Structure of the subducting Nazca plate beneath Peru

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dc.contributorVirginia Techen
dc.contributor.authorNorabuena, E. O.en
dc.contributor.authorSnoke, J. A.en
dc.contributor.authorJames, D. E.en
dc.contributor.departmentGeosciencesen
dc.date.accessed2014-01-31en
dc.date.accessioned2014-02-05T14:20:22Zen
dc.date.available2014-02-05T14:20:22Zen
dc.date.issued1994-05en
dc.description.abstractArrival times from intermediate-depth (110-150 km) earthquakes within the region of flat subduction beneath the subandean zone and foreland basins of east-central Peru provide constraints on the geometry and velocity structure of the subducting Nazca plate. Hypocentral locations and origin times for these events were determined using observations from a 15 station digitally recording locator array deployed in the epicentral region of eastern Peru. Observed P wave arrival times for coastal stations in Peru, some 3-6-degrees from the epicenters, are up to 4 s early relative to predicted arrival times based on the best fit velocity-depth model used for hypocenter locations. These large negative time residuals appear to be the result of propagation paths which have long segments in the colder, higher-velocity subducting plate. P wave travel times were modeled for the effects of the slab using three-dimensional (3-D) ray tracing. Computed ray paths show that travel times to coastal stations for the eastern Peru events can be satisfactorily modeled with average velocities relative to the surrounding mantle 6% lower within the uppermost slab (assumed on the basis of other studies to be unconverted basaltic oceanic crust 6 km thick) and 8% higher within the cold uppermost mantle of the slab. Ray tracing for this plate model shows that P wave ''shadow zones'' can occur if the source-slab-receiver geometry results in seismic rays passing through regions in which the clip angle of the slab changes significantly. Such geometries exist for seismic waves propagating to some coastal stations from intermediate-depth earthquakes located east of the Andes. Observed first-arrival times for such cases do in fact have smaller negative residuals than those for geometries which allow for ''direct'' paths at similar distances. Modeling such arrivals as internally reflected waves propagating through the high-velocity part of the plate produces a significant improvement in the travel time residuals. For the slab velocities given above, we obtain a model thickness of approximately 36 km for the cold slab interior and a slight northwest component of dip in the region of subhorizontal subduction.en
dc.identifier.citationNorabuena, E. O., J. A. Snoke, and D. E. James (1994), Structure of the subducting Nazca Plate beneath Peru, J. Geophys. Res., 99(B5), 9215-9226, doi:10.1029/94JB00126.en
dc.identifier.doihttps://doi.org/10.1029/94jb00126en
dc.identifier.issn0148-0227en
dc.identifier.urihttp://hdl.handle.net/10919/25305en
dc.identifier.urlhttp://onlinelibrary.wiley.com/doi/10.1029/94JB00126/pdfen
dc.language.isoen_USen
dc.publisherAmerican Geophysical Unionen
dc.rightsIn Copyrighten
dc.rights.urihttp://rightsstatements.org/vocab/InC/1.0/en
dc.subjectslab mantle interfaceen
dc.subjectspatial-distributionen
dc.subjectsouth-americaen
dc.subjectseismicityen
dc.subjectearthquakesen
dc.subjectlithosphereen
dc.subjecttraveltimesen
dc.subjecttectonicsen
dc.subjectwavesen
dc.subjectzoneen
dc.titleStructure of the subducting Nazca plate beneath Peruen
dc.title.serialJournal of Geophysical Research-Solid Earthen
dc.typeArticle - Refereeden

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