The Cohomology Ring of the Real Locus of the Moduli Space of Stable Curves of Genus 0 with Marked Points
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The Decomposition Theorem, Perverse Sheaves and the Topology Of
The decomposition theorem, perverse sheaves and the topology of algebraic maps Mark Andrea A. de Cataldo and Luca Migliorini∗ Abstract We give a motivated introduction to the theory of perverse sheaves, culminating in the decomposition theorem of Beilinson, Bernstein, Deligne and Gabber. A goal of this survey is to show how the theory develops naturally from classical constructions used in the study of topological properties of algebraic varieties. While most proofs are omitted, we discuss several approaches to the decomposition theorem, indicate some important applications and examples. Contents 1 Overview 3 1.1 The topology of complex projective manifolds: Lefschetz and Hodge theorems 4 1.2 Families of smooth projective varieties . ........ 5 1.3 Singular algebraic varieties . ..... 7 1.4 Decomposition and hard Lefschetz in intersection cohomology . 8 1.5 Crash course on sheaves and derived categories . ........ 9 1.6 Decomposition, semisimplicity and relative hard Lefschetz theorems . 13 1.7 InvariantCycletheorems . 15 1.8 Afewexamples.................................. 16 1.9 The decomposition theorem and mixed Hodge structures . ......... 17 1.10 Historicalandotherremarks . 18 arXiv:0712.0349v2 [math.AG] 16 Apr 2009 2 Perverse sheaves 20 2.1 Intersection cohomology . 21 2.2 Examples of intersection cohomology . ...... 22 2.3 Definition and first properties of perverse sheaves . .......... 24 2.4 Theperversefiltration . .. .. .. .. .. .. .. 28 2.5 Perversecohomology .............................. 28 2.6 t-exactness and the Lefschetz hyperplane theorem . ...... 30 2.7 Intermediateextensions . 31 ∗Partially supported by GNSAGA and PRIN 2007 project “Spazi di moduli e teoria di Lie” 1 3 Three approaches to the decomposition theorem 33 3.1 The proof of Beilinson, Bernstein, Deligne and Gabber . -
Fundamental Theorems in Mathematics
SOME FUNDAMENTAL THEOREMS IN MATHEMATICS OLIVER KNILL Abstract. An expository hitchhikers guide to some theorems in mathematics. Criteria for the current list of 243 theorems are whether the result can be formulated elegantly, whether it is beautiful or useful and whether it could serve as a guide [6] without leading to panic. The order is not a ranking but ordered along a time-line when things were writ- ten down. Since [556] stated “a mathematical theorem only becomes beautiful if presented as a crown jewel within a context" we try sometimes to give some context. Of course, any such list of theorems is a matter of personal preferences, taste and limitations. The num- ber of theorems is arbitrary, the initial obvious goal was 42 but that number got eventually surpassed as it is hard to stop, once started. As a compensation, there are 42 “tweetable" theorems with included proofs. More comments on the choice of the theorems is included in an epilogue. For literature on general mathematics, see [193, 189, 29, 235, 254, 619, 412, 138], for history [217, 625, 376, 73, 46, 208, 379, 365, 690, 113, 618, 79, 259, 341], for popular, beautiful or elegant things [12, 529, 201, 182, 17, 672, 673, 44, 204, 190, 245, 446, 616, 303, 201, 2, 127, 146, 128, 502, 261, 172]. For comprehensive overviews in large parts of math- ematics, [74, 165, 166, 51, 593] or predictions on developments [47]. For reflections about mathematics in general [145, 455, 45, 306, 439, 99, 561]. Encyclopedic source examples are [188, 705, 670, 102, 192, 152, 221, 191, 111, 635]. -
Lecture 8: More Characteristic Classes and the Thom Isomorphism We
