Search results for "fluid"

showing 10 items of 5513 documents

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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Spin-S Kagome quantum antiferromagnets in a field with tensor networks

2016

Spin-$S$ Heisenberg quantum antiferromagnets on the Kagome lattice offer, when placed in a magnetic field, a fantastic playground to observe exotic phases of matter with (magnetic analogs of) superfluid, charge, bond or nematic orders, or a coexistence of several of the latter. In this context, we have obtained the (zero temperature) phase diagrams up to $S=2$ directly in the thermodynamic limit thanks to infinite Projected Entangled Pair States (iPEPS), a tensor network numerical tool. We find incompressible phases characterized by a magnetization plateau vs field and stabilized by spontaneous breaking of point group or lattice translation symmetry(ies). The nature of such phases may be se…

PhysicsCondensed matter physicsStrongly Correlated Electrons (cond-mat.str-el)Semiclassical physicsFOS: Physical sciences02 engineering and technology021001 nanoscience & nanotechnology01 natural sciences3. Good healthSuperfluidityMagnetizationCondensed Matter - Strongly Correlated ElectronsQuantum mechanics0103 physical sciencesThermodynamic limitCondensed Matter::Strongly Correlated ElectronsSymmetry breakingQuantum spin liquid[PHYS.COND.CM-SCE]Physics [physics]/Condensed Matter [cond-mat]/Strongly Correlated Electrons [cond-mat.str-el]010306 general physics0210 nano-technologyTranslational symmetryComputingMilieux_MISCELLANEOUSPhase diagram
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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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Contribution of the normal component to the thermal resistance of turbulent liquid helium

2015

Previous results for the velocity profile of the normal component of helium II in counterflow are used to evaluate the viscous contribution to the effective thermal resistance. It turns out that such a contribution becomes considerably higher than the usual Landau estimate, because in the presence of vortices, the velocity profile is appreciably different from the Poiseuille parabolic profile. Thus, a marked increase in the contribution of the normal component to the thermal resistance with respect to the viscous Landau estimate does not necessarily imply that the normal component is turbulent. Furthermore, we examine the influence of a possible slip flow along the walls when the radius of …

PhysicsCondensed matter physicsTurbulenceApplied MathematicsGeneral MathematicsThermal resistanceQuantum turbulenceGeneral Physics and AstronomyRadiusHagen–Poiseuille equationVortexPhysics::Fluid DynamicsThermal resistance – Superfluid helium – Quantum turbulence – Normal componentBoundary value problemSettore MAT/07 - Fisica MatematicaSuperfluid helium-4Zeitschrift für angewandte Mathematik und Physik
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Pumping of single electrons with a traveling wave

1995

Abstract We describe the operation and performance of a one-dimensional chain of small metallic islands whose potentials are modulated in a wave-like manner. The sinusoidal voltages, applied to the gate electrodes, carry individual charges coherently through the array. In practice, the wave-like potential is induced on the gates by a surface acoustic wave (SAW) traveling on a piezoelectric substrate. The resulting transfer of charges should produce a DC current I = ± ef through the chain, where f is the frequency of the wave and the sign ofthe current depends on the value of the common DC bias of the islands as well as on the direction of the wave propagation. We observe, however, a much sm…

PhysicsCondensed matter physicsbusiness.industrySurface acoustic waveElectronCondensed Matter PhysicsElectronic Optical and Magnetic MaterialsOpticsSurface waveSurface acoustic wave sensorWave vectorElectrical and Electronic EngineeringCurrent (fluid)businessDC biasVoltagePhysica B: Condensed Matter
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Vortex mutual friction in rotating superfluid 3He

1996

The Manchester rotating cryostat has been used to measure the longitudinal and transverse coefficients of vortex mutual friction in the A and B phases of superfluid 3He. In the B phase the dominant contribution to the mutual friction is scattering of excitations off occupied bound states in the vortex core. The A phase results are explained quantitatively by assuming that doubly quantised continuous vortices are created with a dynamics determined by the equation of motion of the orbital vector I; the measurements enable us to put an upper limit on the orbital inertia of less than 0.01h{stroke} per Cooper pair. History-dependent textural effects which had to be overcome in order to make mean…

PhysicsCondensed matter physicsmedia_common.quotation_subjectPhase (waves)General Physics and AstronomyEquations of motionInertiaRotationVortexSuperfluidityClassical mechanicsBound stateCooper pairmedia_common
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