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dc.contributor.authorTsurutani, B.T.
dc.contributor.authorFalkowski, Barbara J.
dc.contributor.authorPickett, J.S.
dc.contributor.authorVerkhoglyadova, Olga P.
dc.contributor.authorSantolik, Ondrej
dc.contributor.authorLakhina, G.S.
dc.date.accessioned2015-12-03T07:15:54Z
dc.date.accessioned2021-02-12T09:33:44Z-
dc.date.available2015-12-03T07:15:54Z
dc.date.available2021-02-12T09:33:44Z-
dc.date.issued2014
dc.identifier.citationJGR, v.119/2, p.964-977, 2014, doi: 10.1002/2013JA019284en_US
dc.identifier.urihttp://localhost:8080/xmlui/handle/123456789/751-
dc.description.abstractA Polar magnetosonic wave (MSW) study was conducted using 1 year of 1996–1997 data (during solar minimum). Waves at and inside the plasmasphere were detected at all local times with a slight preference for occurrence in the midnight-postmidnight sector. Wave occurrence (and intensities) peaked within~±5° of the magnetic equator, with half maxima at ~±10°. However, MSWs were also detected as far from the equator as +20° and 60° MLAT but with lower intensities. An extreme MSW intensity event of amplitude Bw = ~± 1 nT and Ew = ~± 25 mV/m was detected. This event occurred near local midnight, at the plasmapause, at the magnetic equator, during an intense substorm event, e.g., a perfect occurrence. These results support the idea of generation by protons injected from the plasma sheet into the midnight sector magnetosphere by substorm electric fields. MSWs were also detected near noon (1259 MLT) during relative geomagnetic quiet (low AE). A possible generation mechanism is a recovering/expanding plasmasphere engulfing preexisting energetic ions, in turn leading to ion instability. The wave magnetic field components are aligned along the ambient magnetic field direction, with the wave electric components orthogonal, indicating linear wave polarization. The MSW amplitudes decreased at locations further from the magnetic equator, while transverse whistler mode wave amplitudes (hiss) increased. We argue that intense MSWs are always present somewhere in the magnetosphere during strong substorm/convection events. We thus suggest that modelers use dynamic particle tracing codes and the maximum (rather than average) wave amplitudes to simulate wave-particle interactions.en_US
dc.language.isoenen_US
dc.subjectMagnetosonic waveen_US
dc.subjectELF magnetosonic wavesen_US
dc.subjectPolar observationsen_US
dc.subjectMSWen_US
dc.titleExtremely intense ELF magnetosonic waves: A survey of polar observationsen_US
dc.typeArticleen_US
dc.identifier.accession091415
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