Lecture 3 Supergeometry
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EXERCISES 1 Exercise 1.1. Let X = (|X|,O X) Be a Scheme and I Is A
EXERCISES 1 Exercise 1.1. Let X = (|X|, OX ) be a scheme and I is a quasi-coherent OX -module. Show that the ringed space X[I] := (|X|, OX [I]) is also a scheme. Exercise 1.2. Let C be a category and h : C → Func(C◦, Set) the Yoneda embedding. Show ∼ that for any arrows X → Y and Z → Y in C, there is a natural isomorphism hX×Z Y → hX ×hY hZ . Exercise 1.3. Let A → R be a ring homomorphism. Verify that under the identification 2 of DerA(R, ΩR/A) with the sections of the diagonal map R ⊗A R/J → R given in lecture, 1 the universal derivation d : R → ΩR/A corresponds to the section given by sending x ∈ R to 1 ⊗ x. Exercise 1.4. Let AffZ be the category of affine schemes. The Yoneda functor h gives rise to a related functor hAff : Sch → Func(Aff◦ , Set) Z Z which only considers the functor of points for affine schemes. Is this functor still fully faithful? Cultural note: since Aff◦ is equivalent to the category of rings ( -algebras!), we can also Z Z view h as defining a (covariant) functor on the category of rings. When X is an affine scheme Aff of the form Z[{xi}]/({fj}], the value of hX on A is just the set of solutions of the fj with coordinates in A. Exercise 1.5. Let R be a ring and H : ModR → Set a functor which commutes with finite products. Verify the claim in lecture that H(I) has an R-module structure. -
SUPERSYMMETRY 1. Introduction the Purpose
SUPERSYMMETRY JOSH KANTOR 1. Introduction The purpose of these notes is to give a short and (overly?)simple description of supersymmetry for Mathematicians. Our description is far from complete and should be thought of as a first pass at the ideas that arise from supersymmetry. Fundamental to supersymmetry is the mathematics of Clifford algebras and spin groups. We will describe the mathematical results we are using but we refer the reader to the references for proofs. In particular [4], [1], and [5] all cover spinors nicely. 2. Spin and Clifford Algebras We will first review the definition of spin, spinors, and Clifford algebras. Let V be a vector space over R or C with some nondegenerate quadratic form. The clifford algebra of V , l(V ), is the algebra generated by V and 1, subject to the relations v v = v, vC 1, or equivalently v w + w v = 2 v, w . Note that elements of· l(V ) !can"b·e written as polynomials· in V · and this! giv"es a splitting l(V ) = l(VC )0 l(V )1. Here l(V )0 is the set of elements of l(V ) which can bCe writtenC as a linear⊕ C combinationC of products of even numbers ofCvectors from V , and l(V )1 is the set of elements which can be written as a linear combination of productsC of odd numbers of vectors from V . Note that more succinctly l(V ) is just the quotient of the tensor algebra of V by the ideal generated by v vC v, v 1. -
SHEAVES of MODULES 01AC Contents 1. Introduction 1 2
SHEAVES OF MODULES 01AC Contents 1. Introduction 1 2. Pathology 2 3. The abelian category of sheaves of modules 2 4. Sections of sheaves of modules 4 5. Supports of modules and sections 6 6. Closed immersions and abelian sheaves 6 7. A canonical exact sequence 7 8. Modules locally generated by sections 8 9. Modules of finite type 9 10. Quasi-coherent modules 10 11. Modules of finite presentation 13 12. Coherent modules 15 13. Closed immersions of ringed spaces 18 14. Locally free sheaves 20 15. Bilinear maps 21 16. Tensor product 22 17. Flat modules 24 18. Duals 26 19. Constructible sheaves of sets 27 20. Flat morphisms of ringed spaces 29 21. Symmetric and exterior powers 29 22. Internal Hom 31 23. Koszul complexes 33 24. Invertible modules 33 25. Rank and determinant 36 26. Localizing sheaves of rings 38 27. Modules of differentials 39 28. Finite order differential operators 43 29. The de Rham complex 46 30. The naive cotangent complex 47 31. Other chapters 50 References 52 1. Introduction 01AD This is a chapter of the Stacks Project, version 77243390, compiled on Sep 28, 2021. 1 SHEAVES OF MODULES 2 In this chapter we work out basic notions of sheaves of modules. This in particular includes the case of abelian sheaves, since these may be viewed as sheaves of Z- modules. Basic references are [Ser55], [DG67] and [AGV71]. We work out what happens for sheaves of modules on ringed topoi in another chap- ter (see Modules on Sites, Section 1), although there we will mostly just duplicate the discussion from this chapter. -
