Foliations and Haefliger Structures
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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. -
The Stable Homotopy of Complex Projective Space
THE STABLE HOMOTOPY OF COMPLEX PROJECTIVE SPACE By GRAEME SEGAL [Received 17 March 1972] 1. Introduction THE object of this note is to prove that the space BU is a direct factor of the space Q(CP°°) = Oto5eo(CP00) = HmQn/Sn(CPto). This is not very n surprising, as Toda [cf. (6) (2.1)] has shown that the homotopy groups of ^(CP00), i.e. the stable homotopy groups of CP00, split in the appro- priate way. But the method, which is Quillen's technique (7) of reducing to a problem about finite groups and then using the Brauer induction theorem, may be interesting. If X and Y are spaces, I shall write {X;7}*for where Y+ means Y together with a disjoint base-point, and [ ; ] means homotopy classes of maps with no conditions about base-points. For fixed Y, X i-> {X; Y}* is a representable cohomology theory. If Y is a topological abelian group the composition YxY ->Y induces and makes { ; Y}* into a multiplicative cohomology theory. In fact it is easy to see that {X; Y}° is then even a A-ring. Let P = CP00, and embed it in the space ZxBU which represents the functor K by P — IXBQCZXBU. This corresponds to the natural inclusion {line bundles} c {virtual vector bundles}. There is an induced map from the suspension-spectrum of P to the spectrum representing l£-theory, inducing a transformation of multiplicative cohomology theories T: { ; P}* -*• K*. PROPOSITION 1. For any space, X the ring-homomorphism T:{X;P}°-*K<>(X) is mirjective. COEOLLAKY. The space QP is (up to homotopy) the product of BU and a space with finite homotopy groups. -
FOLIATIONS Introduction. the Study of Foliations on Manifolds Has a Long
BULLETIN OF THE AMERICAN MATHEMATICAL SOCIETY Volume 80, Number 3, May 1974 FOLIATIONS BY H. BLAINE LAWSON, JR.1 TABLE OF CONTENTS 1. Definitions and general examples. 2. Foliations of dimension-one. 3. Higher dimensional foliations; integrability criteria. 4. Foliations of codimension-one; existence theorems. 5. Notions of equivalence; foliated cobordism groups. 6. The general theory; classifying spaces and characteristic classes for foliations. 7. Results on open manifolds; the classification theory of Gromov-Haefliger-Phillips. 8. Results on closed manifolds; questions of compact leaves and stability. Introduction. The study of foliations on manifolds has a long history in mathematics, even though it did not emerge as a distinct field until the appearance in the 1940's of the work of Ehresmann and Reeb. Since that time, the subject has enjoyed a rapid development, and, at the moment, it is the focus of a great deal of research activity. The purpose of this article is to provide an introduction to the subject and present a picture of the field as it is currently evolving. The treatment will by no means be exhaustive. My original objective was merely to summarize some recent developments in the specialized study of codimension-one foliations on compact manifolds. However, somewhere in the writing I succumbed to the temptation to continue on to interesting, related topics. The end product is essentially a general survey of new results in the field with, of course, the customary bias for areas of personal interest to the author. Since such articles are not written for the specialist, I have spent some time in introducing and motivating the subject. -
3. Tensor Fields
3.1 The tangent bundle. So far we have considered vectors and tensors at a point. We now wish to consider fields of vectors and tensors. The union of all tangent spaces is called the tangent bundle and denoted TM: TM = ∪x∈M TxM . (3.1.1) The tangent bundle can be given a natural manifold structure derived from the manifold structure of M. Let π : TM → M be the natural projection that associates a vector v ∈ TxM to the point x that it is attached to. Let (UA, ΦA) be an atlas on M. We construct an atlas on TM as follows. The domain of a −1 chart is π (UA) = ∪x∈UA TxM, i.e. it consists of all vectors attached to points that belong to UA. The local coordinates of a vector v are (x1,...,xn, v1,...,vn) where (x1,...,xn) are the coordinates of x and v1,...,vn are the components of the vector with respect to the coordinate basis (as in (2.2.7)). One can easily check that a smooth coordinate trasformation on M induces a smooth coordinate transformation on TM (the transformation of the vector components is given by (2.3.10), so if M is of class Cr, TM is of class Cr−1). In a similar way one defines the cotangent bundle ∗ ∗ T M = ∪x∈M Tx M , (3.1.2) the tensor bundles s s TMr = ∪x∈M TxMr (3.1.3) and the bundle of p-forms p p Λ M = ∪x∈M Λx . (3.1.4) 3.2 Vector and tensor fields. -
