K-Stability for Kähler Manifolds
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10. Relative Proj and the Blow up We Want to Define a Relative Version Of
10. Relative proj and the blow up We want to define a relative version of Proj, in pretty much the same way we defined a relative version of Spec. We start with a scheme X and a quasi-coherent sheaf S sheaf of graded OX -algebras, M S = Sd; d2N where S0 = OX . It is convenient to make some simplifying assump- tions: (y) X is Noetherian, S1 is coherent, S is locally generated by S1. To construct relative Proj, we cover X by open affines U = Spec A. 0 S(U) = H (U; S) is a graded A-algebra, and we get πU : Proj S(U) −! U a projective morphism. If f 2 A then we get a commutative diagram - Proj S(Uf ) Proj S(U) π U Uf ? ? - Uf U: It is not hard to glue πU together to get π : Proj S −! X. We can also glue the invertible sheaves together to get an invertible sheaf O(1). The relative consruction is very similar to the old construction. Example 10.1. If X is Noetherian and S = OX [T0;T1;:::;Tn]; n then satisfies (y) and Proj S = PX . Given a sheaf S satisfying (y), and an invertible sheaf L, it is easy to construct a quasi-coherent sheaf S0 = S ? L, which satisfies (y). The 0 d graded pieces of S are Sd ⊗ L and the multiplication maps are the obvious ones. There is a natural isomorphism φ: P 0 = Proj S0 −! P = Proj S; which makes the digram commute φ P 0 - P π0 π - S; and ∗ 0∗ φ OP 0 (1) 'OP (1) ⊗ π L: 1 Note that π is always proper; in fact π is projective over any open affine and properness is local on the base. -
CHERN CLASSES of BLOW-UPS 1. Introduction 1.1. a General Formula
CHERN CLASSES OF BLOW-UPS PAOLO ALUFFI Abstract. We extend the classical formula of Porteous for blowing-up Chern classes to the case of blow-ups of possibly singular varieties along regularly embed- ded centers. The proof of this generalization is perhaps conceptually simpler than the standard argument for the nonsingular case, involving Riemann-Roch without denominators. The new approach relies on the explicit computation of an ideal, and a mild generalization of the well-known formula for the normal bundle of a proper transform ([Ful84], B.6.10). We also discuss alternative, very short proofs of the standard formula in some cases: an approach relying on the theory of Chern-Schwartz-MacPherson classes (working in characteristic 0), and an argument reducing the formula to a straight- forward computation of Chern classes for sheaves of differential 1-forms with loga- rithmic poles (when the center of the blow-up is a complete intersection). 1. Introduction 1.1. A general formula for the Chern classes of the tangent bundle of the blow-up of a nonsingular variety along a nonsingular center was conjectured by J. A. Todd and B. Segre, who established several particular cases ([Tod41], [Seg54]). The formula was eventually proved by I. R. Porteous ([Por60]), using Riemann-Roch. F. Hirzebruch’s summary of Porteous’ argument in his review of the paper (MR0121813) may be recommend for a sharp and lucid account. For a thorough treatment, detailing the use of Riemann-Roch ‘without denominators’, the standard reference is §15.4 in [Ful84]. Here is the formula in the notation of the latter reference. -
Algebraic Curves and Surfaces
Notes for Curves and Surfaces Instructor: Robert Freidman Henry Liu April 25, 2017 Abstract These are my live-texed notes for the Spring 2017 offering of MATH GR8293 Algebraic Curves & Surfaces . Let me know when you find errors or typos. I'm sure there are plenty. 1 Curves on a surface 1 1.1 Topological invariants . 1 1.2 Holomorphic invariants . 2 1.3 Divisors . 3 1.4 Algebraic intersection theory . 4 1.5 Arithmetic genus . 6 1.6 Riemann{Roch formula . 7 1.7 Hodge index theorem . 7 1.8 Ample and nef divisors . 8 1.9 Ample cone and its closure . 11 1.10 Closure of the ample cone . 13 1.11 Div and Num as functors . 15 2 Birational geometry 17 2.1 Blowing up and down . 17 2.2 Numerical invariants of X~ ...................................... 18 2.3 Embedded resolutions for curves on a surface . 19 2.4 Minimal models of surfaces . 23 2.5 More general contractions . 24 2.6 Rational singularities . 26 2.7 Fundamental cycles . 28 2.8 Surface singularities . 31 2.9 Gorenstein condition for normal surface singularities . 33 3 Examples of surfaces 36 3.1 Rational ruled surfaces . 36 3.2 More general ruled surfaces . 39 3.3 Numerical invariants . 41 3.4 The invariant e(V ).......................................... 42 3.5 Ample and nef cones . 44 3.6 del Pezzo surfaces . 44 3.7 Lines on a cubic and del Pezzos . 47 3.8 Characterization of del Pezzo surfaces . 50 3.9 K3 surfaces . 51 3.10 Period map . 54 a 3.11 Elliptic surfaces . -
