TY - JOUR
T1 - Matter-wave vortices and solitons in anisotropic optical lattices
AU - Mayteevarunyoo, Thawatchai
AU - Malomed, Boris A.
AU - Baizakov, Bakhtiyor B.
AU - Salerno, Mario
N1 - Funding Information:
We appreciate discussions with J. Yang. The work of T.M. was supported, in a part, by a postdoctoral fellowship from the Pikovsky–Valazzi Foundation, by the Israel Science Foundation through the Center-of-Excellence grant No. 8006/03, and also by the Thailand Research Fund under grant No. MRG5080171. M. S. acknowledges a partial financial support from MIUR through the inter-university project PRIN-2005: “Transport properties of classical and quantum systems”. B.B.B. and B.A.M. appreciate hospitality of the Department of Physics at the University of Salerno.
PY - 2009/7/15
Y1 - 2009/7/15
N2 - Using numerical methods, we construct families of vortical, quadrupole, and fundamental solitons in a two-dimensional (2D) nonlinear-Schrödinger/Gross-Pitaevskii equation which models Bose-Einstein condensates (BECs) or photonic crystals. The equation includes the attractive or repulsive cubic nonlinearity and an anisotropic periodic potential. Two types of anisotropy are considered, accounted for by the difference in the strengths of the 1D sublattices, or by a difference in their periods. The limit case of the quasi-1D optical lattice (OL), when one sublattice is missing, is included too. By means of systematic simulations, we identify stability limits for two species of vortex solitons and quadrupoles, of the rhombus and square types. In the attraction model, rhombic vortices and quadrupoles remain stable up to the limit case of the quasi-1D lattice. In the same model, finite stability limits are found for vortices and quadrupoles of the square type, in terms of the anisotropy parameter. In the repulsion model, rhombic vortices and quadrupoles are stable in large parts of the first finite bandgap (FBG). Another species of partly stable anisotropic states is found in the second FBG, subfundamental dipoles, each squeezed into a single cell of the OL. Square-shaped quadrupoles are completely unstable in the repulsion model, while vortices of the same type are stable only in weakly anisotropic OL potentials.
AB - Using numerical methods, we construct families of vortical, quadrupole, and fundamental solitons in a two-dimensional (2D) nonlinear-Schrödinger/Gross-Pitaevskii equation which models Bose-Einstein condensates (BECs) or photonic crystals. The equation includes the attractive or repulsive cubic nonlinearity and an anisotropic periodic potential. Two types of anisotropy are considered, accounted for by the difference in the strengths of the 1D sublattices, or by a difference in their periods. The limit case of the quasi-1D optical lattice (OL), when one sublattice is missing, is included too. By means of systematic simulations, we identify stability limits for two species of vortex solitons and quadrupoles, of the rhombus and square types. In the attraction model, rhombic vortices and quadrupoles remain stable up to the limit case of the quasi-1D lattice. In the same model, finite stability limits are found for vortices and quadrupoles of the square type, in terms of the anisotropy parameter. In the repulsion model, rhombic vortices and quadrupoles are stable in large parts of the first finite bandgap (FBG). Another species of partly stable anisotropic states is found in the second FBG, subfundamental dipoles, each squeezed into a single cell of the OL. Square-shaped quadrupoles are completely unstable in the repulsion model, while vortices of the same type are stable only in weakly anisotropic OL potentials.
KW - Bose-Einstein condensate
KW - Collapse
KW - Dipole soliton
KW - Gap soliton
KW - Photonic crystal
KW - Quadrupole
KW - Rhombus vortex
KW - Square vortex
UR - http://www.scopus.com/inward/record.url?scp=67349195332&partnerID=8YFLogxK
U2 - 10.1016/j.physd.2008.07.024
DO - 10.1016/j.physd.2008.07.024
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AN - SCOPUS:67349195332
SN - 0167-2789
VL - 238
SP - 1439
EP - 1448
JO - Physica D: Nonlinear Phenomena
JF - Physica D: Nonlinear Phenomena
IS - 15
ER -