• Laser & Optoelectronics Progress
  • Vol. 57, Issue 19, 191203 (2020)
Hai Liu1、2、*, Cancan Chen1, Wen Zhang1, Haoran Wang1, and Shoufeng Tang1
Author Affiliations
  • 1School of Information and Control Engineering, China University of Mining and Technology, Xuzhou, Jiangsu 221116, China
  • 2Xuzhou Key Laboratory of Artificial Intelligence and Big Data, Xuzhou, Jiangsu 221116, China
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    DOI: 10.3788/LOP57.191203 Cite this Article Set citation alerts
    Hai Liu, Cancan Chen, Wen Zhang, Haoran Wang, Shoufeng Tang. Methane Sensing Measurement Based on Photonic Crystal Fiber Four-Wave Mixing Effect[J]. Laser & Optoelectronics Progress, 2020, 57(19): 191203 Copy Citation Text show less
    Cross-section of PCF and experimental principle diagram of the sensor. (a) Cross-section of PCF; (b) experimental principle diagram of the sensor
    Fig. 1. Cross-section of PCF and experimental principle diagram of the sensor. (a) Cross-section of PCF; (b) experimental principle diagram of the sensor
    Plots of the variations of β2, β4, and γ with methane concentrations. (a) Variation of β2; (b) variation of β4; (c) variation of γ
    Fig. 2. Plots of the variations of β2, β4, and γ with methane concentrations. (a) Variation of β2; (b) variation of β4; (c) variation of γ
    Gas-sensitivity graph of Stokes and anti-Stokes spectra。(a) Phase mismatch plots for different methane concentrations; (b) DFWM gain plot of the Stokes and anti-Stokes signals near the pump wavelength; (c) peak wavelength of the gain signal for different methane concentrations; (d) relationship between wavelength shift and methane concentrations at a pump wavelength of 1080 nm
    Fig. 3. Gas-sensitivity graph of Stokes and anti-Stokes spectra。(a) Phase mismatch plots for different methane concentrations; (b) DFWM gain plot of the Stokes and anti-Stokes signals near the pump wavelength; (c) peak wavelength of the gain signal for different methane concentrations; (d) relationship between wavelength shift and methane concentrations at a pump wavelength of 1080 nm
    Phase mismatch plots as well as Stokes and anti-Stokes signal gain plots obtained at different film thicknesses. (a) Phase mismatch plots; (b) Stokes and anti-Stokes signal gain plots
    Fig. 4. Phase mismatch plots as well as Stokes and anti-Stokes signal gain plots obtained at different film thicknesses. (a) Phase mismatch plots; (b) Stokes and anti-Stokes signal gain plots
    Phase mismatch plots as well as Stokes and anti-Stokes signal gain plots obtained at different film thicknesses and methane concentrations. (a) Phase mismatch plots; (b) Stokes and anti-Stokes signal gain plots
    Fig. 5. Phase mismatch plots as well as Stokes and anti-Stokes signal gain plots obtained at different film thicknesses and methane concentrations. (a) Phase mismatch plots; (b) Stokes and anti-Stokes signal gain plots
    Phase mismatch plots as well as Stokes and anti-Stokes signal gain plots obtained at different pump wavelengths. (a) Phase mismatch plots; (b) Stokes and anti-Stokes signal gain plots
    Fig. 6. Phase mismatch plots as well as Stokes and anti-Stokes signal gain plots obtained at different pump wavelengths. (a) Phase mismatch plots; (b) Stokes and anti-Stokes signal gain plots
    Phase mismatch plots as well as Stokes and anti-Stokes signal gain plots obtained at different pump wavelengths and methane concentrations. (a) Phase mismatch plots; (b) Stokes and anti-Stokes signal gain plots
    Fig. 7. Phase mismatch plots as well as Stokes and anti-Stokes signal gain plots obtained at different pump wavelengths and methane concentrations. (a) Phase mismatch plots; (b) Stokes and anti-Stokes signal gain plots
    Plots of the variation of β2, β4, γ, κ, DFWM gain plot of the Stokes and anti-Stokes spectra, peak movement curves and sensitivity fitting curves at a pump wavelength of 1079 nm. (a) β2; (b) β4; (c) γ; (d) κ; (e) Stokes and anti-Stokes spectra gains plots; (f) peak movement curves; (g) sensitivity fitting curves
    Fig. 8. Plots of the variation of β2, β4, γ, κ, DFWM gain plot of the Stokes and anti-Stokes spectra, peak movement curves and sensitivity fitting curves at a pump wavelength of 1079 nm. (a) β2; (b) β4; (c) γ; (d) κ; (e) Stokes and anti-Stokes spectra gains plots; (f) peak movement curves; (g) sensitivity fitting curves
    Movement of Stokes and Anti-Stokes Spectra when methane volume fraction changes from 0% to 0.05%
    Fig. 9. Movement of Stokes and Anti-Stokes Spectra when methane volume fraction changes from 0% to 0.05%
    Λ /μmd /μmt /nmλ /nmL /m
    31.2526010790.2
    Table 1. Structural parameters of the sensor
    TypeYearSensitivity/ (nm/%)Low detection limitRef.
    PCF-LPG20171.0781.8×10-3[21]
    PCF-LPG20152.52×10-3[22]
    Modal interference20160.511.6×10-3[19]
    PC micro-cavity20151.677×10-4[23]
    In this paper2019-4.87/2.835×10-4 /1.66×10-4
    Table 2. Comparison of photonic crystal fiber sensor
    Hai Liu, Cancan Chen, Wen Zhang, Haoran Wang, Shoufeng Tang. Methane Sensing Measurement Based on Photonic Crystal Fiber Four-Wave Mixing Effect[J]. Laser & Optoelectronics Progress, 2020, 57(19): 191203
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