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Yingfeng XU (徐颖峰), Youjun HU (胡友俊), Xiaodong ZHANG (张晓东), Xingyuan XU (徐行远), Lei YE (叶磊), Xiaotao XIAO (肖小涛), Zhen ZHENG (郑振). Simulations of NBI fast ion loss in the presence of toroidal field ripple on EAST[J]. Plasma Science and Technology, 2021, 23(9): 95102-095102. DOI: 10.1088/2058-6272/ac0717
Citation: Yingfeng XU (徐颖峰), Youjun HU (胡友俊), Xiaodong ZHANG (张晓东), Xingyuan XU (徐行远), Lei YE (叶磊), Xiaotao XIAO (肖小涛), Zhen ZHENG (郑振). Simulations of NBI fast ion loss in the presence of toroidal field ripple on EAST[J]. Plasma Science and Technology, 2021, 23(9): 95102-095102. DOI: 10.1088/2058-6272/ac0717

Simulations of NBI fast ion loss in the presence of toroidal field ripple on EAST

  • NBI fast ion losses in the presence of the toroidal field ripple on EAST have been investigated by using the orbit code GYCAVA and the NBI code TGCO. The ripple effect was included in the upgraded version of the GYCAVA code. It is found that loss regions of NBI fast ions are mainly on the low field side near the edge in the presence of ripple. For co-current NBIs, the synergy effect of ripple and Coulomb collision on fast ion losses is dominant, and fast trapped ions located on the low field side are easily lost. The ripple well loss and the ripple stochastic loss of fast ions have been identified from the heat loads of co-current NBI fast ions. The ripple stochastic loss and the collision-induced loss are much larger than the ripple well loss. Heat loads of lost fast ions are mainly localized on the right side of the radio frequency wave antennas from the inside view toward the first wall. For counter-current NBIs, the first orbit loss due to the magnetic drift is the dominant loss channel. In addition, fast ion loss fraction with ripple and collision for each NBI linearly increases with the effective charge number, which is related to the pitch angle scattering effect.
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