4 years ago

Dipolar bright solitons and solitary vortices in a radial lattice.

Chunqing Huang, Yongyao Li, Haishu Tan, Boris A. Malomed, Shenhe Fu, Hao Huang, Zhaopin Chen, Lin Lyu

Stabilizing vortex solitons with high values of the topological charge, S, is a challenging issue in optics, studies of Bose-Einstein condensates (BECs) and other fields. To develop a new approach to the solution of this problem, we consider a two-dimensional dipolar BEC under the action of an axisymmetric radially periodic lattice potential, $V(r)\sim \cos (2r+\delta )$, with dipole moments polarized perpendicular to the system's plane, which gives rise to isotropic repulsive dipole-dipole interactions (DDIs). Two radial lattices are considered, with $\delta =0$ and $\pi $, i.e., a potential maximum or minimum at $r=0$, respectively. Families of vortex gapsoliton (GSs) with $S=1$ and $S\geq 2$, the latter ones often being unstable in other settings, are completely stable in the present system (at least, up to $S=11$), being trapped in different annular troughs of the radial potential. The vortex solitons with different $S$ may stably coexist in sufficiently far separated troughs. Fundamental GSs, with $S=0$, are found too. In the case of $\delta =0$, the fundamental solitons are ring-shaped modes, with a local minimum at $r=0.$At $\delta =\pi $, they place a density peak at the center.

Publisher URL: http://arxiv.org/abs/1708.02011

DOI: arXiv:1708.02011v2

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