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1.
光子晶体光纤色散特性的研究   总被引:4,自引:1,他引:3  
基于标量近似理论,使用有效折射率方法对光子晶体光纤的群速度色散特性进行了详尽研究.由于光子晶体光纤是由单一材料制成,光纤的总色散便由波导色散决定,将群速度色散分为材料色散和波导色散,在分析光纤结构参数与波导色散关系的同时还讨论了剖面色散对总色散的影响.研究表明:调节光子晶体光纤包层空气柱的节距及其有效芯径,可以实现在很宽的波长范围内的单模传输,可以设计零色散光子晶体光纤和在较宽的波长段接近零色散的色散平坦光纤,以及具有较大正常色散的色散补偿光纤,尤其在零色散光纤设计时必须考虑剖面色散的影响.  相似文献   

2.
Wavelength dispersion characteristics of single-mode silica fibers in a very low-loss region, including zero dispersion wavelengths, are studied in detail using a "difference method." Wavelength dispersion of single-mode fibers is compared for fibers with same material dispersion but with different waveguide structure. Material dispersion is evaluated by extracting waveguide dispersion from experimental results. Effects of waveguide dispersion on the zero dispersion wavelength of the single-mode fiber in a longer wavelength region are clearly analyzed. Single-mode fiber design consideration is given from the wavelength dispersion point of view.  相似文献   

3.
单模光纤反常色散区零色散波长附近的啁啾演变   总被引:1,自引:0,他引:1  
当单模光纤的反常色散区二阶,三阶色散同时存在时,首次推出了群速度色散致啁啾的解析表达式,并讨论了啁啾演变过程。利用数值方法,模拟了零色散波长附近群速度色散效应与自相位调制效应共同作用时啁啾的演变。结果表明,三阶色散会导致脉冲铅的畸变。  相似文献   

4.
相对色散斜率(RDS)理论在分析宽带色散补偿时,存在一定的局限性.提出利用色散系数函数在波长上进行泰勒展开或写成多项式形式的分析方法,分析表明宽带内任意波长要实现色散、色散斜率、色散曲度的补偿,必须使总色散多项式前的系数为零.这种把色散系数函数化成多项式的分析方法,适合于任意精度的宽带色散补偿.最后给出了线性补偿和最高二次项的非线性补偿仿真结果.  相似文献   

5.
利用矢量等效折射率法计算了空气孔间距和包层空气填充率对微结构光纤的非线性系数以及结构色散的影响,通过计算发现孔间距对结构色散曲线的走向起决定性作用,而包层空气填充率的影响主要是使得结构色散大小和位置发生变化,同时减小孔间距以及增大包层空气填充率都会提高非线性系数,最终设计出了几种不同特性的800nm处色散平垣高非线性微结构光纤。  相似文献   

6.
研究了色散管理孤子(DMS)系统中影响时间抖动性能的各个因素。理论分析得出:色散管理(DM)的累积色散、附加累积色散和DM强度是影响时间抖动的重要因素,降低路径平均色散和增大DM强度均能减小时间抖动;附加累积色散对系统时间抖动影响较大,当它等于传输总累积色散量的1/2时,时间抖动最小。数值计算的结果验证了理论分析的正确性,得出的结论对DMS系统中时间抖动性能的改善有一定的帮助。  相似文献   

7.
色散管理光纤中超短光脉冲压缩效应研究   总被引:3,自引:0,他引:3  
本文研究了色散管理光纤中超短光脉冲的压缩效应 .对于两种不同的色散管理光纤 ,分析了脉冲压缩机制和效果 .发现总色散为零和总色散不为零的色散管理光纤对超短光脉冲压缩都有较大的压缩比 ,而后者比前者所需最佳纤长缩短一半 .当考虑高阶色散和高阶非线性项效应时 ,发现脉冲压缩质量有所下降 ,其中总色散不为零的色散管理光纤中脉冲压缩质量劣化更快  相似文献   

8.
高非线性色散平坦光子晶体光纤的研究   总被引:2,自引:2,他引:0  
利用矢量等效折射率法计算了空气孔间距和空气填充率对非线性系数以及波导色散的影响,通过计算发现孔间距对波导色散曲线的走向起决定性作用,而空气填充率的影响主要是使得波导色散大小和位置发生变化,同时减小孔间距以及增大空气填充率都会提高非线性系数,最终设计出了几种不同特性的800nm处色散平坦高非线性光子晶体光纤。  相似文献   

