• Acta Optica Sinica
  • Vol. 42, Issue 2, 0206005 (2022)
Xiangjie Jia, Pengfei Hao, Min Li, Xiaoyan Wen, and Haifei Lu*
Author Affiliations
  • School of Science, Wuhan University of Technology, Wuhan, Hubei 430070, China
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    DOI: 10.3788/AOS202242.0206005 Cite this Article Set citation alerts
    Xiangjie Jia, Pengfei Hao, Min Li, Xiaoyan Wen, Haifei Lu. Resonance Modes and Influencing Factors of Micro Sensing Unit on Fiber End Face[J]. Acta Optica Sinica, 2022, 42(2): 0206005 Copy Citation Text show less
    Two-dimensional simulation model of gold grating-insulator-gold film
    Fig. 1. Two-dimensional simulation model of gold grating-insulator-gold film
    Reflection spectra of resonator under different incident light. (a) TE light incident; (b) TM light incidence
    Fig. 2. Reflection spectra of resonator under different incident light. (a) TE light incident; (b) TM light incidence
    Reflection spectra of TM light incident at different dielectric layer thicknesses. (a) 30 nm; (b) 600 nm
    Fig. 3. Reflection spectra of TM light incident at different dielectric layer thicknesses. (a) 30 nm; (b) 600 nm
    Distribution of Y-direction electric field components under different resonance modes. (a) 1st order TM0 resonance mode, λ=1671.69 nm; (b) 2nd order TM0 resonance mode, λ=985.84 nm; (c) 3rd order TM0 resonance mode, λ=795.22 nm; (d) Bloch surface mode, λ=1300.38 nm
    Fig. 4. Distribution of Y-direction electric field components under different resonance modes. (a) 1st order TM0 resonance mode, λ=1671.69 nm; (b) 2nd order TM0 resonance mode, λ=985.84 nm; (c) 3rd order TM0 resonance mode, λ=795.22 nm; (d) Bloch surface mode, λ=1300.38 nm
    Distribution of X-direction electric field component in case of F-P resonance mode with TM light incident and t=600 nm. (a) 1st order F-P resonance mode, λ=1868.91 nm; (b) 2nd order F-P resonance mode, λ=957.16 nm
    Fig. 5. Distribution of X-direction electric field component in case of F-P resonance mode with TM light incident and t=600 nm. (a) 1st order F-P resonance mode, λ=1868.91 nm; (b) 2nd order F-P resonance mode, λ=957.16 nm
    Resonance diagram of TM0 mode
    Fig. 6. Resonance diagram of TM0 mode
    Symmetric metal-coated dielectric waveguide model
    Fig. 7. Symmetric metal-coated dielectric waveguide model
    Performance of MIM structure with cavity length t=70 nm. (a) Reflection spectrum chromatics at different grating widths W; (b) variation curve of effective refractive index of TM0 resonant mode with wavelength
    Fig. 8. Performance of MIM structure with cavity length t=70 nm. (a) Reflection spectrum chromatics at different grating widths W; (b) variation curve of effective refractive index of TM0 resonant mode with wavelength
    Performance of MIM structure under different refractive index of intermediate dielectric layer. (a) Reflection spectrum chromatics; (b) variation curve of effective refractive index of TM0 resonant mode with wavelength
    Fig. 9. Performance of MIM structure under different refractive index of intermediate dielectric layer. (a) Reflection spectrum chromatics; (b) variation curve of effective refractive index of TM0 resonant mode with wavelength
    Reflection spectrum chromatics and Y-direction electric field component at resonant wavelength under different grating thicknesses tg. (a) Reflection spectrum chromatics under different grating thicknesses tg; (b) tg=20 nm, Y-direction electric field component at resonance wavelength; (c) tg=200 nm, Y-direction electric field component at resonance wavelength
    Fig. 10. Reflection spectrum chromatics and Y-direction electric field component at resonant wavelength under different grating thicknesses tg. (a) Reflection spectrum chromatics under different grating thicknesses tg; (b) tg=20 nm, Y-direction electric field component at resonance wavelength; (c) tg=200 nm, Y-direction electric field component at resonance wavelength
    Reflection spectrum and Y-direction electric field component at resonant wavelength under different grating periods P. (a) Reflection spectrum chromatics under different grating periods P; (b) P=900 nm, Y-direction electric field component at resonance wavelength; (c) P=1200 nm, Y-direction electric field component at resonance wavelength
