Confinement and chiral symmetry crossovers
arXiv:1004.3073
Abstract
We study the QCD phase diagram, in particular we study the critical points of the two main QCD phase transitions, confinement and chiral symmetry breaking. Confinement drives chiral symmetry breaking, and, due to the finite quark mass, at small density both transitions are a crossover, while they are a first or second order phase transition in large density. We study the QCD phase diagram with a quark potential model including both confinement and chiral symmetry. This formalism, in the Coulomb gauge hamiltonian formalism of QCD, is presently the only one able to microscopically include both a quark-antiquark confining potential and a vacuum condensate of quark-antiquark pairs. This model is able to address all the excited hadrons, and chiral symmetry breaking, at the same token. Our order parameters are the Polyakov loop and the quark mass gap. The confining potential is extracted from the Lattice QCD data of the Bielefeld group. We address how the quark masses affect the critical point location in the phase diagram.
arXiv comment4 pages, 3 figures, contribution submitted to 45th Rencontres de Moriond, QCD and High Energy Interactions, La Thuile, March 13-20, 2010
References in corpus (8)
- Static quark anti-quark interactions in zero and finite temperature QCD. I. Heavy quark free energies, running coupling and quarkonium binding
- Heavy Quark Potentials in Quenched QCD at High Temperature
- Meson Structure in a Relativistic Many-Body Approach
- Color Screening and Quark-Quark Interactions in Finite Temperature QCD
- Chiral symmetry breaking solutions for QCD in the truncated Coulomb gauge
- Heavy quark free energies for three quark systems at finite temperature
- The QCD string tension curve, the ferromagnetic magnetization, and the quark-antiquark confining potential at finite Temperature
- Static quark anti-quark free and internal energy in 2-flavor QCD and bound states in the QGP