复双球面上变系数奇异积分方程的正则化

利用复双球面上的立体角系数的方法和置换公式,讨论复双球垒域上变系数奇异积分方程的正则化问题,推广了复超球面上变系数奇异积分方程的结论．     

复超球面上奇异积分方程的正则化

<正> 在一维奇异积分方程论中,复变函数的 Cauchy 型积分起着十分重要的作用;但在研究高维奇异积分方程时,利用多复变数 Cauchy 型积分作为工具者,至今尚少(参看[2]—[6]).本文是用复超球的 Cauchy 型积分边界性质,处理复超球面上含 Cauchy 核、B 核与 h 核的奇异积分方程的正则化问题.     

复双球垒域上奇异积分的Cauchy主值

利用一种新的挖法定义复双球垒域上的立体角系数,得到奇异积分的Cauchy主值的存在性.推广了复超球上的奇异积分理论.     

复超球上Poisson-华积分边界性质的一个新证明

把复超球 Bn看作多复变典型域 RI(m,n)当 m=1时的特例 ,本文给出复超球上 Poisson-华积分边界性质的不同于文献 [3 ]的一个新证明 ,并研究了 Cauchy积分的边界性质及 Bn上的 Dirichlet问题     

复双球垒域用“矩形”挖法的Plemelj公式

在［１，２］的基础上，利用“矩形”挖法的柯西主值，获得犆狀空间中复双球垒域上具有局部全纯离散核的Ｃａｕｃｈｙ型积分的含有边界上点的立体角系数的Ｐｌｅｍｅｌｊ公式．     

一类复超球上的Riemann边值问题及其应用

本文将推广一维的 Riemann 边值问题(可参考路见可教授[2])提出复超球上的内外值函数的定义和 Riemann 边值问题,我们将先讨论内外值函数的性质,给出一类Riemmann 问题的解,最后给出一类复超球上一类奇异积分方程的解的具体形式:     

复超球面上的奇异积分及奇异积分方程

龚升、孙继广研究了复超球面上积分密度为 H(?)lder 连续的带有 Cauchy 核的奇异积分,在 Cauchy 主值意义下讨论了复超球面的奇异积分方程在 Halder 连续函数类中的求解问题。N.Kerzman 和 E.M.Stein 对强拟面域,A.Koranyi 和 S.Vagi 对齐性空间在 P 次平均收敛意义下,考虑了积分密度为 L~p 可积的带有某种奇性核的奇异积分的另一种主值,本文在他们定义的主值意义下讨论了复超球面上的带有 Cauchy 核的奇异积分     

带两个Carleman位移的奇异积分方程Noether可解的充分必要条件

带Carleman位移的奇异积分方程理论,近年来得到了很大发展。在[1]中建立了这种奇异积分方程的Noether理论,所用的基本方法是建立所谓的对应方程组(是不带位移的奇异积分方程组,它的理论是已知的,参看[2],[3])。在[4]中讨论了带两个Carleman位移的奇异积分方程Noether可解的充分条件,并给出了计算指数的公式。本文目的是在文章[4]的基础上,利用不同的方法解决带两个Carleman位移的奇异积分方程Noether可解的充分必要条件问题,并把所得结果对带两个Carleman位移及未知函数复共轭值的奇异积分方程进行推广。     

关于非线性奇异积分微分方程解的延拓

在该文中．研究下面的带柯西核的非线性奇异积分微分方程的解这里Γ是简单的李雅普诺夫闭路，u（t）是应当确定的未知函数U（t）=｛u（t），u'（t）.........u（n）（t）｝,uj0是某些实数或复数．（1）型的非线性奇异积分微分方程用插入法或拓扑法在[1]－[5]的论文中已被研究．在[6]．[7]的论文中方程（1）的解用李雅鲁诺夫的分析方法来研究．     

复超球Bergman空间和Bloch空间上的Carleson不等式

本文研究了复超球上Ｃａｒｌｅｓｏｎ测度的特征．特别是用Ｂｅｒｇｍａｎ函数和Ｂｌｏｃｈ函数的导数的积分性质刻画了Ｃａｒｌｅｓｏｎ测度，并建立了复超球上的Ｂｅｒｇｍａｎ空间和Ｂｌｏｃｈ空间的Ｃａｒｌｅｓｏｎ不等式．     

THE POINCAR-BERTRAND FORMULA ON THE BUILDING DOMAIN OF COMPLEX BIBALLS

The Poincaré-Bertrand formula takes an important position in the study of complex singular integral.The Poincaré-Bertrand formula on the complex sphere in the multidimensional complex Euclidian spaces was given by Sheng Gong.Using the method of solid angular coefficient,the authors extend the Poincaré-Bertrand formula on the complex sphere to the building domain of the complex biballs,and obtain a more general Poincaré-Bertrand formula with the solid angular coefficients.     

