von Neumann代数上的Lie可导映射

设A是不含交换中心投影的von Neumann代数,投影P∈A使得P=0, P=I.称可加映射δ:A→A在Ω∈A Lie可导,若δ([A,B])=[δ(A,δ(B)],■A,B∈A,AB=Ω.该文证明,若Ω∈A满足PΩ=Ω,则δ在ΩLie可导当且仅当存在导子τ:A→A和可加映射f:A→Z(A)使得δ(A)=τ(A)+f(A),■A∈A其中f([A,B)=0,■A,B∈A,AB=Ω.特别地,若A是因子von Neumann代数,Ω∈A满足ker(Ω)≠0或ran(Ω)≠H,则可加映射δ:A→A在ΩLie可导当且仅当δ有上述形式.     

广义对称性在积分计算中的应用

设f（P）是对称区域Ω上的连续函数,其中P∈Ω.若f（P）在Ω中各对称点处函数值的绝对值相等且符号相反时,∫Ωf（P）dΩ=0;当f（P）在Ω中各对称点处的函数值相等时,Ω∫f（P）dΩ=2Ω∫1f（P）dΩ,其中Ω1为Ω＂对称的一半＂.此结论称为积分的广义对称性.通过实例说明了利用此结论可以简化很多积分的计算.     

BCI代数的Ω-犹豫模糊P理想

给定一个集合Ω,在BCI代数中引入Ω-犹豫模糊P理想的概念,讨论它的一些性质,研究了Ω-犹豫模糊P理想的同态像与同态原像的性质;研究了BCI代数中的Ω-犹豫模糊P理想与犹豫模糊P理想的相互构造,通过Ω-犹豫模糊P理想的水平P理想,讨论了BCI代数中Ω-犹豫模糊P理想的刻画;研究了Ω-犹豫模糊P理想与乘积型BCI代数的Ω-犹豫模糊P理想的关系.     

锥中边界函数分式Poisson展式的边界极限

设GC_((n))(Ω)为有界开集,f∈L(C_((n))(Ω)),PIΩf(P)=∫s_(((n)(Ω)))(P,Q)f(Q)dσQ,其中PI_((Ω))(P,Q)是锥C_((n))(Ω)内的Poisson核.本文将给出正规化算子(PIΩf(P))/(PIΩXG(P))在锥中的边界极限,所得结果推广了潘国双在半空间中的相关结论.     

关于特征值问题有限元近似解的最大模估计及其校正加速估计

本文记通常CooeB空间W_p~m(Ω)(P=2时记为H~m(Ω))的模为||·||_(m,p),m=0,即空间L_p(Ω)的模简记为||·||_p。 设Ω为平面有界区域,边界?Ω分段光滑,则(1)的解存在,且特征值可列:     

三维光滑区域上Navier-Stokes方程的有限元方法

§1.引言设Ω是R~3中的有界区域,且属于C~2.v是正常数.已知:当f∈(L~2(Ω))~3.且||f||0充分小时,Navier—Stokes方程的解存在且唯一.另外,u∈(H~2(Ω)∩H_1~0(Ω))~3,P∈H~1(Ω)\R. 最近,Bernardi讨论三维多面体区域Ω上Stokes方程的有限元解法.有限元空间由分片多项式(关于u为分片特殊三次多项式,关于p为分片常数)构成,进行误差估计时.要求u∈(H~2(Ω)∩H_0~1(Ω))~3,P∈H~1(Ω)\R.当Ω为二维区域上的凸多角形时,Stokes     

关于平稳过程的0-1律

设(Ω,(?),P)为一概率空间,{A_n}n≥1 是(?)中的一串元素,Borel-Cantelli 引理表明:sum from n=1 to ∞ P(A_n)<∞(?)P(A_n i.o.)=0,其中(A_n.i.o.)=(?)A_n.特别地,当{A_n}n≥1为相互独立时,还有:sum from n=1 to ∞ P(A_n)=∞(?)P(A_n i.o.)=1.在本文中,我们先给出 Borel-Cantlli 引理之逆成立的另一个条件,然后利用这一结果来证明(严)平稳过程的一个0-1律。设 T:Ω→Ω是概率空间(Ω,(?),P)上到其自身的一个保测变换,称 T 为遍历的,若对任一B(?),T~(-1)B=B(?)P(B)=0或 P(B)=1.关于遍历变换,我们有:     

求解Lipschitz型规划全局极小点的改进的填充函数法

1 引言 考虑问题 (P)min(x), x∈Ω其中F:ΩR~n→R是局部Lipschitz函数,Ω为紧集,且F(x)在Ω内有极小点。文[1,2,3]在一定条件下给出了求解一般非光滑规划全局极小点的填充函数法,并给出了求解的全过程。本文根据文[1,2,3]的思想,为求解(P),结合函数的特点,给出了一种改进     

径迹贡献蒙特卡罗方法

考虑不依赖时间的粒子输运问题.不失一般性,还限定问题与能量无关.令P=(r,Ω),其中r和Ω分别表示粒子的位置和运动方向单位矢量.用S(P)表示粒子源;φ(P)表示粒子通量;D(P)表示探测器对粒子通量的响应函数.要计算的是如下积分效应:     

A CHARACTERIZATION OF A TWO-WEIGHT NORM INEQUALITY FOR ERGODIC MAXIMAL OPERATORS

Let(Ω,,P)be a non-atomic probability space and letT:Ω→Ω be an ergodic measure preserving transformation.For each pair of nonnegative integers n,m we define theoperator T_(n,m),acting on measurable functions as     

Existence,uniqueness and asymptotic behavior of traveling wave fronts for a vector disease model

This paper is concerned with the existence, uniqueness and asymptotic behavior of traveling wave fronts for a vector disease model. We first establish the existence of traveling wave fronts by using geometric singular perturbation theory. Then the asymptotic behavior and uniqueness of traveling wave fronts are obtained by using the standard asymptotic theory and sliding method. In addition, our method is also suitable to establish the uniqueness and asymptotic behavior of traveling wave fronts for a cooperative system.     

