Axial Structures of the Alfven Ion Cyclotron Mode in the GAMMA10 Tandem Mirror.
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概要
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Axial structures of the Alfvén ion cyclotron (AIC) mode have been investigated in the GAMMA10 tandem mirror. The AIC mode is a microinstability driven by an anisotropy in the velocity space, and is excited as an axial eigenmode in the GAMMA10. There are several discrete peaks in the frequency range of ω /Ω <SUB> ci</SUB>~ 0.8-0.9, where Ω <SUB> ci</SUB> is the ion cyclotron frequency at the midplane of the central cell. A driving term of the AIC mode is theoretically given by β <SUB>⊥</SUB>(T<SUB>⊥</SUB>/T<SUB>//</SUB>)<SUP>2</SUP>. Here, β <SUB>⊥</SUB> is a perpendicular beta value and T<SUB>⊥</SUB>/T<SUB>//</SUB> is a temperature anisotropy (an ion temperature ratio between perpendicular and parallel to the magnetic field line). In GAMMA10, the AIC mode is observed in the range of β <SUB>⊥</SUB>(T<SUB>⊥</SUB>/T<SUB>//</SUB>)<SUP>2</SUP>≥ 0.3 (which is much smaller than the theoretical prediction of β <SUB>⊥</SUB>(T<SUB>⊥</SUB>/T<SUB>//</SUB>)<SUP>2</SUP>≥ 3.52). This is thought to be related to the wave structure in the axial direction. The frequency ω and axial wave number k<SUB>//</SUB> of each mode changed with β <SUB>⊥</SUB> and T<SUB>⊥</SUB>/T<SUB>//</SUB>. As β <SUB>⊥</SUB> and T<SUB>⊥</SUB>/T<SUB>//</SUB> increased, the AIC frequency range became wide and the AIC wave changed from a propagating wave to a standing wave.
- 公益社団法人 応用物理学会の論文
公益社団法人 応用物理学会 | 論文
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