Scattering of light from a two-layer system with a rough surface

Citation
R. Garcia-llamas et al., Scattering of light from a two-layer system with a rough surface, J OPT SOC A, 16(11), 1999, pp. 2713-2719
Citations number
15
Categorie Soggetti
Apllied Physucs/Condensed Matter/Materiales Science","Optics & Acoustics
Journal title
JOURNAL OF THE OPTICAL SOCIETY OF AMERICA A-OPTICS IMAGE SCIENCE AND VISION
ISSN journal
10847529 → ACNP
Volume
16
Issue
11
Year of publication
1999
Pages
2713 - 2719
Database
ISI
SICI code
1084-7529(199911)16:11<2713:SOLFAT>2.0.ZU;2-N
Abstract
The scattered light from a two-layer system with a shallow, random, one-dim ensional rough surface bounded by semi-infinite dissimilar optical media is calculated. The systems is composed of metallic and weak absorbent dielect ric films between glass and vacuum. The dielectric constant and the thickne ss of the dielectric film are chosen in such a way that in the absence of r oughness the system supports eight transverse magnetic guided modes, whose wave numbers are q(1)((TM))(lambda) , q(2)((TM)) (lambda),..., q(8)((TM)) ( lambda), or nine transverse electric (TE) guided models, whose wave numbers are q(1)((TE)) (lambda), q(2)((TE)) (lambda), ..., q(9)((TE)) (lambda), at the wavelength lambda. The Rayleigh hypothesis is used to obtain an integr al equation relating the amplitudes of the reflected fields to the incident wave. The scattering integral is solved both by perturbation and numerical ly. Results are obtained by assuming a Gaussian roughness spectrum for the surface, and the formalism is applied to simulate the scattering from the s ystem in the attenuated total reflection configuration, allowing the excita tion of guided waves. The angular dependence of the scattering shows four p eaks, in addition to the backscattering effect. The angular positions of th ese peaks are given by (2 pi/lambda)n(1) sin theta(k)((t)) = +/-q(k)((t)) w ith k = 7, 8 when t = {p, TM} or k = 8, 9, when t = {s, TE}; they are also independent of the angle of incidence and are due to single-scattering effe cts. (C) 1999 Optical Society of America [S0740-3232(99)01111-4].