Kosterlitz Thouless Universality in Dimer Models
arXiv:hep-lat/0306034 · doi:10.1103/PhysRevD.68.091502
Abstract
Using the monomer-dimer representation of strongly coupled U(N) lattice gauge theories with staggered fermions, we study finite temperature chiral phase transitions in (2+1) dimensions. A new cluster algorithm allows us to compute monomer-monomer and dimer-dimer correlations at zero monomer density (chiral limit) accurately on large lattices. This makes it possible to show convincingly, for the first time, that these models undergo a finite temperature phase transition which belongs to the Kosterlitz-Thouless universality class. We find that this universality class is unaffected even in the large N limit. This shows that the mean field analysis often used in this limit breaks down in the critical region.
4 pages, 4 figures
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- Scaling Theories of Kosterlitz-Thouless Phase Transitions
- Tensor network calculation of the logarithmic correction exponent in the XY model
- Failure of Mean Field Theory at Large N
- Anomalous superfluidity in 2+1 dimensional two-color lattice QCD
- Asymptotic Freedom at the Berezinskii-Kosterlitz-Thouless Transition without Fine-Tuning Using a Qubit Regularization
- Absence of vortex condensation in a two dimensional fermionic XY model