Search results for "Ferro"

showing 10 items of 2451 documents

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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On the ferroelastic nature of the scheelite-to-fergusonite phase transition in orthotungstates and orthomolybdates

2009

Abstract New evidence supporting the ferroelastic nature of the pressure-induced scheelite-to-fergusonite phase transition in ABO 4 orthotungstates and orthomolybdates (A = Ca, Sr, Ba, Pb, Eu and B = W, Mo) has been obtained from the analysis of Raman spectroscopy data. In the studied scheelite-type compounds, one external translational mode of B g symmetry in the scheelite phase softens up to the transition pressure and then becomes a hard A g mode in the fergusonite high-pressure phase. However, other scheelite-type compounds not undergoing the scheelite-to-fergusonite transition do not show softening of the B g mode. The reported results have allowed us to establish a relationship betwee…

Phase transitionCondensed matter physicsMechanical EngineeringFerroicsCondensed Matter PhysicsFergusoniteLandau theorysymbols.namesakechemistry.chemical_compoundchemistryMechanics of MaterialsPhase (matter)ScheelitesymbolsGeneral Materials ScienceRaman spectroscopyAmbient pressureMaterials Research Bulletin
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Crystal structure and dielectric properties of the [(CH3)2NH2]3Sb2(1-x)Bi2xCl9(DMACAB) mixed crystals

2001

Phase transitions in [(CH3)2NH2]3Sb2(1-x)Bi2xCl9 (DMACAB) mixed salts in the composition range 0≤x≤0.41 have been investigated by the pyroelectric method and dielectric measurements over the frequency range from 75 kHz to 900 MHz. The phase situation is additionally confirmed by the differential scanning calorimetry (DSC) and dilatometric techniques. A transition from the paraelectric (PE) to the ferroelectric (FE) phase is observed for crystals with 0≤x≤0.14. Pyroelectric measurements support the presence of polar phases. The dynamic dielectric behaviour of ferroelectric systems is found to be determined by the existence of two independent relaxators. The low-frequency relaxator reveals a …

Phase transitionCrystallographyDifferential scanning calorimetryStereochemistryChemistryPhase (matter)General Materials ScienceDielectricCrystal structureCondensed Matter PhysicsFerroelectricitySolid solutionPyroelectricityJournal of Physics: Condensed Matter
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Irreversibility of the pressure-induced phase transition of quartz and the relation between three hypothetical post-quartz phases

2004

Our atomistic computer simulations mainly based on classical force fields suggest that the pressure-induced transition from $\ensuremath{\alpha}$ quartz to quartz II at $21\phantom{\rule{0.3em}{0ex}}\mathrm{GPa}$ is irreversible. While quartz II is ferroelastic in principle, the transition itself is coelastic, as the shape of the newly formed crystal is determined by the handedness of $\ensuremath{\alpha}$-quartz. Upon releasing the pressure, our model quartz II remains stable down to $5\phantom{\rule{0.3em}{0ex}}\mathrm{GPa}$, where it undergoes an isosymmetric transformation into a less dense polymorph. If the classical force field model of quartz II is compressed quickly to $50\phantom{\…

Phase transitionEquation of stateFerroelasticityMaterials sciencePhase stabilityThermodynamicsCondensed Matter PhysicsQuartzElectronic Optical and Magnetic MaterialsPhysical Review B
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Morphology and magnetism of Fe on vicinal W(110) surfaces with different step orientation

2000

Abstract Nanostructures of monolayer height of single-crystalline Fe(1 1 0) films were grown on stepped W(1 1 0) surfaces. The growth mode strongly depends on the step orientation of the substrate. Continuous stripes are formed at steps along the [1 0 0] direction whereas triangular shaped islands grow on substrates with [1 −1 0]-oriented step edges. No ferromagnetic order was found in submonolayer films grown on [1 −1 0]-steps. The nanostripe array on [1 0 0] steps shows a ferromagnetic phase-transition with a critical behavior different from the Ising-like phase transition observed for submonolayer films grown on smooth W(1 1 0). The magnetic easy axis in the samples is oriented parallel …

Phase transitionMagnetic anisotropyMaterials scienceCondensed matter physicsFerromagnetismMagnetismFilm planeMonolayerThin filmCondensed Matter PhysicsVicinalElectronic Optical and Magnetic MaterialsJournal of Magnetism and Magnetic Materials
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The Role of Order-Disorder Transitions in the Quest for Molecular Multiferroics: Structural and Magnetic Neutron Studies of a Mixed Valence Iron (II)…

