The Geometry of Bundle Gerbes

Total Page:16

File Type:pdf, Size:1020Kb

The Geometry of Bundle Gerbes L'6 "os The Geometry of Bundle Gerbes Daniel Stevenson Thesis submitted for the degree of Doctor of Philosophy in the Department of Pure Mathematics IJniversity of Adelaide 9 February 2000 Abstract This thesis reviews the theory of bundle gerbes and then examines the higher di mensional notion of a bundle 2-gerbe. The notion of a bundle 2-gerbe connection and 2-curving are introduced. and it is shown that there is a class in Ha(M;Z) associated to any bundle 2-gerbe. n IV Acknowledgement I would like to thank my supervisor Michael Murray for his patience, generosity and expert guidance in the writing of this thesis. He has greatly enhanced my under- standing and enjoyment of mathematics over the past few years and I would like to say that it has been an honour to work \Mith him during this time. It is my pleasure also to thank AIan Carey for some useful conversations and also Ann Ross for help in ad- ministrative matters. I would also like to gratefully acknowledge the support provided by an Australian Post Graduate Award. v vl Contents 1 Introduction 1 2 Review of some simplicial techniques b 2.7 Simplicial spaces 5 2.2 Geometric realisation 8 2.3 Classifying sPaces 11 2.4 BPC" bundles 11 3 Review of bundle gerbes 15 3.1 Properties of C* bundles 15 3.2 Bundle gerbes and the Dixmier-Douady class ' 18 3.3 Bundle gerbe connections and the extended Mayer-Vietoris sequence 23 3.4 Bundle gerbe morphisms and the 2-category of bundle gerbes . 25 4 Singular theory of bundle gerbes 35 4.1 Construction of a classifying map 35 4.2 The singular theory of C" bundles 37 4.3 The singular theory of bundle gerbes 4I 5 Open covers 51 5.1 Bundle gerbes via oPen covers 51 5.2 Bundle gerbes and Deligne cohomology 52 6 Gerbes and bundle gerbes Ðl 6.1 Torsors 57 6.2 Sheaves of categories and gerbes 58 6.3 Properties of gerbes 61 64 6.4 The gerbe HOM(P,Q . ' 6.5 The gerbe associated to a bundie gerbe 66 6.6 Higher gluing laws 69 7 Definition of a bundle 2-gerbe 77 7.1 Simplicial bundle gerbes and bundle 2-gerbes 77 7.2 Stable bundle 2-gerbes 80 8 Relationship of bundle 2-gerbes with bicategories 83 8.1 Bicategories 83 8.2 Bundle 2-gerbes over a point and bicategories 92 vll I Some examples of bundle 2-gerbes 97 9.1 The lifting bundle 2-gerbe 97 9.2 The tautological bundle 2-gerbe 98 9.3 The bundle 2-gerbe of a principal G bundle 100 10 Bundle 2-gerbe connections and 2-curvings 103 10.1 Definitions and some preliminary lemmas . 103 10.2 Proof of the main result 106 11 Comparison of the Cech, Deligne and de Rham classes associated to a bundle 2-gerbe 111 11.1 A Õech three class 111 1I.2 A Deligne hypercohomology class 115 11.3 The first Pontryagin class IL7 12 Trivial bundle 2-gerbes 119 12.1 Tfivial bundle 2-gerbes 119 L2.2 T)ivial stable bundle 2-gerbes I28 13 The relationship of bundle 2-gerbes with 2-gerbes 131 13.1 Simplicial gerbes and 2-gerbes 131 vnl Chapter 1 Introduction. There has been much recent interest in applying the theory of gerbes to differential geometry l22l and mathematical physics ([Za] and [13]). Gerbes were originally in- troduced by Giraud (see [19]) and were extensively studied in [7]. Loosely speaking a gerbe is a 'sheaf of categories' except that the¡e is an extra level of complication when one comes to discuss sheaf-iike glueing laws for objects. Much of the importance of gerbes in the previously cited applications stems from the fact that equivalence classes of gerbes over a manifold M are in a bijective correspondence wifh H3(M;V'). This is entirely similar to the fact that H'(M;Z) lsin abijective correspondence with isomorphism classes of principal C" bundles on M. One can think of Ct bundles and gerbes as a geometric 'realisation' or 'represen- tation' of the cohomology of the manifold in dimensions two and three respectively. Flom this perspective it is natural to look for such objects in other dimensions. In dimension zero we can consider the set of all maps f , M + Z which are, in fact, in bijective correspondence with Ho(M;Z). In dimension one there are various kinds of objects we can consider which are in bijective correspondence with H'(M;Z). For exampie we could consider (isomorphism classes of) principalZbundles over M. Or, because the classifying space of. Z is C" we could equally well consider the space of homotopy classes of maps from M into C'. A similar story is true lor H2(M;Z): one could. consider H'(M;Z) to be the set of all homotopy ciasses of maps Í , M - BC', where BCt is the classifying space for the group C', or, we could think of an element of H2(M;Z) corresponding to a homotopy class of maps M -+ BC' as giving rise to a principal Cx bundle on M. In the case of H'(M;Z) we can go one step further and think of a principal C* bundle on M as a principal BZ bundle on M. The crucial fact here, as pointed out in [36], is that BZ, can be chosen to be an abelian topological group since Z is. This last fact is exploited in the paper [1S] by Gajer where the author introduces a notion of a principal BnCx bundle on M and proves that there is a bijection be- tween ¡{n+z(M;Z) and the set of all principai BPC'bundles on M (here BrC' is the pfotd iterated classifying space B...BC" of the group C"). Therefore, when one comes to consider H3(M;Z) there are several possibilities: one option is to think of Ht(M;Z) as the set of all homotopy classes of maps f , M --+ BBC, another is to think of H3(M;Z) as the set of equivalence classes of gerbes on M. Yet another is to follow Gajer and think of. H3(M;Z) as the set of all principal BC" bundles on M or, alternatively, the set of all principal BBZ bundles on M. gerbes give rise In f33] the notion oî. a bundle gerbe was introduced. Bundle also to 1 classes in H3(M;Z). A bundle gerbe on M is a tripie (P,X,M) where ry : X -+ M is a surjection which locally admits sections and where P is a principai CX bundle over thefibre product ylz): X x¡r,tX. P is required tohave aproduct, that is aC" bundle isomorphism which on the fibres of P takes the form P(r",r")Ø Pçqp2¡ - P(rr,rr) for ø1, 12 aîd z3 in the same fibre of X. It can be shown that every bundie gerbe on M gives rise to a gerbe on M. There is a characteristic class associated to bundle gerbes, the Dixmier-Douady class. This is a class in H3(M;Z) which measures the obstruction to the bundle gerbe being 'trivial' in a certain sense. In [7] the notions of a connectiue structure on a gerbe and a curuing for the con- nective structure were introduced. It was shown that one could associate to a gerbe equipped with a connective structure and curving a closed integral three form ø on M - the three curvature of the curving. In [33], it is shown that by considering a connection on P which is compatible with the product above, it is possible to introduce the notion of a bundle gerbe connection and a curving fo¡ a bundle gerbe connection and that, furthermore, a bundle gerbe on M equipped with a bundle gerbe connection and curving gives rise to a closed integrai three form on M. This three form is a repre- sentative of the image of the Dixmier-Douady class of the bundle gerbe in Ë13(M;R.). It can be shown that a bundle gerbe connection and curving on a bundle gerbe induces a connective structure and curving on the gerbe associated to the bundle gerbe. In the series of papers [S] and [9] the authors considered a certain Z-gerbe associated to a principal G bundle P --+ M where G was a compact, simpie, simply connected Lie group. 2-gerbes, introduced in [5], are higher dimensional analogues of gerbes. Broadly speaking, a2-gerbe on M is a'sheaf of bicategories' on M. Bicategories, defined in [1], are higher dimensional analogues of categories. A bicategory consists of a set of objects and for each pair of objects, a category. The objects of this category are then l-arrows of the bicategory and the arrolvs of the category are 2-arrows of the bicategory. As a result, the giueing iaws involved in the definition of a sheaf of bicategories become quite intricate. One can show that if one considers a certain class of 2-gerbes (2-gerbes bound by C") then one can associate an element of. Ha(M;Z) to each 2-gerbe and moreover it can be shown that H (M;Z) is in a bijective correspondence with 'biequivalence' classes of 2-gerbes. In [14] a related object, a bundle 2-gerbe, was introduced. In the latter part of this thesis we will study bundle 2-gerbes using a variation of the definition given in [t4].
