Alexander R. Hutko's research while affiliated with University of Washington Seattle and other places
What is this page?
This page lists the scientific contributions of an author, who either does not have a ResearchGate profile, or has not yet added these contributions to their profile.
It was automatically created by ResearchGate to create a record of this author's body of work. We create such pages to advance our goal of creating and maintaining the most comprehensive scientific repository possible. In doing so, we process publicly available (personal) data relating to the author as a member of the scientific community.
If you're a ResearchGate member, you can follow this page to keep up with this author's work.
If you are this author, and you don't want us to display this page anymore, please let us know.
It was automatically created by ResearchGate to create a record of this author's body of work. We create such pages to advance our goal of creating and maintaining the most comprehensive scientific repository possible. In doing so, we process publicly available (personal) data relating to the author as a member of the scientific community.
If you're a ResearchGate member, you can follow this page to keep up with this author's work.
If you are this author, and you don't want us to display this page anymore, please let us know.
Publications (34)
The Incorporated Research Institutions for Seismology (IRIS) Data Management Center (DMC) offers and distributes 31 distinct data products derived from raw data. These data products are intended to serve the seismology community as precursory tools and standardized baseline data sets for further research. The number of distinct data products has mo...
We present a new webservice, Syngine, running at the Incorporated Research Institutions for Seismology Data Management Center (IRIS‐DMC), that offers on‐demand and custom‐tailored seismograms served over HTTP. The free service produces full seismic waveforms, including effects like attenuation and anisotropy, that are calculated in commonly used sp...
Earthquake hazard assessments and rupture forecasts are based on the potential length of seismic rupture and whether or not slip is arrested at fault segment boundaries. Such forecasts do not generally consider that one earthquake can trigger a second large event, near-instantaneously, at distances greater than a few kilometres. Here we present a g...
The DMC data product effort represents a unique collaboration between the research community and IRIS. The strengths for distribution, in particular, the authors of the tomographic models in the Earth Model Collaboration product, the Global Centroid Moment Tensor project members, and the Global ShakeMovie project members. Development of data produc...
Teleseismic short-period (0.5-5 s) P waves from the 27 February 2010 Chile earthquake (Mw 8.8) are back projected to the source region to image locations of coherent short-period seismic wave radiation. Several receiver array configurations are analyzed using different P wave arrivals, including networks of stations in North America (P), Japan (PKI...
Within two hours after the great March 11, 2011 Tohoku earthquake the
IRIS DMC started publishing automated data products through its
Searchable Product Depository (SPUD), which provides quick viewing of
many aspects of the data and preliminary analysis of this great
earthquake. These products are part of the DMC's data product
development effort i...
Since publication of the Parametric Earth Model (PEM) in 1975 and the
Preliminary Reference Earth Model (PREM) in1981, there has been a
significant increase in the research activities with the goal of
developing more detailed regional and global 3D velocity models.
Advances in modeling as well as an ever-growing volume of data,
particularly from US...
Earth's largest earthquakes rupture megathrust faults at subduction zone
plate boundaries. The 2004 Sumatra (Mw 9.2), 2010 Chile (Mw 8.8) and
2011 Tohoku (Mw 9.0) great earthquakes exhibit similarities in spatial
variations of seismic wave radiation from their rupture zones, with
coherent short-period radiation preferentially emanating from the dee...
Images of the short-period distribution of energy release from the great
Tohoku-oki earthquake are produced by back-projecting teleseismic P
waves recorded with arrays of seismometers in North America and Europe.
In the band of 0.5-2.0 s both arrays show that energy was primarily
radiated down-dip of the epicenter, deep beneath the Honshu coastline...
The frequency-dependent rupture process of the 11 March 2011
Mw 9.0 off the Pacific coast of Tohoku Earthquake is examined
using backprojection (BP) imaging with teleseismic short-period
(˜1 s) P waves, and finite faulting models (FFMs) of the seismic
moment and slip distributions inverted from broadband (>3 s)
teleseismic P waves, Rayleigh waves a...
