2+1D lattice gauge theory can emerge in a spin system through fractionalization. Usually if the gauge structure is broken down to ZN, it is believed that the fractionalized spinons are deconfined. However in general, ZN gauge theory also have a confined phase. The question is how to determine if the discrete emergent gauge theory is really deconfined or not?
For example, I am considering a Z3 gauge-Higgs model defined on the Kagome lattice with the Hamiltonian H=J∑⟨ij⟩cos(θi−θj−Aij), where θi=0,±2π/3 is the matter field and Aij=0,±2π/3 is the gauge field. If the matter field is in a ferromagnetic phase, then I can understand that the gauge field will be Higgs out. But the matter field here is a Kagome antiferromagnet, which is strongly frustrated and may not order at low temperature. So in this case, I would suspect that the effective Z3 gauge theory will be driven into a confined phase. Is my conjecture right? How to prove or disprove that?
Thanks in advance.
This post imported from StackExchange Physics at 2014-04-05 03:24 (UCT), posted by SE-user Everett You