共查询到19条相似文献,搜索用时 187 毫秒
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基于线性啁啾光纤布拉格光栅的色散补偿原理,探讨了不同的准高斯型耦合系数函数曲线对色散补偿特性的影响,建立使该光栅色散补偿曲线既具有高色散系数和宽带特点,同时对边峰还有相对的抑制能力的设计思想。文中讨论了相关参数对色散补偿曲线的影响。 相似文献
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光纤光栅非线性时延对啁啾的电视信号的影响 总被引:1,自引:1,他引:0
分析了有线电视系统中,用作色散补偿的光纤光栅因色散抖动对信号载波互调比产生的影响,结果显示色散抖动对有线电视信号互调比的影响随拦动幅度、抖动周期、信道数目的加而增加,信道频率的分布也对其的影响。对光栅的色散特性进行数值估算,发现常耦合系数线性啁啾光栅不能用的有线电视系统中进行色散补偿。 相似文献
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Chirped Bragg光纤光栅的优化设计与优化指数 总被引:1,自引:0,他引:1
根据线性ChirpedBragg光纤光栅的一般原理 ,探讨了不同啁啾系数 ,准高斯耦合函数对Bragg反射光栅的反射率及色散补偿特性的响应。结果表明 :增大啁啾系数以及选取适当的准高斯耦合函数 ,在保证反射率较大的情况下 ,能有效地改善色散补偿特性。通过引入微波领域的“优化指数”这一概念 ,量化了色散补偿器的补偿能力。 相似文献
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通过对光栅制作过程的优化设计,解决了光纤光栅温度稳定性、纹波系数、带宽、偏振模色 散补偿等关键技术,所制作光纤光栅已经达到温度系数小于00005 nm/℃,带宽大于14 nm,纹波系数小于50 ps,色散量超过 -1000 ps/nm的先进水平. 采用琼斯矩阵本征值法较 精确地测量了光栅的偏振模色散,并对其进行了补偿,光纤光栅色散补偿器的偏振模色散由 补偿前的91406 ps改善为补偿后的01521 ps. 在此基础上,成功地建立了一个稳定可靠 、速率为40 Gb/s,传输链路为122 km G
关键词:
高速光通信系统
普通单模光纤
光纤光栅
色散补偿 相似文献
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为了提高啁啾长周期光纤光栅(LPFG)光纤通信的色散补偿能力,提出了利用薄包层啁啾LPFG进行包散补偿的方法.首先介绍了根据传输信号确定啁啾LPFG的啁啾系数、光栅长度等参数的方法.然后利用上述方法设计了对光纤中传输的中心波长为1550 nm,带宽为0.2nm的信号进行色散补偿的薄包层啁啾LPFG.利用耦合模理论及传输矩阵法计算了约1m长的此种啁啾LPFG的色散,结果表明可以补偿该光信号通过46 km光纤所产生的色散.进一步分析了切趾函数、啁啾系数、交叉耦合系数等参数对薄包层啁啾LPFG色散的影响. 相似文献
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利用啁啾光纤光栅进行色散补偿的研究 总被引:1,自引:0,他引:1
分析了由于光纤的色散引起的脉冲展宽,并介绍了啁啾布拉格光纤光栅进行色散补偿的基本原理。2-5Gb/s、100km 色散补偿的实验结果表明,利用啁啾光纤光栅进行色散补偿是一种切实可行的色散补偿方案。 相似文献
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Dispersion Compensators Based on Overlaped Linearly Chirped Fiber Gratings for DWDM Systems 总被引:1,自引:0,他引:1
1 Introduction ThereisagreatdealofinterestinfiberBragggratingsduetotheirmanyimportantapplicationsinthefieldoftelecommunicationsandfibersensors .BecausefiberBragggratingsexhibitdispersionbothinreflection ,especiallywhenthe gratingischirped[1] ,andintransm… 相似文献
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By introducing a convergent lens in the phase mask setup and by tilting appropriately the fiber from the phase mask, a linearly chirped fiber grating with an appropriate chirp can be obtained conveniently. Using this method, two groups of fiber gratings, each of them is composed of 8 overlaped linearly chirped fiber gratings but with different center reflection wavelength separations (~0.8 nm and ~1.6 nm, respectively) are fabricated. Experimental results show that, the compensators based on the two groups of fiber gratings can be used to compensate for the dispersion of 8×2.5 Gb/s transmission over 100 km of standard single-mode fiber for multiple channels in optical time-division multiplexing (OTDM) and densed wavelength division multiplexing (DWDM). 相似文献
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N.M. Litchinitser M. Sumetsky P.S. Westbrook 《Journal of Optical and Fiber Communications Reports》2007,4(1):41-85
Tunable dispersion has been implemented in various technology platforms, including fiber gratings, planar waveguides, thin
film etalons, and bulk optic technologies. This paper will focus on fiber grating based tunable dispersion compensation, because
fiber gratings are at present one of the best developed TDC technologies available. The paper is divided into three parts.
