Search results for "metals"

showing 10 items of 2013 documents

Detection of morphotropic phase boundary in A-site/Ca-substituted Na0.5Bi0.5TiO3 complex oxides ferroelectric system

2020

Abstract Vibrational and structural properties of lead-free piezoelectric (1-x)Na0.5Bi0.5TiO3–xCaTiO3 (0 ≤ x ≤ 1.00) solid solutions have been investigated using Raman spectroscopy and X-ray diffraction. Different anomalies were detected and analyzed taking into consideration the phase transition from rhombohedral to orthorhombic phase at room temperature. All Raman bands were interpreted through the variation in the peak positions (frequency) and the corresponding half-widths at half maximum (HWHM) as a function of x. XRD used as a complementary technique to Raman spectroscopy, showed that the rhombohedral – orthorhombic phase transition went gradually through an intermediate phase consist…

DiffractionPhase boundaryPhase transitionMaterials scienceMechanical EngineeringMetals and AlloysAnalytical chemistry02 engineering and technology010402 general chemistry021001 nanoscience & nanotechnology01 natural sciencesFerroelectricity0104 chemical sciencessymbols.namesakeMechanics of MaterialsPhase (matter)Materials Chemistrysymbols[CHIM]Chemical SciencesOrthorhombic crystal system0210 nano-technologyRaman spectroscopySolid solution
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Crystal behavior of potassium bromate under compression.

2015

We report on high-pressure angle-dispersive X-ray diffraction data up to 15 GPa andab initiototal-energy calculations up to 242 GPa for KBrO3. No phase transition was found below 15 Pa in contrast to previously reported data. Its experimental bulk modulus in the quasi-hydrostatic regime isB0= 18.8 (9) GPa with a bulk modulus pressure derivativeB′0= 8.2 (4). However, according to ourab initiocalculations, KBrO3significantly reduces its rhombohedral distortionviasmall cooperative movements of the atoms and the structure progressively approaches the cubic symmetry, where the KBr subarray would adopt a topology similar to that of the corresponding B2-type bromide. This rearrangement of atoms is…

DiffractionPhase transitionBulk modulusChemistryMetals and AlloysAb initioAtomic and Molecular Physics and OpticsElectron localization functionElectronic Optical and Magnetic MaterialsCrystalCrystallographyAb initio quantum chemistry methodsMaterials ChemistryIsostructuralActa crystallographica Section B, Structural science, crystal engineering and materials
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Pressure-induced phase transformations in mineral chalcocite, Cu2S, under hydrostatic conditions

2014

Abstract High-pressure room-temperature angle-dispersive powder X-ray diffraction measurements on Cu2S chalcocite were performed up to 30 GPa using a diamond-anvil cell, He as pressure transmitting medium and synchrotron radiation. Two first-order phase transitions were found at 3.2 and 7.4 GPa. The indexation of the powder diffraction patterns suggests three different monoclinic cells for the low-pressure chalcocite and the two high-pressure phases. Subtle changes in the X-ray diffraction patterns suggest a third pressure-induced transition above 26 GPa. Structural parameters and compressibility are discussed and compared to those reported in a previous study on Cu2S nanowires.

DiffractionPhase transitionChalcociteChemistryMechanical EngineeringMetals and AlloysAnalytical chemistryMineralogySynchrotron radiationmacromolecular substancesengineering.materialPolymorphism (materials science)Mechanics of MaterialsMaterials ChemistryCompressibilityengineeringPowder diffractionMonoclinic crystal systemJournal of Alloys and Compounds
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Chirality effects on 2D phase transitions

1996

Monolayers of the racemate and pure enantiomers of 1-hexadecyl-glycerol were investigated by grazing incidence X-ray diffraction (GID) at 5 and 20 °C on compression from 0 mN m−1 to pressures greater than 30 mN m−1. The racemate lattice is centred-rectangular for both temperatures at all investigated pressures. However, at both temperatures, there is a sharp phase transition from a low-pressure phase, in which the molecules are tilted towards nearest neighbours (NN) and the distortion azimuth also points towards NN, to a high-pressure phase, in which the molecules are tilted towards next-nearest neighbours (NNN) and an NNN-distorted lattice is observed. At 5 °C, the transition pressure is 1…

DiffractionPhase transitionCondensed matter physicsChemistryMetals and AlloysSurfaces and InterfacesTransition pressureSurfaces Coatings and FilmsElectronic Optical and Magnetic MaterialsLattice (order)MonolayerMaterials ChemistryMoleculeEnantiomerThin Solid Films
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Thickness and temperature dependent structure of Cd arachidate Langmuir-Blodgett films

1992

Abstract The structure of monolayers of Cd arachidate on water and on solid support, and the thickness dependent changes when building up a multilayer via the LB technique are studied by means of grazing incidence diffraction of X-ray. In monolayers the perpendicularly oriented amphiphilic molecules are arranged in a hexagonal lattice, whereas for thicker layers (even for three layers) they crystallize in an orthorhombic unit cell with a reduced molecular are ( A = 18.2 A 2 ) compared to that of the monolayer ( A = 19.7 A 2 ). In-plane diffraction measurements with wave vector transfer perpendicular to the surface (rod scans) could prove for multilayers a maximum tilt angle of 2°. The data …

