Principal Bundles and Bundles with Parabolic Structure

Total Page:16

File Type:pdf, Size:1020Kb

Principal Bundles and Bundles with Parabolic Structure Principal Bundles and Bundles with parabolic structure Arijit Dey January 22, 2013 Abstract In this thesis we prove HN reduction for HIggs G-bundles and nonemptyness of parabolic stable bundles Contents 1 Introduction 5 1.0.1 why and how Parabolic Bundle, little bit of history . 8 1.0.2 Balaji’swork ....................... 8 1.0.3 HintofΓ-Balaji ..................... 8 1.0.4 WorkDoneinshort ................... 8 1.1 Introductiontosecondproblem . 8 1.1.1 MainResults ....................... 12 2 Preliminaries 13 2.1 Higgsbundle ........................... 13 2.2 NonemptynessofParabolicModuli . 19 2.2.1 The category of bundles with parabolic structures . 19 2.2.2 The Kawamata Covering lemma ............ 21 2.2.3 The category of Γ–bundles ................ 22 2.2.4 OnlocaltypesofΓ–bundles . 23 2.3 Qin-Li’s proof for rank r case .................. 29 3 Harder-Narasimhan reduction for Higgs G bundle 30 3.1 ProofofexistenceofaHiggsH-Nreduction . 30 3.2 The Higgs structure on the adjoint bundle EG(g) ...... 35 3.3 Proof of the uniqueness of Higgs H-N reduction . 40 4 Nonnemptyness 45 4.0.1 Preliminaries ....................... 46 4.0.2 Proof of Theorem I ................... 53 4.0.3 ProofofTheoremII . 54 5 holonomy 57 2 6 Ramified G-bundle 61 6.1 H-N reduction for ramified G bundles over a smooth curve . 61 6.1.1 H-N reduction for [Γ,G,N]bundle ........... 63 6.1.2 Proof of H-N reduction for ramified G bundle . 64 3 Acknowledgments I would like to thank Prof. V. Balaji , for suggesting me this problem, for many discussions and for his encouragement. I am very grateful to him for introducing me to the study of moduli spaces of vector bundles. I consider myself very fortunate for having found his generous help. I would like to thank Prof. D. S. Nagaraj who introduced me to algebraic geometry. I would also like to thank Shamindra Kumar Ghosh, Paramita Das and T. Muthukumar for their generous help during my course work of Ph.D program. I have also benefited from discussions with R. Parthasarathi, A. Laddha, S. Nayak and many other people as well as from many seminars and courses at Institute of Mathematical Sciences and Chennai Mathematical Institute. I want to thank Institute of Mathematical Sciences for the fellowship that supported my graduate studies. Without their generous support, this thesis couldn’t have been made. Lastly I would like to thank members of IMSc for giving me a very friendly atmosphere during this work. 4 Chapter 1 Introduction In this chapter we will explain the main results of the thesis using as little mathematical background as possible. We will always work over field of complex numbers. Also we assume that varieties are projective, i.e. there is n an embedding in PC. Moduli spaces are fundamental objects of algebraic geometry which have been at the center of interest since the beginnings of the subject. In a nut- shell, moduli spaces are spaces whose points correspond in a natural way with geometric objects that one would like to study, such as Riemann sur- faces, or vector bundles on a fixed space. Understanding the geometry of moduli spaces often helps to understand the underlying geometric objects themselves. For example in [8] by exploiting moduli space of µ-stable bun- dles on a smooth projective surface Donaldson was able to prove some strik- ing new results on smooth classification of certain projective surfaces, for example there is only one differential structure on Rn except when n = 4, in which case there are uncountably many. Moduli are, however, not only of interest to the algebraic geometer. They also play a role in other subjects, like in theoretical Physics. In this thesis we are interested with holomorphic parabolic vector bun- dles (E,D,α∗,r∗) (often denoted as (E∗) if there is no scope of confusion) with normal crossing parabolic divisor D over X, which is a vector bundle E together with a weighted (α∗) flag structure (r∗) on fibres of E|D (for precise definition of parabolic bundle see chapter 2). To distinguish non-isomorphic parabolic vector bundles of fixed quasi-parabolic structure and parabolic weights, we can define certain invariants called parabolic Chern classes. 