Search results for "Phase Transition"

showing 10 items of 1281 documents

Novel bimetallic MOF phosphors with an imidazolium cation: structure, phonons, high- pressure phase transitions and optical response

2018

We report the synthesis, crystal structure, phonons and luminescence properties of three novel heterometallic metal organic frameworks (MOFs) with perovskite-like topology of the following formulas: [C3H5N2]Na0.5Cr0.5(HCOO)3 (ImNaCr), [C3H5N2]Na0.5Al0.5(HCOO)3 (ImNaAl) and [C3H5N2]Na0.5Al0.475Cr0.025(HCOO)3 (ImNaAlCr with 5 mol% of Cr3+). ImNaCr crystallizes in a monoclinic system (P2/n space group) with one imidazolium cation (Im+) in an asymmetric unit forming six N–H⋯O and four C–H⋯O hydrogen bonds. In contrast to other known heterometallic MOFs, the complete substitution of Cr3+ ions with smaller Al3+ ions leads to a change of the crystal symmetry. ImNaAl adopts a monoclinic P21/n space…

Phase transitionMaterials science010405 organic chemistrySpectrochemical seriesCrystal structure010402 general chemistry01 natural sciences0104 chemical sciencesInorganic ChemistryCrystalsymbols.namesakeCrystallographysymbolsMetal-organic frameworkRaman spectroscopyLuminescenceMonoclinic crystal systemDalton Transactions
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Monoclinic-tetragonal-monoclinic phase transitions in Eu0.1Bi0.9VO4 under pressure

2019

The promising technological material Eu0.1Bi0.9VO4, has been studied for the first time at room-temperature under high-pressure, up to 24.9 GPa, by means of in situ angle dispersive powder x-ray diffraction (XRD). The compound undergoes two phase transitions at 1.9 and 16.1 GPa. The first transition is from the monoclinic fergusonite-type structure (space group I2/a) to a tetragonal scheelite-type structure (space group I41/a), being a ferroelastic-paraelastic transformation similar to that previously reported for isomorphic pristine BiVO4. The second phase transition is first-order in nature. The scheelite-type and the second high-pressure phase coexist in a wide pressure range. A monoclin…

Phase transitionMaterials science02 engineering and technologyCrystal structure021001 nanoscience & nanotechnologyCondensed Matter PhysicsFergusonite01 natural sciencesTetragonal crystal systemDodecahedronCrystallographyPhase (matter)0103 physical sciencesX-ray crystallographyGeneral Materials Science010306 general physics0210 nano-technologyMonoclinic crystal systemJournal of Physics: Condensed Matter
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Complex high-pressure polymorphism of barium tungstate

2012

We have studied BaWO 4 under compression at room temperature by means of x-ray diffraction and Raman spectroscopy. When compressed with neon as a pressure-transmitting medium (quasihydrostatic conditions), we found that BaWO 4 transforms from its low-pressure tetragonal structure into a much denser monoclinic structure. This result confirms our previous theoretical prediction based on ab initio calculations that the scheelite to BaWO 4-II transition occurs at room temperature if kinetic barriers are suppressed by pressure. However, our experiment without any pressure- transmitting medium has resulted in a phase transition to a completely different structure, suggesting nonhydrostaticity may…

Phase transitionMaterials science02 engineering and technologyCrystal structureBawo47. Clean energy01 natural sciencesX-rayTetragonal crystal systemsymbols.namesakeAb initio quantum chemistry methods0103 physical sciencesCrystal010306 general physicsCaoo4Refinement021001 nanoscience & nanotechnologyCondensed Matter PhysicsElectronic Optical and Magnetic MaterialsCrystallographyFISICA APLICADA[PHYS.COND.CM-GEN]Physics [physics]/Condensed Matter [cond-mat]/Other [cond-mat.other]X-ray crystallographyTransitionsymbolsPACS: 62.50.−p 61.50.Ks 61.05.cp 63.20.ddCell0210 nano-technologyRaman spectroscopyPowder diffractionPowder DiffractionMonoclinic crystal system
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The Ferroelectric Photo-Groundstate of SrTiO$_3$: Cavity Materials Engineering

