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1.
在单模光纤反常色散区,首次推出了带有初始啁啾的高斯脉冲在二阶,三阶速度色散效作用产生的啁啾解析表达式,用数值法模拟了光纤中啁啾演变过程,研究结果表明,二阶,三阶色散导致非线性啁啾,三阶色散只在脉冲沿附产生啁啾极值,从而使脉冲在前后沿产生振荡结构,当具有负初始啁呼的高斯脉冲入射时,在脉冲中心小区域内净啁啾等于零,可形成孤子。  相似文献   

2.
采用自相似分析方法,基于常系数高阶色散的Ginzburg-Landau方程,通过分离变量法得出了高阶色散效应自相似脉冲演化的解析解,给出了自相似脉冲的振幅、相位、啁啾以及脉冲宽度的一般表达式.研究表明,在增益光纤的二阶正常色散区域,同时考虑高阶色散和增益色散双重效应影响下演化的自相似孤子脉冲仍然保持线性啁啾;振幅解析解的三阶色散效应显著.这与数值计算的结果非常一致. 关键词: 三阶色散 Ginzburg-Landau方程 自相似脉冲 二阶正常色散  相似文献   

3.
啁啾sinc取样光纤光栅研究   总被引:10,自引:9,他引:1  
提出了一种特殊的取样光纤光栅:啁啾sinc取样光纤光栅.研究表明,对于均匀光纤光栅进行啁啾sinc取样,可以实现色散斜率补偿和获得精确的反射波长数控制;对啁啾光纤光栅进行啁啾sinc取样,则能够实现色散和色散斜率的同时补偿,并且可以进行精确的波长数控制及获得各信道一致的反射率.利用啁啾sinc取样光纤光栅,可以对各种传输光纤进行色散和色散斜率的补偿.  相似文献   

4.
啁啾双光纤光栅群时延特性   总被引:2,自引:2,他引:0  
丛军  陈晓明  章献民 《光子学报》2004,33(3):299-302
研究了变迹线性啁啾双光纤光栅的群时延特性及其在高次色散补偿中的应用.分析表明,群时延特性与周期差ΔΛ和不同的啁啾参量C有很大的关系.研究结果表明啁啾双光纤光栅在高次色散补偿和光纤CDMA中有应用价值.  相似文献   

5.
王晶  刘秀敏 《光子学报》1997,26(12):1082-1085
利用傅里叶变换法,首次推出了单模光纤正常色散区中二阶、三阶色散共同决定群速度色散效应时,所致啁啾的解析表达式.利用数位解法,模拟了零色散波长附近群速度色散效应和自相位调制效应共同导致的啁啾演变过程.计算结果表明:啁啾为非线性的,且有极值,因而导致脉冲形状的畸变.  相似文献   

6.
线性啁啾光纤Bragg光栅的实验研究   总被引:2,自引:2,他引:0  
本文给出了142mm长相位掩模板和扩束技术研制的色散补偿线性啁啾Bragg光纤光栅(CFBG)的反射谱特性及传输实验结果,本实验研制的线性啁啾Bragg光纤光栅样品带宽为0.56~0.92mm.可实现对普通光纤色散补偿100km以上,色散代价小于1.5dB.  相似文献   

7.
在理论上,我们利用光波的时域场包络方程分析了光纤CATV系统中的二阶非线性失真问题和获得理论的表达式,且分析的结果和数值模拟的结果很好的吻合。在实验上,利用啁啾光纤光栅的调谐特性来改变系统的色散补偿量进行了125公里的光纤CATV的系统实验,很好的证实了以上的理论推导。理论和实验的结果都证实适当的选择啁啾光纤光栅的色散补偿量可以很好的改善系统二阶非线性失真的性能。  相似文献   

8.
基于在正常色散渐减光纤(ND-DDF)或者正常色散光纤放大器,获得线性啁啾抛物线脉冲,提出并分析了利用ND-DDF放大器获得线性啁啾抛物线脉冲的优化方案.数值研究结果表明:与用ND-DDF或者正常色散光纤放大器获得线性啁啾抛物线脉冲的方案相比,利用ND-DDF放大器获得的抛物线脉冲的线性啁啾更为明显;研究还发现,增益影响着线性啁啾的大小和质量.计算表明,利用ND-DDF放大器产生的抛物线脉冲经啁啾补偿后可获得更大的压缩因子和更高的峰值功率.  相似文献   

9.
色散渐减光纤中自相似脉冲传输特性研究   总被引:7,自引:4,他引:3  
研究了在高阶色散影响下,自相似脉冲在具有正常色散的色散渐减光纤中的演化情况.结果表明:当考虑高阶色散的影响时,脉冲的啁啾仍然具有很强的线性特性,只是中心变得不对称,产生中心漂移.这种啁啾特性使得自相似脉冲在时域中的抛物线形状产生畸形,导致了脉冲峰向一边延迟,并使脉冲的中心位置漂移,同时伴随着脉冲边沿的振荡.但是通过采用色散补偿技术,自相似脉冲强的线性啁啾仍然可以得到高质量的飞秒量级压缩脉冲,与忽略三阶色散影响时得到的压缩脉冲的脉宽近似相等.  相似文献   

10.
苗洪利 《光子学报》1998,27(6):513-516
利用傅里叶变换法得到了色散阶变光纤正常色散区群速度色散导致啁啾的解析表达式;而且,采用数值法模拟了色散阶变光纤正常色散区啁啾演变过程。结果表明:色散阶变光纤中啁啾以色散缓变光纤中啁啾为中心跳跃式变化,但远小于常规光纤中啁啾。选择合适入射脉冲初始啁啾会使净啁啾等于零,从而形成暗孤子。  相似文献   

