迹非零布尔矩阵幂敛指数的极阵刻画

设Ｄｎ（ｄ）是恰含ｄ个非零对角元的ｎ阶布矩阵的集合，１≤ｄ≤ｎ本文完全刻画了Ｄｎ（ｄ）中幂敛指数达到最大值的极矩阵，从而解决了迹非零尔矩阵幂敛指数的极阵刻问题。     

迹非零的布尔矩阵的幂敛指数

本文证明ｄ个正对角元的ｎ阶布尔方阵（１≤ｄ＜ｎ／２）幂敛指数有上界（ｎ－ｄ－１）＾２＋１，ｎ＞４，并给出了幂敛指数达到此上界的这类方阵的完全刻画，由此，即得ｎ阶非零迹布尔方阵幂敛指数的最大值为（ｎ－２）＾２＋１。     

对称本原矩阵指数集的刻画

设Ｓｎ表示由全体ｎ阶对称本原（０，１）－矩所构成的集合，并设Ｓ（ｎ，ｄ）＝｛Ａ∈Ｓｎ│Ａ的伴随有向图中的最小奇圈之长为ｄ≥１｝。本文证明了：Ｓ（ｎ，ｄ）的本原指数集为｛ｄ－１，ｄ，…，２ｎ－ｄ－１｝＼Ｄ，其中Ｄ为｛ｎ－ｄ＋１，ｎ－ｄ＋２，…，２ｎ－ｄ－２｝中的所有奇数与０之并集，同时，我们也给出了Ｓ（ｎ，ｄ）中指数达到上界的矩阵集合的完全刻画。     

对有理指数幂的一点讨论

文[1]、[2]对分数指数幂的定义域提出了两种截然不同的观点，究其原因在于对与当α＜0时之间关系的理解差异．本文将在这方面作进一步探讨，从而给出（m、n为自然数）的定义域．1根式与分数指数幂的关系根式与分数指数幂的关系为：其中m、n为自然数，n＞1．当n为偶数，m为奇数时，其它情形αR．（i）若n为奇数，则（ii）若n、m都为偶数，则（iii）若n为偶数，m为奇数，则此时a≥0，（1）式显然成立．利用（1）式及根式的性质可以定义底非负的正分数指数幂卜十一（sgn。）"X于一yi7i'－－－，并推出其性质．2底为实数的正有理指数幂定义定义…     

布尔矩阵的幂敛指数集

给出了不含非零对角元的ｎ阶布尔矩阵的幂敛指数集的明显表达式,从而完全解决了布尔矩阵依赖于非零对角元个数的幂敛指数集的刻画问题。     

具有给定指数的本原有向图的Hamilton性质

本文解决了１９８２年Ｊ．Ａ．Ｒｏｓｓ提出的两个问题,并得到如下结果：（１）设Ｄ是具有围长ｓ＞１和指数γ（Ｄ）＝ｎ＋ｓ（ｎ－２）的ｎ阶本原有向图,则Ｄ是Ｈａｍｉｌｔｏｎ的;（２）设Ｄ是含有环的ｎ阶本原有向图且γ（Ｄ）＝２ｎ－２,则Ｄ是Ｈａｍｉｌｔｏｎ的当且仅当ｍａｘ｛ｄ（ｕ,ｖ）|γ（ｕ,ｖ）＝２ｎ－２｝＝ｎ－２．     

关于《矩阵正定性的进一步推广》一文的注记

关于《矩阵正定性的进一步推广》一文的注记黎奇升（湖南吉首大学数学系，吉首４１６０００）文［１］给出了下面定义并讨论了它们的一些性质．定义　设Ａ∈Ｒ￣（ｎ×ｎ），若对任何０≠Ｘ∈Ｒ￣（ｎ×１），都有正定矩阵Ｓ＝Ｓｘ，使Ｘ￣ＴＳｘＡＸ＞０，则称Ａ为广义正...     

高阶非线性差分方程的振动性

本文研究了差分方程△ｄｘ（ｎ）＋ｐ（ｎ）△（ｄ－１）ｘ（ｎ）＋Ｈ（ｎ，ｘ（ｎ））＝０，（１．１）△ｄｘ（ｎ）＋ｐ（ｎ）△（ｄ－１）ｘ（ｎ，ｘ（ｎ））＝Ｑ（ｎ）．（１．２）在一定的条件下，证明了方程（１．１）与（１．２）在振动性方面的等价问题．对于方程（１．１）或（１．２），在ｎ是偶数时的每一个有界解是振动的，在ｎ是奇数时，每一个有界解是振动的或当→∞时单调趋于零的充要性定理也建立了．     

关于矩阵迹的平均不等式

关于矩阵迹的平均不等式黄礼平（湘潭矿业学院基础课部４１１２０１）近年来，对矩阵迹的不等式研究活跃，本文给出两个矩阵迹的平均不等式．定理１设Ａ，Ｂ，Ｃ均为ｎ阶半正定Ｈｅｒｍｉｔｅ矩阵，则特别，我们有推论１设Ａ，Ｂ，Ｃ均为ｎ阶正定实对称矩阵，则诸等号当且...     

