Square-root-radius diffusion transform ($x=\sqrt{r},g=\sqrt{r}{\bar{\nu }}_0{\Sigma }_1,g_t=3q{\bar{\nu }}_0{g}_{xx}/(4r)$)

For a steady zero-mass-flux background and constant viscous transport response exponent, this change removes the first derivative in the radial diffusion operator. If ${\Sigma }_0\propto r^{-p}$, the kinematic viscosity scales as $r^{p-1/2}$, so the transformed diffusivity scales as $x^{2p-3}$. It is constant at $p=3/2$.