Banach空间的正规结构与对径点

假设S（X）是Banach空间X的单位球面,作引进了四个新的几何参数：Jε（X）=sup{βε（x）,x∈S（X）},jε（X）=inf{βε（x）,x∈S（X）},Gε（X）=sup{αε（x）,x∈S（X）},gε（X）=inf{αε（x）,x∈S（S）},其中≤ε≤1,βε（x）=sup{min{‖x εy‖,‖x-εy‖,y∈S（X）}},αε（x）=inf{max{‖x εy‖,‖x-εy‖,y∈S（X）}},讨论了这些参数的性质,本主要结果是：如果主要结果是：如果有一个ε,0≤ε≤1,使得Jε（X）＜1 ε/2或gε（X）＞1 ε/3,那末X有一至正规结构。     

条件弱鞅的一类极小值不等式

本文研究了(非负)条件弱鞅的极小值不等式,将相关文献中关于非负条件弱鞅的形如εP~F(min1≤i≤n c_i S_i≤ε)的极小值不等式推广到εP~F(min1≤i≤n c_ig(S_i)≤ε)的情形下,此外,本文还给出了条件弱鞅的形如εP~F(min1≤i≤n g(S_i)≤ε)和εP~F(min1≤i≤n g(S_i)≤-ε)的极小值不等式.     

对流扩散问题流线扩散法的最优误差估计

在本文中,我们考虑对流占优扩散问题流线扩散双线性有限元方法。原先的文献在ε≤h~2的条件下,得到了L~2-模最优误差估计,而本文则在ε≤h的条件下得到了相同估计。     

算术级数中的奇数Goldbach问题(Ⅱ)

本文考察了几乎所有模的算术级数中的奇数Goldbach问题．证明了对几乎所有的模r≤N1/6-ε,充分大的正奇数N可表为三个素数之和,其中每个素数取在模r 的满足必要同余条件的任意剩余系中．     

拟绝对-*-κ-仿正规算子的谱性质

引入了拟绝对-*-k-仿正规算子,获得了拟绝对-*-k-仿正规算子的一个充要条件.并证明了拟绝对-*-k-仿正规算子在0≤k≤1上是有限上升的,作为此性质的应用,证明了若T是拟绝对-*-k-仿正规算子,其中0≤k≤1,则Weyl谱和本质近似点谱的谱映射定理成立.最后证明了若T是拟绝对-*-k-仿正规算子,其中0≤k≤1,则σ_(ja)(T)\{0}=σ_a(T)\{0}.     

On the Equation n_1n_2= n_3n_4 Restricted to Factor Closed Sets

We study the number of solutions N(B,F) of the diophantine equation n_1n_2 = n_3 n_4,where 1 ≤ n_1 ≤ B,1 ≤ n_3 ≤ B,n_2,n_4 ∈ F and F[1,B] is a factor closed set.We study more particularly the case when F={m = p_1~(ε1)···p_k~(εk),ε_j∈{0,1},1 ≤ j ≤ k},p_1,...,p_k being distinct prime numbers.     

常差分方程奇异摄动问题的渐近方法

在本文中,我们讨论如下差分方程问题(P_ε):(L.y)_k≡εy(k+1)+a(k,ε)y(k)+b(k,ε)y(k-1)=f(k,ε)(1≤k≤N-1)B₁y≡-y(0)+c₁y(1)=a,B₂y≡-c₂y(N-1)+y(N)=β这里ε是一个小参数,c₁,c₂,a,β为常数,a(k,ε),b(k,ε),f(k,ε)(1≤k≤N)是k和ε的函数.首先,我们讨论了常系数的情形;接着引进伸长变换对变系数的情形进行了讨论,给出了解的一致渐近展开式;最后给出了一个数值例子.     

长时间相依游动的分形性质

给定ε=(εi)j≥1∈{-1,+1}∞,考虑两种长时间游动和Qn(ε)=,0＜α≤1.我们得到了{Pn(ε)～bna}和{Qn(ε)～bna}的Hausdorff维数.     

关于微分差分方程的边值问题

本文考虑含小参数ε>0且自变量具有固定时滞1的微分差分方程边值问题(?)其中L[y(x,ε)]=εy″(x,ε)-a(x,ε)y′(x,ε)-b(x,ε)y(x,ε),R[y(x,ε)]=A(x,ε)y′(x-1,ε)+B(x,ε)y(x-1,ε)+f(x,ε),T 是一正数,10下讨论了边值问题解的存在性、唯一性和区间-1≤x≤T 上当ε→0~+时解的一致有效估计.     

