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The effects of triangularity and main ion species on the inter-ELM profile evolution in ASDEX Upgrade

机译:三角形和主要离子种类对浅言升级榆树间剖面演变的影响

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In high confinement mode (H-mode) plasmas the steep gradients at the plasma edge (called pedestal) are quasi-periodically destabilised by edge localised modes (ELMs). Since the pedestal strongly affects the global plasma performance, further understanding of the temporal approach towards the pedestal stability limit (also known as pedestal recovery) is needed to optimise plasma scenarios. Previous studies have shown different recovery timescales of the electron density n_e and temperature T_e pedestal in between ELM crashes [1]. In these experiments the n_e pedestal recovered first, while the T_e pedestal started to recover after the n_e pedestal was established. Gyrokinetic modelling attributed the recovery timescales to the domination of different turbulent modes [2]. In the phase of the n_e recovery trapped electron modes were found in the pedestal, whereas in the pre-ELM pedestal after the T_e recovery, especially on large scales, microtearing modes and kinetic-ballooning modes were dominant.
机译:在高限制模式(H-MODE)等离子体中,等离子体边缘(称为基座)的陡梯度通过边缘局部模式(ELM)是准周期性地稳定。由于基座强烈影响全局等离子体性能,因此需要进一步了解朝向基座稳定性极限的时间方法(也称为基座回收)以优化等离子体场景。以前的研究显示了ELM碰撞之间的电子密度N_E和温度T_E基座的不同恢复时间表[1]。在这些实验中,首先回收N_E基座,而T_E基座在建立N_E基座后开始恢复。陀螺模型将恢复时间尺寸归因于不同湍流模式的统治[2]。在N_E恢复捕获的电子模式的阶段中,而在恢复后的ELM基座中,尤其是在大尺度上,显微切割模式和动力学 - 膨胀模式占主导地位。

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