D. Comte et G. Suarez, STRESS-DISTRIBUTION AND GEOMETRY OF THE SUBDUCTING NAZCA PLATE IN NORTHERN CHILE USING TELESEISMICALLY RECORDED EARTHQUAKES, Geophysical journal international, 122(2), 1995, pp. 419-440
The stress distribution along the subducting Nazca plate in northern C
hile is analysed using focal mechanism solutions obtained from the inv
ersion of long-period P, SV, and SH waveforms of 15 earthquakes (m(b)
greater than or equal to 5.5), and from 212 events with reported focal
mechanisms, which occurred between 1962 and 1993. A joint hypocentral
determination was carried out to control the depth of 261 events (m(b
) greater than or equal to 5.0) recorded at teleseismic distances. A c
hange from tensional to compressional stress field along the upper par
t of the subucting slab is associated with the maximum depth extent of
the coupled zone. This change occurs in northern Chile at similar to
200-250km from the trench, at depths of similar to 60 +/- 10 km. This
depth is larger than the maximum depth observed for the thrusting inte
rplate events (40 +/- 10 km), probably meaning that, at depths of betw
een 40 and 60 km, large low-dip angle thrust events do not nucleate. S
eismic slip, however, probably extends down to 40 km in depth. The sha
llow dip angle (up to 60 km in depth) of the Wadati-Benioff zone does
not show variations along the strike of the trench. However, a gradual
southward flattening of the slab is observed at distances greater tha
n 200-250km from the trench. This change, observed from about 21 degre
es S, could be associated with a younger and probably more buoyant lit
hosphere than that observed to the north of this latitude. There are t
wo gaps located between the three main clusters of seismicity; these g
aps are clearly not related to detachments ill the descending litosphe
re. The first cluster is located in and beneath the seismogenic interp
late contact, and is characterized by reverse and thrust faulting even
ts over a scarce tensional activity. In the second cluster, the compre
ssional seismicity is scarce for teleseismic events and is located ben
eath the normal faulting events. The third cluster corresponds to tens
ional events. Therefore, these gaps in seismicity could be associated
with alternating changes from compressional to tensional stress field
in the subducting slab.