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Confinement characteristics of high-energy ions produced by ICRF heating in the large helical device

R Kumazawa1, K Saito1, Y Torii2, T Mutoh1, T Seki1, T Watari1, M Osakabe1, S Murakami1, M Sasao3, T Watanabe1, T Yamamoto2, T Notake2, N Takeuchi2, T Saida4, F Shimpo1, G Nomura1, M Yokota1, A Kato1, Y Zao5, H Okada6, M Isobe1, T Ozaki1, K Narihara1, Y Nagayama1, S Inagaki1, S Morita1, A V Krasilnikov7, H Idei1, S Kubo1, K Ohkubo1, M Sato1, T Shimozuma1, Y Yoshimura1, K Ikeda1, K Nagaoka1, Y Oka1, Y Takeiri1, K Tsumori1, N Ashikawa1, M Emoto1, H Funaba1, M Goto1, K Ida1, T Kobuchi1, Y Liang5, S Masuzaki1, T Minami1, J Miyazawa1, T Morisaki1, S Muto1, Y Nakamura1, H Nakanishi1, K Nishimura1, N Noda1, S Ohdachi1, B J Peterson1, A Sagara1, S Sakakibara1, R Sakamoto1, K Sato1, M Shoji1, H Suzuki1, K Tanaka1, K Toi1, T Tokuzawa1, K Y Watanabe1, I Yamada1, S Yamamoto2, M Yoshinuma1, M Yokoyama1, K-Y Watanabe1, O Kaneko1, K Kawahata1, A Komori1, N Ohyabu1, H Yamada1, K Yamazaki1, S Sudo1, K Matsuoka1, Y Hamada1, O Motojima1, M Fujiwara1 and the LHD Experimental Group

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The behaviour of high-energy ions accelerated by an ion cyclotron range of frequency (ICRF) electric field in the large helical device (LHD) is discussed. A better confinement performance of high-energy ions in the inward-shifted magnetic axis configuration was experimentally verified by measuring their energy spectrum and comparing it with the effective temperature determined by an electron slowing down process. In the standard magnetic axis configuration a saturation of the measured tail temperature was observed as the effective temperature was increased. The ratio between these two quantities is a measure of the quality of transfer efficiency from high-energy ions to a bulk plasma; when this efficiency was compared with Monte Carlo simulations the results agreed fairly well.

The ratio of the stored energy of the high-energy ions to that of the bulk plasma was measured using an ICRF heating power modulation method; it was deduced from phase differences between total and bulk plasma stored energies and the modulated ICRF heating power. The measured high energy fraction agreed with that calculated using the injected ICRF heating power, the transfer efficiency determined in the experiment and the confinement scaling of the LHD plasma.


PACS

52.50.Qt Plasma heating by radio-frequency fields; ICR, ICP, helicons

52.55.-s Magnetic confinement and equilibrium

52.80.-s Electric discharges

52.25.Kn Thermodynamics of plasmas

Subjects

Plasma physics

Dates

Issue 6 (June 2003)

Received 14 February 2003

Published 27 May 2003



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