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Azimuthal anisotropy layering in the Pacific upper mantle
DI21C-07 Azimuthal anisotropy layering in the Pacific upper mantle Huaiyu Yuan1,2,3 , Scott French4 and Barbara A. Romanowicz4,5,6 1 CCFS, EPS, Macquarie University, Australia 2 CET, University of Western Australia, Australia 3 Geological Survey of Western Australia, Australia 4 Berkeley Seismological Laboratory, UC Berkeley 5 Collège de France, Paris, France 6 Institut de Physique du Globe, Paris, France 1
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Lithosphere Layering and the LAB
Lithosphere-asthenosphere-boundary (LAB): one of “Grand Challenges” of modern seismology (Lay 2009) “Elusive” in continents due to smooth transition in seismic velocity (Eaton 2009; Romanowicz 2009; Fischer et al. 2010) Most extensively deformed “first-order structural discontinuity” (Eaton 2009) in the global tectonics due to strong plate-asthenosphere coupling Differential motion accommodated by rock deformation across/at the LAB
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APM: Absolute Plate Motion direction
Layering and the LAB Depth dependent azimuthal anisotropy Craton-wide layering in the upper mantle Domains of anisotropy possessing distinct fast axis directions Fast axis directions Fast axis directions Yuan and Romanowicz 2010 - APM APM: Absolute Plate Motion direction
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Lithosphere Layering and the LAB
Shallow depleted chemical layer (Layer 1; suture-strike parallel) Sub-thermal layer (Layer 2; high angle to APM) Asthenosphere (current APM parallel) Cooper and Conrad 2009 Yuan and Romanowicz 2010
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Lithosphere Layering and the LAB
Shallow depleted chemical layer (Layer 1; suture-strike parallel) Sub-thermal layer (Layer 2; high angle to APM) Asthenosphere (current APM parallel) Anisotropic LAB ( km under NA craton) LAB Depth Yuan and Romanowicz 2010
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The Oceanic LAB Oceanic lithosphere covers much larger surface area than continents Short life span: e.g., Pacific < 200Ma compared with >3Ga of continents Simple tectonic history; perturbed by input of deep seated thermal upwellings (e.g., French 2013).
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Poster: DI21A-2267 this afternoon
The Oceanic LAB Simple tectonic history; perturbed by input of deep seated thermal upwellings (e.g., French 2013). See French 2013 for details Poster: DI21A-2267 this afternoon Talk S21E-07 now
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The Oceanic LAB Thickness of oceanic lithosphere dictated by thermal history Follows 1 half-space cooling model; 2 plate model; 3 or not (Rychert et al. 2013; Schmerr 2012) Thickness in the range ~ 100 km in the oldest (Schmerr 2012) Paleo-APM at shallow and current APM at depth picked up by azimuthal anisotropy (Montagner 2002; Smith et al. 2004; Debayle et al. 2005; Maggi et al. 2006; Debayle and Ricard 2013)
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The Objectives Can we define a Pacific-wide LAB?
Oceanic upper mantle layering and its tectonic implications.
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Pacific Inversion Full waveform inversion using 2D finite-sensitivity kernels (NACT; Li and Romanowicz 1995) Based on an earlier (2007) Berkeley global model that honors true oceanic Moho (Crust2.0); Modified linear crustal correction (Lekic and Romanowicz 2009) applied; 5° lateral model spacing; km vertical spacing B-splines down to 300 km, then down to 1000 km. Isotropic Vs and radial anisotropy ξ; then azimuthal anisotropy strength (G) and fast axis directions
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Pacific Inversion 60-s global fundamental and overtone waveforms (French et al. 2013); 60- and 40-s Pacific regional network data; OBS waveforms Overall 1.3 million paths; or ~25 million waveform points handled by NACT for forward and inverse problems Model error handled by bootstrap resampling (Efron and Tibshitani 1986): standard deviation of the 100 “new” models No SKS dataset due to the sparse coverage
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Anisotropy map views Layered North America confirmed; although weak but AMP-parallel in the asthenosphere Depth dependent anisotropy domains also found in the Pacific Modified linear crustal correction (Lekic and Romanowicz 2009) applied; Full waveform inversion using 2D finite-sensitivity kernels (NACT; Li and Romanowicz 1995) 5° lateral model spacing ; km vertical spacing B-splines down to 300 km, then down to 1000 km. Isotropic Vs and radial anisotropy ξ; then azimuthal anisotropy strength (G) and fast axis Lithosphere depth Asthenosphere depth Below Asthenosphere
