Examples of compact Einstein four-manifolds with negative curvature

IF 3.5 1区 数学 Q1 MATHEMATICS Journal of the American Mathematical Society Pub Date : 2018-02-02 DOI:10.1090/jams/944
J. Fine, Bruno Premoselli
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Our metrics are carried by a sequence of four-manifolds <inline-formula content-type=\"math/mathml\">\n<mml:math xmlns:mml=\"http://www.w3.org/1998/Math/MathML\" alttext=\"left-parenthesis upper X Subscript k Baseline right-parenthesis\">\n <mml:semantics>\n <mml:mrow>\n <mml:mo stretchy=\"false\">(</mml:mo>\n <mml:msub>\n <mml:mi>X</mml:mi>\n <mml:mi>k</mml:mi>\n </mml:msub>\n <mml:mo stretchy=\"false\">)</mml:mo>\n </mml:mrow>\n <mml:annotation encoding=\"application/x-tex\">(X_k)</mml:annotation>\n </mml:semantics>\n</mml:math>\n</inline-formula> previously considered by Gromov and Thurston (Pinching constants for hyperbolic manifolds, <italic>Invent. Math.</italic> <bold>89</bold> (1987), no. 1, 1–12). The construction begins with a certain sequence <inline-formula content-type=\"math/mathml\">\n<mml:math xmlns:mml=\"http://www.w3.org/1998/Math/MathML\" alttext=\"left-parenthesis upper M Subscript k Baseline right-parenthesis\">\n <mml:semantics>\n <mml:mrow>\n <mml:mo stretchy=\"false\">(</mml:mo>\n <mml:msub>\n <mml:mi>M</mml:mi>\n <mml:mi>k</mml:mi>\n </mml:msub>\n <mml:mo stretchy=\"false\">)</mml:mo>\n </mml:mrow>\n <mml:annotation encoding=\"application/x-tex\">(M_k)</mml:annotation>\n </mml:semantics>\n</mml:math>\n</inline-formula> of hyperbolic four-manifolds, each containing a totally geodesic surface <inline-formula content-type=\"math/mathml\">\n<mml:math xmlns:mml=\"http://www.w3.org/1998/Math/MathML\" alttext=\"normal upper Sigma Subscript k\">\n <mml:semantics>\n <mml:msub>\n <mml:mi mathvariant=\"normal\">Σ<!-- Σ --></mml:mi>\n <mml:mi>k</mml:mi>\n </mml:msub>\n <mml:annotation encoding=\"application/x-tex\">\\Sigma _k</mml:annotation>\n </mml:semantics>\n</mml:math>\n</inline-formula> which is nullhomologous and whose normal injectivity radius tends to infinity with <inline-formula content-type=\"math/mathml\">\n<mml:math xmlns:mml=\"http://www.w3.org/1998/Math/MathML\" alttext=\"k\">\n <mml:semantics>\n <mml:mi>k</mml:mi>\n <mml:annotation encoding=\"application/x-tex\">k</mml:annotation>\n </mml:semantics>\n</mml:math>\n</inline-formula>. For a fixed choice of natural number <inline-formula content-type=\"math/mathml\">\n<mml:math xmlns:mml=\"http://www.w3.org/1998/Math/MathML\" alttext=\"l\">\n <mml:semantics>\n <mml:mi>l</mml:mi>\n <mml:annotation encoding=\"application/x-tex\">l</mml:annotation>\n </mml:semantics>\n</mml:math>\n</inline-formula>, we consider the <inline-formula content-type=\"math/mathml\">\n<mml:math xmlns:mml=\"http://www.w3.org/1998/Math/MathML\" alttext=\"l\">\n <mml:semantics>\n <mml:mi>l</mml:mi>\n <mml:annotation encoding=\"application/x-tex\">l</mml:annotation>\n </mml:semantics>\n</mml:math>\n</inline-formula>-fold cover <inline-formula content-type=\"math/mathml\">\n<mml:math xmlns:mml=\"http://www.w3.org/1998/Math/MathML\" alttext=\"upper X Subscript k Baseline right-arrow upper M Subscript k\">\n <mml:semantics>\n <mml:mrow>\n <mml:msub>\n <mml:mi>X</mml:mi>\n <mml:mi>k</mml:mi>\n </mml:msub>\n <mml:mo stretchy=\"false\">→<!