Abstract
Over the past several years, high- βN experiments have been carried out on HL-2A. The high- βN is realized using double transport barriers (DTBs) with hybrid scenarios. A stationary high- βN ( > 2 ) scenario was obtained by pure neutral-beam injection (NBI) heating. Transient high performance was also achieved, corresponding to βN ≥ 3 , ne/neG ∼ 0.6 , H98 ∼ 1.5 , fbs ∼ 30% , q95 ∼ 4.0 , and G ∼ 0.4 . The high- βN scenario was successfully modeled using integrated simulation codes, that is, the one modeling framework for integrated tasks (OMFIT). In high- βN plasmas, magnetohydrodynamic (MHD) instabilities are abundant, including low-frequency global MHD oscillation with n = 1, high-frequency coherent mode (HCM) at the edge, and neoclassical tearing mode (NTM) and Alfvénic modes in the core. In some high- βN discharges, it is observed that the NTMs with m/n = 3/2 limit the growth of the plasma energy and decrease βN . The low-n global MHD oscillation is consistent with the coupling of destabilized internal (m/n = 1/1) and external (m/n = 3/1 or 4/1) modes, and plays a crucial role in triggering the onset of ELMs. Achieving high- βN on HL-2A suggests that core-edge interplay is key to the plasma confinement enhancement mechanism. Experiments to enhance βN will contribute to future plasma operation, such as international thermonuclear experimental reactor .