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High frequency Alfvén eigenmodes detected with ion-cyclotron-emission diagnostics during NBI and ICRF heated plasmas on the ASDEX Upgrade tokamak

  • R. Ochoukov
  • , R. Bilato
  • , V. Bobkov
  • , S. C. Chapman
  • , R. Dendy
  • , M. Dreval
  • , H. Faugel
  • , A. Kappatou
  • , Ye O. Kazakov
  • , M. Mantsinen
  • , K. G. McClements
  • , D. Moseev
  • , S. K. Nielsen
  • , J. M. Noterdaeme
  • , M. Salewski
  • , P. Schneider
  • , M. Weiland
  • Max Planck Institute for Plasma Physics
  • University of Warwick
  • Culham Centre for Fusion Energy
  • National Science Center Kharkiv Institute of Physics and Technology
  • Barcelona Supercomputing Center
  • ICREA
  • Technical University of Denmark
  • University of Ghent

Onderzoeksoutput: Bijdrage aan een tijdschrift › Artikel › peer review

27 Citaten (Scopus)

Samenvatting

The paper presents the first reported observation of high frequency Alfvén eigenmode excitation on the ASDEX Upgrade tokamak. The mode is driven in a novel way using radio frequency (RF) wave acceleration of either beam-injected deuterium ions or thermal He-3 minority ions in a three-ion heating scenario. In the case of beam ion acceleration, the instability only appears during deuteron acceleration at the third beam ion cyclotron harmonic (wave frequency ω = 3ΩD where ΩD is the deuterium cyclotron frequency), as the mode is not detected during the more commonly used second harmonic/minority heating scenario or in the absence of beam-injected ions. The mode frequency is around 0.6-0.7ΩD, where ΩD is evaluated in the low-field side plasma edge, and tracks the magnetic field B and the edge plasma electron density ne via the Alfvénic relation ω ∼ B ne-1/2. The mode does not appear as a single frequency wave but as a bundle of closely spaced (in frequency) sub-modes. When the parallel beam ion velocity component is increased, the sub-mode frequency spacing is observed to decrease, possibly due to a change in the eigenmode structure. Under certain conditions, typically in discharges with a relatively low plasma current, IP < 0.7 MA, the mode appears to be driven directly by sub-Alfvénic deuterium beam ions. Absolute measurements of the mode amplitude show that at least 1% of the beam-injected power is transferred non-collisionally to the instability. While this is too low for practical alpha-channeling applications, discharges are planned with the aim of increasing the level of power transferred non-collisionally between fast ions and the instability.

Originele taal-2Engels
Artikelnummer126043
TijdschriftNuclear Fusion
Volume60
Nummer van het tijdschrift12
DOI's
StatusGepubliceerd - dec 2020

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