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1 - Nuclear Sciences and Applications - IAEA

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lp<br />

[MA)<br />

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<strong>IAEA</strong>-CN-50/A-I-4 79<br />

LIM<br />

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1 2<br />

P[_H (MW)<br />

J7G. 70. LH current drive characteristics.<br />

Current ramp-up by the LH wave [3] has been investigated in low density divertor<br />

discharges, <strong>and</strong> the plasma current was ramped up from 0.46 to 0.60 MA<br />

in 6.4 s at r^ = 0.3 X 10 19 m" 3 with an injected LH power of 1.6 MW. It is estimated<br />

for this discharge that about 5 % of the LH wave energy is transferred to the<br />

poloidal field energy of the driven current.<br />

Current profile modification is another important aspect of current drive [10].<br />

Improved confinement exceeding L-mode scaling has been observed for flattened<br />

current profiles induced by LH wave injection, when the change in the internal inductance<br />

reached A*- « -0.1.<br />

9. FUTURE PROGRAMME OF JT-60<br />

A major role to be played by JT-60 in the future is the improvement of the tokamak<br />

plasma performance so that the Japanese fusion programme can be advanced to<br />

reach the next step ignition device. The JT-60 upgrade programme [11] has started<br />

already; in this programme, the vacuum vessel <strong>and</strong> the poloidal field coil will be<br />

replaced completely in order to allow high current discharges with 6 MA in a divertor<br />

<strong>and</strong> with 7 MA in a limiter configuration.<br />

Deuterium beams will be injected into deuterium instead of hydrogen plasmas<br />

in the upgrade experiment. In conjunction with the change in the beam species, the<br />

beam power is expected to increase up to 40 MW at a beam energy of 120 keV. An<br />

RF heating system such as LHRF <strong>and</strong> ICRF will also be set up with some improvements<br />

in various devices.

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