Here, we follow the same procedure as (, ) for the derivation of the PS-AMO operator.
First, we refer to equations (
) and (
) in order to understand the relationship
between CMP and CCP for the 3D case. We rewrite equation (
) as
80#80
where 81#81 is the angle between the midpoint vector (73#73) and the transformation vector (82#82).
We can then rewrite equation (
) as
| 83#83 | (35) |
82#82 is an extension of 74#74 and lies in the CCP space. Figure
shows both 74#74 and 82#82 in the same plane. Since the vectors are parallel,
the angle between 73#73 and 82#82 is the same as the angle between 73#73 and 74#74.If the coordinate system is
aligned with the midpoint coordinates, then the angle 81#81 is the same as the
azimuth (84#84).
81#81 changes after and
before PS-AMO. This variation is responsible for the event movement along
the common conversion point.
|
rot
Figure 1 Definition of offset vector 74#74 and transformation vector 82#82, before and after PS-AMO | ![]() |
Figure
shows how event movement along CCP changes with depth. This
is due to the dependence of 82#82 with respect to vp, 66#66 and tn. This variance
with depth will persist even in a constant velocity media. Figure
also illustrates that the time after PS-AMO (t2) has a new
74#74 and 82#82, therefore, a new CCP position.
|
plane2
Figure 2 Comparison between the CMP and CCP position in the PS-AMO operator | ![]() |
Continuing with the procedure presented by ()
to obtain the PS-AMO operator, we cascade PS-DMO [equation (
)] with its
inverse. Figure
shows a scheme of the PS-AMO transformation.
A trace with input offset vector 79#79 and midpoint at the
origin is transformed into equivalent data with output offset vector 85#85
and midpoint position 73#73. The data is first transformed to
its corresponding CCP position and 77#77. Subsequently, the
inverse PS-DMO repositions the data to a new midpoint position 73#73 with a
new offset vector 85#85.
|
plane
Figure 3 CMP-CCP plane, PS-AMO geometrical interpretation. | ![]() |
The new trace position is defined by
| 86#86 | (36) |
as
| 89#89 | ||
| 75#75 | (37) |
| 90#90 | ||