TY - JOUR
T1 - Electron cyclotron current drive at the second harmonic in the WT-3 tokamak
AU - Tanaka, H.
AU - Ando, A.
AU - Ogura, K.
AU - Ide, S.
AU - Iida, M.
AU - Oho, K.
AU - Ozaki, S.
AU - Iwamura, K.
AU - Yamazaki, A.
AU - Nakamura, M.
AU - Maekawa, T.
AU - Terumichi, Y.
AU - Tanaka, S.
PY - 1988
Y1 - 1988
N2 - Electron cyclotron current drive (ECCD) at the second harmonic (=2e) is demonstrated for two types of plasma in the WT-3 tokamak. When microwave power PEC is injected into a plasma after Ohmic heating (OH) power is shut down, the plasma current is sustained and ramped up by the EC wave only. Here 2e EC-driven current is generated by 2e EC heating of an energetic electron tail existing in the OH plasma. Further, when PEC is injected into a microwave discharge plasma, 2e EC-driven plasma current is started up and 23 ECCD plasma is formed without OH power. The 2e ECCD efficiency is the same order as that at =e, but the 3e EC-driven current is not generated, in contrast with the theoretical prediction.
AB - Electron cyclotron current drive (ECCD) at the second harmonic (=2e) is demonstrated for two types of plasma in the WT-3 tokamak. When microwave power PEC is injected into a plasma after Ohmic heating (OH) power is shut down, the plasma current is sustained and ramped up by the EC wave only. Here 2e EC-driven current is generated by 2e EC heating of an energetic electron tail existing in the OH plasma. Further, when PEC is injected into a microwave discharge plasma, 2e EC-driven plasma current is started up and 23 ECCD plasma is formed without OH power. The 2e ECCD efficiency is the same order as that at =e, but the 3e EC-driven current is not generated, in contrast with the theoretical prediction.
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U2 - 10.1103/PhysRevLett.60.1033
DO - 10.1103/PhysRevLett.60.1033
M3 - Article
AN - SCOPUS:4243934191
SN - 0031-9007
VL - 60
SP - 1033
EP - 1036
JO - Physical Review Letters
JF - Physical Review Letters
IS - 11
ER -