有理数目标检测题(二)

一、填空１．ａ－１（ａ－１≠０）的相反数是,倒数是．２．如果ｎ为自然数,那么ｎ,１ｎ,－ｎ的大小关系．（从大到小）３．大于或等于－１０且小于１１的所有整数的和是．４．若｜ｘ＋３｜与（ｙ－３）２互为相反数,则３ｘ＋５ｙ＝．５．计算（－４）５×（１４）５＝．６．若３９２０００００＝３．９２×１０ｍ,近似数０．６０８０有ｎ个有效数字,则５ｍ＋２ｎ＝．７．若｜ｘ｜＝３,｜ｙ｜＝４,且ｘ＞ｙ,则３ｘ－２ｙ的值是．８．计算－３２＋（－２）３÷（－１）５＝．９．计算８×（－０．７５）２－２４×（－１６）３÷（…     

三次幻方的构作

给出2k维m阶t次幻方及m模方阵,m模列满秩矩阵,模线,m经典模线集和t次m模基因阵的概念,并用矩阵法和组合法初步研究了t次幻方特别是三次幻方的构作.证明:(i)若存在2k阶t次m模基因阵,则存在2k维m阶t次幻方;(ii)若N=P1α1P2α2…PSαS为N的标准分解式,iα≥3,Piiα≥16(1≤i≤S),则存在二维N阶三次幻方;(iii)若存在二维偶m阶2t+1次幻方和二维n阶2t次幻方,则存在二维mn阶2t+1次幻方;(iv)若存在二维m阶和n阶t次幻方,则存在二维mn阶t次幻方;(v)当t≥3时,不存在二维单偶数阶t次幻方.     

Computation of the Newton step for the even and odd characteristic polynomials of a symmetric positive definite Toeplitz matrix

We compute the Newton step for the characteristic polynomial and for the even and odd characteristic polynomials of a symmetric positive definite Toeplitz matrix as the reciprocal of the trace of an appropriate matrix. We show that, after the Yule-Walker equations are solved, this trace can be computed in additional arithmetic operations, which is in contrast to existing methods, which rely on a recursion, requiring additional arithmetic operations.

     

关于Diophantine 方程xn+2kyn=pz2

设p 为奇素数且对任意的整数m, d, p≠(2^m±1)=/d², 则对任意的素数n > p^8p2, 方程xⁿ+2^kyⁿ=pz², k≥2 没有整数解(x, y, z) 使得x, y, z 两两互素且均不为0.     

Solution of Scott's Problem on the Number of Directions Determined by a Point Set in 3-Space

Let P be a set of n points in R³, not all in a common plane. We solve a problem of Scott (1970) by showing that the connecting lines of P assume at least 2n - 5 different directions if n is odd and at least 2n - 7 if n is even. The bound for odd n is sharp.     

Stability of the Kolmogorov flow and its modifications

Recurrence formulas are obtained for the kth term of the long wavelength asymptotics in the stability problem for general two-dimensional viscous incompressible shear flows. It is shown that the eigenvalues of the linear eigenvalue problem are odd functions of the wave number, while the critical values of viscosity are even functions. If the velocity averaged over the long period is nonzero, then the loss of stability is oscillatory. If the averaged velocity is zero, then the loss of stability can be monotone or oscillatory. If the deviation of the velocity from its period-average value is an odd function of spatial variable about some x ₀, then the expansion coefficients of the velocity perturbations are even functions about x ₀ for even powers of the wave number and odd functions about for x ₀ odd powers of the wave number, while the expansion coefficients of the pressure perturbations have an opposite property. In this case, the eigenvalues can be found precisely. As a result, the monotone loss of stability in the Kolmogorov flow can be substantiated by a method other than those available in the literature.     

关于奇算术图

本文讨论了$n$个$m$长圈有一个公共结点图$C^n_m$, $n$个$m$长圈与$t$长路有一个公共结点图$C^n_m\cdot P_t$, $n$个$m$阶完全图有一个公共结点图$K^n_m$和星形图的同胚图的奇算术性问题.给出了完全图,完全二部图和圈是奇算术的充要条件.     

Remarks on Fourier series

We prove the following propositions. An even integrable function whose Fourier coefficients form a convex sequence is absolutely continuous if and only if its Fourier series converges absolutely. If the function f(t)is convex on [0, ],f(t)=f(—t), then for odd n while for even n, b₀=0.Translated from Matematicheskie Zametki, Vol. 3, No. 5, pp. 597–604, May, 1968.     

On weights in duadic abelian codes

In this note, we prove that if C is a duadic binary abelian code with splitting μ=μ₋₁ and the minimum odd weight of C satisfies d²−d+1≠n, then d(d−1)n+11. We show by an example that this bound is sharp. A series of open problems on this subject are proposed.     

Remarks on the critical graph conjecture

The vertex-critical graph conjecture (critical graph conjecture respectively) states that every vertex-critical (critical) graph has an odd number of vertices. In this note we prove that if G is a critical graph of even order, then G has at least three vertices of less-than-maximum valency. In addition, if G is a 3-critical multigraph of smallest even order, then G is simple and has no triangles.