Abstract
Quark-hadron matter at finite temperature and density is studied using a two-flavor, color SU(2) (P)NJL model. The hadronic effective Lagrangian, derived by bosonization of the quark fields and renormalized using the Eguchi method, emerges in the form of an extended linear σ model with meson and diquark-baryon fields. Chiral and diquark condensates are studied as functions of temperature and baryon density. Masses of mesons and diquark-baryons are calculated with and without the Polyakov loop effect. We investigate the equation of state of quark-hadron matter by taking into account the contributions of mesons and diquark-baryons in addition to the quark quasiparticles.
Original language | English |
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Pages (from-to) | 71-102 |
Number of pages | 32 |
Journal | Nuclear Physics, Section A |
Volume | 913 |
DOIs | |
State | Published - 2 Sep 2013 |
Keywords
- Chiral condensation
- Color SU(2)
- Diquark condensation
- Equation of state of quark-hadron matter
- NJL model
- Polyakov loop