Acta Optica Sinica, Volume. 45, Issue 3, 0306003(2025)

D-Shaped Photonic Crystal Fiber Plasmonic Sensor with Dual-Open-Circular Channel for Low Refractive Index Detection

Kai Yan1, Wei Xu2, Qingyun Chen2, Chen Zhu1, and Wei Li1,2、*
Author Affiliations
  • 1College of Integrated Circuit Science and Engineering (College of Industry-Education Integration), Nanjing University of Posts and Telecommunications, Nanjing 210023, Jiangsu , China
  • 2College of Electronic and Optical Engineering, College of Flexible Electronics (Future Technology), Nanjing University of Posts and Telecommunications, Nanjing 210023, Jiangsu , China
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    Figures & Tables(14)
    Equivalent film structure
    Effects of different film thicknesses on sensitivity and minimum reflectivity when TiO2 is used as adhesive layer. (a) Sensitivity; (b) minimum reflectivity
    Structure of proposed PCF-SPR sensor. (a) Cross-sectional view; (b) mesh subdivision
    Relationship between core mode and SPP mode when analyte RI is 1.25. (a) Real part of effective RI [Re(neff)] and loss spectrum; (b) imaginary part of effective RI [Im(neff)]
    Electric field distributions of x and y polarization modes when analyte RI is 1.25. (a)(b) Core mode at 1610 nm; (c)(d) SPP mode at 1610 nm; (e)(f) coupling mode at 1760 nm
    Influences of diameters (d1,d2,d3) and spacing of air holes Λ on loss spectra when RI of analyte is 1.26 and 1.27. (a) d1; (b) d2; (c) d3; (d) Λ
    Influences of polishing depth H, open ring radius r and different film thicknesses (tTiO2 and tAu) on loss spectra when analyte RI is 1.26 and 1.27. (a) H; (b) r; (c) tTiO2; (d) tAu
    Resonance wavelength shifts of four structures at different TiO2 thicknesses when analyte RI is 1.31
    Loss curves of different structures when analyte RI is 1.32. (a) Without TiO2; (b) with 10 nm TiO2
    Comparison of different structures when analyte RI is 1.31. (a) Resonance wavelength shift; (b) loss peak
    Loss curves with different analyte RI. (a) 1.22‒1.27; (b) 1.28‒1.32
    Fitting curves for analyte RI variation. (a) 1.22‒1.27; (b) 1.28‒1.32
    • Table 1. Sensitivity varies with thickness of TiO2 film when Au film thickness is 43 nm and 59 nm, respectively

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      Table 1. Sensitivity varies with thickness of TiO2 film when Au film thickness is 43 nm and 59 nm, respectively

      Thickness of

      Au /nm

      Sensitivity /(nm/RIU)Maximum change /%
      Without TiO25 nm TiO210 nm TiO215 nm TiO220 nm TiO2
      4360055965593058955865-2.33
      5955905580557555705560-0.54
    • Table 2. Comparison between proposed sensor and formerly reported PCF sensors

      View table

      Table 2. Comparison between proposed sensor and formerly reported PCF sensors

      ReferenceYearFilm structureDetection rangeMaximum SW /(nm/RIU)Resolution /(10-6 RIU)FOM /RIU-1
      Ref. [312019ITO1.19‒1.29107009.93
      Ref. [322020Au1.13‒1.35175005.71186
      Ref. [332021ITO‑graphene1.21‒1.32120008.33
      Ref. [342022Au1.28‒1.32153466.52
      This workTiO2‒Au1.22‒1.32267003.75125
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    Kai Yan, Wei Xu, Qingyun Chen, Chen Zhu, Wei Li. D-Shaped Photonic Crystal Fiber Plasmonic Sensor with Dual-Open-Circular Channel for Low Refractive Index Detection[J]. Acta Optica Sinica, 2025, 45(3): 0306003

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    Paper Information

    Category: Fiber Optics and Optical Communications

    Received: Sep. 21, 2024

    Accepted: Nov. 11, 2024

    Published Online: Feb. 20, 2025

    The Author Email: Li Wei (liw@njupt.edu.cn)

    DOI:10.3788/AOS241578

    CSTR:32393.14.AOS241578

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