THE MODULI SPACE of CURVES 1. the Moduli Space of Curves and a Few Remarks About Its Construction the Theory of Smooth Algebrai
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California State University, Northridge Torsion
CALIFORNIA STATE UNIVERSITY, NORTHRIDGE TORSION CLASSES OF COHERENT SHEAVES ON AN ELLIPTIC OR PRODUCT THREEFOLD A thesis submitted in partial fulfillment of the requirements for the degree of Master of Science in Mathematics By Jeremy Keat-Wah Khoo August 2020 The thesis of Jeremy Keat-Wah Khoo is approved: Katherine Stevenson, Ph.D. Date Jerry D. Rosen, Ph.D. Date Jason Lo, Ph.D., Chair Date California State University, Northridge ii Table of Contents Signature page ii Abstract iv 1 Introduction 1 1.1 Our Methods . .1 1.2 Main Results . .2 2 Background Concepts 3 2.1 Concepts from Homological Algebra and Category Theory . .3 2.2 Concepts from Algebraic Geometry . .8 2.3 Concepts from Scheme theory . 10 3 Main Definitions and “Axioms” 13 3.1 The Variety X ................................. 13 3.2 Supports of Coherent Sheaves . 13 3.3 Dimension Subcategories of AX ....................... 14 3.4 Torsion Pairs . 14 3.5 The Relative Fourier-Mukai Transforms Φ; Φ^ ................ 15 3.6 The Product Threefold and Chern Classes . 16 4 Preliminary Results 18 5 Properties Characterizing Tij 23 6 Generating More Torsion Classes 30 6.1 Generalizing Lemma 4.2 . 30 6.2 “Second Generation” Torsion Classes . 34 7 The Torsion Class hC00;C20i 39 References 42 iii ABSTRACT TORSION CLASSES OF COHERENT SHEAVES ON AN ELLIPTIC OR PRODUCT THREEFOLD By Jeremy Keat-Wah Khoo Master of Science in Mathematics Let X be an elliptic threefold admitting a Weierstrass elliptic fibration. We extend the main results of Angeles, Lo, and Van Der Linden in [1] by providing explicit properties charac- terizing the coherent sheaves contained in the torsion classes constructed there. -
Stack Completions and Morita Equivalence for Categories in a Topos Cahiers De Topologie Et Géométrie Différentielle Catégoriques, Tome 20, No 4 (1979), P
CAHIERS DE TOPOLOGIE ET GÉOMÉTRIE DIFFÉRENTIELLE CATÉGORIQUES MARTA BUNGE Stack completions and Morita equivalence for categories in a topos Cahiers de topologie et géométrie différentielle catégoriques, tome 20, no 4 (1979), p. 401-436 <http://www.numdam.org/item?id=CTGDC_1979__20_4_401_0> © Andrée C. Ehresmann et les auteurs, 1979, tous droits réservés. L’accès aux archives de la revue « Cahiers de topologie et géométrie différentielle catégoriques » implique l’accord avec les conditions générales d’utilisation (http://www.numdam.org/conditions). Toute utilisation commerciale ou impression systématique est constitutive d’une infraction pénale. Toute copie ou impression de ce fichier doit contenir la présente mention de copyright. Article numérisé dans le cadre du programme Numérisation de documents anciens mathématiques http://www.numdam.org/ CAHIERS DE TOPOLOGIE Vol. XX-4 (1979) ET GEOMETRIE DIFFERENTIELLE STACK COMPLETIONS AND MORITA EQUIVALENCE FOR CATEGORIES IN A TOPOS by Marta BUNGE 1) 0. INTRODUCTION. The origin of this paper can be traced back to one of a series of lectures given by F.W. Lawvere [10, Lecture V]. In it, Lawvere dealt for the case of an arbitrary topos S , with the notion of stack, a notion which, for Grothendieck toposes, had been considered by J. Giraud [6], and which is given relative to a site. A topos S may always be regarded as a site with the regular epi- morphism topology, and the notion of stack over S is then defined with respect to this particular topology. Special as it may be, this notion of stack over a topos S plays an important role in the development of Category Theory over a base to- pos S . -
Moduli Spaces