Equivariant De Rham Cohomology and Gauged Field Theories
Equivariant de Rham cohomology and gauged field theories August 15, 2013 Contents 1 Introduction 2 1.1 Differential forms and de Rham cohomology . .2 1.2 A commercial for supermanifolds . .3 1.3 Topological field theories . .5 2 Super vector spaces, super algebras and super Lie algebras 11 2.1 Super algebras . 12 2.2 Super Lie algebra . 14 3 A categorical Digression 15 3.1 Monoidal categories . 15 3.2 Symmetric monoidal categories . 17 4 Supermanifolds 19 4.1 Definition and examples of supermanifolds . 19 4.2 Super Lie groups and their Lie algebras . 23 4.3 Determining maps from a supermanifold to Rpjq ................ 26 5 Mapping supermanifolds and the functor of points formalism 31 5.1 Internal hom objects . 32 5.2 The functor of points formalism . 34 5.3 The supermanifold of endomorphisms of R0j1 .................. 36 5.4 Vector bundles on supermanifolds . 37 5.5 The supermanifold of maps R0j1 ! X ...................... 41 5.6 The algebra of functions on a generalized supermanifold . 43 1 1 INTRODUCTION 2 6 Gauged field theories and equivariant de Rham cohomology 47 6.1 Equivariant cohomology . 47 6.2 Differential forms on G-manifolds. 49 6.3 The Weil algebra . 53 6.4 A geometric interpretation of the Weil algebra . 57 1 Introduction 1.1 Differential forms and de Rham cohomology Let X be a smooth manifold of dimension n. We recall that Ωk(X) := C1(X; ΛkT ∗X) is the vector space of differential k-forms on X. What is the available structure on differential forms? 1. There is the wedge product Ωk(M) ⊗ Ω`(M) −!^ Ωk+`(X) induced by a vector bundle homomorphism ΛkT ∗X ⊗ Λ`T ∗X −! Λk+`T ∗X ∗ Ln k This gives Ω (X) := k=0 Ω (X) the structure of a Z-graded algebra. -
Compact Ringed Spaces
View metadata, citation and similar papers at core.ac.uk brought to you by CORE provided by Elsevier - Publisher Connector JOURNAL OF ALGEBRA 52, 41 l-436 (1978) Compact Ringed Spaces CHRISTOPHER J. MULVEY * Department of Mathematics, Columbia University, New York, New York 10027 and Mathematics Division, University of Sussex, Falmer, Brighton, BNl9QH, England Communicated by Saunders MacLane Received April 16, 1976 The properties of complete regularity, paracompactness, and compactness of a topological space X all may be described in terms of the ring R(X) of continuous real functions on X. In this paper we are concerned with extending these concepts from topological to ringed spaces, replacing the ring of continuous real functions on the space by the ring of sections of the ringed space. Our interest in the problem arose from attempting to construct the tangent module 7M of a smooth manifold IM directly from the sheaf QM of smooth real functions. For each open set U of M, the module rM( U)is the s2,( U)-module of derivations of In,(U). Yet, since taking derivations is not functorial, the evident restriction maps are not canonically forthcoming. For paracompact manifolds the construction needed was known to Boardman [5]. In general, it can be carried out using the complete regularity of the ringed space (M, 62,) [18, 321. Although spaces satisfying these conditions appear naturally in analytical contexts, there emerges a fundamental connection with sectional representations of rings [19, 21, 231. In turn, this has provided a technique for using intuitionistic mathematics in applying these representations [22]. Extending these properties to ringed spaces, we prove a compactness theorem for completely regular ringed spaces generalizing the Gelfand-Kolmogoroff criterion concerning maximal ideals in the ring R(X) of continuous real functions on a completely regular space X. -