Recommended publications
  • Twenty-Five Years of Two-Dimensional Rational Conformal Field Theory
    ZMP-HH/09-21 Hamburger Beitr¨age zur Mathematik Nr. 349 October 2009 TWENTY-FIVE YEARS OF TWO-DIMENSIONAL RATIONAL CONFORMAL FIELD THEORY J¨urgen Fuchs a, Ingo Runkel b and Christoph Schweigert b a Teoretisk fysik, Karlstads Universitet Universitetsgatan 21, S–65188 Karlstad b Organisationseinheit Mathematik, Universit¨at Hamburg Bereich Algebra und Zahlentheorie Bundesstraße 55, D–20146 Hamburg A review for the 50th anniversary of the Journal of Mathematical Physics. 1 Introduction In this article we try to give a condensed panoramic view of the development of two-dimen- sional rational conformal field theory in the last twenty-five years. Given its limited length, our contribution can be, at best, a collection of pointers to the literature. Needless to say, the arXiv:0910.3145v2 [hep-th] 15 Jan 2010 exposition is highly biased, by the taste and the limited knowledge of the authors. We present in advance our apologies to everyone whose work has been inappropriately represented or even omitted. The study of conformal field theories in two dimensions has its origin in several distinct areas of physics: • In the attempt to describe the strong interactions in elementary particle physics in the frame- work of dual models. • Under the label string theory, these models were reinterpreted as a perturbation series containing a gravitational sector. Conformal field theories appear as theories defined on the world sheet that is swept out by the string [56]. • In statistical mechanics, conformal field theory plays a fundamental role in the theory of two- dimensional critical systems [189, 92] by describing fixed points of the renormalization group.
    [Show full text]
  • Arxiv:1401.2824V1 [Math.AT]
    ZMP-HH/14-2 Hamburger Beitr¨age zur Mathematik Nr. 499 January 2014 A Serre-Swan theorem for gerbe modules on ´etale Lie groupoids Christoph Schweigert a, Christopher Tropp b, Alessandro Valentino a a Fachbereich Mathematik, Universit¨at Hamburg Bereich Algebra und Zahlentheorie Bundesstraße 55, D – 20 146 Hamburg b Mathematisches Institut, WWU M¨unster Einsteinstr. 62, D – 48149 M¨unster Abstract Given a bundle gerbe on a compact smooth manifold or, more generally, on a compact ´etale Lie groupoid M, we show that the corresponding category of gerbe modules, if it is non-trivial, is equivalent to the category of finitely generated projective modules over an Azumaya algebra on M. This result can be seen as an equivariant Serre-Swan theorem for twisted vector bundles. 1 Introduction The celebrated Serre-Swan theorem relates the category of vector bundles over a compact smooth manifold M to the category of finite rank projective modules over the algebra of smooth functions C∞(M, C) of M (see [GBV, Mor] for the Serre-Swan theorem in the smooth category). It relates geometric and algebraic notions and is, in particular, the starting point for the definition of vector bundles in non-commutative geometry. arXiv:1401.2824v1 [math.AT] 13 Jan 2014 A bundle gerbe on M can be seen as a geometric realization of its Dixmier-Douady class, which is a class in H3(M; Z). To such a geometric realization, a twisted K-theory group can be associated. Gerbe modules have been introduced to obtain a geometric description of twisted K-theory [BCMMS].
