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(a) Azimuthal variation of the radial component of synthetic receiver functions for a model of a dipping layer over a half-space. The model has an interface at 25 km depth, dipping 20° toward N40°E. We used Vp = 6.3 km/ s, Vp/Vs of 1.80, and a constant ray parameter of 0.06. Note the absence of the PpPp phase (shaded region) along the strike of the dipping interface. (b) Along-strike receiver functions for the same velocity model in Figure 4a but varying dip angle. Note that the Ps amplitude is not very sensitive to the dip angle.  

(a) Azimuthal variation of the radial component of synthetic receiver functions for a model of a dipping layer over a half-space. The model has an interface at 25 km depth, dipping 20° toward N40°E. We used Vp = 6.3 km/ s, Vp/Vs of 1.80, and a constant ray parameter of 0.06. Note the absence of the PpPp phase (shaded region) along the strike of the dipping interface. (b) Along-strike receiver functions for the same velocity model in Figure 4a but varying dip angle. Note that the Ps amplitude is not very sensitive to the dip angle.  

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1] The Central American subduction zone in northern Costa Rica shows along-strike variations in both the incoming and overriding plates. By analyzing the subducting oceanic Moho (M1) and the upper plate Moho (M2) with receiver functions, we investigate the variability in the hydration state of the subducting Cocos Plate and the nature of crustal te...

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... receiver functions were computed by applying the deconvolution procedure (section 4.1) on the synthetic responses. [27] In the presence of a dipping interface, stacking to create an average receiver function risks misin- terpretation of the structure as Ps and multiples may show a strong azimuthal variation in timing, amplitude, and polarity [e.g., Cassidy, 1992;Hayes and Furlong, 2007] (Figure 4). We analyzed the azimuthal behavior of synthetic receiver functions to search for the direction at which the complica- tions are minimized. ...
Context 2
... performed this analysis by creating synthetic receiver functions using a dip- ping interface with the appropriate orientation for our study region. We found that receiver functions along the strike of the dipping interface are similar to a flat interface case, particularly for the Ps phase and the absence of PpPp phases that are observed at other back azimuths (Figure 4a). In addition, the Ps amplitude of receiver functions along the strike is not very sensitive to changes in the dip angle (Figure 4b). ...
Context 3
... found that receiver functions along the strike of the dipping interface are similar to a flat interface case, particularly for the Ps phase and the absence of PpPp phases that are observed at other back azimuths (Figure 4a). In addition, the Ps amplitude of receiver functions along the strike is not very sensitive to changes in the dip angle (Figure 4b). These observations motivated us to stack our observed receiver functions along the strike of the subducting Cocos Plate for individual stations located in the Nicoya Peninsula, in order to compare the Ps amplitude between stations. ...

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... Mann and Burke (1984) reviewed the neotectonic development of the Caribbean Plate using earthquake focal mechanism solutions, faulting, and volcanic activity. Receiver function analysis has been used to study the crustal structure of the local region of the Caribbean (Niu et al., 2007;Linkimer et al., 2010). Investigators have also attempted to image the velocity structure of the subsurface Caribbean using surface waves or teleseismic P-waves, etc., and different mantle velocity models have been proposed successively (e.g., Miller et al., 2009;Bezada et al., 2010;Harris et al., 2018;Braszus et al., 2021). ...
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