Contrast structures in the reaction-diffusion-advection equations in the case of balanced advection

For a singularly perturbed parabolic equation termed in applications as the reaction-diffusion-advection equation, stationary solutions with internal transition layers (contrast structures) are studied. An arbitrary-order asymptotic approximation of such solutions is constructed, and an existence theorem is proved. An efficient algorithm for constructing an asymptotic approximation of the transition point is proposed. The constructed asymptotic approximation is justified by applying the asymptotic method of differential inequalities, which is extended to the class of problems under study. This method is also used to establish the Lyapunov stability of such stationary solutions.     

关于边界层方法

本文指出传统的边界层方法(包括匹配法和Vi?ik—Lyusternik方法)的不足:不能作出边界层项的渐近展开式.提出多重尺度构造边界层项的方法,得到符合实情的结果.又与Levinson所用的方法比较,本方法能更简单地导出后一方法给出的边界层项的渐近展开式.又应用此方法研究现有的关于奇异摄动的某些成果,指出这些成果的局限性,并在一般情况下作出解的渐近展开式.     

An approach to singular perturbation problems insoluble by asymptotic methods

Singular perturbation problems not amenable to solution by asymptotic methods require special treatment, such as the method of Carrier and Pearson. Rather than devising special methods for these problems, this paper suggests that there may be a uniform way to solve singular perturbation problems, which may or may not succumb to asymptotic methods. A potential mechanism for doing this is the author's boundary-value technique, a nonasymptotic method, which previously has only been applied to singular perturbation problems that lend themselves to asymptotic techniques. Two problems, claimed by Carrier and Pearson to be insoluble by asymptotic methods, are solved by the boundary-value method.     

Derivation of transitional asymptotic expansions from integral representations

A method for deriving transitional asymptotic expansions from integral representations is described and applied to Anger function and modified Hankel function. The method consists in deriving asymptotic expansions of the function considered as well as its first derivativeat the transition point using conventional methods such as Laplace’s method or the method of steepest descents. Since both the functions considered satisfy a second order linear differential equation, it is possible to obtain asymptotic expansions of higher order derivatives of the functions from the first two expansions. Thus asymptotic expressions for all the derivatives at the transition point are known and a Taylor expansion of the function in the neighbourhood of the transition point can be written. The method is also applicable to the generalized exponential integral, Weber’s parabolic cylinder function and Poiseuille function.     

An effective asymptotic method in the axisymmetric frictionless contact problem for an elastic layer of finite thickness

A brief review of asymptotic methods to deal with frictionless unilateral contact problems for an elastic layer of finite thickness is presented. Under the assumption that the contact radius is small with respect to the layer thickness, an effective asymptotic method is suggested for solving the unilateral contact problem with a priori unknown contact radius. A specific feature of the method is that the construction of an asymptotic approximation is reduced to a linear algebraic system with respect to integral characteristics (polymoments) of the contact pressure. As an example, the sixth‐order asymptotic model has been written out. Copyright © 2015 John Wiley & Sons, Ltd.     

Note on the homotopy perturbation method for multivariate vector-value oscillatory integrals

This paper considers a homotopy perturbation method for approximating multivariate vector-value highly oscillatory integrals. The asymptotic formulae of the integrals and the asymptotic order of the asymptotic method are presented. Numerical examples show the efficiency of the approximation method.     

Front motion in the parabolic reaction-diffusion problem

A singularly perturbed initial-boundary value problem is considered for a parabolic equation known in applications as the reaction-diffusion equation. An asymptotic expansion of solutions with a moving front is constructed, and an existence theorem for such solutions is proved. The asymptotic expansion is substantiated using the asymptotic method of differential inequalities, which is extended to the class of problems under study. The method is based on well-known comparison theorems and is a development of the idea of using formal asymptotics for the construction of upper and lower solutions in singularly perturbed problems with internal and boundary layers.     

一类二阶微分差分方程边值问题的奇摄动解

本文利用两变量展开直接构造边界层项的方法,讨论了一类二阶微分差分方程边值问题的奇摄动解,构造了形式渐近解,作出了余项估计,从而证明了解的存在性.     

Determining nodes for semilinear parabolic equations

We are concerned with the determination of the asymptotic behavior of strong solutions to the initial-boundary value problem for general semilinear parabolic equations by the asymptotic behavior of these strong solutions on a finite set. More precisely, if the asymptotic behavior of the strong solution is known on a suitable finite set which is called determining nodes, then the asymptotic behavior of the strong solution itself is entirely determined. We prove the above property by the energy method.