Recent results on the application of electron cyclotron heating to tokamaks

Many experiments using Electron Cyclotron Heating (ECH) of plasmas in tokamaks have been reported over the past several years. At a power level of 4 MW, ECH has achieved electron temperatures as high as 10 keV in the T-10 tokamak, and the H-mode has been attained in divertor discharges in DIII-D and JFT-2M. Regarding global energy confinement in either L-mode or Hmode, ECH appears to be quite similar in efficiency to neutral injection, but in addition to bulk heating it has been useful for many purposes, including study of local electron heat diffusivity through pulse-modulated heating; suppression of sawteeth, Edge Localized Modes, and other MHD activity; suppression of disruptions; preionization and startup; and current drive. In this paper, progress in these areas which has been reported since the IAEA meeting in 1986 will be summarized.

[1]  M. W. Alcock,et al.  ECRH current drive studies in the CLEO tokamak , 1988 .

[2]  S. Ide,et al.  Enhancement of efficiency for lower hybrid current drive by electron cyclotron heating in the WT-2 tokamak , 1986 .

[3]  Fom Ecrh Team The electron cyclotron resonance experiment on TFR , 1988 .

[4]  S. Bernabei,et al.  Applications of radio-frequency power to plasmas , 1987 .

[5]  Yamazaki,et al.  Electron cyclotron current drive at the second harmonic in the WT-3 tokamak. , 1988, Physical review letters.

[6]  Snider,et al.  Observation of H-mode confinement in the DIII-D tokamak with electron cyclotron heating. , 1988, Physical review letters.

[7]  R. Cano,et al.  Electron cyclotron emission and absorption in fusion plasmas , 1983 .

[8]  E. Westerhof,et al.  Sawteeth, transport and electron cyclotron heating in T-10 , 1988 .

[9]  B. Lloyd,et al.  LOW VOLTAGE START-UP IN THE CLEO TOKAMAK USING ECRH , 1986 .

[10]  M. M. Dremin,et al.  Power deposition profile effect on the ECH efficiency in T-10 , 1987 .

[11]  S. Kasai,et al.  Behaviour of the peripheral electron temperature at the H-mode transition induced by the peripheral electron cyclotron heating of a tokamak plasma , 1988 .

[12]  H. Matsumoto,et al.  Transition from the L-mode to the H-mode by electron cyclotron heating of a tokamak edge plasma , 1988 .

[13]  Harvey,et al.  Power dependence of electron-cyclotron current drive for low- and high-field absorption in tokamaks. , 1989, Physical review letters.

[14]  John Lohr,et al.  Modification of sawteeth by second harmonic electron-cyclotron heating in a tokamak , 1989 .

[15]  T. K. Chu,et al.  Sawtooth stabilization through island pressure enhancement , 1987 .

[16]  S. M. Kaye,et al.  Global energy confinement scaling for neutral-beam-heated tokamaks , 1985 .

[17]  Measurement of thermal transport by synchronous detection of modulated electron cyclotron heating in the Doublet III tokamak , 1986 .

[18]  I. Fidone,et al.  Absorption of cyclotron waves at down-shifted frequencies by an energetic electron tail in the PLT tokamak , 1985 .

[19]  Mori,et al.  Selective electron-cyclotron heating at down-shifted frequency in the lower-hybrid current driven plasma on the JFT-2M tokamak. , 1987, Physical review letters.