Lecture 8: More characteristic classes and the Thom isomorphism We begin this lecture by carrying out a few of the exercises in Lecture 1. We take advantage of the fact that the Chern classes are stable characteristic classes, which you proved in Exercise 7.71 from the Whitney sum formula. We also give a few more computations. Then we turn to the Euler class, which is decidedly unstable. We approach it via the Thom class of an oriented real vector bundle. We introduce the Thom complex of a real vector bundle. This construction plays an important role in the course. In lecture I did not prove the existence of the Thom class of an oriented real vector bundle. Here I do so—and directly prove the basic Thom isomorphism theorem—when the base is a CW complex. It follows from Morse theory that a smooth manifold is a CW complex, something we may prove later in the course. I need to assume the theorem that a vector bundle over a contractible base (in this case a closed ball) is trivializable. For a smooth bundle this follows immediately from Proposition 7.3. The book [BT] is an excellent reference for this lecture, especially Chapter IV. Elementary computations with Chern classes (8.1) Stable tangent bundle of projective space. We begin with a stronger version of Proposi- tion 7.51. Recall the exact sequence (7.54) of vector bundles over CPn. Proposition 8.2. The tangent bundle of CPn is stably equivalent to (S∗)⊕(n+1). Proof. The exact sequence (7.54) shows that Q ⊕ S =∼ Cn+1. -
Thin Compactifications and Relative Fundamental Classes
THIN COMPACTIFICATIONS AND RELATIVE FUNDAMENTAL CLASSES ELENY-NICOLETA IONEL AND THOMAS H. PARKER Abstract. We define a notion of relative fundamental class that applies to moduli spaces in gauge theory and in symplectic Gromov{Witten theory. For universal moduli spaces over a parameter space, the relative fundamental class specifies an element of the Cechˇ homology of the compactification of each fiber; it is defined if the compactification is \thin" in the sense that the boundary of the generic fiber has homological codimension at least two. The moduli spaces that occur in gauge theories and in symplectic Gromov{Witten theory are often orbifolds that can be compactified by adding \boundary strata" of lower dimension. Often, it is straightforward to prove that each stratum is a manifold, but more difficult to prove \collar theorems" that describe how these strata fit together. The lack of collar theorems is an impediment to applying singular homology to the compactified moduli space, and in particular to defining its fundamental homology class. The purpose of this paper is to show that collar theorems are not needed to define a (relative) fundamental class as an element of Cechˇ homology for families of appropriately compactified manifolds. One can distinguish two types of homology theories. Type I theories, exemplified by singular homology, are based on finite chains and are functorial under continuous maps. Type II theories, exemplified by Borel-Moore singular homology, are based on locally finite (possibly infinite) chains, and are functorial under proper continuous maps. We will use two theories of the second type: (type II) Steenrod homology sH and (type II) Cechˇ homology Hˇ . -
Arxiv:2006.02805V2 [Math.AT] 14 Nov 2020 H Offiin Stering the Is Coefficient the Rbe Ndffrniltplg.W Ics H Rbe N Eae P Let Related Category
REALIZING A HOMOLOGY CLASS OF A COMPACT MANIFOLD BY A HOMOLOGY CLASS OF AN EXPLICIT CLOSED SUBMANIFOLD–A NEW APPROACH TO THOM’S WORKS ON HOMOLOGY CLASSES OF SUBMANIFOLDS– NAOKI KITAZAWA Abstract. It is a classical important problem of differential topology by Thom; for a homology class of a compact manifold, can we realize this by a closed (smooth) submanifold with no boundary? This is true if the degree of the class is smaller or equal to the half of the dimension of the outer man- ifold under the condition that the coefficient ring is Z/2Z and that the outer manifold is closed and smooth. If the degree of the class is smaller or equal to 6 or equal to k − 2 or k − 1 under the condition that the coefficient ring is Z where k is the dimension of the manifold and that the outer manifold is closed, orientable and smooth, then this is also true. As a specific study, for 4- dimensional closed manifolds, the topologies of closed and connected surfaces realizing