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Gardner's approach to constant velocity DMO transforms the nonzero
offset data cube into an output cube with an artificial offset k
and traveltime t1.
After NMO and poststack migration an input impulse results in an output
data cube which depicts the corresponding ellipsoidal surface.
The transformation is defined by:
|  |
(2) |
|  |
(3) |
where tn and h are the traveltime and offset of the original
data input trace, and
b is the distance between the replacement trace's midpoint and
the input trace's midpoint.
t0 is the desired zero offset traveltime at b,
k is defined by equation (1). Equation
(3) shows
t0 to be the NMO corrected time for
offset k using the moveout velocity V.
Transformations (1) and (2) are velocity independent.
The final NMO step (3) permits a standard velocity analysis
.
Equations (1) and (2) define the DMO operator, which
in the input data set
is a slanting hyperbola,
lying in the radial plane.
The DMO operation sums along this hyperbola and stores the sum at the
hyperbola's vertex.
The impulse responses of the DMO process are slanting semicircles.
Next: Stretching the traces
Up: Schwab: DMO after logarithmic
Previous: INTRODUCTION
Stanford Exploration Project
11/18/1997