• Acta Photonica Sinica
  • Vol. 50, Issue 7, 59 (2021)
Junchi LAI, Shanglin HOU, Jingli LEI, and Xiaoxiao LI
Author Affiliations
  • School of Science, Lanzhou University of Technology, Lanzhou730050, China
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    DOI: 10.3788/gzxb20215007.0706005 Cite this Article
    Junchi LAI, Shanglin HOU, Jingli LEI, Xiaoxiao LI. Characteristics of Reflection Spectrum of Brillouin Dynamic Grating in Single Mode Fibers[J]. Acta Photonica Sinica, 2021, 50(7): 59 Copy Citation Text show less

    Abstract

    The Brillouin dynamic grating model is developed based on the stimulated Brillouin scattering and elastic acoustic theory. The reflection spectrum of the Brillouin dynamic grating is calculated based on the fiber Bragg grating theory, and it is demonstrated that the Bragg wavelength downshifts by Brillouin frequency shift equals the Doppler frequency shift. The reflectivity and the spectral width are calculated when the pump power ranges from 0.1 W to 30 W, the pulse width ranges from 2 ns to 10 ns and the core diameter of a single mode fiber ranges from 8 μm to 10 μm. When the power increases to 30 W and the pump pulse width reaches 10 ns, the peak reflectivity is 2.17×10-6 and 7.16×10-9, respectively. The spectral width of the reflection spectrum decreases with the increase of pulse width. When the pulse width is 10 ns, the minimum spectral width is 1.2×10-4 nm. When the fiber core diameter decreases to 8 μm, the peak reflectivity increases to 6.64×10-11. The results show that the reflectivity of the Brillouin dynamic grating is positive correlation with the power and the pulse width of the pump wave, but it is negative correlation with the core diameter of optical fiber. The spectral width of the reflection spectrum is not affected by the power of the pump wave and the diameter of the fiber core, but it is negative correlation with the pulse width.
    E˜(z,t)=i=14E˜i(z,t)(1)

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    E˜i(z,t)=Aiejkiz-ωit+c.c(2)

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    ρ˜(z,t)=Δρejqz-Ωt+c.c(3)

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    Ω=2vc/neffω1(4)

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    P+Γρ0u+ρut=12ε0γe(E˜2)(5)

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    u+1ρ0ρt=0(6)

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    2P-Γρt-2ρt2=12ε0γe2(E˜2)(7)

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    M=ρ0Pρ(8)

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    2ρ-ρ0MΓρt-ρ0M2ρt2=12ρ0Mε0γe2(E˜2)(9)

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    ρ0M=1v2(10)

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    2ρ-1v2Γρt-1v22ρt2=12v2ε0γe2(E˜2)(11)

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    Δρ=1v2ε0γeA1A2(12)

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    v2=1Cρ0(13)

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    Δε˜=ερρ˜=γeρ˜ρ0(14)

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    Δε˜=(Cε0γe2A1A2)ejqz-Ωt(15)

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    n˜=Re1+χ(1)+χ(3)E(z,t)2(16)

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    Δn˜=12neffRe(χ(3))(17)

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    Δn˜=12neffΔε˜=ε0γe2C2neffA1A2ejqz-Ωt(18)

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    Δn˜=ε0γe2CA1A22neffcos(Ωt±qz)(19)

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    n=neff+Δn˜(20)

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    n=neff+Vδneff¯cos(Ωt±2πΛz)(21)

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    r=-κsinh(κ2-σ̂2L)σ̂sinh(κ2-σ̂2L)+iκ2-σ̂2cosh(κ2-σ̂2L)(22)

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    L=tP1+tP2c/4neff(23)

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    κ=π2λneffε0γe2CA1A2(24)

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    σ̂=2πneffΔf/c(25)

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    R=|r|2=sinh2(κ2-σ̂2L)cosh2(κ2-σ̂2L)-σ̂2κ2(26)

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    Rmax=tanh2(κL)(27)

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    ω'=ωpcneff+vcneff-v12(28)

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    Junchi LAI, Shanglin HOU, Jingli LEI, Xiaoxiao LI. Characteristics of Reflection Spectrum of Brillouin Dynamic Grating in Single Mode Fibers[J]. Acta Photonica Sinica, 2021, 50(7): 59
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