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Electromagnetic gyrokinetic turbulence in finite-beta helical plasmas
Author(s) -
A. Ishizawa,
T. Watanabe,
H. Sugama,
S. Maeyama,
N. Nakajima
Publication year - 2014
Publication title -
physics of plasmas
Language(s) - English
Resource type - Journals
SCImago Journal Rank - 0.75
H-Index - 160
eISSN - 1089-7674
pISSN - 1070-664X
DOI - 10.1063/1.4876960
Subject(s) - microturbulence , physics , turbulence , tokamak , plasma , flux tube , shearing (physics) , zonal flow (plasma) , large helical device , mechanics , ballooning , magnetic field , field line , saturation (graph theory) , convection , toroid , atomic physics , magnetic flux , quantum mechanics , thermodynamics , mathematics , combinatorics
A saturation mechanism for microturbulence in a regime of weak zonal flow generation isinvestigated by means of electromagnetic gyrokinetic simulations. The study identifies a newsaturation process of the kinetic ballooning mode (KBM) turbulence originating from the spatial structure of the KBM instabilities in a finite-beta Large Helical Device (LHD) plasma.Specifically, the most unstable KBM in LHD has an inclined mode structure with respect to the mid-plane of a torus, i.e., it has a finite radial wave-number in flux tube coordinates, in contrast to KBMs in tokamaks as well as ion-temperature gradient modes in tokamaks and helical systems. The simulations reveal that the growth of KBMs in LHD is saturated by nonlinear interactions of oppositely inclined convection cells through mutual shearing as well as by the zonal flow. The saturation mechanism is quantitatively investigated by analysis of the nonlinear entropy transfer that shows not only the mutual shearing but also a self-interaction with an elongated mode structure along the magnetic field line

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