“…In fact, taking the oscillations into account, we find that the decay of the envelope M (q, t) depends on the order of the leading nonlinearity of the theory. In the cubic case, M ∝ t −2/3 , while a faster decay, M ∝ t −1 , is found in the quartic one, see equations (17,31). As a consequence, in the two cases, the decay of G(q, t) is, respectively, anomalous (i.e.…”