Hodge Theory on Compact Kähler Manifolds
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Notes on the Atiyah-Singer Index Theorem Liviu I. Nicolaescu
Notes on the Atiyah-Singer Index Theorem Liviu I. Nicolaescu Notes for a topics in topology course, University of Notre Dame, Spring 2004, Spring 2013. Last revision: November 15, 2013 i The Atiyah-Singer Index Theorem This is arguably one of the deepest and most beautiful results in modern geometry, and in my view is a must know for any geometer/topologist. It has to do with elliptic partial differential opera- tors on a compact manifold, namely those operators P with the property that dim ker P; dim coker P < 1. In general these integers are very difficult to compute without some very precise information about P . Remarkably, their difference, called the index of P , is a “soft” quantity in the sense that its determination can be carried out relying only on topological tools. You should compare this with the following elementary situation. m n Suppose we are given a linear operator A : C ! C . From this information alone we cannot compute the dimension of its kernel or of its cokernel. We can however compute their difference which, according to the rank-nullity theorem for n×m matrices must be dim ker A−dim coker A = m − n. Michael Atiyah and Isadore Singer have shown in the 1960s that the index of an elliptic operator is determined by certain cohomology classes on the background manifold. These cohomology classes are in turn topological invariants of the vector bundles on which the differential operator acts and the homotopy class of the principal symbol of the operator. Moreover, they proved that in order to understand the index problem for an arbitrary elliptic operator it suffices to understand the index problem for a very special class of first order elliptic operators, namely the Dirac type elliptic operators. -
Hodge Decomposition
Hodge Decomposition Daniel Lowengrub April 27, 2014 1 Introduction All of the content in these notes in contained in the book Differential Analysis on Complex Man- ifolds by Raymond Wells. The primary objective here is to highlight the steps needed to prove the Hodge decomposition theorems for real and complex manifolds, in addition to providing intuition as to how everything fits together. 1.1 The Decomposition Theorem On a given complex manifold X, there are two natural cohomologies to consider. One is the de Rham Cohomology which can be defined on a general, possibly non complex, manifold. The second one is the Dolbeault cohomology which uses the complex structure. We’ll quickly go over the definitions of these cohomologies in order to set notation but for a precise discussion I recommend Huybrechts or Wells. If X is a manifold, we can define the de Rahm Complex to be the chain complex 0 E(Ω0)(X) −d E(Ω1)(X) −d ::: Where Ω = T∗ denotes the cotangent vector bundle and Ωk is the alternating product Ωk = ΛkΩ. In general, we’ll use the notation! E(E) to! denote the sheaf! of sections associated to a vector bundle E. The boundary operator is the usual differentiation operator. The de Rham cohomology of the manifold X is defined to be the cohomology of the de Rham chain complex: d Ker(E(Ωn)(X) − E(Ωn+1)(X)) n (X R) = HdR , d Im(E(Ωn-1)(X) − E(Ωn)(X)) ! We can also consider the de Rham cohomology with complex coefficients by tensoring the de Rham complex with C in order to obtain the de Rham complex! with complex coefficients 0 d 1 d 0 E(ΩC)(X) − E(ΩC)(X) − ::: where ΩC = Ω ⊗ C and the differential d is linearly extended. -
Introduction to Hodge Theory
