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Download Volume II Accomplisments (28 Mb pdf). - IRIS

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S-Velocity Mantle Structure at the Subducting Chile Ridge<br />

Simon Lloyd (Northwestern University), Suzan van der Lee (Northwestern University), Raymond M Russo (University<br />

of Florida), Diana Comte (University of Chile), Victor I Mocanu (Bucharest University), Alejandro Gallego (University of<br />

Florida), Ruth Elaine Murdie (Gold Fields Australia, St Ives Gold Mine), John C VanDecar (Carnegie Institution of Washington)<br />

At the triple junction between the Nazca, Antarctica and South American plate an actively spreading ridge is currently being subducted.<br />

The ridge continues to spread as it gets subducted beneath South America. However, no new lithosphere is formed in the process.<br />

As a result slab windows likely exist beneath the overiding plate. These gaps allow asthenospheric mantle to flow through the slab,<br />

effecting mantle chemistry and thermal regime, seismic velocities and anisotropy as well as surface geology (e.g. gaps in arc volcanism).<br />

Slab windows have successfully been imaged using P wave tomography [Russo et al., 2009]. In this study we analyze Rayleigh<br />

waves as they traverse the Chile Ridge Subduction Project (CRSP) array, in order to determine if additional constraints may be<br />

obtained from surface wave analysis.<br />

We easily cross-correlated waveforms from an event at different stations to determine the relative arrival times, which allowed<br />

us to image the wavefront as it passes through the array. Typical for many events recorded at the CRSP array are wavepaths following<br />

the boundary between the Nazca and South American plates. For these events the incoming wavefront is not perpendicular<br />

to the great circle paths connecting the source and the receivers.<br />

In order to get a first order estimate of the Rayleigh wave phase velocities we split the array into four regions defined by the<br />

73°W meridian and 46°S parallel. We then invert relative arrival times for the average phase velocity within the defined regions.<br />

We repeat the inversion for several events, and combine the results. We conclude that<br />

• Imaging Rayleigh wavefronts as they traverse the array region shows that particularly at shorter periods (e.g. 30 s) they are<br />

not perpendicular to the great circle path connecting the earthquake source and the seismometers.<br />

• This needs to be taken into consideration when determining the phase velocities.<br />

• A strong velocity contrast between the E (slow) and the W (fast) is derived from the delay times.<br />

• Possibly a similar distinction can be made between the N (fast) and the S (slow).<br />

References:<br />

Russo, R.M., VanDecar, J.C., Comte, D., Mocanu, V.I., Gallego, A. Murdie, R.E., 2010. Subduction of the Chile Ridge: upper mantle structure<br />

and flow, GSA Today, in press.<br />

Acknowledgements: This work was supported by National Science Foundation grant EAR 0538267.<br />

We deployed 39 broadband<br />

seismic stations from<br />

PASSCAL in southern Chile,<br />

aiming to investitgate the<br />

possible existence and<br />

effects of slab windows.<br />

(left) The average Rayleigh wave phase velocity in region A is distinctly higher than in the other regions. (middle)<br />

Velocites in the west of the array are clearly higher than in the east. (right) The north-south contrast is not as<br />

strong, but the south appears be slightly slower than the north.<br />

Owing to the small station spacing, the<br />

recorded waveforms are very similar at<br />

all stations. (below) For wavepaths following<br />

the boundary between the Nazca<br />

and South American plates, the incoming<br />

wavefront is not perpendicular to the<br />

great circle paths.<br />

<strong>II</strong>-180 | 2010 <strong>IRIS</strong> Core Programs Proposal | <strong>Volume</strong> <strong>II</strong> | Upper Mantle Structure and Dynamics

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