Search results for "Fermi gas"

showing 10 items of 86 documents

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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Free fermion antibunching in a degenerate atomic Fermi gas released from an optical lattice

2006

Noise in a quantum system is fundamentally governed by the statistics and the many-body state of the underlying particles. Whereas for bosonic particles the correlated noise observed for e.g. photons or bosonic neutral atoms can still be explained within a classical field description with fluctuating phases, the anticorrelations in the detection of fermionic particles have no classical analogue. The observation of such fermionic antibunching is so far scarce and has been confined to electrons and neutrons. Here we report on the first direct observation of antibunching of neutral fermionic atoms. Through an analysis of the atomic shot noise in a set of standard absorption images, of a gas of…

PhysicsCondensed Matter::Quantum GasesQuantum PhysicsOptical latticeMultidisciplinaryDegenerate energy levelsFOS: Physical sciencesQuantum phasesFermionCondensed Matter - Soft Condensed MatterFermionic condensateCondensed Matter - Other Condensed MatterQuantum mechanicsQuantum systemSoft Condensed Matter (cond-mat.soft)Fermi gasQuantum Physics (quant-ph)QuantumOther Condensed Matter (cond-mat.other)
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BCS-BEC Crossover in Atomic Fermi Gases with a Narrow Resonance

2006

We determine the effects on the BCS-BEC crossover of the energy dependence of the effective two-body interaction, which at low energies is determined by the effective range. To describe interactions with an effective range of either sign, we consider a single-channel model with a two-body interaction having an attractive square well and a repulsive square barrier. We investigate the two-body scattering properties of the model, and then solve the Eagles-Leggett equations for the zero temperature crossover, determining the momentum dependent gap and the chemical potential self-consistently. From this we investigate the dependence of the crossover on the effective range of the interaction.

PhysicsCondensed Matter::Quantum GasesRange (particle radiation)Strongly Correlated Electrons (cond-mat.str-el)Condensed matter physicsNuclear TheoryCondensed Matter - SuperconductivityCrossoverFOS: Physical sciencesBCS theoryTwo-body problemResonance (particle physics)Atomic and Molecular Physics and OpticsSuperconductivity (cond-mat.supr-con)Nuclear Theory (nucl-th)MomentumCondensed Matter - Strongly Correlated ElectronsScattering theoryFermi gas
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Coherence and clock shifts in ultracold fermi gases with resonant interactions.

2007

Using arguments based on sum rules, we derive a general result for the average shifts of rf lines in Fermi gases in terms of interatomic interaction strengths and two-particle correlation functions. We show that near an interaction resonance shifts vary inversely with the atomic scattering length, rather than linearly as in dilute gases, thus accounting for the experimental observation that clock shifts remain finite at Feshbach resonances.

PhysicsCondensed Matter::Quantum GasesStrongly Correlated Electrons (cond-mat.str-el)Condensed Matter - SuperconductivityGeneral Physics and AstronomyResonanceFOS: Physical sciencesScattering lengthSuperconductivity (cond-mat.supr-con)Condensed Matter - Strongly Correlated ElectronsAtomic physicsFermi gasFeshbach resonanceFermi Gamma-ray Space TelescopeCoherence (physics)Physical review letters
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Electron-phonon interaction in thin copper and gold films

2004

We have studied the electron-phonon (e-p) interaction in thin Cu and Au films at sub-Kelvin temperatures with the help of the hot electron effect, using symmetric normal metal-insulator-superconductor tunnel junction pairs as thermometers. By Joule heating the electron gas and measuring the electron and the lattice temperatures simultaneously, we show that the electron-phonon scattering rate follows a $T^{4}$ temperature dependence in both metals. The result is in accordance with the theory of e-p scattering in disordered films with vibrating boudaries and impurities, in contrast to the $T^{3}$-law expected for pure samples, and $T^{2}$-law for static disorder.