spaces. Moduli spaces such as the moduli of elliptic curves (which we discuss below) play a central role Moduli Spaces in a variety of areas that have no immediate link to the geometry being classified, in particular in alge- David D. Ben-Zvi braic number theory and algebraic topology. Moreover, the study of moduli spaces has benefited tremendously in recent years from interactions with Many of the most important problems in mathemat- physics (in particular with string theory). These inter- ics concern classification. One has a class of math- actions have led to a variety of new questions and new ematical objects and a notion of when two objects techniques. should count as equivalent. It may well be that two equivalent objects look superficially very different, so one wishes to describe them in such a way that equiv- 1 Warmup: The Moduli Space of Lines in alent objects have the same description and inequiva- the Plane lent objects have different descriptions. Moduli spaces can be thought of as geometric solu- Let us begin with a problem that looks rather simple, tions to geometric classification problems. In this arti- but that nevertheless illustrates many of the impor- cle we shall illustrate some of the key features of mod- tant ideas of moduli spaces. uli spaces, with an emphasis on the moduli spaces Problem. Describe the collection of all lines in the of Riemann surfaces. (Readers unfamiliar with Rie- real plane R2 that pass through the origin. mann surfaces may find it helpful to begin by reading about them in Part III.) In broad terms, a moduli To save writing, we are using the word “line” to mean problem consists of three ingredients. -
Vector Bundles As Generators on Schemes and Stacks
Vector Bundles as Generators on Schemes and Stacks Inaugural-Dissertation zur Erlangung des Doktorgrades der Mathematisch-Naturwissenschaftlichen Fakult¨at der Heinrich-Heine-Universit¨atD¨usseldorf vorgelegt von Philipp Gross aus D¨usseldorf D¨usseldorf,Mai 2010 Aus dem Mathematischen Institut der Heinrich-Heine-Universit¨atD¨usseldorf Gedruckt mit der Genehmigung der Mathematisch-Naturwissenschaftlichen Fakult¨atder Heinrich-Heine-Universit¨atD¨usseldorf Referent: Prof. Dr. Stefan Schr¨oer Koreferent: Prof. Dr. Holger Reich Acknowledgments The work on this dissertation has been one of the most significant academic challenges I have ever had to face. This study would not have been completed without the support, patience and guidance of the following people. It is to them that I owe my deepest gratitude. I am indebted to my advisor Stefan Schr¨oerfor his encouragement to pursue this project. He taught me algebraic geometry and how to write academic papers, made me a better mathematician, brought out the good ideas in me, and gave me the opportunity to attend many conferences and schools in Europe. I also thank Holger Reich, not only for agreeing to review the dissertation and to sit on my committee, but also for showing an interest in my research. Next, I thank the members of the local algebraic geometry research group for their time, energy and for the many inspiring discussions: Christian Liedtke, Sasa Novakovic, Holger Partsch and Felix Sch¨uller.I have had the pleasure of learning from them in many other ways as well. A special thanks goes to Holger for being a friend, helping me complete the writing of this dissertation as well as the challenging research that lies behind it. -
Jhep05(2019)105
Published for SISSA by Springer Received: March 21, 2019 Accepted: May 7, 2019 Published: May 20, 2019 Modular symmetries and the swampland conjectures JHEP05(2019)105 E. Gonzalo,a;b L.E. Ib´a~neza;b and A.M. Urangaa aInstituto de F´ısica Te´orica IFT-UAM/CSIC, C/ Nicol´as Cabrera 13-15, Campus de Cantoblanco, 28049 Madrid, Spain bDepartamento de F´ısica Te´orica, Facultad de Ciencias, Universidad Aut´onomade Madrid, 28049 Madrid, Spain E-mail: [email protected], [email protected], [email protected] Abstract: Recent string theory tests of swampland ideas like the distance or the dS conjectures have been performed at weak coupling. Testing these ideas beyond the weak coupling regime remains challenging. We propose to exploit the modular symmetries of the moduli effective action to check swampland constraints beyond perturbation theory. As an example we study the case of heterotic 4d N = 1 compactifications, whose non-perturbative effective action is known to be invariant under modular symmetries acting on the K¨ahler and complex structure moduli, in particular SL(2; Z) T-dualities (or subgroups thereof) for 4d heterotic or orbifold compactifications. Remarkably, in models with non-perturbative superpotentials, the corresponding duality invariant potentials diverge at points at infinite distance in moduli space. The divergence relates to towers of states becoming light, in agreement with the distance conjecture. We discuss specific examples of this behavior based on gaugino condensation in heterotic orbifolds. We show that these examples are dual to compactifications of type I' or Horava-Witten theory, in which the SL(2; Z) acts on the complex structure of an underlying 2-torus, and the tower of light states correspond to D0-branes or M-theory KK modes. -
