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首页> 外文期刊>Bulletin of the American Physical Society >APS -59th Annual Meeting of the APS Division of Plasma Physics - Event - Axisymmetric Global Alfven Eigenmodes (GAEs) within the ellipticity-induced frequency gap in the Joint European Torus
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APS -59th Annual Meeting of the APS Division of Plasma Physics - Event - Axisymmetric Global Alfven Eigenmodes (GAEs) within the ellipticity-induced frequency gap in the Joint European Torus

机译:APS-等离子体物理APS部门第59届年会-事件-联合欧洲圆环中由椭圆率引起的频隙内的轴对称全球Alfven本征模(GAE)

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摘要

Alfven eigenmodes with toroidal mode number $n=0$ (i.e. axisymmetric) have been observed in the ellipticity-induced frequency range in JET. The $n=0$ modes are of interest because they may be used to diagnose fast particle energy distributions at the mode location. The modes were identified as Global Alfven Eigenmodes (GAEs), with the ellipticity of the plasma cross-section preventing strong continuum damping of the modes. The MHD codes CSCAS, MISHKA and AEGIS were used to compute the $n=0$ Alfven continuum, eigenmode structure and continuum damping. Finite ellipticity splits the Alfven continuum branch into two branches, producing a frequency gap, and splits the single GAE into two modes. One mode has dominant poloidal harmonics $m=pm 1$ with the same polarity and exists below the minimum of the top branch. The frequency of this mode coincides with the experimentally observed frequency. The other mode is found below the lower branch with opposite polarity of the poloidal harmonics, and is not observed experimentally. Analytical theory for the $n=0$ continuum and GAE mode structure in an elliptical cylinder agree with the numerical modelling. Mode drive and damping calculations will also be presented.
机译:在JET的椭圆率引起的频率范围内,已经观察到环形模数为$ n = 0 $(即轴对称)的Alfven本征模。 $ n = 0 $模式是令人感兴趣的,因为它们可用于诊断模式位置处的快速粒子能量分布。这些模式被标识为全局Alfven本征模式(GAE),其等离子截面的椭圆率阻止了这些模式的强连续衰减。 MHD代码CSCAS,MISHKA和AEGIS用于计算$ n = 0 $ Alfven连续谱,本征模结构和连续谱阻尼。有限椭圆率将Alfven连续谱分支分为两个分支,从而产生一个频率间隙,并将单个GAE分为两个模式。一种模式具有相同极性的主要极性谐波$ m = pm 1 $,并存在于顶部分支的最小值以下。该模式的频率与实验观察到的频率一致。在下部分支下方发现了另一种模式,其极性与极谱谐波的极性相反,因此无法通过实验观察到。 $ n = 0 $连续体的解析理论和椭圆圆柱体中的GAE模式结构与数值模型一致。模式驱动和阻尼计算也将介绍。

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