INTRODUCTION TO HODGE THEORY DANIEL MATEI SNSB 2008 Abstract. This course will present the basics of Hodge theory aiming to familiarize students with an important technique in complex and algebraic geometry. We start by reviewing complex manifolds, Kahler manifolds and the de Rham theorems. We then introduce Laplacians and establish the connection between harmonic forms and cohomology. The main theorems are then detailed: the Hodge decomposition and the Lefschetz decomposition. The Hodge index theorem, Hodge structures and polariza- tions are discussed. The non-compact case is also considered. Finally, time permitted, rudiments of the theory of variations of Hodge structures are given. Date: February 20, 2008. Key words and phrases. Riemann manifold, complex manifold, deRham cohomology, harmonic form, Kahler manifold, Hodge decomposition. 1 2 DANIEL MATEI SNSB 2008 1. Introduction The goal of these lectures is to explain the existence of special structures on the coho- mology of Kahler manifolds, namely, the Hodge decomposition and the Lefschetz decom- position, and to discuss their basic properties and consequences. A Kahler manifold is a complex manifold equipped with a Hermitian metric whose imaginary part, which is a 2-form of type (1,1) relative to the complex structure, is closed. This 2-form is called the Kahler form of the Kahler metric. Smooth projective complex manifolds are special cases of compact Kahler manifolds. As complex projective space (equipped, for example, with the Fubini-Study metric) is a Kahler manifold, the complex submanifolds of projective space equipped with the induced metric are also Kahler. We can indicate precisely which members of the set of Kahler manifolds are complex projective, thanks to Kodaira’s theorem: Theorem 1.1. -
Hodge Theory in Combinatorics
BULLETIN (New Series) OF THE AMERICAN MATHEMATICAL SOCIETY Volume 55, Number 1, January 2018, Pages 57–80 http://dx.doi.org/10.1090/bull/1599 Article electronically published on September 11, 2017 HODGE THEORY IN COMBINATORICS MATTHEW BAKER Abstract. If G is a finite graph, a proper coloring of G is a way to color the vertices of the graph using n colors so that no two vertices connected by an edge have the same color. (The celebrated four-color theorem asserts that if G is planar, then there is at least one proper coloring of G with four colors.) By a classical result of Birkhoff, the number of proper colorings of G with n colors is a polynomial in n, called the chromatic polynomial of G.Read conjectured in 1968 that for any graph G, the sequence of absolute values of coefficients of the chromatic polynomial is unimodal: it goes up, hits a peak, and then goes down. Read’s conjecture was proved by June Huh in a 2012 paper making heavy use of methods from algebraic geometry. Huh’s result was subsequently refined and generalized by Huh and Katz (also in 2012), again using substantial doses of algebraic geometry. Both papers in fact establish log-concavity of the coefficients, which is stronger than unimodality. The breakthroughs of the Huh and Huh–Katz papers left open the more general Rota–Welsh conjecture, where graphs are generalized to (not neces- sarily representable) matroids, and the chromatic polynomial of a graph is replaced by the characteristic polynomial of a matroid. The Huh and Huh– Katz techniques are not applicable in this level of generality, since there is no underlying algebraic geometry to which to relate the problem. -
Hodge Theory
HODGE THEORY PETER S. PARK Abstract. This exposition of Hodge theory is a slightly retooled version of the author's Harvard minor thesis, advised by Professor Joe Harris. Contents 1. Introduction 1 2. Hodge Theory of Compact Oriented Riemannian Manifolds 2 2.1. Hodge star operator 2 2.2. The main theorem 3 2.3. Sobolev spaces 5 2.4. Elliptic theory 11 2.5. Proof of the main theorem 14 3. Hodge Theory of Compact K¨ahlerManifolds 17 3.1. Differential operators on complex manifolds 17 3.2. Differential operators on K¨ahlermanifolds 20 3.3. Bott{Chern cohomology and the @@-Lemma 25 3.4. Lefschetz decomposition and the Hodge index theorem 26 Acknowledgments 30 References 30 1. Introduction Our objective in this exposition is to state and prove the main theorems of Hodge theory. In Section 2, we first describe a key motivation behind the Hodge theory for compact, closed, oriented Riemannian manifolds: the observation that the differential forms that satisfy certain par- tial differential equations depending on the choice of Riemannian metric (forms in the kernel of the associated Laplacian operator, or harmonic forms) turn out to be precisely the norm-minimizing representatives of the de Rham cohomology classes. This naturally leads to the statement our first main theorem, the Hodge decomposition|for a given compact, closed, oriented Riemannian manifold|of the space of smooth k-forms into the image of the Laplacian and its kernel, the sub- space of harmonic forms. We then develop the analytic machinery|specifically, Sobolev spaces and the theory of elliptic differential operators|that we use to prove the aforementioned decom- position, which immediately yields as a corollary the phenomenon of Poincar´eduality. -
