Search results for "Phase Transition"

showing 10 items of 1281 documents

Structural Metastability and Quantum Confinement in Zn1–xCoxO Nanoparticles

2016

This paper investigates the electronic structure of wurtzite (W) and rock-salt (RS) Zn1-xCoxO nanoparticles (NPs) by means of optical measurements under pressure (up to 25 GPa), X-ray absorption, and transmission electron microscopy. W-NPs were chemically synthesized at ambient conditions and RS-NPs were obtained by pressure-induced transformation of W-NPs. In contrast to the abrupt phase transition in W-Zn1-xCoxO as thin film or single crystal, occurring sharply at about 9 GPa, spectroscopic signatures of tetrahedral Co(2+) are observed in NPs from ambient pressure to about 17 GPa. Above this pressure, several changes in the absorption spectrum reveal a gradual and irreversible W-to-RS pha…

Phase transitionCondensed matter physicsAbsorption spectroscopyChemistryMechanical EngineeringBioengineering02 engineering and technologyGeneral ChemistryElectronic structure021001 nanoscience & nanotechnologyCondensed Matter Physics01 natural sciencesAbsorption bandMetastability0103 physical sciencesGeneral Materials Science010306 general physics0210 nano-technologyAbsorption (electromagnetic radiation)Single crystalWurtzite crystal structureNano Letters
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On the commensurate–incommensurate transition in adsorbed monolayers

1999

Abstract A Monte Carlo simulation method is used to study the commensurate–incommensurate phase transition in monolayers and the formation of bilayer films on the (100) face of an fcc crystal. The phase diagram for the system which forms the registered (1×1) and high density incommensurate phases in the monolayer has been determined. It is shown that the registered phase undergoes the transition to a denser incommensurate solid phase when the film density increases. The mechanism of melting of the monolayer film is found to depend on the film density. In particular, the melting of dense incommensurate solid monolayer film is found to be accompanied by the transfer of adsorbed molecules into…

Phase transitionCondensed matter physicsChemistryBilayerSurfaces and InterfacesCondensed Matter PhysicsSurfaces Coatings and FilmsCrystalPhase (matter)MonolayerMaterials ChemistryMoleculeLayer (electronics)Phase diagramSurface Science
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Kinetics of the Formation of Ordered Domains on Surfaces: Theoretical Considerations and Monte-Carlo Simulation

1986

When an adsorbed monolayer which initially is in a disordered state is suddenly brought to a temperature in the regime of the ordered phase, domains of the ordered phase are predicted to form and grow with time t after the quench according to a power law, i.e. linear dimension L(t) ∞ tx. At the same time, the structure function S(k,t) is predicted to satisfy a scaling law, S(k,t) = S(k,tx), k being the difference between the wave vector observed in the scattering and the Bragg wave vector describing the long range order. The theoretical ideas which lead to this behaviour are briefly reviewed, and evidence from simulations of simple lattice gas models and Potts models is presented. Particula…

Phase transitionCondensed matter physicsChemistryCritical point (thermodynamics)General Chemical EngineeringLattice (order)Monte Carlo methodExponentWave vectorPower lawUniversality (dynamical systems)Berichte der Bunsengesellschaft für physikalische Chemie
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Critical effects in optical response due to charge transfer vibronic excitons and their structure in perovskite-like systems

1999

Abstract A mechanism for bilinear interaction between high-frequency light-induced electronic polarization and low-frequency soft lattice polarization is proposed. It is based on the fluctuations of the charge transfer connected with charge transfer vibronic excitons (CTVE). This bilinear mechanism leads to the appearance of the critical peculiarities of the absolute diffraction efficiency of transient gratings near the ferroelectric phase transition. A semi-empirical Hartree–Fock INDO method was used for the evaluation of the energy parameters and the equilibrium displacements for the CTVE in KTaO 3 . This numerical study did confirm the proposed CTVE-model. It was shown that the CTVE-phas…

Phase transitionCondensed matter physicsChemistryExcitonBiophysicsGeneral ChemistrySoft modesCondensed Matter PhysicsBiochemistryFerroelectricityAtomic and Molecular Physics and OpticsDipoleMetastabilityLattice (order)Perovskite (structure)Journal of Luminescence
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Simulation of the glass transition in polymeric systems: Evidence for an underlying phase transition?

