Document Type
Article
Publication Date
4-1-1989
Abstract
The differential reflection phase shift, Δ = δp - δs, associated with the external reflection of monochromatic light at the surface of an absorbing medium is a monotonically decreasing function of the angle of incidence ø which is determined by the complex dielectric function ε. A new special angle of incidence, denoted by øΔ′max, is defined at which the slope Δ′ = ∂Δ/∂ø of the Δ-ø curve is maximum negative, Δ′max, and a transcendental equation is derived that determines this angle. øΔ′max differs from the principal angle øp at which Δ = 90°. As an example, øΔ′max is calculated by numerical iteration for light reflection at the air-Si interface for photon energies hv from 1.7 to 5.6eV in steps of 0.1eV, and is plotted, along with the associated maximum slope Δ′max, vs wavelength λ. It is noted that øΔ′max>øp at every λ, a result that may hold in general. Also, for 4.5 ≤ hv ≤ 5.6 eV, øΔ′max = 90°, so that a maximum negative slope occurs at grazing incidence in this spectral range. Another interesting observation is that, when |ε| >> 1 (e.g., for metals in the IR), Δ′(90°) is a direct measure of the extinction coefficient k = Imε½.
Journal Name
Applied Optics
Recommended Citation
R. M. A. Azzam and A. M. El-Saba, "Maximum rate of change of the differential reflection phase shift with respect to the angle of incidence for light reflection at the surface of an absorbing medium," Appl. Opt. 28, 1365-1368 (1989)
Comments
This paper was published in Applied Optics and is made available as an electronic reprint with the permission of OSA. The paper can be found at the following URL on the OSA website: http://www.opticsinfobase.org/ao/abstract.cfm?URI=ao-28-7-1365. Systematic or multiple reproduction or distribution to multiple locations via electronic or other means is prohibited and is subject to penalties under law.