Dipolar Bose-Einstein condensate soliton on a two-dimensional optical lattice
arXiv:1205.5115 · doi:10.1016/j.physleta.2012.05.030
Abstract
Using a three-dimensional mean-field model we study one-dimensional dipolar Bose-Einstein condensate (BEC) solitons on a weak two-dimensional (2D) square and triangular optical lattice (OL) potentials placed perpendicular to the polarization direction. The stabilization against collapse and expansion of these solitons for a fixed dipolar interaction and a fixed number of atoms is possible for short-range atomic interaction lying between two critical limits. The solitons collapse below the lower limit and escapes to infinity above the upper limit. One can also stabilize identical tiny BEC solitons arranged on the 2D square OL sites forming a stable 2D array of interacting droplets when the OL sites are filled with a filling factor of 1/2 or less. Such an array is unstable when the filling factor is made more than 1/2 by occupying two adjacent sites of OL. These stable 2D arrays of dipolar superfluid BEC solitons are quite similar to the recently studied dipolar Mott insulator states on 2D lattice in the Bose-Hubbard model by Capogrosso-Sansone et al. [B. Capogrosso-Sansone, C. Trefzger, M. Lewenstein, P. Zoller, G. Pupillo, Phys. Rev. Lett. 104 (2010) 125301].
8 pages, 5 figures and 2 tables
References in corpus (8)
- Ultracold atomic gases in optical lattices: mimicking condensed matter physics and beyond
- Strong dipolar effects in a quantum ferrofluid
- Stabilizing a purely dipolar quantum gas against collapse
- d-wave collapse and explosion of a dipolar Bose-Einstein condensate
- Anisotropic solitons in dipolar Bose-Einstein Condensates
- Comparing contact and dipolar interaction in a Bose-Einstein condensate
- Dysprosium magneto-optical traps
- Structure formation during the collapse of a dipolar atomic Bose-Einstein condensate