• Chinese Optics Letters
  • Vol. 18, Issue 3, 030603 (2020)
Zhuang Huo, Exian Liu, and Jianjun Liu*
Author Affiliations
  • Key Laboratory for Micro/Nano Optoelectronic Devices of Ministry of Education & Hunan Provincial Key Laboratory of Low-Dimensional Structural Physics and Devices, School of Physics and Electronics, Hunan University, Changsha 410082, China
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    DOI: 10.3788/COL202018.030603 Cite this Article Set citation alerts
    Zhuang Huo, Exian Liu, Jianjun Liu. Hollow-core photonic quasicrystal fiber with high birefringence and ultra-low nonlinearity[J]. Chinese Optics Letters, 2020, 18(3): 030603 Copy Citation Text show less
    (a) Cross section structure of the six-fold photonic quasicrystal (the origin O of the coordinate system OXY is set at the center of the fiber core); (b) the cross section structure of HC-PQF.
    Fig. 1. (a) Cross section structure of the six-fold photonic quasicrystal (the origin O of the coordinate system OXY is set at the center of the fiber core); (b) the cross section structure of HC-PQF.
    Mode field distribution of HC-PQF: (a) direction of X polarization; (b) direction of Y polarization; (c) the effective refractive index of the X and Y polarization modes, and the corresponding birefringence.
    Fig. 2. Mode field distribution of HC-PQF: (a) direction of X polarization; (b) direction of Y polarization; (c) the effective refractive index of the X and Y polarization modes, and the corresponding birefringence.
    Birefringence of HC-PQF under different d1 values filled with air.
    Fig. 3. Birefringence of HC-PQF under different d1 values filled with air.
    When d1=2.17 μm, the effect of filling ratio on birefringence.
    Fig. 4. When d1=2.17μm, the effect of filling ratio on birefringence.
    When d/Λ=0.910 and d1=2.17 μm, the effect of changing the distance r between the d2 small air hole and the fiber core on birefringence.
    Fig. 5. When d/Λ=0.910 and d1=2.17μm, the effect of changing the distance r between the d2 small air hole and the fiber core on birefringence.
    d/Λ=0.910, d1=2.17 μm, r=1.50Λ, changing the core filling gas: (a) the relationship between mode field area and wavelength, (b) the relationship between nonlinear coefficient and wavelength.
    Fig. 6. d/Λ=0.910, d1=2.17μm, r=1.50Λ, changing the core filling gas: (a) the relationship between mode field area and wavelength, (b) the relationship between nonlinear coefficient and wavelength.
    Influence of the diameter of the hollow core on dispersion characteristics with d/Λ=0.91 and r=1.50Λ.
    Fig. 7. Influence of the diameter of the hollow core on dispersion characteristics with d/Λ=0.91 and r=1.50Λ.
    PCF structureRef.BirefringenceNonlinear coefficient (W-1·km-1)
    PC-PCF[34]0.005/
    HC-PCF[35]5.8×103/
    SGNLC-PCF[36]0.042425.5
    Proposed HC-PQFThis work1.345×1021.63×103
    Table 1. Parameter Comparison of this HC-PQF with Previous Designs
    Zhuang Huo, Exian Liu, Jianjun Liu. Hollow-core photonic quasicrystal fiber with high birefringence and ultra-low nonlinearity[J]. Chinese Optics Letters, 2020, 18(3): 030603
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