K3 Surfaces and String Duality
RU-96-98 hep-th/9611137 November 1996 K3 Surfaces and String Duality Paul S. Aspinwall Dept. of Physics and Astronomy, Rutgers University, Piscataway, NJ 08855 ABSTRACT The primary purpose of these lecture notes is to explore the moduli space of type IIA, type IIB, and heterotic string compactified on a K3 surface. The main tool which is invoked is that of string duality. K3 surfaces provide a fascinating arena for string compactification as they are not trivial spaces but are sufficiently simple for one to be able to analyze most of their properties in detail. They also make an almost ubiquitous appearance in the common statements concerning string duality. We arXiv:hep-th/9611137v5 7 Sep 1999 review the necessary facts concerning the classical geometry of K3 surfaces that will be needed and then we review “old string theory” on K3 surfaces in terms of conformal field theory. The type IIA string, the type IIB string, the E E heterotic string, 8 × 8 and Spin(32)/Z2 heterotic string on a K3 surface are then each analyzed in turn. The discussion is biased in favour of purely geometric notions concerning the K3 surface itself. Contents 1 Introduction 2 2 Classical Geometry 4 2.1 Definition ..................................... 4 2.2 Holonomy ..................................... 7 2.3 Moduli space of complex structures . ..... 9 2.4 Einsteinmetrics................................. 12 2.5 AlgebraicK3Surfaces ............................. 15 2.6 Orbifoldsandblow-ups. .. 17 3 The World-Sheet Perspective 25 3.1 TheNonlinearSigmaModel . 25 3.2 TheTeichm¨ullerspace . .. 27 3.3 Thegeometricsymmetries . .. 29 3.4 Mirrorsymmetry ................................. 31 3.5 Conformalfieldtheoryonatorus . ... 33 4 Type II String Theory 37 4.1 Target space supergravity and compactification . -
Intersection Theory on Algebraic Stacks and Q-Varieties
Journal of Pure and Applied Algebra 34 (1984) 193-240 193 North-Holland INTERSECTION THEORY ON ALGEBRAIC STACKS AND Q-VARIETIES Henri GILLET Department of Mathematics, Princeton University, Princeton, NJ 08544, USA Communicated by E.M. Friedlander Received 5 February 1984 Revised 18 May 1984 Contents Introduction ................................................................ 193 1. Preliminaries ................................................................ 196 2. Algebraic groupoids .......................................................... 198 3. Algebraic stacks ............................................................. 207 4. Chow groups of stacks ....................................................... 211 5. Descent theorems for rational K-theory. ........................................ 2 16 6. Intersection theory on stacks .................................................. 219 7. K-theory of stacks ........................................................... 229 8. Chcrn classes and the Riemann-Roth theorem for algebraic spaces ................ 233 9. comparison with Mumford’s product .......................................... 235 References .................................................................. 239 0. Introduction In his article 1161, Mumford constructed an intersection product on the Chow groups (with rational coefficients) of the moduli space . fg of stable curves of genus g over a field k of characteristic zero. Having such a product is important in study- ing the enumerative geometry of curves, and it is reasonable -
Seven Short Stories on Blowups and Resolutions
