    Velocity continuation and the anatomy of residual prestack time migration  Next: Kinematics of Zero-Offset Velocity Up: Fomel: Velocity continuation Previous: Introduction

# KINEMATICS OF VELOCITY CONTINUATION

From the kinematic point of view, it is convenient to describe the reflector as a locally smooth surface , where is the depth, and is the point on the surface ( is a two-dimensional vector in the 3-D problem). The image of the reflector obtained after a common-offset prestack migration with a half-offset and a constant velocity is the surface . Appendix A provides the derivations of the partial differential equation describing the image surface in the depth-midpoint-offset-velocity space. The purpose of this section is to discuss the laws of kinematic transformations implied by the velocity continuation equation. Later in this paper, I obtain dynamic analogs of the kinematic relationships in order to describe the continuation of migrated sections in the velocity space.

The kinematic equation for prestack velocity continuation, derived in Appendix A, takes the following form: (1)

Here denotes the one-way vertical traveltime . The right-hand side of equation (1) consists of three distinctive terms. Each has its own geophysical meaning. The first term is the only one remaining when the half-offset equals zero. This term corresponds to the procedure of zero-offset residual migration. Setting the traveltime dip to zero eliminates the first and third terms, leaving the second, dip-independent one. One can associate the second term with the process of residual normal moveout. The third term is both dip- and offset- dependent. The process that it describes is residual dip moveout. It is convenient to analyze each of the three processes separately, evaluating their contributions to the cumulative process of prestack velocity continuation.

Subsections    Velocity continuation and the anatomy of residual prestack time migration  Next: Kinematics of Zero-Offset Velocity Up: Fomel: Velocity continuation Previous: Introduction

2014-04-01