Coupling Relativistic Viscous Hydrodynamics to Boltzmann Descriptions
arXiv:1003.0413 · doi:10.1103/PhysRevC.82.044901
Abstract
Models of relativistic heavy ion collisions typically involve both a hydrodynamic module to describe the high density liquid-like phase and a Boltzmann module to simulate the low density break-up phase which is gas-like. Coupling the prescriptions is more complicated for viscous prescriptions if one wants to maintain continuity of the entire stress-energy tensor and currents. Derivations for the viscosity for a gas are reviewed, which then lead to expressions for changes in the phase space occupation based on simple relaxation-time pictures of viscosity. These expressions are shown to consistently reproduce the non-equilibrium components of the stress-energy tensor. An algorithm for generating a Monte Carlo sampling of particles with which to initiate the Boltzmann calculations is also presented.
publication version (minor changes to wording, references added, typos fixed)
References in corpus (10)
- A calculation of the bulk viscosity in SU(3) gluodynamics
- Suppression of elliptic flow in a minimally viscous quark-gluon plasma
- Thermodynamics and bulk viscosity of approximate black hole duals to finite temperature quantum chromodynamics
- Dissipative Hydrodynamics and Heavy Ion Collisions
- Origins of Bulk Viscosity at RHIC
- Relativistic Dynamics of Non-ideal Fluids: Viscous and heat-conducting fluids I. General Aspects and 3+1 Formulation for Nuclear Collisions
- Bulk Viscosity driven clusterization of quark-gluon plasma and early freeze-out in relativistic heavy-ion collisions
- Instability of Boost-invariant hydrodynamics with a QCD inspired bulk viscosity
- Relativistic Dynamics of Non-ideal Fluids: Viscous and heat-conducting fluids II. Transport properties and microscopic description of relativistic nuclear matter
- Covariant description of kinetic freeze out through a finite space-like layer