Search results for "CRITICAL PHENOMENA"

showing 10 items of 91 documents

Physical mechanisms of micro- and nanodomain formation in multicomponent lipid membranes.

2016

This article summarizes a variety of physical mechanisms proposed in the literature, which can generate micro- and nanodomains in multicomponent lipid bilayers and biomembranes. It mainly focusses on lipid-driven mechanisms that do not involve direct protein-protein interactions. Specifically, it considers (i) equilibrium mechanisms based on lipid-lipid phase separation such as critical cluster formation close to critical points, and multiple domain formation in curved geometries, (ii) equilibrium mechanisms that stabilize two-dimensional microemulsions, such as the effect of linactants and the effect of curvature-composition coupling in bilayers and monolayers, and (iii) non-equilibrium me…

0301 basic medicinePhase transitionCytoplasmCritical phenomenaLipid BilayersBiophysicsFOS: Physical sciencesCondensed Matter - Soft Condensed MatterMolecular Dynamics SimulationBiochemistryPhase TransitionQuantitative Biology::Subcellular Processes03 medical and health sciencesSurface-Active AgentsMembrane MicrodomainsMonolayerCluster (physics)AnimalsHumansMicroemulsionPhysics - Biological PhysicsLipid bilayerPhysics::Biological PhysicsBacteriaChemistryBiological membraneCell BiologyCrystallographyActin CytoskeletonKinetics030104 developmental biologyMembraneBiological Physics (physics.bio-ph)Chemical physicsSoft Condensed Matter (cond-mat.soft)ThermodynamicsEmulsionsSignal TransductionBiochimica et biophysica acta. Biomembranes
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Critical behavior of a colloid-polymer mixture confined between walls

2006

We investigate the influence of confinement on phase separation in colloid-polymer mixtures. To describe the particle interactions, the colloid-polymer model of Asakura and Oosawa [J. Chem. Phys. 22, 1255 (1954)] is used. Grand canonical Monte Carlo simulations are then applied to this model confined between two parallel hard walls, separated by a distance D=5 colloid diameters. We focus on the critical regime of the phase separation and look for signs of crossover from three-dimensional (3D) Ising to two-dimensional (2D) Ising universality. To extract the critical behavior, finite size scaling techniques are used, including the recently proposed algorithm of Kim et al. [Phys. Rev. Lett. 91…

BinodalCondensed matter physicsCritical phenomenaFOS: Physical sciencesCondensed Matter - Soft Condensed MatterAtomic packing factorUniversality (dynamical systems)Condensed Matter::Soft Condensed MatterCritical point (thermodynamics)Soft Condensed Matter (cond-mat.soft)Ising modelStatistical physicsCritical exponentScalingMathematicsPhysical Review E
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Concentration and energy fluctuations in a critical polymer mixture

1995

A semi-grand-canonical Monte Carlo algorithm is employed in conjunction with the bond fluctuation model to investigate the critical properties of an asymmetric binary (AB) polymer mixture. By applying the equal peak-weight criterion to the concentration distribution, the coexistence curve separating the A-rich and B-rich phases is identified as a function of temperature and chemical potential. To locate the critical point of the model, the cumulant intersection method is used. The accuracy of this approach for determining the critical parameters of fluids is assessed. Attention is then focused on the joint distribution function of the critical concentration and energy, which is analysed usi…

BinodalCritical point (thermodynamics)Critical phenomenaCondensed Matter (cond-mat)FOS: Physical sciencesIsing modelCondensed MatterStatistical physicsRenormalization groupCritical dimensionCritical exponentMonte Carlo algorithmMathematics
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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
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Electrostatic interactions in critical solvents

2011

The subtle interplay between critical phenomena and electrostatics is investigated by considering the effective force acting on two parallel walls confining a near-critical binary liquid mixture with added salt. The ion-solvent coupling can turn a non-critical repulsive electrostatic force into an attractive one upon approaching the critical point. However, the effective force is eventually dominated by the critical Casimir effect, the universal properties of which are not altered by the presence of salt. This observation allows a consistent interpretation of recent experimental data.

