An Introduction to Equivariant Cohomology and the Equivariant first Chern Class UROP+ Final Paper, Summer 2017
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Connections on Bundles Md
Dhaka Univ. J. Sci. 60(2): 191-195, 2012 (July) Connections on Bundles Md. Showkat Ali, Md. Mirazul Islam, Farzana Nasrin, Md. Abu Hanif Sarkar and Tanzia Zerin Khan Department of Mathematics, University of Dhaka, Dhaka 1000, Bangladesh, Email: [email protected] Received on 25. 05. 2011.Accepted for Publication on 15. 12. 2011 Abstract This paper is a survey of the basic theory of connection on bundles. A connection on tangent bundle , is called an affine connection on an -dimensional smooth manifold . By the general discussion of affine connection on vector bundles that necessarily exists on which is compatible with tensors. I. Introduction = < , > (2) In order to differentiate sections of a vector bundle [5] or where <, > represents the pairing between and ∗. vector fields on a manifold we need to introduce a Then is a section of , called the absolute differential structure called the connection on a vector bundle. For quotient or the covariant derivative of the section along . example, an affine connection is a structure attached to a differentiable manifold so that we can differentiate its Theorem 1. A connection always exists on a vector bundle. tensor fields. We first introduce the general theorem of Proof. Choose a coordinate covering { }∈ of . Since connections on vector bundles. Then we study the tangent vector bundles are trivial locally, we may assume that there is bundle. is a -dimensional vector bundle determine local frame field for any . By the local structure of intrinsically by the differentiable structure [8] of an - connections, we need only construct a × matrix on dimensional smooth manifold . each such that the matrices satisfy II. -
Vector Bundles on Projective Space
Vector Bundles on Projective Space Takumi Murayama December 1, 2013 1 Preliminaries on vector bundles Let X be a (quasi-projective) variety over k. We follow [Sha13, Chap. 6, x1.2]. Definition. A family of vector spaces over X is a morphism of varieties π : E ! X −1 such that for each x 2 X, the fiber Ex := π (x) is isomorphic to a vector space r 0 0 Ak(x).A morphism of a family of vector spaces π : E ! X and π : E ! X is a morphism f : E ! E0 such that the following diagram commutes: f E E0 π π0 X 0 and the map fx : Ex ! Ex is linear over k(x). f is an isomorphism if fx is an isomorphism for all x. A vector bundle is a family of vector spaces that is locally trivial, i.e., for each x 2 X, there exists a neighborhood U 3 x such that there is an isomorphism ': π−1(U) !∼ U × Ar that is an isomorphism of families of vector spaces by the following diagram: −1 ∼ r π (U) ' U × A (1.1) π pr1 U −1 where pr1 denotes the first projection. We call π (U) ! U the restriction of the vector bundle π : E ! X onto U, denoted by EjU . r is locally constant, hence is constant on every irreducible component of X. If it is constant everywhere on X, we call r the rank of the vector bundle. 1 The following lemma tells us how local trivializations of a vector bundle glue together on the entire space X. -
Characteristic Classes and K-Theory Oscar Randal-Williams
Characteristic classes and K-theory Oscar Randal-Williams https://www.dpmms.cam.ac.uk/∼or257/teaching/notes/Kthy.pdf 1 Vector bundles 1 1.1 Vector bundles . 1 1.2 Inner products . 5 1.3 Embedding into trivial bundles . 6 1.4 Classification and concordance . 7 1.5 Clutching . 8 2 Characteristic classes 10 2.1 Recollections on Thom and Euler classes . 10 2.2 The projective bundle formula . 12 2.3 Chern classes . 14 2.4 Stiefel–Whitney classes . 16 2.5 Pontrjagin classes . 17 2.6 The splitting principle . 17 2.7 The Euler class revisited . 18 2.8 Examples . 18 2.9 Some tangent bundles . 20 2.10 Nonimmersions . 