radiation:1||FREEELECTRON LASER:1||REALTIME OBSERVATION:1||TARGET:1||photoionized plasmas:1||fs Xray laser:1||emission profile:1||HIGHORDER HARMONICS:1||Xray laser:1||atomic transition:1||EXCITATION:1||LASERS:1||PERFORMANCE:1||RELATIVISTIC ELECTRONS:1||BI2O3DOPED ZNO:1||INNERSHELL IONIZATION:1||Laser wakefield:1||FREQUENCY:1||SOLIDSTATE LASERS:1||Linearly polarized:1||THERMIONIC EMISSION:1||PULSE AMPLIFICATION SYSTEM:1||BIB3O6:1||NM:1||NONCOVALENT INTERACTIONS:1||CRYSTALLINE:1||INTENSITY:1||JETS:1||COHERENT:1||LINE:1||ANGULARDISTRIBUTION:1||SILVER IONS:1||magnetic anisotropy:1||DEVICES:1||Auger transitions:1||CosterKronig transitions:1||EFFICIENT:1||ELECTRONIMPACT IONIZATION:1||ULTRASHORTPULSE:1||Nanowire:1||Heterostructure:1||soft Xray reflectivity:1||PLASMA ACCELERATOR:1||ZINCOXIDE NANOWIRES:1||CHEMICALVAPORDEPOSITION:1||Electron acceleration:1||Ionization of gases:1||Delay dependent:1||MULTIPHOTON IONIZATION:1||FRAGMENTATION:1||GASJET:1||ultrafast nonlinear optics:1||CYCLE PULSES:1||KHZ:1||chemical vapor deposition:1||ferromagnetism:1||ABSORPTION:1||TERAHERTZ RADIATION:1||SCIENCE:1||FIELDS:1||ELECTRONS:1||nanomultilayer structures:1||YIELDS:1||AUGER:1||10HZ REPETITION RATE:1||MULTITERAWATT:1||SPECTROGRAPH:1||HIGHHARMONICGENERATION:1||spectroscopy:1||level population:1||PARTICLEACCELERATION:1||OPTICAL FREQUENCYMEASUREMENT:1||NANOWALLS:1||ROOMTEMPERATURE:1||AVERAGE OUTPUT POWER:1||GROUPVELOCITYMISMATCH:1||Impact ionization:1||Dynamics:1||Lasers:1||Collisional process:1||ABOVETHRESHOLD IONIZATION:1||MAINGROUP THERMOCHEMISTRY:1||dilute magnetic semiconductors:1||GACRN:1||SIZE:1||ATTOSECOND:1||Ar cluster:1||Xray astrophysics:1||photoionization:1||irons:1||normal incidence pulsed laser deposition:1||SHELLS:1||Silicon Oxide:1||gaspuff Zpinch:1||Xray:1||soft Xray reflectors:1||ESCAPE:1||ZN2SIO4:1||SILICA:1||Time delay:1||Collisional plasmas:1||MASSSPECTROMETRY:1||NUCLEARFUSION:1||PARAMETRIC AMPLIFICATION:1||LYING ELECTRONIC STATES:1||ADJUSTABLEPARAMETERS:1||MAGNETICPROPERTIES:1||LIQUIDPHASE EPITAXY:1||CEP laser:1||REGION:1||Plasma waveguide:1||AMBIENT GAS:1||DEPOSITION:1||HARMONICGENERATION:1||ENHANCEMENT:1||imaging spectrometer:1||Abel inversion:1||Water window:1||Liquid nitrogen jet:1||CHARGEEXCHANGE:1||NOBEL LECTURE:1||VARISTOR:1||EPITAXY:1||THINDISK LASER:1||HIGHREPETITIONRATE:1||Atom lasers:1||Electronimpact excitation:1||High order harmonics:1||ultrafast technology:1||PEAK POWER:1||CHARGED ALUMINUM CLUSTERS:1||GaN:1||THIN:1||Electron beam:1||INTENSE:1||Hard Xray pulse generation:1||NONLINEAR THOMSON SCATTERING:1||MULTILAYER:1||UVvisible spectrometer:1||ATOMS:1||innershell transitions:1||CORRECTED CONCAVE GRATINGS:1||DISCHARGE:1||LASERPLASMA:1||thin film:1||reflectivity:1||opacity:1||gain:1||smallangle Xray scattering:1||SOFTXRAY:1||ZINCOXIDE:1||CYGNUSX3:1||Betatron oscillation:1||ACCELERATOR:1||STRAINEDLAYER SUPERLATTICES:1||OPTICAL PARAMETRIC AMPLIFICATION:1||PASSIVE MODELOCKING:1||Collision dynamics:1||MUM:1||EXACTEXCHANGE:1||BASISSET:1||APPROXIMATION:1||OXYNITRIDES:1||Beam energy modulation:1||polarization spectroscopy:1||REORIENTATION TRANSITION:1||DEPENDENCE:1||sulfurs:1||BUILDINGBLOCKS:1||RATES:1||OPTICAL PULSES:1||toroidal mirror:1||XRAY LASER:1||CALCIUM:1||radially polarized laser:1||GRAINBOUNDARIES:1||VAPORDEPOSITION:1||Xray generation:1||MAGNETIZATION:1||Electric excitation:1||Laserinduced gas plasmas:1||Qualitative analysis:1||SCHEME:1||RADIATION:10||PULSES:8||PHOTOLUMINESCENCE:7||LASER:7||GENERATION:6||NANORODS:6||GROWTH:6||NANOWIRES:5||IMPLANTED GAN:5||SPECTROSCOPY:5||THINFILMS:4||DYNAMICS:4||SILICON:4||EXTREMEULTRAVIOLET:4||AMPLIFICATION:4||PRESSURE:4||PHASE:4||OPTICALPROPERTIES:4||SYSTEM:4||EMISSION:4||FEL:3||N2O:3||FILMS:3||OPTICS:3||SPECTRA:3||FIELD:3||MIRRORS:3||ARRAYS:3||CLUSTERS:3||SIO2:3||IONIZATION:3||VACUUM:3||SCATTERING:3||IONS:2||LUMINESCENCE PROPERTIES:2||ANISOTROPY:2||BEAMS:2||DIFFRACTION:2||DISPERSION:2||chemical vapor deposition (CVD):2||ELECTRONICSTRUCTURE:2||MOSFETS:2||SI3N4:2||DENSITY:2||LIGHT:2||PLASMAS:2||MATTER:2||nanocomposites:2||RAMANSCATTERING:2||NANOPARTICLES:2||OXIDE:2||AMPLIFIED SPONTANEOUS EMISSION:2||NM WAVELENGTH:2||GAIN:2||CARBON NANOTUBES:2||CROSSSECTIONS:2||LIGHTEMITTINGDIODES:2||PULSE:2||CARBON PLASMA:2||TISAPPHIRE LASER:2||Raman scattering:2||ROUTE:2||multilayer:2||CATHODOLUMINESCENCE:2||highresolution transmission electronic microscope (HRTEM):2||DIFFERENCEFREQUENCYGENERATION:2||CRYSTAL:2||laserproduced plasma:2||NANOCABLES:2||photoluminescence:2||MAGNETIC ALLOY SEMICONDUCTORS:2||MOLECULARBEAM EPITAXY:2||EARTHDOPED GAN:2||LASER FIELDS:2||CHIRPEDPULSEAMPLIFICATION:2||ALN:2||GAUSSIANBEAM:2||ASSISTED CATALYTIC GROWTH:2||BLUE:2||NANOSTRUCTURES:2||MAGNETOELECTRONICS:2||MICROSCOPY:2||ELECTROLUMINESCENCE:2||LASERPULSES:2||GaN nanowires:2||GALLIUM NITRIDE NANOWIRES:2||GAMNN:2||NANOTUBES:2||PHYSICS:2||Femtosecond laser:2||parametric oscillators and amplifiers:1||ultrafast lasers:1||VALENCE:1||nanowires:1||DILUTED MAGNETIC SEMICONDUCTOR:1||LUMINESCENCE:1||Density modulation:1||Energy modulation:1||Current enhanced SASE free electron laser:1||Undulator radiation:1||FREEELECTRON LASERS:1||ULTRATHIN FERROMAGNETICFILMS:1||OXIDEFILMS:1||ABLATION:1||COMPONENT:1||METAL:1||innershell excited states:1||Nelike ions:1||TRANSITIONS:1||XUV spectrometer:1||DIAGNOSTICS:1||Xray scattering:1||MO/SI:1||pulsed laser deposition:1||KEV IMPACT ENERGIES:1||vacuum electron acceleration:1||HIGHINTENSITY LASER:1||JUNCTIONS:1||LOWTEMPERATURE GROWTH:1||nanocrystalline materials:1||MOLECULAR PHOTOIONIZATION:1||LOCALIZATION:1||DEUTERIUM CLUSTERS:1||EXPLOSIONS:1||REGENERATIVE AMPLIFIERS:1||RAREGASES:1||THz radiation:1||FREEELECTRON LASER:1||REALTIME OBSERVATION:1||TARGET:1||photoionized plasmas:1||fs Xray laser:1||emission profile:1||HIGHORDER HARMONICS:1||Xray laser:1||atomic transition:1||EXCITATION:1||LASERS:1||PERFORMANCE:1||RELATIVISTIC ELECTRONS:1||BI2O3DOPED ZNO:1||INNERSHELL IONIZATION:1||Laser wakefield:1||FREQUENCY:1||SOLIDSTATE LASERS:1||Linearly polarized:1||THERMIONIC EMISSION:1||PULSE AMPLIFICATION SYSTEM:1||BIB3O6:1||NM:1||NONCOVALENT INTERACTIONS:1||CRYSTALLINE:1||INTENSITY:1||JETS:1||COHERENT:1||LINE:1||ANGULARDISTRIBUTION:1||SILVER IONS:1||magnetic anisotropy:1||DEVICES:1||Auger transitions:1||CosterKronig transitions:1||EFFICIENT:1||ELECTRONIMPACT IONIZATION:1||ULTRASHORTPULSE:1||Nanowire:1||Heterostructure:1||soft Xray reflectivity:1||PLASMA ACCELERATOR:1||ZINCOXIDE NANOWIRES:1||CHEMICALVAPORDEPOSITION:1||Electron acceleration:1||Ionization of gases:1||Delay dependent:1||MULTIPHOTON IONIZATION:1||FRAGMENTATION:1||GASJET:1||ultrafast nonlinear optics:1||CYCLE PULSES:1||KHZ:1||chemical vapor deposition:1||ferromagnetism:1||ABSORPTION:1||TERAHERTZ RADIATION:1||SCIENCE:1||FIELDS:1||ELECTRONS:1||nanomultilayer structures:1||YIELDS:1||AUGER:1||10HZ REPETITION RATE:1||MULTITERAWATT:1||SPECTROGRAPH:1||HIGHHARMONICGENERATION:1||spectroscopy:1||level population:1||PARTICLEACCELERATION:1||OPTICAL FREQUENCYMEASUREMENT:1||NANOWALLS:1||ROOMTEMPERATURE:1||AVERAGE OUTPUT POWER:1||GROUPVELOCITYMISMATCH:1||Impact ionization:1||Dynamics:1||Lasers:1||Collisional process:1||ABOVETHRESHOLD IONIZATION:1||MAINGROUP THERMOCHEMISTRY:1||dilute magnetic semiconductors:1||GACRN:1||SIZE:1||ATTOSECOND:1||Ar cluster:1||Xray astrophysics:1||photoionization:1||irons:1||normal incidence pulsed laser deposition:1||SHELLS:1||Silicon Oxide:1||gaspuff Zpinch:1||Xray:1||soft Xray reflectors:1||ESCAPE:1||ZN2SIO4:1||SILICA:1||Time delay:1||Collisional plasmas:1||MASSSPECTROMETRY:1||NUCLEARFUSION:1||PARAMETRIC AMPLIFICATION:1||LYING ELECTRONIC STATES:1||ADJUSTABLEPARAMETERS:1||MAGNETICPROPERTIES:1||LIQUIDPHASE EPITAXY:1||CEP laser:1||REGION:1||Plasma waveguide:1||AMBIENT GAS:1||DEPOSITION:1||HARMONICGENERATION:1||ENHANCEMENT:1||imaging spectrometer:1||Abel inversion:1||Water window:1||Liquid nitrogen jet:1||CHARGEEXCHANGE:1||NOBEL LECTURE:1||VARISTOR:1||EPITAXY:1||THINDISK LASER:1||HIGHREPETITIONRATE:1||Atom lasers:1||Electronimpact excitation:1||High order harmonics:1||ultrafast technology:1||PEAK POWER:1||CHARGED ALUMINUM CLUSTERS:1||GaN:1||THIN:1||Electron beam:1||INTENSE:1||Hard Xray pulse generation:1||NONLINEAR THOMSON SCATTERING:1||MULTILAYER:1||UVvisible spectrometer:1||ATOMS:1||innershell transitions:1||CORRECTED CONCAVE GRATINGS:1||DISCHARGE:1||LASERPLASMA:1||thin film:1||reflectivity:1||opacity:1||gain:1||smallangle Xray scattering:1||SOFTXRAY:1||ZINCOXIDE:1||CYGNUSX3:1||Betatron oscillation:1||ACCELERATOR:1||STRAINEDLAYER SUPERLATTICES:1||OPTICAL PARAMETRIC AMPLIFICATION:1||PASSIVE MODELOCKING:1||Collision dynamics:1||MUM:1||EXACTEXCHANGE:1||BASISSET:1||APPROXIMATION:1||OXYNITRIDES:1||Beam energy modulation:1||polarization spectroscopy:1||REORIENTATION TRANSITION:1||DEPENDENCE:1||sulfurs:1||BUILDINGBLOCKS:1||RATES:1||OPTICAL PULSES:1||toroidal mirror:1||XRAY LASER:1||CALCIUM:1||radially polarized laser:1||GRAINBOUNDARIES:1||VAPORDEPOSITION:1||Xray generation:1||MAGNETIZATION:1||Electric excitation:1||Laserinduced gas plasmas:1||Qualitative analysis:1||SCHEME:1||RADIATION:10||PULSES:8||PHOTOLUMINESCENCE:7||LASER:7||GENERATION:6||NANORODS:6||GROWTH:6||NANOWIRES:5||IMPLANTED 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SEMICONDUCTORS:2||MOLECULARBEAM EPITAXY:2||EARTHDOPED GAN:2||LASER FIELDS:2||CHIRPEDPULSEAMPLIFICATION:2||ALN:2||GAUSSIANBEAM:2||ASSISTED CATALYTIC GROWTH:2||BLUE:2||NANOSTRUCTURES:2||MAGNETOELECTRONICS:2||MICROSCOPY:2||ELECTROLUMINESCENCE:2||LASERPULSES:2||GaN nanowires:2||GALLIUM NITRIDE NANOWIRES:2||GAMNN:2||NANOTUBES:2||PHYSICS:2||Femtosecond laser:2||parametric oscillators and amplifiers:1||ultrafast lasers:1||VALENCE:1||nanowires:1||DILUTED MAGNETIC SEMICONDUCTOR:1||LUMINESCENCE:1||Density modulation:1||Energy modulation:1||Current enhanced SASE free electron laser:1||Undulator radiation:1||FREEELECTRON LASERS:1||ULTRATHIN FERROMAGNETICFILMS:1||OXIDEFILMS:1||ABLATION:1||COMPONENT:1||METAL:1||innershell excited states:1||Nelike ions:1||TRANSITIONS:1||XUV spectrometer:1||DIAGNOSTICS:1||Xray scattering:1||MO/SI:1||pulsed laser deposition:1||KEV IMPACT ENERGIES:1||vacuum electron acceleration:1||HIGHINTENSITY LASER:1||JUNCTIONS:1||LOWTEMPERATURE GROWTH:1||nanocrystalline materials:1||MOLECULAR PHOTOIONIZATION:1||LOCALIZATION:1||DEUTERIUM CLUSTERS:1||EXPLOSIONS:1||REGENERATIVE AMPLIFIERS:1||RAREGASES:1||THz radiation:1||FREEELECTRON LASER:1||REALTIME OBSERVATION:1||TARGET:1||photoionized plasmas:1||fs Xray laser:1||emission profile:1||HIGHORDER HARMONICS:1||Xray laser:1||atomic transition:1||EXCITATION:1||LASERS:1||PERFORMANCE:1||RELATIVISTIC ELECTRONS:1||BI2O3DOPED ZNO:1||INNERSHELL IONIZATION:1||Laser wakefield:1||FREQUENCY:1||SOLIDSTATE LASERS:1||Linearly polarized:1||THERMIONIC EMISSION:1||PULSE AMPLIFICATION SYSTEM:1||BIB3O6:1||NM:1||NONCOVALENT INTERACTIONS:1||CRYSTALLINE:1||INTENSITY:1||JETS:1||COHERENT:1||LINE:1||ANGULARDISTRIBUTION:1||SILVER IONS:1||magnetic anisotropy:1||DEVICES:1||Auger transitions:1||CosterKronig transitions:1||EFFICIENT:1||ELECTRONIMPACT IONIZATION:1||ULTRASHORTPULSE:1||Nanowire:1||Heterostructure:1||soft Xray reflectivity:1||PLASMA ACCELERATOR:1||ZINCOXIDE NANOWIRES:1||CHEMICALVAPORDEPOSITION:1||Electron acceleration:1||Ionization of gases:1||Delay dependent:1||MULTIPHOTON IONIZATION:1||FRAGMENTATION:1||GASJET:1||ultrafast nonlinear optics:1||CYCLE PULSES:1||KHZ:1||chemical vapor deposition:1||ferromagnetism:1||ABSORPTION:1||TERAHERTZ RADIATION:1||SCIENCE:1||FIELDS:1||ELECTRONS:1||nanomultilayer structures:1||YIELDS:1||AUGER:1||10HZ REPETITION RATE:1||MULTITERAWATT:1||SPECTROGRAPH:1||HIGHHARMONICGENERATION:1||spectroscopy:1||level population:1||PARTICLEACCELERATION:1||OPTICAL FREQUENCYMEASUREMENT:1||NANOWALLS:1||ROOMTEMPERATURE:1||AVERAGE OUTPUT POWER:1||GROUPVELOCITYMISMATCH:1||Impact ionization:1||Dynamics:1||Lasers:1||Collisional process:1||ABOVETHRESHOLD IONIZATION:1||MAINGROUP THERMOCHEMISTRY:1||dilute magnetic semiconductors:1||GACRN:1||SIZE:1||ATTOSECOND:1||Ar cluster:1||Xray astrophysics:1||photoionization:1||irons:1||normal incidence pulsed laser deposition:1||SHELLS:1||Silicon Oxide:1||gaspuff Zpinch:1||Xray:1||soft Xray reflectors:1||ESCAPE:1||ZN2SIO4:1||SILICA:1||Time 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materials:1||MOLECULAR PHOTOIONIZATION:1||LOCALIZATION:1||DEUTERIUM CLUSTERS:1||EXPLOSIONS:1||REGENERATIVE AMPLIFIERS:1||RAREGASES:1||THz radiation:1||FREEELECTRON LASER:1||REALTIME OBSERVATION:1||TARGET:1||photoionized plasmas:1||fs Xray laser:1||emission profile:1||HIGHORDER HARMONICS:1||Xray laser:1||atomic transition:1||EXCITATION:1||LASERS:1||PERFORMANCE:1||RELATIVISTIC ELECTRONS:1||BI2O3DOPED ZNO:1||INNERSHELL IONIZATION:1||Laser wakefield:1||FREQUENCY:1||SOLIDSTATE LASERS:1||Linearly polarized:1||THERMIONIC EMISSION:1||PULSE AMPLIFICATION SYSTEM:1||BIB3O6:1||NM:1||NONCOVALENT INTERACTIONS:1||CRYSTALLINE:1||INTENSITY:1||JETS:1||COHERENT:1||LINE:1||ANGULARDISTRIBUTION:1||SILVER IONS:1||magnetic anisotropy:1||DEVICES:1||Auger transitions:1||CosterKronig transitions:1||EFFICIENT:1||ELECTRONIMPACT IONIZATION:1||ULTRASHORTPULSE:1||Nanowire:1||Heterostructure:1||soft Xray reflectivity:1||PLASMA ACCELERATOR:1||ZINCOXIDE NANOWIRES:1||CHEMICALVAPORDEPOSITION:1||Electron acceleration:1||Ionization of gases:1||Delay dependent:1||MULTIPHOTON IONIZATION:1||FRAGMENTATION:1||GASJET:1||ultrafast nonlinear optics:1||CYCLE PULSES:1||KHZ:1||chemical vapor deposition:1||ferromagnetism:1||ABSORPTION:1||TERAHERTZ RADIATION:1||SCIENCE:1||FIELDS:1||ELECTRONS:1||nanomultilayer structures:1||YIELDS:1||AUGER:1||10HZ REPETITION RATE:1||MULTITERAWATT:1||SPECTROGRAPH:1||HIGHHARMONICGENERATION:1||spectroscopy:1||level population:1||PARTICLEACCELERATION:1||OPTICAL FREQUENCYMEASUREMENT:1||NANOWALLS:1||ROOMTEMPERATURE:1||AVERAGE OUTPUT POWER:1||GROUPVELOCITYMISMATCH:1||Impact ionization:1||Dynamics:1||Lasers:1||Collisional process:1||ABOVETHRESHOLD IONIZATION:1||MAINGROUP THERMOCHEMISTRY:1||dilute magnetic semiconductors:1||GACRN:1||SIZE:1||ATTOSECOND:1||Ar cluster:1||Xray astrophysics:1||photoionization:1||irons:1||normal incidence pulsed laser deposition:1||SHELLS:1||Silicon Oxide:1||gaspuff Zpinch:1||Xray:1||soft Xray reflectors:1||ESCAPE:1||ZN2SIO4:1||SILICA:1||Time delay:1||Collisional plasmas:1||MASSSPECTROMETRY:1||NUCLEARFUSION:1||PARAMETRIC AMPLIFICATION:1||LYING ELECTRONIC STATES:1||ADJUSTABLEPARAMETERS:1||MAGNETICPROPERTIES:1||LIQUIDPHASE EPITAXY:1||CEP laser:1||REGION:1||Plasma waveguide:1||AMBIENT GAS:1||DEPOSITION:1||HARMONICGENERATION:1||ENHANCEMENT:1||imaging spectrometer:1||Abel inversion:1||Water window:1||Liquid nitrogen jet:1||CHARGEEXCHANGE:1||NOBEL LECTURE:1||VARISTOR:1||EPITAXY:1||THINDISK LASER:1||HIGHREPETITIONRATE:1||Atom lasers:1||Electronimpact excitation:1||High order harmonics:1||ultrafast technology:1||PEAK POWER:1||CHARGED ALUMINUM CLUSTERS:1||GaN:1||THIN:1||Electron beam:1||INTENSE:1||Hard Xray pulse generation:1||NONLINEAR THOMSON SCATTERING:1||MULTILAYER:1||UVvisible spectrometer:1||ATOMS:1||innershell transitions:1||CORRECTED CONCAVE GRATINGS:1||DISCHARGE:1||LASERPLASMA:1||thin film:1||reflectivity:1||opacity:1||gain:1||smallangle Xray scattering:1||SOFTXRAY:1||ZINCOXIDE:1||CYGNUSX3:1||Betatron oscillation:1||ACCELERATOR:1||STRAINEDLAYER SUPERLATTICES:1||OPTICAL PARAMETRIC AMPLIFICATION:1||PASSIVE MODELOCKING:1||Collision dynamics:1||MUM:1||EXACTEXCHANGE:1||BASISSET:1||APPROXIMATION:1||OXYNITRIDES:1||Beam energy modulation:1||polarization spectroscopy:1||REORIENTATION TRANSITION:1||DEPENDENCE:1||sulfurs:1||BUILDINGBLOCKS:1||RATES:1||OPTICAL PULSES:1||toroidal mirror:1||XRAY LASER:1||CALCIUM:1||radially polarized laser:1||GRAINBOUNDARIES:1||VAPORDEPOSITION:1||Xray generation:1||MAGNETIZATION:1||Electric excitation:1||Laserinduced gas plasmas:1||Qualitative analysis:1||SCHEME:1||RADIATION:10||PULSES:8||PHOTOLUMINESCENCE:7||LASER:7||GENERATION:6||NANORODS:6||GROWTH:6||NANOWIRES:5||IMPLANTED GAN:5||SPECTROSCOPY:5||THINFILMS:4||DYNAMICS:4||SILICON:4||EXTREMEULTRAVIOLET:4||AMPLIFICATION:4||PRESSURE:4||PHASE:4||OPTICALPROPERTIES:4||SYSTEM:4||EMISSION:4||FEL:3||N2O:3||FILMS:3||OPTICS:3||SPECTRA:3||FIELD:3||MIRRORS:3||ARRAYS:3||CLUSTERS:3||SIO2:3||IONIZATION:3||VACUUM:3||SCATTERING:3||IONS:2||LUMINESCENCE PROPERTIES:2||ANISOTROPY:2||BEAMS:2||DIFFRACTION:2||DISPERSION:2||chemical vapor deposition (CVD):2||ELECTRONICSTRUCTURE:2||MOSFETS:2||SI3N4:2||DENSITY:2||LIGHT:2||PLASMAS:2||MATTER:2||nanocomposites:2||RAMANSCATTERING:2||NANOPARTICLES:2||OXIDE:2||AMPLIFIED SPONTANEOUS EMISSION:2||NM WAVELENGTH:2||GAIN:2||CARBON NANOTUBES:2||CROSSSECTIONS:2||LIGHTEMITTINGDIODES:2||PULSE:2||CARBON PLASMA:2||TISAPPHIRE LASER:2||Raman scattering:2||ROUTE:2||multilayer:2||CATHODOLUMINESCENCE:2||highresolution transmission electronic microscope (HRTEM):2||DIFFERENCEFREQUENCYGENERATION:2||CRYSTAL:2||laserproduced plasma:2||NANOCABLES:2||photoluminescence:2||MAGNETIC ALLOY SEMICONDUCTORS:2||MOLECULARBEAM EPITAXY:2||EARTHDOPED GAN:2||LASER FIELDS:2||CHIRPEDPULSEAMPLIFICATION:2||ALN:2||GAUSSIANBEAM:2||ASSISTED CATALYTIC GROWTH:2||BLUE:2||NANOSTRUCTURES:2||MAGNETOELECTRONICS:2||MICROSCOPY:2||ELECTROLUMINESCENCE:2||LASERPULSES:2||GaN nanowires:2||GALLIUM NITRIDE NANOWIRES:2||GAMNN:2||NANOTUBES:2||PHYSICS:2||Femtosecond laser:2||parametric oscillators and amplifiers:1||ultrafast lasers:1||VALENCE:1||nanowires:1||DILUTED MAGNETIC SEMICONDUCTOR:1||LUMINESCENCE:1||Density modulation:1||Energy modulation:1||Current enhanced SASE free electron laser:1||Undulator radiation:1||FREEELECTRON LASERS:1||ULTRATHIN FERROMAGNETICFILMS:1||OXIDEFILMS:1||ABLATION:1||COMPONENT:1||METAL:1||innershell excited states:1||Nelike ions:1||TRANSITIONS:1||XUV spectrometer:1||DIAGNOSTICS:1||Xray scattering:1||MO/SI:1||pulsed laser deposition:1||KEV IMPACT ENERGIES:1||vacuum electron acceleration:1||HIGHINTENSITY LASER:1||JUNCTIONS:1||LOWTEMPERATURE GROWTH:1||nanocrystalline materials:1||MOLECULAR PHOTOIONIZATION:1||LOCALIZATION:1||DEUTERIUM CLUSTERS:1||EXPLOSIONS:1||REGENERATIVE AMPLIFIERS:1||RAREGASES:1||THz radiation:1||FREEELECTRON LASER:1||REALTIME OBSERVATION:1||TARGET:1||photoionized plasmas:1||fs Xray laser:1||emission profile:1||HIGHORDER HARMONICS:1||Xray laser:1||atomic transition:1||EXCITATION:1||LASERS:1||PERFORMANCE:1||RELATIVISTIC ELECTRONS:1||BI2O3DOPED ZNO:1||INNERSHELL IONIZATION:1||Laser wakefield:1||FREQUENCY:1||SOLIDSTATE LASERS:1||Linearly polarized:1||THERMIONIC EMISSION:1||PULSE AMPLIFICATION SYSTEM:1||BIB3O6:1||NM:1||NONCOVALENT INTERACTIONS:1||CRYSTALLINE:1||INTENSITY:1||JETS:1||COHERENT:1||LINE:1||ANGULARDISTRIBUTION:1||SILVER IONS:1||magnetic anisotropy:1||DEVICES:1||Auger transitions:1||CosterKronig transitions:1||EFFICIENT:1||ELECTRONIMPACT IONIZATION:1||ULTRASHORTPULSE:1||Nanowire:1||Heterostructure:1||soft Xray reflectivity:1||PLASMA ACCELERATOR:1||ZINCOXIDE NANOWIRES:1||CHEMICALVAPORDEPOSITION:1||Electron acceleration:1||Ionization of gases:1||Delay dependent:1||MULTIPHOTON IONIZATION:1||FRAGMENTATION:1||GASJET:1||ultrafast nonlinear optics:1||CYCLE PULSES:1||KHZ:1||chemical vapor deposition:1||ferromagnetism:1||ABSORPTION:1||TERAHERTZ RADIATION:1||SCIENCE:1||FIELDS:1||ELECTRONS:1||nanomultilayer structures:1||YIELDS:1||AUGER:1||10HZ REPETITION RATE:1||MULTITERAWATT:1||SPECTROGRAPH:1||HIGHHARMONICGENERATION:1||spectroscopy:1||level population:1||PARTICLEACCELERATION:1||OPTICAL FREQUENCYMEASUREMENT:1||NANOWALLS:1||ROOMTEMPERATURE:1||AVERAGE OUTPUT POWER:1||GROUPVELOCITYMISMATCH:1||Impact ionization:1||Dynamics:1||Lasers:1||Collisional process:1||ABOVETHRESHOLD IONIZATION:1||MAINGROUP THERMOCHEMISTRY:1||dilute magnetic semiconductors:1||GACRN:1||SIZE:1||ATTOSECOND:1||Ar cluster:1||Xray astrophysics:1||photoionization:1||irons:1||normal incidence pulsed laser deposition:1||SHELLS:1||Silicon Oxide:1||gaspuff Zpinch:1||Xray:1||soft Xray reflectors:1||ESCAPE:1||ZN2SIO4:1||SILICA:1||Time delay:1||Collisional plasmas:1||MASSSPECTROMETRY:1||NUCLEARFUSION:1||PARAMETRIC AMPLIFICATION:1||LYING ELECTRONIC STATES:1||ADJUSTABLEPARAMETERS:1||MAGNETICPROPERTIES:1||LIQUIDPHASE EPITAXY:1||CEP laser:1||REGION:1||Plasma waveguide:1||AMBIENT GAS:1||DEPOSITION:1||HARMONICGENERATION:1||ENHANCEMENT:1||imaging spectrometer:1||Abel inversion:1||Water window:1||Liquid nitrogen jet:1||CHARGEEXCHANGE:1||NOBEL LECTURE:1||VARISTOR:1||EPITAXY:1||THINDISK LASER:1||HIGHREPETITIONRATE:1||Atom lasers:1||Electronimpact excitation:1||High order harmonics:1||ultrafast technology:1||PEAK POWER:1||CHARGED ALUMINUM CLUSTERS:1||GaN:1||THIN:1||Electron beam:1||INTENSE:1||Hard Xray pulse generation:1||NONLINEAR THOMSON SCATTERING:1||MULTILAYER:1||UVvisible spectrometer:1||ATOMS:1||innershell transitions:1||CORRECTED CONCAVE GRATINGS:1||DISCHARGE:1||LASERPLASMA:1||thin film:1||reflectivity:1||opacity:1||gain:1||smallangle Xray scattering:1||SOFTXRAY:1||ZINCOXIDE:1||CYGNUSX3:1||Betatron oscillation:1||ACCELERATOR:1||STRAINEDLAYER SUPERLATTICES:1||OPTICAL PARAMETRIC AMPLIFICATION:1||PASSIVE MODELOCKING:1||Collision dynamics:1||MUM:1||EXACTEXCHANGE:1||BASISSET:1||APPROXIMATION:1||OXYNITRIDES:1||Beam energy modulation:1||polarization spectroscopy:1||REORIENTATION TRANSITION:1||DEPENDENCE:1||sulfurs:1||BUILDINGBLOCKS:1||RATES:1||OPTICAL PULSES:1||toroidal mirror:1||XRAY LASER:1||CALCIUM:1||radially polarized laser:1||GRAINBOUNDARIES:1||VAPORDEPOSITION:1||Xray generation:1||MAGNETIZATION:1||Electric excitation:1||Laserinduced gas plasmas:1||Qualitative analysis:1||SCHEME:1||RADIATION:10||PULSES:8||PHOTOLUMINESCENCE:7||LASER:7||GENERATION:6||NANORODS:6||GROWTH:6||NANOWIRES:5||IMPLANTED 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SEMICONDUCTORS:2||MOLECULARBEAM EPITAXY:2||EARTHDOPED GAN:2||LASER FIELDS:2||CHIRPEDPULSEAMPLIFICATION:2||ALN:2||GAUSSIANBEAM:2||ASSISTED CATALYTIC GROWTH:2||BLUE:2||NANOSTRUCTURES:2||MAGNETOELECTRONICS:2||MICROSCOPY:2||ELECTROLUMINESCENCE:2||LASERPULSES:2||GaN nanowires:2||GALLIUM NITRIDE NANOWIRES:2||GAMNN:2||NANOTUBES:2||PHYSICS:2||Femtosecond laser:2||parametric oscillators and amplifiers:1||ultrafast lasers:1||VALENCE:1||nanowires:1||DILUTED MAGNETIC SEMICONDUCTOR:1||LUMINESCENCE:1||Density modulation:1||Energy modulation:1||Current enhanced SASE free electron laser:1||Undulator radiation:1||FREEELECTRON LASERS:1||ULTRATHIN FERROMAGNETICFILMS:1||OXIDEFILMS:1||ABLATION:1||COMPONENT:1||METAL:1||innershell excited states:1||Nelike ions:1||TRANSITIONS:1||XUV spectrometer:1||DIAGNOSTICS:1||Xray scattering:1||MO/SI:1||pulsed laser deposition:1||KEV IMPACT ENERGIES:1||vacuum electron acceleration:1||HIGHINTENSITY LASER:1||JUNCTIONS:1||LOWTEMPERATURE GROWTH:1||nanocrystalline materials:1||MOLECULAR PHOTOIONIZATION:1||LOCALIZATION:1||DEUTERIUM CLUSTERS:1||EXPLOSIONS:1||REGENERATIVE AMPLIFIERS:1||RAREGASES:1||THz radiation:1||FREEELECTRON LASER:1||REALTIME OBSERVATION:1||TARGET:1||photoionized plasmas:1||fs Xray laser:1||emission profile:1||HIGHORDER HARMONICS:1||Xray laser:1||atomic transition:1||EXCITATION:1||LASERS:1||PERFORMANCE:1||RELATIVISTIC ELECTRONS:1||BI2O3DOPED ZNO:1||INNERSHELL IONIZATION:1||Laser wakefield:1||FREQUENCY:1||SOLIDSTATE LASERS:1||Linearly polarized:1||THERMIONIC EMISSION:1||PULSE AMPLIFICATION SYSTEM:1||BIB3O6:1||NM:1||NONCOVALENT INTERACTIONS:1||CRYSTALLINE:1||INTENSITY:1||JETS:1||COHERENT:1||LINE:1||ANGULARDISTRIBUTION:1||SILVER IONS:1||magnetic anisotropy:1||DEVICES:1||Auger transitions:1||CosterKronig transitions:1||EFFICIENT:1||ELECTRONIMPACT IONIZATION:1||ULTRASHORTPULSE:1||Nanowire:1||Heterostructure:1||soft Xray reflectivity:1||PLASMA ACCELERATOR:1||ZINCOXIDE NANOWIRES:1||CHEMICALVAPORDEPOSITION:1||Electron acceleration:1||Ionization of gases:1||Delay dependent:1||MULTIPHOTON IONIZATION:1||FRAGMENTATION:1||GASJET:1||ultrafast nonlinear optics:1||CYCLE PULSES:1||KHZ:1||chemical vapor deposition:1||ferromagnetism:1||ABSORPTION:1||TERAHERTZ RADIATION:1||SCIENCE:1||FIELDS:1||ELECTRONS:1||nanomultilayer structures:1||YIELDS:1||AUGER:1||10HZ REPETITION RATE:1||MULTITERAWATT:1||SPECTROGRAPH:1||HIGHHARMONICGENERATION:1||spectroscopy:1||level population:1||PARTICLEACCELERATION:1||OPTICAL FREQUENCYMEASUREMENT:1||NANOWALLS:1||ROOMTEMPERATURE:1||AVERAGE OUTPUT POWER:1||GROUPVELOCITYMISMATCH:1||Impact ionization:1||Dynamics:1||Lasers:1||Collisional process:1||ABOVETHRESHOLD IONIZATION:1||MAINGROUP THERMOCHEMISTRY:1||dilute magnetic semiconductors:1||GACRN:1||SIZE:1||ATTOSECOND:1||Ar cluster:1||Xray astrophysics:1||photoionization:1||irons:1||normal incidence pulsed laser deposition:1||SHELLS:1||Silicon Oxide:1||gaspuff Zpinch:1||Xray:1||soft Xray reflectors:1||ESCAPE:1||ZN2SIO4:1||SILICA:1||Time 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materials:1||MOLECULAR PHOTOIONIZATION:1||LOCALIZATION:1||DEUTERIUM CLUSTERS:1||EXPLOSIONS:1||REGENERATIVE AMPLIFIERS:1||RAREGASES:1||THz radiation:1||FREEELECTRON LASER:1||REALTIME OBSERVATION:1||TARGET:1||photoionized plasmas:1||fs Xray laser:1||emission profile:1||HIGHORDER HARMONICS:1||Xray laser:1||atomic transition:1||EXCITATION:1||LASERS:1||PERFORMANCE:1||RELATIVISTIC ELECTRONS:1||BI2O3DOPED ZNO:1||INNERSHELL IONIZATION:1||Laser wakefield:1||FREQUENCY:1||SOLIDSTATE LASERS:1||Linearly polarized:1||THERMIONIC EMISSION:1||PULSE AMPLIFICATION SYSTEM:1||BIB3O6:1||NM:1||NONCOVALENT INTERACTIONS:1||CRYSTALLINE:1||INTENSITY:1||JETS:1||COHERENT:1||LINE:1||ANGULARDISTRIBUTION:1||SILVER IONS:1||magnetic anisotropy:1||DEVICES:1||Auger transitions:1||CosterKronig transitions:1||EFFICIENT:1||ELECTRONIMPACT IONIZATION:1||ULTRASHORTPULSE:1||Nanowire:1||Heterostructure:1||soft Xray reflectivity:1||PLASMA ACCELERATOR:1||ZINCOXIDE NANOWIRES:1||CHEMICALVAPORDEPOSITION:1||Electron acceleration:1||Ionization of gases:1||Delay dependent:1||MULTIPHOTON IONIZATION:1||FRAGMENTATION:1||GASJET:1||ultrafast nonlinear optics:1||CYCLE PULSES:1||KHZ:1||chemical vapor deposition:1||ferromagnetism:1||ABSORPTION:1||TERAHERTZ RADIATION:1||SCIENCE:1||FIELDS:1||ELECTRONS:1||nanomultilayer structures:1||YIELDS:1||AUGER:1||10HZ REPETITION RATE:1||MULTITERAWATT:1||SPECTROGRAPH:1||HIGHHARMONICGENERATION:1||spectroscopy:1||level population:1||PARTICLEACCELERATION:1||OPTICAL FREQUENCYMEASUREMENT:1||NANOWALLS:1||ROOMTEMPERATURE:1||AVERAGE OUTPUT POWER:1||GROUPVELOCITYMISMATCH:1||Impact ionization:1||Dynamics:1||Lasers:1||Collisional process:1||ABOVETHRESHOLD IONIZATION:1||MAINGROUP THERMOCHEMISTRY:1||dilute magnetic semiconductors:1||GACRN:1||SIZE:1||ATTOSECOND:1||Ar cluster:1||Xray astrophysics:1||photoionization:1||irons:1||normal incidence pulsed laser deposition:1||SHELLS:1||Silicon Oxide:1||gaspuff Zpinch:1||Xray:1||soft Xray reflectors:1||ESCAPE:1||ZN2SIO4:1||SILICA:1||Time delay:1||Collisional plasmas:1||MASSSPECTROMETRY:1||NUCLEARFUSION:1||PARAMETRIC AMPLIFICATION:1||LYING ELECTRONIC STATES:1||ADJUSTABLEPARAMETERS:1||MAGNETICPROPERTIES:1||LIQUIDPHASE EPITAXY:1||CEP laser:1||REGION:1||Plasma waveguide:1||AMBIENT GAS:1||DEPOSITION:1||HARMONICGENERATION:1||ENHANCEMENT:1||imaging spectrometer:1||Abel inversion:1||Water window:1||Liquid nitrogen jet:1||CHARGEEXCHANGE:1||NOBEL LECTURE:1||VARISTOR:1||EPITAXY:1||THINDISK LASER:1||HIGHREPETITIONRATE:1||Atom lasers:1||Electronimpact excitation:1||High order harmonics:1||ultrafast technology:1||PEAK POWER:1||CHARGED ALUMINUM CLUSTERS:1||GaN:1||THIN:1||Electron beam:1||INTENSE:1||Hard Xray pulse generation:1||NONLINEAR THOMSON SCATTERING:1||MULTILAYER:1||UVvisible spectrometer:1||ATOMS:1||innershell transitions:1||CORRECTED CONCAVE GRATINGS:1||DISCHARGE:1||LASERPLASMA:1||thin film:1||reflectivity:1||opacity:1||gain:1||smallangle Xray scattering:1||SOFTXRAY:1||ZINCOXIDE:1||CYGNUSX3:1||Betatron oscillation:1||ACCELERATOR:1||STRAINEDLAYER SUPERLATTICES:1||OPTICAL PARAMETRIC AMPLIFICATION:1||PASSIVE MODELOCKING:1||Collision dynamics:1||MUM:1||EXACTEXCHANGE:1||BASISSET:1||APPROXIMATION:1||OXYNITRIDES:1||Beam energy modulation:1||polarization spectroscopy:1||REORIENTATION TRANSITION:1||DEPENDENCE:1||sulfurs:1||BUILDINGBLOCKS:1||RATES:1||OPTICAL PULSES:1||toroidal mirror:1||XRAY LASER:1||CALCIUM:1||radially polarized laser:1||GRAINBOUNDARIES:1||VAPORDEPOSITION:1||Xray generation:1||MAGNETIZATION:1||Electric excitation:1||Laserinduced gas plasmas:1||Qualitative analysis:1||SCHEME:1||RADIATION:10||PULSES:8||PHOTOLUMINESCENCE:7||LASER:7||GENERATION:6||NANORODS:6||GROWTH:6||NANOWIRES:5||IMPLANTED GAN:5||SPECTROSCOPY:5||THINFILMS:4||DYNAMICS:4||SILICON:4||EXTREMEULTRAVIOLET:4||AMPLIFICATION:4||PRESSURE:4||PHASE:4||OPTICALPROPERTIES:4||SYSTEM:4||EMISSION:4||FEL:3||N2O:3||FILMS:3||OPTICS:3||SPECTRA:3||FIELD:3||MIRRORS:3||ARRAYS:3||CLUSTERS:3||SIO2:3||IONIZATION:3||VACUUM:3||SCATTERING:3||IONS:2||LUMINESCENCE PROPERTIES:2||ANISOTROPY:2||BEAMS:2||DIFFRACTION:2||DISPERSION:2||chemical vapor deposition (CVD):2||ELECTRONICSTRUCTURE:2||MOSFETS:2||SI3N4:2||DENSITY:2||LIGHT:2||PLASMAS:2||MATTER:2||nanocomposites:2||RAMANSCATTERING:2||NANOPARTICLES:2||OXIDE:2||AMPLIFIED SPONTANEOUS EMISSION:2||NM WAVELENGTH:2||GAIN:2||CARBON NANOTUBES:2||CROSSSECTIONS:2||LIGHTEMITTINGDIODES:2||PULSE:2||CARBON PLASMA:2||TISAPPHIRE LASER:2||Raman scattering:2||ROUTE:2||multilayer:2||CATHODOLUMINESCENCE:2||highresolution transmission electronic microscope (HRTEM):2||DIFFERENCEFREQUENCYGENERATION:2||CRYSTAL:2||laserproduced plasma:2||NANOCABLES:2||photoluminescence:2||MAGNETIC ALLOY SEMICONDUCTORS:2||MOLECULARBEAM EPITAXY:2||EARTHDOPED GAN:2||LASER FIELDS:2||CHIRPEDPULSEAMPLIFICATION:2||ALN:2||GAUSSIANBEAM:2||ASSISTED CATALYTIC GROWTH:2||BLUE:2||NANOSTRUCTURES:2||MAGNETOELECTRONICS:2||MICROSCOPY:2||ELECTROLUMINESCENCE:2||LASERPULSES:2||GaN nanowires:2||GALLIUM NITRIDE NANOWIRES:2||GAMNN:2||NANOTUBES:2||PHYSICS:2||Femtosecond laser:2||parametric oscillators and amplifiers:1||ultrafast lasers:1||VALENCE:1||nanowires:1||DILUTED MAGNETIC SEMICONDUCTOR:1||LUMINESCENCE:1||Density modulation:1||Energy modulation:1||Current enhanced SASE free electron laser:1||Undulator radiation:1||FREEELECTRON LASERS:1||ULTRATHIN FERROMAGNETICFILMS:1||OXIDEFILMS:1||ABLATION:1||COMPONENT:1||METAL:1||innershell excited states:1||Nelike ions:1||TRANSITIONS:1||XUV spectrometer:1||DIAGNOSTICS:1||Xray scattering:1||MO/SI:1||pulsed laser deposition:1||KEV IMPACT ENERGIES:1||vacuum electron acceleration:1||HIGHINTENSITY LASER:1||JUNCTIONS:1||LOWTEMPERATURE GROWTH:1||nanocrystalline materials:1||MOLECULAR PHOTOIONIZATION:1||LOCALIZATION:1||DEUTERIUM CLUSTERS:1||EXPLOSIONS:1||REGENERATIVE AMPLIFIERS:1||RAREGASES:1||THz radiation:1||FREEELECTRON LASER:1||REALTIME OBSERVATION:1||TARGET:1||photoionized plasmas:1||fs Xray laser:1||emission profile:1||HIGHORDER HARMONICS:1||Xray laser:1||atomic transition:1||EXCITATION:1||LASERS:1||PERFORMANCE:1||RELATIVISTIC ELECTRONS:1||BI2O3DOPED ZNO:1||INNERSHELL IONIZATION:1||Laser wakefield:1||FREQUENCY:1||SOLIDSTATE LASERS:1||Linearly polarized:1||THERMIONIC EMISSION:1||PULSE AMPLIFICATION SYSTEM:1||BIB3O6:1||NM:1||NONCOVALENT INTERACTIONS:1||CRYSTALLINE:1||INTENSITY:1||JETS:1||COHERENT:1||LINE:1||ANGULARDISTRIBUTION:1||SILVER IONS:1||magnetic anisotropy:1||DEVICES:1||Auger transitions:1||CosterKronig transitions:1||EFFICIENT:1||ELECTRONIMPACT IONIZATION:1||ULTRASHORTPULSE:1||Nanowire:1||Heterostructure:1||soft Xray reflectivity:1||PLASMA ACCELERATOR:1||ZINCOXIDE NANOWIRES:1||CHEMICALVAPORDEPOSITION:1||Electron acceleration:1||Ionization of gases:1||Delay dependent:1||MULTIPHOTON IONIZATION:1||FRAGMENTATION:1||GASJET:1||ultrafast nonlinear optics:1||CYCLE PULSES:1||KHZ:1||chemical vapor deposition:1||ferromagnetism:1||ABSORPTION:1||TERAHERTZ RADIATION:1||SCIENCE:1||FIELDS:1||ELECTRONS:1||nanomultilayer structures:1||YIELDS:1||AUGER:1||10HZ REPETITION RATE:1||MULTITERAWATT:1||SPECTROGRAPH:1||HIGHHARMONICGENERATION:1||spectroscopy:1||level population:1||PARTICLEACCELERATION:1||OPTICAL FREQUENCYMEASUREMENT:1||NANOWALLS:1||ROOMTEMPERATURE:1||AVERAGE OUTPUT POWER:1||GROUPVELOCITYMISMATCH:1||Impact ionization:1||Dynamics:1||Lasers:1||Collisional process:1||ABOVETHRESHOLD IONIZATION:1||MAINGROUP THERMOCHEMISTRY:1||dilute magnetic semiconductors:1||GACRN:1||SIZE:1||ATTOSECOND:1||Ar cluster:1||Xray astrophysics:1||photoionization:1||irons:1||normal incidence pulsed laser deposition:1||SHELLS:1||Silicon Oxide:1||gaspuff Zpinch:1||Xray:1||soft Xray reflectors:1||ESCAPE:1||ZN2SIO4:1||SILICA:1||Time delay:1||Collisional plasmas:1||MASSSPECTROMETRY:1||NUCLEARFUSION:1||PARAMETRIC AMPLIFICATION:1||LYING ELECTRONIC STATES:1||ADJUSTABLEPARAMETERS:1||MAGNETICPROPERTIES:1||LIQUIDPHASE EPITAXY:1||CEP laser:1||REGION:1||Plasma waveguide:1||AMBIENT GAS:1||DEPOSITION:1||HARMONICGENERATION:1||ENHANCEMENT:1||imaging spectrometer:1||Abel inversion:1||Water window:1||Liquid nitrogen jet:1||CHARGEEXCHANGE:1||NOBEL LECTURE:1||VARISTOR:1||EPITAXY:1||THINDISK LASER:1||HIGHREPETITIONRATE:1||Atom lasers:1||Electronimpact excitation:1||High order harmonics:1||ultrafast technology:1||PEAK POWER:1||CHARGED ALUMINUM CLUSTERS:1||GaN:1||THIN:1||Electron beam:1||INTENSE:1||Hard Xray pulse generation:1||NONLINEAR THOMSON SCATTERING:1||MULTILAYER:1||UVvisible spectrometer:1||ATOMS:1||innershell transitions:1||CORRECTED CONCAVE GRATINGS:1||DISCHARGE:1||LASERPLASMA:1||thin film:1||reflectivity:1||opacity:1||gain:1||smallangle Xray scattering:1||SOFTXRAY:1||ZINCOXIDE:1||CYGNUSX3:1||Betatron oscillation:1||ACCELERATOR:1||STRAINEDLAYER SUPERLATTICES:1||OPTICAL PARAMETRIC AMPLIFICATION:1||PASSIVE MODELOCKING:1||Collision dynamics:1||MUM:1||EXACTEXCHANGE:1||BASISSET:1||APPROXIMATION:1||OXYNITRIDES:1||Beam energy modulation:1||polarization spectroscopy:1||REORIENTATION TRANSITION:1||DEPENDENCE:1||sulfurs:1||BUILDINGBLOCKS:1||RATES:1||OPTICAL PULSES:1||toroidal mirror:1||XRAY LASER:1||CALCIUM:1||radially polarized laser:1||GRAINBOUNDARIES:1||VAPORDEPOSITION:1||Xray generation:1||MAGNETIZATION:1||Electric excitation:1||Laserinduced gas plasmas:1||Qualitative analysis:1||SCHEME:1||RADIATION:10||PULSES:8||PHOTOLUMINESCENCE:7||LASER:7||GENERATION:6||NANORODS:6||GROWTH:6||NANOWIRES:5||IMPLANTED 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SEMICONDUCTORS:2||MOLECULARBEAM EPITAXY:2||EARTHDOPED GAN:2||LASER FIELDS:2||CHIRPEDPULSEAMPLIFICATION:2||ALN:2||GAUSSIANBEAM:2||ASSISTED CATALYTIC GROWTH:2||BLUE:2||NANOSTRUCTURES:2||MAGNETOELECTRONICS:2||MICROSCOPY:2||ELECTROLUMINESCENCE:2||LASERPULSES:2||GaN nanowires:2||GALLIUM NITRIDE NANOWIRES:2||GAMNN:2||NANOTUBES:2||PHYSICS:2||Femtosecond laser:2||parametric oscillators and amplifiers:1||ultrafast lasers:1||VALENCE:1||nanowires:1||DILUTED MAGNETIC SEMICONDUCTOR:1||LUMINESCENCE:1||Density modulation:1||Energy modulation:1||Current enhanced SASE free electron laser:1||Undulator radiation:1||FREEELECTRON LASERS:1||ULTRATHIN FERROMAGNETICFILMS:1||OXIDEFILMS:1||ABLATION:1||COMPONENT:1||METAL:1||innershell excited states:1||Nelike ions:1||TRANSITIONS:1||XUV spectrometer:1||DIAGNOSTICS:1||Xray scattering:1||MO/SI:1||pulsed laser deposition:1||KEV IMPACT ENERGIES:1||vacuum electron acceleration:1||HIGHINTENSITY LASER:1||JUNCTIONS:1||LOWTEMPERATURE GROWTH:1||nanocrystalline materials:1||MOLECULAR PHOTOIONIZATION:1||LOCALIZATION:1||DEUTERIUM CLUSTERS:1||EXPLOSIONS:1||REGENERATIVE AMPLIFIERS:1||RAREGASES:1||THz radiation:1||FREEELECTRON LASER:1||REALTIME OBSERVATION:1||TARGET:1||photoionized plasmas:1||fs Xray laser:1||emission profile:1||HIGHORDER HARMONICS:1||Xray laser:1||atomic transition:1||EXCITATION:1||LASERS:1||PERFORMANCE:1||RELATIVISTIC ELECTRONS:1||BI2O3DOPED ZNO:1||INNERSHELL IONIZATION:1||Laser wakefield:1||FREQUENCY:1||SOLIDSTATE LASERS:1||Linearly polarized:1||THERMIONIC EMISSION:1||PULSE AMPLIFICATION SYSTEM:1||BIB3O6:1||NM:1||NONCOVALENT INTERACTIONS:1||CRYSTALLINE:1||INTENSITY:1||JETS:1||COHERENT:1||LINE:1||ANGULARDISTRIBUTION:1||SILVER IONS:1||magnetic anisotropy:1||DEVICES:1||Auger transitions:1||CosterKronig transitions:1||EFFICIENT:1||ELECTRONIMPACT IONIZATION:1||ULTRASHORTPULSE:1||Nanowire:1||Heterostructure:1||soft Xray reflectivity:1||PLASMA ACCELERATOR:1||ZINCOXIDE NANOWIRES:1||CHEMICALVAPORDEPOSITION:1||Electron acceleration:1||Ionization of gases:1||Delay dependent:1||MULTIPHOTON IONIZATION:1||FRAGMENTATION:1||GASJET:1||ultrafast nonlinear optics:1||CYCLE PULSES:1||KHZ:1||chemical vapor deposition:1||ferromagnetism:1||ABSORPTION:1||TERAHERTZ RADIATION:1||SCIENCE:1||FIELDS:1||ELECTRONS:1||nanomultilayer structures:1||YIELDS:1||AUGER:1||10HZ REPETITION RATE:1||MULTITERAWATT:1||SPECTROGRAPH:1||HIGHHARMONICGENERATION:1||spectroscopy:1||level population:1||PARTICLEACCELERATION:1||OPTICAL FREQUENCYMEASUREMENT:1||NANOWALLS:1||ROOMTEMPERATURE:1||AVERAGE OUTPUT POWER:1||GROUPVELOCITYMISMATCH:1||Impact ionization:1||Dynamics:1||Lasers:1||Collisional process:1||ABOVETHRESHOLD IONIZATION:1||MAINGROUP THERMOCHEMISTRY:1||dilute magnetic semiconductors:1||GACRN:1||SIZE:1||ATTOSECOND:1||Ar cluster:1||Xray astrophysics:1||photoionization:1||irons:1||normal incidence pulsed laser deposition:1||SHELLS:1||Silicon Oxide:1||gaspuff Zpinch:1||Xray:1||soft Xray reflectors:1||ESCAPE:1||ZN2SIO4:1||SILICA:1||Time 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materials:1||MOLECULAR PHOTOIONIZATION:1||LOCALIZATION:1||DEUTERIUM CLUSTERS:1||EXPLOSIONS:1||REGENERATIVE AMPLIFIERS:1||RAREGASES:1||THz radiation:1||FREEELECTRON LASER:1||REALTIME OBSERVATION:1||TARGET:1||photoionized plasmas:1||fs Xray laser:1||emission profile:1||HIGHORDER HARMONICS:1||Xray laser:1||atomic transition:1||EXCITATION:1||LASERS:1||PERFORMANCE:1||RELATIVISTIC ELECTRONS:1||BI2O3DOPED ZNO:1||INNERSHELL IONIZATION:1||Laser wakefield:1||FREQUENCY:1||SOLIDSTATE LASERS:1||Linearly polarized:1||THERMIONIC EMISSION:1||PULSE AMPLIFICATION SYSTEM:1||BIB3O6:1||NM:1||NONCOVALENT INTERACTIONS:1||CRYSTALLINE:1||INTENSITY:1||JETS:1||COHERENT:1||LINE:1||ANGULARDISTRIBUTION:1||SILVER IONS:1||magnetic anisotropy:1||DEVICES:1||Auger transitions:1||CosterKronig transitions:1||EFFICIENT:1||ELECTRONIMPACT IONIZATION:1||ULTRASHORTPULSE:1||Nanowire:1||Heterostructure:1||soft Xray reflectivity:1||PLASMA ACCELERATOR:1||ZINCOXIDE NANOWIRES:1||CHEMICALVAPORDEPOSITION:1||Electron acceleration:1||Ionization of gases:1||Delay dependent:1||MULTIPHOTON IONIZATION:1||FRAGMENTATION:1||GASJET:1||ultrafast nonlinear optics:1||CYCLE PULSES:1||KHZ:1||chemical vapor deposition:1||ferromagnetism:1||ABSORPTION:1||TERAHERTZ RADIATION:1||SCIENCE:1||FIELDS:1||ELECTRONS:1||nanomultilayer structures:1||YIELDS:1||AUGER:1||10HZ REPETITION RATE:1||MULTITERAWATT:1||SPECTROGRAPH:1||HIGHHARMONICGENERATION:1||spectroscopy:1||level population:1||PARTICLEACCELERATION:1||OPTICAL FREQUENCYMEASUREMENT:1||NANOWALLS:1||ROOMTEMPERATURE:1||AVERAGE OUTPUT POWER:1||GROUPVELOCITYMISMATCH:1||Impact ionization:1||Dynamics:1||Lasers:1||Collisional process:1||ABOVETHRESHOLD IONIZATION:1||MAINGROUP THERMOCHEMISTRY:1||dilute magnetic semiconductors:1||GACRN:1||SIZE:1||ATTOSECOND:1||Ar cluster:1||Xray astrophysics:1||photoionization:1||irons:1||normal incidence pulsed laser deposition:1||SHELLS:1||Silicon Oxide:1||gaspuff Zpinch:1||Xray:1||soft Xray reflectors:1||ESCAPE:1||ZN2SIO4:1||SILICA:1||Time delay:1||Collisional plasmas:1||MASSSPECTROMETRY:1||NUCLEARFUSION:1||PARAMETRIC AMPLIFICATION:1||LYING ELECTRONIC STATES:1||ADJUSTABLEPARAMETERS:1||MAGNETICPROPERTIES:1||LIQUIDPHASE EPITAXY:1||CEP laser:1||REGION:1||Plasma waveguide:1||AMBIENT GAS:1||DEPOSITION:1||HARMONICGENERATION:1||ENHANCEMENT:1||imaging spectrometer:1||Abel inversion:1||Water window:1||Liquid nitrogen jet:1||CHARGEEXCHANGE:1||NOBEL LECTURE:1||VARISTOR:1||EPITAXY:1||THINDISK LASER:1||HIGHREPETITIONRATE:1||Atom lasers:1||Electronimpact excitation:1||High order harmonics:1||ultrafast technology:1||PEAK POWER:1||CHARGED ALUMINUM CLUSTERS:1||GaN:1||THIN:1||Electron beam:1||INTENSE:1||Hard Xray pulse generation:1||NONLINEAR THOMSON SCATTERING:1||MULTILAYER:1||UVvisible spectrometer:1||ATOMS:1||innershell transitions:1||CORRECTED CONCAVE GRATINGS:1||DISCHARGE:1||LASERPLASMA:1||thin film:1||reflectivity:1||opacity:1||gain:1||smallangle Xray scattering:1||SOFTXRAY:1||ZINCOXIDE:1||CYGNUSX3:1||Betatron oscillation:1||ACCELERATOR:1||STRAINEDLAYER SUPERLATTICES:1||OPTICAL PARAMETRIC AMPLIFICATION:1||PASSIVE MODELOCKING:1||Collision dynamics:1||MUM:1||EXACTEXCHANGE:1||BASISSET:1||APPROXIMATION:1||OXYNITRIDES:1||Beam energy modulation:1||polarization spectroscopy:1||REORIENTATION TRANSITION:1||DEPENDENCE:1||sulfurs:1||BUILDINGBLOCKS:1||RATES:1||OPTICAL PULSES:1||toroidal mirror:1||XRAY LASER:1||CALCIUM:1||radially polarized laser:1||GRAINBOUNDARIES:1||VAPORDEPOSITION:1||Xray generation:1||MAGNETIZATION:1||Electric excitation:1||Laserinduced gas plasmas:1||Qualitative analysis:1||SCHEME:1||RADIATION:10||PULSES:8||PHOTOLUMINESCENCE:7||LASER:7||GENERATION:6||NANORODS:6||GROWTH:6||NANOWIRES:5||IMPLANTED GAN:5||SPECTROSCOPY:5||THINFILMS:4||DYNAMICS:4||SILICON:4||EXTREMEULTRAVIOLET:4||AMPLIFICATION:4||PRESSURE:4||PHASE:4||OPTICALPROPERTIES:4||SYSTEM:4||EMISSION:4||FEL:3||N2O:3||FILMS:3||OPTICS:3||SPECTRA:3||FIELD:3||MIRRORS:3||ARRAYS:3||CLUSTERS:3||SIO2:3||IONIZATION:3||VACUUM:3||SCATTERING:3||IONS:2||LUMINESCENCE PROPERTIES:2||ANISOTROPY:2||BEAMS:2||DIFFRACTION:2||DISPERSION:2||chemical vapor deposition (CVD):2||ELECTRONICSTRUCTURE:2||MOSFETS:2||SI3N4:2||DENSITY:2||LIGHT:2||PLASMAS:2||MATTER:2||nanocomposites:2||RAMANSCATTERING:2||NANOPARTICLES:2||OXIDE:2||AMPLIFIED SPONTANEOUS EMISSION:2||NM WAVELENGTH:2||GAIN:2||CARBON NANOTUBES:2||CROSSSECTIONS:2||LIGHTEMITTINGDIODES:2||PULSE:2||CARBON PLASMA:2||TISAPPHIRE LASER:2||Raman scattering:2||ROUTE:2||multilayer:2||CATHODOLUMINESCENCE:2||highresolution transmission electronic microscope (HRTEM):2||DIFFERENCEFREQUENCYGENERATION:2||CRYSTAL:2||laserproduced plasma:2||NANOCABLES:2||photoluminescence:2||MAGNETIC ALLOY SEMICONDUCTORS:2||MOLECULARBEAM EPITAXY:2||EARTHDOPED GAN:2||LASER FIELDS:2||CHIRPEDPULSEAMPLIFICATION:2||ALN:2||GAUSSIANBEAM:2||ASSISTED CATALYTIC GROWTH:2||BLUE:2||NANOSTRUCTURES:2||MAGNETOELECTRONICS:2||MICROSCOPY:2||ELECTROLUMINESCENCE:2||LASERPULSES:2||GaN nanowires:2||GALLIUM NITRIDE NANOWIRES:2||GAMNN:2||NANOTUBES:2||PHYSICS:2||Femtosecond laser:2||parametric oscillators and amplifiers:1||ultrafast lasers:1||VALENCE:1||nanowires:1||DILUTED MAGNETIC SEMICONDUCTOR:1||LUMINESCENCE:1||Density modulation:1||Energy modulation:1||Current enhanced SASE free electron laser:1||Undulator radiation:1||FREEELECTRON LASERS:1||ULTRATHIN FERROMAGNETICFILMS:1||OXIDEFILMS:1||ABLATION:1||COMPONENT:1||METAL:1||innershell excited states:1||Nelike ions:1||TRANSITIONS:1||XUV spectrometer:1||DIAGNOSTICS:1||Xray scattering:1||MO/SI:1||pulsed laser deposition:1||KEV IMPACT ENERGIES:1||vacuum electron acceleration:1||HIGHINTENSITY LASER:1||JUNCTIONS:1||LOWTEMPERATURE GROWTH:1||nanocrystalline materials:1||MOLECULAR PHOTOIONIZATION:1||LOCALIZATION:1||DEUTERIUM CLUSTERS:1||EXPLOSIONS:1||REGENERATIVE AMPLIFIERS:1||RAREGASES:1||THz radiation:1||FREEELECTRON LASER:1||REALTIME OBSERVATION:1||TARGET:1||photoionized plasmas:1||fs Xray laser:1||emission profile:1||HIGHORDER HARMONICS:1||Xray laser:1||atomic transition:1||EXCITATION:1||LASERS:1||PERFORMANCE:1||RELATIVISTIC ELECTRONS:1||BI2O3DOPED ZNO:1||INNERSHELL IONIZATION:1||Laser wakefield:1||FREQUENCY:1||SOLIDSTATE LASERS:1||Linearly polarized:1||THERMIONIC EMISSION:1||PULSE AMPLIFICATION SYSTEM:1||BIB3O6:1||NM:1||NONCOVALENT INTERACTIONS:1||CRYSTALLINE:1||INTENSITY:1||JETS:1||COHERENT:1||LINE:1||ANGULARDISTRIBUTION:1||SILVER IONS:1||magnetic anisotropy:1||DEVICES:1||Auger transitions:1||CosterKronig transitions:1||EFFICIENT:1||ELECTRONIMPACT IONIZATION:1||ULTRASHORTPULSE:1||Nanowire:1||Heterostructure:1||soft Xray reflectivity:1||PLASMA ACCELERATOR:1||ZINCOXIDE NANOWIRES:1||CHEMICALVAPORDEPOSITION:1||Electron acceleration:1||Ionization of gases:1||Delay dependent:1||MULTIPHOTON IONIZATION:1||FRAGMENTATION:1||GASJET:1||ultrafast nonlinear optics:1||CYCLE PULSES:1||KHZ:1||chemical vapor deposition:1||ferromagnetism:1||ABSORPTION:1||TERAHERTZ RADIATION:1||SCIENCE:1||FIELDS:1||ELECTRONS:1||nanomultilayer structures:1||YIELDS:1||AUGER:1||10HZ REPETITION RATE:1||MULTITERAWATT:1||SPECTROGRAPH:1||HIGHHARMONICGENERATION:1||spectroscopy:1||level population:1||PARTICLEACCELERATION:1||OPTICAL FREQUENCYMEASUREMENT:1||NANOWALLS:1||ROOMTEMPERATURE:1||AVERAGE OUTPUT POWER:1||GROUPVELOCITYMISMATCH:1||Impact ionization:1||Dynamics:1||Lasers:1||Collisional process:1||ABOVETHRESHOLD IONIZATION:1||MAINGROUP THERMOCHEMISTRY:1||dilute magnetic semiconductors:1||GACRN:1||SIZE:1||ATTOSECOND:1||Ar cluster:1||Xray astrophysics:1||photoionization:1||irons:1||normal incidence pulsed laser deposition:1||SHELLS:1||Silicon Oxide:1||gaspuff Zpinch:1||Xray:1||soft Xray reflectors:1||ESCAPE:1||ZN2SIO4:1||SILICA:1||Time delay:1||Collisional plasmas:1||MASSSPECTROMETRY:1||NUCLEARFUSION:1||PARAMETRIC AMPLIFICATION:1||LYING ELECTRONIC STATES:1||ADJUSTABLEPARAMETERS:1||MAGNETICPROPERTIES:1||LIQUIDPHASE EPITAXY:1||CEP laser:1||REGION:1||Plasma waveguide:1||AMBIENT GAS:1||DEPOSITION:1||HARMONICGENERATION:1||ENHANCEMENT:1||imaging spectrometer:1||Abel inversion:1||Water window:1||Liquid nitrogen jet:1||CHARGEEXCHANGE:1||NOBEL LECTURE:1||VARISTOR:1||EPITAXY:1||THINDISK LASER:1||HIGHREPETITIONRATE:1||Atom lasers:1||Electronimpact excitation:1||High order harmonics:1||ultrafast technology:1||PEAK POWER:1||CHARGED ALUMINUM CLUSTERS:1||GaN:1||THIN:1||Electron beam:1||INTENSE:1||Hard Xray pulse generation:1||NONLINEAR THOMSON SCATTERING:1||MULTILAYER:1||UVvisible spectrometer:1||ATOMS:1||innershell transitions:1||CORRECTED CONCAVE GRATINGS:1||DISCHARGE:1||LASERPLASMA:1||thin film:1||reflectivity:1||opacity:1||gain:1||smallangle Xray scattering:1||SOFTXRAY:1||ZINCOXIDE:1||CYGNUSX3:1||Betatron oscillation:1||ACCELERATOR:1||STRAINEDLAYER SUPERLATTICES:1||OPTICAL PARAMETRIC AMPLIFICATION:1||PASSIVE MODELOCKING:1||Collision dynamics:1||MUM:1||EXACTEXCHANGE:1||BASISSET:1||APPROXIMATION:1||OXYNITRIDES:1||Beam energy modulation:1||polarization spectroscopy:1||REORIENTATION TRANSITION:1||DEPENDENCE:1||sulfurs:1||BUILDINGBLOCKS:1||RATES:1||OPTICAL PULSES:1||toroidal mirror:1||XRAY LASER:1||CALCIUM:1||radially polarized laser:1||GRAINBOUNDARIES:1||VAPORDEPOSITION:1||Xray generation:1||MAGNETIZATION:1||Electric excitation:1||Laserinduced gas plasmas:1||Qualitative analysis:1||SCHEME:1||RADIATION:10||PULSES:8||PHOTOLUMINESCENCE:7||LASER:7||GENERATION:6||NANORODS:6||GROWTH:6||NANOWIRES:5||IMPLANTED 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SEMICONDUCTORS:2||MOLECULARBEAM EPITAXY:2||EARTHDOPED GAN:2||LASER FIELDS:2||CHIRPEDPULSEAMPLIFICATION:2||ALN:2||GAUSSIANBEAM:2||ASSISTED CATALYTIC GROWTH:2||BLUE:2||NANOSTRUCTURES:2||MAGNETOELECTRONICS:2||MICROSCOPY:2||ELECTROLUMINESCENCE:2||LASERPULSES:2||GaN nanowires:2||GALLIUM NITRIDE NANOWIRES:2||GAMNN:2||NANOTUBES:2||PHYSICS:2||Femtosecond laser:2||parametric oscillators and amplifiers:1||ultrafast lasers:1||VALENCE:1||nanowires:1||DILUTED MAGNETIC SEMICONDUCTOR:1||LUMINESCENCE:1||Density modulation:1||Energy modulation:1||Current enhanced SASE free electron laser:1||Undulator radiation:1||FREEELECTRON LASERS:1||ULTRATHIN FERROMAGNETICFILMS:1||OXIDEFILMS:1||ABLATION:1||COMPONENT:1||METAL:1||innershell excited states:1||Nelike ions:1||TRANSITIONS:1||XUV spectrometer:1||DIAGNOSTICS:1||Xray scattering:1||MO/SI:1||pulsed laser deposition:1||KEV IMPACT ENERGIES:1||vacuum electron acceleration:1||HIGHINTENSITY LASER:1||JUNCTIONS:1||LOWTEMPERATURE GROWTH:1||nanocrystalline materials:1||MOLECULAR PHOTOIONIZATION:1||LOCALIZATION:1||DEUTERIUM CLUSTERS:1||EXPLOSIONS:1||REGENERATIVE AMPLIFIERS:1||RAREGASES:1||THz radiation:1||FREEELECTRON LASER:1||REALTIME OBSERVATION:1||TARGET:1||photoionized plasmas:1||fs Xray laser:1||emission profile:1||HIGHORDER HARMONICS:1||Xray laser:1||atomic transition:1||EXCITATION:1||LASERS:1||PERFORMANCE:1||RELATIVISTIC ELECTRONS:1||BI2O3DOPED ZNO:1||INNERSHELL IONIZATION:1||Laser wakefield:1||FREQUENCY:1||SOLIDSTATE LASERS:1||Linearly polarized:1||THERMIONIC EMISSION:1||PULSE AMPLIFICATION SYSTEM:1||BIB3O6:1||NM:1||NONCOVALENT INTERACTIONS:1||CRYSTALLINE:1||INTENSITY:1||JETS:1||COHERENT:1||LINE:1||ANGULARDISTRIBUTION:1||SILVER IONS:1||magnetic anisotropy:1||DEVICES:1||Auger transitions:1||CosterKronig transitions:1||EFFICIENT:1||ELECTRONIMPACT IONIZATION:1||ULTRASHORTPULSE:1||Nanowire:1||Heterostructure:1||soft Xray reflectivity:1||PLASMA ACCELERATOR:1||ZINCOXIDE NANOWIRES:1||CHEMICALVAPORDEPOSITION:1||Electron acceleration:1||Ionization of gases:1||Delay dependent:1||MULTIPHOTON IONIZATION:1||FRAGMENTATION:1||GASJET:1||ultrafast nonlinear optics:1||CYCLE PULSES:1||KHZ:1||chemical vapor deposition:1||ferromagnetism:1||ABSORPTION:1||TERAHERTZ RADIATION:1||SCIENCE:1||FIELDS:1||ELECTRONS:1||nanomultilayer structures:1||YIELDS:1||AUGER:1||10HZ REPETITION RATE:1||MULTITERAWATT:1||SPECTROGRAPH:1||HIGHHARMONICGENERATION:1||spectroscopy:1||level population:1||PARTICLEACCELERATION:1||OPTICAL FREQUENCYMEASUREMENT:1||NANOWALLS:1||ROOMTEMPERATURE:1||AVERAGE OUTPUT POWER:1||GROUPVELOCITYMISMATCH:1||Impact ionization:1||Dynamics:1||Lasers:1||Collisional process:1||ABOVETHRESHOLD IONIZATION:1||MAINGROUP THERMOCHEMISTRY:1||dilute magnetic semiconductors:1||GACRN:1||SIZE:1||ATTOSECOND:1||Ar cluster:1||Xray astrophysics:1||photoionization:1||irons:1||normal incidence pulsed laser deposition:1||SHELLS:1||Silicon Oxide:1||gaspuff Zpinch:1||Xray:1||soft Xray reflectors:1||ESCAPE:1||ZN2SIO4:1||SILICA:1||Time 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materials:1||MOLECULAR PHOTOIONIZATION:1||LOCALIZATION:1||DEUTERIUM CLUSTERS:1||EXPLOSIONS:1||REGENERATIVE AMPLIFIERS:1||RAREGASES:1||THz radiation:1||FREEELECTRON LASER:1||REALTIME OBSERVATION:1||TARGET:1||photoionized plasmas:1||fs Xray laser:1||emission profile:1||HIGHORDER HARMONICS:1||Xray laser:1||atomic transition:1||EXCITATION:1||LASERS:1||PERFORMANCE:1||RELATIVISTIC ELECTRONS:1||BI2O3DOPED ZNO:1||INNERSHELL IONIZATION:1||Laser wakefield:1||FREQUENCY:1||SOLIDSTATE LASERS:1||Linearly polarized:1||THERMIONIC EMISSION:1||PULSE AMPLIFICATION SYSTEM:1||BIB3O6:1||NM:1||NONCOVALENT INTERACTIONS:1||CRYSTALLINE:1||INTENSITY:1||JETS:1||COHERENT:1||LINE:1||ANGULARDISTRIBUTION:1||SILVER IONS:1||magnetic anisotropy:1||DEVICES:1||Auger transitions:1||CosterKronig transitions:1||EFFICIENT:1||ELECTRONIMPACT IONIZATION:1||ULTRASHORTPULSE:1||Nanowire:1||Heterostructure:1||soft Xray reflectivity:1||PLASMA ACCELERATOR:1||ZINCOXIDE NANOWIRES:1||CHEMICALVAPORDEPOSITION:1||Electron acceleration:1||Ionization of gases:1||Delay dependent:1||MULTIPHOTON IONIZATION:1||FRAGMENTATION:1||GASJET:1||ultrafast nonlinear optics:1||CYCLE PULSES:1||KHZ:1||chemical vapor deposition:1||ferromagnetism:1||ABSORPTION:1||TERAHERTZ RADIATION:1||SCIENCE:1||FIELDS:1||ELECTRONS:1||nanomultilayer structures:1||YIELDS:1||AUGER:1||10HZ REPETITION RATE:1||MULTITERAWATT:1||SPECTROGRAPH:1||HIGHHARMONICGENERATION:1||spectroscopy:1||level population:1||PARTICLEACCELERATION:1||OPTICAL FREQUENCYMEASUREMENT:1||NANOWALLS:1||ROOMTEMPERATURE:1||AVERAGE OUTPUT POWER:1||GROUPVELOCITYMISMATCH:1||Impact ionization:1||Dynamics:1||Lasers:1||Collisional process:1||ABOVETHRESHOLD IONIZATION:1||MAINGROUP THERMOCHEMISTRY:1||dilute magnetic semiconductors:1||GACRN:1||SIZE:1||ATTOSECOND:1||Ar cluster:1||Xray astrophysics:1||photoionization:1||irons:1||normal incidence pulsed laser deposition:1||SHELLS:1||Silicon Oxide:1||gaspuff Zpinch:1||Xray:1||soft Xray reflectors:1||ESCAPE:1||ZN2SIO4:1||SILICA:1||Time delay:1||Collisional plasmas:1||MASSSPECTROMETRY:1||NUCLEARFUSION:1||PARAMETRIC AMPLIFICATION:1||LYING ELECTRONIC STATES:1||ADJUSTABLEPARAMETERS:1||MAGNETICPROPERTIES:1||LIQUIDPHASE EPITAXY:1||CEP laser:1||REGION:1||Plasma waveguide:1||AMBIENT GAS:1||DEPOSITION:1||HARMONICGENERATION:1||ENHANCEMENT:1||imaging spectrometer:1||Abel inversion:1||Water window:1||Liquid nitrogen jet:1||CHARGEEXCHANGE:1||NOBEL LECTURE:1||VARISTOR:1||EPITAXY:1||THINDISK LASER:1||HIGHREPETITIONRATE:1||Atom lasers:1||Electronimpact excitation:1||High order harmonics:1||ultrafast technology:1||PEAK POWER:1||CHARGED ALUMINUM CLUSTERS:1||GaN:1||THIN:1||Electron beam:1||INTENSE:1||Hard Xray pulse generation:1||NONLINEAR THOMSON SCATTERING:1||MULTILAYER:1||UVvisible spectrometer:1||ATOMS:1||innershell transitions:1||CORRECTED CONCAVE GRATINGS:1||DISCHARGE:1||LASERPLASMA:1||thin film:1||reflectivity:1||opacity:1||gain:1||smallangle Xray scattering:1||SOFTXRAY:1||ZINCOXIDE:1||CYGNUSX3:1||Betatron oscillation:1||ACCELERATOR:1||STRAINEDLAYER SUPERLATTICES:1||OPTICAL PARAMETRIC AMPLIFICATION:1||PASSIVE MODELOCKING:1||Collision dynamics:1||MUM:1||EXACTEXCHANGE:1||BASISSET:1||APPROXIMATION:1||OXYNITRIDES:1||Beam energy modulation:1||polarization spectroscopy:1||REORIENTATION TRANSITION:1||DEPENDENCE:1||sulfurs:1||BUILDINGBLOCKS:1||RATES:1||OPTICAL PULSES:1||toroidal mirror:1||XRAY LASER:1||CALCIUM:1||radially polarized laser:1||GRAINBOUNDARIES:1||VAPORDEPOSITION:1||Xray generation:1||MAGNETIZATION:1||Electric excitation:1||Laserinduced gas plasmas:1||Qualitative analysis:1||SCHEME:1||RADIATION:10||PULSES:8||PHOTOLUMINESCENCE:7||LASER:7||GENERATION:6||NANORODS:6||GROWTH:6||NANOWIRES:5||IMPLANTED GAN:5||SPECTROSCOPY:5||THINFILMS:4||DYNAMICS:4||SILICON:4||EXTREMEULTRAVIOLET:4||AMPLIFICATION:4||PRESSURE:4||PHASE:4||OPTICALPROPERTIES:4||SYSTEM:4||EMISSION:4||FEL:3||N2O:3||FILMS:3||OPTICS:3||SPECTRA:3||FIELD:3||MIRRORS:3||ARRAYS:3||CLUSTERS:3||SIO2:3||IONIZATION:3||VACUUM:3||SCATTERING:3||IONS:2||LUMINESCENCE PROPERTIES:2||ANISOTROPY:2||BEAMS:2||DIFFRACTION:2||DISPERSION:2||chemical vapor deposition (CVD):2||ELECTRONICSTRUCTURE:2||MOSFETS:2||SI3N4:2||DENSITY:2||LIGHT:2||PLASMAS:2||MATTER:2||nanocomposites:2||RAMANSCATTERING:2||NANOPARTICLES:2||OXIDE:2||AMPLIFIED SPONTANEOUS EMISSION:2||NM WAVELENGTH:2||GAIN:2||CARBON NANOTUBES:2||CROSSSECTIONS:2||LIGHTEMITTINGDIODES:2||PULSE:2||CARBON PLASMA:2||TISAPPHIRE LASER:2||Raman scattering:2||ROUTE:2||multilayer:2||CATHODOLUMINESCENCE:2||highresolution transmission electronic microscope (HRTEM):2||DIFFERENCEFREQUENCYGENERATION:2||CRYSTAL:2||laserproduced plasma:2||NANOCABLES:2||photoluminescence:2||MAGNETIC ALLOY SEMICONDUCTORS:2||MOLECULARBEAM EPITAXY:2||EARTHDOPED GAN:2||LASER FIELDS:2||CHIRPEDPULSEAMPLIFICATION:2||ALN:2||GAUSSIANBEAM:2||ASSISTED CATALYTIC GROWTH:2||BLUE:2||NANOSTRUCTURES:2||MAGNETOELECTRONICS:2||MICROSCOPY:2||ELECTROLUMINESCENCE:2||LASERPULSES:2||GaN nanowires:2||GALLIUM NITRIDE NANOWIRES:2||GAMNN:2||NANOTUBES:2||PHYSICS:2||Femtosecond laser:2||parametric oscillators and amplifiers:1||ultrafast lasers:1||VALENCE:1||nanowires:1||DILUTED MAGNETIC SEMICONDUCTOR:1||LUMINESCENCE:1||Density modulation:1||Energy modulation:1||Current enhanced SASE free electron laser:1||Undulator radiation:1||FREEELECTRON LASERS:1||ULTRATHIN FERROMAGNETICFILMS:1||OXIDEFILMS:1||ABLATION:1||COMPONENT:1||METAL:1||innershell excited states:1||Nelike ions:1||TRANSITIONS:1||XUV spectrometer:1||DIAGNOSTICS:1||Xray scattering:1||MO/SI:1||pulsed laser deposition:1||KEV IMPACT ENERGIES:1||vacuum electron acceleration:1||HIGHINTENSITY LASER:1||JUNCTIONS:1||LOWTEMPERATURE GROWTH:1||nanocrystalline materials:1||MOLECULAR PHOTOIONIZATION:1||LOCALIZATION:1||DEUTERIUM CLUSTERS:1||EXPLOSIONS:1||REGENERATIVE AMPLIFIERS:1||RAREGASES:1||THz radiation:1||FREEELECTRON LASER:1||REALTIME OBSERVATION:1||TARGET:1||photoionized plasmas:1||fs Xray laser:1||emission profile:1||HIGHORDER HARMONICS:1||Xray laser:1||atomic transition:1||EXCITATION:1||LASERS:1||PERFORMANCE:1||RELATIVISTIC ELECTRONS:1||BI2O3DOPED ZNO:1||INNERSHELL IONIZATION:1||Laser wakefield:1||FREQUENCY:1||SOLIDSTATE LASERS:1||Linearly polarized:1||THERMIONIC EMISSION:1||PULSE AMPLIFICATION SYSTEM:1||BIB3O6:1||NM:1||NONCOVALENT INTERACTIONS:1||CRYSTALLINE:1||INTENSITY:1||JETS:1||COHERENT:1||LINE:1||ANGULARDISTRIBUTION:1||SILVER IONS:1||magnetic anisotropy:1||DEVICES:1||Auger transitions:1||CosterKronig transitions:1||EFFICIENT:1||ELECTRONIMPACT IONIZATION:1||ULTRASHORTPULSE:1||Nanowire:1||Heterostructure:1||soft Xray reflectivity:1||PLASMA ACCELERATOR:1||ZINCOXIDE NANOWIRES:1||CHEMICALVAPORDEPOSITION:1||Electron acceleration:1||Ionization of gases:1||Delay dependent:1||MULTIPHOTON IONIZATION:1||FRAGMENTATION:1||GASJET:1||ultrafast nonlinear optics:1||CYCLE PULSES:1||KHZ:1||chemical vapor deposition:1||ferromagnetism:1||ABSORPTION:1||TERAHERTZ RADIATION:1||SCIENCE:1||FIELDS:1||ELECTRONS:1||nanomultilayer structures:1||YIELDS:1||AUGER:1||10HZ REPETITION RATE:1||MULTITERAWATT:1||SPECTROGRAPH:1||HIGHHARMONICGENERATION:1||spectroscopy:1||level population:1||PARTICLEACCELERATION:1||OPTICAL FREQUENCYMEASUREMENT:1||NANOWALLS:1||ROOMTEMPERATURE:1||AVERAGE OUTPUT POWER:1||GROUPVELOCITYMISMATCH:1||Impact ionization:1||Dynamics:1||Lasers:1||Collisional process:1||ABOVETHRESHOLD IONIZATION:1||MAINGROUP THERMOCHEMISTRY:1||dilute magnetic semiconductors:1||GACRN:1||SIZE:1||ATTOSECOND:1||Ar cluster:1||Xray astrophysics:1||photoionization:1||irons:1||normal incidence pulsed laser deposition:1||SHELLS:1||Silicon Oxide:1||gaspuff Zpinch:1||Xray:1||soft Xray reflectors:1||ESCAPE:1||ZN2SIO4:1||SILICA:1||Time delay:1||Collisional plasmas:1||MASSSPECTROMETRY:1||NUCLEARFUSION:1||PARAMETRIC AMPLIFICATION:1||LYING ELECTRONIC STATES:1||ADJUSTABLEPARAMETERS:1||MAGNETICPROPERTIES:1||LIQUIDPHASE EPITAXY:1||CEP laser:1||REGION:1||Plasma waveguide:1||AMBIENT GAS:1||DEPOSITION:1||HARMONICGENERATION:1||ENHANCEMENT:1||imaging spectrometer:1||Abel inversion:1||Water window:1||Liquid nitrogen jet:1||CHARGEEXCHANGE:1||NOBEL