Percolation and Magnetization in the Continuous Spin Ising Model
arXiv:hep-lat/0003014 · doi:10.1016/S0550-3213(00)00332-1
Abstract
In the strong coupling limit the partition function of SU(2) gauge theory can be reduced to that of the continuous spin Ising model with nearest neighbour pair-interactions. The random cluster representation of the continuous spin Ising model in two dimensions is derived through a Fortuin-Kasteleyn transformation, and the properties of the corresponding cluster distribution are analyzed. It is shown that for this model, the magnetic transition is equivalent to the percolation transition of Fortuin-Kasteleyn clusters, using local bond weights. These results are also illustrated by means of numerical simulations.
Cited by in corpus (11)
- Universality classes in nonequilibrium lattice systems
- Site Percolation and Phase Transitions in Two Dimensions
- Effective Z(2) Spin Models of Deconfinement and Percolation in SU(2) Gauge Theory
- Cluster Percolation in O(n) Spin Models
- Ising-like critical behavior of vortex lattices in an active fluid
- Cluster Percolation and Pseudocritical Behaviour in Spin Models
- Cluster Percolation and Thermal Critical Behaviour
- Cluster Percolation and Critical Behaviour in Spin Models and SU(N) Gauge Theories
- Critical Droplets and Phase Transitions in Two Dimensions
- Second-order critical lines of spin-S Ising models in a splitting field with Grassmann techniques
- Two Geometric Approaches To Study The Deconfinement Phase Transition in (3+1)-Dimensional Gauge Theories