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IUGG XXIV General Assembly July 2-13, 2007 Perugia, Italy<br />

(S) - <strong>IASPEI</strong> - International Association of Seismology and Physics of the Earth's<br />

Interior<br />

JSS012 Poster presentation 2209<br />

Gaussian-beam receiver function synthetics in a 3-D heteregeneous<br />

medium with velocity discontiuities at the Japan subduction zone<br />

Prof. Kazuro Hirahara<br />

Geophysics, Graduate School of Science Kyoto University <strong>IASPEI</strong><br />

Takashi Tonegawa, Takuro Shibutani<br />

We have constructed receiver functions (RFs) observed at high-density broadband and short-period<br />

stations over the Japan Islands to map the Moho beneath the Japan Islands, the slab top and the<br />

oceanic crust of the Pacific and the Philippine Sea slabs, and the lower boundary of the Pacific slab, 410<br />

and 660 km velocity discontinuities. . The mapping, however, depends on the reference velocity model.<br />

Only radial RFs (RRFs) have been employed, though the transverse RFs (TRFs) have considerable<br />

amplitudes in relation to subducting slabs. We propose RF tomography which combines the travel time<br />

tomography and the RF analyses to obtain the 3-D velocity structure including velocity discontinuities.<br />

RF tomography requires iterative forward modeling of RFs in a 3-D heterogeneous medium. The recent<br />

advancement of computer power enables us to synthesize short-period waveforms with SEM and FDM.<br />

However, iterative synthesizing of RFs in RF tomography is still formidable. We extend a computer code<br />

GBM3D (Sekiguchi,1992), which can treat only the waves from the source in the model space and the<br />

plane waves incident vertically at the bottom. Therefore, we implement calculation of teleseismic<br />

waveforms with arbitrarily incident angles in the followings. As in the original code, we assume the 3-D<br />

heterogeneous velocity, Q and density structure in each layer which are interpolated by 3-D cubic spline<br />

functions and the layer boundaries are represented by 2-D ones. We set the dense grids at the bottom<br />

and calculate the slowness vectors and travel times at the grids from a teleseismic source, assuming a<br />

1-D earth model outside of the modeling space. From each grid, we execute kinematic and dynamic raytracings<br />

for a variety of phases, and sum up beams with Gaussian weights to synthesize waveforms at<br />

stations. It has been pointed out that GBM has the several tuning parameters and seems to be less<br />

reliable in some cases. For almost vertical incident teleseismic waves, calculations are stable if ray<br />

beams with enough density are summed. Then RRFs and TRFs are calculated from the synthetic<br />

waveforms. We present the modeling of RFs which include the Ps phases converted at the Moho and<br />

the upper mantle discontinuities with comparisons of observed RFs observed at several regions. The<br />

first is theKii Peninsula region where the Philippine Sea slab subducts steeply with a 3-D complex<br />

configuration, and RF analyses (e.g., Yamauchi et al., 2003) have provided the structure of the slab top<br />

and the subducting oceanic crust. The second is the Tohoku region, where RF analyses have clarified<br />

the subducting oceanic crust overlying the Pacific slab and the lower boundary of the slab, and other<br />

phases. The third is the 410 km and 660km discontinuities across and around the stagnant Pacific slab.<br />

Keywords: receiver function, gaussian beam method, subducting slab

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