Introduction to Algebraic Geometry
Introduction to Algebraic Geometry Jilong Tong December 6, 2012 2 Contents 1 Algebraic sets and morphisms 11 1.1 Affine algebraic sets . 11 1.1.1 Some definitions . 11 1.1.2 Hilbert's Nullstellensatz . 12 1.1.3 Zariski topology on an affine algebraic set . 14 1.1.4 Coordinate ring of an affine algebraic set . 16 1.2 Projective algebraic sets . 19 1.2.1 Definitions . 19 1.2.2 Homogeneous Nullstellensatz . 21 1.2.3 Homogeneous coordinate ring . 22 1.2.4 Exercise: plane curves . 22 1.3 Morphisms of algebraic sets . 24 1.3.1 Affine case . 24 1.3.2 Quasi-projective case . 26 2 The Language of schemes 29 2.1 Sheaves and locally ringed spaces . 29 2.1.1 Sheaves on a topological spaces . 29 2.1.2 Ringed space . 34 2.2 Schemes . 36 2.2.1 Definition of schemes . 36 2.2.2 Morphisms of schemes . 40 2.2.3 Projective schemes . 43 2.3 First properties of schemes and morphisms of schemes . 49 2.3.1 Topological properties . 49 2.3.2 Noetherian schemes . 50 2.3.3 Reduced and integral schemes . 51 2.3.4 Finiteness conditions . 53 2.4 Dimension . 54 2.4.1 Dimension of a topological space . 54 2.4.2 Dimension of schemes and rings . 55 2.4.3 The noetherian case . 57 2.4.4 Dimension of schemes over a field . 61 2.5 Fiber products and base change . 62 2.5.1 Sum of schemes . 62 2.5.2 Fiber products of schemes . -
4 Sheaves of Modules, Vector Bundles, and (Quasi-)Coherent Sheaves
4 Sheaves of modules, vector bundles, and (quasi-)coherent sheaves “If you believe a ring can be understood geometrically as functions its spec- trum, then modules help you by providing more functions with which to measure and characterize its spectrum.” – Andrew Critch, from MathOver- flow.net So far we discussed general properties of sheaves, in particular, of rings. Similar as in the module theory in abstract algebra, the notion of sheaves of modules allows us to increase our understanding of a given ringed space (or a scheme), and to provide further techniques to play with functions, or function-like objects. There are particularly important notions, namely, quasi-coherent and coherent sheaves. They are analogous notions of the usual modules (respectively, finitely generated modules) over a given ring. They also generalize the notion of vector bundles. Definition 38. Let (X, ) be a ringed space. A sheaf of -modules, or simply an OX OX -module, is a sheaf on X such that OX F (i) the group (U) is an (U)-module for each open set U X; F OX ✓ (ii) the restriction map (U) (V ) is compatible with the module structure via the F !F ring homomorphism (U) (V ). OX !OX A morphism of -modules is a morphism of sheaves such that the map (U) F!G OX F ! (U) is an (U)-module homomorphism for every open U X. G OX ✓ Example 39. Let (X, ) be a ringed space, , be -modules, and let ' : OX F G OX F!G be a morphism. Then ker ', im ', coker ' are again -modules. If is an - OX F 0 ✓F OX submodule, then the quotient sheaf / is an -module. -
Topics in Algebraic Supergeometry Over Projective Spaces
Dipartimento di Matematica \Federigo Enriques" Dottorato di Ricerca in Matematica XXX ciclo Topics in Algebraic Supergeometry over Projective Spaces MAT/03 Candidato: Simone Noja Relatore: Prof. Bert van Geemen Correlatore: Prof. Sergio Luigi Cacciatori Coordinatore di Dottorato: Prof. Vieri Mastropietro A.A. 2016/2017 Contents Introduction 4 1 Algebraic Supergeometry 8 1.1 Main Definitions and Fundamental Constructions . .8 1.2 Locally-Free Sheaves on a Supermanifold and Even Picard Group . 14 1.3 Tangent and Cotangent Sheaf of a Supermanifold . 16 1.4 Berezinian Sheaf, First Chern Class and Calabi-Yau Condition . 21 2 Supergeometry of Projective Superspaces 24 2.1 Cohomology of O n|m ` ................................. 24 P p q n|m 2.2 Invertible Sheaves and Even Picard Group Pic0pP q ................ 