Lectures on the Euler Characteristic of Affine Manifolds
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Descartes, Euler, Poincaré, Pólya and Polyhedra Séminaire De Philosophie Et Mathématiques, 1982, Fascicule 8 « Descartes, Euler, Poincaré, Polya and Polyhedra », , P
Séminaire de philosophie et mathématiques PETER HILTON JEAN PEDERSEN Descartes, Euler, Poincaré, Pólya and Polyhedra Séminaire de Philosophie et Mathématiques, 1982, fascicule 8 « Descartes, Euler, Poincaré, Polya and Polyhedra », , p. 1-17 <http://www.numdam.org/item?id=SPHM_1982___8_A1_0> © École normale supérieure – IREM Paris Nord – École centrale des arts et manufactures, 1982, tous droits réservés. L’accès aux archives de la série « Séminaire de philosophie et mathématiques » implique l’accord avec les conditions générales d’utilisation (http://www.numdam.org/conditions). Toute utilisation commerciale ou impression systématique est constitutive d’une infraction pénale. Toute copie ou impression de ce fichier doit contenir la présente mention de copyright. Article numérisé dans le cadre du programme Numérisation de documents anciens mathématiques http://www.numdam.org/ - 1 - DESCARTES, EULER, POINCARÉ, PÓLYA—AND POLYHEDRA by Peter H i l t o n and Jean P e d e rs e n 1. Introduction When geometers talk of polyhedra, they restrict themselves to configurations, made up of vertices. edqes and faces, embedded in three-dimensional Euclidean space. Indeed. their polyhedra are always homeomorphic to thè two- dimensional sphere S1. Here we adopt thè topologists* terminology, wherein dimension is a topological invariant, intrinsic to thè configuration. and not a property of thè ambient space in which thè configuration is located. Thus S 2 is thè surface of thè 3-dimensional ball; and so we find. among thè geometers' polyhedra. thè five Platonic “solids”, together with many other examples. However. we should emphasize that we do not here think of a Platonic “solid” as a solid : we have in mind thè bounding surface of thè solid. -
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. -
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. -
Euler Characteristics, Gauss-Bonnett, and Index Theorems
EULER CHARACTERISTICS,GAUSS-BONNETT, AND INDEX THEOREMS Keefe Mitman and Matthew Lerner-Brecher Department of Mathematics; Columbia University; New York, NY 10027; UN3952, Song Yu. Keywords Euler Characteristics, Gauss-Bonnett, Index Theorems. Contents 1 Foreword 1 2 Euler Characteristics 2 2.1 Introduction . 2 2.2 Betti Numbers . 2 2.2.1 Chains and Boundary Operators . 2 2.2.2 Cycles and Homology . 3 2.3 Euler Characteristics . 4 3 Gauss-Bonnet Theorem 4 3.1 Background . 4 3.2 Examples . 5 4 Index Theorems 6 4.1 The Differential of a Manifold Map . 7 4.2 Degree and Index of a Manifold Map . 7 4.2.1 Technical Definition . 7 4.2.2 A More Concrete Case . 8 4.3 The Poincare-Hopf Theorem and Applications . 8 1 Foreword Within this course thus far, we have become rather familiar with introductory differential geometry, complexes, and certain applications of complexes. Unfortunately, however, many of the geometries we have been discussing remain MARCH 8, 2019 fairly arbitrary and, so far, unrelated, despite their underlying and inherent similarities. As a result of this discussion, we hope to unearth some of these relations and make the ties between complexes in applied topology more apparent. 2 Euler Characteristics 2.1 Introduction In mathematics we often find ourselves concerned with the simple task of counting; e.g., cardinality, dimension, etcetera. As one might expect, with differential geometry the story is no different. 2.2 Betti Numbers 2.2.1 Chains and Boundary Operators Within differential geometry, we count using quantities known as Betti numbers, which can easily be related to the number of n-simplexes in a complex, as we will see in the subsequent discussion. -
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. -
0.1 Euler Characteristic
