Fukaya Categories As Categorical Morse Homology?
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FLOER HOMOLOGY and MIRROR SYMMETRY I Kenji FUKAYA 0
FLOER HOMOLOGY AND MIRROR SYMMETRY I Kenji FUKAYA Abstract. In this survey article, we explain how the Floer homology of Lagrangian submanifold [Fl1],[Oh1] is related to (homological) mirror symmetry [Ko1],[Ko2]. Our discussion is based mainly on [FKO3]. 0. Introduction. This is the first of the two articles, describing a project in progress to study mirror symmetry and D-brane using Floer homology of Lagrangian submanifold. The tentative goal, which we are far away to achiev, is to prove homological mirror symmetry conjecture by M. Kontsevich (see 3.) The final goal, which is yet very § very far away from us, is to find a new concept of spaces, which is expected in various branches of mathematics and in theoretical physics. Together with several joint authors, I wrote several papers on this project [Fu1], [Fu2], [Fu4], [Fu5], [Fu6], [Fu7], [FKO3], [FOh]. The purpose of this article and part II, is to provide an accesible way to see the present stage of our project. The interested readers may find the detail and rigorous proofs of some of the statements, in those papers. The main purose of Part I is to discribe an outline of our joint paper [FKO3] which is devoted to the obstruction theory to the well-definedness of Floer ho- mology of Lagrangian submanifold. Our emphasis in this article is its relation to mirror symmetry. So we skip most of its application to the geometry of Lagrangian submanifolds. In 1, we review Floer homology of Lagrangian submanifold in the form intro- § duced by Floer and Oh. They assumed various conditions on Lagrangian subman- ifold and symplectic manifold, to define Floer homology. -
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................... -
Heegaard Floer Homology
Heegaard Floer Homology Joshua Evan Greene Low-dimensional topology encompasses the study of man- This is a story about Heegaard Floer homology: how it ifolds in dimension four and lower. These are the shapes developed, how it has evolved, what it has taught us, and and dimensions closest to our observable experience in where it may lead. spacetime, and one of the great lessons in topology during the 20th century is that these dimensions exhibit unique Heegaard... phenomena that render them dramatically different from To set the stage, we return to the beginning of the 20th higher ones. Many outlooks and techniques have arisen in century, when Poincar´eforged topology as an area of in- shaping the area, each with its own particular strengths: hy- dependent interest. In 1901, he famously and erroneously perbolic geometry, quantum algebra, foliations, geometric asserted that, as is the case for 1- and 2-manifolds, any 3- analysis,... manifold with the same ordinary homology groups as the Heegaard Floer homology, defined at the turn of the 3-dimensional sphere 푆3 is, in fact, homeomorphic to 푆3. 21st century by Peter Ozsv´ath and Zolt´an Szab´o, sits By 1905, he had vanquished his earlier claim by way of amongst these varied approaches. It consists of a power- an example that now bears his name: the Poincar´ehomol- ful collection of invariants that fit into the framework ofa ogy sphere 푃3. We will describe this remarkable space in (3 + 1)-dimensional topological quantum field theory. It a moment and re-encounter it in many guises. -
Fall 2017 MATH 70330 “Intermediate Geometry and Topology” Pavel Mnev Detailed Plan. I. Characteristic Classes. (A) Fiber/Vec
