• Chinese Optics Letters
  • Vol. 18, Issue 1, 010602 (2020)
Weiqing Gao1, Liang Chen1、3, Wenhui Jiang1, Zhengxiong Zhang1, Xiu Zhang1, Panyun Gao1, Kang Xie2, Wei Zhang1、2、*, Yong Zhou1, Meisong Liao3, Takenobu Suzuki4, and Yasutake Ohishi4
Author Affiliations
  • 1Department of Optical Engineering, School of Electronic Science & Applied Physics, Hefei University of Technology, Hefei 230601, China
  • 2School of Instrument Science and Opto-electronics Engineering, Hefei University of Technology, Hefei 230009, China
  • 3R&D Center of High Power Laser Components, Shanghai Institute of Optics and Fine Mechanics, Chinese Academy of Sciences, Shanghai 201800, China
  • 4Research Center for Advanced Photon Technology, Toyota Technological Institute, Nagoya 468-8511, Japan
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    DOI: 10.3788/COL202018.010602 Cite this Article Set citation alerts
    Weiqing Gao, Liang Chen, Wenhui Jiang, Zhengxiong Zhang, Xiu Zhang, Panyun Gao, Kang Xie, Wei Zhang, Yong Zhou, Meisong Liao, Takenobu Suzuki, Yasutake Ohishi. Stimulated Brillouin scattering by the interaction between different-order optical and acoustical modes in an As2Se3 photonic crystal fiber[J]. Chinese Optics Letters, 2020, 18(1): 010602 Copy Citation Text show less
    Cross section of the As2Se3 PCF.
    Fig. 1. Cross section of the As2Se3 PCF.
    Brillouin gain spectrum in the PCF with a core diameter of 2.32 μm.
    Fig. 2. Brillouin gain spectrum in the PCF with a core diameter of 2.32 μm.
    Brillouin gain spectra in the As2Se3 PCFs with different core diameters.
    Fig. 3. Brillouin gain spectra in the As2Se3 PCFs with different core diameters.
    Frequency curve versus the core diameter for different acoustic modes in a cylindrical acoustic waveguide.
    Fig. 4. Frequency curve versus the core diameter for different acoustic modes in a cylindrical acoustic waveguide.
    (a) Brillouin gain spectra by different pump optical modes. (b) Brillouin gain spectra by the LP11 optical mode pump.
    Fig. 5. (a) Brillouin gain spectra by different pump optical modes. (b) Brillouin gain spectra by the LP11 optical mode pump.
    (a) Brillouin frequency shift versus the core diameter for different optical pump modes. (b) The effective index versus the core diameter for different optical pump modes.
    Fig. 6. (a) Brillouin frequency shift versus the core diameter for different optical pump modes. (b) The effective index versus the core diameter for different optical pump modes.
    Product of Brillouin threshold and effective fiber length versus the core diameter.
    Fig. 7. Product of Brillouin threshold and effective fiber length versus the core diameter.
    ρ(kg·m3)λ(μm)vl(m·s1)p12d(μm)dhole(μm)Λ(μm)
    4640222500.2661.160.841
    2.321.682
    4.763.364
    6.965.046
    9.286.728
    Table 1. Parameters of the As2Se3 PCF Used in Simulation
    Weiqing Gao, Liang Chen, Wenhui Jiang, Zhengxiong Zhang, Xiu Zhang, Panyun Gao, Kang Xie, Wei Zhang, Yong Zhou, Meisong Liao, Takenobu Suzuki, Yasutake Ohishi. Stimulated Brillouin scattering by the interaction between different-order optical and acoustical modes in an As2Se3 photonic crystal fiber[J]. Chinese Optics Letters, 2020, 18(1): 010602
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