Rupture Process During the 2015 Illapel, Chile Earthquake: Zigzag-Along-Dip Rupture Episodes

We constructed a seismic source model for the 2015 MW 8.3 Illapel, Chile earthquake, which was carried out with the kinematic waveform inversion method adopting a novel inversion formulation that takes into account the uncertainty in the Green’s function, together with the hybrid backprojection method enabling us to track the spatiotemporal distribution of high-frequency (0.3–2.0 Hz) sources at high resolution by using globally observed teleseismic P-waveforms. A maximum slip amounted to 10.4 m in the shallow part of the seismic source region centered 72 km northwest of the epicenter and generated a following tsunami inundated along the coast. In a gross sense, the rupture front propagated almost unilaterally to northward from the hypocenter at <2 km/s, however, in detail the spatiotemporal slip distribution also showed a complex rupture propagation pattern: two up-dip rupture propagation episodes, and a secondary rupture episode may have been triggered by the strong high-frequency radiation event at the down-dip edge of the seismic source region. High-frequency sources tends to be distributed at deeper parts of the slip area, a pattern also documented in other subduction zone megathrust earthquakes that may reflect the heterogeneous distribution of fracture energy or stress drop along the fault. The weak excitation of high-frequency radiation at the termination of rupture may represent the gradual deceleration of rupture velocity at the transition zone of frictional property or stress state between the megathrust rupture zone and the swarm area.

[1]  H. Kopp,et al.  Seismic structure of the north‐central Chilean convergent margin: Subduction erosion of a paleomagmatic arc , 2014 .

[2]  Thomas H. Heaton,et al.  Inversion of strong ground motion and teleseismic waveform data for the fault rupture history of the 1979 Imperial Valley, California, earthquake , 1983 .

[3]  C. Amante,et al.  ETOPO1 arc-minute global relief model : procedures, data sources and analysis , 2009 .

[4]  M. Brudzinski,et al.  Megathrust earthquake swarms indicate frictional changes which delimit large earthquake ruptures , 2014 .

[5]  M. Moreno,et al.  2010 Maule earthquake slip correlates with pre-seismic locking of Andean subduction zone , 2010, Nature.

[6]  H. Tu The Cohesive Zone Model , 2018 .

[7]  G. Masters,et al.  Update on CRUST1.0 - A 1-degree Global Model of Earth's Crust , 2013 .

[8]  Peter M. Shearer,et al.  Detailed rupture imaging of the 25 April 2015 Nepal earthquake using teleseismic P waves , 2015 .

[9]  A. Echaurren,et al.  Anatomy of the Andean subduction zone: three-dimensional density model upgraded and compared against global-scale models , 2012 .

[10]  Ryo Okuwaki,et al.  Rupture process of the 2014 Iquique Chile Earthquake in relation with the foreshock activity , 2014 .

[11]  R. Madariaga,et al.  Intense foreshocks and a slow slip event preceded the 2014 Iquique Mw 8.1 earthquake , 2014, Science.

[12]  Yuji Yagi,et al.  Introduction of uncertainty of Green's function into waveform inversion for seismic source processes , 2011 .

[13]  Y. Yagi,et al.  Smooth and rapid slip near the Japan Trench during the 2011 Tohoku-oki earthquake revealed by a hybrid back-projection method , 2012 .

[14]  Allen H. Olson,et al.  Finite faults and inverse theory with applications to the 1979 Imperial Valley earthquake , 1982 .

[15]  R. Madariaga,et al.  Evidence for earthquake interaction in central Chile: the July 1997–September 1998 Sequence , 2001 .

[16]  E. R. Engdahl,et al.  Constraints on seismic velocities in the Earth from traveltimes , 1995 .

[17]  Teruo Yamashita,et al.  A cohesive zone model for dynamic shear faulting based on experimentally inferred constitutive relation and strong motion source parameters , 1989 .

[18]  Igor A. Beresnev,et al.  Uncertainties in Finite-Fault Slip Inversions: To What Extent to Believe? (A Critical Review) , 2003 .

[19]  Masayuki Kikuchi,et al.  Inversion of complex body waves , 1982 .

