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Finite-difference migration in v(x,z)

For the finite-difference migration, I tested the 45-degree equation in $(\omega,x,z)$.The velocity model used has a constant gradient from the left upper side to the right lower side, which is shown in Figure [*](a). Using this velocity model, a syncline reflector was modeled by the finite-difference method using the 45-degree equation and is shown in Figure [*](b). The migration result obtained by the conjugate of the forward modeling is shown in Figure [*](c). The reflector has clearly imaged except for background artifacts which seem to be caused by the boundary reflection. Figure [*](d) shows that we can suppress these artifacts by using the least-squares imaging method.

 
Wxz45miginv
Wxz45miginv
Figure 8
Least-squares finite-difference imaging in $(\omega,x,z)$: (a) The velocity model with a syncline reflector shown in Figure [*](a), (b) 45-degree finite-difference modeling, (c) The image obtained by the 45-degree finite-difference migration for (b), (d) The image obtained by the least-squares finite-difference imaging for (b) (after 10 iterations).
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Next: LEAST-SQUARES DATUMING Up: LEAST-SQUARES IMAGING Previous: Gazdag migration from an
Stanford Exploration Project
11/17/1997