Search results for "Fluids"

showing 10 items of 1936 documents

Properties of the interface in the confined Ising magnet with competing surface fields

2007

Abstract A two-dimensional magnetic Ising system confined in an L × D geometry ( L ⪡ D ) in the presence of competing magnetic fields (h) acting at opposite walls along the D -direction, exhibits an interface between domains of different orientation that run parallel to the walls. In the limit L → ∞ , this interface undergoes a wetting transition that occurs at the critical curve T w ( h ) , so that for T T w ( h ) such an interface is bound to the walls, while for T w ( h ) ⩽ T T cb the interface is freely fluctuating around the center of the film, where T cb is the bulk critical temperature. By considering both short- and long-range magnetic fields acting at the walls, we study the diverg…

PhysicsCondensed matter physicsIsing systemCondensed Matter Physics01 natural sciences010305 fluids & plasmasElectronic Optical and Magnetic MaterialsMagnetic fieldFerromagnetismWetting transitionCritical point (thermodynamics)Magnet0103 physical sciencesIsing modelWettingElectrical and Electronic Engineering010306 general physicsPhysica B: Condensed Matter
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Interference pattern and visibility of a Mott insulator

2005

We analyze theoretically the experiment reported in [F. Gerbier et al, cond-mat/0503452], where the interference pattern produced by an expanding atomic cloud in the Mott insulator regime was observed. This interference pattern, indicative of short-range coherence in the system, could be traced back to the presence of a small amount of particle/hole pairs in the insulating phase for finite lattice depths. In this paper, we analyze the influence of these pairs on the interference pattern using a random phase approximation, and derive the corresponding visibility. We also account for the inhomogeneity inherent to atom traps in a local density approximation. The calculations reproduce the expe…

PhysicsCondensed matter physicsMott insulatorFOS: Physical sciencesInterference (wave propagation)01 natural sciencesAtomic and Molecular Physics and Optics010305 fluids & plasmasCondensed Matter - Other Condensed MatterRadiation pressureLattice (order)[PHYS.COND.CM-GEN]Physics [physics]/Condensed Matter [cond-mat]/Other [cond-mat.other]0103 physical sciencesAtomLocal-density approximation010306 general physicsRandom phase approximationOther Condensed Matter (cond-mat.other)Coherence (physics)
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Effective temperature and scaling laws of polarized quantum vortex bundles

2011

Abstract An effective non-equilibrium temperature is defined for (locally) polarized and dense turbulent superfluid vortex bundles, related to the average energy of the excitations (Kelvin waves) of vortex lines. In the quadratic approximation of the excitation energy in terms of the wave amplitude A, a previously known scaling relation between amplitude and wavelength k of Kelvin waves in polarized bundles, namely A ∝ k − 1 / 2 , follows from the homogeneity of the effective temperature. This result is analogous to that of the well-known equipartition result in equilibrium systems.

PhysicsCondensed matter physicsNon-equilibrium temperature Turbulent superfluids Vortices Scaling laws Non-equilibrium thermodynamicsQuantum vortexGeneral Physics and AstronomyNon-equilibrium thermodynamicsVortexsymbols.namesakeWavelengthAmplitudesymbolsKelvin waveScalingSettore MAT/07 - Fisica MatematicaEquipartition theorem
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Refrigeration of an Array of Cylindrical Nanosystems by Flowing Superfluid Helium

2016

We consider the refrigeration of an array of heat-dissipating cylindrical nanosystems as a simplified model of computer refrigeration. We explore the use of He II as cooling fluid, taking into account forced convection and heat conduction. The main conceptual and practical difficulties arise in the calculation of the effective thermal conductivity. Since He II does not follow Fourier’s law, the effective geometry-dependent conductivity must be extracted from a more general equation for heat transfer. Furthermore, we impose the restrictions that the maximum temperature along the array should be less than (Formula presented.) transition temperature and that quantum turbulence is avoided, in o…

PhysicsCondensed matter physicsQuantum turbulenceRefrigerationConductivityCondensed Matter PhysicsThermal conduction01 natural sciencesNanorefrigerationAtomic and Molecular Physics and Optics010305 fluids & plasmasForced convectionThermal conductivityThermal conductivity0103 physical sciencesHeat transferGeneral Materials ScienceSuperfluid helium010306 general physicsSettore MAT/07 - Fisica MatematicaSuperfluid helium-4Journal of Low Temperature Physics
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Pairing based cooling of Fermi gases

2007

We propose a pairing-based method for cooling an atomic Fermi gas. A three component (labels 1, 2, 3) mixture of Fermions is considered where the components 1 and 2 interact and, for instance, form pairs whereas the component 3 is in the normal state. For cooling, the components 2 and 3 are coupled by an electromagnetic field. Since the quasiparticle distributions in the paired and in the normal states are different, the coupling leads to cooling of the normal state even when initially $T_{paired}\geq T_{normal}$ (notation $T_S\geq T_N$). The cooling efficiency is given by the pairing energy and by the linewidth of the coupling field. No superfluidity is required: any type of pairing, or ot…

