Page 479 - Acquisition and Processing of Marine Seismic Data
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470                      10. NORMAL MOVEOUT CORRECTION AND STACKING


























           FIG. 10.9  A synthetic CDP gather with a single reflection hyperbola (A) before, and (B) after NMO correction. The close-
           ups of NMO corrected gather for (C) near and (D) far offset traces, are indicated by I and II, enclosed by blue and red dashed
           rectangles, respectively. (E) and (F) are corresponding mean amplitude spectra of the close-ups in (C) and (D).


           point to multiple time locations on the corrected  NMO stretch is a frequency distortion in
           trace because of their interference nature   which the dominant frequencies of the reflection
           through more than one individual reflection  events shift to the lower frequencies, and it is
           event. That is, a specific time sample of an uncor-  expressed by
           rected trace may represent more than one reflec-             Δf
           tion hyperbola at the same recording time,                      ¼  Δt NMO         (10.16)
                                                                         f    t 0ðÞ
           which ultimately results in a complete degrada-
           tion of early arrivals at far offset traces in a CDP  where f is the dominant frequency and Δf is the
           gather. As an example, a synthetic CDP with two  amount of shift in the frequency. NMO stretch
           intersecting reflection hyperbolas are illustrated  occurs in the early arrivals of the far offset traces,
           in Fig. 10.10A, with a close-up to emphasize the  which severely distorts the shallow parts of the
           interference effect of two independent events in  CDPs. The stretched parts of the far offset traces
           the intersection zone. A strong degradation  are muted out and this process is known as
           arises after NMO correction due to the interfer-  NMO stretch mute. Muting is performed auto-
           ence along the early arrivals for offsets larger  matically using the expression given by
           than approximately 300 m for shallower reflec-  Eq. (10.16), and the mute zone is determined
           tion, which even influences the deeper reflection  by a percentage value termed the NMO stretch
           hyperbola for offsets larger than approximately  limit. Fig. 10.11 shows a synthetic CDP and its
           750 m (Fig. 10.10B). If two hyperbolas did not  NMO corrected versions for different stretch
           intersect as in Fig. 10.10C, depending on their  limit percentages. The limit can exceed 100%,
           velocities, the degradation would occur for the  and it does not mean that the entire NMO stretch
           offsets greater than approximately 600 m for  zone is successfully muted out when a 100%
           shallower reflection, and there would be no deg-  limit is used. The smaller the percentage mute
           radation for deeper reflection at all (Fig. 10.10D).  limit, the larger the stretch mute zone. For higher
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