0.1 Euler Characteristic Definition 0.1.1. Let X be a finite CW complex of dimension n and denote by ci the number of i-cells of X. The Euler characteristic of X is defined as: n X i χ(X) = (−1) · ci: (0.1.1) i=0 It is natural to question whether or not the Euler characteristic depends on the cell structure chosen for the space X. As we will see below, this is not the case. For this, it suffices to show that the Euler characteristic depends only on the cellular homology of the space X. Indeed, cellular homology is isomorphic to singular homology, and the latter is independent of the cell structure on X. Recall that if G is a finitely generated abelian group, then G decomposes into a free part and a torsion part, i.e., r G ' Z × Zn1 × · · · Znk : The integer r := rk(G) is the rank of G. The rank is additive in short exact sequences of finitely generated abelian groups. Theorem 0.1.2. The Euler characteristic can be computed as: n X i χ(X) = (−1) · bi(X) (0.1.2) i=0 with bi(X) := rk Hi(X) the i-th Betti number of X. In particular, χ(X) is independent of the chosen cell structure on X. Proof. We use the following notation: Bi = Image(di+1), Zi = ker(di), and Hi = Zi=Bi. Consider a (finite) chain complex of finitely generated abelian groups and the short exact sequences defining homology: dn+1 dn d2 d1 d0 0 / Cn / ::: / C1 / C0 / 0 ι di 0 / Zi / Ci / / Bi−1 / 0 di+1 q 0 / Bi / Zi / Hi / 0 The additivity of rank yields that ci := rk(Ci) = rk(Zi) + rk(Bi−1) and rk(Zi) = rk(Bi) + rk(Hi): Substitute the second equality into the first, multiply the resulting equality by (−1)i, and Pn i sum over i to get that χ(X) = i=0(−1) · rk(Hi). -
Lecture Notes on Foliation Theory
INDIAN INSTITUTE OF TECHNOLOGY BOMBAY Department of Mathematics Seminar Lectures on Foliation Theory 1 : FALL 2008 Lecture 1 Basic requirements for this Seminar Series: Familiarity with the notion of differential manifold, submersion, vector bundles. 1 Some Examples Let us begin with some examples: m d m−d (1) Write R = R × R . As we know this is one of the several cartesian product m decomposition of R . Via the second projection, this can also be thought of as a ‘trivial m−d vector bundle’ of rank d over R . This also gives the trivial example of a codim. d- n d foliation of R , as a decomposition into d-dimensional leaves R × {y} as y varies over m−d R . (2) A little more generally, we may consider any two manifolds M, N and a submersion f : M → N. Here M can be written as a disjoint union of fibres of f each one is a submanifold of dimension equal to dim M − dim N = d. We say f is a submersion of M of codimension d. The manifold structure for the fibres comes from an atlas for M via the surjective form of implicit function theorem since dfp : TpM → Tf(p)N is surjective at every point of M. We would like to consider this description also as a codim d foliation. However, this is also too simple minded one and hence we would call them simple foliations. If the fibres of the submersion are connected as well, then we call it strictly simple. (3) Kronecker Foliation of a Torus Let us now consider something non trivial. -
Math 600 Day 6: Abstract Smooth Manifolds
Math 600 Day 6: Abstract Smooth Manifolds Ryan Blair University of Pennsylvania Tuesday September 28, 2010 Ryan Blair (U Penn) Math 600 Day 6: Abstract Smooth Manifolds Tuesday September 28, 2010 1 / 21 Outline 1 Transition to abstract smooth manifolds Partitions of unity on differentiable manifolds. Ryan Blair (U Penn) Math 600 Day 6: Abstract Smooth Manifolds Tuesday September 28, 2010 2 / 21 A Word About Last Time Theorem (Sard’s Theorem) The set of critical values of a smooth map always has measure zero in the receiving space. Theorem Let A ⊂ Rn be open and let f : A → Rp be a smooth function whose derivative f ′(x) has maximal rank p whenever f (x) = 0. Then f −1(0) is a (n − p)-dimensional manifold in Rn. Ryan Blair (U Penn) Math 600 Day 6: Abstract Smooth Manifolds Tuesday September 28, 2010 3 / 21 Transition to abstract smooth manifolds Transition