Search results for "Transition temperature"

showing 10 items of 137 documents

Interpretation of the Electrocaloric Effect in Na1/2Bi1/2TiO3-SrTiO3-PbTiO3Solid Solutions

2015

Results of direct measurements of electrocaloric effect and polarization are mutually compared in solid solutions 0.4Na1/2Bi1/2TiO3-(0.6-x)SrTiO3-xPbTiO3. Three temperature regions are distinguished in respect of a phase transition temperature. Above the phase transition, electrocaloric effect is determined by orientation of polar nanoregions by electric field. In wide temperature regions above and below the phase transition temperature, the difference between results, obtained from direct electrocaloric effect measurements and from polarization hysteresis loops, is explained by temperature dependence of concentration of polar nanoregions, oriented by electric field. Existence of a common Δ…

Phase transitionPhase transition temperatureMaterials scienceCondensed matter physicsThermodynamicsCondensed Matter PhysicsPolarization (waves)FerroelectricityElectronic Optical and Magnetic MaterialsCondensed Matter::Materials ScienceElectric fieldElectrocaloric effectPolarSolid solutionFerroelectrics
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Guest Modulation of Spin-Crossover Transition Temperature in a Porous Iron(II) Metal Organic Framework: Experimental and Periodic DFT Studies

2014

The synthesis, structure, and magnetic properties of three clathrate derivatives of the spin-crossover porous coordination polymer {Fe(pyrazine)[Pt(CN)(4)]} (1) with five-membered aromatic molecules furan, pyrrole, and thiophene is reported. The three derivatives have a cooperative spin-crossover transition with hysteresis loops 14-29 K wide and average critical temperatures T-c=201 K (1.fur), 167 K (1.pyr), and 114.6 K (1.thio) well below that of the parent compound 1 (T-c=295 K), confirming stabilization of the HS state. The transition is complete and takes place in two steps for 1.fur, while 1.pyr and 1.thio show 50% spin transition. For 1.fur the transformation between the HS and IS (mi…

Phase transitionPyrazineMetal–organic frameworksTransition temperatureOrganic ChemistrySpin transitionSpace groupGeneral ChemistryCatalysisSpin-crossover compoundsCrystallographychemistry.chemical_compoundTetragonal crystal systemDensity functional calculationsHofmann clathrateschemistryComputational chemistrySpin crossoverFISICA APLICADAMagnetic propertiesOrthorhombic crystal system
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Meltable Spin Transition Molecular Materials with Tunable Tc and Hysteresis Loop Width.

2015

Herein, we report a way to achieve abrupt high-spin to low-spin transition with controllable transition temperature and hysteresis width, relying not on solid-state cooperative interactions, but utilizing coherency between phase and spin transitions in neutral FeII meltable complexes

Phase transitionThermochromismCondensed matter physicsSpin transitionsMagnetismChemistryTransition temperatureSpin transitionMagnetismGeneral ChemistryCatalysisHysteresisNuclear magnetic resonancePhase transitionsPhase (matter)FISICA APLICADACondensed Matter::Strongly Correlated ElectronsSoft matterSoft matterSpin-½Angewandte Chemie (International ed. in English)
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On the order of the herringbone transition of N2 on graphite: a Monte Carlo study

1993

Using the anisotropic planar-rotor model we investigate the herringbone phase transition of N2 in the (√3 × √3)R30° commensurate phase on graphite by large scale Monte Carlo simulations. The effective correlation length ξ is measured near the transition temperature T0. The data, extrapolated to T0, yield a large but finite ξ at T0 demonstrating that the herringb ordering is a weak first order transition.

Phase transitionYield (engineering)Condensed matter physicsScale (ratio)ChemistryTransition temperatureMonte Carlo methodSurfaces and InterfacesCondensed Matter PhysicsSurfaces Coatings and FilmsPhase (matter)Materials ChemistryPhysical chemistryGraphiteAnisotropySurface Science
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The high-temperature dynamics of a mean-field Potts glass

2002

Abstract We use Monte Carlo simulations to investigate the dynamic properties of the ten-state infinite-range Potts glass. By analyzing the spin autocorrelation function for system sizes up to N = 2560, we show that strong finite size effects are present around the predicted dynamic transition temperature. The autocorrelation function shows strong self-averaging at high temperatures, whereas close to the dynamic transition shows lack of self-averaging.

