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Tsunami - Beckman Institute Laser Resource Center

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P<br />

Lok-to-Clock Electronics<br />

Model 2080<br />

t\<br />

PZT<br />

Signal<br />

-b<br />

<strong>Tsunami</strong> " A<br />

-<br />

- -<br />

Mode1 3930 - REF OUT<br />

Photodiode<br />

Input<br />

<br />

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 />

><br />

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.

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