Study of Edge Plasma Characteristics at H-mode Transition in Heliotron J

  • WATANABE S.
    Graduate School of Energy Science, Kyoto University, Uji 611-0011, Japan
  • NAGASAKI K.
    Institute of Advanced Energy, Kyoto University, Uji 611-0011, Japan
  • MIZUUCHI T.
    Institute of Advanced Energy, Kyoto University, Uji 611-0011, Japan
  • KOBAYASHI S.
    Institute of Advanced Energy, Kyoto University, Uji 611-0011, Japan
  • OKADA H.
    Institute of Advanced Energy, Kyoto University, Uji 611-0011, Japan
  • KONDO K.
    Graduate School of Energy Science, Kyoto University, Uji 611-0011, Japan
  • YAMAMOTO S.
    Graduate School of Engineering, Osaka University, Suita 565-0871, Japan
  • TORII Y.
    High Temperature Plasma Center, The University of Tokyo, Kashiwa 277-8568, Japan
  • KANEKO M.
    National Institute for Fusion Science, Toki 509-5292, Japan
  • ARIMOTO H.
    Graduate School of Energy Science, Kyoto University, Uji 611-0011, Japan
  • MOTOJIMA G.
    Graduate School of Energy Science, Kyoto University, Uji 611-0011, Japan
  • FENG Z.
    Southwestern Institute of Physics, Chengdu 610041, China
  • NOSAKU M.
    Graduate School of Energy Science, Kyoto University, Uji 611-0011, Japan
  • TOMOKIYO T.
    Graduate School of Energy Science, Kyoto University, Uji 611-0011, Japan
  • MATSUOKA S.
    Graduate School of Energy Science, Kyoto University, Uji 611-0011, Japan
  • SANO F.
    Institute of Advanced Energy, Kyoto University, Uji 611-0011, Japan

抄録

Characteristics of spontaneous transition to a high confinement mode (H-mode) have been studied in a helical-axis heliotron device, Heliotron J. The radiation profile measured with a silicon photodiode array shows that a interesting change in the profile occurs at the plasma edge region in the transition phase, forming a strong gradient near the last closed flux surface (LCFS). Relating to the transition, characteristics of bursty density and particle-flux fluctuations current in the scrape off layer (SOL) have been investigated. The probability distribution function for the fluctuations has a tail structure in the L-mode phase, while the tail is suppressed and its direction is reversed after the transition, which may be related to the suppression of edge-plasma turbulence.

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