LECTURE:1||VARISTOR:1||EPITAXY:1||THINDISK LASER:1||HIGHREPETITIONRATE:1||Atom lasers:1||Electronimpact excitation:1||High order harmonics:1||ultrafast technology:1||PEAK POWER:1||CHARGED ALUMINUM CLUSTERS:1||GaN:1||THIN:1||Electron beam:1||INTENSE:1||Hard Xray pulse generation:1||NONLINEAR THOMSON SCATTERING:1||MULTILAYER:1||UVvisible spectrometer:1||ATOMS:1||innershell transitions:1||CORRECTED CONCAVE GRATINGS:1||DISCHARGE:1||LASERPLASMA:1||thin film:1||reflectivity:1||opacity:1||gain:1||smallangle Xray scattering:1||SOFTXRAY:1||ZINCOXIDE:1||CYGNUSX3:1||Betatron oscillation:1||ACCELERATOR:1||STRAINEDLAYER SUPERLATTICES:1||OPTICAL PARAMETRIC AMPLIFICATION:1||PASSIVE MODELOCKING:1||Collision dynamics:1||MUM:1||EXACTEXCHANGE:1||BASISSET:1||APPROXIMATION:1||OXYNITRIDES:1||Beam energy modulation:1||polarization spectroscopy:1||REORIENTATION TRANSITION:1||DEPENDENCE:1||sulfurs:1||BUILDINGBLOCKS:1||RATES:1||OPTICAL PULSES:1||toroidal mirror:1||XRAY LASER:1||CALCIUM:1||radially polarized laser:1||GRAINBOUNDARIES:1||VAPORDEPOSITION:1||Xray generation:1||MAGNETIZATION:1||Electric excitation:1||Laserinduced gas plasmas:1||Qualitative analysis:1||SCHEME:1||RADIATION:10||PULSES:8||PHOTOLUMINESCENCE:7||LASER:7||GENERATION:6||NANORODS:6||GROWTH:6||NANOWIRES:5||IMPLANTED 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SEMICONDUCTORS:2||MOLECULARBEAM EPITAXY:2||EARTHDOPED GAN:2||LASER FIELDS:2||CHIRPEDPULSEAMPLIFICATION:2||ALN:2||GAUSSIANBEAM:2||ASSISTED CATALYTIC GROWTH:2||BLUE:2||NANOSTRUCTURES:2||MAGNETOELECTRONICS:2||MICROSCOPY:2||ELECTROLUMINESCENCE:2||LASERPULSES:2||GaN nanowires:2||GALLIUM NITRIDE NANOWIRES:2||GAMNN:2||NANOTUBES:2||PHYSICS:2||Femtosecond laser:2||parametric oscillators and amplifiers:1||ultrafast lasers:1||VALENCE:1||nanowires:1||DILUTED MAGNETIC SEMICONDUCTOR:1||LUMINESCENCE:1||Density modulation:1||Energy modulation:1||Current enhanced SASE free electron laser:1||Undulator radiation:1||FREEELECTRON LASERS:1||ULTRATHIN FERROMAGNETICFILMS:1||OXIDEFILMS:1||ABLATION:1||COMPONENT:1||METAL:1||innershell excited states:1||Nelike ions:1||TRANSITIONS:1||XUV spectrometer:1||DIAGNOSTICS:1||Xray scattering:1||MO/SI:1||pulsed laser deposition:1||KEV IMPACT ENERGIES:1||vacuum electron acceleration:1||HIGHINTENSITY LASER:1||JUNCTIONS:1||LOWTEMPERATURE GROWTH:1||nanocrystalline materials:1||MOLECULAR PHOTOIONIZATION:1||LOCALIZATION:1||DEUTERIUM CLUSTERS:1||EXPLOSIONS:1||REGENERATIVE AMPLIFIERS:1||RAREGASES:1||THz radiation:1||FREEELECTRON LASER:1||REALTIME OBSERVATION:1||TARGET:1||photoionized plasmas:1||fs Xray laser:1||emission profile:1||HIGHORDER HARMONICS:1||Xray laser:1||atomic transition:1||EXCITATION:1||LASERS:1||PERFORMANCE:1||RELATIVISTIC ELECTRONS:1||BI2O3DOPED ZNO:1||INNERSHELL IONIZATION:1||Laser wakefield:1||FREQUENCY:1||SOLIDSTATE LASERS:1||Linearly polarized:1||THERMIONIC EMISSION:1||PULSE AMPLIFICATION SYSTEM:1||BIB3O6:1||NM:1||NONCOVALENT INTERACTIONS:1||CRYSTALLINE:1||INTENSITY:1||JETS:1||COHERENT:1||LINE:1||ANGULARDISTRIBUTION:1||SILVER IONS:1||magnetic anisotropy:1||DEVICES:1||Auger transitions:1||CosterKronig transitions:1||EFFICIENT:1||ELECTRONIMPACT IONIZATION:1||ULTRASHORTPULSE:1||Nanowire:1||Heterostructure:1||soft Xray reflectivity:1||PLASMA ACCELERATOR:1||ZINCOXIDE NANOWIRES:1||CHEMICALVAPORDEPOSITION:1||Electron acceleration:1||Ionization of gases:1||Delay dependent:1||MULTIPHOTON IONIZATION:1||FRAGMENTATION:1||GASJET:1||ultrafast nonlinear optics:1||CYCLE PULSES:1||KHZ:1||chemical vapor deposition:1||ferromagnetism:1||ABSORPTION:1||TERAHERTZ RADIATION:1||SCIENCE:1||FIELDS:1||ELECTRONS:1||nanomultilayer structures:1||YIELDS:1||AUGER:1||10HZ REPETITION RATE:1||MULTITERAWATT:1||SPECTROGRAPH:1||HIGHHARMONICGENERATION:1||spectroscopy:1||level population:1||PARTICLEACCELERATION:1||OPTICAL FREQUENCYMEASUREMENT:1||NANOWALLS:1||ROOMTEMPERATURE:1||AVERAGE OUTPUT POWER:1||GROUPVELOCITYMISMATCH:1||Impact ionization:1||Dynamics:1||Lasers:1||Collisional process:1||ABOVETHRESHOLD IONIZATION:1||MAINGROUP THERMOCHEMISTRY:1||dilute magnetic semiconductors:1||GACRN:1||SIZE:1||ATTOSECOND:1||Ar cluster:1||Xray astrophysics:1||photoionization:1||irons:1||normal incidence pulsed laser deposition:1||SHELLS:1||Silicon Oxide:1||gaspuff Zpinch:1||Xray:1||soft Xray reflectors:1||ESCAPE:1||ZN2SIO4:1||SILICA:1||Time 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materials:1||MOLECULAR PHOTOIONIZATION:1||LOCALIZATION:1||DEUTERIUM CLUSTERS:1||EXPLOSIONS:1||REGENERATIVE AMPLIFIERS:1||RAREGASES:1||THz radiation:1||FREEELECTRON LASER:1||REALTIME OBSERVATION:1||TARGET:1||photoionized plasmas:1||fs Xray laser:1||emission profile:1||HIGHORDER HARMONICS:1||Xray laser:1||atomic transition:1||EXCITATION:1||LASERS:1||PERFORMANCE:1||RELATIVISTIC ELECTRONS:1||BI2O3DOPED ZNO:1||INNERSHELL IONIZATION:1||Laser wakefield:1||FREQUENCY:1||SOLIDSTATE LASERS:1||Linearly polarized:1||THERMIONIC EMISSION:1||PULSE AMPLIFICATION SYSTEM:1||BIB3O6:1||NM:1||NONCOVALENT INTERACTIONS:1||CRYSTALLINE:1||INTENSITY:1||JETS:1||COHERENT:1||LINE:1||ANGULARDISTRIBUTION:1||SILVER IONS:1||magnetic anisotropy:1||DEVICES:1||Auger transitions:1||CosterKronig transitions:1||EFFICIENT:1||ELECTRONIMPACT IONIZATION:1||ULTRASHORTPULSE:1||Nanowire:1||Heterostructure:1||soft Xray reflectivity:1||PLASMA ACCELERATOR:1||ZINCOXIDE NANOWIRES:1||CHEMICALVAPORDEPOSITION:1||Electron acceleration:1||Ionization of gases:1||Delay dependent:1||MULTIPHOTON IONIZATION:1||FRAGMENTATION:1||GASJET:1||ultrafast nonlinear optics:1||CYCLE PULSES:1||KHZ:1||chemical vapor deposition:1||ferromagnetism:1||ABSORPTION:1||TERAHERTZ RADIATION:1||SCIENCE:1||FIELDS:1||ELECTRONS:1||nanomultilayer structures:1||YIELDS:1||AUGER:1||10HZ REPETITION RATE:1||MULTITERAWATT:1||SPECTROGRAPH:1||HIGHHARMONICGENERATION:1||spectroscopy:1||level population:1||PARTICLEACCELERATION:1||OPTICAL FREQUENCYMEASUREMENT:1||NANOWALLS:1||ROOMTEMPERATURE:1||AVERAGE OUTPUT POWER:1||GROUPVELOCITYMISMATCH:1||Impact ionization:1||Dynamics:1||Lasers:1||Collisional process:1||ABOVETHRESHOLD IONIZATION:1||MAINGROUP THERMOCHEMISTRY:1||dilute magnetic semiconductors:1||GACRN:1||SIZE:1||ATTOSECOND:1||Ar cluster:1||Xray astrophysics:1||photoionization:1||irons:1||normal incidence pulsed laser deposition:1||SHELLS:1||Silicon Oxide:1||gaspuff Zpinch:1||Xray:1||soft Xray reflectors:1||ESCAPE:1||ZN2SIO4:1||SILICA:1||Time delay:1||Collisional plasmas:1||MASSSPECTROMETRY:1||NUCLEARFUSION:1||PARAMETRIC AMPLIFICATION:1||LYING ELECTRONIC STATES:1||ADJUSTABLEPARAMETERS:1||MAGNETICPROPERTIES:1||LIQUIDPHASE EPITAXY:1||CEP laser:1||REGION:1||Plasma waveguide:1||AMBIENT GAS:1||DEPOSITION:1||HARMONICGENERATION:1||ENHANCEMENT:1||imaging spectrometer:1||Abel inversion:1||Water window:1||Liquid nitrogen jet:1||CHARGEEXCHANGE:1||NOBEL LECTURE:1||VARISTOR:1||EPITAXY:1||THINDISK LASER:1||HIGHREPETITIONRATE:1||Atom lasers:1||Electronimpact excitation:1||High order harmonics:1||ultrafast technology:1||PEAK POWER:1||CHARGED ALUMINUM CLUSTERS:1||GaN:1||THIN:1||Electron beam:1||INTENSE:1||Hard Xray pulse generation:1||NONLINEAR THOMSON SCATTERING:1||MULTILAYER:1||UVvisible spectrometer:1||ATOMS:1||innershell transitions:1||CORRECTED CONCAVE GRATINGS:1||DISCHARGE:1||LASERPLASMA:1||thin film:1||reflectivity:1||opacity:1||gain:1||smallangle Xray scattering:1||SOFTXRAY:1||ZINCOXIDE:1||CYGNUSX3:1||Betatron oscillation:1||ACCELERATOR:1||STRAINEDLAYER SUPERLATTICES:1||OPTICAL PARAMETRIC AMPLIFICATION:1||PASSIVE MODELOCKING:1||Collision dynamics:1||MUM:1||EXACTEXCHANGE:1||BASISSET:1||APPROXIMATION:1||OXYNITRIDES:1||Beam energy modulation:1||polarization spectroscopy:1||REORIENTATION TRANSITION:1||DEPENDENCE:1||sulfurs:1||BUILDINGBLOCKS:1||RATES:1||OPTICAL PULSES:1||toroidal mirror:1||XRAY LASER:1||CALCIUM:1||radially polarized laser:1||GRAINBOUNDARIES:1||VAPORDEPOSITION:1||Xray generation:1||MAGNETIZATION:1||Electric excitation:1||Laserinduced gas plasmas:1||Qualitative analysis:1||SCHEME:1||RADIATION:10||PULSES:8||PHOTOLUMINESCENCE:7||LASER:7||GENERATION:6||NANORODS:6||GROWTH:6||NANOWIRES:5||IMPLANTED GAN:5||SPECTROSCOPY:5||THINFILMS:4||DYNAMICS:4||SILICON:4||EXTREMEULTRAVIOLET:4||AMPLIFICATION:4||PRESSURE:4||PHASE:4||OPTICALPROPERTIES:4||SYSTEM:4||EMISSION:4||FEL:3||N2O:3||FILMS:3||OPTICS:3||SPECTRA:3||FIELD:3||MIRRORS:3||ARRAYS:3||CLUSTERS:3||SIO2:3||IONIZATION:3||VACUUM:3||SCATTERING:3||IONS:2||LUMINESCENCE PROPERTIES:2||ANISOTROPY:2||BEAMS:2||DIFFRACTION:2||DISPERSION:2||chemical vapor deposition (CVD):2||ELECTRONICSTRUCTURE:2||MOSFETS:2||SI3N4:2||DENSITY:2||LIGHT:2||PLASMAS:2||MATTER:2||nanocomposites:2||RAMANSCATTERING:2||NANOPARTICLES:2||OXIDE:2||AMPLIFIED SPONTANEOUS EMISSION:2||NM WAVELENGTH:2||GAIN:2||CARBON NANOTUBES:2||CROSSSECTIONS:2||LIGHTEMITTINGDIODES:2||PULSE:2||CARBON PLASMA:2||TISAPPHIRE LASER:2||Raman scattering:2||ROUTE:2||multilayer:2||CATHODOLUMINESCENCE:2||highresolution transmission electronic microscope (HRTEM):2||DIFFERENCEFREQUENCYGENERATION:2||CRYSTAL:2||laserproduced plasma:2||NANOCABLES:2||photoluminescence:2||MAGNETIC ALLOY SEMICONDUCTORS:2||MOLECULARBEAM EPITAXY:2||EARTHDOPED GAN:2||LASER FIELDS:2||CHIRPEDPULSEAMPLIFICATION:2||ALN:2||GAUSSIANBEAM:2||ASSISTED CATALYTIC GROWTH:2||BLUE:2||NANOSTRUCTURES:2||MAGNETOELECTRONICS:2||MICROSCOPY:2||ELECTROLUMINESCENCE:2||LASERPULSES:2||GaN nanowires:2||GALLIUM NITRIDE NANOWIRES:2||GAMNN:2||NANOTUBES:2||PHYSICS:2||Femtosecond laser:2||parametric oscillators and amplifiers:1||ultrafast lasers:1||VALENCE:1||nanowires:1||DILUTED MAGNETIC SEMICONDUCTOR:1||LUMINESCENCE:1||Density modulation:1||Energy modulation:1||Current enhanced SASE free electron laser:1||Undulator radiation:1||FREEELECTRON LASERS:1||ULTRATHIN FERROMAGNETICFILMS:1||OXIDEFILMS:1||ABLATION:1||COMPONENT:1||METAL:1||innershell excited states:1||Nelike ions:1||TRANSITIONS:1||XUV spectrometer:1||DIAGNOSTICS:1||Xray scattering:1||MO/SI:1||pulsed laser deposition:1||KEV IMPACT ENERGIES:1||vacuum electron acceleration:1||HIGHINTENSITY LASER:1||JUNCTIONS:1||LOWTEMPERATURE GROWTH:1||nanocrystalline materials:1||MOLECULAR PHOTOIONIZATION:1||LOCALIZATION:1||DEUTERIUM CLUSTERS:1||EXPLOSIONS:1||REGENERATIVE AMPLIFIERS:1||RAREGASES:1||THz radiation:1||FREEELECTRON LASER:1||REALTIME OBSERVATION:1||TARGET:1||photoionized plasmas:1||fs Xray laser:1||emission profile:1||HIGHORDER HARMONICS:1||Xray laser:1||atomic transition:1||EXCITATION:1||LASERS:1||PERFORMANCE:1||RELATIVISTIC ELECTRONS:1||BI2O3DOPED ZNO:1||INNERSHELL IONIZATION:1||Laser wakefield:1||FREQUENCY:1||SOLIDSTATE LASERS:1||Linearly polarized:1||THERMIONIC EMISSION:1||PULSE AMPLIFICATION SYSTEM:1||BIB3O6:1||NM:1||NONCOVALENT INTERACTIONS:1||CRYSTALLINE:1||INTENSITY:1||JETS:1||COHERENT:1||LINE:1||ANGULARDISTRIBUTION:1||SILVER IONS:1||magnetic anisotropy:1||DEVICES:1||Auger transitions:1||CosterKronig transitions:1||EFFICIENT:1||ELECTRONIMPACT IONIZATION:1||ULTRASHORTPULSE:1||Nanowire:1||Heterostructure:1||soft Xray reflectivity:1||PLASMA ACCELERATOR:1||ZINCOXIDE NANOWIRES:1||CHEMICALVAPORDEPOSITION:1||Electron acceleration:1||Ionization of gases:1||Delay dependent:1||MULTIPHOTON IONIZATION:1||FRAGMENTATION:1||GASJET:1||ultrafast nonlinear optics:1||CYCLE PULSES:1||KHZ:1||chemical vapor deposition:1||ferromagnetism:1||ABSORPTION:1||TERAHERTZ RADIATION:1||SCIENCE:1||FIELDS:1||ELECTRONS:1||nanomultilayer structures:1||YIELDS:1||AUGER:1||10HZ REPETITION RATE:1||MULTITERAWATT:1||SPECTROGRAPH:1||HIGHHARMONICGENERATION:1||spectroscopy:1||level population:1||PARTICLEACCELERATION:1||OPTICAL FREQUENCYMEASUREMENT:1||NANOWALLS:1||ROOMTEMPERATURE:1||AVERAGE OUTPUT POWER:1||GROUPVELOCITYMISMATCH:1||Impact ionization:1||Dynamics:1||Lasers:1||Collisional process:1||ABOVETHRESHOLD IONIZATION:1||MAINGROUP THERMOCHEMISTRY:1||dilute magnetic semiconductors:1||GACRN:1||SIZE:1||ATTOSECOND:1||Ar cluster:1||Xray astrophysics:1||photoionization:1||irons:1||normal incidence pulsed laser deposition:1||SHELLS:1||Silicon Oxide:1||gaspuff Zpinch:1||Xray:1||soft Xray reflectors:1||ESCAPE:1||ZN2SIO4:1||SILICA:1||Time delay:1||Collisional plasmas:1||MASSSPECTROMETRY:1||NUCLEARFUSION:1||PARAMETRIC AMPLIFICATION:1||LYING ELECTRONIC STATES:1||ADJUSTABLEPARAMETERS:1||MAGNETICPROPERTIES:1||LIQUIDPHASE EPITAXY:1||CEP laser:1||REGION:1||Plasma waveguide:1||AMBIENT GAS:1||DEPOSITION:1||HARMONICGENERATION:1||ENHANCEMENT:1||imaging spectrometer:1||Abel inversion:1||Water window:1||Liquid nitrogen jet:1||CHARGEEXCHANGE:1||NOBEL LECTURE:1||VARISTOR:1||EPITAXY:1||THINDISK LASER:1||HIGHREPETITIONRATE:1||Atom lasers:1||Electronimpact excitation:1||High order harmonics:1||ultrafast technology:1||PEAK POWER:1||CHARGED ALUMINUM CLUSTERS:1||GaN:1||THIN:1||Electron beam:1||INTENSE:1||Hard Xray pulse generation:1||NONLINEAR THOMSON SCATTERING:1||MULTILAYER:1||UVvisible spectrometer:1||ATOMS:1||innershell transitions:1||CORRECTED CONCAVE GRATINGS:1||DISCHARGE:1||LASERPLASMA:1||thin film:1||reflectivity:1||opacity:1||gain:1||smallangle Xray scattering:1||SOFTXRAY:1||ZINCOXIDE:1||CYGNUSX3:1||Betatron oscillation:1||ACCELERATOR:1||STRAINEDLAYER SUPERLATTICES:1||OPTICAL PARAMETRIC AMPLIFICATION:1||PASSIVE MODELOCKING:1||Collision dynamics:1||MUM:1||EXACTEXCHANGE:1||BASISSET:1||APPROXIMATION:1||OXYNITRIDES:1||Beam energy modulation:1||polarization spectroscopy:1||REORIENTATION TRANSITION:1||DEPENDENCE:1||sulfurs:1||BUILDINGBLOCKS:1||RATES:1||OPTICAL PULSES:1||toroidal mirror:1||XRAY LASER:1||CALCIUM:1||radially polarized laser:1||GRAINBOUNDARIES:1||VAPORDEPOSITION:1||Xray generation:1||MAGNETIZATION:1||Electric excitation:1||Laserinduced gas plasmas:1||Qualitative analysis:1||SCHEME:1||RADIATION:10||PULSES:8||PHOTOLUMINESCENCE:7||LASER:7||GENERATION:6||NANORODS:6||GROWTH:6||NANOWIRES:5||IMPLANTED 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SEMICONDUCTORS:2||MOLECULARBEAM EPITAXY:2||EARTHDOPED GAN:2||LASER FIELDS:2||CHIRPEDPULSEAMPLIFICATION:2||ALN:2||GAUSSIANBEAM:2||ASSISTED CATALYTIC GROWTH:2||BLUE:2||NANOSTRUCTURES:2||MAGNETOELECTRONICS:2||MICROSCOPY:2||ELECTROLUMINESCENCE:2||LASERPULSES:2||GaN nanowires:2||GALLIUM NITRIDE NANOWIRES:2||GAMNN:2||NANOTUBES:2||PHYSICS:2||Femtosecond laser:2||parametric oscillators and amplifiers:1||ultrafast lasers:1||VALENCE:1||nanowires:1||DILUTED MAGNETIC SEMICONDUCTOR:1||LUMINESCENCE:1||Density modulation:1||Energy modulation:1||Current enhanced SASE free electron laser:1||Undulator radiation:1||FREEELECTRON LASERS:1||ULTRATHIN FERROMAGNETICFILMS:1||OXIDEFILMS:1||ABLATION:1||COMPONENT:1||METAL:1||innershell excited states:1||Nelike ions:1||TRANSITIONS:1||XUV spectrometer:1||DIAGNOSTICS:1||Xray scattering:1||MO/SI:1||pulsed laser deposition:1||KEV IMPACT ENERGIES:1||vacuum electron acceleration:1||HIGHINTENSITY LASER:1||JUNCTIONS:1||LOWTEMPERATURE GROWTH:1||nanocrystalline materials:1||MOLECULAR PHOTOIONIZATION:1||LOCALIZATION:1||DEUTERIUM CLUSTERS:1||EXPLOSIONS:1||REGENERATIVE AMPLIFIERS:1||RAREGASES:1||THz radiation:1||FREEELECTRON LASER:1||REALTIME OBSERVATION:1||TARGET:1||photoionized plasmas:1||fs Xray laser:1||emission profile:1||HIGHORDER HARMONICS:1||Xray laser:1||atomic transition:1||EXCITATION:1||LASERS:1||PERFORMANCE:1||RELATIVISTIC ELECTRONS:1||BI2O3DOPED ZNO:1||INNERSHELL IONIZATION:1||Laser wakefield:1||FREQUENCY:1||SOLIDSTATE LASERS:1||Linearly polarized:1||THERMIONIC EMISSION:1||PULSE AMPLIFICATION SYSTEM:1||BIB3O6:1||NM:1||NONCOVALENT INTERACTIONS:1||CRYSTALLINE:1||INTENSITY:1||JETS:1||COHERENT:1||LINE:1||ANGULARDISTRIBUTION:1||SILVER IONS:1||magnetic anisotropy:1||DEVICES:1||Auger transitions:1||CosterKronig transitions:1||EFFICIENT:1||ELECTRONIMPACT IONIZATION:1||ULTRASHORTPULSE:1||Nanowire:1||Heterostructure:1||soft Xray reflectivity:1||PLASMA ACCELERATOR:1||ZINCOXIDE NANOWIRES:1||CHEMICALVAPORDEPOSITION:1||Electron acceleration:1||Ionization of gases:1||Delay dependent:1||MULTIPHOTON IONIZATION:1||FRAGMENTATION:1||GASJET:1||ultrafast nonlinear optics:1||CYCLE PULSES:1||KHZ:1||chemical vapor deposition:1||ferromagnetism:1||ABSORPTION:1||TERAHERTZ RADIATION:1||SCIENCE:1||FIELDS:1||ELECTRONS:1||nanomultilayer structures:1||YIELDS:1||AUGER:1||10HZ REPETITION RATE:1||MULTITERAWATT:1||SPECTROGRAPH:1||HIGHHARMONICGENERATION:1||spectroscopy:1||level population:1||PARTICLEACCELERATION:1||OPTICAL FREQUENCYMEASUREMENT:1||NANOWALLS:1||ROOMTEMPERATURE:1||AVERAGE OUTPUT POWER:1||GROUPVELOCITYMISMATCH:1||Impact ionization:1||Dynamics:1||Lasers:1||Collisional process:1||ABOVETHRESHOLD IONIZATION:1||MAINGROUP THERMOCHEMISTRY:1||dilute magnetic semiconductors:1||GACRN:1||SIZE:1||ATTOSECOND:1||Ar cluster:1||Xray astrophysics:1||photoionization:1||irons:1||normal incidence pulsed laser deposition:1||SHELLS:1||Silicon Oxide:1||gaspuff Zpinch:1||Xray:1||soft Xray reflectors:1||ESCAPE:1||ZN2SIO4:1||SILICA:1||Time 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materials:1||MOLECULAR PHOTOIONIZATION:1||LOCALIZATION:1||DEUTERIUM CLUSTERS:1||EXPLOSIONS:1||REGENERATIVE AMPLIFIERS:1||RAREGASES:1||THz radiation:1||FREEELECTRON LASER:1||REALTIME OBSERVATION:1||TARGET:1||photoionized plasmas:1||fs Xray laser:1||emission profile:1||HIGHORDER HARMONICS:1||Xray laser:1||atomic transition:1||EXCITATION:1||LASERS:1||PERFORMANCE:1||RELATIVISTIC ELECTRONS:1||BI2O3DOPED ZNO:1||INNERSHELL IONIZATION:1||Laser wakefield:1||FREQUENCY:1||SOLIDSTATE LASERS:1||Linearly polarized:1||THERMIONIC EMISSION:1||PULSE AMPLIFICATION SYSTEM:1||BIB3O6:1||NM:1||NONCOVALENT INTERACTIONS:1||CRYSTALLINE:1||INTENSITY:1||JETS:1||COHERENT:1||LINE:1||ANGULARDISTRIBUTION:1||SILVER IONS:1||magnetic anisotropy:1||DEVICES:1||Auger transitions:1||CosterKronig transitions:1||EFFICIENT:1||ELECTRONIMPACT IONIZATION:1||ULTRASHORTPULSE:1||Nanowire:1||Heterostructure:1||soft Xray reflectivity:1||PLASMA ACCELERATOR:1||ZINCOXIDE NANOWIRES:1||CHEMICALVAPORDEPOSITION:1||Electron acceleration:1||Ionization of gases:1||Delay dependent:1||MULTIPHOTON IONIZATION:1||FRAGMENTATION:1||GASJET:1||ultrafast nonlinear optics:1||CYCLE PULSES:1||KHZ:1||chemical vapor deposition:1||ferromagnetism:1||ABSORPTION:1||TERAHERTZ RADIATION:1||SCIENCE:1||FIELDS:1||ELECTRONS:1||nanomultilayer structures:1||YIELDS:1||AUGER:1||10HZ REPETITION RATE:1||MULTITERAWATT:1||SPECTROGRAPH:1||HIGHHARMONICGENERATION:1||spectroscopy:1||level population:1||PARTICLEACCELERATION:1||OPTICAL FREQUENCYMEASUREMENT:1||NANOWALLS:1||ROOMTEMPERATURE:1||AVERAGE OUTPUT POWER:1||GROUPVELOCITYMISMATCH:1||Impact ionization:1||Dynamics:1||Lasers:1||Collisional process:1||ABOVETHRESHOLD IONIZATION:1||MAINGROUP THERMOCHEMISTRY:1||dilute magnetic semiconductors:1||GACRN:1||SIZE:1||ATTOSECOND:1||Ar cluster:1||Xray astrophysics:1||photoionization:1||irons:1||normal incidence pulsed laser deposition:1||SHELLS:1||Silicon Oxide:1||gaspuff Zpinch:1||Xray:1||soft Xray reflectors:1||ESCAPE:1||ZN2SIO4:1||SILICA:1||Time delay:1||Collisional plasmas:1||MASSSPECTROMETRY:1||NUCLEARFUSION:1||PARAMETRIC AMPLIFICATION:1||LYING ELECTRONIC STATES:1||ADJUSTABLEPARAMETERS:1||MAGNETICPROPERTIES:1||LIQUIDPHASE EPITAXY:1||CEP laser:1||REGION:1||Plasma waveguide:1||AMBIENT GAS:1||DEPOSITION:1||HARMONICGENERATION:1||ENHANCEMENT:1||imaging spectrometer:1||Abel inversion:1||Water window:1||Liquid nitrogen jet:1||CHARGEEXCHANGE:1||NOBEL LECTURE:1||VARISTOR:1||EPITAXY:1||THINDISK LASER:1||HIGHREPETITIONRATE:1||Atom lasers:1||Electronimpact excitation:1||High order harmonics:1||ultrafast technology:1||PEAK POWER:1||CHARGED ALUMINUM CLUSTERS:1||GaN:1||THIN:1||Electron beam:1||INTENSE:1||Hard Xray pulse generation:1||NONLINEAR THOMSON SCATTERING:1||MULTILAYER:1||UVvisible spectrometer:1||ATOMS:1||innershell transitions:1||CORRECTED CONCAVE GRATINGS:1||DISCHARGE:1||LASERPLASMA:1||thin film:1||reflectivity:1||opacity:1||gain:1||smallangle Xray scattering:1||SOFTXRAY:1||ZINCOXIDE:1||CYGNUSX3:1||Betatron oscillation:1||ACCELERATOR:1||STRAINEDLAYER SUPERLATTICES:1||OPTICAL PARAMETRIC AMPLIFICATION:1||PASSIVE MODELOCKING:1||Collision dynamics:1||MUM:1||EXACTEXCHANGE:1||BASISSET:1||APPROXIMATION:1||OXYNITRIDES:1||Beam energy modulation:1||polarization spectroscopy:1||REORIENTATION TRANSITION:1||DEPENDENCE:1||sulfurs:1||BUILDINGBLOCKS:1||RATES:1||OPTICAL PULSES:1||toroidal mirror:1||XRAY LASER:1||CALCIUM:1||radially polarized laser:1||GRAINBOUNDARIES:1||VAPORDEPOSITION:1||Xray generation:1||MAGNETIZATION:1||Electric excitation:1||Laserinduced gas plasmas:1||Qualitative analysis:1||SCHEME:1||RADIATION:10||PULSES:8||PHOTOLUMINESCENCE:7||LASER:7||GENERATION:6||NANORODS:6||GROWTH:6||NANOWIRES:5||IMPLANTED GAN:5||SPECTROSCOPY:5||THINFILMS:4||DYNAMICS:4||SILICON:4||EXTREMEULTRAVIOLET:4||AMPLIFICATION:4||PRESSURE:4||PHASE:4||OPTICALPROPERTIES:4||SYSTEM:4||EMISSION:4||FEL:3||N2O:3||FILMS:3||OPTICS:3||SPECTRA:3||FIELD:3||MIRRORS:3||ARRAYS:3||CLUSTERS:3||SIO2:3||IONIZATION:3||VACUUM:3||SCATTERING:3||IONS:2||LUMINESCENCE PROPERTIES:2||ANISOTROPY:2||BEAMS:2||DIFFRACTION:2||DISPERSION:2||chemical vapor deposition (CVD):2||ELECTRONICSTRUCTURE:2||MOSFETS:2||SI3N4:2||DENSITY:2||LIGHT:2||PLASMAS:2||MATTER:2||nanocomposites:2||RAMANSCATTERING:2||NANOPARTICLES:2||OXIDE:2||AMPLIFIED SPONTANEOUS EMISSION:2||NM WAVELENGTH:2||GAIN:2||CARBON NANOTUBES:2||CROSSSECTIONS:2||LIGHTEMITTINGDIODES:2||PULSE:2||CARBON PLASMA:2||TISAPPHIRE LASER:2||Raman scattering:2||ROUTE:2||multilayer:2||CATHODOLUMINESCENCE:2||highresolution transmission electronic microscope (HRTEM):2||DIFFERENCEFREQUENCYGENERATION:2||CRYSTAL:2||laserproduced plasma:2||NANOCABLES:2||photoluminescence:2||MAGNETIC ALLOY SEMICONDUCTORS:2||MOLECULARBEAM EPITAXY:2||EARTHDOPED GAN:2||LASER FIELDS:2||CHIRPEDPULSEAMPLIFICATION:2||ALN:2||GAUSSIANBEAM:2||ASSISTED CATALYTIC GROWTH:2||BLUE:2||NANOSTRUCTURES:2||MAGNETOELECTRONICS:2||MICROSCOPY:2||ELECTROLUMINESCENCE:2||LASERPULSES:2||GaN nanowires:2||GALLIUM NITRIDE NANOWIRES:2||GAMNN:2||NANOTUBES:2||PHYSICS:2||Femtosecond laser:2||parametric oscillators and amplifiers:1||ultrafast lasers:1||VALENCE:1||nanowires:1||DILUTED MAGNETIC SEMICONDUCTOR:1||LUMINESCENCE:1||Density modulation:1||Energy modulation:1||Current enhanced SASE free electron laser:1||Undulator radiation:1||FREEELECTRON LASERS:1||ULTRATHIN FERROMAGNETICFILMS:1||OXIDEFILMS:1||ABLATION:1||COMPONENT:1||METAL:1||innershell excited states:1||Nelike ions:1||TRANSITIONS:1||XUV spectrometer:1||DIAGNOSTICS:1||Xray scattering:1||MO/SI:1||pulsed laser deposition:1||KEV IMPACT ENERGIES:1||vacuum electron acceleration:1||HIGHINTENSITY LASER:1||JUNCTIONS:1||LOWTEMPERATURE GROWTH:1||nanocrystalline materials:1||MOLECULAR PHOTOIONIZATION:1||LOCALIZATION:1||DEUTERIUM CLUSTERS:1||EXPLOSIONS:1||REGENERATIVE AMPLIFIERS:1||RAREGASES:1||THz radiation:1||FREEELECTRON LASER:1||REALTIME OBSERVATION:1||TARGET:1||photoionized plasmas:1||fs Xray laser:1||emission profile:1||HIGHORDER HARMONICS:1||Xray laser:1||atomic transition:1||EXCITATION:1||LASERS:1||PERFORMANCE:1||RELATIVISTIC ELECTRONS:1||BI2O3DOPED ZNO:1||INNERSHELL IONIZATION:1||Laser wakefield:1||FREQUENCY:1||SOLIDSTATE LASERS:1||Linearly polarized:1||THERMIONIC EMISSION:1||PULSE AMPLIFICATION SYSTEM:1||BIB3O6:1||NM:1||NONCOVALENT INTERACTIONS:1||CRYSTALLINE:1||INTENSITY:1||JETS:1||COHERENT:1||LINE:1||ANGULARDISTRIBUTION:1||SILVER IONS:1||magnetic anisotropy:1||DEVICES:1||Auger transitions:1||CosterKronig transitions:1||EFFICIENT:1||ELECTRONIMPACT IONIZATION:1||ULTRASHORTPULSE:1||Nanowire:1||Heterostructure:1||soft Xray reflectivity:1||PLASMA ACCELERATOR:1||ZINCOXIDE NANOWIRES:1||CHEMICALVAPORDEPOSITION:1||Electron acceleration:1||Ionization of gases:1||Delay dependent:1||MULTIPHOTON IONIZATION:1||FRAGMENTATION:1||GASJET:1||ultrafast nonlinear optics:1||CYCLE PULSES:1||KHZ:1||chemical vapor deposition:1||ferromagnetism:1||ABSORPTION:1||TERAHERTZ RADIATION:1||SCIENCE:1||FIELDS:1||ELECTRONS:1||nanomultilayer structures:1||YIELDS:1||AUGER:1||10HZ REPETITION RATE:1||MULTITERAWATT:1||SPECTROGRAPH:1||HIGHHARMONICGENERATION:1||spectroscopy:1||level population:1||PARTICLEACCELERATION:1||OPTICAL FREQUENCYMEASUREMENT:1||NANOWALLS:1||ROOMTEMPERATURE:1||AVERAGE OUTPUT POWER:1||GROUPVELOCITYMISMATCH:1||Impact ionization:1||Dynamics:1||Lasers:1||Collisional process:1||ABOVETHRESHOLD IONIZATION:1||MAINGROUP THERMOCHEMISTRY:1||dilute magnetic semiconductors:1||GACRN:1||SIZE:1||ATTOSECOND:1||Ar cluster:1||Xray astrophysics:1||photoionization:1||irons:1||normal incidence pulsed laser deposition:1||SHELLS:1||Silicon Oxide:1||gaspuff Zpinch:1||Xray:1||soft Xray reflectors:1||ESCAPE:1||ZN2SIO4:1||SILICA:1||Time delay:1||Collisional plasmas:1||MASSSPECTROMETRY:1||NUCLEARFUSION:1||PARAMETRIC AMPLIFICATION:1||LYING ELECTRONIC STATES:1||ADJUSTABLEPARAMETERS:1||MAGNETICPROPERTIES:1||LIQUIDPHASE EPITAXY:1||CEP laser:1||REGION:1||Plasma waveguide:1||AMBIENT GAS:1||DEPOSITION:1||HARMONICGENERATION:1||ENHANCEMENT:1||imaging spectrometer:1||Abel inversion:1||Water window:1||Liquid nitrogen jet:1||CHARGEEXCHANGE:1||NOBEL LECTURE:1||VARISTOR:1||EPITAXY:1||THINDISK LASER:1||HIGHREPETITIONRATE:1||Atom lasers:1||Electronimpact excitation:1||High order harmonics:1||ultrafast technology:1||PEAK POWER:1||CHARGED ALUMINUM CLUSTERS:1||GaN:1||THIN:1||Electron beam:1||INTENSE:1||Hard Xray pulse generation:1||NONLINEAR THOMSON SCATTERING:1||MULTILAYER:1||UVvisible spectrometer:1||ATOMS:1||innershell transitions:1||CORRECTED CONCAVE GRATINGS:1||DISCHARGE:1||LASERPLASMA:1||thin film:1||reflectivity:1||opacity:1||gain:1||smallangle Xray scattering:1||SOFTXRAY:1||ZINCOXIDE:1||CYGNUSX3:1||Betatron oscillation:1||ACCELERATOR:1||STRAINEDLAYER SUPERLATTICES:1||OPTICAL PARAMETRIC AMPLIFICATION:1||PASSIVE MODELOCKING:1||Collision dynamics:1||MUM:1||EXACTEXCHANGE:1||BASISSET:1||APPROXIMATION:1||OXYNITRIDES:1||Beam energy modulation:1||polarization spectroscopy:1||REORIENTATION TRANSITION:1||DEPENDENCE:1||sulfurs:1||BUILDINGBLOCKS:1||RATES:1||OPTICAL PULSES:1||toroidal mirror:1||XRAY LASER:1||CALCIUM:1||radially polarized laser:1||GRAINBOUNDARIES:1||VAPORDEPOSITION:1||Xray generation:1||MAGNETIZATION:1||Electric excitation:1||Laserinduced gas plasmas:1||Qualitative analysis:1||SCHEME:1||RADIATION:10||PULSES:8||PHOTOLUMINESCENCE:7||LASER:7||GENERATION:6||NANORODS:6||GROWTH:6||NANOWIRES:5||IMPLANTED 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SEMICONDUCTORS:2||MOLECULARBEAM EPITAXY:2||EARTHDOPED GAN:2||LASER FIELDS:2||CHIRPEDPULSEAMPLIFICATION:2||ALN:2||GAUSSIANBEAM:2||ASSISTED CATALYTIC GROWTH:2||BLUE:2||NANOSTRUCTURES:2||MAGNETOELECTRONICS:2||MICROSCOPY:2||ELECTROLUMINESCENCE:2||LASERPULSES:2||GaN nanowires:2||GALLIUM NITRIDE NANOWIRES:2||GAMNN:2||NANOTUBES:2||PHYSICS:2||Femtosecond laser:2||parametric oscillators and amplifiers:1||ultrafast lasers:1||VALENCE:1||nanowires:1||DILUTED MAGNETIC SEMICONDUCTOR:1||LUMINESCENCE:1||Density modulation:1||Energy modulation:1||Current enhanced SASE free electron laser:1||Undulator radiation:1||FREEELECTRON LASERS:1||ULTRATHIN FERROMAGNETICFILMS:1||OXIDEFILMS:1||ABLATION:1||COMPONENT:1||METAL:1||innershell excited states:1||Nelike ions:1||TRANSITIONS:1||XUV spectrometer:1||DIAGNOSTICS:1||Xray scattering:1||MO/SI:1||pulsed laser deposition:1||KEV IMPACT ENERGIES:1||vacuum electron acceleration:1||HIGHINTENSITY LASER:1||JUNCTIONS:1||LOWTEMPERATURE GROWTH:1||nanocrystalline materials:1||MOLECULAR PHOTOIONIZATION:1||LOCALIZATION:1||DEUTERIUM CLUSTERS:1||EXPLOSIONS:1||REGENERATIVE AMPLIFIERS:1||RAREGASES:1||THz radiation:1||FREEELECTRON LASER:1||REALTIME OBSERVATION:1||TARGET:1||photoionized plasmas:1||fs Xray laser:1||emission profile:1||HIGHORDER HARMONICS:1||Xray laser:1||atomic transition:1||EXCITATION:1||LASERS:1||PERFORMANCE:1||RELATIVISTIC ELECTRONS:1||BI2O3DOPED ZNO:1||INNERSHELL IONIZATION:1||Laser wakefield:1||FREQUENCY:1||SOLIDSTATE LASERS:1||Linearly polarized:1||THERMIONIC EMISSION:1||PULSE AMPLIFICATION SYSTEM:1||BIB3O6:1||NM:1||NONCOVALENT INTERACTIONS:1||CRYSTALLINE:1||INTENSITY:1||JETS:1||COHERENT:1||LINE:1||ANGULARDISTRIBUTION:1||SILVER IONS:1||magnetic anisotropy:1||DEVICES:1||Auger transitions:1||CosterKronig transitions:1||EFFICIENT:1||ELECTRONIMPACT IONIZATION:1||ULTRASHORTPULSE:1||Nanowire:1||Heterostructure:1||soft Xray reflectivity:1||PLASMA ACCELERATOR:1||ZINCOXIDE NANOWIRES:1||CHEMICALVAPORDEPOSITION:1||Electron acceleration:1||Ionization of gases:1||Delay dependent:1||MULTIPHOTON IONIZATION:1||FRAGMENTATION:1||GASJET:1||ultrafast nonlinear optics:1||CYCLE PULSES:1||KHZ:1||chemical vapor deposition:1||ferromagnetism:1||ABSORPTION:1||TERAHERTZ RADIATION:1||SCIENCE:1||FIELDS:1||ELECTRONS:1||nanomultilayer structures:1||YIELDS:1||AUGER:1||10HZ REPETITION RATE:1||MULTITERAWATT:1||SPECTROGRAPH:1||HIGHHARMONICGENERATION:1||spectroscopy:1||level population:1||PARTICLEACCELERATION:1||OPTICAL FREQUENCYMEASUREMENT:1||NANOWALLS:1||ROOMTEMPERATURE:1||AVERAGE OUTPUT POWER:1||GROUPVELOCITYMISMATCH:1||Impact ionization:1||Dynamics:1||Lasers:1||Collisional