Temperature and net baryochemical potential dependence of $\eta/s$ in a hybrid approach
In this work, the qualitative impact of the net baryochemical potential dependence of the shear viscosity to entropy density ratio $\eta/s$ in hydrodynamical simulations is studied. The effect of a predicted non-constant $\eta/s$($\mu_B$) is largely unexplored in hydrodynamic simulations. Previous s...
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Zusammenfassung: | In this work, the qualitative impact of the net baryochemical potential
dependence of the shear viscosity to entropy density ratio $\eta/s$ in
hydrodynamical simulations is studied. The effect of a predicted non-constant
$\eta/s$($\mu_B$) is largely unexplored in hydrodynamic simulations. Previous
studies focus only on a temperature dependence or even only a constant
effective shear viscosity. This work addresses this issue by studying
qualitatively the effect of a generalized $\eta/s$($T,\mu_B$) in the hybrid
approach SMASH-vHLLE, composed of the hadronic transport approach SMASH and the
(3+1)d viscous hydrodynamic code vHLLE. In order to reduce the bias of the
result on the equation of state used in the hydrodynamic part of the model,
$\eta/s$ is parameterized directly in the energy density and net baryon number
density. The parameterization takes into account the constraints of matching to
the transport coefficients in the hadronic phase, as well as pQCD results. This
work compares the impact of the density dependence for different system sizes
and energies and compares the observables with experimental results in the RHIC
- BES region $\sqrt{s_{NN}}$ =7.7 - 39.0 GeV, as the effect of this
generalization is especially relevant for intermediate collision energies, for
which the system is in equilibrium for a relevant amount of time, but the net
baryochemical potential does not vanish. It is shown that the effect of an
explicit net baryon number dependence on the elliptic flow is negligible and
only relevant in the early stages of the collision. Additionally, we find that
the proposed parameterization could be a good proxy for the shear viscosity in
the non-equilibrium hadronic transport stage. |
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DOI: | 10.48550/arxiv.2207.05778 |