中国物理B ›› 2026, Vol. 35 ›› Issue (3): 35204-035204.doi: 10.1088/1674-1056/adf828
Yi-Hang Shou(寿毅航)1, Xian-Qu Wang(王先驱)1,†, Zhi-Ru Li(李志儒)1, Yu-Cai Li(栗钰彩)1, Yu-Hong Xu(许宇鸿)1, Jun Cheng(程钧)1, Hai-Feng Liu(刘海峰)1, Jie Huang(黄捷)1, Xin Zhang(张欣)1, Hai Liu(刘海)1, Jun-Feng Shen(沈军峰)1, Jun Hu(胡军)1, and Chang-Jian Tang(唐昌建)2
Yi-Hang Shou(寿毅航)1, Xian-Qu Wang(王先驱)1,†, Zhi-Ru Li(李志儒)1, Yu-Cai Li(栗钰彩)1, Yu-Hong Xu(许宇鸿)1, Jun Cheng(程钧)1, Hai-Feng Liu(刘海峰)1, Jie Huang(黄捷)1, Xin Zhang(张欣)1, Hai Liu(刘海)1, Jun-Feng Shen(沈军峰)1, Jun Hu(胡军)1, and Chang-Jian Tang(唐昌建)2
摘要: Fast particle confinement in the Chinese first quasi-axisymmetric stellarator (CFQS) is investigated using the MEGA code, comparing the standard quasi-axisymmetric (QA) configuration with a finite-beta $(\langle \beta \rangle=0.74%)$ equilibrium featuring magnetic islands. In the standard QA configuration, the drift associated with the vertical magnetic curvature term, $\left( {\bm \nabla \times \bm b} \right)_{z}$, is identified as the dominant loss mechanism, especially for co-passing particles. In the finite-beta configuration, magnetic islands trap low-energy particles. The $\left( {\bm \nabla \times \bm b} \right)_{z}$ drift modulates this trapping, promoting escape for co-passing particles while reinforcing trapping for counter-passing particles, and remains a significant contributor to overall losses. These findings underscore the critical role of the $\left( {\bm \nabla \times \bm b} \right)_{z}$ drift and the added complexities of magnetic islands for energetic particle confinement in finite-beta stellarator plasmas.
中图分类号: (Stellarators, torsatrons, heliacs, bumpy tori, and other toroidal confinement devices)