“…First, in Section 3 we derive upper-bounds for the oscillations |R H1,H2 pt, ωq ´RH1,H2 ps, ωq| that are sharp enough to imply the finiteness of the limits ( 5), ( 6) and (7). This is done by means of the wavelet-type expansion given in [6], see Theorem 3.3 below. Then, in Section 4, we give lower bounds for the so-called wavelet-leaders, see Section 2, of the generalized Rosenblatt process on a given compactly supported wavelet basis.…”