利用普通SMF实现10Gbit＼s 信号全光长距离传输的研究

数值模拟了强度调制光信号在级联光纤放大器普通单模光纤通信系统中的传输,模拟中主要考虑了自相位调制、群速色散和自发辐射噪声,使用负色散补偿光纤去补偿群速色散和自相位调制。结果表明,若色散得到很好补偿,当放大器间距减少到５０ｋｍ时,无误码２０５０ｋｍ传输是可能的。     

应用自相位调制的色散补偿技术

研究了光纤中的自相位调制现象，以及应用ＤＣＦ（色散补偿光纤）进行色散补偿的方法，讨论了自相位调制对色散补偿性能的影响。介绍了应用ＳＰＭ效应提高色散补偿效果的技术，并给出了模拟结果和分析。     

增益饱和半导体激光放大器中的自相位调制效应

本文分析了半导体激光放大器处于增益饱和状态下的自相位调制（SPM）效应,以及SPM效应对传输脉冲波形、相位及频谱的影响。指出了利用这种效应可以补偿传输光纤色散。但是,必须仔细选择传输系统的配置和放大器结构参数,以获得最佳色散补偿效果。     

应用自相位调制的色散补偿技术

研究了光纤中的自相位调制现象．以及应用ＤＣ Ｆ（色散补偿光纤）进行色散补偿的方法。讨论了自相应调制对色散补偿性能的影响、介绍了应用ＳＰＭ效应提高色散补偿效果的技术。并给出了模拟结果和分析。     

WDM+EDFA+DCF光纤传输系统中色散补偿方案的分析

由于在ＷＤＭ＋ＥＤＦＡ光纤传输系统中使用常规单模光纤（ＳＭＦ）在１５５０ｎｍ窗口的大色散限制了传输距离,采用色散补偿光纤（ＤＣＦ）进行色散补偿是上前一种较为理想的方法。本文基于光纤ＷＤＭ＋ＥＤＦＡ＋ＤＣＦ的长距离传输系统,讨论了ＤＣＦ色散补偿对光纤非线性效应交叉相位调制和四波混频（ＦＷＭ）的影响,提出了采用ＤＣＦ集总、后置、非完全补偿的色散补偿方案,这种方案可合系统具有更佳的传输性能。     

色散补偿系统中自相位调制效应的影响

分析了自相位调制效应对正、负色散光纤中光脉冲传输的影响 ,并用数值仿真的方法研究了自相位调制效应对采用色散补偿光纤的高速率光纤通信系统性能的影响 ,获得了一些对实际色散补偿系统有参考价值的结论。     

光纤色散对WDM系统性能的限制

波分复用（ＷＤＭ）技术是增大光纤传输容量的方法，但是在高速率、长距离ＷＤＭ系统中传输性能受到限制。除了多级光纤放大器（ＥＤＦＡ）使带宽减小，噪声增大，光纤的材料色散也是对ＷＤＭ系统影响的重要因素。本文主要分析光纤色散以及有初始啁啾的脉冲、激光器的相位调制噪声、有非线性效应时光纤色散对ＷＤＭ系统传输容量的影响。     

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。     

WDM系统中的非线①性研究及仿真实验

利用分离信道的分步傅立叶法对信道间距为0.8nm的8路10 Gbit/s波分复用色散补偿系统进行仿真实验，分析了在具有级联光放大器系统中光纤色散和各种非线性效应（自相位调制SPM、交叉相位调制XPM、四波混频FWM）对系统传输的影响。仿真结果表明，在色散补偿WDM通信系统中，SPW对系统传输造成的损伤最大。并且由于非线性效应、传输损耗及噪声的综合影响，应当选取合适的系统输入功率。     

1550nm光纤传输技术及其在长距离传输中应用研究

本文针对1550nm光纤长距离传输技术的特点,深入分析了传输中光纤系统中自相位调制等非线性效应及合理的色散补偿等技术问题存在的CSO劣化,同时具体分析了利用1550nm光纤传输长距离有线电视信号技术的实现。     

Transmission distance of in-line amplifier systems withgroup-velocity-dispersion compensation

Group-velocity dispersion (GVD) compensation in in-line amplifier systems is evaluated from the viewpoint of improving the transmission distance. The nonlinear Schrodinger equation, which simulates signal propagation in optical fibers, is numerically evaluated to clarify the optimum configuration for GVD compensation. It is shown that the optimum amount of GVD compensation is about 100% of the GVD experienced by the transmitted signal. The optimum compensation interval is found to be a function of the bit rate, signal power, and dispersion parameter. For dispersion parameter values ranging from about -0.1 ps/nm/km to -10 ps/nm/km, and an amplifier noise figure of about 6 dB, the optimum compensation configuration can eliminate the GVD from in-line amplifier systems, thus improving transmission distances to those limited by self-phase modulation and higher-order GVD     

Analytical study on pulse broadening in chained optical amplifiersystems

Approximate analytical formulas for root mean square pulse width evolution in fiber systems using chained optical amplifiers are derived in this paper. Effects of group velocity dispersion (GVD) and self-phase modulation (SPM) are taken into account, and the system may have axially varying parameters, such as uneven fiber dispersion including dispersion management, nonequal amplifier spacing as well as output power, etc. It is shown that the analytical formulas can be applied to the design and analysis of a wide range of practical chained optical amplifier systems, and is helpful in the understanding of the pulse distortion caused by the interaction between SPM and GVD     

Analytical evaluation of transmission penalty due to group velocitydispersion, self-phase modulation, and amplifier noise in opticalheterodyne CPFSK systems

