{"title":"黎曼流形的平面波极限","authors":"Amir Babak Aazami","doi":"arxiv-2408.02567","DOIUrl":null,"url":null,"abstract":"Utilizing the covariant formulation of Penrose's plane wave limit by Blau et\nal., we construct for any Riemannian metric $g$ a family of \"plane wave limits\"\nof one higher dimension. These limits are taken along geodesics of $g$, yield\nsimpler metrics of Lorentzian signature, and are isometric invariants. They can\nalso be seen to arise locally from a suitable expansion of $g$ in Fermi\ncoordinates, and they directly encode much of $g$'s geometry. For example,\nnormal Jacobi fields of $g$ are encoded as geodesics of its plane wave limits.\nFurthermore, $g$ will have constant sectional curvature if and only if each of\nits plane wave limits is locally conformally flat. In fact $g$ will be flat, or\nRicci-flat, or geodesically complete, if and only if all of its plane wave\nlimits are, respectively, the same. Many other curvature properties are\npreserved in the limit, including certain inequalities, such as signed Ricci\ncurvature.","PeriodicalId":501113,"journal":{"name":"arXiv - MATH - Differential Geometry","volume":"9 1","pages":""},"PeriodicalIF":0.0000,"publicationDate":"2024-08-05","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":"0","resultStr":"{\"title\":\"Plane wave limits of Riemannian manifolds\",\"authors\":\"Amir Babak Aazami\",\"doi\":\"arxiv-2408.02567\",\"DOIUrl\":null,\"url\":null,\"abstract\":\"Utilizing the covariant formulation of Penrose's plane wave limit by Blau et\\nal., we construct for any Riemannian metric $g$ a family of \\\"plane wave limits\\\"\\nof one higher dimension. These limits are taken along geodesics of $g$, yield\\nsimpler metrics of Lorentzian signature, and are isometric invariants. They can\\nalso be seen to arise locally from a suitable expansion of $g$ in Fermi\\ncoordinates, and they directly encode much of $g$'s geometry. For example,\\nnormal Jacobi fields of $g$ are encoded as geodesics of its plane wave limits.\\nFurthermore, $g$ will have constant sectional curvature if and only if each of\\nits plane wave limits is locally conformally flat. In fact $g$ will be flat, or\\nRicci-flat, or geodesically complete, if and only if all of its plane wave\\nlimits are, respectively, the same. Many other curvature properties are\\npreserved in the limit, including certain inequalities, such as signed Ricci\\ncurvature.\",\"PeriodicalId\":501113,\"journal\":{\"name\":\"arXiv - MATH - Differential Geometry\",\"volume\":\"9 1\",\"pages\":\"\"},\"PeriodicalIF\":0.0000,\"publicationDate\":\"2024-08-05\",\"publicationTypes\":\"Journal Article\",\"fieldsOfStudy\":null,\"isOpenAccess\":false,\"openAccessPdf\":\"\",\"citationCount\":\"0\",\"resultStr\":null,\"platform\":\"Semanticscholar\",\"paperid\":null,\"PeriodicalName\":\"arXiv - MATH - Differential Geometry\",\"FirstCategoryId\":\"1085\",\"ListUrlMain\":\"https://doi.org/arxiv-2408.02567\",\"RegionNum\":0,\"RegionCategory\":null,\"ArticlePicture\":[],\"TitleCN\":null,\"AbstractTextCN\":null,\"PMCID\":null,\"EPubDate\":\"\",\"PubModel\":\"\",\"JCR\":\"\",\"JCRName\":\"\",\"Score\":null,\"Total\":0}","platform":"Semanticscholar","paperid":null,"PeriodicalName":"arXiv - MATH - Differential Geometry","FirstCategoryId":"1085","ListUrlMain":"https://doi.org/arxiv-2408.02567","RegionNum":0,"RegionCategory":null,"ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":null,"EPubDate":"","PubModel":"","JCR":"","JCRName":"","Score":null,"Total":0}
Utilizing the covariant formulation of Penrose's plane wave limit by Blau et
al., we construct for any Riemannian metric $g$ a family of "plane wave limits"
of one higher dimension. These limits are taken along geodesics of $g$, yield
simpler metrics of Lorentzian signature, and are isometric invariants. They can
also be seen to arise locally from a suitable expansion of $g$ in Fermi
coordinates, and they directly encode much of $g$'s geometry. For example,
normal Jacobi fields of $g$ are encoded as geodesics of its plane wave limits.
Furthermore, $g$ will have constant sectional curvature if and only if each of
its plane wave limits is locally conformally flat. In fact $g$ will be flat, or
Ricci-flat, or geodesically complete, if and only if all of its plane wave
limits are, respectively, the same. Many other curvature properties are
preserved in the limit, including certain inequalities, such as signed Ricci
curvature.