Smoothing Maps Into Algebraic Sets and Spaces of Flat Connections

Total Page:16

File Type:pdf, Size:1020Kb

Smoothing Maps Into Algebraic Sets and Spaces of Flat Connections SMOOTHING MAPS INTO ALGEBRAIC SETS AND SPACES OF FLAT CONNECTIONS THOMAS BAIRD AND DANIEL A. RAMRAS n Abstract. Let X ⊂ R be a real algebraic set and M a smooth, closed manifold. We show that all continuous maps M ! X are homotopic (in X) to C1 maps. We apply this result to study characteristic classes of vector bundles associated to continuous families of complex group representations, and we establish lower bounds on the ranks of the homotopy groups of spaces of flat connections over aspherical manifolds. 1. Introduction The first goal of this paper is to prove the following result about the differential topology of algebraic sets. Theorem 1.1 (Section2) . Let X ⊂ Rn be a (possibly singular) real algebraic set, and let f : M ! X be a continuous map from a smooth, closed manifold M. Then there exists a map g : M ! X, and a homotopy H : M × I ! X connecting f and g g, such that the composite M ! X,! Rn is C1. The problem of smoothing maps into algebraic sets seems natural, but we have not found mention of it in the literature. We consulted several experts in real algebraic geometry; some expected our result to hold, and some did not. Our proof proceeds by embedding X as the singular set of an irreducible, quasi- projective variety Y and using a resolution of singularities Ye ! Y for which the inverse image of X is a divisor with normal crossing singularities. Basic facts about neighborhoods of algebraic sets then reduce the problem to the case of normal crossing divisors, which can be handled by differential-geometric means. We note that a small modification of our arguments can prove a version of this result for smoothing out maps from non-compact manifolds into compact algebraic sets. In the remainder of the paper, we apply Theorem 1.1 to study the topology of spaces of flat connections over aspherical manifolds and their associated moduli spaces. In particular, given a discrete group Γ such that BΓ has the homotopy type of a finite CW complex, we study the functorial map B (1) Hom(Γ; GLn(C)) −! Map∗(BΓ; BGLn(C)); from the space of complex-valued group homomorphisms to the space of based continuous maps between classifying spaces. If BΓ is homotopy equivalent to a smooth manifold, then (1) may be interpreted as the inclusion of the moduli space of based flat connections into the moduli space of based connections. We prove The first author was partly supported by an NSERC discovery grant. The second author was partially supported by NSF grants DMS-0804553 and DMS-0968766. 2010 Mathematics Subject Classification. Primary 14P05, 53C05; Secondary 57R20, 55R37. 1 2 THOMAS BAIRD AND DANIEL A. RAMRAS Theorem 1.2 (Section4) . Let Γ be a discrete group such that BΓ has the homotopy k type of a finite, d{dimensional CW complex and let βk(BΓ) = Rank(H (BΓ; Q)). Then for each ρ 2 Hom(Γ; GLn(C)) and each m > 0, the induced map on homotopy groups B∗ : πm (Hom(Γ; GLn(C)); ρ) ! πm (Map∗(BΓ;BGLn(C)); Bρ) P1 satisfies Rank(coker(B∗)) > i=1 βm+2i(BΓ) so long as n > (m + d)=2. The strategy behind the proof of Theorem 1.2 is as follows. The space BGLn(C) n classifies C -vector bundles, so an element in πm (Map∗(BΓ;BGLn(C)); Bρ) deter- mines a vector bundle (up to isomorphism) over Sm ×BΓ. Those classes lying in the m image of B∗ correspond to vector bundles over S × BΓ which admit a connection that is “flat in the BΓ direction." We then deduce, using Chern-Weil theory, that