Cohomology of Local Systems on XΓ Cailan Li October 1St, 2019
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Stable Higgs Bundles on Ruled Surfaces 3
STABLE HIGGS BUNDLES ON RULED SURFACES SNEHAJIT MISRA Abstract. Let π : X = PC(E) −→ C be a ruled surface over an algebraically closed field k of characteristic 0, with a fixed polarization L on X. In this paper, we show that pullback of a (semi)stable Higgs bundle on C under π is a L-(semi)stable Higgs bundle. Conversely, if (V,θ) ∗ is a L-(semi)stable Higgs bundle on X with c1(V ) = π (d) for some divisor d of degree d on C and c2(V ) = 0, then there exists a (semi)stable Higgs bundle (W, ψ) of degree d on C whose pullback under π is isomorphic to (V,θ). As a consequence, we get an isomorphism between the corresponding moduli spaces of (semi)stable Higgs bundles. We also show the existence of non-trivial stable Higgs bundle on X whenever g(C) ≥ 2 and the base field is C. 1. Introduction A Higgs bundle on an algebraic variety X is a pair (V, θ) consisting of a vector bundle V 1 over X together with a Higgs field θ : V −→ V ⊗ ΩX such that θ ∧ θ = 0. Higgs bundle comes with a natural stability condition (see Definition 2.3 for stability), which allows one to study the moduli spaces of stable Higgs bundles on X. Higgs bundles on Riemann surfaces were first introduced by Nigel Hitchin in 1987 and subsequently, Simpson extended this notion on higher dimensional varieties. Since then, these objects have been studied by many authors, but very little is known about stability of Higgs bundles on ruled surfaces. -
The Calabi Complex and Killing Sheaf Cohomology
The Calabi complex and Killing sheaf cohomology Igor Khavkine Department of Mathematics, University of Trento, and TIFPA-INFN, Trento, I{38123 Povo (TN) Italy [email protected] September 26, 2014 Abstract It has recently been noticed that the degeneracies of the Poisson bra- cket of linearized gravity on constant curvature Lorentzian manifold can be described in terms of the cohomologies of a certain complex of dif- ferential operators. This complex was first introduced by Calabi and its cohomology is known to be isomorphic to that of the (locally constant) sheaf of Killing vectors. We review the structure of the Calabi complex in a novel way, with explicit calculations based on representation theory of GL(n), and also some tools for studying its cohomology in terms of of lo- cally constant sheaves. We also conjecture how these tools would adapt to linearized gravity on other backgrounds and to other gauge theories. The presentation includes explicit formulas for the differential operators in the Calabi complex, arguments for its local exactness, discussion of general- ized Poincar´eduality, methods of computing the cohomology of locally constant sheaves, and example calculations of Killing sheaf cohomologies of some black hole and cosmological Lorentzian manifolds. Contents 1 Introduction2 2 The Calabi complex4 2.1 Tensor bundles and Young symmetrizers..............5 2.2 Differential operators.........................7 2.3 Formal adjoint complex....................... 11 2.4 Equations of finite type, twisted de Rham complex........ 14 3 Cohomology of locally constant sheaves 16 3.1 Locally constant sheaves....................... 16 3.2 Acyclic resolution by a differential complex............ 18 3.3 Generalized Poincar´eduality................... -
Notes on Principal Bundles and Classifying Spaces
Notes on principal bundles and classifying spaces Stephen A. Mitchell August 2001 1 Introduction Consider a real n-plane bundle ξ with Euclidean metric. Associated to ξ are a number of auxiliary bundles: disc bundle, sphere bundle, projective bundle, k-frame bundle, etc. Here “bundle” simply means a local product with the indicated fibre. In each case one can show, by easy but repetitive arguments, that the projection map in question is indeed a local product; furthermore, the transition functions are always linear in the sense that they are induced in an obvious way from the linear transition functions of ξ. It turns out that all of this data can be subsumed in a single object: the “principal O(n)-bundle” Pξ, which is just the bundle of orthonormal n-frames. The fact that the transition functions of the various associated bundles are linear can then be formalized in the notion “fibre bundle with structure group O(n)”. If we do not want to consider a Euclidean metric, there is an analogous notion of principal GLnR-bundle; this is the bundle of linearly independent n-frames. More generally, if G is any topological group, a principal G-bundle is a locally trivial free G-space with orbit space B (see below for the precise definition). For example, if G is discrete then a principal G-bundle with connected total space is the same thing as a regular covering map with G as group of deck transformations. Under mild hypotheses there exists a classifying space BG, such that isomorphism classes of principal G-bundles over X are in natural bijective correspondence with [X, BG]. -
Group Invariant Solutions Without Transversality 2 in Detail, a General Method for Characterizing the Group Invariant Sections of a Given Bundle
