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A step-by-step separation scheme

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}

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}

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}

\begin{displaymath}
P_{decomposed} = A3\,A2\,A1\ P_{raw}\ A1^T\,a2^T\,A3^T\end{displaymath}

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.


previous up next print clean
Next: VALIDITY OF THE FIRST Up: WAVEFIELD DECOMPOSITION Previous: The first order operator
Stanford Exploration Project
12/18/1997