Phase Structure of {QCD} at High Temperature With Massive Quarks and Finite Quark Density: A ZZ(3) Paradigm

Jul, 1983
31 pages
Published in:
  • Nucl.Phys.B 225 (1983) 590
  • Published: 1983
Report number:
  • UU-HEP-83-8,
  • COLO-HEP-66

Citations per year

1983199320032013202202468
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