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1.
负啁啾脉冲在正负色散光纤中传输特性研究   总被引:5,自引:2,他引:3  
余建军  张晓光 《光学学报》1997,17(10):423-1428
对负啁啾脉冲在正常色散光纤中传输特性进行了数值分析和实验研究,数值分析与实验结果基本一致。数值分析和实验证明正常色散光纤不仅能压窄负啁啾的脉宽而且能压窄频谱,采用正常色散光纤消啁啾后用色散位移光纤为传输媒质成功地进行了一阶和高阶孤子传输。  相似文献   

2.
陈勇  刘艳  曹继红  谭中伟  简水生 《物理学报》2006,55(10):5288-5293
分析了光纤光栅不理想特性的产生机理,对以啁啾光纤光栅为色散补偿器的10Gb/s光传输系统中,啁啾光纤光栅的不理想特性包括群时延纹波、反射纹波及光栅通带带宽对采用归零码(RZ)、非归零码(NRZ)以及载波抑制归零码(CSRZ)三种调制格式传输系统性能的影响进行了详细的数值分析和比较. 同时进行了基于光纤光栅色散补偿的1500km无误码传输实验,通过对啁啾光纤光栅由于不理想特性的差别而导致对实际传输系统不同信道性能影响的比较,进一步验证了仿真分析的正确性. 关键词: 光传输 啁啾光纤光栅 不理想特性 调制码型  相似文献   

3.
优化调制格式实现2560 km低代价无误码传输   总被引:4,自引:4,他引:0  
陈勇  曹继红  陈婷  简水生 《光学学报》2006,26(3):31-335
在单级调制器产生非归零码(NRZ)基础上,分析了利用双级调制器产生归零码(RZ)以及载波抑制归零码(CSRZ)的方法和特点。对非归零码,归零码和载波抑制归零码在以掺铒光纤放大器(EDFA)为单一的功率放大、以啁啾光纤光栅(CFBG)为色散补偿器的10Gb/s系统中的传输性能进行了计算机仿真并比较这三种调制码型的传输特性。同时在实际的2560km G.652光纤链路上利用上述三种调制格式以点对点形式进行了8×10Gb/s传输实验,通过适当控制线路的功率分配以及合理安排系统的色散补偿,实现了三种调制格式的无电中继条件下的零误码传输。计算机仿真和实际实验结果进一步表明,载波抑制归零码的采用有利于优化系统的传输性能,降低传输代价,载波抑制归零码在上述配置的实际传输系统中无误码传输2560km功率代价仅为2.5dB。  相似文献   

4.
啁啾高斯脉冲经啁啾光纤光栅反射后的传输特性   总被引:6,自引:3,他引:3  
舒学文  黄德修  阮玉 《光学学报》1999,19(10):305-1309
在考虑侈阶和高阶色散的情况下,给出了啁啾高斯光脉冲被啁啾光纤光栅反射后在光纤中传输时脉冲展宽的解析析式,。讨论了啁啾光栅脉减压缩和色散补偿中的几个重要问题。以线性啁啾光纤光栅为实例进行了数值计算,发现了脉冲殿宽的对称性质,最后提出一种新颖的可用于估算脉冲受光纤光栅作用后脉宽展宽的简单办法。  相似文献   

5.
从理论上分析了色散缓变单模光纤中啁啾演变特性。采用储里叶变换法得到了只有群速度色散效应或自相位调制效应时皮秒脉立足点啁啾的解析解,利用数值法模拟了色散缓变光纤中皮秒脉立足点秋演变过程。结果表明:色散缓变光纤中的啁啾比常规光纤中的啁啾小,而且,合理选择光纤色散参数可实现脉冲波形无畸变传输。  相似文献   

