Quasi Long Range Order and Vortex Lattice in the Three State Potts Model
arXiv:1507.08766 · doi:10.1103/PhysRevLett.116.097206
Abstract
We show that the order-disorder phase transition in the three state Potts ferromagnet on a square lattice is driven by a coupled proliferation of vortices and domain walls. Raising the vortex core energy above a certain value decouples the proliferation and splits the transition into two. The phase between the two transitions exhibits an emergent U(1) symmetry and quasi long range order. Lowering the core energy also splits the order-disorder transition but the proliferation does not decouple and a vortex lattice appears as the intermediate phase.
5 pages, 4 figures
References in corpus (5)
- Phase diagram of the Parafermionic Chain with Chiral Interactions
- Two step disordering of the vortex lattice across the peak effect in a weakly pinned Type II superconductor, Co0.0075NbSe2
- How the vortex lattice of a superconductor becomes disordered: a study by scanning tunneling spectroscopy
- Phase Transitions In Two Planar Lattice Models And Topological Defects: A Monte Carlo Study
- Thermal Phase Transition of Generalized Heisenberg Models for SU(N) Spins on Square and Honeycomb Lattices
Cited by in corpus (5)
- Gravitational waves from single neutron stars: an advanced detector era survey
- Competing nematic interactions in a generalized XY model in two and three dimensions
- Cross derivative: a universal and efficient method for phase transitions in classical spin models
- Overlap of two topological phases in the antiferromagnetic Potts model
- Two-stage melting of an inter-component Potts long-range order in two dimensions