不同类型光纤对CWDM系统性能的影响

文章比较了目前应用于粗波分复用(CWDM)系统的各类光纤的性能,结合光纤在系统测试中的表现情况对各类光纤的优缺点进行了评价.肯定了标准单模光纤和非零色散位移单模光纤应用于CWDM系统的可靠性,分析了G.652C/D和G.655B/C两类低水峰光纤支持全频谱CWDM传输的优势和在网络升级中的应用潜力,同时与色散位移单模光纤、负色散 (平坦)光纤等非主流光纤的性能作了比较.     

基于光子晶体光纤的宽带色散补偿光纤的设计

采用矢量光束传输法(VBPM)对小纤芯光子晶体光纤(PCF)的色散特性进行了数值分析,研究发现通过调节光子晶体光纤的结构参数可以灵活的对其色散补偿值进行调整,能够实现C L波段(1 530～1 565 nm)的宽带色散补偿功能,并且对标准单模光纤的色散斜率有很好的补偿.在∧=1.0μm,d/∧=0.7时,1 550 nm处的色散值可以达到-339.1 ps/(km×nm),相关色散斜率(RDS)可以达到0.003 2 nm-1,能够有效的对标准单模光纤进行色散斜率补偿.     

基于DCF长距离光纤通信系统的色散补偿

通过介绍光纤色散的产生及其对传输系统的影响,引出了色散补偿技术.在多种色散补偿方法中,侧重探讨了色散补偿光纤(DCF)技术.基于DCF在标准单模光纤上传输2245 km的情况下进行了研究,获得了一些对实际色散补偿系统有参考价值的结论.     

偏振模色散对单模光纤系统的影响：应用概述

1 引言和背景 近年来,为满足日益增长的带宽需求,光纤通讯系统已取得了巨大的进展。单模光纤(SMF)系统性能的主要限制因素包括衰减、色散和非线性,以及最近引起注意的偏振模色散(PMD)。 对于操作在1310nm窗口的传统单模光纤系统,由光纤衰减引起的光功率损失限制了系统的传输距离。在此波段中,单模光纤具有零或非常低的色散,系统的传输速率也较低,且操作在单一波长     

S-C-L三波段传输新型单模光纤的设计和研究

随着光通信技术的发展,各种现有的单模光纤已不能满足宽带光传输密集波分复用(DWDM)系统传输的要求,S C L三波段传输新型单模光纤是在1460～1625nm的波长范围内具有足够大的色散以抑制四波混频效应、交叉相位调制等非线性效应,又使色散及斜率尽可能低,从而使色散管理成本降到最低的新型单模光纤.我们设计和计算了这种新型的光纤的结构并对其性能参数进行了分析和讨论.     

色散补偿准光孤子传输特性数值分析

为了使准光孤子能够在标准单模光纤中稳定地传输,采用了分步傅里叶方法分别模拟了准光孤子在标准单模光纤中的传输和在色散补偿系统中的传输,得到了准光孤子在标准单模光纤中的传输特性和在色散补偿系统中的传输特性。结果表明,准光孤子在标准单模光纤的传输过程中脉冲峰值逐渐降低,脉冲宽度逐渐展宽,不能稳定传输;而准光孤子在采取色散补偿技术的色散补偿系统中传输时,脉冲形状几乎保持不变,与准光孤子直接在标准单模光纤中的传输相比,性能得到了很大改善。     

利用光子晶体光纤实现10 Gb/s光传输系统宽带色散补偿

利用光子晶体光纤（PCF）,在10Gb／s光传输系统中、20nm宽带范围内完成了色散补偿传输实验,得到了很好的色散补偿效果。实验中,10Gb／s光脉冲序列经过2．163km普通单模光纤被展宽后,用26mPCF对其进行色散补偿,此光纤在C波段20nm波长范围内对普通单模光纤能够实现较好的色散斜率补偿。实验结果表明,PCF在色散补偿方面具有很大的潜力,在未来光通信系统中将发挥重要作用。     

用于色散补偿的双芯光子晶体光纤设计

WDM系统的传输速率受单模光纤(SMF)中色散D的制约.针对WDM系统中的色散补偿问题,本文提出了一种新型的用于色散补偿的双芯光子晶体光纤(DCPCF),其构成材料是纯石英和空气.采用高斯--厄密函数法计算了此DCPCF的模场和等效折射率,理论模拟表明这种DCPCF的色散可达-18000 ps/(nm.km),并可补偿超过自身长度1000倍的普通单模光纤.     

