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<title>Bulletin of the Seismological Society of America current issue</title>
<link>http://www.bssaonline.org</link>
<description>BSSA has been the premier journal of research in earthquake seismology and related disciplines since 1911</description>
<prism:coverDisplayDate>Jun  1 2007 12:00:00:000AM</prism:coverDisplayDate>
<prism:publicationName>Bulletin of the Seismological Society of America</prism:publicationName>
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<title>title</title>
<url>http://www.bssaonline.org/icons/home/title.gif</url>
<link>http://www.bssaonline.org</link>
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<item rdf:about="http://www.bssaonline.org/cgi/content/abstract/97/3/671?rss=1">
<title><![CDATA[[Articles] An Overview of the Damaging and Low Magnitude Mw 4.8 La Paca Earthquake on 29 January 2005: Context, Seismotectonics, and Seismic Risk Implications for Southeast Spain]]></title>
<link>http://www.bssaonline.org/cgi/content/abstract/97/3/671?rss=1</link>
<description><![CDATA[
<p>This article presents an overview of the La Paca earthquake of magnitude
<I>m</I><SUB>bLg</SUB> 4.7, which occurred on 29 January 2005, with its
epicenter located near the town of Avil&eacute;s in the Murcia region in
southeast Spain. Despite its low magnitude, the earthquake caused important
damage in two towns of the epicentral area, La Paca and Zarcilla de Ramos. These
areas recorded intensities of VI&ndash;VII
(<cross-ref type="bib" refid="bib64">European Macroseismic Scale, 1998</cross-ref>)
and sustained estimated economic losses amounting to 10 million
;eu<!--CONV-ERROR: Unconverted Unicode Hex Entity Ref -->[|20ac|]. Aftershocks
continued for more than 2 weeks, producing considerable alarm in the population
and mobilizing emergency services from the whole region. The La Paca seismic
series is the third registered in the region in the past 8 years, being preceded
by the Mula (1999) and southwest Bullas (2002) seismic series. These main events
had also low magnitudes (<I>m</I><SUB>bLg</SUB> 4.8) and caused damage levels
similar to the 2005 earthquake. The case is an example of a moderate seismic
zone where low-magnitude and frequent earthquakes have important implications on
the seismic hazard and risk of the region. Although these are not the largest
expected earthquakes, they have yielded important information for improving the
knowledge of the seismic activity of the area. With this aim in mind, different
topics have been analyzed from a multidisciplinary perspective, including
seismicity, local tectonics and surface geology, focal mechanisms, macroseismic
effects, and ground motion. Results indicate a local tectonic interpretation,
consistent with a strike-slip focal mechanism, the confirmation of a triggering
process between the 2002 and 2005 earthquakes, a geotechnical and ground-motion
characterization for the damaged sites (supporting local amplification effects
and estimated peak ground acceleration values of ~0.1<I>g</I>), and an
understanding of damage patterns in relation to local building trends. The
results may be used as guidelines for future revisions of the Spanish Building
Code
(<cross-ref type="bib" refid="bib34">Norma de la Construcci&oacute;n Sismorresistente Espa&ntilde;ola [NCSE-02], 2002</cross-ref>).
The study results should contribute to risk mitigation in a region where
strong-motion records from the maximum expected earthquakes are not available.
This approach can be extended to other regions with similar seismic backgrounds
and a lack of strong-motion records.</p>
]]></description>
<dc:creator><![CDATA[Benito, B., Capote, R., Murphy, P., Gaspar-Escribano, J. M., Martinez-Diaz, J. J., Tsige, M., Stich, D., Garcia-Mayordomo, J., Garcia Rodriguez, M. J., Jimenez, M. E., Insua-Arevalo, J. M., Alvarez-Gomez, J. A., Canora, C.]]></dc:creator>
<dc:date>2007-06-11</dc:date>
<dc:identifier>info:doi/10.1785/0120050150</dc:identifier>
<dc:title><![CDATA[[Articles] An Overview of the Damaging and Low Magnitude Mw 4.8 La Paca Earthquake on 29 January 2005: Context, Seismotectonics, and Seismic Risk Implications for Southeast Spain]]></dc:title>
<dc:publisher>Seismological Society of America</dc:publisher>
<prism:number>3</prism:number>
<prism:volume>97</prism:volume>
<prism:endingPage>690</prism:endingPage>
<prism:publicationDate>2007-06-01</prism:publicationDate>
<prism:startingPage>671</prism:startingPage>
<prism:section>Articles</prism:section>
</item>

<item rdf:about="http://www.bssaonline.org/cgi/content/abstract/97/3/691?rss=1">
<title><![CDATA[[Articles] The 2004 Mw 4.4 Rotenburg, Northern Germany, Earthquake and Its Possible Relationship with Gas Recovery]]></title>
<link>http://www.bssaonline.org/cgi/content/abstract/97/3/691?rss=1</link>
<description><![CDATA[
<p>We study the 20 October 2004 <I>M</I><SUB>w</SUB> 4.4 Rotenburg
(W&uuml;mme)/Neuenkirchen earthquake, located in a previously aseismic region in
the northern German sedimentary basin. We constrain the source parameter by
using different techniques. A possible relationship between this event, the
regional tectonic setting, and local gas recovery is investigated. Different
waveform inversion and modeling approaches constrain the depth of the mainshock
between 5 and 7 km. The source mechanism was oblique normal faulting on planes
striking roughly north&ndash;south. An inversion for kinematic rupture
parameters indicates a unilateral rupture propagation toward the north,
consistent with the higher macroseismic intensities found toward the north in
the region of Hamburg compared with those at a similar distance toward the south
in the region of Hannover. Relocations of the mainshock and three of the largest
aftershocks indicate that these events occurred within a few kilometers of three
major gas fields and at depth close to gas production intervals. Comparison with
seismicity triggered in the northern Netherlands by depletion of similar gas
reservoirs in a similar tectonic environment suggests that the
<I>M</I><SUB>w</SUB> 4.4 Rotenburg event may be related to gas recovery.</p>
<p><I>Online material:</I> Focal mechanism and waveform fit.</p>
]]></description>
<dc:creator><![CDATA[Dahm, T., Kruger, F., Stammler, K., Klinge, K., Kind, R., Wylegalla, K., Grasso, J.-R.]]></dc:creator>
<dc:date>2007-06-11</dc:date>
<dc:identifier>info:doi/10.1785/0120050149</dc:identifier>
<dc:title><![CDATA[[Articles] The 2004 Mw 4.4 Rotenburg, Northern Germany, Earthquake and Its Possible Relationship with Gas Recovery]]></dc:title>
<dc:publisher>Seismological Society of America</dc:publisher>
<prism:number>3</prism:number>
<prism:volume>97</prism:volume>
<prism:endingPage>704</prism:endingPage>
<prism:publicationDate>2007-06-01</prism:publicationDate>
<prism:startingPage>691</prism:startingPage>
<prism:section>Articles</prism:section>
</item>