Hodge Theory and Geometry
HODGE THEORY AND GEOMETRY PHILLIP GRIFFITHS This expository paper is an expanded version of a talk given at the joint meeting of the Edinburgh and London Mathematical Societies in Edinburgh to celebrate the centenary of the birth of Sir William Hodge. In the talk the emphasis was on the relationship between Hodge theory and geometry, especially the study of algebraic cycles that was of such interest to Hodge. Special attention will be placed on the construction of geometric objects with Hodge-theoretic assumptions. An objective in the talk was to make the following points: • Formal Hodge theory (to be described below) has seen signifi- cant progress and may be said to be harmonious and, with one exception, may be argued to be essentially complete; • The use of Hodge theory in algebro-geometric questions has become pronounced in recent years. Variational methods have proved particularly effective; • The construction of geometric objects, such as algebraic cycles or rational equivalences between cycles, has (to the best of my knowledge) not seen significant progress beyond the Lefschetz (1; 1) theorem first proved over eighty years ago; • Aside from the (generalized) Hodge conjecture, the deepest is- sues in Hodge theory seem to be of an arithmetic-geometric character; here, especially noteworthy are the conjectures of Grothendieck and of Bloch-Beilinson. Moreover, even if one is interested only in the complex geometry of algebraic cycles, in higher codimensions arithmetic aspects necessarily enter. These are reflected geometrically in the infinitesimal structure of the spaces of algebraic cycles, and in the fact that the convergence of formal, iterative constructions seems to involve arithmetic 1 2 PHILLIP GRIFFITHS as well as Hodge-theoretic considerations. -
On the L2–Stokes Theorem and Hodge Theory for Singular Algebraic Varieties
On the L2–Stokes theorem and Hodge theory for singular algebraic varieties Daniel Grieser and Matthias Lesch July 19, 2018 Abstract For a projective algebraic variety V with isolated singularities, endowed with a metric induced from an embedding, we consider the analysis of the natural partial differential operators on the regular part of V . We show that, in the complex case, the Laplacians of the de Rham and Dolbeault complexes are discrete operators except possibly in degrees n,n±1, where n is the complex dimension of V . We also prove a Hodge theorem on the operator level and the L2–Stokes theorem outside the degrees n − 1,n. We show that the L2-Stokes theorem may fail to hold in the case of real algebraic varieties, and also discuss the L2-Stokes theorem on more general non-compact spaces. 1991 Mathematics Subject Classification. 58A (32S) Contents 1 Introduction 1 2 The L2–Stokes theorem 4 3 Complex algebraic varieties 12 arXiv:math/9902062v2 [math.DG] 7 May 2002 References 14 1 Introduction The interplay between geometric differential operators on a Riemannian man- ifold and the geometry of the underlying manifold has been the focus of many efforts; one of the early highlights is the Atiyah-Singer Index Theorem. Since the work of Atiyah and Singer one has become more and more in- terested in various types of manifolds with singularities. While the case of a smooth compact manifold is fairly well understood, the picture is far from com- plete for singular manifolds. It is impossible to give a complete account of the existing literature here. -
Representation Theory As Gauge Theory