网络中的TrueWave Rs光纤和其他单模光纤的混合

在今天已建成的网络中可发现各种类型的单模光纤.象IEC和ITU这样的标准组织已认可了四种单模光纤:色散非位移光纤(G.652)、色散位移光纤(G.653)、截止波长位移光纤(G.654)和非零色散光纤(G.655).此外,有两种G.652光纤(传统的和低水峰),和无数的商用G.655光纤(小的、中等的和大的有效区域;低的、中等的和高的色散斜率;负的和正的色散),有时会在一个网络中使用.当将TrueWave RS光纤同色散非位移和其他非零色散光纤混合时,应评价几个方面的指标,包括:(1)接续损耗,(2)单向OTDR异常,(3)链路色散,(4)链路色散斜率,(5)截止波长,(6)非线性效应.     

C波段色散补偿光子晶体光纤的研究和设计

设计了一种新颖结构的双层芯色散补偿光子晶体光纤。此光纤在整个C波段具有高负色散特性。通过合理选取双层芯光纤的外层芯层数,同时优化孔间距和空气孔直径,设计的光纤在C波段的色散值在-520ps/(km.nm)和-390ps/(km.nm)之间近似线性变化,残余有效色散系数近似为零,相关色散斜率(RDS)在0.0032nm-1的色散补偿光纤,其RDS值与标准单模光纤匹配,有效模场面积优于常规色散补偿光纤,可以对其长度30倍以上、用于宽带传输的标准单模光纤进行良好的色散和色散斜率补偿。     

Chromatic dispersion measurement in graded-index multimode opticalfibers

The chromatic dispersion observed in a graded-index multimode optical fiber is a function of the radial position of the launched light. When a graded-index multimode optical fiber is overfilled spatially and angularly, the chromatic dispersion observed is an average (composite) chromatic dispersion over all of the possible launches. Under certain assumptions, the relationship between the chromatic dispersion observed for the overfilled fiber and the chromatic dispersion of any restrictive launch can be determined. This relationship can be used to predict the composite graded-index multimode optical fiber chromatic dispersion from the measurement of the chromatic dispersion of a single simplified launch, such as a single-mode fiber launch. Preliminary experimental results confirm this approach     

非色散位移单模光纤的鉴定与相关检测

本文讨论了鉴定未知光纤是否符合非色散位移单模光纤特征的检测过程。光纤种类繁多,在进行鉴定时应结合非色散位移单模光纤的特征进行系统性的检测。检测过程中可首先判断未知光纤是否属于通信用单模光纤,再通过非色散位移单模光纤与其他通信用单模光纤的技术差异进一步鉴定。鉴定过程可能涉及到光纤几何参数、色散系数、宏弯损耗等多项指标的检测,文中给出了推荐的检测方法。     

Limitations in 10 Gb/s WDM optical-fiber transmission when using avariety of fiber types to manage dispersion and nonlinearities

We analyze the system limitations of WDM transmission when using various types of optical fiber to manage dispersion and nonlinearities. In our model, from two to eight 10 Gb/s WDM channels are transmitted through a cascade of EDFA's experiencing dispersion, stimulated Raman scattering, and self- and cross-phase modulation. The fiber types modeled include: conventional single-mode fiber, dispersion shifted fiber, and dispersion-compensating fiber. These fibers have different dispersion spectral profiles and are combined to manage dispersion to produce a total zero dispersion for a certain fiber span while eliminating four-wave mixing. We find that a system using dispersion-shifted fiber and conventional single-mode fiber exhibits the best performance, with the combination of dispersion and cross-phase modulation as the dominant effects. Furthermore, conventional single-mode fiber combined with dispersion-compensating fiber system exhibits the worst performance, with the combination of dispersion and self-phase modulation as the dominant effects     

自陡峭效应对相位共轭系统脉冲传输的影响

光学相位共轭(OPC)技术能够同时且高效地补偿光纤传输过程中色散及非线性效应所导致的信号失真，且该技术同脉冲调制方式无关。从理论上分析了在自陡峭效应(SS)作用下高斯脉冲信号在中距相位共轭系统中的传输演化特性，数值模拟了在其作用下超短飞秒高斯脉冲的动态传输过程，讨论了自陡峭效应对中距相位共轭系统复原性能的影响。结果表明自陡峭效应将导致高斯脉冲信号发生峰值漂移和脉冲后沿变陡，相位共轭系统不能补偿由此导致的脉冲失真和畸变。引入合适的色散可以减小这种信号失真，并使得相位共轭系统能够同时补偿由于色散、自相位调制和自陡峭效应而引起的信号失真。     

