Tsunami - Beckman Institute Laser Resource Center
Tsunami - Beckman Institute Laser Resource Center
Tsunami - Beckman Institute Laser Resource Center
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P<br />
Lok-to-Clock Electronics<br />
Model 2080<br />
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PZT<br />
Signal<br />
-b<br />
<strong>Tsunami</strong> " A<br />
-<br />
- -<br />
Mode1 3930 - REF OUT<br />
Photodiode<br />
Input<br />
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b<br />
80 MHz<br />
0<br />
v<br />
-<br />
PZT<br />
Signal<br />
Model 3930<br />
- +<br />
REF IN<br />
Photodiode<br />
Input<br />
I I<br />
I<br />
Length Adjustw !<br />
- - -- - - /---<br />
- - -\<br />
Filter Lens I<br />
I<br />
Photodiode Nonlinear<br />
T "<br />
I<br />
Oscilloscope Calibration : c:<br />
2<br />
Etalon ;<br />
I<br />
I<br />
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3<br />
Photodiode Sample Lens<br />
Figure 8-6: Synchronization of two Lok-to-Clock <strong>Tsunami</strong> <strong>Laser</strong>s<br />
To overlap the pulses more precisely in time, focus the two <strong>Tsunami</strong><br />
output beams in a nonlinear crystal such as BBO." As you sweep the<br />
phase-matching angle of the BBO crystal, a frequency-doubled signal<br />
should be observed from each laser. Set the crystal for an intermediate<br />
angle to observe the sum frequency mixed signal from both lasers. By<br />
activating the sweep generator, the crystal can be easily phase-matched<br />
for observation of this sum frequency mixed signal. It will be modulated<br />
at the 10 Hz sweep period. Once the sum frequency mixed signal<br />
is observed, deactivate the sweep generator and use the coarse1<br />
fine TIMING controls to optimize this signal.<br />
* The nonlinear crystal must be cut such that it canfrequency-double the output of each<br />
lasel: Verifi this by temporarily placing a white card at the output of the crystal and<br />
then changing the phase-matching angle of the crystal while watching the laser output<br />
on the card.