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Review and examples of repeating earthquake observations and interpretations, application in various zones, waveforms analysis, moment release distribution, uncertainties in P-wave picks and velocity models. Study of seismic slip activities and stress drops.
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RepeatingEarthquakes Olivier Lengliné - IPGS Strasbourg Cargeseschool
Pleaseinterrupt Questions / remarks
1 – Review of Repeatingearthquake observations & interpretations 2 – Twoexamples of application
Observations - Waveforms Nadeau & Johnson, 1998
Parkfield, California – Mw6.0 De Bilt, The Netherlands USGS Bakun et al., 2005
Off Kamaishi, Japan – M4.9 Time (s) Uchida et al., 2012
Chihshang fault, Taiwan Chen et al., 2008
Soultz-Sous-Forêts geothermal reservoir, France 9 events 9 events 13 events BRGM 19 events Time (s)
San-Andreas Fault Rubinstein et al., 2012 Schaff & Beroza, 1998
u(t) = Source * Path* Station Station is the same Change in medium property, [e.gPoupinet et al., 1984] Change in source properties, [e.g. Lengliné & Got, 2011]
Lengliné and Got, 2011 Directivity Velocity variations Poupinet et al., 1984
u(t) = Source * Path* Station Homogeneous medium waveformsimilarity Station the same Change in medium property, [e.gPoupinet et al., 1984] Change in source properties, [e.g. Lengliné & Got, 2011] !
Observations - Locations Waldhauser et al., 2004
Parkfield Murray & Langbein, 2006
Off Kamaishi Moment release distribution Relative moment releasednormalized by each maximum value Okadaet al., 2002
Earthquake relative relocation • Uncertainties P-wavepicks • Uncertainties of the velocity model
Earthquake relative relocation • Uncertainties P-wavepicks • Uncertainties of the velocity model • More precise data: time delaysestimatedfrom cross-correlation • Ray geometry – rotation • Do not correct absolute position
Earthquake relative relocation • Uncertainties P-wavepicks • Uncertainties of the velocity model • More precise data: time delaysestimatedfrom cross-correlation • Ray geometry – rotation • Do not correct absolute position • From cross-correlation centroid location • Got et al., 1994 • Waldhauser & Ellsworth, 2000
Earthquake relative relocation • Uncertainties P-wavepicks • Uncertainties of the velocity model • More precise data: time delaysestimatedfrom cross-correlation • Ray geometry – rotation • Do not correct absolute position • From cross-correlation centroid location • Got et al., 1994 • Waldhauser & Ellsworth, 2000 • See Tutorial thisafternoon for Methods
Lengliné & Marsan, 2008 Size = Assumed stress drop + circular crack + moment – magnitude relation
Taiwan Soultz-sous-Forêts Bourouis & Bernard, 2007 Radius estimatedfrom corner frequency Chen et al., 2008
Murray & Langbein, 2006 Clusters of co-located, similarwaveformsearthquakes, appearsat the transition betweenfullylocked and fullycreeping areas Rau et al., 2007
ExamplefromNorthern-California Parkfield Waldhauser & Schaff, 2008 Is itrelated to fault slip velocity ?
San Andreas Fault Rubin et al., 1999 Streaks of microearthquakes – along slip direction Rheological/ frictional/ geological / geometrical transition ?
Parkfield Earthquakenumber Time (years) μΔt = 24.5 yrσΔt = 9.5 yr COV = 0.37
Repeaters off Kamaishi Repeatinginterval = 5.35 +/- 0.5 yrs Time (years)
San-Andreas faultatParkfield Year Distance alongstrike (km) Waldhauser et al., 2004
Periodicrepeating ruptures Year Distance alongstrike (km) Waldhauser et al., 2004
Rubinstein et al., 2012 Quasi-periodicbehavior of the slip activity
The simplest model Aseismic slip No interactingasperity A lockedseismic patch embedded in a fullycreeping zone
Slip on the creeping part Slip on the seismicasperity Slip Time
Aseismic slip on the fault = seismic slip dseis Slip Time
Aseismic slip on the fault = seismic slip • Elastic solution for a circular crack
Aseismic slip on the fault = seismic slip • Elastic solution for a circular crack
Aseismic slip on the fault = seismic slip • Elastic solution for a circular crack • Constant stress drop
1st Hypothesis The constant stress drop hypothesisis not correct Empirical fit to the data thensuggests in order to have Tr ~ M01/6 Impliesthat the stress-drop ishigherfor smallevents. Stress levelsreach 2 GPafor the smallestevents(more than 10 times laboratorystrength) This resultisatoddswithestimatesbased on seismicspectra Relation not consistent withestablishedscaling relations for large earthquakes.
Chen & Lapusta, 2009 Chen & Lapusta, 2009
But not the estimated plate velocity – streaks close to locked section reducedvelocity ?
Slip on the creeping part Slip on the seismicasperity Slip Time Seismic slip
Off KamaishirepeatingsequencefollowingTohoku, 2011, Mw9 earthquake Uchida, 2014
Lengliné & Marsan 2008 Schaff & Beroza, 1998
Response of a velocitystrengthening area to a stress-step Marone, 1991 The Omorilikedecay of RES iswellrendered by the slip evolution of the creeping area following a stress step