Phase diagram of interacting pion matter and isospin charge fluctuations
arXiv:2102.02567 · doi:10.1103/PhysRevC.103.065201
Abstract
Equation of state and electric (isospin) charge fluctuations are studied for matter composed of interacting pions. The pion matter is described by self interacting scalar fields via a type Lagrangian. The mean-field approximation is used, and interaction parameters are fixed by fitting lattice QCD results on the isospin density as a function of the isospin chemical potential at zero temperature. Two scenarios for fixing the model parameters -- with and without the first order phase transition -- are considered, both yielding a satisfactory description of the lattice data. Thermodynamic functions and isospin charge fluctuations are studied and systematically compared for these two scenarios, yielding qualitative differences in the behavior of isospin charge susceptibilities. These differences can be probed by lattice simulations at temperatures MeV.
References in corpus (14)
- The equation of state in (2+1)-flavor QCD
- Probing freeze-out conditions in heavy ion collisions with moments of charge fluctuations
- Alpha-particle condensation in 16O via a full four-body OCM calculation
- Fluctuations in the quark-meson model for QCD with isospin chemical potential
- Hadron Resonance Gas Equation of State from Lattice QCD
- Pion and Kaon Condensation at Finite Temperature and Density
- Bose-Einstein condensation of pions in heavy-ion collisions at the CERN Large Hadron Collider (LHC) energies
- Bose-Einstein Condensation in the Relativistic Pion Gas: Thermodynamic Limit and Finite Size Effects
- Bose-Einstein Condensation of Pions in High Multiplicity Events
- Linear sigma model at finite density in the 1/N expansion to next-to-leading order
- Functional renormalization group at finite density and Bose condensation
- Quantum van der Waals and Walecka models of nuclear matter
- Bose-Einstein condensation phenomenology in systems with repulsive interactions
- Higher order conserved charge fluctuations inside the mixed phase