长周期光纤光栅在色散补偿中的应用

通过与以往色散补偿器件的对比说明长周期光栅色散利、偿的优点,较详细地介绍了目前所研制出的两种长周期光栅(啁啾长周期光栅和高△的均匀长周期光栅)用于色散补偿的原理方法和在实际应用中需要解决的问题。     

光纤光栅在色散补偿系统中的应用

全面地介绍了光纤光栅在色散补偿应用中的最新进展，并对各种基于光纤光栅的色散补偿器件的工作机理，性能，特点，优越性及局限性做了深入的阐述，分析和比较。     

光纤光栅在DWDM系统色散补偿中的应用

色散补偿技术是高速率光通信系统中的重要限制因素，本文分析了两种基于光纤光栅在DWDM系统中用于色散补偿的应用技术，一种为离散信道的色散补偿技术，一种为非离散信道的色散补偿。并简要介绍了对前者用于色散补偿的两种改进方案。     

非啁啾光纤光栅在色散补偿中的应用

本文基于均匀布拉格光纤光栅的色散特性和啁啾高斯脉冲的传输演变特性,研究了工作于传输方式的非啁啾光纤光栅的色散补偿性能,讨论了光栅长度,光栅耦合系数等光栅参数以及初始脉宽,初始啁啾等脉冲参量对补偿光纤长度的影响。     

基于光纤光栅的光纤色散补偿

介绍了长距离光纤通信系统中色散补偿的基本原理,对基于光纤光栅的两种色散补偿模式:反射模式与透射模式作了详细的分析,最后对当前国内外基于光纤光栅的色散补偿情况作了介绍。     

基于光纤光栅的光纤色散补偿

介绍了长距离光纤通信系统中色散补偿的基本原理，对基于光纤光栅的两种色散补偿模式：反射模式与透射模式作了详细的分析，最后对当前国内外基于光纤光栅的色散补偿情况作了介绍。     

啁啾光纤光栅在硫系光纤激光器中的色散补偿

中红外波段包含极其重要的大气窗口和众多分子的指纹区,基于硫系玻璃的中红外光纤激光器逐渐引起人们的重视。由于硫系玻璃具有极高的非线性和色散特性,脉冲激光在硫系光纤中的展宽成为发展中红外超短激光必须解决的重要问题。针对脉冲激光在硫系光纤中传输的展宽问题,设计线性啁啾光纤光栅,用于补偿高斯脉冲激光经过光纤之后的色散展宽。模拟结果表明:光纤色散导致的脉冲展宽可以通过线性啁啾光纤光栅进行很好的补偿。进一步研究发现,通过对设计的啁啾光纤光栅运用高斯变迹函数进行切趾优化,可以显著改善色散补偿的效果,以获得对脉冲激光色散展宽的完全补偿。文中的研究对于设计高质量的硫系中红外光纤激光器具有理论指导意义。     

利用均匀光纤光栅进行色散补偿

概述了光纤光栅的基本性质 ,介绍了均匀光纤光栅进行色散补偿的机理以及作者在这方面进行的工作 ,并与传统的啁啾光纤光栅色散补偿做了比较。从而得知 ,利用均匀光纤光栅的传输色散特性进行色散补偿是一种更行之有效的色散补偿方法。     

基于光纤光栅的可调色散补偿

首先对在光网络中进行自适应色散补偿的必要性进行了简单的说明,然后综述了运用光栅的应力特性、压电特性 和温度特性而实现的色散补偿量可调谐的结构,并对各种结构的优缺点进行了分析。     

基于级联光纤光栅的透射色散补偿

分析了光纤光栅的色散特性,介绍了利用均匀光纤光栅透射色散特性进行色散补偿的原理,对级联光纤光栅用于波分复用(WDM)系统多信道色散补偿进行了数值模拟和分析.结果表明,通过选择适当的光纤光栅参数,级联光栅能够对WDM系统中由于常规光纤而色散展宽的光脉冲进行有效的色散补偿.     

