Search results for "Impurity"

showing 10 items of 330 documents

Dipolar order and disorder phenomena in pure CO and dilute (CO)1−x(Ar)x mixtures physisorbed on graphite

1999

Abstract A detailed heat capacity study has been performed to characterize the properties of pure CO and (CO) 1− x (Ar) x mixture films physisorbed on the basal planes of graphite. The phase diagram of CO monolayers will be presented. At T c =5.18 K a phase transition to a novel low temperature phase is found with head-tail (dipolar) order of the molecules in an orientationally ordered herringbone structure. The phase transition is shown to belong to the 2D Ising universality class with anisotropic interactions between the molecules. Diluting CO weakly with Ar impurities leads to a dramatic destruction of the phase transition. This effect can be quantitatively described by the 2D random fie…

Phase transitionChemistryThermodynamicsSurfaces and InterfacesCondensed Matter PhysicsHeat capacitySurfaces Coatings and FilmsImpurityPhase (matter)MonolayerMaterials ChemistryIsing modelGraphitePhase diagramSurface Science
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Tuning the band gap of PbCrO4 through high-pressure: Evidence of wide-to-narrow semiconductor transitions

2014

The electronic transport properties and optical properties of lead(II) chromate (PbCrO4) have been studied at high pressure by means of resistivity, Hall-effect, and optical-absorption measurements. Band-structure first-principle calculations have been also performed. We found that the low-pressure phase is a direct band-gap semiconductor (Eg = 2.3 eV) that shows a high resistivity. At 3.5 GPa, associated to a structural phase transition, a band-gap collapse takes place, becoming Eg = 1.8 eV. At the same pressure the resistivity suddenly decreases due to an increase of the carrier concentration. In the HP phase, PbCrO4 behaves as an n-type semiconductor, with a donor level probably associat…

Phase transitionCondensed Matter - Materials ScienceCondensed matter physicsChemistrybusiness.industryBand gapMechanical EngineeringMetals and AlloysMaterials Science (cond-mat.mtrl-sci)FOS: Physical sciencesSemiconductorMechanics of MaterialsImpurityElectrical resistivity and conductivityHall effectPhase (matter)Materials ChemistryElectronic band structurebusiness
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Self-Ordered Second-Component Nb Clusters in KNbxTa1?xO3 Solid Solutions and Their Physical Properties

1999

Semi-empirical Hartree-Fock calculations using the intermediate neglect of the differential overlap (INDO) method, for self-ordered cubic symmetry clusters of seven Nb ions in KTaO 3 are performed with the aim of verifying the cluster model [1] of second component-induced phase transitions in ferroelectric perovskite matrices. It is shown that a seven-particle cluster in KTaO 3 :Nb has two types of states with different nature. Namely, a state with a dilatation combined with an off-center displacement of the central Nb ion in [111] directions in the cluster, and a state with a full-symmetric compression without any off-center effect. The consequences of such cluster structures on the multi-…

Phase transitionCondensed matter physicsImpurityChemistryExcited stateCluster (physics)Condensed Matter PhysicsFerroelectricityElectronic Optical and Magnetic MaterialsSolid solutionIonPerovskite (structure)physica status solidi (b)
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Computer simulations of a Lennard-Jones model for Ar1—x(N2)x: A prototype system for quadrupolar glasses

1998

Abstract Recent theoretical studies of orientational ordering in pure and diluted nitrogen crystals are summarized. While pure N2 has a first order phase transition from a plastic crystal to a phase with long-range orientational order, dilution with argon atoms leads to a quadrupolar glass phase. Monte Carlo simulations are used to study these phases, considering also the behavior of isolated N2 impurities in Ar crystals. It is shown that a simple model that neglects electrostatic interactions and takes only Lennard-Jones interactions into account can describe already many properties in qualitative agreement with experiment. Even the slow dynamics of the quadrupole moments can be modeled by…

Phase transitionMaterials scienceImpurityPhase (matter)Monte Carlo methodQuadrupolePath integral formulationStatistical physicsPlastic crystalCondensed Matter PhysicsElectrostaticsMolecular physicsElectronic Optical and Magnetic MaterialsFerroelectrics
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Quasiclassical free energy of superconductors : Disorder-driven first-order phase transition in superconductor/ferromagnetic-insulator bilayers

2020

In the seminal work by G. Eilenberger, Z. Phys. 214, 195 (1968), a closed-form expression for the free energy of inhomogeneous spin-singlet superconductor in terms of quasiclassical propagators has been suggested. However, deriving this expression and generalizing it for superconductors or superfluids with general matrix structure, e.g., spin-triplet correlations, has remained problematic. Starting from the Luttinger-Ward formulation, we discuss here the general solution. Besides ordinary superconductors with various scattering mechanisms, the obtained free-energy functional can be used for systems, such as superfluid $^{3}\mathrm{He}$ and superconducting systems with spatially inhomogeneou…

Phase transitionPauli paramagneismmagneetitInsulator (electricity)equation02 engineering and technologymagneettikentät01 natural sciencessuprajohteetSuperfluiditystateImpurityCondensed Matter::Superconductivity0103 physical sciences010306 general physicsSuperconductivityPhysicsCondensed matter physicsScatteringmagnetic-fieldvorticesPropagator021001 nanoscience & nanotechnologyFerromagnetismvortexCondensed Matter::Strongly Correlated Electrons0210 nano-technology
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Photoluminescence of Al2O3 nanopowders of different phases

