• DOI:10.1103/PhysRevC.97.024915
• Corpus ID: 54719982

Coupled kinetic equations for fermions and bosons in the relaxation-time approximation

@article{Florkowski2018CoupledKE,
  title={Coupled kinetic equations for fermions and bosons in the relaxation-time approximation},
  author={Wojciech Florkowski and Ewa Maksymiuk and Radoslaw Ryblewski},
  journal={Physical Review C},
  year={2018},
  volume={97},
  pages={024915}
}

• W. Florkowski, Ewa Maksymiuk, R. Ryblewski
• Published 19 October 2017
• Physics
• Physical Review C

Kinetic equations for quarks and gluons are solved numerically in the relaxation time approximation for the case of one-dimensional boost-invariant geometry. Quarks are massive and described by the Fermi-Dirac statistics, while gluons are massless and obey Bose-Einstein statistics. The conservation laws for the baryon number, energy, and momentum lead to two Landau matching conditions which specify the coupling between the quark and gluon sectors and determine the proper-time dependence of the effective temperature and baryon chemical potential of the system. The numerical results illustrate how a non-equlibrium mixture of quarks and gluons approaches hydrodynamic regime described by the Navier-Stokes equations with appropriate forms of the kinetic coefficients. The shear viscosity of a mixture is the sum of the shear viscosities of quark and gluon components, while the bulk viscosity is given by the formula known for a gas of quarks, however, with the thermodynamic variables characterising the mixture. Thus, we find that massless gluons contribute in a non-trivial way to the bulk viscosity of a mixture, provided quarks are massive. We further observe the hydrodynamization effect which takes place earlier in the shear sector than in the bulk one. The numerical studies of the ratio of the longitudinal and transverse pressures show, to a good approximation, that it depends on the ratio of the relaxation and proper times only. This behaviour is connected with the existence of an attractor solution for conformal systems.