Leg-by-leg机动条件下纯方位跟踪的观测站机动策略

针对观测站机动前目标距离未知导致无法计算Fisher信息矩阵(Fisher information matrix, FIM)的问题, 从粗估目标初始距离和减小粗估误差对FIM行列式影响两方面着手, 提出在转向前计算FIM进而设计机动策略的方法。首先, 在修正极坐标系下建立系统模型, 描述了观测站leg-by-leg机动模式下FIM的计算方法。其次, 通过假设目标速度实现目标初始状态粗估, 提出使归一化初始距离粗估误差最小的目标速度假设方法。然后, 对FIM行列式进行近似及多项式展开, 通过控制前后leg段比例以减小状态粗估误差对FIM行列式的影响。最后, 利用仿真验证了所提机动策略设计方法的可行性和有效性。结果表明, 对于典型的水下目标跟踪场景, FIM行列式的有效估计概率为76.7%, 平均的相对估计误差为0.12。     

运用定态法研究电子在原子核势场中的配置与运动关系

研究量子理论中微观粒子系统对库仑电场势能的影响, 将作用于核与电子间的电磁场进行核心化和定态化处理, 并将原子的电磁作用分解, 分别研究壳层电场和磁场对电子的作用.  通过分析各种原子的壳层球半径、 电子轨道偏角和电子的运动速度, 可知电子运动的“轨道”截面小于且偏离原子“赤道”平面, 并按原子的极相进行配置和运动.  计算主族元素中44种原子的基态能级表明, 所得结果与第一电离电势符合较好.     

对称性原理在求解静电场■空间分布中的应用

本文根据对称性原理直接定性分析了具有面、轴和球对称电荷分布激发的静电场(?)空间分布,在此基础上通过选取合适的高斯定理定量给出上述对称分布电荷激发的空间静电场(?)分布.     

Excitation of seasonal polar motion by atmospheric and oceanic angular momentums

A quantitative study on the seasonal polar motion excitated by the atmospheric angular momentum (AAM) and the oceanic angular momentum (0AM) has been carried out using numerical models. The results show that for the prograde and retrograde components of the seasonal polar motion (the annual polar motion and the semiannual polar motion) , the sum of excitations by both the AAM and the 0AM is closer to the observed results rather than that of the AAM only. This reflects a significant contribution of the 0AM to the seasonal polar motion.     

铌锌酸铅基弛豫型铁电体的偏压介电行为研究

测定了铌锌酸铅基弛豫型铁电体ＰＺＮ－ＢＴ－ＰＴ（８３／１０／７）在不同偏压条件下介电行为随温度的变化，通过介电常数导数与温度关系的研究，有效地分离出了弛豫型铁电体极性微区的偏压响应特征，得到了一系列特征温度，并发现介电常数与介电损耗的特征温度之间有着必然的内在联系．     

关于关孝和对《授时历》交食算法的几点研究

和算大师关孝和（？－1708年），在其《天文数学杂著》中，用了约一半的篇幅讨论《授时历》的交食算法，其中不乏颇具新意的创见。文章分析讨论其中关于定交日与交定度改正算法，日月食食限及定法的数源，以及日月食定用分算法的造术原理等问题，并讨论了《授时历》的月亮极黄纬算法问题。     

Probing the properties of individual nanostructures by novel techniques

Nanomaterials are the fundamental components of nanoscience and nanotechnology, and they are different from bulk materials in grain size, surface/interface-to-volume ratio and grain shape, which are the origins of their unique electrical, optical, thermodynamic, mechanical and chemical properties. The small size of nanostructures hampers the applications of well-established testing and measurement techniques, thus new methods and approaches must be developed for their synthesis, property characterization and device fabrication. This has been the focus of our research, aiming at exploring state-of-the-art techniques for materials processing and characterization. This paper reviews our progress in nanomaterials research.     

新型线性函数光子晶体光子二极管的研究

本文运用费马原理和传输矩阵方法研究线性函数光子晶体,通过计算给出了光正入射和反入射时的透射特性及电场分布.研究发现:线性函数光子晶体的透射特性不同于常规光子晶体,并且能够有效的放大或衰减光的电场强度,这为设计光子放大器件和光子二极管提供了重要的理论依据.     

毫米波星载多频段多极化共馈天线系统

天线工作频率为18.7,23.8GHz和37.0GHz,采用环加载波纹喇叭使工作带宽达到2倍,新型结构的超宽带正交模耦合器实现双极化信号的提取,微波多工器完成3个频段信号的有效分离. 18.7GHz信号交叉极化电平和副瓣电平分别为-32.6,-21.0dB,23.8GHz信号交叉极化电平和副瓣电平分别为-31.6,-30.0dB,37.0GHz信号交叉极化电平和副瓣电平分别为-25.0,-30.0dB. 仿真结果表明馈源系统适合星载天线设计,馈源结构更加紧凑,实能现对同一目标的多频率复用观测.      

Synthesis of few layer single crystal graphene grains on platinum by chemical vapour deposition

The present competition of graphene electronics demands an ef fi cient route which produces high quality and large area graphene. Chemical vapour deposition technique, where hydrocarbons dissociate in to active carbon species and form graphene layer on the desired metal catalyst via nucleation is considered as the most suitable method. In this study, single layer graphene with the presence of few layer single crystal graphene grains were grown on Pt foil via chemical vapour deposition. The higher growth temperature changes the surface morphology of the Pt foil so a delicate process of hydrogen bubbling was used to peel off graphene from Pt foil samples with the mechanical support of photoresist and further transferred to Si O2/Si substrates for analysis. Optical microscopy of the graphene transferred samples showed the regions of single layer along with different oriented graphene domains. Two type of interlayer stacking sequences, Bernal and twisted, were observed in the graphene grains.The presence of different stacking sequences in the graphene layers in fl uence the electronic and optical properties; in Bernal stacking the band gap can be tunable and in twisted stacking the overall sheet resistance can be reduced. Grain boundaries of Pt provides low energy sites to the carbon species, therefore the nucleation of grains are more at the boundaries. The stacking order and the number of layers in grains were seen more clearly with scanning electron microscopy. Raman spectroscopy showed high quality graphene samples due to very small D peak. 2D Raman peak for single layer graphene showed full width half maximum(FWHM) value of 30 cm-1. At points A, B and C, Bernal stacked grain showed FWHM values of 51.22, 58.45 and 64.72 cm-1, while twisted stacked grain showed the FWHM values of 27.26, 28.83 and 20.99 cm-1,respectively. FWHM values of 2D peak of Bernal stacked grain showed an increase of 20–30 cm-1 as compare to single layer graphene which showed its dispersive nature and con fi rmed Bernal sequence. On the other hand, the slightest decrease in FWHM values of 2D peak in twisted grain comparing to single layer con fi rmed the twisted sequence of grains. Atomic force microscopy analysis showed an increasing trend in grain height pro fi le with an increase in the number of layers.