Publications
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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
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
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
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
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
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
Prediction of spectral acceleration response ordinates based on PGA attenuation Prediction of spectral acceleration response ordinates based on PGA attenuation
Developed herein is a new peak ground acceleration (PGA)-based predictive model for 5% damped pseudospectral acceleration (SA) ordinates of free-field horizontal component of ground motion from shallow-crustal earthquakes. The predictive model of ground motion spectral shape (i.e., normalized spectrum) is generated as a continuous function of few parameters. The proposed model eliminates...
Authors
V. Graizer, E. Kalkan
Shallow seismic structure of Kunlun fault zone in northern Tibetan Plateau, China: Implications for the 2001 M s8.1 Kunlun earthquake Shallow seismic structure of Kunlun fault zone in northern Tibetan Plateau, China: Implications for the 2001 M s8.1 Kunlun earthquake
The shallow seismic velocity structure of the Kunlun fault zone (KLFZ) was jointly deduced from seismic refraction profiling and the records of trapped waves that were excited by five explosions. The data were collected after the 2001 Kunlun Ms8.1 earthquake in the northern Tibetan Plateau. Seismic phases for the in-line record sections (26 records up to a distance of 15 km) along the...
Authors
Chun-Yong Wang, Walter D. Mooney, Z. Ding, J. Yang, Z. Yao, H. Lou
Validation of the rupture properties of the 2001 Kunlun, China (Ms = 8.1), earthquake from seismological and geological observations Validation of the rupture properties of the 2001 Kunlun, China (Ms = 8.1), earthquake from seismological and geological observations
We determine the finite-fault slip distribution of the 2001 Kunlun earthquake (Ms = 8.1) by inverting teleseismic waveforms, as constrained by geological and remote sensing field observations. The spatial slip distribution along the 400-km-long fault was divided into five segments in accordance with geological observations. Forward modelling of regional surface waves was performed to...
Authors
Yi-Ying Wen, Ma Kuo-Fong, Teh-Ru Alex Song, Walter D. Mooney
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
The puzzle of the 1996 Bárdarbunga, Iceland, earthquake: no volumetric component in the source mechanism The puzzle of the 1996 Bárdarbunga, Iceland, earthquake: no volumetric component in the source mechanism
A volcanic earthquake with Mw 5.6 occurred beneath the Bárdarbunga caldera in Iceland on 29 September 1996. This earthquake is one of a decade-long sequence of events at Bárdarbunga with non-double-couple mechanisms in the Global Centroid Moment Tensor catalog. Fortunately, it was recorded well by the regional-scale Iceland Hotspot Project seismic experiment. We investigated the event...
Authors
Hrvoje Tkalcic, Douglas S. Dreger, Gillian R. Foulger, Bruce R. Julian
On baseline corrections and uncertainty in response spectrafor baseline variations commonly encountered in digital accelerograph records On baseline corrections and uncertainty in response spectrafor baseline variations commonly encountered in digital accelerograph records
Most digital accelerograph recordings are plagued by long-period drifts, best seen in the velocity and displacement time series obtained from integration of the acceleration time series. These drifts often result in velocity values that are nonzero near the end of the record. This is clearly unphysical and can lead to inaccurate estimates of peak ground displacement and long-period...
Authors
Sinan Akkar, David M. Boore