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Hybrid simulations reveal how energetic particles stabilize resistive ballooning modes in stellarator plasmas, suggesting insights for high-beta operation.
The interaction between energetic particles (EPs) and resistive ballooning modes (RBMs) in quasi-axisymmetric stellarator (QAS) plasmas is investigated via MHD hybrid simulations using the MEGA code for the Chinese First Quasi-axisymmetric Stellarator (CFQS) configuration. Simulations show RBMs ( m= 9/n = −4 ) are stabilized by EPs at low beta values ( β_ℎ < 0.8%), which is consistent with theoretical predictions. However, as β_ℎ exceeds 0.8%, the RBM is suppressed and a new EP-driven reversed shear Alfvén eigenmode (RSAE)-like instability ( m= 4/ n= −2) becomes dominant, with significantly increased frequency and growth rate. A resistivity ( η) scan at high β_ℎ (1.5%) reveals a transition: a mode exhibits RSAE characteristics at low , while transitioning to a resistivity-driven ballooning mode at high η. This suggests the EP-driven instability observed in initial high-resistivity simulations originates from the RSAE branch but its structure is strongly modified, displaying pronounced ballooning features. This work highlights the dual role of EPs and the crucial influence of resistivity on instabilities in QAS, providing insights for high-beta operation.
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Shou et al. (2025) studied this question.
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