2i These are cohomology classes parci(E) ∈ H (X, R), 1 ≤ i ≤ dimC X. We have parci(E)=0if i > rank(E). Even after fixing these discrete invari- 5 ants, we can have continuous families of non-isomorphic parabolic vector bundles. I.e., to specify the isomorphism class of a parabolic vector bundle it is not enough to fix some discrete invariants, but we have to fix also some continuous parameters. For fixed parabolic structure and parabolic Chern classes we would like to define a variety called the moduli space of parabolic vector bundles. Each point of this variety will correspond to a different (at least non-isomorphic) vector bundle. In this thesis first we will study the nonempty-ness of this space for rank 2 parabolic vector bundles over any surfaces and using this we can answer nonempty-ness of higher rank Moduli space of certain type of quasi-parabolic structure. Unfortunately, in order to construct this moduli space we have to restrict our attention to parabolic stable vector bundles (this is not a very strong restriction, since it can be proved that in some sense all parabolic vector bundles can be constructed starting from parabolic stable ones). There are different notions of stability (see 2). Here we will only discuss parabolic Mumford stability (also called parabolic-slope stability). Let X be a projec- tive variety and H an ample divisor. For a parabolic vector bundle E∗ one can define par-degree(E∗)(see chapter 2). We define the parabolic slope of E∗ with respect to H as: par-degree(E ) parµ (E )= ∗ H ∗ rank(E) (the product is the intersection product or cup product in cohomology) E∗ ′ is called parabolic H-stable if for every parabolic subbundle E∗ of E∗ we have ′ parµH (E∗) < parµH (E∗). 0 It can be proved that there is a space PMH (r,D,α∗,pci), called the moduli space of H-stable parabolic vector bundles of rank r and parabolic Chern classes pci (if the quasi-parabolic structure is clear from the context we will drop it from the notation). In many situations it will be a quasi-projective 0 variety (maybe with singularities). In general PMH (r,D,α∗,pci) is not compact but one can compactify this variety in such a way that boundary points correponds to polystable parabolic bundles together with a 0 cycle in X. This compactification is known as Donaldson-Uhlenbeck compacti- fication of parabolic bundles (for details see [4]). Let (X, Θ) be a smooth polarized algebraic surface, this gives rise to a underlying Riemannian mani- fold with metric d. There is an important relationship between gauge theory or Yang-Mills theory and stable holomorphic vector bundles; there is a bi- jection between Θ-stable SU(n) bundles on (X, Θ) and Hermite-Einstein or 6 Anti Self Dual (ASD)1 on a fixed differentiable SU(n) vector bundle over (X,d). This correspondence is known as Hitchin-Kobayashi correspondence. Infact more precisely both these spaces gets a canonical algebraic structure and their underlying topological spacesare homeomorphic. Note that the metric of the manifold appears in the ASD-equation. This is reflected (for bundles) that the stability condition of a bundle depends on the chosen polarization Θ. This relationship has been used, for instance, to calculate Donaldson polynomials for the study of the topology of 4-manifolds [8]. This polynomial denoted as γc2 (X) is of the form : γc (X)(α)= µ(α) ∧··· µα 2 Z Mc2 d 2 2 | {z } where µ : H (X) → H (Mc2 and d = dim(Mc2 )/2 by exploiting the geometry of Mc2 Donaldson was able to prove some strik- ing new results on smooth classification of projective surfaces. By exploiting algebro-geometric description of Mc2 he showed that γc2 (X) is nonzero for large c2. Hence asymptotic nonemptyness is good enough to compute Don- aldson polynomials. While studying the problem of embedding a sphere in a 4-fold Kron- heimer and Mrowka found an analogue of Donaldson polynomial for pairs (X, Σ), where Σ is a surface. They found that obstruction to embedding a sphere into a 4-fold is nonvanishing of this polynomial qk,l. They defined α-twisted anti self dual connections which are actually ASD connection in α X − Σ. let Mk,l be the moduli space of equivalence class of α-twisted connections where α ∈ (0, 1/2) is the holonomy parameter, k is the usual second chern class and l denote the instanton number. In [6] they conjec- tured Hitchin-Kobayashi correspondence i.e. there is a bijection between α-twisted ASD connection and rank 2 stable parabolic bundles (E, L,α) on (X,σ). In their paper they proved this conjecture for some simple case like ruled surfaces and later it was proved in greater generality. for a suitable integer n and is nonzero for large values of c2. In this thesis we prove nonemptiness of rank-2 parabolic stable for ar- bitary c1 and large c2 with suitable bound on α2. The bound on c2 and α2 depends on polarisation. We beleive one should be able to prove Gieseker- Taubes kind of theorem for parabolic bundles for generic choice of parabolic datum, but due to lack of knowledge/patience we could not get such nice theorem. In future we would like to investigate this problem. 1Itoh [11] showed that for SU(n) bundles Hermite-Einstein connection is same as ASD connection 7 1.0.1 why and how Parabolic Bundle, little bit of history 1.0.2 Balaji’s work 1.0.3 Hint of Γ-Balaji 1.0.4 Work Done in short The main strategy used is the categorical correspondence of the category of Γ–bundles of fixed type τ on a certain Kawamata cover Y of the surface X with the category of parabolic bundles on X with fixed parabolic datum (see chapter ?? for definitions and terminology).
