Collision-Induced Instabilities near Electron Cyclotron Harmonics in Plasma
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概要
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Instabilities of longitudinal wave and transverse wave in plasma are discussed by using the Boltzmann equation containing a collision term between an electron and massive particles. It is assumed that the plasma is homogeneous and the unperturbed distribution function in velocity space f_0 is o-functional, i.e. f_0∞o(υ-υ_0), and the collision frequency ν varies as ν∞υ^h. In the case of the propagation perpendicular to the magnetic field, a collision-induced instability occurs near electron cyclotron harmonics (ω〓nω_c) when the condition h>N is satisfied, where N = 2n + 1 for extraordinary wave and N = 2n + 3 for ordinary wave, and the maximum growth rate (ω_i)_<maz> is equal to {(h-N)/N}ν for both waves.
- 社団法人日本物理学会の論文
- 1967-11-05
著者
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Idehara Toshitaka
Department Of Applied Physics Fukui University
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Idehara Toshitaka
Department Of Physics Faculty Of Science University Of Kyoto
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SUGAYA Reiji
Department of Physics, Faculty of Science, University of Kyoto
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Sugaya Reiji
Department Of Physics Faculty Of Science University Of Kyoto
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Sugaya Reiji
Department Of Physics Faculty Of Science Ehime Univerrsity
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