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Annual Report 2000 - WIT

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à Ä_jÄ Å ð ¨<br />

â<br />

76<br />

by the minimal distance of two objects such that their images can still be recognized<br />

as two distinct ones. In this way, resolution is clearly a frequency-domain concept.<br />

For a more practical, time-domain concept, we need a different definition. Guided by<br />

the above section on pulse distortion, we quantify horizontal resolution by means of<br />

the region around the migrated reflection point öA[ that is influenced by the migrated<br />

elementary wave at öA[ .<br />

To obtain an estimate for the mentioned zone of 'horizontal influence' after migration,<br />

we investigate the migration output at the chosen depth point ö ¿ öO[ in the<br />

vicinity of the specular reflection point öA[ (see Figure 1), i.e., when the output point<br />

is moved along the reflector \T[ .<br />

S G r<br />

M<br />

R<br />

x<br />

R<br />

Ω R<br />

z<br />

M R<br />

Σ R<br />

migrated reflector image<br />

Figure 1: Horizontal resolution: influence of the migrated event at the specular reflection<br />

point öA[ on the migration result at the neighboring point ö][ on the reflector.<br />

In particular, we study the horizontal resolution of seismic migration as a function<br />

of offset. As shown by Tygel et al. (1994), the vertical resolution is the worse the<br />

greater the offset becomes. For a horizontal reflector below a constant-velocity overburden,<br />

it decreases proportionally to the cosine of the reflection angle. A similiar<br />

behaviour is expected for horizontal resolution.<br />

MATHEMATICAL DERIVATION<br />

As the starting point, we consider the time-dependent diffraction-stack integral in the<br />

form of Tygel et al. (1994),<br />

Ëa` ¸ ¹ Ë ¼<br />

¹<br />

ö<br />

¸ ¹ Ë ¼ ö ¾" ¼<br />

dif<br />

(1)<br />

^X¸<br />

ö ¼Ó¾ ¿<br />

ÏNOÓ § ¾cb

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