磁共振法研究(Fe1-xCox)84Zr3.5Nb3.5B8Cu1纳米晶薄带的磁各向异性

铁磁共振(FMR)实验研究(Fe1-xCox)84Zr3.5 Nb3.5B8Cu1(x=0.0,0.2,0.4,0.6, 0.8)合金薄带的各向异性,易轴在薄带的横向方向,同等宽度样品的各向异性常数K′随Co掺杂量的增加而减小, K′值在4.67×10-5 J/m(x=0.0)到2.54×10-5 J/m4(x=0.8)之间.由于磁化率的虚部χ″(H)随磁场强度H非线性变化,在低场(0-12 mT)有一个与FMR信号强度相当的低场非共振信号.特别是对Fe84Zr3.5 Nb3.5B8Cu1合金薄带的磁化,在可逆磁化(0-2.0 mT)和趋近饱和磁化(9.0-12 mT)区域, dχ″/dH=0;不可逆畴壁移动过程中,交流磁化率虚部χ″(H)与磁场强度的n次方即Hn(n≥3)有关;在磁畴转动过程中χ″(H)正比于H2(瑞利区),(dχ″)/(dH)为常数;而且发现,有不可逆畴壁移动-磁畴转动三段交替变化的过程,此过程对应三种磁畴的消失过程.     

晶体X射线衍射的发现及其深远影响

 2002年和2003年分别是劳厄(MaxVonLaue)发现晶体X射线衍射和布喇格(W.L.Bragg)建立布喇格方程90周年。劳厄和布喇格的发现是20世纪物理学意义深远的大事。一、X射线的发现1895年11月8日德国维尔茨堡大学校长伦琴在做阴极射线实验时,发现了一种看不见的射线从管中阴极射线轰击的那个电极发射出来,经过一个多月全神贯注的实验探索,终于确认这是一种新的射线---X射线。     

Al/Al2O3P金属基复合材料的静动态压缩性能及损伤分析

用气压浸渗工艺制备了体积分数40％～50％Al2O3颗粒增强纯铝基复合材料，使用了4种不同尺寸的Al2O3颗粒，其平均粒径分别为5μm、10μm、30μm和60μm．测定了这些复合材料的静、动态压缩性能，并通过材料压缩前后密度变化的测量定量表征了材料的累计损伤，结果表明，与基体材料相似，这些复合材料表现出明显的应变率敏感性；当增强颗粒平均粒径小于60μm时，材料的累计损伤基本与应变率无关，而主要取决于材料的应变．材料中颗粒的破裂主要是由颗粒间的相互作用引起的．较小尺寸颗粒增强的复合材料具有较高的流动应力和较小的累计损伤，并随着颗粒体积分数的增加，材料的流动应力和损伤率都相应增加．     

Fe∶LiNbO3全息图热定影及H+浓度的影响

应用光折变效应动力学方程,导出了在Fe∶LiNbO3中对光折变全息图热定影所需的最小H+浓度,以及H+浓度与光栅空间频率的关系.应用光谱比较法测量了不同样品的H+浓度值.得出了进行有效热定影的H+浓度范围.完成了Fe∶LiNbO3全息存储和热定影实验.获得了100 h连续无损读出的良好热定影实验结果.     

溃坝问题的间断有限元方法

本文研究90年代初提出的Runge-Kutta间断Galerkin有限元方法，给出该方法的精度分析，通过经典算例验证该方法处理间断问题、捕捉锐利波形的能力，并将其推广到求解浅水问题．针对坝底无摩擦，无坡度的理想情形进行讨论，给出方溃坝和圆溃坝问题的数值模拟结果．     

Nd：GdVO4单晶的生长、位错和形貌

用提拉法生长出掺钕钒酸钆(Nd：GdVO4)单晶，并且采用化学浸蚀法在偏光显微镜下观察了位错蚀坑，测定了(100)面晶体位错密度为600个／mm^2。观察了不同提拉方向的晶体生长形貌，可采用简单光学方法确定晶体方向。     

THE COUPLING OF NATURAL BOUNDARY ELEMENT AND FINITE ELEMENT METHOD FOR 2D HYPERBOLIC EQUATIONS

In this paper, we investigate the coupling of natural boundary element and finite element methods of exterior initial boundary value problems for hyperbolic equations. The governing equation is first discretized in time, leading to a time-step scheme, where an exterior elliptic problem has to be solved in each time step. Second, a circular artificial boundary FR consisting of a circle of radius R is introduced, the original problem in an unbounded domain is transformed into the nonlocal boundary value problem in abounded subdomain. And the natural integral equation and the Poisson integral formula are obtained in the infinite domainΩ2 outside circle of radius R. The coupled variational formulation is given. Only the function itself, not its normal derivative at artificial boundary ΓR, appears in the variational equation, so that the unknown numbers are reducedand the boundary element stiffness matrix has a few different elements. Such a coupled method is superior to the one based on direct boundary element method. This paper discusses finite element discretization for variational problem and its corresponding numerical technique, and the convergence for the numerical solutions. Finally, the numerical example is presented to illustrate feasibility and efficiency of this method.     

Equivalent Antisymmetry Performance of Three—Dimensional Heterogeneous Anisotropic Composites

Starting from the physical features of materials, heterogeneous anisotropic composites (HAGs) are analysed on the basis of the understanding and applications of its equivalent antisymmetry performance. Moreover, the design parameter is optimized to attain the goal of maximizing the use of materials, which is quite meaningful. The HAG structure is defined as a kind of equivalent structures according to the structure and properties of materials.We apply the mature plate theory and the composite materials laminate theory in analysis of the HAG structure,and in this way a new concept and a new idea are expected.     

一种能补偿热效应的高功率端面泵浦Nd:YVO4激光谐振腔的设计

针对激光二极管端面泵浦的Nd:YVO₄全固态激光器,提出了一种利用双晶体,对Nd:YVO₄的热效应进行补偿的方案,同时该方案又能提高最大输出功率,避免由于插入附加光学元件所导致的损耗,满足调Q以及提高腔内倍频效率的要求.     

Crystal Structure of Adduct 2-Phenyl-imidazo [ 4,5-f ] 1,10-phenanthroline Methanol

The structure of the title adduct comprises a phenanthroline derivative 2-phenyl-imidazo[4,5-f]1,10-phenanthroline and a methanol.The composition of the crystalline adduct was characterized as C19H12N4.CH3OH.It belongs to orthorhombic system,space group Pna21 with a=1.3693(4)nm,b=2.2988(7)nm,c=0.51338(15)nm,V=1.6160(8)nm^3.Z=4,and final R1=0.0423.wR2=0.1012 .Crystal structure shows that all the 19 carbon atoms and 4 nitrogen atoms are coplanar.The bond length data indicated that a very extensive conjugation system was formed.This conjugation makes the compound being a potentially excellent energy transformer used for luminescent materials.