关于Pell方程组x2-(m2-1)y2=z2-(n2-1)y2=1

设m,n,L为正整数,本文证明了:如果mε,ε∈(0,1),且m>(123789LL(1/2))⁽1/(1-ε)),或j>10.25×10¹²log⁴(2(L+1)(123789LL(1/2))⁽1/(1-ε))),Pell方程组x²-(m2-1)y²=z²-(n²-1)y²=1的正整数解满足1≤k≤δL²,这里δ∈[1/2(123787LL(1/2))⁽1/(ε-1)),1],以及■且j=k=1或k+2≤j<1/3(5-2ε)k,2|(j+k),k>3/(1-ε),并改进了文[Proc.Amer.Math.Soc.,2015,143(11):4685-4693]的结果.     

RECENT PROGRESS ON SPHERICAL HARMONIC APPROXIMATION MADE BY BNU RESEARCH GROUP ——In memory of Professor Sun Yongsheng

As early as in 1990, Professor Sun Yongsheng, suggested his students at Beijing Normal University to consider research problems on the unit sphere. Under his guidance and encouragement his students started the research on spherical harmonic analysis and approximation. In this paper, we incompletely introduce the main achievements in this area obtained by our group and relative researchers during recent 5 years （2001-2005）. The main topics are： convergence of Cesaro summability, a.e. and strong summability of Fourier-Laplace series; smoothness and K-functionals; Kolmogorov and linear widths.     

On a class of self-similar processes with stationary increments in higher order Wiener chaoses

We study a class of self-similar processes with stationary increments belonging to higher order Wiener chaoses which are similar to Hermite processes. We obtain an almost sure wavelet-like expansion of these processes. This allows us to compute the pointwise and local Hölder regularity of sample paths and to analyse their behaviour at infinity. We also provide some results on the Hausdorff dimension of the range and graphs of multidimensional anisotropic self-similar processes with stationary increments defined by multiple Wiener–Itô integrals.     

On a class of Riemann surfaces

It is considered the class of Riemann surfaces with dimT1 = 0, where T1 is a subclass of exact harmonic forms which is one of the factors in the orthogonal decomposition of the spaceΩH of harmonic forms of the surface, namely The surfaces in the class OHD and the class of planar surfaces satisfy dimT1 = 0. A.Pfluger posed the question whether there might exist other surfaces outside those two classes. Here it is shown that in the case of finite genus g, we should look for a surface S with dimT1 = 0 among the surfaces of the form Sg\K , where Sg is a closed surface of genus g and K a compact set of positive harmonic measure with perfect components and very irregular boundary.     

A REPRESENTATION FORMULA RELATED TO SCHR(O)DINGER OPERATORS

Schr(o)dinger operator is a central subject in the mathematical study of quantum mechanics.Consider the Schrodinger operator H = -△ V on R, where △ = d2/dx2 and the potential function V is real valued. In Fourier analysis, it is well-known that a square integrable function admits an expansion with exponentials as eigenfunctions of -△. A natural conjecture is that an L2 function admits a similar expansion in terms of "eigenfunctions" of H, a perturbation of the Laplacian (see [7], Ch. Ⅺ and the notes), under certain condition on V.     

Boundedness for commutators of multipliers on Hardy type spaces

In this paper, we study the commutators generalized by multipliers and a BMO function. Under some assumptions, we establish its boundedness properties from certain atomic Hardy space Hb^p（R^n） into the Lebesgue space L^p with p 〈 1.     

A unified approach to certain problems of best local approximation

In this paper we study best local quasi-rational approximation and best local approximation from finite dimensional subspaces of vectorial functions of several variables. Our approach extends and unifies several problems concerning best local multi-point approximation in different norms.     

THE 8~(th) INTERNATIONAL CONGRESS ON INDUSTRIAL AND APPLIED MATHEMATICS

<正>August 10-14,2015Beijing,ChinaThe International Congress on Industrial and Applied Mathematics(ICIAM)is the premier international congress in the field of applied mathematics held every four years under the auspices of the International Council for Industrial and Applied Mathematics.From August 10 to 14,2015,mathematicians,scientists     

Towards Excellence in Science Chinese Academy of Sciences

<正>May 26,2014,Beijing Science is a human enterprise in the pursuit of knowledge.The scientific revolution that occurred in the 17th Century initiated the advances of modern science.The scientific knowledge system created by