M. Beckmann
Max Planck Society
4 Papers
47 Citations
M. Beckmann is an academic researcher from Max Planck Society. The author has contributed to research in topics: Tokamak & ASDEX Upgrade. The author has an hindex of 4, co-authored 4 publications.
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Papers
Experience with the ECRH System of ASDEX Upgrade
F. Leuterer,M. Beckmann,H. Brinkschulte,F. Monaco,M. Münich,F. Ryter,H. Schütz,L. Empacher,G. Gantenbein,W Förster,W. Kasparek,P. G. Schüller,K. Schworer,A Borchegowski,A. Fix,V Illin,L.G. Popov,V. Sigalaev,E.M. Tai +18 more
TL;DR: The 140 GHz ASDEX-Upgrade ECRH system as discussed by the authors uses four gyrotrons to generate a total power of 2 MW in a Gaussian beam for 2 s. External magnetic perturbations, originating from the poloidal stray magnetic field of the tokamak air core transformer and also from the cryomagnet of the adjacent gyrotron, influence the startup of the oscillation and the electron beam deposition in the collector.
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The ECRH system of ASDEX Upgrade
F. Leuterer,M. Beckmann,A Borchegowski,H. Brinkschulte,A. V. Chirkov,Gregory G. Denisov,L. Empacher,W Förster,G. Gantenbein,V Illin,W. Kasparek,K Kirov,F. Monaco,M. Münich,L. G. Popov,F. Ryter,P.G. Schuller,K. Schwörer,H. Schütz +18 more
- 01 Oct 2001
TL;DR: The ECRH system of ASDEX upgrade is now completed as discussed by the authors, and four gyrotrons generate a total Gaussian beam power of 2 MW/2 s at 140 GHz.
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Electron cyclotron current drive at ω≈ωc with X-mode launched from the low field side
M. Beckmann,F. Leuterer +1 more
TL;DR: In this article, a X-mode launched with a nonzero toroidal angle propagates at the cutoff parallel to the magnetic field and has a circular polarisation, which can already interact efficiently with electrons via the Doppler shifted resonance.
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ECRH Experiments in ASDEX Upgrade
F. Leuterer,J. Jaquinot,F. Ryter,G. Van Oost,M. Beckmann,R.R. Weynants,H. Brinkschulte,A.G. Peeters,M. Muenich,G. V. Pereverzev,W. Suttrop,ASDEX-Upgrade-Team,ECRH-Group +12 more
- 01 Jan 1998
TL;DR: In this article, the authors used ECRH and ECCD with a power of up to 2 MW to achieve an electron temperature of ≈13 keV in low density ohmic plasmas.
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