Quark matter phase diagram under the influence of strong magnetic fields with a nonlocal chiral model
arXiv:2211.07368 · doi:10.1002/asna.20220085
Abstract
We study the phase diagram in the plane for quark matter under the influence of a strong uniform magnetic field , in the framework of a non-local extension of the two-flavor Polyakov Nambu-Jona-Lasinio model. We analyze the deconfinement and chiral symmetry restoration transitions in the mean field approximation. For the considered parameterization, it is found that there is always a critical end point (CEP) in the plane that separates a first-order transition line from a smooth crossover. The location of the CEP is studied as a function of the magnetic field.
arXiv comment5 pages, 3 figures
References in corpus (11)
- Phases of QCD: lattice thermodynamics and a field theoretical model
- Event-by-event generation of electromagnetic fields in heavy-ion collisions
- Dense Quarks, and the Fermion Sign Problem, in a SU(N) Matrix Model
- The K/pi ratio from condensed Polyakov loops
- On covariant nonlocal chiral quark models with separable interactions
- Nonlocal chiral quark models with wavefunction renormalization: sigma properties and π-πscattering parameters
- Characteristics of the chiral phase transition in nonlocal quark models
- Quark matter under strong magnetic fields in SU(2) NJL-type models: parameter dependence of the cold dense matter phase diagram
- Strong magnetic fields in nonlocal chiral quark models
- Pion radiative weak decays in nonlocal chiral quark models
- Cold magnetized quark matter at finite density in a nonlocal chiral quark model