基于掺铒光纤/喇曼混合放大的光纤激光器布喇格光栅传感系统

提出了一种提高长距离光纤布喇格光栅信噪比以进行准分布测量的新方法.该方法基于掺铒光纤/喇曼混合放大的光纤激光器结构,掺铒光纤和滤波器构成的环形结构产生激光作为光源,喇曼光纤放大器对布喇格光栅信号进行低噪音的双向放大,置于远处的掺铒光纤利用剩余的泵浦功率产生自发辐射光和放大传感信号,为远处掺铒光纤之后的布喇格光栅传感器提供信号光以及补偿由于长距离传输造成的光纤损耗.实验显示,与使用宽带光源的传感方式相比,系统的性能得到显著提高,仅使用小功率泵浦,分布在50 km光纤上的FBG均获得了超过58 dB的优良信噪比.     

基于喇曼/掺铒光纤混合放大的长距离布喇格光栅传感器系统

提出了一种提高长距离光纤布喇格光栅信噪比以进行准分布测量的新方法.本方法基于双向喇曼放大和双掺铒光纤结构,喇曼光纤放大器对布喇格光栅信号进行低噪音的双向放大,置于远处的掺铒光纤利用剩余的泵浦功率产生自发辐射光和放大传感信号,为第二段掺铒光纤之后的远处布喇格光栅传感器提供光以及补偿由于长距离传输造成的光纤损耗.实验显示传感器系统的性能得到显著提高.使用功率为240 mW的单个普通泵浦,分布在50 km光纤上的FBG均可获得15 dB的良好信噪比,比混合放大前提高了10 dB.     

WDM用增益平坦的高增益低噪声双段级联掺铒光纤放大器

给出了设计波分复用(WDM)用高增益、低噪声和宽带宽增益平坦的双段级联掺铒光纤放大器(EDFA)的一般步骤和方法.通过优化设计各种参量,研制出了一台高增益、低噪声和宽带宽增益平坦的双段级联EDFA样机,实现了从1524.8～1561.4 nm共36.6 nm带宽内±0.325 dB的平坦增益,0 dBm输入时,饱和输出功率大于15 dBm的高功率输出;噪声指数低于5 dB.     

掺铒光纤放大器的增益特性

采用980nm无铝InGaAs/InGAsP/InGaP高功率量子阱激光器泵浦掺铒光纤放大器。在泵浦功率为20mW时,增益为33dB,最大增益系数6．7dB/mW,饱和输出功率为6dBm,并给出掺铒光纤长度和泵浦功率与增益特性的关系。以及输出功率与增益特性的关系。     

利用光敏光纤制作少模光纤布喇格光栅

利用相位掩模技术在光敏光纤中制作出了少模光纤布喇格光栅,1.06μm波长附近有2~3个特征峰,峰值约4~5 dB.对这种光纤光栅的特性进行了分析,结果表明理论与实验结果符合得较好,并对光纤光栅的温度特性进行了实验研究和理论分析,实验结果测得光纤光栅的温度敏感度为9~10 pm/℃.     

双波长全光自动增益箝制掺铒光纤放大器的实验研究

提出了结构简单的光纤布喇格光栅（FBG）双波长全光自动增益箝制方案,并进行了相关实验.结果表明,在三种不同的箝制波长组合1535.64nm+1562.68nm、1530.48nm+1562.68nm、1530.48 nm+1551.36 nm条件下,1540 nm信号的输出增益大小和输入信号功率动态范围几乎一致.对应此三种箝制波长组合,环路内的损耗分别为：14.7 dB、15 dB、15 dB.由此证明,在相同泵浦条件和环路损耗条件下,此三种不同箝制波长组合具有近似相同的箝制效果.而1551.36 nm+1562.68 nm箝制波长组合得到的结果相差甚远.此结果说明,在设计双波长全光自动增益箝制掺铒光纤放大器（OAGC-EDFA）时,为了取得足够大的信号增益,两箝制波长的波长间隔应尽量较大.     

