光纤—光纤光栅脉冲压缩器的研究

本文提出了利用正常色散光纤加线性啁啾光纤光栅组成全光纤光脉冲压缩器方案,理论和数值分析了压缩器的压缩特性,给出光纤－光纤栅压缩器的设计规则,指出了有关文献压缩器设计规则的局限性,提出了新结论。     

电声与音频设备

0115113光纤-光纤光栅脉冲压缩器的研究[刊]/张晓光//光电子·激光.—2001,12(4).—329～333(C)本文提出了利用正常色散光纤加线性啁啾光纤光栅组成全光纤光脉冲压缩器方案。理论和数值分析了压缩器的压缩特性,给出光纤-光纤光栅压缩器的设计     

啁啾光纤光栅色散补偿理论浅析

根据量子力学理论导出光纤色散理论模型,并从光的波动理论出发,给出线性啁啾光纤光栅色散基本方程;然后利用线性啁啾光纤光栅对色散的补偿原理、特性及其局限性作了定性分析.     

无初始啁啾高斯光脉冲的色散展宽及色散补偿

对无初始啁啾高斯脉冲在普通单模光纤中的传输特性及线性啁啾光纤光栅的色散补偿特性进行了理论分析和数值模拟。结果表明,光纤的色散导致了传输脉冲的展宽,线性啁啾光纤光栅能够实现对展宽脉冲的良好补偿,啁啾光栅时延曲线的平滑度和线性度都是影响其色散补偿性能的重要因素。本文对啁啾光纤光栅的制作及其在色散补偿中的应用有一定的指导意义。     

啁啾光纤光栅色散补偿理论浅析

根据量子力学理论导出光纤色散理论模型。并从光的波动理论出发，给出线性啁啾光纤光栅色散基本方程；然后利用线性啁啾光纤光栅对色散的补偿原理，特性及其局限性作了定性分析。     

偏振模色散和时延抖动对啁啾光纤光栅色散补偿特性的影响

对存在偏振模色散(PMD)和群时延(GD)抖动的非理想线性啁啾光纤光栅的色散补偿特性进行了研究。实验测量了啁啾光纤光栅的群时延谱和偏振模色散光谱，理论分析和实验测量表明，啁啾光纤光栅差分群时延(DGD)抖动与其时延抖动密切相关。通过数值模拟方法，计算了线性啁啾光纤光栅偏振模色散眼图代价与入射到啁啾光纤光栅色散补偿器的光信号的偏振方向的关系，计算结果表明在使用啁啾光纤光栅色散补偿器时应对光信号的偏振方向进行调整，以获得最佳补偿效果。另外结合实验数据，模拟计算并讨论了非理想线性啁啾光纤光栅群时延抖动和偏振模色散引起的信号的展宽和脉冲形状的劣化。     

高斯脉冲在光纤中传输的光纤光栅色散补偿研究

高斯脉冲在光纤中传输一段距离后，啁啾系数和脉冲宽度均要发生变化，不同啁啾系数和脉冲宽度的高斯脉冲经过啁啾光纤光栅反射后的脉宽压缩特性也不同。本文介绍了啁啾高斯脉冲在光纤中的传输特性以及啁啾高斯脉冲经啁啾光纤光栅反射后的传输特性。理论分析和实验均表明，使用啁啾光纤光栅实现长距离色散补偿时，最佳色散补偿长度与光栅位置有关。     

利用线性啁啾光纤光栅进行色散补偿的理论研究

利用耦合模方程,对具有不同耦合系数的线性啁啾光纤光栅的色散特性进行了理论和数值分析。通过分析发现,具有余弦函数形式耦合系数的线性啁啾光纤光栅具有良好的色散特性;超高斯函数形式和高斯函数形式的次之;线性函数形式的较差。最后利用部分啁啾光纤光栅对１０Ｇｂ／ｓ、１００ｋｍ的光通信系统进行色散补偿,数值分析结果证实了前面的结论。     

利用相位和强度调制器产生高消光比超短光脉冲

提出了一种产生高消光比超短光脉冲的新方法.利用相位调制器调制连续光生成啾啁光,而后利用M-Z强度调制器的倍频调制抑制对压缩不利的啁啾部分的影响,再通过等效啁啾光纤光栅进行压缩产生光脉冲.理论和仿真结果表明,该方法可以很好地消除光脉冲的基底及减小旁辦,产生消光比大于30 dB、波形理想的光脉冲,具有很强的可实现性.最后利用实际制作的色散系数为-380 ps/nm的等效啁啾光纤光栅对该方法进行了实验验证,结果表明,在重复频率为2.5 GHz、相位调制系数为9时,可产生脉宽小于18 ps的高质量光脉冲.     

