A new large N phase transition in YM2
arXiv:hep-th/0506207 · doi:10.1016/j.nuclphysb.2006.03.017
Abstract
Inspired by the interpretation of two dimensional Yang-Mills theory on a cylinder as a random walk on the gauge group, we point out the existence of a large N transition which is the gauge theory analogue of the cutoff transition in random walks. The transition occurs in the strong coupling region, with the 't Hooft coupling scaling as alpha*log(N), at a critical value of alpha (alpha = 4 on the sphere). The two phases below and above the transition are studied in detail. The effective number of degrees of freedom and the free energy are found to be proportional to N^(2-alpha/2) below the transition and to vanish altogether above it. The expectation value of a Wilson loop is calculated to the leading order and found to coincide in both phases with the strong coupling value.
23 pages, 3 figures
References in corpus (20)
- Two Dimensional QCD is a String Theory
- Large Phase Transition in Continuum QCD
- Twists and Wilson Loops in the String Theory of Two Dimensional QCD
- Instanton Induced Large Phase Transitions in Two and Four Dimensional QCD
- On the Large N Limit of the Itzykson-Zuber Integral
- Equivalence of Two Dimensional QCD and the Matrix Model
- Interacting Fermion Systems from Two Dimensional QCD
- Complex Matrix Models and Statistics of Branched Coverings of 2D Surfaces
- Brownian Motion, Chern-Simons Theory, and 2d Yang-Mills
- Wilson loop for large N Yang-Mills theory on a two-dimensional sphere
- Large-N quantum gauge theories in two dimensions
- Wilson loop on a sphere
- Conformal Field Theory Techniques for Large N Group Theory
- Chern-Simons Theory in Lens Spaces from 2d Yang-Mills on the Cylinder
- Two dimensional QCD is a one dimensional Kazakov-Migdal model
- Two-dimensional QCD on the sphere and on the cylinder
- Wilson Loops in Large N QCD on a Sphere
- Matrix string states in pure 2d Yang Mills theories
- Two-dimensional gauge theories of the symmetric group S_n in the large-n limit
- Macdonald's identities and the large N limit of on the cylinder