温度对单模光纤偏振模色散的影响研究

随着光纤通信系统传输容量的不断发展 ,光纤中的偏振模色散 PMD成为限制高速光纤通信系统传输容量的极限因素。偏振模色散是由于光纤结构的不完善性或者受到外界应力的作用而产生的 ,因此偏振模色散受外界环境因素的影响较大。许多研究表明偏振模色散对温度具有较强的敏感性 ,是温度的函数。采用波长扫描法就温度对单模光纤偏振模色散的影响展开研究 ,研究结果表明 ,单模光纤偏振模色散将随着温度的升高而呈现减小的趋势     

偏振模色散对光纤数字通信系统影响的讨论

详细介绍了光纤偏振模色散产生的原因及描述模型 ,重点分析了光纤偏振模色散对光纤数字通信系统的影响 ,并指出了它是对未来高码率光纤数字传输系统的主要限制。最后讨论了光纤偏振模色散的补偿方法。     

光纤和光缆的偏振模色散系数研究

综述了偏振模色散的概念、偏振模色散对光传输系统的影响、系统对单模光纤偏振模色散系数的要求,以及获得小的偏振模色散光纤和光缆的方法.     

啁啾光纤光栅中偏振模色散的研究

首先介绍了不同种双折射率差Δn的光纤制成的啁啾光纤光栅中偏振模色散现象 ,然后说明了光栅中偏振模色散的大小与 Δ n的相关性 ,并阐述了对用于色散补偿作用的啁啾光纤光栅中偏振模色散的消除 (补偿 )方法 ,最后指出利用啁啾光纤光栅中大的偏振模色散对高速光通信系统传输线路中偏振模色散的补偿方法。     

高速光通信系统中偏振模色散的测量与补偿

论述了偏振模色散的偏振主态理论,在国内首次利用Sagnac干涉仪和偏分孤子法对偏振模色散进行测量,利用偏振控制器和保偏光纤实现光纤系统的偏振模色散补偿.     

高速光通信系统中偏振模色散的测量与补偿

论述了偏振模色散的偏振主态理论,在国内首次利用Sagnac干涉仪和偏分孤子法对偏振模色散进行测量,利用偏振控制器和保偏光纤实现光纤系统的偏振模色散补偿。     

高速光通信系统中偏振模色散的补偿

光纤中偏振模色散已成为高速光通信系统增容的主要障碍,文章对现有的各种偏振模色散补偿方法进行了综合评述。认为用偏振控制器与保偏光纤构成的夺模色散自动补偿系统是一种首选方案。     

光纤光栅偏振模色散研究

对光纤光栅的偏振模色散特性进行了深入的研究，特别是啁啾光纤光栅色散补偿器的偏振模色散。研究表明啁啾光纤光栅色散补偿器的偏振模色散主要由光栅的双折射系数、色散量决定，提出了制作低偏振模色散的色散补偿器的方法。     

光纤光栅偏振模色散的研究

分析了光纤光栅 (FBG)偏振模色散 (PMD)产生的原因 :写入光栅用的光敏光纤对紫外光吸收是不均匀的 ,呈指数型吸收。建立了光栅偏振模色散的模型 ,利用建立的模型计算了不同折射率调制的偏振模色散 ,计算的结果与用偏振模色散分析仪测得的结果符合得很好。理论和实验说明了光栅色散对偏振模色散的影响 :光纤光栅的色散增大 ,光栅的偏振模色散也增大。     

光纤光栅不同温度下偏振模色散的研究

光纤光栅的偏振模色散是由于在侧写入法写入光栅时,光敏光纤对紫外光的吸收不均匀造成的。分析了光纤光栅在不同温度下的偏振模色散,实验研究了光纤光栅的偏振模色散在-20~ 60℃的情况,统计结果表明,在不同温度下,光纤光栅的偏振模色散基本保持不变。     

Degree of Polarization in Anisotropic Single-Mode Optical Fibers: Theory

The degree of polarization for propagation waves in anisotropic single-mode fibers is formulated in terms of light source spectrum, incident polarization condition, and fiber parameters. The polarization degree deterioration is based on the incident wave split into two eigenpolarization modes inherent in the fiber. Since the two eigenpolarization modes have different group velocities from each other, the degree of polarization is degraded when both of the modes are excited. Polarization degree is preserved when only one of the eigenpolarization modes is excited. The degradation is determined by the mutual correlation function gamma, between the two modes, which depends on the light source spectra, fiber polarization dispersion, and fiber length.     

