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High sensitive and large dynamic range quasi-distributed sensing system based on slow-light π-phase-shifted fiber Bragg gratings
Institution:1. Dept. of Electronics and Electrical Engineering, IIT Guwahati, India;2. Warsaw University of Technology, Institute of Electronic Systems, ul. Nowowiejska 15/19, 00-665 Warsaw, Poland;3. National Institute of Telecommunications, ul. Szachowa 1, 04-894 Warsaw, Poland;1. Department of Metallurgical Engineering and Materials Science, IIT Bombay, Mumbai, 400076, India;2. Department of chemical engineering, Monash University, Australia;3. IITB-Monash research academy, Mumbai, 400076, India;1. V.G. Mokerov Institute of Ultra High Frequency Semiconductor Electronics of RAS, Moscow, Russia;2. Center for Photonics and 2D Materials, Moscow Institute of Physics and Technology, Dolgoprudny, Russia;3. Belarusian State University, Minsk, Belarus;4. Institute for Physics of Microstructures of RAS, Nizhny Novgorod, Russia;5. Institute of Radio-Engineering and Electronics of RAS, Moscow, Russia;1. Institute of Applied Physics, Military University of Technology, 2 Gen. S. Kaliskiego St., 00-908 Warsaw, Poland;2. Graduate Institute of Photonics and Optoelectronics, National Taiwan University, Roosevelt Rd., 10617 Taipei, Taiwan
Abstract:In this paper, we theoretically analyze the slow-light π-phase-shifted fiber Bragg grating (π-FBG) and its applications for single and multipoint/quasi-distributed sensing. Coupled-mode theory (CMT) and transfer matrix method (TMM) are used to establish the numerical modeling of slow-light π-FBG. The impact of slow-light FBG parameters, such as grating length (L), index change (Δn), and loss coefficient (α) on the spectral properties of π-FBG along with strain and thermal sensitivities are presented. Simulation results show that for the optimum grating parameters L = 50 mm, Δn = 1.5×10−4, and α = 0.10 m-1, the proposed slow-light π-FBG is characterized with a peak transmissivity of 0.424, the maximum delay of 31.95 ns, strain sensitivity of 8.380 με-1, and temperature sensitivity of 91.064 °C-1. The strain and temperature sensitivity of proposed slow-light π-FBG is the highest as compared to the slow-light sensitivity of apodized FBGs reported in the literature. The proposed grating have the overall full-width at half maximum (FWHM) of 0.2245 nm, and the FWHM of the Bragg wavelength peak transmissivity is of 0.0798 pm. The optimized slow-light π-FBG is used for quasi-distributed sensing applications. For the five-stage strain quasi-distributed sensing network, a high strain dynamic range of value 1469 με is obtained for sensors wavelength spacing as small as 2 nm. In the case of temperature of quasi-distributed sensing network, the obtained dynamic range is of 133 °C. For measurement system with a sufficiently wide spectral range, the π-FBGs wavelength grid can be broadened which results in substantial increase of dynamic range of the system.
Keywords:π-FBG  Slow-light  Sensitivity  Quasi-distributed sensing  Transfer matrix method
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