Viscosity and scale invariance in the unitary Fermi gas

We compute the shear viscosity of the unitary Fermi gas above the superfluid transition temperature, using a diagrammatic technique that starts from the exact Kubo formula. The formalism obeys a Ward identity associated with scale invariance which guarantees that the bulk viscosity vanishes identica...

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Hauptverfasser: Enss, Tilman (VerfasserIn) , Haussmann, Rudolf (VerfasserIn) , Zwerger, Wilhelm (VerfasserIn)
Dokumenttyp: Article (Journal)
Sprache:Englisch
Veröffentlicht: 2011
In: Annals of physics
Year: 2011, Jahrgang: 326, Heft: 3, Pages: 770-796
DOI:10.1016/j.aop.2010.10.002
Online-Zugang:Verlag, Volltext: http://dx.doi.org/10.1016/j.aop.2010.10.002
Verlag, Volltext: http://www.sciencedirect.com/science/article/pii/S000349161000179X
Volltext
Verfasserangaben:Tilman Enss, Rudolf Haussmann, Wilhelm Zwerger

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520 |a We compute the shear viscosity of the unitary Fermi gas above the superfluid transition temperature, using a diagrammatic technique that starts from the exact Kubo formula. The formalism obeys a Ward identity associated with scale invariance which guarantees that the bulk viscosity vanishes identically. For the shear viscosity, vertex corrections and the associated Aslamazov-Larkin contributions are shown to be crucial to reproduce the full Boltzmann equation result in the high-temperature, low fugacity limit. The frequency dependent shear viscosity η(ω) exhibits a Drude-like transport peak and a power-law tail at large frequencies which is proportional to the Tan contact. The weight in the transport peak is given by the equilibrium pressure, in agreement with a sum rule due to Taylor and Randeria. Near the superfluid transition the peak width is of the order of 0.5TF, thus invalidating a quasiparticle description. The ratio η/s between the static shear viscosity and the entropy density exhibits a minimum near the superfluid transition temperature whose value is larger than the string theory bound ℏ/(4πkB) by a factor of about seven. 
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