    Fig. 11. Reflection spectrum and Y-direction electric field component at resonant wavelength under different grating periods P. (a) Reflection spectrum chromatics under different grating periods P; (b) P=900 nm, Y-direction electric field component at resonance wavelength; (c) P=1200 nm, Y-direction electric field component at resonance wavelength
    Reflection spectrum chromatics and Y-direction electric field component at resonant wavelength under different gold film reflector thicknesses tm. (a) Reflection spectrum chromatics under different gold film reflector thicknesses tm; (b) tm=20 nm, Y-direction electric field component at resonance wavelength; (c) tm=200 nm, Y-direction electric field component at resonance wavelength
    Fig. 12. Reflection spectrum chromatics and Y-direction electric field component at resonant wavelength under different gold film reflector thicknesses tm. (a) Reflection spectrum chromatics under different gold film reflector thicknesses tm; (b) tm=20 nm, Y-direction electric field component at resonance wavelength; (c) tm=200 nm, Y-direction electric field component at resonance wavelength
    Performance curves of resonant wavelength and effective refractive index of nano-resonator under different conditions. (a) After refractive index of medium in cavity is fixed, resonant wavelength of nano-resonator varies with length of the cavity; (b) refractive index n of medium in cavity is 1.4, and effective refractive index of nano-resonator with different cavity lengths; (c) after cavity length is fixed, resonant wavelength of nano-resonator varies with refractive index; (d) cavity length t=50 nm, effective refractive index of nano-resonator under different refractive index
    Fig. 13. Performance curves of resonant wavelength and effective refractive index of nano-resonator under different conditions. (a) After refractive index of medium in cavity is fixed, resonant wavelength of nano-resonator varies with length of the cavity; (b) refractive index n of medium in cavity is 1.4, and effective refractive index of nano-resonator with different cavity lengths; (c) after cavity length is fixed, resonant wavelength of nano-resonator varies with refractive index; (d) cavity length t=50 nm, effective refractive index of nano-resonator under different refractive index
    SEM images under different magnification of fiber end grating . (a) 2000×; (b) 10000×
    Fig. 14. SEM images under different magnification of fiber end grating . (a) 2000×; (b) 10000×
    Assembly system diagram and F-P resonant interference spectrum. (a) Five-dimensional displacement control platform, CCDs in horizontal and vertical planes; (b) optical fiber clamp and gold mirror platform; (c) position relative position of optical fiber and gold mirror observed by CCD; (d) F-P resonant interference spectra at different distances
    Fig. 15. Assembly system diagram and F-P resonant interference spectrum. (a) Five-dimensional displacement control platform, CCDs in horizontal and vertical planes; (b) optical fiber clamp and gold mirror platform; (c) position relative position of optical fiber and gold mirror observed by CCD; (d) F-P resonant interference spectra at different distances
    Assembly flowchart of optical fiber end nano-resonant structure
    Fig. 16. Assembly flowchart of optical fiber end nano-resonant structure
    Length sensitivity (λi-λj) /10Refractive index
    1.01.11.21.31.4
    (λ10 nm-λ20 nm)/1014.3316.2018.9322.1126.50
    (λ20 nm-λ30 nm)/106.256.747.237.787.72
    (λ30 nm-λ40 nm)/104.024.794.134.434.77
    (λ40 nm-λ50 nm)/102.562.733.433.162.84
    Table 1. Response sensitivity of nano-resonator to cavity length variation with fixed refractive index of medium in cavity
    ParameterCavity length /nm
    1020304050
    Refractive index sensitivity /(nm·RIU-1)884.86639.77581.86562.37565.63
    Table 2. Response sensitivity of resonator with different cavity length to refractive index change of medium in cavity
    Xiangjie Jia, Pengfei Hao, Min Li, Xiaoyan Wen, Haifei Lu. Resonance Modes and Influencing Factors of Micro Sensing Unit on Fiber End Face[J]. Acta Optica Sinica, 2022, 42(2): 0206005
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