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Influence of plasma pedestal profiles on access to ELM-free regimes in ITER
Authors:S. Yu. Medvedev  A. A. Ivanov  A. A. Martynov  Yu. Yu. Poshekhonov  S. V. Konovalov  A. R. Polevoi
Affiliation:1.Keldysh Institute of Applied Mathematics,Russian Academy of Sciences,Moscow,Russia;2.National Research Nuclear University “MEPhI,”,Moscow,Russia;3.National Research Centre Kurchatov Institute,Moscow,Russia;4.ITER Organization,St. Paul Lez Durance Cedex,France
Abstract:The influence of current density and pressure gradient profiles in the pedestal on the access to the regimes free from edge localized modes (ELMs) like quiescent H-mode in ITER is investigated. Using the simulator of MHD modes localized near plasma boundary based on the KINX code, calculations of the ELM stability were performed for the ITER plasma in scenarios 2 and 4 under variations of density and temperature profiles with the self-consistent bootstrap current in the pedestal. Low pressure gradient values at the separatrix, the same position of the density and temperature pedestals and high poloidal beta values facilitate reaching high current density in the pedestal and a potential transition into the regime with saturated large scale kink modes. New version of the localized MHD mode simulator allows one to compute the growth rates of ideal peeling-ballooning modes with different toroidal mode numbers and to determine the stability region taking into account diamagnetic stabilization. The edge stability diagrams computations and sensitivity studies of the stability limits to the value of diamagnetic frequency show that diamagnetic stabilization of the modes with high toroidal mode numbers can help to access the quiescent H-mode even with high plasma density but only with low pressure gradient values at the separatrix. The limiting pressure at the top of the pedestal increases for higher plasma density. With flat density profile the access to the quiescent H-mode is closed even with diamagnetic stabilization taken into account, while toroidal mode numbers of the most unstable peeling-ballooning mode decrease from n = 10?40 to n = 3?20.
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