Differences in the H-mode pedestal width of temperature and density
P. A. Schneider(Max Planck Society), H. Zohm(Max Planck Institute for Plasma Physics), J.R. Ferron(Lawrence Livermore National Laboratory), P.B. Snyder(Commonwealth Fund), E. Wolfrum(Max Planck Institute for Plasma Physics), K. Lackner(Max Planck Institute for Plasma Physics), S. Günter(Max Planck Institute for Plasma Physics), R. J. Groebner(General Atomics (United States)), M. Beurskens(Japan Atomic Energy Agency), B. Kurzan(Max Planck Society), M. Dunne(Max Planck Institute for Plasma Physics), T.H. Osborne(University of Wisconsin–Madison)
Cited by 56
Related Papers
Edge stability and transport control with resonant magnetic perturbations in collisionless tokamak plasmas
|Nature Physics|2006|631
Active Control of Type-I Edge-Localized Modes with<mml:math xmlns:mml="http://www.w3.org/1998/Math/MathML" display="inline"><mml:mi>n</mml:mi><mml:mo>=</mml:mo><mml:mn>1</mml:mn></mml:math>Perturbation Fields in the JET Tokamak
|Physical Review Letters|2007|595
A first-principles predictive model of the pedestal height and width: development, testing and ITER optimization with the EPED model
|Nuclear Fusion|2011|452
Overview of the SPARC tokamak
|Journal of Plasma Physics|2020|452
Chapter 6: Steady state operation
|Nuclear Fusion|2007|379