Search results for "impur"

showing 10 items of 349 documents

Photosensitivity of silica glass with germanium studied by photoinduced of thermally stimulated luminescence with vacuum ultraviolet radiation

2003

Photosensitivity of the germanium-doped silica was studied through kinetics of recombination of the created defects in isothermal and thermally stimulated luminescence (TSL) regimes. The main observed luminescence contains bands mainly due to Ge oxygen deficient center. The maximum of photosensitivity corresponds to the high-energy part of the 7.6 eV band. The growth of TSL intensity is almost linear for the case of excitation through monochromatic light and growth with saturation in the case of excitation with white light. The efficiency of formation of TSL peaks increases with an increase of the temperature. The result was explained as multi-step process of photochemical dissociation and …

PhotoluminescenceChemistryDopingchemistry.chemical_elementGermaniumCondensed Matter PhysicsPhotochemistryThermoluminescenceDissociation (chemistry)Electronic Optical and Magnetic MaterialsPhotosensitivityImpurityMaterials ChemistryCeramics and CompositesNuclear ExperimentLuminescenceJournal of Non-Crystalline Solids
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Luminescence and Raman Detection of Molecular Cl2 and ClClO Molecules in Amorphous SiO2 Matrix

2017

The support from the Latvian Research Program project IMIS 2 (L.S., K.S.) and Latvian Science Council Grant 302/2012 (A.S.) is acknowledged. K.K. was partially supported by the Collaborative Research Project of Materials and Structures Laboratory, Tokyo Institute of Technology. H.H. was supported by the MEXT Element Strategy Initiative to form research cores.

PhotoluminescenceChemistryPhotodissociationAnalytical chemistry02 engineering and technology010402 general chemistry021001 nanoscience & nanotechnology01 natural sciences0104 chemical sciencesSurfaces Coatings and FilmsElectronic Optical and Magnetic MaterialsAmorphous solidsymbols.namesakeGeneral EnergyAbsorption bandImpurityExcited state:NATURAL SCIENCES:Physics [Research Subject Categories]symbolsPhysical and Theoretical Chemistry0210 nano-technologyLuminescenceRaman spectroscopyThe Journal of Physical Chemistry C
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Temperature and impurity concentration effects on upconversion luminescence in LaInO3 doped with Er3+

2016

In this paper a novel method for synthesis of LaInO3:Er3+ is reported and upconversion luminescence properties of the synthesized material at different temperatures (9–300 K) are studied. The samples were prepared by co-precipitation and subsequent heat treatment of lanthanum, indium and erbium hydroxides. It is shown that the excitation at 980 nm leads to a strong green upconversion luminescence in the material. At the concentrations above 0.1 mol. % of Er3+ the energy transfer upconversion mechanism of the luminescence becomes evident. Further increase of Er3+ content in the material leads to higher red-to-green upconversion luminescence intensity ratio. The mechanisms responsible for the…

PhotoluminescenceEnergy transfer upconversionMaterials sciencePhysics and Astronomy (miscellaneous)DopingGeneral Physics and Astronomychemistry.chemical_element02 engineering and technology010402 general chemistry021001 nanoscience & nanotechnologyPhotochemistry01 natural sciences0104 chemical sciencesErbiumchemistryImpurityLanthanum0210 nano-technologyLuminescenceIndium
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Recombination processes in unintentionally doped GaTe single crystals

2002

Emission spectra of GaTe single crystals in the range of 1.90–1.38 eV have been analyzed at different temperatures and excitation intensities by photoluminescence, photoluminescence excitation, and selective photoluminescence. A decrease in band gap energy with an increase in temperature was obtained from the redshift of the free exciton recombination peak. The energy of longitudinal optical phonons was found to be 14±1 meV. A value of 1.796±0.001 eV for the band gap at 10 K was determined, and the bound exciton energy was found to be 18±0.3 meV. The activation energy of the thermal quenching of the main recombination peaks and of the ones relating to the ionization energy of impurities and…

