“…The stress state of these slabs is generally characterized by down‐dip compression and down‐dip tension along the top and bottom layers of the double zones, respectively [e.g., Hasegawa et al , 1978a; Kawakatsu and Seno , 1983; Matsuzawa et al , 1986]. The origin of such a stress state has been discussed, and unbending of the slab [e.g., Engdahl and Scholz , 1977; Kawakatsu , 1986], thermoelastic stresses [ Fujita and Kanamori , 1981; Hamaguchi et al , 1983; Goto et al , 1985] and sagging of the subducted slab [ Sleep , 1979] have been proposed as possible mechanisms. On the other hand, the double seismic zones observed in Cape Mendocino [ Smith et al , 1993], Alaska [ Ratchkovsky et al , 1997], northeast Taiwan [ Kao and Rau , 1999], and New Zealand [ Eberhart‐Phillips and Reyners , 1997] are relatively shallow and have lateral compression in the shallow portion and down‐dip tension in the deeper portion both for the upper and lower planes.…”