    [Show full text]
  • Fluxes, Bundle Gerbes and 2-Hilbert Spaces
    Lett Math Phys DOI 10.1007/s11005-017-0971-x Fluxes, bundle gerbes and 2-Hilbert spaces Severin Bunk1 · Richard J. Szabo2 Received: 12 January 2017 / Revised: 13 April 2017 / Accepted: 8 May 2017 © The Author(s) 2017. This article is an open access publication Abstract We elaborate on the construction of a prequantum 2-Hilbert space from a bundle gerbe over a 2-plectic manifold, providing the first steps in a programme of higher geometric quantisation of closed strings in flux compactifications and of M5- branes in C-fields. We review in detail the construction of the 2-category of bundle gerbes and introduce the higher geometrical structures necessary to turn their cate- gories of sections into 2-Hilbert spaces. We work out several explicit examples of 2-Hilbert spaces in the context of closed strings and M5-branes on flat space. We also work out the prequantum 2-Hilbert space associated with an M-theory lift of closed strings described by an asymmetric cyclic orbifold of the SU(2) WZW model, pro- viding an example of sections of a torsion gerbe on a curved background. We describe the dimensional reduction of M-theory to string theory in these settings as a map from 2-isomorphism classes of sections of bundle gerbes to sections of corresponding line bundles, which is compatible with the respective monoidal structures and module actions. Keywords Bundle gerbes · Higher geometric quantisation · Fluxes in string and M-theory · Higher geometric structures Mathematics Subject Classification 81S10 · 53Z05 · 18F99 B Severin Bunk [email protected] Richard J.
    [Show full text]
  • A Construction of String 2-Group Modelsusing a Transgression
    A Construction of String 2-Group Models using a Transgression-Regression Technique Konrad Waldorf Fakult¨at f¨ur Mathematik Universit¨at Regensburg Universit¨atsstraße 31 D–93053 Regensburg [email protected] Dedicated to Steven Rosenberg on the occasion of his 60th birthday Abstract In this note we present a new construction of the string group that ends optionally in two different contexts: strict diffeological 2-groups or finite-dimensional Lie 2-groups. It is canonical in the sense that no choices are involved; all the data is written down and can be looked up (at least somewhere). The basis of our construction is the basic gerbe of Gaw¸edzki-Reis and Meinrenken. The main new insight is that under a transgression- regression procedure, the basic gerbe picks up a multiplicative structure coming from the Mickelsson product over the loop group. The conclusion of the construction is a relation between multiplicative gerbes and 2-group extensions for which we use recent work of Schommer-Pries. MSC 2010: Primary 22E67; secondary 53C08, 81T30, 58H05 arXiv:1201.5052v2 [math.DG] 4 May 2012 1 Introduction The string group String(n) is a topological group defined up to homotopy equivalence as the 3-connected cover of Spin(n), for n =3 or n> 4. Concrete models for String(n) have been provided by Stolz [Sto96] and Stolz-Teichner [ST04]. In order to understand, e.g. the differential geometry of String(n), the so-called “string geometry”, it is necessary to have models in better categories than topological groups. Its 3-connectedness implies that String(n) is a K(Z, 2)-fibration over Spin(n), so that it cannot be a (finite-dimensional) Lie group.
    [Show full text]
  • Constructions with Bundle Gerbes
    Constructions with Bundle Gerbes Stuart Johnson Thesis submitted for the degree of Doctor of Philosophy in the School of Pure Mathematics University of Adelaide arXiv:math/0312175v1 [math.DG] 9 Dec 2003 13 December 2002 Abstract This thesis develops the theory of bundle gerbes and examines a number of useful constructions in this theory. These allow us to gain a greater insight into the struc- ture of bundle gerbes and related objects. Furthermore they naturally lead to some interesting applications in physics. i ii Statement of Originality This thesis contains no material which has been accepted for the award of any other degree or diploma at any other university or other tertiary institution and, to the best of my knowledge and belief, contains no material previously published or written by another person, except where due reference has been made in the text. I give consent to this copy of my thesis, when deposited in the University Library, being made available for loan and photocopying. Stuart Johnson Adelaide, 13 December, 2002 iii iv Acknowledgement Firstly I would like to thank my supervisor Michael Murray. He has been extremely helpful, insightful and encouraging at all times and it has been a great pleasure to work with him. I would also like to thank Alan Carey for valuable assistance in the early stages of my work on this thesis and for his continuing support. Thanks are also due to Danny Stevenson for many interesting and helpful conversations and to Ann Ross for always being of assistance with administrative matters. I would also like to acknowledge the support of a University of Adelaide postgraduate scholarship.
