Finite Difference Simulations of Seismic Wave Propagation for the 2007 Mw 6.6 Niigata-ken Chuetsu-Oki Earthquake: Validity of Models and Reliable Input Ground Motion in the Near-Field

Finite difference simulations of seismic wave propagation are performed in the Niigata area, Japan, for the 2007 Mw 6.6 Niigata-ken Chuetsu-Oki earthquake at low frequencies. We test three 3D structural models built independently in various studies. First aftershock simulations are carried out. The model based on 3D tomography yields correct body waves in the near field, but later phases are imperfectly reproduced due to the lack of shallow sediment layers; other models based on various 1D/2D profiles and geological interpretation provide good site responses but generate seismic phases that may be shifted from those actually observed. Next, for the mainshock simulations, we adopt two different finite source models that differ in the near-field ground motion, especially above the fault plane (but under the sea) and then along the coastline. Each model is found to be calibrated differently for the given stations. For engineering purposes, the variations observed in simulated ground motion are significant, but for seismological purposes, additional parameter calibrations would be possible for such a complex 3D case.

[1]  Philip J. Maechling,et al.  ShakeOut‐D: Ground motion estimates using an ensemble of large earthquakes on the southern San Andreas fault with spontaneous rupture propagation , 2009 .

[2]  Pierre-Yves Bard,et al.  Quantitative Comparison of Four Numerical Predictions of 3D Ground Motion in the Grenoble Valley, France , 2010 .

[3]  F. D. Martin,et al.  Verification of a Spectral-Element Method Code for the Southern California Earthquake Center LOH.3 Viscoelastic Case , 2011 .

[4]  Imaging heterogeneous velocity structures and complex aftershock distributions in the source region of the 2007 Niigataken Chuetsu-oki Earthquake by a dense seismic observation , 2008 .

[5]  J. Kristek,et al.  The finite-difference and finite-element modeling of seismic wave propagation and earthquake motion , 2007 .

[6]  J. Douglas,et al.  Influence of super-shear earthquake rupture models on simulated near-source ground motion from the 1999 Izmit, Turkey, earthquake , 2011 .

[7]  S. Aoi,et al.  Source process of the 2007 Niigata-ken Chuetsu-oki earthquake derived from near-fault strong motion data , 2008 .

[8]  J. Kristek,et al.  3D Heterogeneous Staggered-grid Finite-difference Modeling of Seismic Motion with Volume Harmonic and Arithmetic Averaging of Elastic Moduli and Densities , 2002 .

[9]  J. Douglas,et al.  A Survey of Techniques for Predicting Earthquake Ground Motions for Engineering Purposes , 2008 .

[10]  Jean Roman,et al.  Exploiting Intensive Multithreading for the Efficient Simulation of 3D Seismic Wave Propagation , 2008, 2008 11th IEEE International Conference on Computational Science and Engineering.

[11]  A. Levander Fourth-order finite-difference P-SV seismograms , 1988 .

[12]  R. Madariaga,et al.  The 1999 İzmit, Turkey, Earthquake: Nonplanar Fault Structure, Dynamic Rupture Process, and Strong Ground Motion , 2001 .

[13]  Kojiro Irikura,et al.  Three-dimensional simulation of the near-fault ground motion for the 1995 Hyogo-Ken Nanbu (Kobe), Japan, earthquake , 1998, Bulletin of the Seismological Society of America.

[14]  Peter Moczo,et al.  Time-frequency misfit and goodness-of-fit criteria for quantitative comparison of time signals , 2009 .

[15]  Mahito Watanabe,et al.  Rifting and basin inversion in the eastern margin of the Japan Sea , 1995 .

[16]  Kazuhito Hikima,et al.  Source Fault of the 2007 Chuetsu-oki, Japan, Earthquake , 2010 .

[17]  T. Kanazawa,et al.  Reactivation of ancient rift systems triggers devastating intraplate earthquakes , 2009 .

[18]  T. Furumura,et al.  Integrated Ground Motion and Tsunami Simulation for the 1944 Tonankai Earthquake Using High-Performance Supercomputers , 2009 .

[19]  T. Tada,et al.  Continuous GPS Array and Present-day Crustal Deformation of Japan , 2000 .

[20]  D. Komatitsch,et al.  An unsplit convolutional perfectly matched layer improved at grazing incidence for the seismic wave equation , 2007 .

[21]  Fabrice Dupros,et al.  MPI-OpenMP hybrid simulations using boundary integral equation and finite difference methods for earthquake dynamics and wave propagation: Application to the 2007 Niigata Chuetsu-Oki earthquake (Mw6.6) , 2011, ICCS.

[22]  T. Sagiya,et al.  Continuous GPS Array and Present-day Crustal Deformation of Japan , 2000, pure and applied geophysics.

[23]  E. Tinti,et al.  Rupture process of the 2007 Niigata‐ken Chuetsu‐oki earthquake by non‐linear joint inversion of strong motion and GPS data , 2008 .

[24]  Y. Aoki,et al.  Coseismic deformation due to the 2007 Chuetsu-oki earthquake (Mw= 6.8) , 2008 .

[25]  H. Ikeda,et al.  Crustal deformation and a preliminary fault model of the 2007 Chuetsu-oki earthquake observed by GPS, InSAR, and leveling , 2008 .

[26]  T. Kanazawa,et al.  Precise aftershock distribution of the 2007 Chuetsu-oki Earthquake obtained by using an ocean bottom seismometer network , 2008 .

[27]  C. Tsogka,et al.  Application of the perfectly matched absorbing layer model to the linear elastodynamic problem in anisotropic heterogeneous media , 2001 .

[28]  H. Aochi,et al.  Dynamic rupture of crosscutting faults: A possible rupture process for the 2007 Mw 6.6 Niigata‐ken Chuetsu‐Oki earthquake , 2010 .

[29]  Robert W. Graves,et al.  Simulating seismic wave propagation in 3D elastic media using staggered-grid finite differences , 1996, Bulletin of the Seismological Society of America.

[30]  Broadband Ground Motion Reconstruction for the Kanto Basin during the 1923 Kanto Earthquake , 2011 .