software to fit optical spectra - Quantum Materials Group
software to fit optical spectra - Quantum Materials Group
software to fit optical spectra - Quantum Materials Group
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2 f<br />
The model for ε d [cm] -<br />
y<br />
3 f<br />
The model for ε z<br />
- -<br />
4 The model for ε - -<br />
5 s<br />
The model for ε y<br />
- -<br />
6 s<br />
The model for ε z<br />
- -<br />
s<br />
x<br />
Table 4-11 The parameters of the model “Ellipsometry of an orthorhombic film on an orthorhombic substrate”.<br />
An example of such a model is shown in Figure 4-11. It is assumed that the “Model2”,<br />
“Model3” and “Model4” describe the x, y and z components respectively of the film dielectric<br />
tensor. The substrate is uniaxial with the symmetry axis z, normal <strong>to</strong> the sample surface. The x-<br />
and y-components of the substrate dielectric tensor are described by the “Model5”, the zcomponent<br />
is given by the “Model6”. The angle of incidence is 70 o , the angle of polarizer is<br />
45 o and the film thickness 0.000532 cm (5.32 micron).<br />
Figure 4-11 An example of the model “Ellipsometry of an orthorhombic film on an orthorhombic substrate”.<br />
4.7.6. Extended Drude<br />
This model takes as an input a dielectric function ε (ω)<br />
given by some dielectric function<br />
model and converts it <strong>to</strong> the frequency-dependent scattering rate 1/ τ ( ω)<br />
and the normalized<br />
*<br />
frequency-dependent effective mass m ( ω ) / m according <strong>to</strong> the formulas:<br />
2<br />
1 ω p ⎛ 1 ⎞<br />
= − Im ⎜<br />
⎟ , ∞<br />
τ ( ω)<br />
ω ⎝ ε ( ω)<br />
− ε ⎠<br />
*<br />
m ( ω)<br />
m<br />
2<br />
ω p ⎛ 1 ⎞<br />
− Re ⎜<br />
⎟ .<br />
2<br />
ω ⎝ ε ( ω)<br />
− ε ⎠<br />
= ∞<br />
Guide <strong>to</strong> RefFIT Page 70