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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 2211<br />

Body wave travel time anomalies caused by the stagnant slab<br />

Dr. Hiroko Sugioka<br />

IFREE JAMSTEC <strong>IASPEI</strong><br />

Daisuke Suetsugu, Masayuki Obayashi, Yoshio Fukao, Yuan Gao<br />

Previous tomographic studies using short-period P times have commonly shown that the fast Pacific slab<br />

is stagnant in the mantle transition zone beneath the Philippine Sea and eastern Asia (e.g., Fukao et al.,<br />

2001). However, the fast S-velocity anomalies of the stagnant slab have been not commonly obtained<br />

from short-period S-wave time, which is based mostly on the ISC bulletin. The purpose of the present<br />

study is to determine whether the stagnant slab has fast S-velocity anomalies by analyzing arrival times<br />

picked from broadband waveforms and, if any, to determine the velocity perturbation ratio δlnVs/δlnVp<br />

(= R) of the stagnant slab. The parameter R is useful to constrain whether a lateral velocity variation is<br />

caused by thermal and/or chemical origins. We analyzed seismograms of Izu-Bonin deep events<br />

observed by three broadband seismic networks of F-net, IRIS and CDSN (China Digital Seismographic<br />

Network). The CDSN data are important since body waves observed at the CDSN stations should travel<br />

a long distance in the stagnant slab. The observed first arrivals are significantly early relative to the<br />

Iasp91 model beneath northeastern China: Travel time residuals are -3~-4 s for P-wave and -6~-8 s for<br />

S-wave, which implies that the stagnant slab has fast S-velocity anomalies as well as fast P-velocity<br />

anomalies. We computed theoretical travel times of the first P arrivals with a three-dimensional P-<br />

velocity model (Obayashi et al., 2006) using the wave-front propagation method (Sakai, 1992) in which<br />

the stagnant slab beneath the studied region has fast P-velocity anomalies of 1-1.5 %. We calculated S-<br />

wave travel times with the S-velocity model constructed from the P-velocity model using a constant R.<br />

The theoretical travel times are in good agreement with the observed one for both P- and S-wave with<br />

the value of R of ~1.7.<br />

Keywords: stagnant slab, tomography

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