• Chinese Optics Letters
  • Vol. 17, Issue 4, 042801 (2019)
Dejing Gong1、2, Yinquan Yuan1、*, Lei Liang1、2, and Minghong Yang1、**
Author Affiliations
  • 1National Engineering Laboratory for Fiber Optic Sensing Technology, Wuhan University of Technology, Wuhan 430070, China
  • 2School of Information Engineering, Wuhan University of Technology, Wuhan 430070, China
  • show less
    DOI: 10.3788/COL201917.042801 Cite this Article Set citation alerts
    Dejing Gong, Yinquan Yuan, Lei Liang, Minghong Yang. Theoretical study on negative permittivity of the material producing sharp surface plasmon resonance dips[J]. Chinese Optics Letters, 2019, 17(4): 042801 Copy Citation Text show less
    Configuration of optical fiber SPR sensors.
    Fig. 1. Configuration of optical fiber SPR sensors.
    Permittivity of Au and NPM. Squares, Lorent–Drude model; circles, Drude model; solid, real part; open, imaginary part of the permittivity; solid, dash, dot, and dash dot lines are drawn according to εre=εre0−0.065λ, and the values of εre0 are 20, 25, 30, and 35, respectively.
    Fig. 2. Permittivity of Au and NPM. Squares, Lorent–Drude model; circles, Drude model; solid, real part; open, imaginary part of the permittivity; solid, dash, dot, and dash dot lines are drawn according to εre=εre00.065λ, and the values of εre0 are 20, 25, 30, and 35, respectively.
    Normalized transmitted powers corresponding to different values of (a) εim, (b) εre0, and (c) k1.
    Fig. 3. Normalized transmitted powers corresponding to different values of (a) εim, (b) εre0, and (c) k1.
    Effect of NPM layer thickness.
    Fig. 4. Effect of NPM layer thickness.
    Transmitted spectra for the sensing layers with different RIs.
    Fig. 5. Transmitted spectra for the sensing layers with different RIs.
    (a) Resonance wavelengths and (b) FWHMs of optical fiber SPR sensors coated with NPM1, NPM2, and NPM3.
    Fig. 6. (a) Resonance wavelengths and (b) FWHMs of optical fiber SPR sensors coated with NPM1, NPM2, and NPM3.
    Dependence of reflectivity on the wavelength and incident angle for different thicknesses of NPM layers.
    Fig. 7. Dependence of reflectivity on the wavelength and incident angle for different thicknesses of NPM layers.
    Reflected spectra of prism-based SPR sensors corresponding to different values of (a) εim, (b) εre0, and (c) k.
    Fig. 8. Reflected spectra of prism-based SPR sensors corresponding to different values of (a) εim, (b) εre0, and (c) k.
    Reflected spectra of prism-based SPR sensors coated with (a) NPM1, (b) NPM2, and (c) NPM3.
    Fig. 9. Reflected spectra of prism-based SPR sensors coated with (a) NPM1, (b) NPM2, and (c) NPM3.
    (a) Resonance angles and (b) FWHMs of prism-based SPR sensors coated with NPM1, NPM2, and NPM3.
    Fig. 10. (a) Resonance angles and (b) FWHMs of prism-based SPR sensors coated with NPM1, NPM2, and NPM3.
    Dejing Gong, Yinquan Yuan, Lei Liang, Minghong Yang. Theoretical study on negative permittivity of the material producing sharp surface plasmon resonance dips[J]. Chinese Optics Letters, 2019, 17(4): 042801
    Download Citation