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Second definition: MZO extracted from prestack migration

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: 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 $z=\Delta z$  
 \begin{displaymath}
p(\omega,k_h,k_y,z=\Delta z)=
{ e^{ik_z(\omega,k_h,k_y)\Delta z}p(\omega,k_h,k_y,z=0)}\end{displaymath} (7)
for all values of $\omega,k_h,k_y$. The prestack migration imaging step consists of summing for all the values of $\omega$ and kh after downward continuation. To image for t=0 and h=0:  
 \begin{displaymath}
p(t=0,h=0,k_y,z)=
{\int d\omega \int d k_h \; e^{ik_z(\omega,k_h,k_y)z}
p(\omega,k_h,k_y,z=0)}\end{displaymath} (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} (9)

Following Hale's (1984) derivation, introduce a new variable $\omega_0$ 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} (10)
Substituting $\omega$ in equation (9) the downward continuation operator $k_z(\omega,k_h,k_y)$ 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} (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 $\omega_0$ is substituted for $\omega$ and then the order of integration is changed between $\omega_0$ and kh. The integration boundaries have to be observed carefully.


previous up next print clean
Next: Integration limits Up: Introduction Previous: First definition: MZO by
Stanford Exploration Project
11/17/1997