Fabry-Perot Interferometer Curvature Sensor Based on Microwave Photonic Filter Technique

In this letter, we propose and experimentally demonstrate an approach to performing high-resolution and temperature-insensitive idea of a Fabry-Perot interferometer (FPI) curvature sensor utilizing microwave photonic filter (MPF) technique. A section of the capillary fiber is spliced between a single-mode fiber and a core-less fiber to form the air-gap FPI. The bending deformation of the FPI leads to changes in the fringe visibility (V) and free spectral range (FSR) of the interference pattern, which are converted into the changes in peak power and central frequency of the corresponding MPF. Consequently, the bending curvature can be recovered by tracking the frequency shift or the magnitude change. The experimental results show that the peak of the MPF decreases non-linearly with the increased curvature and a second-degree polynomial curve is fitted to predict the relationship. Compared with the fringe visibility change in optical domain, the peak power change of the MPF is enhanced by ~5 times. Meanwhile, the wavelength shift has a linear relationship with the curvature, and the sensitivity of 19.5 pm/m−1 is achieved in the curvature range of 3.3065-9.0552 m<inline-formula xmlns:mml="http://www.w3.org/1998/Math/MathML" xmlns:xlink="http://www.w3.org/1999/xlink"> <tex-math notation="LaTeX">$^{\mathrm {-1}}$ </tex-math></inline-formula> with a resolution of 1.026 m−1. The central frequency shifts linearly with the increase of curvature, and the sensitivity is 0.86 MHz/m<inline-formula xmlns:mml="http://www.w3.org/1998/Math/MathML" xmlns:xlink="http://www.w3.org/1999/xlink"> <tex-math notation="LaTeX">$^{\mathrm {-1}}$ </tex-math></inline-formula> with a resolution of <inline-formula xmlns:mml="http://www.w3.org/1998/Math/MathML" xmlns:xlink="http://www.w3.org/1999/xlink"> <tex-math notation="LaTeX">$1.16\times 10 ^{-3}$ </tex-math></inline-formula>m−1, which is much larger than that obtained by tracking the wavelength shift.

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Publication Details

Journal
IEEE Photonics Technology Letters
Published
2024-11-22
DOI
https://doi.org/10.1109/lpt.2024.3504850
Citations
3
Primary Topic
Photonic and Optical Devices
Type
article
Field-Weighted Citation Impact
0.63

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article

Fabry-Perot Interferometer Curvature Sensor Based on Microwave Photonic Filter Technique

Jintao Wu, Tongqun Zhang, Minghong Wang, Xiaozhong Tian et al.
3 citations
IEEE Photonics Technology Letters
Photonic and Optical Devices
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article

Fabry-Perot Interferometer Curvature Sensor Based on Microwave Photonic Filter Technique

Jintao Wu, Tongqun Zhang, Minghong Wang, Xiaozhong Tian, Yunquan Sun, Lanju Liang, Junbao Wang, Dianguo Ma
article en
3 citations

Abstract

In this letter, we propose and experimentally demonstrate an approach to performing high-resolution and temperature-insensitive idea of a Fabry-Perot interferometer (FPI) curvature sensor utilizing microwave photonic filter (MPF) technique. A section of the capillary fiber is spliced between a single-mode fiber and a core-less fiber to form the air-gap FPI. The bending deformation of the FPI leads to changes in the fringe visibility (V) and free spectral range (FSR) of the interference pattern, which are converted into the changes in peak power and central frequency of the corresponding MPF. Consequently, the bending curvature can be recovered by tracking the frequency shift or the magnitude change. The experimental results show that the peak of the MPF decreases non-linearly with the increased curvature and a second-degree polynomial curve is fitted to predict the relationship. Compared with the fringe visibility change in optical domain, the peak power change of the MPF is enhanced by ~5 times. Meanwhile, the wavelength shift has a linear relationship with the curvature, and the sensitivity of 19.5 pm/m−1 is achieved in the curvature range of 3.3065-9.0552 m<inline-formula xmlns:mml="http://www.w3.org/1998/Math/MathML" xmlns:xlink="http://www.w3.org/1999/xlink"> <tex-math notation="LaTeX">$^{\mathrm {-1}}$ </tex-math></inline-formula> with a resolution of 1.026 m−1. The central frequency shifts linearly with the increase of curvature, and the sensitivity is 0.86 MHz/m<inline-formula xmlns:mml="http://www.w3.org/1998/Math/MathML" xmlns:xlink="http://www.w3.org/1999/xlink"> <tex-math notation="LaTeX">$^{\mathrm {-1}}$ </tex-math></inline-formula> with a resolution of <inline-formula xmlns:mml="http://www.w3.org/1998/Math/MathML" xmlns:xlink="http://www.w3.org/1999/xlink"> <tex-math notation="LaTeX">$1.16\times 10 ^{-3}$ </tex-math></inline-formula>m−1, which is much larger than that obtained by tracking the wavelength shift.

IEEE Photonics Technology LettersVol. 37(1)
Liaocheng University (CN), Zaozhuang University (CN)
National Natural Science Foundation of China
Affordable and clean energy
Openalex Percentile: Top 30%
Photonic and Optical Devices
0.63
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