4.5 Article

Shear viscosity and electric conductivity of a hot and dense QGP with a chiral phase transition

Journal

PHYSICAL REVIEW C
Volume 103, Issue 5, Pages -

Publisher

AMER PHYSICAL SOC
DOI: 10.1103/PhysRevC.103.054901

Keywords

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Funding

  1. Helmholtz Graduate School for Heavy Ion research
  2. Deutsche Forschungsgemeinschaft (DFG, German Research Foundation) [CRC-TR 211, 315477589-TRR 211]
  3. European Union [824093]
  4. COST Action [CA15213]

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In this study, we calculated transport coefficients for strongly interacting quark matter in the extended PNJL model. We found that the shear viscosity over entropy ratio and the ratio of electric conductivity to temperature exhibited similar temperature and chemical potential behaviors when approaching the chiral phase transition. However, the differences between the two methods of calculation increased with temperature.
We calculate two transport coefficients-the shear viscosity over entropy ratio eta/s and the ratio of the electric conductivity to the temperature, sigma(0)/T-of strongly interacting quark matter within the extended N-f = 3 Polyakov Nambu-Jona-Lasinio (PNJL) model along the crossover transition line for moderate values of baryon chemical potential 0 <= mu(B) <= 0.9 GeV as well as in the vicinity of the critical endpoint (CEP) and at large baryon chemical potential mu(B) = 1.2 GeV, where the first-order phase transition takes place. The evaluation of the transport coefficients is performed on the basis of the effective Boltzmann equation in the relaxation time approximation. We employ two different methods for the calculation of the quark relaxation times: (i) using the averaged transition rate defined via thermal averaged quark-quark and quark-antiquark PNJL cross sections and (ii) using the weighted thermal averaged quark-quark and quark-antiquark PNJL cross sections. The eta/s and sigma(0)/T transport coefficients have similar temperature and chemical potential behaviors when approaching the chiral phase transition for both methods for the quark relaxation time; however, the differences grow with increasing temperature. We demonstrate the effect of the first-order phase transition and of the CEP on the transport coefficients in the deconfined QCD medium.

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