Search results for "Statistical Mechanic"

showing 10 items of 707 documents

Structure of metastable 2D liquid helium

2007

We present diffusion Monte Carlo (DMC) results on a novel, superfluid phase in two-dimensional 4He at densities higher than 0.065 A-2, which is very close to the freezing density. The new phase has anisotropic, hexatic orbital order, but the single-particle density remains constant. By increasing density the hexatic superfluid forms a metastable state, which lies above the crystal ground state in energy. This implies that the liquid-solid phase transition takes place in two stages: a second-order phase transition from the isotropic superfluid to the hexatic superfluid, followed by a first-order transition that localizes atoms into the triangular crystal order.

Condensed Matter::Quantum GasesPhase transitionMaterials scienceCondensed matter physicsStatistical Mechanics (cond-mat.stat-mech)Liquid heliumCondensed Matter::OtherGeneral Physics and AstronomyFOS: Physical scienceslaw.inventionCondensed Matter - Other Condensed MatterSuperfluidityCrystalCondensed Matter::Soft Condensed MatterlawPhase (matter)MetastabilityDiffusion Monte CarloGround stateCondensed Matter - Statistical MechanicsOther Condensed Matter (cond-mat.other)
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Universal vortex formation in rotating traps with bosons and fermions.

2004

When a system consisting of many interacting particles is set rotating, it may form vortices. This is familiar to us from every-day life: you can observe vortices while stirring your coffee or watching a hurricane. In the world of quantum mechanics, famous examples of vortices are superconducting films and rotating bosonic $^4$He or fermionic $^3$He liquids. Vortices are also observed in rotating Bose-Einstein condensates in atomic traps and are predicted to exist for paired fermionic atoms. Here we show that the rotation of trapped particles with a repulsive interaction leads to a similar vortex formation, regardless of whether the particles are bosons or (unpaired) fermions. The exact, qu…

Condensed Matter::Quantum GasesPhysicsStatistical Mechanics (cond-mat.stat-mech)Condensed Matter - Mesoscale and Nanoscale PhysicsCondensed matter physicsFOS: Physical sciencesGeneral Physics and AstronomyTourbillonStatistical mechanicsFermionRotationVortexPhysics::Fluid DynamicsCondensed Matter::SuperconductivityMesoscale and Nanoscale Physics (cond-mat.mes-hall)Wave functionQuantumCondensed Matter - Statistical MechanicsBosonPhysical review letters
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Faraday patterns in low-dimensional Bose-Einstein condensates

2004

We show that Faraday patterns can be excited in the weak confinement space of low-dimensional Bose-Einstein condensates by temporal modulation of the trap width, or equivalently of the trap frequency Omega_tight, in the tight confinement space. For slow modulation, as compared with Omega_tight, the low-dimensional dynamics of the condensate in the weak confinement space is described by a Gross-Pitaevskii equation with time modulated nonlinearity coefficient. For increasing modulation frequencies a noticeable reduction of the pattern formation threshold is observed close to 2*Omega_tight, which is related to the parametric excitation of the internal breathing mode in the tight confinement sp…

Condensed Matter::Quantum GasesPhysicsStatistical Mechanics (cond-mat.stat-mech)Condensed matter physicsCondensed Matter::OtherFOS: Physical sciencesPattern formationCondensed Matter - Soft Condensed MatterSpace (mathematics)Wave equationOmegaAtomic and Molecular Physics and Opticslaw.inventionsymbols.namesakelawFaraday effectsymbolsSoft Condensed Matter (cond-mat.soft)Faraday cageCondensed Matter - Statistical MechanicsBose–Einstein condensateExcitationPhysical Review A
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Comment on “Accurate ground-state phase diagram of the one-dimensional extended Hubbard model at half filling”

2004

In PRB 68, 153101 (2003), Guoping Zhang presented density-matrix renormalization group (DMRG) results which contradict my DMRG calculations and Hirsch's quantum Monte Carlo (QMC) simulations for the charge-density-wave (CDW) phase boundary in the one-dimensional extended Hubbard model at half filling. In this Comment I show that Zhang's results are inaccurate and that his criticism of my work is groundless.

Condensed Matter::Quantum GasesPhysicsWork (thermodynamics)Strongly Correlated Electrons (cond-mat.str-el)Hubbard modelZhàngFOS: Physical sciencesBoundary (topology)Condensed Matter PhysicsElectronic Optical and Magnetic MaterialsCondensed Matter - Strongly Correlated ElectronsTheoretical physicsQuantum electrodynamicsCondensed Matter::Statistical MechanicsCondensed Matter::Strongly Correlated ElectronsGround statePhase diagramPhysical Review B
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Quantum Phases in a Resonantly Interacting Boson-Fermion Mixture

2005

We consider a resonantly-interacting Bose-Fermi mixture of $^{40}$K and $^{87}$Rb atoms in an optical lattice. We show that by using a red-detuned optical lattice the mixture can be accurately described by a generalized Hubbard model for $^{40}$K and $^{87}$Rb atoms, and $^{40}$K-$^{87}$Rb molecules. The microscopic parameters of this model are fully determined by the details of the optical lattice and the interspecies Feshbach resonance in the absence of the lattice. We predict a quantum phase transition to occur in this system already at low atomic filling fraction, and present the phase diagram as a function of the temperature and the applied magnetic field.

