Seismic tomography: Art or science?

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Transcription:

Seismic tomography: Art or science? Frederik J Simons Princeton University What s inside the Earth? www.usgs.gov www.glencoe.com Dalton, Nature 2003 Only seismic waves have actually been there, done that This looks more complicated than it is; and that s my point. 1

This looks simpler than it is; and that s my point. X-Ray attenuation tomography Projections from all angles: X-ray intensity Reconstructed image: X-ray attenuation constants 2

Seismic wavespeed tomography Projections from all angles: Waveforms and arrival times Reconstructed image: Wavespeed variations Forward modeling of the wave field, Part I: Ray tracing, most 1-D Before Kennett, GJI, 1995 Bullen & Bolt, 1985 After Buland, BSSA, 1983 Forward modeling of the wave field, Part II: Normal-mode summation, 1-D Before After Dahlen & Tromp, 1998 Simons, Lithos, 1999 3

Forward modeling of the wave field, Part III: Spectral-element methods, 3-D Before Komatitsch, GJI, 2002 After Non-continuous source coverage The CMT catalog of large events 4

Source location (in)extricably linked Before After Source relocation is big business. Schaff, JGR, 2002 Fermat s Principle at Work for you Zhao, PEPI, 2004 5

The reference Earth: Radial models and at least some of it is true Karki et al., Rev. Geoph., 2001 Jackson, 1998 6

Menke, 1989 Receiver coverage Picking the right continent A dense path coverage minimizes the amount of a priori information needed Simons, GJI 2002 7

Regularization: the Mathematics Regularization: the Physics Such fat rays sample more of the Earth and thus we need fewer of them to have a well-constrained tomographic problem. Dahlen, GJI, 2002 Regularization: the Art Too much? Too smooth? Too little? Too rough? Simons, Lithos, 1999 8

How to interpret seismic models Pillet, PEPI, 1999 Demand to see the ray paths Pillet, PEPI, 1999 Nature isn t always kind Shen, Nature, 1998 Wolfe, Nature, 1997 9

Seismic anisotropy Wave speeds depend on propagation direction and polarization: No surprise: elasticity maps stress and strain, and both depend on three directions Polarization anisotropy The particles of Love and Raleigh surface waves move in orthogonal directions SH and SV body waves sometimes exhibit clear splitting Azimuthal anisotropy It s usually very hard to separate whether the time difference arises from an anisotropic direction or an isotropic wave speed difference (aka heterogeneity) Why is this so hard? It s very hard to tell whether a phase comes in early because it went through a fast patch or because it came in a fast direction heterogeneity and anisotropy trade off. 10

Questions to ask of the tomographer How is the forward model computed? What is the ray coverage? What (sort of) damping did you use? What does velocity estimation trade off with? What is the grid size / the correlation length? How are different data sets weighted? How far is the final from the starting model? Does the starting model have discontinuities? How is the surface/depth parameterization Is your sensitivity 1-D, 2-D,or 3-D? Journey to Middle Earth, Part I: The continental lithosphere Simons, GRL, 2002 Gung, Nature, 2003 Journey to Middle Earth, Part II: Subduction zones Replumaz, EPSL, 2004 11

Journey to Middle Earth, Part III: Deep mantle plumes Montelli, Science, 2004 What does it all mean? Part I: Temperature anomalies 110 km Goes, JGR, 2002 What does it all mean? Part II: Compositional anomalies Fe/(Fe + Mg) T 150 km Perry, GJI, 2003 12

What does it all mean? Part III: Deformation in the mantle Fossil Contemporaneous Simons, EPSL, 2003 Conclusions Ultimately, seismology can only tell us where, or in which direction, wave propagation is faster or slower than a reference model The non-seismologist has to know the basics of inverse problem modeling, understand the sometimes poor constraints, and be critical Improvements are being made: better data, better forward models, better inversions As much as with the a posteriori interpretation, the community needs to help defining a priori acceptable starting models 13

More equations, for completeness 14

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