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Ion heating experiments have been carried out in the large helical device using ECH (82.5, 84.0, 168 GHz, ⩽1 MW), ICRF (38.5 MHz, ⩽2.7 MW) and NBI (H° beam: 160 keV, ⩽9 MW). The central ion temperature has been observed from the Doppler broadening of Ti XXI (2.61 Å) and Ar XVII (3.95 Å) x-ray lines, which are measured using a newly installed crystal spectrometer with a charge-coupled device. Recently, in ECH discharges, on-axis heating became possible. As a result, a high T e (0) of 6–10 keV and a high ion temperature of 2.2 keV were obtained at n e = 0.6 × 10 13 cm −3 . A clear increment of T i was also observed with the enhancement of the electron–ion energy flow when the ECH pulse was added to the NBI discharge. These results demonstrate the feasibility towards ECH ignition. A clear T i increment was observed also in ICRF discharges at low density ranges of (0.4–0.6) × 10 13 cm −3 with appearance of a new operational range of T i (0) = 2.8 keV > T e (0) = 1.9 keV. In low power ICRF heating (1 MW), the fraction of bulk ion heating is estimated to be 60% of the total ICRF input power, which means P i > P e . Higher T i (0), up to 3.5 keV, was obtained for a combined heating of NBI (<4 MW) and ICRF (1 MW) at density ranges of (0.5–1.5) × 10 13 cm −3 . The highest T i (0) of 5 keV was recorded in Ne NBI discharges at n e <1 × 10 13 cm −3 with the achievement of T i (0)> T e (0), whereas the T i (0) remained at relatively low values of 2 keV in H 2 and He NBI discharges due to less P i . The main reasons for the high T i achievement in the Ne discharges are: (1) 30% increment of deposition power, (2) increase in P i / n i (five times, P i / n i ≫ P e / n e , P i < P e ) and (3) increase in τ ei (three times). The obtained T i (0) data can be plotted by a smooth function of P i / n i . This result strongly suggests that the ion temperature increases even in the H 2 discharge if the P i can be raised up.
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Morita et al. (2003) studied this question.
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