26 2.3 Maps and Embeddings into Projective Superspaces . 31 2.4 Infinitesimal Automorphisms and First Order Deformations . 32 2.4.1 Supercurves over P1 and the Calabi-Yau Supermanifold P1|2 ......... 35 2.5 P1|2 as N “ 2 Super Riemann Surface . 37 2.6 Aganagic-Vafa's Mirror Supermanifold for P1|2 .................... 41 3 N “ 2 Non-Projected Supermanifolds over Pn 45 3.1 Obstruction to the Splitting of a N “ 2 Supermanifold . 45 3.2 N “ 2 Non-Projected Supermanifolds over Projective Spaces . 49 3.3 Non-Projected Supermanifolds over P1 ......................... 50 1 3.3.1 Even Picard Group of P!pm; nq ......................... 52 1 3.3.2 Embedding of P!p2; 2q: an Example by Witten . 54 3.4 Non-Projected Supermanifolds over P2 ......................... 56 2 3.4.1 P!pFM q is a Calabi-Yau Supermanifold . -
Superfield Equations in the Berezin-Kostant-Leites Category
Superfield equations in the Berezin-Kostant-Leites category Michel Egeileh∗ and Daniel Bennequin† ∗Conservatoire national des arts et m´etiers (ISSAE Cnam Liban) P.O. Box 113 6175 Hamra, 1103 2100 Beirut, Lebanon E-mail: [email protected] †Institut de Math´ematiques de Jussieu-Paris Rive Gauche, Bˆatiment Sophie Germain, 8 place Aur´elie Nemours, 75013 Paris, France E-mail: [email protected] Abstract Using the functor of points, we prove that the Wess-Zumino equations for massive chiral superfields in dimension 4|4 can be represented by supersymmetric equations in terms of superfunctions in the Berezin-Kostant-Leites sense (involving ordinary fields, with real and complex valued components). Then, after introducing an appropriate supersymmetric extension of the Fourier transform, we prove explicitly that these su- persymmetric equations provide a realization of the irreducible unitary representations with positive mass and zero superspin of the super Poincar´egroup in dimension 4|4. 1 Introduction From the point of view of quantum field theory, 1-particle states of a free elementary par- ticle constitute a Hilbert space which, by the requirement of relativistic invariance, must carry an irreducible unitary representation of the Poincar´egroup V ⋊ Spin(V ), where V is a Lorentzian vector space. In signature (1, 3), it is well-known since [Wig] that the irreducible representations of the Poincar´egroup that are of physical interest are classified 1 3 by a nonnegative real number m (the mass), and a half-integer s ∈ {0, 2 , 1, 2 , ...} (the spin)1. It is also known, cf. [BK], that all the irreducible unitary representations of the Poincar´e group of positive (resp. -
Quotient Supermanifolds
BULL. AUSTRAL. MATH. SOC. 58A50 VOL. 58 (1998) [107-120] QUOTIENT SUPERMANIFOLDS CLAUDIO BARTOCCI, UGO BRUZZO, DANIEL HERNANDEZ RUIPEREZ AND VLADIMIR PESTOV A necessary and sufficient condition for the existence of a supermanifold structure on a quotient defined by an equivalence relation is established. Furthermore, we show that an equivalence relation it on a Berezin-Leites-Kostant supermanifold X determines a quotient supermanifold X/R if and only if the restriction Ro of R to the underlying smooth manifold Xo of X determines a quotient smooth manifold XQ/RQ- 1. INTRODUCTION The necessity of taking quotients of supermanifolds arises in a great variety of cases; just to mention a few examples, we recall the notion of supergrassmannian, the definition of the Teichmiiller space of super Riemann surfaces, or the procedure of super Poisson reduction. These constructions play a crucial role in superstring theory as well as in supersymmetric field theories. The first aim of this paper is to prove a necessary and sufficient condition ensuring that an equivalence relation in the category of supermanifolds gives rise to a quotient supermanifold; analogous results, in the setting of Berezin-Leites-Kostant (BLK) super- manifolds, were already stated in [6]. Secondly and rather surprisingly at that, it turns out that for Berezin-Leites-Kostant supermanifolds any obstacles to the existence of a quotient supermanifold can exist only in the even sector and are therefore purely topological. We demonstrate that an equivalence relation Ron a. BLK supermanifold X determines a quotient BLK supermanifold X/R if and only if the restriction of R to the underlying manifold Xo of X determines a quotient smooth manifold. -
