Gross-Witten-Wadia transition in a matrix model of deconfinement
arXiv:1206.1329 · doi:10.1103/PhysRevD.86.081701
Abstract
We study the deconfining phase transition at nonzero temperature in a SU(N) gauge theory, using a matrix model which was analyzed previously at small N. We show that the model is soluble at infinite N, and exhibits a Gross-Witten-Wadia transition. In some ways, the deconfining phase transition is of first order: at a temperature , the Polyakov loop jumps discontinuously from 0 to1/2, and there is a nonzero latent heat . In other ways, the transition is of second order: e.g., the specific heat diverges as when . Other critical exponents satisfy the usual scaling relations of a second order phase transition. In the presence of a nonzero background field for the Polyakov loop, there is a phase transition at the temperature where the value of the loop =1/2, with . Since as , this transition is of third order.
7pages, 1 figure; discussion on matrix models is extended; references are added
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- Effective matrix model for deconfinement in pure gauge theories
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- Collisional energy loss above the critical temperature in QCD
- The Roberge-Weiss transition and 't Hooft loops
- Finite-temperature phase transitions of third and higher order in gauge theories at large
- Effective models of a semi-quark gluon plasma
- Free energy of a Holonomous Plasma
- Zero interface tension at the deconfining phase transition for a matrix model of a gauge theory
- Matrix model for deconfinement in an SU(2) gauge theory in 2+1 dimensions
- Matrix model for deconfinement in a SU(Nc) gauge theory in 2+1 dimensions
- Real-time hard-thermal-loop gluon self-energy in a semiquark-gluon plasma
- The Polyakov loop models in the large N limit: Phase diagram at finite density
- Shear and bulk viscosity for a pure glue theory using an effective matrix model
- Wilson loops in the Hamiltonian formalism