PhotoluminescenceImpurity statesBand gapChemistryExcitonGallium compounds ; III-VI semiconductors ; Photoluminescence ; Impurity states ; Cefect states ; Electron-phonon interactions ; Phonon-exciton interactions ; Excitons ; Red shift ; Radiation quenchingDopingGallium compoundsRadiation quenchingUNESCO::FÍSICAIII-VI semiconductorsGeneral Physics and AstronomyPhonon-exciton interactionsCefect statesAcceptorRed shiftElectron-phonon interactionsCondensed Matter::Materials Science:FÍSICA [UNESCO]ExcitonsPhotoluminescence excitationEmission spectrumIonization energyAtomic physicsPhotoluminescence
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Photoluminescence in AlN: macro‐size and nano‐powder

2007

Photoluminescence (PL) properties in AlN are studied when size of polycrystalline grains is reduced from macro-size (AlN ceramics and macro-size powder) to nano-size (nano-powder). It was found that in all these materials within the UV- blue spectral region two PL bands are observed at ∼400 nm (caused by the oxygen-related defects) and at 480 nm (with unknown defect structure) but the ratio of their intensities depends on the grain size. Reduction of AlN grain size results in decrease of the 400 nm band and increase of the 480 nm band. It allows the following conclusions: i) reduction of AlN grain size results in decrease of oxygen (the native impurity of AlN) content in the crystalline lat…

PhotoluminescenceMaterials scienceAnalytical chemistrychemistry.chemical_elementMineralogyCrystal structureCondensed Matter PhysicsOxygenGrain sizechemistryImpurityvisual_artNano-visual_art.visual_art_mediumCrystalliteCeramicphysica status solidi c
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Fermi energy dependence of the optical emission in core/shell InAs nanowire homostructures.

2017

InAs nanowires grown by vapor–liquid–solid (VLS) method are investigated by photoluminescence. We observe that the Fermi energy of all samples is reduced by ~20 meV when the size of the Au nanoparticle used for catalysis is increased from 5 to 20 nm. Additional capping with a thin InP shell enhances the optical emission and does not affect the Fermi energy. The unexpected behavior of the Fermi energy is attributed to the differences in the residual donor (likely carbon) incorporation in the axial (low) and lateral (high incorporation) growth in the VLS and vapor–solid (VS) methods, respectively. The different impurity incorporation rate in these two regions leads to a core/shell InAs homost…

PhotoluminescenceMaterials scienceCondensed matter physicsMechanical EngineeringDopingNanowireShell (structure)BioengineeringFermi energy02 engineering and technologyGeneral ChemistryCondensed Matter::Mesoscopic Systems and Quantum Hall Effect021001 nanoscience & nanotechnology01 natural sciencesCore (optical fiber)Condensed Matter::Materials ScienceMechanics of MaterialsImpurityElectric field0103 physical sciencesGeneral Materials ScienceElectrical and Electronic Engineering010306 general physics0210 nano-technologyNanotechnology
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Excitation and photoluminescence spectra of single- and non-single-phased phosphors based on LaInO3 doped with Dy3+, Ho3+ activators and Sb3+ probabl…

2017

Abstract Single-phased La 0.95 Ln 0.05 InO 3 ( Ln – Dy, Ho), La 0.90 Dy 0.05 Ho 0.05 InO 3 , LaInO 3 ceramic samples as well as the La 0.95 Ln 0.05 In 0.98 Sb 0.02 O 3 ( Ln – Dy, Ho), La 0.90 Dy 0.05 Ho 0.05 In 0.98 Sb 0.02 O 3 , LaIn 0.98 Sb 0.02 O 3 samples with additional impurity LaSbO 3 phase were prepared by solid-state reactions method. Their excitation and photoluminescence (PL) spectra were measured at room temperature. It was established that PL bands intensity of spectra obtained for samples of nominal composition La 0.95 Dy 0.05 In 0.98 Sb 0.02 O 3 , La 0.95 Ho 0.05 In 0.98 Sb 0.02 O 3 , La 0.90 Dy 0.05 Ho 0.05 In 0.98 Sb 0.02 O 3 is much higher than that of single-phase La 0.95…