Torsion Constraints in Supergeometry
Commun. Math. Phys. 133, 563-615(1990) Communications ΪΠ Mathematical Physics ©Springer-Verlagl990 Torsion Constraints in Supergeometry John Lott* I.H.E.S., F-91440 Bures-sur-Yvette, France Received November 9, 1989; in revised form April 2, 1990 Abstract. We derive the torsion constraints for superspace versions of supergravity theories by means of the theory of G-stmctures. We also discuss superconformal geometry and superKahler geometry. I. Introduction Supersymmetry is a now well established topic in quantum field theory [WB, GGRS]. The basic idea is that one can construct actions in ordinary spacetime which involve both even commuting fields and odd anticommuting fields, with a symmetry which mixes the two types of fields. These actions can then be interpreted as arising from actions in a superspace with both even and odd coordinates, upon doing a partial integration over the odd coordinates. A mathematical framework to handle the differential topology of supermanifolds, manifolds with even and odd coordinates, was developed by Berezin, Kostant and others. A very readable account of this theory is given in the book of Manin [Ma]. The right notion of differential geometry for supermanifolds is less clear. Such a geometry is necessary in order to write supergravity theories in superspace. One could construct a supergeometry by ΊL2 grading what one usually does in (pseudo) Riemannian geometry, to have supermetrics, super Levi-Civita connections, etc. The local frame group which would take the place of the orthogonal group in standard geometry would be the orthosymplectic group. However, it turns out that this would be physically undesirable. Such a program would give more fields than one needs for a minimal supergravity theory, i.e. -
2. the Concept of a Supermanifold
2. THE CONCEPT OF A SUPERMANIFOLD 2.1. Geometry of physical space. 2.2. The mathematical evolution of the concept of space as a geometrical ob- ject. 2.3. Geometry and algebra. 2.4. Supermanifolds and their supersymmetries. 2.1. Geometry of physical space. Someone who is already familiar with the theory of differentiable manifolds or algebraic varieties can be very quickly intro- duced to the notion of a supermanifold and the concept of supersymmetry. Just as the manifolds and varieties are defined by first starting with local pieces on which the coordinate functions are defined, and then gluing these local pieces together, a supermanifold may be defined as a space on which locally one has coordinates x1; : : : ; xn; θ1; : : : θr where the xi are the usual commuting coordinates and the θj, the anticommuting (fermionic) coordinates, with the various sets of local chats be- ing related by transformations of the appropriate smoothness type. Everything is then done exactly as in the classical theory. Supersymmetries are diffeomorphisms of such spaces and these form super Lie groups. One can construct a theory of differentiation and integration on such spaces and write down equations of motions of particles and fields starting from suitable Lagrangians. If one starts with a super- symmetric Lagrangian then one obtains an action of the supersymmetric group on the solutions of the field equations thus defined. The stage on which supersymmetic quantum field theory lives is then a super spacetime, either flat or curved. How- ever, such a treatment, in spite of being very practical and having the advantage of getting into the heart of matters very quickly, does not do full justice either to the understanding of the concepts at a deeper level or to comprehending the boldness of the generalization of conventional geometry that is involved here.