Dip filtering of coherent linear noise

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Seismic Data Analysis
Series Investigations in Geophysics
Author Öz Yilmaz
DOI http://dx.doi.org/10.1190/1.9781560801580
ISBN ISBN 978-1-56080-094-1
Store SEG Online Store

Figure 6.2-5 shows four common-shot gathers, while Figure 6.2-6 shows their f − k spectra before and after f − k dip filtering. The pass or reject zones in the f − k spectra do not need to be constrained to fan shape. The left half of the spectra mostly contain spatially aliased data. By keeping the fan shape in the right quadrant, while zeroing out most of the left quadrant, the coherent noise trains, including the aliased energy, are eliminated.

Because aliasing is a serious concern in f − k filtering, it is advisable to apply it to shot gathers rather than to CMP gathers, since CMP gathers can have twice the trace spacing of shot gathers. Nevertheless, two neighboring CMP gathers can be interleaved before applying f − k dip filtering, then split afterward, thus alleviating aliasing. Such implementation is permissible provided the composite gather does not exhibit any traveltime shifts caused by changes in reflector geometries or lateral variations in velocities. Coherent noise as seen on the shot gathers in Figure 6.2-5 is best attenuated in the shot-gather domain. When sorted into CMP gathers, no significant remnant of this noise is left in the data (Figure 6.2-7). Figure 6.2-8a shows the stacked section derived from the CMP gathers in Figure 6.2-7a with no f − k filtering. Note the linear noise left in the stacked section. The CMP gathers with f − k filtering (Figure 6.2-7b) yield a stack that is virtually free of linear noise (Figure 6.2-8b).

Coherent linear noise on stacked data also can be suppressed by poststack migration that incorporates dip filtering. If coherent linear noise is associated with side scatterers, then much of it can be attenuated by a constant-velocity DMO correction (dip-moveout correction in practice). If f − k filtering were not applied to common-shot gathers containing side-scattered energy, then a stacked section with coherent linear noise could result (Figure 6.2-9a). Figure 6.2-9b shows that this noise can be attenuated by f − k dip filtering the stacked section. Could this noise attenuation be done better? If an f − k filter were applied to shot records, then the stack in Figure 6.2-9c results. When compared to the result in Figure 6.2-9b, the result in Figure 6.2-9c seems to offer better resolution. The prestack f − k filtered data also yield an improved velocity analysis (Figure 6.2-10).

Practical experience with f − k filtering proves that an even better stack may result when both common-shot and common-receiver gathers are f − k filtered. The resulting stack is shown in Figure 6.2-9d. Compare this with stacked sections in Figures 6.2-9b,c. If f − k filtering were done on only the shot gathers, then a good portion of coherent noise may remain in the data. Although this remaining noise may be attenuated by a second pass of f − k filtering on receiver gathers, enhanced smearing of the data can degrade reflector definition.

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