certain Chern classes of these bundles must vanish (see Theorem 3.5). Theorem 1.1 is necessary to make this argument rigorous: to construct the desired connection on the bundle associated to B∗([ ]), we must smooth out the underlying map m from S into the (usually singular) algebraic set Hom(Γ; GLn(C)). In Section 5.2, we prove the following consequence of Theorem 1.2 (recall that U(n) is the maximal compact subgroup of GLn(C)). Corollary 1.3 (Section 5.2). Let M be a closed, smooth, aspherical manifold of dimension d, and let E ! M be a flat principal U(n){bundle over M. Let Aflat(E) denote the space of flat, unitary connections on E. Then for each A0 2 Aflat(E) and for each 0 < m 6 2n − d − 1, we have 1 X Rank (πm(Aflat(E);A0)) > βm+2i+1(M): i=1 P1 Additionally, if i=1 β2i+1(M) > 0 and 2n − d − 1 > 0, then Aflat(E) has infinitely many path components. In particular, the space of flat connections on a flat U(n){bundle (n > 2) over an orientable aspherical 3{manifold has infinitely many path components. This result appears to be new, even for the trivial bundle on the 3{torus, and is in contrast with the case of bundles over surfaces. There, Yang{Mills theory shows that Aflat(E) is highly connected with respect to the rank of E (see Ramras [17, Proposition 4.9], for instance). One fundamental difficulty in proving Corollary 1.3 is that the space of flat connections is not smooth (even in an infinite-dimensional sense) and hence it is unclear whether paths in this space are always homotopic to smooth paths. The methods developed in this paper (Theorem 1.2 in particular) also have applications to the study of Quillen{Lichtenbaum phenomena in the stable topology of representation spaces, as observed for products of surface groups in Ramras [18]. In fact, the desire to understand these phenomena gave rise to the present work. These topics will be discussed in detail elsewhere. Organization: In Section2, we establish our results about maps into real algebraic sets, which are applied to study the characteristic classes in Section3. Theorem 1.2 is proven in Section4, and spaces of flat connections are studied in Section5. Acknowledgements The first author thanks Juan Souto and Frances Kirwan for helpful conversations. The second author thanks Ben Wieland. In addition, the suggestions of the anonymous referees helped to improve the exposition. MAPS INTO ALGEBRAIC SETS AND SPACES OF FLAT CONNECTIONS 3 2. Smoothing maps into real algebraic sets The goal of this section is to prove the following result. Theorem 2.1. Let i : X,! Rn be a real algebraic set and let M be a smooth manifold. Assume that either X or M is compact. Then for every continuous map φ : M ! X there exists a map φ0 : M ! X homotopic to φ such that i ◦ φ0 is smooth.1 The following example helps illustrate the subtlety of Theorem 2.1. Consider the subspace X ⊂ R2 defined as the union of the graph f(x; y) j y = x sin(1=x); x 2 [−1/π; 0) [ (0; 1/π]g [ f(0; 0)g with the polygonal path traveling from (−1/π; 0) to (−1/π; 1) to (1/π; 1) to (1/π; 0). 1 ∼ The subspace X is homeomorphic to S , so π1(X) = Z. However, the non-trivial 1 elements of π1(X) cannot be represented by smooth maps φ : S ! X because the curve x sin(1=x) has infinite arc length. Note, moreover, that just as with the real algebraic sets considered in Theorem 2.1, it is possible to triangulate R2 with X as a subcomplex. This follows from the Schoenflies Theorem (see, for instance, Moise [15, Chapter 10, Theorem 4]) but can in fact be done quite explicitly. For the proof of Theorem 2.1, we assume that M is compact, which is the only case needed in the paper; the argument is similar when X is compact but M is not. Lemma 2.2. Let X ⊂ Rn be a real algebraic set. There exists an irreducible real algebraic set Y ⊂ Rn+2 such that Y is homeomorphic to Rn+1 and the projection map π : Rn+2 = Rn ⊕ R2 ! Rn restricts to a homeomorphism ∼ π : Sing(Y ) −!