Search results for "Phase transition"

showing 10 items of 1281 documents

The pressure-induced ringwoodite to Mg-perovskite and periclase post-spinel phase transition: a Bader’s topological analysis of the ab initio electro…

2011

In order to characterize the pressure-induced decomposition of ringwoodite (c-Mg2SiO4), the topological analysis of the electron density q(r), based upon the theory of atoms in molecules (AIM) developed by Bader in the framework of the catastrophe theory, has been performed. Calculations have been carried out by means of the ab initio CRYSTAL09 code at the HF/DFT level, using Hamiltonians based on the Becke- LYP scheme containing hybrid Hartree– Fock/density functional exchange–correlation terms. The equation of state at 0 K has been constructed for the three phases involved in the post-spinel phase transition (ringwoodite -> Mg-perovskite + periclase) occurring at the transition zone–lower…

Bader’s topological analysisElectron densityEquation of statePhase transitionRingwoodite Post-spinel phase transition Bader’s topological analysis Ab initio Catastrophe theory Critical pointsChemistryCatastrophe theoryAtoms in moleculesRingwooditeAb initioCritical pointsHartreeengineering.materialTopologyRingwoodite; Post-spinel phase transition; Bader’s topological analysis; Ab initio; Catastrophe theory; Critical pointsPost-spinel phase transitionRingwooditeGeochemistry and PetrologyBader’s topological analysiAb initioengineeringGeneral Materials SciencePerovskite (structure)
researchProduct

Finite Size Effects in Thin Film Simulations

2003

Phase transitions in thin films are discussed, with an emphasis on Ising-type systems (liquid-gas transition in slit-like pores, unmixing transition in thin films, orderdisorder transitions on thin magnetic films, etc.) The typical simulation geometry then is a L xL x D system, where at the low confining L x L surfaces appropriate boundary “fields” are applied, while in the lateral directions periodic boundary conditions are used. In the z-direction normal to the film, the order parameter always is inhomogeneous, due to the boundary “fields” at the confining surfaces. When one varies the temperature T from the region of the bulk disordered phase to a temperature below the critical temperatu…

BinodalPhase transitionMaterials scienceCapillary condensationCondensed matter physicsPhase (matter)Periodic boundary conditionsBoundary (topology)Symmetry breakingThin film
researchProduct

Monte carlo studies of phase transitions in polymer blends and block copolymer melts

1994

The unmixing transition of both symmetrical polymer blends AB (i.e. chain lengthsNA=NB=N) and asymmetrical ones (NB/NA=2,3) is studied by large-scale Monte Carlo simulations of the bond fluctuation model. Combination of semi-grand-canonical simulation techniques, «histogram reweighting» and finitesize scaling allows an accurate location of the coexistence curve in the critical region. The variation of the critical temperature with chain length (N) is studied and compared to theoretical predictions. For the symmetrical case, use of chain lengths up toN=512 allows a rough estimation of crossover scaling functions for the crossover from Ising to mean-field exponents. The order-disorder transit…

BinodalPhase transitionMaterials scienceChain (algebraic topology)Vacancy defectMonte Carlo methodGeneral Physics and AstronomyThermodynamicsIsing modelStatistical physicsPolymer blendScalingIl Nuovo Cimento D
researchProduct

Continuum Monte Carlo simulation of phase transitions in rod-like molecules at surfaces

1994

Stiff rod-like chain molecules with harmonic bond length potentials and trigonometric bond angle potentials are used to model Langmuir monolayers at high densities. One end of the rod-like molecules is strongly bound to a flat two-dimensional substrate which represents the air-water interface. A ground-state analysis is performed which suggests phase transitions between phases with and without collective uniform tilt. Large-scale off-lattice Monte Carlo simulations over a wide temperature range show in addition to the tilting transition the presence of a strongly constrained melting transition at high temperatures. The latter transition appears to be related to two-dimensional melting of th…

Bond lengthPhase transitionMolecular geometryMaterials scienceCondensed matter physicsLattice (order)Monte Carlo methodMonolayerGeneral Physics and AstronomyMoleculeAtmospheric temperature rangeIl Nuovo Cimento D
researchProduct

Theoretical modeling of antiferrodistortive phase transition forSrTiO3ultrathin films

2013

Combining group-theoretical analysis and first-principles density functional theory calculations, we confirm theoretically the antiferrodistortive phase transition in ultrathin SrTiO${}_{3}$ (001) TiO${}_{2}$-terminated films and compare it with a similar transition in the bulk. We demonstrate phonon softening at the $M$ point of the surface Brillouin zone and analyze the change in the calculated electronic and phonon properties upon phase transition.

