用等值宽度法测量fs脉冲宽度

本文提出利用等值宽度测量fs光脉冲持续时间的方法.给出了脉冲形状为sech~2 (t/T)、exp(-2t~2/T~2)和exp(-2|t|/T)的干涉相关曲线上包络与相应二阶强度相关曲线半宽度等值的位置,它们分别是3.984、4.875和4.928.定义了两种相关测量的临界延迟速度.理论分析与实验结果符合得很好.所得结果表明,该测量方法可将常规超短脉冲相关测量的时间分辨率提高几倍至几十倍.     

非线性增益和波导结构对半导体激光器的谱线宽度的作用

本文采用半经典理论研究了非线性增益和波导结构对量子相位噪声引起的模式谱线增宽过程的作用,得出谱线宽度不但与线性增益而且与三阶增益有关,并且都受到波导结构的制书。从而提出新的谱线增宽因子和与功率无关的线宽的新机制。 关键词：     

K-原子能移和宽度的唯象分析

尝试用Woods-Saxon形式的光学势来分析K原子，通过拟合一系列K原子数据，得到了一套最佳光学势参数. 把得到的这套光学势和前人的其它几种光学势在接近核表面处作了比较，发现他们彼此符合得很好. 另外，与核子-核势相比较，对于虚部势，K-核的Woods-Saxon势与核子-核的很相似，但是对于实部，K-核势要更深更窄一些.     

由自共轭线性微分算子所确定的函数类在Lq(T)中的相对宽度

得到了使等式Kn(K2(Pr),MK2(Pr),L2(T))=dn(K2(Pr),L2(T))成立的最小M值,并计算了Kn(K2(Pr),K2(Pr),Lq(T))的渐近阶,其中Kn(.,.,Lq(T))和dn(.,Lq(T)),1≤q≤∞,分别代表Kolmogorov意义下在Lq(T)中的相对宽度和宽度,K2(Pr)表示定义在[-π,π]上由自共轭线性微分算子所确定的光滑函数类.     

利用硅光电池测量硅单晶半导体材料的禁带宽度

以白炽灯为光源照射单晶硅光电池,测量在硅光电池前加不同截止波长的滤色片时的短路电流.通过短路电流和截止波长的关系,经拟合得到单晶硅材料的长波限,再利用半导体材料的长波限与半导体的禁带宽度Eg的关系,即Eg=hc/λ,计算得出其禁带宽度.     

多元Sobolev关于Lqp（R^d）下的平均线性宽度

得到了两种多元Sobloev类于Lqp(R^d)下平均线笥宽度的弱渐估计。     

准静态近似下多维裂变宽度的研究

本文采用核变形{c、h、α}参数在准静态近似下计算了二维裂变宽度,分析了一维和二维之间的差别.     

Finite size specimens with cracks of icosahedral AI-Pd-Mn quasicrystals

Icosahedral quasicrystals are the most important and thermodynamically stable in all about 200 kinds of quasicrystals currently observed. Beyond the scope of classical elasticity, apart from a phonon displacement field, there is a phason displacement field in the elasticity of the quasicrystal, which induces an important effect on the mechanical properties of the material and makes an analytical solution difficult to obtain. In this paper, a finite element algorithm for the static elasticity of icosahedral quasicrystals is developed by transforming the elastic boundary value problem of the icosahedral quasicrystals into an equivalent variational problem. Analytical and numerical solutions for an icosahedral A1-Pd-Mn quasicrystal cuboid subjected to a uniaxial tension with different phonon-phason coupling parameters are given to verify the validity of the numerical approach. A comparison between the analytical and numerical solutions of the specimen demonstrates the accuracy and efficiency of the present algorithm. Finally, in order to reveal the fracture behavior of the icosahedral A1-Pd-Mn quasicrystal, a cracked specimen with a finite size of matter is investigated, both with and without phonon-phason coupling. Meanwhile, the geometry factors are calculated, including the stress intensity factor and the crack opening displacement for the finite-size specimen. Computational results reveal the importance of pbonon-phason coupling effect on the icosahedral A1-Pd-Mn quasicrystal. Furthermore, the finite element procedure can be used to solve more complicated boundary value problems.