日本地球惑星科学連合2015年大会

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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-EM26] 宇宙プラズマ理論・シミュレーション

2015年5月24日(日) 11:00 〜 12:45 302 (3F)

コンビーナ:*梅田 隆行(名古屋大学 太陽地球環境研究所)、天野 孝伸(東京大学 地球惑星科学専攻)、成行 泰裕(富山大学人間発達科学部)、杉山 徹(独立行政法人海洋研究開発機構 地球情報基盤センター)、中村 匡(福井県立大学)、座長:中村 匡(福井県立大学)、小路 真史(名古屋大学太陽地球環境研究所)

11:15 〜 11:30

[PEM26-09] コーラス放射発生過程の高エネルギー電子の温度異方性に対する依存性について

*加藤 雄人1大村 善治2三宅 洋平3臼井 英之3中島 浩4 (1.東北大学大学院理学研究科、2.京都大学生存圏研究所、3.神戸大学大学院システム情報学研究科、4.京都大学学術情報メディアセンター)

By a series of electron hybrid simulations, we study dependencies of the generation process of whistler-mode chorus and hiss-like emissions on temperature anisotropy of energetic electrons.
Whistler-mode chorus emissions are electromagnetic plasma waves commonly observed in planetary magnetospheres. In the Earth's inner magnetosphere, chorus emissions are observed mostly on the dawn side and are enhanced during geomagnetically disturbed periods. Chorus emissions appear in the typical frequency range from 0.2 to 0.8 fce0 with a gap at the half fce0, where fce0 represents the electron gyrofrequency at the magnetic equator. Recent in situ observation in the magnetosphere revealed the presence of whistler-mode hiss-like emissions, whose wave amplitude is comparable to those of chorus emissions.
The generation process of chorus has been reproduced in electron hybrid simulations and has been explained by the nonlinear wave growth theory [see review by Omura et al., in AGU Monograph "Dynamics of the Earth's Radiation Belts and Inner Magnetosphere, 2012]. The generation mechanism of hiss-like emissions is also explained by the nonlinear wave growth theory and has been reproduced by simulations [Katoh and Omura, JGR 2013]. In the present study, by an improved electron hybrid code with OhHelp library [Nakashima et al., 2009], we conduct a series of electron hybrid simulations for different temperature anisotropy (AT) of the initial velocity distribution function of energetic electrons. We vary AT in the range from 3 to 9 with changing the number density of energetic electrons (Nh) so as to study whether distinct rising-tone chorus emissions are reproduced or not in the assumed initial condition. Based on the simulation results, we reveal properties of the chorus generation for the assumed AT parameter range.