Strongly interacting one-dimensional bosons in arbitrary-strength optical lattices: from Bose-Hubbard to sine-Gordon and beyond
arXiv:1112.3657 · doi:10.1103/PhysRevA.85.063621
Abstract
We analyze interacting one-dimensional bosons in the continuum, subject to a periodic sinusoidal potential of arbitrary depth. Variation of the lattice depth tunes the system from the Bose-Hubbard limit for deep lattices, through the sine-Gordon regime of weak lattices, to the complete absence of a lattice. Using the Bose-Fermi mapping between strongly interacting bosons and weakly interacting fermions, we derive the phase diagram in the parameter space of lattice depth and chemical potential. This extends previous knowledge from tight-binding (Bose-Hubbard) studies in a new direction which is important because the lattice depth is a readily adjustable experimental parameter. Several other results (equations of state, energy gaps, profiles in harmonic trap) are presented as corollaries to the physics contained in this phase diagram. Generically, both incompressible (gapped) and compressible phases coexist in a trap; this has implications for experimental measurements.
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Cited by in corpus (7)
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- Static and dynamic phases of a Tonks-Girardeau gas in an optical lattice
- A continuous model for bosonic hard spheres in quasi one-dimensional optical lattices
- Zero-temperature phase diagram of hard sphere bosons in asymmetric three dimensional optical lattices
- Quasi-superfluid and Quasi-Mott phases of strongly interacting bosons in shallow optical lattice
- One-Dimensional Quench Dynamics in an Optical Lattice: sine-Gordon and Bose-Hubbard Descriptions