• Chinese Optics Letters
  • Vol. 16, Issue 3, 032301 (2018)
Jing Ma1, Dongdong Liu2, Jicheng Wang1、3、*, and Zhengda Hu1
Author Affiliations
  • 1School of Science, Jiangnan University, Wuxi 214122, China
  • 2School of Mathematics & Physics Science, Xuzhou University of Technology, Xuzhou 221018, China
  • 3State Key Laboratory of Millimeter Waves, Southeast University, Nanjing 210096, China
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    DOI: 10.3788/COL201816.032301 Cite this Article Set citation alerts
    Jing Ma, Dongdong Liu, Jicheng Wang, Zhengda Hu. Plasmonic sensor with variable claddings based on metallic slit arrays[J]. Chinese Optics Letters, 2018, 16(3): 032301 Copy Citation Text show less
    (a) Schematic of the proposed metallic nanoslit arrays with a top variable dielectric and a CYTOP substrate. (b) Schematic of the fabrication process for the proposed structure.
    Fig. 1. (a) Schematic of the proposed metallic nanoslit arrays with a top variable dielectric and a CYTOP substrate. (b) Schematic of the fabrication process for the proposed structure.
    (a) Transmission spectrum of the top-layer silica with normal incidence. Magnetic field distributions of the device region at (b) CM2, (c) SPP-CM, and (d) CM1.
    Fig. 2. (a) Transmission spectrum of the top-layer silica with normal incidence. Magnetic field distributions of the device region at (b) CM2, (c) SPP-CM, and (d) CM1.
    Comparison of the transmission spectra of (a) different top materials and (b) gain-assisted materials (the inset provides a clear picture of the peak position).
    Fig. 3. Comparison of the transmission spectra of (a) different top materials and (b) gain-assisted materials (the inset provides a clear picture of the peak position).
    Transmission spectra for incident angles from 5° to 30°. Different color lines denote distinct incident angles. The inset figure shows the schematic structure of the oblique incidence with variable incident angle α. The wavelength of incident light is 1 μm, and the other parameters remain constant.
    Fig. 4. Transmission spectra for incident angles from 5° to 30°. Different color lines denote distinct incident angles. The inset figure shows the schematic structure of the oblique incidence with variable incident angle α. The wavelength of incident light is 1 μm, and the other parameters remain constant.
    (a) Transmission spectra of the first-order CM of the periodic metal structure with different values of period. (b) Transmission intensities as a function of the corresponding wavelength (λ3) and period.
    Fig. 5. (a) Transmission spectra of the first-order CM of the periodic metal structure with different values of period. (b) Transmission intensities as a function of the corresponding wavelength (λ3) and period.
    Simulated transmission spectra of the designed structure with P = 600 nm, D = 460 nm, and different duty cycle values from 0.05 to 0.15.
    Fig. 6. Simulated transmission spectra of the designed structure with P=600nm, D=460nm, and different duty cycle values from 0.05 to 0.15.
    (a) Transmission intensity as a function of wavelength (λ3) and slit depth. (b) Wavelength sensitivity of the resonance peak of CM1 and its FOM as functions of depth. Other parameters: normal incidence, P = 600 nm, W= 30 nm, and d = 200 nm.
    Fig. 7. (a) Transmission intensity as a function of wavelength (λ3) and slit depth. (b) Wavelength sensitivity of the resonance peak of CM1 and its FOM as functions of depth. Other parameters: normal incidence, P=600nm, W=30nm, and d=200nm.
    Jing Ma, Dongdong Liu, Jicheng Wang, Zhengda Hu. Plasmonic sensor with variable claddings based on metallic slit arrays[J]. Chinese Optics Letters, 2018, 16(3): 032301
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