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DEPARTMENT OF TERRESTRIAL MAGNETISM CARNEGIE INSTITUTION OF WASHINGTON, 5241 BROAD BRANCH ROAD, N.W., WASHINGTON, D.C. 20015
Abstract
A method is proposed for retrieving source-extent parameters from far-field body-wave data. At low frequency, the normalized P- or S-wave displacement amplitude spectrum can be approximated by |
^(r^,
)| = 1
2(r^)
2/2 where r^ specifies a point on the focal sphere. For planar dislocation sources,
2(r^) is linearly related to statistical measures of source dimension, source duration, and directivity.
2(r^) can be measured as the curvature of |
^(r^,
)| at
= 0 or the variance of the pulse
^(r^,t). The quantity
is contrasted with the traditional corner frequency
0, defined as the frequency at the intersection of the low- and high-frequency trends of |
^(r^,
)|. For dislocation models without directivity,
c(P)
c(S) for any r^. A mean corner frequency defined by averaging
2(r^) over the focal sphere,
, satisfies
c(P) >
c(S) for any dislocation source. This behavior is not shared by
0. It is shown that
0 is most sensitive to critical times in the rupture history of the source, whereas
c is determined by the basic parameters of source extent. Evidence is presented that
c is the corner frequency measured on actual seismograms. Thus, the commonly observed corner frequency shift (P-wave corner greater than the S-wave corner), now viewed as a shift in
c is simply a result of spatial finiteness and is expected to be a property of any dislocation source. As a result, the shift cannot be used as a criterion for rejecting particular dislocation models.
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