群对称桁架振动设计的半正定模型与降维问题(英)

桁架振动优化设计可描述为：在给定振动系统最低频率的约束条件下,设计用材最省的桁架结构. 本文针对具有某种结构对称性的桁架,利用有限群描述这一特性,在已有桁架设计的半正定规划模型基 础上,运用最近提出的矩阵代数方法对半正定规划问题的决策变量和数据进行降维,给出了构造有限群 表示的两个充分条件,并实现了一类群对称桁架振动优化设计的半正定模型降维.基于问题的实际背景, 我们又考虑了一个具有八根弹性棒的桁架设计实例,进一步说明在实际问题中根据群对称构造群表示以 及对应不可约表示的具体方法.     

四元Heisenberg群上次拉普拉斯算子的m幂次的基本解

本文研究了四元Heisenberg群上次拉普拉斯算子的m幂次的基本解，该结论是Heisenberg群上结果的推广.本文利用了四元Heisenberg群上的Fourier变换理论构造了该群上次拉普拉斯算子的m幂次的基本解，并且给出了基本解的积分表示.     

四元Heisenberg群上次拉普拉斯算子的m幂次的基本解

本文研究了四元Heisenberg群上次拉普拉斯算子的m幂次的基本解,该结论是Heisenberg群上结果的推广.本文利用了四元Heisenberg群上的Fourier变换理论构造了该群上次拉普拉斯算子的m幂次的基本解,并且给出了基本解的积分表示.     

有限群的一个类函数的模构造

本文研究了有限群上的一个类函数.通过计算它和不可约特征标的内积,证明了它是特征标并且通过复群代数的中心的正则表示给出了它的一个模构造.     

非均匀材料细观结构的定向分布函数（I）—定向分布函数和不可约张量

在最近研究非均匀材料的物理和力学性质的各种基于细观力学的方法中,定向分布函数（ODF）和晶体定向分布函数（CODF）的概念起着重要的作用,它们分别定义在单位球面和旋转群上,本文通过两部分的内空,具有不可约张量系数的傅立叶展开对它们分别作了深入的研究,群表示理论指出平面可积的定向分布函数可以展开为球谐数的绝对收敛的傅立叶级数,而其中的球谐函数又能进一步用不可约张量表示,这样一些不可约张一系数的基本重要性在于它们刻划了材料组元和缺陷的体积,形状,相,位置的宏观或全局影响,第（I)部分对定义在N维单位球上的定向分布函数的不可约张量Fourier展开了一般性质进行了研究,其中重点是构造二维和三维不可约张量的简单表示,以便于得到它们在各种点群（完全正交群的子群）对称性的约束形式,第（II）部分给出了晶体定向分布数的不可约张量展开的显式表示,产工且给出了不可约张量以及定向分布函数的晶体定向分布数不可约张量展开在各种点群下的约束形式。     

非均匀材料细观结构的定向分布函数(Ⅰ)--定向分布函数和不可约张量

在最近研究非均匀材料的物理和力学性质的各种基于细观力学的方法中, 定向分布函数(ODF)和晶体定向分布函数(CODF)的概念起着重要的作用, 它们分别定义在单位球面和旋转群上A *D2本文通过两部分的内容, 用具有不可约张量系数的傅立叶展开对它们分别作了深入的研究A *D2群表示理论指出平方可积的定向分布函数可以展开为球谐函数的绝对收敛的傅立叶级数,而其中的球谐函数又能进一步用不可约张量表示A *D2这样一些不可约张量系数的基本重要性在于它们刻划了材料组元和缺陷的体积、形状、相、位置的宏观或全局影响A *D2第(Ⅰ)部分对定义在N维单位球上的定向分布函数的不可约张量Fourier展开的一般性质进行了研究,其中重点是构造二维和三维不可约张量的简单表示,以便于得到它们在各种点群(完全正交群的子群)对称性的约束形式;第(Ⅱ)部分给出了晶体定向分布函数的不可约张量展开的显式表示,并且给出了不可约张量以及定向分布函数和晶体定向分布函数不可约张量展开在各种点群下的约束形式A *D2     

不可约张量方法与分子结构(Ⅱ)——不可约张量算子矩阵元的计算

本文对文献[1]中的三条群链给出了必要的群间偶合系数(Isoscalar factor)的解析表达式;讨论了文献[1]中所定义的各种不可约张量算子对相应的群链基矢的矩阵元的计算,把描述单体力所需的偶合张量算子和描述二体力所需的四重偶合张量算子约化矩阵元的计算归结于基本张量算子矩阵元的计算,对各种张量算子矩阵元给出了统一表达式。     

在某些正则区域上的多元B形式曲面

本文首先通过在多面体区域上抬高维数的技巧给出了多元Ｂ形式中曲面的一般性定义．由此我们构造了平行四边形域上、正六边形域上和正八边形成上Ｂ形式的同次曲面格式，并给出了其基函数的递推公式和求导公式．同时我们也给出了正六边形域上插值角点的Ｂ形式同次曲面的表示式．     

