“…, generalizes the ones given in [4,13,18,21,22] and in the references therein, in the context of more specific diffusion processes. Moreover, the representation formula of the weak solution used in [13,18,22] is a byproduct of the Duhamel formula (2.3) that is established in theorem 2.1 for a wider set of source terms lying in S ′ + (R, L 2 (Ω)). It is worth pointing out that theorem 2.1 holds provided that the elliptic part A of the diffusion equation (1.1) is symmetric.…”