PhotoluminescenceMaterials scienceDopingBiophysicsAnalytical chemistryPhosphor02 engineering and technologyGeneral Chemistry010402 general chemistry021001 nanoscience & nanotechnologyCondensed Matter Physics01 natural sciencesBiochemistryAtomic and Molecular Physics and OpticsSpectral line0104 chemical sciencesIonImpurity0210 nano-technologyExcitationSolid solutionJournal of Luminescence
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Growth and optical characterization of indirect-gap AlxGa1−xAs alloys

1999

Nonintentionally doped AlxGa1−xAs layers with 0.38 x 0.84 were grown on (100) GaAs substrates by liquid phase epitaxy (LPE) under near-equilibrium conditions. The crystalline quality of the samples was studied by photoluminescence at 2 K and room temperature Raman spectroscopy. The peculiar behavior in the photoluminescence intensities of the indirect bound exciton line and the donor–acceptor pair transition is explained from the evolution of the silicon donor binding energy according to the aluminum composition. It was also possible to observe the excitonic transition corresponding to the AlxGa1−xAs/GaAs interface, despite the disorder and other factors which are normally involved when gro…

PhotoluminescenceMaterials scienceIII-V semiconductorsSiliconExcitonBinding energyGeneral Physics and Astronomychemistry.chemical_elementBinding energyEpitaxyMolecular physicssymbols.namesakePhonon spectraLiquid phase epitaxial growth:FÍSICA [UNESCO]PhotoluminescenceAluminium compoundsX-ray absorption spectroscopyGallium arsenide Semiconductor growthImpurity statesDopingUNESCO::FÍSICASemiconductor epitaxial layersCrystallographychemistrysymbolsPhotoluminescence ; Binding energy ; Raman spectra ; III-V semiconductors ; Aluminium compounds ; Gallium arsenide Semiconductor growth ; Liquid phase epitaxial growth ; Semiconductor epitaxial layers ; Impurity states ; Excitons ; Phonon spectraExcitonsRaman spectraRaman spectroscopy
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Defect Luminescence of LiBaF3 Perovskites

2000

Blue and red luminescence of undoped LiBaF3 crystals was studied. A broad, isotropic photoluminescence band centered at 410 nm can be excited by 210 nm — 275 nm light in as grown crystals. After X-irradiation at RT a new narrower, anisotropic luminescence band appears at 425 mn which has an additional excitation band at 290 nm. The X-irradiation also creates the F- type centres and anisotropic centres with an absorption band at 630 nm and a luminescence band at 700 nm. No F- centre luminescence is observed. All the other centres mentioned act as radiative recombination centers as well. It is speculated that the origin of the blue luminescence is due to oxygen defects and that the red lumine…

PhotoluminescenceMaterials scienceImpurityAbsorption bandExcited stateSpontaneous emissionLuminescenceAnisotropyMolecular physicsExcitation
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Luminescence and optical spectroscopy of charge transfer processes in solid solutions Ni Mg1−O and Ni Zn1−O

2016

Abstract In this work photoluminescence spectra for Ni c Mg 1− c O and Ni x Zn 1− x O solid solutions with the rock-salt crystal structure were obtained under synchrotron radiation excitation. Periodical peaks in the photoluminescence excitation spectrum of Ni c Mg 1− c O ( c =0.008) have been discovered for a wide-gap oxide doped with 3d impurities for the first time. They can be considered as LO phonon repetitions of the narrow zero phonon line resulted from the optical transitions into the p–d charge transfer exciton [d 9 h] state. A close coincidence in energy of different peculiarities in the optical absorption and photoluminescence excitation spectra for the Ni c Mg 1− c O and Ni x Zn…

PhotoluminescenceMaterials sciencePhononExcitonBiophysicsAnalytical chemistry02 engineering and technologyGeneral Chemistry021001 nanoscience & nanotechnologyCondensed Matter Physics01 natural sciencesBiochemistryAtomic and Molecular Physics and OpticsCondensed Matter::Materials ScienceCrystallographyImpurity0103 physical sciencesPhotoluminescence excitation010306 general physics0210 nano-technologySpectroscopyLuminescenceSolid solutionJournal of Luminescence
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