DiffractionPhase transitionGrazing incidence diffractionbusiness.industryChemistryMetals and AlloysSurfaces and InterfacesLangmuir–Blodgett filmSurfaces Coatings and FilmsElectronic Optical and Magnetic MaterialsCrystallographyOpticsMonolayerMaterials ChemistryWave vectorHexagonal latticeOrthorhombic crystal systembusinessThin Solid Films
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Structural and vibrational behavior of cubic Cu1.80(3)Se cuprous selenide, berzelianite, under compression

2020

[EN] We have performed an experimental study of the crystal structure and lattice dynamics of cubic Cu1.80(3)Se at ambient temperature and high pressures. Two reversible phase transitions were found at 2.9 and 8.7 GPa. The indexation of the angle-dispersive synchrotron x-ray diffraction patterns suggests a large orthorhombic cell and a monoclinic cell for the high-pressure phases. Raman measurements provide additional information on the local structure. The compressibility of the three ambient temperature phases has been determined and compared to that of other sulphides and selenides.

DiffractionPhase transitionMaterials scienceHigh-pressureBerzelianiteAnalytical chemistry02 engineering and technologyCrystal structure010402 general chemistry01 natural scienceslaw.inventionchemistry.chemical_compoundsymbols.namesakelawSelenideMaterials ChemistryCompressibilityMechanical EngineeringCrystal structureMetals and Alloys021001 nanoscience & nanotechnologySynchrotron0104 chemical scienceschemistryMechanics of MaterialsPhase transitionsFISICA APLICADAsymbolsOrthorhombic crystal system0210 nano-technologyRaman spectroscopyMonoclinic crystal systemCopper selenide
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High-pressure/high-temperature phase diagram of zinc

2018

The phase diagram of zinc (Zn) has been explored up to 140 GPa and 6000K, by combining optical observations, x-ray diffraction, and ab initio calculations. In the pressure range covered by this study, Zn is found to retain a hexagonal close-packed (hcp) crystal symmetry up to the melting temperature. The known decrease of the axial ratio (c/a) of the hcp phase of Zn under compression is observed in x-ray diffraction experiments from 300K up to the melting temperature. The pressure at which c/a reaches root 3 (approximate to 10GPa) is slightly affected by temperature. When this axial ratio is reached, we observed that single crystals of Zn, formed at high temperature, break into multiple pol…

DiffractionPhase transitionMaterials sciencemeltingPOWDER DIFFRACTIONELECTRONIC TOPOLOGICAL TRANSITIONSThermodynamicschemistry.chemical_elementFOS: Physical sciences02 engineering and technologyCrystal structureZincDIAMOND-ANVIL CELL01 natural scienceshigh temperatureCondensed Matter::Materials ScienceX-RAY-DIFFRACTIONPhase (matter)Condensed Matter::Superconductivity0103 physical sciencesGeneral Materials Science010306 general physicsMELTING CURVEPhase diagramCondensed Matter - Materials ScienceAxial ratioSYNCHROTRONab initio calculationszincMaterials Science (cond-mat.mtrl-sci)021001 nanoscience & nanotechnologyCondensed Matter PhysicsCompression (physics)EQUATION-OF-STATEhigh pressurechemistryx-ray diffractionphase transitionZNMETALS0210 nano-technologyRESISTANCE
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Mechanism of photoluminescence in intrinsically disordered CaZrO3 crystals: First principles modeling of the excited electronic states

2017

Abstract CaZrO3 (CZO) powders obtained by the polymeric precursor method at 400 °C, and then, the samples were annealed at different temperatures (400, 600, 800, and 1000 °C) and characterized by X-ray diffraction, Raman and ultraviolet–visible spectroscopic methods, along with photoluminescence (PL) emissions. First principle calculations based on the density functional theory (DFT), using a periodic cell models, provide a theoretical framework for understanding the PL spectra based on the localization and characterization of the ground and electronic excited states. Fundamental (singlet, s ) and excited (singlet, s* , and triplet, t* ) electronic states were localized and characterized us…

DiffractionPhotoluminescence02 engineering and technologyPL emissionsorder-disorderDFT calculations010402 general chemistry01 natural sciencessymbols.namesakeAtomic orbitalMaterials ChemistrySinglet stateChemistryMechanical EngineeringMetals and Alloys021001 nanoscience & nanotechnologyexcited electronic states0104 chemical sciencesMechanics of MaterialsExcited statesymbolsFirst principleDensity functional theoryAtomic physics0210 nano-technologyRaman spectroscopyJournal of Alloys and Compounds
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Surface plasmon assisted thermal coupling of multiple photon energies

2006

A novel optical effect can be observed in a thin gold foil due to the excitation of surface plasmons which permits a form of all-optical modulation at low pulse rates. Modulated excitation of surface plasmons by infrared photons is shown to couple to several beams at visible-photon energies. The coupling is manifested by the observation of the visible photons being pulsed by the action of the infrared pulses, and by the far field diffraction of the visible beams into concentric rings. When each visible beam also excites surface plasmons, then a quadratic dependence of the visible photon power upon the infrared incident power is measured. The decay of surface plasmons is implicated as the pr…

DiffractionPulse repetition frequencyPhotonInfraredbusiness.industryChemistrySurface plasmonMetals and AlloysPhysics::OpticsNear and far fieldOptical polarizationSurfaces and InterfacesSurfaces Coatings and FilmsElectronic Optical and Magnetic MaterialsOpticsMaterials ChemistrybusinessExcitationThin Solid Films
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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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