Search results for "Phase boundary"

showing 10 items of 41 documents

Ceramics and Thin Films of Some New Pb(B 3+ ,Nb)TiO 3 -PbTiO 3 Systems

2003

The structure, dielectric, and electromechanical properties of (1 m x )Pb(B 3+ ,Nb)TiO 3 - x PbTiO 3 binary systems (B = Lu, Er, Tb, Ho) are reported. The crystallographic features at the morphotropic phase boundary (MPB) between tetragonal P4mm and pseudo-monoclinic M phases are discussed with respect to electro-mechanical properties. Doping effect (with La 3+ ) on the properties of ceramic samples of pseudobinary Pb(Lu 1/2 Nb 1/2 )O 3 -PbTiO 3 (PLuNT) system has been investigated. Pb(Mg 1/3 Nb 2/3 )-PbTiO 3 (PT) solid solutions were studied under different processing conditions for obtaining ceramics of 100% perovskite structure with sufficient high j T EC ∼ 1 K near room temperature. The…

Phase boundaryMaterials scienceAnalytical chemistryDielectricCondensed Matter PhysicsFerroelectricityElectronic Optical and Magnetic MaterialsPulsed laser depositionTetragonal crystal systemvisual_artvisual_art.visual_art_mediumCeramicThin filmSolid solutionFerroelectrics
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Hydrogen Formation on Phase Boundaries of Sn/Al

2002

The present paper continues our earlier study of the embrittlement of Sn-Al eutectic alloy in water vapor and hydrogen emission from it, Atomically clean interfaces of solid phase joints of Sn with Al served as simple phase boundary models for this system. It was found by SIMS, X-ray and SEM techniques that the brittleness is caused by chemical adsorption of hydrogen on phase boundaries. This process is facilitated by structural defects. The reaction of hydrogen with phase boundary occurs first in regions of micro-and submicrocracks. The effect is irreversible one and it is associated with the formation of SnH4 that is instable and decomposes at the room temperature. The phase boundary of S…

Phase boundaryMaterials scienceHydrogenHydrogen formationMetallurgychemistry.chemical_elementThermodynamicsBrittlenesschemistryPhase (matter)Physics::Atomic PhysicsEmbrittlementWater vaporEutectic system
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New high piezoelectric coupling PLuNT binary system ceramics

1999

Abstract The new (1 − x)Pb( Lu 1 2 Nb 1 2 ) O 3 − x PbTiO 3 binary system ceramics in the interval 0 0.49). The morphotropic region extends over the interval x = 0.38–0.49, the concentration ratio M:T ≅ 1 corresponds to x = 0.41. The maximum values of the electromechanical coupling coefficients k p = 0.663, k t = 0.481, k 31 = 0.355 of (1 − x)PLuN-xPT ceramics were attained in compositions PLuNT 59/41 (T m = 353 °C) near the morphotropic phase boundary (MPB). The PLuNT system, having large values of electromechanical coupling and the highest T m (> 350 °C) among binary Pb(B′,B″)O 3 -PT perovskites may be favorable for piezoelectric sensors and actuators, and may have an interest as promisin…

Phase boundaryMaterials sciencePiezoelectric sensorAnalytical chemistryCondensed Matter PhysicsConcentration ratiovisual_artvisual_art.visual_art_mediumGeneral Materials ScienceBinary systemCeramicThin filmPiezoelectric couplingSingle crystalNanostructured Materials
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Near-coincidence lattice method for the determination of epitaxy strains during oxidation of metals

2000

Abstract A theoretical method is proposed to evaluate the strains due to epitaxy between a metal and its oxide. Based on Bollmann’s approach of two adjoining grains, it uses the quantitative texture analysis of the two materials separated by the phase boundary. Our study of the Zr/ZrO 2 and Mo/MoO 3 systems reveals strong correlations between the criterion of best fit proposed by Bollmann and the orientation distribution function obtained by a quantitative texture analysis. The results of this study are used in a thermo-mechano-chemical simulation of the oxidation process of zirconium, which leads to this observation: two different zirconia orientations induce two different oxidation kineti…

Phase boundaryMaterials sciencePolymers and PlasticsOxideAnalytical chemistrychemistry.chemical_element02 engineering and technologyEpitaxy01 natural sciences[SPI.MAT]Engineering Sciences [physics]/Materialschemistry.chemical_compound[SPI]Engineering Sciences [physics]Transition metal0103 physical sciencesCubic zirconiaTexture (crystalline)ComputingMilieux_MISCELLANEOUS010302 applied physicsZirconiumMetals and AlloysRefractory metals021001 nanoscience & nanotechnologyElectronic Optical and Magnetic MaterialsCrystallographychemistryCeramics and Composites0210 nano-technology
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Phase behaviour of binary mixtures of colloidal charged spheres

2008

Abstract As a step towards the modelling of binary metal alloys we here report on the shape of the phase boundary of two deionized charged sphere colloidal suspensions as a function of mixing ratio and particle density. Their size ratios are r = 0.68 and r = 0.56. Both aqueous suspensions of polystyrene copolymer spheres crystallize in a body-centred cubic structure. Interesting differences in the shape of the phase boundary are observed. In the first case a peaked increase of crystal stability was observed for a mixing ratio of p = 0.2–0.3, which gives the fraction of small spheres. Also in the second case the stability of the crystalline phase is larger than expected for an ideal solid so…

Phase boundaryMaterials scienceThermodynamicsColloidal crystallaw.inventionColloidCrystallographyColloid and Surface ChemistrylawPhase (matter)CrystallizationPhase diagramSolid solutionEutectic systemColloids and Surfaces A: Physicochemical and Engineering Aspects
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The high-pressure, high-temperature phase diagram of cerium

