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Grating
Tutorial Link (click here)
- What
type of diffraction gratings (a.k.a. gratings) does Wasatch Photonics
manufacture?
- How
does your Volume Phase Holographic Grating (VPHG) technology differ
from surface relief grating technology?
- What
are some of the other properties of VPHGs?
- How
do you clean VPHGs?
- What
information is available on your gelatin recording medium and
is it stable over time?
- What
is a Dickson Grating®
and why is it different from other gratings?
- What
kind of performance characteristics can be expected from a Dickson
Grating®?
- Can
gratings with different dispersion angles be made?
- Over
what wavelengths can your gratings operate?
- What
physical sizes can be made?
- What
wavefront uniformity/distortion can be expected?
- What
environmental tests have been performed on your gratings?
- What
are the thermal and aiming characteristics?
- How
are DCG gratings affected by continuous wave (CW) and pulsed laser energy density conditions? How about DWDM and input signal conditions?
- Is
grating performance affected at temperature extremes or as a result
of temperature cycling?
- Are
your gratings affected by radiation?
- Holographically
recorded gratings normally have a spatial efficiency dependence
across the grating caused by a laser's Gaussian beam profile.
Do your holographic gratings have this spatial dependence?
Q.
What type of diffraction gratings (a.k.a. gratings) does Wasatch
Photonics manufacture?
A.
We make volume phase holographic gratings (VPHGs) recorded interferometrically
in DiChromated Gelatin (DCG) sealed in glass. There
are many other optical recording media. DCG possesses the
required combination of characteristics to produce very low polarization
dependent loss (PDL), very high efficiencies, and wide bandwidths.
These translate into benefits that enable telecom and other companies
to leverage and capitalize on their own technologies.

Q.
How does your Volume Phase Holographic Grating (VPHG) technology
differ from surface relief grating technology?
A.
VPHGs have a constant thickness (T) with a periodic, typically sinusoidal,
change in refractive index (n). Surface relief gratings have a periodic
change in thickness with a constant refractive index. Most VPHGs
are made in transmission geometry while most surface relief gratings
are made in reflection geometry. Master
VPHGs can usually be made for spatial frequencies >900 lpmm.
These master VPHGs may be copied optically without either
the master or copy VPHG degrading over time. Surface relief
masters are copied mechanically and both the surface relief master
and copy will degrade over time as the number of copies increases.


Q.
What are some of the other properties of VPHGs?
A.
VPHGs possess low stray light and low absorption in the visible
and NIR. They are sealed in glass making them long-lived, easy to
handle, scratch resistant, and easy to clean. VPHGs usually have
anti-reflection (AR) coatings applied to one or both surfaces to
minimize Fresnel reflections and increase overall output.
Q.
How do you clean VPHGs?
A.
VPHGs,
whether they are AR coated or not, can be easily be cleaned just
as you would any other glass optic to remove fingerprints, dust,
and contaminants. Use the standard optics cleaning method
of "drop and drag". Gently wipe the grating with
a clean, lint-free cloth/wipe using acetone or alcohol without much
pressure; reagent-grade methanol or Windex may also be used. Do
not use MEK, polishing compounds, etc. Hard rubbing with such
chemical or polishing compounds may damage the AR coating. AR coated
surfaces will pass the "Scotch Tape" test.