In the first part we describe grating based TDC technologies and discuss their advantages and disadvantages. We focus on thermally
tuned linearly chirped fiber gratings, as these have to date been the most successful grating technology for 40 Gbit/s. We
also compare grating TDCs to two other prominent tunable dispersion technologies: thin film etalons and planar waveguide ring
resonators. In the second section we describe the techniques used to fabricate high performance dispersion compensation gratings
as well as the theory of the primary defect of fiber grating dispersion compensation: group delay ripple (GDR). In the third
section we describe the telecom system related issues for tunable gratings, including characterization of grating performance,
tunability requirements and results from actual system trials using tunable FBGs. 相似文献
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To model chirped fiber Bragg gratings (FBGs) for dispersion compensation in optical fibers a novel method of single expression
(MSE) is used. The reformulation of Helmholtz’s equation in the MSE to the full set of first-order differential equations
leads to dealing with the electric field amplitude, its derivative, power flow density and phase distributions in any aperiodic
media. The phase derivative obtained numerically permits to compute the dispersion slope in the time delay of investigated
chirped gratings. Reflective and time delay spectra of linearly chirped gratings of different lengths and chirp coefficients
are computed. A self-similarity law for the gratings of the same strength but different lengths and chirp coefficients is
revealed. The apodization of gratings is applied to reduce sidelobes in gratings’ reflection spectra and eliminate oscillations
in the time delay characteristics. 相似文献
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To model chirped fiber Bragg gratings (FBGs) for dispersion compensation in optical fibers a novel method of single expression (MSE) is used. The reformulation of Helmholtz's equation in the MSE to the full set of first-order differential equations leads to dealing with the electric field amplitude, its derivative, power flow density and phase distributions in any aperiodic media. The phase derivative obtained numerically permits to compute the dispersion slope in the time delay of investigated chirped gratings. Reflective and time delay spectra of linearly chirped gratings of different lengths and chirp coefficients are computed. A self-similarity law for the gratings of the same strength but different lengths and chirp coefficients is revealed. The apodization of gratings is applied to reduce sidelobes in gratings' reflection spectra and eliminate oscillations in the time delay characteristics. 相似文献
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啁啾光栅色散及时延特性研究 总被引:2,自引:1,他引:1
基于耦合模理论,通过对耦合波方程进行相位共轭变换,将反向耦合波方程变换为Riccati微分方程,利用数值解法对常耦合系数和高斯型耦合系数线性啁啾光栅的反射特性、色散特性和时延特性进行了详细分析,为设计具有理想效果的色散补偿器件提供了有效的理论方法。 相似文献
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Dispersion-compensating fiber Bragg gratings with approximately 99.9% reflectivity that are made by continuous apodization and phase control are demonstrated. These strong dispersion-compensating gratings provide precision second-order, third-order, or even more complex dispersion compensation, as well as sufficient transmission isolation to be used at add-drop stages without additional filtering. A 99.84% grating with a constant approximately 700-ps/nm dispersion and a 99.94% grating with dispersion varying linearly from 1000 to -1000 ps/nm are demonstrated. 相似文献