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dc.contributor.authorMartel, Yvan
dc.contributor.authorPilod, Didier Jacques Francois
dc.date.accessioned2021-08-06T11:33:53Z
dc.date.available2021-08-06T11:33:53Z
dc.date.created2020-09-16T11:54:58Z
dc.date.issued2020
dc.identifier.issn0010-3616
dc.identifier.urihttps://hdl.handle.net/11250/2766804
dc.description.abstractFor the critical generalized KdV equation ∂tu+∂x(∂2xu+u5)=0 on R, we construct a full family of flattening solitary wave solutions. Let Q be the unique even positive solution of Q′′+Q5=Q. For any ν∈(0,13), there exist global (for t≥0) solutions of the equation with the asymptotic behavior u(t,x)=t−ν2Q(t−ν(x−x(t)))+w(t,x) where, for some c>0, x(t)∼ct1−2ν and ∥w(t)∥H1(x>12x(t))→0 as t→+∞. Moreover, the initial data for such solutions can be taken arbitrarily close to a solitary wave in the energy space. The long-time flattening of the solitary wave is forced by a slowly decaying tail in the initial data. This result and its proof are inspired and complement recent blow-up results for the critical generalized KdV equation. This article is also motivated by previous constructions of exotic behaviors close to solitons for other nonlinear dispersive equations such as the energy-critical wave equation.en_US
dc.language.isoengen_US
dc.publisherSpringeren_US
dc.rightsNavngivelse 4.0 Internasjonal*
dc.rights.urihttp://creativecommons.org/licenses/by/4.0/deed.no*
dc.titleFull family of flattening solitary waves for the critical generalized KdV equationen_US
dc.typeJournal articleen_US
dc.typePeer revieweden_US
dc.description.versionpublishedVersionen_US
dc.rights.holderCopyright 2020 The Authorsen_US
cristin.ispublishedtrue
cristin.fulltextoriginal
cristin.qualitycode2
dc.identifier.doi10.1007/s00220-020-03815-z
dc.identifier.cristin1830389
dc.source.journalCommunications in Mathematical Physicsen_US
dc.source.pagenumber1011-1080en_US
dc.identifier.citationCommunications in Mathematical Physics. 2020, 378, 1011-1080.en_US
dc.source.volume378en_US


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