    [Show full text]
  • Supersymmetric Field Theories and Orbifold Cohomology
    SUPERSYMMETRIC FIELD THEORIES AND ORBIFOLD COHOMOLOGY A Dissertation Submitted to the Graduate School of the University of Notre Dame in Partial Fulfillment of the Requirements for the Degree of Doctor of Philosophy by Augusto Stoffel Stephan Stolz, Director Graduate Program in Mathematics Notre Dame, Indiana April 2016 SUPERSYMMETRIC FIELD THEORIES AND ORBIFOLD COHOMOLOGY Abstract by Augusto Stoffel Using the Stolz–Teichner framework of supersymmetric Euclidean field theories (EFTs), we provide geometric interpretations of some aspects of the algebraic topology of orbifolds. We begin with a classification of 0j1-dimensional twists for EFTs over an orbifold X, and show that the collection of concordance classes of twisted EFTs over the inertia ΛX is in natural bijection with the delocalized twisted cohomology of X (which is isomorphic to its complexified K-theory). Then, turning to 1j1-dimensional considerations, we construct a (partial) twist functor over X taking as input a class in H3(X; Z). Next, we define a dimensional reduction procedure relating the 0j1-dimensional Euclidean bordism category over ΛX and its 1j1-dimensional counterpart over X, and explore some applications. As a basic example, we show that dimensional reduction of untwisted EFTs over a global quotient orbifold X==G recovers the equivariant Chern character. Finally, we describe the dimensional reduction of the 1j1-twist built earlier, showing that it has the expected relation to twisted K-theory. CONTENTS ACKNOWLEDGMENTS . iv CHAPTER 1: INTRODUCTION . 1 1.1 Supersymmetric field theories and cohomology theories . 1 1.2 Field theories over orbifolds . 4 1.3 Outline of the dissertation . 7 CHAPTER 2: STACKS IN DIFFERENTIAL GEOMETRY .
    [Show full text]
  • Bundle Gerbes Examples Stable Isomorphism Other Things
    Informal definition of p-gerbes Background Bundle gerbes Examples Stable isomorphism Other things Bundle gerbes Michael Murray University of Adelaide http://www.maths.adelaide.edu.au/˜mmurray Principal Bundles, Gerbes and Stacks 2007 Informal definition of p-gerbes Background Bundle gerbes Examples Stable isomorphism Other things Outline 1 Informal definition of p-gerbes 2 Background 3 Bundle gerbes 4 Examples 5 Stable isomorphism 6 Other things Informal definition of p-gerbes Background Bundle gerbes Examples Stable isomorphism Other things Informal definition of p-gerbe Very informally a p-gerbe is a geometric object representing p + 2 dimensional cohomology. The motivating example is p = 0 and two dimensional cohomology. The geometric objects are then U(1) principal bundles or hermitian line bundles. A little less informally a p-gerbe P is an object of some category C. There is a functor C → Man. If M is the image of P under this functor we say P is (a p-gerbe) over M and write P ⇒ M. This functor has to admit pullbacks. If f : N → M is smooth and P ⇒ M there is a unique p-gerbe f ∗(P) ⇒ N and a commuting diagram f ∗(P) → P ⇓ ⇓ f N → M Informal definition of p-gerbes Background Bundle gerbes Examples Stable isomorphism Other things If P and Q are p-gerbes there is a dual P∗ and a product P ⊗ Q. These have to be well-behaved with respect to pullback. Associated to every p-gerbe P ⇒ M there is a characteristic class c(P) ∈ Hp+2(M, Z) which is natural with respect to pullbacks.
