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Plane-wave source migration

Shot gathers can also be synthesized to a new dataset to represent a physical experiment that does not occur in reality. One of the most important examples is to synthesize shot gathers to plane-wave source gathers. The plane-wave source gathers represent experiments that planar sources originate from all angles at the surface. They can also be regarded as the accurate phase-encoding of the shot gathers Liu et al. (2006). The plane-wave source dataset can be generated by delaying the shot in shot gathers or slant-stacking in receiver gathers as follows:
\begin{displaymath}
R_p(p_x,p_y;r_x,r_y,z=0,\omega)=\int \int R(s_x,s_y;r_x,r_y,z=0,\omega)e^{i\omega (s_xp_x+s_yp_y)}ds_xds_y,\end{displaymath} (4)
where px and py are ray parameters in the in-line and cross-line directions respectively. Its corresponding plane-wave source wavefield at the surface is
\begin{displaymath}
S_p(p_x,p_y;r_x,r_y,z=0,\omega)=\int\int e^{i\omega(s_xp_x+s_yp_y)}ds_xds_y.\end{displaymath} (5)
Similar to the Fourier transformation, we can transform the plane-wave source data back to shot gathers by the inverse slant-stacking Claerbout (1985) as follows
\begin{displaymath}
R(s_x,s_y;r_x,r_y,z=0,\omega)=
 \int \int \omega^2 R_p(p_x,p_y;r_x,r_y,z=0,\omega)e^{-i\omega (s_xp_x+s_yp_y)} dp_xdp_y\end{displaymath} (6)
In contrast to the inverse Fourier transformation, the kernel of the integral is weighted by the square of the frequency $\omega$.

The source wavefield Sp and receiver wavefield Rp are extrapolated into the subsurface independently using the one-way wave equations 1 and 2. The image of a plane-wave source with a ray parameter pair (px,py) is formed by cross-correlating the source and receiver wavefields weighted with the square of the frequency $\omega$:
\begin{displaymath}
I_{p_x,p_y}(x,y,z)=\int \omega^2 \bar{S_p}(p_x,p_y;x,y,z,\omega)R_p(p_x,p_y;x,y,z,\omega) d\omega.\end{displaymath} (7)
The final image is generated by stacking the images of all possible plane-wave sources:
\begin{displaymath}
I_{p}=\int\int I_{p_x,p_y}(x,y,z) dp_xdp_y.\end{displaymath} (8)
Because both slant-stacking and migration are linear operators, the image of the plane-wave migration Ip is equivalent to the image obtained by shot-profile migration Liu et al. (2002); Zhang et al. (2005).


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Next: Conical-wave source migration Up: 3D plane-wave migration Previous: 3D plane-wave migration
Stanford Exploration Project
5/6/2007