<item rdf:about="http://www.bssaonline.org/cgi/content/abstract/97/3/705?rss=1">
<title><![CDATA[[Articles] Tsunami Hazard Evaluation of the Eastern Mediterranean: Historical Analysis and Selected Modeling]]></title>
<link>http://www.bssaonline.org/cgi/content/abstract/97/3/705?rss=1</link>
<description><![CDATA[
<p>Seismic sea waves in the eastern Mediterranean have been reported since
written history first emerged several thousand years ago. We collected and
investigated these ancient and modern reports to understand and model the
typical tsunamigenic sources, with the ultimate purpose of characterizing
tsunami hazard along the Levant coasts. Surprisingly, only 35% of the tsunami
reports could be traced back to primary sources, with the balance remaining
questionable. The tsunamis varied in size, from barely noticeable to greatly
damaging, and their effects ranged from local to regional. Overall, we list 21
reliably reported tsunamis that occurred since the mid second century
<scp>b.c.</scp> along the Levant coast, along with 57 significant historical
earthquakes that originated from the "local" continental Dead Sea
Transform (<scp>dst</scp>) system. An in-depth evaluation shows that 10 tsunamis
are clearly associated with on-land <scp>dst</scp> earthquakes, and therefore,
as formerly suggested, they probably originated from offshore, seismogenically
induced slumps. Eight tsunamis arrived from the "remote" Hellenic
and Cypriot Arcs, one from Italy, and two are left with as yet unrecognized
sources. A major conclusion from this work is that onshore earthquakes commonly
produce tsunamis along the Levant coastline, and that analogous situations are
present elsewhere in the Mediterranean, as well as along the California coast
and in another regions with active faults near the coast.</p>
<p>We modeled three typical scenarios, and in light of the Sumatra experience,
we examined the more likely severe magnitudes. This of course leads us toward
the upper range of expected run-ups. The models show that sooner than five
minutes after a strong earthquake produces an offshore slump, which occurs after
close to a third of the large <scp>dst</scp> earthquakes, a 4- to 6-m run-up may
flood part of the Syrian, Lebanese, and Israeli coasts. Tsunamis from remote
earthquakes, however, arrive later and produce only 1- to 3-m run-ups, but are
more regional in extent.</p>
<p><I>Online material:</I> Tsunami modeling and reports.</p>
]]></description>
<dc:creator><![CDATA[Salamon, A., Rockwell, T., Ward, S. N., Guidoboni, E., Comastri, A.]]></dc:creator>
<dc:date>2007-06-11</dc:date>
<dc:identifier>info:doi/10.1785/0120060147</dc:identifier>
<dc:title><![CDATA[[Articles] Tsunami Hazard Evaluation of the Eastern Mediterranean: Historical Analysis and Selected Modeling]]></dc:title>
<dc:publisher>Seismological Society of America</dc:publisher>
<prism:number>3</prism:number>
<prism:volume>97</prism:volume>
<prism:endingPage>724</prism:endingPage>
<prism:publicationDate>2007-06-01</prism:publicationDate>
<prism:startingPage>705</prism:startingPage>
<prism:section>Articles</prism:section>
</item>

<item rdf:about="http://www.bssaonline.org/cgi/content/abstract/97/3/725?rss=1">
<title><![CDATA[[Articles] Unveiling the Sources of the Catastrophic 1456 Multiple Earthquake: Hints to an Unexplored Tectonic Mechanism in Southern Italy]]></title>
<link>http://www.bssaonline.org/cgi/content/abstract/97/3/725?rss=1</link>
<description><![CDATA[
<p>We revisited data related to the 1456 seismic crisis, the largest earthquake
to have ever occurred in peninsular Italy, in search of its causative source(s).
Data about this earthquake consist solely of historical reports and their
intensity assessment.</p>
<p>Because of the age of this multiple earthquake, the scarcity and sparseness
of the data, and the unusually large damage area, no previous studies have
attempted to attribute the 1456 events to specific faults. Existing analytical
methods to identify a likely source from intensity data also proved
inappropriate for such a sparse dataset, since historical evidence suggests that
the cumulative damage pattern contains at least three widely separated
events.</p>
<p>We subdivided the 1456 damage pattern into three independent mesoseismal
areas; each of these areas falls onto east&ndash;west tectonic trends previously
identified and marked by deep (&gt;10 km) right-lateral slip earthquakes. Based
on this evidence we propose (1) that the 1456 events were generated by
individual segments of regional east&ndash;west structures and are evidence of a
seismogenic style that involves oblique dextral reactivation of east&ndash;west
lower crustal faults; (2) that each event may have triggered subsequent but
relatively distant events in a cascade fashion, as suggested by historical
accounts; hence (3) that the 1456 sequence reveals a fundamental but unexplored
mechanism of tectonic deformation and seismic release in southern Italy. This
style dominates the region that lies between the northwest&ndash;southeast
system of large extensional faults straddling the crest of the southern
Apennines and the buried outer front of the chain.</p>
<p>Although the quality of the available information concerning the 1456
earthquake is naturally limited, we show that the overlap of the damage
distribution, the orientation and characteristics of regional tectonic
structures, the seismicity patterns, and the focal mechanisms all concur with
our interpretations and would be difficult to justify otherwise.</p>
]]></description>
<dc:creator><![CDATA[Fracassi, U., Valensise, G.]]></dc:creator>
<dc:date>2007-06-11</dc:date>
<dc:identifier>info:doi/10.1785/0120050250</dc:identifier>
<dc:title><![CDATA[[Articles] Unveiling the Sources of the Catastrophic 1456 Multiple Earthquake: Hints to an Unexplored Tectonic Mechanism in Southern Italy]]></dc:title>
<dc:publisher>Seismological Society of America</dc:publisher>
<prism:number>3</prism:number>
<prism:volume>97</prism:volume>
<prism:endingPage>748</prism:endingPage>
<prism:publicationDate>2007-06-01</prism:publicationDate>
<prism:startingPage>725</prism:startingPage>
<prism:section>Articles</prism:section>
</item>

<item rdf:about="http://www.bssaonline.org/cgi/content/abstract/97/3/749?rss=1">
<title><![CDATA[[Articles] 12,000-Year-Long Record of 10 to 13 Paleoearthquakes on the Yammouneh Fault, Levant Fault System, Lebanon]]></title>
<link>http://www.bssaonline.org/cgi/content/abstract/97/3/749?rss=1</link>
<description><![CDATA[
<p>We present results of the first paleoseismic study of the Yammo&ucirc;neh
fault, the main on-land segment of the Levant fault system within the Lebanese
restraining bend. A trench was excavated in the Yammo&ucirc;neh paleolake, where
the fault cuts through finely laminated sequences of marls and clays.
First-order variations throughout this outstanding stratigraphic record appear
to reflect climate change at centennial and millennial scales. The lake beds are
offset and deformed in a 2-m- wide zone coinciding with the mapped fault trace.
Ten to thirteen events are identified, extending back more than ~12 kyr.
Reliable age bounds on seven of these events constrain the mean seismic return
time to 1127 &plusmn; 135 yr between ~12 ka and ~6.4 ka, implying that
this fault slips in infrequent but large (<I>M</I> ~7.5) earthquakes. Our
results also provide conclusive evidence that the latest event at this site was
the great <scp>a.d.</scp> 1202 historical earthquake, and suggest that the
Yammo&ucirc;neh fault might have been the source of a less well-known event
circa <scp>a.d.</scp> 350. These findings, combined with previous paleoseismic
data from the Zebadani valley, imply that the parallel faults bounding the Beqaa
release strain in events with comparable recurrence intervals but significantly
different magnitudes. Our results contribute to document the clustering of large
events on the Levant fault into centennial episodes, such as that during the
eleventh through twelfth centuries, separated by millennial periods of
quiescence, and raise the possibility of a <I>M</I> &gt;7 event occurring on
the Yammo&ucirc;neh fault in the coming century. Such a scenario should be taken
into account in regional seismic-hazard assessments and planned for
accordingly.</p>
]]></description>
<dc:creator><![CDATA[Daeron, M., Klinger, Y., Tapponnier, P., Elias, A., Jacques, E., Sursock, A.]]></dc:creator>
<dc:date>2007-06-11</dc:date>
<dc:identifier>info:doi/10.1785/0120060106</dc:identifier>
<dc:title><![CDATA[[Articles] 12,000-Year-Long Record of 10 to 13 Paleoearthquakes on the Yammouneh Fault, Levant Fault System, Lebanon]]></dc:title>
<dc:publisher>Seismological Society of America</dc:publisher>
<prism:number>3</prism:number>
<prism:volume>97</prism:volume>
<prism:endingPage>771</prism:endingPage>
<prism:publicationDate>2007-06-01</prism:publicationDate>
<prism:startingPage>749</prism:startingPage>
<prism:section>Articles</prism:section>
</item>

