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Laramide-style uplifts occurring in South America are<br />

similar to those found in the Southern Rockies that formed<br />

~ 55 Ma. Andean studies provide a natural laboratory for<br />

contrasting lithospheric deformation and volcanic patterns.<br />

These patterns range between flat-slab subduction near 30°S,<br />

which is producing a volcanic gap with characteristic basement-rooted,<br />

Laramide-style uplifts, to steep slab subduction<br />

at 36°S, where a normal volcanic arc exists.<br />

depth (km)<br />

0<br />

100<br />

200<br />

300<br />

400<br />

500<br />

600<br />

Fiji LR CLSC VF<br />

dVp km/s<br />

200 400 600 800 1000 1200 1400<br />

Active and passive seismic experiments employing land and<br />

ocean bottom seismographs have probed subduction-related<br />

processes in the accretionary wedge, the seismogenic zone,<br />

the oceanic crust, and mantle wedge in a variety of trenches,<br />

including those in Central American, Cascadia, Alaska,<br />

and the western Pacific (Figure 5). In Cascadia and Alaska,<br />

high-resolution scattered wave and tomographic images of<br />

the descending plate and the mantle wedge have been used<br />

to identify zones of hydration and serpentinization in the<br />

mantle wedge, and track dehydration and eclogization of<br />

subducting oceanic crust.<br />

The Indian-Asian plate collision zone has produced Earth’s<br />

most extreme topography as ocean-continent subduction<br />

evolved into continent-continent collision. A large<br />

number of recent PASSCAL-supported controlled- and<br />

natural-source experiments have produced a much greater<br />

understanding of large-scale orogenesis and its structural<br />

underpinnings. In the early investigations in Tibet, for<br />

example, combined controlled- and passive-source investigations<br />

identified a wide-spread midcrustal low-velocity zone<br />

beneath the Tibetan plateau that is topped by seismic bright<br />

spots. These observations have been interpreted as a plateauwide<br />

partial melt zone, capped by either lenses of melt and/<br />

or melt-derived fluids. A similar widespread zone of partial<br />

melt was subsequently identified under the Altiplano of the<br />

Andes. More recent experiments have examined mantle<br />

flow fields created adjacent to the edges of collision zone, as<br />

Eurasia deforms in response to the collision. The seismologic<br />

database in Tibet and the Himalayas have led to several<br />

models of lithospheric descent under the Tibetan plateau;<br />

debate still exists as to whether the lithosphere consumption<br />

is one-sided or two-sided (i.e, whether the Indian mantle<br />

lithosphere is subducting alone, or both Indian and the<br />

Eurasian mantle lithosphere are descending into the mantle).<br />

depth (km)<br />

depth (km)<br />

dVp km/s<br />

0<br />

100<br />

200<br />

300<br />

400<br />

500<br />

600<br />

Fiji<br />

dVs km/s<br />

0<br />

100<br />

200<br />

300<br />

400<br />

500<br />

600<br />

dVp/Vs<br />

0.6 0.4 0.2 0 0.2 0.4 0.6<br />

LR<br />

CLSC<br />

dVs km/s<br />

Figure 5. Mantle seismic velocity structure of the Tonga subduction<br />

zone and Lau back arc basin as determined by broadband ocean<br />

bottom seismometers and PASSCAL instruments. Crustal structure is<br />

constrained by seismic refraction results. The figure shows (a) dVp, (b)<br />

dVs, and (c) d(Vp/Vs) anomalies relative to the IASP91 velocity model,<br />

contoured at 0.08 km/s for Vp, 0.06 km/s for Vs, and 0.012 units for<br />

Vp/Vs. Earthquake hypocenters are shown as black circles. The central<br />

Lau spreading center (CLSC) shows a large dVp/Vs anomaly in the<br />

uppermost mantle extending to ~100 km depth, with an anomaly<br />

amplitude larger than expected from thermal effects alone, suggesting<br />

a wide zone of melt production. (From Condor and Wiens, 2006)<br />

VF<br />

200 400 600 800 1000 1200 1400<br />

Fiji<br />

0.5 0 0.5<br />

LR<br />

CLSC<br />

VF<br />

dVp/Vs<br />

200 400 600 800 1000 1200 1400<br />

distance (km)<br />

0.1 0.05 0 0.05

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