Edgepass Filters: Longpass and Shortpass
| ||Longpass Filters||Shortpass|
|Transmission Region||Cut-on λ to 2200 nm (Min)||0.7λ to Cut-off λ (Unless 0.7λ is < 400 nm, then 400 nm to Cut-off λ)|
|Rejection Region||200 nm to Cut-on λ||1.3 times Cut-off λ|
- Emission Filters in Fluorescence Applications
- Order Sorting Filters for Photometry
- Stray Light or Trim Filters to Eliminate any Unwanted Near-Band Radiation
- Raman Spectroscopy Filters
- Astronomy Applications
Thorlabs' longpass and shortpass filters are very useful for isolating regions of a spectrum. These edgepass filters feature durable dielectric coatings that withstand the normal cleaning and handling necessary when using any high-quality optical component. Their film construction is essentially a modified quarter-wave stack, using interference effects rather than absorption, to isolate their spectral bands (see the Specs tab for transmission information).
Unlike colored filter glass, the cut-on and cut-off wavelength of these filters will shift to a shorter wavelength as the angle of incidence is increased. As a rule of thumb, when the angle of incidence goes from 0° to 45°, the central wavlength shifts down by about 10%. This feature can be useful in applications where it is desirable to fine tune the location of the cut-on, or cut-off wavelength. In addition, our edgepass filters are hermetically sealed to provide maximum humidity protection, and they can be stacked to create a custom bandpass filter.
| ||Clicking on this symbol in the tables below will open a window showing transmission and optical density data for the corresponding filter.|
We do not recommend removing the filter from its mount, as the filter consists of several layers of glass that are held together with epoxy and the mounting ring. These glass layers are necessary to protect the dielectric coating from the atmosphere; exposure would significantly reduce the filter's transmission efficiency over time.
These longpass and shortpass filters are also available in kits. To request a quote for custom edgepass filters, please contact Tech Support. For applications with demanding wavefront requirements, such as imaging, please consider our premium edgepass filters.
| ||Longpass Filters||Shortpass Filters|
|Transmission Region||Cut-on λ to 2200 nm Mininmum||0.7λ to Cut-off λ (Unless 0.7λ is < 400 nm, Then 400 nm to Cut-off λ)|
|Transmission at Peak*||400-700 nm, 80% |
750-1000 nm, 75%
>1000 nm, 70%
|550-1000 nm, 80% |
<550 nm, 70%
|Cut-On or Cut-Off Tolerance |
(Δλ @ 50% of Peak)
|±3 nm (400 to 750 nm)|
±15 nm (800 to 1500 nm)
|±3 nm (450 to 750 nm)|
±15 nm (800 to 1000 nm)
|Rejection Region||200 nm to Cut-On||1.3 Times Cut-Off|
|Transmission in Rejection Region||0.01% abs. (OD = 4.0)||0.01% abs., 0.0001% avg. (OD = 4.0-6.0)|
|Cut-off Slope||3%, OD = 0.3 to OD = 4||4-5%, OD = 0.3 to OD = 4|
|Construction||Immersed Dielectric||Immersed Dielectric|
|Surface Quality (Scratch-Dig)||80/50 per Mil-0-13830A||80/50 per Mil-0-13830A|
|Substrate Material||Soda Lime or Equivalent||Soda Lime or Equivalent|
*For FEL0400, the Transmission at Peak from 450-2200 nm is 70%; for FEL0450, the Transmission at Peak from 400-2200 nm is 70%.
Optical Density Equation:
|Click to Enlarge
The number of layers shown in this schematic is not indicative of the number of layers in an actual bandpass filter. Also the drawing is not to scale.
Bandpass/Edgepass Filter Structure
A bandpass or edgepass filter is created by depositing layers of material on the surface of the substrate. Typically, there are several dielectric stacks separated by spacer layers. The dielectric stack is composed of a large number of alternating layers of low-index and high-index dielectric material. The thickness of each layer in the dielectric stack is λ/4, where λ is the central wavelength of the bandpass filter (i.e. the wavelength with the highest transmittance through the filter). The spacer layers are placed in between the dielectric stacks and have a thickness of (nλ)/2, where n is an integer. The spacer layers can be formed from colored glass, epoxy, dyes, metallic, or dielectric layers. A Fabry-Perot cavity is formed by each spacer layer sandwiched between dielectric stacks. The filter is mounted in an engraved metal ring for protection and ease of handling.
Filter Operation Overview
The constructive interference conditions of a Fabry-Perot cavity allow light at the central wavelength, and a small band of wavelengths to either side, to be transmitted efficiently, while destructive interference prevents the light outside the passband from being transmitted. However, the band of blocked wavelengths on either side of the central wavelength is small. In order increase the blocking range of the filter, materials with broad blocking ranges are used for or coated onto the spacer layers and the substrate. Although these materials effectively block out of band transmission of incident radiation they also decrease the transmission through the filter in the passband.
FB800-10 and FB800-40 filters were used to make the measurement that resulted in the plot above.
An engraved arrow on the edge of the filter is used to indicate the recommended direction for the transmission of light through the filter. Although the filter will function with either side facing the source, it is better to place the coated side toward the source. This will minimize any thermal effects or possible thermal damage that blocking intense out-of-band radiation might cause due to the absorption of the out-of-band radiation by the substrate or colored glass filter layers. The plot to the right was made by illuminating the filter with a low intensity broadband light and measuring the transmission as a function of wavelength. The plot shows that the transmission direction through the filter has very little effect on the intensity and the spectrum of the light transmitted through the filter. The minimal variation between the forward and backward traces is most likely due to a small shift in the incident angle of the light on the filter introduced when the filter was removed, flipped over, and replaced in the jig.
The filter is intended to be used with collimated light normally incident on the surface of the filter. For uncollimated light or light striking the surface and an angle not normally incident to the surface the central wavelength (wavelength corresponding to peak transmission) will shift toward lower wavelengths and the shape of the transmission region (passband) will change. As a rule of thumb, when the angle of incidence goes from 0° to 45°, the central wavlength shifts down by about 10%. This feature can be useful in applications where it is desirable to fine tune the location of the cut-on, or cut-off wavelength.
The central wavelength of the bandpass filter can be tuned slightly (~1 nm over the operating range of the filter) by changing the temperature of the filter. This is primarily due to the slight thermal expansion or contraction of the layers.