Classical to quantum mapping for an unconventional phase transition in a three-dimensional classical dimer model
arXiv:0907.1564 · doi:10.1103/PhysRevB.80.134413
Abstract
We study the transition between a Coulomb phase and a dimer crystal observed in numerical simulations of the three-dimensional classical dimer model, by mapping it to a quantum model of bosons in two dimensions. The quantum phase transition that results, from a superfluid to a Mott insulator at fractional filling, belongs to a class that cannot be described within the Landau-Ginzburg-Wilson paradigm. Using a second mapping, to a dual model of vortices, we show that the long-wavelength physics near the transition is described by a U(1) gauge theory with SU(2) matter fields.
15 pages, 5 figures; v2: added appendix
References in corpus (9)
- Evidence for deconfined quantum criticality in a two-dimensional Heisenberg model with four-spin interactions
- Scaling in the Fan of an Unconventional Quantum Critical Point
- Putting competing orders in their place near the Mott transition
- A Three Dimensional Kasteleyn Transition: Spin Ice in a [100] Field
- Coulomb gas transitions in three-dimensional classical dimer models
- SU(2)-invariant continuum theory for an unconventional phase transition in a three-dimensional classical dimer model
- Classical-Quantum Mappings for Geometrically Frustrated Systems: Spin Ice in a [100] Field
- Correlations and order parameter at a Coulomb-crystal phase transition in a three-dimensional dimer model
- Critical phenomena in a highly constrained classical spin system: Neel ordering from the Coulomb phase