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1.
报道了声光光谱色散滤波器(AOPDF)对啁啾脉冲放大系统中脉冲光谱整形及控制技术的实验研究.声光光谱色散滤波器基于共线的声光相互作用,通过控制声光相互作用的位置,产生不同光谱的位相延迟.由于声波信号的幅值决定了光谱的散射效率,因此控制声波信号的振幅可以获得光波频谱的幅值整形.将声光光谱色散滤波器应用到啁啾脉冲放大系统中,可以很好克服增益窄化效应,使放大后脉冲的光谱保持足够的宽度,最终获得更窄脉宽的压缩脉冲.  相似文献   

2.
预啁啾对偏复用孤子技术的补偿   总被引:2,自引:0,他引:2       下载免费PDF全文
王润轩 《激光技术》2005,29(3):315-317,321
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。  相似文献   

3.
物联网、虚拟现实及人工智能等技术的发展加大了对光纤接入无源光网络带宽的需求,其中调制器成为制约无源光网络带宽的关键因素。结合了直接调制激光器和外调制器各自优势的啁啾管理激光器以产生结构简单、便于集成等特点受到了广泛关注。采用耦合速率方程理论研究了啁啾管理激光器的动力学特性,分析了40 Gbit/s啁啾管理调制格式的产生原理及时频域特性,并在高速无色散补偿接入网中与由外调制器产生的40 Gbit/s非归零调制格式进行了性能对比。结果表明,带宽为48.5 GHz的40 Gbit/s啁啾管理调制格式在1 dB灵敏度代价下所对应的色散容限为215 ps/nm,与非归零调制格式相比其无色散补偿传输距离增加了1.6倍,表现出了强的抗色散能力,在高速接入网中也体现了较高的应用价值。相关结果可为实际系统设计提供理论参考。  相似文献   

4.
单量子阱激光器小信号调制时的啁啾噪声   总被引:1,自引:0,他引:1  
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  相似文献   

5.
PSNRZ码在高速光纤通信中的应用研究   总被引:1,自引:0,他引:1  
在分析相位整形不归零(PSNRZ)码基本原理的基础上,提出了一种利用马赫-曾德(MZ)调制器对信号相位进行预调制的方法,该方法能够方便有效地控制信号初始啁啾的形式和大小.文章指出调制深度可以更加直观地反映PSNRZ码的啁啾大小,并推导了调制深度与啁啾系数及链路残余色散之间的关系.最后,在40 Gbit/s通信系统中对P...  相似文献   

6.
分析了空间啁啾对宽带光谱超短脉冲激光系统的影响,提出了利用波前传感器研究神光II 5PW(SG-II-5PW)装置空间啁啾的实验方法。实验中采集了宽光谱超短脉冲激光经过展宽器及多级空间滤波器后的波前特征,测量了系统光路产生的横向空间啁啾和波前像差中心相对系统光轴的偏移量,并通过实时调节色散调节器来消除激光装置的空间啁啾。对比分析了横向空间啁啾被消除前后的波前分布,计算结果表明SG-II-5PW装置激光光束的聚焦性能和远场能量集中度可得到显著提升。  相似文献   

7.
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。  相似文献   

8.
用于飞秒脉冲激光腔内的啁啾镜的优化设计   总被引:3,自引:2,他引:1  
介绍了啁啾镜的基本原理和优化设计思想 ,阐述了优化设计的基本过程 ,并通过计算机优化计算了啁啾镜设计。具体分析了影响啁啾镜色散补偿特性的几个主要因素 ,如色散量、色散带宽、膜层数以及膜层的厚度变化对啁啾镜光学特性造成的影响。其中色散量的控制和色散带宽的选择是最重要的优化设计指标  相似文献   

9.
单模光纤正常色散区啁啾演变研究   总被引:2,自引:1,他引:2  
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。  相似文献   

10.
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。  相似文献   

11.
提出并分析了一种大范围可调谐的通带可变微波光子滤波器。它基于受激布里渊散射(SBS)效应并使用2个调制器与1个光纤布喇格光栅生成泵浦信号。通过分别调节这2个调制器的调制频率,可得双通带滤波器和通带间隔可变的四通带滤波器,并实现滤波器中心频率的大范围连续可调谐,而在整个调谐过程中,滤波器的3dB带宽保持不变。仿真分析了不同调制信号对滤波器通带及中心频率的影响,以及滤波器的带宽与泵浦的功率和SBS增益介质长度的关系。  相似文献   

12.
根据静磁表面波的各向异性色散与传输基本理论,建立了静磁表面波带通滤波器的带宽控制模型。在中心频率及基本带宽一定的情况下,通过调节磁场的方向实现了31MHz的带宽调整。实验结果表明所提出的静磁表面波带通滤波器的带宽控制技术是一种能够有效地控制带宽且易实现的解决方案。  相似文献   

13.
A remnant dispersion monitoring method based on spectral-shift of SOA in high speed optical communication system with CSRZ format and single channel speed of 40 Gbit/s is proposed. The system performance can be optimized by careful choosing bandwidth and center wavelength of the optical fiber grating filter. The dynamical monitoring range is ±60 ps/nm and the monitoring precision is about 5 ps/nm. This method can be suitable for the application in dynamical dispersion compensation of high speed optical communication systems.  相似文献   