-- → --></mml:mo>\n <mml:msub>\n <mml:mi>M</mml:mi>\n <mml:mi>k</mml:mi>\n </mml:msub>\n </mml:mrow>\n <mml:annotation encoding=\"application/x-tex\">X_k \\to M_k</mml:annotation>\n </mml:semantics>\n</mml:math>\n</inline-formula> branched along <inline-formula content-type=\"math/mathml\">\n<mml:math xmlns:mml=\"http://www.w3.org/1998/Math/MathML\" alttext=\"normal upper Sigma Subscript k\">\n <mml:semantics>\n <mml:msub>\n <mml:mi mathvariant=\"normal\">Σ<!-- Σ --></mml:mi>\n <mml:mi>k</mml:mi>\n </mml:msub>\n <mml:annotation encoding=\"application/x-tex\">\\Sigma _k</mml:annotation>\n </mml:semantics>\n</mml:math>\n</inline-formula>. We prove that for any choice of <inline-formula content-type=\"math/mathml\">\n<mml:math xmlns:mml=\"http://www.w3.org/1998/Math/MathML\" alttext=\"l\">\n <mml:semantics>\n <mml:mi>l</mml:mi>\n <mml:annotation encoding=\"application/x-tex\">l</mml:annotation>\n </mml:semantics>\n</mml:math>\n</inline-formula> and all large enough <inline-formula content-type=\"math/mathml\">\n<mml:math xmlns:mml=\"http://www.w3.org/1998/Math/MathML\" alttext=\"k\">\n <mml:semantics>\n <mml:mi>k</mml:mi>\n <mml:annotation encoding=\"application/x-tex\">k</mml:annotation>\n </mml:semantics>\n</mml:math>\n</inline-formula> (depending on <inline-formula content-type=\"math/mathml\">\n<mml:math xmlns:mml=\"http://www.w3.org/1998/Math/MathML\" alttext=\"l\">\n <mml:semantics>\n <mml:mi>l</mml:mi>\n <mml:annotation encoding=\"application/x-tex\">l</mml:annotation>\n </mml:semantics>\n</mml:math>\n</inline-formula>), <inline-formula content-type=\"math/mathml\">\n<mml:math xmlns:mml=\"http://www.w3.org/1998/Math/MathML\" alttext=\"upper X Subscript k\">\n <mml:semantics>\n <mml:msub>\n <mml:mi>X</mml:mi>\n <mml:mi>k</mml:mi>\n </mml:msub>\n <mml:annotation encoding=\"application/x-tex\">X_k</mml:annotation>\n </mml:semantics>\n</mml:math>\n</inline-formula> carries an Einstein metric of negative sectional curvature. The first step in the proof is to find an approximate Einstein metric on <inline-formula content-type=\"math/mathml\">\n<mml:math xmlns:mml=\"http://www.w3.org/1998/Math/MathML\" alttext=\"upper X Subscript k\">\n <mml:semantics>\n <mml:msub>\n <mml:mi>X</mml:mi>\n <mml:mi>k</mml:mi>\n </mml:msub>\n <mml:annotation encoding=\"application/x-tex\">X_k</mml:annotation>\n </mml:semantics>\n</mml:math>\n</inline-formula>, which is done by interpolating between a model Einstein metric near the branch locus and the pull-back of the hyperbolic metric from <inline-formula content-type=\"math/mathml\">\n<mml:math xmlns:mml=\"http://www.w3.org/1998/Math/MathML\" alttext=\"upper M Subscript k\">\n <mml:semantics>\n <mml:msub>\n <mml:mi>M</mml:mi>\n <mml:mi>k</mml:mi>\n </mml:msub>\n <mml:annotation encoding=\"application/x-tex\">M_k</mml:annotation>\n </mml:semantics>\n</mml:math>\n</inline-formula>. The second step in the proof is to perturb this to a genuine solution to Einstein’s equations, by a parameter dependent version of the inverse function theorem. The analysis relies on a delicate bootstrap procedure based on <inline-formula content-type=\"math/mathml\">\n<mml:math xmlns:mml=\"http://www.w3.org/1998/Math/MathML\" alttext=\"upper L squared\">\n <mml:semantics>\n <mml:msup>\n <mml:mi>L</mml:mi>\n <mml:mn>2</mml:mn>\n </mml:msup>\n <mml:annotation encoding=\"application/x-tex\">L^2</mml:annotation>\n </mml:semantics>\n</mml:math>\n</inline-formula> coercivity estimates.