    [Show full text]
  • A Note on Bundle Gerbes and Infinite-Dimensionality
    J. Aust. Math. Soc. 90 (2011), 81–92 doi:10.1017/S1446788711001078 A NOTE ON BUNDLE GERBES AND INFINITE-DIMENSIONALITY MICHAEL MURRAY ˛ and DANNY STEVENSON (Received 18 August 2010; accepted 25 October 2010) Communicated by V. Mathai Dedicated to Alan Carey, on the occasion of his 60th birthday Abstract Let .P; Y / be a bundle gerbe over a fibre bundle Y ! M. We show that if M is simply connected and the fibres of Y ! M are connected and finite-dimensional, then the Dixmier–Douady class of .P; Y / is torsion. This corrects and extends an earlier result of the first author. 2010 Mathematics subject classification: primary 53C08. Keywords and phrases: bundle gerbes, Dixmier–Douady class, infinite-dimensionality. 1. Introduction The idea of bundle gerbes T9U had its original motivation in attempts by the first author and Alan Carey to geometrise degree-three cohomology classes. This, in turn, arose from a shared interest in anomalies in quantum field theory resulting from nontrivial cohomology classes in the space of connections modulo gauge transformations. Even in the earliest of their joint papers on anomalies T6U, which demonstrates that the Wess– Zumino–Witten term can be understood as holonomy for a line bundle on the loop group, there is a bundle gerbe, at that time unnoticed, lurking in the background. It was not until some time later that they realised that a better interpretation of the Wess– Zumino–Witten term for a map of a surface into a compact Lie group is as the surface holonomy of the pullback of the basic bundle gerbe over that group T5U.
    [Show full text]
  • A Serre-Swan Theorem for Gerbe Modules Onétale Lie Groupoids
    Theory and Applications of Categories, Vol. 29, No. 28, 2014, pp. 819{835. A SERRE-SWAN THEOREM FOR GERBE MODULES ON ETALE´ LIE GROUPOIDS CHRISTOPH SCHWEIGERT, CHRISTOPHER TROPP AND ALESSANDRO VALENTINO Abstract. Given a torsion bundle gerbe on a compact smooth manifold or, more generally, on a compact ´etaleLie groupoid M, we show that the corresponding category of gerbe modules is equivalent to the category of finitely generated projective modules over an Azumaya algebra on M. This result can be seen as an equivariant Serre-Swan theorem for twisted vector bundles. 1. Introduction The celebrated Serre-Swan theorem relates the category of vector bundles over a compact smooth manifold M to the category of finite rank projective modules over the algebra of smooth functions C1(M; C) of M (see [GBV, Mor] for the Serre-Swan theorem in the smooth category). It relates geometric and algebraic notions and is, in particular, the starting point for the definition of vector bundles in non-commutative geometry. A bundle gerbe on M can be seen as a geometric realization of its Dixmier-Douady class, which is a class in H3(M; Z). To such a geometric realization, a twisted K-theory group can be associated. Gerbe modules have been introduced to obtain a geometric description of twisted K-theory, see e.g. [BCMMS, TXL, BX]. A bundle gerbe (with connection) describes a string background with non-trivial B-field; gerbe modules (with connection) arise also as Chan-Patton bundles on the worldvolume M of D-branes in such backgrounds [Gaw]. It is an old idea that, in the presence of a non-trivial B-field, the worldvolume of a D-brane should become non-commutative in some appropriate sense.
