“…(13 , T(t,r), B(t,r)) = ρ * km (−F(t,r), T(t,r), −B(t,r)). Thus, magnetic field B on which quasi-equilibrium distribution (11) does depend explicitly may be regarded as a mechanical force and included into vector F. With the Hermitian nature of the operator taken into account, we then obtain ρkm (F(t, r), T(t, r)) = ρmk (−F(t, r)T(t, r)). (20) Equation ( 17) is equivalent to integral equation…”