14.
提出了采用幅移键控(ASK)调制的波分复用(WDM)系统中光滤波器带宽的优化设计问题。并根据对长距离波分复用系统中影响信噪比的主要因素的分析,计算了优化设计问题,数值计算给出了一些有意义的结果  相似文献   

15.
为了提高调制器的灵活性和可扩展性,设计了一个中心频率和符号速率可调,且支持多种调制体制的高速通用数字调制器方案,并能产生中频为80MHz,带宽为7.9365MHz的正交相移键控(QPSK)信号和16QAM(正交幅度调制)信号。集中论述基于软件无线电的通用调制算法、符号映射原理和高速成形滤波模块的具体实现。测试结果表明,该方案开放性好,结构简单,体积小,具有一定的实用性和通用性。  相似文献   

16.
We present the dispersive characteristics of an electronically tunable optical filter, with application toward delaying high speed digital and analog signals. Square waves can be dynamically delayed and reshaped through a change in injection current to the filter. Since the filter is of an all-pass nature, its usable bandwidth is limited primarily by the phase response (dispersion). We show that for 2-GHz square waves, dispersion is not a limiting factor and the filter can be operated over the full range of delays. At 5 GHz, the pulses can still be delayed, however the range of operation is dispersion limited. Additionally, at 5 GHz this dispersion can be harnessed for pulse reshaping applications. The filter is studied both experimentally and theoretically, demonstrating good agreement.  相似文献   

17.
本文首先对开路边缘平行耦合微带带通滤波器的滤波特性进行了分析,接着使用微波仿真软件ADS对其进行了仿真.仿真时根据设计指标用ADS的优化功能对原理图进行多次优化,优化时注重对多个参数实行逐个优化,使得优化的速度更快.通过对一中心频率为3.05GHz带宽为3.3%的带通滤波器进行仿真,结果很好地满足设计指标.基于ADS优...  相似文献   

18.
A new polarization-independent tunable spectral filter based on the combination of a single isotropic acoustooptic cell and a pair of conventional diffraction gratings is suggested and investigated. The filter features narrow bandwidth, frequency shift compensation, and low polarization dependence. Using standard AMTIR-1 chalcogenide glass acoustooptic modulator with frequency 40-77 MHz and ruled diffraction gratings with 600 grooves/mm, a 3-dB bandwidth of 1.1 nm, and a tuning range of 16 nm were obtained. Tuning range can be increased by the use of acoustooptic cell with increased center frequency or diffraction grating of a lower dispersion. Inserting the filter inside a laser cavity, continuous-wave tunable generation of Er-doped fiber laser with maximum output power 3 mW was realized. When a Fabry-Perot etalon (0.166-nm free spectral range, 40% reflectance) was inserted into laser cavity, the linewidth was observed to be less than 0.05 nm  相似文献   

19.
Distributed microelectromechanical varactors on a coplanar waveguide have been used to design a two- and four-pole bandpass tune-all filters. The two-pole initial bandwidth is 6.4% at 44.05 GHz with a mid-band insertion loss of 3.2 dB and with matching better than 15 dB. The four-pole initial bandwidth is 6.1% at 43.25 GHz with a mid-band insertion loss of 6.5 dB and with matching better than 10 dB. The use of microelectromechanical system bridges allows a continuous tuning for both center frequency and bandwidth. The varactors biasing network has been designed so that the center frequency and bandwidth can be tuned separately. The two-pole filter center frequency can be changed from 44.05 to 41.55 GHz (5.6% tuning range), while the bandwidth can be independently changed from 2.8 to 2.05 GHz. The four-pole filter center frequency can be changed from 43.25 to 40.95 GHz (5.3% tuning range) and the bandwidth can be changed from 2.65 to 1.9 GHz.  相似文献   

20.
In this paper, we investigate experimentally and via simulation the pros and cons of a narrow filter receiver for differential quadrature phase-shift keying based on a single optical filter and eschewing the conventional asymmetrical Mach-Zehnder interferometer structure. We quantify the performance differences between the two receivers, allowing system designers and operators to determine when the less complex narrow filter receiver might be the appropriate choice. We numerically optimize the 3-dB bandwidth and center frequency of the narrow filter and show it is more robust to carrier frequency detuning than the conventional solution. We show that the narrow filter receiver is more tolerant to chromatic dispersion (CD) than the conventional one, and equally tolerant to first-order polarization-mode dispersion. We show the impact of the 3-dB bandwidth on the receiver performance when CD accumulates. Finally, we show via experiments and simulations that the 3 dB advantage of the conventional receiver vanishes when the nonlinear impairments are fiber nonlinearities; comparing the two receivers at the optimum launch power for a 25 times 80 km system, the difference in optical SNR margin is reduced to ~1.6 dB. Experiments are conducted at 42 Gb/s using a commercially available narrow filter for reception.  相似文献   

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