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Nearly perfect fluidity: from cold atomic gases to hot quark gluon plasmas

REVIEW ARTICLE

Thomas Schäfer1 and Derek Teaney2,3

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Shear viscosity is a measure of the amount of dissipation in a simple fluid. In kinetic theory shear viscosity is related to the rate of momentum transport by quasi-particles, and the uncertainty relation suggests that the ratio of shear viscosity η to entropy density s in units of planck/kB is bounded by a constant. Here, planck is Planck's constant and kB is Boltzmann's constant. A specific bound has been proposed on the basis of string theory where, for a large class of theories, one can show that η/splanck/(4πkB). We will refer to a fluid that saturates the string theory bound as a perfect fluid. In this review we summarize theoretical and experimental information on the properties of the three main classes of quantum fluids that are known to have values of η/s that are smaller than planck/kB. These fluids are strongly coupled Bose fluids, in particular liquid helium, strongly correlated ultracold Fermi gases and the quark gluon plasma. We discuss the main theoretical approaches to transport properties of these fluids: kinetic theory, numerical simulations based on linear response theory and holographic dualities. We also summarize the experimental situation, in particular with regard to the observation of hydrodynamic behavior in ultracold Fermi gases and the quark gluon plasma.


PACS

12.38.Mh Quark–gluon plasma

05.30.Fk Fermion systems and electron gas

11.27.+d Extended classical solutions; cosmic strings, domain walls, texture

Subjects

Quantum gases, liquids and solids

Statistical physics and nonlinear systems

Particle physics and field theory

Dates

Issue 12 (December 2009)

Received 21 April 2009, in final form 17 July 2009

Published 12 November 2009



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