Condensation of a Hard-Core Bose Gas
arXiv:cond-mat/0001074 · doi:10.1103/PhysRevA.62.023611
Abstract
A grand canonical system of hard-core bosons, subject to thermal fluctuations, is studied on a lattice. Starting from the slave-boson representation with fields for occupied and unoccupied sites, an effective field theory is derived in which a complex field corresponds with the order parameter of the condensate and a real field with the total density of bosons. Near the boundary between the normal and the superfluid phase we obtain the Ginzburg-Landau functional for the superfluid order parameter. A mean-field calculation shows that the critical temperature increases with increasing density up to a maximum and decreases with further increasing density.
10 pages, 3 figures, submitted to Phys. Rev. A
References in corpus (1)
Cited by in corpus (5)
- Interacting bosons in an optical lattice
- Slave particle approach to the finite temperature properties of ultracold Bose gases in optical lattices
- A renormalized Gross-Pitaevskii Theory and vortices in a strongly interacting Bose gas
- Formation of vortices in a dense Bose-Einstein condensate
- Superfluid transition temperature from the Lindemann-like criterion