磁場中のプラズマ振動の安定条件

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The dispersion equation of Cauchy type for longitudinal plasma oscillations in a magnetic field is exactly derived on the basis of Vlasov's collision-free kinetic equation for arbitrary velocity distribution of electron∫∞-∞φ (k, ν) /ν-ζdν=k2/ωp2, where ζ=ω/k11, φ (k, ν) =2π/Nk11 [k11∞∑l=0 A2l (ν) (k⊥/Ω) 2l+k⊥∞∑l=0 A2l+1 (ν) (k⊥/Ω) 2l+1], A2l (ν) =1/ (l!) 222l 2l∑r=0 (-) r (2lr) M12l+1 (ν+l-r/k11Ω), A2l+1 (ν) =1/ (l!) 222l+1 2l∑r=0 (-) r (2l+1r) M2l+1 (ν+l-r/k11Ω) +M2l+1 (ν+l-r+1/k11Ω) M2l+1 (u) =∫∞0w2l+1f0 (w, u) dw, M2l+1 (u) =∂/∂uM2l+1 (u) N and Ω are the total density and the gyration frequency of electron.A2l+1, A2l are determined by the higher order moments of the component of velocity distribution function which is perpendicular to the magnetic field. The motion of the ion is easily taken into account by replacingφ intoφ++φ-. It is found that the terms of lowest order in φ for k⊥/Ωis the predominant factor for the drift instability and that higher terms of more than second order contribute to the instability due to anisotropic velocity distributions The criterion and detailed conditions for plasma instabilities are tabulated through the knowledge of potential theory. This criterion is applied to several intersting distribution functions.
社団法人プラズマ・核融合学会の論文