Page 523 - Acquisition and Processing of Marine Seismic Data
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514                                 11. SEISMIC MIGRATION































           FIG. 11.23  Schematic illustration of the f-k domain migration. (A) A dipping event in the time domain (top) and its f-k
           domain representation (bottom) before the migration. (B) The amplitude value X in the f-k domain is replaced to a point
            0
           X after migration, while its corresponding frequency value A is moved to a lower frequency of A . 0
           The displacement is along the vertical axis, and  migration. Essentially Gazdag migration also
           the horizontal wavenumber (k x ) is not affected.  works using the principle of downward con-
           The frequency value A of amplitude X before  tinuation of the recorded wave field, like the
           migration moves to a relatively lower frequency  finite-difference method, but this process corre-
           A .Inthef-kdomain,theinclinedeventOXisrelo-  sponds to a phase shift in the f-k domain. It can
             0
           cated to an event OX , and the inclination angle θ  also produce correct results up to 90-degree
                             0
           increases to θ after migration.              structural dips, providing that the velocity does
                       0
              Today, Stolt migration is the fastest and  not vary laterally.
           hence the most computationally efficient algo-
           rithm among all available migration algo-    11.4.1 Stolt Stretch Factor (W)
           rithms. It can produce acceptable results up to
           90-degree structural dips when a constant       Stolt migration is valid for constant velocity
           velocity medium is realized. Although the Stolt  media. For media with vertical and lateral veloc-
           stretch factor is used to obtain more correct  ity variations, the Stolt algorithm transforms the
           results in a variable velocity medium, the cor-  input data into a constant velocity section, and
           rection is applicable only for the apex point  then the Stolt migration is applied. This trans-
           and is invalid for the flanks of the diffraction  form induces a stretch to the seismic data along
           hyperbolas. The Stolt migration can be used  the vertical (temporal) axis. An inverse stretch is
           for a fast production or QC purposes to analyze  then performed to obtain the final migrated sec-
           if the input data has unexpected specific noise,  tion after the inverse Fourier transform.
           such as high-amplitude noise bursts or spikes,  Stretch changes between 0 and 2 and it par-
           which then become distinctive smiles after   tially controls the aperture of the Stolt migration.
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