1972 年 33 巻 1 号 p. 206-215
The nonlinear behaviour of Landau damping is investigated numerically. The basic equations are able to describe the amplitude oscillation, linear Landau damping, and intermediate regions of wave behaviour. If q≡γL⁄ωB, where γL is the linear Landau damping coefficient and ωB the bouncing frequency of electron trapped in the wave, we find that for q<<1 a plateau is formed in the time dependence of the amplitude of the electric field D, while for q\lesssim0.5 a plateau may also be formed. Another kind of plateau appears for q≈0.77, but for q<0.77 the wave is damped (not necessarily Landaudamped). The time evolution of the number of “trapped” electrons and also of the distribution of resonant electrons is obtained. It is found that even when D reaches its constant asymptotically for q<<1 the corresponding distribution of resonant electrons is not necessarily uniform in the trapped regions.
この記事は最新の被引用情報を取得できません。