teleseismic surface wave tomography

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From data to model: how should we handle uncertainties in a chain mixing model and data uncertainty? Helle A. Pedersen and Gwenaelle Salaun ISTERRE, University of Grenoble and CNRS Presentation based mainly on results from the Simbaad experiment: A. Paul, H. Karabulut, D. Hatzfeld, C. Papazachos, D. M. Childs, C. Pequegnat and Simbaad Team as well as close collaboration with: V. Farra, M. Bruneton, S. Fishwick, D. Snyder, and others 1

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Page 1: Teleseismic  surface wave tomography

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From data to model: how should we handle uncertainties in a chain mixing model and data

uncertainty?

Helle A. Pedersen and Gwenaelle SalaunISTERRE, University of Grenoble and CNRS

Presentation based mainly on results from the Simbaad experiment: A. Paul, H. Karabulut, D. Hatzfeld, C. Papazachos, D. M.

Childs, C. Pequegnat and Simbaad Teamas well as close collaboration with:

V. Farra, M. Bruneton, S. Fishwick, D. Snyder, and others

Page 2: Teleseismic  surface wave tomography

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Teleseismic surface wave tomography• Give me an array of stations

• Give me recordings of distant seismic events

• I will give you the (=some) model of Vs(x,y,z)

• Can I give you a sensible estimate of the error on Vs(x,y,z)?

Page 3: Teleseismic  surface wave tomography

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What we do• Preprocessing

• At each frequency:• Measure time delays between pairs of stations• Invert for phase velocity maps C(x,y)

• Assemble phase velocities to obtain C(x,y,period)

• For each grid point, invert for Vs(z)

• Assemble shear wave profiles to obtain Vs(x,y,z)

Page 4: Teleseismic  surface wave tomography

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Teleseismic surface wave tomography – different types of difficulties

1) Input data : data quantity and uncertainty

2) Out of array propagation : simplistic models of the incoming waves

3) Propagation effects inside the array: simplistic theory

4) Phase velocity uncertainty: resolution issue

5) Depth inversions uncertainty: resolution issue

Page 5: Teleseismic  surface wave tomography

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Data quality

Data heterogeneity is the norm rather than the exception

Page 6: Teleseismic  surface wave tomography

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Data quality

Data heterogeneity is the norm rather than the exception

Page 7: Teleseismic  surface wave tomography

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Data quality

1) Input data : data quantity and uncertainty – what can we reasonably do

• Available events : long recording period (2 years)

• Signal to noise ratio of signals : strict quality control and rejection of faulty signals …but choices remain subjective

• Systematic errors (glitches, mass centerings, …): we pick up automatically as much as possible, but not all is visible after preprocessing

• Timing errors : regular checks on P-wave arrivals (but what about small and/or random errors?).

• Errors in metadata (instrument response) : big effort => OK phases, amplitudes within ±30% (!)

A thorough (but is it satisfying?) analysis of remaining time delay errors

Page 8: Teleseismic  surface wave tomography

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Data quality

Question:

Can we assume that the remaining data errors follow a normal distribution?

Page 9: Teleseismic  surface wave tomography

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Out of array propagation : great-circle deviation

Maupin, GJI 2011

• Major deterministic diffractions : systematic effects• Multiple diffraction and coda• Presence of higher modes (and body waves)• Great-circle deviation• Finite frequency effects

Page 10: Teleseismic  surface wave tomography

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Out of array propagation : great-circle deviation

Maupin, GJI 2011

50s 25s

Page 11: Teleseismic  surface wave tomography

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Out of array propagation : finite frequency effects

Zhou, Dahlen and Nolet, GJI 2004 (Born)

100s Love wave, phase and arrival angle kernels 100s Rayleigh wave, phase kernel

Page 12: Teleseismic  surface wave tomography

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Chevrot and Zhao, GJI 2007

100s & 150km depth

Out of array propagation : finite frequency effects

Page 13: Teleseismic  surface wave tomography

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Out of array effects

Actions:- Carry out frequency-time filtering - Allow for great circle deviation- Allow for non plane wavefronts

Bruneton et al., GJI, 2002

Question:

Can we create a model of the errors associated with our approximations on wave propagation?

Is it enough to have sensible ‘garbage parameters’ to avoid to project out of array effects into the model?

Page 14: Teleseismic  surface wave tomography

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Snieder, GJRaS, 1986

Scattering by a mountain root Phase velocity at T=50s observed across a circular heterogeneity of 40 km diameter

Bodin and Maupin, GJI, 2008

Inside array propagation : possible to extract useful information from fundamental mode Rayleigh waves using strong approximations

(no scattering, no finite frequency effects)

R->R

R->L

L->L

Page 15: Teleseismic  surface wave tomography

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Phase velocity maps and uncertainty

Page 16: Teleseismic  surface wave tomography

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Without oceanic slab

With oceanic slab

Phase velocity maps and uncertainty: data distribution

Example from teleseismic P wave tomography

But we are fine – aren’t we?

Page 17: Teleseismic  surface wave tomography

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Phase velocity uncertainty: data distribution

With back azimuth weighting

Without back azimuth weighting

Input

Page 18: Teleseismic  surface wave tomography

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Phase velocity uncertainty: a posteriori error maps (of last inversion step)

Page 19: Teleseismic  surface wave tomography

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Questions:

1) Simple, objective tools for regularisation?

2) How can we develop tools to better assess the impact of input data weighting?

Phase velocity uncertainty

Page 20: Teleseismic  surface wave tomography

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Vs(z) uncertainty

- Smooth over depth (correlation length)

- Importance of interfaces

Page 21: Teleseismic  surface wave tomography

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Vs(x,y,z) uncertainty

Questions: 1) Laterally varying depth smoothing? On which criteria?2) Usual resolution issues

Page 22: Teleseismic  surface wave tomography

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Putting the pieces together again

Data processing and delay measurementsEstimate of measurement error (Gaussian?)

Iterative inversion for phase velocity mapsResolution : managed, but partly unsatisfactory trade-off between spatial resolution and parameter resolution

Iterative inversion for Vs(z)Resolution: managed, but partly unsatisfactory trade-off between spatial resolution and parameter resolution

Ignored out of array effects

Ignored inside array effects

?

Page 23: Teleseismic  surface wave tomography

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Going back to where we started• Give me an array of stations• Give me recordings of distant seismic events• I will give you the (=some) model of Vs(x,y,z)• It is possible to give you some estimate of the error on Vs(x,y,z)

BUT• All this careful work boils down to: which features of the model are resolved –

and our tools for error analysis may not be adequate• Many open issues, forcing us to make conservative choices at each step, thereby

reducing vertical and lateral resolution

• What we need is the uncertainty estimate on parameters of our interpretation, not the uncertainty on the parameters themselves• We therefore have got a strong communication problem of error issues towards

the end-users (geology/tectonics)

Page 24: Teleseismic  surface wave tomography

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What do end users do to the output models?

Dipping slab beneith Anatolia (?)

Top of slab geometry

Page 25: Teleseismic  surface wave tomography

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What I would like to learn?

What I am expecting from uncertainty analysis:• Estimate of the probability function of parameters relating to the interpretation• Tools for others to estimate the probability function of their interpretation• Tools to decide how to decrease uncertainties : where will an effort (data,

physics, inversion) be the most efficient?

Can statistical analysis alone solve these issues?• Can we create a library synthetic seismograms for different test structures and

array geometries?• Such a library must make us able to use different analysis techniques• Which hypothesis can we sensibly test?• How can such a library be hypothesis driven (?)• How can we create models of data uncertainty?