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Tsunami - Beckman Institute Laser Resource Center

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I I 0 I I 1 1 LI I lillll Ill I!,lllllllQI 1 I II ! l ll i I I ll,l I 1 I I I1 ii illill Ill I<br />

Pulse Width Measurement<br />

The Spectra-Physics <strong>Laser</strong>s Model 409 -08 scanning autocorrelator operates<br />

in a background-free configuration according to the principles of<br />

noncollinear autocorrelation. It allows the autocorrelator signal to be<br />

conveniently displayed on a high impedance oscilloscope, providing the<br />

user with instantaneous feedback of laser performance. The optical path of<br />

the Model 409 -08 is shown in Figure B-3. The Model 409 -08 uses a<br />

rotating block of fused silica for varying the relative path lengths of both<br />

beam paths, and the scanning time base is calibrated by moving a calibration<br />

etalon of known thickness in and out of one of the beam paths. The<br />

Model 409 -08 can be used over the wavelength range from 650 to 1600<br />

nm and, by changing the rotating blocks, it can be used to measure pulse<br />

widths from 25 ps to c 80 fs.<br />

HRRl<br />

1<br />

I<br />

'<br />

Calibration<br />

HRR2 Rotating<br />

Block 1 I<br />

(Thin Block Shown)<br />

l I<br />

I<br />

I<br />

I<br />

i<br />

t<br />

Alignment<br />

Beam Splitter<br />

~ - - - - - Input - ~<br />

I<br />

i Beam I Alignment<br />

I<br />

Splitter<br />

I Iris<br />

j<br />

t<br />

1 t I<br />

1 I<br />

I<br />

I<br />

I<br />

I<br />

I<br />

& Lens<br />

PMT UV<br />

I<br />

I<br />

5 F r r X i l I<br />

*- ---- ----------- n<br />

M3<br />

I<br />

I<br />

I<br />

I<br />

I<br />

Alignment<br />

Target<br />

M<br />

HRR<br />

Xtal<br />

PMT<br />

Mirror<br />

Hollow Retro-reflector<br />

Non-linear Crystal<br />

Photomultiplier Tube<br />

- Figure B-3: The Model 409 -08 Autocorrelator Optical Path. The beam paths are displaced by<br />

HRRl and HRR2 in and out of the plane of the paper, so the configuration corresponds to the<br />

background-free method shown in Figure B-2.

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