Substantial radio-frequency power in the ion-cyclotron range of freque
ncies can be effectively coupled to a tokamak plasma from poloidal cur
rent strap antennas at the plasma edge. If there exists an ion-ion hyb
rid resonance inside the plasma, then some of the power from the anten
na, delivered into the plasma by fast Alfven waves, can be mode conver
ted to ion-Bernstein waves. In tokamak confinement fields the mode-con
verted ion-Bernstein waves can damp effectively and locally on electro
ns [A. K. Ram and A. Bers, Phys. Fluids B 3, 1059 (1991)]. The usual m
ode-conversion analysis that studies the propagation of fast Alfven wa
ves in the immediate vicinity of the ion-ion hybrid resonance is exten
ded to include the propagation and reflection of the fast Alfven waves
on the high magnetic-field side of the ion-ion hybrid resonance. It i
s shown that there exist plasma conditions for which the entire fast A
lfven wave power incident on the ion-ion hybrid resonance can be conve
rted to ion-Bernstein waves. In this extended analysis of the mode con
version process, the fast Alfven waves can be envisioned as being coup
led to an internal plasma resonator. This resonator extends from the l
ow magnetic-field cutoff near the ion-ion hybrid resonance to the high
magnetic-held cutoff. The condition for 100% mode conversion correspo
nds to a critical coupling of the fast Alfven waves to this internal r
esonator. As an example, the appropriate plasma conditions for 100% mo
de conversion are determined for the Tokamak Fusion Test Reactor (TFTR
) [R. Majeski et al., Proceedings of the 11th Topical Conference on RF
Power in Plasmas, Palm Springs (American Institute of Physics, New Yo
rk, 1995), Vol. 355, p. 63] experimental parameters. (C) 1996 American
Institute of Physics.