关于透镜空间上矢量场的评述

T. Yoshida
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引用次数: 11

摘要

设M为C°-矩阵。M上的(连续)向量场v是M的切束的横截面,而ikί上的&-场是k个向量场vι,•••,vk的集合,使得k个向量v±(x),••-,vk (x)对于每个点x e M是线性无关的。我们用张成(M)表示k的最大个数,其中M允许有一个>场。在这个注释中,我们注意到(2n + L)维模p透镜空间L(p)的张成空间(L(p))部分地由下面的命题给出。设n + l = m2 (m:奇数),(i)如果c = 0,则2t + ll)是单位球面S的商空间S/Γ,通过拓扑变换groupΓ= {1, Γ,•,Γ ~}定义
本文章由计算机程序翻译,如有差异,请以英文原文为准。
A remark on vector fields on lens spaces
Let M be a C°°-manif old. The (continuous) vector field v on M is a crosssection of the tangent bundle of M, and &-field on ikί is a set of k vector fields vι, • ••, vk such that the k vectors v± (x), • •-, vk (x) are linearly independent for each point x e M. We denote by span(M) the maximal number of k where M admits a £>field. In this note, it is remarked that span(L(p)), of the (2n + l)-dimensional mod p lens space L (p), is given partially by the following PROPOSITION. Let n + l = m2 (m: odd), (i) If c = 0, then 2t + l<,span(L(p))<:2t-{-2 (=span(S)). (ii) // c = l, 2, then span(L(p)) = 2t + l (=span (S)). (in) If c = 3, then 2t + l^span(L(p))<,2t + 3 (=span(S)). Here the lens space L(p) (p>l) is the quotient space S/Γ of the unit sphere s by the topological transformation groupΓ= {1, γ, • , γ~} defined by
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