given 2nd homology classes have been actively studied, for example. In the present paper, we consider the following similar problem; can we real- ize a homology class of a compact manifold by a homology class of an explicit closed manifold embedded in the (interior of the) given compact manifold? This problem is considered as a variant of previous problems. We present an affirmative answer via important theory in the singularity theory of differen- tiable maps: lifting a given smooth map to an embedding or obtaining an embedding such that the composition of this with the canonical projection is the given map. -
Introduction to the Equivariant Vertex
Introduction to the equivariant vertex. Andrew Morrison April 14, 2014 1 Introduction. A classical problem in enumerative geometry is: How many lines lie on a generic cubic surface? Let S = V (F ) ⊂ P3 be a cubic surface given by the vanishing of a cubic polynomial F . The Grassmannian G(1; 3) parameterizes the lines L ⊂ 3 P . The polynomial F restricted to the line L gives a cubic form F jL 2 0 H (OL(3)). In this way the restriction of F to each line L gives a section 0 sF of the bundle H (OL(3)) ! G(1; 3). The zeros of this section are lines L with F jL = 0, i.e. those that lie on the cubic surface. 0 Since the section sF takes values in a bundle of rank h (OL(3)) = 4 over a manifold of dimension dim(G(1; 3)) = 4 we expect that, for generic F , the zero locus of sF will consist of a finite number of points. The number of lines can now be interpreted as the degree of the cycle corresponding to the zero locus of sF . This cycle is know to be rationally equivalent to the top Chern class of the bundle so then Z 0 #fL : L ⊂ Sg = c4(H (OL(3))) 2 Z: G(1;3) One way to do this integral is via the method of localization. We have an action of (C∗)4 on the Grassmannian G(1; 3). By lifting this integral to equivariant cohomology we can reduce the integral to a sum over simple con- tributions from each of the six fixed points of G(1; 3). -
Framed Bordism and Lagrangian Embeddings of Exotic Spheres
Annals of Mathematics 175 (2012), 71{185 http://dx.doi.org/10.4007/annals.2012.175.1.4 Framed bordism and Lagrangian embeddings of exotic spheres By Mohammed Abouzaid Abstract In dimensions congruent to 1 modulo 4, we prove that the cotangent bundle of an exotic sphere which does not bound a parallelisable manifold is not symplectomorphic to the cotangent bundle of the standard sphere. More precisely, we prove that such an exotic sphere cannot embed as a Lagrangian in the cotangent bundle of the standard sphere. The main ingredients of the construction are (1) the fact that the graph of the Hopf fibration embeds the standard sphere, and hence any Lagrangian which embeds in its cotangent bundle, as a displaceable Lagrangian in the product a symplectic vector space of the appropriate dimension with its complex projective space, and (2) a moduli space of solutions to a perturbed Cauchy- Riemann equation introduced by Gromov. Contents 1. Introduction 71 2. Construction of the bounding manifold 73 3. Transversality 96 4. Preliminaries for gluing 102 5. Construction of an extended gluing map 112 6. Local injectivity of the gluing map 122 7. Gluing near higher codimension strata 132 8. Construction of a smooth manifold with corners 148 9. Triviality of the tangent space of the cobordism 155 10. Analytic estimates for gluing 165 References 184 1. Introduction Let L be a compact exact Lagrangian submanifold of T ∗Sm whose Maslov class vanishes. By [24], L is a rational homology sphere which represents This research was conducted during the period the author served as a Clay Research Fellow. -
Signatures in Algebra, Topology and Dynamics
