Two-dimensional discrete solitons in rotating lattices
arXiv:0709.3399 · doi:10.1103/PhysRevE.76.046608
Abstract
We introduce a two-dimensional (2D) discrete nonlinear Schrödinger (DNLS) equation with self-attractive cubic nonlinearity in a rotating reference frame. The model applies to a Bose-Einstein condensate stirred by a rotating strong optical lattice, or light propagation in a twisted bundle of nonlinear fibers. Two species of localized states are constructed: off-axis fundamental solitons (FSs), placed at distance from the rotation pivot, and on-axis (R=0) vortex solitons (VSs), with vorticities and 2. At a fixed value of rotation frequency , a stability interval for the FSs is found in terms of the lattice coupling constant , , with monotonically decreasing . VSs with S=1 have a stability interval, $\tilde{C}_{\mathrm{cr}%}^{(S=1)}(Ω)<C<C_{\mathrm{cr}}^{(S=1)}(Ω)$, which exists for below a certain critical value, . This implies that the VSs with S=1 are \emph{destabilized} in the weak-coupling limit by the rotation. On the contrary, VSs with S=2, that are known to be unstable in the standard DNLS equation, with , are \emph{stabilized} by the rotation in region %, with growing as a function of . Quadrupole and octupole on-axis solitons are considered too, their stability regions being weakly affected by .
To be published in Physical Review E
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