The Topology of Moduli Space and Quantum Field Theory* ABSTRACT
SLAC-PUB-4760 October 1988 CT) . The Topology of Moduli Space and Quantum Field Theory* DAVID MONTANO AND JACOB SONNENSCHEIN+ Stanford Linear Accelerator Center Stanford University, Stanford, California 9.4309 ABSTRACT We show how an SO(2,l) gauge theory with a fermionic symmetry may be used to describe the topology of the moduli space of curves. The observables of the theory correspond to the generators of the cohomology of moduli space. This is an extension of the topological quantum field theory introduced by Witten to -- .- . -. investigate the cohomology of Yang-Mills instanton moduli space. We explore the basic structure of topological quantum field theories, examine a toy U(1) model, and then realize a full theory of moduli space topology. We also discuss why a pure gravity theory, as attempted in previous work, could not succeed. Submitted to Nucl. Phys. I3 _- .- --- _ * Work supported by the Department of Energy, contract DE-AC03-76SF00515. + Work supported by Dr. Chaim Weizmann Postdoctoral Fellowship. 1. Introduction .. - There is a widespread belief that the Lagrangian is the fundamental object for study in physics. The symmetries of nature are simply properties of the relevant Lagrangian. This philosophy is one of the remaining relics of classical physics where the Lagrangian is indeed fundamental. Recently, Witten has discovered a class of quantum field theories which have no classical analog!” These topo- logical quantum field theories (TQFT) are, as their name implies, characterized by a Hilbert space of topological invariants. As has been recently shown, they can be constructed by a BRST gauge fixing of a local symmetry. -
X → S Be a Proper Morphism of Locally Noetherian Schemes and Let F Be a Coherent Sheaf on X That Is flat Over S (E.G., F Is Smooth and F Is a Vector Bundle)
COHOMOLOGY AND BASE CHANGE FOR ALGEBRAIC STACKS JACK HALL Abstract. We prove that cohomology and base change holds for algebraic stacks, generalizing work of Brochard in the tame case. We also show that Hom-spaces on algebraic stacks are represented by abelian cones, generaliz- ing results of Grothendieck, Brochard, Olsson, Lieblich, and Roth{Starr. To accomplish all of this, we prove that a wide class of relative Ext-functors in algebraic geometry are coherent (in the sense of M. Auslander). Introduction Let f : X ! S be a proper morphism of locally noetherian schemes and let F be a coherent sheaf on X that is flat over S (e.g., f is smooth and F is a vector bundle). If s 2 S is a point, then define Xs to be the fiber of f over s. If s has residue field κ(s), then for each integer q there is a natural base change morphism of κ(s)-vector spaces q q q b (s):(R f∗F) ⊗OS κ(s) ! H (Xs; FXs ): Cohomology and Base Change originally appeared in [EGA, III.7.7.5] in a quite sophisticated form. Mumford [Mum70, xII.5] and Hartshorne [Har77, xIII.12], how- ever, were responsible for popularizing a version similar to the following. Let s 2 S and let q be an integer. (1) The following are equivalent. (a) The morphism bq(s) is surjective. (b) There exists an open neighbourhood U of s such that bq(u) is an iso- morphism for all u 2 U. (c) There exists an open neighbourhood U of s, a coherent OU -module Q, and an isomorphism of functors: Rq+1(f ) (F ⊗ f ∗ I) =∼ Hom (Q; I); U ∗ XU OXU U OU where fU : XU ! U is the pullback of f along U ⊆ S. -
LOCAL PROPERTIES of GOOD MODULI SPACES We Address The
