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Annual Meeting - SCEC.org

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Group 2 – Seismology | Poster Abstracts<br />

2-110<br />

PRECISE RELATIVE LOCATION OF SAN ANDREAS FAULT TREMORS NEAR<br />

CHOLAME, CA USING SEISMOMETER CLUSTERS Shelly DR, Ellsworth WL, Nadeau<br />

RM, Burgmann R, Ryberg T, Haberland C, Murphy JM, and Fuis GS<br />

Non-volcanic tremor, similar in character to that generated at some subduction zones, was recently<br />

identified beneath the strike-slip San Andreas Fault (SAF) in central California. Using a matched<br />

filter method, we closely examine a 24-hour period of active SAF tremor and show that, like tremor<br />

in the Nankai Trough subduction zone, this tremor is composed of repeated similar events. We<br />

take advantage of this similarity to locate detected similar events relative to several chosen events.<br />

While low signal-to-noise makes location challenging, we compensate for this by estimating eventpair<br />

differential times at “clusters” of nearby temporary and permanent stations rather than at<br />

single stations. We find that the relative locations consistently form a near-linear structure in map<br />

view, striking parallel to the surface trace of the SAF. Therefore, we suggest that at least a portion<br />

of the tremor occurs on the deep extension of the fault, similar to the situation for subduction zone<br />

tremor. Also notable is the small depth range (a few hundred meters or less) of many of the located<br />

tremors, a feature possibly analogous to earthquake streaks observed on the shallower portion of<br />

the fault. The close alignment of the tremor with the SAF slip orientation suggests a shear slip<br />

mechanism, as has been argued for subduction tremor. At times, we observe a clear migration of<br />

the tremor source along the fault, at rates of ~20 km/hr.<br />

2-111<br />

ESTIMATING THE RUPTURE VELOCITY OF SMALL EARTHQUAKES McGuire JJ,<br />

Ide S, Kim M, Iidaka T, and Hirata N<br />

Studies of earthquake scaling are extremely common but have been inconclusive in determining<br />

the existence of any fundamental differences in the mechanical processes controlling small and<br />

large earthquakes. While many studies have found a deficit of radiated energy per unit moment<br />

release in small earthquakes, work by Ide and Beroza (2001) called these interpretations into<br />

question. Much of the uncertainty in whether there are major differences between small and large<br />

earthquakes results directly from the difficulty in measuring the energy radiated by small<br />

earthquakes. Kanamori and Rivera (2004) pointed out that if the observed deficiency in radiated<br />

energy for small earthquakes is real, then either the rupture velocity and/or the static stress drop<br />

must decrease for small earthquakes. A surprising result since some studies have suggested that<br />

small earthquakes have higher stress drops. If this difference was reflected primarily in rupture<br />

velocity, the velocity of magnitude 3 earthquakes would be at most half (for e=0.5) of that in<br />

magnitude 7 earthquakes.<br />

We estimated the rupture velocity of earthquakes between M3 and M5 for faults in California and<br />

Japan using an Empirical Green's Function (EGF) deconvolution technique. The time functions<br />

resulting from the EGF deconvolution show clear variation in their durations as a function of<br />

azimuth for a given earthquake. This signal is inverted for the second moments of the earthquake's<br />

space-time moment-release distribution which provide a lower bound on rupture velocity<br />

(McGuire 2004). The EGF approach leads to relatively tight constraints on earthquake scaling<br />

because the azimuthal variation in time function duration is more clearly resolved than the<br />

azimuthal variation in corner frequency. We find no evidence for a decrease in rupture velocity<br />

with earthquake size. Magnitude 3 events within the rupture zones of the 2000 M6.5 Tottori and<br />

2004 M6 Parkfield earthquakes have rupture velocities that are indistinguishable from those of the<br />

mainshocks on the same faults and error analysis demonstrated that rupture velocities faster than<br />

2.0 km/s are required with best fit values closer to 3 km/s. These general patterns hold true for<br />

crustal earthquakes in many regions of Japan recorded by the HINET array. We find that the value<br />

2008 <strong>SCEC</strong> <strong>Annual</strong> <strong>Meeting</strong> | 201

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