Search results for "tetragonal crystal"

showing 10 items of 216 documents

Elektrónová a pásová štruktúra CuMnAs študovaná optickou a fotoemissinou spektroskopiou

2017

Tetragonal phase of CuMnAs progressively appears as one of the key materials for antiferromagnetic spintronics due to efficient current-induced spin-orbit torques whose existence can be directly inferred from crystal symmetry. Theoretical understanding of spintronic phenomena in this material, however, relies on the detailed knowledge of electronic structure (band structure and corresponding wave functions) which has so far been tested only to a limited extent. We show that AC permittivity (obtained from ellipsometry) and UV photoelectron spectra agree with density functional calculations. Together with the x-ray diffraction and precession electron diffraction tomography, our analysis confi…

DiffractionCondensed Matter - Materials ScienceMaterials scienceSpintronicsCondensed matter physicsPhotoemission spectroscopyMaterials Science (cond-mat.mtrl-sci)FOS: Physical sciencesspintronics DFT photoemission optical properties CuMnAs02 engineering and technologyCrystal structureElectronic structure021001 nanoscience & nanotechnology01 natural sciences3. Good healthTetragonal crystal systemCondensed Matter::Materials ScienceSpintronika DFT fotoemissia optické vlastnosti CuMnAs0103 physical sciencesPrecession electron diffraction010306 general physics0210 nano-technologyElectronic band structure
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Structural evolution of LiOH: evidence of a solid–solid transformation toward Li2O close to the melting temperature

1998

Abstract The structural evolution of LiOH has been studied between 10 K and 1670 K using a combination of neutron and X-ray diffraction and calorimetric measurements. The room temperature tetragonal phase of LiOH has been observed down to 10 K. Above the room temperature a dehydration of solid LiOH into solid Li2O is observed at a temperature and speed which strongly changes with the thermal history and the partial pressure of water vapour. Depending on these conditions the transformation of LiOH in to Li2O before the fusion temperature can be complete, partial or suppressed. In this latter case, as previously reported in the literature, a first order structural phase transition of LiOH is …

DiffractionFusionChemistryNeutron diffractionThermodynamicsGeneral ChemistryPartial pressureCondensed Matter PhysicsTetragonal crystal systemCrystallographyPhase (matter)Materials ChemistryWater vaporPhase diagramSolid State Communications
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Post-spinel transformations and equation of state inZnGa2O4: Determination at high pressure byin situx-ray diffraction

2009

Room-temperature angle-dispersive x-ray diffraction measurements on spinel ZnGa{sub 2}O{sub 4} up to 56 GPa show evidence of two structural phase transformations. At 31.2 GPa, ZnGa{sub 2}O{sub 4} undergoes a transition from the cubic spinel structure to a tetragonal spinel structure similar to that of ZnMn{sub 2}O{sub 4}. At 55 GPa, a second transition to the orthorhombic marokite structure (CaMn{sub 2}O{sub 4}-type) takes place. The equation of state of cubic spinel ZnGa{sub 2}O{sub 4} is determined: V{sub 0} = 580.1(9) {angstrom}{sup 3}, B{sub 0} = 233(8) GPa, B'{sub 0} = 8.3(4), and B''{sub 0} = -0.1145 GPa{sup -1} (implied value); showing that ZnGa{sub 2}O{sub 4} is one of the less comp…

DiffractionMaterials scienceCondensed matter physicsEquation of state (cosmology)Spinelengineering.materialCondensed Matter PhysicsElectronic Optical and Magnetic MaterialsCrystallographyTetragonal crystal systemHigh pressureX-ray crystallographyengineeringOrthorhombic crystal systemAngstromPhysical Review B
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Synchrotron diffraction study of the isothermal oxidation of uranium dioxide at 250°C

2003

ABSTRACTThe structural evolution of UO2 during its oxidation to U3O8 at 250°C in air was studied by in-situ synchrotron X-ray diffraction on the D2AM-CRG beamline at ESRF. The aim of this study is to determine the phases that are likely to appear during the long-term storage of spent nuclear fuel. Our results are in disagreement with the literature in which the existence of an intermediate cubic phase is not reported. Instead, an α-U3O7 tetragonal phase (c/a < 1) was mentioned but not definitively observed. These previous interpretations may have been the result of poor instrumental resolution.

DiffractionMaterials scienceResolution (electron density)Uranium dioxideAnalytical chemistrySynchrotronIsothermal processlaw.inventionCrystallographychemistry.chemical_compoundTetragonal crystal systemBeamlinechemistrylawPhase (matter)
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Structural and electric characteristics of (Na0.5Bi0.5)0.50Ba0.50TiO3 and (Na0.5Bi0.5)0.20Ba0.80TiO3 ceramics

2003

Abstract (Na0.5Bi0.5)0.50Ba0.50TiO3 and (Na0.5Bi0.5)0.20Ba0.80TiO3 ceramics have been prepared by the solid state reaction and studied by X-ray diffraction and by measurements of dielectric and ferroelectric properties between room temperature and 550 °C. A sharp increase in the electric permittivity and dielectric loss near 212 °C (for the first material) and near 205 °C (for the second material) on heating with remarkable thermal hysteresis have been observed. This sharp increase in dielectric responses indicates transformation between normal and relaxor ferroelectric states. The X-ray diffraction study shows that this transformation corresponds to the first order phase transition from te…

DiffractionPermittivityPhase transitionMaterials scienceCondensed matter physicsMechanical EngineeringDielectricCondensed Matter PhysicsFerroelectricityCrystallographyTetragonal crystal systemMechanics of Materialsvisual_artvisual_art.visual_art_mediumGeneral Materials ScienceDielectric lossCeramicMaterials Science and Engineering: B
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High-pressure structural transformations of PbCrO4 up to 51.2 GPa: An angle-dispersive synchrotron X-ray diffraction study

