日本地球惑星科学連合2023年大会

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[E] 口頭発表

セッション記号 P (宇宙惑星科学) » P-EM 太陽地球系科学・宇宙電磁気学・宇宙環境

[P-EM13] Dynamics of the Inner Magnetospheric System

2023年5月23日(火) 15:30 〜 16:45 101 (幕張メッセ国際会議場)

コンビーナ:桂華 邦裕(東京大学大学院理学系研究科地球惑星科学専攻)、三好 由純(名古屋大学宇宙地球環境研究所)、Theodore E Sarris(Democritus University of Thrace)、Evan G Thomas(Dartmouth College)、座長:中村 紗都子(名古屋大学宇宙地球環境研究所)、松田 昇也(金沢大学)、山本 和弘(東京大学理学研究科)、三好 由純(名古屋大学宇宙地球環境研究所)、桂華 邦裕(東京大学大学院理学系研究科地球惑星科学専攻)

16:10 〜 16:25

[PEM13-11] Do the EMIC waves really heat thermal ions in the plasmasphere?

*小路 真史1三好 由純1Lynn Kistler2浅村 和史3笠羽 康正4松岡 彩子6笠原 禎也5松田 昇也5土屋 史紀4熊本 篤志4中村 紗都子1Jun Chae-Woo1篠原 育3 (1.名古屋大学宇宙地球環境研究所、2.ニューハンプシャー大学、3.宇宙科学研究所、4.東北大学、5.金沢大学、6.京都大学)

キーワード:イオン加熱、EMIC波

Electromagnetic ion cyclotron (EMIC) waves are generated through the cyclotron wave-particle interaction, affecting the plasma environment in the magnetosphere. Heating of the ions by EMIC waves in the inner magnetosphere has also been investigated by spacecraft observations by comparing variations of ion distribution and waves. The energy transfer between the plasma waves and ions can be quantitatively evaluated by calculating the inner product between the wave electric field vector and the ion velocity vector, so-called WPIA (wave-particle interaction analysis). We adapt the WPIA method to the Arase spacecraft data and investigate the statistical results of the WPIA and the spatial distribution of the positive qV・E region in the inner magnetosphere. Using 4.5 years data, we choose EMIC wave events associating proton or helium flux enhancements of which the WPIA analysis can be applied for the necessary data sets observed by the Arase satellite. The energization of proton occurs over wide conditions, while the strongest energization of proton appears at Kp = 0 with the energy around 10 eV. On the other hand, the helium heating takes place at higher Kp>4 and with higher energy of the helium (>~ 100 eV). In the low Kp case, the energization of the helium is weak. In the magnetosphere, the occurrence peaks of the proton heating events appear in the dayside and post noon regions. In the higher Kp case, we find the occurrence peaks of heating of both proton and helium close to the Earth, around L=3-4 while in the smaller Kp case, the peaks appear around the noon and dusk side. Comparing the possible theoretical mechanisms of the ion flux enhancement, we conclude that the contribution of the EMIC heating to the warm plasma inside the plasmasphere is not significant.