Phase Structure of {QCD} at High Temperature With Massive Quarks and Finite Quark Density: A (3) Paradigm
Jul, 198331 pages
Published in:
- Nucl.Phys.B 225 (1983) 590
- Published: 1983
Report number:
- UU-HEP-83-8,
- COLO-HEP-66
Citations per year
Abstract: (Elsevier)
The confinement/deconfinement phase transition in SU(3) lattice gauge theories at high temperatures is analogous to that of the Z(3) gauge theories. We study various Z(3) gauge-matter theories that result from replacing the gauge group SU(3) with its center Z(3). We include large-mass fermions in the Wilson formulation and allow a chemical potential. We show that in the limit of strong coupling and high temperature the (3 + 1)-dimensional theory becomes a three state, three-dimensional Potts model with uniform external fields of real and imaginary strengths related to the fermion mass and chemical potential. By studying the phase structure of the q = 3, d = 3 Potts model with external fields we argue that the confinement/deconfinement phase transition is first order, but highly sensitive to external fields, and that it does not occur at “strong coupling” in a Z(3) gauge theory if there is a light enough fermion present. We discuss the consequences of this result for QCD.- GAUGE FIELD THEORY: SU(3)
- LATTICE FIELD THEORY: CRITICAL PHENOMENA
- GAUGE FIELD THEORY: Z(3)
- GAUGE FIELD THEORY: Z(2)
- QUARK: CONFINEMENT
- MODEL: POTTS
- QUANTUM CHROMODYNAMICS
- APPROXIMATION: MEAN FIELD
- FERMION: LATTICE FIELD THEORY
- NUMERICAL CALCULATIONS: MONTE CARLO
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