2014

Abstract We report on high-pressure X-ray diffraction measurements up to 51.2 GPa in PbCrO 4 at room temperature. Three high-pressure phases with structures different than the ambient-pressure monazite-type ( P 2 1 / n ) are reported. One phase transition was found at 3.8 GPa to an isomorphic structure to monazite. A second transition occurs at 11.1 GPa. After this transition, the coexistence of tetragonal ( I 4 1 / a ) and monoclinic ( P 2 1 ) structures is detected up to 21.1 GPa. Beyond this pressure and up to 51.2 GPa, only the high-pressure monoclinic phase is observed. Upon decompression all structural changes are reversible. Finally, the axial compressibilities for the different phas…

DiffractionPhase transitionMaterials scienceMechanical EngineeringSynchrotron radiationCondensed Matter PhysicsCrystallographyTetragonal crystal systemMechanics of MaterialsMonazitePhase (matter)X-ray crystallographyGeneral Materials ScienceMonoclinic crystal systemMaterials Research Bulletin
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Structure and Dielectric Properties of Na1/2Bi1/2TiO3-BaTiO3Solid Solutions

2013

Dielectric properties, polarization and x-ray diffraction are studied for (1-x)Na1/2Bi1/2TiO3-xBaTiO3 solid solutions in a concentration range above the morphotropic phase boundary. It is showed that all the studied compositions have tetragonal structure with maximal tetragonality slightly above the morphotropic phase boundary. Ferroelectric relaxor behavior is observed in a wide concentration range of BaTiO3. Stability of the relaxor state decreases with increasing BaTiO3 concentration, but only for compositions with low Na1/2Bi1/2TiO3 content the normal ferroelectric-paraelectric phase transition, which is characteristic to pure BaTiO3, occurs. Mechanisms, which influence the change of th…

DiffractionPhase transitionPhase boundaryTetragonal crystal systemMaterials scienceNuclear magnetic resonanceThermodynamicsDielectricCondensed Matter PhysicsPolarization (electrochemistry)Electronic Optical and Magnetic MaterialsPhase diagramSolid solutionFerroelectrics
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Vapor growth of Hg1−xCdxI2 on glass using CdTe buffer

2001

Abstract Vapor phase epitaxy (VPE) of Hg1−xCdxI2 layers on glass substrates covered by a CdTe buffer layer has been studied. The buffer layers of 2–4 μm thickness were formed by VPE using polycrystalline CdTe and Cd metal sources. The Hg1−xCdxI2 layers were grown using a (Hg1−yCdy)1−z(I2)z polycrystalline source, with a composition in the range of y=0.1–0.5 and z=0.5–0.8. Scanning electron microscopy and X-ray diffraction studies have shown that the composition and structure of Hg1−xCdxI2 layers depend strongly on the VPE conditions. Varying the growth time and source composition, it has been possible to obtain Hg1−xCdxI2 layers with the composition x in the range from approximately 0 (HgI2…

DiffractionScanning electron microscopeChemistrybusiness.industryMetals and AlloysAnalytical chemistrySurfaces and InterfacesEpitaxyCadmium telluride photovoltaicsSurfaces Coatings and FilmsElectronic Optical and Magnetic MaterialsMetalTetragonal crystal systemOpticsvisual_artMaterials Chemistryvisual_art.visual_art_mediumCrystallitebusinessLayer (electronics)Thin Solid Films
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Structural and elastic properties of defect chalcopyrite HgGa2S4 under high pressure

2014

In this work, we focus on the study of the structural and elastic properties of mercury digallium sulfide (HgGa2S4) at high pressures. This compound belongs to the family of AB(2)X(4) ordered-vacancy compounds and exhibits a tetragonal defect chalcopyrite structure. X-ray diffraction measurements at room temperature have been performed under compression up to 15.1 GPa in a diamond anvil cell. Our measurements have been complemented and compared with ab initio total energy calculations. The axial compressibility and the equation of state of the low-pressure phase of HgGa2S4 have been experimentally and theoretically determined and compared to other related ordered-vacancy compounds. The pres…

DiffractionSulfideHigh-pressureAb initioThermodynamicsMechanical propertiesTetragonal crystal systemMaterials ChemistryElastic moduluschemistry.chemical_classificationEquation of stateChalcopyriteMechanical EngineeringMetals and AlloysElasticityX-ray diffractionCrystallographychemistrySemiconductorsMechanics of Materialsvisual_artFISICA APLICADAX-ray crystallographyCompressibilityvisual_art.visual_art_medium
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Structure and superconducting properties of YBa2(Cu1−x Fex)3O7

1988

Fe-substituted Y-Ba-Cu superconducting oxide compounds were investigated by dc-magnetic susceptibility measurements, powder X-ray diffraction and Mdssbauer spectroscopy. Fe substitution caused a structural transformation from orthorhombic to tetragonal. Up to 4 at% Fe Tc was almost unaffected. It was found that superconductivity in Cu oxides does not depend on orthorhombic crystal symmetry.

DiffractionSuperconductivityMaterials scienceCondensed matter physicsOxideEnergy Engineering and Power TechnologyCondensed Matter PhysicsStructural transformationElectronic Optical and Magnetic MaterialsTetragonal crystal systemCrystallographychemistry.chemical_compoundchemistryOrthorhombic crystal systemElectrical and Electronic EngineeringSpectroscopyPhysica C: Superconductivity
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