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 Colored-Glass Alternative Filters
 
 Colored Glass Filters

 
 
  • RoHS compliant (unconditional)
  • Steep transitions from blocking to transmission
  • Low autofluorescence
  • High transmission - >90% average (typical)
  • Excellent blocking - >5 OD
  • Patented Stabilife® coatings
  • Wavelength stability in any environment
  • Exceptional durability
  • 34 Standard cut-on wavelengths in 4 standard sizes
  • Custom cut-on wavelength availability from 225 to 1000 nm
Product Description

Newport's patent-pending Colored-Glass Alternative filters are constructed using optical thin-film coating technology. Using Newport's patented Stabilife® coating technology, many layers of refractory metal oxide film are deposited under vacuum in a precise sequence, defining the spectral signature of the filters. Unlike Colored-Glass filters which rely upon absorption to create the filter's spectral response, CGA filters utilize optical interference phenomena to create wide bands of very-high reflectance to create the blocking region of the filters, and wide bands of very-low reflectance to create the transmission bands of the filters.

Using optical interference coatings to create longwave pass filters provides some distinct advantages over using absorptive colored-glass. Transition slopes between the rejection or blocking band and the transmission band can be made much steeper using interference coatings. On average, CGA filter slopes are 3 times steeper than the transition slopes of corresponding Colored-Glass filters. The spectral response of CGA filters are not dependent upon thickness of the the filters. By contrast, the degree of rejection or blocking and the cut-on wavelength of a filter constructed using colored-glass is directly dependent upon its thickness. The relationship between the thickness of the absorbing colored-glass is explained by the Bouguer-Lambert Law (also known as the Lambert Law) which defines the effect on the intensity of light transmitted through an absorbing substance in respect to its thickness. This feature allows Colored-Glass Alternative filters to be manufactured using very thin substrates while maintaining the required depth of blocking, enabling their use in a variety of applications where "small & thin" are desirable features. Filters manufactured using interference coatings also provide an advantage over colored-glass filters in their ability to provide any desired cut-on wavelength without incurring the time and expense of developing custom-formulated glass melts to achieve the desired cut-on wavelength. An equally important advantage of CGA filters is their formulation from 100% environmentally safe materials. This attribute stands in contrast to many colored-glass longwave pass filters that rely upon the use of Lead and Cadmium compounds to achieve their spectral signature.

In addition to the abovementioned benefits of Colored-Glass Alternative filters over colored-glass filters, the cut-on wavelength of CGA filters can be tuned to slightly shorter wavelengths by positioning the filter at off-normal incidence to the source of illumination. This capability is a common phenomena associated with thin-film optical interference coatings.

Our catalog offering of Colored-Glass Alternative filters is a series of fully-blocked, all-dielectric longwave pass filters at thirty-four (34) different cut-on wavelengths. The group of standard wavelengths was developed as a compilation of the cut-on wavelengths of longwave pass filter glasses currently offered by the major manufacturers of colored-glass filters, as well as some wavelengths that have been discontinued by these manufacturers. Four (4) different sizes are available at each wavelength: ½" diameter, 1" diameter, 2" square, and 6½" square. Standard CGA filters are supplied with a thickness of 1.1 mm.

In addition to our standard CGA products, we routinely provide custom products based upon the basic product concept and designs. Custom capabilities are discussed in the section following the pages devoted to our catalog products.



Product Detail

 

Angle of Incidence Effects

The cut-on wavelength of Newport Stabilife® Colored-Glass Alternative filters will slightly shift lower in wavelength with an increase in the angle of incident collimated light. The amount of wavelength shift is dependent upon the incident angle and the effective index (ne) of the filter. This feature can be very useful in research applications by being able to custom tune a CGA filter to a specific desired wavelength. The following formula may be used to determine the wavelength shift of a filter in random polarized collimated light:

λΘ = λ0 (ne2 – sin2 Θ)½ (ne)-1

where

λΘ = Cut-on wavelength at Θ° angle of incidence

λ0 = Cut-on wavelength at 0° angle of incidence

Θ = Angle of incident light off normal incidence

ne = Effective index of refraction; specified as a numerical value derived from the indices of the thin film layers of the CGA filter

 


 

Example of Angle of Incidence Effects on a typical CGA filter


Typical angle of incidence effects for CGA-345 filters with effective index of refraction (ne) of 2.147
 
 Incident Radiation  Effective Cut-on λ at 50% Transmittance
 Collimated @ Normal Incidence  345.0 nm
 Collimated @ 10° off-normal (Random POL)  343.9 nm
 Collimated @ 10° off-normal (P-POL)  343.4 nm
 Collimated @ 10° off-normal (S-POL)  344.2 nm
 Collimated @ 20° off-normal (Random POL)  340.3 nm
 Collimated @ 20° off-normal (P-POL)  338.8 nm
 Collimated @ 20° off-normal (S-POL)  341.8 nm

 

Cone-Angle Effects

In the preceding example, the wavelength changes were modeled under the assumption that the incident light was collimated. In some applications, the incident light is presented at the filter in a convergent or divergent cone. The cone is made up of many light rays at various angles ranging from normal incidence to the extreme angle defining the full cone. The effect of this collection of rays is a weighted average of incident light, producing a wavelength shift toward shorter wavelengths that is smaller than the shift that would be produced if collimated light was presented to the filter at the extreme angle of the full cone.


