Abstract
Monte Carlo simulations are performed for first-order phase-transition models. The three-dimensional three-state Potts model has a weak first-order transition. For this model we calculate the density of states on block lattices (L up to size 36) and obtain high-precision estimates for the leading partition-function zeros. The finite-size-scaling analysis of the first zero exhibits the expected convergence of the critical exponent ν toward 1/D for large L; in particular, we find ν=2.955(26) from our two largest lattices. Analysis of our specific-heat data yields l=0.080 31(26) for the latent heat. Along another line of approach, we calculate the mass gap m=1/ξ (ξ is the correlation length) for cylindrical lattices (L up to 24 and =256). The finite size-scaling analysis of these results is also consistent with the convergence of ν toward 1/D, but that the limiting value is 1/D is not yet conclusively established. Some theoretical arguments favor ν→0 in case of a first-order transition in a cylindrical ∞ geometry. Therefore, we also applied our approach to the 2D ten-state Potts model, which is known to have a strong first-order transition. In this case we find unambiguous evidence in favor of 1/D as the limiting value.
- Received 9 October 1990
DOI:https://doi.org/10.1103/PhysRevB.43.5846
©1991 American Physical Society