TY - JOUR
T1 - Tomography of the 1995 Kobe earthquake area
T2 - Comparison of finite-frequency and ray approaches
AU - Tong, Ping
AU - Zhao, Dapeng
AU - Yang, Dinghui
PY - 2011/10
Y1 - 2011/10
N2 - We determined a detailed 3-D crustal model in the 1995 Kobe earthquake (M 7.2) area in southwest Japan using both finite-frequency and ray tomography methods. Our finite-frequency tomography technique is based on the single-scattering theory. The finite-frequency sensitivity kernel derived in this study reflects correctly the sensitivity of the heterogeneity off the geometrical ray path and the existence of Fresnel volume, and the kernel depends on the dominant frequency of the observed wave. The dominant frequency is estimated directly from the earthquake magnitude based on a relation that is obtained by regressively analyzing the displacement spectra of 20 earthquakes in the study area. We used 141118 P-wave and 133648 S-wave high-quality arrival-time data from 2813 Kobe aftershocks and 3140 other local earthquakes during 1995-2010. The tomographic images obtained with the finite-frequency and ray tomography methods show a high level of similarity, which is verified quantitatively by adopting the structural similarity index. Our results show that the Kobe main shock hypocentre is located in a distinctive zone characterized by a high Poisson's ratio and a low product VP×VS of P- and S-wave velocities, which is interpreted as a fluid-filled, fractured rock matrix that may have triggered the 1995 Kobe earthquake.
AB - We determined a detailed 3-D crustal model in the 1995 Kobe earthquake (M 7.2) area in southwest Japan using both finite-frequency and ray tomography methods. Our finite-frequency tomography technique is based on the single-scattering theory. The finite-frequency sensitivity kernel derived in this study reflects correctly the sensitivity of the heterogeneity off the geometrical ray path and the existence of Fresnel volume, and the kernel depends on the dominant frequency of the observed wave. The dominant frequency is estimated directly from the earthquake magnitude based on a relation that is obtained by regressively analyzing the displacement spectra of 20 earthquakes in the study area. We used 141118 P-wave and 133648 S-wave high-quality arrival-time data from 2813 Kobe aftershocks and 3140 other local earthquakes during 1995-2010. The tomographic images obtained with the finite-frequency and ray tomography methods show a high level of similarity, which is verified quantitatively by adopting the structural similarity index. Our results show that the Kobe main shock hypocentre is located in a distinctive zone characterized by a high Poisson's ratio and a low product VP×VS of P- and S-wave velocities, which is interpreted as a fluid-filled, fractured rock matrix that may have triggered the 1995 Kobe earthquake.
KW - Crustal structure
KW - Dynamics: seismotectonics
KW - Earthquake dynamics
KW - Seismic tomography
KW - Seismicity and tectonics
KW - Wave propagation
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U2 - 10.1111/j.1365-246X.2011.05139.x
DO - 10.1111/j.1365-246X.2011.05139.x
M3 - Article
AN - SCOPUS:80052970613
SN - 0956-540X
VL - 187
SP - 278
EP - 302
JO - Geophysical Journal International
JF - Geophysical Journal International
IS - 1
ER -