Observation and Simulation of $n=1$ Reversed Shear Alfvén Eigenmode on the HL-2A Tokamak
P. W. Shi1, Y. R. Yang2, W. Chen1, Z. B. Shi1*, Z. C. Yang1, L. M. Yu1, T. B. Wang1, X. X. He1, X. Q. Ji1, W. L. Zhong1, M. Xu1, and X. R. Duan1
1Southwestern Institute of Physics, Chengdu 610041, China 2State Key Laboratory of Intense Pulsed Radiation Simulation and Effect, Northwest Institute of Nuclear Technology, Xi'an 710024, China
Abstract：A branch of high-frequency Alfvénic modes is observed on the HL-2A tokamak. The electromagnetic mode can be driven unstably in the plasma with an off-axis neutral beam heating. Its mode frequency keeps almost unchanged or presents a slow-sweeping behavior, depending on the detail current evolution. The poloidal and toroidal mode numbers are $m/n=1/1$. The mode has a quite short duration ($\leq$20 ms) and usually appears 5–10 ms after the neutral beam being injected into the plasma. Hybrid simulations based on M3D-K have also been carried out. The result suggests that co-passing energetic particles are responsible for the mode excitation. The simulated mode structures are localized nearby location of minimum safety factor ($q_{\rm min}$) and agree with the structures obtained through tomography of soft x-ray arrays. Further, the modes are localized in the continuum gap and their frequencies increase with variation of $q_{\rm min}$ in a wide range. Last but not least, the characteristic of unchanged frequency on experiment is also reproduced by the nonlinear simulation with a fixed safety factor. All those evidences indicate that the $n=1$ high-frequency mode may belong to a reversed shear Alfvén eigenmode.
. [J]. 中国物理快报, 2022, 39(10): 105201-.
P. W. Shi, Y. R. Yang, W. Chen, Z. B. Shi, Z. C. Yang, L. M. Yu, T. B. Wang, X. X. He, X. Q. Ji, W. L. Zhong, M. Xu, and X. R. Duan. Observation and Simulation of $n=1$ Reversed Shear Alfvén Eigenmode on the HL-2A Tokamak. Chin. Phys. Lett., 2022, 39(10): 105201-.
2022, Vol. 39 
