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Tsunami - Beckman Institute Laser Resource Center

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I I 0 I I 1 I )I Ulllllll ill I<br />

Mode Locking<br />

locked, and mode beating generates a modulation of the laser output at a<br />

frequency of CI2,. This mode beating is detected by a photodiode and then<br />

amplified. Since this signal is twice the required AOM modulation frequency<br />

(aML), it is divided by two, then the phase is adjusted such that the<br />

modulator is always at maximum transmission when the pulse is present.<br />

Finally, the signal is reamplified and fed to the AOM.<br />

Most actively mode-locked systems run on resonance for maximum<br />

diffraction efficiency. The AOM in a <strong>Tsunami</strong> is operated off-resonance<br />

with a diffraction efficiency of about 1 %. The output pulse width is not<br />

controlled by the AOM diffraction efficiency. Rather, pulse shortening in<br />

the <strong>Tsunami</strong> occurs through a combination of positive GVD and nonlinear<br />

effects (self phase modulation) in the Ti:sapphire rod. Ultimately, the<br />

output pulse width is controlled by adding net negative GVD to the cavity<br />

to balance these effects. (Refer to the following section on GVD.)<br />

<strong>Tsunami</strong><br />

Modulator<br />

Driver Amplifier<br />

+<br />

Divider<br />

Phase<br />

Adjust<br />

Photodiode<br />

Amplifier<br />

Model 3930<br />

Figure A-4: Configuration of the electronics for a regenerative modelocked<br />

laser.

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