Recommended publications
  • Unstable Bundles in Quantum Field Theory
    Contemporary Mathematics Volume 17, 1998 Unstable Bundles in Quantum Field Theory M. Asorey†, F. Falceto† and G. Luz´on‡ Abstract. The relation between connections on 2-dimensional manifolds and holomorphic bundles provides a new perspective on the role of classical gauge fields in quantum field theory in two, three and four dimensions. In particular we show that there is a close relation between unstable bundles and monopoles, sphalerons and instantons. Some of these classical configurations emerge as nodes of quantum vacuum states in non-confining phases of quantum field theory which suggests a relevant role for those configurations in the mechanism of quark confinement in QCD. 1. Introduction The role of principal bundles in the theory of gauge fields is now well established as the kinematical geometric background where classical and quantum fluctuations of gauge fields evolve. However, it is much less known that holomorphic bundles also play a fundamental role in the dynamics of the theory. There are two cases where the theory of holomorphic bundles proved to be very useful in the analysis of the classical dynamics of Yang-Mills fields. The first applica- tion arises in the construction of self-dual solutions of four-dimensional Yang-Mills equations (instantons), i.e. connections which minimize the Yang-Mills functional in non-trivial bundles. U(N) instantons in S4 are in one–to–one correspondence with holomorphic bundles of rank N on CP 3 which are trivial along the canonical U(1) fibres [29]. The second application occurs in 2-D Yang-Mills theory, where arXiv:hep-th/9812173v1 18 Dec 1998 the Yang-Mills functional becomes an almost equivariantly perfect Morse function in the space of 2-D connections [8].
    [Show full text]
  • On Fibre Bundles and Differential Geometry
    Lectures On Fibre Bundles and Differential Geometry By J.L. Koszul Notes by S. Ramanan No part of this book may be reproduced in any form by print, microfilm or any other means without written permission from the Tata Insti- tute of Fundamental Research, Apollo Pier Road, Bombay-1 Tata Institute of Fundamental Research, Bombay 1960 Contents 1 Differential Calculus 1 1.1 .............................. 1 1.2 Derivationlaws ...................... 2 1.3 Derivation laws in associated modules . 4 1.4 TheLiederivative... ..... ...... ..... .. 6 1.5 Lie derivation and exterior product . 8 1.6 Exterior differentiation . 8 1.7 Explicit formula for exterior differentiation . 10 1.8 Exterior differentiation and exterior product . 11 1.9 The curvature form . 12 1.10 Relations between different derivation laws . 16 1.11 Derivation law in C .................... 17 1.12 Connections in pseudo-Riemannian manifolds . 18 1.13 Formulae in local coordinates . 19 2 Differentiable Bundles 21 2.1 .............................. 21 2.2 Homomorphisms of bundles . 22 2.3 Trivial bundles . 23 2.4 Induced bundles . 24 2.5 Examples ......................... 25 2.6 Associated bundles . 26 2.7 Vector fields on manifolds . 29 2.8 Vector fields on differentiable principal bundles . 30 2.9 Projections vector fields . 31 iii iv Contents 3 Connections on Principal Bundles 35 3.1 .............................. 35 3.2 Horizontal vector fields . 37 3.3 Connection form . 39 3.4 Connection on Induced bundles . 39 3.5 Maurer-Cartan equations . 40 3.6 Curvatureforms. 43 3.7 Examples ......................... 46 4 Holonomy Groups 49 4.1 Integral paths . 49 4.2 Displacement along paths . 50 4.3 Holonomygroup ....................