Q.
What information is available on your gelatin recording medium and
is it stable over time?
A. Our gelatin recording medium is very similar to the gelatin that
has been used in the photography industry for more than 100 years.
As you may know, properly processed photographs are very stable
and will retain their properties for decades. One of the major reasons
for this excellent stability of photographs is the stability of
the gelatin base. The discoloration of very old black and white
photographs is a result of insufficient removal of fixer from the
paper base, which results in a yellowing of the paper. It has nothing
to do with the gelatin.
Wasatch Photonics uses a dichromated gelatin (DCG) mixture as its
recording medium of choice. Once this mixture is processed and the
chromium removed, it is essentially pure gelatin and is very stable.
During the past thirty years, there has been no measurable degradation
in gelatin gratings that are properly sealed.
The DCG holographic scanning disks used in some of the early optical
bar code scanners still function exactly as they did over 20 years
ago. 
Q.
What is a Dickson Grating®
and why is it different from other gratings?
A. A Dickson Grating® is a highly specialized
volume phase transmission grating. It can diffract both orthogonal
linear polarizations with equal and high efficiency at included
angles greater than 90 degrees over 40 nm bandwidths. Other
gratings designed to be used at these high diffraction angles will
have much greater PDL, lower diffraction efficiency, and a greater
variation in diffraction efficiency across a 40 nm bandwidth. The
40 nm bandwidth and favorable high dispersion angles combined with
efficiencies near 95% make the Dickson Grating®
highly desirable for Telecom applications such as Mux/Demux/Remux,
OSA, monitors, filters and Raman Spectroscopy. The grating
is named after the grating designer, and Wasatch Photonics Co-Founder,
Lee Dickson. 
Q.
What kind of performance characteristics can be expected from a
Dickson Grating®?
A. Dickson Gratings®
can easily be designed for almost any spectral range. For
instance, a 940 lpmm Dickson Grating®
designed for 1525-1565nm will have these high performance characteristics:
Q.
Can gratings with different dispersion angles be made?
A. VPHGs can be made at almost any angle. Dickson
Gratings®
perform in narrow angular ranges, it is this limitation that allows
them to work as well as they do. There are however two classes of
realizable Dickson Gratings®
with the first working near a half angle of 46.5 degrees in air
and the other working at internal angles too high to escape from
a flat substrate which must therefore be used with prisms. This
latter design is termed the Dickson
Grism®
and has nearly TWICE the dispersion per pass of a Dickson Grating®.
In January of 2005, we delivered samples of our latest
high dispersion product, the Dickson 1350®
for 1525-1565nm which produces >2 times the dispersion of a 940 lpmm Dickson Grating®.

Q.
Over what wavelengths can your gratings operate?
A. We cover 350 -2400 nm (the entire visible range and
NIR) with a single recording material on your choice of glass substrates
and prisms. 
Q.
What physical sizes can be made?
A. Typical ruggedized sizes with perfect hermetic
seals begin at approximately 20 mm x 30 mm. Smaller sizes
have to be externally sealed. Gratings as large as 400 mm x 400 mm
have been made by the Wasatch Photonics team. 
Q.
What wavefront uniformity/distortion can be expected?
A. 1/4 wave is typical. Wavefront uniformity
<lambda/40 rms at 633 nm can be achieved for additional costs
using superior substrates, polishing techniques, etc. See this link
as an example of a Zygo interferometer measurement for a very
low wavefront error Dickson Grating®. 
Q.
What environmental tests have been performed on your gratings?
A. Our telecom-grade, epoxy
sealed gratings have survived boiling water for several days
with no degradation and 95o C at saturated humidities
for more than 2 weeks. A collapse of the grating structure has been
observed after several days at 120o C. Some of
our similar, but non-Dickson design, gratings are currently in commercial
multiplexers and are surviving real world tests as well as having
passed standard compliance testing. The DCG is hermetically
sealed between various substrates such as BK-7, Borofloat, low iron
sheet glass and fused silica, making it impervious to everything
but extreme heat. 
Q.
What are the thermal and aiming characteristics?
A. Aiming stability over time and temperature
is completely dependent upon the substrate used. Near zero drift
is obtained by using a substrate with a low thermal coefficient
of expansion (TCE) such as fused silica. See these links to
Angular Deviation vs. Temperature
and Lateral Dispersion (using
a 50 mm FL lens vs. Temperature. 
Q.
How is DCG affected by DWDM and input signal conditions?
A. There is hardly any absorption
in a phase grating. The more common reflection gratings absorb as
much as 20% and get really hot. It is not uncommon for communication
signals to be between 5 and 50 mw, so adding up a hundred or more
channels is a lot of heat. The gratings can take the heat but the
losses at the fiber ends will be measured in watts, so heat dissipation
probably has to be considered in a device's package. Total absorption
and scatter in the grating is about 2 or 3% so it is not a problem.
Depending upon the glue, it can begin to soften or degrade between
10 to 100 watts per square cm continuous wave. Properly hardened
gelatin can withstand >100
watts per square cm continuous wave. Peak power from pulsed laser energy applications can have energy densities in the megawatts. See our Pulsed Laser page. 
Q.
Is grating performance affected at temperature extremes or as a
result of temperature cycling?
A. Test results over a temperature
range of 0-100o C indicate no significant change in efficiency,
<0.5%, for a typical Dickson Grating®.
Gratings can also withstand repeated temperature cycling with no
measurable degradation in performance. 
Q.
Are
your gratings affected by radiation?
A.
See this link on Radiation
Effects on DiChromated Gelatin Gratings.
Q.
Holographically recorded gratings normally have a spatial efficiency
dependence across the grating caused by a laser's Gaussian beam
profile. Do your holographic gratings have this spatial dependence?
A. We have developed novel techniques that significantly
reduce variations in diffraction efficiency across our gratings.
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