process:1||ABOVETHRESHOLD IONIZATION:1||MAINGROUP THERMOCHEMISTRY:1||dilute magnetic semiconductors:1||GACRN:1||SIZE:1||ATTOSECOND:1||Ar cluster:1||Xray astrophysics:1||photoionization:1||irons:1||normal incidence pulsed laser deposition:1||SHELLS:1||Silicon Oxide:1||gaspuff Zpinch:1||Xray:1||soft Xray reflectors:1||ESCAPE:1||ZN2SIO4:1||SILICA:1||Time 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materials:1||MOLECULAR PHOTOIONIZATION:1||LOCALIZATION:1||DEUTERIUM CLUSTERS:1||EXPLOSIONS:1||REGENERATIVE AMPLIFIERS:1||RAREGASES:1||THz radiation:1||FREEELECTRON LASER:1||REALTIME OBSERVATION:1||TARGET:1||photoionized plasmas:1||fs Xray laser:1||emission profile:1||HIGHORDER HARMONICS:1||Xray laser:1||atomic transition:1||EXCITATION:1||LASERS:1||PERFORMANCE:1||RELATIVISTIC ELECTRONS:1||BI2O3DOPED ZNO:1||INNERSHELL IONIZATION:1||Laser wakefield:1||FREQUENCY:1||SOLIDSTATE LASERS:1||Linearly polarized:1||THERMIONIC EMISSION:1||PULSE AMPLIFICATION SYSTEM:1||BIB3O6:1||NM:1||NONCOVALENT INTERACTIONS:1||CRYSTALLINE:1||INTENSITY:1||JETS:1||COHERENT:1||LINE:1||ANGULARDISTRIBUTION:1||SILVER IONS:1||magnetic anisotropy:1||DEVICES:1||Auger transitions:1||CosterKronig transitions:1||EFFICIENT:1||ELECTRONIMPACT IONIZATION:1||ULTRASHORTPULSE:1||Nanowire:1||Heterostructure:1||soft Xray reflectivity:1||PLASMA ACCELERATOR:1||ZINCOXIDE NANOWIRES:1||CHEMICALVAPORDEPOSITION:1||Electron acceleration:1||Ionization of gases:1||Delay dependent:1||MULTIPHOTON IONIZATION:1||FRAGMENTATION:1||GASJET:1||ultrafast nonlinear optics:1||CYCLE PULSES:1||KHZ:1||chemical vapor deposition:1||ferromagnetism:1||ABSORPTION:1||TERAHERTZ RADIATION:1||SCIENCE:1||FIELDS:1||ELECTRONS:1||nanomultilayer structures:1||YIELDS:1||AUGER:1||10HZ REPETITION RATE:1||MULTITERAWATT:1||SPECTROGRAPH:1||HIGHHARMONICGENERATION:1||spectroscopy:1||level population:1||PARTICLEACCELERATION:1||OPTICAL FREQUENCYMEASUREMENT:1||NANOWALLS:1||ROOMTEMPERATURE:1||AVERAGE OUTPUT POWER:1||GROUPVELOCITYMISMATCH:1||Impact ionization:1||Dynamics:1||Lasers:1||Collisional process:1||ABOVETHRESHOLD IONIZATION:1||MAINGROUP THERMOCHEMISTRY:1||dilute magnetic semiconductors:1||GACRN:1||SIZE:1||ATTOSECOND:1||Ar cluster:1||Xray astrophysics:1||photoionization:1||irons:1||normal incidence pulsed laser deposition:1||SHELLS:1||Silicon Oxide:1||gaspuff Zpinch:1||Xray:1||soft Xray reflectors:1||ESCAPE:1||ZN2SIO4:1||SILICA:1||Time delay:1||Collisional plasmas:1||MASSSPECTROMETRY:1||NUCLEARFUSION:1||PARAMETRIC AMPLIFICATION:1||LYING ELECTRONIC STATES:1||ADJUSTABLEPARAMETERS:1||MAGNETICPROPERTIES:1||LIQUIDPHASE EPITAXY:1||CEP laser:1||REGION:1||Plasma waveguide:1||AMBIENT GAS:1||DEPOSITION:1||HARMONICGENERATION:1||ENHANCEMENT:1||imaging spectrometer:1||Abel inversion:1||Water window:1||Liquid nitrogen jet:1||CHARGEEXCHANGE:1||NOBEL LECTURE:1||VARISTOR:1||EPITAXY:1||THINDISK LASER:1||HIGHREPETITIONRATE:1||Atom lasers:1||Electronimpact excitation:1||High order harmonics:1||ultrafast technology:1||PEAK POWER:1||CHARGED ALUMINUM CLUSTERS:1||GaN:1||THIN:1||Electron beam:1||INTENSE:1||Hard Xray pulse generation:1||NONLINEAR THOMSON SCATTERING:1||MULTILAYER:1||UVvisible spectrometer:1||ATOMS:1||innershell transitions:1||CORRECTED CONCAVE GRATINGS:1||DISCHARGE:1||LASERPLASMA:1||thin film:1||reflectivity:1||opacity:1||gain:1||smallangle Xray scattering:1||SOFTXRAY:1||ZINCOXIDE:1||CYGNUSX3:1||Betatron oscillation:1||ACCELERATOR:1||STRAINEDLAYER SUPERLATTICES:1||OPTICAL PARAMETRIC AMPLIFICATION:1||PASSIVE MODELOCKING:1||Collision dynamics:1||MUM:1||EXACTEXCHANGE:1||BASISSET:1||APPROXIMATION:1||OXYNITRIDES:1||Beam energy modulation:1||polarization spectroscopy:1||REORIENTATION TRANSITION:1||DEPENDENCE:1||sulfurs:1||BUILDINGBLOCKS:1||RATES:1||OPTICAL PULSES:1||toroidal mirror:1||XRAY LASER:1||CALCIUM:1||radially polarized laser:1||GRAINBOUNDARIES:1||VAPORDEPOSITION:1||Xray generation:1||MAGNETIZATION:1||Electric excitation:1||Laserinduced gas plasmas:1||Qualitative analysis:1||SCHEME:1||RADIATION:10||PULSES:8||PHOTOLUMINESCENCE:7||LASER:7||GENERATION:6||NANORODS:6||GROWTH:6||NANOWIRES:5||IMPLANTED GAN:5||SPECTROSCOPY:5||THINFILMS:4||DYNAMICS:4||SILICON:4||EXTREMEULTRAVIOLET:4||AMPLIFICATION:4||PRESSURE:4||PHASE:4||OPTICALPROPERTIES:4||SYSTEM:4||EMISSION:4||FEL:3||N2O:3||FILMS:3||OPTICS:3||SPECTRA:3||FIELD:3||MIRRORS:3||ARRAYS:3||CLUSTERS:3||SIO2:3||IONIZATION:3||VACUUM:3||SCATTERING:3||IONS:2||LUMINESCENCE PROPERTIES:2||ANISOTROPY:2||BEAMS:2||DIFFRACTION:2||DISPERSION:2||chemical vapor deposition (CVD):2||ELECTRONICSTRUCTURE:2||MOSFETS:2||SI3N4:2||DENSITY:2||LIGHT:2||PLASMAS:2||MATTER:2||nanocomposites:2||RAMANSCATTERING:2||NANOPARTICLES:2||OXIDE:2||AMPLIFIED SPONTANEOUS EMISSION:2||NM WAVELENGTH:2||GAIN:2||CARBON NANOTUBES:2||CROSSSECTIONS:2||LIGHTEMITTINGDIODES:2||PULSE:2||CARBON PLASMA:2||TISAPPHIRE LASER:2||Raman scattering:2||ROUTE:2||multilayer:2||CATHODOLUMINESCENCE:2||highresolution transmission electronic microscope (HRTEM):2||DIFFERENCEFREQUENCYGENERATION:2||CRYSTAL:2||laserproduced plasma:2||NANOCABLES:2||photoluminescence:2||MAGNETIC ALLOY SEMICONDUCTORS:2||MOLECULARBEAM EPITAXY:2||EARTHDOPED GAN:2||LASER FIELDS:2||CHIRPEDPULSEAMPLIFICATION:2||ALN:2||GAUSSIANBEAM:2||ASSISTED CATALYTIC GROWTH:2||BLUE:2||NANOSTRUCTURES:2||MAGNETOELECTRONICS:2||MICROSCOPY:2||ELECTROLUMINESCENCE:2||LASERPULSES:2||GaN nanowires:2||GALLIUM NITRIDE NANOWIRES:2||GAMNN:2||NANOTUBES:2||PHYSICS:2||Femtosecond laser:2||parametric oscillators and amplifiers:1||ultrafast lasers:1||VALENCE:1||nanowires:1||DILUTED MAGNETIC SEMICONDUCTOR:1||LUMINESCENCE:1||Density modulation:1||Energy modulation:1||Current enhanced SASE free electron laser:1||Undulator radiation:1||FREEELECTRON LASERS:1||ULTRATHIN FERROMAGNETICFILMS:1||OXIDEFILMS:1||ABLATION:1||COMPONENT:1||METAL:1||innershell excited states:1||Nelike ions:1||TRANSITIONS:1||XUV spectrometer:1||DIAGNOSTICS:1||Xray scattering:1||MO/SI:1||pulsed laser deposition:1||KEV IMPACT ENERGIES:1||vacuum electron acceleration:1||HIGHINTENSITY LASER:1||JUNCTIONS:1||LOWTEMPERATURE GROWTH:1||nanocrystalline materials:1||MOLECULAR PHOTOIONIZATION:1||LOCALIZATION:1||DEUTERIUM CLUSTERS:1||EXPLOSIONS:1||REGENERATIVE AMPLIFIERS:1||RAREGASES:1||THz radiation:1||FREEELECTRON LASER:1||REALTIME OBSERVATION:1||TARGET:1||photoionized plasmas:1||fs Xray laser:1||emission profile:1||HIGHORDER HARMONICS:1||Xray laser:1||atomic transition:1||EXCITATION:1||LASERS:1||PERFORMANCE:1||RELATIVISTIC ELECTRONS:1||BI2O3DOPED ZNO:1||INNERSHELL IONIZATION:1||Laser wakefield:1||FREQUENCY:1||SOLIDSTATE LASERS:1||Linearly polarized:1||THERMIONIC EMISSION:1||PULSE AMPLIFICATION SYSTEM:1||BIB3O6:1||NM:1||NONCOVALENT INTERACTIONS:1||CRYSTALLINE:1||INTENSITY:1||JETS:1||COHERENT:1||LINE:1||ANGULARDISTRIBUTION:1||SILVER IONS:1||magnetic anisotropy:1||DEVICES:1||Auger transitions:1||CosterKronig transitions:1||EFFICIENT:1||ELECTRONIMPACT IONIZATION:1||ULTRASHORTPULSE:1||Nanowire:1||Heterostructure:1||soft Xray reflectivity:1||PLASMA ACCELERATOR:1||ZINCOXIDE NANOWIRES:1||CHEMICALVAPORDEPOSITION:1||Electron acceleration:1||Ionization of gases:1||Delay dependent:1||MULTIPHOTON IONIZATION:1||FRAGMENTATION:1||GASJET:1||ultrafast nonlinear optics:1||CYCLE PULSES:1||KHZ:1||chemical vapor deposition:1||ferromagnetism:1||ABSORPTION:1||TERAHERTZ RADIATION:1||SCIENCE:1||FIELDS:1||ELECTRONS:1||nanomultilayer structures:1||YIELDS:1||AUGER:1||10HZ REPETITION RATE:1||MULTITERAWATT:1||SPECTROGRAPH:1||HIGHHARMONICGENERATION:1||spectroscopy:1||level population:1||PARTICLEACCELERATION:1||OPTICAL FREQUENCYMEASUREMENT:1||NANOWALLS:1||ROOMTEMPERATURE:1||AVERAGE OUTPUT POWER:1||GROUPVELOCITYMISMATCH:1||Impact ionization:1||Dynamics:1||Lasers:1||Collisional process:1||ABOVETHRESHOLD IONIZATION:1||MAINGROUP THERMOCHEMISTRY:1||dilute magnetic semiconductors:1||GACRN:1||SIZE:1||ATTOSECOND:1||Ar cluster:1||Xray astrophysics:1||photoionization:1||irons:1||normal incidence pulsed laser deposition:1||SHELLS:1||Silicon Oxide:1||gaspuff Zpinch:1||Xray:1||soft Xray reflectors:1||ESCAPE:1||ZN2SIO4:1||SILICA:1||Time delay:1||Collisional plasmas:1||MASSSPECTROMETRY:1||NUCLEARFUSION:1||PARAMETRIC AMPLIFICATION:1||LYING ELECTRONIC STATES:1||ADJUSTABLEPARAMETERS:1||MAGNETICPROPERTIES:1||LIQUIDPHASE EPITAXY:1||CEP laser:1||REGION:1||Plasma waveguide:1||AMBIENT GAS:1||DEPOSITION:1||HARMONICGENERATION:1||ENHANCEMENT:1||imaging spectrometer:1||Abel inversion:1||Water window:1||Liquid nitrogen jet:1||CHARGEEXCHANGE:1||NOBEL LECTURE:1||VARISTOR:1||EPITAXY:1||THINDISK LASER:1||HIGHREPETITIONRATE:1||Atom lasers:1||Electronimpact excitation:1||High order harmonics:1||ultrafast technology:1||PEAK POWER:1||CHARGED ALUMINUM CLUSTERS:1||GaN:1||THIN:1||Electron beam:1||INTENSE:1||Hard Xray pulse generation:1||NONLINEAR THOMSON SCATTERING:1||MULTILAYER:1||UVvisible spectrometer:1||ATOMS:1||innershell transitions:1||CORRECTED CONCAVE GRATINGS:1||DISCHARGE:1||LASERPLASMA:1||thin film:1||reflectivity:1||opacity:1||gain:1||smallangle Xray scattering:1||SOFTXRAY:1||ZINCOXIDE:1||CYGNUSX3:1||Betatron oscillation:1||ACCELERATOR:1||STRAINEDLAYER SUPERLATTICES:1||OPTICAL PARAMETRIC AMPLIFICATION:1||PASSIVE MODELOCKING:1||Collision dynamics:1||MUM:1||EXACTEXCHANGE:1||BASISSET:1||APPROXIMATION:1||OXYNITRIDES:1||Beam energy modulation:1||polarization spectroscopy:1||REORIENTATION TRANSITION:1||DEPENDENCE:1||sulfurs:1||BUILDINGBLOCKS:1||RATES:1||OPTICAL PULSES:1||toroidal mirror:1||XRAY LASER:1||CALCIUM:1||radially polarized laser:1||GRAINBOUNDARIES:1||VAPORDEPOSITION:1||Xray generation:1||MAGNETIZATION:1||Electric excitation:1||Laserinduced gas plasmas:1||Qualitative analysis:1||SCHEME:1||RADIATION:10||PULSES:8||PHOTOLUMINESCENCE:7||LASER:7||GENERATION:6||NANORODS:6||GROWTH:6||NANOWIRES:5||IMPLANTED 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SEMICONDUCTORS:2||MOLECULARBEAM EPITAXY:2||EARTHDOPED GAN:2||LASER FIELDS:2||CHIRPEDPULSEAMPLIFICATION:2||ALN:2||GAUSSIANBEAM:2||ASSISTED CATALYTIC GROWTH:2||BLUE:2||NANOSTRUCTURES:2||MAGNETOELECTRONICS:2||MICROSCOPY:2||ELECTROLUMINESCENCE:2||LASERPULSES:2||GaN nanowires:2||GALLIUM NITRIDE NANOWIRES:2||GAMNN:2||NANOTUBES:2||PHYSICS:2||Femtosecond laser:2||parametric oscillators and amplifiers:1||ultrafast lasers:1||VALENCE:1||nanowires:1||DILUTED MAGNETIC SEMICONDUCTOR:1||LUMINESCENCE:1||Density modulation:1||Energy modulation:1||Current enhanced SASE free electron laser:1||Undulator radiation:1||FREEELECTRON LASERS:1||ULTRATHIN FERROMAGNETICFILMS:1||OXIDEFILMS:1||ABLATION:1||COMPONENT:1||METAL:1||innershell excited states:1||Nelike ions:1||TRANSITIONS:1||XUV spectrometer:1||DIAGNOSTICS:1||Xray scattering:1||MO/SI:1||pulsed laser deposition:1||KEV IMPACT ENERGIES:1||vacuum electron acceleration:1||HIGHINTENSITY LASER:1||JUNCTIONS:1||LOWTEMPERATURE GROWTH:1||nanocrystalline materials:1||MOLECULAR PHOTOIONIZATION:1||LOCALIZATION:1||DEUTERIUM CLUSTERS:1||EXPLOSIONS:1||REGENERATIVE AMPLIFIERS:1||RAREGASES:1||THz radiation:1||FREEELECTRON LASER:1||REALTIME OBSERVATION:1||TARGET:1||photoionized plasmas:1||fs Xray laser:1||emission profile:1||HIGHORDER HARMONICS:1||Xray laser:1||atomic transition:1||EXCITATION:1||LASERS:1||PERFORMANCE:1||RELATIVISTIC ELECTRONS:1||BI2O3DOPED ZNO:1||INNERSHELL IONIZATION:1||Laser wakefield:1||FREQUENCY:1||SOLIDSTATE LASERS:1||Linearly polarized:1||THERMIONIC EMISSION:1||PULSE AMPLIFICATION SYSTEM:1||BIB3O6:1||NM:1||NONCOVALENT INTERACTIONS:1||CRYSTALLINE:1||INTENSITY:1||JETS:1||COHERENT:1||LINE:1||ANGULARDISTRIBUTION:1||SILVER IONS:1||magnetic anisotropy:1||DEVICES:1||Auger transitions:1||CosterKronig transitions:1||EFFICIENT:1||ELECTRONIMPACT IONIZATION:1||ULTRASHORTPULSE:1||Nanowire:1||Heterostructure:1||soft Xray reflectivity:1||PLASMA ACCELERATOR:1||ZINCOXIDE NANOWIRES:1||CHEMICALVAPORDEPOSITION:1||Electron acceleration:1||Ionization of gases:1||Delay dependent:1||MULTIPHOTON IONIZATION:1||FRAGMENTATION:1||GASJET:1||ultrafast nonlinear optics:1||CYCLE PULSES:1||KHZ:1||chemical vapor deposition:1||ferromagnetism:1||ABSORPTION:1||TERAHERTZ RADIATION:1||SCIENCE:1||FIELDS:1||ELECTRONS:1||nanomultilayer structures:1||YIELDS:1||AUGER:1||10HZ REPETITION RATE:1||MULTITERAWATT:1||SPECTROGRAPH:1||HIGHHARMONICGENERATION:1||spectroscopy:1||level population:1||PARTICLEACCELERATION:1||OPTICAL FREQUENCYMEASUREMENT:1||NANOWALLS:1||ROOMTEMPERATURE:1||AVERAGE OUTPUT POWER:1||GROUPVELOCITYMISMATCH:1||Impact ionization:1||Dynamics:1||Lasers:1||Collisional process:1||ABOVETHRESHOLD IONIZATION:1||MAINGROUP THERMOCHEMISTRY:1||dilute magnetic semiconductors:1||GACRN:1||SIZE:1||ATTOSECOND:1||Ar cluster:1||Xray astrophysics:1||photoionization:1||irons:1||normal incidence pulsed laser deposition:1||SHELLS:1||Silicon Oxide:1||gaspuff Zpinch:1||Xray:1||soft Xray reflectors:1||ESCAPE:1||ZN2SIO4:1||SILICA:1||Time 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materials:1||MOLECULAR PHOTOIONIZATION:1||LOCALIZATION:1||DEUTERIUM CLUSTERS:1||EXPLOSIONS:1||REGENERATIVE AMPLIFIERS:1||RAREGASES:1||THz radiation:1||FREEELECTRON LASER:1||REALTIME OBSERVATION:1||TARGET:1||photoionized plasmas:1||fs Xray laser:1||emission profile:1||HIGHORDER HARMONICS:1||Xray laser:1||atomic transition:1||EXCITATION:1||LASERS:1||PERFORMANCE:1||RELATIVISTIC ELECTRONS:1||BI2O3DOPED ZNO:1||INNERSHELL IONIZATION:1||Laser wakefield:1||FREQUENCY:1||SOLIDSTATE LASERS:1||Linearly polarized:1||THERMIONIC EMISSION:1||PULSE AMPLIFICATION SYSTEM:1||BIB3O6:1||NM:1||NONCOVALENT INTERACTIONS:1||CRYSTALLINE:1||INTENSITY:1||JETS:1||COHERENT:1||LINE:1||ANGULARDISTRIBUTION:1||SILVER IONS:1||magnetic anisotropy:1||DEVICES:1||Auger transitions:1||CosterKronig transitions:1||EFFICIENT:1||ELECTRONIMPACT IONIZATION:1||ULTRASHORTPULSE:1||Nanowire:1||Heterostructure:1||soft Xray reflectivity:1||PLASMA ACCELERATOR:1||ZINCOXIDE NANOWIRES:1||CHEMICALVAPORDEPOSITION:1||Electron acceleration:1||Ionization of gases:1||Delay dependent:1||MULTIPHOTON IONIZATION:1||FRAGMENTATION:1||GASJET:1||ultrafast nonlinear optics:1||CYCLE PULSES:1||KHZ:1||chemical vapor deposition:1||ferromagnetism:1||ABSORPTION:1||TERAHERTZ RADIATION:1||SCIENCE:1||FIELDS:1||ELECTRONS:1||nanomultilayer structures:1||YIELDS:1||AUGER:1||10HZ REPETITION RATE:1||MULTITERAWATT:1||SPECTROGRAPH:1||HIGHHARMONICGENERATION:1||spectroscopy:1||level population:1||PARTICLEACCELERATION:1||OPTICAL FREQUENCYMEASUREMENT:1||NANOWALLS:1||ROOMTEMPERATURE:1||AVERAGE OUTPUT POWER:1||GROUPVELOCITYMISMATCH:1||Impact ionization:1||Dynamics:1||Lasers:1||Collisional process:1||ABOVETHRESHOLD IONIZATION:1||MAINGROUP THERMOCHEMISTRY:1||dilute magnetic semiconductors:1||GACRN:1||SIZE:1||ATTOSECOND:1||Ar cluster:1||Xray astrophysics:1||photoionization:1||irons:1||normal incidence pulsed laser deposition:1||SHELLS:1||Silicon Oxide:1||gaspuff Zpinch:1||Xray:1||soft Xray reflectors:1||ESCAPE:1||ZN2SIO4:1||SILICA:1||Time delay:1||Collisional plasmas:1||MASSSPECTROMETRY:1||NUCLEARFUSION:1||PARAMETRIC AMPLIFICATION:1||LYING ELECTRONIC STATES:1||ADJUSTABLEPARAMETERS:1||MAGNETICPROPERTIES:1||LIQUIDPHASE EPITAXY:1||CEP laser:1||REGION:1||Plasma waveguide:1||AMBIENT GAS:1||DEPOSITION:1||HARMONICGENERATION:1||ENHANCEMENT:1||imaging spectrometer:1||Abel inversion:1||Water window:1||Liquid nitrogen jet:1||CHARGEEXCHANGE:1||NOBEL LECTURE:1||VARISTOR:1||EPITAXY:1||THINDISK LASER:1||HIGHREPETITIONRATE:1||Atom lasers:1||Electronimpact excitation:1||High order harmonics:1||ultrafast technology:1||PEAK POWER:1||CHARGED ALUMINUM CLUSTERS:1||GaN:1||THIN:1||Electron beam:1||INTENSE:1||Hard Xray pulse generation:1||NONLINEAR THOMSON SCATTERING:1||MULTILAYER:1||UVvisible spectrometer:1||ATOMS:1||innershell transitions:1||CORRECTED CONCAVE GRATINGS:1||DISCHARGE:1||LASERPLASMA:1||thin film:1||reflectivity:1||opacity:1||gain:1||smallangle Xray scattering:1||SOFTXRAY:1||ZINCOXIDE:1||CYGNUSX3:1||Betatron oscillation:1||ACCELERATOR:1||STRAINEDLAYER SUPERLATTICES:1||OPTICAL PARAMETRIC AMPLIFICATION:1||PASSIVE MODELOCKING:1||Collision dynamics:1||MUM:1||EXACTEXCHANGE:1||BASISSET:1||APPROXIMATION:1||OXYNITRIDES:1||Beam energy modulation:1||polarization spectroscopy:1||REORIENTATION TRANSITION:1||DEPENDENCE:1||sulfurs:1||BUILDINGBLOCKS:1||RATES:1||OPTICAL PULSES:1||toroidal mirror:1||XRAY LASER:1||CALCIUM:1||radially polarized laser:1||GRAINBOUNDARIES:1||VAPORDEPOSITION:1||Xray generation:1||MAGNETIZATION:1||Electric excitation:1||Laserinduced gas plasmas:1||Qualitative analysis:1||SCHEME:1||RADIATION:10||PULSES:8||PHOTOLUMINESCENCE:7||LASER:7||GENERATION:6||NANORODS:6||GROWTH:6||NANOWIRES:5||IMPLANTED GAN:5||SPECTROSCOPY:5||THINFILMS:4||DYNAMICS:4||SILICON:4||EXTREMEULTRAVIOLET:4||AMPLIFICATION:4||PRESSURE:4||PHASE:4||OPTICALPROPERTIES:4||SYSTEM:4||EMISSION:4||FEL:3||N2O:3||FILMS:3||OPTICS:3||SPECTRA:3||FIELD:3||MIRRORS:3||ARRAYS:3||CLUSTERS:3||SIO2:3||IONIZATION:3||VACUUM:3||SCATTERING:3||IONS:2||LUMINESCENCE PROPERTIES:2||ANISOTROPY:2||BEAMS:2||DIFFRACTION:2||DISPERSION:2||chemical vapor deposition (CVD):2||ELECTRONICSTRUCTURE:2||MOSFETS:2||SI3N4:2||DENSITY:2||LIGHT:2||PLASMAS:2||MATTER:2||nanocomposites:2||RAMANSCATTERING:2||NANOPARTICLES:2||OXIDE:2||AMPLIFIED SPONTANEOUS EMISSION:2||NM WAVELENGTH:2||GAIN:2||CARBON NANOTUBES:2||CROSSSECTIONS:2||LIGHTEMITTINGDIODES:2||PULSE:2||CARBON PLASMA:2||TISAPPHIRE LASER:2||Raman scattering:2||ROUTE:2||multilayer:2||CATHODOLUMINESCENCE:2||highresolution transmission electronic microscope (HRTEM):2||DIFFERENCEFREQUENCYGENERATION:2||CRYSTAL:2||laserproduced plasma:2||NANOCABLES:2||photoluminescence:2||MAGNETIC ALLOY SEMICONDUCTORS:2||MOLECULARBEAM EPITAXY:2||EARTHDOPED GAN:2||LASER FIELDS:2||CHIRPEDPULSEAMPLIFICATION:2||ALN:2||GAUSSIANBEAM:2||ASSISTED CATALYTIC GROWTH:2||BLUE:2||NANOSTRUCTURES:2||MAGNETOELECTRONICS:2||MICROSCOPY:2||ELECTROLUMINESCENCE:2||LASERPULSES:2||GaN nanowires:2||GALLIUM NITRIDE NANOWIRES:2||GAMNN:2||NANOTUBES:2||PHYSICS:2||Femtosecond laser:2||parametric oscillators and amplifiers:1||ultrafast lasers:1||VALENCE:1||nanowires:1||DILUTED MAGNETIC SEMICONDUCTOR:1||LUMINESCENCE:1||Density modulation:1||Energy modulation:1||Current enhanced SASE free electron laser:1||Undulator radiation:1||FREEELECTRON LASERS:1||ULTRATHIN FERROMAGNETICFILMS:1||OXIDEFILMS:1||ABLATION:1||COMPONENT:1||METAL:1||innershell excited states:1||Nelike ions:1||TRANSITIONS:1||XUV spectrometer:1||DIAGNOSTICS:1||Xray scattering:1||MO/SI:1||pulsed laser deposition:1||KEV IMPACT ENERGIES:1||vacuum electron acceleration:1||HIGHINTENSITY LASER:1||JUNCTIONS:1||LOWTEMPERATURE GROWTH:1||nanocrystalline materials:1||MOLECULAR PHOTOIONIZATION:1||LOCALIZATION:1||DEUTERIUM CLUSTERS:1||EXPLOSIONS:1||REGENERATIVE AMPLIFIERS:1||RAREGASES:1||THz radiation:1||FREEELECTRON LASER:1||REALTIME OBSERVATION:1||TARGET:1||photoionized plasmas:1||fs Xray laser:1||emission profile:1||HIGHORDER HARMONICS:1||Xray laser:1||atomic transition:1||EXCITATION:1||LASERS:1||PERFORMANCE:1||RELATIVISTIC ELECTRONS:1||BI2O3DOPED ZNO:1||INNERSHELL IONIZATION:1||Laser wakefield:1||FREQUENCY:1||SOLIDSTATE LASERS:1||Linearly polarized:1||THERMIONIC EMISSION:1||PULSE AMPLIFICATION SYSTEM:1||BIB3O6:1||NM:1||NONCOVALENT INTERACTIONS:1||CRYSTALLINE:1||INTENSITY:1||JETS:1||COHERENT:1||LINE:1||ANGULARDISTRIBUTION:1||SILVER IONS:1||magnetic anisotropy:1||DEVICES:1||Auger transitions:1||CosterKronig transitions:1||EFFICIENT:1||ELECTRONIMPACT IONIZATION:1||ULTRASHORTPULSE:1||Nanowire:1||Heterostructure:1||soft Xray reflectivity:1||PLASMA ACCELERATOR:1||ZINCOXIDE NANOWIRES:1||CHEMICALVAPORDEPOSITION:1||Electron acceleration:1||Ionization of gases:1||Delay dependent:1||MULTIPHOTON IONIZATION:1||FRAGMENTATION:1||GASJET:1||ultrafast nonlinear optics:1||CYCLE PULSES:1||KHZ:1||chemical vapor deposition:1||ferromagnetism:1||ABSORPTION:1||TERAHERTZ RADIATION:1||SCIENCE:1||FIELDS:1||ELECTRONS:1||nanomultilayer structures:1||YIELDS:1||AUGER:1||10HZ REPETITION RATE:1||MULTITERAWATT:1||SPECTROGRAPH:1||HIGHHARMONICGENERATION:1||spectroscopy:1||level population:1||PARTICLEACCELERATION:1||OPTICAL FREQUENCYMEASUREMENT:1||NANOWALLS:1||ROOMTEMPERATURE:1||AVERAGE OUTPUT POWER:1||GROUPVELOCITYMISMATCH:1||Impact ionization:1||Dynamics:1||Lasers:1||Collisional process:1||ABOVETHRESHOLD IONIZATION:1||MAINGROUP THERMOCHEMISTRY:1||dilute magnetic semiconductors:1||GACRN:1||SIZE:1||ATTOSECOND:1||Ar cluster:1||Xray astrophysics:1||photoionization:1||irons:1||normal incidence pulsed laser deposition:1||SHELLS:1||Silicon Oxide:1||gaspuff Zpinch:1||Xray:1||soft Xray reflectors:1||ESCAPE:1||ZN2SIO4:1||SILICA:1||Time delay:1||Collisional plasmas:1||MASSSPECTROMETRY:1||NUCLEARFUSION:1||PARAMETRIC AMPLIFICATION:1||LYING ELECTRONIC STATES:1||ADJUSTABLEPARAMETERS:1||MAGNETICPROPERTIES:1||LIQUIDPHASE EPITAXY:1||CEP laser:1||REGION:1||Plasma waveguide:1||AMBIENT GAS:1||DEPOSITION:1||HARMONICGENERATION:1||ENHANCEMENT:1||imaging spectrometer:1||Abel inversion:1||Water window:1||Liquid nitrogen jet:1||CHARGEEXCHANGE:1||NOBEL LECTURE:1||VARISTOR:1||EPITAXY:1||THINDISK LASER:1||HIGHREPETITIONRATE:1||Atom lasers:1||Electronimpact excitation:1||High order harmonics:1||ultrafast technology:1||PEAK POWER:1||CHARGED ALUMINUM CLUSTERS:1||GaN:1||THIN:1||Electron beam:1||INTENSE:1||Hard Xray pulse generation:1||NONLINEAR THOMSON SCATTERING:1||MULTILAYER:1||UVvisible spectrometer:1||ATOMS:1||innershell transitions:1||CORRECTED CONCAVE GRATINGS:1||DISCHARGE:1||LASERPLASMA:1||thin film:1||reflectivity:1||opacity:1||gain:1||smallangle Xray scattering:1||SOFTXRAY:1||ZINCOXIDE:1||CYGNUSX3:1||Betatron oscillation:1||ACCELERATOR:1||STRAINEDLAYER SUPERLATTICES:1||OPTICAL PARAMETRIC AMPLIFICATION:1||PASSIVE MODELOCKING:1||Collision dynamics:1||MUM:1||EXACTEXCHANGE:1||BASISSET:1||APPROXIMATION:1||OXYNITRIDES:1||Beam energy modulation:1||polarization spectroscopy:1||REORIENTATION TRANSITION:1||DEPENDENCE:1||sulfurs:1||BUILDINGBLOCKS:1||RATES:1||OPTICAL PULSES:1||toroidal mirror:1||XRAY LASER:1||CALCIUM:1||radially polarized laser:1||GRAINBOUNDARIES:1||VAPORDEPOSITION:1||Xray generation:1||MAGNETIZATION:1||Electric excitation:1||Laserinduced gas plasmas:1||Qualitative analysis:1||SCHEME:1||RADIATION:10||PULSES:8||PHOTOLUMINESCENCE:7||LASER:7||GENERATION:6||NANORODS:6||GROWTH:6||NANOWIRES:5||IMPLANTED 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SEMICONDUCTORS:2||MOLECULARBEAM EPITAXY:2||EARTHDOPED GAN:2||LASER FIELDS:2||CHIRPEDPULSEAMPLIFICATION:2||ALN:2||GAUSSIANBEAM:2||ASSISTED CATALYTIC GROWTH:2||BLUE:2||NANOSTRUCTURES:2||MAGNETOELECTRONICS:2||MICROSCOPY:2||ELECTROLUMINESCENCE:2||LASERPULSES:2||GaN nanowires:2||GALLIUM NITRIDE NANOWIRES:2||GAMNN:2||NANOTUBES:2||PHYSICS:2||Femtosecond laser:2||parametric oscillators and amplifiers:1||ultrafast lasers:1||VALENCE:1||nanowires:1||DILUTED MAGNETIC SEMICONDUCTOR:1||LUMINESCENCE:1||Density modulation:1||Energy modulation:1||Current enhanced SASE free electron laser:1||Undulator radiation:1||FREEELECTRON LASERS:1||ULTRATHIN FERROMAGNETICFILMS:1||OXIDEFILMS:1||ABLATION:1||COMPONENT:1||METAL:1||innershell excited states:1||Nelike ions:1||TRANSITIONS:1||XUV spectrometer:1||DIAGNOSTICS:1||Xray scattering:1||MO/SI:1||pulsed laser deposition:1||KEV IMPACT ENERGIES:1||vacuum electron acceleration:1||HIGHINTENSITY LASER:1||JUNCTIONS:1||LOWTEMPERATURE GROWTH:1||nanocrystalline materials:1||MOLECULAR PHOTOIONIZATION:1||LOCALIZATION:1||DEUTERIUM CLUSTERS:1||EXPLOSIONS:1||REGENERATIVE AMPLIFIERS:1||RAREGASES:1||THz radiation:1||FREEELECTRON LASER:1||REALTIME OBSERVATION:1||TARGET:1||photoionized plasmas:1||fs Xray laser:1||emission profile:1||HIGHORDER HARMONICS:1||Xray laser:1||atomic transition:1||EXCITATION:1||LASERS:1||PERFORMANCE:1||RELATIVISTIC ELECTRONS:1||BI2O3DOPED ZNO:1||INNERSHELL IONIZATION:1||Laser wakefield:1||FREQUENCY:1||SOLIDSTATE LASERS:1||Linearly polarized:1||THERMIONIC EMISSION:1||PULSE AMPLIFICATION SYSTEM:1||BIB3O6:1||NM:1||NONCOVALENT INTERACTIONS:1||CRYSTALLINE:1||INTENSITY:1||JETS:1||COHERENT:1||LINE:1||ANGULARDISTRIBUTION:1||SILVER IONS:1||magnetic anisotropy:1||DEVICES:1||Auger transitions:1||CosterKronig transitions:1||EFFICIENT:1||ELECTRONIMPACT IONIZATION:1||ULTRASHORTPULSE:1||Nanowire:1||Heterostructure:1||soft Xray reflectivity:1||PLASMA ACCELERATOR:1||ZINCOXIDE NANOWIRES:1||CHEMICALVAPORDEPOSITION:1||Electron acceleration:1||Ionization of gases:1||Delay dependent:1||MULTIPHOTON IONIZATION:1||FRAGMENTATION:1||GASJET:1||ultrafast nonlinear optics:1||CYCLE PULSES:1||KHZ:1||chemical vapor deposition:1||ferromagnetism:1||ABSORPTION:1||TERAHERTZ RADIATION:1||SCIENCE:1||FIELDS:1||ELECTRONS:1||nanomultilayer structures:1||YIELDS:1||AUGER:1||10HZ REPETITION RATE:1||MULTITERAWATT:1||SPECTROGRAPH:1||HIGHHARMONICGENERATION:1||spectroscopy:1||level population:1||PARTICLEACCELERATION:1||OPTICAL FREQUENCYMEASUREMENT:1||NANOWALLS:1||ROOMTEMPERATURE:1||AVERAGE OUTPUT POWER:1||GROUPVELOCITYMISMATCH:1||Impact ionization:1||Dynamics:1||Lasers:1||Collisional process:1||ABOVETHRESHOLD IONIZATION:1||MAINGROUP THERMOCHEMISTRY:1||dilute magnetic semiconductors:1||GACRN:1||SIZE:1||ATTOSECOND:1||Ar cluster:1||Xray astrophysics:1||photoionization:1||irons:1||normal incidence pulsed laser deposition:1||SHELLS:1||Silicon Oxide:1||gaspuff Zpinch:1||Xray:1||soft Xray reflectors:1||ESCAPE:1||ZN2SIO4:1||SILICA:1||Time 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materials:1||MOLECULAR PHOTOIONIZATION:1||LOCALIZATION:1||DEUTERIUM CLUSTERS:1||EXPLOSIONS:1||REGENERATIVE AMPLIFIERS:1||RAREGASES:1||THz radiation:1||FREEELECTRON LASER:1||REALTIME OBSERVATION:1||TARGET:1||photoionized plasmas:1||fs Xray laser:1||emission profile:1||HIGHORDER HARMONICS:1||Xray laser:1||atomic transition:1||EXCITATION:1||LASERS:1||PERFORMANCE:1||RELATIVISTIC ELECTRONS:1||BI2O3DOPED ZNO:1||INNERSHELL IONIZATION:1||Laser wakefield:1||FREQUENCY:1||SOLIDSTATE LASERS:1||Linearly polarized:1||THERMIONIC EMISSION:1||PULSE AMPLIFICATION SYSTEM:1||BIB3O6:1||NM:1||NONCOVALENT INTERACTIONS:1||CRYSTALLINE:1||INTENSITY:1||JETS:1||COHERENT:1||LINE:1||ANGULARDISTRIBUTION:1||SILVER IONS:1||magnetic anisotropy:1||DEVICES:1||Auger transitions:1||CosterKronig transitions:1||EFFICIENT:1||ELECTRONIMPACT IONIZATION:1||ULTRASHORTPULSE:1||Nanowire:1||Heterostructure:1||soft Xray reflectivity:1||PLASMA ACCELERATOR:1||ZINCOXIDE NANOWIRES:1||CHEMICALVAPORDEPOSITION:1||Electron acceleration:1||Ionization of gases:1||Delay dependent:1||MULTIPHOTON IONIZATION:1||FRAGMENTATION:1||GASJET:1||ultrafast nonlinear optics:1||CYCLE PULSES:1||KHZ:1||chemical vapor deposition:1||ferromagnetism:1||ABSORPTION:1||TERAHERTZ RADIATION:1||SCIENCE:1||FIELDS:1||ELECTRONS:1||nanomultilayer structures:1||YIELDS:1||AUGER:1||10HZ REPETITION RATE:1||MULTITERAWATT:1||SPECTROGRAPH:1||HIGHHARMONICGENERATION:1||spectroscopy:1||level population:1||PARTICLEACCELERATION:1||OPTICAL FREQUENCYMEASUREMENT:1||NANOWALLS:1||ROOMTEMPERATURE:1||AVERAGE OUTPUT POWER:1||GROUPVELOCITYMISMATCH:1||Impact ionization:1||Dynamics:1||Lasers:1||Collisional process:1||ABOVETHRESHOLD IONIZATION:1||MAINGROUP THERMOCHEMISTRY:1||dilute magnetic semiconductors:1||GACRN:1||SIZE:1||ATTOSECOND:1||Ar cluster:1||Xray astrophysics:1||photoionization:1||irons:1||normal incidence pulsed laser deposition:1||SHELLS:1||Silicon Oxide:1||gaspuff Zpinch:1||Xray:1||soft Xray reflectors:1||ESCAPE:1||ZN2SIO4:1||SILICA:1||Time delay:1||Collisional plasmas:1||MASSSPECTROMETRY:1||NUCLEARFUSION:1||PARAMETRIC AMPLIFICATION:1||LYING ELECTRONIC STATES:1||ADJUSTABLEPARAMETERS:1||MAGNETICPROPERTIES:1||LIQUIDPHASE EPITAXY:1||CEP laser:1||REGION:1||Plasma waveguide:1||AMBIENT GAS:1||DEPOSITION:1||HARMONICGENERATION:1||ENHANCEMENT:1||imaging spectrometer:1||Abel inversion:1||Water window:1||Liquid nitrogen jet:1||CHARGEEXCHANGE:1||NOBEL LECTURE:1||VARISTOR:1||EPITAXY:1||THINDISK LASER:1||HIGHREPETITIONRATE:1||Atom lasers:1||Electronimpact excitation:1||High order harmonics:1||ultrafast technology:1||PEAK POWER:1||CHARGED ALUMINUM CLUSTERS:1||GaN:1||THIN:1||Electron beam:1||INTENSE:1||Hard Xray pulse generation:1||NONLINEAR THOMSON SCATTERING:1||MULTILAYER:1||UVvisible spectrometer:1||ATOMS:1||innershell transitions:1||CORRECTED CONCAVE GRATINGS:1||DISCHARGE:1||LASERPLASMA:1||thin film:1||reflectivity:1||opacity:1||gain:1||smallangle Xray scattering:1||SOFTXRAY:1||ZINCOXIDE:1||CYGNUSX3:1||Betatron oscillation:1||ACCELERATOR:1||STRAINEDLAYER SUPERLATTICES:1||OPTICAL PARAMETRIC AMPLIFICATION:1||PASSIVE MODELOCKING:1||Collision dynamics:1||MUM:1||EXACTEXCHANGE:1||BASISSET:1||APPROXIMATION:1||OXYNITRIDES:1||Beam energy modulation:1||polarization spectroscopy:1||REORIENTATION TRANSITION:1||DEPENDENCE:1||sulfurs:1||BUILDINGBLOCKS:1||RATES:1||OPTICAL PULSES:1||toroidal mirror:1||XRAY LASER:1||CALCIUM:1||radially polarized laser:1||GRAINBOUNDARIES:1||VAPORDEPOSITION:1||Xray generation:1||MAGNETIZATION:1||Electric excitation:1||Laserinduced gas plasmas:1||Qualitative