6.
皮秒脉冲在零平均色散光纤链中传输的数值模拟   总被引:2,自引:0,他引:2  
基于一种二阶和三阶色散都作了完全补偿(路径平均色散为零)的光纤级联系统模型,用数值法对1ps脉宽的高斯光脉冲长距离传输作了数值模拟.结果表明:这种完全补偿的高阶色散控制系统消除了三阶色散引起的脉冲边沿部的振荡,减弱了脉冲峰的时间移动.在不同的入上分别给输入脉冲附加以最佳的频率啁啾,可使得光脉冲的宽度`啁啾及振都围绕在初始值附近波动,在每个补偿端末基本恢复到初值,从而形成光脉冲的推稳定传输.功率增大,稳定传输的距离减小.预啁啾和零平均色散传输并不能完全消除脉冲峰的时间移动。累积的脉冲峰移与预啁啾无关,随功率增大而增大。脉宽的变化与功率和预啁啾都相关。另外,我们也考察了掺饵光纤放大器EDFA的噪声在该系统中引起的时间抖动特性。  相似文献   

7.
徐永钊  张耿  叶海  刘敏霞 《发光学报》2016,(11):1360-1366
采用两段级联单模光纤对高阶孤子脉冲进行压缩。两段光纤具有不同的反常色散值,当高阶孤子脉冲在第一段光纤中获得最大程度压缩时,通过转换色散值不同的光纤,使压缩脉冲继续以高阶孤子的形式在第二段光纤中再次被压缩。每段光纤的长度都进行了优化,使得脉冲在每段光纤中都获得最大程度的压缩。基于非线性薛定谔方程,数值研究了初始啁啾对高阶孤子脉冲压缩的影响。研究结果表明,初始啁啾对高阶孤子脉冲的压缩有重要影响。与无初始啁啾时的情形相比,正的初始啁啾能增强每段光纤中脉冲的压缩效果,降低压缩脉冲的基座能量,而负初始啁啾的影响则相反。随着初始啁啾参量Cp的增大,脉冲在每段光纤中的压缩因子均增加,而基座能量、最优光纤长度均减小。  相似文献   

8.
单模光纤中三阶色散对超短光脉冲传输的影响   总被引:4,自引:0,他引:4  
刘群  励强华  牟艳秋 《光学技术》2006,32(1):148-150
基于超短光脉冲在单模光纤中传输时高阶非线性效应的影响。应用非线性薛定谔方程(HONLS)理论,考虑光纤色散三阶效应,推导出无啁啾的高斯脉冲沿光纤传输时脉冲变化的表达式,并对理论结果进行了数值模拟与分析。结果表明,三阶色散会引起光脉冲形状发生畸变,会在其前沿或后沿附近形成非对称的振荡结构。  相似文献   

9.
初始啁啾补偿光纤色散效应的适用范围   总被引:6,自引:5,他引:1  
王润轩 《光子学报》2005,34(1):78-81
以啁啾高斯脉冲在单模光纤中的传输为例,分别就线性初始啁啾对光纤二阶和三阶色散的补偿进行了系统的理论分析和数值计算,结果表明:线性初始啁啾对光纤的二阶色散(线性色散)有一定的补偿作用,但不能有效地用于三阶色散的补偿.  相似文献   

10.
类明孤子在光纤中传输特性的变分研究   总被引:10,自引:4,他引:6  
谢应茂 《光学学报》2004,24(4):52-455
应用变分法,研究了微扰对类明孤子在光纤巾非线性传输特性的影响,导出了类明孤子脉冲参量演化的动力学方程。它统一了在单模光纤、色散缓变光纤或色散控制光纤中类明孤子脉冲参量演化的动力学方程。在此基础上,计算了色散缓变光纤中的线性高阶色散微扰。结果表明:线性高阶色散对类明孤子脉冲的位置和相位有影响,而对振幅、宽度和啁啾没有影响;光纤色散缓变对类明孤子脉冲的所有参量均有影响。  相似文献   

