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(EX9/2) Runaway Current Termination in JT-60U

H. Tamai1), R. Yoshino1), S. Tokuda1), G. Kurita1), Y. Neyatani1), M. Bakhtiari2), R. Khayrutdinov3), V. Lukash4), M. N. Rosenbluth5), and the JT-60U Team1)
 
1) Japan Atomic Energy Research Institute, Naka-machi, Ibaraki-ken, 311-0193, Japan
2) Utsunomiya University, Utsunomiya, Tochigi, 321-8585, Japan
3) Troitsk Institute, 142092 Moscow, Russia
4) RRC Kurchatov Institute, 123182, Moscow, Russia
5) General Atomics, San Diego, California 92186-5698, USA

Abstract.  Spontaneous termination of runaway current, generated at the plasma disruption, is found in JT-60U during the vertical plasma displacement event, where the safety factor at the plasma surface, qs decreases. For all shots with runaway electron generation, runaway current termination starts with the appearance of a spike in magnetic fluctuation and finishes at qs $ \geq$ 2. Growth rates of the spikes in the magnetic fluctuations decrease by an order of magnitude during the termination of runaway current. When each magnetic fluctuation with a slow growth rate appears, runaway current decays, and heat flux pulses are generated. Halo current during the runaway termination is small. Halo current is generated after the runaway termination, and reaches the maximum level at qs $ \sim$ 1.

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IAEA 2001