to abstract smooth manifolds Up to this point, we have viewed smooth manifolds as subsets of Euclidean spaces, and in that setting have defined: 1 coordinate systems 2 manifolds-with-boundary 3 tangent spaces 4 differentiable maps and stated the Chain Rule and Inverse Function Theorem. Ryan Blair (U Penn) Math 600 Day 6: Abstract Smooth Manifolds Tuesday September 28, 2010 4 / 21 Transition to abstract smooth manifolds Now we want to define differentiable (= smooth) manifolds in an abstract setting, without assuming they are subsets of some Euclidean space. Many differentiable manifolds come to our attention this way. Here are just a few examples: 1 tangent and cotangent bundles over smooth manifolds 2 Grassmann manifolds 3 manifolds built by ”surgery” from other manifolds Ryan Blair (U Penn) Math 600 Day 6: Abstract Smooth Manifolds Tuesday September 28, 2010 5 / 21 Transition to abstract smooth manifolds Our starting point is the definition of a topological manifold of dimension n as a topological space Mn in which each point has an open neighborhood homeomorphic to Rn (locally Euclidean property), and which, in addition, is Hausdorff and second countable. -
Recognizing Surfaces
RECOGNIZING SURFACES Ivo Nikolov and Alexandru I. Suciu Mathematics Department College of Arts and Sciences Northeastern University Abstract The subject of this poster is the interplay between the topology and the combinatorics of surfaces. The main problem of Topology is to classify spaces up to continuous deformations, known as homeomorphisms. Under certain conditions, topological invariants that capture qualitative and quantitative properties of spaces lead to the enumeration of homeomorphism types. Surfaces are some of the simplest, yet most interesting topological objects. The poster focuses on the main topological invariants of two-dimensional manifolds—orientability, number of boundary components, genus, and Euler characteristic—and how these invariants solve the classification problem for compact surfaces. The poster introduces a Java applet that was written in Fall, 1998 as a class project for a Topology I course. It implements an algorithm that determines the homeomorphism type of a closed surface from a combinatorial description as a polygon with edges identified in pairs. The input for the applet is a string of integers, encoding the edge identifications. The output of the applet consists of three topological invariants that completely classify the resulting surface. Topology of Surfaces Topology is the abstraction of certain geometrical ideas, such as continuity and closeness. Roughly speaking, topol- ogy is the exploration of manifolds, and of the properties that remain invariant under continuous, invertible transforma- tions, known as homeomorphisms. The basic problem is to classify manifolds according to homeomorphism type. In higher dimensions, this is an impossible task, but, in low di- mensions, it can be done. Surfaces are some of the simplest, yet most interesting topological objects. -
Higher Euler Characteristics: Variations on a Theme of Euler
HIGHER EULER CHARACTERISTICS: VARIATIONS ON A THEME OF EULER NIRANJAN RAMACHANDRAN ABSTRACT. We provide a natural interpretation of the secondary Euler characteristic and gener- alize it to higher Euler characteristics. For a compact oriented manifold of odd dimension, the secondary Euler characteristic recovers the Kervaire semi-characteristic. We prove basic properties of the higher invariants and illustrate their use. We also introduce their motivic variants. Being trivial is our most dreaded pitfall. “Trivial” is relative. Anything grasped as long as two minutes ago seems trivial to a working mathematician. M. Gromov, A few recollections, 2011. The characteristic introduced by L. Euler [7,8,9], (first mentioned in a letter to C. Goldbach dated 14 November 1750) via his celebrated formula V − E + F = 2; is a basic ubiquitous invariant of topological spaces; two extracts from the letter: ...Folgende Proposition aber kann ich nicht recht rigorose demonstriren ··· H + S = A + 2: ...Es nimmt mich Wunder, dass diese allgemeinen proprietates in der Stereome- trie noch von Niemand, so viel mir bekannt, sind angemerkt worden; doch viel mehr aber, dass die furnehmsten¨ davon als theor. 