Experiments with high-power electron cyclotron heating (ECH) and current drive(ECCD) in the TCV tokamak are discussed. Power up to 2.7 MW from six gyrotronsis delivered to the tokamak at the second-harmonic frequency (82.7 GHz) inX-mode. The power is transmitted to the plasma by six independent launchers,each equipped with steerable mirrors that allow a wide variety of injectionangles in both the poloidal and toroidal directions. Fully non-inductiveoperation of the tokamak has been achieved in steady state, for the full 2 sgyrotron pulse duration, by co-ECCD with a highest current to date of 210 kAat full power. The experimentally measured ECCD efficiency agrees well withpredictions obtained from linear modelling. We have observed that the highestglobal efficiency attainable at a given power is limited by stabilityconstraints. While the efficiency is maximum on the magnetic axis, adisruptive MHD instability occurs when the width of the deposition profile islower than a minimum value, which increases with total power. Many ECCDdischarges display a high level of electron energy confinement, enhanced by upto a factor of two over the Rebut-Lallia-Watkins (RLW) scaling law, which bycontrast is well satisfied in ohmic conditions. The longest confinement times(up to four times RLW) are observed with central counter-ECCD. Centralelectron heat diffusivities comparable to ohmic levels are obtained in thesescenarios, with electron temperatures in excess of 10 keV.
Impact of hot plasma effects on electron cyclotron current drive in tokamak plasmas
Detailed measurements of the electron cyclotron current drive efficiency on DIII-D