Search results for "superfluid"

showing 10 items of 171 documents

Bloch oscillations in Fermi gases

2003

The possibility of Bloch oscillations for a degenerate and superfluid Fermi gas of atoms in an optical lattice is considered. For a one-component degenerate gas the oscillations are suppressed for high temperatures and band fillings. For a two-component gas the Landau criterion is used for specifying the regime where Bloch oscillations of the superfluid may be observed. We show how the amplitude of Bloch oscillations varies along the BCS-BEC crossover.

PhysicsCondensed Matter::Quantum GasesOptical latticeCondensed matter physicsCondensed Matter - Mesoscale and Nanoscale PhysicsCondensed Matter::OtherDegenerate energy levelsQuantum oscillationsFOS: Physical sciencesAtomic and Molecular Physics and Opticslaw.inventionSuperfluiditylawQuantum electrodynamicsMesoscale and Nanoscale Physics (cond-mat.mes-hall)Bloch oscillationsFermi gasBose–Einstein condensateBloch wave
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Sound velocity and dimensional crossover in a superfluid Fermi gas in an optical lattice

2005

We study the sound velocity in cubic and non-cubic three-dimensional optical lattices. We show how the van Hove singularity of the free Fermi gas is smoothened by interactions and eventually vanishes when interactions are strong enough. For non-cubic lattices, we show that the speed of sound (Bogoliubov-Anderson phonon) shows clear signatures of dimensional crossover both in the 1D and 2D limits.

PhysicsCondensed Matter::Quantum GasesOptical latticeCondensed matter physicsPhononCondensed Matter - SuperconductivityCrossoverVan Hove singularityFOS: Physical sciences01 natural sciencesAtomic and Molecular Physics and Optics010305 fluids & plasmasSuperconductivity (cond-mat.supr-con)SuperfluiditySingularitySpeed of soundQuantum mechanicsCondensed Matter::Superconductivity0103 physical sciencesCondensed Matter::Strongly Correlated Electrons010306 general physicsFermi gas
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Formation of spatial shell structures in the superfluid to Mott insulator transition

2006

International audience; We report on the direct observation of the transition from a compressible superfluid to an incompressible Mott insulator by recording the in-trap density distribution of a Bosonic quantum gas in an optical lattice. Using spatially selective microwave transitions and spin changing collisions, we are able to locally modify the spin state of the trapped quantum gas and record the spatial distribution of lattice sites with different filling factors. As the system evolves from a superfluid to a Mott insulator, we observe the formation of a distinct shell structure, in good agreement with theory.

PhysicsCondensed Matter::Quantum GasesOptical latticeSpin statesCondensed matter physicsMott insulatorFOS: Physical sciencesGeneral Physics and Astronomy01 natural sciences010305 fluids & plasmasMott transitionCondensed Matter - Other Condensed MatterSuperfluidityLattice (order)[PHYS.COND.CM-GEN]Physics [physics]/Condensed Matter [cond-mat]/Other [cond-mat.other]0103 physical sciencesCondensed Matter::Strongly Correlated ElectronsMetal–insulator transition010306 general physicsJaynes–Cummings–Hubbard modelOther Condensed Matter (cond-mat.other)
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Co-existence and shell structures of several superfluids in trapped three-component Fermi mixtures

2006

We study the properties of a trapped interacting three component Fermi gas. We assume that one of the components can have a different mass from the other two. We calculate the different phases of the three component mixture and find a rich variety of different phases corresponding to different pairing channels, and simple ways of tuning the system from one phase to another. In particular, we predict co-existence of several different superfluids in the trap, forming a shell structure, and phase transitions from this mixture of superfluids to a single superfluid when the system parameters or temperature is varied. Such shell structures realize superfluids with a non-trivial spatial topology a…

PhysicsCondensed Matter::Quantum GasesPhase transitionCondensed matter physicsComponent (thermodynamics)Condensed Matter - SuperconductivityShell (structure)FOS: Physical sciencesObservable01 natural sciencesMolecular physicsAtomic and Molecular Physics and Optics3. Good health010305 fluids & plasmasSuperfluiditySuperconductivity (cond-mat.supr-con)PairingPhase (matter)0103 physical sciences010306 general physicsFermi gas
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Quasiparticles, coherence and nonlinearity: exact simulations of RF-spectroscopy of strongly interacting one-dimensional Fermi gases

2008

We consider RF-spectroscopy of ultracold Fermi gases by exact simulations of the many-body state and the coherent dynamics in one dimension. Deviations from the linear response sum rule result are found to suppress the pairing contribution to the RF line shifts. We compare the coherent rotation and quasiparticle descriptions of RF-spectroscopy which are analogous to NMR experiments in superfluid $^3$He and tunneling in solids, respectively. We suggest that RF-spectroscopy in ultracold gases provides an interesting crossover between these descriptions that could be used for studying decoherence in quantum measurement, in the context of many-body quantum states.

PhysicsCondensed Matter::Quantum GasesQuantum decoherenceCondensed matter physicsCondensed Matter - SuperconductivityFOS: Physical sciencesAtomic and Molecular Physics and OpticsSuperfluiditySuperconductivity (cond-mat.supr-con)Condensed Matter - Other Condensed MatterQuantum statePairingQuantum mechanicsQuasiparticleSum rule in quantum mechanicsSpectroscopyCoherence (physics)Other Condensed Matter (cond-mat.other)
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The growth of atomically rough 4He crystals

1986

We have studied the growth of atomically rough bcc and hcp4He crystals from the superfluid phase for temperaturesT>0.9 K. The growth coefficient displays a temperature dependence which can be represented bym 4 K∝ $$e^{\Delta E/k_B T} $$ . The parameter ΔE is found to be in close agreement with the energy gap of rotons, suggesting that these thermal excitations dominate the growth kinetics. Besides, the absolute value of the growth coefficient depends on crystal orientation, with an anisotropy for the hcp phase of about a factor of 2.5 between the $$\left\{ {10\bar 10} \right\}$$ and {0001} planes.

PhysicsCondensed matter physicsBand gapCondensed Matter::OtherThermodynamicsAbsolute valueCrystal growthCondensed Matter PhysicsElectronic Optical and Magnetic MaterialsSuperfluidityHelium-4Phase (matter)General Materials Scienceddc:530AnisotropyBar (unit)
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Nonlocal effects in superfluid turbulence: Application to the low-density- to high-density-state transition and to vortex decay

2005

We discuss a phenomenological equation for the evolution of vortex tangle in counterflow superfluid turbulence, which takes into account the influence of the nonlocal effects, introducing into the original equation of Vinen two simple corrective terms dependent on a nonvanishing ratio between the average separation between vortex lines and the diameter of the channel. The equation allows one to describe, in relatively good agreement with experimental results, the two turbulent regimes present in counterflow superfluid turbulence and the transition between them. The decay rate of the vortex line density L, when the heat flux is suddenly turned off, is also investigated; due to the simplicity…

PhysicsCondensed matter physicsCondensed Matter::OtherTurbulenceQuantum vortexCondensed Matter PhysicsElectronic Optical and Magnetic MaterialsVortexSuperfluidityHelium-4Heat fluxQuantum electrodynamicsPhenomenological modelIsotopes of heliumPhysical Review B
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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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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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