Semrock Master Catalog 2018
Semrock Master Catalog 2018
Semrock Master Catalog 2018
Create successful ePaper yourself
Turn your PDF publications into a flip-book with our unique Google optimized e-Paper software.
StopLine ® Single-notch Filter Common Specifications<br />
Property Value Comment<br />
Laser Line<br />
Blocking:<br />
Typical 50%<br />
Notch Bandwidth<br />
E- & U-grade > 6 OD<br />
E- & U-grade<br />
NBW = 55 × 10 –6 2<br />
× λ L<br />
+ 14 × 10 –3 ×λ L<br />
– 5.9<br />
e.g. 17 nm (600 cm –1 ) for 532.0 nm filter<br />
All other General Specifications are the same as the RazorEdge ® specifications on page 95.<br />
At the design laser wavelength;<br />
OD = - log 10<br />
(transmission)<br />
Full width at 50% transmission;<br />
λ L<br />
is design laser wavelength<br />
(NBW and λ L<br />
in nm)<br />
Maximum 50% Notch Bandwidth < 1.1 × NBW<br />
90% Notch Bandwidth < 1.3 × NBW Full width at 90% transmission<br />
Passband<br />
E-grade 350 –1600 nm Excluding notch<br />
U-grade from 0.75 × λ L<br />
to λ L<br />
/ 0.75<br />
λ L<br />
is design laser wavelength (nm)<br />
Average<br />
Passband<br />
Transmission<br />
E-grade > 80% 350 – 400 nm, > 93% 400 – 1600 nm Excluding notch<br />
U-grade > 90%<br />
Lowest wavelength is 330 nm for NF03-405E<br />
Passband Transmission Ripple < 2.5% Calculated as standard deviation<br />
Angle of Incidence 0.0° ± 5.0° See technical note on page 105<br />
Angle Tuning Range [1]<br />
- 1% of laser wavelength<br />
(- 5.3 nm or + 190 cm –1 for 532 nm filter)<br />
Wavelength “blue-shift” attained by<br />
increasing angle from 0° to 14°<br />
Laser Damage Threshold 1 J/cm 2 @ 532 nm (10 ns pulse width) Tested for 532 nm filter only (see page 108)<br />
Coating Type<br />
“Hard” ion-beam-sputtered<br />
Clear Aperture ≥ 22 mm For all optical specifications<br />
Outer Diameter 25.0 + 0.0 / - 0.1 mm Black-anodized aluminum ring<br />
Overall Thickness 3.5 ± 0.1 mm Black-anodized aluminum ring<br />
[1]<br />
For small angles q (in degrees), the wavelength shift near the laser wavelength is D l (nm) = - 5.0 × 10 –5 × l L<br />
× q 2 and the wavenumber<br />
shift is D(wavenumbers) (cm –1 ) = 500 × q 2 / l L<br />
, where l L<br />
(in nm) is the laser wavelength. See Technical Note on wavenumbers on page 101.<br />
PRODUCT NOTE<br />
Notch Filters<br />
Notch filters are ideal for applications that require nearly complete<br />
rejection of a laser line while passing as much non-laser light as possible.<br />
Hard-coated thin-film notch filters offer a superior solution due to their<br />
excellent transmission (> 90%), deep laser-line blocking (OD > 6) with a<br />
narrow notch bandwidth (~ 3% of the laser wavelength), environmental<br />
reliability, high laser damage threshold (> 1 J/cm 2 ), and compact format<br />
with convenient back-reflection of the rejected laser light. However,<br />
until now, the main drawback of standard thin-film notch filters has been<br />
a limited passband range due to the fundamental and higher-harmonic<br />
spectral stop bands (see red curve on graph at right).<br />
To achieve a wider passband than standard thin-film notch filters<br />
could provide, optical engineers had to turn to “holographic” or<br />
0<br />
400 500 600 700 800 900 1000 1100<br />
“Rugate” notch filters. Unfortunately, holographic filters suffer from<br />
Wavelength (nm)<br />
lower reliability and transmission (due to the gelatin-based, laminated<br />
structure), higher cost (resulting from the sequential production process), and poorer system noise performance and/or higher<br />
system complexity. Rugate notch filters, based on a sinusoidally varying index of refraction, generally suffer from lower<br />
transmission, especially at shorter wavelengths, and less deep notches.<br />
0<br />
<strong>Semrock</strong> E-grade StopLine notch filters offer a breakthrough in optical notch filter technology, bringing together all the<br />
advantages of hard-coated standard thin-film notch filters with the ultrawide passbands 2 that were previously possible only with<br />
holographic and Rugate notch filters. The spectral performance of the E-grade StopLine filters is virtually identical to that of<br />
3<br />
<strong>Semrock</strong>’s renowned U-grade StopLine filters, but with passbands that extend from the UV (< 350 nm) to the near-IR (> 1600 nm).<br />
Transmission (%)<br />
Optical Density<br />
100<br />
90<br />
80<br />
70<br />
60<br />
50<br />
40<br />
30<br />
20<br />
10<br />
1<br />
4<br />
5<br />
6<br />
NF03-532E<br />
NF01-532U<br />
Typical<br />
measured<br />
spectral data<br />
NF03-532E<br />
Typical<br />
measured<br />
spectral data<br />
NIR Filters Mirrors Polarizers<br />
Edge<br />
Filters<br />
Dichroic<br />
Beamsplitters<br />
Laser-line<br />
Filters<br />
Laser Diode<br />
Filters<br />
Notch<br />
Filters<br />
Lamp Clean-up<br />
Filters<br />
7<br />
490 500 510 520 530 540 550 560 570 580<br />
Wavelength (nm)<br />
103<br />
More