Fall 2017 MATH 70330 \Intermediate Geometry and Topology" Pavel Mnev Detailed plan. I. Characteristic classes. (a) Fiber/vector/principal bundles. Examples. Connections, curvature. Rie- mannian case. Ref: [MT97]. (b) (2 classes.) Stiefel-Whitney, Chern and Pontryagin classes { properties, axiomatic definition. Classifying map and classifying bundle. RP 1; CP 1, infinite Grassmanians Gr(n; 1), CW structure, cohomology ring (univer- sal characteristic classes). Characteristic classes as obstructions (e.g. for embeddability of projective spaces). Euler class. Also: Chern character, splitting principle, Chern roots. Also: BG for a finite group/Lie group, group cohomology. Ref: [MS74]; also: [BT82, Hat98, LM98, May99]. (c) Chern-Weil homomorphism. Example: Chern-Gauss-Bonnet formula. Chern- Simons forms. Ref: Appendix C in [MS74]; [AM05, Dup78, MT97]. (d) Equivariant cohomology. Borel model (homotopy quotient), algebraic ver- sion { Cartan and Weil models. Ref: [GS99, Mei06, Tu13]. II. Bits of symplectic geometry. (a) Symplectic linear algebra, Lagrangian Grassmanian, Maslov class. Ref: [BW97, Ran, MS17]. (b) Symplectic manifolds, Darboux theorem (proof via Moser's trick). Dis- tinguished submanifolds (isotropic, coisotropic, Lagrangian). Examples. Constructions of Lagrangians in T ∗M (graph, conormal bundle). Ref: [DS00]. (c) Hamiltonian group actions, moment maps, symplectic reduction. Ref: [Jef] (lectures 2{4,7), [DS00]. (d) (Optional) Convexity theorem (Atyiah-Guillemin-Sternberg) for the mo- ment map of a Hamiltonian torus action. Toric varieties as symplectic re- ductions, their moment polytopes, Delzant's theorem. Ref: [Pra99, Sch], Part XI in [DS00], lectures 5,6 in [Jef]. (e) Localization theorems: Duistermaat-Heckman and Atiyah-Bott. Ref: [Mei06, Tu13], [Jef] (lecture 10). (f) (Optional) Classical field theory via Lagrangian correspondences. -
[Math.SG] 22 Mar 2004
A SURVEY OF FLOER HOMOLOGY FOR MANIFOLDS WITH CONTACT TYPE BOUNDARY OR SYMPLECTIC HOMOLOGY ALEXANDRU OANCEA Abstract. The purpose of this paper is to give a survey of the various versions of Floer homology for manifolds with contact type boundary that have so far appeared in the literature. Under the name of “Symplectic homology” or “Floer homology for manifolds with boundary” they bear in fact common features and we shall try to underline the principles that unite them. Once this will be accomplished we shall proceed to describe the peculiarity of each of the constructions and the specific applications that unfold out of it: classification of ellipsoids and polydiscs in Cn, stability of the action spectrum for contact type boundaries of symplectic manifolds, existence of closed characteristics on contact type hypersurfaces and obstructions to exact Lagrange embeddings. The computation of the Floer cohomology for balls in Cn is carried by explicitly perturbing the nondegenerate Morse-Bott spheres of closed characteristics. Contents 1. Constructions of Floer homological invariants 2 1.1. Morse homology 2 1.2. Floer homology for closed manifolds 3 1.3. Floer homology for manifolds with contact type boundary or Symplectic homology 6 2. Comments and further properties 15 2.1. C0 bounds. 15 2.2. Relations between different symplectic homologies. 15 2.3. Invariance through isotopies. 16 3. A computation: balls in Cn 17 3.1. Recollections on the Robbin-Salamon index 18 3.2. Direct computation of the cohomology of a ball. 19 3.3. Alternative point of view: perturbation of critical Morse-Bott manifolds. 20 4. -
AN INTRODUCTION to INSTANTON KNOT FLOER HOMOLOGY These
