埋入光纤挠性基板的光电耦合模块设计

为了提高埋入光纤挠性基板光电互联系统中激光束与光纤之间的耦合效率,设计了一种可分离式的高效光电耦合模块。对耦合模块的结构尺寸进行了设计,并运用Matlab软件分析了激光束经过45°全反射镜时的能流变化情况;针对芯径为62.5μm、数值孔径为0.25的多模光纤,利用Zemax软件仿真模拟光纤耦合系统,并用正交下降法优化耦合系统结构,将单路波长为1 310 nm、输出功率为1 W的垂直腔面激光束耦合进光纤。分析结果表明,耦合效率与轴向偏差、角向偏差成中心对称分布,当制造误差最大时,耦合效率达到79.37%,耦合损耗为1. 00 d B。该光电耦合模块具有较高的定位误差,最高耦合效率可达85.35%,最低耦合损耗为0.69 d B。     

复合抛物面型集光器与多模光纤的耦合

分析讨论了复合抛物面型集光器与多模光纤的耦合效率和集光器设计之间的关系，提出了采用截底法和截顶法提高集光器与多模光纤耦合效率的方案。     

高功率激光光纤耦合系统设计与分析

端面抽运耦合是高功率光纤激光器的常用耦合方式之一.在不考虑像差的情况下,采用高斯光束传输的ABCD定律,参照混合模系数M2的定义,研究了类高斯光束通过双透镜后腰斑和发散角的变化规律,设计了一种将LD尾纤输出的大功率多模激光耦合进双包层光纤的透镜耦合系统,针对透镜组通光孔径、透镜加工要求、系统尺寸等影响耦合系统效率的各种因素作了简要分析.该系统已成功运用于光纤激光器实验,验证了设计方案的可行性.     

大气湍流像差对单模光纤耦合效率的影响分析及实验研究

空间激光到单模光纤(SMF)耦合技术是自由空间激光通信中的关键技术之一。在Matlab环境下仿真分析了单项波前像差和大气湍流像差对空间光到SMF耦合效率的影响,研究了随机并行梯度下降(SPGD)算法校正大气湍流中整体倾斜像差的迭代过程及对耦合效率的影响。仿真结果表明,SMF耦合效率随单项波前像差均方根(RMS)增加而降低,校正大气湍流中整体倾斜像差后,SMF耦合效率都有提高;当D/r0较小时,大气湍流像差中影响SMF耦合效率的主要像差为倾斜像差。搭建了基于SPGD算法的闭环控制系统,利用自适应光纤耦合器(AFC)校正模拟湍流倾斜像差后,SMF平均耦合效率从30.07%提升到了61.72%;耦合效率的均方误差(MSE)从7.28%降低到2.16%。     

外场紫外与可见光双波段可调焦装置校准设计

设计了一种用来校准紫外与可见光光轴平行性的可调焦光学系统,调焦范围为70 m~。针对目前大多数校准系统无法进行调焦的问题,提出一种既能校准紫外与可见光光轴平行性又能对紫外部分进行调焦的方法。采用离轴卡塞格林系统作为初始结构进行设计,通过在传统的卡塞格林系统中加入调焦组和补偿组来实现调焦以及像差补偿,所设计的系统可以有效地解决紫外与可见光双光轴平行性失调的校准问题,提高紫外与可见光双光轴平行性校准效率,并且在不同视距下光学传递函数值及点列斑均接近衍射极限,能量集中度达到90%,整个视场的像质均匀,像面清晰,有利于后续的图像处理工作。     

多模光纤中简并模式群的分别探测

用多模倾斜光纤光栅(Tilted fiber Bragg grating,TFBG)实现多模光纤中简并模式群(Degenerated modegroup,DMG)的分别探测。多模倾斜光纤光栅将光纤中的导模耦合到辐射光线,用透镜将辐射光线聚焦在焦平面上,使非简并模式群对应的辐射光线的像在焦平面上分离。在焦平面上用空间滤波器使简并模式群选择透过并进行分别探测。用芯径为62.5μm的标准通信多模光纤进行了简并模式群分别探测实验,用单模光纤激励多模光纤,测量简并模式群功率随激励光纤的横向对准偏差的变化关系。低阶简并模式群的测量结果与仿真计算结果基本一致,高阶简并模式群的测量结果与仿真结果有一些不同。用倾斜光纤光栅进行单简并模式群激励,在单简并模式群条件下测量简并模式群耦合效率的想法还需进一步实验验证。     