Condensed Matter::Quantum GasesQuantum phase transitionPhysicsOptical latticeStatistical Mechanics (cond-mat.stat-mech)Hubbard modelFOS: Physical sciencesGeneral Physics and AstronomyQuantum phasesFermionAtomic physicsFeshbach resonanceCondensed Matter - Statistical MechanicsBosonPhase diagramPhysical Review Letters
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Crossover scaling in two dimensions

1997

We determine the scaling functions describing the crossover from Ising-like critical behavior to classical critical behavior in two-dimensional systems with a variable interaction range. Since this crossover spans several decades in the reduced temperature as well as in the finite-size crossover variable, it has up to now largely evaded a satisfactory numerical determination. Using a new Monte Carlo method, we could obtain accurate results for sufficiently large interactions ranges. Our data cover the full crossover region both above and below the critical temperature and support the hypothesis that the crossover functions are universal. Also the so-called effective exponents are discussed …

Condensed Matter::Quantum GasesStatistical Mechanics (cond-mat.stat-mech)Monte Carlo methodCrossoverFOS: Physical sciencesCondensed Matter - Soft Condensed MatterReduced propertiesCover (topology)Soft Condensed Matter (cond-mat.soft)Statistical physicsCritical exponentScalingCondensed Matter - Statistical MechanicsInteraction rangeVariable (mathematics)Mathematics
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Small-Angle Excess Scattering: Glassy Freezing or Local Orientational Ordering?

1996

We present Monte Carlo simulations of a dense polymer melt which shows glass-transition-like slowing-down upon cooling, as well as a build up of nematic order. At small wave vectors q this model system shows excess scattering similar to that recently reported for light-scattering experiments on some polymeric and molecular glass-forming liquids. For our model system we can provide clear evidence that this excess scattering is due to the onset of short-range nematic order and not directly related to the glass transition.

Condensed Matter::Soft Condensed MatterMaterials scienceStatistical Mechanics (cond-mat.stat-mech)Condensed matter physicsScatteringLiquid crystalMonte Carlo methodFOS: Physical sciencesGeneral Physics and AstronomyModel systemGlass transitionCondensed Matter - Statistical MechanicsPolymer meltPhysical Review Letters
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Glass transitions and scaling laws within an alternative mode-coupling theory

2015

Idealized glass transitions are discussed within an alternative mode-coupling theory (TMCT) proposed by Tokuyama [Physica A 395, 31 (2014)]. This is done in order to identify common ground with and differences from the conventional mode-coupling theory (MCT). It is proven that both theories imply the same scaling laws for the transition dynamics, which are characterized by two power-law decay functions and two diverging power-law time scales. However, the values for the corresponding anomalous exponents calculated within both theories differ from each other. It is proven that the TMCT, contrary to the MCT, does not describe transitions with continuously vanishing arrested parts of the corre…

Condensed Matter::Soft Condensed MatterScaling lawTheoretical physicsStatistical Mechanics (cond-mat.stat-mech)Mode couplingFOS: Physical sciencesOrder (group theory)Gravitational singularityDisordered Systems and Neural Networks (cond-mat.dis-nn)Schematic modelCondensed Matter - Disordered Systems and Neural NetworksCondensed Matter - Statistical MechanicsMathematics
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Testing Mode-Coupling Theory for a Supercooled Binary Lennard-Jones Mixture I: The van Hove Correlation Function

1995

We report the results of a large scale computer simulation of a binary supercooled Lennard-Jones liquid. We find that at low temperatures the curves for the mean squared displacement of a tagged particle for different temperatures fall onto a master curve when they are plotted versus rescaled time $tD(T)$, where $D(T)$ is the diffusion constant. The time range for which these curves follow the master curve is identified with the $\alpha$-relaxation regime of mode-coupling theory (MCT). This master curve is fitted well by a functional form suggested by MCT. In accordance with idealized MCT, $D(T)$ shows a power-law behavior at low temperatures. The critical temperature of this power-law is t…

Condensed matter physicsCondensed Matter (cond-mat)FOS: Physical sciencesThermodynamicsCondensed MatterPower lawFick's laws of diffusionMean squared displacementCondensed Matter::Soft Condensed MatterCorrelation function (statistical mechanics)AmplitudeMode couplingRelaxation (physics)Critical exponentMathematics
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Glass transition of hard spheres in high dimensions

2009

We have investigated analytically and numerically the liquid-glass transition of hard spheres for dimensions $d\to \infty $ in the framework of mode-coupling theory. The numerical results for the critical collective and self nonergodicity parameters $f_{c}(k;d) $ and $f_{c}^{(s)}(k;d) $ exhibit non-Gaussian $k$ -dependence even up to $d=800$. $f_{c}^{(s)}(k;d) $ and $f_{c}(k;d) $ differ for $k\sim d^{1/2}$, but become identical on a scale $k\sim d$, which is proven analytically. The critical packing fraction $\phi_{c}(d) \sim d^{2}2^{-d}$ is above the corresponding Kauzmann packing fraction $\phi_{K}(d)$ derived by a small cage expansion. Its quadratic pre-exponential factor is different fr…

Condensed matter physicsStatistical Mechanics (cond-mat.stat-mech)FOS: Physical sciencesGeometryScale (descriptive set theory)Hard spheresCondensed Matter - Soft Condensed MatterAtomic packing factorQuadratic equationExponentSoft Condensed Matter (cond-mat.soft)Glass transitionCritical exponentCondensed Matter - Statistical MechanicsMathematics
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