Three-frequency motion and chaos in the Ginzburg-Landau equation

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dc.contributor.authorMoon, Hie-Taeko
dc.contributor.authorHuerre, P.ko
dc.contributor.authorRedekopp, L. G.ko
dc.date.accessioned2013-02-27T05:28:20Z-
dc.date.available2013-02-27T05:28:20Z-
dc.date.created2012-02-06-
dc.date.created2012-02-06-
dc.date.issued1982-
dc.identifier.citationPHYSICAL REVIEW LETTERS, v.49, no.7, pp.458 - 460-
dc.identifier.issn0031-9007-
dc.identifier.urihttp://hdl.handle.net/10203/66720-
dc.description.abstractThe Ginzburg-Landau equation with periodic boundary conditions on the interval (0, 2pi/q) is integrated numerically for large times. As q is decreased, the motion in phase space exhibits a sequence of bifurcations from a limit cycle to a two-torus to a three-torus to a choatic regime. The three-torus is observed for a finite range of q and transition to chaotic flow is preceded by frequency locking.-
dc.languageEnglish-
dc.publisherAmer Physical Soc-
dc.titleThree-frequency motion and chaos in the Ginzburg-Landau equation-
dc.typeArticle-
dc.type.rimsART-
dc.citation.volume49-
dc.citation.issue7-
dc.citation.beginningpage458-
dc.citation.endingpage460-
dc.citation.publicationnamePHYSICAL REVIEW LETTERS-
dc.contributor.localauthorMoon, Hie-Tae-
dc.contributor.nonIdAuthorHuerre, P.-
dc.contributor.nonIdAuthorRedekopp, L. G.-
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