<item rdf:about="http://www.bssaonline.org/cgi/content/abstract/97/3/772?rss=1">
<title><![CDATA[[Articles] Tectonic Processes in the Jan Mayen Fracture Zone Based on Earthquake Occurrence and Bathymetry]]></title>
<link>http://www.bssaonline.org/cgi/content/abstract/97/3/772?rss=1</link>
<description><![CDATA[
<p>Jan Mayen is an active volcanic island situated along the mid-Atlantic Ridge
north of Iceland. It is closely connected with the geodynamic processes
associated with the interaction between the Jan Mayen Fracture Zone
(<scp>jmfz</scp>) and the slowly spreading Kolbeinsey and Mohns Ridges. Despite
the significant tectonic activity expressed by the frequent occurrence of medium
to large earthquakes, detailed correlation between individual events and the
causative faults along the <scp>jmfz</scp> has been lacking. Recently acquired
detailed bathymetric data in the vicinity of Jan Mayen has allowed us to
document such correlation for the first time. The earthquake of 14 April 2004
(<I>M</I><SUB>w</SUB> 6), which occurred along the <scp>jmfz</scp>, was
studied in detail and correlated with the bathymetry. Locations of aftershocks
within the first 12 hours after the mainshock outline a 10-km-long fault plane.
Interactions between various fault systems are demonstrated through locations of
later aftershocks, which indicate that supposedly normal fault structures to the
north of the ruptured fault, in the Jan Mayen Platform, have been reactivated.
Correlation of the waveforms shows that events located on these structures are
significantly different from activity at neighboring structures. Coulomb stress
modeling gives an explanation to the locations of the aftershocks but cannot
reveal any information about their mechanisms.</p>
]]></description>
<dc:creator><![CDATA[Sorensen, M. B., Ottemoller, L., Havskov, J., Atakan, K., Hellevang, B., Pedersen, R. B.]]></dc:creator>
<dc:date>2007-06-11</dc:date>
<dc:identifier>info:doi/10.1785/0120060025</dc:identifier>
<dc:title><![CDATA[[Articles] Tectonic Processes in the Jan Mayen Fracture Zone Based on Earthquake Occurrence and Bathymetry]]></dc:title>
<dc:publisher>Seismological Society of America</dc:publisher>
<prism:number>3</prism:number>
<prism:volume>97</prism:volume>
<prism:endingPage>779</prism:endingPage>
<prism:publicationDate>2007-06-01</prism:publicationDate>
<prism:startingPage>772</prism:startingPage>
<prism:section>Articles</prism:section>
</item>

<item rdf:about="http://www.bssaonline.org/cgi/content/abstract/97/3/780?rss=1">
<title><![CDATA[[Articles] Aftershock Detection Thresholds as a Function of Time: Results from the ANZA Seismic Network following the 31 October 2001 ML 5.1 Anza, California, Earthquake]]></title>
<link>http://www.bssaonline.org/cgi/content/abstract/97/3/780?rss=1</link>
<description><![CDATA[
<p>We examine aftershock detectability thresholds for events in the initial part
of the 31 October 2001, <I>M</I><SUB>L</SUB> 5.1 sequence in southern
California. This sequence occurred directly below the broadband <scp>anza</scp>
seismic network, which recorded continuous waveform data at 13 azimuthally
well-distributed stations within the study region (seven had epicentral
distances &lt; 20 km). Of the 608 aftershocks (0 &lt; <I>M</I><SUB>L</SUB>
&lt; ~2.8) in the initial 2 hr of this sequence, the first five aftershocks
recorded were only identifiable at stations within 30 km after applying a
high-pass filter. Using a cluster (radius &le; 1.1 km) of 200 representative
aftershocks, we track the maximum seismogram amplitude versus earthquake
magnitude. This relationship helps us quantify the visibility of aftershocks
within the mainshock coda and assess our detection capabilities. We estimate
that detectable aftershocks within the mainshock coda include (1) those over
magnitude ~3 that are within 15 km of the network centroid that occur 12 sec
or more into the sequence, and (2) those over magnitude ~2 that are within
30 km of the centroid of the network that occur 60 sec or more into the
sequence. We find a lack of large aftershocks in this sequence. The largest
aftershock (<I>M</I><SUB>L</SUB> ~2.8) is substantially smaller than the
mainshock (<I>M</I><SUB>L</SUB> 5.1). We suggest this relatively
large-magnitude differential is dictated by a combination of factors that
includes complexity of the San Jacinto fault system and the lack of large
earthquakes in the region in the past ~20 years.</p>
<p><I>Online material:</I> Quicktime movies juxtaposing a 3.2 aftershock in
the coda of a 5.1 mainshock.</p>
]]></description>
<dc:creator><![CDATA[Kilb, D., Martynov, V. G., Vernon, F. L.]]></dc:creator>
<dc:date>2007-06-11</dc:date>
<dc:identifier>info:doi/10.1785/0120060116</dc:identifier>
<dc:title><![CDATA[[Articles] Aftershock Detection Thresholds as a Function of Time: Results from the ANZA Seismic Network following the 31 October 2001 ML 5.1 Anza, California, Earthquake]]></dc:title>
<dc:publisher>Seismological Society of America</dc:publisher>
<prism:number>3</prism:number>
<prism:volume>97</prism:volume>
<prism:endingPage>792</prism:endingPage>
<prism:publicationDate>2007-06-01</prism:publicationDate>
<prism:startingPage>780</prism:startingPage>
<prism:section>Articles</prism:section>
</item>

<item rdf:about="http://www.bssaonline.org/cgi/content/abstract/97/3/793?rss=1">
<title><![CDATA[[Articles] Wavelet Transform Methods for Azimuth Estimation in Local Three-Component Seismograms]]></title>
<link>http://www.bssaonline.org/cgi/content/abstract/97/3/793?rss=1</link>
<description><![CDATA[
<p>We have developed a new method for estimating azimuth in local three-
component seismograms through wavelet analysis. The proposed process proceeds in
three stages. First, the seismogram is filtered through a wavelet packet
approach. Second, the first arrival is determined through a <I>P</I> picker
similar to a short-term- average long-term-average scheme that is applied on the
wavelet domain. Finally, an adaptive-length window around the pick is selected
and used for determining the azimuth, using the property of linear polarization
of the first arrival.</p>
<p>The proposed method has been applied to three-component short-period
seismograms for local earthquakes recorded by the seismic network of Alicante
province in southeastern Spain. The locations of these events were previously
obtained through the software HYPO71PC
(<cross-ref type="bib" refid="bib7">Lee and Valdes, 1989</cross-ref>) and the
seismograms recorded by four analog stations of vertical component distributed
within the province of Alicante. The results obtained by the wavelet-based
algorithm have been compared with the azimuth angles obtained through the
results from the location software. The comparison indicates that the proposed
algorithm can determine the azimuth of the analyzed events to within a mean bias
of 4.5&deg;.</p>
]]></description>
<dc:creator><![CDATA[Galiana-Merino, J. J., Rosa-Herranz, J., Jauregui, P., Molina, S., Giner, J.]]></dc:creator>
<dc:date>2007-06-11</dc:date>
<dc:identifier>info:doi/10.1785/0120050225</dc:identifier>
<dc:title><![CDATA[[Articles] Wavelet Transform Methods for Azimuth Estimation in Local Three-Component Seismograms]]></dc:title>
<dc:publisher>Seismological Society of America</dc:publisher>
<prism:number>3</prism:number>
<prism:volume>97</prism:volume>
<prism:endingPage>803</prism:endingPage>
<prism:publicationDate>2007-06-01</prism:publicationDate>
<prism:startingPage>793</prism:startingPage>
<prism:section>Articles</prism:section>
</item>