    [Show full text]
  • Many Finite-Dimensional Lifting Bundle Gerbes Are Torsion. 2
    Many finite-dimensional lifting bundle gerbes are 1 torsion. 1 This document is released under a Creative Commons Zero license 2 David Michael Roberts creativecommons.org/publicdomain/zero/1.0/ 2 orcid.org/0000-0002-3478-0522 April 26, 2021 Many bundle gerbes constructed in practice are either infinite-dimensional, or finite-dimensional but built using submersions that are far from be- ing fibre bundles. Murray and Stevenson proved that gerbes on simply- connected manifolds, built from finite-dimensional fibre bundles with connected fibres, always have a torsion DD-class. In this note I prove an analogous result for a wide class of gerbes built from principal bundles, relaxing the requirements on the fundamental group of the base and the connected components of the fibre, allowing both to be nontrivial. This has consequences for possible models for basic gerbes, the classification of crossed modules of finite-dimensional Lie groups, the coefficient Lie-2-algebras for higher gauge theory on principal 2-bundles, and finite-dimensional twists of topological K-theory. 1 Introduction A bundle gerbe [Mur96] is a geometric object that sits over a given space or manifold X classified by elements of H3(X, Z), in the same way that (complex) line bundles on X are classified by elements of H2(X, Z). And, just as line bundles on manifolds have connections 3 giving rise to curvature, a 2-form, giving a class in HdR(X), bundle gerbes have a notion of geometric ‘connection’ data, with curvature a 3 3-form and hence a class in HdR(X). Since de Rham cohomology sees only the non-torsion part of integral cohomology, bundle gerbes that are classified by torsion classes in H3 are thus trickier in one sense to ‘see’ geometrically.
    [Show full text]
  • BUNDLE GERBES and FIELD THEORY 1. Introduction in [Br
    BUNDLE GERBES AND FIELD THEORY ALAN L. CAREY, JOUKO MICKELSSON, AND MICHAEL K. MURRAY Abstract. This paper reviews recent work on a new geometric object called a bundle gerbe and discusses examples arising in quantum field theory. One ap- plication is to an Atiyah-Patodi-Singer index theory construction of the bundle of fermionic Fock spaces parametrized by vector potentials in odd space dimen- sions and a proof that this leads in a simple manner to the known Schwinger terms (Faddeev-Mickelsson cocycle) for the gauge group action. This gives an explicit computation of the Dixmier-Douady class of the associated bundle gerbe. The method works also in other cases of fermions in external fields (external gravitational field, for example) provided that the APS theorem can be applied; however, we have worked out the details only in the case of vec- tor potentials. Another example arises from the WZW model on Riemann surfaces. A common viewpoint for both of these applications is the ‘lifting’ problem for principal bundles formulated in terms of bundle gerbes. The latter is an abstract version of the ‘existence of string structures’ question. 1. Introduction In [Br] Brylinski describes Giraud’s theory of gerbes. Loosely speaking a gerbe over a manifold M is a sheaf of groupoids over M. Gerbes, via their Dixmier- Douady class, provide a geometric realisation of the elements of H3(M, Z) analogous to the way that line bundles provide, via their Chern class, a geometric realisation of the elements of H2(M, Z). There is a simpler way of achieving this end which somewhat surprisingly is nicely adapted to the kind of geometry arising in quantum field theory applications.
    [Show full text]
  • An Introduction to Gerbes
    An Introduction to Gerbes Nino Scalbi May 20, 2020 Instituto Superior T´ecnico Table of Contents 1. Motivation 2. Bundle Gerbes 3. Gerbes via sheaves of groupoids 1 Motivation Given a line bundle L ! M denote by L+ = L − Z(M) where Z : M ! L is the zero section. Then L+ ! M defines a principal C×-bundle over M. × Conversely, given a principal C×-bundle P ! M we denote by P ×C C × the complex line bundle defined as follows: P ×C C = P × C=C× where the action is given by λ · (y; w) = (λ−1 · y; λw). × The assignments L 7! L+ and P 7! P ×C C give an equivalence of categories between the category of complex line bundles over M and the category of principal C×-bundles over M. Complex line and principal C×-bundles Given a smooth manifold M the structures of complex line bundles over M and principal C×-bundles over M are equivalent in the following sense: 2 × Conversely, given a principal C×-bundle P ! M we denote by P ×C C × the complex line bundle defined as follows: P ×C C = P × C=C× where the action is given by λ · (y; w) = (λ−1 · y; λw). × The assignments L 7! L+ and P 7! P ×C C give an equivalence of categories between the category of complex line bundles over M and the category of principal C×-bundles over M. Complex line and principal C×-bundles Given a smooth manifold M the structures of complex line bundles over M and principal C×-bundles over M are equivalent in the following sense: Given a line bundle L ! M denote by L+ = L − Z(M) where Z : M ! L is the zero section.
    [Show full text]