利用光脉冲传输特性抑制偏振模色散

基于双折射光纤中光脉冲传输方程，详细分析了二阶色散、自相位调制以及交叉相位调制在光脉冲传输过程中引起的啁啾。分析结果显示：通过合理选取入射功率，二阶色散引起的啁啾与自相位调制引起的啁啾在脉冲中心附近可以相互抵消，从而使脉冲展宽最小；交叉相位调制产生的两偏振分量的啁啾引起的频移，可使两偏振分量间产生互束缚，利用这种现象可以抑制偏振模色散。     

预啁啾对偏复用孤子技术的补偿

在导出自相位调制和交叉相位调制共同作用所致相位调制频率啁啾的基础上,数值研究了相位调制频率啁啾与初始啁啾的关系,并对有和无初始啁啾40Gbit/s归零码(RZ)在二阶和三阶色散完全补偿(路径平均色散为0)的色散管理偏振复用孤子传输系统中的传输效果进行计算。结果表明,在输入功率达到一定值时,初始啁啾参量C对相位调制频率啁啾的作用,决定着系统偏振复用孤子技术的成效及传输性能,适当选取初始啁啾参量C能够有效抑制偏振模色散,提高孤子脉冲稳定传输距离。     

光纤中双脉冲传输的频率啁啾及脉冲压缩

对双脉冲在光纤中传输时所满足的非线性耦舍方程进行了理论分析和数值计算,求得了脉冲演化时啁啾参量的一般表达式。结果表明,利用交叉相位调制效应压缩光脉冲时,无论泵浦脉冲还是信号脉冲,其线性源啁啾都对光脉冲的压缩产生重要影响。在泵浦功率一定的条件下,选取负啁啾的泵浦脉冲和正啁啾的信号脉冲易于获得更短的压缩光脉冲。     

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。     

基于相位调制和光参量放大的光短脉冲源实验研究

提出了一种基于光参量放大和相位调制加色散压窄产生高消光比短脉冲源的新方法.连续抽运光首先经过LiNbO<,3>强度调制器,利用强度调制的倍频调制特性产生占空比为33%的光脉冲,再经相位调制器在脉冲的主体部分引入最大线性正啁啾,经参量放大后所生成的闲频光的啁啾为抽运光的2倍,通过合适的色散介质得到了11.4 ps的短脉冲...     

利用相位和强度调制器产生高消光比超短光脉冲

提出了一种产生高消光比超短光脉冲的新方法.利用相位调制器调制连续光生成啾啁光,而后利用M-Z强度调制器的倍频调制抑制对压缩不利的啁啾部分的影响,再通过等效啁啾光纤光栅进行压缩产生光脉冲.理论和仿真结果表明,该方法可以很好地消除光脉冲的基底及减小旁辦,产生消光比大于30 dB、波形理想的光脉冲,具有很强的可实现性.最后利用实际制作的色散系数为-380 ps/nm的等效啁啾光纤光栅对该方法进行了实验验证,结果表明,在重复频率为2.5 GHz、相位调制系数为9时,可产生脉宽小于18 ps的高质量光脉冲.     

单量子阱激光器小信号调制时的啁啾噪声

量子阱激光器具有良好的小信号调制频率响应 ,能作为高速光通信光源采用直接调制方式进行信号传输。与普通半导体激光器一样 ,直接调制将引起啁啾 ,从而影响光纤通信系统的性能。文中对小信号调制下单量子阱激光器的啁啾特性进行了研究和分析。得出了啁啾幅度和啁啾相位与调制频率的关系。对考虑与不考虑啁啾两种情况下 ,光脉冲在常规光纤中传输时的色散特性进行了模拟分析 ,发现了啁啾对系统的高阶色散有较大影响     

光纤GVD和SPM效应所致频率啁啾的匹配

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，推导出GVD和SPM共同作用引起的啁啾表达式；全面分析了色散长度LD、非线性长度LNL与啁啾变化的关系。结果表明，随着LD／LNI的不同，啁啾特性有着显著变化；当N=LD／LNL=1，即实现了单模光线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，可望实现光脉冲无啁啾的稳定传输。     

五阶非线性下双脉冲相移和啁啾的解析研究

从光纤中扩展的耦合非线性薛定谔方程组出发,在同时考虑五阶非线性、脉冲间群速度失配和初始时延的情况下,忽略光纤色散效应,导出了载频不同的两高斯脉冲由于交叉相位调制所致的非线性相移和频率啁啾的解析公式.结果表明,与只有三阶非线性的情况相比,三五阶非线性的共同存在会使脉冲间群速度失配,且初始时延对脉冲的非线性相移和频率啁啾会产生更为综合和复杂的影响.该研究在光开关器件和频率转换等方面有一定的指导意义.     

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朦胧（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LD、非线性长度LNL与啁啾变化的关系。结果表明：随着LD/LNL的不同，啁啾特性有着显著变化，当N=LD/LNL=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。     

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.     