<item rdf:about="http://www.bssaonline.org/cgi/content/abstract/97/3/804?rss=1">
<title><![CDATA[[Articles] Regional Travel-Time Uncertainty and Seismic Location Improvement Using a Three-Dimensional a priori Velocity Model]]></title>
<link>http://www.bssaonline.org/cgi/content/abstract/97/3/804?rss=1</link>
<description><![CDATA[
<p>We demonstrate our ability to improve regional travel-time prediction and
seismic event location accuracy using an <I>a priori</I> 3D velocity model of
Western Eurasia and North Africa (WENA1.0). Travel-time residuals are assessed
relative to the <I>iasp91</I> model for approximately 6000 <I>Pg, Pn</I>,
and <I>P</I> arrivals, from seismic events having 2<I></I> epicenter
accuracy between 1 km and 25 km (ground truth 1 [GT1] and GT25,
respectively), recorded at 39 stations throughout the model region. Ray paths
range in length between 0&deg; and 40&deg; (local, regional, and near
teleseismic) providing depth sounding that spans the crust and upper mantle. The
dataset also provides representative geographic sampling across Eurasia and
North Africa including aseismic areas. The WENA1.0 model markedly improves
travel-time predictions for most stations with an average variance reduction of
29% for all ray paths from the GT25 events; when we consider GT5 and better
events alone, the variance reduction is 49%. For location tests we use 196
geographically distributed GT5 and better events. In 134 cases (68% of the
events), locations are improved, and average mislocation is reduced from 24.9 km
to 17.7 km. We develop a travel-time uncertainty model that is used to calculate
location coverage ellipses. The coverage ellipses for WENA1.0 are validated to
be representative of epicenter error and are smaller than those for
<I>iasp91</I> by 37%. We conclude that <I>a priori</I> models are directly
applicable where data coverage limits tomographic and empirical approaches, and
the development of the uncertainty model enables merging of <I>a priori</I>
and data-driven approaches using Bayesian techniques.</p>
<p><I>Online material:</I> Correction surfaces and histograms of travel-time
residuals for 40 stations.</p>
]]></description>
<dc:creator><![CDATA[Flanagan, M. P., Myers, S. C., Koper, K. D.]]></dc:creator>
<dc:date>2007-06-11</dc:date>
<dc:identifier>info:doi/10.1785/0120060079</dc:identifier>
<dc:title><![CDATA[[Articles] Regional Travel-Time Uncertainty and Seismic Location Improvement Using a Three-Dimensional a priori Velocity Model]]></dc:title>
<dc:publisher>Seismological Society of America</dc:publisher>
<prism:number>3</prism:number>
<prism:volume>97</prism:volume>
<prism:endingPage>825</prism:endingPage>
<prism:publicationDate>2007-06-01</prism:publicationDate>
<prism:startingPage>804</prism:startingPage>
<prism:section>Articles</prism:section>
</item>

<item rdf:about="http://www.bssaonline.org/cgi/content/abstract/97/3/826?rss=1">
<title><![CDATA[[Articles] Seismic Velocity Structure and Seismotectonics of the Eastern San Francisco Bay Region, California]]></title>
<link>http://www.bssaonline.org/cgi/content/abstract/97/3/826?rss=1</link>
<description><![CDATA[
<p>The Hayward Fault System is considered the most likely fault system in the
San Francisco Bay Area, California, to produce a major earthquake in the next 30
years. To better understand this fault system, we use microseismicity to study
its structure and kinematics. We present a new 3D seismic-velocity model for the
eastern San Francisco Bay region, using microseismicity and controlled sources,
which reveals a ~10% velocity contrast across the Hayward fault in the upper
10 km, with higher velocity in the Franciscan Complex to the west relative to
the Great Valley Sequence to the east. This contrast is imaged more sharply in
our localized model than in previous regional-scale models. Thick Cenozoic
sedimentary basins, such as the Livermore basin, which may experience
particularly strong shaking during an earthquake, are imaged in the model.</p>
<p>The accurate earthquake locations and focal mechanisms obtained by using the
3D model allow us to study fault complexity and its implications for seismic
hazard. The relocated hypocenters along the Hayward Fault in general are
consistent with a near-vertical or steeply east-dipping fault zone. The southern
Hayward fault merges smoothly with the Calaveras fault at depth, suggesting that
large earthquakes may rupture across both faults. The use of the 3D velocity
model reveals that most earthquakes along the Hayward fault have near-vertical
strike-slip focal mechanisms, consistent with the large-scale orientation and
sense of slip of the fault, with no evidence for zones of complex fracturing
acting as barriers to earthquake rupture.</p>
<p><I>Online material:</I> Velocity model validation experiments and
additional seismicity plots.</p>
]]></description>
<dc:creator><![CDATA[Hardebeck, J. L., Michael, A. J., Brocher, T. M.]]></dc:creator>
<dc:date>2007-06-11</dc:date>
<dc:identifier>info:doi/10.1785/0120060032</dc:identifier>
<dc:title><![CDATA[[Articles] Seismic Velocity Structure and Seismotectonics of the Eastern San Francisco Bay Region, California]]></dc:title>
<dc:publisher>Seismological Society of America</dc:publisher>
<prism:number>3</prism:number>
<prism:volume>97</prism:volume>
<prism:endingPage>842</prism:endingPage>
<prism:publicationDate>2007-06-01</prism:publicationDate>
<prism:startingPage>826</prism:startingPage>
<prism:section>Articles</prism:section>
</item>

<item rdf:about="http://www.bssaonline.org/cgi/content/abstract/97/3/843?rss=1">
<title><![CDATA[[Articles] A Regional Ground-Motion Excitation/Attenuation Model for the San Francisco Region]]></title>
<link>http://www.bssaonline.org/cgi/content/abstract/97/3/843?rss=1</link>
<description><![CDATA[
<p>By using small-to-moderate earthquakes located within ~200 km of San
Francisco, we characterize the scaling of the ground motions for frequencies
ranging between 0.25 and 20 Hz, obtaining results for geometric spreading,
<I>Q</I>(<I>f</I>), and site parameters using the methods of
<cross-ref type="bib" refid="bib31">Mayeda <I>et al.</I> (2005)</cross-ref>
and
<cross-ref type="bib" refid="bib28">Malagnini <I>et al.</I> (2004)</cross-ref>.
The results of the analysis show that, throughout the Bay Area, the average
regional attenuation of the ground motion can be modeled with a bilinear
geometric spreading function with a 30-km crossover distance, coupled to an
anelastic function exp(&ndash;<I>fr</I>/<I>Q</I>(<I>f</I>),
where: <I>Q</I>(<I>f</I>) = 180 <I>f</I><sup>0.42</sup>. A
body-wave geometric spreading, <I>g</I>(<I>r</I>) =
<I>r</I><sup>&ndash;1.0</sup>, is used at short hypocentral distances
(<I>r</I> &lt; 30 km), whereas <I>g</I>(<I>r</I>) =
<I>r</I><sup>&ndash;0.6</sup> fits the attenuation of the spectral amplitudes
at hypocentral distances beyond the crossover.</p>
<p>The frequency-dependent site effects at twelve of the Berkeley Digital
Seismic Network stations were evaluated in an absolute sense using coda-derived
source spectra. Our results show the following. (1) The absolute site response
for frequencies ranging between 0.3 Hz and 2.0 Hz correlate with independent
estimates of the local magnitude residuals (<I>M</I><SUB>L</SUB>) for
each of the stations. (2) Moment magnitudes (<I>M</I><SUB>w</SUB>) derived
from our path and site-corrected spectra are in excellent agreement with those
independently derived using full-waveform modeling as well as coda-derived
source spectra. (3) We use our weak-motion-based relationships to predict
motions regionwide for the Loma Prieta earthquake, well above the maximum
magnitude spanned by our data set, on a completely different set of stations.
Results compare well with measurements taken at specific National Earthquake
Hazards Reduction Program site classes. (4) An empirical, magnitude-dependent
scaling was necessary for the Brune stress parameter to match the
large-magnitude spectral accelerations and peak ground velocities with our
weak-motion-based model.</p>
<p><I>Online material:</I> Tables of peak ground acceleration, peak ground
velocity, and pseudo-spectral acceleration at 0.3 sec, 1.0 sec, and 3.0 sec.</p>
]]></description>
<dc:creator><![CDATA[Malagnini, L., Mayeda, K., Uhrhammer, R., Akinci, A., Herrmann, R. B.]]></dc:creator>
<dc:date>2007-06-11</dc:date>
<dc:identifier>info:doi/10.1785/0120060101</dc:identifier>
<dc:title><![CDATA[[Articles] A Regional Ground-Motion Excitation/Attenuation Model for the San Francisco Region]]></dc:title>
<dc:publisher>Seismological Society of America</dc:publisher>
<prism:number>3</prism:number>
<prism:volume>97</prism:volume>
<prism:endingPage>862</prism:endingPage>
<prism:publicationDate>2007-06-01</prism:publicationDate>
<prism:startingPage>843</prism:startingPage>
<prism:section>Articles</prism:section>
</item>