2021

Significance Controlling collective phenomena in quantum materials is a promising route toward engineering material properties on demand. Strong THz lasers have been successful at inducing ferroelectricity in S r T i O 3 . Here we demonstrate, from atomistic calculations, that cavity quantum vacuum fluctuations induce a change in the collective phase of S r T i O 3 in the strong light–matter coupling regime. Under these conditions, the ferroelectric phase is stabilized as the ground state, instead of the quantum paraelectric one. We conceptualize this light–matter hybrid state as a material photo ground state: Fundamental properties such as crystal structure, phonon frequencies, and the col…

Phase transitionMaterials science3SrTiO3PolaritonsFOS: Physical sciences02 engineering and technologyStrong light–matter hybrids01 natural sciencesSettore FIS/03 - Fisica Della MateriaCondensed Matter::Materials SciencequantumQuantum state0103 physical sciencesPolariton010306 general physicsquantum paraelectric to ferroelectric transitionsQuantumCavity materials engineeringQuantum fluctuationcavity materials engineeringCondensed Matter - Materials ScienceMultidisciplinaryCondensed matter physicsSrTiOMaterials Science (cond-mat.mtrl-sci)Quantum paraelectric to ferroelectric transitionComputational Physics (physics.comp-ph)021001 nanoscience & nanotechnologyFerroelectricitystructural phase-transitionscavity phase diagramExcited statetrong light-matter hybrids0210 nano-technologyGround statePhysics - Computational Physicspolaritons
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Structural and vibrational study of cubic Sb2O3under high pressure

2012

We report an experimental and theoretical study of antimony oxide (Sb${}_{2}$O${}_{3}$) in its cubic phase (senarmontite) under high pressure. X-ray diffraction and Raman scattering measurements up to 18 and 25 GPa, respectively, have been complemented with ab initio total-energy and lattice-dynamics calculations. X-ray diffraction measurements do not provide evidence of a space-group symmetry change in senarmontite up to 18 GPa. However, Raman scattering measurements evidence changes in the pressure coefficients of the Raman mode frequencies at 3.5 and 10 GPa, respectively. The behavior of the Raman modes with increasing pressure up to 25 GPa is fully reproduced by the lattice-dynamics cal…

Phase transitionMaterials scienceAb initioCondensed Matter PhysicsElectronic Optical and Magnetic MaterialsCondensed Matter::Materials Sciencechemistry.chemical_compoundsymbols.namesakeCrystallographychemistryAntimony trioxideX-ray crystallographysymbolsOrthorhombic crystal systemRaman spectroscopyPowder diffractionRaman scatteringPhysical Review B
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Combined Raman scattering andab initioinvestigation of pressure-induced structural phase transitions in the scintillatorZnWO4

2008

The room-temperature Raman scattering was measured in ${\text{ZnWO}}_{4}$ up to 45 GPa. We report the pressure dependence of all the Raman-active phonons of the low-pressure wolframite phase. As pressure increases additional Raman peaks appear at 30.6 GPa due to the onset of a reversible structural phase transition to a distorted monoclinic $\ensuremath{\beta}$-fergusonite-type phase. The low-pressure and high-pressure phases coexist from 30.6 to 36.5 GPa. In addition to the Raman measurements we also report ab initio total-energy and lattice-dynamics calculations for the two phases. These calculations helped us to determine the crystalline structure of the high-pressure phase and to assign…

Phase transitionMaterials scienceAb initioCondensed Matter PhysicsMolecular physicsElectronic Optical and Magnetic MaterialsCondensed Matter::Materials Sciencesymbols.namesakeAb initio quantum chemistry methodssymbolsOrthorhombic crystal systemRaman spectroscopyRaman scatteringMonoclinic crystal systemSolid solutionPhysical Review B
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High-pressure polymorphs of gadolinium orthovanadate: X-ray diffraction, Raman spectroscopy, and ab initio calculations

2019

We present a study of the different high-pressure polymorphs of $\mathrm{GdV}{\mathrm{O}}_{4}$ and its stability. Powder x-ray diffraction and Raman experiments show a phase transition from a zircon- to a scheelite-type structure taking place at 6.8(4) GPa. Ab initio density functional theory calculations support this conclusion. The equations of state of these two phases are reported. In addition, we studied the pressure evolution of the Raman modes for the zircon and scheelite phases, showing good agreement between calculations and experiments. For the sake of completeness, we performed optical-absorption measurements up to 16 GPa, showing a band-gap collapse at the transition point. Beyo…

