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Slab deformation and seismicity Thorsten W. Becker Lisa A. Alpert Iain W. Bailey Melanie Gerault Meghan S. Miller University of Southern California Los Angeles EGU meeting, Vienna April 26, 2012
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Harvard gCMT catalog, Engdahl et al. hypocenters, and P-wave tomography (Li et al. 2008) Objective: Use global subduction zoo to infer mantle dynamics (e.g. slab strength)
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cf. Isacks & Molnar (1969); Chen et al. (2004) Bailey et al. (2012) We use the Harvard/Lamont GCMT catalog up to 2010 down slab along slab Global CMT analysis depth All CMTs are rotated into a slab-local coordinate system based on Benioff seismicity contours New coordinate system shows CMTs looking at slab from side Compressional-Oblique-Extensional Largest earthquake in depth bin strain in down-dip direction, f
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Bailey et al. (2012) Global CMT analysis Kostrov- summed moment tensors Compressional-Oblique-Extensional Largest earthquake in depth bin Kostrov summation normalized summation strain in down-dip direction, f
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down dip angle Bailey et al. (2012) P axis T axis Non-double couple components: Compensated Linear Vector Dipole (CLVD, ) Extensional – Oblique - Compressional Extensional Compressional pure double couple strain in down-dip direction, f
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Kuge and Kawakatsu (1993); Bailey et al. (2012) P axis T axis Extensional, shallow Compressional, deep Trends in actual CMTs
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Alisic et al. (2010) Alpert et al. (2010)cf. Vassiliou & Hager (1988) Global geodynamic models
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8/18 Circulation modeling Incompressible, laminar (Stokes) flow Boundary conditions: weak zones with plate motions driven by density anomalies, or prescribed plate motions Layered viscosity structure, with lateral viscosity variations, Newtonian Density anomalies assigned to Wadati-Benioff zones for slabs Solve with MILAMIN (Dabrowski et al., 2008) or CitcomS (Zhong et al., 2000), with modifications as in Becker & Faccenna (2011) and Gerault et al. (2012) Resolution ~5 – 20 km (global 3D), 1 km (cylindrical) (Alpert et al., 2010; Gerault et al., 2012)
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Effect of lower mantle viscosity on in slab stress orientations η slab /η mantle = 100 Alpert et al. (2010) P axes: blue = model predictions, green = at centroid, red = data lm / um = 1
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Effect of lower mantle viscosity on in slab stress orientations η slab /η mantle = 100 Lower mantle viscosity increase is required to generate significant compression Alpert et al. (2010) P axes: blue = model predictions, green = at centroid, red = data lm / um = 1 lm / um = 100 cf. Vassiliou & Hager (1988)
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Alpert et al. (2010) Regional misfits of depth averaged P/T axes for different rheologies Moderately strong (viscosity <~ 100 upper mantle) slabs preferred, lower mantle viscosity increase required
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Bailey et al. (2012) Regional CMT summation cf. Isacks & Molnar (1969); Chen et al. (2004) Compressional-Oblique-Extensional strain in down-dip direction, f
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Compressional-Oblique-Extensional Alpert et al. (2010); Bailey et al. (2012) Geodynamic modeling results strain in down-dip direction, f
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Geodynamic model predictions Compressional-Oblique-Extensional strain in down-dip direction, f Regional selection of intermediate depth extension- deep compression type subduction Box size scales with number of CMTs in summation Bailey et al. (2012)
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CLVD component Compressional-Oblique-Extensional Model predictions for stress state and CLVD component strain in down-dip direction, f
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Bailey et al. (2012) Intermediate depth extension- deep compression slabs Model predictions Model misfit
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Bailey et al. (2012) Intermediate depth compression- deep compression slabs Model predictions Model misfit
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Conclusions Global circulation models provide good (“reference”?) fit to deep, co-seismic slab deformation style world wide (Newtonian, isotropic flow works) Moderately strong slabs (viscosity ~100 upper mantle) and ~50 viscosity increase in lower mantle preferred Non double couple (CLVD) components of CMTs, and dependency of CLVD style on major stress axis, are newly predicted by fluid models
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