Cross-field electron heat diffusion due to thermally excited high frequency electrostatic waves propagating almost perpendicular to the magnetic field is studied using a 2–1 /2-dimensional simulation code. It is shown that the electron heat diffusion coefficient D H is an order of magnitude greater than the electron particle diffusion coefficient D p , which is essentially collisional. The characteristic feature of wave transport is observed, namely an increase of D H with increasing values of the characteristic temperature scale length L x . The heat diffusion coefficients D // H and D ⊥ H for the parallel and perpendicular temperatures ( D H ≃ D // H + D ⊥ H ) show quite different magnetic field scalings since D // H is due to ion modes while D ⊥ H arises from electron modes. This is also confirmed by treating the ions as an immobile background.
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Hiroshi Naitou (1980) studied this question.
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