corner
corner

Phys. Rev. A 77, 023615 (2008) [13 pages]

Localized modes of binary mixtures of Bose-Einstein condensates in nonlinear optical lattices

Download: PDF (881 kB) Buy this article Export: BibTeX or EndNote (RIS)

F. Kh. Abdullaev1,2, A. Gammal3, M. Salerno2,4, and Lauro Tomio2
1Physical-Technical Institute of the Academy of Sciences, Tashkent, Uzbekistan
2Instituto de Física Teórica, Universidade Estadual Paulista, Rua Pamplona, 145, 01405-900, São Paulo, SP, Brazil
3Instituto de Física, Universidade de São Paulo, 05315-970, C.P. 66318, São Paulo, SP, Brazil
4Dipartimento di Fisica “E. R. Caianiello,” Consorzio Nazionale Interuniversitario per le Scienze Fisiche della Materia (CNISM), Universitá di Salerno, I-84081, Baronissi (SA), Italy

Received 2 October 2007; published 12 February 2008

The properties of the localized states of a two-component Bose-Einstein condensate confined in a nonlinear periodic potential (nonlinear optical lattice) are investigated. We discuss the existence of different types of solitons and study their stability by means of analytical and numerical approaches. The symmetry properties of the localized states with respect to nonlinear optical lattices are also investigated. We show that nonlinear optical lattices allow the existence of bright soliton modes with equal symmetry in both components and bright localized modes of mixed symmetry type, as well as dark-bright bound states and bright modes on periodic backgrounds. In spite of the quasi-one-dimensional nature of the problem, the fundamental symmetric localized modes undergo a delocalizing transition when the strength of the nonlinear optical lattice is varied. This transition is associated with the existence of an unstable solution, which exhibits a shrinking (decaying) behavior for slightly overcritical (undercritical) variations in the number of atoms.

© 2008 The American Physical Society

URL:
http://link.aps.org/doi/10.1103/PhysRevA.77.023615
DOI:
10.1103/PhysRevA.77.023615
PACS:
03.75.Lm, 05.45.Yv, 42.65.Tg, 02.30.Jr