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dc.contributor.authorButi, B.
dc.contributor.authorJayanti, V.
dc.contributor.authorViñas, A.F.
dc.contributor.authorGhosh, S.
dc.contributor.authorGoldstein, M.L.
dc.contributor.authorRoelandts, D.A.
dc.contributor.authorLakhina, G.S.
dc.contributor.authorTsurutani, B.T.
dc.date.accessioned2015-09-29T11:40:27Z
dc.date.accessioned2021-02-12T09:30:11Z-
dc.date.available2015-09-29T11:40:27Z
dc.date.available2021-02-12T09:30:11Z-
dc.date.issued1998
dc.identifier.citationGeophysical Research Letters, v.25/13, p.2377-2380, 1998, doi: 10.1029/98GL01688en_US
dc.identifier.urihttp://localhost:8080/xmlui/handle/123456789/514-
dc.description.abstractAlfvén waves are a ubiquitous feature of the solar wind. One approach to studying the evolution of such waves has been to study exact solutions to approximate evolution equations. Here we compare soliton solutions of the Derivative Nonlinear Schrödinger evolution equation (DNLS) to solutions of the compressible MHD equations. We find that the soliton solutions of the DNLS equation are not stable solutions of Hall-MHD—they evolve and dissipate with time. Although such solitons may serve as approximate initial conditions to the Hall-MHD equations, they are not stationary solutions. This may account for the absence of soliton-like wave forms in the free-flowing solar wind.en_US
dc.language.isoenen_US
dc.subjectAlfvén wavesen_US
dc.subjectSolar winden_US
dc.subjectDNLSen_US
dc.titleNonlinear evolution of Alfvénic wave packetsen_US
dc.typeArticleen_US
dc.identifier.accession091026
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