Abstract
We have investigated the phase transition of a two-dimensional system described by the Hamiltonian H=-J cos(-)-K JNN cos(++), for J,K>0 and 0≤K/J≤1, and where NN denotes nearest neighbors, which has both Ising-like domain-wall (string) and XY-like vortex excitations. Migdal-Kadanoff and Monte Carlo renormalization-group studies indicate that there is only one transition which is Ising-like. The roles of string and vortex excitations in the phase transition are discussed by an energy-entropy argument and are found to be consistent with Monte Carlo quench results.
- Received 3 September 1985
DOI:https://doi.org/10.1103/PhysRevB.33.3419
©1986 American Physical Society