Robert J. Bell, Mark A. Ordal, and Ralph W. Alexander, "Equations linking different sets of optical properties for nonmagnetic materials," Appl. Opt. 24, 3680-3682 (1985)
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In the Drude Model the Real and Imaginary Parts of nc, ∊c, zc, andσcare Presented In Terms ofω, ωτ, ωp, and∊∞.a
The scattering ωτ and plasma ωp frequencies are given in terms of the real and imaginary parts of nc, ∊c, zc, and σc. The high frequency resistivity, the real part of the complex optical resistivity, is given in the four sets of parameters. Also the dc conductivity, σ0 (sec−1), is related to the dc resistivity ρ0 (Ω-cm).
Table III
Reflectances at Normal Incidence (Vacuum Overlayer) for any Material.a
For R (ω,ωτ,ωp) there is an approximation [as stated in the text in Eq. (17)].
Tables (3)
Table I
Linkage Equations
Table II
In the Drude Model the Real and Imaginary Parts of nc, ∊c, zc, andσcare Presented In Terms ofω, ωτ, ωp, and∊∞.a
The scattering ωτ and plasma ωp frequencies are given in terms of the real and imaginary parts of nc, ∊c, zc, and σc. The high frequency resistivity, the real part of the complex optical resistivity, is given in the four sets of parameters. Also the dc conductivity, σ0 (sec−1), is related to the dc resistivity ρ0 (Ω-cm).
Table III
Reflectances at Normal Incidence (Vacuum Overlayer) for any Material.a
For R (ω,ωτ,ωp) there is an approximation [as stated in the text in Eq. (17)].