Characteristics of edge fluctuation and transport in the edge localized mode suppressed plasmas by the resonant magnetic perturbation field

ORAL

Abstract

The stochastic layer at the pedestal top by the resonant magnetic perturbation (RMP) field penetration has been known as a key mechanism in the RMP edge localized mode (ELM) suppression in tokamak plasmas. The local pressure profile flattening and broadband fluctuation increase characterize the pedestal top during the RMP ELM suppression. Despite the importance of turbulence to understand the pedestal transport, the origin of the increased fluctuation and its characteristics were not fully understood. Here, we suggest that the partially stochastic island at the pedestal top can play a significant role. The nonlinear mode coupling between an island and fluctuations can result in the fluctuation growth, and the stochastic fields around the island can make the spatial structure of turbulence less predictable. We used the bicoherence and the rescaled Jensen-Shannon complexity to analyze the three-wave coupling and the statistical characteristics of fluctuations, respectively. We show that (1) the weak but significant nonlinear mode coupling exists in the narrow region at the pedestal top and (2) the spatial structure of turbulence becomes less predictable around the pedestal top. These observations are not inconsistent with the expectation of the partially stochastic island. The latter can be used to estimate the effective width of the stochastic layer over which the characteristics of fluctuations and so transport are statistically distinguished from those over the normal field geometry. In addition, we found that the divertor particle flux near the striking point becomes less predictable with the more penetration of the RMP field into the plasma.

*This research was supported by R&D Programs of "KSTAR Experimental Collaboration and Fusion Plasma Research(EN2101-12)" and "High Performance Fusion Simulation R&D(EN21417)" through Korea Institute of Fusion Energy (KFE) funded by the Government funds and by National Research Foundation of Korea under NRF-2019M1A7A1A03088462.

Presenters

  • Minjun J Choi

    • Korea Institute of Fusion Energy
    • Natl Fusion Res Inst

Authors

  • Minjun J Choi

    • Korea Institute of Fusion Energy
    • Natl Fusion Res Inst
  • Jae-Min Kwon

    • Korea Institute of Fusion Energy
    • Korea Institute of Fusion Energy (KFE)
  • Juhyung Kim

    • Korea Institute of Fusion Energy
    • Korea Institute of Fusion Energy (KFE)
  • Tongnyeol Rhee

    • Korea Institute of Fusion Energy
  • Jun-Gyo Bak

    • Korea Institute of Fusion Energy
    • KFE
    • Korea Institute of Fusion Energy (KFE)
  • G. Shin

    • Korea Institute of Fusion Energy (KFE)
    • Korea Institute of Fusion Energy
  • H.S. Kim

    • Korea Institute of Fusion Energy (KFE)
    • Korea Institute of Fusion Energy
  • Kimin Kim

    • Korea Institute of Fusion Energy
  • Byoung-Ho Park

    • Korea Institute of Fusion Energy
  • Hogun Jhang

    • Korea Institute of Fusion Energy
  • Gunsu S Yun

    • Pohang Univ of Sci & Tech
    • Pohang University of Science and Technology
  • Minwoo Kim

    • Korea Institute of Fusion Energy (KFE)
    • Korea Institute of Fusion Energy
  • Jong-Kyu Park

    • Princeton Plasma Physics Laboratory
  • SangKyeun Kim

    • Princeton University
    • Princeton Plasma Physics Laboratory
    • Princeton University, Princeton, U.S.A.
  • Hyung H Lee

    • Korea Institute of Fusion Energy
  • Yongkyoon In

    • Ulsan Natl Inst of Sci & Tech
    • Ulsan National Institute of Science and Technology
    • Ulsan National Institute of Science and Technology (UNIST)
  • J. H. Lee

    • Korea Institute of Fusion Energy
    • Korea Institute for Fusion Energy, Daejeon, Republic of Korea
    • Korea Institute of Fusion Energy (KFE)
  • Minho H Kim

    • Korea Institute of Fusion Energy (KFE)
    • Korea Institute of Fusion Energy
  • Hyeon K Park

    • Ulsan National Institute of Science and Technology