Mk. Savage et Af. Sheehan, Seismic anisotropy and mantle flow from the Great Basin to the Great Plains, western United States, J GEO R-SOL, 105(B6), 2000, pp. 13715-13734
Shear wave splitting and P, SKS, and S travel time residuals are calculated
for teleseismic arrivals recorded on the Colorado Plateau-Great Basin Prog
ram far Array Seismic Studies of the Continental Lithosphere (PASSCAL) port
able broadband seismic deployment and for permanent stations in the western
United States. Little shear wave splitting is observed for broadband recor
dings in the northern Colorado Plateau, the Rocky Mountains, or the central
Great Basin. The transition between the Colorado Plateau and the Great Bas
in is marked by moderate shear wave splitting (1.0 s) and unusually late te
leseismic phase arrivals. This suggests material with a higher content of m
antle melt or volatiles than regions to either side. Splitting in the trans
ition between the Colorado Plateau and Great Basin is part of a pattern of
fast polarizations that align in a semicircle, surrounding a central Great
Basin region of null (no splitting) measurements. Away from the California
plate boundary, splitting to the north and south of our study region aligns
roughly parallel to the absolute plate motion of the North American plate.
No simple spatial relation of splitting with geological and geophysical fe
atures such as mountain ranges, velocity anomalies, gravity, magnetics, or
heat flow is evident in most of the western United States. However, splitti
ng in the Great Basin is compatible with asthenospheric flow. The smallest
shear wave splitting delay times coincide with the Eureka Low in heat flow,
also having low S velocity at 300 km depth. We suggest that the circumfere
ntial pattern of fast polarization directions ringing a central region of n
ulls in the Great Basin is caused by mantle flow, by the interaction of man
tle upwelling and the absolute motion of the North American plate.