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dc.contributor.authorAblowitz, M. J.en
dc.contributor.authorNixon, S. D.en
dc.contributor.authorHorikis, T. P.en
dc.contributor.authorFrantzeskakis, D. J.en
dc.date.accessioned2015-11-24T17:27:32Z-
dc.date.available2015-11-24T17:27:32Z-
dc.identifier.issn1364-5021-
dc.identifier.urihttps://olympias.lib.uoi.gr/jspui/handle/123456789/13399-
dc.rightsDefault Licence-
dc.subjectperturbation theoryen
dc.subjectsolitonsen
dc.subjectopticsen
dc.subjectsquared jost solutionsen
dc.subjectoptical fibersen
dc.subjectcomplete seten
dc.subjectpropagationen
dc.subjectdynamicsen
dc.titlePerturbations of dark solitonsen
heal.typejournalArticle-
heal.type.enJournal articleen
heal.type.elΆρθρο Περιοδικούel
heal.identifier.primaryDOI 10.1098/rspa.2010.0663-
heal.identifier.secondary<Go to ISI>://000293168300010-
heal.identifier.secondaryhttp://rspa.royalsocietypublishing.org/content/467/2133/2597-
heal.languageen-
heal.accesscampus-
heal.recordProviderΠανεπιστήμιο Ιωαννίνων. Σχολή Θετικών Επιστημών. Τμήμα Μαθηματικώνel
heal.publicationDate2011-
heal.abstractA direct perturbation method for approximating dark soliton solutions of the nonlinear Schrodinger (NLS) equation under the influence of perturbations is presented. The problem is broken into an inner region, where the core of the soliton resides, and an outer region, which evolves independently of the soliton. It is shown that a shelf develops around the soliton that propagates with speed determined by the background intensity. Integral relations obtained from the conservation laws of the NLS equation are used to determine the properties of the shelf. The analysis is developed for both constant and slowly evolving backgrounds. A number of problems are investigated, including linear and nonlinear damping type perturbations.en
heal.publisherThe Royal Societyen
heal.journalNameProceedings of the Royal Society a-Mathematical Physical and Engineering Sciencesen
heal.journalTypepeer reviewed-
heal.fullTextAvailabilityTRUE-
Appears in Collections:Άρθρα σε επιστημονικά περιοδικά ( Ανοικτά). ΜΑΘ

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