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(EX2/2) Transition from L Mode to High Ion Temperature Mode in CHS Heliotron/Torsatron Plasmas

K. Ida, M. Osakabe, K. Tanaka, T. Minami, S. Nishimura, S. Okamura, A. Fujisawa, K. Yamazaki, Y. Yoshimura, S. Kubo, R. Akiyama, D. S. Darrow1, H. Idei,. H. Iguchi, M. Isobe, S. Kado, T. Kondo2, S. Lee, K. Matsuoka, S. Morita, I. Nomura, S. Ohdachi, M. Sasao, A. Shimizu3, K. Tumori, S. Takayama2, M. Takechi3, S. Takagi3, C. Takahashi, K. Toi, T. Watari

National Institute for Fusion Science, Oroshi-cho, Toki-shi, Gifu, 509-5292, Japan
1 Princeton Plasma Physics Laboratory, Princeton, NJ 08543, U.S.A.
2 Graduate University for Advanced Studies, Hayama, 240-01, Japan
3 Dept. Energy Engineering Science, Nagoya Univ., Nagoya, 464-01, Japan

Abstract.  A high ion temperature mode (high Ti mode) is observed for neutral beam heated plasmas in the Compact Helical System (CHS) Heliotron/torsatron. The high Ti mode plasma is characterized by a high central ion temperature, Ti(0), and is associated with a peaked electron density profile produced by neutral beam fueling with low wall recycling. Transition from L mode to high Ti mode has been studied in CHS. The central ion temperature in the high Ti mode discharges reaches to 1 keV which is 2.5 times higher than that in the L mode discharges. The ion thermal diffusivity is significantly reduced by a factor of more than 2-3 in the high Ti mode plasma. The ion loss cone is observed in neutral particle flux in the energy range of 1-6 keV with a narrow range of pitch angle (90 ± 10 degree) in the high Ti mode. However, the degradation of ion energy confinement due to this loss cone is negligible.

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IAEA 2001