The 25 October 2010 Mentawai, Indonesia earthquake (Mw 7.8) ruptured the shallow portion of the subduction zone seaward of the Mentawai islands, off-shore of Sumatra, generating 3 to 9 m tsunami run-up along southwestern coasts of the Pagai Islands that took at least 431 lives. Analyses of teleseismic P, SH and Rayleigh waves for finite-fault sourc...
A magnitude 8.8 (Mw) earthquake struck the central coast of Chile on 27 February 2010 at 06:34:14 UTC. It was the fifth largest earthquake to be seismically recorded. Initial modeling of teleseismic P, SH, and Rayleigh waves (Lay et al., 2010) showed that the earthquake ruptured a length of ~550 km, with an average rupture velocity of 2.0-2.5 km/s,...
Great earthquakes (having seismic magnitudes of at least 8) usually involve abrupt sliding of rock masses at a boundary between tectonic plates. Such interplate ruptures produce dynamic and static stress changes that can activate nearby intraplate aftershocks, as is commonly observed in the trench-slope region seaward of a great subduction zone thr...
The 27 February 2010 Chile (Mw 8.8) earthquake is the fifth largest earthquake to strike during the age of seismological instrumentation. The faulting geometry, slip distribution, seismic moment, and moment-rate function are estimated from broadband teleseismic P, SH, and Rayleigh wave signals. We explore some of the trade-offs in the rupture-proce...
Using an unusually large earthquake near the big island of Hawaii, we study the core mantle boundary (CMB) beneath the north-northeastern Pacific between Hawaii and North America. A dense sampling of the CMB is achieved using the core-reflected phase PcP recorded at a large number of high-quality stations in North America, including networks in Cal...
Deterministic imaging of 3D elastic wave scattering structures in Earth's deep interior is an important approach for quantifying mantle convection. Seismic migrations with minimal a priori assumptions about structural geometry can exploit scattered wavefields to image complex velocity interfaces. These can be combined with volumetric heterogeneitie...
Two great underthrusting earthquakes that occurred along the coast of Peru in 2001 and 2007 involve spatiotemporal slip distributions that differ from the predominantly unilateral or bilateral rupture expansion of many great events. Commonly used finite-source rupture model parameterizations, with specified rupture velocity and/or short duration of...
Applications of teleseismic P-wave back-projection to image gross characteristics of large earthquake finite-source ruptures have been enabled by ready availability of large digital data sets. Imaging with short-period data from dense arrays or broadband data from global networks can place constraints on rupture attributes that otherwise have to be...
The southwestern half of a ˜500 km long seismic gap in the central Kuril Island arc subduction zone experienced two great earthquakes with extensive preshock and aftershock sequences in late 2006 to early 2007. The nature of seismic coupling in the gap had been uncertain due to the limited historical record of prior large events and the presence of...
The Mw 7.9 Wenchuan earthquake of 12 May 2008 was the most destructive Chinese earthquake since the 1976 Tangshan event. Tens of thousands of people were killed, hundreds of thousands were injured, and millions were left homeless. Here we infer the detailed rupture process of the Wenchuan earthquake by back-projecting teleseismic P energy from seve...
A large, high quality P-wave data set comprising short-period and broadband signals sampling four separate regions in the lowermost mantle beneath the Cocos plate, Mexico, the central Pacific, and the north Pacific is analyzed using regional one-dimensional double-array stacking and modelling with reflectivity synthetics. A data-screening criterion...
Applications of seismic wave back-projection and reverse-time methods to earthquake finite-source rupture imaging have increased with ready availability of large digital data sets and expanded computer processing capabilities. For large earthquakes, these approaches offer potential for explicitly resolving rupture attributes that are treated parame...
Detailed P-wave and S-wave velocity structures for the lowermost mantle beneath the central and eastern Pacific obtained by broadband waveform stacking and modeling procedures indicate distinctive characteristics of low- and high-velocity regions in the deep mantle. The central Pacific region is located within the tomographically-resolved large low...
