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A self-consistent model of the L to H transition is derived from coupled nonlinear envelope equations for the fluctuation level and radial electric field shear Eᵣ^'. These equations exhibit a supercritical bifurcation between dual L-mode and H-mode fixed points. The transition occurs when the turbulence level is large enough for the Reynolds stress drive to overcome the damping of the E×{}B flow. This defines a power threshold for the transition, which is calculated and found to be consistent with experimental findings.
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Diamond et al. (1994) studied this question.
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