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-EM19] 太陽圏・惑星間空間

2016年5月25日(水) 10:45 〜 12:15 302 (3F)

コンビーナ:*坪内 健(東京工業大学大学院理工学研究科)、西野 真木(名古屋大学宇宙地球環境研究所)、成行 泰裕(富山大学人間発達科学部)、座長:塩田 大幸(名古屋大学 宇宙地球環境研究所)

10:45 〜 11:00

[PEM19-01] 超臨界垂直衝撃波における微視的不安定性再考

*松清 修一1梅田 隆行2 (1.九州大学、2.名古屋大学)

キーワード:無衝突衝撃波、微視的不安定性、数値実験

It is considered that reflected ions play decisive roles in the dissipation processes at a supercritical collisionless shock. Local non-equilibrium plasma distribution function in the foot of a perpendicular shock leads to a variety of microscale instabilities. Two of the major instabilities which have been extensively studied for the parameters of typical heliospheric shocks are the electron cyclotron-drift instability and the modified two-stream instability. They have been often discussed separately, because of the large difference in dominant wave frequency between them. Although only a few of the past studies tried to examine the nonlinear evolutions and competing processes of them, the physical parameters used in the past numerical simulations were not realisitic. The relative importance of the instabilities may be a function of ion-to-electron mass ratio as well as the ratio of electron plasma to cyclotron frequiencies, while these two ratios are hard to be simultaneously realistic in a full particle-in-cell simulation due to the limited computational resources.
In this study microinstabilities in the foot of a supercritical perpendicular shock is revisited. We perform a number of local simulations representing a part of the foot region with systematically changing the two ratios, mass ratio and frequency ratio, by using two-dimensional full particle-in-cell code. The foot plasma is assumed to be consist of incoming ions, electrons, and reflected ions. The system size is smaller than ion gyro radius in X, which is parallel to the shock normal, and a few times ion inertial length in Y, which is along a shock surface and the ambient magnetic field. The boundary conditions are periodic in both directions. We will report the results of the simulations in which the mass ratio and the frequency ratio are systematically varied with fixing the local Alfven Mach number, plasma beta, and relative density of the reflected ions.