A large, high quality P-wave data set comprising short-period and
broadband signals sampling four regions in the lowermost mantle beneath
the Cocos plate, Mexico, the north Pacific, and the central Pacific is
analyzed using regional one-dimensional double-array stacking and
synthetic modeling. A data-screening criterion retains only events with
sta...
Earth's lowermost mantle has thermal, chemical, and mineralogical complexities that require precise seismological characterization. Stacking, migration, and modeling of over 10,000 P and S waves that traverse the deep mantle under the Cocos plate resolve structures above the core-mantle boundary. A small -0.07 +/- 0.15% decrease of P wave velocity...
The Earth's core-mantle boundary (CMB) is the site of the largest density contrast and most profound chemical contrast within the planet. The CMB separates the vigorously convecting molten iron-alloy outer core and the more slowly convecting crystalline silicate/oxide mantle. The lowermost few hundred kilometers of the mantle, known as the D" regio...
An abrupt 1-2.5% S-wave velocity increase has been observed in the
lowermost mantle beneath the Cocos plate in several studies. This is
commonly attributed to the perovskite to post-perovskite phase
transition. This phase transition is expected to have much weaker
effects on P-wave velocities than on S-wave velocities and the depth
range of the tra...
We use tens of thousands of seismograms from South and Central American earthquakes recorded by western North American seismic networks to image the lowermost mantle beneath Central America using a 3D Kirchhoff migration method. P wave studies of the deep mantle often rely on some form of stacking of many records in order to enhance the signal-to-n...
We use thousands of seismograms from South and Central American
earthquakes recorded by western North American seismic networks to image
the lowermost mantle beneath Central America using a 3D Kirchhoff
migration scheme. P wave studies of the deep mantle often rely on some
form of stacking of many records in order to enhance the signal-to-noise
rat...
Seismic tomography has been used to infer that some descending slabs of oceanic lithosphere plunge deep into the Earth's lower mantle. The fate of these slabs has remained unresolved, but it has been postulated that their ultimate destination is the lowermost few hundred kilometres of the mantle, known as the D'' region. Relatively cold slab materi...
We use 270 horizontally-polarized S waves from 15 deep earthquakes under South America recorded at broadband stations in western North America to image shear-velocity structure in the deep mantle beneath the Cocos Plate. We use a Kirchhoff migration approach, assuming isotropic scattering from a three-dimensional grid of possible scattering nodes i...
The discovery of the post-perovskite phase transition presents a new context for interpreting seismological observations of deep mantle structure. As is the case for seismic velocity discontinuities detected in the upper mantle transition zone, interpretation as an expression of a phase change provides an opportunity to infer thermal and dynamical...
Lower mantle migration applications have generally used a 1D reference model for computing travel times. Resulting images of reflectors or scatterers are intrinsically biased by inaccuracies of the background model. Given that differential time variations for shear wave phases can range over 5 s over 1000 km dimension regions, failure to account fo...
Broadband data from North American permanent and temporary stations
recording events 20-60 degrees away in Central America and northern
South America are used to study the lower mantle by analyzing PcP, ScP
and their precursors (topside reflections and back-scattered arrivals
). The lowermost few hundred km of the mantle, D", is physically and
chem...
Citations
... To generate the synthetic wa veforms, w e used a Green's functions database computed for AK135f using the spectral element solv er AxiSEM (Nissen-Me yer et al. 2014 ), obtained from the IRIS DMC Syngine web service (Krischer et al. 2017 ), and parsed using Instaseis for efficient buffered I/O ( van Driel et al. 2015 ). The Green's functions in the database are accurate down to periods of 2 s. ...
... Seismic networks produce catalogs that are often the basis of other products relating to seismic hazards, making the accuracy and reliability of catalogs crucial. Considering the power law increase of the volume of seismic data in recent years (e.g., Hutko et al., 2017), there is an urgent need for improved algorithms to process seismograms for event detection. ...
