化合物半导体-绝缘体界面的界面态(续)

 三、界面态连续体的动态响应和分布多年来的大量研究结果表明把界面态处理为局域在半导体界面平面处的经典理论完全不能够解释化合物半导体-绝缘体界面的行为特点,从而使人们逐渐认识到界面态的空间分布特征.图3为半导体界面的能带结构示意图.在实际的I-S界面上,界面态是在绝缘体-半导体界面附近,在能量上和空间上的连续分布体(如图中点所示). 这里以n型半导体为例,通过绝缘体中的界面态对电子的捕获和发射过程说明界面态动态响应的特点.由于势垒△Ec的存在,空间分布的界面态与电子的作用只能依介量子力学的隧道效应得以进行.     

二参数Ornstein—Uhlenbeck过程的象集的一些性质

本文研究二参数 d 维 Ornstein-Uhlenbeck 过程 X(t)(t∈R_+~2)的象集 X(E)的性质,得到了 X(E)的 Hausdorff 维数,并证明了若 dim E>d/2,则 X(E)的 Lebesgue测度 a.s.大于0,且对于几乎所有的θ∈[0,2π]若,θ(E)(?)CR_+~2,则 X(θ(E))a.s.具有内点。     

关于B值随机和的完全收敛性的进一步讨论

该文在深入揭示B值非随机和完全收敛性中的一系列等价关系的基础上，给出了随机和完全收敛的充分条件，改进和完善了有关文献中的既有成果，并对矩条件的必要性问题做了初步讨论．     

利用有限几何构作3-PBIB（2）设计和3-设计

The concept of t-PBIB design was introduced by Wei Wandi and Yang Benfu as a generalization of G-design and PBIB design. In this paper, a number of 3-associntion schemes and 3-PBIB(2) designs are constructed on the bases of the finite vector space over Fq and the finite unitary geometry over Fq2. Then a number of 3-designs are constructed on the bases of the finite orthogonal geometries over Fq. The parameters of all these designs are computed.     

拟阵与概念格的关系

本文以构造的方式建立起拟阵与概念格的联系,得到在同构意义下每个拟阵是一个概念格,但反之不然的结论;该结论使得利用概念格的性质研究拟阵成为现实,特别为将建造概念格的算法尤其是已计算机化的算法应用于求取拟阵奠定了基础,也为拟阵论成为研究概念格性质的辅助工具打下基础．     

Bifurcation and Isochronicity at Infinity in a Class of Cubic Polynomial Vector Fields

In this paper, we study the appearance of limit cycles from the equator and isochronicity of infinity in polynomial vector fields with no singular points at infinity. We give a recursive formula to compute the singular point quantities of a class of cubic polynomial systems, which is used to calculate the first seven singular point quantities. Further, we prove that such a cubic vector field can have maximal seven limit cycles in the neighborhood of infinity. We actually and construct a system that has seven limit cycles. The positions of these limit cycles can be given exactly without constructing the Poincare cycle fields. The technique employed in this work is essentially different from the previously widely used ones. Finally, the isochronous center conditions at infinity are given.     

Pregelation Behaviour of Coagulation Processes with the Constant-Reaction-Number Kernel

We propose an irreversible binary coagulation model with a constant-reaction-number kernel, in which, among all the possible binary coagulation reactions, only p reactions are permitted to take place at every time. By means of the generalized rate equation we investigate the kinetic behaviour of the system with the reaction rate kernel K（i;j） = （ij）^w （0 ≤w〈1/2）, at which an i-mer and a j-mer coagulate together to form a large one. It is found that for such a system there always exists a gelation transition at a finte time to, which is in contrast to the ordinary binary coagulation with the same rate kernel. Moreover, the pre-gelation behaviour of the cluster size distribution near the gelation point falls in a scaling regime and the typical cluster size grows as （to - t）-1/（1-2w）. On the other hand, our model can also provide some predictions for the evolution of the cluster distribution in multicomponent complex networks.     

二元不等式（组）解集的图示及应用

对于不等式 ｇ(ｘ ,ｙ)≤ 0 ,或 ｇ(ｘ ,ｙ)≥0 ,若曲线 ｇ(ｘ ,ｙ) =0将平面分成两部分 ,则不等式的解集通常是其中的一部分 ,利用平面上的点集表示二元不等式 (组 )的解集 ,可为求以二元不等式 (组 )为约束条件的某些二元函数的最值提供方便 ,新教材中关于线性规划问题的求解正是这一思想的体现 .例 1　已知ｘ + ｙ≤ 4ｘ - 2 ｙ≤ 03ｘ - ｙ≥ 0( 1 )( 2 )( 3)求ｘ2 + ｙ2 的最大值 .图 1　例 1图解　如图 1 ,不等式 ( 1 )的解集是直线ｘ+ ｙ =4下方的半平面 .不等式 ( 2 )的解集是直线ｘ - 2 ｙ =0上方的半平面 .不等式 ( 3)的解集是直…     

凸集的广义Reuleaux三角形

常宽凸集的面积最小者为Reulaux三角形，而非常宽凸集的面积最小者为何呢？它就是本文将给出的广义Reuleaux三角形△R。