多模光纤中基于模斑整形和反馈均衡的传输性能研究

总结了多模光纤用于数据通信的优劣点,并分析多模光纤在未来高速大容量长距离无源光接入网(PON)中应用的可行性。从弱导光纤波导理论出发,忽略模内色散以及非线性效应的影响,建立多模光纤的简化模型,并在该简化多模光纤模型的基础上,采用仿真实验的方式,对一些改善多模光纤传输性能的技术:偏心注入,改变模斑尺寸,环形注入以及判决反馈均衡进行了分析,研究和比较。实验结果证明,采用模斑整形(主要是环形注入)与反馈均衡结合的方式可以有效地改善多模光纤的传输性能,使得10Gb/s信号在多模光纤中传输超过1km。     

有方向性锥形光纤连接器及其耦合特征

光纤续接时,横向偏移对耦合效率的影响非常显著,为了降低光纤续接对横向偏移的敏感性,提出了新型有方向性锥形通信光纤连接器。采用了沿信号传输方向的锥形结构,从而提高其可靠性。根据波动理论,对新连接器的纵向传播常数进行泰勒级数展开,得到了锥形光纤功率分布的近似解。分析了锥体长度、锥度以及和光纤折射率等参数对耦合效率的影响。还试制了6个锥形连接器样品,进行了耦合效率实验测量,实验测量结果和理论分析是一致的,从而验证了理论分析的正确性。     

大容差光纤耦合技术研究

设计了一种新型的耦合系统,该耦合系统由大口径聚焦透镜、1/4节距自聚焦透镜、锥形光纤和球端光纤四部分组成.分析了自聚焦透镜压缩发散角和球端光纤增大数值孔径的机理,给出了计算锥形光纤参量的详细流程.采用大口径透镜和1/4节距自聚焦透镜有效增大径向位置容差和角度容差,然后通过锥形光纤压缩光束半径将激光耦合进球端光纤.仿真实验结果表明,该系统耦合在r<3 mm,－1<θ<1.5范围内的耦合效率稳定保持在50%以上.     

楔形光纤与半导体多量子阱平面光波光路芯片的耦合分析

采用楔形光纤(WSF)实现了与半导体多量子阱(MQW)平面光波光路(PLC)芯片的高效耦合。在多量子阱-平面光波光路前置模斑转换器(SSC)和不加模斑转换器的情况下,用阶梯串联法(SCM)数值模拟并优化设计了楔形光纤-平面光波光路间最佳耦合参量:楔形光纤楔角45°、端面圆柱透镜曲率半径2.5μm、模斑转换器-多量子阱-平面光波光路出射椭圆光斑长半轴3.5μm、纵横比5、楔形光纤-平面光波光路间垂直方向和水平方向无偏移、纵向间距5.5μm。用反向推演法(IDM)实验分析了楔形光纤样品的出射光场,与阶梯串联法(SCM)计算结果相比长轴误差为3.125%,短轴误差为0.8%。建立楔形光纤-平面光波光路-单模光纤(SMF)的耦合实验系统,在1.55μm波长处以单模光纤作为出纤的相同条件下,发现楔形光纤激励入射平面光波光路比单模光纤和锥形透镜光纤(TLF)作为入纤的耦合效率分别提高了24.827 dB和16.22 dB,为多量子阱-平面光波光路芯片尾纤封装技术提供了实验原型。     

The impact of the off-axis for the spatial light to multimode fiber coupling system

The electric field distribution of Gaussian beam and properties of Cassegrain optical antenna are discussed and their images have been simulated. By analysis of Cassegrain optical antenna with collimation and off-axis circumstance, laser power distribution and the curve of coupling efficiency are obtained. The question of spatial light to multimode fiber coupling efficiency with alignment and off-axis are researched. At last, taking into account off-axis situation of Cassegrain and laser beam to multimode fiber, the coupling efficiency of the whole system is discussed. These researches are necessary and useful for increasing spatial light to multimode fiber coupling efficiency.     

大功率激光二极管与多模光纤耦合效率分析

提出了一种用于大功率激光二极管与多模光纤耦合的新颖的铲形整形系统，详细分析了铲形光纤端头不同的切割角度、切割深度以及耦合距离对激光二极管与铲形光纤耦合效率的影响。提出了一种计算该系统耦合效率的方法，同时给出了耦合效率的计算实例，得出了可以最大程度地提高铲形耦合头作用的优化参量。     

Simulation and experimental research on polymer fiber mode selection polished coupler

Multimode dispersion is the main obstacle for high bandwidth in multimode optical fiber （MMF） communication system. Mode selection is an effective method to oppress multimode dispersion. We propose and investigate a kind of polymer optical fiber polished coupler. Beam propagation method （BPM） is employed to calculate the coupling coefficient of transmission modes in MMF coupler, and an output pattern from coupling branch is obtained. Analysis and experiment show that this coupler can select certain modes by changing polished depth, contact area, and intersection angle of two branches, which means that the device can be employed both as a mode selector and a sensor. In addition, simulation shows that five times bandwidth enhancement may be realized by selecting modes with the polymer fiber polished coupler.     

