High-power gyrotron development at Forschungszentrum Karlsruhe for fusion applications

In the first part of this paper, the status of the 140-GHz continuously operated gyrotrons with an output power of 1 MW for the stellarator Wendelstein 7-X will be described. With the first series tube, an output power of 1000 kW has been achieved in short pulse operation (milliseconds) with an electron beam current of 40 A, and of 1150 kW at 50 A. With a pulse length of 3 min limited by the available high-voltage (HV) power supply, an output power of 920 kW at an electron beam current of about 40 A with an efficiency of 45% and a mode purity of 97.5% has been obtained. At a reduced beam current of 29 A, an output power of 570 kW was measured with a pulse length of 1893 s without significant increase in tube pressure. The energy content of this pulse is almost 1.1 GJ. For the next fusion plasma device, International Thermonuclear Experimental Reactor (ITER), gyrotrons with a higher output power of about 2 MW are desirable. In short-pulse experiments, the feasibility of the fabrication of coaxial cavity gyrotrons with an output power up to 2-MW, continuous wave (CW), has been demonstrated, and the information necessary for a technical design has been obtained. The development of a long-pulse 2-MW coaxial cavity gyrotron started within a European cooperation. In parallel to the design and fabrication of an industrial prototype gyrotron, a short-pulse preprototype gyrotron has been operated to verify the design of critical components. An output power of 1.2 MW with an efficiency of 20% has been achieved. The development of frequency tunable gyrotrons operating in the range from 105 to 140 GHz for stabilization of current driven plasma instabilities in fusion plasma devices (neoclassical tearing modes) is another task in the development of gyrotrons at the Forschungszentrum Karlsruhe.

[1]  M. Thumm,et al.  165 GHz, 1.5 MW-coaxial cavity gyrotron with depressed collector , 1999 .

[2]  Richard J. Temkin,et al.  Long-pulse and CW tests of a 110-GHz gyrotron with an internal, quasi-optical converter , 1996 .

[3]  Yoshika Mitsunaka,et al.  Development of 170 and 110 GHz gyrotrons for fusion devices , 2003 .

[4]  Stefan Illy,et al.  A 2 MW, 170 GHz coaxial cavity gyrotron , 2003 .

[5]  M. Thumm,et al.  Step-tunable 1 MW broadband gyrotron with Brewster window , 1997 .

[6]  G. Gantenbein,et al.  Progress in the Development of 1 MW CW Gyrotrons for the Stellarator W7-X , 2004 .

[7]  Stefan Illy,et al.  Coaxial cavity gyrotron with dual RF beam output , 1998 .

[8]  M. Schmid,et al.  Development of multimegawatt gyrotrons for fusion plasma heating and current drive , 2005, Fifth IEEE International Vacuum Electronics Conference (IEEE Cat. No.04EX786).

[9]  Manfred Thumm,et al.  Frequency step-tunable (114–170 GHz) megawatt gyrotrons for plasma physics applications , 2001 .

[10]  G. Dammertz,et al.  165-GHz coaxial cavity gyrotron , 2004, IEEE Transactions on Plasma Science.

[11]  L. G. Popov,et al.  Development of 170 GHz/1 MW Russian gyrotron for ITER , 2001 .

[12]  K. E. Kreischer High frequency, megawatt gyrotron experiments at MIT , 1993, International Conference on Infrared and Millimeter Waves.

[13]  Manfred Thumm,et al.  On the use of step-tuneable gyrotrons in ITER , 2005 .

[14]  Stefan Illy,et al.  Possibilities for multifrequency operation of a gyrotron at FZK , 2002 .

[15]  G. Gantenbein,et al.  Development of a 140 GHz, 1 MW, Continuous Wave Gyrotron for the W7-X Stellarator , 2001 .

[16]  Manfred Thumm,et al.  An advanced dimple-wall launcher for a 140 GHz 1 MW continuous wave gyrotron , 2004 .

[17]  Manfred Thumm,et al.  Fast frequency-step-tunable high-power gyrotron with hybrid-magnet-system , 2001 .

[18]  Manfred Thumm,et al.  Recent results of the 1-MW, 140-GHz, TE/sub 22,6/-mode gyrotron , 1999 .

[19]  B. Piosczyk,et al.  A novel 4.5-MW electron gun for a coaxial cavity gyrotron , 2001 .

[20]  G. Michel,et al.  Synthesis of YETI-Footprint-Mirrors with Low Stray Radiation , 2004 .

[21]  Andreas Meier,et al.  CVD diamond windows studied with low- and high-power millimeter waves , 2002 .

[22]  G. Gantenbein,et al.  The physics of neoclassical tearing modes and their stabilization by ECCD in ASDEX Upgrade , 2001 .

[23]  S. Kern,et al.  Numerische Simulation der Gyrotron- Wechselwirkung in koaxialen Resonatoren , 1996 .

[24]  Thomas M. Antonsen,et al.  Effect of the azimuthal inhomogeneity of electron emission on gyrotron operation , 2001 .

[25]  Manfred Thumm,et al.  Long-pulse operation of a 0.5 MW TE/sub 10.4/ gyrotron at 140 GHz , 1996 .

[26]  T. C. Luce,et al.  Applications of high-power millimeter waves in fusion energy research , 2002 .