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@ARTICLE{Moghadas:11776,
author = {Moghadas, D. and André, F. and Slob, E.C. and Vereecken,
H. and Lambot, S.},
title = {{J}oint full-waveform analysis of off-ground zero-offset
ground penetrating radar and electromagnetic induction
synthetic data for estimating soil electrical properties},
journal = {Geophysical journal international},
volume = {182},
issn = {0956-540X},
address = {Oxford . Wiley-Blackwell},
publisher = {Wiley-Blackwell - STM},
reportid = {PreJuSER-11776},
pages = {1267 - 1278},
year = {2010},
note = {This research was supported by the Forschungszentrum Julich
(Germany), Universite catholique de Louvain and FNRS
(Belgium) in the framework of the DIGISOIL project, financed
by the European Commission under the 7th Framework Programme
for Research and Technological Development, Area
'Environment', Activity 6.3 'Environmental Technologies'.},
abstract = {A joint analysis of full-waveform information content in
ground penetrating radar (GPR) and electromagnetic induction
(EMI) synthetic data was investigated to reconstruct the
electrical properties of multilayered media. The GPR and EMI
systems operate in zero-offset, off-ground mode and are
designed using vector network analyser technology. The
inverse problem is formulated in the least-squares sense. We
compared four approaches for GPR and EMI data fusion. The
two first techniques consisted of defining a single
objective function, applying different weighting methods. As
a first approach, we weighted the EMI and GPR data using the
inverse of the data variance. The ideal point method was
also employed as a second weighting scenario. The third
approach is the naive Bayesian method and the fourth
technique corresponds to GPR–EMI and EMI–GPR sequential
inversions. Synthetic GPR and EMI data were generated for
the particular case of a two-layered medium. Analysis of the
objective function response surfaces from the two first
approaches demonstrated the benefit of combining the two
sources of information. However, due to the variations of
the GPR and EMI model sensitivities with respect to the
medium electrical properties, the formulation of an optimal
objective function based on the weighting methods is not
straightforward. While the Bayesian method relies on
assumptions with respect to the statistical distribution of
the parameters, it may constitute a relevant alternative for
GPR and EMI data fusion. Sequential inversions of different
configurations for a two layered medium show that in the
case of high conductivity or permittivity for the first
layer, the inversion scheme can not fully retrieve the soil
hydrogeophysical parameters. But in the case of low
permittivity and conductivity for the first layer, GPR–EMI
inversion provides proper estimation of values compared to
the EMI–GPR inversion.},
cin = {ICG-4 / JARA-ENERGY},
ddc = {550},
cid = {I:(DE-Juel1)VDB793 / $I:(DE-82)080011_20140620$},
pnm = {Terrestrische Umwelt},
pid = {G:(DE-Juel1)FUEK407},
shelfmark = {Geochemistry $\&$ Geophysics},
typ = {PUB:(DE-HGF)16},
UT = {WOS:000280997700012},
doi = {10.1111/j.1365-246X.2010.04706.x},
url = {https://juser.fz-juelich.de/record/11776},
}