Two end member models of how the high elevations in Tibet formed are (i) co
ntinuous thickening and widespread viscous flow of the crust and mantle of
the entire plateau and (ii) time-dependent, localized shear between coheren
t lithospheric blocks. Recent studies of Cenozoic deformation, magmatism, a
nd seismic structure lend support to the latter. Since India collided with
Asia similar to 55 million years ago, the rise of the high Tibetan plateau
likely occurred in three main steps, by successive growth and uplift of 300
- to 500-kilometer-wide crustal thrust-wedges. The crust thickened, while t
he mantle, decoupled beneath gently dipping shear zones, did not. Sediment
infilling, bathtub-like, of dammed intermontane basins formed flat high pla
ins at each step. The existence of magmatic belts younging northward implie
s that stabs of Asian mantle subducted one after another under ranges north
of the Himalayas. Subduction was oblique and accompanied by extrusion alon
g the left lateral strike-slip faults that slice Tibet's east side. These m
echanisms, akin to plate tectonics hidden by thickening crust, with slip-pa
rtitioning, account for the dominant growth of the Tibet Plateau toward the
east and northeast.