Fast frequency‐wavenumber migration for depth‐dependent velocity
Fast frequency‐wavenumber migration for a constant‐velocity medium is generalized for a medium with depth‐dependent velocity and density. As in the constant‐velocity case, the migrated section is obtained with one inverse Fourier transformation of the modified spectrum of the observed wave field. The migrated section is exact in a preselected focusing depth (in the case of common‐midpoint and plane‐wave migration) or in a preselected focusing point (in the case of single‐shot migration) and in the vicinity of this depth or point. Elsewhere the migrated section is distorted. The method is in essence a constant‐velocity migration with the velocity [Formula: see text] at the target depth [Formula: see text] (not with an average velocity), extended by a phase‐shift operation which takes account of the true velocity‐depth function v(z) between z = 0 and [Formula: see text]. If the focusing depth or point is located in a layer with constant velocity and density, the migrated section is exact throughout the layer (for CMP and plane‐wave migration) or along the segment of the ray from shot to focusing point, running through the layer (for single‐shot migration). Examples are given for the successful migration of the plane‐wave response of a horizontally layered medium at vertical and oblique incidence and for the single‐shot response of a horizontally layered structure with embedded reflector elements. The method appears to be particularly useful for the investigation of subsurface structures with restricted dimensions; because of its speed, interactive data interpretation is possible.