排序方式: 共有38条查询结果,搜索用时 78 毫秒
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利用非线性光纤环镜160Gb/s到10Gb/s解时分复用 总被引:1,自引:0,他引:1
研究了160 Gb/s光时分复用(OTDM)系统的解复用技术.针对160 Gb/s速率的特点,对高非线性光纤(HNLF)的光纤环镜(NOLM)特性及解复用进行了数值仿真.计算了低信号光时间抖动下解复用误码特性对时钟与信号的走离及时钟功率的依赖关系.计算了三种走离值消光比随时钟功率增加的变化趋势并给出:存在一个能获得最大的解复用窗口消光比、并能降低相邻信道串扰的合适的时钟功率范围.利用自制的基于电吸收调制器和压缩技术的超短光脉冲源建立了160 Gb/s OTDM实验系统,测量了不同信号光功率下NOLM的消光比,它基本不随信号增大而变化,在信号功率为7.3 dBm时仍大于23 dB.利用上述装置实现了无误码的160 Gb/s到10 Gb/s全光解复用. 相似文献
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一种可编程PMD模拟器 总被引:5,自引:3,他引:2
为了研究光纤通信中的偏振模色散(PMD)及其对高速光通信系统的影响和补偿技术,研制了一种可编程控制的PMD模拟器,它由6组双折射晶体和磁光晶体组成,群时延差(DGD)变化范围为±(0.3~35) ps,可设为不同平均值的Maxwell统计分布随机变化,也可以设为其它要求的数学分布.实验证明,该模拟器测量值与理论符合得很好,且具有较高的重复性和稳定性,响应时间小于1 ms.这种模拟器可用于10 Gb/s和40 Gb/s光传输系统PMD问题的研究. 相似文献
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A Fabry-Perot (F-P) etalon and a semiconductor optical amplifier (SOA) were combined to preprocess the data signals before clock recovery. With this technology in the 10-Gb/s clock recovery utilizing injection mode-locked laser (IMLL) based on SOA, the amplitude fluctuation and timing jitters caused by the pattern effect in recovered clock pulses were greatly reduced, experimentally. It also demonstrated that clock could be recovered from the very degraded signals. 相似文献
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Mitigation of signal quality degradation induced by PMD using synchronous modulation 总被引:1,自引:0,他引:1
In-line synchronous modulation as a way of mitigating the signal quality degradation induced by polarization mode dispersion (PMD) was experimentally studied using 10-Gb/s return to zero signal. Bit error rate of the degraded signal and the synchronously modulated signal under the differential group delay (DGD) values of 10, 20, 34, and 70 ps was measured and compared. The experimental results showed that in-line synchronous modulation is useful to mitigate the signal quality degeneration induced by PMD. 1-dB power penalty reduction was obtained even when the PMD was as high as 70% of the bit interval. The limitation of method is also discussed. 相似文献
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利用半导体激光器的单模速率方程及超短光脉冲在光纤中传输的非线性薛定谔(NLS)方程,从理论及实验上研究了增益开关DFB半导体激光器出射的啁啾光脉冲在色散补偿光纤(DCF)及色散位移光纤(DSF)中的压缩过程与规律.实验上,从1.55μm增益开关DFB半导体激光器出射的重复频率为2.5GHz、脉冲宽度为53.8ps的光脉冲经色散补偿光纤压缩至12ps,而后利用色散位移光纤中的高阶孤子压缩效应将脉冲压缩至2.5ps.改变色散位移光纤参数及入射光功率后获得最窄光脉冲宽度为2.1ps.理论与实验结果符合.
关键词: 相似文献
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