    [Show full text]
  • Group-Valued Momentum Maps for Actions of Automorphism Groups
    Group-valued momentum maps for actions of automorphism groups Tobias Dieza and Tudor S. Ratiub February 5, 2020 The space of smooth sections of a symplectic fiber bundle carries a natural symplectic structure. We provide a general framework to determine the momentum map for the action of the group of bundle automorphism on this space. Since, in general, this action does not admit a classical momentum map, we introduce the more general class of group-valued momentum maps which is inspired by the Poisson Lie setting. In this approach, the group-valued momentum map assigns to every section of the symplectic fiber bundle a principal circle-bundle with connection. The power of this general framework is illustrated in many examples: we construct generalized Clebsch variables for fluids with integral helicity; the anti-canonical bundle turns out to be the momentum map for the action of the group of symplectomorphisms on the space of compatible complex structures; the Teichmüller moduli space is realized as a symplectic orbit reduced space associated to a coadjoint orbit of SL 2; R and spaces related to the other coadjoint orbits are identified and studied.¹ º Moreover, we show that the momentum map for the group of bundle automorphisms on the space of connections over a Riemann surface encodes, besides the curvature, also topological information of the bundle. Keywords: symplectic structure on moduli spaces of geometric structures, infinite- dimensional symplectic geometry, momentum maps, symplectic fiber bundles, differential characters, Kähler geometry, Teichmüller space MSC 2010: 53D20, (58D27, 53C08, 53C10, 58B99, 32G15) a Max Planck Institute for Mathematics in the Sciences, 04103 Leipzig, Germany and Institut für Theoretische Physik, Universität Leipzig, 04009 Leipzig, Germany and Institute of Ap- arXiv:2002.01273v1 [math.DG] 4 Feb 2020 plied Mathematics, Delft University of Technology, 2628 XE Delft, Netherlands.
    [Show full text]
  • Field Theory from a Bundle Point of View
    Field theory from a bundle point of view Laurent Claessens December 8, 2008 2 Contents 1 Differential geometry 9 1.1 Differentiable manifolds ................................ 9 1.1.1 Definition and examples ............................ 9 Example: the sphere .............................. 10 Example: projective space ........................... 10 1.1.2 Topology on manifold and submanifold ................... 10 1.1.3 Tangent vector ................................. 12 1.1.4 Differential of a map .............................. 14 1.1.5 Tangent and cotangent bundle ........................ 15 Tangent bundle ................................. 15 Commutator of vector fields .......................... 16 Some Leibnitz formulas ............................ 16 Cotangent bundle ............................... 17 Exterior algebra ................................ 17 Pull-back and push-forward .......................... 18 Differential of k-forms ............................. 19 Hodge operator ................................. 19 Volume form and orientation ......................... 20 1.1.6 Musical isomorphism .............................. 20 1.1.7 Lie derivative .................................. 20 1.2 Example: Lie groups .................................. 22 1.2.1 Connected component of Lie groups ..................... 22 Õ 1.2.2 The Lie algebra of SUÔ2 ........................... 23 1.2.3 What is g ¡1dg ? ................................ 24 1.2.4 Exponential map ................................ 24 1.2.5 Invariant vector fields ............................
    [Show full text]
  • Connections on Principal Bundles
    LECTURE 5: CONNECTIONS 1. INTRODUCTION:THE MATHEMATICAL FRAMEWORK OF GAUGE THEORIES Gauge theories such are extremely important in physics. Examples are given by Maxwell’s theory of electromagnetism but also the Yang–Mills theories describing the strong and weak forces in the standard model. Central ingredient in this is the choice of a compact Lie group G that physicist call the gauge group. For Maxwell theory this group is abelian, namely G = U(1), but for other important examples this group must be chosen to be nonabelian, e.g. G = SU(N). Mathematically, the framework for such gauge theories is given by the theory of principal bundles. Each ingredient of the phys- ical theory has a solid mathematical meaning in the theory of principal bundles. The table below gives a “dictionary” to translate from physics to mathematics, and back: Physics Mathematics Gauge group Structure group G of a principal bundle P ! M Gauge field Connection A on P Field strength Curvature F(A) Gauge transformation Bundle isomorphism j : P ! P Matter fields in a representation V of G Sections of the associated vector bundle (P × V)/G The most important ingredient of gauge theories is of course the gauge field itself, which, mathematically, corresponds to connections on a principal bundle. The goal of this lecture is to explain what a connection precisely is. We explain this concept on a principal bundle, as well as on a vector bundle, in view of the last item when we want to introduce matter fields. 2. CONNECTIONS In the previous lecture we have discussed the fundamental dichotomy Associated bundle / Principal bundles o Vector bundles Frame bundle Let us briefly recall the associated bundle construction: suppose p : P ! M is a prin- cipal G-bundle, and let V be a representation of G.