</p>","PeriodicalId":54764,"journal":{"name":"Journal of the American Mathematical Society","volume":" ","pages":""},"PeriodicalIF":3.5000,"publicationDate":"2018-02-02","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"https://sci-hub-pdf.com/10.1090/jams/944","citationCount":"9","resultStr":null,"platform":"Semanticscholar","paperid":null,"PeriodicalName":"Journal of the American Mathematical Society","FirstCategoryId":"100","ListUrlMain":"https://doi.org/10.1090/jams/944","RegionNum":1,"RegionCategory":"数学","ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":null,"EPubDate":"","PubModel":"","JCR":"Q1","JCRName":"MATHEMATICS","Score":null,"Total":0}
引用次数: 9

Abstract

We give new examples of compact, negatively curved Einstein manifolds of dimension 4 4 . These are seemingly the first such examples which are not locally homogeneous. Our metrics are carried by a sequence of four-manifolds ( X k ) (X_k) previously considered by Gromov and Thurston (Pinching constants for hyperbolic manifolds, Invent. Math. 89 (1987), no. 1, 1–12). The construction begins with a certain sequence ( M k ) (M_k) of hyperbolic four-manifolds, each containing a totally geodesic surface Σ k \Sigma _k which is nullhomologous and whose normal injectivity radius tends to infinity with k k . For a fixed choice of natural number l l , we consider the l l -fold cover X k M k X_k \to M_k branched along Σ k \Sigma _k . We prove that for any choice of l l and all large enough k k (depending on l l ), X k X_k carries an Einstein metric of negative sectional curvature. The first step in the proof is to find an approximate Einstein metric on X k X_k , which is done by interpolating between a model Einstein metric near the branch locus and the pull-back of the hyperbolic metric from M k M_k . The second step in the proof is to perturb this to a genuine solution to Einstein’s equations, by a parameter dependent version of the inverse function theorem. The analysis relies on a delicate bootstrap procedure based on L 2 L^2 coercivity estimates.

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具有负曲率的紧致Einstein四流形的例子
我们给出了4维负弯曲的紧致爱因斯坦流形的新例子。这些似乎是第一个不具有局部同质性的例子。我们的度量由四流形序列(xk) (X_k)承载,之前由Gromov和Thurston(双曲流形的捏紧常数,Invent)考虑。数学89(1987),第1期。1、1 - 12)。构造从双曲四流形的一定序列(M k) (M_k)开始,每个序列包含一个完全测地曲面Σ k \Sigma _k,该曲面是零同源的,其法向注入半径随k k趋于无穷大。对于一个固定选择的自然数l l,我们考虑l l折叠覆盖X k→M k X_k \到M_k沿Σ k \Sigma _k分支。我们证明了对于任何ll的选择和所有足够大的k k(取决于ll), X k X_k携带负截面曲率的爱因斯坦度规。证明的第一步是在X k X_k上找到一个近似的爱因斯坦度规,这是通过在分支轨迹附近的模型爱因斯坦度规和从M k M_k的双曲度规的回拉之间进行插值来完成的。证明的第二步是通过反函数定理的参数依赖版本,将其扰动为爱因斯坦方程的真正解。分析依赖于基于l2 L^2矫顽力估计的精细自举程序。
本文章由计算机程序翻译,如有差异,请以英文原文为准。
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7.60
自引率
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>12 weeks
期刊介绍: All articles submitted to this journal are peer-reviewed. The AMS has a single blind peer-review process in which the reviewers know who the authors of the manuscript are, but the authors do not have access to the information on who the peer reviewers are. This journal is devoted to research articles of the highest quality in all areas of pure and applied mathematics.
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