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Hale (1984) starts with the prestack migration equation in
common-midpoint and offset coordinates and tries to
isolate four major processing steps.
The four steps are
- 1.
- DMO,
- 2.
- NMO,
- 3.
- Stacking,
- 4.
- Zero-offset migration.
By considering steps 1, 2, and 3 as a single process (MZO), I isolate
only two steps:
- Migration to zero-offset.
- Zero-offset migration.
After extracting the zero-offset migration from the prestack migration
equation, we are left with the migration to zero-offset operator.
For a constant velocity,
downward continue the field p(t,h,y,z=0)
recorded at the surface, to a depth
|  |
(7) |
for all values of
.
The prestack migration imaging step consists of
summing for all
the values of
and kh after downward
continuation. To image for
t=0 and h=0:
|  |
(8) |
where kz is given by
| ![\begin{displaymath}
{k_z(\omega,k_h,k_y)} \equiv
{ -{\omega \over v} \left\{ \le...
...2 \over {4\omega^2}}
(k_y-k_h)^2\right]^{1 \over 2} \right\} }.\end{displaymath}](img16.gif) |
(9) |
Following Hale's (1984) derivation, introduce
a new variable
in order to
isolate the zero-offset migration operator.
The substitution is based on the equation
| ![\begin{displaymath}
\omega \equiv
{\omega_0 { \left[ 1+{ {v^2 k_h^2 } \over
{ 4 \omega_0^2-v^2 k_y^2}} \right]}^{1 \over 2}}.\end{displaymath}](img18.gif) |
(10) |
Substituting
in equation (9)
the downward continuation operator
is transformed into
| ![\begin{displaymath}
k_z \equiv
-{ {2 \omega_0} \over v} {\left[ 1 -
{{v^2 k_y^2} \over {4 \omega_0^2}} \right]}^{1 \over 2}\end{displaymath}](img20.gif) |
(11) |
The downward continuation operator now has the same form as the
one for zero-offset. In order to isolate the zero-offset
migration operator, the variable
is substituted for
and then the order
of integration is changed between
and kh.
The integration boundaries have to be observed carefully.
Next: Integration limits
Up: Introduction
Previous: First definition: MZO by
Stanford Exploration Project
11/17/1997