Ground states of hard-core bosons in one dimensional periodic potentials
arXiv:cond-mat/0612544 · doi:10.1103/PhysRevA.75.023613
Abstract
With Girardeau's Fermi-Bose mapping, we find the exact ground states of hard-core bosons residing in a one dimensional periodic potential. The analysis of these ground states shows that when the number of bosons is commensurate with the number of wells in the periodic potential, the boson system is a Mott insulator whose energy gap, however, is given by the single-particle band gap of the periodic potential; when is not commensurate with , the system is a metal (not a superfluid). In fact, we argue that there may be no superfluid phase for any one-dimensional boson system in terms of Landau's criterion of superfluidity. The Kronig-Penney potential is used to illustrate our results.
6 pages, 6 figures
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- Optical lattices as a tool to study defect-induced superfluidity
- Low-energy excitations of a boson pair in a double-well trap
- The single-particle density matrix and the momentum distribution of dark "solitons" in a Tonks-Girardeau gas
- Ground state properties of a Tonks-Girardeau Gas in a periodic potential
- Spin-flip induced superfluidity in a ring of spinful hard-core bosons
- One Dimensional Magnetized TG Gas Properties in an External Magnetic Field
- Probing the thermal atoms of a Bose gas through Raman transition