Edinburgh Research Explorer Signatures in algebra, topology and dynamics Citation for published version: Ghys, E & Ranicki, A 2016, 'Signatures in algebra, topology and dynamics', Ensaios Matemáticos, vol. 30, pp. 1-173. <http://www.sbm.org.br/docs/ensaios-volumes/em_30_1_ghys_ranicki.pdf> Link: Link to publication record in Edinburgh Research Explorer Document Version: Peer reviewed version Published In: Ensaios Matemáticos General rights Copyright for the publications made accessible via the Edinburgh Research Explorer is retained by the author(s) and / or other copyright owners and it is a condition of accessing these publications that users recognise and abide by the legal requirements associated with these rights. Take down policy The University of Edinburgh has made every reasonable effort to ensure that Edinburgh Research Explorer content complies with UK legislation. If you believe that the public display of this file breaches copyright please contact [email protected] providing details, and we will remove access to the work immediately and investigate your claim. Download date: 10. Oct. 2021 Signatures in algebra, topology and dynamics Etienne´ Ghys, Andrew Ranicki 31st December, 2015 arXiv:1512.09258v1 [math.AT] 31 Dec 2015 E.G A.R. UMPA UMR 5669 CNRS School of Mathematics, ENS Lyon University of Edinburgh Site Monod James Clerk Maxwell Building 46 All´eed'Italie Peter Guthrie Tait Road 69364 Lyon Edinburgh EH9 3FD France Scotland, UK [email protected] [email protected] 1 Contents 1 Algebra 6 1.1 The basic definitions . .6 1.2 Linear congruence . .7 1.3 The signature of a symmetric matrix . 11 1.4 Orthogonal congruence . -
Notes on Cobordism
Notes on Cobordism Haynes Miller Author address: Department of Mathematics, Massachusetts Institute of Technology, Cambridge, MA Notes typed by Dan Christensen and Gerd Laures based on lectures of Haynes Miller, Spring, 1994. Still in preliminary form, with much missing. This version dated December 5, 2001. Contents Chapter 1. Unoriented Bordism 1 1. Steenrod's Question 1 2. Thom Spaces and Stable Normal Bundles 3 3. The Pontrjagin{Thom Construction 5 4. Spectra 9 5. The Thom Isomorphism 12 6. Steenrod Operations 14 7. Stiefel-Whitney Classes 15 8. The Euler Class 19 9. The Steenrod Algebra 20 10. Hopf Algebras 24 11. Return of the Steenrod Algebra 28 12. The Answer to the Question 32 13. Further Comments on the Eilenberg{Mac Lane Spectrum 35 Chapter 2. Complex Cobordism 39 1. Various Bordisms 39 2. Complex Oriented Cohomology Theories 42 3. Generalities on Formal Group Laws 46 4. p-Typicality of Formal Group Laws 53 5. The Universal p-Typical Formal Group Law 61 6. Representing (R) 65 F 7. Applications to Topology 69 8. Characteristic Numbers 71 9. The Brown-Peterson Spectrum 78 10. The Adams Spectral Sequence 79 11. The BP -Hopf Invariant 92 12. The MU-Cohomology of a Finite Complex 93 iii iv CONTENTS 13. The Landweber Filtration Theorem 98 Chapter 3. The Nilpotence Theorem 101 1. Statement of Nilpotence Theorems 101 2. An Outline of the Proof 103 3. The Vanishing Line Lemma 106 4. The Nilpotent Cofibration Lemma 108 Appendices 111 Appendix A. A Construction of the Steenrod Squares 111 1. The Definition 111 2. -
Invariants from Curvature 3 2.1. Constructing Curvature Invariants 6 3
CHERN-WEIL THEORY ADEL RAHMAN Abstract. We give an introduction to the Chern-Weil construction of char- acteristic classes of complex vector bundles. We then relate this to the more classical notion of Chern classes as described in [2]. Contents 1. Introduction 1 1.1. Conventions 2 2. Chern-Weil Theory: Invariants from Curvature 3 2.1. Constructing Curvature Invariants 6 3. The Euler Class 7 4. The Chern Class 10 4.1. Constructing Chern Classes: Existence 10 4.2. Properties 11 4.3. Uniqueness of the Chern Classes 14 5. An Example: The Gauss-Bonnet Theorem 16 6. Describing the Curvature Invariants 17 Appendix A. Sums and Products of Vector Bundles 18 Appendix B. Connections and Curvatures of Complex Vector Bundles 19 Appendix C. Complex Grassmann Manifolds 21 Acknowledgments 22 References 22 1. Introduction One of the fundamental problems of topology is that of the classification of topo- logical spaces. Algebraic topology helps provide useful tools for this quest by means of functors from topological spaces into algebraic spaces (e.g. groups, rings, and modules). By