Eastward Propagating Second Harmonic Poloidal Waves Triggered by Temporary Outward Gradient of Proton Phase Space Density: Van Allen Probe A Observation

K. Yamamoto, M. Nosé, K. Keika, D. P. Hartley, C. W. Smith, R. J. MacDowall, L. J. Lanzerotti, D. G. Mitchell, H. E. Spence, G. D. Reeves, J. R. Wygant, J. W. Bonnell, S. Oimatsu

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3 Scopus citations

Abstract

Two wave packets of second harmonic poloidal Pc 4 waves with a wave frequency of ~7 mHz were detected by Van Allen Probe A at a radial distance of ~5.8 RE and magnetic local time of 13 hr near the magnetic equator, where plasmaspheric refilling was in progress. Proton butterfly distributions with energy dispersions were also measured at the same time; the proton fluxes at 10–30 keV oscillated with the same frequency as the Pc 4 waves. Using the ion sounding technique, we find that the Pc 4 waves propagated eastward with an azimuthal wave number (m number) of ~220 and ~260 for each wave packet, respectively. Such eastward propagating high-m (m > 100) waves were seldom reported in previous studies. The condition of drift-bounce resonance is well satisfied for the estimated m numbers in both events. Proton phase space density was also examined to understand the wave excitation mechanism. We obtained temporal variations of the energy and radial gradient of the proton phase space density and find that temporal intensification of the radial gradient can generate the two wave packets. The cold electron density around the spacecraft apogee was >100 cm−3 in the present events, and hence the eigenfrequency of the Pc 4 waves became lower. This causes the increase of the m number which satisfies the resonance condition of drift-bounce resonance for 10–30 keV protons and meets the condition for destabilization due to gyrokinetic effect.

Original languageEnglish (US)
Pages (from-to)9904-9923
Number of pages20
JournalJournal of Geophysical Research: Space Physics
Volume124
Issue number12
DOIs
StatePublished - Dec 1 2019

Bibliographical note

Funding Information:
All Van Allen Probes data used in this study are publicly available at following sources: EMFISIS ( https://emfisis.physics.uiowa.edu/ ); EFW ( http://www.space.umn.edu/missions/rbspefw‐home‐university‐of‐minnesota/ ); RBSPICE ( http://rbspice.ftecs.com/ ); ETC/HOPE ( http://www.RBSP‐ect.lanl.gov/ ). Processing and analysis of the HOPE data was supported by Energetic Particle, Composition, and Thermal Plasma (RBSP‐ECT) investigation funded under NASA's Prime contract no. NAS5‐01072. The SYM‐H index is provided by the World Data Center for Geomagnetism, Kyoto, and is available at their website ( http://wdc.kugi.kyoto‐u.ac.jp ). The OMNI data are obtained from OMNIWeb ( https://omniweb.gsfc.nasa.gov/html/ow_data.html ). The Kp index is provided by GeoForschungsZentrum (GFZ) Potsdam and is available at their website ( https://www.gfz‐potsdam.de/kp‐index ). This study is supported by Japan Society for the Promotion of Science (JSPS) (19J14222), Grants‐in‐Aid for Scientific Research (B) (16H04057), Challenging Research (Pioneering) (17K18804), and Grants‐in‐Aid for Specially Promoted Research (16H06286). Work at NJIT was supported by JHU/APL subcontract 131803 under NASA Prime contract NNN06AA01C.Work at APL was supported under JHU/APL Subcontract 937836 to the New Jersey Institute of Technology under NASA Prime Contract NAS5‐01072. Work at Iowa was performed under the support of JHU/APL contract 921647 under NASA Prime contract NAS5‐01072.

Keywords

  • ULF wave
  • drift-bounce resonance
  • geomagnetic storm
  • plasmasphere
  • ring current
  • substorm

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