Characterize the relation between diffusion-induced streaming flux and Dμμ
Characterize and derive the relation between diffusion-induced streaming flux in pitch-angle space and the pitch-angle diffusion coefficient so that the total flux can be decomposed into streaming and diffusive components and Dμμ can be solved near the source in the stationary method.
References
Whether or not this can be directly translated to the streaming flux is unclear because it follows from the Fokker-Planck equation (see, e.g., vandenBerg2023) that \begin{align} \frac{\partial f}{\partial t} & = - \frac{\partial}{\partial \mu} \left[ \left\langle \frac{\Delta \mu}{\Delta t} \right\rangle f \right] + \frac{\partial2}{\partial2 \mu} \left[ \left\langle \frac{(\Delta \mu)2}{2\Delta t} \right\rangle f \right] \nonumber \ & = \frac{\partial}{\partial \mu} \left[ \left\langle \frac{(\Delta \mu)2}{2 \Delta t} \right\rangle \frac{\partial f}{\partial \mu} \right] \nonumber \ & = - \frac{\partial \dot{\cal N}{\partial \mu}, \end{align} implying a total flux of $\dot{\cal N} = - \langle (\Delta \mu)2 / 2 \Delta t \rangle$, which is again just Fick's law. Hence, if it is unknown exactly how such a ‘diffusion-induced streaming’ flux is related to the diffusion coefficient, then $\dot{\cal N} = \dot{\cal N}{\rm stream} - D{\mu\mu} ({\rm d}F / {\rm d}\mu)$ cannot be solved for the diffusion coefficient.