Scattering of a Gaussian beam from a row of cylinders with rectangular cross section

被引:1
作者
Daniel Valenzuela-Sau, Jesus [1 ]
Munguia-Arvayo, Ramon [1 ]
Gastelum-Acuna, Sandra [2 ]
Gaspar-Armenta, Jorge [2 ]
Napoles-Duarte, Jose [3 ]
Garcia-Llamas, Raul [2 ]
机构
[1] Univ Sonora, Programa Doctorado Ciencias Fis, Apdo Postal 5-88, Hermosillo, Sonora, Mexico
[2] Univ Sonora, Dept Invest Fis, Apdo Postal 5-88, Hermosillo, Sonora, Mexico
[3] Univ Autonoma Chihuahua, Fac Ciencia Quim, Apdo Postal 669, Chihuahua, Mexico
关键词
STRATIFIED DIELECTRIC MEDIA; LIGHT-SCATTERING; OBLIQUE-INCIDENCE; ELECTROMAGNETIC SCATTERING; INFINITE CYLINDERS; PARALLEL CYLINDERS; WAVE PROPAGATION; GLASS CYLINDERS; PLANE-WAVE; DIFFRACTION;
D O I
10.1364/JOSAA.34.001369
中图分类号
O43 [光学];
学科分类号
070207 ; 0803 ;
摘要
The transverse magnetic Gaussian beam diffraction from a finite number, equally spaced and rectangular cross section dielectric cylinder row is studied. The infinitely long cylinders' axes are perpendicular to the beam's direction of propagation. The cylinder row, with dielectric constant epsilon(c) = n(c)(2), is treated as a periodic inhomogeneous film, with period a(x) and thickness w(y), bounded by two semi-infinite homogeneous media. With this restriction, the method is valid only for square or rectangular cross section cylinders. The supercell and the plane wave expansion methods are used to calculate the eigenfrequencies and eigenvectors supported for a one-dimensional photonic crystal. Then, these eigenfrequencies and eigenvectors are used to expand the field in the inhomogeneous film. Numerical results are presented for ax greater than. (the incident light wavelength), w(x) (the cylinder width), and w(g) (Gaussian beam waist). Two cases are studied. In the first (second) case, the unit cell contains one cylinder (a cylinder row), which simulates the scattering from a single cylinder (an inhomogeneous thin film). The total integrated scattering in transmission (reflection) shows three well-defined minima (maxima), which are due to interference effects. Its positions can be approximately obtained with the formula. lambda(k) = 4n(c)w(y)/k, with k = 3, 4, and 6. The total integrated scattering in transmission decreases linearly as a function of the cylinder number. (C) 2017 Optical Society of America
引用
收藏
页码:1369 / 1375
页数:7
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