An analytical bit error rate evaluation of an optical heterodyne continuous-phase frequency shift keying (CPFSK) transmission system affected by group-velocity dispersion (GVD), self-phase modulation (SPM), and erbium-doped fiber amplifier (EDFA) amplifier spontaneous emission noise (ASE) in a nonlinear fiber medium is carried out following a perturbative and a transfer matrix approach. The utility of both approaches has been exemplified by applying them to different dispersion compensation schemes in optical and electronic domains. The theoretical penalty estimates are found to have good agreement with both the reported experimental results and those obtained by the Q-value simulation     

Comparison between NRZ and RZ signal formats for in-line amplifiertransmission in the zero-dispersion regime

Nonreturn-to-zero (NRZ) and return-to-zero (RZ) signal formats are experimentally and numerically compared for single-channel long-distance transmission in an in-line amplifier system with dispersion management providing average zero dispersion and local nonzero dispersion at an interval equal to the in-line amplifier spacing. Among a 20-ps RZ signal, a 40-ps RZ signal, and an NRZ signal transmitted in 10 Gb/s straight-line experiments, the last signal achieves the longest transmission distance of 6000 km while the others are limited to 4400 km. Numerical simulations explain these results well and show that, along with linear amplified spontaneous emission (ASE) accumulation, signal waveform distortion due to the combined effect of higher order group-velocity dispersion (GVD) and self-phase modulation (SPM) dominates the performance. Nonlinear optical noise enhancement is not obvious because of the fiber dispersion arrangement. Signals with large pulse widths are less affected by the combined effect, while small-width signals yield superior initial signal-to-noise ratio (SNR) as determined by optical noise. A detailed simulation indicates that a pulse width of about 60 ps is optimum for long distance transmission under the fiber dispersion arranged in this paper     

单模光纤正常色散区啁啾演变研究

对单模光纤正常色散区，群速度色散所致啁啾、自相位调制所致啁啾以及两者共同作用所致啁啾的演变过程进行了研究。利用傅里叶变换法获得群速度色散所致啁啾、自相位调制所致啁啾的解析解，采用数值法得到了群速度色散效应与自相位调制效应共同起作用时，啁啾演变过程。由啁啾演变结果可得，在正常色散区可形成暗孤子，也可实现对皮秒脉冲压缩。     

单模光纤中高斯脉冲无啁啾稳定传输

在分析单模光纤群速度色散(GVD)效应和自相位调制(SPM)效应相互作用的基础上,导出GVD和SPM共同作用引起的啁啾表达式,全面分析了色散长度L_D、非线性长度L_(NL)与啁啾变化的关系。结果表明:随着L_D/L_(NL)的不同,啁啾特性有着显著变化,当N=L_D/L_(NL)=1,即实现了单模光纤中群速度色散效应与非线性效应相互作用所致啁啾的最佳匹配,通过控制脉冲输入功率,可望实现高斯光脉冲无啁啾的稳定传输。     

损耗作用下混频时调制不稳定性耦合模分析法

在考虑光纤损耗的情况下，以两载频以及混频过程中产生的边带频率成分为研究对象，给出了研究群速度色散（GVD）、自相位调制（SPM）、交叉相位调制（XPM）综合作用下混频过程中调制不稳定性（MI）的耦合模分析法。导出了当某一相位匹配较好、其他相位失配严重时，两载频自相位调制或交叉相位调制引起的调制不稳定性增益的解析表达式。分析发现，当调制不稳定性主要由自相位调制或交叉相位调制引起时，增益的最大值与色散无关，交叉相位调制在各边带引起的调制不稳定性最大增益相等，同时，考虑损耗后，幅度增益减小的大小受功率、非线性系数、色散情况、损耗系数和传输距离等因素共同影响，调制小稳定性产生的增益只有当频率偏移量足够大时才会出现，载频自相位调制引起的最大增益对应的频率偏移量减小。     

超高斯啁啾光脉冲在单模光纤中传输的演化行为

本文从激光脉冲在单模光纤中传输所满足的非线性薛定谔方程出发,通过分步傅里叶变换方法,数值研究了超高斯啁啾光脉冲在单模光纤中脉冲形状的演化.研究表明,超高斯脉冲在单模光纤中传输将经历一个从近平顶、多峰、最后到单峰的演变过程,且高阶色散将引起脉冲形状发生畸变;在GVD和SPM效应的共同作用下,无啁啾的超高斯脉冲在特定条件下将出现孤子演变,具有正啁啾的超高斯脉冲在传输的初始阶段,脉冲形状的变化非常剧烈,而由于负初始啁啾减弱了非线性与色散效应引起的频率啁啾,所以其脉冲波形的变化平缓一些.研究表明,SPM产生的啁啾对入射脉冲的初始啁啾有一定的补偿作用.     

光纤中超连续谱的产生与分析

利用MATLAB分析光纤中产生的超连续谱谱线展宽情况。结果表明．光纤中超连续谱的产生主要是拉曼自频移、群速度色散、自相位调制和三阶色散效应共同作用的结果。给出了光纤传输过程中增宽谱线的方法。     

Cancellation of the signal fading for 60 GHz subcarrier multiplexedoptical DSB signal transmission in nondispersion shifted fiber usingmidway optical phase conjugation

In millimeter-wave (mm-wave) optical double sideband (DSB) signal transmission systems, the received radio frequency (RF) power fades periodically because of the group velocity dispersion (GVD) and the self-phase modulation (SPM) of optical fibers. In this paper, cancellation of the signal fading by using midway optical phase conjugation in mm-wave subcarrier multiplexed (SCM) optical DSB signal is analyzed. Fading-free 60 GHz mm-wave optical DSB signal transmission over 100 km-long nondispersion shifted single-mode fiber at 1550 nm by using a semiconductor optical amplifier (SOA) optical phase conjugator (OPC) in the midway of optical link is experimentally demonstrated for the first time. Finally, the degradation factor of the OPC system is also discussed