Beyond Riemannian Geometry: the Affine Connection Setting For
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Geometric Manifolds
Wintersemester 2015/2016 University of Heidelberg Geometric Structures on Manifolds Geometric Manifolds by Stephan Schmitt Contents Introduction, first Definitions and Results 1 Manifolds - The Group way .................................... 1 Geometric Structures ........................................ 2 The Developing Map and Completeness 4 An introductory discussion of the torus ............................. 4 Definition of the Developing map ................................. 6 Developing map and Manifolds, Completeness 10 Developing Manifolds ....................................... 10 some completeness results ..................................... 10 Some selected results 11 Discrete Groups .......................................... 11 Stephan Schmitt INTRODUCTION, FIRST DEFINITIONS AND RESULTS Introduction, first Definitions and Results Manifolds - The Group way The keystone of working mathematically in Differential Geometry, is the basic notion of a Manifold, when we usually talk about Manifolds we mean a Topological Space that, at least locally, looks just like Euclidean Space. The usual formalization of that Concept is well known, we take charts to ’map out’ the Manifold, in this paper, for sake of Convenience we will take a slightly different approach to formalize the Concept of ’locally euclidean’, to formulate it, we need some tools, let us introduce them now: Definition 1.1. Pseudogroups A pseudogroup on a topological space X is a set G of homeomorphisms between open sets of X satisfying the following conditions: • The Domains of the elements g 2 G cover X • The restriction of an element g 2 G to any open set contained in its Domain is also in G. • The Composition g1 ◦ g2 of two elements of G, when defined, is in G • The inverse of an Element of G is in G. • The property of being in G is local, that is, if g : U ! V is a homeomorphism between open sets of X and U is covered by open sets Uα such that each restriction gjUα is in G, then g 2 G Definition 1.2. -
Ricci, Levi-Civita, and the Birth of General Relativity Reviewed by David E
BOOK REVIEW Einstein’s Italian Mathematicians: Ricci, Levi-Civita, and the Birth of General Relativity Reviewed by David E. Rowe Einstein’s Italian modern Italy. Nor does the author shy away from topics Mathematicians: like how Ricci developed his absolute differential calculus Ricci, Levi-Civita, and the as a generalization of E. B. Christoffel’s (1829–1900) work Birth of General Relativity on quadratic differential forms or why it served as a key By Judith R. Goodstein tool for Einstein in his efforts to generalize the special theory of relativity in order to incorporate gravitation. In This delightful little book re- like manner, she describes how Levi-Civita was able to sulted from the author’s long- give a clear geometric interpretation of curvature effects standing enchantment with Tul- in Einstein’s theory by appealing to his concept of parallel lio Levi-Civita (1873–1941), his displacement of vectors (see below). For these and other mentor Gregorio Ricci Curbastro topics, Goodstein draws on and cites a great deal of the (1853–1925), and the special AMS, 2018, 211 pp. 211 AMS, 2018, vast secondary literature produced in recent decades by the world that these and other Ital- “Einstein industry,” in particular the ongoing project that ian mathematicians occupied and helped to shape. The has produced the first 15 volumes of The Collected Papers importance of their work for Einstein’s general theory of of Albert Einstein [CPAE 1–15, 1987–2018]. relativity is one of the more celebrated topics in the history Her account proceeds in three parts spread out over of modern mathematical physics; this is told, for example, twelve chapters, the first seven of which cover episodes in [Pais 1982], the standard biography of Einstein. -
Affine Connections and Second-Order Affine Structures
