Abstract
We consider the phase diagrams of modified action gauge and spin models and concentrate on their periphery - infinitely far from their origins (zero temperature - β-1 = 0). In this limit the exact positions of the phase transitions are found by looking for the global minimum of the single plaquette action (for a spin system - the single link energy). As the parameters of the model are varied, the position of such a global minimum is in general changed. When this changed is non-analytic, a phase transition takes place. The phase structure for finite β is clearly similar, but not identical to the infinite β one. We discuss several finite β corrections that should be applied to the exactly known infinite β picture. We confront our analysis for infinite β2 = ∑iβ2i with the Monte Carlo simulations for two four-dimensional gauge systems: an SU(3) gauge model with action S=-Re∑p(β1trUp+β2(tr Up)2) and an SU(2) model with S=-Re Σp[β1 1 2trUp+β2( 1 2trUp)2+β3( 1 2trU p)3].
| Original language | English |
|---|---|
| Pages (from-to) | 236-240 |
| Number of pages | 5 |
| Journal | Physics Letters, Section B: Nuclear, Elementary Particle and High-Energy Physics |
| Volume | 126 |
| Issue number | 3-4 |
| DOIs | |
| State | Published - 30 Jun 1983 |
| Externally published | Yes |
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