矩阵之和的加权Moore—Penrose逆

§1.引言 Cline在[2]中讨论了矩阵UU~* VV~*的广义逆,并当UV~*=0(或U~*V=0)时给出了矩阵之和U V的广义逆的表达式。本文讨论矩阵UW_1U~* VW_2V~* VT~*U~* UTV~*的加权广义逆,其中[_(T~*W_2)~(W_1T)]是正定矩阵。并当UN~(-1)V~*=0(或U~*MV=0)时给出了矩阵之和U V的加权广义逆的表示。作为特例,给出了不同于[2]的UU~* VV~*及U V的广义逆的表达式。     

关于Quantale矩阵M-P广义逆的注记

主要指出文[1]关于M-P广义逆若干定理成立遗漏的条件,并在文[1]的基础上对M-P广义逆进行深入研究,得到关于Quantale矩阵M-P广义逆的一些新结论.     

r-循环阵的逆阵或广义逆阵

在应用数学和其他学科(如数理统计、固态物理等)中,都将遇到求循环阵的逆阵或广义逆阵的问题.如何求非奇异循环阵的逆阵?文[1]提出了一种算法而无证明,文[2]则给出了这种算法的一个证明,文[3]又提出一种新算法,但上述两种算法的计算量大,实际使用时是很繁的.针对这一情况,文[4]除了对[1]中提出的方法重新给了一个初等证明外,还导出了一些特殊循环阵的逆阵公式.关于求奇异循环阵的广义逆阵的问题,则除了[3]中给出了某类特殊的奇异循环阵的 Moor-Penrose 逆阵外,还未见到有文章论述求奇异循环阵的广义逆阵的一般方法.本文给出了 r-循环阵的逆阵或一个反射 g 逆阵的公式和具体算法.特别,这个公式可用来求通常的循环阵及反循环阵的逆阵和 Moor-Penrose 逆阵.文[3]、[4]中的各个公式可用本文的统一方法推广到 r-循环阵的情形.     

带重点的广义Cauchy矩阵及其相关问题

本文详细讨论了带重点的广义Cauchy矩阵的位移结构、快速求逆公式、可逆性判别条件及其与矩阵有理切插值问题的关系,并给出了求解此类矩阵的线性方程组的快速算法,推广了文[1]和[2]的结果.     

广义二阶差分矩阵的逆与幂

广义二阶差分矩阵是指如下m+1阶方阵方程ax~2+bx+c=0称为T_(m+1)的特征方程,其根称为T_(m+1)的特征根。文[1]、[2]中均研究了T=T_(m+1)(-1,2,-1),[2]中并称其为二阶差分矩阵。两文采用与二阶微分算子相类比的方法求得了T~(-1)的元素的简单表达式。对于更广泛的矩阵(1),我们用残数方法求得了其逆的元素的     

基于广义逆的多元矩阵有理插值

本文借助于文[5]给出的一种矩阵广义逆，构造了二元Stieltjes型矩阵连分式的截断连分式，以此首次定义了平面上拟三角形网格上的二元矩阵有理插道值函数。文中给出了存在性的一个有用的判别条件。重要的特征定理和唯一性定理得到证明，并借助了实例说明了本文的结果。     

"魔(n,k)方"的广义Fibonacci数列解

文 [1 ]将文 [2 ]中的“魔八方”问题推广为“魔(ｎ,ｋ)方”问题 ,研究不定方程ｘ2 +ｘｙ-ｙ2 +ｋ=0　　 (1 )的广义Ｆｉｂｏｎａｃｃｉ数列解 .结束时 ,提出可以证明“魔 (ｎ ,2 )方”和“魔 (ｎ ,3 )方”不可实现 ,未能方便地给出证明 ,也未能很好地实现进一步的探讨 .本文将在文 [1 ]的基础上 ,得出广义Ｆｉｂｏｎａｃｃｉ数列解的首项的充要条件 ,并应用这个充要条件进行简便求解和证明 ,最后对ｋ进行分类讨论 .为了本文叙述的连贯性 ,先摘录文 [1 ]中的 2个定义和定理 1 .1　广义Ｆｉｂｏｎａｃｃｉ数列和“魔 (ｎ ,ｋ)方”问题定义 1…     

广义逆A(2)T,S的一种计算方法

本文给出了利用特征多项式求矩阵广义逆AT，S^(2)的一种计算方法，并由此得到了加权M—P逆AM，N^ 、M—P逆A^ 、Drain逆Ad及群逆A9的相应计算方法，推广了文献[2]的结果．     

