Elastic wave-equation-based reflection kernel analysis and traveltime inversion using wave mode decomposition
Elastic wave-equation-based reflection kernel analysis and traveltime inversion using wave mode decomposition
复制标题
基于弹性波方程的反射核分析和波模分解走时反演
DOI:
10.1093/gji/ggy291
复制
发表时间:
2018
影响因子:
2.8
通讯作者:
Chenlong Wang
中科院分区:
文献类型:
--
作者:
Tengfei Wang;Jiubing Cheng;Qiang Guo;Chenlong Wang
Elastic reflection waveform inversion (ERWI) utilizes reflections to update the low and intermediate wavenumbers in the deeper part of elastic models and can provide good initial models for elastic full waveform inversion (EFWI). Although ERWI aims to mitigate the nonlinearity of inversion when starting from a poor initial model, it suffers from the cycle-skipping problem due to the objective function of waveform fitting. Building initialP- andS-wave velocity models for EFWI through elastic wave-equation reflection traveltime inversion (ERTI) would be effective and robust since traveltime information relates to the background model more linearly. However, the current implementations of acoustic traveltime inversion is not straightforward in elastic media due to the existence ofS-wavefields. Wave mode decomposition, both on the recording surface and in the extrapolated wavefields, is important for ERTI. First, for seismic data withP-wave sources, theP/Sseparation of multicomponent seismograms isolates thePPandPSreflection events and thus make it possible to extract the event-to-event time-shifts of these isolated reflections through dynamic image warping (DIW). Then, we can use the traveltime residuals ofPPandPSreflections to build the objective function for ERTI. Second, based on the investigation of the complicated reflection kernels in an elastic medium, we demonstrate the necessity of wave mode decomposition applied on the extrapolated elastic wavefields, to suppress the artefacts induced by the undesirable cross-correlations of the components in forward and back-propagated wavefields. Therefore, the decomposition of surface recording data and extrapolated wavefields guarantees the dominate contribution of the traveltime is included during the ERTI. Accordingly, we propose a two-stage method to first build theP-wave background velocity using the separatedPPreflections and then build theS-wave background velocity using the separatedPSreflections based on the well-recoveredP-wave velocity model. A numerical example of the Sigsbee2A model shows the effectiveness of the proposed ERTI approach.