• Acta Optica Sinica
  • Vol. 37, Issue 8, 0828002 (2017)
Jiantao Lü1、2, Chunming Wang2、*, Chenghao Zhu3, and Hai Liu3
Author Affiliations
  • 1 School of Physics and Optoelectronic Engineering, Foshan University, Foshan, Guangdong 528000, China
  • 2 School of Materials Science and Engineering, Huazhong University of Science and Technology, Wuhan, Hubei 430074, China
  • 3 School of Information and Control Engineering, China University of Mining and Technology, Xuzhou, Jiangsu 221116, China
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    DOI: 10.3788/AOS201737.0828002 Cite this Article Set citation alerts
    Jiantao Lü, Chunming Wang, Chenghao Zhu, Hai Liu. Dual-Core Photonic Crystal Fiber Transverse-Stress Sensor Based on Surface Plasmon Resonance[J]. Acta Optica Sinica, 2017, 37(8): 0828002 Copy Citation Text show less
    Diagram of cross section structure of dual-core PCF transverse-stress sensor based on SPR
    Fig. 1. Diagram of cross section structure of dual-core PCF transverse-stress sensor based on SPR
    Deformation in x direction for different air hole layers of PCF when F=3 N
    Fig. 2. Deformation in x direction for different air hole layers of PCF when F=3 N
    Change of deformation under different diameters of big hole. (a) x direction; (b) y direction
    Fig. 3. Change of deformation under different diameters of big hole. (a) x direction; (b) y direction
    Change of deformation under different diameters of small hole. (a) x direction; (b) y direction
    Fig. 4. Change of deformation under different diameters of small hole. (a) x direction; (b) y direction
    Change of deformation under different lattice periods of small hole. (a) x direction; (b) y direction
    Fig. 5. Change of deformation under different lattice periods of small hole. (a) x direction; (b) y direction
    (a) Loss of fundamental mode under different transverse stresses; (b) relationship between wavelength of resonance peak and transverse stress (d1=8.3 μm, d2=7.06 μm, Λ1=8.68 μm, Λ2=8.15 μm)
    Fig. 6. (a) Loss of fundamental mode under different transverse stresses; (b) relationship between wavelength of resonance peak and transverse stress (d1=8.3 μm, d2=7.06 μm, Λ1=8.68 μm, Λ2=8.15 μm)
    (a) Loss of fundamental mode under different transverse stresses; (b) relationship between wavelength of resonance peak and transverse stress (d1=7.3 μm, d2=6.26 μm, Λ1=8.68 μm, Λ2=8.55 μm)
    Fig. 7. (a) Loss of fundamental mode under different transverse stresses; (b) relationship between wavelength of resonance peak and transverse stress (d1=7.3 μm, d2=6.26 μm, Λ1=8.68 μm, Λ2=8.55 μm)
    Jiantao Lü, Chunming Wang, Chenghao Zhu, Hai Liu. Dual-Core Photonic Crystal Fiber Transverse-Stress Sensor Based on Surface Plasmon Resonance[J]. Acta Optica Sinica, 2017, 37(8): 0828002
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