光纤布喇格光栅的制作和应用

本文简要介绍光纤布喇格光栅（ＦＢＧ）的原理及性能，并给出ＦＢＧ的制作方法。     

掺铒光纤放大器的频率响应和瞬态增益

根据掺铒光纤放大器（ＥＤＦＡ）的速率方程和传播方程,忽略自发辐射噪声,推导出了小信号调制时频率响应函数的解析表达工以及大信号调制时描述瞬态增益的方程。数值计算表明,当输入信号的调制频率大于５ｋＨｚ时,放大器的瞬态增益变化很小,频率响应很弱。通过计算机仿真,描述了关闭一个信道时的放大器的增益变化过程。     

基于高双折射光纤布拉格光栅的自动增益控制掺铒光纤放大器

掺铒光纤非均匀展宽引起的空间烧孔现象导致单波长激光并不能完全控制放大器增益,提出了一种新颖的自动增益控制掺铒光纤放大器的结构:即采用高双折射光纤布拉格光栅产生抽运光,其写制光栅的波峰对应的波长分别为1549.3 nm和1549.83 nm,波长间隔为0.53 nm。通过调整偏振控制器,就实现了单激光或双激光的增益控制。这种设计增益控制范围为40 nm(1530~1570 nm),当输入功率在-40~-15 dBm的动态范围内,双激光增益控制的掺铒光纤放大器的平均增益和噪声系数分别约为22.22 dB和8.69 dB,而它们的漂移分别被钳制在0.69 dB和1.51 dB。系统性能测试表明:双激光控制掺饵光纤放大器在稳定性方面比单激光有着明显的优势。     

基于新型长周期光纤光栅的掺铒光纤放大器

报道了基于高频CO₂激光脉冲写入的新型长周期光纤光栅的低噪音掺铒光纤放大器,这种新型长周期光纤光栅是用大约几千Hz的高频CO₂激光脉冲对光纤玻璃热冲击作用而形成的.在铒纤中插入一个长周期光纤光栅,会明显减少掺铒光纤放大器的放大自发辐射(ASE)噪音.报道了两种低噪音掺铒光纤放大器,作为前置放大器和线路放大器,它们的ASE噪音指数分别从4.0 dB减少到3.5 dB和从4.8 dB减少到4.3 dB,并且在作为线放时,其小信号增益从30 dB提高到37 dB,降噪及提高增益效应十分显著.     

DESIGN CONSIDERATION OF ERBIUM DOPED FIBER FOR EFFICIENT L-BAND EDFAs

0　Introduction　　Recently,therapidgrowthofInternetanddatacommunicationsserviceshasdriventhedemandforbandwidthinthelong-distancenetworkstodoubleatleasteverytwoyears.Inordertoexploitthelargebandwidthofopticalfiber,technologiessuchaserbium-dopedfiberamplifiers(EDFAs)anddensewavelengthdivisionmultiplexing(DWDM)arewidelyused.Theconventionalwavelengthband(C-band)ofEDFAsextendsfromabout1530to1562nm.Ithasbeenusedforup-to96channelsinDWDMsystem.Itshouldbenotedthatopticalfibernonlineareffectsbe…     

变迹啁啾Bragg光纤光栅的矩阵分析

本文用传输矩阵法分析了各种变迹与线性啁啾Bragg光纤光栅的响应特性,构造了各种变迹函数,进行了比较.分析了变迹函数、啁啾系数、折射率变化量以及光栅长度对反射带宽、最大反射率的影响.找到了最佳变迹函数和量佳啁啾系数.特例中的数值分析表明,补偿100km光纤色散带宽为1nm的最佳光栅长度是140mm,最佳啁啾系数为0.048nm/cm.     

光纤Bragg光栅的饱和效应

光纤 Bragg光栅的饱和效应可引起二阶衍射,并使一阶衍射的峰值反射率下降.本文利用折射率变化模型和耦合模理论,模拟了饱和情况下 Bragg光栅的一阶和二阶衍射谱,并讨论了饱和系数对一阶和二阶衍射的 Bragg波长和峰值反射率的影响.数值模拟结果与参考文献中的实验结果相吻合.     

掺铒光纤放大器的理论模拟与全局分析

基于Giles模型并考虑了ASE噪音,对各种泵浦方式下的掺铒光纤放大器(EDFA)进行了数值模拟.提出了一种新的分析方法(增益噪音指数全局分析法),直观有效地分析了EDFA的增益和噪音指数与掺铒光纤长度和泵浦功率的依赖关系,并对各种EDFA的性能作了全面的比较.     

