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A guide to differences between stochastic point-source and stochastic finite-fault simulations A guide to differences between stochastic point-source and stochastic finite-fault simulations

Why do stochastic point-source and finite-fault simulation models not agree on the predicted ground motions for moderate earthquakes at large distances? This question was posed by Ken Campbell, who attempted to reproduce the Atkinson and Boore (2006) ground-motion prediction equations for eastern North America using the stochastic point-source program SMSIM (Boore, 2005) in place of the...
Authors
G. M. Atkinson, K. Assatourians, D.M. Boore, K. Campbell, D. Motazedian

Microseismicity at the North Anatolian Fault in the Sea of Marmara offshore Istanbul, NW Turkey Microseismicity at the North Anatolian Fault in the Sea of Marmara offshore Istanbul, NW Turkey

The North Anatolian Fault Zone (NAFZ) below the Sea of Marmara forms a “seismic gap” where a major earthquake is expected to occur in the near future. This segment of the fault lies between the 1912 Ganos and 1999 İzmit ruptures and is the only NAFZ segment that has not ruptured since 1766. To monitor the microseismic activity at the main fault branch offshore of Istanbul below the...
Authors
Fatih Bulut, Marco Bohnhoff, William L. Ellsworth, Mustafa Aktar, Georg Dresen

Developing framework to constrain the geometry of the seismic rupture plane on subduction interfaces a priori - A probabilistic approach Developing framework to constrain the geometry of the seismic rupture plane on subduction interfaces a priori - A probabilistic approach

A key step in many earthquake source inversions requires knowledge of the geometry of the fault surface on which the earthquake occurred. Our knowledge of this surface is often uncertain, however, and as a result fault geometry misinterpretation can map into significant error in the final temporal and spatial slip patterns of these inversions. Relying solely on an initial hypocentre and...
Authors
G.P. Hayes, D.J. Wald

Diffusion-equation representations of landform evolution in the simplest circumstances: Appendix C Diffusion-equation representations of landform evolution in the simplest circumstances: Appendix C

The diffusion equation is one of the three great partial differential equations of classical physics. It describes the flow or diffusion of heat in the presence of temperature gradients, fluid flow in porous media in the presence of pressure gradients, and the diffusion of molecules in the presence of chemical gradients. [The other two equations are the wave equation, which describes the
Authors
Thomas C. Hanks

Broadband records of earthquakes in deep gold mines and a comparison with results from SAFOD, California Broadband records of earthquakes in deep gold mines and a comparison with results from SAFOD, California

For one week during September 2007, we deployed a temporary network of field recorders and accelerometers at four sites within two deep, seismically active mines. The ground-motion data, recorded at 200 samples/sec, are well suited to determining source and ground-motion parameters for the mining-induced earthquakes within and adjacent to our network. Four earthquakes with magnitudes...
Authors
Arthur F. McGarr, M. Boettcher, Jon Peter B. Fletcher, Russell Sell, Malcolm J. S. Johnston, R. Durrheim, S. Spottiswoode, A. Milev

Extension of Gutenberg‐Richter distribution to MW −1.3, no lower limit in sight Extension of Gutenberg‐Richter distribution to MW −1.3, no lower limit in sight

With twelve years of seismic data from TauTona Gold Mine, South Africa, we show that mining‐induced earthquakes follow the Gutenberg‐Richter relation with no scale break down to the completeness level of the catalog, at moment magnitude MW −1.3. Events recorded during relatively quiet hours in 2006 indicate that catalog detection limitations, not earthquake source physics, controlled the
Authors
Margaret S. Boettcher, Arthur F. McGarr, Malcolm J. S. Johnston

Preparing a population for an earthquake like Chi-Chi: The Great Southern California ShakeOut Preparing a population for an earthquake like Chi-Chi: The Great Southern California ShakeOut

The Great Southern California ShakeOut was a week of special events featuring the largest earthquake drill in United States history. On November 13, 2008, over 5 million southern Californians pretended that a magnitude-7.8 earthquake had occurred and practiced actions that could reduce its impact on their lives. The primary message of the ShakeOut is that what we do now, before a big...
Authors
Lucile M. Jones

New research and tools lead to improved earthquake alerting protocols New research and tools lead to improved earthquake alerting protocols

What’s the best way to get alerted about the occurrence and potential impact of an earthquake? The answer to that question has changed dramatically of late, in part due to improvements in earthquake science, and in part by the implementation of new research in the delivery of earthquake information
Authors
David J. Wald

A grid-doubling finite-element technique for calculating dynamic three-dimensional spontaneous rupture on an earthquake fault A grid-doubling finite-element technique for calculating dynamic three-dimensional spontaneous rupture on an earthquake fault

We present a new finite-element technique for calculating dynamic 3-D spontaneous rupture on an earthquake fault, which can reduce the required computational resources by a factor of six or more, without loss of accuracy. The grid-doubling technique employs small cells in a thin layer surrounding the fault. The remainder of the modelling volume is filled with larger cells, typically two...
Authors
Michael Barall

Review: Progress in rotational ground-motion observations from explosions and local earthquakes in Taiwan Review: Progress in rotational ground-motion observations from explosions and local earthquakes in Taiwan

Rotational motions generated by large earthquakes in the far field have been successfully measured, and observations agree well with the classical elasticity theory. However, recent rotational measurements in the near field of earthquakes in Japan and in Taiwan indicate that rotational ground motions are 10 to 100 times larger than expected from the classical elasticity theory. The near...
Authors
William H. K. Lee, Bor-Shouh Huang, Charles A. Langston, Chin-Jen Lin, Chun-Chi Liu, Tzay-Chyn Shin, Ta-Liang Teng, Chien-Fu Wu

Deep low-frequency earthquakes in tremor localize to the plate interface in multiple subduction zones Deep low-frequency earthquakes in tremor localize to the plate interface in multiple subduction zones

Deep tremor under Shikoku, Japan, consists primarily, and perhaps entirely, of swarms of low-frequency earthquakes (LFEs) that occur as shear slip on the plate interface. Although tremor is observed at other plate boundaries, the lack of cataloged low-frequency earthquakes has precluded a similar conclusion about tremor in those locales. We use a network autocorrelation approach to...
Authors
Justin R. Brown, Gregory C. Beroza, Satoshi Ide, David R. Shelly, Kazuaki Ohta, Susan Y. Schwartz, Wolfgang Rabbel, M. Thorwart, Honn Kao

Data from theodolite measurements of creep rates on San Francisco Bay region faults, California Data from theodolite measurements of creep rates on San Francisco Bay region faults, California

Introduction Our purpose is to annually update our creep-data archive on San Francisco Bay region active faults for use by the scientific research community. Earlier data (1979-2001) were reported in Galehouse (2002) and were analyzed and described in detail in a summary report (Galehouse and Lienkaemper, 2003). A complete analysis of our earlier results obtained on the Hayward Fault was...
Authors
Forrest S. McFarland, James J. Lienkaemper, S. John Caskey
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