First Order Chiral Phase Transition from a Six-fermion ''Instanton''-Interaction
arXiv:hep-ph/0309101 · doi:10.1016/j.nuclphysa.2003.11.060
Abstract
We compute the first order chiral phase transition for an instanton motivated quark model with a local six-quark interaction. In order to compare different solutions of the gap equation we compute the bosonic effective action -- a two particle irreducible free energy functional. We find that the first order transition ends for a critical current quark mass, with continuous crossover for larger quark masses. Furthermore, we investigate different possible order parameters, including a color octet condensate. We also compare our formalism with mean field theory.
10 pages, 3 figures, uses revtex4
References in corpus (16)
- Instantons in QCD
- QCD at Finite Baryon Density: Nucleon Droplets and Color Superconductivity
- Color-Flavor Locking and Chiral Symmetry Breaking in High Density QCD
- Dyson-Schwinger Equations and the Application to Hadronic Physics
- The Infrared Behavior of QCD Green's Functions - Confinement, Dynamical Symmetry Breaking, and Hadrons as Relativistic Bound States
- Diquark Bose Condensates in High Density Matter and Instantons
- Dyson-Schwinger Equations: Density, Temperature and Continuum Strong QCD
- Color Superconductivity and Chiral Symmetry Restoration at Nonzero Baryon Density and Temperature
- Continuity of Quark and Hadron Matter
- The Crystallography of Color Superconductivity
- Flow Equations without Mean Field Ambiguity
- Spontaneously broken color
- Gluon-Meson Duality
- Spontaneous symmetry breaking in the colored Hubbard model
- Gluon-Meson Duality in the Mean Field Approximation
- Instantons and color symmetry breaking in the vacuum
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