Global simulations of energetic electron excitation of beta-induced Alfven eigenmodes

None Bao Jian, None Zhang Wenlu, None Li Ding
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Abstract

The energetic electron (EE) excitation of beta-induced Alfvén eigenmodes is investigated by using the newly developed global eigenvalue code MAS, which is based on a hybrid model that consists of Landau fluid bulk plasma and drift kinetic EE. Specifically, the bulk plasma kinetic effects such as finite Larmor radius, diamagnetic drifts and Landau dampings, and the EE adiabatic fluid response of convection and non-adiabatic kinetic response of precessional drift resonance are incorporated in the simulations. The global eigenmode equation is solved for e-BAE mode structure and linear dispersion relation in tokamak non-perturbatively. The radial width of e-BAE mode structure becomes narrower as the toroidal mode number increases, which can be explained by the change of Alfvén continuous spectra that interact with kinetic Alfvén waves for corresponding eigenmode formation. The e-BAE growth rate exhibits a non-monotonic variation with toroidal mode number for precessional drift resonance destabilization, while the e-BAE real frequency is close to the continuum accumulation point that almost remains the same. The parametric dependence of e-BAE stability on EE density and that on temperature are analyzed by MAS non-perturbative simulations, which shows that the EE density can affect e-BAE real frequency and thus changes the resonance condition, resulting in e-BAE stabilization in the strong EE drive regime. Further, the EE non-perturbative effect on the symmetry breaking of e-BAE mode structure is reported. The poloidal symmetry breaking characterized by the ‘boomerang’ shape two-dimensional (2D) structure can be greatly enhanced by increasing EE temperature, together with the large radial variation of the poloidal phase angle of dominant principal poloidal harmonic. The radial symmetry breaking of e-BAE mode structure arises when EE density/temperature drive is not symmetric with respect to corresponding rational surface, which can lead to a net volume-averaged value of e-BAE parallel wave number which drives plasma intrinsic rotation. These results are helpful in understanding the e-BAE dynamics observed in recent experiments.
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β诱导Alfven本征模的高能电子激发的全局模拟
采用基于朗道流体体等离子体和漂移动力学电子特征模混合模型的全局特征值编码MAS,研究了β诱导的alfvsamn特征模的高能电子激发。具体来说,模拟中考虑了有限拉莫尔半径、抗磁漂移和朗道阻尼等体等离子体动力学效应,以及对流的EE绝热流体响应和进动漂移共振的非绝热动力学响应。对托卡马克中e-BAE模结构和线性色散关系的全局特征模方程进行了非摄动求解。e-BAE模态结构的径向宽度随着环向模态数的增加而变窄,这可以解释为与动力学alfvsamn波相互作用的alfvsamn连续谱的变化导致了相应特征模态的形成。进动漂移共振失稳时,e-BAE增长率随环面模态数呈非单调变化,而e-BAE实际频率接近连续累积点,且几乎保持不变。通过MAS非微扰模拟分析了e-BAE稳定性对EE密度和温度的参数依赖性,结果表明EE密度会影响e-BAE的实际频率,从而改变谐振条件,使e-BAE在强EE驱动状态下稳定。此外,还报道了EE对e-BAE模式结构对称性破缺的非微扰效应。随着EE温度的升高,主极向谐波相位角的径向变化较大,极向对称破缺的“回飞棒”形状二维结构得到了显著增强。当EE密度/温度驱动相对于相应的有理面不对称时,e-BAE模式结构的径向对称破缺会导致驱动等离子体本禀旋转的e-BAE平行波数的净体积平均值。这些结果有助于理解最近实验中观察到的e-BAE动力学。
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