<item rdf:about="http://www.bssaonline.org/cgi/content/abstract/97/3/863?rss=1">
<title><![CDATA[[Articles] Anomalous Propagation of Long-Period Ground Motions Recorded in Tokyo during the 23 October 2004 Mw 6.6 Niigata-ken Chuetsu, Japan, Earthquake]]></title>
<link>http://www.bssaonline.org/cgi/content/abstract/97/3/863?rss=1</link>
<description><![CDATA[
<p>Unusually large (&gt;5 cm) and prolonged shaking associated with long- period
ground motions at periods of about 7 sec were observed in central Tokyo during
the <I>M</I><SUB>w</SUB> 6.6 Niigata-ken Chuetsu earthquake of 23 October
2004. The long- period ground motions caused significant resonance in high-rise
buildings of about 70 floors in height. Thus, it is an urgent matter to
understand the development and amplification properties of long-period ground
motions in Tokyo associated with large earthquakes.</p>
<p>In this study, we use numerous waveform records from 585 stations in a
nationwide accelerometer network (K-NET, KiK-net) and 495 intensity meters in
the area around Tokyo. The data reveal that the long-period ground motion is
characterized in most part by a surface, Rayleigh wave generated at the northern
edge of Kanto basin, and the surface wave is developed as propagating through a
thick cover of sediments (&gt;3000&ndash;4000 m) that overlies rigid
bedrock.</p>
<p>To complement the observational data, we conducted a large-scale computer
simulation of seismic-wave propagation by employing the Earth Simulator
supercomputer with a detailed source-slip model and a high-resolution 3D
sedimentary structural model of central Japan. The results of the computer
simulation demonstrate that the anomalously prolonged ground shaking of the
long-period signal recorded in the center of Tokyo occurred because of the
stagnation of seismic energy resulting from the multipathing and focusing of
Rayleigh waves toward the bottom of the Kanto basin from surrounding mountain
regions with interaction to the 3D basin structure.</p>
<p><I>Online material:</I> Animations of long-period ground motions in
Tokyo.</p>
]]></description>
<dc:creator><![CDATA[Furumura, T., Hayakawa, T.]]></dc:creator>
<dc:date>2007-06-11</dc:date>
<dc:identifier>info:doi/10.1785/0120060166</dc:identifier>
<dc:title><![CDATA[[Articles] Anomalous Propagation of Long-Period Ground Motions Recorded in Tokyo during the 23 October 2004 Mw 6.6 Niigata-ken Chuetsu, Japan, Earthquake]]></dc:title>
<dc:publisher>Seismological Society of America</dc:publisher>
<prism:number>3</prism:number>
<prism:volume>97</prism:volume>
<prism:endingPage>880</prism:endingPage>
<prism:publicationDate>2007-06-01</prism:publicationDate>
<prism:startingPage>863</prism:startingPage>
<prism:section>Articles</prism:section>
</item>

<item rdf:about="http://www.bssaonline.org/cgi/content/abstract/97/3/881?rss=1">
<title><![CDATA[[Articles] Sensitivity of Ground-Motion Simulations to Earthquake Source Parameters: A Case Study for Istanbul, Turkey]]></title>
<link>http://www.bssaonline.org/cgi/content/abstract/97/3/881?rss=1</link>
<description><![CDATA[
<p>Following the disastrous earthquakes in Izmit and D&uuml;zce along the North
Anatolian fault in 1999, the earthquake hazard in the Istanbul area became a
great concern. In this study we simulate strong ground motions caused by a
scenario earthquake (<I>M</I> 7.5) in the Marmara Sea, and investigate the
effect of varying the input parameters on the broadband frequency ground motion.
Simulations are based on a multiasperity source model that involves the combined
rupture of the North Anatolian fault segments beneath the Marmara Sea. We use a
hybrid model combining a deterministic simulation of the low frequencies
(0.1&ndash;1.0 Hz) with a semistochastic simulation of the high frequencies
(1.0&ndash;10.0 Hz). Computation at each frequency range is performed separately
and the total ground motion is combined in the time domain. Computations are
linear and are performed at bedrock level, thereby not taking any effect of
local geological conditions into account. We calculate a total of 17 earthquake
scenarios corresponding to different source and attenuation parameters to study
their effect on the ground motion. The most significant parameters in terms of
ground-shaking level are the rise time, rupture velocity, rupture initiation
point, and stress drop. The largest variability of strong ground motions is
observed in regions adjacent to asperities and is associated with frequencies
higher than 5 Hz. For lower frequencies our simulated velocity spectra within
the Istanbul area are fairly stable among scenarios. The average standard
deviations of all ground-motion measures are less than 35% of the mean.</p>
<p><I>Online material:</I> Figures of peak ground acceleration and peak ground
velocity and their differences to the reference scenario values.</p>
]]></description>
<dc:creator><![CDATA[Sorensen, M. B., Pulido, N., Atakan, K.]]></dc:creator>
<dc:date>2007-06-11</dc:date>
<dc:identifier>info:doi/10.1785/0120060044</dc:identifier>
<dc:title><![CDATA[[Articles] Sensitivity of Ground-Motion Simulations to Earthquake Source Parameters: A Case Study for Istanbul, Turkey]]></dc:title>
<dc:publisher>Seismological Society of America</dc:publisher>
<prism:number>3</prism:number>
<prism:volume>97</prism:volume>
<prism:endingPage>900</prism:endingPage>
<prism:publicationDate>2007-06-01</prism:publicationDate>
<prism:startingPage>881</prism:startingPage>
<prism:section>Articles</prism:section>
</item>

<item rdf:about="http://www.bssaonline.org/cgi/content/abstract/97/3/901?rss=1">
<title><![CDATA[[Articles] Assessment of a Nonlinear Dynamic Rupture Inversion Technique Applied to a Synthetic Earthquake]]></title>
<link>http://www.bssaonline.org/cgi/content/abstract/97/3/901?rss=1</link>
<description><![CDATA[
<p>Dynamic rupture inversion is a powerful tool for learning why and how faults
fail, but much more work has been done in developing inversion methods than
evaluating how well these methods work. This study examines how well a nonlinear
rupture inversion method recovers a set of known dynamic rupture parameters on a
synthetic fault based on the 2000 western Tottori, Japan earthquake
(<I>M</I><SUB>w</SUB> 6.6). Rupture evolution on the fault is governed by a
slip-weakening friction law. A direct-search method known as the neighborhood
algorithm (<cross-ref type="bib" refid="bib23">Sambridge, 1999</cross-ref>) is
used to find optimal values of both the initial stress distribution and the
slip-weakening distance on the fault, based on misfit values between known and
predicted strong-motion displacement records. The yield stress and frictional
sliding stress on the fault are held constant. A statistical assessment of the
results shows that, for this test case, the inversion succeeds in locating all
parameters to within &plusmn;14% of their true values. With the model
configuration used in this study, the parameters located in the central rupture
area are better resolved than the parameters located at the sides and bottom of
the fault. In addition, a positive linear correlation between the mean initial
stress and the slip-weakening distance is identified. The investigation confirms
that dynamic rupture inversion is useful for determining rupture parameters on
the fault, but that intrinsic trade-offs and poor resolution of some parameters
limit the amount of information that can be unambiguously inferred from the
results. In addition, this study demonstrates that using a statistical approach
to assess nonlinear inversion results shows how sensitive the misfit measure is
to the various parameters, and allows a level of confidence to be attached to
the output parameter values.</p>
]]></description>
<dc:creator><![CDATA[Corish, S. M., Bradley, C. R., Olsen, K. B.]]></dc:creator>
<dc:date>2007-06-11</dc:date>
<dc:identifier>info:doi/10.1785/0120060066</dc:identifier>
<dc:title><![CDATA[[Articles] Assessment of a Nonlinear Dynamic Rupture Inversion Technique Applied to a Synthetic Earthquake]]></dc:title>
<dc:publisher>Seismological Society of America</dc:publisher>
<prism:number>3</prism:number>
<prism:volume>97</prism:volume>
<prism:endingPage>914</prism:endingPage>
<prism:publicationDate>2007-06-01</prism:publicationDate>
<prism:startingPage>901</prism:startingPage>
<prism:section>Articles</prism:section>
</item>

