“…The Lg waves have been modeled as higher-mode surface waves [Herrmann and Kijko, 1983] or as multiple reflected S waves [Campillo et al, 1984;Campillo, 1990], which propagate in the crust. The characteristics of the propagation of Lg waves have been discussed for many regions [e.g., Ruzaikin et al, 1977;Campillo and Plantet, 1991;Campillo et al, 1993;Chazalon et al, 1993;McNamara et al, 1996;Shi et al, 1996;Benz et al, 1997;Rial and Ritzwoller, 1997;Rodgers et al, 1997;Mellors et al, 1999;Calvert et al, 2000] and have been studied using numerical simulations [e.g., Kennett, 1986;Maupin, 1989;Regan and Harkrider, 1989;Cao and Muirhead, 1993;Gibson and Campillo, 1994;Kennett, 1997, 1998;Vaccari and Gregersen, 1998]. It has been observed that Lg propagation becomes inefficient or is blocked if the crustal structure undergoes fast lateral changes [Ruzaikin et al, 1977;Baumgardt, 1990;Campillo et al, 1993;Chazalon et al, 1993] or if the travel path crosses oceanic crust [Press and Ewing, 1952;Knopoff et al, 1979;Kennett et al, 1985;Gregersen and Vaccari, 1993;Shapiro et al, 1996].…”