Foundations of Supermanifold Theory: the Axiomatic Approach*
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Arxiv:0704.2891V3 [Math.AG] 5 Dec 2007 Schwartz Functions on Nash Manifolds
Schwartz functions on Nash manifolds Avraham Aizenbud and Dmitry Gourevitch ∗ July 11, 2011 Abstract In this paper we extend the notions of Schwartz functions, tempered func- tions and generalized Schwartz functions to Nash (i.e. smooth semi-algebraic) manifolds. We reprove for this case classically known properties of Schwartz functions on Rn and build some additional tools which are important in rep- resentation theory. Contents 1 Introduction 2 1.1 Mainresults................................ 3 1.2 Schwartz sections of Nash bundles . 4 1.3 Restricted topologyand sheaf properties . .... 4 1.4 Possibleapplications ........................... 5 1.5 Summary ................................. 6 1.6 Remarks.................................. 6 2 Semi-algebraic geometry 8 2.1 Basicnotions ............................... 8 arXiv:0704.2891v3 [math.AG] 5 Dec 2007 2.2 Tarski-Seidenberg principle of quantifier elimination anditsapplications............................ 8 2.3 Additional preliminary results . .. 10 ∗Avraham Aizenbud and Dmitry Gourevitch, Faculty of Mathematics and Computer Science, The Weizmann Institute of Science POB 26, Rehovot 76100, ISRAEL. E-mails: [email protected], [email protected]. Keywords: Schwartz functions, tempered functions, generalized functions, distributions, Nash man- ifolds. 1 3 Nash manifolds 11 3.1 Nash submanifolds of Rn ......................... 11 3.2 Restricted topological spaces and sheaf theory over them........ 12 3.3 AbstractNashmanifolds . 14 3.3.1 ExamplesandRemarks. 14 3.4 Nashvectorbundles ........................... 15 3.5 Nashdifferentialoperators . 16 3.5.1 Algebraic differential operators on a Nash manifold . .... 17 3.6 Nashtubularneighborhood . 18 4 Schwartz and tempered functions on affine Nash manifolds 19 4.1 Schwartzfunctions ............................ 19 4.2 Temperedfunctions. .. .. .. 20 4.3 Extension by zero of Schwartz functions . .. 20 4.4 Partitionofunity ............................. 21 4.5 Restriction and sheaf property of tempered functions . -
From Topological Field Theory to Deformation Quantization and Reduction
Cattaneo, Alberto (2006). From topological field theory to deformation quantization and reduction. In: International Congress of Mathematicians. Vol. III. 339-365. Postprint available at: http://www.zora.uzh.ch University of Zurich Posted at the Zurich Open Repository and Archive, University of Zurich. Zurich Open Repository and Archive http://www.zora.uzh.ch Originally published at: 2006. International Congress of Mathematicians. Vol. III. 339-365. Winterthurerstr. 190 CH-8057 Zurich http://www.zora.uzh.ch Year: 2006 From topological field theory to deformation quantization and reduction Cattaneo, Alberto Cattaneo, Alberto (2006). From topological field theory to deformation quantization and reduction. In: International Congress of Mathematicians. Vol. III. 339-365. Postprint available at: http://www.zora.uzh.ch Posted at the Zurich Open Repository and Archive, University of Zurich. http://www.zora.uzh.ch Originally published at: 2006. International Congress of Mathematicians. Vol. III. 339-365. From topological field theory to deformation quantization and reduction Alberto S. Cattaneo∗ Abstract. This note describes the functional-integral quantization of two-dimensional topolog- ical field theories together with applications to problems in deformation quantization of Poisson manifolds and reduction of certain submanifolds. A brief introduction to smooth graded mani- folds and to the Batalin–Vilkovisky formalism is included. Mathematics Subject Classification (2000). Primary 81T45; Secondary 51P05, 53D55, 58A50, 81T70. Keywords. Topological quantum field theory, BV formalism, graded manifolds, deformation quantization, formality, Poisson reduction, L∞- and A∞-algebras. 1. Introduction: a 2D TFT 0 1.1. The basic setting. Let be a smooth compact 2-manifold. On M1 := ()⊕ 1() one may define the following very simple action functional: S(ξ,η) := η dξ, ξ ∈ 0(), η ∈ 1(), (1.1) which is invariant under the distribution 0 ⊕ dβ, β ∈ 0(). -
Introduction to Graded Geometry, Batalin-Vilkovisky Formalism and Their Applications
ARCHIVUM MATHEMATICUM (BRNO) Tomus 47 (2011), 415–471 INTRODUCTION TO GRADED GEOMETRY, BATALIN-VILKOVISKY FORMALISM AND THEIR APPLICATIONS Jian Qiu and Maxim Zabzine Abstract. These notes are intended to provide a self-contained introduction to the basic ideas of finite dimensional Batalin-Vilkovisky (BV) formalism and its applications. A brief exposition of super- and graded geometries is also given. The BV–formalism is introduced through an odd Fourier transform and the algebraic aspects of integration theory are stressed. As a main application we consider the perturbation theory for certain finite dimensional integrals within BV-formalism. As an illustration we present a proof of the isomorphism between the graph complex and the Chevalley-Eilenberg complex of formal Hamiltonian vectors fields. We briefly discuss how these ideas can be extended to the infinite dimensional setting. These notes should be accessible toboth physicists and mathematicians. Table of Contents 1. Introduction and motivation 416 2. Supergeometry 417 2.1. Idea 418 2.2. Z2-graded linear algebra 418 2.3. Supermanifolds 420 2.4. Integration theory 421 3. Graded geometry 423 3.1. Z-graded linear algebra 423 3.2. Graded manifold 425 4. Odd Fourier transform and BV-formalism 426 4.1. Standard Fourier transform 426 4.2. Odd Fourier transform 427 4.3. Integration theory 430 4.4. Algebraic view on the integration 433 5. Perturbation theory 437 5.1. Integrals in Rn-Gaussian Integrals and Feynman Diagrams 437 2010 Mathematics Subject Classification: primary 58A50; secondary 16E45, 97K30. Key words and phrases: Batalin-Vilkovisky formalism, graded symplectic geometry, graph homology, perturbation theory. -
