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Article |
Institute of Geophysics and Planetary Physics
Scripps
Institution of Oceanography
University of California, San Diego
La
Jolla, California
92093-0225
vschulte{at}ucsd.edu
We measure the plane wavefront incidence azimuth for teleseismic P
at large-aperture (
50 km) broadband arrays. The incidence azimuth is
determined by crosscorrelation of the P arrivals on the vertical
component seismograms filtered in successive frequency bands. The periods
considered range from 10 to 35 sec. At the Anza array in southern California,
the plane wave direction is deflected from the great circle azimuth of the
event by up to 20°. In addition, we find a surprisingly strong frequency
dependence of the same magnitude and a striking antisymmetric pattern of the
deflection as a function of backazimuth, whereas the curvature of the
wavefront is small. Similar characteristics are found at the Gräfenberg
array in Germany and the NORSAR array in Norway, however, with much weaker
amplitudes of
5°. We ascribe the behavior at Anza to structure in the
lower crust and uppermost mantle beneath the array, given that the
observations are only a function of source backazimuth and not of source depth
and source mechanism, that the wavelengths under consideration range from 50
to 270 km, and that the sign of the deviation is opposite to that predicted
from shallow crustal structure and Moho topography. We are able to reproduce
the magnitude and frequency dependence of the wavefront deflection using
finite difference numerical modeling of plane wave propagation through simple
2D structures.
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