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dc.creatorGligorić, Goran
dc.creatorMaluckov, Aleksandra
dc.creatorSalasnich, L.
dc.creatorMalomed, B. A.
dc.creatorHadžievski, Ljupčo
dc.date.accessioned2018-03-01T21:02:01Z
dc.date.available2018-03-01T21:02:01Z
dc.date.issued2009
dc.identifier.issn1054-1500 (print)
dc.identifier.urihttp://vinar.vin.bg.ac.rs/handle/123456789/3866
dc.description.abstractThe Bose-Einstein condensate (BEC), confined in a combination of the cigar-shaped trap and axial optical lattice, is studied in the framework of two models described by two versions of the one-dimensional (1D) discrete nonpolynomial Schrodinger equation (NPSE). Both models are derived from the three-dimensional Gross-Pitaevskii equation (3D GPE). To produce model 1 (which was derived in recent works), the 3D GPE is first reduced to the 1D continual NPSE, which is subsequently discretized. Model 2, which was not considered before, is derived by first discretizing the 3D GPE, which is followed by the reduction in the dimension. The two models seem very different; in particular, model 1 is represented by a single discrete equation for the 1D wave function, while model 2 includes an additional equation for the transverse width. Nevertheless, numerical analyses show similar behaviors of fundamental unstaggered solitons in both systems, as concerns their existence region and stability limits. Both models admit the collapse of the localized modes, reproducing the fundamental property of the self-attractive BEC confined in tight traps. Thus, we conclude that the fundamental properties of discrete solitons predicted for the strongly trapped self-attracting BEC are reliable, as the two distinct models produce them in a nearly identical form. However, a difference between the models is found too, as strongly pinned (very narrow) discrete solitons, which were previously found in model 1, are not generated by model 2-in fact, in agreement with the continual 1D NPSE, which does not have such solutions either. In that respect, the newly derived model provides for a more accurate approximation for the trapped BEC. (C) 2009 American Institute of Physics. [doi: 10.1063/1.3248269]en
dc.relationMinistry of Science, Serbia [141034], CARIPARO Foundation through Progetti di Eccellenza 2006., German-Israel Foundation [149/2006]
dc.rightsclosedAccessen
dc.sourceChaosen
dc.titleTwo routes to the one-dimensional discrete nonpolynomial Schrodinger equationen
dc.typearticleen
dcterms.abstractСаласницх, Л.; Маломед, Б. A.; Глигорић Горан; Малуцков Aлександра; Хаджиевски Љупчо;
dc.citation.volume19
dc.citation.issue4
dc.identifier.wos000273221500006
dc.identifier.doi10.1063/1.3248269
dc.citation.otherArticle Number: 043105
dc.citation.rankM21a
dc.identifier.pmid20059201
dc.identifier.scopus2-s2.0-74349123035


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