LOCAL PROPERTIES OF GOOD MODULI SPACES JAROD ALPER ABSTRACT. We study the local properties of Artin stacks and their good moduli spaces, if they exist. We show that near closed points with linearly reductive stabilizer, Artin stacks formally locally admit good moduli spaces. In particular, the geometric invariant theory is developed for actions of linearly reductive group schemes on formal affine schemes. We also give conditions for when the existence of good moduli spaces can be deduced from the existence of etale´ charts admitting good moduli spaces. 1. INTRODUCTION We address the question of whether good moduli spaces for an Artin stack can be constructed “locally.” The main results of this paper are: (1) good moduli spaces ex- ist formally locally around points with linearly reductive stabilizer and (2) sufficient conditions are given for the Zariski-local existence of good moduli spaces given the etale-local´ existence of good moduli spaces. We envision that these results may be of use to construct moduli schemes of Artin stacks without the classical use of geometric invariant theory and semi-stability computations. The notion of a good moduli space was introduced in [1] to assign a scheme or algebraic space to Artin stacks with nice geometric properties reminiscent of Mumford’s good GIT quotients. While good moduli spaces cannot be expected to distinguish between all points of the stack, they do parameterize points up to orbit closure equivalence. See Section 2 for the precise definition of a good moduli space and for a summary of its properties. While the paper [1] systematically develops the properties of good moduli spaces, the existence was only proved in certain cases. -
Donaldson Invariants and Moduli of Yang-Mills Instantons
Donaldson Invariants and Moduli of Yang-Mills Instantons Jacob Gross Lincoln College Oxford University (slides posted at users.ox.ac.uk/ linc4221) ∼ The ASD Equation in Low Dimensions, 17 November 2017 Jacob Gross Donaldson Invariants and Moduli of Yang-Mills Instantons Moduli and Invariants Invariants are gotten by cooking up a number (homology group, derived category, etc.) using auxiliary data (a metric, a polarisation, etc.) and showing independence of that initial choice. Donaldson and Seiberg-Witten invariants count in moduli spaces of solutions of a pde (shown to be independent of conformal class of the metric). Example (baby example) f :(M, g) R, the number of solutions of → gradgf = 0 is independent of g (Poincare-Hopf).´ Jacob Gross Donaldson Invariants and Moduli of Yang-Mills Instantons Recall (Setup) (X, g) smooth oriented Riemannian 4-manifold and a principal G-bundle π : P X over it. → Consider the Yang-Mills functional YM(A) = F 2dμ. | A| ZM The corresponding Euler-Lagrange equations are dA∗FA = 0. Using the gauge group one generates lots of solutions from one. But one can fix aG gauge dA∗a = 0 Jacob Gross Donaldson Invariants and Moduli of Yang-Mills Instantons Recall (ASD Equations) 2 2 2 In dimension 4, the Hodge star splits the 2-forms Λ = Λ+ Λ . This splits the curvature ⊕ − + FA = FA + FA−. Have + 2 2 + 2 2 κ(P) = F F − YM(A) = F + F − , k A k − k A k ≤ k A k k A k where κ(P) is a topological invariant (e.g. for SU(2)-bundles, 2 κ(P) = 8π c2(P)). -
The Scheme of Monogenic Generators and Its Twists
THE SCHEME OF MONOGENIC GENERATORS AND ITS TWISTS SARAH ARPIN, SEBASTIAN BOZLEE, LEO HERR, HANSON SMITH Abstract. Given an extension of algebras B/A, when is B generated by a M single element θ ∈ B over A? We show there is a scheme B/A parameterizing the choice of a generator θ ∈ B, a “moduli space” of generators. This scheme relates naturally to Hilbert schemes and configuration spaces. We give explicit equations and ample examples. M A choice of a generator θ is a point of the scheme B/A. This inspires a local-to-global study of monogeneity, piecing together monogenerators over points, completions, open sets, and so on. Local generators may not come from global ones, but they often glue to twisted monogenerators that we de- fine. We show a number ring has class number one if and only if each twisted monogenerator is in fact a global generator θ. The moduli spaces of various M twisted monogenerators are either a Proj or stack quotient of B/A by natural symmetries. The various moduli spaces defined can be used to apply cohomo- logical tools and other geometric methods for finding rational points to the classical problem of monogenic algebra extensions. Contents 1. Introduction 2 1.1. Twists 3 1.2. Summary of the paper 4 1.3. Guide to notions of “Monogeneity” 4 1.4. Summary of Previous Results 5 1.5. Acknowledgements 6 2. The Scheme of Monogenic Generators 7 2.1. Functoriality of MX 10 2.2. Relation to the Hilbert Scheme 12 M arXiv:2108.07185v1 [math.AG] 16 Aug 2021 3. -