AN采用FBG温度机械合成调谐技术的光滤波器

报道了一种采用特别设计的调节结构,并与温度机械相结合的方法来调谐FBG的中心波长的新颖光滤波器,它在温度变化60°范围内波长可线性调节9nm以上,线性度达0.9999.     

The L-band EDFA of high clamped gain and low noise figure implemented using fiber Bragg grating and double-pass method

The L-band erbium-doped fiber amplifier (EDFA) of low noise figure and high clamped-gain using gain-clamped and double-pass configuration is presented in this paper. A total of five different configurations of EDFAs by reflection scheme with single forward pumping schemes are examined and compared here. Among these configurations, we first find the configuration of 1480-nm pumped L-band EDFA with optimum gain and noise figure value. To further minimize the gain variation, a fiber Bragg grating (FBG) with 1615-nm center wavelength and 1-nm bandwidth is determined and added in double-pass L-band EDFA. The gain variation and maximum noise figure of EDFA while channel dropping is investigated. As the number of channel dropping from 32 to 4, the L-band type-A EDFA keep the variation of gain within 2.9 dB and the maximum noise figure below 5 dB with each channel’s input power of −23 dBm.     

Gain clamped L-band EDFA with forward–backward pumping scheme using fiber Bragg grating

The paper proposes a novel two stage L-band erbium doped fiber amplifier with forward–backward pumping scheme for transmission of 32 wavelength division multiplexed (WDM) channels. It is gain clamped with an in-line fiber Bragg grating (FBG) to provide flat gain over 45 nm by restricting and reutilizing amplified spontaneous emission (ASE). We demonstrate that it provides an efficient small signal gain with minimum noise figure of over 20 dB and 5.5 dB, respectively, in the L-band region (1565–1610 nm) by comparing with its forward and backward pumped counterparts with fixed Er³⁺ fiber length of 20 m for −30 dBm/channel input power. We also obtain the gain and noise figure dependence as a function of each of the Er³⁺ fiber lengths, pump power (both 1480 and 980 nm), and temperature. Hence a 10 nm region (1580–1590 nm) has been acknowledged where temperature variations become constricted for 30 °C variations (15–45 °C).     

低噪声、高增益的L -band EDFA的实验研究

针对传统的L-band EDFA的工作效率低,提出了一种基于单根光纤光栅、泵浦分配、两段级联的EDFA的新结构,其中的光纤光栅用来反射无用的后向C-band ASE.系统地研究了泵浦比例和光纤光栅波长对增益噪声指数的影响关系.最后经实验验证,得到了低噪声、高增益的L-band的EDFA.其在输入信号光（1570 nm）功率为-30 dBm及泵浦功率为70 mW时,增益为22.26 dB,增益噪声指数为4.96 dB.     

Gain-clamped two-stage L-band EDFA with a FBG laser in second stage

A gain-clamped two-stage L-band EDFA is demonstrated by simply incorporating two different FBGs on both side of EDF in the second stage. It forms a FBG laser at 1560 nm to clamp the gain in the system. The gain is clamped at about 16.5 dB with gain variation of less than 1.0 dB at dynamic range up to −10 dBm. A flat gain is obtained over 30 nm of wavelength range from 1568 to 1598 nm with a gain variation of less than 1.1 dB. At the flat region, the noise figure varies from 5.0 to 5.8 dB, which is slightly higher compared to those of unclamped amplifier. The advantage of this technique is that the FBG laser does not disturb the WDM signals in the flat gain region.     

An optimized strain demodulation method based on dynamic double matched fiber Bragg grating filtering

An optimized strain demodulation method based on dynamic double matched fiber Bragg grating (FBG) filtering driven by a piezoelectric transducer (PZT) is proposed and experimentally demonstrated. Using an optimized triangular waveform to drive PZT, the nonlinear effect is eliminated, and extraction and processing of the peak signals are more convenient. Furthermore, taking advantage of double matched-FBGs and strain amplification structure to demodulate the Bragg wavelength, the wavelength scanning range can be extended to 6.3 nm, so that a large-scale and high-precision strain measurement can be achieved. The experimental results show that in the strain range of 0-3800με, the linearity of the relationship between strain and scanning time-difference is greater than 99.8%, and the stability of repeated measurements is up to 99.5%. This demodulation method can be widely applied in the FBG measurement system.