纯切趾线性啁啾长周期光纤光栅的研究

为进一步拓宽长周期光纤光栅在光通信领域中的应用,在长周期光纤光栅中引入纯切趾包络和线性啁啾,构成光谱特性更为丰富的纯切趾线性啁啾长周期光纤光栅。采用耦合模理论,对纯切趾线性啁啾长周期光纤光栅中的模式耦合特性进行了研究,给出了纯切趾线性啁啾长周期光纤光栅的耦合系数和耦合模方程。在此基础上,详细研究了啁啾和切趾对长周期光纤光栅光谱特性的影响,讨论了纯切趾长周期光纤光栅用作色散补偿器的结构特性和色散补偿机制。最后,设计出一种采用两个相同光栅对称级联的基于纯切趾线性啁啾长周期光纤光栅的色散补偿器,该器件的3dB带宽为0.16nm,3dB带宽内的色散值约为-1954psnm,时延曲线偏离线性的波动幅度小于±2.5ps。     

The compression of optical pulses using self-phase-modulation andlinearly chirped Bragg-gratings in fibers

We report the first demonstration of pulse compression in optical fiber using linearly chirped Bragg gratings as quadratic compressors for pulses spectrally broadened by self-phase modulation. With the system investigated an initial 2 ps, bandwidth limited pulse is compressed by a factor of >10. The experimental results are found to be in good agreement with analytical and numerical calculations. Such a system allows high quality compression of pulses in optical fiber for the first time     

Photonic Generation of Chirped Microwave Pulses Using Superimposed Chirped Fiber Bragg Gratings

A novel approach to generating linearly chirped microwave pulses in the optical domain based on spectral shaping and linear frequency-to-time mapping is proposed and experimentally demonstrated. In the proposed system, the spectrum of a femtosecond pulse generated by a mode-locked fiber laser is spectrum-shaped by an optical filter that consists of two superimposed chirped fiber Bragg gratings (SI-CFBGs) with different chirp rates. The SI-CFBGs form a Fabry-Perot cavity with a cavity length linearly dependent on the resonance wavelength, thus a spectral response with an increased or decreased free spectral range is generated. A chirped microwave pulse with the pulse shape identical to the shaped spectrum is obtained at the output of a high-speed photodetector thanks to the frequency-to-time mapping in a dispersive device. The proposed technique is experimentally demonstrated, a linearly chirped microwave pulse with a central frequency of 15 GHz and a chirp rate of 0.0217 GHz/ps is experimentally generated.     

Theoretical Discussion of Couple-Mode Using Chirped Fiber Grating for Dispersion Compensation

１ＩｎｔｒｏｄｕｃｔｉｏｎＡｔｐｒｅｓｅｎｔ，ａｓｔｈｅｅｒｂｉｕｍｄｏｐｅｄａｍｐｌｉｆｉｅｒｓｈａｖｅｓｕｃｅｓｆｕｌｙｂｅｅｎａｐｐｌｉｅｄｔｏｏｐｔｉｃａｌｆｉｂｅｒｌｉｎｋｓ，ｔｈｅｌｏｎｇｈａｕｌｈｉｇｈｂｉｔｒａｔｅｏｆｏｐｔｉｃ...     

增益开关DFB激光器啁啾消除技术的研究

对线性啁啾光纤光栅消啁啾技术进行了理论和数值分析,给出光纤光栅设计中的一些重要参数,并与Ｆ－Ｐ光谱窗消啁啾法和正常色散光纤消啁啾法做了比较。研究结果表明,光纤光栅的啁啾消除效果要好于其他两种方法,尤其是在消除非线性啁啾方面效果更为突出。     

线性chirp光纤光栅色散补偿器的理论与计算

从物理上解释了线性ｃｈｉｒｐ光纤光栅色散补偿器的工作原理，根据耦合理论，导出光纤光栅的基本方程，利用这一方程，计算了线性ｃｈｉｒｐ光纤光栅的响应特性。     

线性啁啾光纤光栅变迹函数的研究

文中利用传输矩阵法对我们构造的四种变迹函数所描述的线性啁啾光纤光栅的光学特性进行了数值计算,并与常用的高斯型变迹线性啁啾光纤光栅的最佳光学特性进行了比较和分析,得出了一些有意义的结论,为设计和制作合适的线性啁啾光纤光栅用作色散补偿器提供了一定的理论依据。     

Bragg光纤光栅

详细阐述了光纤光栅的原理以及光纤光栅在光纤通信、光纤激光器、光纤放大器、光纤滤波器、光纤传感器和高速光纤通信系统中色散补偿方面的重要应用，并对线性啁啾Ｂｒａｇｇ光栅色散补偿技术进行了全面分析。     

Generation of a 100-GHz optical pulse train by pulse repetition-rate multiplication using superimposed fiber Bragg gratings

We demonstrate the use of superimposed fiber Bragg gratings (FBGs) operating in reflection as amplitude and phase filtering stages for multiplying the repetition rate of a given optical pulse sequence. In particular, we use a 1-cm-long structure of two superimposed linearly chirped FBGs to generate a continuous optical pulse train with a repetition rate of 100 GHz (duty cycle /spl ap/50%) at a wavelength of 1.55 /spl mu/m from a 10-GHz mode-locked fiber laser.     

Generation of customized ultrahigh repetition rate pulse sequences using superimposed fiber Bragg gratings

We propose and experimentally demonstrate the use of superimposed fiber Bragg gratings (FBGs) as amplitude or phase filtering stages for generating ultrahigh-repetition-rate optical pulse bursts from a single ultrashort pulse. This approach offers the advantages of a compact all-fiber solution and provides high flexibility in tailoring the temporal features of the generated pulse sequence, namely, the repetition rate, as well as the shape and duration of both the individual pulses and the temporal envelope of the burst. To demonstrate the capabilities of the proposed approach, we generate near-flat-topped optical pulse bursts with repetition rates as high as /spl ap/170 GHz at a wavelength of 1.55 /spl mu/m using uniform and linearly chirped superimposed FBGs. We show that superimposed linearly chirped FBGs are more energetically efficient and provide increased design flexibility than superimposed uniform FBGs. Our experimental results also show the robustness of the technique to imperfections in the grating structures and to variations in the input pulse quality.