直接解亥姆霍兹方程的二元透镜数值模拟

G. R. Hadley
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引用次数: 0

摘要

二元衍射光学已成为用于光纤互连和耦合的一类重要结构。这样的结构已经成功地设计在过去使用傅立叶分析技术。这些技术完全适用于近傍轴光学,如高f值透镜。然而,快速(F<1.5)透镜的设计,如将光耦合到光纤中所需要的透镜,需要使用更精确的技术,其中大多数是基于模态扩展的2,3。在本文中,我们描述了一种新的有限差分方法,用于模拟小特征尺寸的二元光学结构,该方法涉及到结构附近标量亥姆霍兹的直接解,然后(在透镜的情况下)通过广角光束传播来预测焦斑的大小。在这种方法中,结构完全由其产生的介电函数来描述,允许处理任意复杂性的非周期二元结构。所有反射以及由于亚波长特征尺寸而产生的影响都会自动包含在内。由于在所有介电界面上使用了半矢量边界条件,偏振效应被近似地处理。这种技术先前已被证明可以正确地模拟蚀刻在波导中的一阶和二阶衍射光栅的行为。(本方法与文献4的解法略有不同,其解法为直接矩阵反演,而不是文献4所述的迭代法。)它不涉及展开或简化假设(除了矢量考虑之外),而且非常快,只需要几分钟的工作站运行时间。
本文章由计算机程序翻译,如有差异,请以英文原文为准。
Numerical Simulation of Binary Lenses by Direct Solution of the Helmholtz Equation
Binary diffractive optics have become an important class of structures for use in optical interconnects and coupling into fibers1. Such structures have been successfully designed in the past using the techniques of Fourier analysis. These techniques are entirely adequate for near-paraxial optics such as occur with high-F-number lenses. The design of fast (F<1.5) lenses such as those required for coupling light into optical fibers, however, requires the use of more accurate techniques, most of which are based upon modal expansions2,3. In this paper we describe a new finite-difference method for modeling small-feature-size binary optical structures that involves the direct solution of the scalar Helmholtz in the vicinity of the structure, followed (in the case of lenses) by wide-angle beam propagation to predict the size of the focal spot. In this approach, the structure is described entirely by by its resulting dielectric function, allowing the treatment of aperiodic binary structures of arbitrary complexity. All reflections together with effects due to sub-wavelength feature sizes are automatically included. Polarization effects are treated approximately owing to the use of semivectorial boundary conditions at all dielectric interfaces. This technique has been shown previously4 to correctly model the behavior of first-and second-order diffraction gratings etched into waveguides. (The present method differs slightly from that described in reference 4 in that the solution method is direct matrix inversion instead of the iterative method described therein.) It involves no expansions or simplifying assumptions (aside from vectorial considerations) and is quite fast, requiring only a few minutes of workstation runtime.
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