2012

Abstract Photoluminescence was studied in six samples of Al2O3 nanopowders produced from the same initial material by calcination in the 800–1400 °C temperature range. At temperature around 1200 °C phase transition in aluminum oxide lattice occurs; the samples produced at temperatures up to 1200 °C contain mainly δ phase, while those obtained at 1400 °C contain pure α phase. In all studied samples of nominally pure aluminum oxide nanopowders photoluminescence is determined by trace level concentrations of uncontrolled impurities. It was found that phase transition is accompanied with modification of the emission spectrum: a broad band centered around 750 nm presumably ascribed to emission o…

Phase transitionPhotoluminescenceMaterials scienceOrganic ChemistryAnalytical chemistryAtmospheric temperature rangeAtomic and Molecular Physics and OpticsElectronic Optical and Magnetic MaterialsIonInorganic ChemistryImpurityAtomic electron transitionEmission spectrumElectrical and Electronic EngineeringPhysical and Theoretical ChemistryLuminescenceSpectroscopyOptical Materials
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Quantum chemical modelling of perovskite solid solutions

2000

In line with our previous study (Eglitis R I et al 1998 J. Phys.: Condens. Matter 10 6271) for a single Nb impurity and Nb clusters in KTaO3 we present here the results of calculations for a series of perovskite KNbx Ta 1−x O3 (KTN) solid solutions (x = 0, 0.125, 0.25, 0.75, and 1). The quantum chemical method of the intermediate neglect of the differential overlap (INDO) combined with the large unit cell (LUC) periodic model is used. According to the INDO calculations, Nb impurity becomes off-centre in KTaO3 already at the lowest studied Nb concentration. Its off-centre displacement is in a good agreement with XAFS measurements. We compare our results with previous FP-LMTO calculations. Pe…

Phase transitionchemistry.chemical_compoundPotassium niobateCondensed matter physicsChemistryPhononImpurityGeneral Materials ScienceElectronic structureCondensed Matter PhysicsFerroelectricitySolid solutionPerovskite (structure)Journal of Physics: Condensed Matter
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Comparison of the electrochemical properties of hematite thin films prepared by spray pyrolysis and electrodeposition

2015

Abstract This manuscript reports differences between the photoelectrochemical (PEC) activity of hematite (α-Fe 2 O 3 ) photoanodes produced by cathodic electrodeposition (ED) and spray pyrolysis (SP) methods. Both methods yield nanostructured polycrystalline α-Fe 2 O 3 thin films without additional impurity phases. However, α-Fe 2 O 3 produced by ED is characterised to have better crystallinity and higher porosity, which was confirmed by XRD and SEM analysis. Owing to this, α-Fe 2 O 3 obtained by ED generates a photocurrent that is 2.5 times higher than α-Fe 2 O 3 thin films prepared by SP. Furthermore, the influence of the thickness of the α-Fe 2 O 3 thin films on the flat-band potential p…

PhotocurrentMaterials scienceProcess Chemistry and TechnologyNanotechnologyHematiteElectrochemistrySurfaces Coatings and FilmsElectronic Optical and Magnetic MaterialsCrystallinityChemical engineeringImpurityvisual_artMaterials ChemistryCeramics and Compositesvisual_art.visual_art_mediumWater splittingCrystalliteThin filmCeramics International
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Energy transport in silica to oxygen-deficient luminescence centers. Comparison with other luminescence centers in silica and α-quartz

2004

Abstract The transport of energy absorbed by silica glass to oxygen-deficient luminescence centers in was studied in the range of intrinsic absorption from 8.2 up to 35 eV. The low efficiency of exciting those luminescence centers by transport of energy could not be ascribed merely to carrier scattering by the disordered structure. Other centers (Cu + , for example) could be excited in such process with sufficiently high efficiency, albeit lower than that in crystals. The low efficiency of interaction of oxygen deficient centers with quasi-particles is attributed to isolation of these centers in clusters and the non-radiative annihilation of the quasi-particles on the boundaries of these cl…

PhotoluminescenceAbsorption spectroscopyImpurityCarrier scatteringChemistryExcited stateDopingMaterials ChemistryAnalytical chemistryGeneral ChemistryCondensed Matter PhysicsLuminescenceAbsorption (electromagnetic radiation)Solid State Communications
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Excitation and emission spectra of LaInO3-based solid solutions doped with Sm3+, Sb3+

2017

Abstract X-ray analysis showed that all the ceramic samples of La 1- x Sm x InO 3 (0.010≤ x ≤0.025) solid solutions were single-phased but the samples of nominal composition of LaIn 0.98 Sb 0.02 O 3 , La 0.98 Sm 0.02 In 0.98 Sb 0.02 O 3 contained a small amount of impurity phase of LaSbO 3 -based solid solutions. It was established that La 0.98 Sm 0.02 InO 3 solid solution under the excitation of 275 nm and 320 nm exhibits the strongest photoluminescence among La 1- x Sm x InO 3 solid solutions with 0.010≤ x ≤0.025. Photoluminescence bands located in wavelength ranges of 550–580 nm, 585–625 nm and 630–680 nm exhibit 2–3 clear maxima each. According to the locations of these maxima we calcul…

PhotoluminescenceChemistryDopingBiophysicsAnalytical chemistry02 engineering and technologyGeneral Chemistry010402 general chemistry021001 nanoscience & nanotechnologyCondensed Matter Physics01 natural sciencesBiochemistryAtomic and Molecular Physics and Optics0104 chemical sciencesIonCrystalImpurityPhase (matter)Emission spectrum0210 nano-technologySolid solutionJournal of Luminescence
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