... To date, such tsunami scenario faults have been proposed to rupture individually, and triggering or simultaneous ruptures along with other adjacent scenario faults with considerably different fault geometries have not been specifically supposed. However, multiplex rupturing across a complex fault network or segmented multi-fault triggering has been reported for earthquakes in variable tectonic environments (e.g., Fan et al., 2017;Hamling et al., 2017;Kuge et al., 1996;Lay et al., 2018;Nissen et al., 2016;Satriano et al., 2012;Vasyura-Bathke et al., 2024;. This can result in diverse rupture behaviors, including the rupture of faults with conjugate dip directions and apparent backward rupture propagation. ...
... The 3D models of isotropic V P , azimuthal anisotropy, and radial anisotropy (RAN) determined by this study can be obtained from the website (doi: 10.5281/zenodo.10677143). The tomographic models of previous studies were obtained from the Earth Model Collaboration repository of the Incorporated Research Institutions for Seismology (IRIS; Trabant et al., 2012; https:// ds.iris.edu/ds/products/emc-earthmodels). The Generic Mapping Tool (GMT) software package (Wessel et al., 2019) is available at https:// github.com/GenericMappingTools/. The information about ISC earthquake locations is available at http://www.isc.ac.uk. ...
... Backprojection is a primary array processing technique for imaging large earthquake rupture propagation, and its first application was to the 2004 Sumatra-Andaman earthquake (Ishii et al., , 2007. With the development of large-scale dense seismic networks or arrays, backprojection has proved to be a valuable technique for studying complex earthquake ruptures (e.g., Walker et al., 2005;Allmann and Shearer, 2007;Ishii, 2011, 2012;Koper et al., 2011;Meng et al., 2011;Wang et al., 2012), early aftershock detection (Fan and Shearer, 2017), hazard early warning (An and Meng, 2016), and body-wave microseism detection and source location (Zhang et al., 2009;Liu et al., 2016Liu et al., , 2020. Furthermore, significant efforts have been made to improve the accuracy and resolution of backprojection results. ...
... : 2020 50 1 [45]. , , . ...
Reference: 从地震到星震
... Another type of dispersive model called depth-integrated non-hydrostatic model, has comparable accuracy to the classical Boussinesq equations, but has no higher-order derivatives in the governing equations. This model can be solved efficiently and stably with a semi-implicit scheme (Stelling and Zijlema, 2003;Yamazaki et al., 2009), and has been used in many real events for modeling dispersive tsunamis (e.g., Lay et al., 2011;Bai et al., 2014;Aranguiz et al., 2019). Here, we develop our dispersive tsunami numerical model based on the depth-integrated non-hydrostatic model, and apply it to the high-resolution tsunami hazard assessment for the GBA. ...
... Tong et al. (2010) quantitatively derived the coseismic slip distribution based on the elastic dislocation model with a combination of GPS and ALOS data. Lay et al. (2010) inferred the finite-fault slip distribution using the teleseismic P, SH, and Rayleigh wave data. Delouis et al. (2010) presented the slip distribution based on the static and High-Rate GPS, teleseismic, and InSAR data. ...
... Various geophysical investigations have illuminated the structural alterations suffered by the incoming plate due to the vast number of extensional faulting and rupturing generated with the bending of the subducting plate (Fujie et al., 2013(Fujie et al., , 2018Grevemeyer et al., 2018;Key et al., 2012;Naif et al., 2015). Such alterations primarily include the breaking of the lithosphere (Abe, 1972;Lay et al., 2009) creating conduits for fluid migration, through extensive damage, into the previously intact rocks. This ultimately leads to serpentinization of the mantle, that has been well identified by V P /V S anomalies (e.g., Grevemeyer et al., 2018) and electrical resistivity anomalies (e.g., Naif et al., 2015). ...
... PcP waves experience more attenuative energy loss compared to direct P waves, and the resultant waveform differences need to be corrected to make the P and PcP stacks more comparable. Each P stack was convolved with a series of t* operators, ranging from 0.2 to 2.0, which represent progressively greater attenuation (16,21,(53)(54). The optimal t* operator is the one that creates an attenuated P-wave response that most closely matches the PcP signal (15). ...