Local QCD Action at Finite Temperature

Abstract

In this article, we carefully derive the horizon condition at finite temperature. Only the zero Matsubara mode is affected, and this result is consistent with the suitably modified Maggiore-Schaden shift, which takes into account temporal periodicity. We thus obtain a local, BRST-invariant action for QCD at finite temperature. The large-N limit and other calculational schemes for the magnetic mass and its relation to the Gribov mass are also discussed.

References in corpus (10)

• A refinement of the Gribov-Zwanziger approach in the Landau gauge: infrared propagators in harmony with the lattice results
• The Physics of Glueballs
• Infrared properties of propagators in Landau-gauge pure Yang-Mills theory at finite temperature
• Dielectric function of the QCD vacuum
• Quark-Gluon Plasmas and Thermalization
• Equation of State of Gluon Plasma from Local Action
• BRST Cohomology and Physical Space of the GZ Model
• Poincare' Symmetry of the GZ-Model
• Exploring dynamical gluon mass generation in three dimensions
• Finiteness of the Coulomb gauge QCD perturbative effective action

Cited by in corpus (5)

• Transport coefficients of the Gribov-Zwanziger plasma
• A Gribov-Zwanziger type action invariant under background gauge transformations
• The Gribov problem in presence of background field for $SU(2)$ Yang-Mills theory
• Schwinger-Dyson Equations in Coulomb Gauge Consistent with Numerical Simulation
• Some Developments in Gribov's Approach to QCD