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DAZZLER
TM
system manual Part I : installation & operation
2.3
Limitations to the compensation of the crystal dispersion
The maximum group delay variation that can be introduced is limited by the maximal pulse
shaping capability
τ
max
of the system (section
). For large spectral optical bandwidths,
the group delay variation that enables to compensate for the crystal dispersion exceeds the
maximal pulse shaping capability.
2.2.9
Beam orientations
As shown on
, the diffracted beam makes an angle with the input direction. Actually
in Fastlite crystals the transmitted beam is also deviated from the input beam because the
output face is set at an angle with the input face. The refraction on the output face is designed
to compensate small changes of the diffraction angle with wavelength. Please note that this
implies that the input and output faces are not interchangeable The table below gives the angles
of the diffracted and transmitted beams with regards to the input direction for the HR and
WB Dazzler models.
WB model
HRmodel
Diffracted beam angle (
◦
)
1.0
1.4
Transmitted beam angle (
◦
)
3.6
4.5
Another point to note is that there is inherently a displacement (no angular change) of the
diffracted beam depending on the point of diffraction in the acoustic column. This phenomenon
is called
walk-off
and it implies that the spectrum and/or delay depends slightly on position
in the beam. This weak effect can be eliminated if needed by using a double pass geometry
(application note ”double pass”).
Input Optical Beam
Reflection on
the input face
Reflection on
the ouput face
14°
3.6°
1°
Diffracted
Beam
Direct
Beam
Acoustic
Wave
Te02
Crystal
Transducer
Adaptation
Circuitry
SMA Plug
Figure 2.3: Diffracted and transmitted beams orientation for Dazzler
TM
HR model
2.3
Formulæ
See a collection of useful formulæ overleaf.
V3.00 - 8
th
April 2019