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Global upper mantle azimuthal anisotropy and the peculiar behavior of the Australian plate

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Title: Global upper mantle azimuthal anisotropy and the peculiar behavior of the Australian plate


1
Global upper mantle azimuthal anisotropy and the
peculiar behavior of the Australian plate
  • Eric Debayle1, Brian Kennett 2 and Keith
    Priestley3
  • 1 Ecole et Observatoire des Sciences de la
    Terre, CNRS and Université Louis Pasteur,
    Strasbourg
  • 2 Research School of Earth Sciences, The
    Australian National University, Canberra,
    Australia.
  • 2 Bullard Laboratories, University of Cambridge,
    Cambridge, United Kingdom.
  • This work is subject to press embargo

2
Our global SV-wave heterogeneities azimuthal
anisotropy model
  • 100779 Rayleigh waveforms (fundamental plus 4
    higher modes) matched between 50 s and 160 s.
  • Short paths (1200-6000 km)
  • improve the lateral resolution ( 800 km -1500
    km)

Number of paths
Paths length (km)
3
100 km Vs ref 4.41 km/s
200 km Vs ref 4.44 km/s
4
Depth-distribution of azimuthal anisotropy
5
Synthetic experiment
Input model
6
Azimuthal distribution of rays
Optimized Voronoi diagram (Debayle and
Sambridge, JGR 2004) each geographical point
belongs to the smallest cell for which the
azimuthal variation of Sv waves can be resolved.
7
Correlation between fast anisotropic direction
and absolute plate motion
good correlation
bad correlation
FastSVAPMcos(2f)
8
Averaged correlation between fast anisotropic
direction and absolute plate motion
9
Debayke, Kennett and Prietsley (Nature, 2005)
Australia
Other continents
(VSH/VSV)2
SKS
SKS
(VSH/VSV)2
1.1
1
0
gt1
1
crust
crust
Moho
Moho
50
Frozen in anisotropy (east-west)
Frozen in anisotropy
?
Debayle and Kennett (EPSL 2000) Gaherty and
Jordan (Science 1995)
100
150
MBL
MBL
Plate-motion azimuthal anisotropy (north-south)
Weak or null azimuthal anisotropy
200
HVL
HVL
250
Depth (km)
HVL Base of the High Velocity Lid MBL
Mechanical Boundary Layer
10
Conclusions
  • The fast-moving Australian plate would contain
    the only continental region with a sufficiently
    large deformation at its base to be transformed
    into azimuthal anisotropy.
  • For continents other than Australia, weak
    influence of basal drag on the lithosphere may
    explain why azimuthal anisotropy is observed only
    in a layer located in the uppermost 100 km of the
    mantle. This layer shows a complex organisation
    of azimuthal anisotropy suggesting a frozen in
    origin of deformation, compatible with SKS
    observations.
  • NB we have performed various tests on our model
    that will be available on line on the Nature
    website in early 2005 as supplementary
    information on the paper.

11
Effect of the non-inverted 4q azimuthal terms
a) C0 2q terms inversion (only 2q terms shown)
b) C0 2q 4q terms inversion (only C0 and 2q
shown)
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