日本地球惑星科学連合2016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-EM17] 宇宙プラズマ理論・シミュレーション

2016年5月24日(火) 15:30 〜 17:00 302 (3F)

コンビーナ:*梅田 隆行(名古屋大学 宇宙地球環境研究所)、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)、中村 匡(福井県立大学)、杉山 徹(国立研究開発法人海洋研究開発機構 地球情報基盤センター)、座長:簑島 敬(海洋研究開発機構 数理科学・先端技術研究分野)、松本 洋介(千葉大学大学院理学研究科)

15:30 〜 15:45

[PEM17-07] 実験室宇宙物理学における協同トムソン散乱計測に向けた数値実験

*松清 修一1潮崎 幸太1香月 のどか1坂和 洋一2富田 健太郎1森田 太智1佐野 孝好2蔵満 康浩3山崎 了4羽田 亨1 (1.九州大学、2.大阪大学、3.国立中央大学、4.青山学院大学)

キーワード:協同トムソン散乱、実験室宇宙物理学、数値実験

We have performed the laboratory experiment on collisionless shocks by using high power laser in collaboration with the Institute of Laser Engineering (ILE) at Osaka university for the past few years. To measure the local plasma quantities in the shock transition region, collective Thomson scattering (CTS) measurement is utilized. The CTS is the scattering of low frequency incident electromagnetic waves by collective oscillations of plasma electrons. The spectrum of the scattered waves enables us to infer the local plasma quantities like electron density, electron and ion temperature, valence of ions, etc, as a function of local position along the path of the incident probe laser light.
The CTS measurement has been widely used so far to measure experimental as well as space plasmas. However, details of the scattering theory are complex. In particular the theory of the CTS in a non-equilibrium plasma has not been established. In this study we build the numerical simulation system of virtual CTS applicable to the measurement system in the ILE experiment. A local non-equilibrium plasma near a shock is reproduced by using standard full particle-in-cell (PIC) simulation. The time-series data of electron density obtained from the PIC simulation is used to solve a wave equation of the scattered waves separately. Since the frequencies of the scattered waves as well as the incident probe light are much higher than the plasma frequency, the wave equation should be solved with the temporal resolution much higher than that in the PIC simulation. Furthermore, the measurement system at ILE is essentially two dimensional. We will report preliminary results of the virtual CTS simulation with realistic parameters in the ILE experiment.