A Blast Wave Model With Viscous Corrections
arXiv:1612.05629 · doi:10.1088/1742-6596/832/1/012056
Abstract
Hadronic observables in the final stage of heavy ion collision can be described well by fluid dynamics or blast wave parameterizations. We improve existing blast wave models by adding shear viscous corrections to the particle distributions in the Navier-Stokes approximation. The specific shear viscosity of a hadron gas at the freeze-out temperature is a new parameter in this model. We extract the blast wave parameters with viscous corrections from experimental data which leads to constraints on the specific shear viscosity at kinetic freeze-out. Preliminary results show is rather small.
arXiv commentProceedings for HQ 2016,4 pages,3 figures
References in corpus (8)
- Hydrodynamic Modeling of Heavy-Ion Collisions
- Causal viscous hydrodynamics in 2+1 dimensions for relativistic heavy-ion collisions
- Applying Bayesian parameter estimation to relativistic heavy-ion collisions: simultaneous characterization of the initial state and quark-gluon plasma medium
- Observable implications of geometrical and dynamical aspects of freeze-out in heavy ion collisions
- Radiative energy loss and v2 spectra for viscous hydrodynamics
- Centrality dependence of the nuclear modification factor of charged pions, kaons, and protons in Pb-Pb collisions at TeV
- Evolution of Hot, Dissipative Quark Matter in Relativistic Nuclear Collisions
- A viscous blast-wave model for relativistic heavy-ion collisions
Cited by in corpus (5)
- Higher-order anisotropies in the Blast-Wave Model - disentangling flow and density field anisotropies
- Bayesian Inference of the Specific Shear and Bulk Viscosities of the Quark-Gluon Plasma at Crossover from and Observables
- Higher order anisotropies in the Buda-Lund model: Disentangling flow and density field anisotropies
- Exploring Anisotropic flow via the Boltzmann Transport Equation Employing the Tsallis Blast Wave Description at LHC energies
- Phenomenological models of two-particle correlation distributions on transverse momentum in relativistic heavy-ion collisions