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Field arrays cancel random noise but their main function,
I believe, is to cancel low-velocity coherent noises,
something we now see is handled effectively by steep-dip deconvolution.
While I do not advocate abandoning field arrays,
it is pleasing to notice that with the arrival of steep-dip deconvolution,
we are no longer so dependent on field arrays
and perhaps coherent noises can be controlled
where field arrays are impractical,
such as certain 3-D geometries.
wz.10
Figure 2
Bottom is a North African vibrator shot profile (Y&C #10) after AGC.
Middle is gapped 1-D decon. Top is steep-dip decon.
wz.25
Figure 3
Bottom is an Alberta dynamite shot profile (Y&C #25) after AGC.
Middle is gapped 1-D decon. Top is steep-dip decon.
wz.31
Figure 4
Bottom is a North Sea air gun shot profile (Y&C #30) after AGC.
Middle is gapped 1-D decon. Top is steep-dip decon.
wz.32
Figure 5
Bottom is a North Sea air gun shot profile (Y&C #31) after AGC.
Middle is gapped 1-D decon. Top is steep-dip decon.
wz.39
Figure 6
Bottom is a Middle east Geoflex shot profile (Y&C #39) after AGC.
Middle is gapped 1-D decon. Top is steep-dip decon.
Next: REFERENCES
Up: Claerbout: Steep-dip deconvolution
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Stanford Exploration Project
11/17/1997