Figure shows the results of the isotropic migration for this dataset. Figure (a) is the result of the isotropic plane-wave migration in Cartesian coordinates, and Figure (b) is the result of the isotropic plane-wave migration in tilted coordinates. In Figure (a), the salt flank is totally lost. This is because waves related to the salt flank are overturned, and the one-way wave-equation downward continuation method can not extrapolate them correctly. In Figure (b), although a weak steeply dipping reflector can be seen, it is not at the correct position, because the anisotropy in the sediment layer was neglected.
Figure shows the results of the anisotropic migration for this dataset. Figure (a) is the anisotropic plane-wave migration in Cartesian coordinates, and Figure (b) is the anisotropic plane-wave migration in tilted coordinates. In Figure (a), the top part of the salt flank is lost due to overturned waves, but the bottom part of the salt flank is correctly imaged, but is not focused by the isotropic migration (Figures (a) and (b)). In Figure (b), the image is greatly improved compared to the previous three images. Both the top and bottom parts of the salt flank are well imaged. In Figure (b), the reflector below the anisotropic layer is stronger and more continuous near the salt flank compared to that in the isotropic migration result. To check if the reflectors are imaged at the correct positions, we overlay the images with the density model in Figure . Figure (a) is the isotropic migration result overlaid with the density model. Figure (b) is the anisotropic migration result overlaid with the density model. The salt flank matches the density model very well in the image obtained by the anisotropic migration, while it deviates from the model in the isotropic one. The flat part of the reflector below the anisotropic layer is not affected much by the anisotropy. Both the isotropic and anisotropic migration image it at the correction position.
Figure shows the horizontal angle-domain CIGs at the horizontal location x=4000m. Figure (a) is obtained by the isotropic migration, and Figure (b) is obtained by the anisotropic migration. Figure shows the vertical angle-domain CIGs at the vertical location z=1500m. Figure (a) is obtained by the isotropic migration, and Figure (b) is obtained by the anisotropic migration. Although we use the true, vertical P-wave velocity in the isotropic migration, we find a small curvature in the horizontal angle gathers at the reflector below the anisotropic layer (at z=3300 m in Figure ), and a big curvature in the vertical angle gathers at the salt flank (x between 1000 m and 1500 m in Figure ). In the anisotropic migration, the angle gathers are flat at these locations. The big curvature of the angle gathers at the steeply dipping reflectors can be used as a tool to estimate the error in the anisotropy parameters used in the migrations.