啁啾光纤光栅补偿光纤色散的研究

啁啾光纤光栅被认为是目前最有实用价值的色散补偿方案之一。分析了啁啾光纤光栅补偿色散的基本原理,从简单模型出发分析了啁啾光纤光栅的色散补偿能力,用数值法研究了啁啾光纤光栅的时延及色散特性,并比较了变迹型与非变迹型啁啾光纤光栅。结果表明要获得较大的色散,要求光纤光栅有较长的长度和较小的啁啾。同时为了消除色散曲线的振荡还必须采取适当的变迹方法。     

光纤布拉格光栅温度补偿研究

提出了一种新颖结构的光纤光栅温度补偿器件,它由两种不同的热膨胀系数的材料组成。利用该器件实现了光纤光栅的温度补偿。在-18~50℃温度范围内光栅波长变化0.028nm,是未补偿光纤光栅的1/23倍。     

Ramped, unchirped fiber gratings for dispersion compensation

The effective medium method is used to analyze an unchirped fiber grating in which the coupling strength between the light field and grating is monotonically increasing with penetration depth into the grating. The potential use of this type of grating for dispersion compensation in intensity modulated optical systems is discussed. It is shown that, when this type of grating is used in reflection, appropriately designed linearly ramped gratings can be used to compensate fiber dispersion over a wide range of bandwidth-distance product values. In contrast, when the grating is used in transmission, there are strong limits on the bandwidth-distance product     

温度调谐型均匀光纤光栅级联进行色散补偿

本文提出使用级联的温度调谐均匀光纤光栅对光纤进行宽带色散补偿，对所需光纤光栅的变迹函数和耦合长度进行了优化设计，并讨论了光纤光栅的温度增敏措施。     

基于啁啾光纤光栅色散补偿问题的思考

色散已成为光纤长距离、高速率通信中的巨大障碍.鉴于色散补偿光纤插入损耗大、易引入非线性效应等缺点,文章采用啁啾光纤光栅对系统进行色散补偿,克服了以上不足.通过分析啁啾光纤光栅色散补偿的原理,结合理论分析,提出在多通道波分复用系统中使用啁啾光纤光栅,以实现长距离无中继传输.     

Phased-only sampled fiber Bragg gratings for high-channel-count chromatic dispersion compensation

Binary and multilevel phase-only sampling functions are proposed for the sampled fiber Bragg gratings (FBGs) with high channel count, which require significantly less refractive-index modulation than that does the sampled grating with amplitude sampling. The design using the new simulated quenching optimization with temperature rescaling results in high channel uniformity and minimum energy in the out-of-band channels. The technique can be applied to the sampled FBGs with very high channel count. A five-channel nonlinearly chirped multilevel phase-only sampled FBG for tunable chromatic dispersion compensation is demonstrated.     

Dispersion compensation of fiber Bragg gratings in 3100 km high speed optical fiber transmission system

By optimizing the fabrication process of the chirped optical fiber Bragg grating (CFBG), some key problems of CFBG are solved, such as fabrication repetition, temperature stability, group delay ripple (GDR), fluctuation of the reflection spectrum, polarization mode dispersion (PMD), interaction of cascaded CFBG, and so on. The CFBG we fabricated can attain a temperature coefficient less than 0.0005 nm/℃, and the smoothed GDR and the fluctuation of the reflection spectrum are smaller than 10ps and 0.5dB, respec-tively. The PMD of each CFBG is less than 1 ps and the dispersion of each grating is larger than -2600 ps/(nm·km). With dispersion compensated by the CFBGs we fabricated, a 13×10 Gbit/s 3100 km ultra long G.652 fiber transmission system is successfully imple-mented without electric regenerator. The bit error rate (BER) of the system is below 10-4 without forward error correction (FEC); when FEC is added, the BER is below 10-12. The power penalty of the carrier-suppressed return-to-zero (CSRZ) code transmission system is only 2.5 dB.     

Purely phase-sampled fiber Bragg gratings for broad-band dispersion and dispersion slope compensation

We demonstrated numerically that both the chromatic dispersion and the dispersion slope can be compensated by using purely phase-sampled superstructure fiber Bragg gratings provided both the grating period and the sampling period are chirped linearly along the grating. Adjusting the refractive index modulation and the chirp of sampling function, they can be designed to compensate dispersion of a large number of wavelength-division-multiplexing channels.     

Analysis of fiber Bragg gratings for dispersion compensation inreflective and transmissive geometries

Numerical analysis of the dispersion-compensating properties of fiber Bragg gratings (FBGs) in both reflective and transmissive modes is presented. First, the sensitivity of chirped, reflective gratings to the grating chirp parameter, index modulation, and grating length is examined, showing that apodization provides lower sensitivity to variations in these parameters. Second, we introduce a new transmissive geometry for grating-based dispersion compensation that utilizes the dispersive properties of a uniform Bragg grating in transmission