 

Example of Cone-Angle Effects on a typical CGA Filter

The following table illustrates the theoretical blue-shift that would result in the cut-on wavelength of a typical Colored-Glass Alternative filter when illuminated with incident radiation in a 10° full-cone and a 20° full-cone.

CGA-345
 Incident Radiation  Effective Cut-on λ at 50% Transmittance
 Collimated @ Normal Incidence  345.0 nm
 10° Full-Cone  344.9 nm
 20° Full-Cone  344.4 nm

 

Physical Properties

Manufactured using Newport's patented Stabilife® coating technology, our Colored-Glass Alternative (CGA) filters deliver exceptional durability in environments ranging from the most benign conditions found in a typical research laboratory to the most extreme conditions such as those found in nuclear reactors or desert battlefields.

Abrasion Resistance, Adhesion, & Humidity Resistance

CGA filters have been qualified for adhesion using the snap tape test specified in MIL-C-48497, for abrasion resistance using the eraser test specified in MIL-C-675, and for humidity resistance using the aggravated test specified in MIL-STD-810E. These tests are commonly used as benchmarks for determining the robustness of thin film coatings.

Stain Resistance

CGA filters have been evaluated for stain resistance using the Acid Resistance test set forth in ISO 8424. This test is used to to determine the surface change that results from exposure to a strong acidic substance. The surface is exposed to a Nitric Acid solution (0.5M/l) having a pH of 0.3 ± 0.05. Testing is conducted to determine the amount of time needed to etch into the surface to a depth of 0.1 µm. Newport's CGA filters have been confirmed to meet an SR1 rating which corresponds to greater than 100 hours of exposure. Since CGA filters are constructed of very thin layers of vacuum-deposited thin-film coating, an etch depth of 0.1 µm would likely result in a significant change in the spectral performance of the filter. No spectral change was evident after testing indicating an absence of any significant etching after the 100 hour exposure.

Solubility

The extreme hardness of the Stabilife® coatings used to manufacture Colored-Glass Alternative Filters allows these filters to be subjected to normal and severe weather conditions as well as to the repeated handling and cleaning that is commonplace for filters that are used in a lab environment, without sustaining any surface degradation. Unlike some Colored-Glass Filters that can suffer surface damage from prolonged exposure to rain or submersion in water, CGA filters maintain their clarity and spectral performance under such extreme conditions.

Optical Radiation

Stabilife® coatings used to manufacture our CGA filters have been deployed in applications where they are exposed intense ultraviolet and high energy visible radiation with no change in spectral performance after prolonged exposure. These filters have also been evaluated for Laser Damage Threshold using a frequency-doubled Nd:YAG laser operating at 532 nm with a pulse width of 10 ns and a repetition rate of 20 Hz. Typical damage threshold values exceed 1.0 J/cm2 .

Extreme Temperature

Colored-Glass Alternative filters are qualified for use at continuous operating temperatures between -100°C and +400°C.

Restrictions on Hazardous Substances (RoHS)

The proliferation of electronics in virtually every part of the average person's life has brought many capabilities and conveniences that were unimaginable only a short time ago. However, as is often the case, along with the many benefits that these technological advances have conferred, some unintended negative consequences have resulted from this proliferation in the form of potential environmental harm from the disposal of waste electronics. In recognition of the present and potential risks to the health of our society as a result of the disposal of waste electronic equipment, the European Union (EU) has developed regulations to reduce the amount of potential pollutants used in manufactured products and to control the disposal of products that can not be manufactured without containing the certain targeted potential pollutants. The principal guiding regulations are the DIRECTIVE 2002/95/EC OF THE EUROPEAN PARLIAMENT AND OF THE COUNCIL of 27 January 2003 on the restriction of the use of certain hazardous substances in electrical and electronic equipment(RoHS), and the DIRECTIVE 2002/96/EC OF THE EUROPEAN PARLIAMENT AND OF THE COUNCIL of 27 January 2003 on waste electrical and electronic equipment (WEEE).