21 3 K-theory 23 3.1 The functor K ................................. 23 3.2 The fundamental product theorem . 26 3.3 Bott periodicity and the cohomological structure of K-theory . 28 3.4 The Mayer–Vietoris sequence . 36 3.5 The Fundamental Product Theorem for K−1 . 36 3.6 K-theory and degree . 38 4 Further structure of K-theory 39 4.1 The yoga of symmetric polynomials . 39 4.2 The Chern character . 41 n 4.3 K-theory of CP and the projective bundle formula . 44 4.4 K-theory Chern classes and exterior powers . 46 4.5 The K-theory Thom isomorphism, Euler class, and Gysin sequence . 47 n 4.6 K-theory of RP ................................ 49 4.7 Adams operations . 51 4.8 The Hopf invariant . 53 4.9 Correction classes . 55 4.10 Gysin maps and topological Grothendieck–Riemann–Roch . 58 Last updated May 22, 2018. -
Formal GAGA for Good Moduli Spaces
FORMAL GAGA FOR GOOD MODULI SPACES ANTON GERASCHENKO AND DAVID ZUREICK-BROWN Abstract. We prove formal GAGA for good moduli space morphisms under an assumption of “enough vector bundles” (which holds for instance for quotient stacks). This supports the philoso- phy that though they are non-separated, good moduli space morphisms largely behave like proper morphisms. 1. Introduction Good moduli space morphisms are a common generalization of good quotients by linearly re- ductive group schemes [GIT] and coarse moduli spaces of tame Artin stacks [AOV08, Definition 3.1]. Definition ([Alp13, Definition 4.1]). A quasi-compact and quasi-separated morphism of locally Noetherian algebraic stacks φ: X → Y is a good moduli space morphism if • (φ is Stein) the morphism OY → φ∗OX is an isomorphism, and • (φ is cohomologically affine) the functor φ∗ : QCoh(OX ) → QCoh(OY ) is exact. If φ: X → Y is such a morphism, then any morphism from X to an algebraic space factors through φ [Alp13, Theorem 6.6].1 In particular, if there exists a good moduli space morphism φ: X → X where X is an algebraic space, then X is determined up to unique isomorphism. In this case, X is said to be the good moduli space of X . If X = [U/G], this corresponds to X being a good quotient of U by G in the sense of [GIT] (e.g. for a linearly reductive G, [Spec R/G] → Spec RG is a good moduli space). In many respects, good moduli space morphisms behave like proper morphisms. They are uni- versally closed [Alp13, Theorem 4.16(ii)] and weakly separated [ASvdW10, Proposition 2.17], but since points of X can have non-proper stabilizer groups, good moduli space morphisms are gen- erally not separated (e.g. -
256B Algebraic Geometry
256B Algebraic Geometry David Nadler Notes by Qiaochu Yuan Spring 2013 1 Vector bundles on the projective line This semester we will be focusing on coherent sheaves on smooth projective complex varieties. The organizing framework for this class will be a 2-dimensional topological field theory called the B-model. Topics will include 1. Vector bundles and coherent sheaves 2. Cohomology, derived categories, and derived functors (in the differential graded setting) 3. Grothendieck-Serre duality 4. Reconstruction theorems (Bondal-Orlov, Tannaka, Gabriel) 5. Hochschild homology, Chern classes, Grothendieck-Riemann-Roch For now we'll introduce enough background to talk about vector bundles on P1. We'll regard varieties as subsets of PN for some N. Projective will mean that we look at closed subsets (with respect to the Zariski topology). The reason is that if p : X ! pt is the unique map from such a subset X to a point, then we can (derived) push forward a bounded complex of coherent sheaves M on X to a bounded complex of coherent sheaves on a point Rp∗(M). Smooth will mean the following. If x 2 X is a point, then locally x is cut out by 2 a maximal ideal mx of functions vanishing on x. Smooth means that dim mx=mx = dim X. (In general it may be bigger.) Intuitively it means that locally at x the variety X looks like a manifold, and one way to make this precise is that the completion of the local ring at x is isomorphic to a power series ring C[[x1; :::xn]]; this is the ring where Taylor series expansions live. -
