Effective holographic models for QCD: Thermodynamics and viscosity coefficients

TL;DR

This paper extends effective holographic QCD models to finite temperature, analyzing black hole solutions, thermodynamics, and viscosity coefficients, and compares results with lattice and experimental data.

Contribution

It introduces a finite temperature extension of EHQCD models, classifies black hole solutions, and computes thermodynamic and viscosity properties, linking them to lattice and experimental results.

Findings

Large black holes are thermally stable and dual to non-conformal plasma.

Shear viscosity to entropy ratio remains universal at 1/4π.

Bulk viscosity varies with temperature and model parameters, increasing near T_min.

Abstract

A finite temperature extension of the effective holographic models for QCD (EHQCD), proposed in Ref.[1], is investigated in the present work. EHQCD models are characterized by two parameters, the conformal dimension of the relevant operator that deforms the CFT and the associated coupling. We find that black hole solutions appear at temperatures higher than some temperature $T_{min}$ and can be categorized in two classes: large and small black holes. A large black hole is thermally stable and it is therefore interpreted as the gravity dual of a non-conformal plasma. A small black hole, on the other hand, is thermally unstable. We show that thermodynamic quantities such as the entropy density $s$, specific heat $C_V$, and speed of sound $c_s$ are sensitive to the model parameters. We investigate perturbations of the black hole solutions and calculate the viscosity coefficients of the corresponding dual non-conformal plasma. For the shear viscosity, we confirm that the ratio $\eta/s$ is given by the universal result $1/4\pi$. For the bulk viscosity, the ratio $\zeta/s$ varies with the temperature, displaying a rapid growth close to $T_{min}$, and it is sensitive to the model parameters. We compare our results for the thermodynamic quantities with the lattice $SU(N_C)$ results and find that they are compatible as long as the coupling is fixed appropriately as a function of the conformal dimension. We also compare our results for the viscosity coefficients against the JETSCAPE results that are obtained from the analysis of experimental data on heavy ion collisions.