11.
Parabolic pulse propagation in a dispersion-decreasing fiber with normal group velocity dispersion (ND-DDF) has been studied when the third-order dispersion (TOD) is included. The results show that the characteristic of exact self-similarity and linear chirp will be lost due to the third-order dispersion. However, by using the dispersion compensation technique, one can obtain efficient and high-quality compressed pulses. The analytic results have been confirmed using numerical simulations.  相似文献   

12.
This article investigates the interaction between the third-order dispersion in optical fiber and the nonlinear (quadratic) chirp of Gaussian impulses. A formula is obtained for the impulse form at the fiber far end. The impulse propagation in nonlinear fiber is also examined by means of a computer simulation. The obtained results indicate that the interaction may lead to significant distortion of optical impulses at the fiber output even when the second-order dispersion is entirely canceled and the input impulse has no linear chirp. This distortion is more pronounced when the dispersion slope, fiber length, and nonlinear chirp parameter increase.  相似文献   

13.
The impacts of polarization mode dispersion (PMD) on the pulse-width in linear systems have been investigated. The analytical solutions, including the effects of initial frequency chirp and group velocity dispersion (GVD), are derived. Analyses show that the pulse broadening effects induced by the second-order PMD depend on GVD and chirp parameter, which are different from those induced by the first-order PMD. An initially chirped Gaussian pulse is taken as an example, upon which analytical solutions of rms pulse-width are derived before and after the first-order PMD compensation. The first-order PMD compensator is also evaluated based on these solutions. The results show that the pulse broadening effects will be resisted efficiently by choosing appropriate GVD and chirp parameter; in general, the post-transmission compensation method will be less efficient than the PSP-transmission method.  相似文献   

14.
By numerical simulations, we show that picosecond Gaussian optical pulses with a precise optimal frequency chirping can transmit stably in full-dispersion compensation optical fiber links, with not only second- but also third-order dispersion compensation, using dispersion shift fibers with opposite dispersion sign. The optimal pre-chirp is determined principally by the second-order dispersion scheme and scarcely affected by third-order dispersion scheme. It demonstrates that, to a high bit rate transmission system, the pre-chirping technology and higher-order dispersion compensation are two very efficient measures in improving performance of system.  相似文献   

15.
The paper deals with the influence of higher-order effects of dispersion on the femto-second transform limited pulse generation by compensating for linear chirp of self-phase modulation spectra in the dispersion-shifted fibers. It has been shown that the minimum propagation length with first-order dispersion term is 23 m, as reported earlier. If the higher-order dispersion effects are taken into consideration, this length is reduced to 11.5 m. With compensation of the first-order dispersion term, this length can be enhanced to 6.8161 × 103 km. This length can further be improved to 6.0343 × 109 km by compensation of first- and second-order dispersion terms together. The minimum pulse width and linewidth product without dispersion, with dispersion including higher-order dispersion effects, and with dispersion compensation, is found to be 0.44, 0.4418, and 0.4411, respectively.  相似文献   

16.
In this paper,we report on the enhanced pulse compression due to the interaction between the positive third-order dispersion (TOD) and the nonlinear effect (cross-phase modulation effect) in birefringent fibres.Polarization soliton compression along the slow axis can be enhanced in a birefringent fibre with positive third-order dispersion,while the polarization soliton compression along the fast axis can be enhanced in the fibre with negative third-order dispersion.Moreover,there is an optimal third-order dispersion parameter for obtaining the optimal pulse compression.Redshifted initial chirp is helpful to the pulse compression,while blueshifted chirp is detrimental to the pulse compression.There is also an optimal chirp parameter to reach maximum pulse compression.The optimal pulse compression for TOD parameters under different N-order solitons is also found.  相似文献   

17.
The paper deals with the influence of higher-order effects of dispersion on the femto-second transform limited pulse generation by compensating for linear chirp of self-phase modulation spectra in the dispersion-shifted fibers. It has been shown that the minimum propagation length with first-order dispersion term is 23 m, as reported earlier. If the higher-order dispersion effects are taken into consideration, this length is reduced to 11.5 m. With compensation of the first-order dispersion term, this length can be enhanced to 6.8161 × 103 km. This length can further be improved to 6.0343 × 109 km by compensation of first- and second-order dispersion terms together. The minimum pulse width and linewidth product without dispersion, with dispersion including higher-order dispersion effects, and with dispersion compensation, is found to be 0.44, 0.4418, and 0.4411, respectively.  相似文献   

18.
In this article we present improved theoretical investigations into relative intensity noise (RIN), including the impact of a third-order dispersion term for dispervive optical communication systems. It has been shown that the third-order dispersion term has no impact on RIN even at high noise frequencies as reported by other authors, but with second-order dispersion compensation, the RIN can be dramatically reduced, thereby improving overall system performance. Further, the impact of fiber length and laser linewidth has been investigated for RIN. It has been shown that, as the fiber length increases, the value of RIN increases but the improvement over RIN with second-order dispersion compensation decreases. Also, with decrease in the value of linewidth, the RIN can be reduced to a great extent.  相似文献   

19.
Optical pulse compression using high-order dispersion compensation is proposed and theoretically analyzed. Firstly, the required dispersion profile for the high-order dispersion compensation is derived, according to the linear chirp and the nonlinear chirp of a phase-modulated continuous-wave (CW) laser source. With the use of the high-order dispersion compensation, such as the combination compensation of the second order dispersion (SOD) and the fourth order dispersion (FOD), an efficient pulse compression having a less time-bandwidth product and a greater peak power is realized. A sampled fiber Bragg grating (FBG) with both the SOD and the FOD is then designed using the equivalent chirp and the reconstruction algorithm. Finally, in the numerical simulation an optical pulse with a time-bandwidth product of 0.79 is generated via high-order dispersion compensation that is performed by using the sampled FBG.  相似文献   

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