2020

Abstract We present an experimental study of the high-pressure, high-temperature behaviour of cerium up to ∼22 GPa and 820 K using angle-dispersive x-ray diffraction and external resistive heating. Studies above 820 K were prevented by chemical reactions between the samples and the diamond anvils of the pressure cells. We unambiguously measure the stability region of the orthorhombic oC4 phase and find it reaches its apex at 7.1 GPa and 650 K. We locate the α-cF4–oC4–tI2 triple point at 6.1 GPa and 640 K, 1 GPa below the location of the apex of the oC4 phase, and 1–2 GPa lower than previously reported. We find the α-cF4 → tI2 phase boundary to have a positive gradient of 280 K (GPa)−1, less…

Phase boundaryMaterials scienceTriple pointThermodynamicsDiamondchemistry.chemical_element02 engineering and technologyengineering.material021001 nanoscience & nanotechnologyCondensed Matter Physics01 natural sciencesCeriumchemistryPhase (matter)0103 physical sciencesX-ray crystallographyengineeringGeneral Materials ScienceOrthorhombic crystal system010306 general physics0210 nano-technologyPhase diagramJournal of Physics: Condensed Matter
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High-pressure, high-temperature phase diagram of InSe: A comprehensive study of the electronic and structural properties of the monoclinic phase of I…

2006

We report on an investigation of the high-pressure, high-temperature phase diagram of InSe. We optically observed the phase transition from the rhombohedral polytype (InSe-I) to the monoclinic phase (InSe-II) and determined the phase boundary up to $10\phantom{\rule{0.3em}{0ex}}\mathrm{GPa}$. High-pressure resistivity measurements were performed to complement the optical measurements. Monoclinic and cubic InSe (InSe-III) were observed to be metastable around $14.5\phantom{\rule{0.3em}{0ex}}\mathrm{GPa}$ and $420\phantom{\rule{0.3em}{0ex}}\mathrm{K}$, and evidence suggesting the existence of an as yet unidentified new high-pressure and high-temperature phase was found. By means of optical ab…

Phase boundaryPhase transitionMaterials scienceCondensed matter physicsbusiness.industryCondensed Matter PhysicsElectronic Optical and Magnetic MaterialsPhysics::Fluid DynamicsCondensed Matter::Materials ScienceOpticsAbsorption edgePhase (matter)Absorption (logic)businessRefractive indexMonoclinic crystal systemPhase diagramPhysical Review B
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Structure and Properties of Novel Pb(B’1/2Nb1/2)O3-PbTiO3 Binary Systems with High Piezoelectric Coupling

2000

The (l-x)Pb(Lu1/2Nb1/2)O3-xPbTiO3 (PLuNT) and (l-x)Pb(Er1/2Nb1/2)O3-xPbTiO3 (PErNT) binary systems have been originally synthesized. Pure lutecium niobate (PLuN) (x = 0) has a pronounced long-range order in the B-sublattice and an antiferroelectric to paraelectric phase transition at ~258°C. The phase structure of the PLuNT system, at room temperature, changes from a pseudomonoclinic (psd-M, space group Bmm2) to tetragonal (T, space group P4mm). The pseudomonoclinic phase extends over the 0 ≤ x ≤ 0.38 interval within which the monoclinic angle β proceeds a minimum near to 90° at x≅0.2. The morphotropic region covers over the interval x = 0.38–0.49, the concentration ratio psd-M:T≅l (the mor…

Phase boundaryPhase transitionTetragonal crystal systemchemistry.chemical_compoundMaterials sciencechemistryPhase (matter)Analytical chemistryAntiferroelectricityDielectricLead titanateMonoclinic crystal system
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Interdiffusion in blends of polystyrene and polymethylstyrene studied by light scattering after temperature jumps across the phase boundary

1992

Abstract We describe a simple light scattering set-up for measuring interdiffusion coefficients D in polymer blends by generating spinodal decomposition and subsequent dissolution after temperature jumps across the phase boundary. In blends of polystyrene and polymethylstyrene (random copolymer of 60% m-methylstyrene and 40% p-methylstyrene) D values were obtained between 10−11 and 10−15 cm2s−1 at temperatures up to 50 K above the upper critical solution temperature. The results are discussed in relation to tracer diffusion in the same system.

Phase boundaryPolymers and PlasticsChemistrySpinodal decompositionDiffusionOrganic ChemistryThermodynamicsLight scatteringchemistry.chemical_compoundUpper critical solution temperaturePolymer chemistryMaterials ChemistryPolymer blendPolystyreneDissolutionPolymer
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The Role of Diffusion Accommodation and Phase Boundary Wetting in the Deformation Behaviour of Ultrafine Grained Sn-Pb Eutectic

2010

Mechanical properties, microstructure of the Sn–38wt. %Pb eutectic and the development of deformation - induced diffusion processes on interphase boundaries (IB) were investigated. Experiments were carried out both in deformed and annealed states of eutectic using micro- and nanoindentation, SEM, AFM and optical microscopy techniques. It was found that the deformation of the annealed alloy is localized at the Pb/Sn interphase boundaries and occurs by grain boundary sliding (GBS) accompanied by sintering micropore processes under the action of the capillary forces on the Pb/Sn IB. During severe plastic deformation of Sn-Pb eutectic phase transition in the Sn grain boundary occurs. This defor…

Phase boundaryRadiationMaterials scienceMetallurgyCondensed Matter PhysicsGeneral Materials ScienceGrain boundaryWettingDeformation (engineering)Composite materialSevere plastic deformationElastic modulusGrain Boundary SlidingEutectic systemDefect and Diffusion Forum
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