GROUP INVARIANT SOLUTIONS WITHOUT TRANSVERSALITY Ian M. Anderson Mark E. Fels Charles G. Torre Department of Mathematics Department of Mathematics Department of Physics Utah State University Utah State University Utah State University Logan, Utah 84322 Logan, Utah 84322 Logan, Utah 84322 Abstract. We present a generalization of Lie’s method for finding the group invariant solutions to a system of partial differential equations. Our generalization relaxes the standard transversality assumption and encompasses the common situation where the reduced differential equations for the group invariant solutions involve both fewer dependent and independent variables. The theoretical basis for our method is provided by a general existence theorem for the invariant sections, both local and global, of a bundle on which a finite dimensional Lie group acts. A simple and natural extension of our characterization of invariant sections leads to an intrinsic characterization of the reduced equations for the group invariant solutions for a system of differential equations. The char- acterization of both the invariant sections and the reduced equations are summarized schematically by the kinematic and dynamic reduction diagrams and are illustrated by a number of examples from fluid mechanics, harmonic maps, and general relativity. This work also provides the theoretical foundations for a further detailed study of the reduced equations for group invariant solutions. Keywords. Lie symmetry reduction, group invariant solutions, kinematic reduction diagram, dy- namic reduction diagram. arXiv:math-ph/9910015v2 13 Apr 2000 February , Research supported by NSF grants DMS–9403788 and PHY–9732636 1. Introduction. Lie’s method of symmetry reduction for finding the group invariant solutions to partial differential equations is widely recognized as one of the most general and effective methods for obtaining exact solutions of non-linear partial differential equations. -
Composable Geometric Motion Policies Using Multi-Task Pullback Bundle Dynamical Systems
Composable Geometric Motion Policies using Multi-Task Pullback Bundle Dynamical Systems Andrew Bylard, Riccardo Bonalli, Marco Pavone Abstract— Despite decades of work in fast reactive plan- ning and control, challenges remain in developing reactive motion policies on non-Euclidean manifolds and enforcing constraints while avoiding undesirable potential function local minima. This work presents a principled method for designing and fusing desired robot task behaviors into a stable robot motion policy, leveraging the geometric structure of non- Euclidean manifolds, which are prevalent in robot configuration and task spaces. Our Pullback Bundle Dynamical Systems (PBDS) framework drives desired task behaviors and prioritizes tasks using separate position-dependent and position/velocity- dependent Riemannian metrics, respectively, thus simplifying individual task design and modular composition of tasks. For enforcing constraints, we provide a class of metric-based tasks, eliminating local minima by imposing non-conflicting potential functions only for goal region attraction. We also provide a geometric optimization problem for combining tasks inspired by Riemannian Motion Policies (RMPs) that reduces to a simple least-squares problem, and we show that our approach is geometrically well-defined. We demonstrate the 2 PBDS framework on the sphere S and at 300-500 Hz on a manipulator arm, and we provide task design guidance and an open-source Julia library implementation. Overall, this work Fig. 1: Example tree of PBDS task mappings designed to move a ball along presents a fast, easy-to-use framework for generating motion the surface of a sphere to a goal while avoiding obstacles. Depicted are policies without unwanted potential function local minima on manifolds representing: (black) joint configuration for a 7-DoF robot arm general manifolds. -
4 Fibered Categories (Aaron Mazel-Gee) Contents
4 Fibered categories (Aaron Mazel-Gee) Contents 4 Fibered categories (Aaron Mazel-Gee) 1 4.0 Introduction . .1 4.1 Definitions and basic facts . .1 4.2 The 2-Yoneda lemma . .2 4.3 Categories fibered in groupoids . .3 4.3.1 ... coming from co/groupoid objects . .3 4.3.2 ... and 2-categorical fiber product thereof . .4 4.0 Introduction In the same way that a sheaf is a special sort of functor, a stack will be a special sort of sheaf of groupoids (or a special special sort of groupoid-valued functor). It ends up being advantageous to think of the groupoid associated to an object X as living \above" X, in large part because this perspective makes it much easier to study the relationships between the groupoids associated to different objects. For this reason, we use the language of fibered categories. We note here that throughout this exposition we will often say equal (as opposed to isomorphic), and we really will mean it. 4.1 Definitions and basic facts φ Definition 1. Let C be a category. A category over C is a category F with a functor p : F!C. A morphism ξ ! η p(φ) in F is called cartesian if for any other ζ 2 F with a morphism ζ ! η and a factorization p(ζ) !h p(ξ) ! p(η) of φ p( ) in C, there is a unique morphism ζ !λ η giving a factorization ζ !λ η ! η of such that p(λ) = h. Pictorially, ζ - η w - w w 9 w w ! w w λ φ w w w w - w w w w ξ w w w w w w p(ζ) w p(η) w w - w h w ) w (φ w p w - p(ξ): In this case, we call ξ a pullback of η along p(φ). -
Fukaya Categories As Categorical Morse Homology?