11.
We demonstrate propagation of femtosecond pulses in the 800-nm range through a hollow-core photonic crystal fiber with preserved temporal and spectral profiles for pulse energies up to 4.6 nJ. Without the use of a prechirping unit, 170-fs pulses were transmitted essentially undistorted at 812 nm, near the zero-dispersion wavelength. Because of the air guidance of pulses, intensity-dependent nonlinear effects were minimal, with only 15% pulse broadening occurring at 350-mW average output power. This fiber thus is excellently suited for applications that require single-mode delivery of high-energy ultrashort pulses to the fiber output face such as, for example, miniaturized multiphoton microscopes.  相似文献   

12.
采用反射式达曼光栅建立了一种产生飞秒激光双脉冲的新装置.由于采用反射式结构,避免了材料色散和吸收导致的脉冲畸变,并构建了一台二次谐波-频率分辨光学开关装置对产生的双脉冲进行了测量.实验结果表明可以实现脉冲强度相等、时间宽度相同、不同间隔的双脉冲输出.产生双脉冲的装置在飞秒激光领域有着应用的价值. 关键词: 飞秒激光双脉冲 达曼光栅 二次谐波-频率分辨光学开关  相似文献   

13.
The simple and efficient fiber delivery of 5-ns pulses from a XeCl excimer laser operating at a wavelength of 308 nm is demonstrated. The coupling scheme uses all of the output energy of the XeCl excimer laser and benefits from a simple and easy-to-adjust fiber coupling. Experiments on the 308-nm fiber delivery for more than 2.5 million laser pulses of 8-ns pulse width (FWHM) and up to 8-mJ stabilized pulse energy are performed. The long-time pulsed UV laser transmission is found to be different for individual samples of optical fibers that perform very similarly in low-intensity UV light applications. For applications with strict demands on the long-time stability, a critical evaluation of the fiber performance with the 308-nm laser under operating conditions is necessary. Measurements between 1 and 200 Hz show a negligible dependence of the fiber delivery performance on the repetition rate of the transmitted laser pulses. PACS 42.55.Lt; 42.81.Cn; 07.69.Vg  相似文献   

14.
多路窄脉冲功率线路合成   总被引:3,自引:3,他引:0       下载免费PDF全文
介绍了传输线变压器的结构特点,对其进行了理论分析和实验研究。采用传输线变压器结构将每路幅度约为4.5 kV/50Ω的4路脉冲合成了幅度约8.8 kV/50Ω的脉冲,通过实验证实了采用多根传输线串并联方式构成的传输线变压器装置可以将多路窄脉冲进行线路功率合成。应用此类结构设计了一种紧凑的高压窄脉冲发生器,将36路8 kV/50Ω的脉冲合成了约46 kV/50Ω的脉冲。采用传输线变压器合成器,应确保各路输入脉冲的前沿抖动足够小和高精度同步。  相似文献   

15.
This paper presents the influences of polarization mode dispersion (PMD) on the performance of soliton transmission system in birefringent fibers. Dispersive waves generated in single mode fibers due to PMD degrade the soliton transmission system in two aspects. First, solitons continuously lose their energy, thus cause enhancement in pulse width. Second, the dispersive waves interact with neighboring pulses and cause distortion in a sequence of pulses. Both these effects reduce the effective bit-rate and degrade the performance of high-speed optical transmission systems. Optical fibers with large group velocity dispersion (GVD) have less dispersive waves and are relatively robust to pulse broadening, but it enhances the interaction between the adjacent pulses. In this paper, we analyzed these effects of PMD on soliton propagation in birefringent fibers and introduced nonlinear gain devices with perturbation terms proportional to second and fourth power of amplitudes to reduce these effects. We proposed Symmetric Split-Step Fourier Method to solve the coupled nonlinear Schrödinger equations (CNLSE); which yields better results over the existing Split-Step Fourier Method.  相似文献   

