Tsunami - Beckman Institute Laser Resource Center
Tsunami - Beckman Institute Laser Resource Center
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.