ensuring that these functors are suitably invariant under topologi- cally irrelevant deformation (e.g homeomorphism, or often just the weaker notion of homotopy equivalence), these functors provide us with a means by which to classify spaces|if the targets of two spaces don't match, then they are surely not homeomorphic (precisely due to this invariance property). Characteristic classes provide us with a tool of the same nature, but for the more specialized notion of fibre bundles. A characteristic class is a map c from a bundle ξ = (E; π; B) into the cohomology of B, c : ξ ! H∗(B) that satisfies a naturality Date: September 26, 2017. -
Introduction to Algebraic Topology
INTRODUCTION TO ALGEBRAIC TOPOLOGY MARTIN CADEKˇ 9. Poincare´ duality Many interesting spaces used in geometry are closed oriented manifolds. Poincar´e duality expresses a remarkable symmetry between their homology and cohomology. 9.1. Manifolds. A manifold of dimension n is a Hausdorff space M in which each point has an open neighbourhood U homeomorphic to Rn. The dimension of M is characterized by the fact that for each x 2 M, the local homology group Hi(M; M − fxg; Z) is nonzero only for i = n since by excision and homotopy equivalence ∼ ∼ n n ∼ ~ n−1 Hi(M; M − fxg; Z) = Hi(U; U − fxg; Z) = Hi(R ; R − f0g; Z) = Hi−1(S ; Z): A compact manifold is called closed. Example. Examples of closed manifolds are spheres, real and complex projective spaces, orthogonal groups O(n) and SO(n), unitary groups U(n) and SU(n), real and complex Stiefel and Grassmann manifolds. The real Stiefel manifold Vn;k is the space n of k-tuples of orthonormal vectors in R . The real Grassmann manifolds Gn;k is the space of k-dimensional vector subspaces of Rn. 9.2. Orientation of manifolds. Consider a manifold M of dimension n.A local ∼ orientation of M in a point x 2 M is a choice of a generator µx 2 Hn(M; M −fxg; Z) = Z. i To shorten our notation we will use Hi(MjA) for Hi(M; M − A; Z) and H (MjA) for Hi(M; M − A; Z) if A ⊆ M. An orientation of M is a function assigning to each point x 2 M a local orientation µx 2 Hn(Mjx) such that each point has an open neighbourhood B with the property that all local orientations µy for y 2 B are images of an element µB 2 Hn(MjB) under the map ρy∗ : Hn(MjB) ! Hn(Mjx) where ρy :(M; M − fxg) ! (M; M − B) is the natural inclusion. -
The Cobordism Hypothesis
THE COBORDISM HYPOTHESIS DANIEL S. FREED Abstract. In this expository paper we introduce extended topological quantum field theories and the cobordism hypothesis. 1. Introduction The cobordism hypothesis was conjectured by Baez-Dolan [BD] in the mid 1990s. It has now been proved by Hopkins-Lurie in dimension two and by Lurie in higher dimensions. There are many complicated foundational issues which lie behind the definitions and the proof, and only a detailed sketch [L1] has appeared so far.1 The history of the Baez-Dolan conjecture goes most directly through quantum field theory and its adaptation to low-dimensional topology. Yet in retrospect it is a theorem about the structure of manifolds in all dimensions, and at the core of the proof lies Morse theory. Hence there are two routes to the cobordism hypothesis: algebraic topology and quantum field theory. SO Consider the abelian group Ω0 generated by compact oriented 0-dimensional manifolds, that is, finite sets Y of points each labeled with + or . The group operation is disjoint union. We deem Y − 0 equivalent to Y1 if there is a compact oriented 1-manifold X with oriented boundary Y1 Y0. SO ∐− Then a basic theorem in differential topology [Mi1, Appendix] asserts that Ω0 is the free abelian 2 group with a single generator, the positively oriented point pt+. This result is the cornerstone of smooth intersection theory. From the point of view of algebraic topology the cobordism hypothesis is a similar statement about a more ornate structure built from smooth manifolds. The simplest version is for framed manifolds. The language is off-putting if unfamiliar, and it will be explained in due course.