<item rdf:about="http://www.bssaonline.org/cgi/content/abstract/97/3/915?rss=1">
<title><![CDATA[[Articles] A Constitutive Criterion for the Fault: Modified Velocity-Weakening Law]]></title>
<link>http://www.bssaonline.org/cgi/content/abstract/97/3/915?rss=1</link>
<description><![CDATA[
<p>Expanding on a previous article, constitutive laws for solid friction are
examined jointly with available experimental results. The models are evaluated
by means of numerical dynamic analysis of two sliding blocks simulating adjacent
fault sections. Effective constitutive laws are determined as relations between
mean values of the relevant variables on a selected area of the sliding
surfaces. The material is initially assumed elastic and homogeneous and the
influence of nonhomogeneity evaluated next by modeling mass density,
Young&rsquo;s modulus, and friction coefficient as correlated random fields. The
effect of fractures in rock close to the fault is also numerically assessed.
Finally, the influence of rupture of protrusions (microasperities) between the
sliding surfaces is analyzed. The influence of size of the averaging interface
area on the parameters of the effective constitutive law is then obtained by
means of Monte Carlo simulation. When the rock regions adjacent to the fault are
assumed to be linearly elastic and homogeneous or nonhomogeneous no size effect
is observed. On the other hand, when the friction coefficient is characterized
by a random field, a size effect is detected. Fracture occurrence in the region
surrounding the fault does not cause significant alteration of the
macroconstitutive law, producing only minor perturbations of the <I>mean</I>
law determined without fracture, but it should also introduce high-frequency
<I>slave</I> vibrations. Finally, a macroconstitutive law that takes into
account the shear rupture of microasperities on the sliding surfaces is
suggested. The proposed modified velocity-weakening law, constitutes a more
general and flexible constitutive law.</p>
]]></description>
<dc:creator><![CDATA[Miguel, L. F. F., Riera, J. D.]]></dc:creator>
<dc:date>2007-06-11</dc:date>
<dc:identifier>info:doi/10.1785/0120060107</dc:identifier>
<dc:title><![CDATA[[Articles] A Constitutive Criterion for the Fault: Modified Velocity-Weakening Law]]></dc:title>
<dc:publisher>Seismological Society of America</dc:publisher>
<prism:number>3</prism:number>
<prism:volume>97</prism:volume>
<prism:endingPage>925</prism:endingPage>
<prism:publicationDate>2007-06-01</prism:publicationDate>
<prism:startingPage>915</prism:startingPage>
<prism:section>Articles</prism:section>
</item>

<item rdf:about="http://www.bssaonline.org/cgi/content/abstract/97/3/926?rss=1">
<title><![CDATA[[Articles] Wave Gradiometry in the Time Domain]]></title>
<link>http://www.bssaonline.org/cgi/content/abstract/97/3/926?rss=1</link>
<description><![CDATA[
<p>A time-domain approach for solving for the change in geometrical spreading
and horizontal wave slowness in wave gradiometry is presented based on the use
of the analytic signal. The horizontal displacement gradient of a wave is
linearly related to the displacement and its time derivative. The coefficients
of this relationship give the change of geometrical spreading, the change in
radiation pattern, and horizontal slowness. The new time-domain technique
incorporates estimates of the instantaneous amplitude and frequency of the three
time series to solve uniquely for the wave-field coefficients. The analysis is
simpler and more suited to fast array processing of displacement gradient data
sets compared with a spectral ratio method.</p>
]]></description>
<dc:creator><![CDATA[Langston, C. A.]]></dc:creator>
<dc:date>2007-06-11</dc:date>
<dc:identifier>info:doi/10.1785/0120060152</dc:identifier>
<dc:title><![CDATA[[Articles] Wave Gradiometry in the Time Domain]]></dc:title>
<dc:publisher>Seismological Society of America</dc:publisher>
<prism:number>3</prism:number>
<prism:volume>97</prism:volume>
<prism:endingPage>933</prism:endingPage>
<prism:publicationDate>2007-06-01</prism:publicationDate>
<prism:startingPage>926</prism:startingPage>
<prism:section>Articles</prism:section>
</item>

<item rdf:about="http://www.bssaonline.org/cgi/content/abstract/97/3/934?rss=1">
<title><![CDATA[[Articles] Damping Correction Factors for Horizontal Ground-Motion Response Spectra]]></title>
<link>http://www.bssaonline.org/cgi/content/abstract/97/3/934?rss=1</link>
<description><![CDATA[
<p>Damping correction factors (<scp>dcf</scp>s) are used to adjust response
spectral values corresponding to damping 5% of critical to other damping levels.
Trends in the analytical response of viscously damped, linear-elastic
<scp>sdof</scp> oscillators subjected to finite-duration, sinusoidal base
excitations show that <scp>dcf</scp>s depend on both the frequency and duration
of the ground motion, where the latter becomes significantly less influential as
damping increases. These analytical trends, in conjunction with correlations
relating duration and frequency content to earthquake magnitude, site- to-source
distance, site classification, and tectonic setting, are used to explain/study
observations in <scp>dcf</scp>s computed from a large ground-motion database for
the central- eastern and western United States. For <I></I> &ge; 2%, the
<scp>dcf</scp>s proposed by the authors depend on earthquake magnitude, site
classification, and tectonic setting, all of which significantly influence the
frequency content of ground motions. For <I></I> = 1%, the
<scp>dcf</scp>s proposed by the authors additionally depend on site-to-source
distance, which significantly influences the duration of ground motion. In
comparison with the <scp>dcf</scp>s proposed by the authors, commonly used and
recently proposed <scp>dcf</scp>s were shown to be both too low and too high,
depending on the relation, period range, damping ratio, earthquake magnitude,
site classification, and tectonic setting. Additionally, the <scp>dcf</scp>
relations proposed in the literature for ground motions exhibiting near-fault
effects should not be used for <I></I> &lt; 5%, and will likely be
significantly too high for periods close to that of the near-fault velocity
pulse(s) for <I></I> &ge; 5%.</p>
]]></description>
<dc:creator><![CDATA[Cameron, W. I., Green, R. A.]]></dc:creator>
<dc:date>2007-06-11</dc:date>
<dc:identifier>info:doi/10.1785/0120060034</dc:identifier>
<dc:title><![CDATA[[Articles] Damping Correction Factors for Horizontal Ground-Motion Response Spectra]]></dc:title>
<dc:publisher>Seismological Society of America</dc:publisher>
<prism:number>3</prism:number>
<prism:volume>97</prism:volume>
<prism:endingPage>960</prism:endingPage>
<prism:publicationDate>2007-06-01</prism:publicationDate>
<prism:startingPage>934</prism:startingPage>
<prism:section>Articles</prism:section>
</item>

<item rdf:about="http://www.bssaonline.org/cgi/content/abstract/97/3/961?rss=1">
<title><![CDATA[[Articles] Liquefaction, Ground Oscillation, and Soil Deformation at the Wildlife Array, California]]></title>
<link>http://www.bssaonline.org/cgi/content/abstract/97/3/961?rss=1</link>
<description><![CDATA[
<p>Excess pore-water pressure and liquefaction at the Wildlife Liquefaction
Array in 1987 were caused by deformation associated with both high-frequency
strong ground motion and 5.5-second-period Love waves. The Love waves produced
large (~1.5%) cyclic shear strains well after the stronger high-frequency
ground motion abated. These cyclic strains generated approximately from 13 to
35% of the excess pore-water pressure in the liquefied layer and caused excess
pore-water pressures ultimately to reach effective overburden stress. The
deformation associated with the Love waves explains the
"postearthquake" increase of pore-water pressure that was recorded
at the array. This explanation suggests that conventional methods for predicting
liquefaction based on peak ground acceleration are incomplete and may need to
consider cyclic strains associated with long-period surface waves. A
postearthquake survey of an inclinometer casing indicated permanent shear strain
associated with lateral spreading primarily occurred in the upper part of the
liquefied layer. Comparison of cone penetration test soundings conducted after
the earthquake with pre-earthquake soundings suggests sleeve friction increased.
Natural lateral variability of the liquefied layer obscured changes in tip
resistance despite a ~1% reduction in volume. The large oscillatory motion
associated with surface waves explains ground oscillation that has been reported
at some liquefaction sites during earthquakes.</p>
]]></description>
<dc:creator><![CDATA[Holzer, T. L., Youd, T. L.]]></dc:creator>
<dc:date>2007-06-11</dc:date>
<dc:identifier>info:doi/10.1785/0120060156</dc:identifier>
<dc:title><![CDATA[[Articles] Liquefaction, Ground Oscillation, and Soil Deformation at the Wildlife Array, California]]></dc:title>
<dc:publisher>Seismological Society of America</dc:publisher>
<prism:number>3</prism:number>
<prism:volume>97</prism:volume>
<prism:endingPage>976</prism:endingPage>
<prism:publicationDate>2007-06-01</prism:publicationDate>
<prism:startingPage>961</prism:startingPage>
<prism:section>Articles</prism:section>
</item>

