Sellmeier equation
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In optics, the Sellmeier equation is an empirical relationship between refractive index n and wavelength λ for a particular transparent medium. The usual form of the equation for glasses is:
- [n^2(\lambda) = 1 + \frac+ \frac+ \frac]
The equation is used to determine the dispersion of light in a refracting medium. A different form of the equation is sometimes used for certain types of materials, e.g. crystals.
The equation was deduced in 1871 by W. Sellmeier, and was a development of the work of Augustin Cauchy on Cauchy's equation for modelling dispersion.
As an example, the coefficients for a common borosilicate crown glass known as BK7 are shown below:
| Coefficient | Value |
|---|---|
| B1 | 1.03961212 |
| B2 | 2.31792344x10−1 |
| B3 | 1.01046945 |
| C1 | 6.00069867x10−3 μm2 |
| C2 | 2.00179144x10−2 μm2 |
| C3 | 1.03560653x102 μm2 |
The Sellmeier coefficients for many common optical glasses can be found in the Schott Glass catalogue.
In its most general form, the Sellmeier equation is given as:
- [n^2(\lambda) = 1 + \sum_i \frac]
At long wavelengths far from the absorption peaks, the value of n tends to:
- [\beginn \approx \sqrt \approx \sqrt\end]
The Sellmeier equation can also be given in another form:
- [n^2(\lambda) = A + \frac + \frac]
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