Plasma and Fusion Research
Volume 5, S2065 (2010)
Regular Articles
- Department of Physics, Nagoya University, Nagoya 464-8602, Japan
Abstract
A magnetosonic shock wave propagating obliquely to an external magnetic field can repeatedly accelerate thermal ions if θ0 45°C , where θ0 is the angle between the wave normal and the external magnetic field. The ion energy gains in this process are theoretically analyzed, and an expression for the maximum energy is derived. This theory is verified using a two-dimensional, electromagnetic particle code. Furthermore, whistler wave instabilities generated by the accelerated ions are studied. The simulation demonstrates that whistler waves are excited in both the upstream and downstream regions, but that the whistler waves in these two regions have different frequencies and wavenumbers. It is shown that the characteristics of these waves can be explained by linear theory.
Keywords
collisionless shock, ion acceleration, whistler wave instability, particle simulation
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This paper may be cited as follows:
Mieko TOIDA and Taku GOHIRA, Plasma Fusion Res. 5, S2065 (2010).