Transportation of H2O associated with subduction of the Pacific plate benea
th the northeast Japan are is modeled to predict distribution of aqueous so
lution and melt, and the consequent P-wave velocity structure. The observed
velocity structure coincides well with the model for equilibrium transport
of H2O: most of H2O subducted is brought down to 150-200 km depth along th
e slab, then the aqueous fluid generated ascends to initiate melting, which
explains the low velocity regions (similar to 6% reduction) observed benea
th the backarc, rather than beneath the volcanic front. If equilibrium tran
sport of H2O occurs, initiation of melting beneath the backarc with deep su
bduction of H2O is likely to be the case also for other subduction zones wi
th slabs older than several tens of m.y., cold enough to stabilize serpenti
ne to a great depth.