Symmetry, Integrability and Geometry: Methods and Applications SIGMA 10 (2014), 018, 47 pages Fukaya Categories as Categorical Morse Homology? David NADLER Department of Mathematics, University of California, Berkeley, Berkeley, CA 94720-3840, USA E-mail: [email protected] URL: http://math.berkeley.edu/~nadler/ Received May 16, 2012, in final form February 21, 2014; Published online March 01, 2014 http://dx.doi.org/10.3842/SIGMA.2014.018 Abstract. The Fukaya category of a Weinstein manifold is an intricate symplectic inva- riant of high interest in mirror symmetry and geometric representation theory. This paper informally sketches how, in analogy with Morse homology, the Fukaya category might result from gluing together Fukaya categories of Weinstein cells. This can be formalized by a re- collement pattern for Lagrangian branes parallel to that for constructible sheaves. Assuming this structure, we exhibit the Fukaya category as the global sections of a sheaf on the conic topology of the Weinstein manifold. This can be viewed as a symplectic analogue of the well-known algebraic and topological theories of (micro)localization. Key words: Fukaya category; microlocalization 2010 Mathematics Subject Classification: 53D37 1 Introduction To realize \compact, smooth" global objects as glued together from simpler local pieces, one often pays the price that the local pieces are \noncompact" or \singular". For several representative examples, one could think about compact manifolds versus cells and simplices, smooth projective varieties versus smooth affine varieties and singular hyperplane sections, vector bundles with flat connection versus regular holonomic D-modules, or perhaps most universally of all, irreducible modules versus induced modules. -
Chapter 3 Connections
Chapter 3 Connections Contents 3.1 Parallel transport . 69 3.2 Fiber bundles . 72 3.3 Vector bundles . 75 3.3.1 Three definitions . 75 3.3.2 Christoffel symbols . 80 3.3.3 Connection 1-forms . 82 3.3.4 Linearization of a section at a zero . 84 3.4 Principal bundles . 88 3.4.1 Definition . 88 3.4.2 Global connection 1-forms . 89 3.4.3 Frame bundles and linear connections . 91 3.1 The idea of parallel transport A connection is essentially a way of identifying the points in nearby fibers of a bundle. One can see the need for such a notion by considering the following question: Given a vector bundle π : E ! M, a section s : M ! E and a vector X 2 TxM, what is meant by the directional derivative ds(x)X? If we regard a section merely as a map between the manifolds M and E, then one answer to the question is provided by the tangent map T s : T M ! T E. But this ignores most of the structure that makes a vector 69 70 CHAPTER 3. CONNECTIONS bundle interesting. We prefer to think of sections as \vector valued" maps on M, which can be added and multiplied by scalars, and we'd like to think of the directional derivative ds(x)X as something which respects this linear structure. From this perspective the answer is ambiguous, unless E happens to be the trivial bundle M × Fm ! M. In that case, it makes sense to think of the section s simply as a map M ! Fm, and the directional derivative is then d s(γ(t)) − s(γ(0)) ds(x)X = s(γ(t)) = lim (3.1) dt t!0 t t=0 for any smooth path with γ_ (0) = X, thus defining a linear map m ds(x) : TxM ! Ex = F : If E ! M is a nontrivial bundle, (3.1) doesn't immediately make sense because s(γ(t)) and s(γ(0)) may be in different fibers and cannot be added. -
Local Systems and Constructible Sheaves
Local Systems and Constructible Sheaves Fouad El Zein and Jawad Snoussi Abstract. The article describes Local Systems, Integrable Connections, the equivalence of both categories and their relations to Linear di®erential equa- tions. We report in details on Regular Singularities of Connections and on Singularities of local systems which leads to the theory of Intermediate ex- tensions and the Decomposition theorem. Mathematics Subject Classi¯cation (2000). Primary 32S60,32S40, Secondary 14F40. Keywords. Algebraic geometry, Analytic geometry, Local systems, Linear Dif- ferential Equations, Connections, constructible sheaves, perverse sheaves, Hard Lefschetz theorem. Introduction The purpose of these notes is to indicate a path for students which starts from a basic theory in undergraduate studies, namely the structure of solutions of Linear Di®erential Equations which is a classical subject in mathematics (see Ince [9]) that has been constantly enriched with developments of various theories and ends in a subject of research in contemporary mathematics, namely perverse sheaves. We report in these notes on the developments that occurred with the introduction of sheaf theory and vector bundles in the works of Deligne [4] and Malgrange [3,2)]. Instead of continuing with di®erential modules developed by Kashiwara and ex- plained in [12], a subject already studied in a Cimpa school, we shift our attention to the geometrical aspect represented by the notion of Local Systems which de- scribe on one side the structure of solutions of linear di®erential equations and on the other side the cohomological higher direct image of a constant sheaf by a proper smooth di®erentiable morphism. Then we introduce the theory of Connections on vector bundles generalizing to analytic varieties the theory of linear di®erential equations on a complex disc. -
