{"title":"几何","authors":"Michael Potter","doi":"10.4324/9781315776187-25","DOIUrl":null,"url":null,"abstract":": We study the noncommutative Riemannian geometry of the alternating group A 4 = ( Z 2 × Z 2 ) >⊳ Z 3 using the recent formulation for finite groups in [2]. We find a unique ‘Levi-Civita’ connection for the invariant metric, and find that it has Ricci-flat but nonzero Riemann curvature. We show that it is the unique Ricci-flat connection on A 4 with the standard framing (we solve the vacuum Einstein’s equation). We also propose a natural Dirac operator for the associated spin connection and solve the Dirac equation. Some of our results hold for any finite group equipped with a cyclic conjugacy class of 4 elements. In this case the exterior algebra Ω( A 4 ) has dimensions 1 : 4 : 8 : 11 : 12 : 12 : 11 : 8 : 4 : 1 with top-form 9-dimensional. We also find the noncommutative cohomology H 1 ( A 4 ) = C .","PeriodicalId":368340,"journal":{"name":"The Rise of Analytic Philosophy 1879–1930","volume":"80 1-2 1","pages":"0"},"PeriodicalIF":0.0000,"publicationDate":"2019-10-08","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":"0","resultStr":"{\"title\":\"Geometry\",\"authors\":\"Michael Potter\",\"doi\":\"10.4324/9781315776187-25\",\"DOIUrl\":null,\"url\":null,\"abstract\":\": We study the noncommutative Riemannian geometry of the alternating group A 4 = ( Z 2 × Z 2 ) >⊳ Z 3 using the recent formulation for finite groups in [2]. We find a unique ‘Levi-Civita’ connection for the invariant metric, and find that it has Ricci-flat but nonzero Riemann curvature. We show that it is the unique Ricci-flat connection on A 4 with the standard framing (we solve the vacuum Einstein’s equation). We also propose a natural Dirac operator for the associated spin connection and solve the Dirac equation. Some of our results hold for any finite group equipped with a cyclic conjugacy class of 4 elements. In this case the exterior algebra Ω( A 4 ) has dimensions 1 : 4 : 8 : 11 : 12 : 12 : 11 : 8 : 4 : 1 with top-form 9-dimensional. We also find the noncommutative cohomology H 1 ( A 4 ) = C .\",\"PeriodicalId\":368340,\"journal\":{\"name\":\"The Rise of Analytic Philosophy 1879–1930\",\"volume\":\"80 1-2 1\",\"pages\":\"0\"},\"PeriodicalIF\":0.0000,\"publicationDate\":\"2019-10-08\",\"publicationTypes\":\"Journal Article\",\"fieldsOfStudy\":null,\"isOpenAccess\":false,\"openAccessPdf\":\"\",\"citationCount\":\"0\",\"resultStr\":null,\"platform\":\"Semanticscholar\",\"paperid\":null,\"PeriodicalName\":\"The Rise of Analytic Philosophy 1879–1930\",\"FirstCategoryId\":\"1085\",\"ListUrlMain\":\"https://doi.org/10.4324/9781315776187-25\",\"RegionNum\":0,\"RegionCategory\":null,\"ArticlePicture\":[],\"TitleCN\":null,\"AbstractTextCN\":null,\"PMCID\":null,\"EPubDate\":\"\",\"PubModel\":\"\",\"JCR\":\"\",\"JCRName\":\"\",\"Score\":null,\"Total\":0}","platform":"Semanticscholar","paperid":null,"PeriodicalName":"The Rise of Analytic Philosophy 1879–1930","FirstCategoryId":"1085","ListUrlMain":"https://doi.org/10.4324/9781315776187-25","RegionNum":0,"RegionCategory":null,"ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":null,"EPubDate":"","PubModel":"","JCR":"","JCRName":"","Score":null,"Total":0}
: We study the noncommutative Riemannian geometry of the alternating group A 4 = ( Z 2 × Z 2 ) >⊳ Z 3 using the recent formulation for finite groups in [2]. We find a unique ‘Levi-Civita’ connection for the invariant metric, and find that it has Ricci-flat but nonzero Riemann curvature. We show that it is the unique Ricci-flat connection on A 4 with the standard framing (we solve the vacuum Einstein’s equation). We also propose a natural Dirac operator for the associated spin connection and solve the Dirac equation. Some of our results hold for any finite group equipped with a cyclic conjugacy class of 4 elements. In this case the exterior algebra Ω( A 4 ) has dimensions 1 : 4 : 8 : 11 : 12 : 12 : 11 : 8 : 4 : 1 with top-form 9-dimensional. We also find the noncommutative cohomology H 1 ( A 4 ) = C .