“…where, again with an abuse of notation, Γ e (x 1 , x 2 ) = Γ e (x 1 , x 2 , 0), defines the inverse source problem for partially coherent sources and fields [2], [8], [11], [14], and, in particular, that of deducing second order statistics of the source from second order statistics of the radiated field on D I . In this paper, we consider the case of incoherent (i.e., delta correlated sources), for which Γ j (x , x ) = I(x )δ(x − x ), I being the intensity of the source [2], [8], [11], [14], so that eq.…”