PhysicsCondensed matter physicsCondensed Matter - Mesoscale and Nanoscale PhysicsScatteringCondensed Matter - Superconductivitychemistry.chemical_elementFOS: Physical sciencesElectronCondensed Matter::Mesoscopic Systems and Quantum Hall Effect01 natural sciencesCopper010305 fluids & plasmasSuperconductivity (cond-mat.supr-con)chemistryImpurityTunnel junctionScattering rateCondensed Matter::Superconductivity0103 physical sciencesMesoscale and Nanoscale Physics (cond-mat.mes-hall)Condensed Matter::Strongly Correlated Electrons010306 general physicsFermi gasJoule heating
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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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Complete dipole response in [sup 208]Pb from high-resolution polarized proton scattering at 0°

2009

At the Research Center for Nuclear Physics, Osaka, Japan, the 208Pb(p,p´) reaction was measured at Ep=295 MeV and scattering angles Θlab= 0° - 10°. A high energy resolution of the order of ΔE/E ≈ 8x10^-5 was achieved, corresponding to ΔE=25-30 keV (FWHM). Cross sections were extracted by a multipole decomposition analysis of the angular distributions. Dominant contributions at very forward angles originate from E1 excitation due to Coulomb projectile-target interaction and spin M1 transitions caused by the spin-isospin part of the proton-nucleus interaction. A separation of these contributions was performed with two independent methods, viz. a multipole decomposition of the angular distribu…

PhysicsDipolePolarizabilityScatteringNeutronAtomic physicsFermi gasMultipole expansionSpin (physics)Resonance (particle physics)AIP Conference Proceedings
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Landau Fermi Liquid Theory and Beyond

2014

In this chapter we consider the Landau theory of the Fermi liquid that has a long history and remarkable results in describing a numerous properties of the electron liquid in ordinary metals and Fermi liquids of the \(^3\)He type. The theory is based on the assumption that elementary excitations determine the physics at low temperatures, resembling that of weakly interacting Fermi gas. These excitations behave as quasiparticles with a certain effective mass. The effective mass \(M^*\) exhibits a simple universal behavior, for it is independent of the temperature, pressure, and magnetic field strength and is a parameter of the theory. Microscopically deriving the equation determining the eff…

PhysicsEffective mass (solid-state physics)Condensed matter physicsElectron liquidQuantum oscillationsFermi liquid theoryLandau quantizationFermi gasShubnikov–de Haas effectLandau theory
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Spin-density waves in superdeformed quantum dots

1998

Abstract Electronic shell structure and spin effects in deformed quantum dots are investigated using spin-density functional theory. We recently suggested (Koskinen et al., Phys. Rev. Lett. 79 (1997) 1389) that for circular dots, depending on the density of the two-dimensional electron gas and the electron number, a spin-density wave-like state can occur as a possible ground state. Here these studies are extended to deformed and superdeformed dots, which approach the limit of a finite quantum wire.

PhysicsElectron densityCondensed matter physicsQuantum wireQuantum point contactCondensed Matter::Mesoscopic Systems and Quantum Hall EffectCondensed Matter PhysicsAtomic and Molecular Physics and OpticsElectronic Optical and Magnetic MaterialsQuantum dotPrincipal quantum numberGround stateFermi gasSpin-½Physica E: Low-dimensional Systems and Nanostructures
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Tuning the exciton luminescence in an acoustically depleted two-dimensional electron gas

2007

Standing-wave piezoelectric fields can be used to vary spatially and temporally charge conditions in $\mathrm{Ga}\mathrm{As}∕\mathrm{Al}\mathrm{Ga}\mathrm{As}$ quantum wells (QWs), offering a versatile tool to control the two-dimensional electron gas (2DEG) density in the well. A $\mathrm{Li}\mathrm{Nb}{\mathrm{O}}_{3}$ piezoelectric resonator imparts a MHz-frequency oscillating piezoelectric field with a controllable ratio of the in-plane and the vertical field components to a 2DEG placed in close proximity to the plate surface. This allows us to dynamically tune the charge state in the plane of the QW and to influence the photoluminescence spectra. It is found that spatially distributed r…

PhysicsElectron densityPhotoluminescenceCondensed Matter::OtherExcitonQuantum point contactElectronCondensed Matter::Mesoscopic Systems and Quantum Hall EffectCondensed Matter PhysicsElectronic Optical and Magnetic MaterialsCondensed Matter::Materials ScienceAtomic physicsTrionFermi gasQuantum wellPhysical Review B
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