Elastic envelope inversion using multicomponent seismic data with filtered-out low frequencies

The absence of low-frequency information in seismic data is one of the most difficult problems in elastic full waveform inversion. Without low-frequency data, it is difficult to recover the long-wavelength components of subsurface models and the inversion converges to local minima. To solve this problem, the elastic envelope inversion method is introduced. Based on the elastic envelope operator that is capable of retrieving lowfrequency signals hidden in multicomponent data, the proposed method uses the envelope of multicomponent seismic signals to construct a misfit function and then recover the longwavelength components of the subsurface model. Numerical tests verify that the elastic envelope method reduces the inversion nonlinearity and provides better starting models for the subsequent conventional elastic full waveform inversion and elastic depth migration, even when low frequencies are missing in multicomponent data and the starting model is far from the true model. Numerical tests also suggest that the proposed method is more effective in reconstructing the long-wavelength components of the S-wave velocity model. The inversion of synthetic data based on the Marmousi-2 model shows that the resolution of conventional elastic full waveform inversion improves after using the starting model obtained using the elastic envelope method. Finally, the limitations of the elastic envelope inversion method are discussed.

[1]  R. G. Pratt,et al.  Full waveform tomography for lithospheric imaging: results from a blind test in a realistic crustal model , 2007 .

[2]  Sanyi Yuan,et al.  Simultaneous multitrace impedance inversion with transform-domain sparsity promotionStructures — Exploring impedance inversion , 2015 .

[3]  René-Édouard Plessix,et al.  The use of low frequencies in a full‐waveform inversion and impedance inversion land seismic case study , 2013 .

[4]  Paul L. Stoffa,et al.  Vp/Vs—A POTENTIAL HYDROCARBON INDICATOR , 1976 .

[5]  C. Shin,et al.  Waveform inversion in the Laplace domain , 2008 .

[6]  Liangguo Dong,et al.  Full Waveform Inversion Based on Envelope Objective Function , 2013 .

[7]  Hicks,et al.  Gauss–Newton and full Newton methods in frequency–space seismic waveform inversion , 1998 .

[8]  R. Gerhard Pratt,et al.  Efficient waveform inversion and imaging: A strategy for selecting temporal frequencies , 2004 .

[9]  Ru-Shan Wu,et al.  Seismic envelope inversion and modulation signal model , 2014 .

[10]  Gerard T. Schuster,et al.  Wave-equation traveltime inversion , 1991 .

[11]  Liangguo Dong,et al.  Full waveform inversion method using envelope objective function without low frequency data , 2014 .

[12]  C. Bunks,et al.  Multiscale seismic waveform inversion , 1995 .

[13]  Gerard T. Schuster,et al.  Wave-equation Reflection Traveltime Inversion , 2011 .

[14]  S. Operto,et al.  lastic frequency-domain full-waveform inversion , 2009 .

[15]  Jean Virieux,et al.  An overview of full-waveform inversion in exploration geophysics , 2009 .

[16]  P. Mora Nonlinear two-dimensional elastic inversion of multioffset seismic data , 1987 .

[17]  René-Édouard Plessix,et al.  A parametrization study for surface seismic full waveform inversion in an acoustic vertical transversely isotropic medium , 2011 .

[18]  Gary Martin,et al.  Marmousi-2: An Updated Model for the Investigation of AVO in Structurally Complex Areas , 2002 .

[19]  Guy Chavent,et al.  Nonlinear Least Squares for Inverse Problems: Theoretical Foundations and Step-by-Step Guide for Applications , 2009 .

[20]  R. Plessix A review of the adjoint-state method for computing the gradient of a functional with geophysical applications , 2006 .

[21]  J. Tromp,et al.  Misfit functions for full waveform inversion based on instantaneous phase and envelope measurements , 2011 .