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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

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