Advances in the physics understanding of ELM suppression using resonant magnetic perturbations in DIII-D

M. R. Wade, R. Nazikian, J. S. DeGrassie, T. E. Evans, N. M. Ferraro, R. A. Moyer, D. M. Orlov, R. J. Buttery, M. E. Fenstermacher, A. M. Garofalo, M. A. Lanctot, G. R. McKee, T. H. Osborne, M. A. Shafer, W. M. Solomon, P. B. Snyder, W. Suttrop, A. Wingen, E. A. Unterberg, L. Zeng

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Abstract

Recent experiments on DIII-D have increased confidence in the ability to suppress edge-localized modes (ELMs) using edge-resonant magnetic perturbations (RMPs) in ITER, including an improved physics basis for the edge response to RMPs as well as expansion of RMP ELM suppression to more ITER-like conditions. Complete ELM suppression has been achieved utilizing n = 3 RMPs in the ITER baseline scenario. In addition, RMP ELM suppression has been expanded to include plasmas with helium concentrations near 25% and the use of n = 2 RMPs. Analysis of the kinetic profile response suggests that ELM suppression is correlated with the co-alignment of the ω⊥e = 0 location, an n = 3 rational surface, and the top of the pedestal. Modelling predicts that such a co-alignment could potentially lead to island (or island chain) formation just inside the top of the pedestal, inhibiting the growth of the pedestal and thereby maintaining the ELM-free state. Detailed analysis of data obtained during toroidal phase variations of the applied n = 3 RMPs have provided further evidence of an island-like structure at the top of the pedestal. In addition, nearly matched discharges with co-neutral-beam-injection (co-NBI) and counter-NBI have demonstrated the importance of the presence of the ω⊥e = 0 location for ELM suppression. In the counter-NBI cases, the toroidal rotation profile is such that there is no ω⊥e = 0 location and ELMs are not suppressed in conditions in which ELM suppression is generally observed with co-NBI.

Original languageEnglish
Article number023002
JournalNuclear Fusion
Volume55
Issue number2
DOIs
StatePublished - Feb 1 2015

Keywords

  • DIII-D
  • ELM control
  • MHD plasma response
  • Non-axisymmetric fields
  • Resonant magnetic perturbation

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