    [Show full text]
  • INTRODUCTION to GAUGE THEORY 1. Bundles, Connections
    INTRODUCTION TO GAUGE THEORY LORENZO FOSCOLO 1. Bundles, connections and curvature M smooth manifold + G Lie group with Lie algebra g • principal G–bundle P over M • – smooth manifold P – free right G–action R: P G P × → – smooth projection to orbit space π : P M = P/G → – local G-equivariant trivialisations π 1(U) U G − ≃ × gauge group = Aut(P ) • G principal bundles and vector bundles • – representation ρ: G GL(V ) ❀ vector bundle E = P V → ×ρ e.g. ρ = Ad ❀ adjoint bundle ad P – G = stabiliser of φ r V s V , (E, φ) modelled on (V, φ ) ❀ principal G–bundle 0 ∈ ⊗ ∗ 0 of φ–adapted frames � � Examples: Hopf circle bundle S3 S1, quaternionic Hopf bundle S7 S4, frame bundle • → → Exercise 5.1 A connection on π : P M is a G–invariant splitting T P = ker π H of • → ∗ ⊕ 0 ker π T P π∗T M 0 → ∗ → → → H is called the horizontal subspace 1 Since ker π P g, a connection is a 1-form A: T P g such that Rg∗A = Ad(g− )A • ∗ ≃ × → – Product/trivial connection on M G induced from identification T G G g × ≃ × – loc. trivialisation P U G: A = trivial + a for a g-valued 1-form a on U |U ≃ × – change trivialisation given by u: U G ❀ A = trivial + u 1du + u 1au → − − infinite-dimensional affine space of connections on P modelled on Ω1(M; ad P ) • A Note: action of gauge group on by pull-back G A Exercise 5.2 horizontal lift XH of a vector field X on M: the unique G–invariant vector field on P such • that XH H T P at every point of P and π XH = X ∈ ⊂ ∗ parallel transport of A • – hor.
    [Show full text]
  • Introduction to Quantum Principal Bundles
    INTRODUCTION TO QUANTUM PRINCIPAL BUNDLES MICHO DURDEVICH 1. Introduction In diversity of mathematical concepts and theories a fundamental role is played by those giving a unified treatment of different and at a first sight mutually inde- pendent circles of problems. As far as classical differential geometry is concerned, such a fundamental role is given to the theory of principal bundles. Various basic concepts of theoretical physics are also naturally expressible in the language of principal bundles. Classical gauge theory and general relativity theory are paradigmic examples. But classical geometry is just a very special case of a much deeper quantum geometry. So it is natural to ask what would be the analogs of principal bundles in quantum geometry. And it is reasonable to expect that such quantum principal bundles would play a similar fundamental role in quantum geometry, as is the role of classical principal bundles in classical geometry. A general theory of quantum principal bundles, where quantum groups play the role of structure groups and general quantum spaces play the role of base manifolds, has been developed in [3, 4]. A very brief exposition (without proofs) can be found in [2]. Here we shall discuss basic ideas of the theory of quantum principal bundles, trying to speak informally and paying a special attention to interesting purely quantum phenomenas appearing in the game. It is not difficult to incorporate the basic geometrical idea of a principal bundle, into the noncommutative context. Let G be a compact matrix quantum group [20], represented by a Hopf *-algebra A (here, A plays the role of polynomial functions over G).
