1. Evaluation of the Huber Function
Performance in 1D Frequency-Domain Full
Waveform Inversion
Kamal Aghazade1, Navid Amini2
1Msc student, Institute of Geophysics, University of Tehran,
aghazade.kamal@ut.ac.ir
2Assistant professor, Institute of Geophysics, University of Tehran,
navidamini@ut.ac.ir
2. Presentation outline
Introduction Methodology Results Conclusion
Introduction Methodology Results Conclusions
β’FWI problem
β’Literature Review
β’ Huber Function
β’ FWI problems Based
on Huber Function
β’ implementation of The Huber
Function in 1-D Frequency-
Domain
β’ numerical tests
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3. β’ Full Waveform Inversion (FWI) is a data fitting
procedure which is used to obtain high resolution
quantitative models of the subsurface by
exploiting the full information content of the data
recorded by seismograms.
β’ FWI is an ill-posed and high nonlinear problem.
β’ The presence of errors (e.g. noise) in the data can
lead to undesirable results.
β’ The question is which data residual norm has a
good performance in FWI problem?
Introduction Methodology Results Conclusion
π2 β ππππ , π1 β ππππ , π»π¦ππππ
π1
π2
ππ π»π’πππ?
β’ Huber, 1973 : introduced a new Criteria
to incorporate l1 β norm for large
residuals and l2 β norm for small
residuals.
β’ (Guitton and Symes , 2003), used
Huber Function for linear inverse
problem for velocity analysis with both
synthetic and field
data.
β’ Bube and Nemeth, 2007, studied fast
line search method for Huber and
hybrid l1
l2
norms.
β’ Ha et al, 2009, studied Huber function
in Frequency Domain FWI.
β’ (Brossier et al, 2010), studied the
robustness of different data residual
norms in elastic-domain FWI.
Literature Review
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4. β’ in the presence of noise in data, π1_ππππ is more
robust than π2_ππππ.
β’ The main difficulty with π1_ππππ is itβs gradient
singularity when data residuals tends toward zero.
β’ Huber Function :
Combining the features of π1 πππ π2 norms in theory.
π1_ππππ for large residuals and π2_ππππ for small
residuals.
β’ the transition between two types of norms
controls by some threshold.
Introduction Methodology Results Conclusion
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5. FWI problem in frequency-domain by using
Huber Function ( synthetic data) :
β’ Employing 1D frequency domain Forward
modeling to generate synthetic data .
β’ extracting the gradient formulae for Huber
function in frequency- domain.
β’ optimization procedure.
Because π π_ππππ is always greater than π π_ππππ we
eq.1 can be replaced by :
The Gradient formulae :
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Introduction Methodology Results Conclusion
7. Numerical results for 2 velocity models:
Source : Ricker wavelet with dominant
frequency 25 Hz.
Receiver spacing : 5 m
Frequency range : 0 β 60 Hz
Employing ABC in frequency-domain for
eliminating undesirable reflections from
boundaries.
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Introduction Methodology Results Conclusion
8. Inversion results for velocity model 1 :
group 1 2 3 4 5 6 7 8 9
frequency 6.8Hz 11.4 Hz 16 Hz 20.6 Hz 25.2 Hz 34.4 Hz 39 Hz 48.2 Hz 52.8 Hz
0.3 ( )thr stdο½ r
Introduction Methodology Results Conclusion
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9. Introduction Methodology Results Conclusion
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0.4 ( )thr stdο½ r
Inversion results for velocity model 1 :
group 1 2 3 4 5 6 7 8 9
frequency 6.7Hz 12.6 Hz 24.4 Hz 30.3 Hz 42.1 Hz 53.9 Hz - - -
10. β’ in the presence of noise in data Huber function
based FWI in frequency-domain leads to
acceptable results.
β’ the main challenge with Huber function is itβs
threshold, need consideration for kinds of velocity
models.
β’ For the smooth velocity model (model 1) we can
not see the importance of the threshold, but for
smooth-blocky model(model 2) we can see the
balancing effect of Huber function.
Introduction Methodology Results Conclusion
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