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Annual Report 2000 - WIT

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44<br />

The optimized radii of curvatures of the NIP waves are shown in Figure 8. For<br />

comparison, in Figure 9, we have the optimized NIP wave radii of curvatures (cross<br />

line) and the ray theoretical calculated values (dot line). We observe that in caustic<br />

region the radius of curvature of the NIP wave is only poorly estimated. This last<br />

result is due to the destructive interference of caustic events.<br />

Time [s]<br />

0.2<br />

0.4<br />

0.6<br />

0.8<br />

1<br />

1.2<br />

Distance [m]<br />

1000 1500 <strong>2000</strong> 2500 3000 3500<br />

5000<br />

4500<br />

4000<br />

3500<br />

3000<br />

2500<br />

<strong>2000</strong><br />

1500<br />

1000<br />

500<br />

Figure 8: ô¤õ§ö©÷ section with the best estimated results of the CRS stack.<br />

500<br />

R NIP<br />

[m]<br />

400<br />

300<br />

200<br />

100<br />

5000<br />

First reflector<br />

1000 1500 <strong>2000</strong> 2500 3000 3500<br />

Distance [m]<br />

R NIP<br />

[m]<br />

4000<br />

3000<br />

<strong>2000</strong><br />

1000<br />

0<br />

Second reflector<br />

1000 1500 <strong>2000</strong> 2500 3000 3500<br />

Distance [m]<br />

Figure 9: Comparison of ô¤õ§ö©÷ . Direct calculated values (dot line) and estimated<br />

values (cross line). Top: First interface and bottom: second interface.

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