基于时域模糊决策融合的雷达工作模式识别方法

在雷达工作模式识别中,侦察设备对雷达信号参数的测量误差严重影响了识别效果,针对这一问题文中提出时域模糊决策融合(TFDF)的雷达工作模式识别方法。首先分析了雷达脉冲组特征,在脉冲组层次提取雷达信号的脉冲组描述字(PGDW);然后基于联合隶属度函数改进传统的神经网络硬判决方式,实现雷达信号识别的模糊决策;最后运用DS证据理论将多个时刻的模糊决策融合,从而完成雷达工作模式的最终识别。基于时域模糊决策融合的识别方法可以有效改善参数测量误差对工作模式识别效果的影响。仿真结果以及对比实验表明,文中所提算法具有更好的抗噪性能,在雷达信号的参数测量误差为15%时仍具有90%以上的识别率。     

RLC振荡的脉冲激光器驱动特性

在飞行时间测距(TOF)的脉冲激光雷达(lidar)中,激光器驱动十分重要,其性能直接影响激光雷达系统的作用距离、信噪比和虚警率等指标,是激光雷达的关键组成部分.本文在目前常见的激光器驱动电路模型基础上进行创新,在储能电容的充电电路中引入适当电感,形成电阻电感电容(RLC)二阶微分振荡电路,可以大幅度提高脉冲激光器的驱...     

利用Microsoft Excel嵌套函数自动检索引水月报特征值研究与应用

本文利用统计报表常用的Microsoft Excel软件自身具备的函数功能,反复摸索、组合、试验,组成能够自动查找特征值并在制定单元格内输出其对应出现日期的嵌套函数公式,实现了引水旬、月引水指标各项特征值与发生日期自动过滤并填制到指定单元格内的目的。     

关于东平湖防汛工作若干问题灼思考

东平湖蓄滞洪区是防御黄河下游大洪水的重要分滞洪工程，承担分滞黄河洪水和接纳汶河来水的双重任务。针对东平湖防汛工作存有排水系统不配套，二级湖堤工程标准低，分泄洪闸供电系统不可靠，群众迁安救护难度大，群众队伍建设难落实等问题提出了建议与措施。     

基于互为主体的电子系统架构与任务决策

针对传统电子系统架构和任务决策机制无法满足航空集群遂行复杂任务需求的现状,提出一种基于互为主体的电子系统架构与任务决策机制。首先,从航空集群电子系统的实际应用需求出发,分析了电子系统的物理组成基础和电子资源的柔性聚合;其次,建立基于互为主体的电子系统架构模型,实现电子系统在物理域、信息域和认知域等不同层次能力之间的有机结合;然后,提出基于互为主体的信息交互与决策方法,提高航空集群作战运用的灵活性和整体效能;最后,给出了互为主体在航空集群作战中的应用实例。     

共轭微孔聚合物的制备与应用

共轭微孔聚合物(CMPs)是一类有机多孔聚合物,与常规共轭聚合物或多孔材料相比,其最大的特点是既有π共轭骨架又具有大量微孔.这类材料在解决能源和环境问题方面显示出巨大的潜力,已在气体吸附、非均相催化、发光材料、化学传感器、电能存储和生物杂化物等领域显示出巨大的应用前景.目前已开发出多种用于CMPs结构单元设计与合成的新...     

Bolometric effect in a waveguide-integrated graphene photodetector

Graphene is an alternative material for photodetectors owing to its unique properties.These include its uniform absorption of light from ultraviolet to infrared and its ultrahigh mobility for both electrons and holes.Unfortunately,due to the low absorption of light,the photoresponsivity of graphene-based photodetectors is usually low,only a few milliamps per watt.In this letter,we fabricate a waveguide-integrated graphene photodetector.A photoresponsivity exceeding0.11 A·W ~(-1) is obtained which enables most optoelectronic applications.The dominating mechanism of photoresponse is investigated and is attributed to the photo-induced bolometric effect.Theoretical calculation shows that the bolometric photoresponsivity is 4.6 A·W ~(-1).The absorption coefficient of the device is estimated to be 0.27 dB·μm ~(-1).     

Design and fabrication of multi-channel photodetector array monolithic with arrayed waveguide grating

We have provided optical simulations of the evanescently coupled waveguide photodiodes integrated with a 13-channels AWGs. The photodiode could exhibit high internal efficiency by appropriate choice of layers geometry and refractive index. Aseamless joint structure has been designed and fabricated for integrating the output waveguides of AWGs with the evanescently coupled waveguide photodiode array. The highest simulation quantum efficiency could achieve 92% when the matching layer thickness of the PD is 120 nm and the insertion length is 2 μm. The fabricated PD with 320-nm-thick matching layer and 2-μm-length insertion matching layer present a responsivity of 0.87 A/W.     

参数寻优LSSVM的机载火控雷达工作模式判定中的应用

针对机载火控雷达工作模式判定问题，本文应用一种基于网格搜索和交叉验证的参数寻优最小二乘支持向量机（LSSVM）算法，实现对四种典型空空工作模式的自学习判定。首先，从非合作雷达信号中提取特征参数并构建雷达信号特征库作为训练样本；然后通过网格搜索进行参数寻优模型训练，实现样本范围不确定条件下的模型调整；最后应用K-fold交叉验证方法进行训练性能评价，减小样本随机性导致的模型误差，提高泛化能力。仿真结果表明，该方法对速度搜索模式、边搜索边测距模式、边扫描边跟踪模式和单目标跟踪模式的判定准确率达97%，具有应用价值和理论指导意义。     

Photoconductive multi-layer graphene photodetectors fabricated on etched silicon-on-insulator substrates

Recently, graphene-based photodetectors have been rapidly developed. However, their photoresponsivities are generally low due to the weak optical absorption strength of graphene. In this paper, we fabricate photoconductive multi-layer graphene(MLG) photodetectors on etched silicon-on-insulator substrates. A photoresponsivity exceeding 200 A·W-1is obtained, which enables most optoelectronic application. In addition, according to the analyses of the high photoresponsivity and long photoresponse time, we conclude that the working mechanism of the device is photoconductive effect. The process of photons conversion into conducting electrons is also described in detail. Finally, according to the distinct difference between the photoresponses at 1550 nm and 808 nm, we estimate that the position of the trapping energy is somewhere between 0.4 e V and 0.76 e V, higher than the Fermi energy of MLG. Our work paves a new way for fabricating the graphene photoconductive photodetectors.