Incoherent multiple internal reflection
The following figure illustrates the effects of incoherent multiple internal reflections on the energy flow through a finite thickness substrate. For a given optical substrate of finite thickness (t), absorption coefficient (α), and reflectivity from front and rear surfaces of (Ra-) and (Rb+), the amount of transmitted radiation traversing the first interface Ta+ will be (1-Ra+)Io, where Io is the intensity of the incident wave. After travelling through a distance (t) of the substrate the incident radiation is attenuated by
e-αt. The radiation therefore reaching the second interface (Ta-) is (1-Ra+)Ioe-αt. Due to reflection (Rb-) at the interface of the second surface, only the fraction given by
(1-Ra+)(1-Rb-)Ioe-αt will emerge. The amount internally reflected as Rb-(1-Rb-)Ioe-αt will become progressively more attenuated as a result of the multiple internal reflections becoming absorbed within the material or emerging as a negligible contribution compared to the first order reflectivity.

Analysis of the energy flow through a substrate of finite thickness inclusive of multiple internal reflections

Variation in transmission (Tab) vs absorption coefficient (α) for different refractive indices between 1.0-6.0 for a 1mm substrate

Variation in transmission (Tab) vs absorption coefficient for different thicknesses of Germanium in the range (0.5 - 3.0mm) at 10µm
Germanium absorption topography - plan view (thickness 1-6mm at 293K)

Fz Silicon absorption topography - plan view (thickness 1-6mm at 293K)

Zinc Sulphide absorption topography - plan view (thickness 1-6mm at 293K)
Zinc Selenide absorption topography - plan view (thickness 1-6mm at 293K)

Cadmium Telluride absorption topography - plan view (thickness 1-6mm at 293K)
Substrate optical theory
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