The transition between the anomalous diffusion previously reported in pulsed multipoles and classical diffusion has been observed at low poloidal magnetic fields, B≲100 G. The helium plasma parameters were ne =1010–1011 cm−3, Ti∼Te∼0.2 eV. The anomalous diffusion seen at higher magnetic fields scaled like vortex diffusion, but the transition point corresponds to a nonthermal vortex spectrum with effective temperature, T*∼106 eV. Transition from anomalous to classical regime is observed on a classical viscous damping time scale.
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Navratil et al. (1977) studied this question.
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