analysis:1||SCHEME:1||RADIATION:10||PULSES:8||PHOTOLUMINESCENCE:7||LASER:7||GENERATION:6||NANORODS:6||GROWTH:6||NANOWIRES:5||IMPLANTED GAN:5||SPECTROSCOPY:5||THINFILMS:4||DYNAMICS:4||SILICON:4||EXTREMEULTRAVIOLET:4||AMPLIFICATION:4||PRESSURE:4||PHASE:4||OPTICALPROPERTIES:4||SYSTEM:4||EMISSION:4||FEL:3||N2O:3||FILMS:3||OPTICS:3||SPECTRA:3||FIELD:3||MIRRORS:3||ARRAYS:3||CLUSTERS:3||SIO2:3||IONIZATION:3||VACUUM:3||SCATTERING:3||IONS:2||LUMINESCENCE PROPERTIES:2||ANISOTROPY:2||BEAMS:2||DIFFRACTION:2||DISPERSION:2||chemical vapor deposition (CVD):2||ELECTRONICSTRUCTURE:2||MOSFETS:2||SI3N4:2||DENSITY:2||LIGHT:2||PLASMAS:2||MATTER:2||nanocomposites:2||RAMANSCATTERING:2||NANOPARTICLES:2||OXIDE:2||AMPLIFIED SPONTANEOUS EMISSION:2||NM WAVELENGTH:2||GAIN:2||CARBON NANOTUBES:2||CROSSSECTIONS:2||LIGHTEMITTINGDIODES:2||PULSE:2||CARBON PLASMA:2||TISAPPHIRE LASER:2||Raman scattering:2||ROUTE:2||multilayer:2||CATHODOLUMINESCENCE:2||highresolution transmission electronic microscope (HRTEM):2||DIFFERENCEFREQUENCYGENERATION:2||CRYSTAL:2||laserproduced plasma:2||NANOCABLES:2||photoluminescence:2||MAGNETIC ALLOY SEMICONDUCTORS:2||MOLECULARBEAM EPITAXY:2||EARTHDOPED GAN:2||LASER FIELDS:2||CHIRPEDPULSEAMPLIFICATION:2||ALN:2||GAUSSIANBEAM:2||ASSISTED CATALYTIC GROWTH:2||BLUE:2||NANOSTRUCTURES:2||MAGNETOELECTRONICS:2||MICROSCOPY:2||ELECTROLUMINESCENCE:2||LASERPULSES:2||GaN nanowires:2||GALLIUM NITRIDE NANOWIRES:2||GAMNN:2||NANOTUBES:2||PHYSICS:2||Femtosecond laser:2||parametric oscillators and amplifiers:1||ultrafast lasers:1||VALENCE:1||nanowires:1||DILUTED MAGNETIC SEMICONDUCTOR:1||LUMINESCENCE:1||Density modulation:1||Energy modulation:1||Current enhanced SASE free electron laser:1||Undulator radiation:1||FREEELECTRON LASERS:1||ULTRATHIN FERROMAGNETICFILMS:1||OXIDEFILMS:1||ABLATION:1||COMPONENT:1||METAL:1||innershell excited states:1||Nelike ions:1||TRANSITIONS:1||XUV spectrometer:1||DIAGNOSTICS:1||Xray scattering:1||MO/SI:1||pulsed laser deposition:1||KEV IMPACT ENERGIES:1||vacuum electron acceleration:1||HIGHINTENSITY LASER:1||JUNCTIONS:1||LOWTEMPERATURE GROWTH:1||nanocrystalline materials:1||MOLECULAR PHOTOIONIZATION:1||LOCALIZATION:1||DEUTERIUM CLUSTERS:1||EXPLOSIONS:1||REGENERATIVE AMPLIFIERS:1||RAREGASES:1||THz radiation:1||FREEELECTRON LASER:1||REALTIME OBSERVATION:1||TARGET:1||photoionized plasmas:1||fs Xray laser:1||emission profile:1||HIGHORDER HARMONICS:1||Xray laser:1||atomic transition:1||EXCITATION:1||LASERS:1||PERFORMANCE:1||RELATIVISTIC ELECTRONS:1||BI2O3DOPED ZNO:1||INNERSHELL IONIZATION:1||Laser wakefield:1||FREQUENCY:1||SOLIDSTATE LASERS:1||Linearly polarized:1||THERMIONIC EMISSION:1||PULSE AMPLIFICATION SYSTEM:1||BIB3O6:1||NM:1||NONCOVALENT INTERACTIONS:1||CRYSTALLINE:1||INTENSITY:1||JETS:1||COHERENT:1||LINE:1||ANGULARDISTRIBUTION:1||SILVER IONS:1||magnetic anisotropy:1||DEVICES:1||Auger transitions:1||CosterKronig transitions:1||EFFICIENT:1||ELECTRONIMPACT IONIZATION:1||ULTRASHORTPULSE:1||Nanowire:1||Heterostructure:1||soft Xray reflectivity:1||PLASMA ACCELERATOR:1||ZINCOXIDE NANOWIRES:1||CHEMICALVAPORDEPOSITION:1||Electron acceleration:1||Ionization of gases:1||Delay dependent:1||MULTIPHOTON IONIZATION:1||FRAGMENTATION:1||GASJET:1||ultrafast nonlinear optics:1||CYCLE PULSES:1||KHZ:1||chemical vapor deposition:1||ferromagnetism:1||ABSORPTION:1||TERAHERTZ RADIATION:1||SCIENCE:1||FIELDS:1||ELECTRONS:1||nanomultilayer structures:1||YIELDS:1||AUGER:1||10HZ REPETITION RATE:1||MULTITERAWATT:1||SPECTROGRAPH:1||HIGHHARMONICGENERATION:1||spectroscopy:1||level population:1||PARTICLEACCELERATION:1||OPTICAL FREQUENCYMEASUREMENT:1||NANOWALLS:1||ROOMTEMPERATURE:1||AVERAGE OUTPUT POWER:1||GROUPVELOCITYMISMATCH:1||Impact ionization:1||Dynamics:1||Lasers:1||Collisional process:1||ABOVETHRESHOLD IONIZATION:1||MAINGROUP THERMOCHEMISTRY:1||dilute magnetic semiconductors:1||GACRN:1||SIZE:1||ATTOSECOND:1||Ar cluster:1||Xray astrophysics:1||photoionization:1||irons:1||normal incidence pulsed laser deposition:1||SHELLS:1||Silicon Oxide:1||gaspuff Zpinch:1||Xray:1||soft Xray reflectors:1||ESCAPE:1||ZN2SIO4:1||SILICA:1||Time delay:1||Collisional plasmas:1||MASSSPECTROMETRY:1||NUCLEARFUSION:1||PARAMETRIC AMPLIFICATION:1||LYING ELECTRONIC STATES:1||ADJUSTABLEPARAMETERS:1||MAGNETICPROPERTIES:1||LIQUIDPHASE EPITAXY:1||CEP laser:1||REGION:1||Plasma waveguide:1||AMBIENT GAS:1||DEPOSITION:1||HARMONICGENERATION:1||ENHANCEMENT:1||imaging spectrometer:1||Abel inversion:1||Water window:1||Liquid nitrogen jet:1||CHARGEEXCHANGE:1||NOBEL LECTURE:1||VARISTOR:1||EPITAXY:1||THINDISK LASER:1||HIGHREPETITIONRATE:1||Atom lasers:1||Electronimpact excitation:1||High order harmonics:1||ultrafast technology:1||PEAK POWER:1||CHARGED ALUMINUM CLUSTERS:1||GaN:1||THIN:1||Electron beam:1||INTENSE:1||Hard Xray pulse generation:1||NONLINEAR THOMSON SCATTERING:1||MULTILAYER:1||UVvisible spectrometer:1||ATOMS:1||innershell transitions:1||CORRECTED CONCAVE GRATINGS:1||DISCHARGE:1||LASERPLASMA:1||thin film:1||reflectivity:1||opacity:1||gain:1||smallangle Xray scattering:1||SOFTXRAY:1||ZINCOXIDE:1||CYGNUSX3:1||Betatron oscillation:1||ACCELERATOR:1||STRAINEDLAYER SUPERLATTICES:1||OPTICAL PARAMETRIC AMPLIFICATION:1||PASSIVE MODELOCKING:1||Collision dynamics:1||MUM:1||EXACTEXCHANGE:1||BASISSET:1||APPROXIMATION:1||OXYNITRIDES:1||Beam energy modulation:1||polarization spectroscopy:1||REORIENTATION TRANSITION:1||DEPENDENCE:1||sulfurs:1||BUILDINGBLOCKS:1||RATES:1||OPTICAL PULSES:1||toroidal mirror:1||XRAY LASER:1||CALCIUM:1||radially polarized laser:1||GRAINBOUNDARIES:1||VAPORDEPOSITION:1||Xray generation:1||MAGNETIZATION:1||Electric excitation:1||Laserinduced gas plasmas:1||Qualitative analysis:1||SCHEME:1||RADIATION:10||PULSES:8||PHOTOLUMINESCENCE:7||LASER:7||GENERATION:6||NANORODS:6||GROWTH:6||NANOWIRES:5||IMPLANTED 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SEMICONDUCTORS:2||MOLECULARBEAM EPITAXY:2||EARTHDOPED GAN:2||LASER FIELDS:2||CHIRPEDPULSEAMPLIFICATION:2||ALN:2||GAUSSIANBEAM:2||ASSISTED CATALYTIC GROWTH:2||BLUE:2||NANOSTRUCTURES:2||MAGNETOELECTRONICS:2||MICROSCOPY:2||ELECTROLUMINESCENCE:2||LASERPULSES:2||GaN nanowires:2||GALLIUM NITRIDE NANOWIRES:2||GAMNN:2||NANOTUBES:2||PHYSICS:2||Femtosecond laser:2||parametric oscillators and amplifiers:1||ultrafast lasers:1||VALENCE:1||nanowires:1||DILUTED MAGNETIC SEMICONDUCTOR:1||LUMINESCENCE:1||Density modulation:1||Energy modulation:1||Current enhanced SASE free electron laser:1||Undulator radiation:1||FREEELECTRON LASERS:1||ULTRATHIN FERROMAGNETICFILMS:1||OXIDEFILMS:1||ABLATION:1||COMPONENT:1||METAL:1||innershell excited states:1||Nelike ions:1||TRANSITIONS:1||XUV spectrometer:1||DIAGNOSTICS:1||Xray scattering:1||MO/SI:1||pulsed laser deposition:1||KEV IMPACT ENERGIES:1||vacuum electron acceleration:1||HIGHINTENSITY LASER:1||JUNCTIONS:1||LOWTEMPERATURE GROWTH:1||nanocrystalline materials:1||MOLECULAR PHOTOIONIZATION:1||LOCALIZATION:1||DEUTERIUM CLUSTERS:1||EXPLOSIONS:1||REGENERATIVE AMPLIFIERS:1||RAREGASES:1||THz radiation:1||FREEELECTRON LASER:1||REALTIME OBSERVATION:1||TARGET:1||photoionized plasmas:1||fs Xray laser:1||emission profile:1||HIGHORDER HARMONICS:1||Xray laser:1||atomic transition:1||EXCITATION:1||LASERS:1||PERFORMANCE:1||RELATIVISTIC ELECTRONS:1||BI2O3DOPED ZNO:1||INNERSHELL IONIZATION:1||Laser wakefield:1||FREQUENCY:1||SOLIDSTATE LASERS:1||Linearly polarized:1||THERMIONIC EMISSION:1||PULSE AMPLIFICATION SYSTEM:1||BIB3O6:1||NM:1||NONCOVALENT INTERACTIONS:1||CRYSTALLINE:1||INTENSITY:1||JETS:1||COHERENT:1||LINE:1||ANGULARDISTRIBUTION:1||SILVER IONS:1||magnetic anisotropy:1||DEVICES:1||Auger transitions:1||CosterKronig transitions:1||EFFICIENT:1||ELECTRONIMPACT IONIZATION:1||ULTRASHORTPULSE:1||Nanowire:1||Heterostructure:1||soft Xray reflectivity:1||PLASMA ACCELERATOR:1||ZINCOXIDE NANOWIRES:1||CHEMICALVAPORDEPOSITION:1||Electron acceleration:1||Ionization of gases:1||Delay dependent:1||MULTIPHOTON IONIZATION:1||FRAGMENTATION:1||GASJET:1||ultrafast nonlinear optics:1||CYCLE PULSES:1||KHZ:1||chemical vapor deposition:1||ferromagnetism:1||ABSORPTION:1||TERAHERTZ RADIATION:1||SCIENCE:1||FIELDS:1||ELECTRONS:1||nanomultilayer structures:1||YIELDS:1||AUGER:1||10HZ REPETITION RATE:1||MULTITERAWATT:1||SPECTROGRAPH:1||HIGHHARMONICGENERATION:1||spectroscopy:1||level population:1||PARTICLEACCELERATION:1||OPTICAL FREQUENCYMEASUREMENT:1||NANOWALLS:1||ROOMTEMPERATURE:1||AVERAGE OUTPUT POWER:1||GROUPVELOCITYMISMATCH:1||Impact ionization:1||Dynamics:1||Lasers:1||Collisional process:1||ABOVETHRESHOLD IONIZATION:1||MAINGROUP THERMOCHEMISTRY:1||dilute magnetic semiconductors:1||GACRN:1||SIZE:1||ATTOSECOND:1||Ar cluster:1||Xray astrophysics:1||photoionization:1||irons:1||normal incidence pulsed laser deposition:1||SHELLS:1||Silicon Oxide:1||gaspuff Zpinch:1||Xray:1||soft Xray reflectors:1||ESCAPE:1||ZN2SIO4:1||SILICA:1||Time 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materials:1||MOLECULAR PHOTOIONIZATION:1||LOCALIZATION:1||DEUTERIUM CLUSTERS:1||EXPLOSIONS:1||REGENERATIVE AMPLIFIERS:1||RAREGASES:1||THz radiation:1||FREEELECTRON LASER:1||REALTIME OBSERVATION:1||TARGET:1||photoionized plasmas:1||fs Xray laser:1||emission profile:1||HIGHORDER HARMONICS:1||Xray laser:1||atomic transition:1||EXCITATION:1||LASERS:1||PERFORMANCE:1||RELATIVISTIC ELECTRONS:1||BI2O3DOPED ZNO:1||INNERSHELL IONIZATION:1||Laser wakefield:1||FREQUENCY:1||SOLIDSTATE LASERS:1||Linearly polarized:1||THERMIONIC EMISSION:1||PULSE AMPLIFICATION SYSTEM:1||BIB3O6:1||NM:1||NONCOVALENT INTERACTIONS:1||CRYSTALLINE:1||INTENSITY:1||JETS:1||COHERENT:1||LINE:1||ANGULARDISTRIBUTION:1||SILVER IONS:1||magnetic anisotropy:1||DEVICES:1||Auger transitions:1||CosterKronig transitions:1||EFFICIENT:1||ELECTRONIMPACT IONIZATION:1||ULTRASHORTPULSE:1||Nanowire:1||Heterostructure:1||soft Xray reflectivity:1||PLASMA ACCELERATOR:1||ZINCOXIDE NANOWIRES:1||CHEMICALVAPORDEPOSITION:1||Electron acceleration:1||Ionization of gases:1||Delay dependent:1||MULTIPHOTON IONIZATION:1||FRAGMENTATION:1||GASJET:1||ultrafast nonlinear optics:1||CYCLE PULSES:1||KHZ:1||chemical vapor deposition:1||ferromagnetism:1||ABSORPTION:1||TERAHERTZ RADIATION:1||SCIENCE:1||FIELDS:1||ELECTRONS:1||nanomultilayer structures:1||YIELDS:1||AUGER:1||10HZ REPETITION RATE:1||MULTITERAWATT:1||SPECTROGRAPH:1||HIGHHARMONICGENERATION:1||spectroscopy:1||level population:1||PARTICLEACCELERATION:1||OPTICAL FREQUENCYMEASUREMENT:1||NANOWALLS:1||ROOMTEMPERATURE:1||AVERAGE OUTPUT POWER:1||GROUPVELOCITYMISMATCH:1||Impact ionization:1||Dynamics:1||Lasers:1||Collisional process:1||ABOVETHRESHOLD IONIZATION:1||MAINGROUP THERMOCHEMISTRY:1||dilute magnetic semiconductors:1||GACRN:1||SIZE:1||ATTOSECOND:1||Ar cluster:1||Xray astrophysics:1||photoionization:1||irons:1||normal incidence pulsed laser deposition:1||SHELLS:1||Silicon Oxide:1||gaspuff Zpinch:1||Xray:1||soft Xray reflectors:1||ESCAPE:1||ZN2SIO4:1||SILICA:1||Time delay:1||Collisional plasmas:1||MASSSPECTROMETRY:1||NUCLEARFUSION:1||PARAMETRIC AMPLIFICATION:1||LYING ELECTRONIC STATES:1||ADJUSTABLEPARAMETERS:1||MAGNETICPROPERTIES:1||LIQUIDPHASE EPITAXY:1||CEP laser:1||REGION:1||Plasma waveguide:1||AMBIENT GAS:1||DEPOSITION:1||HARMONICGENERATION:1||ENHANCEMENT:1||imaging spectrometer:1||Abel inversion:1||Water window:1||Liquid nitrogen jet:1||CHARGEEXCHANGE:1||NOBEL LECTURE:1||VARISTOR:1||EPITAXY:1||THINDISK LASER:1||HIGHREPETITIONRATE:1||Atom lasers:1||Electronimpact excitation:1||High order harmonics:1||ultrafast technology:1||PEAK POWER:1||CHARGED ALUMINUM CLUSTERS:1||GaN:1||THIN:1||Electron beam:1||INTENSE:1||Hard Xray pulse generation:1||NONLINEAR THOMSON SCATTERING:1||MULTILAYER:1||UVvisible spectrometer:1||ATOMS:1||innershell transitions:1||CORRECTED CONCAVE GRATINGS:1||DISCHARGE:1||LASERPLASMA:1||thin film:1||reflectivity:1||opacity:1||gain:1||smallangle Xray scattering:1||SOFTXRAY:1||ZINCOXIDE:1||CYGNUSX3:1||Betatron oscillation:1||ACCELERATOR:1||STRAINEDLAYER SUPERLATTICES:1||OPTICAL PARAMETRIC AMPLIFICATION:1||PASSIVE MODELOCKING:1||Collision dynamics:1||MUM:1||EXACTEXCHANGE:1||BASISSET:1||APPROXIMATION:1||OXYNITRIDES:1||Beam energy modulation:1||polarization spectroscopy:1||REORIENTATION TRANSITION:1||DEPENDENCE:1||sulfurs:1||BUILDINGBLOCKS:1||RATES:1||OPTICAL PULSES:1||toroidal mirror:1||XRAY LASER:1||CALCIUM:1||radially polarized laser:1||GRAINBOUNDARIES:1||VAPORDEPOSITION:1||Xray generation:1||MAGNETIZATION:1||Electric excitation:1||Laserinduced gas plasmas:1||Qualitative analysis:1||SCHEME:1||RADIATION:10||PULSES:8||PHOTOLUMINESCENCE:7||LASER:7||GENERATION:6||NANORODS:6||GROWTH:6||NANOWIRES:5||IMPLANTED GAN:5||SPECTROSCOPY:5||THINFILMS:4||DYNAMICS:4||SILICON:4||EXTREMEULTRAVIOLET:4||AMPLIFICATION:4||PRESSURE:4||PHASE:4||OPTICALPROPERTIES:4||SYSTEM:4||EMISSION:4||FEL:3||N2O:3||FILMS:3||OPTICS:3||SPECTRA:3||FIELD:3||MIRRORS:3||ARRAYS:3||CLUSTERS:3||SIO2:3||IONIZATION:3||VACUUM:3||SCATTERING:3||IONS:2||LUMINESCENCE PROPERTIES:2||ANISOTROPY:2||BEAMS:2||DIFFRACTION:2||DISPERSION:2||chemical vapor deposition (CVD):2||ELECTRONICSTRUCTURE:2||MOSFETS:2||SI3N4:2||DENSITY:2||LIGHT:2||PLASMAS:2||MATTER:2||nanocomposites:2||RAMANSCATTERING:2||NANOPARTICLES:2||OXIDE:2||AMPLIFIED SPONTANEOUS EMISSION:2||NM WAVELENGTH:2||GAIN:2||CARBON NANOTUBES:2||CROSSSECTIONS:2||LIGHTEMITTINGDIODES:2||PULSE:2||CARBON PLASMA:2||TISAPPHIRE LASER:2||Raman scattering:2||ROUTE:2||multilayer:2||CATHODOLUMINESCENCE:2||highresolution transmission electronic microscope (HRTEM):2||DIFFERENCEFREQUENCYGENERATION:2||CRYSTAL:2||laserproduced plasma:2||NANOCABLES:2||photoluminescence:2||MAGNETIC ALLOY SEMICONDUCTORS:2||MOLECULARBEAM EPITAXY:2||EARTHDOPED GAN:2||LASER FIELDS:2||CHIRPEDPULSEAMPLIFICATION:2||ALN:2||GAUSSIANBEAM:2||ASSISTED CATALYTIC GROWTH:2||BLUE:2||NANOSTRUCTURES:2||MAGNETOELECTRONICS:2||MICROSCOPY:2||ELECTROLUMINESCENCE:2||LASERPULSES:2||GaN nanowires:2||GALLIUM NITRIDE NANOWIRES:2||GAMNN:2||NANOTUBES:2||PHYSICS:2||Femtosecond laser:2||parametric oscillators and amplifiers:1||ultrafast lasers:1||VALENCE:1||nanowires:1||DILUTED MAGNETIC SEMICONDUCTOR:1||LUMINESCENCE:1||Density modulation:1||Energy modulation:1||Current enhanced SASE free electron laser:1||Undulator radiation:1||FREEELECTRON LASERS:1||ULTRATHIN FERROMAGNETICFILMS:1||OXIDEFILMS:1||ABLATION:1||COMPONENT:1||METAL:1||innershell excited states:1||Nelike ions:1||TRANSITIONS:1||XUV spectrometer:1||DIAGNOSTICS:1||Xray scattering:1||MO/SI:1||pulsed laser deposition:1||KEV IMPACT ENERGIES:1||vacuum electron acceleration:1||HIGHINTENSITY LASER:1||JUNCTIONS:1||LOWTEMPERATURE GROWTH:1||nanocrystalline materials:1||MOLECULAR PHOTOIONIZATION:1||LOCALIZATION:1||DEUTERIUM CLUSTERS:1||EXPLOSIONS:1||REGENERATIVE AMPLIFIERS:1||RAREGASES:1||THz radiation:1||FREEELECTRON LASER:1||REALTIME OBSERVATION:1||TARGET:1||photoionized plasmas:1||fs Xray laser:1||emission profile:1||HIGHORDER HARMONICS:1||Xray laser:1||atomic transition:1||EXCITATION:1||LASERS:1||PERFORMANCE:1||RELATIVISTIC ELECTRONS:1||BI2O3DOPED ZNO:1||INNERSHELL IONIZATION:1||Laser wakefield:1||FREQUENCY:1||SOLIDSTATE LASERS:1||Linearly polarized:1||THERMIONIC EMISSION:1||PULSE AMPLIFICATION SYSTEM:1||BIB3O6:1||NM:1||NONCOVALENT INTERACTIONS:1||CRYSTALLINE:1||INTENSITY:1||JETS:1||COHERENT:1||LINE:1||ANGULARDISTRIBUTION:1||SILVER IONS:1||magnetic anisotropy:1||DEVICES:1||Auger transitions:1||CosterKronig transitions:1||EFFICIENT:1||ELECTRONIMPACT IONIZATION:1||ULTRASHORTPULSE:1||Nanowire:1||Heterostructure:1||soft Xray reflectivity:1||PLASMA ACCELERATOR:1||ZINCOXIDE NANOWIRES:1||CHEMICALVAPORDEPOSITION:1||Electron acceleration:1||Ionization of gases:1||Delay dependent:1||MULTIPHOTON IONIZATION:1||FRAGMENTATION:1||GASJET:1||ultrafast nonlinear optics:1||CYCLE PULSES:1||KHZ:1||chemical vapor deposition:1||ferromagnetism:1||ABSORPTION:1||TERAHERTZ RADIATION:1||SCIENCE:1||FIELDS:1||ELECTRONS:1||nanomultilayer structures:1||YIELDS:1||AUGER:1||10HZ REPETITION RATE:1||MULTITERAWATT:1||SPECTROGRAPH:1||HIGHHARMONICGENERATION:1||spectroscopy:1||level population:1||PARTICLEACCELERATION:1||OPTICAL FREQUENCYMEASUREMENT:1||NANOWALLS:1||ROOMTEMPERATURE:1||AVERAGE OUTPUT POWER:1||GROUPVELOCITYMISMATCH:1||Impact ionization:1||Dynamics:1||Lasers:1||Collisional process:1||ABOVETHRESHOLD IONIZATION:1||MAINGROUP THERMOCHEMISTRY:1||dilute magnetic semiconductors:1||GACRN:1||SIZE:1||ATTOSECOND:1||Ar cluster:1||Xray astrophysics:1||photoionization:1||irons:1||normal incidence pulsed laser deposition:1||SHELLS:1||Silicon Oxide:1||gaspuff Zpinch:1||Xray:1||soft Xray reflectors:1||ESCAPE:1||ZN2SIO4:1||SILICA:1||Time delay:1||Collisional plasmas:1||MASSSPECTROMETRY:1||NUCLEARFUSION:1||PARAMETRIC AMPLIFICATION:1||LYING ELECTRONIC STATES:1||ADJUSTABLEPARAMETERS:1||MAGNETICPROPERTIES:1||LIQUIDPHASE EPITAXY:1||CEP laser:1||REGION:1||Plasma waveguide:1||AMBIENT GAS:1||DEPOSITION:1||HARMONICGENERATION:1||ENHANCEMENT:1||imaging spectrometer:1||Abel inversion:1||Water window:1||Liquid nitrogen jet:1||CHARGEEXCHANGE:1||NOBEL LECTURE:1||VARISTOR:1||EPITAXY:1||THINDISK LASER:1||HIGHREPETITIONRATE:1||Atom lasers:1||Electronimpact excitation:1||High order harmonics:1||ultrafast technology:1||PEAK POWER:1||CHARGED ALUMINUM CLUSTERS:1||GaN:1||THIN:1||Electron beam:1||INTENSE:1||Hard Xray pulse generation:1||NONLINEAR THOMSON SCATTERING:1||MULTILAYER:1||UVvisible spectrometer:1||ATOMS:1||innershell transitions:1||CORRECTED CONCAVE GRATINGS:1||DISCHARGE:1||LASERPLASMA:1||thin film:1||reflectivity:1||opacity:1||gain:1||smallangle Xray scattering:1||SOFTXRAY:1||ZINCOXIDE:1||CYGNUSX3:1||Betatron oscillation:1||ACCELERATOR:1||STRAINEDLAYER SUPERLATTICES:1||OPTICAL PARAMETRIC AMPLIFICATION:1||PASSIVE MODELOCKING:1||Collision dynamics:1||MUM:1||EXACTEXCHANGE:1||BASISSET:1||APPROXIMATION:1||OXYNITRIDES:1||Beam energy modulation:1||polarization spectroscopy:1||REORIENTATION TRANSITION:1||DEPENDENCE:1||sulfurs:1||BUILDINGBLOCKS:1||RATES:1||OPTICAL PULSES:1||toroidal mirror:1||XRAY LASER:1||CALCIUM:1||radially polarized laser:1||GRAINBOUNDARIES:1||VAPORDEPOSITION:1||Xray generation:1||MAGNETIZATION:1||Electric excitation:1||Laserinduced gas plasmas:1||Qualitative analysis:1||SCHEME:1||RADIATION:10||PULSES:8||PHOTOLUMINESCENCE:7||LASER:7||GENERATION:6||NANORODS:6||GROWTH:6||NANOWIRES:5||IMPLANTED 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SEMICONDUCTORS:2||MOLECULARBEAM EPITAXY:2||EARTHDOPED GAN:2||LASER FIELDS:2||CHIRPEDPULSEAMPLIFICATION:2||ALN:2||GAUSSIANBEAM:2||ASSISTED CATALYTIC GROWTH:2||BLUE:2||NANOSTRUCTURES:2||MAGNETOELECTRONICS:2||MICROSCOPY:2||ELECTROLUMINESCENCE:2||LASERPULSES:2||GaN nanowires:2||GALLIUM NITRIDE NANOWIRES:2||GAMNN:2||NANOTUBES:2||PHYSICS:2||Femtosecond laser:2||parametric oscillators and amplifiers:1||ultrafast lasers:1||VALENCE:1||nanowires:1||DILUTED MAGNETIC SEMICONDUCTOR:1||LUMINESCENCE:1||Density modulation:1||Energy modulation:1||Current enhanced SASE free electron laser:1||Undulator radiation:1||FREEELECTRON LASERS:1||ULTRATHIN FERROMAGNETICFILMS:1||OXIDEFILMS:1||ABLATION:1||COMPONENT:1||METAL:1||innershell excited states:1||Nelike ions:1||TRANSITIONS:1||XUV spectrometer:1||DIAGNOSTICS:1||Xray scattering:1||MO/SI:1||pulsed laser deposition:1||KEV IMPACT ENERGIES:1||vacuum electron acceleration:1||HIGHINTENSITY LASER:1||JUNCTIONS:1||LOWTEMPERATURE GROWTH:1||nanocrystalline materials:1||MOLECULAR PHOTOIONIZATION:1||LOCALIZATION:1||DEUTERIUM CLUSTERS:1||EXPLOSIONS:1||REGENERATIVE AMPLIFIERS:1||RAREGASES:1||THz radiation:1||FREEELECTRON LASER:1||REALTIME OBSERVATION:1||TARGET:1||photoionized plasmas:1||fs Xray laser:1||emission profile:1||HIGHORDER HARMONICS:1||Xray laser:1||atomic transition:1||EXCITATION:1||LASERS:1||PERFORMANCE:1||RELATIVISTIC ELECTRONS:1||BI2O3DOPED ZNO:1||INNERSHELL IONIZATION:1||Laser wakefield:1||FREQUENCY:1||SOLIDSTATE LASERS:1||Linearly polarized:1||THERMIONIC EMISSION:1||PULSE AMPLIFICATION SYSTEM:1||BIB3O6:1||NM:1||NONCOVALENT INTERACTIONS:1||CRYSTALLINE:1||INTENSITY:1||JETS:1||COHERENT:1||LINE:1||ANGULARDISTRIBUTION:1||SILVER IONS:1||magnetic anisotropy:1||DEVICES:1||Auger transitions:1||CosterKronig transitions:1||EFFICIENT:1||ELECTRONIMPACT IONIZATION:1||ULTRASHORTPULSE:1||Nanowire:1||Heterostructure:1||soft Xray reflectivity:1||PLASMA ACCELERATOR:1||ZINCOXIDE NANOWIRES:1||CHEMICALVAPORDEPOSITION:1||Electron acceleration:1||Ionization of gases:1||Delay dependent:1||MULTIPHOTON IONIZATION:1||FRAGMENTATION:1||GASJET:1||ultrafast nonlinear optics:1||CYCLE PULSES:1||KHZ:1||chemical vapor deposition:1||ferromagnetism:1||ABSORPTION:1||TERAHERTZ RADIATION:1||SCIENCE:1||FIELDS:1||ELECTRONS:1||nanomultilayer structures:1||YIELDS:1||AUGER:1||10HZ REPETITION RATE:1||MULTITERAWATT:1||SPECTROGRAPH:1||HIGHHARMONICGENERATION:1||spectroscopy:1||level population:1||PARTICLEACCELERATION:1||OPTICAL FREQUENCYMEASUREMENT:1||NANOWALLS:1||ROOMTEMPERATURE:1||AVERAGE OUTPUT POWER:1||GROUPVELOCITYMISMATCH:1||Impact ionization:1||Dynamics:1||Lasers:1||Collisional process:1||ABOVETHRESHOLD IONIZATION:1||MAINGROUP THERMOCHEMISTRY:1||dilute magnetic semiconductors:1||GACRN:1||SIZE:1||ATTOSECOND:1||Ar cluster:1||Xray astrophysics:1||photoionization:1||irons:1||normal incidence pulsed laser deposition:1||SHELLS:1||Silicon Oxide:1||gaspuff Zpinch:1||Xray:1||soft Xray reflectors:1||ESCAPE:1||ZN2SIO4:1||SILICA:1||Time 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materials:1||MOLECULAR PHOTOIONIZATION:1||LOCALIZATION:1||DEUTERIUM CLUSTERS:1||EXPLOSIONS:1||REGENERATIVE AMPLIFIERS:1||RAREGASES:1||THz radiation:1||FREEELECTRON LASER:1||REALTIME OBSERVATION:1||TARGET:1||photoionized plasmas:1||fs Xray laser:1||emission profile:1||HIGHORDER HARMONICS:1||Xray laser:1||atomic transition:1||EXCITATION:1||LASERS:1||PERFORMANCE:1||RELATIVISTIC ELECTRONS:1||BI2O3DOPED ZNO:1||INNERSHELL IONIZATION:1||Laser wakefield:1||FREQUENCY:1||SOLIDSTATE LASERS:1||Linearly polarized:1||THERMIONIC EMISSION:1||PULSE AMPLIFICATION SYSTEM:1||BIB3O6:1||NM:1||NONCOVALENT INTERACTIONS:1||CRYSTALLINE:1||INTENSITY:1||JETS:1||COHERENT:1||LINE:1||ANGULARDISTRIBUTION:1||SILVER IONS:1||magnetic anisotropy:1||DEVICES:1||Auger transitions:1||CosterKronig transitions:1||EFFICIENT:1||ELECTRONIMPACT IONIZATION:1||ULTRASHORTPULSE:1||Nanowire:1||Heterostructure:1||soft Xray reflectivity:1||PLASMA ACCELERATOR:1||ZINCOXIDE NANOWIRES:1||CHEMICALVAPORDEPOSITION:1||Electron acceleration:1||Ionization of gases:1||Delay dependent:1||MULTIPHOTON IONIZATION:1||FRAGMENTATION:1||GASJET:1||ultrafast nonlinear optics:1||CYCLE PULSES:1||KHZ:1||chemical vapor deposition:1||ferromagnetism:1||ABSORPTION:1||TERAHERTZ RADIATION:1||SCIENCE:1||FIELDS:1||ELECTRONS:1||nanomultilayer structures:1||YIELDS:1||AUGER:1||10HZ REPETITION RATE:1||MULTITERAWATT:1||SPECTROGRAPH:1||HIGHHARMONICGENERATION:1||spectroscopy:1||level population:1||PARTICLEACCELERATION:1||OPTICAL FREQUENCYMEASUREMENT:1||NANOWALLS:1||ROOMTEMPERATURE:1||AVERAGE OUTPUT POWER:1||GROUPVELOCITYMISMATCH:1||Impact ionization:1||Dynamics:1||Lasers:1||Collisional process:1||ABOVETHRESHOLD IONIZATION:1||MAINGROUP THERMOCHEMISTRY:1||dilute magnetic semiconductors:1||GACRN:1||SIZE:1||ATTOSECOND:1||Ar cluster:1||Xray astrophysics:1||photoionization:1||irons:1||normal incidence pulsed laser deposition:1||SHELLS:1||Silicon Oxide:1||gaspuff Zpinch:1||Xray:1||soft Xray reflectors:1||ESCAPE:1||ZN2SIO4:1||SILICA:1||Time delay:1||Collisional plasmas:1||MASSSPECTROMETRY:1||NUCLEARFUSION:1||PARAMETRIC AMPLIFICATION:1||LYING ELECTRONIC STATES:1||ADJUSTABLEPARAMETERS:1||MAGNETICPROPERTIES:1||LIQUIDPHASE EPITAXY:1||CEP laser:1||REGION:1||Plasma waveguide:1||AMBIENT GAS:1||DEPOSITION:1||HARMONICGENERATION:1||ENHANCEMENT:1||imaging spectrometer:1||Abel inversion:1||Water window:1||Liquid nitrogen jet:1||CHARGEEXCHANGE:1||NOBEL LECTURE:1||VARISTOR:1||EPITAXY:1||THINDISK LASER:1||HIGHREPETITIONRATE:1||Atom lasers:1||Electronimpact excitation:1||High order harmonics:1||ultrafast technology:1||PEAK POWER:1||CHARGED ALUMINUM CLUSTERS:1||GaN:1||THIN:1||Electron beam:1||INTENSE:1||Hard Xray pulse generation:1||NONLINEAR THOMSON SCATTERING:1||MULTILAYER:1||UVvisible spectrometer:1||ATOMS:1||innershell transitions:1||CORRECTED CONCAVE GRATINGS:1||DISCHARGE:1||LASERPLASMA:1||thin film:1||reflectivity:1||opacity:1||gain:1||smallangle Xray scattering:1||SOFTXRAY:1||ZINCOXIDE:1||CYGNUSX3:1||Betatron oscillation:1||ACCELERATOR:1||STRAINEDLAYER SUPERLATTICES:1||OPTICAL PARAMETRIC AMPLIFICATION:1||PASSIVE MODELOCKING:1||Collision dynamics:1||MUM:1||EXACTEXCHANGE:1||BASISSET:1||APPROXIMATION:1||OXYNITRIDES:1||Beam energy modulation:1||polarization spectroscopy:1||REORIENTATION TRANSITION:1||DEPENDENCE:1||sulfurs:1||BUILDINGBLOCKS:1||RATES:1||OPTICAL PULSES:1||toroidal mirror:1||XRAY LASER:1||CALCIUM:1||radially polarized laser:1||GRAINBOUNDARIES:1||VAPORDEPOSITION:1||Xray generation:1||MAGNETIZATION:1||Electric excitation:1||Laserinduced gas plasmas:1||Qualitative analysis:1||SCHEME:1||RADIATION:10||PULSES:8||PHOTOLUMINESCENCE:7||LASER:7||GENERATION:6||NANORODS:6||GROWTH:6||NANOWIRES:5||IMPLANTED GAN:5||SPECTROSCOPY:5||THINFILMS:4||DYNAMICS:4||SILICON:4||EXTREMEULTRAVIOLET:4||AMPLIFICATION:4||PRESSURE:4||PHASE:4||OPTICALPROPERTIES:4||SYSTEM:4||EMISSION:4||FEL:3||N2O:3||FILMS:3||OPTICS:3||SPECTRA:3||FIELD:3||MIRRORS:3||ARRAYS:3||CLUSTERS:3||SIO2:3||IONIZATION:3||VACUUM:3||SCATTERING:3||IONS:2||LUMINESCENCE PROPERTIES:2||ANISOTROPY:2||BEAMS:2||DIFFRACTION:2||DISPERSION:2||chemical vapor deposition (CVD):2||ELECTRONICSTRUCTURE:2||MOSFETS:2||SI3N4:2||DENSITY:2||LIGHT:2||PLASMAS:2||MATTER:2||nanocomposites:2||RAMANSCATTERING:2||NANOPARTICLES:2||OXIDE:2||AMPLIFIED SPONTANEOUS EMISSION:2||NM WAVELENGTH:2||GAIN:2||CARBON NANOTUBES:2||CROSSSECTIONS:2||LIGHTEMITTINGDIODES:2||PULSE:2||CARBON PLASMA:2||TISAPPHIRE LASER:2||Raman scattering:2||ROUTE:2||multilayer:2||CATHODOLUMINESCENCE:2||highresolution transmission electronic microscope (HRTEM):2||DIFFERENCEFREQUENCYGENERATION:2||CRYSTAL:2||laserproduced plasma:2||NANOCABLES:2||photoluminescence:2||MAGNETIC ALLOY SEMICONDUCTORS:2||MOLECULARBEAM EPITAXY:2||EARTHDOPED GAN:2||LASER FIELDS:2||CHIRPEDPULSEAMPLIFICATION:2||ALN:2||GAUSSIANBEAM:2||ASSISTED CATALYTIC GROWTH:2||BLUE:2||NANOSTRUCTURES:2||MAGNETOELECTRONICS:2||MICROSCOPY:2||ELECTROLUMINESCENCE:2||LASERPULSES:2||GaN nanowires:2||GALLIUM NITRIDE NANOWIRES:2||GAMNN:2||NANOTUBES:2||PHYSICS:2||Femtosecond laser:2||parametric oscillators and amplifiers:1||ultrafast lasers:1||VALENCE:1||nanowires:1||DILUTED MAGNETIC SEMICONDUCTOR:1||LUMINESCENCE:1||Density modulation:1||Energy modulation:1||Current enhanced SASE free electron laser:1||Undulator radiation:1||FREEELECTRON LASERS:1||ULTRATHIN FERROMAGNETICFILMS:1||OXIDEFILMS:1||ABLATION:1||COMPONENT:1||METAL:1||innershell excited states:1||Nelike ions:1||TRANSITIONS:1||XUV spectrometer:1||DIAGNOSTICS:1||Xray scattering:1||MO/SI:1||pulsed laser deposition:1||KEV IMPACT ENERGIES:1||vacuum electron acceleration:1||HIGHINTENSITY LASER:1||JUNCTIONS:1||LOWTEMPERATURE GROWTH:1||nanocrystalline materials:1||MOLECULAR PHOTOIONIZATION:1||LOCALIZATION:1||DEUTERIUM CLUSTERS:1||EXPLOSIONS:1||REGENERATIVE AMPLIFIERS:1||RAREGASES:1||THz radiation:1||FREEELECTRON LASER:1||REALTIME OBSERVATION:1||TARGET:1||photoionized plasmas:1||fs Xray laser:1||emission profile:1||HIGHORDER HARMONICS:1||Xray laser:1||atomic transition:1||EXCITATION:1||LASERS:1||PERFORMANCE:1||RELATIVISTIC ELECTRONS:1||BI2O3DOPED ZNO:1||INNERSHELL IONIZATION:1||Laser wakefield:1||FREQUENCY:1||SOLIDSTATE LASERS:1||Linearly polarized:1||THERMIONIC EMISSION:1||PULSE AMPLIFICATION SYSTEM:1||BIB3O6:1||NM:1||NONCOVALENT INTERACTIONS:1||CRYSTALLINE:1||INTENSITY:1||JETS:1||COHERENT:1||LINE:1||ANGULARDISTRIBUTION:1||SILVER IONS:1||magnetic anisotropy:1||DEVICES:1||Auger transitions:1||CosterKronig transitions:1||EFFICIENT:1||ELECTRONIMPACT IONIZATION:1||ULTRASHORTPULSE:1||Nanowire:1||Heterostructure:1||soft Xray reflectivity:1||PLASMA ACCELERATOR:1||ZINCOXIDE NANOWIRES:1||CHEMICALVAPORDEPOSITION:1||Electron acceleration:1||Ionization of gases:1||Delay dependent:1||MULTIPHOTON IONIZATION:1||FRAGMENTATION:1||GASJET:1||ultrafast nonlinear optics:1||CYCLE PULSES:1||KHZ:1||chemical vapor deposition:1||ferromagnetism:1||ABSORPTION:1||TERAHERTZ RADIATION:1||SCIENCE:1||FIELDS:1||ELECTRONS:1||nanomultilayer structures:1||YIELDS:1||AUGER:1||10HZ REPETITION RATE:1||MULTITERAWATT:1||SPECTROGRAPH:1||HIGHHARMONICGENERATION:1||spectroscopy:1||level population:1||PARTICLEACCELERATION:1||OPTICAL FREQUENCYMEASUREMENT:1||NANOWALLS:1||ROOMTEMPERATURE:1||AVERAGE OUTPUT POWER:1||GROUPVELOCITYMISMATCH:1||Impact ionization:1||Dynamics:1||Lasers:1||Collisional process:1||ABOVETHRESHOLD IONIZATION:1||MAINGROUP THERMOCHEMISTRY:1||dilute magnetic semiconductors:1||GACRN:1||SIZE:1||ATTOSECOND:1||Ar cluster:1||Xray astrophysics:1||photoionization:1||irons:1||normal incidence pulsed laser