K-Theory and Characteristic Classes in Topology and Complex Geometry (A Tribute to Atiyah and Hirzebruch)
K-theory and characteristic classes in topology and complex geometry (a tribute to Atiyah and Hirzebruch) Claire Voisin CNRS, Institut de math´ematiquesde Jussieu CMSA Harvard, May 25th, 2021 Plan of the talk I. The early days of Riemann-Roch • Characteristic classes of complex vector bundles • Hirzebruch-Riemann-Roch. Ref. F. Hirzebruch. Topological Methods in Algebraic Geometry (German, 1956, English 1966) II. K-theory and cycle class • The Atiyah-Hirzebruch spectral sequence and cycle class with integral coefficients. • Resolutions and Chern classes of coherent sheaves Ref. M. Atiyah, F. Hirzebruch. Analytic cycles on complex manifolds (1962) III. Later developments on the cycle class • Complex cobordism ring. Kernel and cokernel of the cycle class map. • Algebraic K-theory and the Bloch-Ogus spectral sequence The Riemann-Roch formula for curves • X= compact Riemann surface (= smooth projective complex curve). E ! X a holomorphic vector bundle on X. •E the sheaf of holomorphic sections of E. Sheaf cohomology H0(X; E)= global sections, H1(X; E) (eg. computed as Cˇech cohomology). Def. (holomorphic Euler-Poincar´echaracteristic) χ(X; E) := h0(X; E) − h1(X; E). • E has a rank r and a degree deg E = deg (det E) := e(det E). • X has a genus related to the topological Euler-Poincar´echaracteristic: 2 − 2g = χtop(X). • Hopf formula: 2g − 2 = deg KX , where KX is the canonical bundle (dual of the tangent bundle). Thm. (Riemann-Roch formula) χ(X; E) = deg E + r(1 − g) Sketch of proof Sketch of proof. (a) Reduction to line bundles: any E has a filtration by subbundles Ei such that Ei=Ei+1 is a line bundle. -
The Chern Characteristic Classes
The Chern characteristic classes Y. X. Zhao I. FUNDAMENTAL BUNDLE OF QUANTUM MECHANICS Consider a nD Hilbert space H. Qauntum states are normalized vectors in H up to phase factors. Therefore, more exactly a quantum state j i should be described by the density matrix, the projector to the 1D subspace generated by j i, P = j ih j: (I.1) n−1 All quantum states P comprise the projective space P H of H, and pH ≈ CP . If we exclude zero point from H, there is a natural projection from H − f0g to P H, π : H − f0g ! P H: (I.2) On the other hand, there is a tautological line bundle T (P H) over over P H, where over the point P the fiber T is the complex line generated by j i. Therefore, there is the pullback line bundle π∗L(P H) over H − f0g and the line bundle morphism, π~ π∗T (P H) T (P H) π H − f0g P H . Then, a bundle of Hilbert spaces E over a base space B, which may be a parameter space, such as momentum space, of a quantum system, or a phase space. We can repeat the above construction for a single Hilbert space to the vector bundle E with zero section 0B excluded. We obtain the projective bundle PEconsisting of points (P x ; x) (I.3) where j xi 2 Hx; x 2 B: (I.4) 2 Obviously, PE is a bundle over B, p : PE ! B; (I.5) n−1 where each fiber (PE)x ≈ CP . -
Differential Geometry of Complex Vector Bundles
