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Cometary ion distributions near the pickup energy outside comet Halley's bow shock

dc.contributor.authorGombosi, Tamas I.en_US
dc.contributor.authorNeugebauer, Marciaen_US
dc.contributor.authorJohnstone, A. D.en_US
dc.contributor.authorCoates, A. J.en_US
dc.contributor.authorHuddleston, D. E.en_US
dc.date.accessioned2006-04-10T14:53:44Z
dc.date.available2006-04-10T14:53:44Z
dc.date.issued1991en_US
dc.identifier.citationGombosi, T. I., Neugebauer, M., Johnstone, A. D., Coates, A. J., Huddleston, D. E. (1991)."Cometary ion distributions near the pickup energy outside comet Halley's bow shock." Advances in Space Research 11(9): 275-278. <http://hdl.handle.net/2027.42/29590>en_US
dc.identifier.urihttp://www.sciencedirect.com/science/article/B6V3S-472C8N2-JX/2/18df2551866ef8f0874ebcf202977383en_US
dc.identifier.urihttps://hdl.handle.net/2027.42/29590
dc.description.abstractThis paper compares calculated and measured energy spectra of implanted H+ and O+ ions on the assumption that the pick-up geometry is quasi-parallel and about 1% of the waves generated by the cometary pickup process propagates backward (towards the comet). The model provides a good description of the implanted O+ and H+ energy distribution near the pickup energies. The thickness of the implanted ion velocity distribution shells was nearly constant between 2.50 x 106 km and 1.20 x 106 km (just outside the shock) along the inbound Giotto trajectory. The explanation is that the velocity diffusion coefficient and characteristic diffusion time vary approximately as 1/r and r, respectively, therefore their product (which determines the velocity shell thickness) remains nearly constant.en_US
dc.format.extent460004 bytes
dc.format.extent3118 bytes
dc.format.mimetypeapplication/pdf
dc.format.mimetypetext/plain
dc.language.isoen_US
dc.publisherElsevieren_US
dc.titleCometary ion distributions near the pickup energy outside comet Halley's bow shocken_US
dc.typeArticleen_US
dc.rights.robotsIndexNoFollowen_US
dc.subject.hlbsecondlevelAtmospheric, Oceanic and Space Sciencesen_US
dc.subject.hlbsecondlevelAerospace Engineeringen_US
dc.subject.hlbtoplevelScienceen_US
dc.subject.hlbtoplevelEngineeringen_US
dc.description.peerreviewedPeer Revieweden_US
dc.contributor.affiliationumSpace Physics Research Laboratory, The University of Michigan, Ann Arbor, MI 48109, U.S.A.en_US
dc.contributor.affiliationotherJet Propulsion Laboratory, California Institute of Technology, 4800 Oak Grove Drive, Pasadena, CA 91109, U.S.A.en_US
dc.contributor.affiliationotherMullard Space Science Laboratory, University College London, Holmbury St. Mary, Dorking, Surrey RH5 6NT, U.K.en_US
dc.contributor.affiliationotherMullard Space Science Laboratory, University College London, Holmbury St. Mary, Dorking, Surrey RH5 6NT, U.K.en_US
dc.contributor.affiliationotherMullard Space Science Laboratory, University College London, Holmbury St. Mary, Dorking, Surrey RH5 6NT, U.K.en_US
dc.description.bitstreamurlhttp://deepblue.lib.umich.edu/bitstream/2027.42/29590/1/0000679.pdfen_US
dc.identifier.doihttp://dx.doi.org/10.1016/0273-1177(91)90047-Nen_US
dc.identifier.sourceAdvances in Space Researchen_US
dc.owningcollnameInterdisciplinary and Peer-Reviewed


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