Migration/inversion: think image point coordinates, process in acquisition surface coordinates

被引:40
作者
Bleistein, N [1 ]
Zhang, Y
Xu, S
Zhang, GQ
Gray, SH
机构
[1] Colorado Sch Mines, Dept Geophys, Ctr Wave Phenomena, Golden, CO 80401 USA
[2] Veritas DGC Inc, Houston, TX 77072 USA
[3] Chinese Acad Sci, Inst Computat Math & Sci Eng Comp, Acad Math & Syst Sci, Beijing 100080, Peoples R China
[4] Veritas DGC Inc, Calgary, AB T2P 5A2, Canada
关键词
D O I
10.1088/0266-5611/21/5/013
中图分类号
O29 [应用数学];
学科分类号
070104 ;
摘要
We state a general principle for seismic migration/inversion (M/I) processes: think image point coordinates; compute in surface coordinates. This principle allows the natural separation of multiple travel paths of energy from a source to a reflector to a receiver. Further, the Beylkin determinant (Jacobian of transformation between processing parameters and acquisition surface coordinates) is particularly simple in stark contrast to the common-offset Beylkin determinant in standard single arrival Kirchhoff M/I. A feature of this type of processing is that it changes the deconvolution structure of Kirchhoff M/I operators or the deconvolution imaging operator of wave equation migration into convolution operators; that is, division by Green's functions is replaced by multiplications by adjoint Green's functions. This transformation from image point coordinates to surface coordinates is also applied to a recently developed extension of the standard Kirchhoff inversion method. The standard method uses WKBJ Green's functions in the integration process and tends to produce more imaging artefacts than alternatives, such as methods using Gaussian beam representations of Green's functions in the inversion formula. These methods point to the need for a true-amplitude Kirchhoff technique that uses more general Green's functions: Gaussian beams, true-amplitude one-way Green's functions, or Green's functions from the two-way wave equation. Here, we present a derivation of a true-amplitude Kirchhoff M/I that uses these more general Green's functions. When this inversion is recast as an integral over all Sources and receivers, the formula is surprisingly simple.
引用
收藏
页码:1715 / 1744
页数:30
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