基于Apollo信号控制台的NQR炸药探测方法

介绍了一种基于Apollo信号控制台的核四极矩共振（NQR）炸药探测方法，描述了系统的结构组成、工作原理和实现方法，并给出了对RDX的测试试验结果. 试验表明该方法可实现对RDX信号的探测.     

多段构件组成的压杆平面内稳定

分析由若干段等截面或者变截面构件组成的压杆平面内稳定问题．从由三段等截面构件组成的压杆平面内稳定问题出发，对两端为变截面、中间为等截面构件组成的压杆的平面内稳定问题进行了分析，得出和两端为等截面构件情况类似的屈曲荷载计算公式．并对两端固接的情况进行了研究分析．     

Ontology-Based Semantic Annotation for Problem Set Archives in the Web

0 IntroductionAsneim mapnotircta nWte pbre i-sco tnhdieti oabnilfiotry r etaoli zainnngotthatee go aWle obf trhe-esources with semanticinformation[1]. However ,annotationtools so far basically allowthe user to annotate with plaintext using the method of information extraction.In manycases ,one can hardly extract semantics from Web docu-ments ,such as problemset archivesinthe Web.Massive problemset archives are availableinthe Web,for example,http://acm.uva.es, while each problemsetarchives pr…     

Delphi语言的菜单动态生成技术

介绍了用Delphi语言动态生成菜单的技术，这种技术编制的程序能依据控制文件中的一些数据，系统自动产生相应的菜单，并连接控制程序．     

压电结构作动/传感器配置优化

提出了一种压电结构中作动／传感器优化配置的新方法．首先用有限元方法建立结构的动力学方程，并用模态方法进行降阶，然后通过Lyapunov方程分别求解扰动输入和作动器输入的能控性Grammian矩阵，通过使作动器输入的能控性矩阵向量在扰动能控性矩阵上投影长度的平方和最大值得到压电作动器的最优位置，同样的思想用于确定传感器的最优位置。     

含内聚空洞的固体发动机药柱结构完整性分析

为评估固体发动机药柱含内聚空洞时的结构完整性，通过在药柱后部不同应变梯度的部位设置不同直径的内聚空洞，基于三维黏弹性有限元分析方法，计算了在燃气内压和轴向过载作用下发动机的应变场。由不同直径内聚空洞的最大Von Mises应变值随着直径变化的规律及最大Von Mises应变准则判断出内聚空洞位于药柱不同位置时允许的最大直径。     

Theoretical Studies on Dihedral Angle-Bending Isomers of M2Pt20/-Clusters

The structures and electronic properties of the gaseous M\begin{document}$ _2 $\end{document}Pt\begin{document}$ _2 $\end{document}\begin{document}$ ^{0/-} $\end{document} clusters (M represents the alkaline earth metal) were investigated using the density functional theory (B3LYP and PBE0) and wave function theory (SCS-MP2, CCSD and CCSD (T)). The results indicate that the D\begin{document}$ _{2{h}} $\end{document} isomers with the planar structures are more stable than the C\begin{document}$ _{2v} $\end{document} isomers with smaller dihedral angles and shorter Pt-Pt bond lengths. The mutual competition of M(s, p)-Pt(5d) interaction and Pt-Pt covalent bonding contributes to the different stabilizations of the two kinds of isomers. The M(s, p)-Pt(5d) interaction favors the planar isomers with D\begin{document}$ _{2h} $\end{document} symmetry, while the Pt-Pt covalent bonding leads to the C\begin{document}$ _{2v} $\end{document} isomers with bending structures. Two different crossing points are determined in the potential energy curves of Be\begin{document}$ _2 $\end{document}Pt\begin{document}$ _2 $\end{document} with the singlet and triplet states. But there is just one crossing point in potential energy curves of Ra\begin{document}$ _2 $\end{document}Pt\begin{document}$ _2 $\end{document} and Ca\begin{document}$ _2 $\end{document}Pt\begin{document}$ _2 $\end{document}\begin{document}$ ^- $\end{document} because of flatter potential energy curves of Ra\begin{document}$ _2 $\end{document}Pt\begin{document}$ _2 $\end{document} with the triplet state or Ca\begin{document}$ _2 $\end{document}Pt\begin{document}$ _2 $\end{document}\begin{document}$ ^- $\end{document} with quartet state. The results reveal a unique example of dihedral angle-bending isomers with the smallest number of atoms and may help the understanding of the bonding properties of other potential angle-bending isomers.     

中频反应磁控溅射Al2O3薄膜的光学性质

采用中频反应磁控溅射技术在玻璃基片上制备了Al2O3薄膜,提出了一种利用透射光谱来简单有效地分析弱吸收薄膜的光学特性及与光学相关的其他物理特性的方法.对Al2O3薄膜进行透射谱测量,通过对薄膜折射率、吸收系数、膜厚度与入射光波长相互关系的分析,获得了Al2O3薄膜在400~1 100 nm区域内的折射率、吸收系数与入射光波长的关系式,以及Al2O3薄膜厚度的计算公式.     

金属光栅表面增强喇曼散射TE模的计算分析

以纳米量级金属履带矩形光栅为模型,研究了表面增强喇曼散射的特性.针对TE模的入射光,采用耦合波原理对金属表面的衍射场进行了讨论,并用数值计算方法讨论了光栅周期、光栅深度等参量对表面增强的影响以及增强因子随第一级瑞利系数的变化关系.结果表明：在入射光波长为700 nm、光栅周期p=400 nm、 光栅深度d=150 nm、占空比为1/3、入射角度为10°时,获得最大增强,增强因子G可达102.     

Quantum Size Effect of the Magnetism of an Electron in a Metal Layer of the Layered Compounds M/I/M/I…

The energies and the magnetization of an electron in a piece of metal in the structure of Metal/Insulator/Metal/Insulator…(M/I/M/I…), in a magnetic field, at high temperature, and in range of quantum size thickness of the piece of metal layer have been obtained. The results show that when the thickness of the metal layer becomes smaller, the orbital magnetism of the charged particles which collide with the wall of the metal layer is to vary from diamagnetism to paramagnetism. The smaller the thickness of the metal layer becomes, the more particles will collide with the boundary of the metal layer, and then the paramagnetism becomes stronger. Finally, when the thickness of the metal layer becomes very small (＜100 nm), all of the orbital diamagnetism will reverse to paramagnetism, and then the paramagnetization will be almost a maximum constant.