Proceedings of 12th G¨okova Published online at Geometry-Topology Conference GokovaGT.org pp. 1 – 48 Seven short stories on blowups and resolutions Herwig Hauser To Raoul Bott – with great respect. “At that time, blowups were the poor man’s tool to resolve singularities.” This phrase of the late 21st century mathematician J.H.Φ. Leicht could become correct. In our days, however, blowups are still the main device for resolution purposes (cf. fig. 1). Figure 1: Resolution of the surface Helix: x2 − x4 = y2z2 by two blowups. These notes shall give an informal introduction to the subject. They are complemented by the discussion of many special and less known features of blowups. The lectures adress to students and geometers who are not experts in the field, but who need to use blowups occasionally or who just want to have a good comprehension of them. References are scattered in the literature and mostly concentrate on only part of the story. This text is neither complete, but hints at least at the variety of properties, results and techniques which are related to blowups and which make them so attractive. Actually, it may serve as the starting point to write a comprehensive treatise on blowups (which should in particular include the solutions to all exercises). The obvious objection from algebraic geometers to such a project will be that blowups are too simple to deserve a separate treatment. The many open and intricate questions listed in these notes may serve as a reply to this reproach. The material stems from lectures held by the author at the Mathematical Sciences Re- search Institute (MSRI) at Berkeley in April and May 2004 and during the Conference on Geometry and Topology at G¨okova, Turkey, in June 2005. -
Intersection Theory
William Fulton Intersection Theory Second Edition Springer Contents Introduction. Chapter 1. Rational Equivalence 6 Summary 6 1.1 Notation and Conventions 6 .2 Orders of Zeros and Poles 8 .3 Cycles and Rational Equivalence 10 .4 Push-forward of Cycles 11 .5 Cycles of Subschemes 15 .6 Alternate Definition of Rational Equivalence 15 .7 Flat Pull-back of Cycles 18 .8 An Exact Sequence 21 1.9 Affine Bundles 22 1.10 Exterior Products 24 Notes and References 25 Chapter 2. Divisors 28 Summary 28 2.1 Cartier Divisors and Weil Divisors 29 2.2 Line Bundles and Pseudo-divisors 31 2.3 Intersecting with Divisors • . 33 2.4 Commutativity of Intersection Classes 35 2.5 Chern Class of a Line Bundle 41 2.6 Gysin Map for Divisors 43 Notes and References 45 Chapter 3. Vector Bundles and Chern Classes 47 Summary 47 3.1 Segre Classes of Vector Bundles 47 3.2 Chern Classes . ' 50 • 3.3 Rational Equivalence on Bundles 64 Notes and References 68 Chapter 4. Cones and Segre Classes 70 Summary . 70 . 4.1 Segre Class of a Cone . 70 X Contents 4.2 Segre Class of a Subscheme 73 4.3 Multiplicity Along a Subvariety 79 4.4 Linear Systems 82 Notes and References 85 Chapter 5. Deformation to the Normal Cone 86 Summary 86 5.1 The Deformation 86 5.2 Specialization to the Normal Cone 89 Notes and References 90 Chapter 6. Intersection Products 92 Summary 92 6.1 The Basic Construction 93 6.2 Refined Gysin Homomorphisms 97 6.3 Excess Intersection Formula 102 6.4 Commutativity 106 6.5 Functoriality 108 6.6 Local Complete Intersection Morphisms 112 6.7 Monoidal Transforms 114 Notes and References 117 Chapter 7. -
'Cycle Groups for Artin Stacks'
Cycle groups for Artin stacks Andrew Kresch1 28 October 1998 Contents 1 Introduction 2 2 Definition and first properties 3 2.1 Thehomologyfunctor .......................... 3 2.2 BasicoperationsonChowgroups . 8 2.3 Results on sheaves and vector bundles . 10 2.4 Theexcisionsequence .......................... 11 3 Equivalence on bundles 12 3.1 Trivialbundles .............................. 12 3.2 ThetopChernclassoperation . 14 3.3 Collapsing cycles to the zero section . ... 15 3.4 Intersecting cycles with the zero section . ..... 17 3.5 Affinebundles............................... 19 3.6 Segre and Chern classes and the projective bundle theorem...... 20 4 Elementary intersection theory 22 4.1 Fulton-MacPherson construction for local immersions . ........ 22 arXiv:math/9810166v1 [math.AG] 28 Oct 1998 4.2 Exteriorproduct ............................. 