Concave
Gratings Rowland Type
Standard
products
Information
about our Concave Gratings...
When
ordering a grating, please use the following example format:
C
1800 Dia 63.5xThk12.5 190-400 (TM+TE)/2 (-1) deviation angle 30°,
RoC 500 mm
| 1. |
C
stands for Concave |
| 2. |
1800
is the groove density (groove frequency) in grooves/mm |
| 3. |
W
is the blank dimension in mm parallell with the grating grooves |
| 4. |
H
is the blank dimension in mm perpendicular to the grating grooves |
| 5. |
Dia
is the diameter in mm |
| 6. |
Thk
is the blank centre thickness in mm |
| 7. |
190-400
nm is the desired optimization range. A specific wavelength or range
with peaked wavelength can also be specified |
| 8. |
(TM+TE)/2
(-1) is desired polarization state and diffraction order the grating
should be optimized for. TE or TM can also be specified |
| 9. |
Constant
deviation angle 30° is the configuration the grating should
be optimized for. Constant incidence angle °
can also be specified |
Standard tolerances on W, H, Dia: ± 0.2 mm Thk ± 0.5 mm
CA > 90 % of blank size
Standard
concave gratings type C, specified by combining from:
Grooves/mm |
Wavelength
range: |
Concave
Radius: |
Sizes: |
0300
0600
1200
1800
2400
3600 |
UV
190-400 nm
UV-VIS
VIS 400-750 nm
VIS-NIR
NIR 750-1600 nm |
500.0
400.0
750.1
998.8
2000.0 |
50
x 50 x 10 mm
dia 50 x 12.5 mm
dia 63.5 x 12.5 mm
dia 63.5 x 12.5 mm
dia 63.5 x 12.5 mm |
Other specifications available on request, contact our sales department!
Concave
Gratings Rowland Type
This type of grating is the holographic counterpart of the classically
ruled concave grating, invented by Rowland in the 19th century. The
Rowland grating has straight grooves which are equally spaced along
a chord of the concave surface.
Rowland
circle
These gratings are preferably used in mountings based on the Rowland
circle, i.e. a circle with a diameter equal to the radius of curvature
of the grating. If the entrance slit is located on the Rowland circle,
then the spectral focus will also be on this circle.
If R is the radius of curvature, and a and b are the angles of incidence
and diffraction, respectively, then
LA = Rcosa
LB = Rcosb
where LA and LB are the distances from grating centre to the entrance
slit and spectral focus.
Good
resolution
The aberrations (except astigmatism) are small for all points on the
Rowland circle, making the gratings useful for wide spectral ranges.
Since all diffracted orders are focused on the Rowland circle, it is
possible to make measurements on different orders simultaneously.
Extremely
low stray light
Spectrogon's Rowland holographic gratings are fabricated with the same
proprietary technique as our low stray light plane gratings.
Good
efficiency
The sinusoidal groove profile of holographic gratings gives a better
overall performance than a triangular "blazed" profile. Though
a blazed concave grating may have higher efficiency at the grating centre,
other points on the surface are "off blaze", giving lower
efficiency.
Accurate
groove frequency
The groove frequency (at the grating centre) is accurate within ±0.2
grooves/mm of the nominal value. The gratings are holographically exposed
using optically flat wavefronts, ensuring straight and equispaced grooves.