Affine connections and second-order affine structures Filip Bár Dedicated to my good friend Tom Rewwer on the occasion of his 35th birthday. Abstract Smooth manifolds have been always understood intuitively as spaces with an affine geometry on the infinitesimal scale. In Synthetic Differential Geometry this can be made precise by showing that a smooth manifold carries a natural struc- ture of an infinitesimally affine space. This structure is comprised of two pieces of data: a sequence of symmetric and reflexive relations defining the tuples of mu- tual infinitesimally close points, called an infinitesimal structure, and an action of affine combinations on these tuples. For smooth manifolds the only natural infin- itesimal structure that has been considered so far is the one generated by the first neighbourhood of the diagonal. In this paper we construct natural infinitesimal structures for higher-order neighbourhoods of the diagonal and show that on any manifold any symmetric affine connection extends to a second-order infinitesimally affine structure. Introduction A deeply rooted intuition about smooth manifolds is that of spaces that become linear spaces in the infinitesimal neighbourhood of each point. On the infinitesimal scale the geometry underlying a manifold is thus affine geometry. To make this intuition precise requires a good theory of infinitesimals as well as defining precisely what it means for two points on a manifold to be infinitesimally close. As regards infinitesimals we make use of Synthetic Differential Geometry (SDG) and adopt the neighbourhoods of the diagonal from Algebraic Geometry to define when two points are infinitesimally close. The key observations on how to proceed have been made by Kock in [8]: 1) The first neighbourhood arXiv:1809.05944v2 [math.DG] 29 Aug 2020 of the diagonal exists on formal manifolds and can be understood as a symmetric, reflexive relation on points, saying when two points are infinitesimal neighbours, and 2) we can form affine combinations of points that are mutual neighbours. -
Connections on Bundles Md
Dhaka Univ. J. Sci. 60(2): 191-195, 2012 (July) Connections on Bundles Md. Showkat Ali, Md. Mirazul Islam, Farzana Nasrin, Md. Abu Hanif Sarkar and Tanzia Zerin Khan Department of Mathematics, University of Dhaka, Dhaka 1000, Bangladesh, Email: [email protected] Received on 25. 05. 2011.Accepted for Publication on 15. 12. 2011 Abstract This paper is a survey of the basic theory of connection on bundles. A connection on tangent bundle , is called an affine connection on an -dimensional smooth manifold . By the general discussion of affine connection on vector bundles that necessarily exists on which is compatible with tensors. I. Introduction = < , > (2) In order to differentiate sections of a vector bundle [5] or where <, > represents the pairing between and ∗. vector fields on a manifold we need to introduce a Then is a section of , called the absolute differential structure called the connection on a vector bundle. For quotient or the covariant derivative of the section along . example, an affine connection is a structure attached to a differentiable manifold so that we can differentiate its Theorem 1. A connection always exists on a vector bundle. tensor fields. We first introduce the general theorem of Proof. Choose a coordinate covering { }∈ of . Since connections on vector bundles. Then we study the tangent vector bundles are trivial locally, we may assume that there is bundle. is a -dimensional vector bundle determine local frame field for any . By the local structure of intrinsically by the differentiable structure [8] of an - connections, we need only construct a × matrix on dimensional smooth manifold . each such that the matrices satisfy II. -
2. Chern Connections and Chern Curvatures1
1 2. Chern connections and Chern curvatures1 Let V be a complex vector space with dimC V = n. A hermitian metric h on V is h : V £ V ¡¡! C such that h(av; bu) = abh(v; u) h(a1v1 + a2v2; u) = a1h(v1; u) + a2h(v2; u) h(v; u) = h(u; v) h(u; u) > 0; u 6= 0 where v; v1; v2; u 2 V and a; b; a1; a2 2 C. If we ¯x a basis feig of V , and set hij = h(ei; ej) then ¤ ¤ ¤ ¤ h = hijei ej 2 V V ¤ ¤ ¤ ¤ where ei 2 V is the dual of ei and ei 2 V is the conjugate dual of ei, i.e. X ¤ ei ( ajej) = ai It is obvious that (hij) is a hermitian positive matrix. De¯nition 0.1. A complex vector bundle E is said to be hermitian if there is a positive de¯nite hermitian tensor h on E. r Let ' : EjU ¡¡! U £ C be a trivilization and e = (e1; ¢ ¢ ¢ ; er) be the corresponding frame. The r hermitian metric h is represented by a positive hermitian matrix (hij) 2 ¡(; EndC ) such that hei(x); ej(x)i = hij(x); x 2 U Then hermitian metric on the chart (U; ') could be written as X ¤ ¤ h = hijei ej For example, there are two charts (U; ') and (V; Ã). We set g = à ± '¡1 :(U \ V ) £ Cr ¡¡! (U \ V ) £ Cr and g is represented by matrix (gij). On U \ V , we have X X X ¡1 ¡1 ¡1 ¡1 ¡1 ei(x) = ' (x; "i) = à ± à ± ' (x; "i) = à (x; gij"j) = gijà (x; "j) = gije~j(x) j j For the metric X ~ hij = hei(x); ej(x)i = hgike~k(x); gjle~l(x)i = gikhklgjl k;l that is h = g ¢ h~ ¢ g¤ 12008.04.30 If there are some errors, please contact to: [email protected] 2 Example 0.2 (Fubini-Study metric on holomorphic tangent bundle T 1;0Pn). -
