Abstract

The cross-correlation imaging condition between source- and receiver-wavefields is often used in the elastic wave reverse-time migration (RTM) to utilize P- and S-waves. However, it cannot be applied in the absence of source information (e.g., source location, and source wavelet), which is quite common in passive source exploration. We employ a source-free P-SV converted-wave imaging condition, which only requires the back-propagating receiver-wavefield to utilize the P-SV converted waves in imaging the subsurface structures. The imaging condition is independent of source information, which can avoid the extrapolation and reconstruction of the source-wavefield. As a result, the computational cost is decreased to about one-third of conventional RTM that uses source-wavefield reconstruction strategies, e.g., random boundaries. The memory requirement could be also reduced by avoiding the calculation of source-wavefield. Because our imaging condition uses the vector P-wavefield and vector S-wavefield to utilize the P-SV waves, it is necessary to decouple P-wavefield and S-wavefield during the reverse-time extrapolation of receiver-wavefield. We use the first-order velocity-dilatation-rotation elastic wave equations to realize the reverse-time propagation of vector receiver-wavefield, where the vector P-wavefield and vector S-wavefield can be obtained directly. Based on the above methods, a source-free P-SV converted-wave RTM of multi-component seismic data is realized. The model tests show that this method can generate promising subsurface images and can be complementarily used when conventional cross-correlation imaging conditions are not suitable.

Highlights

  • Techniques based on reflected P-wave have played an important role in seismic exploration

  • This paper demonstrates a converted-wave reverse-time migration (RTM) method that can avoid the two issues of existing traditional elastic techniques

  • The method in this paper can only be used for the P-SV converted-wave RTM, but the process of multi-component seismic data includes the imaging of both converted-wave and reflected P-wave

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Summary

INTRODUCTION

Techniques based on reflected P-wave have played an important role in seismic exploration. The cross-correlation imaging is carried out by using the source- and receiver-wavefields of the opposite propagation directions to obtain P- and S-waves migration results Their method does not require the scalarization of the vector S-wave, and the vector properties of the S-wave remain during the imaging process. Based on the relationship between the P-wavefield and converted S-wavefield in the receiver extrapolation, Shabelansky et al (2017) demonstrated a source-free converted-wave RTM imaging condition, which only uses the back-propagation Pand S-waves to perform cross-correlation imaging.

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