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Decoupled polarization dynamics of incoherent waves and bimodal spectral incoherent solitons

机译:非相干波和双峰谱非相干孤子的解耦极化动力学

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We consider the propagation of strongly incoherent waves in optical fibers in the framework of the vector nonlinear Schrodinger equation (VNLSE) accounting for the Raman effect. On the basis of the wave turbulence theory, we derive a kinetic equation that greatly simplifies the VNLSE and provides deep physical insight into incoherent wave dynamics. When applied to the study of polarization effects, the theory unexpectedly reveals that the linear polarization components of the incoherent wave evolve independently from each other, even in the presence of weak fiber birefringence. When applied to light propagation in bimodal fibers, the theory reveals that the incoherent modal components can be strongly coupled. After a complex transient, the modal components self-organize into a vector spectral incoherent soliton: The two solitons self-trap and propagate with a common velocity in frequency space. (C) 2016 Optical Society of America
机译:我们在考虑拉曼效应的矢量非线性薛定inger方程(VNLSE)的框架内考虑了强非相干波在光纤中的传播。基于波湍流理论,我们得出了一个动力学方程,该方程极大地简化了VNLSE,并为非相干波动力学提供了深刻的物理见解。当应用于偏振效应研究时,该理论出乎意料地揭示出,即使在存在弱双折射光纤的情况下,非相干波的线性偏振分量也彼此独立地发展。当应用于双峰光纤中的光传播时,该理论表明,非相干模态分量可以强耦合。经过复杂的瞬变后,模态分量会自组织为矢量谱非相干孤子:两个孤子会自陷并以相同的速度在频率空间中传播。 (C)2016美国眼镜学会

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