Z. Chang et al., ALPHA-DRIVEN MAGNETOHYDRODYNAMICS (MHD) AND MHD-INDUCED ALPHA-LOSS INTHE TOKAMAK FUSION TEST REACTOR, Physics of plasmas, 4(5), 1997, pp. 1610-1616
Alpha-driven toroidal Alfven eigenmodes (TAEs) are observed as predict
ed by theory in the post-neutral beam phase in high central q (safety
factor) deuterium-tritium (D-T) plasmas in the Tokamak Fusion Test Rea
ctor (TFTR) [D. J. Grove and D. M. Meade, Nucl. Fusion 25, 1167 (1985)
]. The mode location, poloidal structure, and the importance of q prof
ile for TAE instability are discussed. So far no alpha particle loss d
ue to these modes was detected due to the small mode amplitude. Howeve
r, alpha loss induced by kinetic ballooning modes (KBMs) was observed
in high-confinement D-T discharges. Particle orbit simulation demonstr
ates that the wave-particle resonant interaction can explain the obser
ved correlation between the increase in alpha loss and appearance of m
ultiple high-n (n greater than or equal to 6, n is the toroidal mode n
umber) modes.