Author_Institution :
Inst. fur Hochleistungsimpuls-und Mikrowellentech., Assoc. EURATOM-KIT, Karlsruhe, Germany
Abstract :
Progress in the worldwide development of high-power gyrotrons for magnetic confinement fusion plasma applications is presented. Gyrotron oscillators are used for electron cyclotron heating, electron cyclotron current drive, stability control, and plasma diagnostics. After technology breakthroughs in the research on gyrotron components in the 1990s, significant progress has been achieved in the 2000s, in the field of long-pulse and continuous wave (CW) operation for a wide range of frequencies. Currently, the development of 1-MW-class CW gyrotrons for the tokamak ITER (170 GHz), the stellarator Wendelstein 7-X (140 GHz), and the tokamaks DIII-D and JT-60SA (110 GHz) has been very successful in EU, Japan, Russia, and USA. The Japan 170-GHz ITER gyrotron holds the energy world record of 2.88 GJ (0.8 MW at 1-h pulse duration). For this progress in the field of high-power long-pulse gyrotrons, innovations such as the realization of high-efficiency stable oscillation in very high-order cavity modes with low ohmic losses, the use of single-stage depressed collectors for energy recovery (efficiency enhancement and simpler power supplies), highly efficient internal quasi-optical (q.o.) mode converters (low level of internal stray radiation), and synthetic diamond windows have essentially contributed. The total tube efficiencies are around 50% and the purity of the linearly polarized fundamental Gaussian output mode is 97% and higher. Power modulation technologies for stabilization of neoclassical tearing modes have proceeded. Future prospects of advanced high-power fusion gyrotrons are in the areas of two- and three-frequency gyrotrons, fast step-wise frequency tuneability, higher unit power (coaxial cavities), and higher frequencies for more efficient plasma stabilization and noninductive current drive as well as reliability, availability, maintainability and inspectability for next step fusion power stations. The GYCOM step-tuneable 1-MW gyrotron for ASDEX Upgrade employi- g a broadband travelling-wave-resonator window (with two diamond disks) operates at 105, 117, 127 and 140 GHz. The EU 170 GHz coaxial-cavity gyrotron prototype achieved in millisecond pulses the power of 2.1 MW at 46% efficiency and 96% Gaussian mode purity. A new power record of second harmonic oscillation has been achieved in the subterahertz band (83 kW/389 GHz/3 ms) in Japan for application to collective Thomson scattering diagnostics. A fundamental frequency 670-GHz gyrotron with pulsed magnet generated 210 kW in 20-30- μs pulses at 20% efficiency (collaboration of institutions in Russia and USA).
Keywords :
Tokamak devices; cyclotrons; gyrotrons; millimetre wave oscillators; millimetre wave tubes; plasma confinement; plasma diagnostics; plasma instability; ASDEX Upgrade; CW gyrotrons; GYCOM step-tuneable gyrotron; Gaussian mode purity; JT-60SA; Japan ITER gyrotron; advanced high-power fusion gyrotrons; broadband travelling-wave-resonator window; coaxial-cavity gyrotron prototype; collective Thomson scattering diagnostics; continuous wave operation; efficiency 20 percent; efficiency 46 percent; efficiency 96 percent; electron cyclotron current drive; electron cyclotron heating; energy 2.88 GJ; energy recovery; fast step-wise frequency tuneability; frequency 105 GHz; frequency 110 GHz; frequency 117 GHz; frequency 127 GHz; frequency 140 GHz; frequency 170 GHz; frequency 389 GHz; frequency 670 GHz; gyrotron oscillators; high-efficiency stable oscillation; high-order cavity modes; high-power long-pulse gyrotrons; internal quasioptical mode converters; linearly polarized fundamental Gaussian output mode; long-pulse operation; low ohmic losses; magnetic confinement fusion plasma applications; neoclassical tearing mode stabilization; next step fusion power stations; noninductive current drive; plasma diagnostics; plasma stabilization; power 0.8 MW; power 1 MW; power 2.1 MW; power 210 kW; power 83 kW; power modulation technology; second harmonic oscillation; single-stage depressed collectors; stability control; stellarator Wendelstein 7-X; synthetic diamond windows; three-frequency gyrotrons; time 1 h; time 20 mus to 30 mus; time 3 ms; tokamak ITER; tokamaks DIII-D; two-frequency gyrotrons; worldwide fusion gyrotron development; Cavity resonators; Cyclotrons; Diamonds; Electron beams; Electron tubes; Gyrotrons; Radio frequency; Collective Thomson scattering (CTS); electron cyclotron current drive (ECCD); electron cyclotron heating (ECH); high-power gyrotrons; plasma stabilization;