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Integrate urban‐scale seismic hazard analyses with the U.S. National Seismic Hazard Model Integrate urban‐scale seismic hazard analyses with the U.S. National Seismic Hazard Model

For more than 20 yrs, damage patterns and instrumental recordings have highlighted the influence of the local 3D geologic structure on earthquake ground motions (e.g., MM 6.7 Northridge, California, Gao et al., 1996; MM 6.9 Kobe, Japan, Kawase, 1996; MM 6.8 Nisqually, Washington, Frankel, Carver, and Williams, 2002). Although this and other local‐scale features are critical to improving...
Authors
Morgan P. Moschetti, Nico Luco, Arthur D. Frankel, Mark D. Petersen, Brad T. Aagaard, Annemarie S. Baltay Sundstrom, Michael L. Blanpied, Oliver S. Boyd, Richard W. Briggs, Ryan D. Gold, Robert Graves, Stephen H. Hartzell, Sanaz Rezaeian, William J. Stephenson, David J. Wald, Robert A. Williams, Kyle Withers

Spatial and spectral interpolation of ground-motion intensity measure observations Spatial and spectral interpolation of ground-motion intensity measure observations

Following a significant earthquake, ground‐motion observations are available for a limited set of locations and intensity measures (IMs). Typically, however, it is desirable to know the ground motions for additional IMs and at locations where observations are unavailable. Various interpolation methods are available, but because IMs or their logarithms are normally distributed, spatially...
Authors
Charles Worden, Eric M. Thompson, Jack W. Baker, Brendon A. Bradley, Nico Luco, David J. Wald

The 2013–2016 induced earthquakes in Harper and Sumner Counties, southern Kansas The 2013–2016 induced earthquakes in Harper and Sumner Counties, southern Kansas

We examine the first four years (2013–2016) of the ongoing seismicity in southern Kansas using high‐precision locations derived from a local seismometer network. The earthquakes occur almost exclusively in the shallow crystalline basement, below the wastewater injection horizon of the Arbuckle Group at the base of the sedimentary section. Multiple lines of evidence lead us to conclude...
Authors
Justin L. Rubinstein, William L. Ellsworth, Sara L. Dougherty

A flatfile of ground motion intensity measurements from induced earthquakes in Oklahoma and Kansas A flatfile of ground motion intensity measurements from induced earthquakes in Oklahoma and Kansas

We have produced a uniformly processed database of orientation-independent (RotD50, RotD100) ground motion intensity measurements containing peak horizontal ground motions (accelerations and velocities) and 5-percent-damped pseudospectral accelerations (0.1–10 s) from more than 3,800 M ≥ 3 earthquakes in Oklahoma and Kansas that occurred between January 2009 and December 2016. Ground...
Authors
Steven B. Rennolet, Morgan P. Moschetti, Eric M. Thompson, William L. Yeck

Rayleigh and S wave tomography constraints on subduction termination and lithospheric foundering in central California Rayleigh and S wave tomography constraints on subduction termination and lithospheric foundering in central California

The crust and upper mantle structure of central California have been modified by subduction termination, growth of the San Andreas plate boundary fault system, and small-scale upper mantle convection since the early Miocene. Here we investigate the contributions of these processes to the creation of the Isabella Anomaly, which is a high seismic velocity volume in the upper mantle. There...
Authors
Chengxin Jiang, Brandon Schmandt, Steven M. Hansen, Sara L. Dougherty, Robert W. Clayton, Jamie Farrell, Fan-Chi Lin

Temporal stress changes caused by earthquakes: A review Temporal stress changes caused by earthquakes: A review

Earthquakes can change the stress field in the Earth’s lithosphere as they relieve and redistribute stress. Earthquake-induced stress changes have been observed as temporal rotations of the principal stress axes following major earthquakes in a variety of tectonic settings. The stress changes due to the 2011 Mw9.0 Tohoku-Oki, Japan, earthquake were particularly well documented...
Authors
Jeanne L. Hardebeck, Tomomi Okada

Testing for the ‘predictability’ of dynamically triggered earthquakes in Geysers Geothermal Field Testing for the ‘predictability’ of dynamically triggered earthquakes in Geysers Geothermal Field

The Geysers geothermal field is well known for being susceptible to dynamic triggering of earthquakes by large distant earthquakes, owing to the introduction of fluids for energy production. Yet, it is unknown if dynamic triggering of earthquakes is ‘predictable’ or whether dynamic triggering could lead to a potential hazard for energy production. In this paper, our goal is to...
Authors
Chastity Aiken, Xiaofeng Meng, Jeanne L. Hardebeck

Ground-motion models for very-hard rock sites in eastern North America: An update Ground-motion models for very-hard rock sites in eastern North America: An update

The ground‐motion models provided by me to the Next Generation Attenuation‐East (NGA‐East) project in 2015 have been updated by considering three additional Fourier spectra attenuation models and by conducting a mixed‐effect analysis of the residuals between the ground‐motion intensity measures computed from the attenuation models and the data from nine relatively well‐recorded events in...
Authors
David Boore

On the depth extent of co-seismic rupture On the depth extent of co-seismic rupture

We investigate the implications of deformation experiments for the coseismic down‐dip extent of rupture in quasi‐dynamic, whole‐cycle earthquake models of a fault for which the depth of the transition between seismic and aseisimic fault slip depends on strain rate. The calculations use a dislocation fault model from Tse and Rice (1986) with a vertical strike‐slip orientation, mode III...
Authors
Nicholas M. Beeler, G. Hirth, T.E. Tullis, C. H. Webb

Stress rotation across the Cascadia megathrust requires a weak subduction plate boundary at seismogenic depths Stress rotation across the Cascadia megathrust requires a weak subduction plate boundary at seismogenic depths

The Mendocino Triple Junction region is the most seismically active part of the Cascadia Subduction Zone. The northward moving Pacific plate collides with the subducting Gorda plate causing intense internal deformation within it. Here we show that the stress field rotates rapidly with depth across the thrust interface from a strike-slip regime within the subducting plate, reflecting the...
Authors
Duo Li, Jeffrey J. McGuire, Yajing Liu, Jeanne L. Hardebeck

Maturity of nearby faults influences seismic hazard from hydraulic fracturing Maturity of nearby faults influences seismic hazard from hydraulic fracturing

Understanding the causes of human-induced earthquakes is paramount to reducing societal risk. We investigated five cases of seismicity associated with hydraulic fracturing (HF) in Ohio since 2013 that, because of their isolation from other injection activities, provide an ideal setting for studying the relations between high-pressure injection and earthquakes. Our analysis revealed two...
Authors
Maria Kozlowska, Michael R. Brudzinski, Paul A. Friberg, Robert J. Skoumal, Nicholas Baxter, Brian S. Currie

Euler-vector clustering of GPS velocities defines microplate geometry in southwest Japan Euler-vector clustering of GPS velocities defines microplate geometry in southwest Japan

I have used Euler-vector clustering to assign 469 GEONET stations in southwest Japan to k clusters (k = 2, 3,..., 9) so that, for any k, the velocities of stations within each cluster are most consistent with rigid-block motion on a sphere. That is, I attempt to explain the raw (i.e., uncorrected for strain accumulation), 1996–2006 velocities of those 469 Global Positioning System...
Authors
James C. Savage
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