Xj. Song et al., BROAD-BAND MODELING OF REGIONAL SEISMOGRAMS - THE BASIN AND RANGE CRUSTAL STRUCTURE, Geophysical journal international, 125(1), 1996, pp. 15-29
Three-component broad-band displacement seismograms with paths samplin
g the Basin and Range province are studied to constrain the crustal st
ructure. To find an average model that fits the data in both absolute
time and waveform, we generate broad-band reflectivity synthetics and
conduct sensitivity tests on different parts of a layered crustal mode
l, where only a few layers are involved. Generalized rays are used to
help identify the various phases. It proves useful to decompose a regi
onal seismogram into segments so that the impact of model parameters o
n each segment can be clearly identified. Thus, for mid-crustal earthq
uakes, it is established that the top crustal layer controls the Rayle
igh wave, the Airy phase, in shape over the range from 300 to 600 km,
and the crustal layer just above the source depth controls its timing.
The P-nl waves, the P-n and P-L portion, are controlled in broad-band
character by the mid-crust while the top layer contributes to their l
ong-period motion. These crustal parameters control the tangential mot
ion similarly. The SV wave, the segment between the P-nl wave and the
Rayleigh wave, is mostly controlled by the shear velocity of the lower
crust. In judging the goodness of fit between the array observations
and synthetic waveforms, we allow individual data segments to shift re
lative to the 1-D synthetics by a few seconds to account for some late
ral variation. The amount of time shift is found by the cross-correlat
ion in displacement between the data segment and the synthetics. Apply
ing these tests in a forward modelling approach, we find that a simple
two-layer crustal model is effective in explaining this data set. In
this model, the main crustal layer has P and S velocities of 6.1 km s(
-1) and 3.6 km s(-1), similar to those found by Langston & Helmberger
(1974). A surface layer of thickness 2.5 to 3.5 km is required to fit
the Rayleigh waves. The refined model can be used as a reference model
for further studies in this region.