1) affine connection space
仿射联络空间
2) affine connection
仿射联络
1.
Based on first-hand materials, this article mainly focuses on Hermann Weyl s systematical elucidation and significant generalization about Riemann geometry during the year 1917—1923, including the intrinsic definition of affine connection, the foundation of purely infinitesimal geometry, the introduction of projective and conformal structure, and group analysis of the nature of metric space.
在一手文献的基础上 ,重点考察了外尔 1917— 192 3年间对黎曼几何的系统阐述和重大推广 ,包括内蕴地定义仿射联络、建立“纯粹无穷小几何”、引入投影和保形结构 ,以及对“度量本质”的群论分析。
3) affine space
仿射空间
1.
Product structure model based on n-dimensional affine space;
基于n维仿射空间的产品结构模型的研究与应用
2.
We give a new construction of a series of optimal(q~m- 1,q,1)-OOCs through affine space,where q is any prime power and m is any positive integer.
利用仿射空间给出了参数为(q~m-1,q,1)的最优光正交码的构作,其中q为质数幂,m为任意正整数。
3.
Let AG(n , Fq)be an n-dimerensional affine space.
设AG(n,F_q)是一个n维仿射空间。
4) affine subspace
仿射子空间
1.
Construct some affine subspace,which ensures a Boolean function has no annihilator with degree less than n/2(n is even).
通过构造适当的仿射子空间,保证布尔函数不存在低次零化子,得到偶数元最优代数免疫布尔函数的一种构造方法,并对此类函数进行了计数。
5) affine symplectic space
仿射辛空间
1.
Let ASG(2v,F_q)be the 2u-dimensional affine symplectic space over the finite field F_q,let ASp_(2v)(F_q)be the affine symplectic group of degree 2v over F_q,M(m,s)any orbit of(m,s) flats in under ASG(2v,F_q).
设ASU(2v,F_q)是F_q上的2v维仿射辛空间,ASp_(2v)(F_q)是F_q上的2v次仿射辛群,设M(m,s)是ASp_(2v)(F_q)作用下的(m,s)面的轨道,用L(m,s)表示M(m,s)中面的交生成的集合。
6) affine unitary space
仿射酉空间
1.
Let AUG(n,Fq2) be the n-dimensional affine unitary space over the finite field Fq2,let AUn(Fq2) be the affine unitary group of degree n over Fq2.
设AUG(n,Fq2)是Fq2上的n维仿射酉空间,AUn(Fq2)是Fq2上的n次仿射酉群,设M(m,r)是AUn(Fq2)作用下的(m,r)面的轨道。
补充资料：仿射
仿射
affinity
仿射!确nity;呻中Ifu盯er] 仿射变换陌币ne transfo瓜atlon)的简称定义为非退化线性代换 二A派丰“
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参考词条