= X: Proof. We may suppose that X is equal to the zero set of a single polynomial p = p(x1; : : : ; xn), that is: X = Z(p): 2 Introduce new variables y1; y2 and consider the polynomial g(x; y) = p(x) + 2 3 y1 + y2. Define Y = Z(g): It is not hard to verify that the corresponding inclusion Rn ,! Rn+2 identifies X bijectively with the singular locus of Y , so the projection onto Rn identifies Sing(Y ) =∼ X. 2 2 1=3 Given x1; : : : ; xn; y1 2 R, the formula y2 = (g(x; y) − p(x) − y1) gives the unique solution to g(x; y) = 0. Hence Y is homeomorphic to Rn+1. Furthermore, 2 3 the polynomial g(x; y) is irreducible, since its reduction y1 + y2 is irreducible (see, for example, Dummit and Foote [1, Section 9.1]). In particular, a map into X is smooth as a map into Rn if and only if the corresponding map into Sing(Y ) is smooth as a map into Rn+2. We identify X with Sing(Y ) in what follows. The following version of Hironaka's resolution of singularities theorem appears in Koll´ar[13, Theorem 3.27]. 1We use Euclidean topology throughout, except that \irreducible algebraic set" means irre- ducible in the Zariski topology. We will identify all real algebraic sets with their real points throughout this section. 4 THOMAS BAIRD AND DANIEL A. RAMRAS Theorem 2.3. Given a quasiprojective real algebraic variety Y ⊂ Rn+2 with sin- gular set X, there exists a nonsingular real algebraic variety Ye and a birational and projective morphism Π: Ye ! Y which restricts to an isomorphism over Y − X and for which Xe := Π−1(X) is a divisor with simple normal crossings.
Recommended publications
  • Elementary Differential Geometry
    ELEMENTARY DIFFERENTIAL GEOMETRY YONG-GEUN OH { Based on the lecture note of Math 621-2020 in POSTECH { Contents Part 1. Riemannian Geometry 2 1. Parallelism and Ehresman connection 2 2. Affine connections on vector bundles 4 2.1. Local expression of covariant derivatives 6 2.2. Affine connection recovers Ehresmann connection 7 2.3. Curvature 9 2.4. Metrics and Euclidean connections 9 3. Riemannian metrics and Levi-Civita connection 10 3.1. Examples of Riemannian manifolds 12 3.2. Covariant derivative along the curve 13 4. Riemann curvature tensor 15 5. Raising and lowering indices and contractions 17 6. Geodesics and exponential maps 19 7. First variation of arc-length 22 8. Geodesic normal coordinates and geodesic balls 25 9. Hopf-Rinow Theorem 31 10. Classification of constant curvature surfaces 33 11. Second variation of energy 34 Part 2. Symplectic Geometry 39 12. Geometry of cotangent bundles 39 13. Poisson manifolds and Schouten-Nijenhuis bracket 42 13.1. Poisson tensor and Jacobi identity 43 13.2. Lie-Poisson space 44 14. Symplectic forms and the Jacobi identity 45 15. Proof of Darboux' Theorem 47 15.1. Symplectic linear algebra 47 15.2. Moser's deformation method 48 16. Hamiltonian vector fields and diffeomorhpisms 50 17. Autonomous Hamiltonians and conservation law 53 18. Completely integrable systems and action-angle variables 55 18.1. Construction of angle coordinates 56 18.2. Construction of action coordinates 57 18.3. Underlying geometry of the Hamilton-Jacobi method 61 19. Lie groups and Lie algebras 62 1 2 YONG-GEUN OH 20. Group actions and adjoint representations 67 21.
