Thermal Phase transitions in attractive extended Bose-Hubbard Model with three-body constraint
arXiv:1101.4461 · doi:10.1103/PhysRevB.83.100511
Abstract
By means of quantum Monte Carlo simulations implemented with a two-loop update scheme, the finite-temperature phase diagram of a three-body constrained attractive Bose lattice gas is investigated. The nature of the thermal phase transitions around the dimer superfluid and the atomic superfluid is unveiled. We find that the symmetry-breaking transitions between these two superfluid phases are of first order even at nonzero temperatures. More interestingly, the thermal transition from the dimer superfluid to the normal fluid is found to be consistent with the Kosterlitz-Thouless type but giving an anomalous universal stiffness jump. It demonstrates that this transition is driven by unbinding of pairs of fractional vortices.
4.2 pages, 4 figures; minor changes, published version
References in corpus (8)
- Observation of scale invariance and universality in two-dimensional Bose gases
- Atomic three-body loss as a dynamical three-body interaction
- Topological defects and the superfluid transition of the spinor condensate in two dimensions
- Superfluidity and phase transitions in a resonant Bose gas
- Single-particle versus pair condensation of hard-core bosons with correlated hopping
- Feshbach-Einstein condensates
- Mott insulator to superfluid transition of ultracold bosons in an optical lattice near a Feshbach resonance
- Comment on "Feshbach-Einstein Condensates" by V. G. Rousseau and P. J. H. Denteneer