The RoHS regulation specifies that Member States of the European Union shall ensure that, from 1 July 2006, new electrical and electronic equipment put on the market does not contain lead, mercury, cadmium, hexavalent chromium, polybrominated biphenyls (PBB) or polybrominated diphenyl ethers (PBDE). During the development of these regulations, the council recognized and made provisions for the fact that the complete elimination of these named materials could involve significant scientific development and therefore, established provisions for granting exemptions for a period of four years to allow sufficient time for the scientific development enabling the elimination of the hazardous substances to be completed.

The relevance of these regulations to optical components lies in the fact that many electronics-based instruments employ optical technology as a key enabler. Just as all of the electronic components of these instruments are subject to the RoHS and WEEE regulations, so are all of the other components of the instrument including the optical elements. Many electronic-based instruments have employed colored-glass filters containing Lead and Cadmium compounds. Exemption status was established for Optical and Filter Glasses containing Lead and Cadmium for a period of four (4) years. The regulation requires that four years after an item is added to the list, a review is to be conducted with the aim of considering the removal of the component/s from the list of exempted materials.

Unlike several Yellow, Orange, and Red Colored-Glass filters, Newport's Colored-Glass Alternative filters are fully compliant with RoHS regulations They do not rely on a exemption and therefore, are not subject to the uncertainty of the review process.

Specifications:

RoHS Status  Fully compliant (without 4-year exemption granted to non-compliant colored-glass filters)
 Standard Sizes  0.500" dia. ± 0.005"; 1.000" dia. ± 0.005"; 2.000" sq. ± 0.010"; 6.500" sq. ± 0.010";
 Active Area  ≥90% of filter size with film to the edge
 Thickness  1.1 mm ± 0.1 mm
 Surface Quality  F/F (80/50) per MIL-F-48616
 Coating Abrasion Resistance, Adhesion, & Hardness  MIL-C-48497
 Coating Humidity Resistance  MIL-STD-810, Method 507.3, Procedure III, Modified to 40 cycles
 Coating Operating Temperature Range  -100 º C to 400 º C
 Chemical Resistance  SR Class 1.0 per ISO 8424
 Laser Damage Threshold  ≥ 1J/cm2 (typical) tested at 532 nm, Pulse width 10 ns, Repetition rate 20Hz
 Cleaning  Non-abrasive method, acetone or isopropyl alcohol on lens tissue recommended
 Cut-on Wavelength Tolerance  ± 5 nm (typical); (± 6 nm typical for NIR wavelengths)
 Transmittance  ≥ 90% average (typical)
 Range of Transmittance  λ of 90% Transmission to 2500 nm
 Spectral Blocking  ≥OD5 to 200 nm (typical)

 