    [Show full text]
  • Complete Connections on Fiber Bundles
    Complete connections on fiber bundles Matias del Hoyo IMPA, Rio de Janeiro, Brazil. Abstract Every smooth fiber bundle admits a complete (Ehresmann) connection. This result appears in several references, with a proof on which we have found a gap, that does not seem possible to remedy. In this note we provide a definite proof for this fact, explain the problem with the previous one, and illustrate with examples. We also establish a version of the theorem involving Riemannian submersions. 1 Introduction: A rather tricky exercise An (Ehresmann) connection on a submersion p : E → B is a smooth distribution H ⊂ T E that is complementary to the kernel of the differential, namely T E = H ⊕ ker dp. The distributions H and ker dp are called horizontal and vertical, respectively, and a curve on E is called horizontal (resp. vertical) if its speed only takes values in H (resp. ker dp). Every submersion admits a connection: we can take for instance a Riemannian metric ηE on E and set H as the distribution orthogonal to the fibers. Given p : E → B a submersion and H ⊂ T E a connection, a smooth curve γ : I → B, t0 ∈ I, locally defines a horizontal lift γ˜e : J → E, t0 ∈ J ⊂ I,γ ˜e(t0)= e, for e an arbitrary point in the fiber. This lift is unique if we require J to be maximal, and depends smoothly on e. The connection H is said to be complete if for every γ its horizontal lifts can be defined in the whole domain. In that case, a curve γ induces diffeomorphisms between the fibers by parallel transport.
    [Show full text]
  • 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].
    [Show full text]
  • Automorphisms of Ehresmann Connections
    Acta Math. Hungar., 123 (4) (2009), 379395. DOI: 10.1007/s10474-008-8139-x First published online December 12, 2008 AUTOMORPHISMS OF EHRESMANN CONNECTIONS J. PÉK and J. SZILASI¤ Institute of Mathematics, University of Debrecen, H-4010 Debrecen, P.O.B. 12, Hungary e-mail: [email protected] (Received July 14, 2008; accepted July 28, 2008) Abstract. We prove that a dieomorphism of a manifold with an Ehresmann connection is an automorphism of the Ehresmann connection, if and only if, it is a totally geodesic map (i.e., sends the geodesics, considered as parametrized curves, to geodesics) and preserves the strong torsion of the Ehresmann connection. This result generalizes and to some extent strengthens the classical theorem on the automorphisms of a D-manifold (manifold with covariant derivative). 1. Introduction It is well-known (and almost trivial) that two covariant derivative oper- ators on a manifold are equal, if and only if, they have the same geodesics and equal torsion tensors. Heuristically, this implies that a dieomorphism of a manifold with a covariant derivative is an automorphism of the covari- ant derivative, if and only if, it is a totally geodesic map (i.e. sends geodesics, considered as parametrized curves, to geodesics) and preserves the torsion. ¤The second author is supported by the Hungarian Nat. Sci. Found. (OTKA), Grant No. NK68040. Key words and phrases: Ehresmann connection, automorphism, strong torsion, totally geodesic map. 2000 Mathematics Subject Classication: 53C05, 53C22. 02365294/$ 20.00 °c 2008 Akadémiai Kiadó, Budapest 380 J. PÉK and J. SZILASI A formal proof of this conceptually important result may be found e.g.
    [Show full text]
  • Projective Connections and the Algebra of Densities
    , Projective Connections and the Algebra of Densities Jacob George School of Mathematics, University of Manchester, Oxford Road, Manchester M13 9PL, UK Abstract. Projective connections first appeared in Cartan’s papers in the 1920’s. Since then they have resurfaced periodically in, for example, integrable systems and perhaps most recently in the context of so called projectively equivariant quantisation. We recall the notion of projective connection and describe its relation with the algebra of densities on a manifold. In particular, we construct a Laplace-type operator on functions using a Thomas projective connection and a symmetric contravariant tensor of rank 2 (‘upper metric’). Keywords: Projective connections, densities PACS: PACS 02.40.Dr Euclidean and projective geometries, PACS 02.10.De Algebraic structures and number theory INTRODUCTION This paper is concerned with the geometry of differential operators on a manifold and their relation with projective connections. The notion of projective connection is an old one, first appearing in Cartan’s papers of the 1920s and then in various modified forms throughout the 20th century. They have surfaced periodically in mathematical physics, in particular in integrable systems and more recently in projectively equivariant quantisation. This paper establishes that the algebra of densities introduced in [1] and projective connections on a given manifold are fundamentally linked. We recall the notion of a projective connection; in fact there are two distinct but related notions which will be detailed here. We define the manifold M (cf. Mˆ in [1]) for which the algebra of densities V(M) may be interpreted as a subalgebra of the algebra of smooth ∞ b functions C (M).