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Depth cross-section Isotropic Vs Radial Anisotropy Azimuthal
Strength (%) Fast-axis direction
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Resolution Tests Azimuthal Anisotropy Strength (%) Fast-axis Input
direction Input Azimuthal Anisotropy Strength (%) Fast-axis direction Output
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Age Profiles: Vs and LAB
Plate-model like Punctuated between Ma Radial Anisotropy Ritzwoller et al Vs Profile Isotropic Vs Age Profile Priestley & McKenzie 2006 Vs Profile
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Age Profiles: Vs and LAB
Defined by maximum Vs depth gradient Seismic LAB: km depth range Consistent with S-receiver functions and SS-precursor studies LAB from negative Vs gradient
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Age Profiles: Azimuthal Anisotropy
Current APM direction > km High angle to the APM at shallow depth Two domains of anisotropy Paleo-plate motion Fast axis directions with APM removed Current Plate Motion Azimuthal anisotropy Strength (%)
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Age Profiles: Azimuthal Anisotropy
Oceanic lithosphere LAB: km Defined by azimuthal anisotropy LAB from Azimuthal anisotorpy
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Azimuthal anisotropy LAB
Two LAB horizons Shallower Vs LAB Deeper anisotropy LAB Velocity LAB Azimuthal anisotropy LAB
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LAB Age Profiles Shallower Vs LAB Deeper Anisotropy LAB LAB from Vs
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Chemical oceanic layer?
Resembles the continent layer model LAB from Vs Cooper and Conrad 2009 LAB from anisotropy
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Depleted chemical oceanic layer?
Depleted Layer in the oceanic lithosphere (Hirth & Kohlstedt 1996; Lee et al. 2005); thickness dependent on ambient mantle temperature Growth of thermal sub-layer when thermal effect out-weights chemical effect LAB from Vs LAB from anisotropy Lee et al. 2005
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Green area: Large Igneous Provinces (LIPs) Azimuthal anisotropy LAB
Role of LIPs Correlation of deep Anisotropic LAB with Large Igneous Provinces? Green area: Large Igneous Provinces (LIPs) Velocity LAB Azimuthal anisotropy LAB
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Conclusions Layered oceanic upper mantle
Uniform fossil lithosphere structure APM parallel asthenosphere Vs LAB shallower than anisotropy LAB Chemical depleted oceanic layer
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Age Profiles and Error Estimates
Based on an early Berkeley global model that honors true oceanic Moho (Crust2.0); Modified linear crustal correction (Lekic and Romanowicz 2009) applied; Full waveform inversion using 2D finite-sensitivity kernels (NACT; Li and Romanowicz 1995) 5° lateral model spacing ; km vertical spacing B-splines down to 300 km, then down to 1000 km. Isotropic Vs and radial anisotropy ξ; then azimuthal anisotropy strength (G) and fast axis
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Pacific Inversion Model error handled by bootstrap resampling (Efron and Tibshitani 1986): standard deviation of the 100 “new” models 60-s global fundamental and overtone waveforms (French et al. 2013) and 60- and 40-s Pacific regional network data Overall 1.3 million paths (~30 million waveform points) handled by NACT forward and inversion Good azimuthal coverage for Pacific
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Age Profiles: Vs & ζ Model points sorted by age and averaged for model parameters Isotropic Vs Radial Anisotropy
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Age Profiles: Azimuthal Anisotropy
Model points sorted by age and averaged for model parameters Isotropic Vs Radial Anisotropy
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Resolution Tests Model error handled by bootstrap resampling (Efron and Tibshitani 1986): standard deviation of the 100 “new” models 60-s global fundamental and overtone waveforms (French et al. 2013) and 60- and 40-s Pacific regional network data Overall 1.3 million paths (~30 million waveform points) handled by NACT forward and inversion Good azimuthal coverage for Pacific
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Resolution Tests Model error handled by bootstrap resampling (Efron and Tibshitani 1986): standard deviation of the 100 “new” models 60-s global fundamental and overtone waveforms (French et al. 2013) and 60- and 40-s Pacific regional network data Overall 1.3 million paths (~30 million waveform points) handled by NACT forward and inversion Good azimuthal coverage for Pacific
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