NJL Model at Finite Chemical Potential in a Constant Magnetic Field
arXiv:hep-ph/0404219 · doi:10.1143/PTPS.153.321
Abstract
We investigate the influence of an external magnetic field on chiral symmetry breaking in the Nambu-Jona-Lasinio (NJL) model at finite temperature and chemical potential. According to the Fock-Schwinger proper-time method, we calculate the effective potential in the leading order of the expansion. The phase boundary dividing the symmetric phase and the broken phase is illustrated numerically. A complex behavior of the phase boundary is found for large chemical potential.
arXiv comment6 pages, 2 figures, Poster talk presented at the Workshop on Finite Density QCD at Nara, Japan, 10-12 July 2003; replaced two references
Cited by in corpus (15)
- Quantum field theory in a magnetic field: From quantum chromodynamics to graphene and Dirac semimetals
- Magnetic Catalysis: A Review
- Anomalous magnetic moment of hot quarks, inverse magnetic catalysis and reentrance of chiral symmetry broken phase
- Effect of anomalous magnetic moment of quarks on the phase structure and mesonic properties in the NJL model
- Chiral density waves in the NJL model with quark number and isospin chemical potentials
- Effects of quark anomalous magnetic moment on the thermodynamical properties and mesonic excitations of magnetized hot and dense matter in PNJL model
- Effects of anomalous magnetic moment of quarks on the dilepton production from hot and dense magnetized quark matter using the NJL model
- Pion condensation of quark matter in the static Einstein universe
- Cooper pairing and finite-size effects in a NJL-type four-fermion model
- Parameter fitting in three-flavor Nambu--Jona-Lasinio model with various regularizations
- Does there arise a significant enhancement of the dynamical quark mass in external magnetic field?
- Inverse magnetic catalysis and confinement within a contact interaction model for quarks
- Chiral susceptibility in Nambu Jona Lasinio model: a Wigner function approach
- Insignificance of the anomalous magnetic moment of the quarks in presence of chiral imbalance
- Magnetic-Field Induced Critical Endpoint