“…For example, the Compact Ignition Tokamak (CIT) design 1 includes 30 MW of 280 GHz radiation and the International Thermonuclear Experimental Reactor (ITER) design 2 requires 20 MW of 140 GHz rf power. The leading candidate for such a source is the waveguide cavity gyrotLoui, 3 having produced an output power of 940 kW at an efficiency of 35% and a frequency of 140 GHz,' and 1.2 MW at an efficiency of 20% at 148 GHz' in a continuous-wave (CW) relevant COnfin,,ra)t"n Howc ,-A, s the frequency and power are increased, these gyrotrons are forced to use more highly overmoded cavities, larger collectors, and vacuum output windows capable of handling the higher powers. The quasioptical gyrotron 6 (QOG) is a reasonable alternative to the cavity gyrotrons that offers several advantages.…”