The thermodynamic and transport properties of the unitary Fermi gas at finite temperature T are governed by a quantum critical point at $T=0$ and zero density. We compute the universal shear viscosity to entropy ratio η/s in the high-temperature quantum critical regime T|μ| and find that this strongly coupled quantum fluid comes close to perfect fluidity η/s=/(4πkB). Using a controlled large-N expansion, we show that already at the first nontrivial order the equation of state and the Tan contact density C agree well with the most recent experimental measurements and theoretical Luttinger-Ward and bold diagrammatic Monte Carlo calculations.
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Tilman Enss (2012) studied this question.
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