Merged Sagnac-Michelson interferometer for distributed disturbance detection

• Published in: Journal of lightwave technology Vol. 15; no. 6; pp. 972 - 976
• Main Authors: Spammer, S.J., Swart, P.L., Chtcherbakov, A.A.
• Format: Journal Article
• Language: English
• Published: New York, NY IEEE 01-06-1997; Institute of Electrical and Electronics Engineers
• Subjects: Capacitive sensors; Exact sciences and technology; Frequency; Instruments, apparatus, components and techniques common to several branches of physics and astronomy; Interferometers; Mirrors; Optical fibers; Optical instruments, equipment and techniques; Optical interferometry; Phase detection; Phase shifting interferometry; Physics; Sagnac interferometers; Temperature dependence; Temperature sensors; Optical fibers; Experimental result; Signal detector; Distributed system; Michelson interferometers; Sagnac effect
• ISSN: 0733-8724; 1558-2213
• DOI: 10.1109/50.588669

An interferometric technique is described to detect and locate perturbations along an optical fiber. This distributed sensor has a position dependent response to time-varying disturbances such as strain or temperature. These disturbances cause a phase shift which is detected and converted to spatial information, The sensor consists of a Sagnac interferometer merged with a Michelson interferometer. This is achieved by a frequency selective mirror in the center of the Sagnac-loop. The sensor is illuminated by two light sources with wavelengths /spl lambda//sub 1/ and /spl lambda//sub 2/, respectively. The mirror reflects /spl lambda//sub 1/ and transmits /spl lambda//sub 2/, causing the interferometer to operate as a Michelson at wavelength /spl lambda//sub 1/ and as a Sagnac at wavelength /spl lambda//sub 2/. Any time-varying perturbation on, the fiber will, result in a signal at /spl lambda//sub 2/ proportional to the product of the rate of phase change caused by the perturbation and the distance of the perturbation relative to the position of the mirror. The output of the Michelson interferometer at wavelength /spl lambda//sub 1/ is proportional to the phase change caused by the unknown perturbation. By dividing the output of the Sagnac interferometer by the time rate of change of the Michelson interferometer signal, the position of the disturbance relative to the mirror is located. Results obtained with a 200 m-distributed fiber sensor are discussed.