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CGG, Massy, France
Corresponding author: rgarotta@compuserve.com
| The first 20% of the full text of this article appears below. |
For land seismic surveys, it is still commonly thought that switching from conventional to multicomponent acquisition merely requires replacing vertical receivers with 3C receivers. This may work in some but not all cases. Fortunately, when it doesn't, the situation may be rectified by accounting for the physics of PS-mode propagation. In fact, this is often the prerequisite for obtaining comparable resolution of P and PS reflections at the target levelthe condition for obtaining full benefit from the combined use of P and PS data for determining appropriate exploration attributes and seismic inversion.
Two major properties of PS mode, that have already been widely recognized and analyzed, are:
This article will review some other physical phenomenainvolving reflectivity, conversion, absorption, and intra-array staticsthat should also be considered when field conditions require quantifying appropriate compensation for these negative effects.
| Comparison of P and PS waves |
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Poisson's reflectivity is the difference between P- and S-velocity contrasts 2
VP/VP - 2
VS/VS. This relationship is important because the seismic amplitude of P-wave sections mainly reflects density and P-mode velocity contrast but PS-wave sections mainly reflect density and S-mode velocity contrast. Fortunately, for most geologic interfaces, Poisson's reflectivity is weak and P or PS events can generally be correlated.
However, Poisson's reflectivity is sometimes observed in sand/shale sequences in which P or S contrasts can be quite different. Perhaps most importantly, strong Poisson's reflectivity may exist in the presence of
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