    [Show full text]
  • Ehresmann Connection of Foliation with Singularities
    Russian Mathematics Iz VUZ Izvestiya VUZ Matematika Vol No pp UDC EHRESMANN CONNECTION OF FOLIATION WITH SINGULARITIES AND GLOBAL STABILITY OF LEAVES NI Zhukova Intro duction The theory of connections in b er bundles plays central role in mo dern dierential geometry Unlike the base of b er bundle the top ological space of foliation leaves is in general bad For example the leaf space of linear irrational foliation on the torus T has trivial top ology In the notion of Ehresmann connection for foliations is intro duced as a natural generalization of the Ehresmann connection in b er bundle The construction of Ehresmann connection is based on the existence of parallel transp ort of horizontal curves along vertical curves by the verticalhorizontal homotopy Note that this homotopy has b een already used in the global dierential geometry see e g In the present pap er we dene the Ehresmann connection for the foliation M F with singu larities considered by HJ Sussman and P Stefan as a generalized distribution M on M whichmakes it p ossible to transp ort horizontal curves a curve is horizontal if its tangent vectors lie in M along vertical curves Unlike the regular case such a transp ort is a manyvalued map Therefore we dene the Mholonomy group H L a of an arbitrary leaf L of M F as the M transformation group of the quotient set of horizontal curves A foliation with singularities admitting an Ehresmann connection is called an Ehresmann foli ation We also intro duce generalized Ehresmann foliations such that the horizontal curves are
    [Show full text]
  • Connections on Smooth Lie Algebra Bundles
    Indian J. Pure Appl. Math., 50(4): 891-901, December 2019 °c Indian National Science Academy DOI: 10.1007/s13226-019-0362-3 CONNECTIONS ON SMOOTH LIE ALGEBRA BUNDLES K. Ajaykumar and B. S. Kiranagi Department of Studies in Mathematics, University of Mysore, Mysore 570 006, India e-mails: [email protected]; [email protected] (Received 25 April 2018; accepted 4 September 2018) We define the notion of Lie Ehresmann connection on Lie algebra bundles and show that a Lie connection on a Lie algebra bundle induces a Lie Ehresmann connection. The converse is proved for normed Lie algebra bundles. We then show that the connection on adjoint bundle corre- sponding to the connection on principal G¡bundle to which it is associated is a Lie Ehresmann connection. Further it is shown that the Lie Ehresmann connection on adjoint bundle induced by a universal G-connection is universal over the family of adjoint bundles associated to G-bundles. Key words : Adjoint bundle; Lie algebra bundle; Lie connection; Lie Ehresmann connection; parallel transport, universal connection. 1. INTRODUCTION Transporting a certain motion in the base manifold of a Lie algebra bundle to the motion in its fibres, needs an additional structure. This is provided by the notion of connection on Lie algebra bundle. Mackenzie [9], defines Lie connection on a Lie algebra bundle in terms of covariant derivative by defining Lie connection on Lie algebroids and proves the existence. A proof of the existence of Lie connection on Lie algebra bundles is also in Hasan Gu¨ndog˘an’s diploma thesis [5].