6 et theor. 11 so schwer zu beweisen sind, den ich kann dieselben noch nicht so beweisen, dass ich damit zufrieden bin.... When the Euler characteristic vanishes, other invariants are necessary to study topological spaces. For instance, an odd-dimensional compact oriented manifold has vanishing Euler characteristic; the semi-characteristic of M. Kervaire [16] provides an important invariant of such manifolds. In recent years, the ”secondary” or ”derived” Euler characteristic has made its appearance in many disparate fields [2, 10, 14,4,5, 18,3]; in fact, this secondary invariant dates back to 1848 when it was introduced by A. -
Hausdorff Morita Equivalence of Singular Foliations
Hausdorff Morita Equivalence of singular foliations Alfonso Garmendia∗ Marco Zambony Abstract We introduce a notion of equivalence for singular foliations - understood as suitable families of vector fields - that preserves their transverse geometry. Associated to every singular foliation there is a holonomy groupoid, by the work of Androulidakis-Skandalis. We show that our notion of equivalence is compatible with this assignment, and as a consequence we obtain several invariants. Further, we show that it unifies some of the notions of transverse equivalence for regular foliations that appeared in the 1980's. Contents Introduction 2 1 Background on singular foliations and pullbacks 4 1.1 Singular foliations and their pullbacks . .4 1.2 Relation with pullbacks of Lie groupoids and Lie algebroids . .6 2 Hausdorff Morita equivalence of singular foliations 7 2.1 Definition of Hausdorff Morita equivalence . .7 2.2 First invariants . .9 2.3 Elementary examples . 11 2.4 Examples obtained by pushing forward foliations . 12 2.5 Examples obtained from Morita equivalence of related objects . 15 3 Morita equivalent holonomy groupoids 17 3.1 Holonomy groupoids . 17 arXiv:1803.00896v1 [math.DG] 2 Mar 2018 3.2 Morita equivalent holonomy groupoids: the case of projective foliations . 21 3.3 Pullbacks of foliations and their holonomy groupoids . 21 3.4 Morita equivalence for open topological groupoids . 27 3.5 Holonomy transformations . 29 3.6 Further invariants . 30 3.7 A second look at Hausdorff Morita equivalence of singular foliations . 31 4 Further developments 33 4.1 An extended equivalence for singular foliations . 33 ∗KU Leuven, Department of Mathematics, Celestijnenlaan 200B box 2400, BE-3001 Leuven, Belgium. -
DIFFERENTIAL GEOMETRY COURSE NOTES 1.1. Review of Topology. Definition 1.1. a Topological Space Is a Pair (X,T ) Consisting of A
DIFFERENTIAL GEOMETRY COURSE NOTES KO HONDA 1. REVIEW OF TOPOLOGY AND LINEAR ALGEBRA 1.1. Review of topology. Definition 1.1. A topological space is a pair (X; T ) consisting of a set X and a collection T = fUαg of subsets of X, satisfying the following: (1) ;;X 2 T , (2) if Uα;Uβ 2 T , then Uα \ Uβ 2 T , (3) if Uα 2 T for all α 2 I, then [α2I Uα 2 T . (Here I is an indexing set, and is not necessarily finite.) T is called a topology for X and Uα 2 T is called an open set of X. n Example 1: R = R × R × · · · × R (n times) = f(x1; : : : ; xn) j xi 2 R; i = 1; : : : ; ng, called real n-dimensional space. How to define a topology T on Rn? We would at least like to include open balls of radius r about y 2 Rn: n Br(y) = fx 2 R j jx − yj < rg; where p 2 2 jx − yj = (x1 − y1) + ··· + (xn − yn) : n n Question: Is T0 = fBr(y) j y 2 R ; r 2 (0; 1)g a valid topology for R ? n No, so you must add more open sets to T0 to get a valid topology for R . T = fU j 8y 2 U; 9Br(y) ⊂ Ug: Example 2A: S1 = f(x; y) 2 R2 j x2 + y2 = 1g. A reasonable topology on S1 is the topology induced by the inclusion S1 ⊂ R2. Definition 1.2. Let (X; T ) be a topological space and let f : Y ! X.