• Acta Optica Sinica
  • Vol. 39, Issue 6, 0606001 (2019)
Wei Wang1、2、*, Ying Tang1, Xiongxing Zhang1、2, Haibin Chen1、2, Zilong Guo1, and Kening Wang1
Author Affiliations
  • 1 School of Optoelectronics Engineering, Xi'an Technological University, Xi'an, Shaanxi 710021, China
  • 2 Shaanxi Key Laboratory of Integrated and Intelligent Navigation, Xi'an, Shaanxi 710068, China
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    DOI: 10.3788/AOS201939.0606001 Cite this Article Set citation alerts
    Wei Wang, Ying Tang, Xiongxing Zhang, Haibin Chen, Zilong Guo, Kening Wang. Elliptical-Fitting Cavity Length Demodulation Algorithm for Compound Fiber-Optic Fabry-Perot Pressure Sensor with Short Cavity[J]. Acta Optica Sinica, 2019, 39(6): 0606001 Copy Citation Text show less
    Basic structure of compound fiber-optic Fabry-Perot pressure sensor
    Fig. 1. Basic structure of compound fiber-optic Fabry-Perot pressure sensor
    Lissajous figure obtained by six-parameter ellipse-fitting algorithm
    Fig. 2. Lissajous figure obtained by six-parameter ellipse-fitting algorithm
    Reflection spectrum of compound FP sensor with short cavity and interferometric signal for cavity filling with air
    Fig. 3. Reflection spectrum of compound FP sensor with short cavity and interferometric signal for cavity filling with air
    Lissajous figure when interferometric signal has translation of τ=1.238 THz along frequency axis
    Fig. 4. Lissajous figure when interferometric signal has translation of τ=1.238 THz along frequency axis
    Demodulation system for fiber-optic Fabry-Perot sensor. (a) Schematic; (b) physical map
    Fig. 5. Demodulation system for fiber-optic Fabry-Perot sensor. (a) Schematic; (b) physical map
    Compound fiber-optic Fabry-Perot pressure sensor with short cavity. (a) Physical map; (b) SEM image
    Fig. 6. Compound fiber-optic Fabry-Perot pressure sensor with short cavity. (a) Physical map; (b) SEM image
    Experimental setup for pressure sensing
    Fig. 7. Experimental setup for pressure sensing
    Experimental results of pressure sensing. (a) Reflection spectra for cavity filling with air under three kinds of pressure-loading conditions of 0.1, 0.3, and 0.5 MPa; (b) sensor cavity length versus pressure
    Fig. 8. Experimental results of pressure sensing. (a) Reflection spectra for cavity filling with air under three kinds of pressure-loading conditions of 0.1, 0.3, and 0.5 MPa; (b) sensor cavity length versus pressure
    MethodQRLUImproved Cholesky
    Multiplication(3n3-n)/2(n3+2n)/3n(n-1)2/3
    Division(3n2-n)/2n(n-1)/2n(n-1)/2
    Addition3n2(n-1)/2(3n2-4n+1)/2n(n-1)
    Table 1. Complexity statistics of QR, LU, and improved Cholesky decomposition methods
    Simulated cavity length /μmDemodulation cavity length /μmPeriod /THzError /μmR2
    3029.9895.000-0.0110.984
    2928.9955.173-0.0050.998
    2828.0245.3520.0240.986
    2727.0505.5450.0500.998
    2625.9725.775-0.0280.996
    Table 2. Calculation results of length of cavity filling with air obtained by two-parameter ellipse-fitting algorithm for cavity length in range of 26-30 μm
    Wei Wang, Ying Tang, Xiongxing Zhang, Haibin Chen, Zilong Guo, Kening Wang. Elliptical-Fitting Cavity Length Demodulation Algorithm for Compound Fiber-Optic Fabry-Perot Pressure Sensor with Short Cavity[J]. Acta Optica Sinica, 2019, 39(6): 0606001
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