2013
DOI: 10.1785/0120120148
|View full text |Cite
|
Sign up to set email alerts
|

Rupture History of the 2011 M 9 Tohoku Japan Earthquake Determined from Strong-Motion and High-Rate GPS Recordings: Subevents Radiating Energy in Different Frequency Bands

Abstract: Strong-motion records from KiK-net and K-NET, along with 1 sample/s Global Positioning System (GPS) records from GEONET, were analyzed to determine the location, timing, and slip of subevents of the M 9 2011 Tohoku earthquake. Timing of arrivals on stations along the coast shows that the first subevent was located closer to the coast than subevent (2), which produced the largest slip. A waveform inversion of data from 0 to 0.2 Hz indicates that the first subevent primarily ruptured down-dip and north of the hy… Show more

Help me understand this report

Search citation statements

Order By: Relevance

Paper Sections

Select...
1
1
1
1

Citation Types

0
15
0

Year Published

2014
2014
2023
2023

Publication Types

Select...
4
1
1

Relationship

0
6

Authors

Journals

citations
Cited by 35 publications
(15 citation statements)
references
References 32 publications
0
15
0
Order By: Relevance
“…This depth corresponds to the location on the fault plane with a coupling factor of approximately 0.25. Given the observation that the down-dip portion of the rupture zone of the 2011 M w 9.0 Tohoku earthquake that generated significant strong ground motions had a coseismic slip much lower than the peak slip determined for the rupture (Frankel, 2013), workshop participants thought that using the 1-cm/yr locking contour (about 25 percent locking) for the consensus estimate of the downdip edge was a reasonable strategy.…”
Section: Logic Tree For Down-dip Edge Of Rupturementioning
confidence: 99%
“…This depth corresponds to the location on the fault plane with a coupling factor of approximately 0.25. Given the observation that the down-dip portion of the rupture zone of the 2011 M w 9.0 Tohoku earthquake that generated significant strong ground motions had a coseismic slip much lower than the peak slip determined for the rupture (Frankel, 2013), workshop participants thought that using the 1-cm/yr locking contour (about 25 percent locking) for the consensus estimate of the downdip edge was a reasonable strategy.…”
Section: Logic Tree For Down-dip Edge Of Rupturementioning
confidence: 99%
“…These earthquakes had a return period of approximately 500 years and were derived by combining synthetic seismograms from 3D finite‐difference simulations (≥1 s) with finite‐source stochastic synthetics (<1 s), produced by Frankel et al 15 The M9 simulations considered various rupture scenarios, hypocenter locations, and slip distributions and were found to match the BC Hydro GMM 35 well for locations outside of the deep basins. The modeling methodology was also found to sufficiently replicate recordings from the 2010 M8.8 Maule (Chile) earthquake 36 and the 2011 M9 Tohoku (Japan) earthquake 37 . The resulting synthetics highlight the considerable amplification of spectral accelerations, ranging from factors of 2 to 5, for periods of 1 to 10 s, for sites within the Seattle basin.…”
Section: Seismic Performance Assessment Methodologymentioning
confidence: 84%
“…The modeling methodology was also found to sufficiently replicate recordings from the 2010 M8.8 Maule (Chile) earthquake 36 and the 2011 M9 Tohoku (Japan) earthquake. 37 The resulting synthetics highlight the considerable amplification of spectral accelerations, ranging from factors of 2 to 5, for periods of 1 to 10 s, for sites within the Seattle basin. Marafi et al 12 showed that inside the basin the spectral accelerations of the simulated M9 CSZ ground motions at periods of 1.5 to 4 s were greater than the spectral accelerations of the ASCE 7-16 risk-targeted maximum considered earthquake (MCE R ), which has a return period of around 2000 years in Seattle.…”
Section: Seismic Hazard and Ground Motionsmentioning
confidence: 93%
“…The earthquake source was spatially distributed over the fault plane and temporally distributed over the duration of rupture [e.g., Frankel, 2013]. Strong body waves and surface waves thus arrived together from Geochemistry, Geophysics, Geosystems 10.1002/2015GC005832 the distributed sources over an extended interval at a given station.…”
Section: Suppression Of High-frequency S Waves By Low-frequency Raylementioning
confidence: 99%