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Previous: The first order operator
The first order operator can be further approximated as a cascade of
three operators.
![\begin{displaymath}
A3\ =\ \left[
\begin{array}
{ccccc}
1 & & 0 & & 0 \\ & & &...
...}.p_y \\ & & & & \\ 0 &
& y_{32}.p_y & & 1\end{array}\right]\end{displaymath}](img9.gif)
pre-multiplying,
![\begin{displaymath}
A2\ =\ \left[
\begin{array}
{ccccc}
1 & & 0 & & x_{13}.p_x ...
... & & 0 \\ & & & & \\ x_{31}.p_x & & 0 & & 1\end{array}\right]\end{displaymath}](img10.gif)
pre-multiplying,
![\begin{displaymath}
A1\ =\ \left[
\begin{array}
{ccccc}
\cos(\phi)/2 & & \sin(\...
...\phi)/2 & & 0 \\ & & & & \\ 0 & & 0 & & 1/2\end{array}\right]\end{displaymath}](img11.gif)
![\begin{displaymath}
P_{decomposed} = A3\,A2\,A1\ P_{raw}\ A1^T\,a2^T\,A3^T\end{displaymath}](img12.gif)
The separation procedure has three stages.
- A1
- A rotation about the z-axis to separate the two S-wavetypes.
- A2
- An operator to separate P from S1. This operator has two free parameters that need to be estimated.
- A3
- An operator to separate P from S2. This operator also has two
free parameters that need to be estimated.
Next: VALIDITY OF THE FIRST
Up: WAVEFIELD DECOMPOSITION
Previous: The first order operator
Stanford Exploration Project
12/18/1997