矩阵对角占优性的推广及应用

§1.引言设 A=(a_(ij))_(n×n)为一复矩阵,若有一正向量 d=(d_1,d_2,…,d_n)~T 使得d_i|a_(ij)|≥sum from j≠1 d_j|a_(ij)|,(1)对每一 i∈N={1,2,…,n}都成立,则称 A 为广义对角占优矩阵,记为 A∈D_0~*;如若(1)式中每一不等号都是严格的,则称 A 为广义严格对角占优矩阵,记为 A∈D~*.特别地,当 d=(1,1,…,1)~T 时,A∈D_0~*及 A∈D~*即是通常的对角占优与严格对角占优,分别记作 A∈D_0及 A∈D.利用矩阵的对角占优性质讨论其特征值分布是矩阵论中的重要课题,文献[5]—[10]给出了这方面的重要结果.n 阶实方阵 A 称为 M-矩阵,如果 A具有形式:A=sI-B,s>ρ(B),其中 B 为 n 阶非负方阵,ρ(B)表 B 之谱半径,利用广义严格对角占优的概念,文[1]给出了 M-矩阵的等价表征:若 n 阶实方阵     

求矩阵广义逆的另一种初等变换方法

讨论了当矩阵A为满秩矩阵时求其广义逆的一种方法,并将此方法推广,给出当A为非满秩矩阵时求其广义逆的一般方法,同时给出算例.本文推广了文献[1]的结果.     

Cubic Lienard equation with quadradic damping (I)

1. IntroductionLienard equationdZx dx~ f(.)g g(x) = 0 (l.0)dtZ dthas been extensively studied with particular emphasis on the ekistence and uniqueness oflimit cycles (see e.g. [l--4] and references there in). The number of limit cycles of (l.0) hasbeen also investigated by several authors (see e.g. [5--8]).In the present paper we study the general cubic Lienard equation, namelydx da~ = y ~ F(x), Z ~ ~g(x) (1.1)dt' dtwhereF(x) = ale a,x: a,x', (l.2)g(x) = blx b,x' b,x'. (1.3)Clea…     

Cubic Lienard Equations with Quadratic Damping (II)

Abstract   Applying Hopf bifurcation theory and qualitative theory, we show that the general cubic Lienard equations with quadratic damping have at most three limit cycles. This implies that the guess in which the system has at most two limit cycles is false. We give the sufficient conditions for the system has at most three limit cycles or two limit cycles. We present two examples with three limit cycles or two limit cycles by using numerical simulation. Supported by the National Natural Science Foundation of China and National Key Basic Research Special Found (No. G1998020307).     

Erratum to “Uniform convergence and chaotic behavior” [Nonlinear Anal. TMA 65 (4) (2006) 933–937]

We present counterexamples which show that the uniform limit of topologically transitive maps on a compact metric space is not necessarily topologically transitive. We also give stronger conditions that ensure the inheritance of topological transitivity for the case of uniform convergence and other situations.     

Kronecker limit formula for real quadratic number fields (III)

For a kind ofL-function of the real quadratic number fields, we prove a Kronecker limit formula which generalized a result of Hecke. And taking an example we give an interesting identity on a fundamental unit of such a field     

On the Distributions δk and (δ')k

Powers and products of distributions have not as yet been defined to hold true in general. In this paper, we choose a fixed δ-sequence and use the concept of neutrix limit to give meaning to the distributions δ^k and (δ')^k for some k. These may be regarded as powers of Dirac delta functions.     

Sur quelques limites de la physique des particules chargées vers la (magnéto)hydrodynamiqueOn some limits in charged particle physics towards (magneto)hydrodynamic equations

We discuss the connection between different scalings limits of the quantum-relativistic Dirac–Maxwell system. In particular we give rigorous results for the quasi-neutral/non-relativistic limit of the Vlasov–Maxwell system: we obtain a magneto-hydro-dynamic system when we consider the magnetic field as a non-relativistic effect and we obtain the Euler equation when we see it as a relativistic effect. A mathematical key is the modulated energy method. To cite this article: Y. Brenier et al., C. R. Acad. Sci. Paris, Ser. I 334 (2002) 239–244.     

函数列的黎曼积分极限定理的应用

利用函数列的极限理论方法,研究函数列积分极限中积分和极限可交换次序的问题.对一致收敛的可积函数列给出积分的极限定理,对一致有界局部一致收敛函数列给出积分控制收敛定理,通过大量实例表明该理论的意义所在.     

SYNTOPOFORMIC SPACES (SYNTOPOGENOUS LIMIT SPACES)

Abstract

Császár generalized the uniform spaces, the proximity spaces and the topological spaces to syntopogenous spaces. Cook and Fischer generalized the uniform spaces to uniform limit spaces. Finally Marny generalized the proximity spaces to proximal limit spaces. Analogously we generalize the syntopogenous spaces to syntopoformic spaces (syntopogenous limit spaces). These spaces include all the above mentioned in a suitable sense. We extend some of the well-known results of compactness and completeness to syntopoformic spaces.     

Bifurcation of periodic orbits in a class of planar Filippov systems

In this paper we discuss the perturbations of a general planar Filippov system with exactly one switching line. When the system has a limit cycle, we give a condition for its persistence; when the system has an annulus of periodic orbits, we give a condition under which limit cycles are bifurcated from the annulus. We also further discuss the stability and bifurcations of a nonhyperbolic limit cycle. When the system has an annulus of periodic orbits, we show via an example how the number of limit cycles bifurcated from the annulus is affected by the switching.