Gromov-Witten Invariants and Localization
Gromov–Witten invariants and localization David R. Morrison Departments of Mathematics and Physics University of California, Santa Barbara Santa Barbara, CA 93106 USA [email protected] Abstract We give a pedagogical review of the computation of Gromov–Witten invariants via localiza- tion in 2D gauged linear sigma models. We explain the relationship between the two-sphere partition function of the theory and the K¨ahler potential on the conformal manifold. We show how the K¨ahler potential can be assembled from classical, perturbative, and non- perturbative contributions, and explain how the non-perturbative contributions are related to the Gromov-Witten invariants of the corresponding Calabi–Yau manifold. We then ex- plain how localization enables efficient calculation of the two-sphere partition function and, ultimately, the Gromov–Witten invariants themselves. This is a contribution to the review volume “Localization techniques in quantum field theories” (eds. V. Pestun and M. Zabzine) which contains 17 Chapters available at [1] Contents 1 Introduction 2 2 K¨ahler potentials and 2-sphere partition functions 3 arXiv:1608.02956v3 [hep-th] 15 Oct 2016 3 Metrics on conformal manifolds 6 3.1 Nonlinearsigmamodels ............................. 6 3.2 Gaugedlinearsigmamodels ........................... 8 3.3 PhasesofanabelianGLSM ........................... 10 4 Quantum corrections to the K¨ahler potential 14 4.1 Nonlinear σ-modelactionandtheeffectiveaction . 14 4.2 Perturbative corrections to the K¨ahler potential . ....... 16 4.3 Nonperturbative corrections and Gromov–Witten invariants . ....... 17 5 The two-sphere partition function and Gromov–Witten invariants 20 5.1 The S2 partitionfunctionforaGLSM . 20 5.2 The hemisphere partition function and the tt∗ equations ........... 21 5.3 Extracting Gromov–Witten invariants from the partition function ..... -
The Orbifold Chow Ring of Toric Deligne-Mumford Stacks
JOURNAL OF THE AMERICAN MATHEMATICAL SOCIETY Volume 18, Number 1, Pages 193–215 S 0894-0347(04)00471-0 Article electronically published on November 3, 2004 THE ORBIFOLD CHOW RING OF TORIC DELIGNE-MUMFORD STACKS LEVA.BORISOV,LINDACHEN,ANDGREGORYG.SMITH 1. Introduction The orbifold Chow ring of a Deligne-Mumford stack, defined by Abramovich, Graber and Vistoli [2], is the algebraic version of the orbifold cohomology ring in- troduced by W. Chen and Ruan [7], [8]. By design, this ring incorporates numerical invariants, such as the orbifold Euler characteristic and the orbifold Hodge num- bers, of the underlying variety. The product structure is induced by the degree zero part of the quantum product; in particular, it involves Gromov-Witten invariants. Inspired by string theory and results in Batyrev [3] and Yasuda [28], one expects that, in nice situations, the orbifold Chow ring coincides with the Chow ring of a resolution of singularities. Fantechi and G¨ottsche [14] and Uribe [25] verify this conjecture when the orbifold is Symn(S)whereS is a smooth projective surface n with KS = 0 and the resolution is Hilb (S). The initial motivation for this project was to compare the orbifold Chow ring of a simplicial toric variety with the Chow ring of a crepant resolution. To achieve this goal, we first develop the theory of toric Deligne-Mumford stacks. Modeled on simplicial toric varieties, a toric Deligne-Mumford stack corresponds to a combinatorial object called a stacky fan. As a first approximation, this object is a simplicial fan with a distinguished lattice point on each ray in the fan.