内部边界球可达域和拟共形映射的H(o)lder连续性

定义了内部边界球可达域,利用曲线族的模证明了D是Rn中的有界Jordan域,f:Bn→D是K-拟共形映射,若D是内部边界球可达域,则f∈H1/K(Bn).     

内部边界球可达域和拟共形映射的Hlder连续性

定义了内部边界球可达域,利用曲线族的模证明了D是R~n中的有界Jordan域,f:B~n→D是K-拟共形映射,若D是内部边界球可达域,则f∈H_(1/K)(B~n).     

有界凸域上拟共形映射的Hoelder连续性

该文利用曲线族的模,得到了n维空间中的有界凸域D到单位球B^n上的K-拟共形映射f的全局Hoelder连续性,且Hoelder指数α=K^1/1-n是最佳的.     

有界凸域上拟共形映射的Holder连续性

该文利用曲线族的模,得到了n维空间中的有界凸域 D 到单位球 Bⁿ上的 K -拟共形映射f的全局Holder连续性, 且Holder指数α=K^1/(1-n)是最佳的.     

Lip_J-扩张域和一致域(英文)

本文证明了如下两个结果:(1)域D(?)R~n是一致域当且仅当D是Lip_J-扩张域;(2)Jordan域D(?)R~2是拟圆当且仅当对在D上满足|f′(z)|≤d(z,(?)D)~(-1)的任意的解析函数f恒有f∈Lip_J(D),其中J(x_1,x_2)=1/2 log(1+|x_1-x_2|/d(x_1,(?)D))(1+|x_1-x_2|/d(x_2,(?)D)),x_1,x_2∈D.     

Apollonian度量与Apollonian边界条件

证明了(1)■中真子域D上的Apollonian度量αD是拟共形映射的拟不变量;(2)■中严格一致域是拟共形不变的;(3)■中的Jordan域D是拟圆当且仅当D是严格一致域,作为应用,进一步得到了Apollonian边界条件,拟共形映射和局部Lipschitz映射之间的关系。     

高维空间中的有界凸域

证明n维空间中的有界凸域D能被拟共形映射到n维单位球B~n(0,1),即D是拟球,从而说明拟共形映射中的黎曼定理在n维空间中的有界凸域类中是成立的．     

双曲测地线与拟圆

设D是R2中的有界Jordan域,证明了D是拟圆当且仅当存在常数M≥1,对D中任意 两条不相交的闭双曲测地线段α1,α2,恒有mod(△(α1,α2;R2))≤Mmod(△(α1,α2;D)).     

拟圆的三个充要条件

设D是R2中的Jordan域,D*=R2＼D是D的外部,本文证明了拟圆的下面三个充要条件:(1)D是拟圆当且仅当D和D*都是弱拟凸域;(2)D是拟圆当且仅当D和D*都是弱Cigar域;(3)D是拟圆当且仅当D是弱一致域.     

Cn单位球上的一类Hilbert值函数的收敛性

本文主要研究了Cn单位球上Hilbert值Dμ,q函数的收敛性,得到了若f=∑α≥0xαzα∈Dμ,q,q＞(2n)/(μ),则φ(z)=∑α≥0‖xα‖zα∈Lipγ,其中0＜μ＜1(n=1)或0＜μ＜2(n＞1).此外还得到若f∈Dμ,q,q＞(2n)/(μ),则对几乎所有的{εα}有fω(z)∈H∞,其中0＜μ＜1(n=1)或0＜μ＜2(n＞1).在此过程中,我们利用了Banach空间几何学和Rademacher函数序列的知识.     

拟共形映射和弱John域

作为John域的推广,本文定义了弱John域,并讨论了弱John域与拟圆、弱John域与拟共形 映射之间的关系,得到(1)若(?)。中的Jordan域D和它的外部 均是弱John域,则D 是拟圆;(2)R2中的弱John域是拟共不变的;(3)R2中的有界拟圆必是弱John域．最后构造例子 说明R2中的无界拟圆不一定是弱John域．     

The boundary integral method for the steady rotating Navier–Stokes equations in exterior domain (I): the existence of solution

In this paper, we apply the boundary integral method to the steady rotating Navier–Stokes equations in exterior domain. Introducing some open ball which decomposes the exterior domain into a finite domain and a infinite domain, we obtain a coupled problem by the steady rotating Navier–Stokes equations in finite domain and a boundary integral equation without using the artificial boundary condition. For the coupled problem, we show the existence of solution in a convex set.     