Stable Homology of Surface Diffeomorphism Groups Made Discrete
STABLE HOMOLOGY OF SURFACE DIFFEOMORPHISM GROUPS MADE DISCRETE SAM NARIMAN Abstract. We answer affirmatively a question posed by Morita [Mor06] on homological stability of surface diffeomorphisms made discrete. In particular, we prove that C -diffeomorphisms of surfaces as family of discrete groups exhibit homological∞ stability. We show that the stable homology of C - diffeomorphims of surfaces as discrete groups is the same as homology of cer-∞ tain infinite loop space related to Haefliger’s classifying space of foliations of codimension 2. We use this infinite loop space to obtain new results about (non)triviality of characteristic classes of flat surface bundles and codimension 2 foliations. 0. Statements of the main results This paper is a continuation of the project initiated in [Nar14] on the homological stability and the stable homology of discrete surface diffeomorphisms. 0.1. Homological stability for surface diffeomorphisms made discrete. To fix some notations, let Σg,n denote a surface of genus g with n boundary com- δ ponents and let Diff Σg,n, ∂ denote the discrete group of orientation preserving diffeomorphisms of Σg,n that are supported away from the boundary. The starting point( of this) paper is a question posed by Morita [Mor06, Prob- lem 12.2] about an analogue of Harer stability for surface diffeomorphisms made δ discrete. In light of the fact that all known cohomology classes of BDiff Σg are stable with respect to g, Morita [Mor06] asked ( ) δ Question (Morita). Do the homology groups of BDiff Σg stabilize with respect to g? ( ) In order to prove homological stability for a family of groups, it is more conve- nient to have a map between them. -
Algebraic Topology I Fall 2016
31 Local coefficients and orientations The fact that a manifold is locally Euclidean puts surprising constraints on its cohomology, captured in the statement of Poincaré duality. To understand how this comes about, we have to find ways to promote local information – like the existence of Euclidean neighborhoods – to global information – like restrictions on the structure of the cohomology. Today we’ll study the notion of an orientation, which is the first link between local and global. The local-to-global device relevant to this is the notion of a “local coefficient system,” which is based on the more primitive notion of a covering space. We merely summarize that theory, since it is a prerequisite of this course. Definition 31.1. A continuous map p : E ! B is a covering space if (1) every point pre-image is a discrete subspace of E, and (2) every b 2 B has a neighborhood V admitting a map p−1(V ) ! p−1(b) such that the induced map =∼ p−1(V ) / V × p−1(b) p pr1 # B y is a homeomorphism. The space B is the “base,” E the “total space.” Example 31.2. A first example is given by the projection map pr1 : B × F ! B where F is discrete. A covering space of this form is said to be trivial, so the covering space condition can be rephrased as “local triviality.” The first interesting example is the projection map Sn ! RPn obtained by identifying antipodal maps on the sphere. This example generalizes in the following way. Definition 31.3. -
Chapter 5 Curvature on Bundles
Chapter 5 Curvature on Bundles Contents 5.1 Flat sections and connections . 115 5.2 Integrability and the Frobenius theorem . 117 5.3 Curvature on a vector bundle . 122 5.1 Flat sections and connections A connection on a fiber bundle π : E ! M allows one to define when a section is \constant" along smooth paths γ(t) 2 M; we call such sections horizontal, or in the case of a vector bundle, parallel. Since by defini- tion horizontal sections always exist along any given path, the nontrivial implications of the following question may not be immediately obvious: Given p 2 M and a sufficiently small neighborhood p 2 U ⊂ M, does E admit any section s 2 Γ(EjU ) for which rs ≡ 0? A section whose covariant derivative vanishes identically is called a flat or covariantly constant section. It may seem counterintuitive that the an- swer could possibly be no|after all, one of the most obvious facts about smooth functions is that constant functions exist. This translates easily into a statement about sections of trivial bundles. Of course, all bun- dles are locally trivial, thus locally one can always find sections that are constant with respect to a trivialization. These sections are covariantly constant with respect to a connection determined by the trivialization. As we will see however, connections of this type are rather special: for generic connections, flat sections do not exist, even locally! 115 116 CHAPTER 5. CURVATURE ON BUNDLES PSfrag replacements γ X(p0) M v R4 0 p0 C x y Ex Ey Figure 5.1: Parallel transport along a closed path on S2.