PhysicsCondensed matter physicsResolved sideband coolingCondensed Matter - SuperconductivityFOS: Physical sciencesCoupling (probability)7. Clean energy01 natural sciencesAtomic and Molecular Physics and Optics010305 fluids & plasmasSuperconductivity (cond-mat.supr-con)Condensed Matter - Other Condensed MatterLaser coolingPairing0103 physical sciencesQuasiparticleAtomic physicsConnection (algebraic framework)010306 general physicsFermi gasEnergy (signal processing)Other Condensed Matter (cond-mat.other)
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Microscopic theory for the glass transition in a system without static correlations

2002

We study the orientational dynamics of infinitely thin hard rods of length L, with the centers-of-mass fixed on a simple cubic lattice with lattice constant a.We approximate the influence of the surrounding rods onto dynamics of a pair of rods by introducing an effective rotational diffusion constant D(l),l=L/a. We get D(l) ~ [1-v(l)], where v(l) is given through an integral of a time-dependent torque-torque correlator of an isolated pair of rods. A glass transition occurs at l_c, if v(l_c)=1. We present a variational and a numerically exact evaluation of v(l).Close to l_c the diffusion constant decreases as D(l) ~ (l_c-l)^\gamma, with \gamma=1. Our approach predicts a glass transition in t…

PhysicsCondensed matter physicsStatistical Mechanics (cond-mat.stat-mech)General Physics and AstronomyRotational diffusionFOS: Physical sciencesCondensed Matter - Soft Condensed Matter01 natural sciencesFick's laws of diffusionRod010305 fluids & plasmasCondensed Matter::Soft Condensed MatterLattice constant0103 physical sciencesMode couplingSoft Condensed Matter (cond-mat.soft)Microscopic theory010306 general physicsGlass transitionConstant (mathematics)Condensed Matter - Statistical Mechanics
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Stochastic Models of Higher Order Dielectric Responses

2018

The nonlinear response for systems exhibiting Markovian stochastic dynamics is calculated using time-dependent perturbation theory for the Green’s function, the conditional probability to find the system in a given configuration at a certain time given it was in another configuration at an earlier time. In general, the Green’s function obeys a so-called master-equation for the balance of the gain and loss of probability in the various configurations of the system. Using various models for the reorientational motion of molecules it is found that the scaled modulus of the third-order response, \(X_3\), shows a hump-like behavior for random rotational motion in some cases and it exhibits “triv…

PhysicsCondensed matter physicsStochastic modellingIsotropyConditional probabilityRotational diffusion01 natural sciences010305 fluids & plasmasDipoleNonlinear system0103 physical sciencesRelaxation (physics)Perturbation theory010306 general physics
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Universal behavior of two-dimensional 3He at low temperatures.

2008

On the example of two-dimensional (2D) 3He we demonstrate that the main universal features of its experimental temperature T - density x phase diagram [see M. Neumann, J. Ny\'{e}ki, J. Saunders, Science 317, 1356 (2007)] look like those in the heavy-fermion metals. Our comprehensive theoretical analysis of experimental situation in 2D 3He allows us to propose a simple expression for effective mass M^*(T,x), describing all diverse experimental facts in 2D 3He in unified manner and demonstrating that the universal behavior of M^*(T,x) coincides with that observed in HF metals.

PhysicsCondensed matter physicsStrongly Correlated Electrons (cond-mat.str-el)General Physics and AstronomyFOS: Physical sciences01 natural sciences010305 fluids & plasmasCondensed Matter - Strongly Correlated ElectronsEffective mass (solid-state physics)0103 physical sciencesStrongly correlated material010306 general physicsPhase diagramMathematical physicsPhysical review letters
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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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Low-frequency internal waves in magnetized rotating stellar radiation zones

2012

Context. With the progress of observational constraints on dynamical processes in stars, it becomes necessary to understand the angular momentum and the rotation profile history. In this context, internal waves constitute an efficient transport mechanism over long distances in stellar radiation zones. Indeed, they could be one of the mechanisms responsible for the quasi-flat rotation profile of the solar radiative region up to 0.2 R ⊙ .Aims. Angular momentum transport induced by internal waves depends on the properties of their excitation regions and of their dissipation during propagation. Then, the bottom of convective envelopes (the top of convective cores, respectively) are differential…

PhysicsConvectionAngular momentumAstronomy and AstrophysicsAstrophysicsInternal wave01 natural sciences010305 fluids & plasmasMagnetic fieldsymbols.namesakeClassical mechanicsSpace and Planetary ScienceQuantum electrodynamics0103 physical sciencesAngular momentum of lightsymbolsRadiative transferDifferential rotation010303 astronomy & astrophysicsLorentz forceAstronomy & Astrophysics
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