具有饱和非线性的非克尔光纤中自相位调制效应所致啁啾

在考虑光纤损耗下,从理论上推导出具有饱和非线性的非克尔光纤中自相位调制效应产生啁啾的解析表达式;并在计算机上模拟了光纤中啁啾的演变过程。结果表明,非克尔光纤中的饱和效应越强,自相位效应所产生的啁啾越小;随着光纤传输,啁啾不断增大;而且啁啾与光纤损耗、入射脉冲的峰值功率等因素有关。     

The Effect of Fiber Non-Linearity on Two Dispersion Compensation Schemes

1introductionTheintroductionofErbium-dopedfiberamplifier(EDFA)hasbroughthigh-capacityopticalnetWorksoperatingaround1550urn.Theultimatetransmissionlimitationsarenowchirp,chromaticdispersion,fibernon-linearityandnoisefromEDFAs.Sincethemajorityoftoday'sinstalledfiberisdesignedtooperatearound1310urn,greateffortsaremadetocommerciallyexploitandupgradethembydispersioncompensation.ChirpedBraggfibergratingsusedasdispersioncompensatorshavereceivedconsiderableattentionlatelybecauseoftheirlow-inseFti…     

Practical considerations for optical polarization-mode dispersion compensators

For transmission systems at 10 Gb/s and beyond, polarization-mode dispersion (PMD) is one of the limiting factors. Optical PMD compensators aim at increasing the PMD value tolerated by the system; however, they do not cancel out its effects. Therefore, the performance of a PMD compensator is assessed statistically. Requirements for optical PMD compensators include a response time in the range of 1 ms in order to follow polarization fluctuations over the line. The system design should account for the interaction of other transmission impairments with the PMD compensator operation. For instance, transmitter chirp and residual chromatic dispersion have a deleterious impact on the compensator performance. While self-phase modulation is harmless, cross-phase modulation greatly reduces the compensator efficiency. System design rules have been applied to a one-year field trial, showing the compensator's efficiency and reliability. However, reducing their cost is the next challenge that will bring optical PMD compensators to be used in installed systems.     

基于SOA啁啾管理的连续可调谐色度色散补偿的研究

提出了一种新型的可小范围连续调谐的色度色散(CD)补偿方案.该CD补偿方案包括一个半导体光放大器(SOA)和一段固定长度的色散补偿光纤(DCF).利用SOA的交叉相位调制(XPM)效应,通过调节SOA的偏置电流和控制脉冲光的强度,可以对进入SOA的光信号引入不同大小的附加啁啾量,从而可以利用固定长度的DCF得到补偿后的无啁啾光信号.实验中,实现了10 Gb/s可调谐CD补偿器,在无需替换DCF的情况下,实现了补偿范围为-40 ps/nm到60 ps/nm的连续可调谐CD补偿.     

脉冲形状对半导体激光放大器用于啁啾补偿的影响

光脉冲经过增益饱和的行波半导体激光放大器后,由于放大器的自相位调制,使放大脉冲附加上频率啁啾。合适的附加啁啾不但能抵销入射脉冲的初始啁啾,而且还有可能借助简单的群速度延迟线对脉冲进行压缩。本文计算了不同形状的入射脉冲经光放大器放大后的输出脉冲形状及其附加的频率啁啾,分析了它们对光放大器用于啁啾补偿的影响。     

偏振度方法监测和控制偏振模色散的失效概率

依据主偏振态理论和一阶偏振模色散(PMD)近似,给出了信号偏振度(DOP)与PMD的解析关系式.考虑到光纤通信链路中光放大器造成的自相位调制(SPM)的影响,通过数值仿真,量化了DOP方法监测40 Gbit/s系统的PMD的失效概率.发现降低放大器输出峰值功率(10～12 dB*m)和引入适当的初始负啁啾(-1)可以显著增大PMD补偿系统作用距离.     

Link Performance Monitoring Technique for Measuring Residual Chromatic Dispersion of Optical Links

We propose a simple technique for measuring the residual chromatic dispersion (CD) of optical links based on two single-sideband tones. The residual CD was measured with an accuracy of +/- 10 ps/nm, regardless of the effect of self-phase modulation.     

SPM对啁啾超高斯脉冲频谱演变的影响

本文通过理论计算,给出了带有初始啁啾的超高斯脉冲由于SPM影响所致的频谱表达式。在此表达式的基础上,利用数值模拟的办法,对照分析了初始啁啾对超高斯脉冲频谱演变的影响。研究结果表明:初始啁啾非常明显的影响超高斯脉冲的频谱,初始正啁啾加剧频谱展宽,初始负啁啾减小频谱展宽。可见,引入初始负啁啾有利于优化超高斯脉冲传输系统的性能。     

Transmission limitations due to self-phase modulation in opticalPSK heterodyne detection systems employing chromatic dispersionequalization

Even if the amplitude of a phase-modulated optical signal is constant before transmission, amplitude modulation is caused by fiber chromatic dispersion. As a result, self-phase modulation (SPM) is induced. In optical heterodyne detection, SPM cannot be compensated for by the delay equalizer (electrical domain) used to compensate fiber chromatic dispersion. However, the transmission distance limitation of multi-repeatered coherent transmission systems has not been investigated in the presence of SPM. This paper theoretically and experimentally investigates the transmission distance achievable with a phase-shift-keying (PSK) heterodyne detection system employing in-line optical amplifiers and delay equalization. The calculated results show that equalization is effective when γP₀/2B²|β₂|<10 in the normal dispersion regime, and γP₀/2B²|β ₂|<15 in the anomalous dispersion regime. Furthermore, the increase in transmission distance achieved by using equalization is experimentally shown in an 8 Gb/s PSK heterodyne transmission experiment using a conventional single-mode (SM) fiber and in-line fiber amplifiers