Nuclear Fusion (Jan 2022)

Characteristics of electron temperature profile stiffness in electron-heated plasmas on EAST

  • J.W. Liu,
  • Q. Zang,
  • Y. Liang,
  • Y.H. Huang,
  • E.Z. Li,
  • L.Q. Xu,
  • A. Knieps,
  • Y.Q. Chu,
  • Y. Chao,
  • Y.C. Hu,
  • Y.F. Jin,
  • H.Q. Liu,
  • H.L. Zhao,
  • B. Lyu,
  • X.Z. Gong,
  • the EAST Team

DOI
https://doi.org/10.1088/1741-4326/aca168
Journal volume & issue
Vol. 63, no. 1
p. 016011

Abstract

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A very high core electron temperature ( T _e0 ∼ 10 keV) plasma has been established and stably sustained by applying both lower hybrid wave (LHW) and on-axis electron cyclotron resonance heating (ECRH) in the Experimental Advanced Superconducting Tokamak (EAST). In this work, power balance analysis shows that the increase of ECRH power can increase the normalized T _e gradient significantly at the plasma core region ( ρ < 0.6), but does not change the T _e profile stiffness in the low-density L-mode plasmas. This has been considered to be due to a strong synergistic effect between ECRH and LHW. Furthermore, three distinguishable stages characterized by different T _e profile stiffnesses can be identified from the density ramp-up in the electron-heated plasma on EAST. A stronger T _e profile stiffness at ρ = 0.3 has been observed in the Stage-II, where the LHW power deposition gradually moves away from the plasma core region, following the electron density increases. Furthermore, the formation of an internal plasma density transport barrier inside ρ ∼ 0.6, accompanied by a sudden drop in core T _e and a rise in both core plasma density and ion temperature, has been observed for the first time during the transition from the Stage-II to the Stage-III when the central line-averaged plasma density reaches a threshold of 2.2 × 10 ^19 m ^−3 . This finding strongly affects further development of high-performance gas-fueled electron-heated plasma scenarios in EAST and suggests an advanced operational regime with a wide internal plasma density transport barrier.

Keywords