Difficulties in Inducing a Gauge Theory at Large N
arXiv:hep-th/9212158 · doi:10.1103/PhysRevD.49.R24
Abstract
It is argued that the recently proposed Kazakov-Migdal model of induced gauge theory, at large , involves only the zero area Wilson loops that are effectively trees in the gauge action induced by the scalars. This retains only a constant part of the gauge action excluding plaquettes or anything like them and the gauge variables drop out.
6 pages, Latex, AZPH-TH/93-01, COLO-HEP/303
References in corpus (10)
- Induced QCD at Large N
- Area Law and Continuum Limit in "Induced QCD"
- Induced QCD and Hidden Local ZN Symmetry
- Some Remarks About Induced QCD
- Exact solution of d=1 Kazakov-Migdal induced gauge theory
- 1/N Expansion and Particle Spectrum in Induced QCD
- The Problem of Large-N Phase Transition in Kazakov-Migdal Model of Induced QCD
- The Phase Diagram of the Kazakov-Migdal Model
- Phase Transitions in Induced QCD
- Induced QCD Without Local Confinement