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中国物理学会期刊

声波导单模光纤中后向受激布里渊散射的声模分析

CSTR: 32037.14.aps.73.20231710

Analysis of acoustic modes induced by backward stimulated Brillouin scattering in acoustic wave-guided single mode optical fibers

CSTR: 32037.14.aps.73.20231710
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  • 本文推导了单模光纤中的声波亥姆霍兹方程, 利用分离变量法求解并获得正规声波导导模的特征方程, 定义了声模的归一化频率, 结合贝塞尔函数的宗量近似分析了声波模式的特征值范围、截止频率和远离截止, 探讨了声模的色散和布里渊增益谱的多峰成因. 研究结果表明单模光纤中纵向声波基模L01模无截止, 主要被限制在纤芯中, 与光基模耦合形成布里渊增益谱的主峰; 高阶声模都存在低频截止, 在包层分布比基模多, 与LP01模耦合形成布里渊增益谱的次峰. 只有纵向L0n声模对后向布里渊增益谱有贡献, 纤芯掺锗浓度增大能使布里渊增益谱发生红移, 声模数量增多, L01模的增益峰值逐渐变大而高阶模的贡献减小. 泵浦波长为1.55 μm, 纤芯掺锗浓度3.65%、纤芯半径4.2 μm的单模光纤存在4个L0n和16个Lmn (m > 0)声模, 声模L01, L03, L04与光模LP01声光耦合产生布里渊增益谱的1个主峰和2个弱峰; 纤芯掺锗浓度15%, 纤芯半径1.3 μm的单模光纤存在3个L0n模和7个Lmn (m > 0)模, L01, L02, L03模与LP01模声光耦合使得布里渊增益谱呈现3个主峰. 这些结论可以完全解释相应的实验现象, 也为光纤SBS声波导研究及应用提供理论参考.

     

    In this work, the acoustic Helmholtz equation is derived, and its analytical solution and the characteristic equation of the uniform guide mode in single mode fibers are obtained by the method of separation of variables. The normalized frequency of the acoustic mode is defined. By combining the argument approximation of the Bessel function are analyzed the eigenvalue range of the acoustic mode, the cut-off frequency, far from the cut-off state of the acoustic mode induced by backward stimulated Brillouin scattering, the dispersion and the multi-peak Brillouin gain spectrum. The research results indicate that the longitudinal acoustic fundamental mode L01 cannot be cut-off and is mainly confined in the fiber core, which is coupled with the optical fundamental mode LP01 to form the main peak of the Brillouin gain spectrum. The other higher-order acoustic modes all have low cut-off frequencies and are distributed more in the fiber cladding than mode L01 which couples with the optical fundamental mode LP01 to form the subpeaks of the Brillouin gain spectrum. The transverse normalized phase constant and effective refractive index of the acoustic mode increase with normalized frequency increasing. Only longitudinal acoustic modes L0n contribute to backward Brillouin gain spectrum in single mode fiber. When the GeO2 concentration is less than 4% and core radius is 4.5 μm, the single mode characteristics of the fiber remain unchanged, but the maximum number of acoustic L0n modes is 4. With the increase of GeO2 concentration in the fiber core, the Brillouin gain spectrum is red-shifted and the number of acoustic modes increases, the Brillouin gain peak value of L01 mode gradually increases, and the contributions of higher-order modes decrease. The single-mode fiber with a core’s germanium doped concentration of 3.65% and core radius of 4.3 μm has 4 L0n modes and 16 Lmn (m>0) modes at a wavelength of 1.55 μm, with one main peak and two subpeaks in the Brillouin gain spectrum appearing due to the acousto-optic coupling of the acoustic L01, L03, and L04 modes with the optical LP01 mode. The single-mode fiber with a core’s germanium doped concentration of 15% and core radius of 1.3 μm has 3 L0n modes and 7 Lmn (m>0) modes, with the Brillouin gain spectrum having 3 main peaks due to the acousto-optic coupling of the L01, L02, and L03 modes with the LP01 mode. These conclusions are well consistent with the reported experimental phenomena and provide theoretical references for studying and utilizing the SBS acoustic waveguide in optical fibers.

     

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