“…We point out that the motion of theP R,K -superdiffusion remains unchanged and it is therefore different from the motion of the P R,K -branching diffusion in Definition 4. However, setũ R f (x, t) = λ * (1 − p K (x))(1 − u R f (x, t)), where u R f is the Laplace functional of theP R,K -branching diffusion (Laplace functionals for branching diffusions are defined in a similar fashion to Lemma 6, see for instance Section 4.1.4 [Dyn02]). Then together with the relations (6.5) and (6.6) we can find thatũ R f is the Laplace functional of theP R,K -superdiffusion.…”