deposition:1||SHELLS:1||Silicon Oxide:1||gaspuff Zpinch:1||Xray:1||soft Xray reflectors:1||ESCAPE:1||ZN2SIO4:1||SILICA:1||Time delay:1||Collisional plasmas:1||MASSSPECTROMETRY:1||NUCLEARFUSION:1||PARAMETRIC AMPLIFICATION:1||LYING ELECTRONIC STATES:1||ADJUSTABLEPARAMETERS:1||MAGNETICPROPERTIES:1||LIQUIDPHASE EPITAXY:1||CEP laser:1||REGION:1||Plasma waveguide:1||AMBIENT GAS:1||DEPOSITION:1||HARMONICGENERATION:1||ENHANCEMENT:1||imaging spectrometer:1||Abel inversion:1||Water window:1||Liquid nitrogen jet:1||CHARGEEXCHANGE:1||NOBEL LECTURE:1||VARISTOR:1||EPITAXY:1||THINDISK LASER:1||HIGHREPETITIONRATE:1||Atom lasers:1||Electronimpact excitation:1||High order harmonics:1||ultrafast technology:1||PEAK POWER:1||CHARGED ALUMINUM CLUSTERS:1||GaN:1||THIN:1||Electron beam:1||INTENSE:1||Hard Xray pulse generation:1||NONLINEAR THOMSON SCATTERING:1||MULTILAYER:1||UVvisible spectrometer:1||ATOMS:1||innershell transitions:1||CORRECTED CONCAVE GRATINGS:1||DISCHARGE:1||LASERPLASMA:1||thin film:1||reflectivity:1||opacity:1||gain:1||smallangle Xray scattering:1||SOFTXRAY:1||ZINCOXIDE:1||CYGNUSX3:1||Betatron oscillation:1||ACCELERATOR:1||STRAINEDLAYER SUPERLATTICES:1||OPTICAL PARAMETRIC AMPLIFICATION:1||PASSIVE MODELOCKING:1||Collision dynamics:1||MUM:1||EXACTEXCHANGE:1||BASISSET:1||APPROXIMATION:1||OXYNITRIDES:1||Beam energy modulation:1||polarization spectroscopy:1||REORIENTATION TRANSITION:1||DEPENDENCE:1||sulfurs:1||BUILDINGBLOCKS:1||RATES:1||OPTICAL PULSES:1||toroidal mirror:1||XRAY LASER:1||CALCIUM:1||radially polarized laser:1||GRAINBOUNDARIES:1||VAPORDEPOSITION:1||Xray generation:1||MAGNETIZATION:1||Electric excitation:1||Laserinduced gas plasmas:1||Qualitative analysis:1||SCHEME:1||RADIATION:10||PULSES:8||PHOTOLUMINESCENCE:7||LASER:7||GENERATION:6||NANORODS:6||GROWTH:6||NANOWIRES:5||IMPLANTED 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SEMICONDUCTORS:2||MOLECULARBEAM EPITAXY:2||EARTHDOPED GAN:2||LASER FIELDS:2||CHIRPEDPULSEAMPLIFICATION:2||ALN:2||GAUSSIANBEAM:2||ASSISTED CATALYTIC GROWTH:2||BLUE:2||NANOSTRUCTURES:2||MAGNETOELECTRONICS:2||MICROSCOPY:2||ELECTROLUMINESCENCE:2||LASERPULSES:2||GaN nanowires:2||GALLIUM NITRIDE NANOWIRES:2||GAMNN:2||NANOTUBES:2||PHYSICS:2||Femtosecond laser:2||parametric oscillators and amplifiers:1||ultrafast lasers:1||VALENCE:1||nanowires:1||DILUTED MAGNETIC SEMICONDUCTOR:1||LUMINESCENCE:1||Density modulation:1||Energy modulation:1||Current enhanced SASE free electron laser:1||Undulator radiation:1||FREEELECTRON LASERS:1||ULTRATHIN FERROMAGNETICFILMS:1||OXIDEFILMS:1||ABLATION:1||COMPONENT:1||METAL:1||innershell excited states:1||Nelike ions:1||TRANSITIONS:1||XUV spectrometer:1||DIAGNOSTICS:1||Xray scattering:1||MO/SI:1||pulsed laser deposition:1||KEV IMPACT ENERGIES:1||vacuum electron acceleration:1||HIGHINTENSITY LASER:1||JUNCTIONS:1||LOWTEMPERATURE GROWTH:1||nanocrystalline materials:1||MOLECULAR PHOTOIONIZATION:1||LOCALIZATION:1||DEUTERIUM CLUSTERS:1||EXPLOSIONS:1||REGENERATIVE AMPLIFIERS:1||RAREGASES:1||THz radiation:1||FREEELECTRON LASER:1||REALTIME OBSERVATION:1||TARGET:1||photoionized plasmas:1||fs Xray laser:1||emission profile:1||HIGHORDER HARMONICS:1||Xray laser:1||atomic transition:1||EXCITATION:1||LASERS:1||PERFORMANCE:1||RELATIVISTIC ELECTRONS:1||BI2O3DOPED ZNO:1||INNERSHELL IONIZATION:1||Laser wakefield:1||FREQUENCY:1||SOLIDSTATE LASERS:1||Linearly polarized:1||THERMIONIC EMISSION:1||PULSE AMPLIFICATION SYSTEM:1||BIB3O6:1||NM:1||NONCOVALENT INTERACTIONS:1||CRYSTALLINE:1||INTENSITY:1||JETS:1||COHERENT:1||LINE:1||ANGULARDISTRIBUTION:1||SILVER IONS:1||magnetic anisotropy:1||DEVICES:1||Auger transitions:1||CosterKronig transitions:1||EFFICIENT:1||ELECTRONIMPACT IONIZATION:1||ULTRASHORTPULSE:1||Nanowire:1||Heterostructure:1||soft Xray reflectivity:1||PLASMA ACCELERATOR:1||ZINCOXIDE NANOWIRES:1||CHEMICALVAPORDEPOSITION:1||Electron acceleration:1||Ionization of gases:1||Delay dependent:1||MULTIPHOTON IONIZATION:1||FRAGMENTATION:1||GASJET:1||ultrafast nonlinear optics:1||CYCLE PULSES:1||KHZ:1||chemical vapor deposition:1||ferromagnetism:1||ABSORPTION:1||TERAHERTZ RADIATION:1||SCIENCE:1||FIELDS:1||ELECTRONS:1||nanomultilayer structures:1||YIELDS:1||AUGER:1||10HZ REPETITION RATE:1||MULTITERAWATT:1||SPECTROGRAPH:1||HIGHHARMONICGENERATION:1||spectroscopy:1||level population:1||PARTICLEACCELERATION:1||OPTICAL FREQUENCYMEASUREMENT:1||NANOWALLS:1||ROOMTEMPERATURE:1||AVERAGE OUTPUT POWER:1||GROUPVELOCITYMISMATCH:1||Impact ionization:1||Dynamics:1||Lasers:1||Collisional process:1||ABOVETHRESHOLD IONIZATION:1||MAINGROUP THERMOCHEMISTRY:1||dilute magnetic semiconductors:1||GACRN:1||SIZE:1||ATTOSECOND:1||Ar cluster:1||Xray astrophysics:1||photoionization:1||irons:1||normal incidence pulsed laser deposition:1||SHELLS:1||Silicon Oxide:1||gaspuff Zpinch:1||Xray:1||soft Xray reflectors:1||ESCAPE:1||ZN2SIO4:1||SILICA:1||Time 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materials:1||MOLECULAR PHOTOIONIZATION:1||LOCALIZATION:1||DEUTERIUM CLUSTERS:1||EXPLOSIONS:1||REGENERATIVE AMPLIFIERS:1||RAREGASES:1||THz radiation:1||FREEELECTRON LASER:1||REALTIME OBSERVATION:1||TARGET:1||photoionized plasmas:1||fs Xray laser:1||emission profile:1||HIGHORDER HARMONICS:1||Xray laser:1||atomic transition:1||EXCITATION:1||LASERS:1||PERFORMANCE:1||RELATIVISTIC ELECTRONS:1||BI2O3DOPED ZNO:1||INNERSHELL IONIZATION:1||Laser wakefield:1||FREQUENCY:1||SOLIDSTATE LASERS:1||Linearly polarized:1||THERMIONIC EMISSION:1||PULSE AMPLIFICATION SYSTEM:1||BIB3O6:1||NM:1||NONCOVALENT INTERACTIONS:1||CRYSTALLINE:1||INTENSITY:1||JETS:1||COHERENT:1||LINE:1||ANGULARDISTRIBUTION:1||SILVER IONS:1||magnetic anisotropy:1||DEVICES:1||Auger transitions:1||CosterKronig transitions:1||EFFICIENT:1||ELECTRONIMPACT IONIZATION:1||ULTRASHORTPULSE:1||Nanowire:1||Heterostructure:1||soft Xray reflectivity:1||PLASMA ACCELERATOR:1||ZINCOXIDE NANOWIRES:1||CHEMICALVAPORDEPOSITION:1||Electron acceleration:1||Ionization of gases:1||Delay dependent:1||MULTIPHOTON IONIZATION:1||FRAGMENTATION:1||GASJET:1||ultrafast nonlinear optics:1||CYCLE PULSES:1||KHZ:1||chemical vapor deposition:1||ferromagnetism:1||ABSORPTION:1||TERAHERTZ RADIATION:1||SCIENCE:1||FIELDS:1||ELECTRONS:1||nanomultilayer structures:1||YIELDS:1||AUGER:1||10HZ REPETITION RATE:1||MULTITERAWATT:1||SPECTROGRAPH:1||HIGHHARMONICGENERATION:1||spectroscopy:1||level population:1||PARTICLEACCELERATION:1||OPTICAL FREQUENCYMEASUREMENT:1||NANOWALLS:1||ROOMTEMPERATURE:1||AVERAGE OUTPUT POWER:1||GROUPVELOCITYMISMATCH:1||Impact ionization:1||Dynamics:1||Lasers:1||Collisional process:1||ABOVETHRESHOLD IONIZATION:1||MAINGROUP THERMOCHEMISTRY:1||dilute magnetic semiconductors:1||GACRN:1||SIZE:1||ATTOSECOND:1||Ar cluster:1||Xray astrophysics:1||photoionization:1||irons:1||normal incidence pulsed laser deposition:1||SHELLS:1||Silicon Oxide:1||gaspuff Zpinch:1||Xray:1||soft Xray reflectors:1||ESCAPE:1||ZN2SIO4:1||SILICA:1||Time delay:1||Collisional plasmas:1||MASSSPECTROMETRY:1||NUCLEARFUSION:1||PARAMETRIC AMPLIFICATION:1||LYING ELECTRONIC STATES:1||ADJUSTABLEPARAMETERS:1||MAGNETICPROPERTIES:1||LIQUIDPHASE EPITAXY:1||CEP laser:1||REGION:1||Plasma waveguide:1||AMBIENT GAS:1||DEPOSITION:1||HARMONICGENERATION:1||ENHANCEMENT:1||imaging spectrometer:1||Abel inversion:1||Water window:1||Liquid nitrogen jet:1||CHARGEEXCHANGE:1||NOBEL LECTURE:1||VARISTOR:1||EPITAXY:1||THINDISK LASER:1||HIGHREPETITIONRATE:1||Atom lasers:1||Electronimpact excitation:1||High order harmonics:1||ultrafast technology:1||PEAK POWER:1||CHARGED ALUMINUM CLUSTERS:1||GaN:1||THIN:1||Electron beam:1||INTENSE:1||Hard Xray pulse generation:1||NONLINEAR THOMSON SCATTERING:1||MULTILAYER:1||UVvisible spectrometer:1||ATOMS:1||innershell transitions:1||CORRECTED CONCAVE GRATINGS:1||DISCHARGE:1||LASERPLASMA:1||thin film:1||reflectivity:1||opacity:1||gain:1||smallangle Xray scattering:1||SOFTXRAY:1||ZINCOXIDE:1||CYGNUSX3:1||Betatron oscillation:1||ACCELERATOR:1||STRAINEDLAYER SUPERLATTICES:1||OPTICAL PARAMETRIC AMPLIFICATION:1||PASSIVE MODELOCKING:1||Collision dynamics:1||MUM:1||EXACTEXCHANGE:1||BASISSET:1||APPROXIMATION:1||OXYNITRIDES:1||Beam energy modulation:1||polarization spectroscopy:1||REORIENTATION TRANSITION:1||DEPENDENCE:1||sulfurs:1||BUILDINGBLOCKS:1||RATES:1||OPTICAL PULSES:1||toroidal mirror:1||XRAY LASER:1||CALCIUM:1||radially polarized laser:1||GRAINBOUNDARIES:1||VAPORDEPOSITION:1||Xray generation:1||MAGNETIZATION:1||Electric excitation:1||Laserinduced gas plasmas:1||Qualitative analysis:1||SCHEME:1||RADIATION:10||PULSES:8||PHOTOLUMINESCENCE:7||LASER:7||GENERATION:6||NANORODS:6||GROWTH:6||NANOWIRES:5||IMPLANTED GAN:5||SPECTROSCOPY:5||THINFILMS:4||DYNAMICS:4||SILICON:4||EXTREMEULTRAVIOLET:4||AMPLIFICATION:4||PRESSURE:4||PHASE:4||OPTICALPROPERTIES:4||SYSTEM:4||EMISSION:4||FEL:3||N2O:3||FILMS:3||OPTICS:3||SPECTRA:3||FIELD:3||MIRRORS:3||ARRAYS:3||CLUSTERS:3||SIO2:3||IONIZATION:3||VACUUM:3||SCATTERING:3||IONS:2||LUMINESCENCE PROPERTIES:2||ANISOTROPY:2||BEAMS:2||DIFFRACTION:2||DISPERSION:2||chemical vapor deposition (CVD):2||ELECTRONICSTRUCTURE:2||MOSFETS:2||SI3N4:2||DENSITY:2||LIGHT:2||PLASMAS:2||MATTER:2||nanocomposites:2||RAMANSCATTERING:2||NANOPARTICLES:2||OXIDE:2||AMPLIFIED SPONTANEOUS EMISSION:2||NM WAVELENGTH:2||GAIN:2||CARBON NANOTUBES:2||CROSSSECTIONS:2||LIGHTEMITTINGDIODES:2||PULSE:2||CARBON PLASMA:2||TISAPPHIRE LASER:2||Raman scattering:2||ROUTE:2||multilayer:2||CATHODOLUMINESCENCE:2||highresolution transmission electronic microscope (HRTEM):2||DIFFERENCEFREQUENCYGENERATION:2||CRYSTAL:2||laserproduced plasma:2||NANOCABLES:2||photoluminescence:2||MAGNETIC ALLOY SEMICONDUCTORS:2||MOLECULARBEAM EPITAXY:2||EARTHDOPED GAN:2||LASER FIELDS:2||CHIRPEDPULSEAMPLIFICATION:2||ALN:2||GAUSSIANBEAM:2||ASSISTED CATALYTIC GROWTH:2||BLUE:2||NANOSTRUCTURES:2||MAGNETOELECTRONICS:2||MICROSCOPY:2||ELECTROLUMINESCENCE:2||LASERPULSES:2||GaN nanowires:2||GALLIUM NITRIDE NANOWIRES:2||GAMNN:2||NANOTUBES:2||PHYSICS:2||Femtosecond laser:2||parametric oscillators and amplifiers:1||ultrafast lasers:1||VALENCE:1||nanowires:1||DILUTED MAGNETIC SEMICONDUCTOR:1||LUMINESCENCE:1||Density modulation:1||Energy modulation:1||Current enhanced SASE free electron laser:1||Undulator radiation:1||FREEELECTRON LASERS:1||ULTRATHIN FERROMAGNETICFILMS:1||OXIDEFILMS:1||ABLATION:1||COMPONENT:1||METAL:1||innershell excited states:1||Nelike ions:1||TRANSITIONS:1||XUV spectrometer:1||DIAGNOSTICS:1||Xray scattering:1||MO/SI:1||pulsed laser deposition:1||KEV IMPACT ENERGIES:1||vacuum electron acceleration:1||HIGHINTENSITY LASER:1||JUNCTIONS:1||LOWTEMPERATURE GROWTH:1||nanocrystalline materials:1||MOLECULAR PHOTOIONIZATION:1||LOCALIZATION:1||DEUTERIUM CLUSTERS:1||EXPLOSIONS:1||REGENERATIVE AMPLIFIERS:1||RAREGASES:1||THz radiation:1||FREEELECTRON LASER:1||REALTIME OBSERVATION:1||TARGET:1||photoionized plasmas:1||fs Xray laser:1||emission profile:1||HIGHORDER HARMONICS:1||Xray laser:1||atomic transition:1||EXCITATION:1||LASERS:1||PERFORMANCE:1||RELATIVISTIC ELECTRONS:1||BI2O3DOPED ZNO:1||INNERSHELL IONIZATION:1||Laser wakefield:1||FREQUENCY:1||SOLIDSTATE LASERS:1||Linearly polarized:1||THERMIONIC EMISSION:1||PULSE AMPLIFICATION SYSTEM:1||BIB3O6:1||NM:1||NONCOVALENT INTERACTIONS:1||CRYSTALLINE:1||INTENSITY:1||JETS:1||COHERENT:1||LINE:1||ANGULARDISTRIBUTION:1||SILVER IONS:1||magnetic anisotropy:1||DEVICES:1||Auger transitions:1||CosterKronig transitions:1||EFFICIENT:1||ELECTRONIMPACT IONIZATION:1||ULTRASHORTPULSE:1||Nanowire:1||Heterostructure:1||soft Xray reflectivity:1||PLASMA ACCELERATOR:1||ZINCOXIDE NANOWIRES:1||CHEMICALVAPORDEPOSITION:1||Electron acceleration:1||Ionization of gases:1||Delay dependent:1||MULTIPHOTON IONIZATION:1||FRAGMENTATION:1||GASJET:1||ultrafast nonlinear optics:1||CYCLE PULSES:1||KHZ:1||chemical vapor deposition:1||ferromagnetism:1||ABSORPTION:1||TERAHERTZ RADIATION:1||SCIENCE:1||FIELDS:1||ELECTRONS:1||nanomultilayer structures:1||YIELDS:1||AUGER:1||10HZ REPETITION RATE:1||MULTITERAWATT:1||SPECTROGRAPH:1||HIGHHARMONICGENERATION:1||spectroscopy:1||level population:1||PARTICLEACCELERATION:1||OPTICAL FREQUENCYMEASUREMENT:1||NANOWALLS:1||ROOMTEMPERATURE:1||AVERAGE OUTPUT POWER:1||GROUPVELOCITYMISMATCH:1||Impact ionization:1||Dynamics:1||Lasers:1||Collisional process:1||ABOVETHRESHOLD IONIZATION:1||MAINGROUP THERMOCHEMISTRY:1||dilute magnetic semiconductors:1||GACRN:1||SIZE:1||ATTOSECOND:1||Ar cluster:1||Xray astrophysics:1||photoionization:1||irons:1||normal incidence pulsed laser deposition:1||SHELLS:1||Silicon Oxide:1||gaspuff Zpinch:1||Xray:1||soft Xray reflectors:1||ESCAPE:1||ZN2SIO4:1||SILICA:1||Time delay:1||Collisional plasmas:1||MASSSPECTROMETRY:1||NUCLEARFUSION:1||PARAMETRIC AMPLIFICATION:1||LYING ELECTRONIC STATES:1||ADJUSTABLEPARAMETERS:1||MAGNETICPROPERTIES:1||LIQUIDPHASE EPITAXY:1||CEP laser:1||REGION:1||Plasma waveguide:1||AMBIENT GAS:1||DEPOSITION:1||HARMONICGENERATION:1||ENHANCEMENT:1||imaging spectrometer:1||Abel inversion:1||Water window:1||Liquid nitrogen jet:1||CHARGEEXCHANGE:1||NOBEL LECTURE:1||VARISTOR:1||EPITAXY:1||THINDISK LASER:1||HIGHREPETITIONRATE:1||Atom lasers:1||Electronimpact excitation:1||High order harmonics:1||ultrafast technology:1||PEAK POWER:1||CHARGED ALUMINUM CLUSTERS:1||GaN:1||THIN:1||Electron beam:1||INTENSE:1||Hard Xray pulse generation:1||NONLINEAR THOMSON SCATTERING:1||MULTILAYER:1||UVvisible spectrometer:1||ATOMS:1||innershell transitions:1||CORRECTED CONCAVE GRATINGS:1||DISCHARGE:1||LASERPLASMA:1||thin film:1||reflectivity:1||opacity:1||gain:1||smallangle Xray scattering:1||SOFTXRAY:1||ZINCOXIDE:1||CYGNUSX3:1||Betatron oscillation:1||ACCELERATOR:1||STRAINEDLAYER SUPERLATTICES:1||OPTICAL PARAMETRIC AMPLIFICATION:1||PASSIVE MODELOCKING:1||Collision dynamics:1||MUM:1||EXACTEXCHANGE:1||BASISSET:1||APPROXIMATION:1||OXYNITRIDES:1||Beam energy modulation:1||polarization spectroscopy:1||REORIENTATION TRANSITION:1||DEPENDENCE:1||sulfurs:1||BUILDINGBLOCKS:1||RATES:1||OPTICAL PULSES:1||toroidal mirror:1||XRAY LASER:1||CALCIUM:1||radially polarized laser:1||GRAINBOUNDARIES:1||VAPORDEPOSITION:1||Xray generation:1||MAGNETIZATION:1||Electric excitation:1||Laserinduced gas plasmas:1||Qualitative analysis:1||SCHEME:1||RADIATION:10||PULSES:8||PHOTOLUMINESCENCE:7||LASER:7||GENERATION:6||NANORODS:6||GROWTH:6||NANOWIRES:5||IMPLANTED 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SEMICONDUCTORS:2||MOLECULARBEAM EPITAXY:2||EARTHDOPED GAN:2||LASER FIELDS:2||CHIRPEDPULSEAMPLIFICATION:2||ALN:2||GAUSSIANBEAM:2||ASSISTED CATALYTIC GROWTH:2||BLUE:2||NANOSTRUCTURES:2||MAGNETOELECTRONICS:2||MICROSCOPY:2||ELECTROLUMINESCENCE:2||LASERPULSES:2||GaN nanowires:2||GALLIUM NITRIDE NANOWIRES:2||GAMNN:2||NANOTUBES:2||PHYSICS:2||Femtosecond laser:2||parametric oscillators and amplifiers:1||ultrafast lasers:1||VALENCE:1||nanowires:1||DILUTED MAGNETIC SEMICONDUCTOR:1||LUMINESCENCE:1||Density modulation:1||Energy modulation:1||Current enhanced SASE free electron laser:1||Undulator radiation:1||FREEELECTRON LASERS:1||ULTRATHIN FERROMAGNETICFILMS:1||OXIDEFILMS:1||ABLATION:1||COMPONENT:1||METAL:1||innershell excited states:1||Nelike ions:1||TRANSITIONS:1||XUV spectrometer:1||DIAGNOSTICS:1||Xray scattering:1||MO/SI:1||pulsed laser deposition:1||KEV IMPACT ENERGIES:1||vacuum electron acceleration:1||HIGHINTENSITY LASER:1||JUNCTIONS:1||LOWTEMPERATURE GROWTH:1||nanocrystalline materials:1||MOLECULAR PHOTOIONIZATION:1||LOCALIZATION:1||DEUTERIUM CLUSTERS:1||EXPLOSIONS:1||REGENERATIVE AMPLIFIERS:1||RAREGASES:1||THz radiation:1||FREEELECTRON LASER:1||REALTIME OBSERVATION:1||TARGET:1||photoionized plasmas:1||fs Xray laser:1||emission profile:1||HIGHORDER HARMONICS:1||Xray laser:1||atomic transition:1||EXCITATION:1||LASERS:1||PERFORMANCE:1||RELATIVISTIC ELECTRONS:1||BI2O3DOPED ZNO:1||INNERSHELL IONIZATION:1||Laser wakefield:1||FREQUENCY:1||SOLIDSTATE LASERS:1||Linearly polarized:1||THERMIONIC EMISSION:1||PULSE AMPLIFICATION SYSTEM:1||BIB3O6:1||NM:1||NONCOVALENT INTERACTIONS:1||CRYSTALLINE:1||INTENSITY:1||JETS:1||COHERENT:1||LINE:1||ANGULARDISTRIBUTION:1||SILVER IONS:1||magnetic anisotropy:1||DEVICES:1||Auger transitions:1||CosterKronig transitions:1||EFFICIENT:1||ELECTRONIMPACT IONIZATION:1||ULTRASHORTPULSE:1||Nanowire:1||Heterostructure:1||soft Xray reflectivity:1||PLASMA ACCELERATOR:1||ZINCOXIDE NANOWIRES:1||CHEMICALVAPORDEPOSITION:1||Electron acceleration:1||Ionization of gases:1||Delay dependent:1||MULTIPHOTON IONIZATION:1||FRAGMENTATION:1||GASJET:1||ultrafast nonlinear optics:1||CYCLE PULSES:1||KHZ:1||chemical vapor deposition:1||ferromagnetism:1||ABSORPTION:1||TERAHERTZ RADIATION:1||SCIENCE:1||FIELDS:1||ELECTRONS:1||nanomultilayer structures:1||YIELDS:1||AUGER:1||10HZ REPETITION RATE:1||MULTITERAWATT:1||SPECTROGRAPH:1||HIGHHARMONICGENERATION:1||spectroscopy:1||level population:1||PARTICLEACCELERATION:1||OPTICAL FREQUENCYMEASUREMENT:1||NANOWALLS:1||ROOMTEMPERATURE:1||AVERAGE OUTPUT POWER:1||GROUPVELOCITYMISMATCH:1||Impact ionization:1||Dynamics:1||Lasers:1||Collisional process:1||ABOVETHRESHOLD IONIZATION:1||MAINGROUP THERMOCHEMISTRY:1||dilute magnetic semiconductors:1||GACRN:1||SIZE:1||ATTOSECOND:1||Ar cluster:1||Xray astrophysics:1||photoionization:1||irons:1||normal incidence pulsed laser deposition:1||SHELLS:1||Silicon Oxide:1||gaspuff Zpinch:1||Xray:1||soft Xray reflectors:1||ESCAPE:1||ZN2SIO4:1||SILICA:1||Time 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materials:1||MOLECULAR PHOTOIONIZATION:1||LOCALIZATION:1||DEUTERIUM CLUSTERS:1||EXPLOSIONS:1||REGENERATIVE AMPLIFIERS:1||RAREGASES:1||THz radiation:1||FREEELECTRON LASER:1||REALTIME OBSERVATION:1||TARGET:1||photoionized plasmas:1||fs Xray laser:1||emission profile:1||HIGHORDER HARMONICS:1||Xray laser:1||atomic transition:1||EXCITATION:1||LASERS:1||PERFORMANCE:1||RELATIVISTIC ELECTRONS:1||BI2O3DOPED ZNO:1||INNERSHELL IONIZATION:1||Laser wakefield:1||FREQUENCY:1||SOLIDSTATE LASERS:1||Linearly polarized:1||THERMIONIC EMISSION:1||PULSE AMPLIFICATION SYSTEM:1||BIB3O6:1||NM:1||NONCOVALENT INTERACTIONS:1||CRYSTALLINE:1||INTENSITY:1||JETS:1||COHERENT:1||LINE:1||ANGULARDISTRIBUTION:1||SILVER IONS:1||magnetic anisotropy:1||DEVICES:1||Auger transitions:1||CosterKronig transitions:1||EFFICIENT:1||ELECTRONIMPACT IONIZATION:1||ULTRASHORTPULSE:1||Nanowire:1||Heterostructure:1||soft Xray reflectivity:1||PLASMA ACCELERATOR:1||ZINCOXIDE NANOWIRES:1||CHEMICALVAPORDEPOSITION:1||Electron acceleration:1||Ionization of gases:1||Delay dependent:1||MULTIPHOTON IONIZATION:1||FRAGMENTATION:1||GASJET:1||ultrafast nonlinear optics:1||CYCLE PULSES:1||KHZ:1||chemical vapor deposition:1||ferromagnetism:1||ABSORPTION:1||TERAHERTZ RADIATION:1||SCIENCE:1||FIELDS:1||ELECTRONS:1||nanomultilayer structures:1||YIELDS:1||AUGER:1||10HZ REPETITION RATE:1||MULTITERAWATT:1||SPECTROGRAPH:1||HIGHHARMONICGENERATION:1||spectroscopy:1||level population:1||PARTICLEACCELERATION:1||OPTICAL FREQUENCYMEASUREMENT:1||NANOWALLS:1||ROOMTEMPERATURE:1||AVERAGE OUTPUT POWER:1||GROUPVELOCITYMISMATCH:1||Impact ionization:1||Dynamics:1||Lasers:1||Collisional process:1||ABOVETHRESHOLD IONIZATION:1||MAINGROUP THERMOCHEMISTRY:1||dilute magnetic semiconductors:1||GACRN:1||SIZE:1||ATTOSECOND:1||Ar cluster:1||Xray astrophysics:1||photoionization:1||irons:1||normal incidence pulsed laser deposition:1||SHELLS:1||Silicon Oxide:1||gaspuff Zpinch:1||Xray:1||soft Xray reflectors:1||ESCAPE:1||ZN2SIO4:1||SILICA:1||Time delay:1||Collisional plasmas:1||MASSSPECTROMETRY:1||NUCLEARFUSION:1||PARAMETRIC AMPLIFICATION:1||LYING ELECTRONIC STATES:1||ADJUSTABLEPARAMETERS:1||MAGNETICPROPERTIES:1||LIQUIDPHASE EPITAXY:1||CEP laser:1||REGION:1||Plasma waveguide:1||AMBIENT GAS:1||DEPOSITION:1||HARMONICGENERATION:1||ENHANCEMENT:1||imaging spectrometer:1||Abel inversion:1||Water window:1||Liquid nitrogen jet:1||CHARGEEXCHANGE:1||NOBEL LECTURE:1||VARISTOR:1||EPITAXY:1||THINDISK LASER:1||HIGHREPETITIONRATE:1||Atom lasers:1||Electronimpact excitation:1||High order harmonics:1||ultrafast technology:1||PEAK POWER:1||CHARGED ALUMINUM CLUSTERS:1||GaN:1||THIN:1||Electron beam:1||INTENSE:1||Hard Xray pulse generation:1||NONLINEAR THOMSON SCATTERING:1||MULTILAYER:1||UVvisible spectrometer:1||ATOMS:1||innershell transitions:1||CORRECTED CONCAVE GRATINGS:1||DISCHARGE:1||LASERPLASMA:1||thin film:1||reflectivity:1||opacity:1||gain:1||smallangle Xray scattering:1||SOFTXRAY:1||ZINCOXIDE:1||CYGNUSX3:1||Betatron oscillation:1||ACCELERATOR:1||STRAINEDLAYER SUPERLATTICES:1||OPTICAL PARAMETRIC AMPLIFICATION:1||PASSIVE MODELOCKING:1||Collision dynamics:1||MUM:1||EXACTEXCHANGE:1||BASISSET:1||APPROXIMATION:1||OXYNITRIDES:1||Beam energy modulation:1||polarization spectroscopy:1||REORIENTATION TRANSITION:1||DEPENDENCE:1||sulfurs:1||BUILDINGBLOCKS:1||RATES:1||OPTICAL PULSES:1||toroidal mirror:1||XRAY LASER:1||CALCIUM:1||radially polarized laser:1||GRAINBOUNDARIES:1||VAPORDEPOSITION:1||Xray generation:1||MAGNETIZATION:1||Electric excitation:1||Laserinduced gas plasmas:1||Qualitative analysis:1||SCHEME:1||RADIATION:10||PULSES:8||PHOTOLUMINESCENCE:7||LASER:7||GENERATION:6||NANORODS:6||GROWTH:6||NANOWIRES:5||IMPLANTED GAN:5||SPECTROSCOPY:5||THINFILMS:4||DYNAMICS:4||SILICON:4||EXTREMEULTRAVIOLET:4||AMPLIFICATION:4||PRESSURE:4||PHASE:4||OPTICALPROPERTIES:4||SYSTEM:4||EMISSION:4||FEL:3||N2O:3||FILMS:3||OPTICS:3||SPECTRA:3||FIELD:3||MIRRORS:3||ARRAYS:3||CLUSTERS:3||SIO2:3||IONIZATION:3||VACUUM:3||SCATTERING:3||IONS:2||LUMINESCENCE PROPERTIES:2||ANISOTROPY:2||BEAMS:2||DIFFRACTION:2||DISPERSION:2||chemical vapor deposition (CVD):2||ELECTRONICSTRUCTURE:2||MOSFETS:2||SI3N4:2||DENSITY:2||LIGHT:2||PLASMAS:2||MATTER:2||nanocomposites:2||RAMANSCATTERING:2||NANOPARTICLES:2||OXIDE:2||AMPLIFIED SPONTANEOUS EMISSION:2||NM WAVELENGTH:2||GAIN:2||CARBON NANOTUBES:2||CROSSSECTIONS:2||LIGHTEMITTINGDIODES:2||PULSE:2||CARBON PLASMA:2||TISAPPHIRE LASER:2||Raman scattering:2||ROUTE:2||multilayer:2||CATHODOLUMINESCENCE:2||highresolution transmission electronic microscope (HRTEM):2||DIFFERENCEFREQUENCYGENERATION:2||CRYSTAL:2||laserproduced plasma:2||NANOCABLES:2||photoluminescence:2||MAGNETIC ALLOY SEMICONDUCTORS:2||MOLECULARBEAM EPITAXY:2||EARTHDOPED GAN:2||LASER FIELDS:2||CHIRPEDPULSEAMPLIFICATION:2||ALN:2||GAUSSIANBEAM:2||ASSISTED CATALYTIC GROWTH:2||BLUE:2||NANOSTRUCTURES:2||MAGNETOELECTRONICS:2||MICROSCOPY:2||ELECTROLUMINESCENCE:2||LASERPULSES:2||GaN nanowires:2||GALLIUM NITRIDE NANOWIRES:2||GAMNN:2||NANOTUBES:2||PHYSICS:2||Femtosecond laser:2||parametric oscillators and amplifiers:1||ultrafast lasers:1||VALENCE:1||nanowires:1||DILUTED MAGNETIC SEMICONDUCTOR:1||LUMINESCENCE:1||Density modulation:1||Energy modulation:1||Current enhanced SASE free electron laser:1||Undulator radiation:1||FREEELECTRON LASERS:1||ULTRATHIN FERROMAGNETICFILMS:1||OXIDEFILMS:1||ABLATION:1||COMPONENT:1||METAL:1||innershell excited states:1||Nelike ions:1||TRANSITIONS:1||XUV spectrometer:1||DIAGNOSTICS:1||Xray scattering:1||MO/SI:1||pulsed laser deposition:1||KEV IMPACT ENERGIES:1||vacuum electron acceleration:1||HIGHINTENSITY LASER:1||JUNCTIONS:1||LOWTEMPERATURE GROWTH:1||nanocrystalline materials:1||MOLECULAR PHOTOIONIZATION:1||LOCALIZATION:1||DEUTERIUM CLUSTERS:1||EXPLOSIONS:1||REGENERATIVE AMPLIFIERS:1||RAREGASES:1||THz radiation:1||FREEELECTRON LASER:1||REALTIME OBSERVATION:1||TARGET:1||photoionized plasmas:1||fs Xray laser:1||emission profile:1||HIGHORDER HARMONICS:1||Xray laser:1||atomic transition:1||EXCITATION:1||LASERS:1||PERFORMANCE:1||RELATIVISTIC ELECTRONS:1||BI2O3DOPED ZNO:1||INNERSHELL IONIZATION:1||Laser wakefield:1||FREQUENCY:1||SOLIDSTATE LASERS:1||Linearly polarized:1||THERMIONIC EMISSION:1||PULSE AMPLIFICATION SYSTEM:1||BIB3O6:1||NM:1||NONCOVALENT INTERACTIONS:1||CRYSTALLINE:1||INTENSITY:1||JETS:1||COHERENT:1||LINE:1||ANGULARDISTRIBUTION:1||SILVER IONS:1||magnetic anisotropy:1||DEVICES:1||Auger transitions:1||CosterKronig transitions:1||EFFICIENT:1||ELECTRONIMPACT IONIZATION:1||ULTRASHORTPULSE:1||Nanowire:1||Heterostructure:1||soft Xray reflectivity:1||PLASMA ACCELERATOR:1||ZINCOXIDE NANOWIRES:1||CHEMICALVAPORDEPOSITION:1||Electron acceleration:1||Ionization of gases:1||Delay dependent:1||MULTIPHOTON IONIZATION:1||FRAGMENTATION:1||GASJET:1||ultrafast nonlinear optics:1||CYCLE PULSES:1||KHZ:1||chemical vapor deposition:1||ferromagnetism:1||ABSORPTION:1||TERAHERTZ RADIATION:1||SCIENCE:1||FIELDS:1||ELECTRONS:1||nanomultilayer structures:1||YIELDS:1||AUGER:1||10HZ REPETITION RATE:1||MULTITERAWATT:1||SPECTROGRAPH:1||HIGHHARMONICGENERATION:1||spectroscopy:1||level population:1||PARTICLEACCELERATION:1||OPTICAL FREQUENCYMEASUREMENT:1||NANOWALLS:1||ROOMTEMPERATURE:1||AVERAGE OUTPUT POWER:1||GROUPVELOCITYMISMATCH:1||Impact ionization:1||Dynamics:1||Lasers:1||Collisional process:1||ABOVETHRESHOLD IONIZATION:1||MAINGROUP THERMOCHEMISTRY:1||dilute magnetic semiconductors:1||GACRN:1||SIZE:1||ATTOSECOND:1||Ar cluster:1||Xray astrophysics:1||photoionization:1||irons:1||normal incidence pulsed laser deposition:1||SHELLS:1||Silicon Oxide:1||gaspuff Zpinch:1||Xray:1||soft Xray reflectors:1||ESCAPE:1||ZN2SIO4:1||SILICA:1||Time delay:1||Collisional plasmas:1||MASSSPECTROMETRY:1||NUCLEARFUSION:1||PARAMETRIC AMPLIFICATION:1||LYING ELECTRONIC STATES:1||ADJUSTABLEPARAMETERS:1||MAGNETICPROPERTIES:1||LIQUIDPHASE EPITAXY:1||CEP laser:1||REGION:1||Plasma waveguide:1||AMBIENT GAS:1||DEPOSITION:1||HARMONICGENERATION:1||ENHANCEMENT:1||imaging spectrometer:1||Abel inversion:1||Water window:1||Liquid nitrogen jet:1||CHARGEEXCHANGE:1||NOBEL LECTURE:1||VARISTOR:1||EPITAXY:1||THINDISK LASER:1||HIGHREPETITIONRATE:1||Atom lasers:1||Electronimpact excitation:1||High order harmonics:1||ultrafast technology:1||PEAK POWER:1||CHARGED ALUMINUM CLUSTERS:1||GaN:1||THIN:1||Electron beam:1||INTENSE:1||Hard Xray pulse generation:1||NONLINEAR THOMSON SCATTERING:1||MULTILAYER:1||UVvisible spectrometer:1||ATOMS:1||innershell transitions:1||CORRECTED CONCAVE GRATINGS:1||DISCHARGE:1||LASERPLASMA:1||thin film:1||reflectivity:1||opacity:1||gain:1||smallangle Xray scattering:1||SOFTXRAY:1||ZINCOXIDE:1||CYGNUSX3:1||Betatron oscillation:1||ACCELERATOR:1||STRAINEDLAYER SUPERLATTICES:1||OPTICAL PARAMETRIC AMPLIFICATION:1||PASSIVE MODELOCKING:1||Collision dynamics:1||MUM:1||EXACTEXCHANGE:1||BASISSET:1||APPROXIMATION:1||OXYNITRIDES:1||Beam energy modulation:1||polarization spectroscopy:1||REORIENTATION TRANSITION:1||DEPENDENCE:1||sulfurs:1||BUILDINGBLOCKS:1||RATES:1||OPTICAL PULSES:1||toroidal mirror:1||XRAY LASER:1||CALCIUM:1||radially polarized laser:1||GRAINBOUNDARIES:1||VAPORDEPOSITION:1||Xray generation:1||MAGNETIZATION:1||Electric excitation:1||Laserinduced gas plasmas:1||Qualitative analysis:1||SCHEME:1||RADIATION:10||PULSES:8||PHOTOLUMINESCENCE:7||LASER:7||GENERATION:6||NANORODS:6||GROWTH:6||NANOWIRES:5||IMPLANTED 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SEMICONDUCTORS:2||MOLECULARBEAM EPITAXY:2||EARTHDOPED GAN:2||LASER FIELDS:2||CHIRPEDPULSEAMPLIFICATION:2||ALN:2||GAUSSIANBEAM:2||ASSISTED CATALYTIC GROWTH:2||BLUE:2||NANOSTRUCTURES:2||MAGNETOELECTRONICS:2||MICROSCOPY:2||ELECTROLUMINESCENCE:2||LASERPULSES:2||GaN nanowires:2||GALLIUM NITRIDE NANOWIRES:2||GAMNN:2||NANOTUBES:2||PHYSICS:2||Femtosecond laser:2||parametric oscillators and amplifiers:1||ultrafast lasers:1||VALENCE:1||nanowires:1||DILUTED MAGNETIC SEMICONDUCTOR:1||LUMINESCENCE:1||Density modulation:1||Energy modulation:1||Current enhanced SASE free electron laser:1||Undulator radiation:1||FREEELECTRON LASERS:1||ULTRATHIN FERROMAGNETICFILMS:1||OXIDEFILMS:1||ABLATION:1||COMPONENT:1||METAL:1||innershell excited states:1||Nelike ions:1||TRANSITIONS:1||XUV spectrometer:1||DIAGNOSTICS:1||Xray scattering:1||MO/SI:1||pulsed laser deposition:1||KEV IMPACT ENERGIES:1||vacuum electron acceleration:1||HIGHINTENSITY LASER:1||JUNCTIONS:1||LOWTEMPERATURE GROWTH:1||nanocrystalline materials:1||MOLECULAR PHOTOIONIZATION:1||LOCALIZATION:1||DEUTERIUM CLUSTERS:1||EXPLOSIONS:1||REGENERATIVE AMPLIFIERS:1||RAREGASES:1||THz radiation:1||FREEELECTRON LASER:1||REALTIME OBSERVATION:1||TARGET:1||photoionized plasmas:1||fs Xray laser:1||emission profile:1||HIGHORDER HARMONICS:1||Xray laser:1||atomic transition:1||EXCITATION:1||LASERS:1||PERFORMANCE:1||RELATIVISTIC ELECTRONS:1||BI2O3DOPED ZNO:1||INNERSHELL IONIZATION:1||Laser wakefield:1||FREQUENCY:1||SOLIDSTATE LASERS:1||Linearly polarized:1||THERMIONIC EMISSION:1||PULSE AMPLIFICATION SYSTEM:1||BIB3O6:1||NM:1||NONCOVALENT INTERACTIONS:1||CRYSTALLINE:1||INTENSITY:1||JETS:1||COHERENT:1||LINE:1||ANGULARDISTRIBUTION:1||SILVER IONS:1||magnetic anisotropy:1||DEVICES:1||Auger transitions:1||CosterKronig transitions:1||EFFICIENT:1||ELECTRONIMPACT IONIZATION:1||ULTRASHORTPULSE:1||Nanowire:1||Heterostructure:1||soft Xray reflectivity:1||PLASMA ACCELERATOR:1||ZINCOXIDE NANOWIRES:1||CHEMICALVAPORDEPOSITION:1||Electron acceleration:1||Ionization of gases:1||Delay dependent:1||MULTIPHOTON IONIZATION:1||FRAGMENTATION:1||GASJET:1||ultrafast