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For orthorhombic media with a horizontal plane of symmetry there are
certain symmetries to the operator. The elements of the operator will
be either symmetric or anti-symmetric functions of the slowness:
![\begin{displaymath}
\left[
\begin{array}
{ccccc}
{\rm Symm} & & {\rm Symm} & & ...
...\ {\rm Anti} & & {\rm Anti} &
& {\rm Symm}\end{array}\right].\end{displaymath}](img6.gif)
The exact linear operator has elements that can be expressed as
polynomial functions of the horizontal slowness. By truncating the
operator to low order in slowness I obtain an approximate operator
that is valid for small angles of propagation (Nichols, 1989).
Next: The zeroth order operator
Up: WAVEFIELD DECOMPOSITION
Previous: WAVEFIELD DECOMPOSITION
Stanford Exploration Project
12/18/1997