Collision energy dependence of the critical end point from baryon number fluctuations in the Linear Sigma Model with quarks
arXiv:2108.02362 · doi:10.1140/epja/s10050-022-00732-8
Abstract
We show that the Linear Sigma Model with quarks produces an effective description of the QCD phase diagram and of the system's equilibrium distribution properties that deviate from those of the Hadron Resonance Gas Model. The deviation is due to the inclusion of plasma screening properties, encoded in the contribution of the ring diagrams and thus to the introduction of a key feature of plasmas near phase transitions, namely, long-range correlations. After fixing the model parameters using input from LQCD for the crossover transition at vanishing chemical potential, we study the location of the Critical End Point in the effective QCD phase diagram. We use the model to study baryon number fluctuations and show that in heavy-ion collisions, the CEP can be located for collision energies GeV, namely, in the lowest NICA or within the HADES energy domain.
9 pages, 7 figures, expanded discussion and conclusions unchanged. Version to appear in EPJA
References in corpus (9)
- The order of the quantum chromodynamics transition predicted by the standard model of particle physics
- The renormalization group and quark number fluctuations in the Polyakov loop extended quark-meson model at finite baryon density
- Critical endpoint in the Polyakov-loop extended NJL model
- Hot and dense quark-gluon plasma thermodynamics from holographic black holes
- QCD phase transitions via a refined truncation of Dyson-Schwinger equations
- QCD phase diagram in a magnetized medium from the chiral symmetry perspective: The linear sigma model with quarks and the Nambu--Jona-Lasinio model effective descriptions
- Effects of Nuclear Potential on the Cumulants of Net-Proton and Net-Baryon Multiplicity Distributions in Au+Au Collisions at
- Calculating the initial energy density in heavy ion collisions by including the finite nuclear thickness
- Lattice QCD results on cumulant ratios at freeze-out