nonlinear optics:1||CYCLE PULSES:1||KHZ:1||chemical vapor deposition:1||ferromagnetism:1||ABSORPTION:1||TERAHERTZ RADIATION:1||SCIENCE:1||FIELDS:1||ELECTRONS:1||nanomultilayer structures:1||YIELDS:1||AUGER:1||10HZ REPETITION RATE:1||MULTITERAWATT:1||SPECTROGRAPH:1||HIGHHARMONICGENERATION:1||spectroscopy:1||level population:1||PARTICLEACCELERATION:1||OPTICAL FREQUENCYMEASUREMENT:1||NANOWALLS:1||ROOMTEMPERATURE:1||AVERAGE OUTPUT POWER:1||GROUPVELOCITYMISMATCH:1||Impact ionization:1||Dynamics:1||Lasers:1||Collisional process:1||ABOVETHRESHOLD IONIZATION:1||MAINGROUP THERMOCHEMISTRY:1||dilute magnetic semiconductors:1||GACRN:1||SIZE:1||ATTOSECOND:1||Ar cluster:1||Xray astrophysics:1||photoionization:1||irons:1||normal incidence pulsed laser deposition:1||SHELLS:1||Silicon Oxide:1||gaspuff Zpinch:1||Xray:1||soft Xray reflectors:1||ESCAPE:1||ZN2SIO4:1||SILICA:1||Time 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materials:1||MOLECULAR PHOTOIONIZATION:1||LOCALIZATION:1||DEUTERIUM CLUSTERS:1||EXPLOSIONS:1||REGENERATIVE AMPLIFIERS:1||RAREGASES:1||THz radiation:1||FREEELECTRON LASER:1||REALTIME OBSERVATION:1||TARGET:1||photoionized plasmas:1||fs Xray laser:1||emission profile:1||HIGHORDER HARMONICS:1||Xray laser:1||atomic transition:1||EXCITATION:1||LASERS:1||PERFORMANCE:1||RELATIVISTIC ELECTRONS:1||BI2O3DOPED ZNO:1||INNERSHELL IONIZATION:1||Laser wakefield:1||FREQUENCY:1||SOLIDSTATE LASERS:1||Linearly polarized:1||THERMIONIC EMISSION:1||PULSE AMPLIFICATION SYSTEM:1||BIB3O6:1||NM:1||NONCOVALENT INTERACTIONS:1||CRYSTALLINE:1||INTENSITY:1||JETS:1||COHERENT:1||LINE:1||ANGULARDISTRIBUTION:1||SILVER IONS:1||magnetic anisotropy:1||DEVICES:1||Auger transitions:1||CosterKronig transitions:1||EFFICIENT:1||ELECTRONIMPACT IONIZATION:1||ULTRASHORTPULSE:1||Nanowire:1||Heterostructure:1||soft Xray reflectivity:1||PLASMA ACCELERATOR:1||ZINCOXIDE NANOWIRES:1||CHEMICALVAPORDEPOSITION:1||Electron acceleration:1||Ionization of gases:1||Delay dependent:1||MULTIPHOTON IONIZATION:1||FRAGMENTATION:1||GASJET:1||ultrafast nonlinear optics:1||CYCLE PULSES:1||KHZ:1||chemical vapor deposition:1||ferromagnetism:1||ABSORPTION:1||TERAHERTZ RADIATION:1||SCIENCE:1||FIELDS:1||ELECTRONS:1||nanomultilayer structures:1||YIELDS:1||AUGER:1||10HZ REPETITION RATE:1||MULTITERAWATT:1||SPECTROGRAPH:1||HIGHHARMONICGENERATION:1||spectroscopy:1||level population:1||PARTICLEACCELERATION:1||OPTICAL FREQUENCYMEASUREMENT:1||NANOWALLS:1||ROOMTEMPERATURE:1||AVERAGE OUTPUT POWER:1||GROUPVELOCITYMISMATCH:1||Impact ionization:1||Dynamics:1||Lasers:1||Collisional process:1||ABOVETHRESHOLD IONIZATION:1||MAINGROUP THERMOCHEMISTRY:1||dilute magnetic semiconductors:1||GACRN:1||SIZE:1||ATTOSECOND:1||Ar cluster:1||Xray astrophysics:1||photoionization:1||irons:1||normal incidence pulsed laser deposition:1||SHELLS:1||Silicon Oxide:1||gaspuff Zpinch:1||Xray:1||soft Xray reflectors:1||ESCAPE:1||ZN2SIO4:1||SILICA:1||Time delay:1||Collisional plasmas:1||MASSSPECTROMETRY:1||NUCLEARFUSION:1||PARAMETRIC AMPLIFICATION:1||LYING ELECTRONIC STATES:1||ADJUSTABLEPARAMETERS:1||MAGNETICPROPERTIES:1||LIQUIDPHASE EPITAXY:1||CEP laser:1||REGION:1||Plasma waveguide:1||AMBIENT GAS:1||DEPOSITION:1||HARMONICGENERATION:1||ENHANCEMENT:1||imaging spectrometer:1||Abel inversion:1||Water window:1||Liquid nitrogen jet:1||CHARGEEXCHANGE:1||NOBEL LECTURE:1||VARISTOR:1||EPITAXY:1||THINDISK LASER:1||HIGHREPETITIONRATE:1||Atom lasers:1||Electronimpact excitation:1||High order harmonics:1||ultrafast technology:1||PEAK POWER:1||CHARGED ALUMINUM CLUSTERS:1||GaN:1||THIN:1||Electron beam:1||INTENSE:1||Hard Xray pulse generation:1||NONLINEAR THOMSON SCATTERING:1||MULTILAYER:1||UVvisible spectrometer:1||ATOMS:1||innershell transitions:1||CORRECTED CONCAVE GRATINGS:1||DISCHARGE:1||LASERPLASMA:1||thin film:1||reflectivity:1||opacity:1||gain:1||smallangle Xray scattering:1||SOFTXRAY:1||ZINCOXIDE:1||CYGNUSX3:1||Betatron oscillation:1||ACCELERATOR:1||STRAINEDLAYER SUPERLATTICES:1||OPTICAL PARAMETRIC AMPLIFICATION:1||PASSIVE MODELOCKING:1||Collision dynamics:1||MUM:1||EXACTEXCHANGE:1||BASISSET:1||APPROXIMATION:1||OXYNITRIDES:1||Beam energy modulation:1||polarization spectroscopy:1||REORIENTATION TRANSITION:1||DEPENDENCE:1||sulfurs:1||BUILDINGBLOCKS:1||RATES:1||OPTICAL PULSES:1||toroidal mirror:1||XRAY LASER:1||CALCIUM:1||radially polarized laser:1||GRAINBOUNDARIES:1||VAPORDEPOSITION:1||Xray generation:1||MAGNETIZATION:1||Electric excitation:1||Laserinduced gas plasmas:1||Qualitative analysis:1||SCHEME:1||RADIATION:10||PULSES:8||PHOTOLUMINESCENCE:7||LASER:7||GENERATION:6||NANORODS:6||GROWTH:6||NANOWIRES:5||IMPLANTED GAN:5||SPECTROSCOPY:5||THINFILMS:4||DYNAMICS:4||SILICON:4||EXTREMEULTRAVIOLET:4||AMPLIFICATION:4||PRESSURE:4||PHASE:4||OPTICALPROPERTIES:4||SYSTEM:4||EMISSION:4||FEL:3||N2O:3||FILMS:3||OPTICS:3||SPECTRA:3||FIELD:3||MIRRORS:3||ARRAYS:3||CLUSTERS:3||SIO2:3||IONIZATION:3||VACUUM:3||SCATTERING:3||IONS:2||LUMINESCENCE PROPERTIES:2||ANISOTROPY:2||BEAMS:2||DIFFRACTION:2||DISPERSION:2||chemical vapor deposition (CVD):2||ELECTRONICSTRUCTURE:2||MOSFETS:2||SI3N4:2||DENSITY:2||LIGHT:2||PLASMAS:2||MATTER:2||nanocomposites:2||RAMANSCATTERING:2||NANOPARTICLES:2||OXIDE:2||AMPLIFIED SPONTANEOUS EMISSION:2||NM WAVELENGTH:2||GAIN:2||CARBON NANOTUBES:2||CROSSSECTIONS:2||LIGHTEMITTINGDIODES:2||PULSE:2||CARBON PLASMA:2||TISAPPHIRE LASER:2||Raman scattering:2||ROUTE:2||multilayer:2||CATHODOLUMINESCENCE:2||highresolution transmission electronic microscope (HRTEM):2||DIFFERENCEFREQUENCYGENERATION:2||CRYSTAL:2||laserproduced plasma:2||NANOCABLES:2||photoluminescence:2||MAGNETIC ALLOY SEMICONDUCTORS:2||MOLECULARBEAM EPITAXY:2||EARTHDOPED GAN:2||LASER FIELDS:2||CHIRPEDPULSEAMPLIFICATION:2||ALN:2||GAUSSIANBEAM:2||ASSISTED CATALYTIC GROWTH:2||BLUE:2||NANOSTRUCTURES:2||MAGNETOELECTRONICS:2||MICROSCOPY:2||ELECTROLUMINESCENCE:2||LASERPULSES:2||GaN nanowires:2||GALLIUM NITRIDE NANOWIRES:2||GAMNN:2||NANOTUBES:2||PHYSICS:2||Femtosecond laser:2||parametric oscillators and amplifiers:1||ultrafast lasers:1||VALENCE:1||nanowires:1||DILUTED MAGNETIC SEMICONDUCTOR:1||LUMINESCENCE:1||Density modulation:1||Energy modulation:1||Current enhanced SASE free electron laser:1||Undulator radiation:1||FREEELECTRON LASERS:1||ULTRATHIN FERROMAGNETICFILMS:1||OXIDEFILMS:1||ABLATION:1||COMPONENT:1||METAL:1||innershell excited states:1||Nelike ions:1||TRANSITIONS:1||XUV spectrometer:1||DIAGNOSTICS:1||Xray scattering:1||MO/SI:1||pulsed laser deposition:1||KEV IMPACT ENERGIES:1||vacuum electron acceleration:1||HIGHINTENSITY LASER:1||JUNCTIONS:1||LOWTEMPERATURE GROWTH:1||nanocrystalline materials:1||MOLECULAR PHOTOIONIZATION:1||LOCALIZATION:1||DEUTERIUM CLUSTERS:1||EXPLOSIONS:1||REGENERATIVE AMPLIFIERS:1||RAREGASES:1||THz radiation:1||FREEELECTRON LASER:1||REALTIME OBSERVATION:1||TARGET:1||photoionized plasmas:1||fs Xray laser:1||emission profile:1||HIGHORDER HARMONICS:1||Xray laser:1||atomic transition:1||EXCITATION:1||LASERS:1||PERFORMANCE:1||RELATIVISTIC ELECTRONS:1||BI2O3DOPED ZNO:1||INNERSHELL IONIZATION:1||Laser wakefield:1||FREQUENCY:1||SOLIDSTATE LASERS:1||Linearly polarized:1||THERMIONIC EMISSION:1||PULSE AMPLIFICATION SYSTEM:1||BIB3O6:1||NM:1||NONCOVALENT INTERACTIONS:1||CRYSTALLINE:1||INTENSITY:1||JETS:1||COHERENT:1||LINE:1||ANGULARDISTRIBUTION:1||SILVER IONS:1||magnetic anisotropy:1||DEVICES:1||Auger transitions:1||CosterKronig transitions:1||EFFICIENT:1||ELECTRONIMPACT IONIZATION:1||ULTRASHORTPULSE:1||Nanowire:1||Heterostructure:1||soft Xray reflectivity:1||PLASMA ACCELERATOR:1||ZINCOXIDE NANOWIRES:1||CHEMICALVAPORDEPOSITION:1||Electron acceleration:1||Ionization of gases:1||Delay dependent:1||MULTIPHOTON IONIZATION:1||FRAGMENTATION:1||GASJET:1||ultrafast nonlinear optics:1||CYCLE PULSES:1||KHZ:1||chemical vapor deposition:1||ferromagnetism:1||ABSORPTION:1||TERAHERTZ RADIATION:1||SCIENCE:1||FIELDS:1||ELECTRONS:1||nanomultilayer structures:1||YIELDS:1||AUGER:1||10HZ REPETITION RATE:1||MULTITERAWATT:1||SPECTROGRAPH:1||HIGHHARMONICGENERATION:1||spectroscopy:1||level population:1||PARTICLEACCELERATION:1||OPTICAL FREQUENCYMEASUREMENT:1||NANOWALLS:1||ROOMTEMPERATURE:1||AVERAGE OUTPUT POWER:1||GROUPVELOCITYMISMATCH:1||Impact ionization:1||Dynamics:1||Lasers:1||Collisional process:1||ABOVETHRESHOLD IONIZATION:1||MAINGROUP THERMOCHEMISTRY:1||dilute magnetic semiconductors:1||GACRN:1||SIZE:1||ATTOSECOND:1||Ar cluster:1||Xray astrophysics:1||photoionization:1||irons:1||normal incidence pulsed laser deposition:1||SHELLS:1||Silicon Oxide:1||gaspuff Zpinch:1||Xray:1||soft Xray reflectors:1||ESCAPE:1||ZN2SIO4:1||SILICA:1||Time delay:1||Collisional plasmas:1||MASSSPECTROMETRY:1||NUCLEARFUSION:1||PARAMETRIC AMPLIFICATION:1||LYING ELECTRONIC STATES:1||ADJUSTABLEPARAMETERS:1||MAGNETICPROPERTIES:1||LIQUIDPHASE EPITAXY:1||CEP laser:1||REGION:1||Plasma waveguide:1||AMBIENT GAS:1||DEPOSITION:1||HARMONICGENERATION:1||ENHANCEMENT:1||imaging spectrometer:1||Abel inversion:1||Water window:1||Liquid nitrogen jet:1||CHARGEEXCHANGE:1||NOBEL LECTURE:1||VARISTOR:1||EPITAXY:1||THINDISK LASER:1||HIGHREPETITIONRATE:1||Atom lasers:1||Electronimpact excitation:1||High order harmonics:1||ultrafast technology:1||PEAK POWER:1||CHARGED ALUMINUM CLUSTERS:1||GaN:1||THIN:1||Electron beam:1||INTENSE:1||Hard Xray pulse generation:1||NONLINEAR THOMSON SCATTERING:1||MULTILAYER:1||UVvisible spectrometer:1||ATOMS:1||innershell transitions:1||CORRECTED CONCAVE GRATINGS:1||DISCHARGE:1||LASERPLASMA:1||thin film:1||reflectivity:1||opacity:1||gain:1||smallangle Xray scattering:1||SOFTXRAY:1||ZINCOXIDE:1||CYGNUSX3:1||Betatron oscillation:1||ACCELERATOR:1||STRAINEDLAYER SUPERLATTICES:1||OPTICAL PARAMETRIC AMPLIFICATION:1||PASSIVE MODELOCKING:1||Collision dynamics:1||MUM:1||EXACTEXCHANGE:1||BASISSET:1||APPROXIMATION:1||OXYNITRIDES:1||Beam energy modulation:1||polarization spectroscopy:1||REORIENTATION TRANSITION:1||DEPENDENCE:1||sulfurs:1||BUILDINGBLOCKS:1||RATES:1||OPTICAL PULSES:1||toroidal mirror:1||XRAY LASER:1||CALCIUM:1||radially polarized laser:1||GRAINBOUNDARIES:1||VAPORDEPOSITION:1||Xray generation:1||MAGNETIZATION:1||Electric excitation:1||Laserinduced gas plasmas:1||Qualitative analysis:1||SCHEME:1||RADIATION:10||PULSES:8||PHOTOLUMINESCENCE:7||LASER:7||GENERATION:6||NANORODS:6||GROWTH:6||NANOWIRES:5||IMPLANTED 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SEMICONDUCTORS:2||MOLECULARBEAM EPITAXY:2||EARTHDOPED GAN:2||LASER FIELDS:2||CHIRPEDPULSEAMPLIFICATION:2||ALN:2||GAUSSIANBEAM:2||ASSISTED CATALYTIC GROWTH:2||BLUE:2||NANOSTRUCTURES:2||MAGNETOELECTRONICS:2||MICROSCOPY:2||ELECTROLUMINESCENCE:2||LASERPULSES:2||GaN nanowires:2||GALLIUM NITRIDE NANOWIRES:2||GAMNN:2||NANOTUBES:2||PHYSICS:2||Femtosecond laser:2||parametric oscillators and amplifiers:1||ultrafast lasers:1||VALENCE:1||nanowires:1||DILUTED MAGNETIC SEMICONDUCTOR:1||LUMINESCENCE:1||Density modulation:1||Energy modulation:1||Current enhanced SASE free electron laser:1||Undulator radiation:1||FREEELECTRON LASERS:1||ULTRATHIN FERROMAGNETICFILMS:1||OXIDEFILMS:1||ABLATION:1||COMPONENT:1||METAL:1||innershell excited states:1||Nelike ions:1||TRANSITIONS:1||XUV spectrometer:1||DIAGNOSTICS:1||Xray scattering:1||MO/SI:1||pulsed laser deposition:1||KEV IMPACT ENERGIES:1||vacuum electron acceleration:1||HIGHINTENSITY LASER:1||JUNCTIONS:1||LOWTEMPERATURE GROWTH:1||nanocrystalline materials:1||MOLECULAR PHOTOIONIZATION:1||LOCALIZATION:1||DEUTERIUM CLUSTERS:1||EXPLOSIONS:1||REGENERATIVE AMPLIFIERS:1||RAREGASES:1||THz radiation:1||FREEELECTRON LASER:1||REALTIME OBSERVATION:1||TARGET:1||photoionized plasmas:1||fs Xray laser:1||emission profile:1||HIGHORDER HARMONICS:1||Xray laser:1||atomic transition:1||EXCITATION:1||LASERS:1||PERFORMANCE:1||RELATIVISTIC ELECTRONS:1||BI2O3DOPED ZNO:1||INNERSHELL IONIZATION:1||Laser wakefield:1||FREQUENCY:1||SOLIDSTATE LASERS:1||Linearly polarized:1||THERMIONIC EMISSION:1||PULSE AMPLIFICATION SYSTEM:1||BIB3O6:1||NM:1||NONCOVALENT INTERACTIONS:1||CRYSTALLINE:1||INTENSITY:1||JETS:1||COHERENT:1||LINE:1||ANGULARDISTRIBUTION:1||SILVER IONS:1||magnetic anisotropy:1||DEVICES:1||Auger transitions:1||CosterKronig transitions:1||EFFICIENT:1||ELECTRONIMPACT IONIZATION:1||ULTRASHORTPULSE:1||Nanowire:1||Heterostructure:1||soft Xray reflectivity:1||PLASMA ACCELERATOR:1||ZINCOXIDE NANOWIRES:1||CHEMICALVAPORDEPOSITION:1||Electron acceleration:1||Ionization of gases:1||Delay dependent:1||MULTIPHOTON IONIZATION:1||FRAGMENTATION:1||GASJET:1||ultrafast nonlinear optics:1||CYCLE PULSES:1||KHZ:1||chemical vapor deposition:1||ferromagnetism:1||ABSORPTION:1||TERAHERTZ RADIATION:1||SCIENCE:1||FIELDS:1||ELECTRONS:1||nanomultilayer structures:1||YIELDS:1||AUGER:1||10HZ REPETITION RATE:1||MULTITERAWATT:1||SPECTROGRAPH:1||HIGHHARMONICGENERATION:1||spectroscopy:1||level population:1||PARTICLEACCELERATION:1||OPTICAL FREQUENCYMEASUREMENT:1||NANOWALLS:1||ROOMTEMPERATURE:1||AVERAGE OUTPUT POWER:1||GROUPVELOCITYMISMATCH:1||Impact ionization:1||Dynamics:1||Lasers:1||Collisional process:1||ABOVETHRESHOLD IONIZATION:1||MAINGROUP THERMOCHEMISTRY:1||dilute magnetic semiconductors:1||GACRN:1||SIZE:1||ATTOSECOND:1||Ar cluster:1||Xray astrophysics:1||photoionization:1||irons:1||normal incidence pulsed laser deposition:1||SHELLS:1||Silicon Oxide:1||gaspuff Zpinch:1||Xray:1||soft Xray reflectors:1||ESCAPE:1||ZN2SIO4:1||SILICA:1||Time 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materials:1||MOLECULAR PHOTOIONIZATION:1||LOCALIZATION:1||DEUTERIUM CLUSTERS:1||EXPLOSIONS:1||REGENERATIVE AMPLIFIERS:1||RAREGASES:1||THz radiation:1||FREEELECTRON LASER:1||REALTIME OBSERVATION:1||TARGET:1||photoionized plasmas:1||fs Xray laser:1||emission profile:1||HIGHORDER HARMONICS:1||Xray laser:1||atomic transition:1||EXCITATION:1||LASERS:1||PERFORMANCE:1||RELATIVISTIC ELECTRONS:1||BI2O3DOPED ZNO:1||INNERSHELL IONIZATION:1||Laser wakefield:1||FREQUENCY:1||SOLIDSTATE LASERS:1||Linearly polarized:1||THERMIONIC EMISSION:1||PULSE AMPLIFICATION SYSTEM:1||BIB3O6:1||NM:1||NONCOVALENT INTERACTIONS:1||CRYSTALLINE:1||INTENSITY:1||JETS:1||COHERENT:1||LINE:1||ANGULARDISTRIBUTION:1||SILVER IONS:1||magnetic anisotropy:1||DEVICES:1||Auger transitions:1||CosterKronig transitions:1||EFFICIENT:1||ELECTRONIMPACT IONIZATION:1||ULTRASHORTPULSE:1||Nanowire:1||Heterostructure:1||soft Xray reflectivity:1||PLASMA ACCELERATOR:1||ZINCOXIDE NANOWIRES:1||CHEMICALVAPORDEPOSITION:1||Electron acceleration:1||Ionization of gases:1||Delay dependent:1||MULTIPHOTON IONIZATION:1||FRAGMENTATION:1||GASJET:1||ultrafast nonlinear optics:1||CYCLE PULSES:1||KHZ:1||chemical vapor deposition:1||ferromagnetism:1||ABSORPTION:1||TERAHERTZ RADIATION:1||SCIENCE:1||FIELDS:1||ELECTRONS:1||nanomultilayer structures:1||YIELDS:1||AUGER:1||10HZ REPETITION RATE:1||MULTITERAWATT:1||SPECTROGRAPH:1||HIGHHARMONICGENERATION:1||spectroscopy:1||level population:1||PARTICLEACCELERATION:1||OPTICAL FREQUENCYMEASUREMENT:1||NANOWALLS:1||ROOMTEMPERATURE:1||AVERAGE OUTPUT POWER:1||GROUPVELOCITYMISMATCH:1||Impact ionization:1||Dynamics:1||Lasers:1||Collisional process:1||ABOVETHRESHOLD IONIZATION:1||MAINGROUP THERMOCHEMISTRY:1||dilute magnetic semiconductors:1||GACRN:1||SIZE:1||ATTOSECOND:1||Ar cluster:1||Xray astrophysics:1||photoionization:1||irons:1||normal incidence pulsed laser deposition:1||SHELLS:1||Silicon Oxide:1||gaspuff Zpinch:1||Xray:1||soft Xray reflectors:1||ESCAPE:1||ZN2SIO4:1||SILICA:1||Time delay:1||Collisional plasmas:1||MASSSPECTROMETRY:1||NUCLEARFUSION:1||PARAMETRIC AMPLIFICATION:1||LYING ELECTRONIC STATES:1||ADJUSTABLEPARAMETERS:1||MAGNETICPROPERTIES:1||LIQUIDPHASE EPITAXY:1||CEP laser:1||REGION:1||Plasma waveguide:1||AMBIENT GAS:1||DEPOSITION:1||HARMONICGENERATION:1||ENHANCEMENT:1||imaging spectrometer:1||Abel inversion:1||Water window:1||Liquid nitrogen jet:1||CHARGEEXCHANGE:1||NOBEL LECTURE:1||VARISTOR:1||EPITAXY:1||THINDISK LASER:1||HIGHREPETITIONRATE:1||Atom lasers:1||Electronimpact excitation:1||High order harmonics:1||ultrafast technology:1||PEAK POWER:1||CHARGED ALUMINUM CLUSTERS:1||GaN:1||THIN:1||Electron beam:1||INTENSE:1||Hard Xray pulse generation:1||NONLINEAR THOMSON SCATTERING:1||MULTILAYER:1||UVvisible spectrometer:1||ATOMS:1||innershell transitions:1||CORRECTED CONCAVE GRATINGS:1||DISCHARGE:1||LASERPLASMA:1||thin film:1||reflectivity:1||opacity:1||gain:1||smallangle Xray scattering:1||SOFTXRAY:1||ZINCOXIDE:1||CYGNUSX3:1||Betatron oscillation:1||ACCELERATOR:1||STRAINEDLAYER SUPERLATTICES:1||OPTICAL PARAMETRIC AMPLIFICATION:1||PASSIVE MODELOCKING:1||Collision dynamics:1||MUM:1||EXACTEXCHANGE:1||BASISSET:1||APPROXIMATION:1||OXYNITRIDES:1||Beam energy modulation:1||polarization spectroscopy:1||REORIENTATION TRANSITION:1||DEPENDENCE:1||sulfurs:1||BUILDINGBLOCKS:1||RATES:1||OPTICAL PULSES:1||toroidal mirror:1||XRAY LASER:1||CALCIUM:1||radially polarized laser:1||GRAINBOUNDARIES:1||VAPORDEPOSITION:1||Xray generation:1||MAGNETIZATION:1||Electric excitation:1||Laserinduced gas plasmas:1||Qualitative analysis:1||SCHEME:1||RADIATION:10||PULSES:8||PHOTOLUMINESCENCE:7||LASER:7||GENERATION:6||NANORODS:6||GROWTH:6||NANOWIRES:5||IMPLANTED GAN:5||SPECTROSCOPY:5||THINFILMS:4||DYNAMICS:4||SILICON:4||EXTREMEULTRAVIOLET:4||AMPLIFICATION:4||PRESSURE:4||PHASE:4||OPTICALPROPERTIES:4||SYSTEM:4||EMISSION:4||FEL:3||N2O:3||FILMS:3||OPTICS:3||SPECTRA:3||FIELD:3||MIRRORS:3||ARRAYS:3||CLUSTERS:3||SIO2:3||IONIZATION:3||VACUUM:3||SCATTERING:3||IONS:2||LUMINESCENCE PROPERTIES:2||ANISOTROPY:2||BEAMS:2||DIFFRACTION:2||DISPERSION:2||chemical vapor deposition (CVD):2||ELECTRONICSTRUCTURE:2||MOSFETS:2||SI3N4:2||DENSITY:2||LIGHT:2||PLASMAS:2||MATTER:2||nanocomposites:2||RAMANSCATTERING:2||NANOPARTICLES:2||OXIDE:2||AMPLIFIED SPONTANEOUS EMISSION:2||NM WAVELENGTH:2||GAIN:2||CARBON NANOTUBES:2||CROSSSECTIONS:2||LIGHTEMITTINGDIODES:2||PULSE:2||CARBON PLASMA:2||TISAPPHIRE LASER:2||Raman scattering:2||ROUTE:2||multilayer:2||CATHODOLUMINESCENCE:2||highresolution transmission electronic microscope (HRTEM):2||DIFFERENCEFREQUENCYGENERATION:2||CRYSTAL:2||laserproduced plasma:2||NANOCABLES:2||photoluminescence:2||MAGNETIC ALLOY SEMICONDUCTORS:2||MOLECULARBEAM EPITAXY:2||EARTHDOPED GAN:2||LASER FIELDS:2||CHIRPEDPULSEAMPLIFICATION:2||ALN:2||GAUSSIANBEAM:2||ASSISTED CATALYTIC GROWTH:2||BLUE:2||NANOSTRUCTURES:2||MAGNETOELECTRONICS:2||MICROSCOPY:2||ELECTROLUMINESCENCE:2||LASERPULSES:2||GaN nanowires:2||GALLIUM NITRIDE NANOWIRES:2||GAMNN:2||NANOTUBES:2||PHYSICS:2||Femtosecond laser:2||parametric oscillators and amplifiers:1||ultrafast lasers:1||VALENCE:1||nanowires:1||DILUTED MAGNETIC SEMICONDUCTOR:1||LUMINESCENCE:1||Density modulation:1||Energy modulation:1||Current enhanced SASE free electron laser:1||Undulator radiation:1||FREEELECTRON LASERS:1||ULTRATHIN FERROMAGNETICFILMS:1||OXIDEFILMS:1||ABLATION:1||COMPONENT:1||METAL:1||innershell excited states:1||Nelike ions:1||TRANSITIONS:1||XUV spectrometer:1||DIAGNOSTICS:1||Xray scattering:1||MO/SI:1||pulsed laser deposition:1||KEV IMPACT ENERGIES:1||vacuum electron acceleration:1||HIGHINTENSITY LASER:1||JUNCTIONS:1||LOWTEMPERATURE GROWTH:1||nanocrystalline materials:1||MOLECULAR PHOTOIONIZATION:1||LOCALIZATION:1||DEUTERIUM CLUSTERS:1||EXPLOSIONS:1||REGENERATIVE AMPLIFIERS:1||RAREGASES:1||THz radiation:1||FREEELECTRON LASER:1||REALTIME OBSERVATION:1||TARGET:1||photoionized plasmas:1||fs Xray laser:1||emission profile:1||HIGHORDER HARMONICS:1||Xray laser:1||atomic transition:1||EXCITATION:1||LASERS:1||PERFORMANCE:1||RELATIVISTIC ELECTRONS:1||BI2O3DOPED ZNO:1||INNERSHELL IONIZATION:1||Laser wakefield:1||FREQUENCY:1||SOLIDSTATE LASERS:1||Linearly polarized:1||THERMIONIC EMISSION:1||PULSE AMPLIFICATION SYSTEM:1||BIB3O6:1||NM:1||NONCOVALENT INTERACTIONS:1||CRYSTALLINE:1||INTENSITY:1||JETS:1||COHERENT:1||LINE:1||ANGULARDISTRIBUTION:1||SILVER IONS:1||magnetic anisotropy:1||DEVICES:1||Auger transitions:1||CosterKronig transitions:1||EFFICIENT:1||ELECTRONIMPACT IONIZATION:1||ULTRASHORTPULSE:1||Nanowire:1||Heterostructure:1||soft Xray reflectivity:1||PLASMA ACCELERATOR:1||ZINCOXIDE NANOWIRES:1||CHEMICALVAPORDEPOSITION:1||Electron acceleration:1||Ionization of gases:1||Delay dependent:1||MULTIPHOTON IONIZATION:1||FRAGMENTATION:1||GASJET:1||ultrafast nonlinear optics:1||CYCLE PULSES:1||KHZ:1||chemical vapor deposition:1||ferromagnetism:1||ABSORPTION:1||TERAHERTZ RADIATION:1||SCIENCE:1||FIELDS:1||ELECTRONS:1||nanomultilayer structures:1||YIELDS:1||AUGER:1||10HZ REPETITION RATE:1||MULTITERAWATT:1||SPECTROGRAPH:1||HIGHHARMONICGENERATION:1||spectroscopy:1||level population:1||PARTICLEACCELERATION:1||OPTICAL FREQUENCYMEASUREMENT:1||NANOWALLS:1||ROOMTEMPERATURE:1||AVERAGE OUTPUT POWER:1||GROUPVELOCITYMISMATCH:1||Impact ionization:1||Dynamics:1||Lasers:1||Collisional process:1||ABOVETHRESHOLD IONIZATION:1||MAINGROUP THERMOCHEMISTRY:1||dilute magnetic semiconductors:1||GACRN:1||SIZE:1||ATTOSECOND:1||Ar cluster:1||Xray astrophysics:1||photoionization:1||irons:1||normal incidence pulsed laser deposition:1||SHELLS:1||Silicon Oxide:1||gaspuff Zpinch:1||Xray:1||soft Xray reflectors:1||ESCAPE:1||ZN2SIO4:1||SILICA:1||Time delay:1||Collisional plasmas:1||MASSSPECTROMETRY:1||NUCLEARFUSION:1||PARAMETRIC AMPLIFICATION:1||LYING ELECTRONIC STATES:1||ADJUSTABLEPARAMETERS:1||MAGNETICPROPERTIES:1||LIQUIDPHASE EPITAXY:1||CEP laser:1||REGION:1||Plasma waveguide:1||AMBIENT GAS:1||DEPOSITION:1||HARMONICGENERATION:1||ENHANCEMENT:1||imaging spectrometer:1||Abel inversion:1||Water window:1||Liquid nitrogen jet:1||CHARGEEXCHANGE:1||NOBEL LECTURE:1||VARISTOR:1||EPITAXY:1||THINDISK LASER:1||HIGHREPETITIONRATE:1||Atom lasers:1||Electronimpact excitation:1||High order harmonics:1||ultrafast technology:1||PEAK POWER:1||CHARGED ALUMINUM CLUSTERS:1||GaN:1||THIN:1||Electron beam:1||INTENSE:1||Hard Xray pulse generation:1||NONLINEAR THOMSON SCATTERING:1||MULTILAYER:1||UVvisible spectrometer:1||ATOMS:1||innershell transitions:1||CORRECTED CONCAVE GRATINGS:1||DISCHARGE:1||LASERPLASMA:1||thin film:1||reflectivity:1||opacity:1||gain:1||smallangle Xray scattering:1||SOFTXRAY:1||ZINCOXIDE:1||CYGNUSX3:1||Betatron oscillation:1||ACCELERATOR:1||STRAINEDLAYER SUPERLATTICES:1||OPTICAL PARAMETRIC AMPLIFICATION:1||PASSIVE MODELOCKING:1||Collision dynamics:1||MUM:1||EXACTEXCHANGE:1||BASISSET:1||APPROXIMATION:1||OXYNITRIDES:1||Beam energy modulation:1||polarization spectroscopy:1||REORIENTATION TRANSITION:1||DEPENDENCE:1||sulfurs:1||BUILDINGBLOCKS:1||RATES:1||OPTICAL PULSES:1||toroidal mirror:1||XRAY LASER:1||CALCIUM:1||radially polarized laser:1||GRAINBOUNDARIES:1||VAPORDEPOSITION:1||Xray generation:1||MAGNETIZATION:1||Electric excitation:1||Laserinduced gas plasmas:1||Qualitative analysis:1||SCHEME:1||RADIATION:10||PULSES:8||PHOTOLUMINESCENCE:7||LASER:7||GENERATION:6||NANORODS:6||GROWTH:6||NANOWIRES:5||IMPLANTED 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SEMICONDUCTORS:2||MOLECULARBEAM EPITAXY:2||EARTHDOPED GAN:2||LASER FIELDS:2||CHIRPEDPULSEAMPLIFICATION:2||ALN:2||GAUSSIANBEAM:2||ASSISTED CATALYTIC GROWTH:2||BLUE:2||NANOSTRUCTURES:2||MAGNETOELECTRONICS:2||MICROSCOPY:2||ELECTROLUMINESCENCE:2||LASERPULSES:2||GaN nanowires:2||GALLIUM NITRIDE NANOWIRES:2||GAMNN:2||NANOTUBES:2||PHYSICS:2||Femtosecond laser:2||parametric oscillators and amplifiers:1||ultrafast lasers:1||VALENCE:1||nanowires:1||DILUTED MAGNETIC SEMICONDUCTOR:1||LUMINESCENCE:1||Density modulation:1||Energy modulation:1||Current enhanced SASE free electron laser:1||Undulator radiation:1||FREEELECTRON LASERS:1||ULTRATHIN FERROMAGNETICFILMS:1||OXIDEFILMS:1||ABLATION:1||COMPONENT:1||METAL:1||innershell excited states:1||Nelike ions:1||TRANSITIONS:1||XUV spectrometer:1||DIAGNOSTICS:1||Xray scattering:1||MO/SI:1||pulsed laser deposition:1||KEV IMPACT ENERGIES:1||vacuum electron acceleration:1||HIGHINTENSITY LASER:1||JUNCTIONS:1||LOWTEMPERATURE GROWTH:1||nanocrystalline materials:1||MOLECULAR PHOTOIONIZATION:1||LOCALIZATION:1||DEUTERIUM CLUSTERS:1||EXPLOSIONS:1||REGENERATIVE AMPLIFIERS:1||RAREGASES:1||THz radiation:1||FREEELECTRON LASER:1||REALTIME OBSERVATION:1||TARGET:1||photoionized plasmas:1||fs Xray laser:1||emission profile:1||HIGHORDER HARMONICS:1||Xray laser:1||atomic transition:1||EXCITATION:1||LASERS:1||PERFORMANCE:1||RELATIVISTIC ELECTRONS:1||BI2O3DOPED ZNO:1||INNERSHELL IONIZATION:1||Laser wakefield:1||FREQUENCY:1||SOLIDSTATE LASERS:1||Linearly polarized:1||THERMIONIC EMISSION:1||PULSE AMPLIFICATION SYSTEM:1||BIB3O6:1||NM:1||NONCOVALENT INTERACTIONS:1||CRYSTALLINE:1||INTENSITY:1||JETS:1||COHERENT:1||LINE:1||ANGULARDISTRIBUTION:1||SILVER IONS:1||magnetic anisotropy:1||DEVICES:1||Auger transitions:1||CosterKronig transitions:1||EFFICIENT:1||ELECTRONIMPACT IONIZATION:1||ULTRASHORTPULSE:1||Nanowire:1||Heterostructure:1||soft Xray reflectivity:1||PLASMA ACCELERATOR:1||ZINCOXIDE NANOWIRES:1||CHEMICALVAPORDEPOSITION:1||Electron acceleration:1||Ionization of gases:1||Delay dependent:1||MULTIPHOTON IONIZATION:1||FRAGMENTATION:1||GASJET:1||ultrafast nonlinear optics:1||CYCLE PULSES:1||KHZ:1||chemical vapor deposition:1||ferromagnetism:1||ABSORPTION:1||TERAHERTZ RADIATION:1||SCIENCE:1||FIELDS:1||ELECTRONS:1||nanomultilayer structures:1||YIELDS:1||AUGER:1||10HZ REPETITION RATE:1||MULTITERAWATT:1||SPECTROGRAPH:1||HIGHHARMONICGENERATION:1||spectroscopy:1||level population:1||PARTICLEACCELERATION:1||OPTICAL FREQUENCYMEASUREMENT:1||NANOWALLS:1||ROOMTEMPERATURE:1||AVERAGE OUTPUT POWER:1||GROUPVELOCITYMISMATCH:1||Impact ionization:1||Dynamics:1||Lasers:1||Collisional process:1||ABOVETHRESHOLD IONIZATION:1||MAINGROUP THERMOCHEMISTRY:1||dilute magnetic semiconductors:1||GACRN:1||SIZE:1||ATTOSECOND:1||Ar cluster:1||Xray astrophysics:1||photoionization:1||irons:1||normal incidence pulsed laser deposition:1||SHELLS:1||Silicon Oxide:1||gaspuff Zpinch:1||Xray:1||soft Xray reflectors:1||ESCAPE:1||ZN2SIO4:1||SILICA:1||Time 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materials:1||MOLECULAR PHOTOIONIZATION:1||LOCALIZATION:1||DEUTERIUM CLUSTERS:1||EXPLOSIONS:1||REGENERATIVE AMPLIFIERS:1||RAREGASES:1||THz radiation:1||FREEELECTRON LASER:1||REALTIME OBSERVATION:1||TARGET:1||photoionized plasmas:1||fs Xray laser:1||emission profile:1||HIGHORDER HARMONICS:1||Xray laser:1||atomic transition:1||EXCITATION:1||LASERS:1||PERFORMANCE:1||RELATIVISTIC ELECTRONS:1||BI2O3DOPED ZNO:1||INNERSHELL IONIZATION:1||Laser wakefield:1||FREQUENCY:1||SOLIDSTATE LASERS:1||Linearly polarized:1||THERMIONIC EMISSION:1||PULSE AMPLIFICATION SYSTEM:1||BIB3O6:1||NM:1||NONCOVALENT INTERACTIONS:1||CRYSTALLINE:1||INTENSITY:1||JETS:1||COHERENT:1||LINE:1||ANGULARDISTRIBUTION:1||SILVER IONS:1||magnetic anisotropy:1||DEVICES:1||Auger transitions:1||CosterKronig transitions:1||EFFICIENT:1||ELECTRONIMPACT IONIZATION:1||ULTRASHORTPULSE:1||Nanowire:1||Heterostructure:1||soft Xray reflectivity:1||PLASMA ACCELERATOR:1||ZINCOXIDE NANOWIRES:1||CHEMICALVAPORDEPOSITION:1||Electron acceleration:1||Ionization of gases:1||Delay dependent:1||MULTIPHOTON IONIZATION:1||FRAGMENTATION:1||GASJET:1||ultrafast nonlinear optics:1||CYCLE PULSES:1||KHZ:1||chemical vapor deposition:1||ferromagnetism:1||ABSORPTION:1||TERAHERTZ RADIATION:1||SCIENCE:1||FIELDS:1||ELECTRONS:1||nanomultilayer structures:1||YIELDS:1||AUGER:1||10HZ REPETITION RATE:1||MULTITERAWATT:1||SPECTROGRAPH:1||HIGHHARMONICGENERATION:1||spectroscopy:1||level population:1||PARTICLEACCELERATION:1||OPTICAL FREQUENCYMEASUREMENT:1||NANOWALLS:1||ROOMTEMPERATURE:1||AVERAGE OUTPUT POWER:1||GROUPVELOCITYMISMATCH:1||Impact ionization:1||Dynamics:1||Lasers:1||Collisional process:1||ABOVETHRESHOLD IONIZATION:1||MAINGROUP THERMOCHEMISTRY:1||dilute magnetic semiconductors:1||GACRN:1||SIZE:1||ATTOSECOND:1||Ar cluster:1||Xray astrophysics:1||photoionization:1||irons:1||normal incidence pulsed laser deposition:1||SHELLS:1||Silicon Oxide:1||gaspuff Zpinch:1||Xray:1||soft Xray reflectors:1||ESCAPE:1||ZN2SIO4:1||SILICA:1||Time delay:1||Collisional plasmas:1||MASSSPECTROMETRY:1||NUCLEARFUSION:1||PARAMETRIC AMPLIFICATION:1||LYING ELECTRONIC STATES:1||ADJUSTABLEPARAMETERS:1||MAGNETICPROPERTIES:1||LIQUIDPHASE EPITAXY:1||CEP laser:1||REGION:1||Plasma waveguide:1||AMBIENT GAS:1||DEPOSITION:1||HARMONICGENERATION:1||ENHANCEMENT:1||imaging spectrometer:1||Abel inversion:1||Water window:1||Liquid nitrogen jet:1||CHARGEEXCHANGE:1||NOBEL LECTURE:1||VARISTOR:1||EPITAXY:1||THINDISK LASER:1||HIGHREPETITIONRATE:1||Atom lasers:1||Electronimpact excitation:1||High order harmonics:1||ultrafast technology:1||PEAK POWER:1||CHARGED ALUMINUM CLUSTERS:1||GaN:1||THIN:1||Electron beam:1||INTENSE:1||Hard Xray pulse generation:1||NONLINEAR THOMSON SCATTERING:1||MULTILAYER:1||UVvisible spectrometer:1||ATOMS:1||innershell transitions:1||CORRECTED CONCAVE GRATINGS:1||DISCHARGE:1||LASERPLASMA:1||thin film:1||reflectivity:1||opacity:1||gain:1||smallangle Xray scattering:1||SOFTXRAY:1||ZINCOXIDE:1||CYGNUSX3:1||Betatron oscillation:1||ACCELERATOR:1||STRAINEDLAYER