Witold Roter (1932-2015)
COLLOQUIUMMATHEMATICUM Online First version WITOLD ROTER (1932–2015) BY ANDRZEJ DERDZIŃSKI (Columbus, OH) Witold Roter was born on September 20th, 1932 and died on June 19th, 2015. He authored or co-authored 40 papers in differential geometry, pub- lished between 1961 and 2010. His nine Ph.D. advisees, listed here along with the year of receiving the degree, are: Czesław Konopka (1972), Edward Głodek (1973), Andrzej Gębarowski (1975), Andrzej Derdziński (1976), Zbig- niew Olszak (1978), Ryszard Deszcz (1980), Marian Hotloś (1980), Wiesław Grycak (1984), and Marek Lewkowicz (1989). Also, for many years, he ran the Wrocław seminar on differential geome- try, first started by Władysław Ślebodziński, who had been Witold Roter’s Ph.D. advisor. For more biographical information (in Polish), see Zbigniew Olszak’s article [44]. This is a brief summary of Witold Roter’s selected results, divided into four sections devoted to separate topics. Since he repeatedly returned to questions he had worked on earlier, our presentation is not chronological. 1. Parallel Weyl tensor in the Riemannian case. The curvature tensor R of a given n-dimensional pseudo-Riemannian manifold (M; g) is naturally decomposed into the sum R = S + E + W of its irreducible com- ponents [41, p. 47]. The first two correspond to the scalar curvature and Einstein tensor (the traceless part of the Ricci tensor). The third component is the Weyl tensor W , also known as the conformal curvature tensor, which is of interest only in dimensions n ≥ 4 since, for algebraic reasons, W = 0 whenever n ≤ 3. Viewed as a (1; 3) tensor field, so that it sends three vector fields trilin- early to a vector field, W is a conformal invariant: it remains unchanged when the metric g is replaced by the product φg, where φ is any smooth positive function. -
Cartan Connections to Connections on fibre Bundles, and Some Modern Applications
The works of Charles Ehresmann on connections: from Cartan connections to connections on fibre bundles, and some modern applications Charles-Michel Marle Universite´ Pierre et Marie Curie Paris, France The works of Charles Ehresmann on connections: from Cartan connections to connections on fibre bundles, and some modern applications – p. 1/40 Élie Cartan’s affine connections (1) Around 1923, Élie Cartan [1, 2, 3] introduced the notion of an affine connection on a manifold. That notion was previously used, in a less general setting, by H. Weyl [16] and rests on the idea of parallel transport due to T. Levi-Civita [11]. The works of Charles Ehresmann on connections: from Cartan connections to connections on fibre bundles, and some modern applications – p. 2/40 Élie Cartan’s affine connections (1) Around 1923, Élie Cartan [1, 2, 3] introduced the notion of an affine connection on a manifold. That notion was previously used, in a less general setting, by H. Weyl [16] and rests on the idea of parallel transport due to T. Levi-Civita [11]. A large part of [1, 2] is devoted to applications of affine connections to Newtonian and Einsteinian Mechanics. Cartan show that the principle of inertia (which is at the foundations of Mechanics), according to which a material point particle, when no forces act on it, moves along a straight line with a constant velocity, can be expressed locally by the use of an affine connection. Under that form, that principle remains valid in (curved) Einsteinian space-times. The works of Charles Ehresmann on connections: from Cartan connections to connections on fibre bundles, and some modern applications – p. -
226 NAW 5/2 Nr. 3 September 2001 Honderdjaarslezing Dirk Struik Dirk Struik Honderdjaarslezing NAW 5/2 Nr