Analysis on state of polarization of stimulated Brillouinscattering in an optical fiber ring-resonator

As a basic study of a Brillouin fiber-optic gyro, the state of polarization of stimulated Brillouin scattering in an optical fiber ring-resonator is analyzed. A high-birefringent fiber ring-resonator with 90° polarization axis rotation at the splice is considered as a candidate to have a stable lasing. It has two special states of polarization as the lasing modes, namely the polarization lateral modes. The lasing frequencies, namely the longitudinal modes for one state are fixed just in the middle point between the two neighboring lasing frequencies for the other in this resonator. This means that the stable single mode lasing may be obtained. The lasing threshold, the alternation of the lasing modes are discussed both by the simplified theory and the strict theory     

Polarization Rotation in Twisted Polarization Maintaining Fibers Using a Fixed Reference Frame

In previous studies addressing polarization evolution in optical fibers, the frame of reference in which polarization rotation in twisted optical fibers is described lacks the compatibility with the modeling of some fiber sensor applications. We therefore introduce a formulation of the polarization evolution in a twisted optical and birefringent fiber, which is based on a laboratory coordinate system. We employ coupled mode theory using the fundamental modes of a single mode fiber as a basis. We treat the birefringence of the polarization maintaining fiber and the twist induced birefringence as perturbations introduced into this mode system.      

Polarization rotation in nonlinear bimodal optical fibers

The effect of nonlinear interactions on second-order modes in circular cross-section optical fibers is considered. In the linear case, analysis using the proper modes reveals that the fiber is a natural polarization rotator. An initial linearly polarized (LP) mode is actually a mixture of proper modes and recurs only periodically as the field propagates; at half-periods the input polarization and field pattern are rotated by 90°. Complete analytical expressions and numerical examples describing the modification of this phenomenon by nonlinearity are presented. For lower powers, the phenomenon persists with period increasing toward infinity at a transition point, beyond which complete polarization rotation is suppressed. At very high powers, the Kerr effect dominates: polarization is fixed in one direction and an LP mode does become a real mode of the system     

Coupling Charactor of Polarization Maintaining Optical Fiber Under the Condition of Bend^①②

In the field of optical fiber communication and sensing,polarization maintaining optical fiber with special polarization wave transmit character has been taken more and more attentions.It is more mportant of couple between polarization modes,with the help of microdisturbed and coupled mode theories ,the couples characters of high birefracting Bow-Tie optical fiber in the condition of pure bend are analysed,and power coupling relationships between transmit modes are also derivated.     

Investigation of polarization dispersion in long lengths of single-mode fiber using multilongitudinal mode lasers

We have used multilongitudinal mode lasers to investigate the polarization properties of long lengths of single-mode fiber cable. We find that the individual longitudinal modes are >99-percent polarized after propagation through 54.6 km of cabled fiber; however, the different longitudinal modes have different states of polarization at the output. This difference is caused by polarization dispersion, and we estimate a propagation delay difference for the two principal states of polarization to be 0.42 ps in the 54.6 km of cabled fiber.     

Use of a doubly polarized laser for remote powering of anintegrated optical modulator

Stable operation of an integrated optic modulator is demonstrated using a 1.3 μm doubly polarized laser as a depolarized source in conjunction with a long run of ordinary fiber. The laser is found to be unusually susceptible to feedback due to gain competition between the polarization modes. The resulting low-frequency polarization noise is significantly reduced by the addition of fiber isolators to the system     

Coupling Character of Polarization Maintaining Optical Fiber Under the Condition of Bend

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刻蚀光纤布喇格反射器的特性

从实验和理论上研究了刻蚀光纤布喇格反射器的频谱响应和偏振特性。分析表明反射器的偏振敏感性是因为光纤截面的圆对称性被破坏，其反射谱呈现多峰结构则是反射器波导支持偶、奇对称两个模式以及偏振敏感性共同起作用的结果，并给出了高阶模截止的条件。通过反射器结构参数的优化，可以减小其反射带宽和偏振敏感性。     

声扭波在单模光纤中的应用

光纤中的基模LP01有两种偏振态,通过在油光纤方面加入声扭波可以引起两个偏振模发生耦合,本文主要介绍了声扭波和振幅和色散关系,同时也发现,采用高阶声扭波可以提高耦合系数的值。