It is pointed out that the use of kinetic models for drift wave transport in general makes it necessary to treat consistently the transport in both real space and velocity space. For a broad class of collisionless or marginally collisionless plasmas, nonlinear effects in velocity space will effectively remove the dissipative kinetic type wave–particle resonances, leaving only a type of fluid two-stream resonance. At the same time a two-dimensional treatment of the turbulence becomes realistic. This is important for explaining the magnitude and radial profiles of diffusion coefficients in tokamaks and may also have important consequences for low-k damping and pinch effects.
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J. Weiland (1992) studied this question.
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