非负不可约矩阵的广义Perron补矩阵

1989年Meyor为计算马尔可夫链的平稳分布向量构造了一个算法，首次提出非负不可约矩阵的Perron补矩阵的概念，本给出非负不可约矩阵A的广义Perron补矩阵若干性质，并且证明若矩阵A是不可约逆M-矩阵，其广义Perron补矩阵也是不可约逆M-矩阵。     

辫子群的全部二维不可约表示

通过直接解矩阵方程给出了Bn群的全部二维不可约表示．     

The Hurwitz determinants and the signatures of irreducible representations of simple real Lie algebras

The paper deals with the real classical Lie algebras and their finite dimensional irreducible representations. Signature formulae for Hermitian forms invariant relative to these representations are considered. It is possible to associate with the irreducible representation a Hurwitz matrix of special kind. So the calculation of the signatures is reduced to the calculation of Hurwitz determinants. Hence it is possible to use the Routh algorithm for the calculation.     

Schur Orthogonality Relations for the Finitary Infinite Symmetric Group

Let S f be the finitary infinite symmetric group. For a certain class of irreducible unitary representations of S f , a version of Schur orthogonality relations is proved. That is, we construct an invariant inner product on the matrix coefficient space of each representation and show that matrix coefficients for distinct representations are orthogonal with respect to these norms.     

Schur Orthogonality Relations for the Finitary Infinite Symmetric Group

Let S f be the finitary infinite symmetric group. For a certain class of irreducible unitary representations of S f , a version of Schur orthogonality relations is proved. That is, we construct an invariant inner product on the matrix coefficient space of each representation and show that matrix coefficients for distinct representations are orthogonal with respect to these norms.     

Cuntz-Krieger algebras representations from orbits of interval maps

Let f be an expansive Markov interval map with finite transition matrix Af. Then for every point, we yield an irreducible representation of the Cuntz-Krieger algebra OAf and show that two such representations are unitarily equivalent if and only if the points belong to the same generalized orbit. The restriction of each representation to the gauge part of OAf is decomposed into irreducible representations, according to the decomposition of the orbit.     

A geometrical approach to maximizing a variance

The matrix form for the variance of n independently chosen real numbers, x₁, x₂,…, x_n, is observed to be the same as that for the potential energy matrix for n coupled oscillators symmetrically arranged on a circle. Unitary matrices that have previously been developed from the irreducible representations of the circular symmetries to diagonalize the potential energy matrices are given. These transformations are applied to the variance.

A geometric setting is provided for the transformations, and the maximum variance is found for real numbers x_i subject to linear constraints on the choices of the numbers.     

Weyl–Pedersen calculus for some semidirect products of nilpotent Lie groups

For certain nilpotent real Lie groups constructed as semidirect products, algebras of invariant differential operators on some coadjoint orbits are used in the study of boundedness properties of the Weyl–Pedersen calculus of their corresponding unitary irreducible representations. Our main result is applicable to all unitary irreducible representations of arbitrary 3-step nilpotent Lie groups.     

Gaussian fluctuations of characters of symmetric groups and of Young diagrams

We study asymptotics of reducible representations of the symmetric groups S _q for large q. We decompose such a representation as a sum of irreducible components (or, alternatively, Young diagrams) and we ask what is the character of a randomly chosen component (or, what is the shape of a randomly chosen Young diagram). Our main result is that for a large class of representations the fluctuations of characters (and fluctuations of the shape of the Young diagrams) are asymptotically Gaussian; in this way we generalize Kerov's central limit theorem. The considered class consists of representations for which the characters almost factorize and this class includes, for example, the left-regular representation (Plancherel measure), irreducible representations and tensor representations. This class is also closed under induction, restriction, outer product and tensor product of representations. Our main tool in the proof is the method of genus expansion, well known from the random matrix theory.     

Spectral Properties of Second Order Differential Operators on Two-step Nilpotent Lie Groups

In this paper, spectral properties of certain left invariant differential operators on two-step nilpotent Lie groups are completely described by using the theory of unitary irreducible representations and the Plancherel formulae on nilpotent Lie groups.     

Polynomial representations of the orthogonal groups

This paper is concerned with realizations of the irreducible representations of the orthogonal group and construction of specific bases for the representation spaces. As is well known, Weyl's branching theorem for the orthogonal group provides a labeling for such bases, called Gelfand-Žetlin labels. However, it is a difficult problem to realize these representations in a way that gives explicit orthogonal bases indexed by these Gelfand-–etlin labels. Thus, in this paper the irreducible representations of the orthogonal group are realized in spaces of polynomial functions over the general linear groups and equipped with an invariant differentiation inner product, and the Gelfand-Žetlin bases in these spaces are constructed explicitly. The algorithm for computing these polynomial bases is illustrated by a number of examples. Partially supported by a grant from the Department of Energy. Partially supported by NSF grant No. MCS81-02345.