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[[File:Sellmeier-equation.svg|thumb|right|Refractive index vs. wavelength for [[BK7 glass]], showing measured points (blue crosses) and the Sellmeier equation (red line).]]
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The '''Sellmeier equation''' is an [[empirical relationship]] between [[refractive index]]  and [[wavelength]] for a particular [[transparency (optics)|transparent]] [[optical medium|medium]]. The equation is used to determine the [[dispersion (optics)|dispersion]] of [[light]] in the medium.
 
It was first proposed in 1871 by Wilhelm Sellmeier, and was a development of the work of [[Augustin Louis Cauchy|Augustin Cauchy]] on [[Cauchy's equation]] for modelling dispersion.
 
==The equation==
The usual form of the equation for glasses is
 
:<math>
n^2(\lambda) = 1
+ \frac{B_1 \lambda^2 }{ \lambda^2 - C_1}
+ \frac{B_2 \lambda^2 }{ \lambda^2 - C_2}
+ \frac{B_3 \lambda^2 }{ \lambda^2 - C_3},
</math>
 
where ''n'' is the refractive index, ''λ'' is the wavelength, and ''B''<sub>1,2,3</sub> and ''C''<sub>1,2,3</sub> are experimentally determined ''Sellmeier [[coefficient]]s''.<ref>[http://www.us.schott.com/advanced_optics/english/download/schott_tie-29_refractive_index_v3_jan_2007_us.pdf Refractive index and dispersion]. Schott technical information document TIE-29 (2007).</ref> These coefficients are usually quoted for λ in [[micrometre]]s. Note that this λ is the vacuum wavelength, not that in the material itself, which is λ/''n''(λ). A different form of the equation is sometimes used for certain types of materials, e.g. [[crystal]]s.
 
As an example, the coefficients for a common [[borosilicate glass|borosilicate]] [[Crown glass (optics)|crown glass]] known as ''BK7'' are shown below:
{| class="wikitable"
|-
! Coefficient !! Value
|-
| B<sub>1</sub> || 1.03961212
|-
| B<sub>2</sub> || 0.231792344
|-
| B<sub>3</sub> || 1.01046945
|-
| C<sub>1</sub> || 6.00069867×10<sup>&minus;3</sup> μm<sup>2</sup>
|-
| C<sub>2</sub> || 2.00179144×10<sup>&minus;2</sup> μm<sup>2</sup>
|-
| C<sub>3</sub> || 1.03560653×10<sup>2</sup> μm<sup>2</sup>
|}
 
The Sellmeier coefficients for many common optical materials can be found in the online database of [http://refractiveindex.info RefractiveIndex.info].
 
For common optical glasses, the refractive index calculated with the three-term Sellmeier equation deviates from the actual refractive index by less than 5×10<sup>−6</sup> over the wavelengths range<ref>http://oharacorp.com/o2.html</ref> of 365&nbsp;nm to 2.3&nbsp;µm, which is of the order of the homogeneity of a glass sample.<ref>http://oharacorp.com/o7.html</ref> Additional terms are sometimes added to make the calculation even more precise. In its most general form, the Sellmeier equation is given as
:<math>
n^2(\lambda) = 1 + \sum_i \frac{B_i \lambda^2}{\lambda^2 - C_i},
</math>
with each term of the sum representing an [[absorption (optics)|absorption]] resonance of strength ''B''<sub>i</sub> at a wavelength √''C''<sub>i</sub>. For example, the coefficients for BK7 above correspond to two absorption resonances in the [[ultraviolet]], and one in the mid-[[infrared]] region. Close to each absorption peak, the equation gives non-physical values of ''<math>n^2</math>''=±∞, and in these wavelength regions a more precise model of dispersion such as [[Helmholtz dispersion|Helmholtz's]] must be used.
 
If all terms are specified for a material, at long wavelengths far from the absorption peaks the value of ''n'' tends to
:<math>\begin{matrix}
n \approx \sqrt{1 + \sum_i  B_i } \approx \sqrt{\varepsilon_r}
\end{matrix},</math>
where ε<sub>r</sub> is the relative [[dielectric constant]] of the medium.
 
The Sellmeier equation can also be given in another form:
:<math>
n^2(\lambda) = A + \frac{B_1}{\lambda^2 - C_1} + \frac{ B_2 \lambda^2}{\lambda^2 - C_2}.
</math>
Here the coefficient ''A'' is an approximation of the short-wavelength (e.g., ultraviolet) absorption contributions to the refractive index at longer wavelengths. Other variants of the Sellmeier equation exist that can account for a material's refractive index change due to [[temperature]], [[pressure]], and other parameters.
 
==Coefficients==
{| class="wikitable" style="text-align:center"
|+ Table of coefficients of Sellmeier equation<ref>http://cvimellesgriot.com/products/Documents/Catalog/Dispersion_Equations.pdf</ref>
|-
!Material||B<sub>1||B<sub>2||B<sub>3||C<sub>1||C<sub>2||C<sub>3
|-
|[[borosilicate glass|borosilicate]] [[glass|crown glass]]<br>(known as ''BK7'')||1.03961212||0.231792344||1.01046945||6.00069867×10<sup>&minus;3</sup>µm<sup>2</sup>|| 2.00179144×10<sup>&minus;2</sup>µm<sup>2</sup>||1.03560653×10<sup>2</sup>µm<sup>2</sup>
|-
|sapphire<br>(for [[ordinary wave]])||1.43134930||0.65054713||5.3414021||5.2799261×10<sup>&minus;3</sup>µm<sup>2</sup>|| 1.42382647×10<sup>&minus;2</sup>µm<sup>2</sup>||3.25017834×10<sup>2</sup>µm<sup>2</sup>
|-
|sapphire<br>(for [[extraordinary wave]])||1.5039759||0.55069141||6.5927379||5.48041129×10<sup>&minus;3</sup>µm<sup>2</sup>|| 1.47994281×10<sup>&minus;2</sup>µm<sup>2</sup>||4.0289514×10<sup>2</sup>µm<sup>2</sup>
|-
|[[Fused quartz|fused silica]]||0.696166300||0.407942600||0.897479400||4.67914826×10<sup>&minus;3</sup>µm<sup>2</sup>|| 1.35120631×10<sup>&minus;2</sup>µm<sup>2</sup>||97.9340025&nbsp;µm<sup>2</sup>
|}
 
== See also ==
*[[Cauchy's equation]]
*[[Kramers–Kronig relation]]
 
==References==
<references />
*W. Sellmeier, Zur Erklärung der abnormen Farbenfolge im Spectrum einiger Substanzen, ''Annalen der Physik und Chemie'' '''219''', 272-282 (1871).
 
==External links==
*[http://RefractiveIndex.INFO/ RefractiveIndex.INFO] Refractive index database featuring Sellmeier coefficients for many hundreds of materials.
*[http://www.calctool.org/CALC/phys/optics/sellmeier A browser-based calculator giving refractive index from Sellmeier coefficients.]
*[http://gallica.bnf.fr/ark:/12148/cb34462944f/date Annalen der Physik] - free Access, digitized by the French national library
 
[[Category:Optics]]
[[Category:Equations]]

Revision as of 23:04, 22 February 2014

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