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?WHAT IS... a Gerbe?

Nigel Hitchin

One of the achievements of algebraic is holomorphic gerbe is analogously defined by ∗ to breathe life into obstructions: to turn what pre- functions hαβγ : Uα ∩ Uβ ∩ Uγ → C satisfying vents us from doing something into an object with skew-symmetry in the indices and a cocycle con- structure which allows us to see why we can’t do dition on fourfold intersections. Although this it. Can’t get a single-valued solution to a differen- literal translation of the definition of H2 in Cˇech tial equation? Look at the monodromy, a repre- is not the best way to understand sentation of the fundamental group. Algebraic gerbes, it is adequate to understand the following geometry is similar. Can’t find an elliptic function simple case. Suppose that P is a holomorphic with a zero at p and a pole at q? Look at p − q in 1 ∗ bundle of projective spaces over M. It is defined the group of divisor classes H (M,O ), where M n by patching together the local products Uα × CP is the elliptic curve and O∗ is the of nonzero by transition functions g on U ∩ U with val- holomorphic functions on it. αβ α β ues in the projective linear group PGL(n +1, C). But there is another level of understanding be- Over each open set we can choose a lift g˜ to the yond this, which is the territory where the notion αβ general linear group GL(n +1, C) and set h equal of gerbe lies. Much of the theory of Riemann αβγ surfaces established in the nineteenth century to the scalar matrix g˜αβg˜βγg˜γα. This defines a 2 O∗ treated divisor classes by using meromorphic gerbe: its cohomology class in H (M, ) is the functions and periods of integrals, but nowadays obstruction to finding a rank n +1 vector bundle we find it much easier to use the language of line V such that our given projective space over a point ∗ bundles: an element in H1(M,O ) is an equiva- m ∈ M is the projective space of Vm. lence class of holomorphic line bundles, and the Unfortunately threefold intersections cause a group structure is defined by tensor product for conceptual block. With the transition functions multiplication and dual for the inverse. A modern gαβ of a line bundle, we can patch the local prod- geometer finds it much easier to deal with these ucts Uα × C to get a complex manifold, the total objects, which can be manipulated and conceptu- space of the line bundle. A gerbe, however, is not alized. A holomorphic gerbe is then the geometri- a space, because we can’t patch together in threes. cal object whose equivalence classes are elements There is an alternative to the hαβγ, which is to use 2 O∗ in the next sheaf cohomology group H (M, ). line bundles Lαβ over Uα ∩ Uβ satisfying relations A holomorphic line bundle is defined by tran- like those above for the transition functions gαβ sition functions relative to open sets Uα of a (see [2]). The price to pay is that although we can covering. They are holomorphic functions take products and inverses of line bundles, unlike ∗ gαβ : Uα ∩ Uβ → C functions they do not form a group—only the set of equivalence classes H1(M,O∗) does. Line bun- −1 which satisfy gβα = gαβ and the cocycle condition dles themselves belong instead to a category. In on threefold intersections gαβgβγgγα =1. A −1 particular, the equality gβα = gαβ must be replaced ∼ −1 by a choice of isomorphism L = L . This road is the Savilian Professor of Geometry, Uni- αβ βα versity of Oxford, United Kingdom. His email address is leads to a gerbe being described as in [1] by a sheaf [email protected]. of categories, or in this case.

