An optical Etalon (also named Fabry–Pérot Etalon) was originally a Fabry–Pérot interferometer in the form of a transparent plate (usual made of fused silica) with parallel reflecting surfaces (solid Etalon). However, the term is often also used for Fabry–Pérots consisting of two mirrors with some air gap in between (air-spaced Etalon).
Figure 1: Tilted solid Etalon in a laser beam.
When inserted into a laser beam, an Etalon acts as an optical resonator (cavity), where the transmissivity varies approximately periodically with the optical frequency. (Some deviations from perfect periodicity result from chromatic dispersion.) In resonance, the reflections from the two surfaces cancel each other via destructive interference. The highest reflection losses and thus the lowest transmissivity occur in anti-resonance. The transmissivity versus frequency can be described with an Airy function, which approximately fits a simple sinusoidal function for not too high surface reflectivity.
The resonance effects occur even with some tilt (Figure 1), provided that the tilt angle is so small that the overlap of counter propagating waves is not significantly reduced. (That works well for a small Etalon thickness and a large beam radius.) The tilt angle can then be used to control the resonance frequencies. An Etalon can therefore be used as an adjustable optical filter, e.g. for tuning the wavelength of a laser.
The reflectivity of the Etalon's surfaces may simply result from the refractive index discontinuity between the Etalon material and air (Fresnel reflection) or may be modified with dielectric coatings.
By increasing the reflectivity, it is possible to increase the finesse, i.e., to sharpen the resonances without reducing the free spectral range.
The effective finesse of an Etalon may not reach the value which could be expected based on the surface reflectivities: it can be reduced, for example, if the reflecting surfaces are not perfectly parallel and flat. For high surface reflectivities, one may require an extremely high surface quality (low roughness) to realize the theoretically possible finesse. A reduced finesse can also result from using a too small or not properly collimated beam, a too large tilt angle, or a reduced beam quality.
Etern Optoelctronics are deliverying the Etalon series product to market, the typical specification is showing as below table.
Type |
Fabry–Pérot Etalon |
Thickness |
50um to 10mm |
Spectrum Range |
10GHz to 2000GHz |
Material |
Fused silica |
Parallelism |
λ/100 @ 633nm |
Flatness |
λ/200 @ 633nm |
Coating Wavelength |
350 to 2000nm |
Clear aperture |
∅1 to 10mm |
Additional information
For more information about Etern Etalon technology, visit Etern Optoelectronics website:
https://www.szetern.com, or email to: sales@szetern.com