“…In previous works [1] we described the expansion of (1) in the small parameter δ = τ t,b /τ D , where τ t,b is the electron's transit or bounce time, and τ D is a typical time for radial drift of the electron. The result, in analogy with standard neoclassical theory [3,4], is f = f 0 + δf 1 = f 0 +f + g,where…”