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Annual Report 2000 - WIT

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100<br />

weight during the stacking process, dynamic wavefield attributes need to be known,<br />

which in turn enables us also to sort the migrated/demigrated output by angle instead<br />

of offset, thus yielding AVA curves.<br />

0 0.5 1 1.5 2 2.5 3<br />

Time (sec)<br />

¢<br />

Time Domain<br />

Distance (km)<br />

2 3 4 5 6 7 8 9 10<br />

£<br />

Section<br />

Kirchhoff Migration<br />

Shot/Receiver Location<br />

x<br />

Macro Model Information<br />

Distance [km]<br />

3.5 4 4.5 5 5.5 6 6.5 7 7.5<br />

¡<br />

z<br />

Kirchhoff Demigration<br />

0.5 1 1.5 2 2.5 3 3.5<br />

Depth [km]<br />

Migrated image<br />

Depth Domain<br />

Figure 1: Principle of time/depth transformations by using Migration/Demigration<br />

based on the Unified Approach.<br />

THE UNIFIED APPROACH<br />

We give an brief outline of the concept of the unified approach which is the underlying<br />

theory to the method presented in this paper. A more complete discussion of the theory<br />

and implementation can be found in Hertweck et al. (this issue). As shown by (Tygel<br />

et al., 1996), there exists another inverse to the Kirchhoff migration integral that has<br />

the same integral structure. It is given by a stacking process which is applied to the<br />

depth migrated section. The stacking surfaces are now the isochrones, i.e., the surface<br />

of equal reflection time for a given source and receiver pair. These isochrones are<br />

defined by the same traveltimes as Kirchhoff-type diffraction traveltime surfaces that<br />

define the stacking surface for migration. Thus, the same macro-velocity model as<br />

previously used for Kirchhoff migration can be taken to transform the data. We can<br />

then set up an integral transformation pair to convert from time to depth and vice

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