SUPERLATTICES:1||OPTICAL PARAMETRIC AMPLIFICATION:1||PASSIVE MODELOCKING:1||Collision dynamics:1||MUM:1||EXACTEXCHANGE:1||BASISSET:1||APPROXIMATION:1||OXYNITRIDES:1||Beam energy modulation:1||polarization spectroscopy:1||REORIENTATION TRANSITION:1||DEPENDENCE:1||sulfurs:1||BUILDINGBLOCKS:1||RATES:1||OPTICAL PULSES:1||toroidal mirror:1||XRAY LASER:1||CALCIUM:1||radially polarized laser:1||GRAINBOUNDARIES:1||VAPORDEPOSITION:1||Xray generation:1||MAGNETIZATION:1||Electric excitation:1||Laserinduced gas plasmas:1||Qualitative analysis:1||SCHEME:1||RADIATION:10||PULSES:8||PHOTOLUMINESCENCE:7||LASER:7||GENERATION:6||NANORODS:6||GROWTH:6||NANOWIRES:5||IMPLANTED GAN:5||SPECTROSCOPY:5||THINFILMS:4||DYNAMICS:4||SILICON:4||EXTREMEULTRAVIOLET:4||AMPLIFICATION:4||PRESSURE:4||PHASE:4||OPTICALPROPERTIES:4||SYSTEM:4||EMISSION:4||FEL:3||N2O:3||FILMS:3||OPTICS:3||SPECTRA:3||FIELD:3||MIRRORS:3||ARRAYS:3||CLUSTERS:3||SIO2:3||IONIZATION:3||VACUUM:3||SCATTERING:3||IONS:2||LUMINESCENCE PROPERTIES:2||ANISOTROPY:2||BEAMS:2||DIFFRACTION:2||DISPERSION:2||chemical vapor deposition (CVD):2||ELECTRONICSTRUCTURE:2||MOSFETS:2||SI3N4:2||DENSITY:2||LIGHT:2||PLASMAS:2||MATTER:2||nanocomposites:2||RAMANSCATTERING:2||NANOPARTICLES:2||OXIDE:2||AMPLIFIED SPONTANEOUS EMISSION:2||NM WAVELENGTH:2||GAIN:2||CARBON NANOTUBES:2||CROSSSECTIONS:2||LIGHTEMITTINGDIODES:2||PULSE:2||CARBON PLASMA:2||TISAPPHIRE LASER:2||Raman scattering:2||ROUTE:2||multilayer:2||CATHODOLUMINESCENCE:2||highresolution transmission electronic microscope (HRTEM):2||DIFFERENCEFREQUENCYGENERATION:2||CRYSTAL:2||laserproduced plasma:2||NANOCABLES:2||photoluminescence:2||MAGNETIC ALLOY SEMICONDUCTORS:2||MOLECULARBEAM EPITAXY:2||EARTHDOPED GAN:2||LASER FIELDS:2||CHIRPEDPULSEAMPLIFICATION:2||ALN:2||GAUSSIANBEAM:2||ASSISTED CATALYTIC GROWTH:2||BLUE:2||NANOSTRUCTURES:2||MAGNETOELECTRONICS:2||MICROSCOPY:2||ELECTROLUMINESCENCE:2||LASERPULSES:2||GaN nanowires:2||GALLIUM NITRIDE NANOWIRES:2||GAMNN:2||NANOTUBES:2||PHYSICS:2||Femtosecond laser:2||parametric oscillators and amplifiers:1||ultrafast lasers:1||VALENCE:1||nanowires:1||DILUTED MAGNETIC SEMICONDUCTOR:1||LUMINESCENCE:1||Density modulation:1||Energy modulation:1||Current enhanced SASE free electron laser:1||Undulator radiation:1||FREEELECTRON LASERS:1||ULTRATHIN FERROMAGNETICFILMS:1||OXIDEFILMS:1||ABLATION:1||COMPONENT:1||METAL:1||innershell excited states:1||Nelike ions:1||TRANSITIONS:1||XUV spectrometer:1||DIAGNOSTICS:1||Xray scattering:1||MO/SI:1||pulsed laser deposition:1||KEV IMPACT ENERGIES:1||vacuum electron acceleration:1||HIGHINTENSITY LASER:1||JUNCTIONS:1||LOWTEMPERATURE GROWTH:1||nanocrystalline materials:1||MOLECULAR PHOTOIONIZATION:1||LOCALIZATION:1||DEUTERIUM CLUSTERS:1||EXPLOSIONS:1||REGENERATIVE AMPLIFIERS:1||RAREGASES:1||THz radiation:1||FREEELECTRON LASER:1||REALTIME OBSERVATION:1||TARGET:1||photoionized plasmas:1||fs Xray laser:1||emission profile:1||HIGHORDER HARMONICS:1||Xray laser:1||atomic transition:1||EXCITATION:1||LASERS:1||PERFORMANCE:1||RELATIVISTIC ELECTRONS:1||BI2O3DOPED ZNO:1||INNERSHELL IONIZATION:1||Laser wakefield:1||FREQUENCY:1||SOLIDSTATE LASERS:1||Linearly polarized:1||THERMIONIC EMISSION:1||PULSE AMPLIFICATION SYSTEM:1||BIB3O6:1||NM:1||NONCOVALENT INTERACTIONS:1||CRYSTALLINE:1||INTENSITY:1||JETS:1||COHERENT:1||LINE:1||ANGULARDISTRIBUTION:1||SILVER IONS:1||magnetic anisotropy:1||DEVICES:1||Auger transitions:1||CosterKronig transitions:1||EFFICIENT:1||ELECTRONIMPACT IONIZATION:1||ULTRASHORTPULSE:1||Nanowire:1||Heterostructure:1||soft Xray reflectivity:1||PLASMA ACCELERATOR:1||ZINCOXIDE NANOWIRES:1||CHEMICALVAPORDEPOSITION:1||Electron acceleration:1||Ionization of gases:1||Delay dependent:1||MULTIPHOTON IONIZATION:1||FRAGMENTATION:1||GASJET:1||ultrafast nonlinear optics:1||CYCLE PULSES:1||KHZ:1||chemical vapor deposition:1||ferromagnetism:1||ABSORPTION:1||TERAHERTZ RADIATION:1||SCIENCE:1||FIELDS:1||ELECTRONS:1||nanomultilayer structures:1||YIELDS:1||AUGER:1||10HZ REPETITION RATE:1||MULTITERAWATT:1||SPECTROGRAPH:1||HIGHHARMONICGENERATION:1||spectroscopy:1||level population:1||PARTICLEACCELERATION:1||OPTICAL FREQUENCYMEASUREMENT:1||NANOWALLS:1||ROOMTEMPERATURE:1||AVERAGE OUTPUT POWER:1||GROUPVELOCITYMISMATCH:1||Impact ionization:1||Dynamics:1||Lasers:1||Collisional process:1||ABOVETHRESHOLD IONIZATION:1||MAINGROUP THERMOCHEMISTRY:1||dilute magnetic semiconductors:1||GACRN:1||SIZE:1||ATTOSECOND:1||Ar cluster:1||Xray astrophysics:1||photoionization:1||irons:1||normal incidence pulsed laser deposition:1||SHELLS:1||Silicon Oxide:1||gaspuff Zpinch:1||Xray:1||soft Xray reflectors:1||ESCAPE:1||ZN2SIO4:1||SILICA:1||Time delay:1||Collisional plasmas:1||MASSSPECTROMETRY:1||NUCLEARFUSION:1||PARAMETRIC AMPLIFICATION:1||LYING ELECTRONIC STATES:1||ADJUSTABLEPARAMETERS:1||MAGNETICPROPERTIES:1||LIQUIDPHASE EPITAXY:1||CEP laser:1||REGION:1||Plasma waveguide:1||AMBIENT GAS:1||DEPOSITION:1||HARMONICGENERATION:1||ENHANCEMENT:1||imaging spectrometer:1||Abel inversion:1||Water window:1||Liquid nitrogen jet:1||CHARGEEXCHANGE:1||NOBEL LECTURE:1||VARISTOR:1||EPITAXY:1||THINDISK LASER:1||HIGHREPETITIONRATE:1||Atom lasers:1||Electronimpact excitation:1||High order harmonics:1||ultrafast technology:1||PEAK POWER:1||CHARGED ALUMINUM CLUSTERS:1||GaN:1||THIN:1||Electron beam:1||INTENSE:1||Hard Xray pulse generation:1||NONLINEAR THOMSON SCATTERING:1||MULTILAYER:1||UVvisible spectrometer:1||ATOMS:1||innershell transitions:1||CORRECTED CONCAVE GRATINGS:1||DISCHARGE:1||LASERPLASMA:1||thin film:1||reflectivity:1||opacity:1||gain:1||smallangle Xray scattering:1||SOFTXRAY:1||ZINCOXIDE:1||CYGNUSX3:1||Betatron oscillation:1||ACCELERATOR:1||STRAINEDLAYER SUPERLATTICES:1||OPTICAL PARAMETRIC AMPLIFICATION:1||PASSIVE MODELOCKING:1||Collision dynamics:1||MUM:1||EXACTEXCHANGE:1||BASISSET:1||APPROXIMATION:1||OXYNITRIDES:1||Beam energy modulation:1||polarization spectroscopy:1||REORIENTATION TRANSITION:1||DEPENDENCE:1||sulfurs:1||BUILDINGBLOCKS:1||RATES:1||OPTICAL PULSES:1||toroidal mirror:1||XRAY LASER:1||CALCIUM:1||radially polarized laser:1||GRAINBOUNDARIES:1||VAPORDEPOSITION:1||Xray generation:1||MAGNETIZATION:1||Electric excitation:1||Laserinduced gas plasmas:1||Qualitative analysis:1||SCHEME:1||RADIATION:10||PULSES:8||PHOTOLUMINESCENCE:7||LASER:7||GENERATION:6||NANORODS:6||GROWTH:6||NANOWIRES:5||IMPLANTED 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SEMICONDUCTORS:2||MOLECULARBEAM EPITAXY:2||EARTHDOPED GAN:2||LASER FIELDS:2||CHIRPEDPULSEAMPLIFICATION:2||ALN:2||GAUSSIANBEAM:2||ASSISTED CATALYTIC GROWTH:2||BLUE:2||NANOSTRUCTURES:2||MAGNETOELECTRONICS:2||MICROSCOPY:2||ELECTROLUMINESCENCE:2||LASERPULSES:2||GaN nanowires:2||GALLIUM NITRIDE NANOWIRES:2||GAMNN:2||NANOTUBES:2||PHYSICS:2||Femtosecond laser:2||parametric oscillators and amplifiers:1||ultrafast lasers:1||VALENCE:1||nanowires:1||DILUTED MAGNETIC SEMICONDUCTOR:1||LUMINESCENCE:1||Density modulation:1||Energy modulation:1||Current enhanced SASE free electron laser:1||Undulator radiation:1||FREEELECTRON LASERS:1||ULTRATHIN FERROMAGNETICFILMS:1||OXIDEFILMS:1||ABLATION:1||COMPONENT:1||METAL:1||innershell excited states:1||Nelike ions:1||TRANSITIONS:1||XUV spectrometer:1||DIAGNOSTICS:1||Xray scattering:1||MO/SI:1||pulsed laser deposition:1||KEV IMPACT ENERGIES:1||vacuum electron acceleration:1||HIGHINTENSITY LASER:1||JUNCTIONS:1||LOWTEMPERATURE GROWTH:1||nanocrystalline materials:1||MOLECULAR PHOTOIONIZATION:1||LOCALIZATION:1||DEUTERIUM CLUSTERS:1||EXPLOSIONS:1||REGENERATIVE AMPLIFIERS:1||RAREGASES:1||THz radiation:1||FREEELECTRON LASER:1||REALTIME OBSERVATION:1||TARGET:1||photoionized plasmas:1||fs Xray laser:1||emission profile:1||HIGHORDER HARMONICS:1||Xray laser:1||atomic transition:1||EXCITATION:1||LASERS:1||PERFORMANCE:1||RELATIVISTIC ELECTRONS:1||BI2O3DOPED ZNO:1||INNERSHELL IONIZATION:1||Laser wakefield:1||FREQUENCY:1||SOLIDSTATE LASERS:1||Linearly polarized:1||THERMIONIC EMISSION:1||PULSE AMPLIFICATION SYSTEM:1||BIB3O6:1||NM:1||NONCOVALENT INTERACTIONS:1||CRYSTALLINE:1||INTENSITY:1||JETS:1||COHERENT:1||LINE:1||ANGULARDISTRIBUTION:1||SILVER IONS:1||magnetic anisotropy:1||DEVICES:1||Auger transitions:1||CosterKronig transitions:1||EFFICIENT:1||ELECTRONIMPACT IONIZATION:1||ULTRASHORTPULSE:1||Nanowire:1||Heterostructure:1||soft Xray reflectivity:1||PLASMA ACCELERATOR:1||ZINCOXIDE NANOWIRES:1||CHEMICALVAPORDEPOSITION:1||Electron acceleration:1||Ionization of gases:1||Delay dependent:1||MULTIPHOTON IONIZATION:1||FRAGMENTATION:1||GASJET:1||ultrafast nonlinear optics:1||CYCLE PULSES:1||KHZ:1||chemical vapor deposition:1||ferromagnetism:1||ABSORPTION:1||TERAHERTZ RADIATION:1||SCIENCE:1||FIELDS:1||ELECTRONS:1||nanomultilayer structures:1||YIELDS:1||AUGER:1||10HZ REPETITION RATE:1||MULTITERAWATT:1||SPECTROGRAPH:1||HIGHHARMONICGENERATION:1||spectroscopy:1||level population:1||PARTICLEACCELERATION:1||OPTICAL FREQUENCYMEASUREMENT:1||NANOWALLS:1||ROOMTEMPERATURE:1||AVERAGE OUTPUT POWER:1||GROUPVELOCITYMISMATCH:1||Impact ionization:1||Dynamics:1||Lasers:1||Collisional process:1||ABOVETHRESHOLD IONIZATION:1||MAINGROUP THERMOCHEMISTRY:1||dilute magnetic semiconductors:1||GACRN:1||SIZE:1||ATTOSECOND:1||Ar cluster:1||Xray astrophysics:1||photoionization:1||irons:1||normal incidence pulsed laser deposition:1||SHELLS:1||Silicon Oxide:1||gaspuff Zpinch:1||Xray:1||soft Xray reflectors:1||ESCAPE:1||ZN2SIO4:1||SILICA:1||Time 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materials:1||MOLECULAR PHOTOIONIZATION:1||LOCALIZATION:1||DEUTERIUM CLUSTERS:1||EXPLOSIONS:1||REGENERATIVE AMPLIFIERS:1||RAREGASES:1||THz radiation:1||FREEELECTRON LASER:1||REALTIME OBSERVATION:1||TARGET:1||photoionized plasmas:1||fs Xray laser:1||emission profile:1||HIGHORDER HARMONICS:1||Xray laser:1||atomic transition:1||EXCITATION:1||LASERS:1||PERFORMANCE:1||RELATIVISTIC ELECTRONS:1||BI2O3DOPED ZNO:1||INNERSHELL IONIZATION:1||Laser wakefield:1||FREQUENCY:1||SOLIDSTATE LASERS:1||Linearly polarized:1||THERMIONIC EMISSION:1||PULSE AMPLIFICATION SYSTEM:1||BIB3O6:1||NM:1||NONCOVALENT INTERACTIONS:1||CRYSTALLINE:1||INTENSITY:1||JETS:1||COHERENT:1||LINE:1||ANGULARDISTRIBUTION:1||SILVER IONS:1||magnetic anisotropy:1||DEVICES:1||Auger transitions:1||CosterKronig transitions:1||EFFICIENT:1||ELECTRONIMPACT IONIZATION:1||ULTRASHORTPULSE:1||Nanowire:1||Heterostructure:1||soft Xray reflectivity:1||PLASMA ACCELERATOR:1||ZINCOXIDE NANOWIRES:1||CHEMICALVAPORDEPOSITION:1||Electron acceleration:1||Ionization of gases:1||Delay dependent:1||MULTIPHOTON IONIZATION:1||FRAGMENTATION:1||GASJET:1||ultrafast nonlinear optics:1||CYCLE PULSES:1||KHZ:1||chemical vapor deposition:1||ferromagnetism:1||ABSORPTION:1||TERAHERTZ RADIATION:1||SCIENCE:1||FIELDS:1||ELECTRONS:1||nanomultilayer structures:1||YIELDS:1||AUGER:1||10HZ REPETITION RATE:1||MULTITERAWATT:1||SPECTROGRAPH:1||HIGHHARMONICGENERATION:1||spectroscopy:1||level population:1||PARTICLEACCELERATION:1||OPTICAL FREQUENCYMEASUREMENT:1||NANOWALLS:1||ROOMTEMPERATURE:1||AVERAGE OUTPUT POWER:1||GROUPVELOCITYMISMATCH:1||Impact ionization:1||Dynamics:1||Lasers:1||Collisional process:1||ABOVETHRESHOLD IONIZATION:1||MAINGROUP THERMOCHEMISTRY:1||dilute magnetic semiconductors:1||GACRN:1||SIZE:1||ATTOSECOND:1||Ar cluster:1||Xray astrophysics:1||photoionization:1||irons:1||normal incidence pulsed laser deposition:1||SHELLS:1||Silicon Oxide:1||gaspuff Zpinch:1||Xray:1||soft Xray reflectors:1||ESCAPE:1||ZN2SIO4:1||SILICA:1||Time delay:1||Collisional plasmas:1||MASSSPECTROMETRY:1||NUCLEARFUSION:1||PARAMETRIC AMPLIFICATION:1||LYING ELECTRONIC STATES:1||ADJUSTABLEPARAMETERS:1||MAGNETICPROPERTIES:1||LIQUIDPHASE EPITAXY:1||CEP laser:1||REGION:1||Plasma waveguide:1||AMBIENT GAS:1||DEPOSITION:1||HARMONICGENERATION:1||ENHANCEMENT:1||imaging spectrometer:1||Abel inversion:1||Water window:1||Liquid nitrogen jet:1||CHARGEEXCHANGE:1||NOBEL LECTURE:1||VARISTOR:1||EPITAXY:1||THINDISK LASER:1||HIGHREPETITIONRATE:1||Atom lasers:1||Electronimpact excitation:1||High order harmonics:1||ultrafast technology:1||PEAK POWER:1||CHARGED ALUMINUM CLUSTERS:1||GaN:1||THIN:1||Electron beam:1||INTENSE:1||Hard Xray pulse generation:1||NONLINEAR THOMSON SCATTERING:1||MULTILAYER:1||UVvisible spectrometer:1||ATOMS:1||innershell transitions:1||CORRECTED CONCAVE GRATINGS:1||DISCHARGE:1||LASERPLASMA:1||thin film:1||reflectivity:1||opacity:1||gain:1||smallangle Xray scattering:1||SOFTXRAY:1||ZINCOXIDE:1||CYGNUSX3:1||Betatron oscillation:1||ACCELERATOR:1||STRAINEDLAYER SUPERLATTICES:1||OPTICAL PARAMETRIC AMPLIFICATION:1||PASSIVE MODELOCKING:1||Collision dynamics:1||MUM:1||EXACTEXCHANGE:1||BASISSET:1||APPROXIMATION:1||OXYNITRIDES:1||Beam energy modulation:1||polarization spectroscopy:1||REORIENTATION TRANSITION:1||DEPENDENCE:1||sulfurs:1||BUILDINGBLOCKS:1||RATES:1||OPTICAL PULSES:1||toroidal mirror:1||XRAY LASER:1||CALCIUM:1||radially polarized laser:1||GRAINBOUNDARIES:1||VAPORDEPOSITION:1||Xray generation:1||MAGNETIZATION:1||Electric excitation:1||Laserinduced gas plasmas:1||Qualitative analysis:1||SCHEME:1||RADIATION:10||PULSES:8||PHOTOLUMINESCENCE:7||LASER:7||GENERATION:6||NANORODS:6||GROWTH:6||NANOWIRES:5||IMPLANTED GAN:5||SPECTROSCOPY:5||THINFILMS:4||DYNAMICS:4||SILICON:4||EXTREMEULTRAVIOLET:4||AMPLIFICATION:4||PRESSURE:4||PHASE:4||OPTICALPROPERTIES:4||SYSTEM:4||EMISSION:4||FEL:3||N2O:3||FILMS:3||OPTICS:3||SPECTRA:3||FIELD:3||MIRRORS:3||ARRAYS:3||CLUSTERS:3||SIO2:3||IONIZATION:3||VACUUM:3||SCATTERING:3||IONS:2||LUMINESCENCE PROPERTIES:2||ANISOTROPY:2||BEAMS:2||DIFFRACTION:2||DISPERSION:2||chemical vapor deposition (CVD):2||ELECTRONICSTRUCTURE:2||MOSFETS:2||SI3N4:2||DENSITY:2||LIGHT:2||PLASMAS:2||MATTER:2||nanocomposites:2||RAMANSCATTERING:2||NANOPARTICLES:2||OXIDE:2||AMPLIFIED SPONTANEOUS EMISSION:2||NM WAVELENGTH:2||GAIN:2||CARBON NANOTUBES:2||CROSSSECTIONS:2||LIGHTEMITTINGDIODES:2||PULSE:2||CARBON PLASMA:2||TISAPPHIRE LASER:2||Raman scattering:2||ROUTE:2||multilayer:2||CATHODOLUMINESCENCE:2||highresolution transmission electronic microscope (HRTEM):2||DIFFERENCEFREQUENCYGENERATION:2||CRYSTAL:2||laserproduced plasma:2||NANOCABLES:2||photoluminescence:2||MAGNETIC ALLOY SEMICONDUCTORS:2||MOLECULARBEAM EPITAXY:2||EARTHDOPED GAN:2||LASER FIELDS:2||CHIRPEDPULSEAMPLIFICATION:2||ALN:2||GAUSSIANBEAM:2||ASSISTED CATALYTIC GROWTH:2||BLUE:2||NANOSTRUCTURES:2||MAGNETOELECTRONICS:2||MICROSCOPY:2||ELECTROLUMINESCENCE:2||LASERPULSES:2||GaN nanowires:2||GALLIUM NITRIDE NANOWIRES:2||GAMNN:2||NANOTUBES:2||PHYSICS:2||Femtosecond laser:2||parametric oscillators and amplifiers:1||ultrafast lasers:1||VALENCE:1||nanowires:1||DILUTED MAGNETIC SEMICONDUCTOR:1||LUMINESCENCE:1||Density modulation:1||Energy modulation:1||Current enhanced SASE free electron laser:1||Undulator radiation:1||FREEELECTRON LASERS:1||ULTRATHIN FERROMAGNETICFILMS:1||OXIDEFILMS:1||ABLATION:1||COMPONENT:1||METAL:1||innershell excited states:1||Nelike ions:1||TRANSITIONS:1||XUV spectrometer:1||DIAGNOSTICS:1||Xray scattering:1||MO/SI:1||pulsed laser deposition:1||KEV IMPACT ENERGIES:1||vacuum electron acceleration:1||HIGHINTENSITY LASER:1||JUNCTIONS:1||LOWTEMPERATURE GROWTH:1||nanocrystalline materials:1||MOLECULAR PHOTOIONIZATION:1||LOCALIZATION:1||DEUTERIUM CLUSTERS:1||EXPLOSIONS:1||REGENERATIVE AMPLIFIERS:1||RAREGASES:1||THz radiation:1||FREEELECTRON LASER:1||REALTIME OBSERVATION:1||TARGET:1||photoionized plasmas:1||fs Xray laser:1||emission profile:1||HIGHORDER HARMONICS:1||Xray laser:1||atomic transition:1||EXCITATION:1||LASERS:1||PERFORMANCE:1||RELATIVISTIC ELECTRONS:1||BI2O3DOPED ZNO:1||INNERSHELL IONIZATION:1||Laser wakefield:1||FREQUENCY:1||SOLIDSTATE LASERS:1||Linearly polarized:1||THERMIONIC EMISSION:1||PULSE AMPLIFICATION SYSTEM:1||BIB3O6:1||NM:1||NONCOVALENT INTERACTIONS:1||CRYSTALLINE:1||INTENSITY:1||JETS:1||COHERENT:1||LINE:1||ANGULARDISTRIBUTION:1||SILVER IONS:1||magnetic anisotropy:1||DEVICES:1||Auger transitions:1||CosterKronig transitions:1||EFFICIENT:1||ELECTRONIMPACT IONIZATION:1||ULTRASHORTPULSE:1||Nanowire:1||Heterostructure:1||soft Xray reflectivity:1||PLASMA ACCELERATOR:1||ZINCOXIDE NANOWIRES:1||CHEMICALVAPORDEPOSITION:1||Electron acceleration:1||Ionization of gases:1||Delay dependent:1||MULTIPHOTON IONIZATION:1||FRAGMENTATION:1||GASJET:1||ultrafast nonlinear optics:1||CYCLE PULSES:1||KHZ:1||chemical vapor deposition:1||ferromagnetism:1||ABSORPTION:1||TERAHERTZ RADIATION:1||SCIENCE:1||FIELDS:1||ELECTRONS:1||nanomultilayer structures:1||YIELDS:1||AUGER:1||10HZ REPETITION RATE:1||MULTITERAWATT:1||SPECTROGRAPH:1||HIGHHARMONICGENERATION:1||spectroscopy:1||level population:1||PARTICLEACCELERATION:1||OPTICAL FREQUENCYMEASUREMENT:1||NANOWALLS:1||ROOMTEMPERATURE:1||AVERAGE OUTPUT POWER:1||GROUPVELOCITYMISMATCH:1||Impact ionization:1||Dynamics:1||Lasers:1||Collisional process:1||ABOVETHRESHOLD IONIZATION:1||MAINGROUP THERMOCHEMISTRY:1||dilute magnetic semiconductors:1||GACRN:1||SIZE:1||ATTOSECOND:1||Ar cluster:1||Xray astrophysics:1||photoionization:1||irons:1||normal incidence pulsed laser deposition:1||SHELLS:1||Silicon Oxide:1||gaspuff Zpinch:1||Xray:1||soft Xray reflectors:1||ESCAPE:1||ZN2SIO4:1||SILICA:1||Time delay:1||Collisional plasmas:1||MASSSPECTROMETRY:1||NUCLEARFUSION:1||PARAMETRIC AMPLIFICATION:1||LYING ELECTRONIC STATES:1||ADJUSTABLEPARAMETERS:1||MAGNETICPROPERTIES:1||LIQUIDPHASE EPITAXY:1||CEP laser:1||REGION:1||Plasma waveguide:1||AMBIENT GAS:1||DEPOSITION:1||HARMONICGENERATION:1||ENHANCEMENT:1||imaging spectrometer:1||Abel inversion:1||Water window:1||Liquid nitrogen jet:1||CHARGEEXCHANGE:1||NOBEL LECTURE:1||VARISTOR:1||EPITAXY:1||THINDISK LASER:1||HIGHREPETITIONRATE:1||Atom lasers:1||Electronimpact excitation:1||High order harmonics:1||ultrafast technology:1||PEAK POWER:1||CHARGED ALUMINUM CLUSTERS:1||GaN:1||THIN:1||Electron beam:1||INTENSE:1||Hard Xray pulse generation:1||NONLINEAR THOMSON SCATTERING:1||MULTILAYER:1||UVvisible spectrometer:1||ATOMS:1||innershell transitions:1||CORRECTED CONCAVE GRATINGS:1||DISCHARGE:1||LASERPLASMA:1||thin film:1||reflectivity:1||opacity:1||gain:1||smallangle Xray scattering:1||SOFTXRAY:1||ZINCOXIDE:1||CYGNUSX3:1||Betatron oscillation:1||ACCELERATOR:1||STRAINEDLAYER SUPERLATTICES:1||OPTICAL PARAMETRIC AMPLIFICATION:1||PASSIVE MODELOCKING:1||Collision dynamics:1||MUM:1||EXACTEXCHANGE:1||BASISSET:1||APPROXIMATION:1||OXYNITRIDES:1||Beam energy modulation:1||polarization spectroscopy:1||REORIENTATION TRANSITION:1||DEPENDENCE:1||sulfurs:1||BUILDINGBLOCKS:1||RATES:1||OPTICAL PULSES:1||toroidal mirror:1||XRAY LASER:1||CALCIUM:1||radially polarized laser:1||GRAINBOUNDARIES:1||VAPORDEPOSITION:1||Xray generation:1||MAGNETIZATION:1||Electric excitation:1||Laserinduced gas plasmas:1||Qualitative analysis:1||SCHEME:1||RADIATION:10||PULSES:8||PHOTOLUMINESCENCE:7||LASER:7||GENERATION:6||NANORODS:6||GROWTH:6||NANOWIRES:5||IMPLANTED GAN:5||SPECTROSCOPY:5||THINFILMS:4||DYNAMICS:4||SILICON:4||EXTREMEULTRAVIOLET:4||AMPLIFICATION:4||PRESSURE:4||PHASE:4||OPTICALPROPERTIES:4||SYSTEM:4||EMISSION:4||FEL:3||N2O:3||FILMS:3||OPTICS:3||SPECTRA:3||FIELD:3||MIRRORS:3||ARRAYS:3||CLUSTERS:3||SIO2:3||IONIZATION:3||VACUUM:3||SCATTERING:3||IONS:2||LUMINESCENCE PROPERTIES:2||ANISOTROPY:2||BEAMS:2||DIFFRACTION:2||DISPERSION:2||chemical vapor deposition (CVD):2||ELECTRONICSTRUCTURE:2||MOSFETS:2||SI3N4:2||DENSITY:2||LIGHT:2||PLASMAS:2||MATTER:2||nanocomposites:2||RAMANSCATTERING:2||NANOPARTICLES:2||OXIDE:2||AMPLIFIED SPONTANEOUS EMISSION:2||NM WAVELENGTH:2||GAIN:2||CARBON NANOTUBES:2||CROSSSECTIONS:2||LIGHTEMITTINGDIODES:2||PULSE:2||CARBON PLASMA:2||TISAPPHIRE LASER:2||Raman scattering:2||ROUTE:2||multilayer:2||CATHODOLUMINESCENCE:2||highresolution transmission electronic microscope (HRTEM):2||DIFFERENCEFREQUENCYGENERATION:2||CRYSTAL:2||laserproduced plasma:2||NANOCABLES:2||photoluminescence:2||MAGNETIC ALLOY SEMICONDUCTORS:2||MOLECULARBEAM EPITAXY:2||EARTHDOPED GAN:2||LASER FIELDS:2||CHIRPEDPULSEAMPLIFICATION:2||ALN:2||GAUSSIANBEAM:2||ASSISTED CATALYTIC GROWTH:2||BLUE:2||NANOSTRUCTURES:2||MAGNETOELECTRONICS:2||MICROSCOPY:2||ELECTROLUMINESCENCE:2||LASERPULSES:2||GaN nanowires:2||GALLIUM NITRIDE NANOWIRES:2||GAMNN:2||NANOTUBES:2||PHYSICS:2||Femtosecond laser:2||parametric oscillators and amplifiers:1||ultrafast lasers:1||VALENCE:1||nanowires:1||DILUTED MAGNETIC SEMICONDUCTOR:1||LUMINESCENCE:1||Density modulation:1||Energy modulation:1||Current enhanced SASE free electron laser:1||Undulator radiation:1||FREEELECTRON LASERS:1||ULTRATHIN FERROMAGNETICFILMS:1||OXIDEFILMS:1||ABLATION:1||COMPONENT:1||METAL:1||innershell excited states:1||Nelike ions:1||TRANSITIONS:1||XUV spectrometer:1||DIAGNOSTICS:1||Xray scattering:1||MO/SI:1||pulsed laser deposition:1||KEV IMPACT ENERGIES:1||vacuum electron acceleration:1||HIGHINTENSITY LASER:1||JUNCTIONS:1||LOWTEMPERATURE GROWTH:1||nanocrystalline materials:1||MOLECULAR PHOTOIONIZATION:1||LOCALIZATION:1||DEUTERIUM CLUSTERS:1||EXPLOSIONS:1||REGENERATIVE AMPLIFIERS:1||RAREGASES:1||THz radiation:1||FREEELECTRON LASER:1||REALTIME OBSERVATION:1||TARGET:1||photoionized plasmas:1||fs Xray laser:1||emission profile:1||HIGHORDER HARMONICS:1||Xray laser:1||atomic transition:1||EXCITATION:1||LASERS:1||PERFORMANCE:1||RELATIVISTIC ELECTRONS:1||BI2O3DOPED ZNO:1||INNERSHELL IONIZATION:1||Laser wakefield:1||FREQUENCY:1||SOLIDSTATE LASERS:1||Linearly polarized:1||THERMIONIC EMISSION:1||PULSE AMPLIFICATION SYSTEM:1||BIB3O6:1||NM:1||NONCOVALENT INTERACTIONS:1||CRYSTALLINE:1||INTENSITY:1||JETS:1||COHERENT:1||LINE:1||ANGULARDISTRIBUTION:1||SILVER IONS:1||magnetic anisotropy:1||DEVICES:1||Auger transitions:1||CosterKronig transitions:1||EFFICIENT:1||ELECTRONIMPACT IONIZATION:1||ULTRASHORTPULSE:1||Nanowire:1||Heterostructure:1||soft Xray reflectivity:1||PLASMA ACCELERATOR:1||ZINCOXIDE NANOWIRES:1||CHEMICALVAPORDEPOSITION:1||Electron acceleration:1||Ionization of gases:1||Delay dependent:1||MULTIPHOTON IONIZATION:1||FRAGMENTATION:1||GASJET:1||ultrafast nonlinear optics:1||CYCLE PULSES:1||KHZ:1||chemical vapor deposition:1||ferromagnetism:1||ABSORPTION:1||TERAHERTZ RADIATION:1||SCIENCE:1||FIELDS:1||ELECTRONS:1||nanomultilayer structures:1||YIELDS:1||AUGER:1||10HZ REPETITION RATE:1||MULTITERAWATT:1||SPECTROGRAPH:1||HIGHHARMONICGENERATION:1||spectroscopy:1||level population:1||PARTICLEACCELERATION:1||OPTICAL FREQUENCYMEASUREMENT:1||NANOWALLS:1||ROOMTEMPERATURE:1||AVERAGE OUTPUT POWER:1||GROUPVELOCITYMISMATCH:1||Impact ionization:1||Dynamics:1||Lasers:1||Collisional process:1||ABOVETHRESHOLD IONIZATION:1||MAINGROUP THERMOCHEMISTRY:1||dilute magnetic semiconductors:1||GACRN:1||SIZE:1||ATTOSECOND:1||Ar cluster:1||Xray astrophysics:1||photoionization:1||irons:1||normal incidence pulsed laser deposition:1||SHELLS:1||Silicon Oxide:1||gaspuff Zpinch:1||Xray:1||soft Xray reflectors:1||ESCAPE:1||ZN2SIO4:1||SILICA:1||Time delay:1||Collisional plasmas:1||MASSSPECTROMETRY:1||NUCLEARFUSION:1||PARAMETRIC AMPLIFICATION:1||LYING ELECTRONIC STATES:1||ADJUSTABLEPARAMETERS:1||MAGNETICPROPERTIES:1||LIQUIDPHASE EPITAXY:1||CEP laser:1||REGION:1||Plasma waveguide:1||AMBIENT GAS:1||DEPOSITION:1||HARMONICGENERATION:1||ENHANCEMENT:1||imaging spectrometer:1||Abel inversion:1||Water window:1||Liquid nitrogen jet:1||CHARGEEXCHANGE:1||NOBEL LECTURE:1||VARISTOR:1||EPITAXY:1||THINDISK LASER:1||HIGHREPETITIONRATE:1||Atom lasers:1||Electronimpact excitation:1||High order harmonics:1||ultrafast technology:1||PEAK POWER:1||CHARGED ALUMINUM CLUSTERS:1||GaN:1||THIN:1||Electron beam:1||INTENSE:1||Hard Xray pulse generation:1||NONLINEAR THOMSON SCATTERING:1||MULTILAYER:1||UVvisible spectrometer:1||ATOMS:1||innershell transitions:1||CORRECTED CONCAVE GRATINGS:1||DISCHARGE:1||LASERPLASMA:1||thin film:1||reflectivity:1||opacity:1||gain:1||smallangle Xray scattering:1||SOFTXRAY:1||ZINCOXIDE:1||CYGNUSX3:1||Betatron oscillation:1||ACCELERATOR:1||STRAINEDLAYER SUPERLATTICES:1||OPTICAL PARAMETRIC AMPLIFICATION:1||PASSIVE MODELOCKING:1||Collision dynamics:1||MUM:1||EXACTEXCHANGE:1||BASISSET:1||APPROXIMATION:1||OXYNITRIDES:1||Beam energy modulation:1||polarization spectroscopy:1||REORIENTATION TRANSITION:1||DEPENDENCE:1||sulfurs:1||BUILDINGBLOCKS:1||RATES:1||OPTICAL PULSES:1||toroidal mirror:1||XRAY LASER:1||CALCIUM:1||radially polarized laser:1||GRAINBOUNDARIES:1||VAPORDEPOSITION:1||Xray generation:1||MAGNETIZATION:1||Electric excitation:1||Laserinduced gas plasmas:1||Qualitative analysis:1||SCHEME:1||RADIATION:10||PULSES:8||PHOTOLUMINESCENCE:7||LASER:7||GENERATION:6||NANORODS:6||GROWTH:6||NANOWIRES:5||IMPLANTED GAN:5||SPECTROSCOPY:5||THINFILMS:4||DYNAMICS:4||SILICON:4||EXTREMEULTRAVIOLET:4||AMPLIFICATION:4||PRESSURE:4||PHASE:4||OPTICALPROPERTIES:4||SYSTEM:4||EMISSION:4||FEL:3||N2O:3||FILMS:3||OPTICS:3||SPECTRA:3||FIELD:3||MIRRORS:3||ARRAYS:3||CLUSTERS:3||SIO2:3||IONIZATION:3||VACUUM:3||SCATTERING:3||IONS:2||LUMINESCENCE PROPERTIES:2||ANISOTROPY:2||BEAMS:2||DIFFRACTION:2||DISPERSION:2||chemical vapor deposition (CVD):2||ELECTRONICSTRUCTURE:2||MOSFETS:2||SI3N4:2||DENSITY:2||LIGHT:2||PLASMAS:2||MATTER:2||nanocomposites:2||RAMANSCATTERING:2||NANOPARTICLES:2||OXIDE:2||AMPLIFIED SPONTANEOUS EMISSION:2||NM WAVELENGTH:2||GAIN:2||CARBON NANOTUBES:2||CROSSSECTIONS:2||LIGHTEMITTINGDIODES:2||PULSE:2||CARBON PLASMA:2||TISAPPHIRE LASER:2||Raman scattering:2||ROUTE:2||multilayer:2||CATHODOLUMINESCENCE:2||highresolution transmission electronic microscope (HRTEM):2||DIFFERENCEFREQUENCYGENERATION:2||CRYSTAL:2||laserproduced plasma:2||NANOCABLES:2||photoluminescence:2||MAGNETIC ALLOY SEMICONDUCTORS:2||MOLECULARBEAM EPITAXY:2||EARTHDOPED GAN:2||LASER FIELDS:2||CHIRPEDPULSEAMPLIFICATION:2||ALN:2||GAUSSIANBEAM:2||ASSISTED CATALYTIC GROWTH:2||BLUE:2||NANOSTRUCTURES:2||MAGNETOELECTRONICS:2||MICROSCOPY:2||ELECTROLUMINESCENCE:2||LASERPULSES:2||GaN nanowires:2||GALLIUM NITRIDE NANOWIRES:2||GAMNN:2||NANOTUBES:2||PHYSICS:2||Femtosecond laser:2||parametric oscillators and amplifiers:1||ultrafast lasers:1||VALENCE:1||nanowires:1||DILUTED MAGNETIC SEMICONDUCTOR:1||LUMINESCENCE:1||Density modulation:1||Energy modulation:1||Current enhanced SASE free electron laser:1||Undulator radiation:1||FREEELECTRON LASERS:1||ULTRATHIN FERROMAGNETICFILMS:1||OXIDEFILMS:1||ABLATION:1||COMPONENT:1||METAL:1||innershell excited states:1||Nelike ions:1||TRANSITIONS:1||XUV spectrometer:1||DIAGNOSTICS:1||Xray scattering:1||MO/SI:1||pulsed laser deposition:1||KEV IMPACT ENERGIES:1||vacuum electron acceleration:1||HIGHINTENSITY LASER:1||JUNCTIONS:1||LOWTEMPERATURE GROWTH:1||nanocrystalline materials:1||MOLECULAR PHOTOIONIZATION:1||LOCALIZATION:1||DEUTERIUM CLUSTERS:1||EXPLOSIONS:1||REGENERATIVE AMPLIFIERS:1||RAREGASES:1||THz radiation:1||FREEELECTRON LASER:1||REALTIME OBSERVATION:1||TARGET:1||photoionized plasmas:1||fs Xray laser:1||emission profile:1||HIGHORDER HARMONICS:1||Xray laser:1||atomic transition:1||EXCITATION:1||LASERS:1||PERFORMANCE:1||RELATIVISTIC ELECTRONS:1||BI2O3DOPED ZNO:1||INNERSHELL IONIZATION:1||Laser wakefield:1||FREQUENCY:1||SOLIDSTATE LASERS:1||Linearly polarized:1||THERMIONIC EMISSION:1||PULSE AMPLIFICATION SYSTEM:1||BIB3O6:1||NM:1||NONCOVALENT INTERACTIONS:1||CRYSTALLINE:1||INTENSITY:1||JETS:1||COHERENT:1||LINE:1||ANGULARDISTRIBUTION:1||SILVER IONS:1||magnetic anisotropy:1||DEVICES:1||Auger transitions:1||CosterKronig transitions:1||EFFICIENT:1||ELECTRONIMPACT IONIZATION:1||ULTRASHORTPULSE:1||Nanowire:1||Heterostructure:1||soft Xray reflectivity:1||PLASMA ACCELERATOR:1||ZINCOXIDE NANOWIRES:1||CHEMICALVAPORDEPOSITION:1||Electron acceleration:1||Ionization of gases:1||Delay dependent:1||MULTIPHOTON IONIZATION:1||FRAGMENTATION:1||GASJET:1||ultrafast nonlinear optics:1||CYCLE PULSES:1||KHZ:1||chemical vapor deposition:1||ferromagnetism:1||ABSORPTION:1||TERAHERTZ RADIATION:1||SCIENCE:1||FIELDS:1||ELECTRONS:1||nanomultilayer structures:1||YIELDS:1||AUGER:1||10HZ REPETITION RATE:1||MULTITERAWATT:1||SPECTROGRAPH:1||HIGHHARMONICGENERATION:1||spectroscopy:1||level population:1||PARTICLEACCELERATION:1||OPTICAL FREQUENCYMEASUREMENT:1||NANOWALLS:1||ROOMTEMPERATURE:1||AVERAGE OUTPUT POWER:1||GROUPVELOCITYMISMATCH:1||Impact ionization:1||Dynamics:1||Lasers:1||Collisional process:1||ABOVETHRESHOLD IONIZATION:1||MAINGROUP THERMOCHEMISTRY:1||dilute magnetic semiconductors:1||GACRN:1||SIZE:1||ATTOSECOND:1||Ar cluster:1||Xray astrophysics:1||photoionization:1||irons:1||normal incidence pulsed laser deposition:1||SHELLS:1||Silicon Oxide:1||gaspuff Zpinch:1||Xray:1||soft Xray reflectors:1||ESCAPE:1||ZN2SIO4:1||SILICA:1||Time delay:1||Collisional plasmas:1||MASSSPECTROMETRY:1||NUCLEARFUSION:1||PARAMETRIC AMPLIFICATION:1||LYING ELECTRONIC STATES:1||ADJUSTABLEPARAMETERS:1||MAGNETICPROPERTIES:1||LIQUIDPHASE EPITAXY:1||CEP laser:1||REGION:1||Plasma waveguide:1||AMBIENT GAS:1||DEPOSITION:1||HARMONICGENERATION:1||ENHANCEMENT:1||imaging spectrometer:1||Abel inversion:1||Water window:1||Liquid nitrogen jet:1||CHARGEEXCHANGE:1||NOBEL LECTURE:1||VARISTOR:1||EPITAXY:1||THINDISK LA