AN INTRODUCTION TO INSTANTON KNOT FLOER HOMOLOGY NIKOLAI SAVELIEV These notes are intended to serve as an informal introduction to instan- ton Floer homology of knots. We begin by developing a version of instanton Floer homology for closed 3-manifolds [2], [5] associated with admissible SO(3) bundles, and then briefly review three instanton knot homology the- ories due to Floer [5] and to Kronheimer and Mrowka [6], [7]. 1. Stiefel–Whithey classes Let Y be a finite CW-complex of dimension at most three and P → Y an SO(3) bundle. Associated with P are its Stiefel–Whitney classes wi(P ) ∈ Hi(Y ; Z/2), i = 1, 2, 3. Only one of them, namely, 2 w2(P ) ∈ H (Y ; Z/2), will be of importance to us, for the reason that w1(P ) = 0 since P is ori- 1 entable, and w3(P )=Sq (w2(P )) by the Wu formula. The class w2(P ) can be defined as follows. Let { Uα } be a trivializing cover for the bundle P then the gluing functions ϕαβ : Uα ∩ Uβ −→ SO(3) (1) define a class [P ] ∈ H1(Y ; SO(3)) in Cechˇ cohomology. Conversely, a co- homology class in H1(Y ; SO(3)) defines a unique SO(3) bundle up to an isomorphism. The short exact sequence of Lie groups 1 −−−−→ Z/2 −−−−→ SU(2) −−−−→Ad SO(3) −−−−→ 1, where Z/2 = {±1} is the center of SU(2), gives rise to the exact sequence in Cechˇ cohomology, . → H1(Y ; SU(2)) −−−−→ H1(Y ; SO(3)) −−−−→δ H2(Y ; Z/2) → . 1 1 The class w2(P ) is the image of [P ] ∈ H (Y ; SO(3)) under the connecting homomorphism δ. -
Remarks on A-Branes, Mirror Symmetry, and the Fukaya Category
CALT-68-2348 Remarks On A-branes, Mirror Symmetry, And The Fukaya Category Anton Kapustin∗ Dmitri Orlov† Abstract We discuss D-branes of the topological A-model (A-branes), which are believed to be closely related to the Fukaya category. We give string theory arguments which show that A-branes are not necessarily Lagrangian submanifolds in the Calabi-Yau: more general coisotropic branes are also allowed, if the line bundle on the brane is not flat. We show that a coisotropic A-brane has a natural structure of a foliated manifold with a transverse holomorphic structure. We argue that the Fukaya category must be enlarged with such objects for the Homological Mirror Symmetry conjecture to be true. arXiv:hep-th/0109098v1 12 Sep 2001 ∗California Institute of Technology, Pasadena, CA 91125, E-mail: [email protected] †Algebra Section, Steklov Mathematical Institute, Russian Academy of Sciences, 8 Gubkin str., GSP-1, Moscow 117966, Russia, E-mail: [email protected] 1 1 Introduction Let X be a weak Calabi-Yau manifold, i.e. a complex manifold with c1(X) = 0 which admits a K¨ahler metric. Given a Ricci-flat K¨ahler metric G on X, and a B-field (a class in H2(X, R)) , one can canonically construct an N = 2 supersymmetric sigma-model with “target” X. On physical grounds, the quantized version of this model has N = 2 superconformal symmetry and describes propagation of closed strings on X. In this note we set B = 0 for simplicity. According to Calabi’s conjecture proved by Yau, we can parametrize G by the cohomology class of its K¨ahler form ω. -
Floer Homology, Gauge Theory, and Low-Dimensional Topology
Floer Homology, Gauge Theory, and Low-Dimensional Topology Clay Mathematics Proceedings Volume 5 Floer Homology, Gauge Theory, and Low-Dimensional Topology Proceedings of the Clay Mathematics Institute 2004 Summer School Alfréd Rényi Institute of Mathematics Budapest, Hungary June 5–26, 2004 David A. Ellwood Peter S. Ozsváth András I. Stipsicz Zoltán Szabó Editors American Mathematical Society Clay Mathematics Institute 2000 Mathematics Subject Classification. Primary 57R17, 57R55, 57R57, 57R58, 53D05, 53D40, 57M27, 14J26. The cover illustrates a Kinoshita-Terasaka knot (a knot with trivial Alexander polyno- mial), and two Kauffman states. These states represent the two generators of the Heegaard Floer homology of the knot in its topmost filtration level. The fact that these elements are homologically non-trivial can be used to show that the Seifert genus of this knot is two, a result first proved by David Gabai. Library of Congress Cataloging-in-Publication Data Clay Mathematics Institute. Summer School (2004 : Budapest, Hungary) Floer homology, gauge theory, and low-dimensional topology : proceedings of the Clay Mathe- matics Institute 2004 Summer School, Alfr´ed R´enyi Institute of Mathematics, Budapest, Hungary, June 5–26, 2004 / David A. Ellwood ...