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FIBER OPTIC SENSORS BASED ON THE MACH–ZEHNDER AND MICHELSON INTERFEROMETERS

天文干涉仪 马赫-曾德尔干涉仪 光纤 光学 迈克尔逊干涉仪 光纤传感器 物理 干涉测量
作者
A. Dandridge
标识
DOI:10.1002/9781119678892.ch10
摘要

Chapter 10 FIBER OPTIC SENSORS BASED ON THE MACH–ZEHNDER AND MICHELSON INTERFEROMETERS Anthony Dandridge, Anthony Dandridge Optical Sciences Division, U.S. Naval Research Laboratory, Washington, DC, USASearch for more papers by this author Anthony Dandridge, Anthony Dandridge Optical Sciences Division, U.S. Naval Research Laboratory, Washington, DC, USASearch for more papers by this author Book Editor(s):Eric Udd, Eric Udd Columbia Gorge Research LLC, Fairview, OR, USA McDonnell Douglas Electronic Systems Company, Santa Ana, CA, USASearch for more papers by this authorWilliam B. Spillman Jr., William B. Spillman Jr. Columbia Gorge Research LLC, Fairview, OR, USASearch for more papers by this author First published: 05 April 2024 https://doi.org/10.1002/9781119678892.ch10 AboutPDFPDF ToolsRequest permissionExport citationAdd to favoritesTrack citation ShareShareShare a linkShare onEmailFacebookTwitterLinkedInRedditWechat Summary Fiber optic interferometric sensors, as well as having the advantages generally attributed to fiber sensors, such as electrically passive, lightweight, immunity to electromagnetic interference, and multiplexing, have the additional advantages of geometric versatility of the sensing element, wide dynamic range, and extremely high sensitivity. This chapter explains the basic principle of operation of the sensors: two-beam interferometry. It also describes two of the basic methods of interferometer demodulation. The first is the active homodyne approach, which although not applicable to most real-world systems has had widespread use in the laboratory and may be described as the "beginners' " demodulator. Unlike the active scheme, the second demodulation approach has no electrical components in the interferometer, and because of this and the fact that the approach does not form a feedback loop to the interferometer, this is termed a passive approach. The chapter also describes various interferometer configurations: Mach-Zehnder, Michelson, reflectometric, and Fabry-Perot. REFERENCES T. G. Giallorenzi , J. A. Bucaro , A. Dandridge , G. H. Sigel , J. H. Cole , S. C. Rashleigh , and R.G. Priest , Optical fiber sensor technology , IEEE J. Quantum Electron. 18 , 626 ( 1982 ). 10.1109/JQE.1982.1071566 Web of Science®Google Scholar C. D. Butter and G. B. Hocker , Fiber optic strain gauge , Appl. Opt. 17 , 2867 ( 1978 ). 10.1364/AO.17.002867 CASPubMedWeb of Science®Google Scholar A. Dandridge , A. B. 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