Photonics Research, Volume. 2, Issue 2, 59(2014)

Engineering ultra-flattened-dispersion photonic crystal fibers with uniform holes by rotations of inner rings

Jin Hou1、*, Jiajia Zhao1, Chunyong Yang1, Zhiyou Zhong1, Yihua Gao2, and and Shaoping Chen1
Author Affiliations
  • 1Hubei Key Laboratory of Intelligent Wireless Communications, College of Electronics and Information Engineering, South-central University for Nationalities, Wuhan, Hubei 430074, China
  • 2Wuhan National Laboratory for Optoelectronics (WNLO), School of Physics, Huazhong University of Science and Technology, Wuhan, Hubei 430074, China
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    Figures & Tables(8)
    Schematic topology of the proposed PCFs structure. The air holes in the silica background are arranged in a triangular configuration of lattice constant Λ with the central air hole missing, and all air holes have a uniform diameter d. The first and second innermost air-hole rings (colored green and yellow, respectively) are rotated around the fiber core with angles of α degrees and β degrees relative to their original positions, respectively. And the original positions of air holes in the inner rings are denoted as dashed circles in the right panel.
    Chromatic dispersion D as a function of wavelength λ with Λ=2.3 μm and d=0.61 μm for changing one of the design parameters: (a) α is changing from 0° to 30°, while β is fixed, and (b) β is changing from 0° to 30°, while α is fixed.
    Fundamental mode transverse electric field intensity (Et2) distributions at 1.45 μm (upper figures) and 1.75 μm (lower figures) wavelengths, for nearly zero-dispersion flattened PCFs with Λ=2.3 μm and d=0.61 μm for (a) α=0° and β=0°, (b) α=30° and β=0°, (c) α=0° and β=30°, (d) α=0° and β=0°, (e) α=30° and β=0°, and (f) α=0° and β=30°.
    Chromatic dispersion D as a function of wavelength λ with Λ=2.3 μm and d=0.61 μm for changing α from 0° to 59°, while β has an optimized value of 20°.
    Chromatic dispersion D as a function of the wavelength λ, for changing structure parameters α or β from 0° to 30° while reserving the other parameters, for (a) normal ultra-flattened-dispersion PCF with Λ=2.7 μm and d=0.75 μm, and (b) abnormal ultra-flattened-dispersion PCF with Λ=2.2 μm and d=0.54 μm.
    Chromatic dispersion as a function of the wavelength λ, for the changing α (a) normal ultra-flattened-dispersion PCF with β=16°, Λ=2.7 μm, and d=0.75 μm, and (b) abnormal ultra-flattened-dispersion PCF with β=22°, Λ=2.2 μm, and d=0.54 μm.
    Chromatic dispersion D as a function of the wavelength λ with Λ=2.3 μm and d=0.61 μm; α or/ and β are varied from their optimum values of α=0° and β=20°.
    • Table 1. Effective Mode Areas at λ=1.55μm for Different Parameters with Λ=2.3μm and d=0.61μm

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      Table 1. Effective Mode Areas at λ=1.55μm for Different Parameters with Λ=2.3μm and d=0.61μm

      α[°]β[°]Aeff[μm2]
      02031.7186
      0+020+331.8863
      0+020331.3310
      0+320+031.5597
      0320+031.8842
      0+320331.1745
      0320+332.0136
      0+320+331.7454
      0320331.5134
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    Jin Hou, Jiajia Zhao, Chunyong Yang, Zhiyou Zhong, Yihua Gao, and Shaoping Chen, "Engineering ultra-flattened-dispersion photonic crystal fibers with uniform holes by rotations of inner rings," Photonics Res. 2, 59 (2014)

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    Paper Information

    Category: Photonic Crystals

    Received: Nov. 1, 2013

    Accepted: Feb. 21, 2014

    Published Online: Nov. 5, 2014

    The Author Email: Jin Hou (houjin@mail.scuec.edu.cn)

    DOI:10.1364/PRJ.2.000059

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