12.02.2015 Views

Tsunami - Beckman Institute Laser Resource Center

Tsunami - Beckman Institute Laser Resource Center

Tsunami - Beckman Institute Laser Resource Center

SHOW MORE
SHOW LESS

Create successful ePaper yourself

Turn your PDF publications into a flip-book with our unique Google optimized e-Paper software.

Mode Locking<br />

is chosen to be the same as the laser repetition rate C/2L. The AOM diffracts<br />

light out of the cavity only when the acoustic grating is present and, thus,<br />

functions as a time-dependent loss. In the frequency domain, this loss<br />

imparts modulation sidebands when a wave passes through the modulator<br />

(Figure A-2). In this manner, the AOM "comrnunicates" the phase between<br />

the longitudinal modes of the laser cavity. The final amplitude and frequency<br />

of the phase-locked longitudinal modes is shown in Figure A-3.<br />

'"m~<br />

-<br />

-<br />

-<br />

-5<br />

A<br />

- -2<br />

/<br />

/<br />

3<br />

Cavity<br />

End<br />

Mirror<br />

1-A",<br />

Acousto-optic Modulator (AOM)<br />

C/2L = 2WmL<br />

W-WmL<br />

W<br />

W+Wm~<br />

Figure A-2: Active mode locking using an AOM. Modulation sidebands are produced when a<br />

wave passes through an amplitude modulator.<br />

-<br />

Frequency (v)<br />

<strong>Laser</strong> Repetition Rate =<br />

= 2wmL<br />

Figure A-3: Amplitude and frequency of longitudinal modes in a<br />

mode-locked laser.

Hooray! Your file is uploaded and ready to be published.

Saved successfully!

Ooh no, something went wrong!