<item rdf:about="http://www.bssaonline.org/cgi/content/abstract/97/3/977?rss=1">
<title><![CDATA[[Articles] Corner Frequency Scaling of Regional Seismic Phases for Underground Nuclear Explosions at the Nevada Test Site]]></title>
<link>http://www.bssaonline.org/cgi/content/abstract/97/3/977?rss=1</link>
<description><![CDATA[
<p>Model fits are used to estimate source spectral corner frequencies of
regional seismic phases <I>Pn</I>, <I>Pg</I>, and <I>Lg</I> from
underground nuclear explosions (<scp>une</scp>s) at the Nevada Test Site
(<scp>nts</scp>), based on recordings by Lawrence Livermore National Laboratory
(<scp>llnl</scp>) <scp>nts</scp> Network stations. The spectra are corrected for
instrument response, distance, and station effects, and then network averaged.
Explicit information regarding geophysical working-point properties, depth of
burial, and some announced yields for <scp>nts</scp> explosions
(<cross-ref type="bib" refid="bib18">Springer <I>et al.</I>, 2002</cross-ref>)
is utilized for the spectral modeling. Scaling of <I>Pn</I>, <I>Pg</I>, and
<I>Lg</I> corner frequencies with source yield is examined for sets of
explosions at Yucca Flat, Pahute Mesa, and Rainier Mesa with similar material
properties (medium type, density, velocities, and gas porosity). The
<scp>une</scp>s are limited to those in media with gas porosity of 10% or less
so that a source spectral model with a rolloff of <I>f</I><sup>&ndash;2</sup>
is applicable. Model comparisons are also examined for regional
<I>P</I>/<I>Lg</I> discriminants. A key result is that <I>Lg</I> corner
frequencies for <scp>nts</scp> <scp>une</scp>s exhibit similar scaling with
source size as for <I>P</I> waves, but shifted lower, analogous to
observations by <cross-ref type="bib" refid="bib4">Fisk (2006)</cross-ref> for
the Lop Nor, Semipalatinsk, and Novaya Zemlya test sites. This appears to
corroborate an important effect, that is, that major contributions to
<I>S</I>-wave generation by explosions occur near the source with a similar
length scale, comparable to the elastic radius, as for <I>P</I> waves from
explosions. Although the explicit physical mechanism is not yet understood, the
implications are important regarding where and perhaps how <I>S</I> waves are
predominantly generated by explosions. A related, key result is that the
increasing separation of <I>P</I>/<I>Lg</I> at higher frequencies between
<scp>nts</scp> explosions and earthquakes has a consistent model-based
explanation, as at other nuclear test sites, in terms of the difference between
explosion <I>P</I> and <I>S</I> corner frequencies.</p>
]]></description>
<dc:creator><![CDATA[Fisk, M. D.]]></dc:creator>
<dc:date>2007-06-11</dc:date>
<dc:identifier>info:doi/10.1785/0120060186</dc:identifier>
<dc:title><![CDATA[[Articles] Corner Frequency Scaling of Regional Seismic Phases for Underground Nuclear Explosions at the Nevada Test Site]]></dc:title>
<dc:publisher>Seismological Society of America</dc:publisher>
<prism:number>3</prism:number>
<prism:volume>97</prism:volume>
<prism:endingPage>988</prism:endingPage>
<prism:publicationDate>2007-06-01</prism:publicationDate>
<prism:startingPage>977</prism:startingPage>
<prism:section>Articles</prism:section>
</item>

<item rdf:about="http://www.bssaonline.org/cgi/content/abstract/97/3/989?rss=1">
<title><![CDATA[[Articles] Identification of Delay-Fired Mining Explosions Using Seismic Arrays: Application to the PDAR Array in Wyoming, USA]]></title>
<link>http://www.bssaonline.org/cgi/content/abstract/97/3/989?rss=1</link>
<description><![CDATA[
<p>We extend a time-frequency discrimination algorithm, developed in an earlier
article
(<cross-ref type="bib" refid="bib1">Arrowsmith <I>et al.</I>, 2006</cross-ref>),
for application to seismic-array data. Spectrograms evaluated at each component
of an array are stacked and then converted into binary form for computation of
discriminants. Because noise can bias the discriminants, we develop a procedure
for removing the effect of noise on the discriminants. The binary spectrograms
are randomized where the spectral amplitude of the signal is similar to the mean
spectral amplitude of the pre-event noise at that frequency. The formulism of
<cross-ref type="bib" refid="bib1">Arrowsmith <I>et al.</I> (2006)</cross-ref>
is further extended by modifying the objective function used to optimize the
values of input parameters and by removing high-frequency and low-frequency
spectral content. We apply the method to a dataset of regional recordings of
earthquakes and delay-fired mine blasts recorded at the Pinedale seismic array
in Wyoming. Our results show that the utilization of array data improves the
success rate for source identification. Furthermore, we find that incorporating
the noise-correction procedure increases the separation between earthquakes and
cast overburden blasts (the largest type of delay-fired mine blasts). In total,
the algorithm successfully identifies 97.4% of the events (74 of a total of 76
events, which comprise earthquakes and cast overburden blasts).</p>
]]></description>
<dc:creator><![CDATA[Arrowsmith, S. J., Hedlin, M. A. H., Arrowsmith, M. D., Stump, B. W.]]></dc:creator>
<dc:date>2007-06-11</dc:date>
<dc:identifier>info:doi/10.1785/0120060136</dc:identifier>
<dc:title><![CDATA[[Articles] Identification of Delay-Fired Mining Explosions Using Seismic Arrays: Application to the PDAR Array in Wyoming, USA]]></dc:title>
<dc:publisher>Seismological Society of America</dc:publisher>
<prism:number>3</prism:number>
<prism:volume>97</prism:volume>
<prism:endingPage>1001</prism:endingPage>
<prism:publicationDate>2007-06-01</prism:publicationDate>
<prism:startingPage>989</prism:startingPage>
<prism:section>Articles</prism:section>
</item>

<item rdf:about="http://www.bssaonline.org/cgi/content/abstract/97/3/1002?rss=1">
<title><![CDATA[[Articles] Imaging the Three-Dimensional Crust of the Korean Peninsula by Joint Inversion of Surface-Wave Dispersion and Teleseismic Receiver Functions]]></title>
<link>http://www.bssaonline.org/cgi/content/abstract/97/3/1002?rss=1</link>
<description><![CDATA[
<p>A detailed study of the 3D variation of shear-wave velocities in the southern
part of the Korean Peninsula is made by combining high-frequency surface- wave
tomography results of
<cross-ref type="bib" refid="bib7">Cho <I>et al.</I> (2006b)</cross-ref> with
teleseismic <I>P</I>-wave receiver functions at 80 locations on the peninsula.
Receiver functions were derived from high-gain acceleration, short-period, and
broadband digital data streams of the Korea Meteorological Administration
(<scp>kma</scp>) and Korean Institute for Geosciences and Mineral Resources
(<scp>kigam</scp>) networks. Vertical cross sections trace the lateral variation
in the depth to the Moho, the variation of low velocities near the surface, and
the variable thickness of the transition from surface velocities to midcrustal
velocities. The derived crustal structure provides new insights on the evolution
of the Korean crust.</p>
]]></description>
<dc:creator><![CDATA[Yoo, H. J., Herrmann, R. B., Cho, K. H., Lee, K.]]></dc:creator>
<dc:date>2007-06-11</dc:date>
<dc:identifier>info:doi/10.1785/0120060134</dc:identifier>
<dc:title><![CDATA[[Articles] Imaging the Three-Dimensional Crust of the Korean Peninsula by Joint Inversion of Surface-Wave Dispersion and Teleseismic Receiver Functions]]></dc:title>
<dc:publisher>Seismological Society of America</dc:publisher>
<prism:number>3</prism:number>
<prism:volume>97</prism:volume>
<prism:endingPage>1011</prism:endingPage>
<prism:publicationDate>2007-06-01</prism:publicationDate>
<prism:startingPage>1002</prism:startingPage>
<prism:section>Articles</prism:section>
</item>