Notes on Principal Bundles and Classifying Spaces
Notes on principal bundles and classifying spaces Stephen A. Mitchell August 2001 1 Introduction Consider a real n-plane bundle ξ with Euclidean metric. Associated to ξ are a number of auxiliary bundles: disc bundle, sphere bundle, projective bundle, k-frame bundle, etc. Here “bundle” simply means a local product with the indicated fibre. In each case one can show, by easy but repetitive arguments, that the projection map in question is indeed a local product; furthermore, the transition functions are always linear in the sense that they are induced in an obvious way from the linear transition functions of ξ. It turns out that all of this data can be subsumed in a single object: the “principal O(n)-bundle” Pξ, which is just the bundle of orthonormal n-frames. The fact that the transition functions of the various associated bundles are linear can then be formalized in the notion “fibre bundle with structure group O(n)”. If we do not want to consider a Euclidean metric, there is an analogous notion of principal GLnR-bundle; this is the bundle of linearly independent n-frames. More generally, if G is any topological group, a principal G-bundle is a locally trivial free G-space with orbit space B (see below for the precise definition). For example, if G is discrete then a principal G-bundle with connected total space is the same thing as a regular covering map with G as group of deck transformations. Under mild hypotheses there exists a classifying space BG, such that isomorphism classes of principal G-bundles over X are in natural bijective correspondence with [X, BG]. -
WHAT IS a CONNECTION, and WHAT IS IT GOOD FOR? Contents 1. Introduction 2 2. the Search for a Good Directional Derivative 3 3. F
WHAT IS A CONNECTION, AND WHAT IS IT GOOD FOR? TIMOTHY E. GOLDBERG Abstract. In the study of differentiable manifolds, there are several different objects that go by the name of \connection". I will describe some of these objects, and show how they are related to each other. The motivation for many notions of a connection is the search for a sufficiently nice directional derivative, and this will be my starting point as well. The story will by necessity include many supporting characters from differential geometry, all of whom will receive a brief but hopefully sufficient introduction. I apologize for my ungrammatical title. Contents 1. Introduction 2 2. The search for a good directional derivative 3 3. Fiber bundles and Ehresmann connections 7 4. A quick word about curvature 10 5. Principal bundles and principal bundle connections 11 6. Associated bundles 14 7. Vector bundles and Koszul connections 15 8. The tangent bundle 18 References 19 Date: 26 March 2008. 1 1. Introduction In the study of differentiable manifolds, there are several different objects that go by the name of \connection", and this has been confusing me for some time now. One solution to this dilemma was to promise myself that I would some day present a talk about connections in the Olivetti Club at Cornell University. That day has come, and this document contains my notes for this talk. In the interests of brevity, I do not include too many technical details, and instead refer the reader to some lovely references. My main references were [2], [4], and [5]. -
Differential Topology