Brillouin zoneSurface (mathematics)Condensed Matter::Materials SciencePhase transitionMaterials scienceCondensed matter physicsPhononCondensed Matter::SuperconductivityCondensed Matter::Strongly Correlated ElectronsDensity functional theoryCondensed Matter PhysicsSofteningElectronic Optical and Magnetic MaterialsPhysical Review B
researchProduct

Lattice dynamics of wurtzite and rocksalt AlN under high pressure: Effect of compression on the crystal anisotropy of wurtzite-type semiconductors

2008

Raman spectra of aluminum nitride (AlN) under pressure have been measured up to $25\phantom{\rule{0.3em}{0ex}}\mathrm{GPa}$, i.e., beyond the onset of the wurtzite-to-rocksalt phase transition around $20\phantom{\rule{0.3em}{0ex}}\mathrm{GPa}$. The experimental pressure coefficients for all the Raman-active modes of the wurtzite phase are reported and compared to those obtained from ab initio lattice dynamical calculations, as well as to previous experimental and theoretical results. The pressure coefficients of all the Raman-active modes in wurtzite-type semiconductors (AlN, GaN, InN, ZnO, and BeO), as well as the relatively low bulk modulus and phase transition pressure in wurtzite AlN, a…

Bulk modulusPhase transitionMaterials scienceCondensed matter physicsCondensed Matter::Otherbusiness.industryAb initioNitrideCondensed Matter::Mesoscopic Systems and Quantum Hall EffectCondensed Matter PhysicsElectronic Optical and Magnetic MaterialsCondensed Matter::Materials Sciencesymbols.namesakeSemiconductorLattice (order)symbolsbusinessRaman spectroscopyWurtzite crystal structurePhysical Review B
researchProduct

Electrochemical deposition of CZTS thin films on flexible substrate

2014

Abstract In this work, we report some preliminary results concerning the fabrication of quaternary semiconductor Cu2ZnSnS4 (CZTS) thin films on a flexible substrate through the simultaneous electrodeposition of elements having different standard electrochemical potentials. CZTS thin films were obtained by potentiostatic deposition from aqueous baths at room temperature and under N2 atmosphere, varying bath composition. Chemical composition and structure of the electrodeposited films were evaluated by EDS, SEM, RAMAN and XRD. Preliminary results on the photoelectrochemical behaviour of the films will be also presented.

CZTS solar cellMaterials scienceFabricationbusiness.industryMetallurgySubstrate (electronics)Electrochemistrysymbols.namesakechemistry.chemical_compoundSemiconductorSettore ING-IND/23 - Chimica Fisica ApplicataEnergy(all)chemistryChemical engineeringthin filmsCZTS solar cellssymbolselectrodepositionDeposition (phase transition)CZTSThin filmRaman spectroscopybusiness
researchProduct

Canonical versus microcanonical analysis of first-order phase transitions

1998

Abstract I discuss the relation between canonical and microcanonical analyses of first-order phase transitions. In particular it is shown that the microcanonical Maxwell construction is equivalent to the equal-peak-height criterion often employed in canonical simulations. As a consequence the microcanonical finite-size estimators for the transition point, latent heat and interface tension are identical to standard estimators in the canonical ensemble. Special emphasis is placed on various ways for estimating interface tensions. The theoretical considerations are illustrated with numerical data for the two-dimensional 10-state Potts model.

Canonical ensembleNuclear and High Energy PhysicsPhase transitionMicrocanonical ensembleTransition pointCritical phenomenaMaxwell constructionEstimatorStatistical physicsAtomic and Molecular Physics and OpticsPotts modelMathematicsNuclear Physics B - Proceedings Supplements
researchProduct

Quantum Effects and Phase Transitions in Adsorbed Molecular Layers

1998

Phase transitions in adsorbed (two dimensional) fluids and in adsorbed layers of molecules are studied with a combination of path integral Monte Carlo (PIMC), Gibbs ensemble Monte Carlo (GEMC) and finite size scaling techniques. Entropy driven phase transitions in systems with purely repulsive interactions are analyzed as well phase diagrams of fluids with internal quantum states. Adsorbed layers of H 2 molecules at a full monolayer coverage in the \(\sqrt 3 \times \sqrt 3 \) structure have a higher transition temperature to the disordered phase compared to the system with the heavier D 2 molecules, this effect is analyzed by PIMC. Linear N 2 molecules adsorbed on graphite show a transition…

Canonical ensemblePhase transitionMaterials scienceMean field theoryTricritical pointQuantum mechanicsPhase (matter)MonolayerPhysics::Chemical PhysicsPath integral Monte CarloPhase diagram
researchProduct

Monte Carlo Simulation of Alloy Phase Diagrams and Short-Range Order

1986

As a prototype model for order-disorder phenomena in binary alloys, a face-centered cubic lattice is considered,the sites of which can be taken by either A-atoms or B-atoms, assuming pair-wise interactions between nearest (J) and next nearest neighbours (J). The phase diagram is constructed from Monte Carlo calculations. Some technical aspects essential for the success of such calculations are briefly mentioned (use of grand-canonical rather than canonical ensemble, how to obtain the free energy needed to locate first-order phase transitions, etc.). It is shown that the topology of the phase diagram changes when the ratio R = Jnnn/Jnn is varied, and this behaviour is discussed in the contex…

Canonical ensemblePhase transitionMean field theoryLattice (order)Monte Carlo methodBinary numberStatistical physicsRenormalization groupMathematicsPhase diagram
researchProduct