V2Ga5的晶体结构

本文利用单晶与粉末衍射方法测定了V₂Ga₅的晶体结构。V₂Ga₅属四方晶系,其单相区约为VGa₂—V₂Ga₅。在18℃的点阵常数是a=8.9540?,c=2.6892?,每个晶胞含有二个化合式量,空间羣为D_4h⁵—P4/mbm。V原子与Ga原子分别占据在4(h)与8(i),2(d)的等效位置上。参数为:x相似文献   

Low cost, practical, all-digital open-loop fiber-optic gyroscope

A novel all-digital scheme for open-loop fiber-optic gyroscope (POG), where only two key points of output wave were digitized directly, has been proposed. A control equation, with which the modulation depth of PZT modulator is stable when setting the modulation depth as 4.35 and a calculation equation, with which the Sagnac phase can be worked out, are derived. A modulation depth control and an automatic correlation sampling and a gain control technology were induced. A photo-type FOG was made and tested. The good performance was achieved.     

几何光学的现代理论—光线力学

本文介绍了几何光学的最新发展，系统论述了经典光线力学和量子光线力学的基本概念，讨论了光线力学对传统几何光学和波动光学的影响及其发展前景．     

含有长程拓扑性无序螺位错晶格中因势场引起的散射态和束缚态

螺位错的长程拓扑性无序对固体中所传播的波提供特殊的介体。用这种介体研究电势对电子态的影响。作为简单的例子要使用方势阱模型。在这种介体中用相移分析法能成功地得到散射解。未微扰的波函数不是平面波而是Aharouov-Bohm方程的严格解。束缚态能级的数目和位置依赖于电子的耦合和拓扑性无序。     

铜氧化物超导体的电子结构

本文主要很据光电子能谱和电子能量损失谱的实验结果，综述目前对铜氧化物超导体的铜原子的价态、强电子相关作用、反铁磁性、空穴导电及其对称性和费米面的性质等电子结构问题的认识．     

芳氧端基的聚二甲基硅氧烷

通过酚类与六甲基环三硅氧烷（Ｄ３）的调聚反应，首先合成了一类含芳氧端基的聚二甲基硅氧烷（ＡＯＳ）．采用ＵＶ、ＩＲ、１ＨＮＭＲ、元素分析、分子量测定等方法，确证了所合成聚合物的结构．讨论了反应试剂摩尔比和反应条件对调聚产物分子量的影响；研究了ＡＯＳ的结构与杀菌功能、絮凝作用以及水解速度的关系．     

铝、铜、镍三元合金系中τ相的晶体结构变迁

A thorough investigation by means of X-rays has been carried out with the purpose to determine the nature of the ternary phase τ in Al-Cu-Ni alloys. In contrast with the conventional concept of alloy phase which is characterized by a definite type of crystal structure, systematic structure changes are found in the single phase field of τ which occupies quite an extensive area in the isothermal section of the phase diagram at room temperature. There are eight types of structures altogether, all derived from a basic rhombohedron with corners occupied by Al atoms and centres either occupied by the heavy atoms or remaining vacant. The basic rhombohedron is the building stone in the crystal architecture. By transforming the basic rhombohedron into a hexagonal prism in the usual way, all structures may be considered to be built up by stacking together a number of these hexagonal prisms along the triad. The transformation of one structure into another is quite systematic in the way that the number of the stacking stories in the unit cell increases according to the order 10, 11, 12, 13, 14, 15, 16, 17. The atomic arrangements in the different structures are closely related too, in the respect that they are all superstructures due to the presence of ordered vacancies in the rhombohedral centres.The principal factor controlling the formation of these structures has been fully considered. In view of the fact that the change of structure types follows closely with the content of Ni or Cu for alloys of constant Al content, the atomic size factor appears to be unimportant in the formation of these alloys. It has been shown that for alloy phases of the defect lattice type as the r-phase, the most fundamental factor is the average number of valency electrons per structural unit which is the basic rhombohedron in the present case. By assuming Hume-Rothery's valencies, the average number of valency electrons remains remarkably constant throughout the entire phase field, while the electron concentration varies with compositions. It has also been pointed out that for alloy phases where there is no unit cell change, the average number of electrons per structural unit is equivalent to the number of electrons per unit cell, and for alloy phase where there is no defect, this is in effect equivalent to the electron concentration.     

关于不定方程 x~2-Dy~2=4在两种特殊情形下的最小解

在数论方面的专著中,对不定方程(1) x~2-Dy~2=4 (D>0且非完全平方数)作了重要的介绍.我们知道,方程(1)恒可解.若已知 x_0,y_0为(1)之最小正整数解,则(1)的一切解x,y 可由下式