DIFFERENTIAL GEOMETRY OF COMPLEX VECTOR BUNDLES by Shoshichi Kobayashi This is re-typesetting of the book first published as PUBLICATIONS OF THE MATHEMATICAL SOCIETY OF JAPAN 15 DIFFERENTIAL GEOMETRY OF COMPLEX VECTOR BUNDLES by Shoshichi Kobayashi Kan^oMemorial Lectures 5 Iwanami Shoten, Publishers and Princeton University Press 1987 The present work was typeset by AMS-LATEX, the TEX macro systems of the American Mathematical Society. TEX is the trademark of the American Mathematical Society. ⃝c 2013 by the Mathematical Society of Japan. All rights reserved. The Mathematical Society of Japan retains the copyright of the present work. No part of this work may be reproduced, stored in a retrieval system, or transmitted, in any form or by any means, electronic, mechanical, photocopying, recording or otherwise, without the prior permission of the copy- right owner. Dedicated to Professor Kentaro Yano It was some 35 years ago that I learned from him Bochner's method of proving vanishing theorems, which plays a central role in this book. Preface In order to construct good moduli spaces for vector bundles over algebraic curves, Mumford introduced the concept of a stable vector bundle. This concept has been generalized to vector bundles and, more generally, coherent sheaves over algebraic manifolds by Takemoto, Bogomolov and Gieseker. As the dif- ferential geometric counterpart to the stability, I introduced the concept of an Einstein{Hermitian vector bundle. The main purpose of this book is to lay a foundation for the theory of Einstein{Hermitian vector bundles. We shall not give a detailed introduction here in this preface since the table of contents is fairly self-explanatory and, furthermore, each chapter is headed by a brief introduction. -
Vector Bundles. Characteristic Classes. Cobordism. Applications
Math 754 Chapter IV: Vector Bundles. Characteristic classes. Cobordism. Applications Laurenţiu Maxim Department of Mathematics University of Wisconsin [email protected] May 3, 2018 Contents 1 Chern classes of complex vector bundles 2 2 Chern classes of complex vector bundles 2 3 Stiefel-Whitney classes of real vector bundles 5 4 Stiefel-Whitney classes of manifolds and applications 5 4.1 The embedding problem . .6 4.2 Boundary Problem. .9 5 Pontrjagin classes 11 5.1 Applications to the embedding problem . 14 6 Oriented cobordism and Pontrjagin numbers 15 7 Signature as an oriented cobordism invariant 17 8 Exotic 7-spheres 19 9 Exercises 20 1 1 Chern classes of complex vector bundles 2 Chern classes of complex vector bundles We begin with the following Proposition 2.1. ∗ ∼ H (BU(n); Z) = Z [c1; ··· ; cn] ; with deg ci = 2i ∗ Proof. Recall that H (U(n); Z) is a free Z-algebra on odd degree generators x1; ··· ; x2n−1, with deg(xi) = i, i.e., ∗ ∼ H (U(n); Z) = ΛZ[x1; ··· ; x2n−1]: Then using the Leray-Serre spectral sequence for the universal U(n)-bundle, and using the fact that EU(n) is contractible, yields the desired result. Alternatively, the functoriality of the universal bundle construction yields that for any subgroup H < G of a topological group G, there is a fibration G=H ,! BH ! BG. In our A 0 case, consider U(n − 1) as a subgroup of U(n) via the identification A 7! . Hence, 0 1 there exists fibration U(n)=U(n − 1) ∼= S2n−1 ,! BU(n − 1) ! BU(n): Then the Leray-Serre spectral sequence and induction on n gives the desired result, where 1 ∗ 1 ∼ we use the fact that BU(1) ' CP and H (CP ; Z) = Z[c] with deg c = 2. -
Arxiv:1505.02430V1 [Math.CT] 10 May 2015 Bundle Functors and Fibrations
Bundle functors and fibrations Anders Kock Introduction The notions of bundle, and bundle functor, are useful and well exploited notions in topology and differential geometry, cf. e.g. [12], as well as in other branches of mathematics. The category theoretic set up relevant for these notions is that of fibred category, likewise a well exploited notion, but for certain considerations in the context of bundle functors, it can be carried further. In particular, we formalize and develop, in terms of fibred categories, some of the differential geometric con- structions: tangent- and cotangent bundles, (being examples of bundle functors, respectively star-bundle functors, as in [12]), as well as jet bundles (where the for- mulation of the functorality properties, in terms of fibered categories, is probably new). Part of the development in the present note was expounded in [11], and is repeated almost verbatim in the Sections 2 and 4 below. These sections may have interest as a piece of pure category theory, not referring to differential geometry. 