Strongly Interacting Atom Lasers in Three Dimensional Optical Lattices
arXiv:1010.5553 · doi:10.1103/PhysRevLett.105.180401
Abstract
We show that the dynamical melting of a Mott insulator in a three-dimensional lattice leads to condensation at nonzero momenta, a phenomenon that can be used to generate strongly interacting atom lasers in optical lattices. For infinite onsite repulsion, the case considered here, the momenta at which bosons condense is determined analytically and found to have a simple dependence on the hopping amplitudes. The occupation of the condensates is shown to scale linearly with the total number of atoms in the initial Mott insulator. Our results are obtained using a Gutzwiller-type mean-field approach, gauged against exact diagonalization solutions of small systems.
8 pages, 9 figures
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Cited by in corpus (14)
- Expansion dynamics of interacting bosons in homogeneous lattices in one and two dimensions
- Dynamical Quasicondensation of Hard-Core Bosons at Finite Momenta
- Sudden expansion of Mott insulators in one dimension
- Non-Equilibrium Mass Transport in the 1D Fermi-Hubbard Model
- Expansion of one-dimensional lattice hard-core bosons at finite temperature
- Expansion velocity of a one-dimensional, two-component Fermi gas during the sudden expansion in the ballistic regime
- Expansion of Bose-Hubbard Mott insulators in optical lattices
- Rigorous mean-field dynamics of lattice bosons: Quenches from the Mott insulator
- Finite-momentum Bose-Einstein condensates in shaken 2D square optical lattices
- Sudden expansion and domain-wall melting of strongly interacting bosons in two-dimensional optical lattices and on multileg ladders
- Self trapping in the two-dimensional Bose-Hubbard model
- Finite Temperature Phase Transition in a Cross-Dimensional Triangular Lattice
- Realizable Quantum Adiabatic Search
- Efficiency of fermionic quantum distillation