T. Stern et al., Teleseismic P wave delays and modes of shortening the mantle lithosphere beneath South Island, New Zealand, J GEO R-SOL, 105(B9), 2000, pp. 21615-21631
A high-speed zone in the mantle directly beneath the Southern Alps of New Z
ealand is required by the recorded pattern of teleseismic P waves. Two para
llel lines of 80 seismographs spaced at similar to 2 km intervals recorded
three earthquakes from the western Pacific with epicentral distances of 52
degrees, 53 degrees and 78 degrees. Azimuthal bearings were all within 15 d
egrees of the mean trends of the seismograph lines. Differences between mea
sured delays and those predicted from the crustal structure reach 0.8 s alo
ng one line and 1.0 s along the other, with the rays for the earliest arriv
ing signals passing the depth of similar to 120 km beneath the center of th
e island. Assuming these early arrivals are due to structure within the man
tle shallower than 200 km, they imply that the core of the high-speed zone
lies beneath the thickest crust, which has been shortened by similar to 100
km of convergence during the past 6-7 Myr. Although the shape and position
of the high-speed body cannot be fixed uniquely, a roughly symmetric body
centered about a depth of 120 km, 80-100 km wide, with a depth extent of 10
0 km and with a maximum speed advance of similar to 7% satisfies the observ
ations. The pattern of residuals does not fit with those predicted by simpl
e models of intracontinental subduction in which crust and mantle lithosphe
re are detached and one slab of mantle lithosphere underthrusts the other.
Rather, the residuals favor thickening of mantle lithosphere by a more homo
genous straining of it, as if mantle lithosphere beneath continental crust
behaved as a continuum. An excess mass in the mantle is also required by th
e observed gravity anomalies, once allowance is made for the seismically de
termined crustal thickness. This high-density mantle anomaly provides suffi
cient force (per unit length) to maintain the crustal root, which is approx
imately twice as thick as that necessary to support the topography.