复双球垒域上一些奇异积分方程的直接求解（英文）

By means of the method of solid angle coefficients and the permutation formula on the building domain of complex biballs,direct solutions of some singular integral equations with variable coefficients are discussed and the explicit formulas for these solutions are obtained.     

Spherical Singular Integrals, Monogenic Kernels and Wavelets on the Three-Dimensional Sphere

The construction of wavelets relies on translations and dilations which are perfectly given in . On the sphere translations can be considered as rotations but it is difficult to say what are dilations. For the 2-dimensional sphere there exist two different approaches to obtain wavelets which are worth to be considered. The first concept goes back to W. Freeden and collaborators who define wavelets by means of kernels of spherical singular integrals. The other concept developed by J.P. Antoine and P. Vandergheynst is a purely group theoretical approach and defines dilations as dilations in the tangent plane. Surprisingly both concepts coincides for zonal functions. We will define singular integrals and kernels of singular integrals on the three dimensional sphere which are also approximate identities. In particular the Cauchy kernel in Clifford analysis is a kernel of a singular integral, the singular Cauchy integral, and an approximate identity. Furthermore, we will define wavelets on the 3-dimensional sphere by means of kernels of singular integrals. This paper is dedicated to the memory of our friend and colleague Jarolim Bureš Received: October, 2007. Accepted: February, 2008.     

Integrable nonconservative dynamical systems on the tangent bundle of the multidimensional sphere

We construct a class of nonconservative systems of differential equations on the tangent bundle of the sphere of any finite dimension. This class has a complete set of first integrals, which can be expressed as finite combinations of elementary functions. Most of these first integrals consist of transcendental functions of their phase variables. Here the property of being transcendental is understood in the sense of the theory of functions of the complex variable in which transcendental functions are functions with essentially singular points.     

SINGULAR INTEGRALS IN SEVERAL COMPLEX VARIABLES(Ⅱ)——HADAMARD PRINCIPAL VALUE ON A SPHERE

Hadamard introduced the concept of finite parts of divergent integrals.i.e.Hadamardprincipal value,when he researched the Cauehy problems of the hyperbolic type partialdifferential equations.In this paper,the authors try to generalize this concept to the singularintegrals on a sphere of several complex variables space C~n.The Hadamard principal valueof higher order singular integralis defined and the corresponding Plemelj formula is obtained.     

Geometric bounds on the linearization domain and analytic dependence on parameters for families of analytic vector fields in a neighborhood of a singular point

We study families of holomorphic vector fields, holomorphically depending on parameters, in a neighborhood of an isolated singular point. When the singular point is in the Poincaré domain for every vector field of the family we prove, through a modification of classical Sternberg's linearization argument, cf. Nelson (1969) [7] too, analytic dependence on parameters of the linearizing maps and geometric bounds on the linearization domain: each vector field of the family is linearizable inside the smallest Euclidean sphere which is not transverse to the vector field, cf. Brushlinskaya (1971) [2], Ilyashenko and Yakovenko (2008) [5] for related results. We also prove, developing ideas in Martinet (1980) [6], a version of Brjuno's Theorem in the case of linearization of families of vector fields near a singular point of Siegel type, and apply it to study some 1-parameter families of vector fields in two dimensions.     

Semi-analytic treatment of the three-dimensional Poisson equation via a Galerkin BIE method

A systematic treatment of the three-dimensional Poisson equation via singular and hypersingular boundary integral equation techniques is investigated in the context of a Galerkin approximation. Developed to conveniently deal with domain integrals without a volume-fitted mesh, the proposed method initially converts domain integrals featuring the Newton potential and its gradient into equivalent surface integrals. Then, the resulting boundary integrals are evaluated by means of well-established cubature methods. In this transformation, weakly-singular domain integrals, defined over simply- or multiply-connected domains with Lipschitz boundaries, are rigorously converted into weakly-singular surface integrals. Combined with the semi-analytic integration approach developed for potential problems to accurately calculate singular and hypersingular Galerkin surface integrals, this technique can be employed to effectively deal with mixed boundary-value problems without the need to partition the underlying domain into volume cells. Sample problems are included to validate the proposed approach.     

Semi-analytic treatment of the three-dimensional Poisson equation via a Galerkin BIE method

A systematic treatment of the three-dimensional Poisson equation via singular and hypersingular boundary integral equation techniques is investigated in the context of a Galerkin approximation. Developed to conveniently deal with domain integrals without a volume-fitted mesh, the proposed method initially converts domain integrals featuring the Newton potential and its gradient into equivalent surface integrals. Then, the resulting boundary integrals are evaluated by means of well-established cubature methods. In this transformation, weakly-singular domain integrals, defined over simply- or multiply-connected domains with Lipschitz boundaries, are rigorously converted into weakly-singular surface integrals. Combined with the semi-analytic integration approach developed for potential problems to accurately calculate singular and hypersingular Galerkin surface integrals, this technique can be employed to effectively deal with mixed boundary-value problems without the need to partition the underlying domain into volume cells. Sample problems are included to validate the proposed approach.