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Sellmeier formula
modelname
Sellmeier
Real part of dielectric function is described by two parameters \(B_1, \lambda_1\). Imaginary part is zero:
$$
\varepsilon_{r} = 1 + \frac{B_1 \lambda^2 }{ \lambda^2 - \lambda_1^2} \,.
$$
attributes
-
A - Adds parameter \(A\).
-
eV - Parameterization using \(N_1\) and \(E_1\) instead \(B_1\) and \(\lambda_1\):
$$
\varepsilon_r = A + \frac{2}{\pi} \frac{N_1}{E_1^2 - E^2} \,.
$$
-
number_of_terms - Adds terms and corresponding parameters \(B_2, \lambda_2, \dots\)
$$
\varepsilon_r = A + \frac{B_1 \lambda^2 }{ \lambda^2 - \lambda_1^2} + \frac{B_2 \lambda^2 }{\lambda^2 - \lambda_2^2} + \dots \,.
$$
Example
media:
f = Sellmeier:A:2
newAD2> par
Af = 1 fixed [1,inf)
B1f = 1 fixed [0,inf)
lambda1f = 100 fixed (0,inf) nm
B2f = 0 fixed [0,inf)
lambda2f = 110 fixed (0,inf) nm
newAD2>