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Since in the conventional surface seismic experiment, geophones are located only at the surface, the data is the receiver wavefield at z=0. This can be represented in equation (9) as a truncation operation (transpose of zero padding
):
|  |
(11) |
Then the expression for linear shot-profile modeling one-way wave equation operator is
|  |
(12) |
a chain of linear operators.
Next: Summary
Up: Forward operator
Previous: Receiver wavefield extrapolation
Stanford Exploration Project
5/23/2004