2012

Neutron diffraction studies have been carried out to shed light on the unprecedented order-disorder phase transition (ca. 155 K) observed in the mixed-valence iron(II)-iron(III) formate framework compound [NH 2(CH3)2]n[FeIIIFe II(HCOO)6]n. The crystal structure at 220 K was first determined from Laue diffraction data, then a second refinement at 175 K and the crystal structure determination in the low temperature phase at 45 K were done with data from the monochromatic high resolution single crystal diffractometer D19. The 45 K nuclear structure reveals that the phase transition is associated with the order-disorder of the dimethylammonium counterion that is weakly anchored in the cavities …

Phase transitionMagnetic structureChemistryNeutron diffraction02 engineering and technologyGeneral ChemistryCrystal structure010402 general chemistry021001 nanoscience & nanotechnology01 natural sciencesBiochemistryCatalysis0104 chemical sciencesCrystallographyColloid and Surface ChemistryFerrimagnetismX-ray crystallographyMultiferroics0210 nano-technologySingle crystal
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Dipolar superferromagnetism in monolayer nanostripes of Fe(110) on vicinal W(110) surfaces

1998

By epitaxial growth of Fe on a vicinal W~110! substrate, densely spaced and continuous monolayer stripes of Fe~110! were prepared, directed along @001#. They exhibit a sharp phase transition to ferromagnetic order, free from relaxations. The magnetic easy axis is in the plane, but along @110# that means across the stripes. This cross magnetization induces ferromagnetic dipolar coupling between the spin blocks in adjacent stripes, which are preformed by exchange interactions. The resulting superferromagnetic phase transition is therefore driven by dipolar interactions. @S0163-1829~98!52002-4#

Phase transitionMagnetizationMagnetic anisotropyMaterials scienceCondensed matter physicsFerromagnetismCondensed Matter::SuperconductivityMonolayerCondensed Matter::Strongly Correlated ElectronsSuperferromagnetismVicinalMagnetic dipole–dipole interactionPhysical Review B
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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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Crystal structure transformations induced by surface stresses in BaTiO3and BaTiO3@SiO2nanoparticles and ceramics

2015

International audience; Lattice structure transformations in nanopowders of ferroelectric BaTiO3 and BaTiO3@SiO2 core-shell nanostructured ceramics were studied by nuclear magnetic resonance (NMR) and electron paramagnetic resonance (EPR) at the temperatures 120–450 K and particle size of 300 and 500 nm. NMR spectra of all studied samples in the paraelectric phase are identical to the spectra in bulk material indicating their perfect perovskite structure without visible influence of particle surface. However, we have found that surface of particles essentially influence the ferroelectric phase transitions detected by both NMR and EPR techniques. The strongest changes as compared to bulk mat…

Phase transitionMaterials scienceAnalytical chemistry02 engineering and technologyCrystal structureceramics01 natural scienceslaw.inventionCondensed Matter::Materials Sciencechemistry.chemical_compoundNuclear magnetic resonancelawPhase (matter)barium titanate0103 physical sciencesGeneral Materials Science010306 general physicsElectron paramagnetic resonanceInstrumentation[CHIM.MATE]Chemical Sciences/Material chemistry021001 nanoscience & nanotechnologyFerroelectricityNMR spectra databasenuclear magnetic resonanceferroelectric phase transitionchemistryBarium titanateCurie temperaturenanoparticlesCondensed Matter::Strongly Correlated Electrons0210 nano-technologyPhase Transitions
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DIELECTRIC PROPERTIES OF LEAD-FREE [(1-x)(Na0.5Bi0.5)-xBa]Zr1−yTiyO3CERAMICS (x = 0.01, 0.06, 0.085, 0.09, 0.1 AND y = 0.96, 0.97)

2008

ABSTRACT Lead-free ceramics based on (Na0.5Bi0.5TiO3, NBT)-(Ba(Ti, Zr)O3, BTZ) were prepared by solid phase synthesis and hot pressing sintering process and their dielectric properties have been studied. The obtained results were compared with these for pure NBT. The obtained samples show pure perovskite structure. Low frequency (100 Hz-100 kHz) investigations reveal the diffuse phase transitions and relaxorlike behaviour. The obtained results are discussed in terms of inhomogeneity of ions distribution, their ferro- and antiferroactivity and internal stresses. The NBT-BTZ system is expected to be a new promising candidate for lead-free electronic ceramics.

Phase transitionMaterials scienceAnalytical chemistryMineralogySinteringDielectricLow frequencyCondensed Matter PhysicsHot pressingFerroelectricityElectronic Optical and Magnetic MaterialsIonControl and Systems Engineeringvisual_artMaterials ChemistryCeramics and Compositesvisual_art.visual_art_mediumCeramicElectrical and Electronic EngineeringIntegrated Ferroelectrics
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