Abstract
We investigate the temperature dependence of the shear viscosity to entropy density ratio $\eta/s$ using a piecewise linear parametrization. To determine the optimal values of the parameters and the associated uncertainties, we perform a global Bayesian model-to-data comparison on Au+Au collisions at $\sqrt{s_{NN}}=200$ GeV and Pb+Pb collisions at $2.76$ TeV and $5.02$ TeV, using a 2+1D hydrodynamical model with the EKRT initial state. We provide three new parametrizations of the equation of state (EoS) based on contemporary lattice results and hadron resonance gas, and use them and the widely used $s95p$ parametrization to explore the uncertainty in the analysis due to the choice of the equation of state. We found that $\eta/s$ is most constrained in the temperature range $T\approx 150$--$220$ MeV, where, for all EoSs, $0.08 < \eta/s < 0.23$ when taking into account the 90% credible intervals. In this temperature range the EoS parametrization has only a small $\approx 10\%$ effect on the favored $\eta/s$ value, which is less than the $\approx 30\%$ uncertainty of the analysis using a single EoS parametrization. Our parametrization of $(\eta/s)(T)$ leads to a slightly larger minimum value of $\eta/s$ than the previously used parametrizations. When we constrain our parametrization to mimic the previously used parametrizations, our favored value is reduced, and the difference becomes statistically insignificant.
Highlights
The main goal of the ultrarelativistic heavy-ion collisions at the Large Hadron Collider (LHC) and the Relativistic Heavy-Ion Collider (RHIC) is to understand the properties of the strongly interacting matter produced in these collisions
We obtain well constrained η/s in a temperature range 150
We have introduced three new parametrizations of the equation of state based on the contemporary lattice data: 044911-11
Summary
The main goal of the ultrarelativistic heavy-ion collisions at the Large Hadron Collider (LHC) and the Relativistic Heavy-Ion Collider (RHIC) is to understand the properties of the strongly interacting matter produced in these collisions. To study the temperature dependence of η/s we use a piecewise linear parametrization in three parts: linearly decreasing and increasing regions at low and high temperatures are connected by a constant-value plateau of variable range. With this parametrization, data favoring a strong temperature dependence will lead to large slopes and a narrow plateau; an approximately constant η/s can be obtained with small slope parameter values and a wide plateau. A comparison of the final probability distributions of the parameters will tell whether the most probable parameter values depend on the EoS used, and whether that difference is significant when the overall uncertainty in the fitting procedure is taken into account
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