[et al.], editors. p. cm. — (Clay mathematics proceedings, ISSN 1534-6455 ; v. 5) ISBN 0-8218-3845-8 (alk. paper) 1. Low-dimensional topology—Congresses. 2. Symplectic geometry—Congresses. 3. Homol- ogy theory—Congresses. 4. Gauge fields (Physics)—Congresses. I. Ellwood, D. (David), 1966– II. Title. III. Series. QA612.14.C55 2004 514.22—dc22 2006042815 Copying and reprinting. Material in this book may be reproduced by any means for educa- tional and scientific purposes without fee or permission with the exception of reproduction by ser- vices that collect fees for delivery of documents and provided that the customary acknowledgment of the source is given. -
Math 283 - Instanton Floer Homology
Math 283 - Instanton Floer Homology Taught by Peter B. Kronheimer Notes by Dongryul Kim Spring 2018 The course was taught by Peter Kronheimer, on Mondays, Wednesdays, and Fridays from 11am to 12pm. There were three assignements throughout the course. Contents 1 January 22, 2018 5 1.1 Topology of smooth 4-manifolds . .5 1.2 Connections . .7 2 January 24, 2018 8 2.1 Curvature . .8 3 January 26, 2018 11 3.1 Moduli spaces of connections . 11 3.2 Elliptic operators . 11 3.3 Linear gauge-fixing . 12 4 January 29, 2018 14 4.1 Sobolev embeddings . 14 4.2 Moduli space of anti-self-dual connections . 15 5 January 31, 2018 17 5.1 Reducibles on M ........................... 18 6 February 2, 2018 19 6.1 Uhlenbeck's compactness theorem . 19 7 February 5, 2018 22 7.1 Uhlenbeck compactification . 22 7.2 Three-manifolds and the Chern{Simons functional . 23 1 Last Update: August 27, 2018 8 February 7, 2018 25 8.1 Chern{Simons functional under gauge transformations . 25 8.2 Representation variety . 26 9 February 9, 2018 28 9.1 Gradient flows and PDE . 28 10 February 12, 2018 30 10.1 SO(3)-bundle as a SU(2)-bundle . 30 10.2 Morse theory . 31 11 February 14, 2018 33 11.1 Operator on a cylinder . 33 12 February 16, 2018 35 12.1 Spectral flow . 35 12.2 Negative gradient flow . 35 13 February 21, 2018 37 13.1 Morse homology . 37 13.2 Morse theory on the space of connections . 38 14 February 23, 2018 40 14.1 Instanton Floer homology . -
SPECULATIONS on HOMOLOGICAL MIRROR SYMMETRY for HYPERSURFACES in (C∗)N
SPECULATIONS ON HOMOLOGICAL MIRROR SYMMETRY FOR HYPERSURFACES IN (C∗)n DENIS AUROUX Abstract. Given an algebraic hypersurface H = f −1(0) in (C∗)n, homological mirror symmetry relates the wrapped Fukaya category of H to the derived category of singularities of the mirror Landau-Ginzburg model. We propose an enriched version of this picture which also features the wrapped Fukaya category of the complement (C∗)n \ H and the Fukaya-Seidel category of the Landau-Ginzburg model ((C∗)n,f). We illustrate our speculations on simple examples, and sketch a proof of homological mirror symmetry for higher-dimensional pairs of pants. 1. Introduction Let H = f −1(0) ⊂ (C∗)n be a smooth algebraic hypersurface (close to a maximal degeneration limit), whose defining equation is a Laurent polynomial of the form ρ(α) α1 αn (1.1) f(x1,...,xn)= cατ x1 ...xn , α∈A n ∗X where A is a finite subset of Z , cα ∈ C , τ ∈ R+ is assumed to be sufficiently small, and ρ : A → R is a convex function. More precisely, we require that ρ is the restriction to A of a convex piecewise linear functionρ ˆ defined on the convex hull Conv(A) ⊂ Rn. The maximal domains of linearity ofρ ˆ define a polyhedral decomposition P of Conv(A), whose set of vertices is required to be exactly A. We further assume that all the cells of P are congruent under the action of GL(n, Z) to standard simplices; this ensures that the limit τ → 0 corresponds to a maximal degeneration, and that the mirror is smooth. -
