Accelerating seismicity and stress accumulation before large earthquakes

The stress field that existed before a large earth- quake can be calculated based on the known source parame- ters of the event. This stress field can be used to define a region that shows greater seismic moment rate changes prior to the event than arbitrarily shaped regions, allowing us to link two previously unrelated subjects: Coulomb stress interactions and accelerating seismicity before large earthquakes. As an example, we have examined all M≥6.5 earthquakes in California since 1950. While we illustrate the model using seismicity in California, the technique i s general and can be applied to any tectonically active re- gion. We show that where sufficient knowledge of the re- gional tectonics exists, this method can be used to aug- ment current techniques for seismic hazard estimation.

[1]  John B. Rundle,et al.  A physical model for earthquakes: 3. Thermodynamical approach and its relation to nonclassical theories of nucleation , 1989 .

[2]  Bertrand Meyer,et al.  Seismic hazard in the Marmara Sea region following the 17 August 1999 Izmit earthquake , 2000, Nature.

[3]  H. Johnson,et al.  A new statistical test for static stress triggering: Application to the 1987 Superstition Hills earthquake sequence , 1999 .

[4]  L. Sykes,et al.  Evolution of the stress field in southern California and triggering of moderate-size earthquakes: A 200-year perspective , 1997 .

[5]  Lawrence W. Braile,et al.  Intermediate-term earthquake prediction using precursory events in the New Madrid Seismic Zone , 1998, Bulletin of the Seismological Society of America.

[6]  Ruth A. Harris,et al.  Introduction to Special Section: Stress Triggers, Stress Shadows, and Implications for Seismic Hazard , 1998 .

[7]  Claude J. Allègre,et al.  Introduction of scaling techniques in brittle fracture of rocks , 1994 .

[8]  Yehuda Ben-Zion,et al.  Earthquake cycle, fault zones, and seismicity patterns in a rheologically layered lithosphere , 2001 .

[9]  Didier Sornette,et al.  Discrete scale invariance, complex fractal dimensions, and log‐periodic fluctuations in seismicity , 1996 .

[10]  David J. Varnes,et al.  Predictive modeling of the seismic cycle of the Greater San Francisco Bay Region , 1993 .

[11]  C. Sammis,et al.  Seismic Cycles and the Evolution of Stress Correlation in Cellular Automaton Models of Finite Fault Networks , 1999 .

[12]  L. R. Sykes,et al.  Evolving Towards a Critical Point: A Review of Accelerating Seismic Moment/Energy Release Prior to Large and Great Earthquakes , 1999 .

[13]  G. King,et al.  Stress coupling between earthquakes in northwest Turkey and the north Aegean Sea , 1996 .

[14]  Lynn R. Sykes,et al.  Evolution of moderate seismicity in the San Francisco Bay region, 1850 to 1993: Seismicity changes related to the occurrence of large and great earthquakes , 1996 .

[15]  D. Sornette,et al.  Precursors, aftershocks, criticality and self-organized criticality , 1998 .

[16]  R. Simpson,et al.  In the shadow of 1857‐the effect of the Great Ft. Tejon Earthquake on subsequent earthquakes in southern California , 1996 .

[17]  Massimo Cocco,et al.  Fault interaction by elastic stress changes: New clues from earthquake sequences , 2001 .

[18]  J. C. Savage A dislocation model of strain accumulation and release at a subduction zone , 1983 .

[19]  Didier Sornette,et al.  Complex Critical Exponents from Renormalization Group Theory of Earthquakes: Implications for Earthquake Predictions , 1995 .

[20]  D. Sornette,et al.  An observational test of the critical earthquake concept , 1998 .

[21]  D. Jackson,et al.  Dislocation model for aseismic crustal deformation at Hollister, California , 1986 .

[22]  James H. Dieterich,et al.  Progressive failure on the North Anatolian fault since 1939 by earthquake stress triggering , 1997 .

[23]  Y. Okada Internal deformation due to shear and tensile faults in a half-space , 1992, Bulletin of the Seismological Society of America.