ON THE GROWTH OF SOLUTIONS OF A CLASS OF HIGHER ORDER DIFFERENTIAL EQUATIONS

In this paper, authors investigate the order of growth and the hyper order of solutions of a class of the higher order linear differential equation, and improve results of M. Ozawa^[6], G. Gundersen^[7] and J.K. Langley^[8], Li Chun-hong^[11].     

sl玻色子体系在U(2l+1)O(2l+2)过渡区的严格解

利用无穷维李代数方法得到了相互作用sl玻色子体系在U( 2l+ 1 ) O( 2l+ 2 )过渡区的能谱和波函数的严格解 .给出了该系统Bethe假定方程的数值解法 .     

Dromion and Multi—soliton Structures of the （2＋1）—Dimensional Higher—Order Broer—Kaup System

Using the standard truncated Painleve analysis and the Backlund transformation,we can obtain many significant exact soliton solutions of the (2 1)-dimensional higher-order Broer-Kaup(HBK) system.A special type of soliton solution is described by the variable coefficient heat-conduction-liker equation.The inclusion of three arbitrary functions in the general expressions of the solitons makes the solitons of the (2 1)-dimensional HBK system possess abundant structures such as solitoff solutions,multi-dromion solutions,ring solitons and so on.     

Erds方程的全等解

本文运用初等方法给出了Erds方程的所有全等解.     

关于矩阵方程AXB=C

关于矩阵方程ＡＸＢ＝Ｃ丁永臻（胜利油田师专数学系２５７０９７）文［１］给出了矩阵方程ＡＸＢ＝Ｃ有解和有唯一解的一个充要条件．本文借助于近代数学常用的矩阵广义逆、直积和拉直化运算的概念及性质详细讨论矩阵方程ＡＸＢ＝Ｃ解的一般理论，包括解的存在性、唯一性...     

二阶强次线性常微分方程解的振动性

本文讨论二阶非线性常微分方程 (a(t)ψ(x(t))x’(t))’+q(t)f(x(t))g(x’(t))=0 (1)的解的振动性质。在方程(1)中,α∈C[[t_0,∞),(0,∞)],ψ∈C[R,(0,∞)](R=(-∞,+∞)),q∈C[[t_0,∞),[0,∞)]且在任意的区间(t,∞)(t≥t_0)上不恒等于0,f∈C’[R,R],g∈C[R,R]。关于微分方程振动性的定义,如通常定义,不再详述。在下面的定理中,以下条件将要用到:     

SOLUTIONS OF THE EQUATION x^m＋y^m=z^m IN SL2z

This paper solves an open problem of Vaserstein. The main result is: the equation x^m y^m=z^m has a solution in SL2z if and only if m is not divisible by 4 or 6 and m is not congruent to 3 modulo 6.     

关于一类常微分方程亚纯解的个数的注记

本文讨论微分方程u′=sum from k=0 P_k(z)u~k (1)在某些条件下亚纯解的个数问题。得到定理1、2,它们分别是[1]定理1、2的推广。     

BIN PACKING中γm≤1.20的直接证明

ＢＩＮＰＡＣＫＩＮＧ中γ_ｍ≤１．２０的直接证明刘明堂，越民义（中国科学院应用数学研究所，北京１０００８０）ＡＤＩＲＥＣＴＰＲＯＯＦＯＦＴＨＥＩＮＥＱＵＡＬＩＴＹγ_ｍ≤１．２０ＩＮＭＵＬＴＩＰＲＯＣＥＳＳＯＲＳＣＨＥＤＵＬＩＮＧ￥ＬＩＵＭＩＮＧＴＡＮ...     

半线性抛物型方程初边值问题解的性态

1.引言对于半线性抛物型议程的初边值问题■解的性质有许多作者进行了讨论,设λ_0是-T(D(x)T)所对应的最小特征值,φ(x)为对应的特征函数,则λ_0>0,且可取φ(x)>0,x∈Ω它们是如下问题的解