Initial results of electron cyclotron range of frequency (ECRF) operation and experiments in JT-60U

The 110 GHz 1 MW electron cyclotron range of frequency (ECRF) system was designed and constructed on JT-60U to locally heat and control the plasmas. The gyrotron has a diamond window to transmit RF power with Gaussian mode, which is easily transformed to HE 11 mode for the transmission line of the c...

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Bibliographic Details
Published in:Fusion engineering and design 2001, Vol.53 (1), p.351-363
Main Authors: Ikeda, Y., Kasugai, A., Takahashi, K., Kajiwara, K., Isayama, A., Ide, S., Terakado, M., Shinozaki, S., Yokokura, K., Anno, K., Shimono, M., Hiranai, S., Haga, K., Kajiyama, A., Ikeda, Yu, Moriyama, S., Tsuneoka, M., Sakamoto, K., Hamamatsu, K., Oikawa, T., Kamada, Y., Naito, O., Seki, M., Ushigusa, K., Imai, T., Yamamoto, T., Fujii, T.
Format: Article
Language:English
Subjects:
Applied sciences
Controled nuclear fusion plants
Energy
Energy. Thermal use of fuels
Exact sciences and technology
Gyrotrons
Installations for energy generation and conversion: thermal and electrical energy
Plasma filled waveguides
Plasma heating
Process control
Vacuum applications
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Summary:The 110 GHz 1 MW electron cyclotron range of frequency (ECRF) system was designed and constructed on JT-60U to locally heat and control the plasmas. The gyrotron has a diamond window to transmit RF power with Gaussian mode, which is easily transformed to HE 11 mode for the transmission line of the corrugated waveguide. The second diamond window is installed at the inlet of the antenna for a vacuum seal between the transmission line and the JT-60U tokamak. The total length of the transmission line from the gyrotron to the antenna is about 60 m including nine meter bends, The antenna has a focusing mirror and a flat steerable one to focus and to control the RF beam angle mainly in the poloidal direction. In the initial operation, the power of P EC∼0.75 MW for 2 s was successfully injected into plasma when the gyrotron generated the power up to 1 MW. The total transmission efficiency from the gyrotron to the plasma was about 75%. A controllability of local electron heating with the deposition width of =15 cm was well demonstrated by using the steerable mirror. A large downshift in the deposition position was observed at the high T e plasma. Strong central electron heating was obtained from 2.2 to 6.6 keV for P EC∼0.75 MW, 0.3 s at the optimized polarization. An effective electron heating was also obtained up to ∼10 keV during EC injection for ∼1.6 s in the high β p H-mode plasma produced by NBI.
ISSN:0920-3796
1873-7196
DOI:10.1016/S0920-3796(00)00511-1