“…The above reasoning, however, does not work in the vector case treated in the next section. So, for the sake of completeness and as an introduction to the vector case, let us derive (49) anew starting from (41) when the wave function on the left-hand-side is outgoing and the ones on the right-hand-side incoming, and t > r. We assume that a out-in l,m;n,p has a far field limit according to (18) and a radiation pattern denoted by (a out-in l,m;n,p ) ∞ . Then, by taking the limits on both sides, now with respect to t instead of r, we obtain…”