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Global gyrokinetic stability of collisionless microtearing modes in large aspect ratio tokamaks

机译:大纵横比托卡马克无碰撞微撕裂模式的整体动力学动力学稳定性

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Linear full radius gyrokinetic calculations show the existence of unstable microtearing modes (MTMs) in purely collisionless, high temperature, large aspect ratio tokamak plasmas. The present study takes into account fully gyrokinetic highly passing ions and electrons. The global 2-D structures of the collisionless mode with full radius coupling of the poloidal modes is obtained and compared with another electromagnetic mode, namely, the Alfvén Ion Temperature Gradient (AITG) mode (or Kinetic Ballooning Mode, KBM) for the same equilibrium profile. Several important characteristics of the modes are brought out and compared, such as a clear signature in the symmetry properties of the two modes, the plasma–β dependence, and radial and poloidal length scales of the electrostatic and magnetic vector potential fluctuations. Extensive parameter scans for this collisionless microtearing mode reveal the scaling of the growth rate with β and the electron temperature gradient η_e. Scans at different β values show an inverse relationship between the η_e threshold and β, leading to a stability diagram, and implying that the mode might exist at moderate to strong temperature gradients for finite β plasmas in large aspect ratio tokamaks. In contrast to small aspect ratio tokamaks where the trapped electron magnetic drift resonance is found to be important, in large aspect ratio tokamaks, a strong destabilization due to the magnetic drift resonance of passing electrons is observed and is identified as a possible collisionless drive mechanism for the collisionless MTM.
机译:线性全半径陀螺动力学计算表明,在纯无碰撞,高温,高长宽比的托卡马克等离子体中,存在不稳定的微撕裂模式(MTM)。本研究考虑了完全回旋的高传递离子和电子。获得了具有无极性模式和极向模式全半径耦合的整体二维结构,并将其与另一个电磁模式进行比较,即相同平衡的Alfvén离子温度梯度(AITG)模式(或动力学气球模式,KBM)个人资料。提出并比较了这些模式的几个重要特征,例如两种模式的对称性的清晰特征,等离子-β依赖性以及静电和磁矢量电势波动的径向和倍数长度尺度。对该无碰撞微撕裂模式进行的广泛参数扫描揭示了增长率与β的比例关系以及电子温度梯度η_e。在不同的β值处进行扫描显示η_e阈值与β之间存在反比关系,从而形成了稳定性图,这意味着对于宽高比托卡马克中的有限β等离子体,该模式可能存在于中等到强的温度梯度下。与小纵横比的托卡马克相比,在其中捕获电子磁漂移共振很重要,而在大纵横比的托卡马克中,观察到由于经过的电子的磁漂移共振而引起的强烈失稳,并且被确定为可能的无碰撞驱动机制。无碰撞的MTM。

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