“…In addition, in nature, the potential seismogenic volume, hence the released magnitude, is often reduced by regional factors, such as lithological, fluids pressure and thermal variations modifying the frictional behavior of rocks determining creeping versus locked portions of the faults (Ahrens, 1995;Albaric et al, 2009;Doglioni, Barba, et al, 2015;Keefner et al, 2011;Scholz, 1988;Sibson, 1983), along-strike discontinuity of faults limiting the potential dimension of single coseismic ruptures (Bonini et al, 2010;Butler et al, 2006;Calamita, 1990;Carrera et al, 2006;Goldsworthy et al, 2002). It is also observed that, while the steeper (40°-70°) normal fault rupture tends to propagate cutting the entire brittle crust (Chiarabba & De Gori, 2016;Marone & Scholz, 1988;Petricca et al, 2015;Sibson, 1986), thrust faults are less inclined (0-45°) and do not necessarily reach the BDT (Hyndman et al, 1997). For given convergence and subduction rates, the depth of the decollement in an accretionary prism determines the volume of the accreted rocks: The deeper the decollement, the largest the volume.…”