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Foreshock wave interaction with the magnetopause: Signatures of mode conversion


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dc.contributorLin Y, ylin@physics.auburn.eduen_US
dc.creatorFeng, Shi
dc.creatorCheng, Lei
dc.creatorLin, Yu
dc.creatorWang, Xueyi
dc.date.accessioned2022-09-30T13:28:12Z
dc.date.available2022-09-30T13:28:12Z
dc.date.created2017
dc.identifier10.1002/2016JA023114en_US
dc.identifier.urihttps://agupubs.onlinelibrary.wiley.com/doi/full/10.1002/2014JA020005en_US
dc.identifier.urihttps://aurora.auburn.edu/handle/11200/50371
dc.identifier.urihttp://dx.doi.org/10.35099/aurora-439
dc.description.abstractOur previous hybrid simulation (Shi et al., 2013) under a radial interplanetary magnetic field (IMF) and a supercritical solar wind Mach number has shown that foreshock compressional waves originated from the quasi-parallel (Q-parallel to) shock are mode converted to kinetic Alfven waves (KAWs) at the Alfven resonance surface of the subsolar magnetopause. In this paper, three-dimensional global dayside mode conversion is investigated for cases under various solar wind conditions using the global hybrid model. The global patterns and propagations of KAWs are distinguished and presented. Under a near-critical Mach number (M-A = 3), KAW structures due to mode conversion exhibit a feature of broader excitation regions in the magnetopause boundary layer (MPBL) compared to supercritical Mach number (M-A = 5) shocks. For cases with an oblique IMF with supercritical Mach numbers (M-A = 5), the amplitude of magnetosheath compressional waves is larger at the quasi-parallel shock (Q-parallel to) than at the quasi-perpendicular (Q-perpendicular to) shock. Downstream of the Q-parallel to shock, there is a general trend that the perturbations of density (N) and magnetic field (B) change from predominantly in-phase in the magnetosheath to antiphase near the MPBL. While downstream of the Q-perpendicular to shock, an antiphase relation between N and B is dominant throughout the magnetosheath and magnetopause except near the shock transition. The compressional drivers are found to reach an extended region of the magnetopause due to the combined effects of wave propagation in the plasma frame and flow convection, leading to a broad region of mode conversion at the magnetopause. Subsequently, the resulting KAWs can be carried to the regions downstream of the Q-perpendicular to shock owing to the flow convection at the magnetopause. The KAWs propagate poleward along the geomagnetic field lines and meanwhile are carried tailward by the ambient flows, and they are more intense in the downstream of Q-parallel to shocks than downstream of Q-perpendicular to shocks.en_US
dc.formatPDFen_US
dc.relation.ispartofseries2169-9380en_US
dc.rights©American Geophysical Union 2017. 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: Lin, Y., et al. "Investigation of storm time magnetotail and ion injection using three‐dimensional global hybrid simulation." Journal of Geophysical Research: Space Physics 119.9 (2014): 7413-7432.en_US
dc.titleForeshock wave interaction with the magnetopause: Signatures of mode conversionen_US
dc.typeTexten_US
dc.type.genreJournal Article, Academic Journalen_US
dc.citation.volume122en_US
dc.citation.issue7en_US
dc.citation.spage7057en_US
dc.citation.epage7076en_US
dc.description.statusPublisheden_US
dc.description.peerreviewYesen_US

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