Differential Topology: Homework Set # 3. 1) Basic on tangent bundles. Recall that the tangent bundle TM to an extrinsicly defined manifold M k ⊂ Rn is defined to be: n n k n ∼ n TM := {(p, v) ∈ R × R | p ∈ M , v ∈ TpM ⊂ TpR = R } This exercise is designed to give you some practice working with tangent bundles. (i) Show that for a manifold M, the tangent bundle TM is well-defined, i.e. does not depend on the embedding M k ⊂ Rn. (ii) If M, N are a pair of smooth manifolds, show that T (M × N) is diffeomorphic to TM × TN. (iii) If f : M → R is a smooth, positive function, show that the corresponding scaling map φ : TM → TM defined by φ(p, v) = (p, f(p) · v) is a diffeomorphism. (iv) Show that the tangent bundle to S1 (the unit sphere) is diffeomorphic to the cylinder S1 × R. (v) Show that if Sn is an arbitrary sphere, then there exists a diffeomorphism between (TSn) × R and Sn × Rn+1. 2) Relatives of the tangent bundle. Closely associated to the tangent bundle are some other manifolds: (i) For an extrinsicly defined manifold M k ⊂ Rn, define the normal bundle as follows: n n k ⊥ n ∼ n N(M) := {(p, v) ∈ R × R | p ∈ M , v ∈ TpM ⊂ TpR = R } Show that N(M) is an n-dimensional manifold. (ii) Show that for the standard n-sphere Sn ⊂ Rn+1, the normal bundle N(Sn) is diffeomorphic to Sn × R. (iii) Consider the subset T 1M of TM consisting of pairs (p, v) ∈ TM with ||v|| = 1 (where || · || denotes the standard norm on Rn). -
Lectures on the Stable Homotopy of BG 1 Preliminaries
Geometry & Topology Monographs 11 (2007) 289–308 289 arXiv version: fonts, pagination and layout may vary from GTM published version Lectures on the stable homotopy of BG STEWART PRIDDY This paper is a survey of the stable homotopy theory of BG for G a finite group. It is based on a series of lectures given at the Summer School associated with the Topology Conference at the Vietnam National University, Hanoi, August 2004. 55P42; 55R35, 20C20 Let G be a finite group. Our goal is to study the stable homotopy of the classifying space BG completed at some prime p. For ease of notation, we shall always assume that any space in question has been p–completed. Our fundamental approach is to decompose the stable type of BG into its various summands. This is useful in addressing many questions in homotopy theory especially when the summands can be identified with simpler or at least better known spaces or spectra. It turns out that the summands of BG appear at various levels related to the subgroup lattice of G. Moreover since we are working at a prime, the modular representation theory of automorphism groups of p–subgroups of G plays a key role. These automorphisms arise from the normalizers of these subgroups exactly as they do in p–local group theory. The end result is that a complete stable decomposition of BG into indecomposable summands can be described (Theorem 6) and its stable homotopy type can be characterized algebraically (Theorem 7) in terms of simple modules of automorphism groups. This paper is a slightly expanded version of lectures given at the International School of the Hanoi Conference on Algebraic Topology, August 2004. -
Vector Bundles and Connections
VECTOR BUNDLES AND CONNECTIONS WERNER BALLMANN The exposition of vector bundles and connections below is taken from my lecture notes on differential geometry at the University of Bonn. I included more material than I usually cover in my lectures. On the other hand, I completely deleted the discussion of “concrete examples”, so that a pinch of salt has to be added by the customer. Standard references for vector bundles and connections are [GHV] and [KN], where the interested reader finds a rather comprehensive discussion of the subject. I would like to thank Andreas Balser for pointing out some misprints. The exposition is still in a preliminary state. Suggestions are very welcome. Contents 1. Vector Bundles 2 1.1. Sections 4 1.2. Frames 5 1.3. Constructions 7 1.4. Pull Back 9 1.5. The Fundamental Lemma on Morphisms 10 2. Connections 12 2.1. Local Data 13 2.2. Induced Connections 15 2.3. Pull Back 16 3. Curvature 18 3.1. Parallel Translation and Curvature 21 4. Miscellanea 26 4.1. Metrics 26 4.2. Cocycles and Bundles 27 References 28 Date: December 1999. Last corrections March 2002. 1 2 WERNERBALLMANN 1. Vector Bundles A bundle is a triple (π,E,M), where π : E → M is a map. In other words, a bundle is nothing else but a map. The term bundle is used −1 when the emphasis is on the preimages Ep := π (p) of the points p ∈ M; we call Ep the fiber of π over p and p the base point of Ep. -
On Manifolds of Negative Curvature, Geodesic Flow, and Ergodicity
