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dc.contributor.authorEbihara, Yen
dc.contributor.authorTanaka, Ten
dc.contributor.alternative海老原, 祐輔ja
dc.date.accessioned2019-03-08T01:36:31Z-
dc.date.available2019-03-08T01:36:31Z-
dc.date.issued2018-01-
dc.identifier.issn0741-3335-
dc.identifier.urihttp://hdl.handle.net/2433/237229-
dc.descriptionSpecial issue featuring the invited talks from the 44th EPS Conference on Plasma Physics, Belfast, 26-30 June 2017en
dc.description.abstractA substorm is a long-standing unsolved issue in solar-terrestrial physics. One of the big challenges is to explain reasonably the evolution of the morphological structure of the aurora associated with the substorm. The sudden appearance of a bright aurora and an auroral surge traveling westward (westward traveling surge, WTS) are noticeable features of the aurora during the substorm expansion phase. By using a global magnetohydrodynamics (MHD) simulation, we obtained the following results regarding the WTS. When the interplanetary magnetic field turns southward, a persistent dynamo appears in the cusp/mantle region, driving the two-cell magnetospheric convection. Then, the substorm growth phase begins. When magnetic reconnection takes place in the magnetotail, plasma is accelerated earthward in the plasma sheet, and accelerated toward the equatorial plane in the lobe. The second dynamo appears in the near-Earth region, which is closely associated with the generation of the field-aligned current (FAC) on the nightside. When the FAC reaches the ionosphere, the aurora becomes bright, and the onset of the expansion phase begins. In the ionosphere, the conductivity is intensified in the bright aurora due to the precipitation of accelerated electrons. The conductivity gradient gives rise to the overflow of the Hall current, which acts as the third dynamo. The overflow results in the accumulation of space charge, which causes a divergent electric field. The divergent electric field generates a thin, structured upward FAC adjacent to the bright aurora. The opposite process takes place on the opposite side of the bright aurora. In short, the upward FAC increases (appearance of aurora) at the leading edge of the surge, and decreases (disappearance of aurora) at the trailing edge of the surge. By repeating these processes, the surge seems to travel westward.en
dc.format.mimetypeapplication/pdf-
dc.language.isoeng-
dc.publisherIOP Publishingen
dc.rightsThis is an author-created, un-copyedited version of an article accepted for publication in Plasma Physics and Controlled Fusion. The publisher is not responsible for any errors or omissions in this version of the manuscript or any version derived from it. The Version of Record is available online at https://orcid.org/0000-0002-2293-1557.en
dc.rightsThis is not the published version. Please cite only the published version.en
dc.rightsこの論文は出版社版でありません。引用の際には出版社版をご確認ご利用ください。ja
dc.titleWhy does substorm-associated auroral surge travel westward?en
dc.typejournal article-
dc.type.niitypeJournal Article-
dc.identifier.jtitlePlasma Physics and Controlled Fusionen
dc.identifier.volume60-
dc.identifier.issue1-
dc.relation.doi10.1088/1361-6587/aa89fd-
dc.textversionauthor-
dc.identifier.artnum14024-
dc.addressRISH, Kyoto Universityen
dc.addressICSWSE, Kyushu Universityen
dcterms.accessRightsopen access-
datacite.awardNumber15H03732-
datacite.awardNumber15H05815-
jpcoar.funderName日本学術振興会ja
jpcoar.funderName日本学術振興会ja
jpcoar.funderName.alternativeJapan Society for the Promotion of Science (JSPS)en
jpcoar.funderName.alternativeJapan Society for the Promotion of Science (JSPS)en
出現コレクション:学術雑誌掲載論文等

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