226 NAW 5/2 nr. 3 september 2001 Honderdjaarslezing Dirk Struik Dirk Struik Honderdjaarslezing NAW 5/2 nr. 3 september 2001 227 Afscheid van Dirk Struik Honderdjaarslezing Op 21 oktober 2000 overleed Dirk Struik in kringen. Zij ging een heel andere richting uit vriend Klaas Kooyman, de botanist die later zijn huis in Belmont (Massachusetts). Een In dan Anton en ik. Ik heb natuurlijk in die hon- bibliothecaris in Wageningen is geworden, La- Memoriam verscheen in het decembernum- derd jaar zoveel meegemaakt, dat ik in een tijn en Grieks geleerd bij meneer De Vries in mer van het Nieuw Archief. Ter afscheid van paar kwartier dat niet allemaal kan vertellen. Den Haag. We gingen daarvoor op en neer met deze beroemde wetenschapper van Neder- Ik zal een paar grepen doen uit mijn leven, het electrische spoortje van Rotterdam naar landse afkomst publiceren we in dit nummer mensen die me bijzonder hebben geboeid en Den Haag. We hebben er alleen maar het een- vijf artikelen over Dirk Struik. Het eerste ar- gebeurtenissen die me hebben be¨ınvloed. voudigste Latijn en Grieks geleerd, Herodo- tikel is van Struik zelf. In oktober 1994 orga- Mijn vroegste herinnering is aan de Boe- tus, Caesar — De Bello Gallico: “Gallia divisa niseerde het CWI een symposium ter ere van renoorlog, omstreeks 1900.2 Ik was een jaar est in partes tres ...” Dat heeft me heel wei- de honderdste verjaardag van Dirk Struik. Ter of vijf, zes en vroeg aan mijn vader: “Vader, nig geholpen bij de studie van de wiskunde. afsluiting heeft Struik toen zelf de volgen- wat betekent toch dat woord oorlog?” — dat Je kunt heel goed tensors doen zonder Latijn de redevoering gehouden, met als geheugen- hoef je tegenwoordig niet meer uit te leggen- te kennen, hoewel het wel goed is om te we- steun enkel wat aantekeningen op een velle- aan zesjarigen. -
EXOTIC SPHERES and CURVATURE 1. Introduction Exotic
BULLETIN (New Series) OF THE AMERICAN MATHEMATICAL SOCIETY Volume 45, Number 4, October 2008, Pages 595–616 S 0273-0979(08)01213-5 Article electronically published on July 1, 2008 EXOTIC SPHERES AND CURVATURE M. JOACHIM AND D. J. WRAITH Abstract. Since their discovery by Milnor in 1956, exotic spheres have pro- vided a fascinating object of study for geometers. In this article we survey what is known about the curvature of exotic spheres. 1. Introduction Exotic spheres are manifolds which are homeomorphic but not diffeomorphic to a standard sphere. In this introduction our aims are twofold: First, to give a brief account of the discovery of exotic spheres and to make some general remarks about the structure of these objects as smooth manifolds. Second, to outline the basics of curvature for Riemannian manifolds which we will need later on. In subsequent sections, we will explore the interaction between topology and geometry for exotic spheres. We will use the term differentiable to mean differentiable of class C∞,and all diffeomorphisms will be assumed to be smooth. As every graduate student knows, a smooth manifold is a topological manifold that is equipped with a smooth (differentiable) structure, that is, a smooth maximal atlas. Recall that an atlas is a collection of charts (homeomorphisms from open neighbourhoods in the manifold onto open subsets of some Euclidean space), the domains of which cover the manifold. Where the chart domains overlap, we impose a smooth compatibility condition for the charts [doC, chapter 0] if we wish our manifold to be smooth. Such an atlas can then be extended to a maximal smooth atlas by including all possible charts which satisfy the compatibility condition with the original maps. -
Riemannian Geometry and Multilinear Tensors with Vector Fields on Manifolds Md
International Journal of Scientific & Engineering Research, Volume 5, Issue 9, September-2014 157 ISSN 2229-5518 Riemannian Geometry and Multilinear Tensors with Vector Fields on Manifolds Md. Abdul Halim Sajal Saha Md Shafiqul Islam Abstract-In the paper some aspects of Riemannian manifolds, pseudo-Riemannian manifolds, Lorentz manifolds, Riemannian metrics, affine connections, parallel transport, curvature tensors, torsion tensors, killing vector fields, conformal killing vector fields are focused. The purpose of this paper is to develop the theory of manifolds equipped with Riemannian metric. I have developed some theorems on torsion and Riemannian curvature tensors using affine connection. A Theorem 1.20 named “Fundamental Theorem of Pseudo-Riemannian Geometry” has been established on Riemannian geometry using tensors with metric. The main tools used in the theorem of pseudo Riemannian are tensors fields defined on a Riemannian manifold. Keywords: Riemannian manifolds, pseudo-Riemannian manifolds, Lorentz manifolds, Riemannian metrics, affine connections, parallel transport, curvature tensors, torsion tensors, killing vector fields, conformal killing vector fields. —————————— —————————— I. Introduction (c) { } is a family of open sets which covers , that is, 푖 = . Riemannian manifold is a pair ( , g) consisting of smooth 푈 푀 manifold and Riemannian metric g. A manifold may carry a (d) ⋃ is푈 푖푖 a homeomorphism푀 from onto an open subset of 푀 ′ further structure if it is endowed with a metric tensor, which is a 푖 . 푖 푖 휑 푈 푈 natural generation푀 of the inner product between two vectors in 푛 ℝ to an arbitrary manifold. Riemannian metrics, affine (e) Given and such that , the map = connections,푛 parallel transport, curvature tensors, torsion tensors, ( ( ) killingℝ vector fields and conformal killing vector fields play from푖 푗 ) to 푖 푗 is infinitely푖푗 −1 푈 푈 푈 ∩ 푈 ≠ ∅ 휓 important role to develop the theorem of Riemannian manifolds. -