卡塞格伦光学天线偏轴及性能分析

设计了具有抛物面结构的卡塞格伦光学天线.通过对偏轴下的卡塞格伦光学天线系统的分析,得到了不同偏转角所对应的接收光斑面积表达式和功率衰减曲线.讨论了偏轴下的接收天线增益与波长及偏转角的关系,仿真出在偏轴与轴对准两种情形下的增益曲线.仿真结果表明,〖JP2〗最大偏轴比轴对准情形增益降低了6.564dB.最后分别针对轴对准与某种偏轴情形下的系统做了光斑测试实验与天线耦合效率测试实验.结果为：偏轴下天线耦合效率降低了26.966%.这些研究为星间光通信中控制系统实现光轴的精确对准提供了理论依据,具有重要的实用价值 关键词： 偏轴 卡塞格伦光学天线 偏转角 增益     

圆锥透镜对倾斜球面波光束的衍射模式

由于球面波入射圆锥透镜所产生的出射光束具有焦深长和中心光斑直径较小的特点,适合激光通信以及长距离测量.在实际使用中,入射球面波很可能与圆锥透镜的光轴发生倾斜.研究了圆锥透镜对倾斜球面波光束的衍射特性,通过基尔霍夫衍射理论以及稳相法分析,分析了其径向衍射光场分布形式,并用计算机进行了仿真.使用了半径为15 mm、底角为1°的圆锥透镜进行实验,并对仿真结果进行了验证.仿真和实验证明,减小入射球面波曲率半径、出射光束传输距离和入射光束倾斜角都可以减弱入射光束倾斜对衍射图的影响.     

Highly efficient fiber-to-chip evanescent coupling based on subwavelength-diameter optical fibers

A novel, compact, and highly efficient fiber-to-chip evanescent coupling structure is proposed based on a subwavelength-diameter fiber. The coupling structure is characterized by a large misalignment tolerance and easy fabrication. The dependence of coupling efficiency on various parameters is calculated and analyzed. The simulation results show that a coupling efficiency as high as 95% can be obtained within a coupling length of <4 μm.     

A novel spectroscopic filter used in rotational Raman lidar for the temperature profiling

We perform the rotational Raman temperature measurements in the troposphere and lower stratosphere with high performance. Depending on the aerosol content and presence of clouds in the lower troposphere, the rotational Raman lidar (RRL) is the lidar technique of choice for temperature measurements. However, the Raman filter design is a technical difficulty in RRL systems. Considering the higher spectral resolution and compactness, we select several photonic crystals to construct a novel spectroscopic filter for extracting the required rotational Raman spectrum (RRS) signals of atmospheric molecules. We describe in detail the principle to design the photonic-crystal filter. To verify the feasibility of the novel spectroscopic filter, we carry out some numerical calculations, and our results show that the novel spectroscopic filter has the capability to fine draw the required RRS signal and suppress sufficiently elastic signals. For the RRL system which uses the novel spectroscopic filter, we obtain that a statistical temperature error is less than 1 K up to a height of 3.2 and 5.6 km for daytime and nighttime measurements, respectively. Our simulation conditions are as follows: 532 nm laser with 500 mJ energy, and 10 Hz pulse repeating rate, a 300 mm diameter Cassegrain reflecting telescope with 1000 mm focus length, 0.2 mm diameter multimode optical fiber which sets the field of view (FOV) of receiving system to 0.2 mrad, 45 m range resolution, 9 min observation time, overall optical-system efficiency of 0.6, and a special atmospheric model which integrates the US standard model of 1976 with an actual Mie scattering profile obtained from practical observations.     

Multi-coupler side-pumped Yb-doped double-clad fiber laser

The side-coupler of angle polished method, using angle-polished multimode fiber and optical adhesive, is used to efficiently pump an Yb-doped double-clad fiber laser. The maximum coupling efficiency of 78.6% is achieved by the side-coupler for a multimode fiber with a circular core of 200 μm and a double-clad fiber with a 350/400 μm D-shaped inner cladding. While laser diodes (LDs) with three side-couplers are simultaneously used as pump sources, maximum output power of 1.38 W and slope efficiency of 48.9% are demonstrated in the fiber laser system.