Fe-C合金膜光纤腐蚀传感器传感规律研究

利用PVD溅射镀以及PVD与电镀复合两种方法在光纤纤芯上制备了不同厚度的Fe-C合金膜,对其进行X-射线衍射分析,所制膜层晶体结构类型与普通碳钢基本一致.通过将镀膜光纤放入不同浓度的HNO3溶液中以及埋入混凝土结构中,进行了腐蚀实验.结果表明:在低浓度的腐蚀溶液中,不同厚度的Fe-C合金膜会从外到内被均匀地腐蚀掉,输出光功率会在腐蚀末期有一个急剧的增大现象;在高浓度的腐蚀溶液中,Fe-C合金膜会在各个局部产生裂纹,膜层被一块一块地腐蚀掉;输出光功率整体趋势增大,但并没有特别急剧的增大现象;混凝土试块中的腐蚀实验中,输出光功率的变化复杂多变,但整体趋势还是一个增大的过程.     

级联双包层铒镱共掺光纤放大器的性能分析

基于速率方程和光传输方程,对级联双包层铒镱共掺光纤放大器(Er3+/Yb3+ co-Doped Fiber Amplifier,EYDFA)进行了研究.数值模拟计算得到级联双包层EYDFA的最佳光纤长度,以及前后向泵浦功率之比和光隔离器位置对于增益以及噪音系数的影响.通过选择合适的前后向泵浦功率之比和隔离器的位置优化级联放大器结构,其增益提高了4 dB,噪音系数降低了近3 dB.     

一种高速多通道光纤阵列光开关

为了对短时间大视场一维光强信息进行采集,采用编码转换技术和自聚焦透镜矩形阵列设计了光开关,用小口径电光晶体实现了大视场的测量.采用MOS管级联的高压同步电路,使得系统具有结构紧凑、性价比高、寿命长等优点.实验结果表明:开关选通时间100±5 ns,前后沿小于25 ns,消光比1 100∶1.     

高功率光子晶体光纤放大器内超短脉冲的放大传输特性

由速率方程和功率传输方程得到信号脉冲平均功率和增益系数随脉冲传输距离的变化关系.利用Ginzburg-landau方程,在信号脉冲功率的不断增强和增益系数的不断变化的情况下,研究超短脉冲的传输演化特性,发现信号脉冲平均功率、能量和增益系数等参量受到色散和非线性效应的影响相对较小,而信号脉冲的峰值功率、时域和频域特性则易受到色散和非线性效应的影响.探讨了在非线性作用下,脉冲分裂和展宽等所导致的脉宽不稳定性对传输特性的影响,表明研究脉冲传输问题时,引入脉宽不稳定性有利于提高数值模拟准确度.     

梯度型聚合物通信光纤制备的理论分析

对直接挤出法制备梯度型聚合物光纤的工艺流程进行了分析,根据双组分混合物折射率计算理论和梯度型聚合物光纤径向折射率分布函数,计算了梯度型聚合物光纤单位长度中所含掺杂剂的质量;将非稳态扩散理论和有限差分法结合起来,对梯度型聚合物光纤折射率分布的形成进行了理论研究,建立了数学物理模型,得到描述梯度型聚合物光纤径向折射率形成的普遍性近似方法.     

高双折射光纤环镜应变传感研究

研究了高双折射光纤环镜的应变传感原理,推导了谐振波长与轴向应变的关系式,并进行了实验研究.该传感器具有很高的灵敏度：谐振波长漂移为0.031 8 nm/με,约是裸光纤光栅的32倍.谐振波长和轴向应变之间的线性拟合度为0.999 4.该传感器具有灵敏度高、结构紧凑、使用方便等优点.     

Formation of domain reversal by direct irradiation with femtosecond laser in lithium niobate

We propose that domain inversion can be directly induced by femtosecond laser both theoretically and experimentally, which opens a path to achieve three-dimensional （3D） nonlinear crystal with a period in sub-micron-scale. A simulation of domain inversion is modeled by considering the temporal distribution of femtosecond pulses. The calculation results clarify that the domain inversions can happen within or after the interaction with the laser pulse, and the response time of domain inversion is in the picosecond level depending on the intensity and the materials. The domain reversal windows of lithium niobate by femtosecond laser are observed which agrees with theoretical predictions qualitatively.     

Localization theory of distributed fiber vibration sensor

Based on Sagnac interferometer, a simple distributed optical fiber sensing system with sub-loop is presented to monitor the vibration applied on the sensing fiber. By introducing a sub-loop, three output beams of interference with different delay time are gotten. Location of the vibration is analyzed through mathematical-physical equations. The vibration frequency, amplitude, and location are theoretically simulated. The results agree well with the previous experiments.     

Robustness estimation of software-synchronized all-optical sampling for fiber communication systems

The robustness of the software-synchronized all-optical sampling for optical performance monitoring is estimated for 10-Gb/s fiber communication systems. It reveals that the software-synchronized algorithm is sensitive to the signal degradation caused by chromatic dispersion and nonlinearity in optical fibers. The influence of timing jitter and amplitude fluctuation of the sampling pulses is also investigated. It is found that stringent requirements are imposed on the quality of the sampling pulse and the tolerance of 1-dB Q penalty is measured. Considering the practically available optical sampling pulse sources, the results indicate that the amplitude fluctuation of the sampling pulses has the dominant impacts on the software-synchronized method.     

Amplification effect on SBS and Rayleigh scattering in the backward pumped distributed fiber Raman amplifier

The amplification effect on stimulated Brillouin scattering （SBS） and Rayleigh scattering in the backward pumped G652 fiber Raman amplifier （FRA） is studied. The pump source is a 1427.2-nm fiber Raman laser whose power is tunable between 0 - 1200 mW, and the signal source is a tunable narrow spectral bandwidth （〈 10 MHz） external cavity laser （ECL）. The Rayleigh scattering lines are amplified by the FRA and Stokes SBS lines are amplified by the FRA and the fiber Brillouin amplifier. The total gain of SBS lines is the production of the gain of Raman amplifier and that of Brillouin amplifier. In experiment, the SBS gain is about 42 dB and the saturation gain of 25-km G652 backward FRA is about 25 dB, so the gain of fiber Brillouin amplifier is about 17 dB.