2013
DOI: 10.1190/geo2013-0004.1
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Wave-equation reflection traveltime inversion with dynamic warping and full-waveform inversion

Abstract: In reflection seismology, full-waveform inversion (FWI) can generate high-wavenumber subsurface velocity models but often suffers from an objective function with local minima caused mainly by the absence of low frequencies in seismograms. These local minima cause cycle skipping when the low-wavenumber component in the initial velocity model for FWI is far from the true model. To avoid cycle skipping, we discovered a new wave-equation reflection traveltime inversion (WERTI) to update the low-wavenumber componen… Show more

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Cited by 254 publications
(114 citation statements)
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“…Similar to Ma and Hale (2013), we can calculate the gradient of the objective function 13 with respect to v and w as follows:…”
Section: Appendix B Gradient Calculationmentioning
confidence: 99%
“…Similar to Ma and Hale (2013), we can calculate the gradient of the objective function 13 with respect to v and w as follows:…”
Section: Appendix B Gradient Calculationmentioning
confidence: 99%
“…However, with reflection geometries, FWI fails to invert for volumetric changes in velocity and the result tends to be like that of a least-squares migration. Ma and Hale (2013) successfully overcome this problem. However, to extend their method to time-lapse applications requires further study.…”
Section: Discussionmentioning
confidence: 99%
“…WT was previously implemented under the isotropic approximation (Zhou et al, 1995(Zhou et al, , 1997Van Leeuwen and Mulder, 2010;Ma and Hale, 2013;Zhang et al, 2015). However, the first arrivals may be strongly influenced by anisotropy at the near-surface with the consequence that isotropic migration will mis-position reflectors in depth (Shen et al, 2012).…”
Section: Introductionmentioning
confidence: 99%