Asymptotic pseudounitary stacking operators |

where , , and and are the midpoint coordinates before and after the continuation. The summation path of the reverse continuation is found from inverting (73) to be

The Jacobian of the time coordinate transformation in this case is simply

Differentiating summation paths (73) and (74), we can define the product of the weighting functions according to formula (10), as follows:

The weighting functions of the amplitude-preserving offset continuation have the form (Fomel, 2001b)

It easy to verify that they satisfy relationship (76); therefore, they appear to be asymptotically inverse to each other.

The weighting functions of the asymptotic pseudo-unitary offset
continuation are defined from formulas (28) and (29), as follows:

The most important case of offset continuation is the continuation
to zero offset. This type of continuation is known as *dip moveout
(DMO)*. Setting the initial offset
equal to zero in the general
offset continuation formulas, we deduce that the inverse and forward
DMO operators have the summation paths

The weighting functions of the amplitude-preserving inverse and forward DMO are

and the weighting functions of the asymptotic pseudo-unitary DMO are

Equations similar to (83) and (84) have been published by Stovas and Fomel (1996). Equation (84) differs from the similar result of Black et al. (1993) by a simple time multiplication factor. This difference corresponds to the difference in definition of the amplitude preservation criterion. Equation (84) agrees asymptotically with the frequency-domain Born DMO operators (Bleistein and Cohen, 1995; Bleistein, 1990; Liner, 1991). Likewise, the stacking operator with the weighting function (83) corresponds to Ronen's inverse DMO (Ronen, 1987), as discussed by Fomel (2001b). Its adjoint, which has the weighting function

corresponds to Hale's DMO (Hale, 1984).

Asymptotic pseudounitary stacking operators |

2013-03-03