On ion cyclotron current drive for sawtooth control

Experiments using ion cyclotron current drive (ICCD) to control sawteeth are presented. In particular, discharges demonstrating shortening of fast ion induced long sawteeth reported in (Eriksson et al 2004 Phys. Rev. Lett. 92 235004) by ICCD have been analysed in detail. Numerical simulations of the ICCD driven currents are shown to be consistent with the experimental observations. They support the hypothesis that an increase in the magnetic shear, due to the driven current, at the surface where the safety factor is unity was the critical factor for the shortening of the sawteeth. In view of the potential utility of ICCD, the mechanisms for the current drive have been further investigated experimentally. This includes the influence of the averaged energy of the resonating ions carrying the current and the spectrum of the launched waves. The results of these experiments are discussed in the light of theoretical considerations.

[1]  F. Hinton,et al.  Trapped electron correction to beam driven current in general tokamak equilibria , 1997 .

[2]  Torbjörn Hellsten,et al.  The influence of finite drift orbit width on ICRF heating in toroidal plasmas , 2002 .

[3]  R J Buttery,et al.  Destabilization of fast-ion-induced long sawteeth by localized current drive in the JET tokamak. , 2004, Physical review letters.

[4]  M. Rosenbluth,et al.  Model for the sawtooth period and amplitude , 1996 .

[5]  Francesco Porcelli,et al.  Local magnetic shear control in a tokamak via fast wave minority ion current drive : theory and experiments in jet , 1994 .

[6]  R. Gruber,et al.  Global Waves in Cold-Plasmas , 1986 .

[7]  J. G. Cordey,et al.  Beam‐induced currents in toroidal plasmas of arbitrary aspect ratio , 1980 .

[8]  K-D Zastrow,et al.  Plasma rotation induced by directed waves in the ion-cyclotron range of frequencies. , 2004, Physical review letters.

[9]  Ion cyclotron range of frequency mode conversion physics in Alcator C-Mod: Experimental measurements and modelinga) , 2005 .

[10]  Carlsson,et al.  Minority ion cyclotron current drive in tokamaks. , 1995, Physical review letters.

[11]  O. Sauter,et al.  Control of neoclassical tearing modes by sawtooth control. , 2002, Physical review letters.

[12]  Nathaniel J. Fisch,et al.  Theory of current-drive in plasmas , 1987 .

[13]  T. H. Stix Fast-wave heating of a two-component plasma , 1975 .

[14]  Ambrogio Fasoli,et al.  Evidence for a Wave-Induced Particle Pinch in the Presence of Toroidally Asymmetric ICRF Waves , 1998 .

[15]  L.-G. Eriksson,et al.  Dynamics of energetic ion orbits in magnetically confined plasmas , 2001 .

[16]  O. Sauter,et al.  Studies of burning plasma physics in the Joint European Torus , 2004 .

[17]  A. S. Kaye,et al.  Present and future JET ICRF antennae , 1994 .

[18]  T. Hellsten,et al.  Comparison of time dependent simulations with experiments in ion cyclotron heated plasmas , 1993 .

[19]  Olivier Sauter,et al.  Control of sawteeth and triggering of NTMs with ion cyclotron resonance frequency waves in JET , 2002 .

[20]  Interpretation of measurements of ICRF heated minority proton distributions in JET , 1997 .

[21]  Olivier Sauter,et al.  Effects of localized electron heating and current drive on the sawtooth period , 2003 .

[22]  A. Gondhalekar,et al.  Impurity induced neutralization of megaelectronvolt energy protons in JET plasmas , 1997 .

[23]  Per Helander,et al.  Monte Carlo operators for orbit‐averaged Fokker–Planck equations , 1994 .

[24]  T. Hellsten,et al.  Modelling of minority ion cyclotron current drive during the activated phase of ITER , 2005 .

[25]  M-L Mayoral,et al.  Controlling the profile of ion-cyclotron-resonant ions in JET with the wave-induced pinch effect. , 2002, Physical review letters.