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DAZZLER
TM
system manual Part I : installation & operation
3.3
Figure 3.7: Short Acoustic Pulse and Typical Oscilloscope Measure
Put the detection diode on the transmitted beam (
). Change the second order phase
value to cover 2/3 of the full time window on the software time graph and apply full power.
Observe the drop of signal on the scope. The maximum drop corresponds to the diffraction
efficiency of your Dazzler system. It should be at least 50% for a laser source of bandwidth
smaller than 100
nm
.
Your Dazzler system is now ready to be used. You can unblock the beam after the Dazzler and
seed the amplifier with the diffracted beam.
3.3.4
Dazzler operating in other setups
The procedure follows:
1. measure the spectrum of the incident pulse with a spectrometer and save it as reference.
2. increase the second order phase coefficient (”order 2”) on the GUI to produce a quasi-flat
signal covering the full time window (
). Do not pay attention to the red curve
on the spectrum graph. The signal is willfully truncated in the crystal to adjust the
superposition of the optical incident pulse with the acoustic wave. Please keep in mind
that for other Dazzler operations, the red and black curves have to be superimposed.
3. measure the diffracted spectrum.
4. adjust the
x
and
y
position of the crystal to closely match the reference spectrum shape.
5. check that the input beam is still autocollimated.
6. finely adjust the synchronization between the optical wave and the acoustic wave using
the trigger settings as described in chapter
7. check as the spectral clipping displayed on the spectrum graph is the same than the one
measured on the diffracted spectrum (
Your Dazzler system is now ready to be used.
V3.00 - 8
th
April 2019