1998

Abstract The bond fluctuation model of polymer chains on sc lattices with an energy that favours long bonds can describe the slowing down of supercooled melts that approach the glass transition in qualitative similarity with various experiments. In this paper we focus on the question of whether there exists a correlation length that increases to large values when the temperature is lowered towards the glass transition. Two types of analysis are presented: firstly density oscillations near hard walls become long range, and the resulting correlation length becomes larger than the gyration radius, secondly oscillations in the pair correlation function in real space also become long range, and …

Phase transitionCondensed matter physicsChemistryGeneral Chemical EngineeringGeneral Physics and AstronomyPeriodic boundary conditionsRadiusSupercoolingRadial distribution functionGlass transitionGyrationScalingPhilosophical Magazine B
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Monte Carlo investigation of head-tail ordering of CO monolayers on graphite

1994

Abstract Heat capacity measurements recently showed that CO physisorbed on graphite undergoes a head-tail ordering transition at roughly 5 K. The present paper is a detailed Monte Carlo study of this phase transition and the ordered state. The simulations are based on an ab initio pair potential and rely crucially on a thorough finite-size scaling study of various quantities. In agreement with experiments we find that the transition belongs to the universality class of the Ising model in two dimensions. We go beyond experimental knowledge by revealing the particular ferrielectric structure of the ground state, and show that the transition is due to the molecule's shape asymmetry rather than…

Phase transitionCondensed matter physicsChemistryMonte Carlo methodAb initioSurfaces and InterfacesCondensed Matter PhysicsHeat capacitySurfaces Coatings and FilmsDipoleMaterials ChemistryIsing modelGround statePair potentialSurface Science
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Phase Transitions in Dense Lipid Monolayers Grafted to a Surface:  Monte Carlo Investigation of a Coarse-Grained Off-Lattice Model

1996

Semiflexible amphiphilic molecules end-grafted at a flat surface are modeled by a bead-spring chain with stiff bond angle potentials. Constant density Monte Carlo simulations are performed varying temperature, density, and chain length of the molecules, whose effective monomers interact with Lennard-Jones potentials. For not too large densities and low temperatures the monolayer is in a quasi-two-dimensional crystalline state, characterized by uniform tilt of the (stretched) chains. Raising the temperature causes a second-order transition into a (still solid) phase with no tilt. For the first time, finite size scaling concepts are applied to a model of a surfactant monolayer, and it is foun…

Phase transitionCondensed matter physicsChemistryMonte Carlo methodGeneral EngineeringCondensed Matter::Soft Condensed MatterTilt (optics)Molecular geometryChemical physicsPhase (matter)MonolayerPhysical and Theoretical ChemistryScalingLattice model (physics)The Journal of Physical Chemistry
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Mössbauer study of properties and phase transitions of Cd2Nb2–2xSn2xO7–2xF2x

1973

With the aid of Mossbauer spectroscopy the solid solution series Cd2Nb2–2xSn2xO7–2xF2x are investigated in the temperature range 4.2 to 400 K. The crystal structure belongs to the cubic pyrochlore type. The BY6 octahedra (B = Nb, Sn; Y = O, F) are linked three-dimensionally through their corners, forming groups of four octahedra which are extended or compressed in the (111)-direction for x ≤ 0.375 or x ≥ 0.400 respectively. The dependence of the quadrupole splitting ΔEQ on x shows a small but significant discontinuity in the region 0.375 < x < 0.400. This can be attributed to a first order phase-transition which depends on concentration, but not on temperature over the temperature region st…

Phase transitionCondensed matter physicsChemistryPyrochloreQuadrupole splittingSoft modesCrystal structureAtmospheric temperature rangeengineering.materialCondensed Matter PhysicsElectronic Optical and Magnetic MaterialsCrystallographyOctahedronMössbauer spectroscopyengineeringPhysica Status Solidi (a)
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In-Plane Anisotropy and Phase Change in Langmuir-Blodgett Films of a Triphenylene Derivative

1993

Abstract The “in-plane anisotropy” of a triphenylene derivative in Langmuir-Blodgett (L.B.) films has been investigated. Upon heating, L.B. films exhibit a reversible phase transition appearing as an abrupt increase from a low to a high “in-plane anisotropy” corresponding to the formation of the same hexagonal liquid crystal phase observed in the bulk material at almost the same temperature, with the columnar axis aligned along the dipping direction.

Phase transitionCondensed matter physicsChemistryTriphenyleneCondensed Matter PhysicsPhotochemistryLangmuir–Blodgett filmCondensed Matter::Soft Condensed Matterchemistry.chemical_compoundIn planeLiquid crystalCondensed Matter::SuperconductivityPhase (matter)AnisotropyDerivative (chemistry)Molecular Crystals and Liquid Crystals Science and Technology. Section A. Molecular Crystals and Liquid Crystals
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Pressure Dependence of the Low-Frequency Dielectric Constant in III-VI Semiconductors

1999

In this work we report on the pressure dependence of the low-frequency dielectric constant parallel to the c-axis (e∥) in GaS, GaSe, and InSe as obtained from direct capacitance measurements. A large increase of e∥ with pressure has been observed. The pressure change of the lattice polarizability along the c-axis is calculated in the framework of a rigid-ion model from the change of the angle of the anion–cation bond with respect to the layer plane, which results in a slight increase of the lattice contribution. Consequently, the pressure behaviour of e∥ is proposed to arise from the large increase of the electronic polarizability along the c-axis. This is explained through a decrease of th…

Phase transitionCondensed matter physicsChemistrybusiness.industryDielectricLow frequencyPressure dependenceCondensed Matter PhysicsCapacitanceElectronic Optical and Magnetic MaterialsSemiconductorPolarizabilityLattice (order)businessphysica status solidi (b)
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