Representation theory Quantum Field Theory Gauge Theory Representation Theory as Gauge Theory David Ben-Zvi University of Texas at Austin Clay Research Conference Oxford, September 2016 Representation theory Quantum Field Theory Gauge Theory Themes I. Harmonic analysis as the exploitation of symmetry1 II. Commutative algebra signals geometry III. Topology provides commutativity IV. Gauge theory bridges topology and representation theory 1Mackey, Bull. AMS 1980 Representation theory Quantum Field Theory Gauge Theory Themes I. Harmonic analysis as the exploitation of symmetry1 II. Commutative algebra signals geometry III. Topology provides commutativity IV. Gauge theory bridges topology and representation theory 1Mackey, Bull. AMS 1980 Representation theory Quantum Field Theory Gauge Theory Themes I. Harmonic analysis as the exploitation of symmetry1 II. Commutative algebra signals geometry III. Topology provides commutativity IV. Gauge theory bridges topology and representation theory 1Mackey, Bull. AMS 1980 Representation theory Quantum Field Theory Gauge Theory Themes I. Harmonic analysis as the exploitation of symmetry1 II. Commutative algebra signals geometry III. Topology provides commutativity IV. Gauge theory bridges topology and representation theory 1Mackey, Bull. AMS 1980 Representation theory Quantum Field Theory Gauge Theory Outline Representation theory Quantum Field Theory Gauge Theory Representation theory Quantum Field Theory Gauge Theory Fourier Series G = U(1) acts on S1, hence on L2(S1): Fourier series 2 1 [M 2πinθ L (S ) ' Ce n2Z joint eigenspaces of rotation operators See last slide for all image credits Representation theory Quantum Field Theory Gauge Theory The dual Basic object in representation theory: describe the dual of a group G: Gb = f irreducible (unitary) representations of Gg e.g. -
Hodge Theory on Metric Spaces
Hodge Theory on Metric Spaces Laurent Bartholdi∗ Georg-August-Universit¨atG¨ottingen Deutschland Thomas Schick∗ Nat Smale Georg-August-Universit¨atG¨ottingen University of Utah Deutschland Steve Smaley City University of Hong Kong With an appendix by Anthony W. Baker z Mathematics and Computing Technology The Boeing Company. Last compiled December 1, 2009; last edited December 1, by LB Abstract Hodge theory is a beautiful synthesis of geometry, topology, and anal- ysis, which has been developed in the setting of Riemannian manifolds. On the other hand, spaces of images, which are important in the math- ematical foundations of vision and pattern recognition, do not fit this framework. This motivates us to develop a version of Hodge theory on metric spaces with a probability measure. We believe that this constitutes a step towards understanding the geometry of vision. The appendix by Anthony Baker provides a separable, compact metric space with infinite dimensional α-scale homology. 1 Introduction Hodge Theory [21] studies the relationships of topology, functional analysis and geometry of a manifold. It extends the theory of the Laplacian on domains of Euclidean space or on a manifold. ∗email: [email protected] and [email protected] www: http://www.uni-math.gwdg.de/schick Laurent Bartholdi and Thomas Schick were partially supported by the Courant Research Center \Higher order structures in Mathematics" of the German Initiative of Excellence ySteve Smale was supported in part by the NSF, and the Toyota Technological Institute, Chicago zemail: [email protected] 1 2 Laurent Bartholdi, Thomas Schick, Nat Smale, Steve Smale However, there are a number of spaces, not manifolds, which could ben- efit from an extension of Hodge theory, and that is the motivation here. -
Cohomology and Hodge Theory on Symplectic Manifolds: I
