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Nonlinear coupling induced toroidal structure of edge localized modes

  • A. F. Mink
  • , M. Hoelzl
  • , E. Wolfrum
  • , F. Orain
  • , M. Dunne
  • , A. Lessig
  • , S. Pamela
  • , P. Manz
  • , M. Maraschek
  • , G. T.A. Huijsmans
  • , M. Becoulet
  • , F. M. Laggner
  • , M. Cavedon
  • , K. Lackner
  • , S. Günter
  • , U. Stroth
  • Max Planck Institute for Plasma Physics
  • Technical University of Munich
  • Culham Centre for Fusion Energy
  • Eindhoven University of Technology
  • IRFM, CEA
  • Princeton University
  • Center for Molecular Medicine of the Austrian Academy of Sciences

Research output: Contribution to journalArticlepeer-review

43 Scopus citations

Abstract

Edge localized modes (ELMs) are magnetohydrodynamic (MHD) instabilities that cause fast periodic relaxations of the strong edge pressure gradient in tokamak fusion plasmas. A novel diagnostic method allows the extraction of toroidal mode numbers, rotation velocities and spatial information during the ELM cycle including the crash. While mode number branches n = 3-6 and n = 8-10 are dominant just before the ELM crash, during the ELM crash n = 2-5 are observed in typical discharges with type-I ELMs in the tokamak experiment. These findings are compared to results from nonlinear MHD simulations. Although n = 6 is linearly dominant, nonlinear coupling in which n = 1 is particularly important leads to the dominance of n = 3-5 during the ELM crash, in excellent agreement with experimental observations. The simultaneous occurrence of these modes over a wide radial region leads to high stochasticity and thus increased transport.

Original languageEnglish
Article number026011
JournalNuclear Fusion
Volume58
Issue number2
DOIs
StatePublished - Feb 2018
Externally publishedYes

Keywords

  • Edge localized mode
  • JOREK
  • Mode number
  • Nonlinear
  • Plasma

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