Phase transitionMaterials scienceAb initioSTRUCTURAL STABILITYPhysics::GeophysicsELECTRONIC-PROPERTIESCondensed Matter::Materials Sciencesymbols.namesakeCrystallographyTransition pointBRILLOUIN-SCATTERINGAb initio quantum chemistry methodsX-ray crystallographysymbolsCondensed Matter::Strongly Correlated ElectronsOrthorhombic crystal systemELECTRONIC-PROPERTIES STRUCTURAL STABILITY BRILLOUIN-SCATTERINGRaman spectroscopyMonoclinic crystal systemPhysical Review B
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High-pressure study of ScVO4by Raman scattering andab initiocalculations

2011

We report results of experimental and theoretical lattice-dynamics studies on scandium orthovanadate up to 35 GPa. Raman-active modes of the low-pressure zircon phase are measured up to 8.2 GPa, where the onset of an irreversible zircon-to-scheelite phase transition is detected. Raman-active modes in the scheelite structure are observed up to 16.5 GPa. Beyond 18.2 GPa we detected a gradual splitting of the ${E}_{g}$ modes of the scheelite phase, indicating the onset of a second phase transition. Raman symmetries, frequencies, and pressure coefficients in the three phases of ScVO${}_{4}$ are discussed in the light of ab initio lattice-dynamics calculations that support the experimental resul…

Phase transitionMaterials scienceAb initiochemistry.chemical_elementCondensed Matter PhysicsMolecular physicsElectronic Optical and Magnetic Materialssymbols.namesakechemistryAb initio quantum chemistry methodsPhase (matter)X-ray crystallographysymbolsScandiumRaman spectroscopyRaman scatteringPhysical Review B
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Attosecond state-resolved carrier motion in quantum materials probed by soft x-ray XANES

2021

Recent developments in attosecond technology led to tabletop X-ray spectroscopy in the soft X-ray range, thus uniting the element- and state-specificity of core-level x-ray absorption spectroscopy with the time resolution to follow electronic dynamics in real time. We describe recent work in attosecond technology and investigations into materials such as Si, SiO2, GaN, Al2O3, Ti, TiO2, enabled by the convergence of these two capabilities. We showcase the state-of-the-art on isolated attosecond soft x-ray pulses for x-ray absorption near edge spectroscopy (XANES) to observe the 3d-state dynamics of the semi-metal TiS2 with attosecond resolution at the Ti L-edge (460 eV). We describe how the …

Phase transitionMaterials scienceAbsorption spectroscopyAttosecondGeneral Physics and AstronomyFOS: Physical sciences02 engineering and technologyElectron01 natural sciences7. Clean energy0103 physical sciencesSpectroscopy010302 applied physicsCondensed Matter - Materials Science:Física [Àrees temàtiques de la UPC]business.industryX-RaysMaterials Science (cond-mat.mtrl-sci)FísicaÒptica021001 nanoscience & nanotechnologyBrillouin zoneSemiconductorx-rayCharge carrierRaigs XAtomic physics0210 nano-technologybusiness
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Phase transition of tetragonal copper sulfide Cu2S at low temperatures

2017

The low-temperature behavior of tetragonal copper sulfide, ${\mathrm{Cu}}_{2}\mathrm{S}$, was investigated by powder and single-crystal x-ray diffraction, calorimetry, electrical resistance measurements, and ambient temperature optical absorption spectroscopy. The experiments were complemented by density-functional-theory-based calculations. High-quality, polycrystalline samples and single crystals of tetragonal copper sulfide were synthesized at 5 GPa and 700 K in a large volume multianvil press. Tetragonal ${\mathrm{Cu}}_{2}\mathrm{S}$ undergoes a temperature-induced phase transition to an orthorhombic structure at around 202 K with a hysteresis of $\ifmmode\pm\else\textpm\fi{}21$ K, an e…

Phase transitionMaterials scienceAbsorption spectroscopyBand gapTransition temperaturechemistry.chemical_element02 engineering and technology010402 general chemistry021001 nanoscience & nanotechnology01 natural sciencesCopperHeat capacity0104 chemical sciencesCrystallographyTetragonal crystal systemchemistryOrthorhombic crystal system0210 nano-technologyPhysical Review B
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