    [Show full text]
  • The Topology of Fiber Bundles Lecture Notes Ralph L. Cohen
    The Topology of Fiber Bundles Lecture Notes Ralph L. Cohen Dept. of Mathematics Stanford University Contents Introduction v Chapter 1. Locally Trival Fibrations 1 1. Definitions and examples 1 1.1. Vector Bundles 3 1.2. Lie Groups and Principal Bundles 7 1.3. Clutching Functions and Structure Groups 15 2. Pull Backs and Bundle Algebra 21 2.1. Pull Backs 21 2.2. The tangent bundle of Projective Space 24 2.3. K - theory 25 2.4. Differential Forms 30 2.5. Connections and Curvature 33 2.6. The Levi - Civita Connection 39 Chapter 2. Classification of Bundles 45 1. The homotopy invariance of fiber bundles 45 2. Universal bundles and classifying spaces 50 3. Classifying Gauge Groups 60 4. Existence of universal bundles: the Milnor join construction and the simplicial classifying space 63 4.1. The join construction 63 4.2. Simplicial spaces and classifying spaces 66 5. Some Applications 72 5.1. Line bundles over projective spaces 73 5.2. Structures on bundles and homotopy liftings 74 5.3. Embedded bundles and K -theory 77 5.4. Representations and flat connections 78 Chapter 3. Characteristic Classes 81 1. Preliminaries 81 2. Chern Classes and Stiefel - Whitney Classes 85 iii iv CONTENTS 2.1. The Thom Isomorphism Theorem 88 2.2. The Gysin sequence 94 2.3. Proof of theorem 3.5 95 3. The product formula and the splitting principle 97 4. Applications 102 4.1. Characteristic classes of manifolds 102 4.2. Normal bundles and immersions 105 5. Pontrjagin Classes 108 5.1. Orientations and Complex Conjugates 109 5.2.
    [Show full text]
  • Gauge Theory Summer Term 2009 OTSDAM P EOMETRIE in G
    Christian B¨ar Gauge Theory Summer Term 2009 OTSDAM P EOMETRIE IN G Version of July 26, 2011 c Christian B¨ar 2011. All rights reserved. Picture on the title page is taken from www.sxc.hu Contents Preface v 1 Lie groups and Lie algebras 1 1.1 Liegroups.................................... 1 1.2 Liealgebras................................... 4 1.3 Representations................................. 7 1.4 Theexponentialmap.............................. 15 1.5 Groupactions.................................. 21 2 Bundle theory 31 2.1 Fiberbundles.................................. 31 2.2 Principalbundles................................ 35 2.3 Connections................................... 44 2.4 Curvature.................................... 49 2.5 Characteristicclasses. 53 2.6 Paralleltransport............................... 59 2.7 Gaugetransformations. 69 3 Applications to Physics 73 3.1 TheHodge-staroperator. 73 3.2 Electrodynamics ................................ 78 3.3 Yang-Millsfields ................................ 91 4 Algebraic Topology 101 4.1 Homotopytheory................................101 4.2 Homologytheory ................................110 4.3 Orientations and the fundamental class . 120 5 4-dimensional Manifolds 125 5.1 Theintersectionform ............................. 125 5.2 Classificationresults . 132 5.3 Donaldson’stheorem .............................. 138 iii Preface These are the lecture notes of an introductory course on gauge theory which I taught at Potsdam University in 2009. The aim was to develop the mathematical underpinnings
    [Show full text]
  • A Criterion for Flatness of Sections of Adjoint Bundle of a Holomorphic Principal Bundle Over a Riemann Surface
    Documenta Math. 111 A Criterion for Flatness of Sections of Adjoint Bundle of a Holomorphic Principal Bundle over a Riemann Surface Indranil Biswas Received: August 8, 2013 Communicated by Edward Frenkel Abstract. Let EG be a holomorphic principal G–bundle over a com- pact connected Riemann surface, where G is a connected reductive affine algebraic group defined over C, such that EG admits a holo- 0 morphic connection. Take any β ∈ H (X, ad(EG)), where ad(EG) is the adjoint vector bundle for EG, such that the conjugacy class β(x) ∈ g/G, x ∈ X, is independent of x. We give a sufficient condi- tion for the existence of a holomorphic connection on EG such that β is flat with respect to the induced connection on ad(EG). 2010 Mathematics Subject Classification: 14H60, 14F05, 53C07 Keywords and Phrases: Holomorphic connection, adjoint bundle, flat- ness, canonical connection 1. Introduction A holomorphic vector bundle E over a compact connected Riemann surface X admits a holomorphic connection if and only if every indecomposable com- ponent of E is of degree zero [We], [At]. This criterion generalizes to the holomorphic principal G–bundles over X, where G is a connected reductive affine algebraic group defined over C [AB]. Let EG be a holomorphic principal G–bundle over X, where X and G are as above. Let g denote the Lie algebra of G. Let β be a holomorphic section G of the adjoint vector bundle ad(EG) = EG × g. Our aim here is to find a criterion for the existence of a holomorphic connection on EG such that β is flat with respect to the induced connection on ad(EG).
    [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]