    [Show full text]
  • Connections on Principal Bundles
    Connections on principal bundles Santiago Quintero de los Ríos* December 16, 2020 Contents 1 Connections on principal bundles 1 1.1 Connections as horizontal distributions ........................ 1 1.2 Connections as 1-forms ................................ 3 1.3 Local expressions, or, why physicists did nothing wrong ............... 5 1.4 Horizontal lifts, parallel transport and holonomy ................... 8 2 Curvature 11 2.1 The curvature 2-form and structure equation ..................... 11 2.2 Local expressions (Curvature Edition) ......................... 14 2.3 The exterior covariant derivative ........................... 15 3 The relation with connections on vector bundles 17 3.1 From vector bundles to principal bundles ....................... 17 3.2 Interlude: Associated bundles ............................. 19 3.3 From principal bundles to vector bundles ....................... 22 3.4 In physics language .................................. 24 Notation These notes compile some general facts about connections on principal bundles, and their relation to connections on vector bundles. A few notes on notation: Weare working in the context of a principal 퐺-bundle 푃 over a manifold 휋 푀. This we denote as 퐺 ↪ 푃 → 푀; where 휋 ∶ 푃 → 푀 is the projection map. The right action of 퐺 on 푃 is denoted as 휎 ∶ 푃 ×퐺 → 푃. For any 푔 ∈ 퐺, we denote right multiplication by 푔 as 휎푔 ∶ 푃 → 푃; and for every 푝 ∈ 푃, we denote the orbit map as 휎푝 ∶ 퐺 → 푃. Given a smooth function 푓 ∶ 푀 → 푁 between manifolds, we denote the tangent map at some 푥 ∈ 푀 as 푇푥푓 ∶ 푇푥푀 → 푇푓(푥)푁. This is to explicitly show the functoriality of 푇푥. 1 Connections on principal bundles 1.1 Connections as horizontal distributions Recall that a vector 푣 ∈ 푇푝푃 is called vertical if 푇푝휋(푣) = 0.
    [Show full text]
  • Connections on Principal Bundles
    CONNECTIONS ON PRINCIPAL BUNDLES by Matt Lewis SUBMITTED IN PARTIAL FULFILLMENT OF THE REQUIREMENTS FOR THE DEGREE OF MASTER OF SCIENCE AT DALHOUSIE UNIVERSITY HALIFAX, NOVA SCOTIA DECEMBER 2007 (c) Copyright by Matt Lewis, 2007 Library and Bibliotheque et 1*1 Archives Canada Archives Canada Published Heritage Direction du Branch Patrimoine de I'edition 395 Wellington Street 395, rue Wellington Ottawa ON K1A0N4 Ottawa ON K1A0N4 Canada Canada Your file Votre reference ISBN: 978-0-494-39133-4 Our file Notre reference ISBN: 978-0-494-39133-4 NOTICE: AVIS: The author has granted a non­ L'auteur a accorde une licence non exclusive exclusive license allowing Library permettant a la Bibliotheque et Archives and Archives Canada to reproduce, Canada de reproduire, publier, archiver, publish, archive, preserve, conserve, sauvegarder, conserver, transmettre au public communicate to the public by par telecommunication ou par Plntemet, prefer, telecommunication or on the Internet, distribuer et vendre des theses partout dans loan, distribute and sell theses le monde, a des fins commerciales ou autres, worldwide, for commercial or non­ sur support microforme, papier, electronique commercial purposes, in microform, et/ou autres formats. paper, electronic and/or any other formats. The author retains copyright L'auteur conserve la propriete du droit d'auteur ownership and moral rights in et des droits moraux qui protege cette these. this thesis. Neither the thesis Ni la these ni des extraits substantiels de nor substantial extracts from it celle-ci ne doivent etre imprimes ou autrement may be printed or otherwise reproduits sans son autorisation. reproduced without the author's permission.
