It is shown that electron transport due to a generic low-frequency electrostatic turbulence in tokamak geometry results in the relaxation to a peaked, self-sustained plasma density profile n₀(r), rather than to a diffusion-induced flat distribution. The relaxed density profile depends on the magnetic geometry and the distribution of turbulence. The associated inward pinch velocity Vᵣ0ex0ex=0ex0exD∇lnn₀ results from the competition of the turbulent diffusion of trapped electrons over the poloidal magnetic flux coordinate ψ and the collisional relaxation toward a Maxwellian distribution function.
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Isichenko et al. (1995) studied this question.
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