Cut-on/Cut-off wavelengths available from 400 nm to 1000 nm
Blocked to X-ray (LWP) and 1200 nm (SWP)
Product Description
Our short and long-wave pass filters have a steep transition between the region of transmission and reflection much steeper than colored glass filters. Both the short and long-wave pass filters have out-of-band rejection ³OD 3 to X-ray (for LWP) and to 1200nm (for SWP). Typical transmission is ³80% for long-wave pass and ³65% for short-wave pass filters. These filters are available individually and in sets.
Product Detail
These short and
long-wave pass filters have a very steep transition between
the region of transmission and reflection — much steeper
than colored glass filters. They have a hard, dielectric
filter coating using interference effects rather than
absorption to isolate the spectral bands. Unlike colored
glass filters, the center wavelength will shift to shorter
wavelengths with an increase in angle of incidence (see
Laser Line Filters for formula). This can be useful for
tilt tuning these filters to your exact wavelength. A custom
bandpass filter with excellent performance can be
constructed using a combination of a short-wave pass and a
long-wave pass filter.
These filters are available individually and in sets. The
sets consist of one of each, of either the short or
long-wave pass filters listed. They are shipped in a
hardwood box for convenient storage and protection.
Newport long and short-wave pass filters are manufactured
using methods and materials designed to deliver the highest
spectral performance while providing a robust construction
capable of withstanding variable climatic conditions.
Transition slopes of £6% are
established by a dielectric thin-film coating. This coating
is optimized to provide a wide band of high average
transmission. Blocking to X-ray on long wave pass filters,
and to 1200 nm on short wave pass filters, is accomplished
by a combination of reflection from dielectric thin-film
coatings, and absorption from filter glasses. We manufacture
these filters using scribed and laminated construction. This
method provides a glass-epoxy-glass seal around the
perimeter of the filter, which prevents the ingress of
moisture into the thin-film filter elements. The resulting
filter assemblies deliver excellent field life in harsh
climatic conditions.
These filters are available individually and in sets. The
sets consist of one of each of either the short or long-wave
pass filters listed. They are shipped in a hardwood box for
convenient storage and protection.
In addition to using these filters in the traditional
manner, they can be used to create custom bandpass filters
with excellent performance by using a combination of a
short-wave pass and a long-wave pass filter in series.
Specifications
Minimum
Active Area
20.2 mm
Surface
Quality
80-50
scratch-dig; F/F per MIL-F-48616
Diameter
25.4
+0/-0.5 mm
Thickness
2.0 to 7.6
mm
Angle of
Incidence
Normal
Tav
Minimum Average Transmittance
Short Wave
Pass: 65%
Long Wave Pass: 80%
Rejection
(spectral)
Short Wave
Pass: 1.2lc
to 1200 nm, =0.1% T or =10-3
Long Wave Pass: X-Ray to 0.85 lc,
=0.1% T or =10-3
Slope*
£6%
where slope%=100% (l80%Tpk-l5%Tabs)/l5%Tabs
Effective
Index of Refraction ne
1.7
Wavelength
Shift with Temperature
Short Wave
Pass: 0.02 nm/°C
Long Wave Pass: 0.025 nm/°C
Humidity
Per
MIL-STD-810E, Method 507.3, Procedure III Modified to 7
cycles
Temperature
Range
-50°C to +
100 °C
Cleaning
Non-abrasive method, acetone or isopropyl alcohol
on lens tissue recommended
Short-Wave Pass Filters
Model
lc Cut-On Wavelength
@ 50% of Tpk (nm)
Minimum Spectral range of
Transmittance l1 to l2(nm)
Oriel Model
Corion Model
10SWF-450-B
450 ± 5
415–440
57371
LS-450-F
10SWF-500-B
500 ± 5
415–490
57373
LS-500-F
10SWF-550-B
550 ± 5
415–540
57375
LS-550-F
10SWF-600-B
600 ± 5
415–590
57377
LS-600-F
10SWF-650-B
650 ± 5
415–640
57379
LS-650-F
10SWF-700-B
700 ± 6
440–685
57381
LS-700-F
10SWF-750-B
750 ± 6
475–735
57383
LS-750-F
10SWF-800-B
800 ± 6
475–785
57385
LS-800-F
10SWF-850-B
850 ± 6
475–835
57387
LS-850-F
10SWF-900-B
900 ± 7
475–880
57389
LS-900-F
10SWF-950-B
950 ± 7
475–930
57391
LS-950-F
10SWF-1000-B
1000 ± 7
475–980
57393
LS-1000-F
Long-Wave Pass Filters
Model
lc Cut-On Wavelength
@ 50% of Tpk (nm)
Minimum Spectral range of
Transmittance l1 to l2(nm)
Oriel Model
Corion Model
10LWF-400-B
400 ± 5
410–1200
57345
LL-400-F
10LWF-450-B
450 ± 5
460–1200
57347
LL-450-F
10LWF-500-B
500 ± 5
510–1200
57349
LL-500-F
10LWF-550-B
550 ± 5
560–1200
57351
LL-550-F
10LWF-600-B
600 ± 5
610–1200
57353
LL-600-F
10LWF-650-B
650 ± 5
660–1200
57355
LL-650-F
10LWF-700-B
700 ± 6
715–1200
57357
LL-700-F
10LWF-750-B
750 ± 6
765–1200
57359
LL-750-F
10LWF-800-B
800 ± 6
815–1200
57361
LL-800-F
10LWF-850-B
850 ± 6
865–1200
57363
LL-850-F
10LWF-900-B
900 ± 7
920–1200
57365
LL-900-F
10LWF-950-B
950 ± 7
970–1200
57367
LL-950-F
10LWF-1000-B
1000 ± 7
1020–2200
57369
LL-1000-F
*Slope is given by: | [ {l (80%Tpk) - l (5%Tpk)} ÷ l (5%Tpk)] | × 100
Founded in 1969, Newport Corporation
is a pioneering single-source solutions provider of laser and
photonics components to the leaders in scientific research, life and health
sciences, microelectronics,industrial manufacturing, and homeland security markets.