    [Show full text]
  • Principal Bundles and Connections
    CHAPTER Principal bundles and connections Motivation Gauge theory The simplest example of a gauge theory in physics is electromagnetism Recall Maxwells equations for an electromagentic eld B homogeneous equations r B r E t and r E r B E j inhomogeneous equations t Here we have chosen units so that and c are equal to E is the electric eld B the magnetic eld j the current density and the electric charge density All of these elds are functions on spacetime R with co ordinates x t and x x x x One can rewrite Maxwells equations in more concise co ordinate free form Let the electromagnetic eld strength F b e the following form on R F dx E dx E dx E dx B dx dx B dx dx B dx dx and dene a chargecurrent density form by J d x dx dx dx j dx dx j dx dx j dx d x k k Also R R b e the star op erator with resp ect to the standard ori entation and the Minkowski metric on R Then Maxwells equations are equivalent to dF homogeneous equations and d F J inhomogeneous equations The inhomogeneous equations require the integrability condition dJ which is easily recognized as charge conservation Note that the Equations are not quite as natural as the homogenous Maxwellequations The homogeneous Maxwell equations make sense 1 k For any pseudoRiemannian manifold M g of dimension n g extends to a metric on T M 2 If M is oriented one therefore obtains a unique oriented volume form such that jjjj The k nk 4 Ho dge star op erator M
    [Show full text]
  • Ehresmann Connections, Metrics and Good Metric Derivatives
    Advanced Studies in Pure Mathematics 48, 2007 Finsler Geometry, Sapporo 2005 − In Memory of Makoto Matsumoto pp. 263–308 Ehresmann connections, metrics and good metric derivatives Rezs˝o L. Lovas, Johanna P´ek and J´ozsef Szilasi Abstract. In this survey we approach some aspects of tangent bundle geom- etry from a new viewpoint. After an outline of our main tools, i.e., the pull-back bundle formalism, we give an overview of Ehresmann connections and covariant derivatives in the pull-back bundle of a tan- gent bundle over itself. Then we define and characterize some special classes of generalized metrics. By a generalized metric we shall mean a pseudo-Riemannian metric tensor in our pull-back bundle. The main new results are contained in Section 5. We shall say, informally, that a metric covariant derivative is ‘good’ if it is related in a natural way to an Ehresmann connection determined by the metric alone. We shall find a family of good metric derivatives for the so-called weakly normal Mo´or – Vanstone metrics and a distinguished good metric derivative for a certain class of Miron metrics. Contents 1. Introduction 264 Acknowledgement 267 2. Framework and tools 268 2.1. Notation 268 2.2. Conventions and basic technicalities 268 2.3. The pull-back bundle π∗τ 271 2.4. Tensors along π 271 2.5. The basic short exact sequence 272 2.6. Brackets 273 2.7. The canonical v-covariant derivative 273 2.8. Lagrangian forms and Hessians 274 2.9. Semisprays and Lagrangian vector fields 274 3.
    [Show full text]
  • A Historical Overview of Connections in Geometry A
    A HISTORICAL OVERVIEW OF CONNECTIONS IN GEOMETRY A Thesis by Kamielle Freeman Bachelor of Arts, Wichita State University, 2008 Submitted to the Department of Mathematics and Statistics and the faculty of the Graduate School of Wichita State University in partial fulfillment of the requirements for the degree of Master of Science May 2011 c Copyright 2011 by Kamielle Freeman All Rights Reserved A HISTORICAL OVERVIEW OF CONNECTIONS IN GEOMETRY The following faculty members have examined the final copy of this thesis for form and content, and recommend that it be accepted in partial fulfillment of the requirement for the degree of Master of Science with a major in Mathematics. Phillip E. Parker, Committee Chair Thalia Jeffres, Committee Member Elizabeth Behrman, Committee Member iii DEDICATION To Pandora. This thesis was accomplished for you and in spite of you. iv \Mathematics is very akin to Art; a mathematical theory not only must be rigorous, but it must also satisfy our mind in quest of simplicity, of harmony, of beauty..." |Charles Ehresmann v ACKNOWLEDGEMENTS I would like to thank Esau Freeman and Denise Unruh for making this thesis possible through their loving support, Dr. Phillip E. Parker for his mentoring and excellent mathe- matical instruction, Emma Traore Zohner for help translating, Raja Balakrishnan and Justin Ryan for their helpful conversations and proof-reading, and all of my friends on the 3rd floor of Jabara Hall for their encouraging words and moral support. vi ABSTRACT This thesis is an attempt to untangle/clarify the modern theory of connections in Geometry. Towards this end a historical approach was taken and original as well as secondary sources were used.
    [Show full text]