以ns脉冲泵浦的扭曲光纤中脉冲破碎过程中产生的孤子的偏振特性

Ariel Flores Rosas, Orlando Díaz Hernández, Roberto Arceo, Gerardo J. Escalera Santos, Sergio Mendoza Vázquez, Elizeth Ramírez Álvarez, Christian I. Enriquez Flores, E. Kuzin
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摘要

普通光纤是随机双折射的,在光纤中形成和传播的孤子是随机偏振的。然而,我们希望孤子具有明确定义的极化。当泵浦脉冲相对较长时,调制不稳定性(MI)和受激拉曼散射(SRS)的非线性效应在超连续谱(SC)产生的初始阶段占主导地位;调制不稳定性导致脉冲破裂和形成短脉冲,最终演变成一堆孤子和色散波。本文研究了在标准光纤(SMF-28)中,受纳秒级泵浦脉冲调制不稳定性的影响,在光纤扭曲引入圆形双折射的情况下,脉冲破裂过程中形成的孤子的偏振特性,发现扭曲光纤减轻了随机线性双折射。研究发现,孤子的极化椭圆率是随机分布的;然而,平均极化椭圆度比输入脉冲的极化椭圆度更接近圆形。在实验装置中。采用200 m的SMF-28纤维,捻制6匝/m。我们用1ns脉冲泵浦光纤。结果表明,在圆偏振处,输入脉冲孤子在光纤输出处具有接近圆的偏振,而在无扭转光纤中,孤子的偏振是随机的。
本文章由计算机程序翻译,如有差异,请以英文原文为准。
Polarization Properties of the Solitons Generated in the Process of Pulse Breakup in Twisted Fiber Pumped by ns Pulses
Common optical fibers are randomly birefringent, and solitons formatting and traveling in them are randomly polarized. However, it is desirable to have solitons with a well-defined polarization. With pump relatively long pulses, the nonlinear effects of modulation instability (MI) and stimulated Raman scattering (SRS) are dominant at the initial stage of the process of supercontinuum (SC) generation; modulation instability results in pulse breakup and formation of short pulses that evolve finally to a bunch of solitons and dispersive waves. We do the research of the polarization of solitons formed by the pulse breakup process by the effect of modulation instability with pump pulses of nanoseconds in standard fiber (SMF-28) with circular birefringence introduced by fiber twist, and the twisted fiber mitigates the random linear birefringence. In this work, we found that polarization ellipticity of solitons is distributed randomly; nevertheless, the average polarization ellipticity is closer to the circular than the polarization ellipticity of the input pulse. In the experimental setup. 200 m of SMF-28 fiber twisted by 6 turns/m was used. We used 1 ns pulse to pump the fiber. The results showed that at circular polarization of the input pulse solitons at the fiber output have polarizations close to the circular, while in the fiber without twist, the soliton polarization was random.
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