Propagation of first and second sound in a two-dimensional Fermi superfluid

Sound propagation is a macroscopic manifestation of the interplay between the equilibrium thermodynamics and the dynamical transport properties of fluids. Here, for a two-dimensional system of ultracold fermions, we calculate the first and second sound velocities across the whole BCS-BEC crossover,...

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Hauptverfasser: Tononi, Andrea (VerfasserIn) , Cappellaro, A. (VerfasserIn) , Bighin, Giacomo (VerfasserIn) , Salasnich, L. (VerfasserIn)
Dokumenttyp: Article (Journal)
Sprache:Englisch
Veröffentlicht: 14 June 2021
In: Physical review
Year: 2021, Jahrgang: 103, Heft: 6, Pages: 1-6
ISSN:2469-9934
DOI:10.1103/PhysRevA.103.L061303
Online-Zugang:Verlag, lizenzpflichtig, Volltext: https://doi.org/10.1103/PhysRevA.103.L061303
Verlag, lizenzpflichtig, Volltext: https://link.aps.org/doi/10.1103/PhysRevA.103.L061303
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Verfasserangaben:A. Tononi, A. Cappellaro, G. Bighin, and L. Salasnich
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Zusammenfassung:Sound propagation is a macroscopic manifestation of the interplay between the equilibrium thermodynamics and the dynamical transport properties of fluids. Here, for a two-dimensional system of ultracold fermions, we calculate the first and second sound velocities across the whole BCS-BEC crossover, and we analyze the system response to an external perturbation. In the low-temperature regime we reproduce the recent measurements [Phys. Rev. Lett. 124, 240403 (2020)] of the first sound velocity, which, due to the decoupling of density and entropy fluctuations, is the sole mode excited by a density probe. Conversely, a heat perturbation excites only the second sound, which, being sensitive to the superfluid depletion, vanishes in the deep BCS regime and jumps discontinuously to zero at the Berezinskii-Kosterlitz-Thouless superfluid transition. A mixing between the modes occurs only in the finite-temperature BEC regime, where our theory converges to the purely bosonic results.
Beschreibung:Gesehen am 13.08.2021
Beschreibung:Online Resource
ISSN:2469-9934
DOI:10.1103/PhysRevA.103.L061303