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Hall effect control of magnetotail dawn-dusk asymmetry: A three-dimensional global hybrid simulation


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dc.creatorLu, San
dc.creatorLin, Y.
dc.creatorAngelopoulos, V
dc.creatorArtemyev, A
dc.creatorPritchett, P
dc.creatorLu, Quanming
dc.creatorWang, X
dc.date.accessioned2022-10-27T19:13:50Z
dc.date.available2022-10-27T19:13:50Z
dc.date.created2016
dc.identifier10.1002/2016JA023325en_US
dc.identifier.urihttps://agupubs.onlinelibrary.wiley.com/doi/full/10.1002/2016JA023325en_US
dc.identifier.urihttps://aurora.auburn.edu/handle/11200/50435
dc.identifier.urihttp://dx.doi.org/10.35099/aurora-503
dc.description.abstractMagnetotail reconnection and related phenomena (e.g., flux ropes, dipolarizing flux bundles, flow bursts, and particle injections) occur more frequently on the duskside than on the dawnside. Because this asymmetry can directly result in dawn-dusk asymmetric space weather effects, uncovering its physical origin is important for better understanding, modeling, and prediction of the space weather phenomena. However, the cause of this pervasive asymmetry is unclear. Using three-dimensional global hybrid simulations, we demonstrate that the Hall physics in the magnetotail current sheet is responsible for the asymmetry. The current sheet thins progressively under enhanced global convection; when its thickness reaches ion kinetic scales, some ions are decoupled from the magnetized electrons (the Hall effect). The resultant Hall electric field E-z is directed toward the neutral plane. The Hall effect is stronger (grows faster) on the duskside; i.e., more ions become unmagnetized there and do not comove with the magnetized dawnward E-z x B-x drifting electrons, thus creating a larger additional cross-tail current intensity j(y) (in addition to the diamagnetic current) on the duskside, compared to the dawnside. The stronger Hall effect strength on the duskside is controlled by the higher ion temperature, thinner current sheet, and smaller normal magnetic field B-z there. These asymmetric current sheet properties are in turn controlled by two competing processes that correspond to the Hall effect: (1) the dawnward E x B drift of the magnetic flux and magnetized ions and electrons and (2) the transient motion of the unmagnetized ions which do not execute E x B drift.en_US
dc.formatPDFen_US
dc.publisherAmerican Geophysical Unionen_US
dc.relation.ispartofJOURNAL OF GEOPHYSICAL RESEARCH-SPACE PHYSICSen_US
dc.relation.ispartofseries2169-9380en_US
dc.rights©American Geophysical Union 2016. This is this the version of record co-published by the American Geophysical Union and John Wiley & Sons, Inc. It is made available under the CC-BY-NC-ND 4.0 license. Item should be cited as: Lu, S., Lin, Y., Angelopoulos, V., Artemyev, A. V., Pritchett, P. L., Lu, Q., & Wang, X. Y. (2016). Hall effect control of magnetotail dawn‐dusk asymmetry: A three‐dimensional global hybrid simulation. Journal of Geophysical Research: Space Physics, 121(12), 11-882.en_US
dc.titleHall effect control of magnetotail dawn-dusk asymmetry: A three-dimensional global hybrid simulationen_US
dc.typeTexten_US
dc.type.genreJournal Article, Academic Journalen_US
dc.citation.volume121en_US
dc.citation.issue12en_US
dc.citation.spage11882en_US
dc.citation.epage11895en_US
dc.description.statusPublisheden_US
dc.description.peerreviewYesen_US
dc.creator.orcid0000-0003-3041-2682en_US
dc.creator.orcid0000-0003-2085-1171en_US

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