[20]  Raul Madariaga,et al.  High-frequency radiation from crack (stress drop) models of earthquake faulting , 1977 .

[21]  Y. Yagi,et al.  Integrated seismic source model of the 2015 Gorkha, Nepal, earthquake , 2015 .

[22]  E. R. Engdahl,et al.  41 - Global Seismicity: 1900–1999 , 2002 .

[23]  R. Madariaga,et al.  The Large Chilean Historical Earthquakes of 1647, 1657, 1730, and 1751 from Contemporary Documents , 2012 .

[24]  P. Shearer,et al.  Rupture details of the 28 March 2005 Sumatra Mw 8.6 earthquake imaged with teleseismic P waves , 2005 .

[25]  GPS-derived interseismic coupling on the subduction and seismic hazards in the Atacama region, Chile , 2014 .

[26]  Nadia Lapusta,et al.  Towards inferring earthquake patterns from geodetic observations of interseismic coupling , 2010 .

[27]  Hiroo Kanamori,et al.  Depth‐varying rupture properties of subduction zone megathrust faults , 2011 .

[28]  R. Madariaga,et al.  Modeling of stress transfer in the Coquimbo region of central Chile , 2006 .

[29]  S. Beck,et al.  Source characteristics of historic earthquakes along the central Chile subduction Askew et alzone , 1998 .

[30]  Y. Yagi,et al.  Relationship between High-frequency Radiation and Asperity Ruptures, Revealed by Hybrid Back-projection with a Non-planar Fault Model , 2014, Scientific Reports.

[31]  Peter M. Shearer,et al.  Extent, duration and speed of the 2004 Sumatra–Andaman earthquake imaged by the Hi-Net array , 2005, Nature.

[32]  Masayuki Kikuchi,et al.  Inversion of complex body waves—III , 1991, Bulletin of the Seismological Society of America.

[33]  R. Madariaga,et al.  Rupture dynamics of a planar fault in a 3D elastic medium: Rate- and slip-weakening friction , 1998, Bulletin of the Seismological Society of America.

[34]  K. Koper,et al.  Along‐dip variation of teleseismic short‐period radiation from the 11 March 2011 Tohoku earthquake (Mw 9.0) , 2011 .

[35]  Rubén Boroschek,et al.  The October 15, 1997 Punitaqui earthquake (Mw=7.1): a destructive event within the subducting Nazca plate in central Chile , 2002 .

[36]  L. Neil Frazer,et al.  Use of ray theory to calculate high-frequency radiation from earthquake sources having spatially variable rupture velocity and stress drop , 1984 .

[37]  Ryo Okuwaki,et al.  The 16 September 2015 Chile Tsunami from the Post-Tsunami Survey and Numerical Modeling Perspectives , 2016, Pure and Applied Geophysics.

[38]  Richard G. Gordon,et al.  Geologically current plate motions , 2010 .

[39]  D. Melgar,et al.  Slip segmentation and slow rupture to the trench during the 2015, Mw 8.3 Illapel, Chile earthquake: SLIP DURING THE Mw 8.3 ILLAPEL EARTHQUAKE , 2016 .

[40]  David J. Wald,et al.  Slab1.0: A three‐dimensional model of global subduction zone geometries , 2012 .

[41]  The Fracture Energy of Earthquakes , 1975 .

[42]  Walter H. F. Smith,et al.  New, improved version of generic mapping tools released , 1998 .

[43]  Cinna Lomnitz,et al.  Major Earthquakes of Chile: A Historical Survey, 1535-1960 , 2004 .

[44]  Hirotugu Akaike,et al.  Likelihood and the Bayes procedure , 1980 .

[45]  Matthias Ohrnberger,et al.  Tracking the rupture of the Mw = 9.3 Sumatra earthquake over 1,150 km at teleseismic distance , 2005, Nature.

[46]  Hiroo Kanamori,et al.  Rapidly Estimated Seismic Source Parameters for the 16 September 2015 Illapel, Chile Mw 8.3 Earthquake , 2016, Pure and Applied Geophysics.

[47]  P. Bernard,et al.  A new asymptotic method for the modeling of near-field accelerograms , 1984 .