Casimir effectMaterials scienceCritical point (thermodynamics)Chemical physicsEffective forceCritical phenomenaGeneral Physics and AstronomySoft Condensed Matter (cond-mat.soft)FOS: Physical sciencesCondensed Matter - Soft Condensed MatterElectrostatics
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Scaling behavior of an airplane-boarding model

2013

An airplane-boarding model, introduced earlier by Frette and Hemmer [Phys. Rev. E 85, 011130 (2012)], is studied with the aim of determining precisely its asymptotic power-law scaling behavior for a large number of passengers $N$. Based on Monte Carlo simulation data for very large system sizes up to $N={2}^{16}=65\phantom{\rule{0.16em}{0ex}}536$, we have analyzed numerically the scaling behavior of the mean boarding time $\ensuremath{\langle}{t}_{b}\ensuremath{\rangle}$ and other related quantities. In analogy with critical phenomena, we have used appropriate scaling Ans\"atze, which include the leading term as some power of $N$ (e.g., $\ensuremath{\propto}$${N}^{\ensuremath{\alpha}}$ for …

CombinatoricsPhysicsCritical phenomenaExponentSecond moment of areaTime stepScalingPhysical Review E
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Exact and Variational Treatment of Ferroelectric Thin Films with Different Materials of Electrodes

2005

We trace the influence of metallic electrodes on the properties of thin ferroelectric films. This has been done in the framework of the phenomenological Landau theory. We present both exact analytical solution of the problem in terms of Weierstrass elliptic functions and the variational solution. We calculate polarization, dielectric susceptibility, pyroelectric coefficient and depolarization field. We have shown that the ferroelectric phase of the film can be destroyed by the choice of material of electrodes with screening length exceeding some critical value. This demonstrates that we can control the physical properties of thin ferroelectric films by the proper choice of the electrode mat…

Condensed Matter::Materials ScienceVariational methodMaterials scienceCondensed matter physicsCritical phenomenaPhenomenological modelDielectricThin filmCondensed Matter PhysicsFerroelectricityLandau theoryElectronic Optical and Magnetic MaterialsPyroelectricityFerroelectrics
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Three-step decay of time correlations at polymer-solid interfaces

2012

Two-step decay of relaxation functions, i.e., time scale separation between microscopic dynamics and structural relaxation, is the defining signature of the structural glass transition. We show that for glass-forming polymer melts at an attractive surface slow desorption kinetics introduces an additional time scale separation among the relaxational degrees of freedom leading to a three-step decay. The inherent length scale of this process is the radius of gyration in contrast to the segmental scale governing the glass transition. We show how the three-step decay can be observed in incoherent scattering experiments and discuss its relevance for the glass transition of confined polymers by an…

Condensed Matter::Soft Condensed MatterLength scaleMaterials scienceCondensed matter physicsScale (ratio)Critical phenomenaDegrees of freedom (physics and chemistry)Radius of gyrationIncoherent scatterGeneral Physics and AstronomyRelaxation (physics)Glass transitionEPL (Europhysics Letters)
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Dynamic Anomalies and their Relation to the Glass Transition: A Neutron Scattering Study of the Glass Forming Van der Waals Liquid Ortho-terphenyl

1991

Neutron scattering experiments on the molecular glass former ortho-terphenyl reveal a dynamic anomaly at a temperature Tc ≈ 290 K well above the calorimetric glass temperature Tg = 243 K. Close above Tc the density autocorrelation function ΦQ(t) shows a two step decay over 4–5 decades in time. The slower component obeys the time-temperature superposition principle. Its line shape can be well parametrized by a Kohlrausch law and is strongly temperature dependent as its relaxation time scales with the shear viscosity. Thus this component is identified with the structural relaxation (α-process). The faster component (β-process) is much less temperature dependent. Its line shape factorizes in a…

Condensed matter physicsChemistryGeneral Chemical EngineeringCritical phenomenaRelaxation (NMR)ThermodynamicsNeutron scatteringPlateau (mathematics)Power lawsymbols.namesakesymbolsvan der Waals forceGlass transitionCritical exponentBerichte der Bunsengesellschaft für physikalische Chemie
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Critical phenomena in colloid-polymer mixtures: interfacial tension, order parameter, susceptibility, and coexistence diameter.

2004

The critical behavior of a model colloid-polymer mixture, the so-called AO model, is studied using computer simulations and finite size scaling techniques. Investigated are the interfacial tension, the order parameter, the susceptibility and the coexistence diameter. Our results clearly show that the interfacial tension vanishes at the critical point with exponent 2\nu ~ 1.26. This is in good agreement with the 3D Ising exponent. Also calculated are critical amplitude ratios, which are shown to be compatible with the corresponding 3D Ising values. We additionally identify a number of subtleties that are encountered when finite size scaling is applied to the AO model. In particular, we find …

Condensed matter physicsCritical phenomenaExtrapolationThermodynamicsFOS: Physical sciencesCondensed Matter - Soft Condensed MatterCondensed Matter::Soft Condensed MatterSurface tensionAmplitudeCritical point (thermodynamics)ExponentSoft Condensed Matter (cond-mat.soft)Ising modelScalingMathematicsPhysical review. E, Statistical, nonlinear, and soft matter physics
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