Seminar (Homological) Mirror Symmetry Wintersemester 2019/20
Seminar (Homological) Mirror Symmetry Wintersemester 2019/20 Description Content: Mirror symmetry is one of the oldest and best understood dualities that have emerged from string theory and has had a profound impact in certain areas of pure mathemat- ics. The original statements, motivated by Conformal Field Theory, concerned certain enumerative questions in algebraic geometry and their solution in terms of Hodge theory. Soon after, two mathematical formulations were put forward: Kontsevich's Homological Mirror Symmetry inteprets the duality as an equivalence of symplectic and algebraic cat- egories. The study of torus fibrations initiated by Strominger, Yau and Zaslow gives an explicit geometric correspondence. Today, mirror symmetry remains an extremely active research field, reaching in influence far beyond its original formulation as a duality be- tween Calabi-Yau manifolds, to such subjects as representation theory, singularity theory, and knot theory. This seminar will trace mirror symmetry from its origins to some modern developments. One of our main goals will be to understand Nick Sheridan's 2011 proof of homological mirror symmetry for the quintic threefold. Audience: The seminar is aimed at Masters students in mathematics and mathematical physics. Participants should have a solid background at least one of symplectic geometry, algebraic geometry or quantum field and string theory, with nodding acquaintance of the other two. Evaluation: This seminar is listed in the LSF as “Masterpflichtseminar" in Physics and as \Master- Seminar" in Mathematics. To receive credit in the Physics program, you have to prepare a 6{10 page write-up of your talk, and the final grade will be based (in roughly equal amounts) on both the talk and the writeup. -
Essays on Mirror Manifolds, International Press, Hong Kong, 1992
Contents 1 Introduction 2 1.1 What is Mirror Symmetry? . 2 1.2 Summary . 3 2 Enumerative aspects (following R. Dijkgraaf) 3 3 Homological Mirror Symmetry 11 3.1 The derived category of coherent sheaves . 12 3.1.1 The construction . 12 3.1.2 Triangulated categories . 14 3.1.3 Derived functors . 16 3.2 The Fukaya Category . 16 3.2.1 A -categories . 16 1 3.2.2 Fukaya category: The objects . 17 3.2.3 Fukaya category: The morphisms . 18 3.3 A duality in both categories . 19 3.4 The elliptic curve . 21 3.4.1 The derived catory on the elliptic curve . 21 3.4.2 Description of the functor . 24 3.4.3 Consequences . 27 4 Fourier-Mukai transforms 29 4.1 A report . 29 4.2 Auto-equivalences of Db(Coh E) . 30 5 More about Fukaya categories 33 5.1 Transversal Fukaya category . 33 5.2 Fukaya functors . 33 5.3 Conclusion . 36 A The Maslov index 38 B Morphisms for non-transversal intersection in the Fukaya cat- egory 38 1 1 Introduction 1.1 What is Mirror Symmetry? It is now roughly 10 years ago when physicists first discovered that a special duality in conformal field theory might have interesting mathematical appli- cations. Under the name of \mirror symmetry", this phaenomenom quickly became famous and rised interest among mathematicians and physicists. Since then, many purely mathematical statements arised from the rather vague con- jecture, and a lot of effort has been put into setting up the right language to formulate them.