24 4.3 Intersections on Deligne-Mumford stacks . .... 24 4.4 Boundedness by dimension . 25 4.5 Stratificationsbyquotientstacks . .. 26 5 Extended excision axiom 29 5.1 AfirsthigherChowtheory. 29 5.2 The connecting homomorphism . 34 5.3 Homotopy invariance for vector bundle stacks . .... 36 1Funded by a Fannie and John Hertz Foundation Fellowship for Graduate Study and an Alfred P. Sloan Foundation Dissertation Fellowship 1 6 Intersection theory 37 6.1 IntersectionsonArtinstacks . 37 6.2 Virtualfundamentalclass . 39 6.3 Localizationformula ........................... 39 1 Introduction We define a Chow homology functor A∗ for Artin stacks and prove that it satisfies some of the basic properties expected from intersection theory. Consequences in- clude an integer-valued intersection product on smooth Deligne-Mumford stacks, an affirmative answer to the conjecture that any smooth stack with finite but possibly nonreduced point stabilizers should possess an intersection product (this provides a positive answer to Conjecture 6.6 of [V2]), and more generally an intersection prod- uct (also integer-valued) on smooth Artin stacks which admit stratifications by global quotient stacks. -
UC Berkeley UC Berkeley Electronic Theses and Dissertations
UC Berkeley UC Berkeley Electronic Theses and Dissertations Title The arithmetic Hodge-index theorem and rigidity of algebraic dynamical systems over function fields Permalink https://escholarship.org/uc/item/4xb7w3f8 Author Carney, Alexander Publication Date 2019 Peer reviewed|Thesis/dissertation eScholarship.org Powered by the California Digital Library University of California The arithmetic Hodge-index theorem and rigidity of algebraic dynamical systems over function fields by Alexander Carney Adissertationsubmittedinpartialsatisfactionofthe requirements for the degree of Doctor of Philosophy in Mathematics in the Graduate Division of the University of California, Berkeley Committee in charge: Associate Professor Xinyi Yuan, Chair Associate Professor Burkhard Militzer Associate Professor Sug Woo Shin Spring 2019 The arithmetic Hodge-index theorem and rigidity of algebraic dynamical systems over function fields Copyright 2019 by Alexander Carney 1 Abstract The arithmetic Hodge-index theorem and rigidity of algebraic dynamical systems over function fields by Alexander Carney Doctor of Philosophy in Mathematics University of California, Berkeley Associate Professor Xinyi Yuan, Chair In one of the fundamental results of Arakelov’s arithmetic intersection theory, Faltings and Hriljac (independently) proved the Hodge-index theorem for arithmetic surfaces by relating the intersection pairing to the negative of the Neron-Tate height pairing. More recently, Moriwaki and Yuan–Zhang generalized this to higher dimension. In this work, we extend these results to projective varieties over transcendence degree one function fields. The new challenge is dealing with non-constant but numerically trivial line bundles coming from the constant field via Chow’s K/k-image functor. As an application of the Hodge-index theorem to heights defined by intersections of adelic metrized line bundles, we also prove a rigidity theorem for the set height zero points of polarized algebraic dynamical systems over function fields. -
Intersection Theory
APPENDIX A Intersection Theory In this appendix we will outline the generalization of intersection theory and the Riemann-Roch theorem to nonsingular projective varieties of any dimension. To motivate the discussion, let us look at the case of curves and surfaces, and then see what needs to be generalized. For a divisor D on a curve X, leaving out the contribution of Serre duality, we can write the Riemann-Roch theorem (IV, 1.3) as x(.!Z'(D)) = deg D + 1 - g, where xis the Euler characteristic (III, Ex. 5.1). On a surface, we can write the Riemann-Roch theorem (V, 1.6) as 1 x(!l'(D)) = 2 D.