9.
The transmission of ultrashort optical pulses over long distances in optical fibers is limited by pulse broadening due to group velocity dispersion. A grating and telescope dispersion compensator with group velocity dispersion of equal magnitude and opposite sign can compensate for the fiber dispersion. The possible benefits of such dispersion compensation in the 1.3-1.6-μm wavelength region are investigated. The results show that compensation of first-order dispersion at 1.55 μm in a fiber with zero dispersion near 1.3 μm is primarily limited by the second-order dispersion of the grating and the telescope compensator. For a wavelength slightly greater than the zero dispersion wavelength, both the first- and second-order group velocity dispersion can be canceled by the grating and telescope dispersion compensator, allowing transmission exceeding 100 Gb/s over 100 km  相似文献   

10.
A single-mode optical fiber with a convex chromatic dispersion profile is proposed for generating a flat supercontinuum(SC).The fiber has normal dispersion and the dispersion parameter D(λ,z) is a convex function of wavelengths.It is shown from the numerical results that the chromatic dispersion,the flatness of the dispersion curve and the pump conditions have significant effect on SC generation.A flat and broad SC without strong residual pump component can be obtained when the pump wavelength is set in the...  相似文献   

11.
卫星飞秒激光测距理论上可达到亚微米量级的测距精度,但飞秒激光脉冲在大气中传输时由色散导致的脉冲展宽显著,会使测距精度下降。为补偿飞秒激光脉冲在大气中的色散需对其色散量进行定量计算。推导了飞秒激光脉冲在大气中的群速度色散和脉冲展宽公式,表明脉冲展宽程度和群速度色散及传输距离有关;中心波长相同的飞秒激光脉冲脉宽越窄色散越严重,而当脉宽相同时,中心波长越短色散越严重。计算比较了大气和BK7玻璃的群延时、群速度色散和三阶色散。卫星激光测距系统应采用中心波长较长的1 550 nm的飞秒激光脉冲,脉宽应适当选取。由于飞秒激光色散严重,提出了采用单模光纤序列进行粗补偿和采用光栅对进行精密补偿的两种补偿相结合的方式对其色散进行补偿。  相似文献   

12.
依据强双折射光纤中两垂直偏振分量所满足的非线性耦合模方程,研究了三阶色散对偏振分量间的时延差的影响。结果表明,当二阶色散、三阶色散同时存在时,三阶色散可以减小时延差;当只有三阶色散时,除了产生较大时延差外,还会在两个偏振脉冲的前后沿产生较大的色散波。  相似文献   

13.
Dispersion Properties in Total Internal Reflective Photonic Crystal Fiber   总被引:2,自引:2,他引:0  
The dispersion properties in the short wavelength region of total internal reflective photonic crystal fiber have been studied by using the models of the equivalent twin waveguide soliton coupling, effective refractive index,effective normalized frequency and dispersion management solitons. It is shown that the dispersion in the cladding waveguide of the total internal reflective photonic crystal fiber is a positive dispersion,and the dispersion of its core waveguide is a negative dispersion. The method of the compensated probing laser diffraction by the phase hole induced by the stationary pumping laser in the cladding waveguide enables the average dispersion value of the total internal reflective photonic crystal fiber to be close to zero and the zero dispersion point to shift to the short wavelength region.  相似文献   

14.
对色散对光通信系统的影响进行了理论分析;然后以光纤光栅色散补偿和色散补偿光纤为重点,讨论了目前高速光通信系统中的各种色散补偿方案,并对各种方案进行了分析比较,结果表明啁啾光纤光栅色散补偿是最有前途的一种方案;最后对今后色散补偿技术的趋势进行了展望。  相似文献   

15.
An overview is given of dispersion measurements on fluoride glasses and fibers, and the dispersion compensating capability of fluoride fibers is discussed. The temperature dependence of refractive-index dispersion and material dispersion of fluoride glasses is measured. These measurements indicate that fluoride glasses can compensate for temperature-dependent changes of refractive indices and material dispersion in silica glasses and fibers  相似文献   

