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On the parasitic absorption in FWCD experiments in JET ITB plasmas

  • T. Hellsten
  • , M. Laxåback
  • , T. Bergkvist
  • , T. Johnson
  • , F. Meo
  • , F. Nguyen
  • , C. C. Petty
  • , M. Mantsinen
  • , G. Matthews
  • , J. M. Noterdaeme
  • , T. Tala
  • , D. Van Eester
  • , P. Andrew
  • , P. Beaumont
  • , V. Bobkov
  • , M. Brix
  • , J. Brzozowski
  • , L. G. Eriksson
  • , C. Giroud
  • , E. Joffrin
  • V. Kiptily, J. Mailloux, M. L. Mayoral, I. Monakhov, R. Sartori, A. Staebler, E. Rachlew, E. Tennfors, A. Tuccillo, A. Walden, K. D. Zastrow
  • Swedish Research Council
  • National Laboratory
  • Commissariat à l'Énergie Atomique (CEA)
  • General Atomics
  • Helsinki University of Technology
  • Culham Centre for Fusion Energy
  • Max-Planck-Institut für Plasmaphysik
  • University of Ghent
  • EFDA CSU-Garching
  • Association Euratom-ENEA

Research output: Contribution to journalArticlepeer-review

16 Citations (Scopus)

Abstract

Fast wave current drive (FWCD) experiments have been performed in JET plasmas with electron internal transport barriers produced with LHCD. Because of a large fraction of parasitic absorption, owing to weak single pass damping, the inductive nature of the plasma current and the interplay between the RF-driven current and the bootstrap current only small changes are seen in the central current profiles. The measured difference in the central current density for co- and counter-current drive is larger than the response expected from current diffusion calculations, but smaller than the driven currents, suggesting a faster current diffusion than that given by neo-classical resistivity. A large fraction of the power is absorbed by cyclotron damping on residual 3He ions while a significant fraction appears not to have been deposited in the plasma. The strong degradation of heating and current drive occurs simultaneously with strong increases in the Be II and C IV line intensities in the divertor. The degradation depends on the phasing of the antennas and increases with reduced single pass damping which is consistent with RF-power being lost by dissipation of rectified RF-sheath potentials at the antennas and walls. Asymmetries in direct electron heating, lost power and production of impurities, fast ions and gamma-rays are seen for co- and counter-current drive. These differences are consistent with the differences in the absorption on residual 3He ions owing to the RF-induced pinch. Effective direct electron heating, comparable to the indirect electron heating with H-minority heating, occurs for dipole phasing of the antennas without producing a significant fast ion pressure and with low impurity content in the divertor plasma.

Original languageEnglish
Pages (from-to)706-720
Number of pages15
JournalNuclear Fusion
Volume45
Issue number7
DOIs
Publication statusPublished - 1 Jul 2005

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