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Tsunami - Beckman Institute Laser Resource Center

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I I I I I I B I IL 1 1 i 1111 I L I I a,i I I I UUAI 11 I<br />

Pulse Width Measurement<br />

Example 1: Calculating pulse width measured by a Model 409 -08<br />

without pre-compensation.<br />

Assume an 800 nm pulse at the output coupler surface of a <strong>Tsunami</strong> laser<br />

is 55 fs long and transform limited. It passes through 1.9 cm of fused silica<br />

before exiting the <strong>Tsunami</strong>, and 0.25 cm of BK-7 glass and 0.26 cm of<br />

fused silica in the Model 409 -08.<br />

Therefore S = 76O(fs2)/(55 f ~ = ) 0.251 ~<br />

Then, looking at our normalized curve (Figure B-5) S = 0.251, and B =<br />

1.22, toat = 1.22 . tin = 67 f ~.<br />

Example 2: Calculating the prism spacing necessary for pre-compensating<br />

the Model 409 -08.<br />

Since dispersion is additive, it is only necessary to make the total dispersion<br />

equal to zero to eliminate all broadening effects. This allows a direct<br />

calculation of the required prism spacing without finding the actual broadening.<br />

Again, start with a 55 fs transform-limited, 800 nm pulse going through<br />

2.16 cm of fused silica and 0.25 cm of BK-7. Also assume the use of an<br />

SF-10 prism-pair pre-compensator where the beam passes through a total<br />

of 2 mm of prism tip per pass, or 8 mm total. The GVD for all parts of the<br />

system and the length for everything but the prism spacing are known.<br />

The length can be calculated by setting total GVD = 0.<br />

Therefore<br />

L = 25.3 cm ( = 10 in.).<br />

Note: the spacing L is the distance between the two tips of a prism in a<br />

double-pass configuration, or the distance between the two tips in one leg<br />

of a four-prism sequence.<br />

The calculated L is shorter than recommended above, but since the<br />

material dispersion value of SF-10 prisms is so high, sliding just a bit more<br />

glass in will add a large amount of positive GVD, thereby balancing out<br />

the prism spacing.

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