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dc.contributor.authorTsurutani, B.T.-
dc.contributor.authorDasgupta, B.-
dc.contributor.authorGalvan, C.-
dc.contributor.authorNeugebauer, M.-
dc.contributor.authorLakhina, G.S.-
dc.contributor.authorArballo, J.K.-
dc.contributor.authorWinterhalter, D.-
dc.contributor.authorGoldstein, B.E.-
dc.contributor.authorButi, B.-
dc.date.accessioned2015-08-19T11:01:51Z-
dc.date.accessioned2021-02-12T09:27:23Z-
dc.date.available2015-08-19T11:01:51Z-
dc.date.available2021-02-12T09:27:23Z-
dc.date.issued2002-
dc.identifier.citationGRL, v.29/24, p.86-1 to 86-4, 2002, doi: 10.1029/2002GL015652en_US
dc.identifier.urihttp://localhost:8080/xmlui/handle/123456789/237-
dc.description.abstract[1] Solar wind protons detected within Magnetic Holes (MHs) and Magnetic Decreases (MDs) are found to be preferentially heated perpendicular to equation image0. The MHs/MDs are associated with the phase-steepened edges of nonlinear Alfvén waves. The proton anisotropies can lead to the proton cyclotron and mirror mode plasma instabilities. We examine the Ponderomotive Force (PF), a phenomenon due to wave pressure gradients, and show that for this plasma regime and for phase-steepened Alfvén waves, the PF proton acceleration/energization will primarily be orthogonal to B0. It is suggested that accelerated ions create the MHs/MDs by a diamagnetic effect.en_US
dc.language.isoenen_US
dc.subjectAlfvén wavesen_US
dc.subjectPonderomotive forceen_US
dc.subjectMagnetic holesen_US
dc.subjectMagnetic Decreasesen_US
dc.subjectDiamagnetic effecten_US
dc.subjectInterplanetary physicsen_US
dc.titlePhase-steepened Alfvén waves, proton perpendicular energization and the creation of magnetic holes and magnetic decreases: The ponderomotive forceen_US
dc.typeArticleen_US
dc.identifier.accession090722-
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