16.
申静  李俊奇 《激光技术》2019,43(5):641-645
为了研究光差分相移键控(DPSK)调制格式在光纤高速传输系统中的色散补偿, 利用色散补偿光纤(DCF)的色散补偿原理, 对40Gbit/s光纤传输系统进行色散补偿, 分析了40Gbit/s单通道光纤传输系统中3种DPSK调制格式信号的频谱特性; 仿真了3种码型的色散容忍度以及3种调制格式在考虑光纤的非线性下的色散补偿方案。结果表明, 光非归零码差分相移键控(NRZ-DPSK)信号具有最好的色散容忍度, 但其受非线性的影响比较大; 33%归零码差分相移键控(33%RZ-DPSK)信号的色散容忍度差, 但其色散补偿后的效果优于NRZ-DPSK; 而载波抑制归零码差分相移键控信号对色散和非线性效应都有较好的抑制; 3种DPSK调制格式均在对称补偿2方案中色散补偿的效果最佳。此仿真研究对光DPSK信号在光纤中的色散补偿具有参考意义。  相似文献   

17.
This paper proposes a novel adaptive dispersion equalization system that equalizes the temperature-induced dispersion fluctuation in long-span ultra-high-speed optical transmission systems. The system monitors the dispersion fluctuation by measuring the relative delay between two wavelength division multiplexed (WDM) signals, and equalizes the dispersion fluctuation by wavelength tuning. A variable-dispersion equalizer can be used instead of wavelength tuning. Adaptive equalization is successfully demonstrated in 40-Gb/s (8-ps-RZ pulses) 400-km transmission. Furthermore, the proposed equalization system is shown to be applicable to WDM systems that use dispersion and dispersion slope compensation. Since the sensitivity to the dispersion fluctuation is improved by extending the wavelength spacing of the signal and monitor channels, the system is shown to operate even when polarization-mode dispersion (PMD) of the transmission fiber must be taken into account  相似文献   

18.
Ultralong nonreturn-to-zero optical transmission systems with incomplete dispersion compensations are studied. The dispersion of transmission fiber is periodically under- or overcompensated. Postdispersion compensation (PDC) at the receiver is used to compensate for the residual dispersion caused by incomplete compensation and to tailor the signal pulse shape. Formulas estimating the change of pulse width in the absence of amplifier noise during signal transmission and after PDC are given. During signal transmission, pulse width may be compressed or broadened by the combined effect of the dispersion and self-phase modulation (SPM). The change of pulse width nearly increases with the square of the distance during signal transmission. With amplifier noise, system performance evaluated by Q factor is studied. Several types of transmission fibers are considered. The Q factor can be significantly improved by proper PDC. Signal pulse is compressed when PDC is optimized. The characteristics of the maximum Q factor and the residual dispersion are studied, in which PDC is optimized. The results show that to achieve the best system performance, fiber dispersion should be undercompensated for positive dispersion parameter and overcompensated for negative dispersion parameter. The optimal fiber dispersion lies in the range from 4 to 10 ps/km/nm for the considered systems, and the optimal ratio of residual dispersion and fiber dispersion is about 1%  相似文献   

19.
色散管理孤子的传输特性   总被引:1,自引:1,他引:0  
何琼  王晶 《激光技术》2002,26(5):367-369,372
论述了色散管理孤子的传输原理,并利用数值方法模拟了色散管理孤子在不同的传输模式中的传输,研究了色散管理孤子特性及其应用。研究结果表明,色散管理孤子具有很明显的周期性,尤其采用平均路径色散为0的模型传输性能更佳。  相似文献   

20.
Waveform degradation due to polarization and chromatic dispersions in a single-mode fiber is calculated for a coherent CPFSK signal. For a single-mode fiber with polarization dispersion of ⩽1 ps, chromatic dispersion almost dominates the system. However, if a fiber has polarization dispersion of more than a few picoseconds and a chromatic dispersion of less than 0.1 ps/km/nm, which can be attained by using a dispersion-shifted fiber and/or by electric dispersion compensation, polarization dispersion will restrict transmission capacity. For instance, polarization dispersion of 5 ps will restrict a bit rate by ~60 Gb/s when chromatic dispersion is fully reduced using a dispersion-shifted fiber or applying electrical equalization  相似文献   

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