Status of
the New Multi-Frequency ECRH System for ASDEX Upgrade
D. Wagner, F.
Leuterer, A. Manini, F. Monaco, M. Münich, H. Schütz,
J. Stober, H.
Zohm, T. Franke
M. Thumm1,
R. Heidinger2, I. Danilov2, G. Gantenbein1, J.
Flamm1
Forschungszentrum
Karlsruhe, EURATOM-FZK
1Institut für Hochleistungsimpuls- und
Mikrowellentechnik,
2Institut für Materialforschung,
PO Box 3640, D-76021 Karlsruhe,
Germany
W. Kasparek
Institut für Plasmaforschung, Universität Stuttgart,
Pfaffenwaldring 31,
D-70569
Stuttgart, Germany
A.G. Litvak3,
L.G. Popov4, V.O. Nichiporenko4, V.E. Myasnikov4,
G.G. Denisov3,
E.M. Tai4,
E.A. Solyanova4, S.A. Malygin4
3 Institute of Applied Physics, RAS, 46 Ulyanov St.,
Nizhny Novgorod, 603950, Russia
4 GYCOM Ltd, 46 Ulyanov St., Nizhny Novgorod, 603155,
Russia
A
two-frequency GYCOM gyrotron, Odissey-2, has been installed and put into
operation in the new multi-frequency ECRH system at the ASDEX Upgrade tokamak
experiment. It works at 105GHz and 140GHz with output power 640kW and 880kW
respectively at a pulse length of 10s. Meanwhile, the first two-frequency
gyrotron Odissey-1, which was damaged last year, is back at GYCOM for repair. It will be
equipped with a broadband Brewster output window and therefore become a
multi-frequency gyrotron. A further extension of the system with 2 more
gyrotrons is underway. Depending on the success of Odissey-1, these gyrotrons
will also be step-tunable and operate at two additional intermediate
frequencies between 105 and 140GHz. Construction and cold test of a first
broadband double-disc torus window are completed. The transmission to the torus
is in normal air, through corrugated aluminum HE11 waveguides with I.D.=87mm
over a total length of about 70m. Calorimetric measurements gave a total
transmission loss of only 12% at 105GHz and 10% at 140GHz. The variable
frequency will significantly extend the operating range of the ECRH system with
respect to the applied toroidal magnetic field. A feedback system for the
mirror control is under development, to keep the ECRH deposition on the
resonant q-surface while the plasma is evolving. This is required for
applications such as the suppression of neoclassical tearing modes.