Viscosity of strongly interacting quantum fluids: spectral functions and sum rules

The viscosity of strongly interacting systems is a topic of great interest in diverse fields. We focus here on the bulk and shear viscosities of \emph{non-relativistic} quantum fluids, with particular emphasis on strongly interacting ultracold Fermi gases. We use Kubo formulas for the bulk and shear viscosity spectral functions, $ζ(ω)$ and $η(ω)$ respectively, to derive exact, non-perturbative results. Our results include: a microscopic connection between the shear viscosity $η$ and the normal fluid density $ρ_n$; sum rules for $ζ(ω)$ and $η(ω)$ and their evolution through the BCS-BEC crossover; universal high-frequency tails for $η(ω)$ and the dynamic structure factor $S({\bf q}, ω)$. We use our sum rules to show that, at unitarity, $ζ(ω)$ is identically zero and thus relate $η(ω)$ to density-density correlations. We predict that frequency-dependent shear viscosity $η(ω)$ of the unitary Fermi gas can be experimentally measured using Bragg spectroscopy.

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