2010
DOI: 10.1109/tgrs.2010.2046670
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A New Vector Waveform Inversion Algorithm for Simultaneous Updating of Conductivity and Permittivity Parameters From Combination Crosshole/Borehole-to-Surface GPR Data

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Cited by 186 publications
(135 citation statements)
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“…In crosshole GPR full-waveform inversion the long spatial wavelengths of the model are typically used as a starting model. This model is obtained through ray-based inversion of first-arrival traveltimes and amplitudes of the waveform data (Ernst et al, 2007a;Meles et al, 2010). The data set considered in our study is expected to be too sparse to provide any useful information for a ray-based starting model.…”
Section: Discussionmentioning
confidence: 99%
“…In crosshole GPR full-waveform inversion the long spatial wavelengths of the model are typically used as a starting model. This model is obtained through ray-based inversion of first-arrival traveltimes and amplitudes of the waveform data (Ernst et al, 2007a;Meles et al, 2010). The data set considered in our study is expected to be too sparse to provide any useful information for a ray-based starting model.…”
Section: Discussionmentioning
confidence: 99%
“…The full-waveform inversion (FWI) approach used for this work is the FWI algorithm of Meles et al (2010), which extended the work of Ernst et al (2007) by honoring the EM vector character and introducing a simultaneous updating of the electrical permittivity and conductivity.…”
Section: Gpr Post-processing and Inversionmentioning
confidence: 99%
“…where ( ) , s syn E ε σ and s obs E are the synthetic and observed data, respectively, that contain the data for all sources, receivers and observation times according to the Meles et al (2010) formalism. Here, T denotes the transpose conjugate and the synthetic data are calculated using a 2D finite-difference time-domain (FDTD) solution of Maxwell's equations.…”
Section: Full-waveform Inversion Of Crosshole Gpr Datamentioning
confidence: 99%
“…Here, T denotes the transpose conjugate and the synthetic data are calculated using a 2D finite-difference time-domain (FDTD) solution of Maxwell's equations. The gradients of the misfit function with respect to the permittivity and conductivity S ∇ ε , and S ∇ σ are obtained by cross-correlating the incident wave field emitted from the source with the residual wave fields ∆E S that are back-propagating using the backpropagation operator ˆT G from the receiver at all medium locations in the time domain for all sources and receiver combinations as follows (see also Yang et al, 2013b;Meles et al, 2010) …”
Section: Full-waveform Inversion Of Crosshole Gpr Datamentioning
confidence: 99%