Improved Efficiency Narrow-Band Acoustooptic Tunable Reflector using Fibre Bragg Grating

W.F. Liu, L. Dong, L. Reekie, D. Culverhouse, P. Russell
{"title":"Improved Efficiency Narrow-Band Acoustooptic Tunable Reflector using Fibre Bragg Grating","authors":"W.F. Liu, L. Dong, L. Reekie, D. Culverhouse, P. Russell","doi":"10.1364/bgppf.1997.pdp4","DOIUrl":null,"url":null,"abstract":"All-fibre versions of bulk devices are very attractive in fibre systems where low insertion loss is always desirable. We have greatly improved the performance of a recently reported [1] Bragg-grating-based acousto-optic superiattice modulator (AOSLM) by reducing the fibre diameter by HF etching. This improves the overlap of acoustic and optical power, resulting in modulator efficiencies as high as 90%. The modulator produces narrow-band amplitude-adjustable reflections that can be tuned over several nm, which is attractive for WDM and laser applications. In the device, an extensional acoustic wave is launched along a fibre Bragg grating. The ensuing superiattice modulation causes additional bands of reflection to appear on both sides of the Bragg condition. The device works by coupling together the forward and backward propagating Bloch modes in the grating (a principle first proposed in 1986 [2,3]) and operates in reflection mode. This differentiates the AOSLM from all previously reported acousto-optic fibre devices, which all rely on intermodal coupling, examples being LP01 to LP11 coupling in dual-mode [4] and twin-core [5] fibres, four-port null-couplers [6], polarisation mode couplers in Hi-Bi fibre [7] and guided-to-cladding mode coupling in standard telecom fibre [8]. In all these devices the intermodal beat length L\n B\n = λ /(n1 – n2) at optical wavelength λ between two modes with phase indices n1, and n2 is matched by the acoustic wavelength v\n s\n / f\n s\n where v\n s\n and f\n s\n are the acoustic phase velocity and frequency.","PeriodicalId":182420,"journal":{"name":"Bragg Gratings, Photosensitivity, and Poling in Glass Fibers and Waveguides: Applications and Fundamentals","volume":"1 1","pages":"0"},"PeriodicalIF":0.0000,"publicationDate":"1900-01-01","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":"0","resultStr":null,"platform":"Semanticscholar","paperid":null,"PeriodicalName":"Bragg Gratings, Photosensitivity, and Poling in Glass Fibers and Waveguides: Applications and Fundamentals","FirstCategoryId":"1085","ListUrlMain":"https://doi.org/10.1364/bgppf.1997.pdp4","RegionNum":0,"RegionCategory":null,"ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":null,"EPubDate":"","PubModel":"","JCR":"","JCRName":"","Score":null,"Total":0}
引用次数: 0

Abstract

All-fibre versions of bulk devices are very attractive in fibre systems where low insertion loss is always desirable. We have greatly improved the performance of a recently reported [1] Bragg-grating-based acousto-optic superiattice modulator (AOSLM) by reducing the fibre diameter by HF etching. This improves the overlap of acoustic and optical power, resulting in modulator efficiencies as high as 90%. The modulator produces narrow-band amplitude-adjustable reflections that can be tuned over several nm, which is attractive for WDM and laser applications. In the device, an extensional acoustic wave is launched along a fibre Bragg grating. The ensuing superiattice modulation causes additional bands of reflection to appear on both sides of the Bragg condition. The device works by coupling together the forward and backward propagating Bloch modes in the grating (a principle first proposed in 1986 [2,3]) and operates in reflection mode. This differentiates the AOSLM from all previously reported acousto-optic fibre devices, which all rely on intermodal coupling, examples being LP01 to LP11 coupling in dual-mode [4] and twin-core [5] fibres, four-port null-couplers [6], polarisation mode couplers in Hi-Bi fibre [7] and guided-to-cladding mode coupling in standard telecom fibre [8]. In all these devices the intermodal beat length L B = λ /(n1 – n2) at optical wavelength λ between two modes with phase indices n1, and n2 is matched by the acoustic wavelength v s / f s where v s and f s are the acoustic phase velocity and frequency.
利用光纤光栅改进效率的窄带声光可调谐反射器
在低插入损耗的光纤系统中,散装器件的全光纤版本非常有吸引力。我们通过HF蚀刻减小光纤直径,极大地提高了最近报道的[1]基于bragg光栅的声光超晶格调制器(AOSLM)的性能。这改善了声学和光功率的重叠,从而使调制器效率高达90%。该调制器产生窄带幅度可调反射,可调谐到几纳米,这对波分复用和激光应用具有吸引力。在该装置中,一个扩展声波沿着光纤布拉格光栅发射。随后的超晶格调制导致在布拉格条件的两侧出现额外的反射带。该装置通过将光栅中的正向和反向传播布洛赫模式耦合在一起工作(该原理于1986年首次提出[2,3]),并在反射模式下工作。这将aslm与之前报道的所有声光光纤设备区别开,这些设备都依赖于多模耦合,例如双模[4]和双芯[5]光纤中的LP01到LP11耦合,四端口零耦合器[6],Hi-Bi光纤中的偏振模式耦合器[7]和标准电信光纤中的引导到包层模式耦合[8]。在两个相位指数为n1的模式之间,在光学波长λ处,模间拍长L B = λ /(n1 - n2), n2与声波波长v s / f s相匹配,其中v s和f s为声波相速度和频率。
本文章由计算机程序翻译,如有差异,请以英文原文为准。
求助全文
约1分钟内获得全文 求助全文
来源期刊
自引率
0.00%
发文量
0
×
引用
GB/T 7714-2015
复制
MLA
复制
APA
复制
导出至
BibTeX EndNote RefMan NoteFirst NoteExpress
×
提示
您的信息不完整,为了账户安全,请先补充。
现在去补充
×
提示
您因"违规操作"
具体请查看互助需知
我知道了
×
提示
确定
请完成安全验证×
copy
已复制链接
快去分享给好友吧!
我知道了
右上角分享
点击右上角分享
0
联系我们:info@booksci.cn Book学术提供免费学术资源搜索服务,方便国内外学者检索中英文文献。致力于提供最便捷和优质的服务体验。 Copyright © 2023 布克学术 All rights reserved.
京ICP备2023020795号-1
ghs 京公网安备 11010802042870号
Book学术文献互助
Book学术文献互助群
群 号:604180095
Book学术官方微信