218 NOTICES OF THE AMS VOLUME 50, NUMBER 2 One way to get a more concrete idea of a gerbe represented by a projective bundle. is to break away from its origins in algebraic geom- This approach forms the basis of the active area etry and see it more as a differential geometric of twisted K-theory. To a bundle of projective object, as its recent appearance in theoretical physics Hilbert spaces one can associate a bundle of Fred- suggests. We now replace local holomorphic holm operators Fred(P), since the scalars act triv- functions hαβγ on a complex manifold by smooth ially by conjugation and the twisted K-group functions and assume that the values lie in the KP (M) is defined to be the space of homotopy group U(1) of unit complex numbers. There is then classes of sections of Fred(P) → M. This group, a the notion of a unitary connection on the gerbe, module over K(M), has generated much interest provided by real differential 1-forms Aαβ and recently, particularly in the theory of D-brane 2-forms Fα such that charges in superstring theory, but quite often ex- −1 plicit calculations using Mayer-Vietoris sequences iAαβ + iAβγ + iAγα = hαβγdhαβγ, are handled by using the line bundles Lαβ defin- Fβ − Fα = dAαβ. ing the gerbe rather than appealing to the infinite- dimensional projective bundle. Then H = dF = dF is a global closed 3-form, α β There is clearly a larger picture here: unitary which is defined to be the curvature of the con- gerbes take their place in a hierarchy, beginning nection. The de Rham class [H/2π] ∈ H3(M,R) is with functions to the circle, then principal circle integral, just as [F/2π] is the first Chern class if F bundles, then gerbes and next 2-gerbes, and so on. is the curvature form for a connection on a line The canonical line bundle of a complex manifold bundle. In another language, equivalence classes is the object underlying the first Chern class, and of gerbes with connection like this have been understanding the geometry of the 2-gerbe behind around for decades in the theory of Cheeger-Simons the first Pontryagin class is one of the challenges differential characters in degree 2. for understanding the next level. The best-known example of a gerbe with con- nection arises when the manifold M is a compact References simple Lie group G. There is a natural gerbe on G [1] J.-L. BRYLINSKI, Loop spaces, characteristic classes and whose curvature is a multiple of the bi-invariant geometric quantization, Progr. Math., vol. 107, 3-form B(X,[Y,Z]), where B is the Killing form— Birkhäuser, Boston, MA, 1993. −1 3 for G = U(n) this is tr(g dg) . Whereas a line [2] N. J. HITCHIN, Lectures on special Lagrangian bundle has holonomy around a closed curve, a submanifolds, Winter School on Mirror Symmetry, gerbe has holonomy around a closed surface. More Vector Bundles and Lagrangian Submanifolds generally, if the curvature of the gerbe vanishes, (Cambridge, MA, 1999), AMS/IP Stud. Adv. Math., then there is holonomy in H2(M,U(1)). As an ex- vol. 23, Amer. Math. Soc., Providence, RI, 2001, ample, B(X,[Y,Z]) vanishes on a maximal torus pp. 151–82. T ⊂ G because T is abelian, so the gerbe is flat there, but the holonomy is nonzero—it is a rather subtle mod 2 invariant of the group. For a map of a closed surface f : Σ → G, the curvature is zero on the 2-manifold Σ; in this case the holonomy evaluated on the fundamental cycle of Σ is the R/Z invari- ant which physicists call the Wess-Zumino term. The integral cohomology class in H3(M,Z) defined by the curvature form of a gerbe with connection exists for topological reasons: in Cˇech cohomology it is represented by δ log hαβγ/2πi. Since the homotopy classes [X,K(Z, 3)] of the Eilenberg-MacLane space K(Z, 3) are just the degree 3 cohomology, a topologist who wants to understand gerbes has to ask himself the question: what structure does this space have? One model for K(Z, 3) which is currently providing the basis for developments of gerbes both in topology and physics is the classifying space BPU(H) for the The “WHAT IS...?” column carries short (one- or two- projective unitary group of Hilbert space. A map page), nontechnical articles aimed at graduate stu- X → BPU(H) defines a bundle of projective Hilbert dents. Each article focuses on a single mathematical spaces over X, and this provides a gerbe just as object, rather than a whole theory. The Notices wel- the earlier finite-dimensional example did. The comes feedback and suggestions for topics for future difference is that the class in H3(X,Z) is (n +1)- columns. Messages may be sent to notices- [email protected]. torsion for PGL(n +1, C), whereas any class can be

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