(D - K) + 1 + Pa· In each case, on the left-hand side we have something involving cohomol ogy groups of the sheaf !l'(D), while on the right-hand side we have some numerical data involving the divisor D, the canonical divisor K, and some invariants of the variety X. Of course the ultimate aim of a Riemann-Roch type theorem is to compute the dimension of the linear system IDI or of lnDI for large n (II, Ex. 7.6). This is achieved by combining a formula for x(!l'(D)) with some vanishing theorems for Hi(X,!l'(D)) fori > 0, such as the theorems of Serre (III, 5.2) or Kodaira (III, 7.15). We will now generalize these results so as to give an expression for x(!l'(D)) on a nonsingular projective variety X of any dimension. And while we are at it, with no extra effort we get a formula for x(t&"), where @" is any coherent locally free sheaf. -
2 May 2020 Real Intersection Theory (II)
Real intersection theory (II) B. Wang (汪 镔) May 5, 2020 Abstract Continuing from part (I), we develop properties of real intersection theory that turns out to be an extension of the well-established theory in algebraic geometry. Contents 1 Introduction 2 2 Basic properties 3 2.1 Basicproperties.......................... 7 2.2 ProductandInclusion ...................... 11 3 Dependence of the local data 18 3.1 Realcase ............................. 18 arXiv:1801.01364v4 [math.AG] 2 May 2020 3.2 Complexcase........................... 25 4 Tools for application 30 4.1 Correspondenceofacurrent . 30 4.2 Functoriality ........................... 35 4.3 Familyofcurrents ........................ 38 5 Generalized Hodge conjecture on 3-folds 41 Key words: currents, De Rham, intersection. 2000 Mathematics subject classification : 53C65, 32C30, 14C17, 14C30. 1 1 INTRODUCTION 2 Appendices 43 A Support of the projection 43 1 Introduction Intersection in mathematics has a long history. But the systemically devel- oped theories only started appearing in the 20th century. They are centered around the quotient rings that are derived from freely generated Abelian groups of non-quotient objects. While the quotient rings fit into the known axiomatic system well, the non-quotient groups do not. For instance in classical approach the topological intersection for a real compact manifold X in homology or/and cohomology (quotient groups) are obtained from the non quotient objects – singular chains. Once the theory is set up, quotient groups are well-adapted to the axiomatic environment, but the groups of singular chains are not. Using cohomology we can let Hi(X; Z) be the cohomology of degree i with integer coefficients. The product is defined in an elaborated method through the intersection of chains as the cup product, ∪ : Hp(X; Q) × Hq(X; Z) → Hp+q(X; Z). -
Theoretical Physics
IC/93/53 HftTH INTERNATIONAL CENTRE FOR THEORETICAL PHYSICS ENUMERATIVE GEOMETRY OF DEL PEZZO SURFACES D. Avritzer INTERNATIONAL ATOMIC ENERGY AGENCY UNITED NATIONS EDUCATIONAL, SCIENTIFIC AND CULTURAL ORGANIZATION MIRAMARE-TRIESTE IC/93/53 1 Introduction International Atomic Energy Agency and Let H be the Hilbert scheme component parametrizing all specializations of complete intersections of two quadric hypersurfaces in Pn. In jlj it is proved that for n > 2. H is United Nations Educational Scientific and Cultural Organization isomorphic to the grassmannian of pencils of hyperquadrics blown up twice at appropriate smooth subvarieties. The case n = 3 was done in [5j. INTERNATIONAL CENTRE FOR THEORETICAL PHYSICS The aim of this paper is to apply the results of [1] and [5] to enuinerative geometry. The number 52 832 040 of elliptic quartic curves of P3 that meet 16 Sines'in general position; as well as, the number 47 867 287 590 090 of Del Pezzo surfaces in ¥* that meet 26 lines in general position are computed. In particular, the number announced in [5] is ENUMERATIVE GEOMETRY OF DEL PEZZO SURFACES corrected. Let us summarize the contents of the paper. There is a natural rational map, /?, from the grassmannian G of pencils of quadrics to W, assigning to w its base locus /3(ir). The map j3 is not defined along the subvariety B = P" x £7(2, n + 1) of G consisting of pencils with a fixed component. Let Cj,C2 C G be cycles of codimensions ai,« and suppose D. Avritzer * 2 we want to compute the number International Centre for Theoretical Physics, Trieste, Italy.