<item rdf:about="http://www.bssaonline.org/cgi/content/abstract/97/3/1012?rss=1">
<title><![CDATA[[Articles] Spatial Distribution of Coda Q in South Korea]]></title>
<link>http://www.bssaonline.org/cgi/content/abstract/97/3/1012?rss=1</link>
<description><![CDATA[
<p>Analyzing spectral attenuation of coda waves, we first mapped coda
<I>Q</I>- values in the crust over the whole of South Korea. During the period
from 1995 to 2004, we selected 574 north&ndash;south-component seismograms with
epicentral distances less than 100 km from 328 earthquakes with magnitudes
between 1.4 and 5.2. We estimated coda <I>Q</I>-values using the single
isotropic scattering model at center frequencies of 1.5, 3, 6, 9, 12, 15, and 18
Hz, and found significant spatial variation over all frequency ranges and strong
frequency dependence of coda <I>Q</I> in the region. The estimated coda
<I>Q</I>-value at 1 Hz (<I>Q</I><SUB>0</SUB>) and the <I></I>-value
ranges are 80&ndash;300 and 0.4&ndash;1.1, respectively. The values have strong
correlation with the regional geology in the Korean peninsula. Low
<I>Q</I><SUB>0</SUB>-values are mainly obtained in the regions comprising
sedimentary strata in southeastern South Korea, whereas granite regions in the
northern part of South Korea show high <I>Q</I><SUB>0</SUB>. The
<I>Q</I><SUB>0</SUB>-values in the study area agree well with those of the
eastern China and Kyushu, western Japan. Furthermore, our <I></I>-values
are also in good agreement with those of Japan.</p>
<p><I>Online material:</I> Locations of seismometers, list of event-station
pairs, and linear regression of <I>Q<SUB>C</SUB></I> measurements.</p>
]]></description>
<dc:creator><![CDATA[Yun, S., Lee, W. S., Lee, K., Noh, M. H.]]></dc:creator>
<dc:date>2007-06-11</dc:date>
<dc:identifier>info:doi/10.1785/0120060097</dc:identifier>
<dc:title><![CDATA[[Articles] Spatial Distribution of Coda Q in South Korea]]></dc:title>
<dc:publisher>Seismological Society of America</dc:publisher>
<prism:number>3</prism:number>
<prism:volume>97</prism:volume>
<prism:endingPage>1018</prism:endingPage>
<prism:publicationDate>2007-06-01</prism:publicationDate>
<prism:startingPage>1012</prism:startingPage>
<prism:section>Articles</prism:section>
</item>

<item rdf:about="http://www.bssaonline.org/cgi/content/abstract/97/3/1019?rss=1">
<title><![CDATA[[Short Notes] Holocene Slip Rate for the Western Segment of the Castle Mountain Fault, Alaska]]></title>
<link>http://www.bssaonline.org/cgi/content/abstract/97/3/1019?rss=1</link>
<description><![CDATA[
<p>The western segment of the Castle Mountain fault poses a significant seismic
hazard to the most populated region of south-central Alaska. We identify a
previously unrecognized margin of a postglacial outwash channel that is offset
right laterally 36 &plusmn; 4 m across the western segment of the Castle
Mountain fault. This offset occurred after glaciers withdrew from the lowland
11,300&ndash;15,380 cal yr <scp>b.p.</scp> and after outwash channel margins
were cut and stabilized 11,210&ndash;13,470 cal yr <scp>b.p.</scp> Using these
ages and the measured separation, we obtain a maximum slip rate of 3.0 
&plusmn; 0.6 mm yr<sup>&ndash;1</sup> and a minimum slip rate of 2.8 &plusmn;
0.7 mm yr<sup>&ndash;1</sup>. These are the first lateral slip rates for the
Castle Mountain fault established by a field measurement. Based on timing of the
most recent earthquake, 670 &plusmn; 60 yr <scp>b.p.</scp>, the Castle Mountain
fault could have accumulated an average single-event slip of about 1.9 m
(extremes range from 1.3 to 2.6 m). The fault consists of two segments; a
surface-rupturing earthquake likely will be limited to the 62-km-long western
segment. Area-magnitude regression calculations suggest that such an earthquake
on the western Castle Mountain fault would have a moment magnitude of 6.9 to
7.3.</p>
]]></description>
<dc:creator><![CDATA[Willis, J. B., Haeussler, P. J., Bruhn, R. L., Willis, G. C.]]></dc:creator>
<dc:date>2007-06-11</dc:date>
<dc:identifier>info:doi/10.1785/0120060109</dc:identifier>
<dc:title><![CDATA[[Short Notes] Holocene Slip Rate for the Western Segment of the Castle Mountain Fault, Alaska]]></dc:title>
<dc:publisher>Seismological Society of America</dc:publisher>
<prism:number>3</prism:number>
<prism:volume>97</prism:volume>
<prism:endingPage>1024</prism:endingPage>
<prism:publicationDate>2007-06-01</prism:publicationDate>
<prism:startingPage>1019</prism:startingPage>
<prism:section>Short Notes</prism:section>
</item>

<item rdf:about="http://www.bssaonline.org/cgi/content/abstract/97/3/1025?rss=1">
<title><![CDATA[[Short Notes] Wave Propagation in Irregularly Layered Elastic Models: A Boundary Element Approach with a Global Reflection/Transmission Matrix Propagator]]></title>
<link>http://www.bssaonline.org/cgi/content/abstract/97/3/1025?rss=1</link>
<description><![CDATA[
<p>A direct boundary element method that uses the full-space Green&rsquo;s
function is proposed for calculating elastic wave propagation in two-dimensional
irregularly stratified models. The global matrix equation becomes larger as the
number of layers increases. These equations are usually solved by improved block
Gaussian elimination, conjugate gradient algorithms, or other approaches based
on different approximations. In this article, we adopt the global generalized
reflection/transmission matrix method
(<cross-ref type="bib" refid="bib7">Chen, 1990</cross-ref>,
<cross-ref type="bib" refid="bib8">1995</cross-ref>,
<cross-ref type="bib" refid="bib9">1996</cross-ref>) to solve this problem. This
method can prevent excessive requirement of both computer memory and CPU time.
The method is validated by comparing its results with those obtained using the
finite- difference method.</p>
]]></description>
<dc:creator><![CDATA[Ge, Z., Chen, X.]]></dc:creator>
<dc:date>2007-06-11</dc:date>
<dc:identifier>info:doi/10.1785/0120060216</dc:identifier>
<dc:title><![CDATA[[Short Notes] Wave Propagation in Irregularly Layered Elastic Models: A Boundary Element Approach with a Global Reflection/Transmission Matrix Propagator]]></dc:title>
<dc:publisher>Seismological Society of America</dc:publisher>
<prism:number>3</prism:number>
<prism:volume>97</prism:volume>
<prism:endingPage>1031</prism:endingPage>
<prism:publicationDate>2007-06-01</prism:publicationDate>
<prism:startingPage>1025</prism:startingPage>
<prism:section>Short Notes</prism:section>
</item>

<item rdf:about="http://www.bssaonline.org/cgi/content/short/97/3/1032?rss=1">
<title><![CDATA[[Errata] Earthquake Ground-Motion Prediction Equations for Eastern North America]]></title>
<link>http://www.bssaonline.org/cgi/content/short/97/3/1032?rss=1</link>
<description><![CDATA[]]></description>
<dc:creator><![CDATA[Atkinson, G. M., Boore, D. M.]]></dc:creator>
<dc:date>2007-06-11</dc:date>
<dc:identifier>info:doi/10.1785/0120070023</dc:identifier>
<dc:title><![CDATA[[Errata] Earthquake Ground-Motion Prediction Equations for Eastern North America]]></dc:title>
<dc:publisher>Seismological Society of America</dc:publisher>
<prism:number>3</prism:number>
<prism:volume>97</prism:volume>
<prism:endingPage>1032</prism:endingPage>
<prism:publicationDate>2007-06-01</prism:publicationDate>
<prism:startingPage>1032</prism:startingPage>
<prism:section>Errata</prism:section>
</item>

</rdf:RDF>