{"title":"对某个$G$结构的评论","authors":"T. Nasu","doi":"10.32917/hmj/1206139239","DOIUrl":null,"url":null,"abstract":"Since the notion of G-struetures on a differentiable manifold M was introduced by S. S. Chern [2] ( 1 ) in 1953, a number of papers on this subject have been published by many writers, such as D. Bernard, R. S. Clark and M. Bruckheimer. Many structures which appear in differential geometry are closely related to the G-structures defined by certain special tensor fields whose components relative to some covering of M by moving frames are constants. Especially, among the G-structures defined by special vector 1-forms one finds the almost product, the almost complex and the almost tangent structures, etc.. As is well known, for such a G-structure we can define two tensors, that is, the Chern invariant and the Nijenhuis tensor. These two tensors play an impotant role in the theory of connections and the integrability of the Gstructures. So far, however, we have known of the relation between them only in some special cases. For example, the Chern invariant vanishes if and only if the Nijenhuis tensor vanishes for almost product, almost complex and almost tangent structures [3]. The main purpose of this paper is to investigate how such a relation will be generalized in the case of the real G-structure defined by any special vector 1-form whose eigenvalues are all real. As usual, we assume that all the objects we encounter in this paper are of class C°°.","PeriodicalId":17080,"journal":{"name":"Journal of science of the Hiroshima University Ser. A Mathematics, physics, chemistry","volume":"14 1","pages":"253-270"},"PeriodicalIF":0.0000,"publicationDate":"1965-01-01","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":"0","resultStr":"{\"title\":\"A remark on a certain $G$-structure\",\"authors\":\"T. Nasu\",\"doi\":\"10.32917/hmj/1206139239\",\"DOIUrl\":null,\"url\":null,\"abstract\":\"Since the notion of G-struetures on a differentiable manifold M was introduced by S. S. Chern [2] ( 1 ) in 1953, a number of papers on this subject have been published by many writers, such as D. Bernard, R. S. Clark and M. Bruckheimer. Many structures which appear in differential geometry are closely related to the G-structures defined by certain special tensor fields whose components relative to some covering of M by moving frames are constants. Especially, among the G-structures defined by special vector 1-forms one finds the almost product, the almost complex and the almost tangent structures, etc.. As is well known, for such a G-structure we can define two tensors, that is, the Chern invariant and the Nijenhuis tensor. These two tensors play an impotant role in the theory of connections and the integrability of the Gstructures. So far, however, we have known of the relation between them only in some special cases. For example, the Chern invariant vanishes if and only if the Nijenhuis tensor vanishes for almost product, almost complex and almost tangent structures [3]. The main purpose of this paper is to investigate how such a relation will be generalized in the case of the real G-structure defined by any special vector 1-form whose eigenvalues are all real. As usual, we assume that all the objects we encounter in this paper are of class C°°.\",\"PeriodicalId\":17080,\"journal\":{\"name\":\"Journal of science of the Hiroshima University Ser. A Mathematics, physics, chemistry\",\"volume\":\"14 1\",\"pages\":\"253-270\"},\"PeriodicalIF\":0.0000,\"publicationDate\":\"1965-01-01\",\"publicationTypes\":\"Journal Article\",\"fieldsOfStudy\":null,\"isOpenAccess\":false,\"openAccessPdf\":\"\",\"citationCount\":\"0\",\"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/1206139239\",\"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/1206139239","RegionNum":0,"RegionCategory":null,"ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":null,"EPubDate":"","PubModel":"","JCR":"","JCRName":"","Score":null,"Total":0}
引用次数: 0
摘要
自1953年S. S. Chern bbb(1)提出可微流形M上g结构的概念以来,许多作者如D. Bernard, R. S. Clark和M. Bruckheimer发表了许多关于这一主题的论文。微分几何中出现的许多结构与由某些特殊张量场定义的g结构密切相关,这些张量场的分量相对于运动坐标系对M的某些覆盖是常数。特别地,在由特殊向量1形式定义的g结构中,我们发现了几乎积、几乎复和几乎切结构等。众所周知,对于这样一个g结构,我们可以定义两个张量,即Chern不变量和Nijenhuis张量。这两个张量在连接理论和g结构的可积性中起着重要的作用。然而,到目前为止,我们只在一些特殊的情况下才知道它们之间的关系。例如,当且仅当Nijenhuis张量对于几乎积,几乎复和几乎切结构[3]消失时,Chern不变量消失。本文的主要目的是研究由特征值全为实数的特殊向量1-形式所定义的实数g结构如何推广这一关系。像往常一样,我们假设本文中遇到的所有物体都是C°°类。
Since the notion of G-struetures on a differentiable manifold M was introduced by S. S. Chern [2] ( 1 ) in 1953, a number of papers on this subject have been published by many writers, such as D. Bernard, R. S. Clark and M. Bruckheimer. Many structures which appear in differential geometry are closely related to the G-structures defined by certain special tensor fields whose components relative to some covering of M by moving frames are constants. Especially, among the G-structures defined by special vector 1-forms one finds the almost product, the almost complex and the almost tangent structures, etc.. As is well known, for such a G-structure we can define two tensors, that is, the Chern invariant and the Nijenhuis tensor. These two tensors play an impotant role in the theory of connections and the integrability of the Gstructures. So far, however, we have known of the relation between them only in some special cases. For example, the Chern invariant vanishes if and only if the Nijenhuis tensor vanishes for almost product, almost complex and almost tangent structures [3]. The main purpose of this paper is to investigate how such a relation will be generalized in the case of the real G-structure defined by any special vector 1-form whose eigenvalues are all real. As usual, we assume that all the objects we encounter in this paper are of class C°°.