Traces of the nuclear liquid-gas phase transition in the analytic properties of hot QCD
arXiv:1909.04461 · doi:10.1103/PhysRevC.101.035205
Abstract
The nuclear liquid-gas transition at normal nuclear densities, fm, and small temperatures, MeV, has a large influence on analytic properties of the QCD grand-canonical thermodynamic potential. A classical van der Waals equation is used to determine these unexpected features due to dense cold matter qualitatively. The existence of the nuclear matter critical point results in thermodynamic branch points, which are located at complex chemical potential values, for MeV, and exhibit a moderate model dependence up to rather large temperatures MeV. The behavior at higher temperatures is studied using the van der Waals hadron resonance gas (vdW-HRG) model. The baryon-baryon interactions have a decisive influence on the QCD thermodynamics close to . In particular, nuclear matter singularities limit the radius of convergence of the Taylor expansion in , with values at MeV obtained in the vdW-HRG model.
11 pages, 5 figures
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- Higher order conserved charge fluctuations inside the mixed phase
- Diffusion and fluctuations of open charmed hadrons in an interacting hadronic medium
- Critical point influenced by Bose-Einstein condensation
- Effect of Coriolis Force on Diffusion of D Meson
- Shear viscosity and electrical conductivity of rotating quark matter in Nambu--Jona-Lasinio Model
- Lattice-based equation of state with a critical point from constant entropy contours and its comparison to effective QCD approaches
- Shear Viscosity and Electrical Conductivity of Rotating Nuclear Medium in Hadron Resonance Gas and Nambu-Jona Lasinio Models