λ=1.31和1.55μm的K+和Ag+离子交换的y支波长多/解复用器

F. Xiang, G. Yip
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引用次数: 0

摘要

光波导y分支具有较小的分支角度和两个不对称臂,可以作为波长多/解复用器(见图1)[1,2]。一个小的分支角θ将导致y分支作为一个模式分离器。两个几何形状或折射率不同的不对称臂将在两个要解复用的波长之间产生两个相交的波导色散曲线。交集设计为λ2 = 1.31μm与λ1 = 1.55μm之间,如图2所示。因此,在λ1 = 1.55μm处,臂1的有效指数高于臂2,在λ2 = 1.31μm处,臂1的有效指数低于臂2。来自主分支的λ1和λ2处的波可以分别分成臂1和臂2,分别为[2]。一般来说,不对称的两个分支臂越强,消光比就越高,消光比定义为两个分支臂输出功率的比值。
本文章由计算机程序翻译,如有差异,请以英文原文为准。
A Y-branch Wavelength Multi/Demultiplexer by K+ and Ag+ Ion-exchange for λ=1.31 and 1.55μm-Device Fabrication and Measurement Results
An optical waveguide Y-branch, with a small branch angle and two asymmetric arms, can function as a wavelength multi/demultiplexer (see Fig.1)[1,2]. A small branch angle θ will cause the Y-branch to perform as a mode splitter. Two asymmetric arms, differing either in the geometric shape or refractive index, will yield two intersecting waveguide dispersion curves between the two wavelengths to be demultiplexed. The intersection is designed to be between λ2 = 1.31μm and λ1 = 1.55μm as shown in Fig.2. Thus, the effective index of arm 1 will be higher than that of arm 2 at λ1 = 1.55μm and lower at λ2 = 1.31μm. The waves at λ1 and λ2 from the main branch can then be separated into arm 1 and arm 2, respectively [2]. Generally, the stronger asymmetric two branch arms are, the higher will be the extinction ratios, which are defined as the ratios of the output power from the two arms.
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