Bulletin of the Seismological Society of America
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Bulletin of the Seismological Society of America; February 2006; v. 96; no. 1; p. 328-333; DOI: 10.1785/0120050074
© Seismological Society of America
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Figure 004


Figure 4. (a) and (b) Comparisons between the principal component of deconvolved seismograms and synthetic seismograms. For time-domain deconvolution (T.D.), we applied a Gaussian filter: G(f) = exp(–{pi}2f2/a2), where f is frequency and a is the Gaussian width (set to 5 sec–1). For frequency- domain deconvolution (F.D.), we used a six-pole, zero-phase Butterworth filter between 0.1 and 1.2 Hz. (c) Crustal model used to generate synthetic seismograms by the reflectivity algorithm of Randall (1989). For crustal thickness and VS, we smooth the model of Rai et al. (2003) with a single, linear gradient in the crust. The gradient of VP is assumed to be 0.025 km/ sec/km, close to the global average of 0.031 km/sec/ km (Christensen and Mooney, 1995).





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