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Computation of scaling factor $W_{\gamma,\phi}$

The last step is the computation of the scaling factor $W_{\gamma,\phi}$ from the partial derivatives ${\partial k_{x_h}}/{\partial \phi}$and ${\partial k_{y_h}}/{\partial \phi}$.

The unit vector ${\bf u}$tangent to the integration line at constant $\gamma$is given by
\begin{displaymath}
{\bf u}
=
\left(
\frac{
\frac{\partial k_{x_h}}{\partial \ph...
 ...+
\frac{\partial k_{y_h}}{\partial \phi}^2
}
}
{\bf y}
\right).\end{displaymath} (23)
The mapping along the azimuth axis of a vector of the same direction as u and length proportional to the sampling in the offset wavenumber domain $\left(\Delta k_{x_h},\Delta k_{y_h}\right)$is a segment of length
\begin{displaymath}
\delta \phi=
\frac{2 \sqrt{\Delta k_{x_h}^2 + \Delta k_{y_h}...
 ...partial \phi}^2
+
\frac{\partial k_{y_h}}{\partial \phi}^2
}
}.\end{displaymath} (24)
If $\Delta \phi$ is the azimuthal range of the stacking at $\gamma=0$,the scaling factor is set as in the following:  
 \begin{displaymath}
W_{\gamma,\phi}=
\left\{
\begin{array}
{ll}
1 
&
{\rm if}\; ...
 ...hi}
&{\rm if}\; \delta \phi< \Delta \phi. \\ \end{array}\right.\end{displaymath} (25)

 


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Stanford Exploration Project
10/14/2003