PhysicsCondensed matter physicsMean field theoryGeneral Chemical EngineeringTransition temperatureDynamics (mechanics)Monte Carlo methodAutocorrelationDynamic Monte Carlo methodGeneral Physics and AstronomyStatistical physicsSpin-½Philosophical Magazine B
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Anisotropic interfacial tension, contact angles, and line tensions: A graphics-processing-unit-based Monte Carlo study of the Ising model

2014

As a generic example for crystals where the crystal-fluid interface tension depends on the orientation of the interface relative to the crystal lattice axes, the nearest neighbor Ising model on the simple cubic lattice is studied over a wide temperature range, both above and below the roughening transition temperature. Using a thin film geometry $L_x \times L_y \times L_z$ with periodic boundary conditions along the z-axis and two free $L_x \times L_y$ surfaces at which opposing surface fields $\pm H_{1}$ act, under conditions of partial wetting, a single planar interface inclined under a contact angle $\theta < \pi/2$ relative to the yz-plane is stabilized. In the y-direction, a generaliza…

PhysicsCondensed matter physicsStatistical Mechanics (cond-mat.stat-mech)Transition temperatureThermodynamic integrationFOS: Physical sciencesComputational Physics (physics.comp-ph)MagnetizationLattice (order)Periodic boundary conditionsIsing modelBoundary value problemAnisotropyPhysics - Computational PhysicsCondensed Matter - Statistical Mechanics
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Properties of the Ising magnet confined in a corner geometry

2007

Abstract The properties of Ising square lattices with nearest neighbor ferromagnetic exchange confined in a corner geometry, are studied by means of Monte Carlo simulations. Free boundary conditions at which boundary magnetic fields ± h are applied, i.e., at the two boundary rows ending at the lower left corner a field + h acts, while at the two boundary rows ending at the upper right corner a field − h acts. For temperatures T less than the critical temperature T c of the bulk, this boundary condition leads to the formation of two domains with opposite orientation of the magnetization direction, separated by an interface which for T larger than the filling transition temperature T f ( h ) …

PhysicsCondensed matter physicsTransition temperatureGeneral Physics and AstronomyBoundary (topology)GeometrySurfaces and InterfacesGeneral ChemistryCondensed Matter Physics01 natural sciences010305 fluids & plasmasSurfaces Coatings and FilmsMagnetic fieldMagnetizationFerromagnetism0103 physical sciencesIsing modelBoundary value problem010306 general physicsConfined spaceApplied Surface Science
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Quantum effects on the herringbone ordering ofN2on graphite

1993

The effects of quantum fluctuations on the ``2-in'' herringbone ordering in a realistic model of 900 ${\mathrm{N}}_{2}$ molecules adsorbed in the (\ensuremath{\surd}3 \ifmmode\times\else\texttimes\fi{} \ensuremath{\surd}3 )R30\ifmmode^\circ\else\textdegree\fi{} structure on graphite are studied via path-integral Monte Carlo (PIMC) simulations. Quasiclassical and quasiharmonic calculations agree for high and low temperatures, respectively, but only PIMC gives satisfactory results over the entire temperature range. We can quantify the lowering of the transition temperature and the depression of the ground state order to 10% as compared to classical modeling.

PhysicsCondensed matter physicsTransition temperatureMonte Carlo methodPath integral formulationGeneral Physics and AstronomyOrder (ring theory)Atmospheric temperature rangeGround stateQuantum statistical mechanicsQuantum fluctuationPhysical Review Letters
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Highly Correlated Fermi Liquid in Heavy-Fermion Metals: The Scaling Behavior

2014

In this chapter we show how the FCQPT theory works. We do that on the base of experimentally relevant examples. Namely, as noted in the Introduction (Chap. 1), the challenge for the theories is to explain the scaling behavior of the normalized effective mass \(M^*_N(y)\) displayed in Fig. 1.3. The theories analyzing only the critical exponents characterizing \(M^*_N(y)\) at \(y\gg 1\) consider only a part of the problem. In this section we analyze and derive the scaling behavior of the normalized effective mass near QCP as reported in Fig. 1.3. We start with describing magnetic field dependence of the quasiparticle effective mass in Sect. 6.1. Quasiparticle damping and the temperature depen…

PhysicsEffective mass (solid-state physics)Condensed matter physicsTransition temperatureQuasiparticleFermi liquid theoryScalingCritical exponentPhase diagramMagnetic field
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Numerical test of finite-size scaling predictions for the droplet condensation-evaporation transition

2016

We numerically study the finite-size droplet condensation-evaporation transition in two dimensions. We consider and compare two orthogonal approaches, namely at fixed temperature and at fixed density, making use of parallel multicanonical simulations. The equivalence between Ising model and lattice gas allows us to compare to analytical predictions. We recover the known background density (at fixed temperature) and transition temperature (at fixed density) in the thermodynamic limit and compare our finite-size deviations to the predicted leading-order finite-size corrections.

PhysicsHistoryStatistical Mechanics (cond-mat.stat-mech)010308 nuclear & particles physicsTransition temperatureFOS: Physical sciencesCondensed Matter - Soft Condensed Matter01 natural sciences010305 fluids & plasmasComputer Science ApplicationsEducationLattice (order)0103 physical sciencesThermodynamic limitSoft Condensed Matter (cond-mat.soft)Ising modelNumerical testsStatistical physicsScalingCondensed Matter - Statistical Mechanics
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