用于DWDM应用的非均匀布拉格光栅

O. Baum, A. I. Khudobenko, G. Mishakov, V. Panchenko, V. Sokolov, A. Zherikhin
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引用次数: 0

摘要

光纤网络中密集波分复用(DWDM)技术的出现,使得基于亚微米布拉格光栅的新型光加/丢复用器(oadm)的开发成为必要。对于每信道比特率为10-40 gbit /s、信道间距为200、100和50 GHz的密集多信道ofn, oadm必须在停止/通带内具有矩形反射/透射光谱和线性相位特性。这些特性不能用均匀的布拉格光栅来实现,因此应该使用具有空间调制耦合系数和/或相移π的非均匀光栅。本文介绍了基于亚微米非均匀布拉格光栅的窄带波长选择滤波器的设计和制造的最新进展。研究了电磁波在非均匀光栅结构中的传播、相互作用和衍射特性。设计并制作了基于单模石英光纤的窄带反射滤波器,并在介质和聚合物材料上进行了侧抛光和浮雕光栅。滤光片的阻带形状接近矩形,宽度为0.4 ~ 1.6 nm,在1.55 μm波长区域的峰值反射率R > 99%。讨论了采用具有相移π的双谐波Bragg光栅的平面聚合物集成光子电路(IPCs)用于高速OFNs的多通道oadm的结构。
本文章由计算机程序翻译,如有差异,请以英文原文为准。
Nonuniform Bragg gratings for DWDM applications
The advent of the Dense Wavelength Division Multiplexing (DWDM) technology in Optical Fiber Networks (OFNs) has resulted in the necessity of developing advanced Optical Add/Drop Multiplexers (OADMs) on the basis of submicron Bragg gratings. The OADMs for dense multichannel OFNs with bit rates 10-40 Gbits/s per channel and channel spacing 200, 100 and 50 GHz must possess rectangular-shaped reflection/transmission spectra and linear phase characteristic within the stop/passband. These features can not be achieved using uniform Bragg gratings and therefore nonuniform gratings with space-modulated coupling coefficient and/or phase shifts π should be used. We present the recent advances in the design and fabrication of narrowband wavelength-selective filters for DWDM applications using submicron nonuniform Bragg gratings. The peculiarities of propagation, interaction and diffraction of electromagnetic waves in nonuniform grating structures are considered. Narrowband reflection filters using single-mode quartz fibers with side-polishing and relief gratings on dielectric and polymeric materials are designed and fabricated. The filters have nearly rectangular shape of the stopband with 0.4-1.6 nm width and peak reflectivity R > 99% in the 1.55 μm wavelength region. The architecture of multichannel OADMs for high-speed OFNs using planar polymer Integrated Photonic Circuits (IPCs) with biharmonic Bragg gratings, possessing phase shifts π, is discussed.
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