Large Trench-Parallel Gravity Variations Predict Seismogenic Behavior in Subduction Zones

We demonstrate that great earthquakes occur predominantly in regions with a strongly negative trench-parallel gravity anomaly (TPGA), whereas regions with strongly positive TPGA are relatively aseismic. These observations suggest that, over time scales up to at least 1 million years, spatial variations of seismogenic behavior within a given subduction zone are stationary and linked to the geological structure of the fore-arc. The correlations we observe are consistent with a model in which spatial variations in frictional properties on the plate interface control trench-parellel variations in fore-arc topography, gravity, and seismogenic behavior.

[1]  Paul A. Rosen,et al.  Co-seismic slip from the 1995 July 30 Mw= 8.1 Antofagasta, Chile, earthquake as constrained by InSAR and GPS observations , 2002 .

[2]  Walter H. F. Smith,et al.  Marine gravity anomaly from Geosat and ERS 1 satellite altimetry , 1997 .

[3]  M. Gurnis,et al.  Viscous flow model of a subduction zone with a faulted lithosphere: Long and short wavelength topography, gravity and geoid , 1992 .

[4]  S. Buiter,et al.  A modelling study of vertical surface displacements at convergent plate margins , 2001 .

[5]  S. Beck,et al.  Rupture process of the February 4, 1965, Rat Islands Earthquake , 1991 .

[6]  Olafur Gudmundsson,et al.  A regionalized upper mantle (RUM) seismic model , 1998 .

[7]  K. Satake,et al.  Asperity Distribution of the 1952 Great Kamchatka Earthquake and its Relation to Future Earthquake Potential in Kamchatka , 1999 .

[8]  H. Kanamori Rupture Process of Subduction-Zone Earthquakes , 1986 .

[9]  Magali I. Billen,et al.  A low viscosity wedge in subduction zones , 2001 .

[10]  G. Bebout Subduction top to bottom , 1996 .

[11]  E. Engdahl,et al.  Global teleseismic earthquake relocation with improved travel times and procedures for depth determination , 1998, Bulletin of the Seismological Society of America.

[12]  Richard G. Gordon,et al.  Effect of recent revisions to the geomagnetic reversal time scale on estimates of current plate motions , 1994 .

[13]  S. Wdowinski Dynamically supported trench topography , 1992 .

[14]  K. Satake,et al.  Coseismic slip distribution of the 1946 Nankai earthquake and aseismic slips caused by the earthquake , 2001 .

[15]  Stuart P. Nishenko,et al.  Circum-Pacific seismic potential: 1989–1999 , 1991 .

[16]  John H. Woodhouse,et al.  Determination of earthquake source parameters from waveform data for studies of global and regional seismicity , 1981 .

[17]  Yan Y. Kagan,et al.  New seismic gap hypothesis: Five years after , 1995 .

[18]  C. Scholz,et al.  On the mechanism of seismic decoupling and back arc spreading at subduction zones , 1995 .

[19]  J. Kelleher,et al.  Buoyant zones, great earthquakes, and unstable boundaries of subduction , 1976 .

[20]  High interseismic coupling of the Alaska Subduction Zone SW of Kodiak Island inferred from GPS data , 2001 .

[21]  H. Kanamori,et al.  The rupture process and asperity distribution of three great earthquakes from long-period diffracted P-waves , 1983 .

[22]  H. Kanamori,et al.  Back-arc opening and the mode of subduction , 1979 .

[23]  Strain accumulation in the Shumagin Islands: Results of initial GPS measurements , 1994 .

[24]  C. Marone LABORATORY-DERIVED FRICTION LAWS AND THEIR APPLICATION TO SEISMIC FAULTING , 1998 .

[25]  J. Freymueller,et al.  Absence of strain accumulation in the Western Shumagin Segment of the Alaska Subduction Zone , 1999 .

[26]  J. Chéry,et al.  Quantification of interplate coupling in subduction zones and forearc topography , 1997 .

[27]  Steven N. Ward,et al.  The 1960 Chile earthquake: inversion for slip distribution from surface deformation , 1990 .

[28]  Shijie Zhong,et al.  Controls on trench topography from dynamic models of subducted slabs , 1994 .