Hu Linlin, Ma Guowu, Sun Dimin, et al. A 28 GHz/50 kW continuous wave gyrotron with quasi-optical output[J]. High Power Laser and Particle Beams, 2019, 31: 060101. doi: 10.11884/HPLPB201931.190139
Citation:
Hu Linlin, Ma Guowu, Sun Dimin, et al. A 28 GHz/50 kW continuous wave gyrotron with quasi-optical output[J]. High Power Laser and Particle Beams, 2019, 31: 060101. doi: 10.11884/HPLPB201931.190139
Hu Linlin, Ma Guowu, Sun Dimin, et al. A 28 GHz/50 kW continuous wave gyrotron with quasi-optical output[J]. High Power Laser and Particle Beams, 2019, 31: 060101. doi: 10.11884/HPLPB201931.190139
Citation:
Hu Linlin, Ma Guowu, Sun Dimin, et al. A 28 GHz/50 kW continuous wave gyrotron with quasi-optical output[J]. High Power Laser and Particle Beams, 2019, 31: 060101. doi: 10.11884/HPLPB201931.190139
Aiming for electron cyclotron heating application in plasma fusion system, a 28 GHz 50 kW gyrotron has been developed and fabricated. The gyrotron employs a triode magnetron injection gun, a conventional cylindrical cavity working under TE02 mode, a built-in quasi-optical mode converter with conversion efficiency of about 95%. In the experiment, Gaussian beams of 54.8 kW for 1 s pulse and 45.6 kW for 30 s continuous wave at 28.08 GHz were achieved. The corresponding total efficiency is 57%.
Gregory S N, Manfred K A T, Michael I P. The gyrotron at 50: historical overview[J]. Journal of Infrared Millimeter and Terahertz Waves, 2014, 35: 325-381. doi: 10.1007/s10762-014-0050-7
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Kariya T, Minami R, Imai T, et al. Development of 28 GHz and 77 GHz, mega-watt gyrotrons for fusion devices[J]. Journal of Infrared Millimeter and Terahertz Waves, 2011, 32(3): 295-310. doi: 10.1007/s10762-010-9727-8