Emil De Souza Sбnchez Filho
Emil de Souza Sánchez Filho Tensor Calculus for Engineers and Physicists Tensor Calculus for Engineers and Physicists Emil de Souza Sa´nchez Filho Tensor Calculus for Engineers and Physicists Emil de Souza Sa´nchez Filho Fluminense Federal University Rio de Janeiro, Rio de Janeiro Brazil ISBN 978-3-319-31519-5 ISBN 978-3-319-31520-1 (eBook) DOI 10.1007/978-3-319-31520-1 Library of Congress Control Number: 2016938417 © Springer International Publishing Switzerland 2016 This work is subject to copyright. All rights are reserved by the Publisher, whether the whole or part of the material is concerned, specifically the rights of translation, reprinting, reuse of illustrations, recitation, broadcasting, reproduction on microfilms or in any other physical way, and transmission or information storage and retrieval, electronic adaptation, computer software, or by similar or dissimilar methodology now known or hereafter developed. The use of general descriptive names, registered names, trademarks, service marks, etc. in this publication does not imply, even in the absence of a specific statement, that such names are exempt from the relevant protective laws and regulations and therefore free for general use. The publisher, the authors and the editors are safe to assume that the advice and information in this book are believed to be true and accurate at the date of publication. Neither the publisher nor the authors or the editors give a warranty, express or implied, with respect to the material contained herein or for any errors or omissions that may have been made. Printed on acid-free paper This Springer imprint is published by Springer Nature The registered company is Springer International Publishing AG Switzerland To Sandra, Yuri, Natalia and Lara Preface The Tensor Calculus for Engineers and Physicist provides a rigorous approach to tensor manifolds and their role in several issues of these professions. -
Pseudogroups Via Pseudoactions: Unifying Local, Global, and Infinitesimal Symmetry
PSEUDOGROUPS VIA PSEUDOACTIONS: UNIFYING LOCAL, GLOBAL, AND INFINITESIMAL SYMMETRY ANTHONY D. BLAOM Abstract. A multiplicatively closed, horizontal foliation on a Lie groupoid may be viewed as a `pseudoaction' on the base manifold M. A pseudoaction generates a pseudogroup of transformations of M in the same way an ordinary Lie group action generates a transformation group. Infinitesimalizing a pseu- doaction, one obtains the action of a Lie algebra on M, possibly twisted. A global converse to Lie's third theorem proven here states that every twisted Lie algebra action is integrated by a pseudoaction. When the twisted Lie algebra action is complete it integrates to a twisted Lie group action, according to a generalization of Palais' global integrability theorem. Dedicated to Richard W. Sharpe 1. Introduction 1.1. Pseudoactions. Unlike transformation groups, pseudogroups of transfor- mations capture simultaneously the phenomena of global and local symmetry. On the other hand, a transformation group can be replaced by the action of an ab- stract group which may have nice properties | a Lie group in the best scenario. Here we show how to extend the abstraction of group actions to handle certain pseudogroups as well. These pseudogroups include: (i) all Lie pseudogroups of finite type (both transitive and intransitive) and hence the isometry pseudogroups of suitably regular geometric structures of finite type; (ii) all pseudogroups gen- erated by the local flows of a smooth vector field; and, more generally (iii) any pseudogroup generated by the infinitesimal action of a finite-dimensional Lie al- gebra. Our generalization of a group action on M, here called a pseudoaction, consists of a multiplicatively closed, horizontal foliation on a Lie groupoid G over arXiv:1410.6981v4 [math.DG] 3 Oct 2015 M.