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(EXP2/01) Study on the Behaviour of High Energy Electrons in REPUTE-1 ULQ Plasmas

Y. Ogawa1), H. Nihei2), J. Morikawa1), T. Nakajima2), D. Ozawa2), M. Ohno2), T. Suzuki3), H. Himura4), Z. Yoshida4), S. Morita5), Y. Shirai5)
 
1) High Temperature Plasma Center, the University of Tokyo, Tokyo, Japan
2) School of Engineering, the University of Tokyo, Tokyo, Japan
3) Japan Atomic Energy Research Institute, Naka, Ibaraki, Japan
4) School of Frontier Science, the University of Tokyo, Tokyo, Japan
5) National Institute for Fusion Science, Toki, Gifu, Japan

Abstract.  In REPUTE-1 Ultra-Low-q (ULQ) plasmas, behaviors of high energy electrons have been studied through a low-Z pellet injection experiment, in addition to the measurements of soft-X ray PHA and Electron Energy Analyzer(EEA). The high energy tail has been measured in the soft-X ray spectrum, and EEA signal has shown a strong anisotropy of the electron distribution function (i.e., the electron flux to the electron drift side is dominant). To study temporal and spatial information on these high energy electrons, a low-Z pellet injection experiment has been conducted. A small piece of plastic pellet is injected from the top of the REPUTE-1 device, and the trajectory of the pellet inside the plasma is measured by CCD camera. We have observed a large deflection of the pellet trajectory to the toroidal direction opposite to the plasma current (i.e., the electron drift side). This suggests that a pellet is ablated selectively only from one side due to the high energy electrons with a large heat flux. We have calculated the heat flux carried by high energy electrons. Since the repulsion force to the pellet can be calculated with the 2nd derivative of the pellet trajectory, we have estimated the heat flux of high energy electrons to be a few tens MW/m2 around the plasma center. Experimental data by EEA measurement and low-Z pellet ablation show the large population of the high energy electrons at the core region in comparison with the edge region, suggesting a MHD dynamo mechanism for the production of the high energy electrons.

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IAEA 2001