光纤OFDM系统中的色散补偿技术研究

为了减小光纤的色度色散对光纤正交频分复用（OFDM）系统性能的影响,提出了将无线通信中的信道估计器引入光纤OFDM系统进行信道估计的色散补偿方法。在理论上分析了光纤的色度色散对于传输OFDM信号的影响,并在实验中采用梳状导频的形式,在每个OFDM码元的特定的子载波上插入导频,在接收端通过基于最小平方（LS）原则的LS估计器进行信道估计,得到了OFDM光纤传输的信道幅度响应和相位响应,通过使用LS估计器,直接调制的光OFDM信号在单模光纤中传输200km,误比特率低于10-6 ,功率代价小于2dB。结果表明,高频子载波较低频子载波更容易受到色散的影响,在光纤OFDM系统中引入信道估计器进行信道估计能够有效补偿由色度色散带来的相位偏移和幅度衰减。     

初始啁啾补偿光纤色散效应的数值研究

以具有初始啁啾的高斯脉冲在单模光纤中的传输为例,分析、计算了线性初始啁啾对光纤二阶、三阶色散效应的影响,指出了初始啁啾进行色散补偿的适用范围和条件,并对二阶、三阶色散完全补偿光纤链路中40Gbit/s短脉冲传输效果进行了数值计算,结果表明,依据入射功率选择合适的初始啁啾,能使脉冲稳定传输距离大幅提升.     

非色散位移单模光纤的鉴定与相关检测

讨论了鉴定未知光纤是否符合非色散位移单模光纤特征的检测过程。光纤种类繁多。在进行鉴定时应结合非色散位移单模光纤的特征进行系统性的检测。检测过程中可首先判断未知光纤是否属于通信用单模光纤,再通过非色散位移单模光纤与其他通信用单模光纤的技术差异进一步鉴定。鉴定过程可能涉及到光纤几何参数、色散系数、宏弯损耗等多项指标的检测,文中给出了推荐的检测方法。     

The impact of group velocity on frequency-hopping optical codedivision multiple access system

In this paper, we develop a systematic method that employs transfer function considering encoder, fiber channel, and decoder to analyze the frequency-hopping (FH) optical code-division multiple-access (OCDMA) system. We analyze the FH-OCDMA system when both single-mode fiber and dispersion-shifted fiber are employed as the transmission medium. The difference of group velocities affects system performance more seriously than dispersion effect does. The results show that single-mode fiber is not proper for a FH-OCDMA system, even if the transmission length is no more than 1 km. The dispersion-shifted fiber is suitable for a FH-OCDMA system, especially in an access network. We also propose an optical device to compensate the group velocities     

25-Gb/s optical NRZ transmission over 40 km of single-mode fiber at 1550 nm without dispersion compensation

We present a method for transmitting 25-Gb/s optical nonreturn-to-zero signals at a wavelength of 1550 nm over a 40-km single-mode fiber without any dispersion compensation methods. We propose optimized self-phase modulation by varying parameters of the fiber launching power and the extinction ratio of optical non-return to zero signals to overcome severe signal distortions by the chromatic dispersion effect. Using the optimization of the self-phase modulation effect, we were able to transmit 25-Gb/s optical nonreturn-to-zero signals over a 40-km single-mode fiber, which can be applicable to passive optical networks with a single wavelength channel and a high split ratio. We demonstrated that the self-phase modulation effect can be controlled by the extinction ratio and the fiber launching power.     

Integrated dispersion slope equalizer of AWG-based optical CDMA for radio-over-fiber transmissions

Chromatic dispersion from optical fiber is the most important problem that produces temporal skews and destroys the rectangular structure of code patterns in the spectra-amplitude-coding optical code-division multiple-access (SAC-OCDMA) system. Thus, the balance detection does not work perfectly and the system performance will be degraded. In order to improve the distortion, we apply cascaded Mach–Zehnder interferometers (MZIs) to design a dispersion slope equalizer for the SAC-OCDMA system integrated with arrayed-waveguide grating (AWG) router coder. The dispersion slopes of a cascaded MZI compensator could be adjusted by the arm length differences of MZIs and be complementary with the fiber links. In this study, we present a set of length differences for 10 km long single-mode fiber (SMF) and verify the compensation scheme by relative delay time slope and signal-to-interference ratio (SIR). The dispersion slope equalizer with perfect complementary slope successfully compensates the dispersion from SMF and the system performance with dispersion slope equalizer is highly improved.