{"title":"Differential geometry and general relativity with algebraifolds","authors":"Tobias Fritz","doi":"10.1016/j.geomphys.2024.105327","DOIUrl":null,"url":null,"abstract":"<div><div>It is often noted that many of the basic concepts of differential geometry, such as the definition of connection, are purely algebraic in nature. Here, we review and extend existing work on fully algebraic formulations of differential geometry which eliminate the need for an underlying manifold. While the literature contains various independent approaches to this, we focus on one particular approach that we argue to be the most natural one based on the definition of <em>algebraifold</em>, by which we mean a commutative algebra <span><math><mi>A</mi></math></span> for which the module of derivations of <span><math><mi>A</mi></math></span> is finitely generated projective. Over <span><math><mi>R</mi></math></span> as the base ring, this class of algebras includes the algebra <span><math><msup><mrow><mi>C</mi></mrow><mrow><mo>∞</mo></mrow></msup><mo>(</mo><mi>M</mi><mo>)</mo></math></span> of smooth functions on a manifold <em>M</em>, and similarly for analytic functions. An importantly different example is the Colombeau algebra of generalized functions on <em>M</em>, which makes distributional differential geometry an instance of our formalism. Another instance is a fibred version of smooth differential geometry, since any smooth submersion <span><math><mi>M</mi><mo>→</mo><mi>N</mi></math></span> makes <span><math><msup><mrow><mi>C</mi></mrow><mrow><mo>∞</mo></mrow></msup><mo>(</mo><mi>M</mi><mo>)</mo></math></span> into an algebraifold with <span><math><msup><mrow><mi>C</mi></mrow><mrow><mo>∞</mo></mrow></msup><mo>(</mo><mi>N</mi><mo>)</mo></math></span> as the base ring. Over any field <em>k</em> of characteristic zero, examples include the algebra of regular functions on a smooth affine variety as well as any function field.</div><div>Our development of differential geometry in terms of algebraifolds comprises tensors, connections, curvature, geodesics and we briefly consider general relativity.</div></div>","PeriodicalId":55602,"journal":{"name":"Journal of Geometry and Physics","volume":"206 ","pages":"Article 105327"},"PeriodicalIF":1.6000,"publicationDate":"2024-09-21","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":"0","resultStr":null,"platform":"Semanticscholar","paperid":null,"PeriodicalName":"Journal of Geometry and Physics","FirstCategoryId":"100","ListUrlMain":"https://www.sciencedirect.com/science/article/pii/S0393044024002286","RegionNum":3,"RegionCategory":"数学","ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":null,"EPubDate":"","PubModel":"","JCR":"Q1","JCRName":"MATHEMATICS","Score":null,"Total":0}
引用次数: 0
Abstract
It is often noted that many of the basic concepts of differential geometry, such as the definition of connection, are purely algebraic in nature. Here, we review and extend existing work on fully algebraic formulations of differential geometry which eliminate the need for an underlying manifold. While the literature contains various independent approaches to this, we focus on one particular approach that we argue to be the most natural one based on the definition of algebraifold, by which we mean a commutative algebra for which the module of derivations of is finitely generated projective. Over as the base ring, this class of algebras includes the algebra of smooth functions on a manifold M, and similarly for analytic functions. An importantly different example is the Colombeau algebra of generalized functions on M, which makes distributional differential geometry an instance of our formalism. Another instance is a fibred version of smooth differential geometry, since any smooth submersion makes into an algebraifold with as the base ring. Over any field k of characteristic zero, examples include the algebra of regular functions on a smooth affine variety as well as any function field.
Our development of differential geometry in terms of algebraifolds comprises tensors, connections, curvature, geodesics and we briefly consider general relativity.
人们经常注意到,微分几何的许多基本概念,如连接的定义,在本质上都是纯代数的。在此,我们回顾并扩展了微分几何全代数公式的现有工作,这些公式不需要底层流形。我们指的是交换代数 A,A 的导数模块是有限生成的射影。以 R 为基环,这一类代数包括流形 M 上光滑函数的代数 C∞(M),解析函数也是如此。一个重要的不同例子是 M 上广义函数的科隆博代数,它使分布微分几何学成为我们形式主义的一个实例。另一个例子是光滑微分几何的纤维化版本,因为任何光滑潜入 M→N 都会使 C∞(M)成为以 C∞(N)为基环的代数折叠。在任何特征为零的域 k 上,例子包括光滑仿射变体上的正则函数代数以及任何函数域。我们用代数折叠来发展微分几何,包括张量、连接、曲率、大地线,并简要考虑广义相对论。
期刊介绍:
The Journal of Geometry and Physics is an International Journal in Mathematical Physics. The Journal stimulates the interaction between geometry and physics by publishing primary research, feature and review articles which are of common interest to practitioners in both fields.
The Journal of Geometry and Physics now also accepts Letters, allowing for rapid dissemination of outstanding results in the field of geometry and physics. Letters should not exceed a maximum of five printed journal pages (or contain a maximum of 5000 words) and should contain novel, cutting edge results that are of broad interest to the mathematical physics community. Only Letters which are expected to make a significant addition to the literature in the field will be considered.
The Journal covers the following areas of research:
Methods of:
• Algebraic and Differential Topology
• Algebraic Geometry
• Real and Complex Differential Geometry
• Riemannian Manifolds
• Symplectic Geometry
• Global Analysis, Analysis on Manifolds
• Geometric Theory of Differential Equations
• Geometric Control Theory
• Lie Groups and Lie Algebras
• Supermanifolds and Supergroups
• Discrete Geometry
• Spinors and Twistors
Applications to:
• Strings and Superstrings
• Noncommutative Topology and Geometry
• Quantum Groups
• Geometric Methods in Statistics and Probability
• Geometry Approaches to Thermodynamics
• Classical and Quantum Dynamical Systems
• Classical and Quantum Integrable Systems
• Classical and Quantum Mechanics
• Classical and Quantum Field Theory
• General Relativity
• Quantum Information
• Quantum Gravity