1 Basics on Cartesian arrows We recall here some classical notions. arXiv:1505.02430v1 [math.CT] 10 May 2015 Let π : X → B be any functor. For α : A → B in B, and for objects X,Y ∈ X with π(X) = A and π(Y ) = B, let homα (X,Y) be the set of arrows h : X → Y in X with π(h) = α. The fibre over A ∈ B is the category, denoted XA, whose objects are the X ∈ X with π(X) = A, and whose arrows are arrows in X which by π map to 1A; such arrows are called vertical (over A). -
Cohomology of Line Bundles: Proof Of
arXiv:1003.5217 Cohomology of Line Bundles: A Computational Algorithm Ralph Blumenhagen,1,2, a) Benjamin Jurke,1,2, b) Thorsten Rahn,1, c) and Helmut Roschy1, d) 1)Max-Planck-Institut f¨ur Physik, F¨ohringer Ring 6, 80805 M¨unchen, Germany 2)Kavli Institute for Theoretical Physics, Kohn Hall, UCSB, Santa Barbara, CA 93106, USA (Dated: 29 October 2010) We present an algorithm for computing line bundle valued cohomology classes over toric varieties. This is the basic starting point for computing massless modes in both heterotic and Type IIB/F-theory compactifica- tions, where the manifolds of interest are complete intersections of hypersurfaces in toric varieties supporting additional vector bundles. CONTENTS classes Hi(Y ; V ) of the vector bundle V over a Calabi- Yau three-fold Y . The largest class of such Calabi-Yau I. Introduction 1 threefolds is given by complete intersections over toric ambient varieties X. For the vector bundles various con- II. Algorithm for line bundle cohomology 2 structions have been discussed in the literature. The A. Preliminaries 2 three most prominent ones are, on the one hand, monad B. Cechˇ cohomology for P2 3 and extension constructions, for which the vector bundle C. A preliminary algorithm conjecture 4 is defined via (exact) sequences of direct sums of line bun- D. Further examples 4 dles. On the other hand, for elliptically fibered Calabi- delPezzo-1surface 4 Yau manifolds, the spectral cover construction provides a large class of stable holomorphic vector bundles. How- delPezzo-3surface 5 ever, in all three cases, the computation of the massless E. -
CHERN CLASSES Juan Moreno
CHERN CLASSES Juan Moreno §1. INTRODUCTION A characteristic class associates to a vector bundle ! (E,¼,B) a cohomology class ® H¤(B), which Æ ! 2 respects bundle maps, that is, if f : ! ´ is a bundle map, then f ¤® ® . Chern classes, denoted ! ´ Æ ! ck(!) for k N, are characteristic classes associated to complex vector bundles which satisfy the 2 following properties: 0 2k • c0(!) 1 H (B), ck(!) H (B), k N. Æ 2 2 8 2 n • Let C denote the trival rank n complex vector bundle. Then ck(E) 0, k 0. Æ 8 È • If rank(!) n then ck(!) 0 for all k n. Æ Æ È P • Let c(!) denote the formal sum i ci(!) called the total Chern class. Then we have the Whitney Product formula c(! ´) c(!)c(´). © Æ One can give an axiomatic definition of Chern classes, however, we will instead focus on definitions which are more tractible for computations, and give intuition as to what the Chern classes measure. We will give two different perspectives on Chern classes: the first is uses an auxilliary characteristic class, while the second uses the geometry of a connection. These notes do not present a full intro- duction to Chern classes. In particular, we do not provide any proofs of these important properties described above. The purpose of these notes is simply to give explicit constructions of Chern classes so that one can compute them at least for simple examples. For a detailed account of Chern classes and the theory of characteristic classes in general see [Sta74]. In order to construct characteristic classes we must fix a particular cohomology theory to work with.