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NEW_Accomplishments.indd - IRIS

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2006 <strong>IRIS</strong> 5-YEAR PROPOSAL UPWELLING AND DOWNWELLING<br />

Finite Difference Synthetic Test for Kirchhoff Migration of Receiver Function on<br />

Subducting Slab<br />

Sangwon Ham, Alan Levander, Fenglin Niu • Rice University<br />

Receiver function imaging enables higher resolution imaging than traveltime tomography, and dense and portable seismic<br />

array deployments permitting the migration techniques are possible with the Japanese seismic networks and <strong>IRIS</strong> PASS-<br />

CAL deployments. We conducted Kirchhoff migration for the synthetic data generated from two-dimentional elastic wave<br />

finite-difference modeling to verify the imaging quality of the migration code and to understand the relationship between the<br />

physical parameters of the subsurface and the migrated image (Levander, 1988; Levander 2005). The slab geometry from<br />

High-Resolution tomography in Japan (Zhao et al., 1994) was used to construct a synthetic model. We set up the parameters<br />

for the synthetic modeling, receiver function generation, and migration to simulate the geometry of the earthquake on February<br />

26, 2001, in India.<br />

We can verify that migration with a smoothed 2D version of the velocity distribution gives an improved image of the slab<br />

geometry than that with a 1D velocity model (Figure 1). We simulated the effect of various model parameters like epicentral<br />

distances (i.e. incidence angle of the incoming wave) on the migrated image. We found that the conversion coefficient in the<br />

migrated image is strongly dependent on the P-wave incidence angle, hence the epicentral distance (Figure 2). We will get<br />

more quantitative results for the effect of the subsurface parameters on the migrated image that are the subject of a forthcoming<br />

publication.<br />

Figure 1. Effect of velocity model on<br />

the migrated image. Migration with<br />

2D velocity model (right) shows<br />

better top boundary constraint of<br />

the slab geometry than that with 1D<br />

velocity model (left).<br />

Figure 2. Effect of epicentral<br />

distance on the migrated image. Migration<br />

with 55° epicental distance<br />

(right) shows stronger boundary<br />

constraint of the slab geometry than<br />

that with 45° epicental distance<br />

(left).<br />

Zhao, D., A. Hasegawa, and H. Kanamori, Deep structure of Japan subduction zone as derived from local, regional, and teleseismic events, J. Geophys. Res.,<br />

99, 22,313-22,329, 1994.<br />

Levander, A., F. Niu, C.-T.A. Lee, and X. Cheng, Imag(in)ing the Continental Lithosphere, Physics of the Earth and Planetary Interiors, accepted, 2005.<br />

This research is supported by NSF CMG 0222270<br />

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