Microwave Attenuation by Cyclotron Resonance in a Slightly Ionized Gas

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概要

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• The Boltzmann equation is solved for the distribution function of electrons in a static uniform magnetic field B_0 and a high frequency electric field. The tensor of dielectric constant and the propagation constant k are obtained from this solution. The calculations are made by neglecting the square of the amplitude of electric field for two cases: (1) k//B_0, (2)K⊥B_0. The attenuation apectrum for the case (2) is not a Lorentzian type and its maximum occurs at the microwave frequency ω=(w_c^2+w_p^2+vm^2)^<1/2>. If the electron density in high, the attenuation spectrum deffers from a Lorentzian type even for the case (1).

• 社団法人日本物理学会の論文
• 1961-02-05

著者

• Dodo Taro

  Hitachi Central Research Laboratory

• Dodo T.

  Hitachi Central Research Laboratory

関連論文

• Formation of a Plasma by Low Energy Ion Injection and Cyclotron Heating
• Microwave Attenuation by Cyclotron Resonance in a Slightly Ionized Gas
• Heating of a Plasma by Acoustic Waves
• Spectrum of the Electron Cyelotron Resonance in a Plasma
• Measurements on Collision Frequencies of Electrons in Neon Gas

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