Spectral Specifications
 Model
0.5 in. dia.
 Model
1 in. dia.
 Model
2 in. sq.
 Model
6.5 in. sq.
 Cut-on/Cut-off Wavelength (nm)  λ @ 90% Transmission  λ @ OD 5  Effective Index of Refraction ne
 5CGA-225  10CGA-225  20CGA-225  65CGA-225  225 nm  ≤ 260 nm  N/A  2.242
 5CGA-280  10CGA-280  20CGA-280  65CGA-280  280 nm  ≤ 365 nm  ≥ 250 nm  1.943
 5CGA-295  10CGA-295  20CGA-295  65CGA-295  295 nm  ≤ 322 nm  ≥ 270 nm  3.856
 5CGA-305  10CGA-305  20CGA-305  65CGA-305  305 nm  ≤ 325 nm  ≥ 285 nm  2.725
 5CGA-320  10CGA-320  20CGA-320  65CGA-320  320 nm  ≤ 340 nm  ≥ 300 nm  2.243
 5CGA-335  10CGA-335  20CGA-335  65CGA-335  335 nm  ≤ 345 nm  ≥ 317 nm  2.079
 5CGA-345  10CGA-345  20CGA-345  65CGA-345  345 nm  ≤ 367 nm  ≥ 326 nm  2.147
 5CGA-360  10CGA-360  20CGA-360  65CGA-360  360 nm  ≤ 367 nm  ≥ 338 nm  2.085
 5CGA-375  10CGA-375  20CGA-375  65CGA-375  375 nm  ≤ 390 nm  ≥ 345 nm  2.454
 5CGA-385  10CGA-385  20CGA-385  65CGA-385  385 nm  ≤ 405 nm  ≥ 360 nm  2.321
 5CGA-395  10CGA-395  20CGA-395  65CGA-395  395 nm  ≤ 410 nm  ≥ 370 nm  2.176
 5CGA-400  10CGA-400  20CGA-400  65CGA-400  400 nm  ≤ 415 nm  ≥ 375 nm  2.174
 5CGA-420  10CGA-420  20CGA-420  65CGA-420  420 nm  ≤ 435 nm  ≥ 390 nm  2.176
 5CGA-435  10CGA-435  20CGA-435  65CGA-435  435 nm  ≤ 450 nm  ≥ 400 nm  1.966
 5CGA-455  10CGA-455  20CGA-455  65CGA-455  455 nm  ≤ 470 nm  ≥ 420 nm  2.054
 5CGA-475  10CGA-475  20CGA-475  65CGA-475  475 nm  ≤ 490 nm  ≥ 440 nm  1.948
 5CGA-495  10CGA-495  20CGA-495  65CGA-495  495 nm  ≤ 510 nm  ≥ 455 nm  1.853
 5CGA-515  10CGA-515  20CGA-515  65CGA-515  515 nm  ≤ 530 nm  ≥ 485 nm  1,856
 5CGA-530  10CGA-530  20CGA-530  65CGA-530  530 nm  ≤ 545 nm  ≥ 495 nm  1.854
 5CGA-550  10CGA-550  20CGA-550  65CGA-550  550 nm  ≤ 565 nm  ≥ 515 nm  1.861
 5CGA-570  10CGA-570  20CGA-570  65CGA-570  570 nm  ≤ 585 nm  ≥ 535 nm  1.856
 5CGA-590  10CGA-590  20CGA-590  65CGA-590  590 nm  ≤ 605 nm  ≥ 555 nm  1.855
 5CGA-610  10CGA-610  20CGA-610  65CGA-610  610 nm  ≤ 625 nm  ≥ 575 nm  1.854
 5CGA-630  10CGA-630  20CGA-630  65CGA-630  630 nm  ≤ 645 nm  ≥ 595 nm  1.856
 5CGA-645  10CGA-645  20CGA-645  65CGA-645  645 nm  ≤ 660 nm  ≥ 615 nm  1.778
 5CGA-665  10CGA-665  20CGA-665  65CGA-665  665 nm  ≤ 680 nm  ≥ 630 nm  1.831
 5CGA-695  10CGA-695  20CGA-695  65CGA-695  695 nm  ≤ 710 nm  ≥ 645 nm  1.853
 5CGA-715  10CGA-715  20CGA-715  65CGA-715  715 nm  ≤ 730 nm  ≥ 665 nm  1.777
 5CGA-760  10CGA-760  20CGA-760  65CGA-760  760 nm  ≤ 775 nm  ≥ 705 nm  1.856
 5CGA-780  10CGA-780  20CGA-780  65CGA-780  780 nm  ≤ 795 nm  ≥ 710 nm  1.776
 5CGA-800  10CGA-800  20CGA-800  65CGA-800  800 nm  ≤ 815 nm  ≥ 730 nm  1.855
 5CGA-830  10CGA-830  20CGA-830  65CGA-830  830 nm  ≤ 845 nm  ≥ 755 nm  1.775
 5CGA-850  10CGA-850  20CGA-850  65CGA-850  850 nm  ≤ 865 nm  ≥ 775 nm  1.778
 5CGA-1000  10CGA-1000  20CGA-1000  65CGA-1000  1000 nm  ≤ 1030 nm  ≥ 860 nm  1.776

 

Custom Capability

Newport's Colored-Glass Alternative filters were originally developed for custom and OEM applications either as alternatives to a Colored-Glass filter that utilized non-RoHS compliant material in it formulation, as replacements of a Colored-Glass filter that had been discontinued by one of the major Colored-Glass filter manufacturers, or as a new product to fill a gap in the wavelength offering of the major Colored-Glass filter manufacturers. The versatility of our coating processes and equipment support our ability to offer unlimited combinations of wavelength, size, shape, thickness, optical figure, surface quality, etc.. In the table that follows, we have listed some of the principle capability specifications for CGA filters Please provide your detailed requirements to our technical sales team and allow us to engineer the exact solution to meet your application.

Custom Capability Specifications
 RoHS Status  Fully compliant (without 4-year exemption granted to non-compliant colored-glass filters)
 Passband Transmittance  ≥90% average (typical)
 Cut-on Wavelength Availability  300 - 1000 nm
 Spectral Blocking  ≥ 5 OD
 Surface Quality  F/F (80/50) per MIL-F-48616 (typical)
 Coating Hardness  MIL-C-48497
 Coating Abrasion Resistance  MIL-C-48497
 Coating Adhesion  MIL-C-48497
 Coating Humidity Resistance  MIL-STD-810, Method 507.3, Procedure III, Modified to 40 cycles
 Coating Operating Temperature Range  -100 º C to 400 º C
 Chemical Resistance  SR Class 1.0 per ISO 8424
 Filter Size Range  1.0 mm sq. to 380 mm dia.
 Filter Thickness  1.1 mm (typical)

 

 

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.
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