Hybrid simulations of Alfven modes driven by energetic particles

被引:22
|
作者
Zhu, J. [1 ]
Ma, Z. W. [1 ]
Wang, S. [1 ]
机构
[1] Zhejiang Univ, Inst Fus Theory & Simulat, Hangzhou 310027, Zhejiang, Peoples R China
基金
中国博士后科学基金; 中国国家自然科学基金;
关键词
GYROKINETIC EQUATIONS; STABILITY PROPERTIES; INTERNAL KINK; PLASMA; BEAM; DESTABILIZATION; EXCITATION; WAVES;
D O I
10.1063/1.4971806
中图分类号
O35 [流体力学]; O53 [等离子体物理学];
学科分类号
070204 ; 080103 ; 080704 ;
摘要
A hybrid kinetic-magnetohydrodynamic code (CLT-K) is developed to study nonlinear dynamics of Alfven modes driven by energetic particles (EP). A n = 2 toroidicity-induced discrete shear Alfven eigenmode (TAE)-type energetic particle mode (EPM) with two dominant poloidal harmonics (m = 2 and 3) is first excited and its frequency remains unchanged in the early phase. Later, a new branch of the n = 2 frequency with a single dominant poloidal mode (m = 3) splits from the original TAE-type EPM. The new single m EPM (m = 3) slowly moves radially outward with the downward chirping of the frequency and the mode amplitude remains at a higher level. The original EPM remains at its original position without the frequency chirping, but its amplitude decays with time. Finally, the m = 3 EPM becomes dominant and the frequency falls into the beta-induced gap of the Alfven continuum. The redistribution of the delta f in the phase space is consistent with the mode frequency downward chirping and the drifting direction of the resonance region is mainly due to the biased free energy profile. The transition from a TAE-type EPM to a single m EPM is mainly caused by extension of the p = 0 trapped particle resonance in the phase space. Published by AIP Publishing.
引用
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页数:10
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