The boundary integral method for the linearized rotating Navier-Stokes equations in exterior domain

In this paper, we apply the boundary integral method to the linearized rotating Navier-Stokes equations in exterior domain. Introducing some open ball which decomposes the exterior domain into a finite domain and an infinite domain, we obtain a coupled problem by the linearized rotating Navier-Stokes equations in finite domain and a boundary integral equation without using the artificial boundary condition. For the coupled problem, we show the existence and uniqueness of solution. Finally, we study the finite element approximation for the coupled problem and obtain the error estimate between the solution of the coupled problem and its approximation solution.     

Stability of a finite element method for 3D exterior stationary Navier-Stokes flows

We consider numerical approximations of stationary incompressible Navier-Stokes flows in 3D exterior domains, with nonzero velocity at infinity. It is shown that a P1-P1 stabilized finite element method proposed by C. Rebollo: A term by term stabilization algorithm for finite element solution of incompressible flow problems, Numer. Math. 79 (1998), 283–319, is stable when applied to a Navier-Stokes flow in a truncated exterior domain with a pointwise boundary condition on the artificial boundary.     

Finite element error estimates for 3D exterior incompressible flow with nonzero velocity at infinity

We consider a stationary incompressible Navier–Stokes flow in a 3D exterior domain, with nonzero velocity at infinity. In order to approximate this flow, we use the stabilized P1–P1 finite element method proposed by Rebollo (Numer Math 79:283–319, 1998). Following an approach by Guirguis and Gunzburger (Model Math Anal Numer 21:445–464, 1987), we apply this method to the Navier–Stokes system with Oseen term in a truncated exterior domain, under a pointwise boundary condition on the artificial boundary. This leads to a discrete problem whose solution approximates the exterior flow, as is shown by error estimates.     

Привалов定理的拓广

<正> 设Ω是 m 个实变数 u_1,…,u_m 空间中的-p 维可定向流形Ω:(?)Ω称为属于 C~e 类(e是非负的整数),如果实函数 f_1,…,f_(m-p)皆有e次连续偏微商.Ω称为平滑的,如Ω属于 C~1 类并且矩阵     

Two theorems on boundary properties of minimal surfaces in nonparametric form

Let D be a region with rectifiable Jordan boundary , and let z=f(x, y) be a minimal surface defined over D. This paper establishes that: 1) function z=f(x, y) almost everywhere on has finite or infinite angular boundary values; 2) if region D is the exterior of a circle then, almost everywhere on boundary , function z=f(x, y) can be continued by continuity.Translated from Matematicheskie Zametki, Vol. 21, No. 4, pp. 551–556, April, 1977.     

圓環上的單葉函數

<正> 1.設G是z平面上的兩連區域,它的每一個境界部分都不止含有一點.我們知道有唯一的半徑R使圓環1<|ζ|相似文献   

ON INITIAL BOUNDARY VALUE PROBLEMS FOR NONLINEAR SCHRDINGER EQUATIONS

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Stabilization and control for the subcritical semilinear wave equation

In this paper, we analyze the exponential decay property of solutions of the semilinear wave equation in with a damping term which is effective on the exterior of a ball. Under suitable and natural assumptions on the nonlinearity we prove that the exponential decay holds locally uniformly for finite energy solutions provided the nonlinearity is subcritical at infinity. Subcriticality means, roughly speaking, that the nonlinearity grows at infinity at most as a power p<5. The method of proof combines classical energy estimates for the linear wave equation allowing to estimate the total energy of solutions in terms of the energy localized in the exterior of a ball, Strichartz's estimates and results by P. Gérard on microlocal defect measures and linearizable sequences. We also give an application to the stabilization and controllability of the semilinear wave equation in a bounded domain under the same growth condition on the nonlinearity but provided the nonlinearity has been cut-off away from the boundary.