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Shear Viscosities from the Chapman-Enskog and the Relaxation Time Approaches

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arxiv 1203.0281 v1 pith:6NPKWXA4 submitted 2012-03-01 nucl-th hep-ph

classification nucl-thhep-ph
keywords crossdifferentialsectionsshearchapman-enskogdependselasticemployed
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The interpretation of the measured elliptic and higher order collective flows in heavy-ion collisions in terms of viscous hydrodynamics depends sensitively on the ratio of shear viscosity to entropy density. Here we perform a quantitative comparison between the results of shear viscosities from the Chapman-Enskog and relaxation time methods for selected test cases with specified elastic differential cross sections: (i) The non-relativistic, relativistic and ultra-relativistic hard sphere gas with angle and energy independent differential cross section (ii) The Maxwell gas, (iii) chiral pions and (iv) massive pions for which the differential elastic cross section is taken from experiments. Our quantitative results reveal that (i) the extent of agreement (or disagreement) depends sensitively on the energy dependence of the differential cross sections employed, and (ii) stress the need to perform quantum molecular dynamical (URQMD) simulations that employ Green-Kubo techniques with similar cross sections to validate the codes employed and to test the accuracy of other methods.

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Cited by 2 Pith papers

Reviewed papers in the Pith corpus that reference this work. Sorted by Pith novelty score. Full citation record

  1. Bulk viscosity of a binary mixture: the role of the intra-species interaction

    hep-ph 2026-06 unverdicted novelty 6.0 of 10

    Derives second-order Chapman-Enskog bulk viscosity for binary mixtures showing improved physical properties and agreement with Green-Kubo.

  2. Viscous coefficients and thermal conductivity of a $\pi K N$ gas mixture in the medium

    nucl-th 2019-08 conditional novelty 6.0 of 10

    Transport coefficients of a hot πKN gas are computed with in-medium cross sections from thermal field theory, showing medium effects increase relaxation times and modify η, ζ, and λ.

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