16.
In this paper, we have investigated the performance of first- and second-order path-averaged soliton long-haul transmission link including the impact of third-order dispersion (TOD) at varied chirp. Here, the varied chirp is considered keeping in view the inadvertent frequency chirp imposed on all practical sources of short optical pulses. The propagation of strongly chirped pulses in loss-managed long-haul path-averaged soliton transmission network has been shown. The investigations reveal that in first-order (N=1) path-averaged soliton transmission link at 10 and 20 Gb/s, SPM effect on the rising and falling edges of a pulse results in spectral broadening for all values of induced chirp. On the contrary, spectral narrowing of the pulses is observed in second-order negatively chirped path-averaged soliton pulses. The effect of the nonlinearity changes from narrowing to broadening of pulses if the sign of the initial chirp is changed to positive. The results ascertain that the system is capable of transmitting a pulse up to the distance of 24,500 km at bit rates of 10 and 20 Gb/s. Investigations have been carried out by varying the chirp factor in the range −1 to 1 and −1 to 0.4] for 10 and 20 Gb/s, respectively, to demonstrate the robustness of the long-haul soliton link. The observations establish that the pulse width (full-width at half-maximum (FWHM)) remains within the optimal range even at the transmission distance of 24,500 km without and at discrete values of the chirp factor.  相似文献   

17.
A new scheme for two-dimensional parallel data transmission with a femtosecond laser pulse through a single-mode fiber, which is based upon one-dimensional space-time conversion technique in conjunction with code division multiple access (CDMA), is implemented and numerically demonstrated. Since many one-dimensional spatial data, which are encoded with their own M-sequence code, must be embedded in a single pulse, the bit-error rate performance degrades compared with conventional CDMA driven by many unsynchronized pulses. Still, two-dimensional digital images in a 16 bits × 16 bits plane (256-bits parallel data) are successfully transmitted by a single femtosecond laser pulse at an equivalent transmission rate of 1.6 Tbit/s and recovered by spectral holography.  相似文献   

18.
For Gaussian, Lorentzian, and square pulses passing through an absorbing medium the transmission is calculated. The atoms in the medium are regarded as two-level-systems. The pulses are assumed to be so weak that the change of population in the lower level is small. The transmission in our case of (weak) non-linear absorption depends on the shape of the pulse and the longitudinal relaxation time. Knowing the transmission the relaxation time can be determined by means of the computed curves of the mentioned three types of pulses.  相似文献   

19.
Mode-locked lasers, Q-switch systems and discrimination amplifiers make use of saturable absorbers. The interaction of those absorbers with light pulses is well known, either for very long or very short pulses, but not, if the pulse width is comparable with the absorber life time, which occurs very often in experiments. Moreover, the spatial structure of the pulse is mostly not considered. In this paper, we investigate in detail the interaction of gaussian pulses (spatial and temporal) with the two-level-absorber. Energy transmission, pulse shortening and pulse asymmetry are calculated as functions of pulse width and small signal transmission of the absorber.  相似文献   

20.
快脉冲直线型变压器驱动源同步触发系统   总被引:1,自引:1,他引:0       下载免费PDF全文
提出了一种基于单传输线脉冲成形技术的模块化快脉冲直线型变压器驱动源的同步触发系统的概念设计,主要由级数较少的Marx发生器、脉冲形成线、主开关、脉冲传输线及触发引出电缆等组成。利用等效电路模型,研究了Marx发生器与脉冲形成线的配合关系,当发生器同时驱动多路形成线时,可以有效增加触发脉冲的数量,并能提高能量利用效率,但触发脉冲的幅值会降低。研究了水介质线阻抗与引出电缆数量对触发脉冲的影响,结果表明:随着电缆序号的增加,触发脉冲的幅值逐渐降低,并且水介质线的阻抗越高,幅值降低的速度越快。触发脉冲也可同时引出,驱动单路形成线输出60路时,触发脉冲的峰值约为293 kV,前沿约11 ns;当驱动5路形成线输出300路时,触发脉冲的峰值约为151 kV,前沿约11 ns。  相似文献   

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