The Kazakov-Migdal Model as a High Temperature Lattice Gauge Theory
arXiv:hep-th/9212074 · doi:10.1016/0370-2693(93)90639-Y
Abstract
We show that the Kazakov-Migdal (K-M) induced gauge model in dimensions describes the high temperature limit of ordinary lattice gauge theories in dimensions. The matter fields are related to the Polyakov loops, while the spatial gauge variables become the gauge fields of the K-M model. This interpretation of the K-M model is in agreement with some recent results in high temperature lattice QCD.
arXiv comment12 pages, plain latex, DFTT 71/92
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Cited by in corpus (12)
- Phase Transitions in Particle Physics -- Results and Perspectives from Lattice Quantum Chromo-Dynamics
- Two dimensional QCD is a one dimensional Kazakov-Migdal model
- Toward an analytic determination of the deconfinement temperature in SU(2) L.G.T.
- Large N QCD at High Energies as Two-Dimensional Field Theory
- Kazakov--Migdal Model with Logarithmic Potential and the Double Penner Matrix Model
- Deconfinement Transition in Large N Lattice Gauge Theory
- A Simple Model Inducing QCD
- The Spectrum of the Kazakov Migdal-Model
- The Spatial String Tension in High Temperature Lattice Gauge Theories
- Gross-Witten-Wadia Phase Transition in Induced QCD on the Graph
- Vector Induced Lattice Gauge Theories
- Large-N Quenching in the Kazakov-Migdal Model