SM41E-2537
Generation mechanism of L-value dependence of oxygen flux enhancements during substorms

Thursday, 17 December 2015
Poster Hall (Moscone South)
Yohei Nakayama1, Yusuke Ebihara1, Takashi Tanaka2, Shinichi Ohtani3, Matina Gkioulidou3, Kazue Takahashi3, Lynn M Kistler4 and Craig Kletzing5, (1)Kyoto University, Kyoto, Japan, (2)Kyushu University, Fukuoka, Japan, (3)Applied Physics Laboratory Johns Hopkins, Laurel, MD, United States, (4)University of New Hampshire Main Campus, Durham, NH, United States, (5)University of Iowa, Iowa City, IA, United States
Abstract:
The Van Allen Probes Helium Oxygen Proton Electron (HOPE) instrument measures charged particles with an energy range from ~eV to ~ tens of keV. The observation shows that the energy flux of the particles increases inside the geosynchronous orbit during substorms. For some night-side events around the apogee, the energy flux of O+ ion enhances below ~10 keV at lower L shell, whereas the flux below ~8 keV sharply decreases at higher L shells. This structure of L-energy spectrogram of flux is observed only for the O+ ions. The purpose of this study is to investigate the generation mechanism of the structure by using numerical simulations.

We utilized the global MHD simulation developed by Tanaka et al (2010, JGR) to simulate the electric and magnetic fields during substorms. We performed test particle simulation under the electric and magnetic fields by applying the same model introduced by Nakayama et al. (2015, JGR). In the test particle simulation each test particle carries the real number of particles in accordance with the Liouville theorem. Using the real number of particles, we reconstructed 6-dimensional phase space density and differential flux of O+ ions in the inner magnetosphere.

We obtained the following results. (1) Just after the substorm onset, the dawn-to-dusk electric field is enhanced to ~ 20 mV/m in the night side tail region at L > 7. (2) The O+ ions are accelerated and transported to the inner region (L > ~5.5) by the large-amplitude electric field. (3) The reconstructed L-energy spectrogram shows a similar structure to the Van Allen Probes observation. (4) The difference in the flux enhancement between at lower L shell and higher L shells is due to two distinct acceleration processes: adiabatic and non-adiabatic. We will discuss the relationship between the particle acceleration and the structure of L-energy spectrogram of flux enhancement in detail.