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For two non-absorbing components with volume fractions fi and refractive indices ni, the Bruggemann effective medium approximation gives [18] Figure 3 The refractive index spectra and refractive index at a wavelength of the TiN films.
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This approximation gives the refractive index of an effective medium from the refractive indices of the constituent materials and their corresponding volume fractions.
The approximation gives an analytical solution to the scattering cross section of spherical scatterers, which tells us that the periodicity of the spectral oscillations depends on size, as well as on the ratio between the RI of the scatterer and surrounding medium [ 23].
Equations for the hydraulic conductivity tensor in "composite medium approximation" (COMA) are given in a coordinate system aligned with bedding.
Thus, the CAT approximation gave acceptable branch lengths.
The dashed lines show the approximation given in Equation (6).
As it can be seen Fig. 1, the approximation to the radiance given by the cDA agrees better with the RTE than the approximation given by the DA.
In contrast, an ODE that used the approximation given in Eqs.
The porosity of a thin film can be estimated from measured refractive index of the thin film using the Bruggemann effective medium approximation [60, 61] which gives effective refractive index of the thin film consisting of two components, air and the depositing material.
For these non-regular structures, the effective medium approximation is better at reproducing their optical properties.
For the TM calculations, we employed the effective medium approximation model for the AgMy nanosheets.
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