ON MANIFOLDS OF NEGATIVE CURVATURE, GEODESIC FLOW, AND ERGODICITY CLAIRE VALVA Abstract. We discuss geodesic flow on manifolds of negative sectional curva- ture. We find that geodesic flow is ergodic on the tangent bundle of a manifold, and present the proof for both n = 2 on surfaces and general n. Contents 1. Introduction 1 2. Riemannian Manifolds 1 2.1. Geodesic Flow 2 2.2. Horospheres and Horocycle Flows 3 2.3. Curvature 4 2.4. Jacobi Fields 4 3. Anosov Flows 4 4. Ergodicity 5 5. Surfaces of Negative Curvature 6 5.1. Fuchsian Groups and Hyperbolic Surfaces 6 6. Geodesic Flow on Hyperbolic Surfaces 7 7. The Ergodicity of Geodesic Flow on Compact Manifolds of Negative Sectional Curvature 8 7.1. Foliations and Absolute Continuity 9 7.2. Proof of Ergodicity 12 Acknowledgments 14 References 14 1. Introduction We want to understand the behavior of geodesic flow on a manifold M of constant negative curvature. If we consider a vector in the unit tangent bundle of M, where does that vector go (or not go) when translated along its unique geodesic path. In a sense, we will show that the vector goes \everywhere," or that the vector visits a full measure subset of T 1M. 2. Riemannian Manifolds We first introduce some of the initial definitions and concepts that allow us to understand Riemannian manifolds. Date: August 2019. 1 2 CLAIRE VALVA Definition 2.1. If M is a differentiable manifold and α :(−, ) ! M is a dif- ferentiable curve, where α(0) = p 2 M, then the tangent vector to the curve α at t = 0 is a function α0(0) : D ! R, where d(f ◦ α) α0(0)f = j dt t=0 for f 2 D, where D is the set of functions on M that are differentiable at p. -
MATH534A, Problem Set 8, Due Nov 13
MATH534A, Problem Set 8, due Nov 13 All problems are worth the same number of points. 1. Let M; N be smooth manifolds of the same dimension, F : M ! N be a smooth map, and let A ⊂ M have measure 0. Prove that F (A) has measure 0. 2. Let M be a smooth manifold, and let A ⊂ M have measure 0. Prove that A 6= M. 3. Let M be a smooth manifold of dimension m, and let π : TM ! M be the natural projection, −1 m m π(p; v) = p. For a chart (U; φ) on M, define φ^: π (U) ! R × R by φ^(p; v) = (φ(p); dpφ(v)): (a) Prove that there is a unique topology on TM such that for any chart (U; φ) on M the set −1 −1 2m π (U) ⊂ TM is open, and φ^ maps π (U) homeomorphically to an open subset of R . (b) Show that TM with this topology is Hausdorff and second countable. Hence show that TM endowed with charts (π−1(U); φ^) is a smooth manifold. 4. (a) Let F : M ! N be a smooth map. Consider the map dF : TM ! TN given by dF (p; v) = (F (p); dpF (v)). This map is sometimes called the global differential of F (but it is also okay to call it the differential of F ). Prove that this map is smooth. n n (b) Let F : M ! R be a smooth map. Consider the map TM ! R given by (p; v) 7! dpF (v). Prove that this map is smooth. -
The Classifying Space of the G-Cobordism Category in Dimension Two
The classifying space of the G-cobordism category in dimension two Carlos Segovia Gonz´alez Instituto de Matem´aticasUNAM Oaxaca, M´exico 29 January 2019 The classifying space I Graeme Segal, Classifying spaces and spectral sequences (1968) I A. Grothendieck, Th´eorie de la descente, etc., S´eminaire Bourbaki,195 (1959-1960) I S. Eilenberg and S. MacLane, Relations between homology and homotopy groups of spaces I and II (1945-1950) I P.S. Aleksandrov-E.Chec,ˇ Nerve of a covering (1920s) I B. Riemann, Moduli space (1857) Definition A simplicial set X is a contravariant functor X : ∆ ! Set from the simplicial category to the category of sets. The geometric realization, denoted by jX j, is the topological space defined as ` jX j := n≥0(∆n × Xn)= ∼, where (s; X (f )a) ∼ (∆f (s); a) for all s 2 ∆n, a 2 Xm, and f :[n] ! [m] in ∆. Definition For a small category C we define the simplicial set N(C), called the nerve, denoted by N(C)n := Fun([n]; C), which consists of all the functors from the category [n] to C. The classifying space of C is the geometric realization of N(C). Denote this by BC := jN(C)j. Properties I The functor B : Cat ! Top sends a category to a topological space, a functor to a continuous map and a natural transformation to a homotopy. 0 0 I B conmutes with products B(C × C ) =∼ BC × BC . I A equivalence of categories gives a homotopy equivalence. I A category with initial or final object is contractil.