j. differential geometry 91 (2012) 383-416 COHOMOLOGY AND HODGE THEORY ON SYMPLECTIC MANIFOLDS: I Li-Sheng Tseng & Shing-Tung Yau Abstract We introduce new finite-dimensional cohomologies on symplec- tic manifolds. Each exhibits Lefschetz decomposition and contains a unique harmonic representative within each class. Associated with each cohomology is a primitive cohomology defined purely on the space of primitive forms. We identify the dual currents of lagrangians and more generally coisotropic submanifolds with el- ements of a primitive cohomology, which dualizes to a homology on coisotropic chains. 1. Introduction The importance of Hodge theory in Riemannian and complex geome- try is without question. But in the symplectic setting, although a notion of symplectic Hodge theory was discussed in the late 1940s by Ehres- mann and Libermann [7, 15] and re-introduced by Brylinski [4] about twenty years ago, its usefulness has been rather limited. To write down a symplectic adjoint, one makes use of the symplectic star operator s, defined analogously to the Hodge star operator but with respect to∗ a symplectic form ω instead of a metric. Specifically, on a symplectic man- ifold (M,ω) with dimension 2n, the symplectic star acts on a differential k-form by ′ −1 k ′ A sA = (ω ) (A, A ) dvol ∧ ∗ ωn 1 −1 i1j1 −1 i2j2 −1 ikjk ′ = (ω ) (ω ) . (ω ) Ai i ...i A k! 1 2 k j1j2...jk n! with repeated indices summed over. The adjoint of the standard exterior derivative takes the form Λ k+1 d = ( 1) s d s, − ∗ ∗ acting on a k-form. A differential form is then called “symplectic har- monic” if it is both d-closed and dΛ-closed. -
The Decomposition Theorem, Perverse Sheaves and the Topology of Algebraic Maps
BULLETIN (New Series) OF THE AMERICAN MATHEMATICAL SOCIETY Volume 46, Number 4, October 2009, Pages 535–633 S 0273-0979(09)01260-9 Article electronically published on June 26, 2009 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 alge- braic varieties. While most proofs are omitted, we discuss several approaches to the decomposition theorem and indicate some important applications and examples. Contents 1. Overview 536 1.1. The topology of complex projective manifolds: Lefschetz and Hodge theorems 538 1.2. Families of smooth projective varieties 538 1.3. Singular algebraic varieties 540 1.4. Decomposition and hard Lefschetz in intersection cohomology 540 1.5. Crash course on sheaves and derived categories 541 1.6. Decomposition, semisimplicity and relative hard Lefschetz theorems 545 1.7. Invariant cycle theorems 547 1.8. A few examples 548 1.9. The decomposition theorem and mixed Hodge structures 549 1.10. Historical and other remarks 550 2. Perverse sheaves 551 2.1. Intersection cohomology 552 2.2. Examples of intersection cohomology 553 2.3. Definition and first properties of perverse sheaves 555 2.4. The perverse filtration 558 2.5. Perverse cohomology 559 2.6. t-exactness and the Lefschetz hyperplane theorem 560 2.7. Intermediate extensions 561 3. -
On Deligne's Monodromy Finiteness Theorem
ON DELIGNE'S MONODROMY FINITENESS THEOREM (MIMUW AG SEMINAR, DEC 13, 2018) PIOTR ACHINGER Abstract. Let S be a smooth complex algebraic variety with a base point 0. If X=S is a family of smooth projective varieties, one obtains the associ- ∗ ated monodromy representation π1(S; 0) ! GL(H (X0; Q)) of the topological fundamental group of S on the rational cohomology of X0. Let us say that a representation π1(S; 0) ! GLN (Q) \comes from geometry" if it is a direct summand of such a monodromy representation. Representations coming from geometry are quite special: they factor through GLN (Z) up to conjugation, their monodromy groups are semisimple, and the corresponding local system on S underlies a polarizable variation of Hodge structures. Inspired by a theo- rem of Faltings, Deligne proved in the mid-80s that there are only finitely many such representations of rank N for fixed S and N. We explain the beautifully simple proof of this result, based on Griffiths’ study of the geometry of period domains. We also discuss the very recent results of Litt which in particular imply a suitable analog for the ´etalefundamental group. 1. Monodromy representations Ehresmann's theorem in differential geometry states that if f : X −! S is a proper submersion of smooth manifolds, then f is a fiber bundle. Consequently, n the cohomology groups of the fibers H (Xs; Q)(s 2 S) assemble into a local system n R f∗Q on S. If S is connected and 0 2 S, such a local system corresponds to a representation n σ : π1(S; 0) −! GL(H (X0; Q)); called the monodromy representation associated to f : X ! S (in degree n).