Solution
= Solution
With $A_i=a_{ij}x_j$ and constant $B_{ij}=b_{ij}$, the <Fokker-Planck probability current> becomes
$$
\boxed{J_i=a_{ij}x_jP-\frac12b_{ij}\frac{\partial P}{\partial x_j}.}
$$
In the stationary state we impose the stronger zero-current condition $J_i=0$, corresponding to <detailed balance>.