Introduction | Types of Planar Etalons | Fabry-Perot Etalon Theory

Planar Etalon Theory

The equation for the transmission of an ideal etalon, an Airy Function, is

where

T = transmission

R = reflectivity of the mirrors

Φ = the roundtrip phase change of the light ray

If any phase change at the mirror surfaces is ignored then

where

l = the wavelength of the light

n = the index of refraction of the material between the mirrors

d = the distance between the mirrors

q = the angle of the incoming light beam

The above figure plots the etalon spectral transmission. The distance between adjacent peaks is the Free Spectral Range (D) and the width (FWHM) of each peak is the resolution (d). The Free Spectral Range can be written three ways:

Another useful concept for etalons is the finesse (F). This dimensionless parameter is the ratio of the free spectral range to the peak width.

For an ideal etalon, only the mirror reflectivity determines the finesse.

Imperfections in the etalon such as not-perfect flatness and parallelism will degrade the finesse. TecOptics includes the various imperfections into our etalon design calculations so we guarantee all quoted specifications.

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