{"title":"关于透镜空间上矢量场的评述","authors":"T. Yoshida","doi":"10.32917/HMJ/1206139052","DOIUrl":null,"url":null,"abstract":"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","PeriodicalId":17080,"journal":{"name":"Journal of science of the Hiroshima University Ser. A Mathematics, physics, chemistry","volume":"30 1","pages":"13-15"},"PeriodicalIF":0.0000,"publicationDate":"1967-01-01","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":"11","resultStr":"{\"title\":\"A remark on vector fields on lens spaces\",\"authors\":\"T. Yoshida\",\"doi\":\"10.32917/HMJ/1206139052\",\"DOIUrl\":null,\"url\":null,\"abstract\":\"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\",\"PeriodicalId\":17080,\"journal\":{\"name\":\"Journal of science of the Hiroshima University Ser. A Mathematics, physics, chemistry\",\"volume\":\"30 1\",\"pages\":\"13-15\"},\"PeriodicalIF\":0.0000,\"publicationDate\":\"1967-01-01\",\"publicationTypes\":\"Journal Article\",\"fieldsOfStudy\":null,\"isOpenAccess\":false,\"openAccessPdf\":\"\",\"citationCount\":\"11\",\"resultStr\":null,\"platform\":\"Semanticscholar\",\"paperid\":null,\"PeriodicalName\":\"Journal of science of the Hiroshima University Ser. A Mathematics, physics, chemistry\",\"FirstCategoryId\":\"1085\",\"ListUrlMain\":\"https://doi.org/10.32917/HMJ/1206139052\",\"RegionNum\":0,\"RegionCategory\":null,\"ArticlePicture\":[],\"TitleCN\":null,\"AbstractTextCN\":null,\"PMCID\":null,\"EPubDate\":\"\",\"PubModel\":\"\",\"JCR\":\"\",\"JCRName\":\"\",\"Score\":null,\"Total\":0}","platform":"Semanticscholar","paperid":null,"PeriodicalName":"Journal of science of the Hiroshima University Ser. A Mathematics, physics, chemistry","FirstCategoryId":"1085","ListUrlMain":"https://doi.org/10.32917/HMJ/1206139052","RegionNum":0,"RegionCategory":null,"ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":null,"EPubDate":"","PubModel":"","JCR":"","JCRName":"","Score":null,"Total":0}
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
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