Quasiequilibrium Mixture of Itinerant and Localized Bose Atoms in Optical Lattice
arXiv:1101.0499 · doi:10.1134/S1054660X11010233
Abstract
Conditions are studied under which there can exist a quasiequilibrium mixture of itinerant and localized bosonic atoms in an optical lattice, even at zero temperature and at integer filling factor, when such a coexistence is impossible for an equilibrium lattice. The consideration is based on a model having the structure of a two-band, or two-component, boson Hubbard Hamiltonian. The minimal value for the ratio of on-site repulsion to tunneling parameter, necessary for the occurrence of such a mixture, is found.
Latex file, 15 pages, one figure
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Cited by in corpus (10)
- Difference in Bose-Einstein condensation of conserved and unconserved particles
- Macroscopic properties of triplon Bose-Einstein condensates
- Bose - Einstein condensation of triplons with a weakly broken U(1) symmetry
- Critical temperature of noninteracting bosonic gases in cubic optical lattices at arbitrary integer fillings
- Tunneling of polarized fermions in 3D double wells
- Phase Transitions in Three-Dimensional Bosonic Systems in Optical Lattices
- Optical lattice with heterogeneous atomic density
- Photonic spectral density of coupled microwave cavities
- Hugenholtz -- Pines relations and the critical temperature of a Rabi coupled binary Bose system
- Dynamical entanglement in coupled optical cavities