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. -
University of Alberta
University of Alberta Extensions of Skorohod’s almost sure representation theorem by Nancy Hernandez Ceron A thesis submitted to the Faculty of Graduate Studies and Research in partial fulfillment of the requirements for the degree of Master of Science in Mathematics Department of Mathematical and Statistical Sciences ©Nancy Hernandez Ceron Fall 2010 Edmonton, Alberta Permission is hereby granted to the University of Alberta Libraries to reproduce single copies of this thesis and to lend or sell such copies for private, scholarly or scientific research purposes only. Where the thesis is converted to, or otherwise made available in digital form, the University of Alberta will advise potential users of the thesis of these terms. The author reserves all other publication and other rights in association with the copyright in the thesis and, except as herein before provided, neither the thesis nor any substantial portion thereof may be printed or otherwise reproduced in any material form whatsoever without the author's prior written permission. Library and Archives Bibliothèque et Canada Archives Canada Published Heritage Direction du Branch Patrimoine de l’édition 395 Wellington Street 395, rue Wellington Ottawa ON K1A 0N4 Ottawa ON K1A 0N4 Canada Canada Your file Votre référence ISBN:978-0-494-62500-2 Our file Notre référence ISBN: 978-0-494-62500-2 NOTICE: AVIS: The author has granted a non- L’auteur a accordé une licence non exclusive exclusive license allowing Library and permettant à la Bibliothèque et Archives Archives Canada to reproduce, Canada de reproduire, publier, archiver, publish, archive, preserve, conserve, sauvegarder, conserver, transmettre au public communicate to the public by par télécommunication ou par l’Internet, prêter, telecommunication or on the Internet, distribuer et vendre des thèses partout dans le loan, distribute and sell theses monde, à des fins commerciales ou autres, sur worldwide, for commercial or non- support microforme, papier, électronique et/ou commercial purposes, in microform, autres formats. -
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. -
A Radial Basis Function Partition of Unity Method for Transport on the Sphere
A RADIAL BASIS FUNCTION PARTITION OF UNITY METHOD FOR TRANSPORT ON THE SPHERE by Kevin Aiton A thesis submitted in partial fulfillment of the requirements for the degree of Master of Science in Mathematics Boise State University May 2014 c 2014 Kevin Aiton ALL RIGHTS RESERVED BOISE STATE UNIVERSITY GRADUATE COLLEGE DEFENSE COMMITTEE AND FINAL READING APPROVALS of the thesis submitted by Kevin Aiton Thesis Title: A Radial Basis Function Partition of Unity Method for Transport on the Sphere Date of Final Oral Examination: 06 December 2013 The following individuals read and discussed the thesis submitted by student Kevin Aiton, and they evaluated his presentation and response to questions during the final oral examination. They found that the student passed the final oral examination. Grady Wright, Ph.D. Chair, Supervisory Committee Donna Calhoun, Ph.D. Member, Supervisory Committee Inanc Senocak, Ph.D. Member, Supervisory Committee The final reading approval of the thesis was granted by Grady Wright, Ph.D., Chair of the Supervisory Committee. The thesis was approved for the Graduate College by John R. Pelton, Ph.D., Dean of the Graduate College. ACKNOWLEDGMENTS This work was supported, in part, by the National Science Foundation (NSF) under grant DMS-0934581 and also by the Boise State Mathematics Department under the 2013 summer graduate fellowship. I would like to express gratitude to Professor Grady Wright. He has been both kind and patient. I would also like to thank the MOOSE development team at Idaho National Laboratory for letting me work remotely so I could work on my thesis. Finally, I would like to give gratitude to my family. -
Chapter 9 Partitions of Unity, Covering Maps ~
Chapter 9 Partitions of Unity, Covering Maps ~ 9.1 Partitions of Unity To study manifolds, it is often necessary to construct var- ious objects such as functions, vector fields, Riemannian metrics, volume forms, etc., by gluing together items con- structed on the domains of charts. Partitions of unity are a crucial technical tool in this glu- ing process. 505 506 CHAPTER 9. PARTITIONS OF UNITY, COVERING MAPS ~ The first step is to define “bump functions”(alsocalled plateau functions). For any r>0, we denote by B(r) the open ball n 2 2 B(r)= (x1,...,xn) R x + + x <r , { 2 | 1 ··· n } n 2 2 and by B(r)= (x1,...,xn) R x1 + + xn r , its closure. { 2 | ··· } Given a topological space, X,foranyfunction, f : X R,thesupport of f,denotedsuppf,isthe closed set! supp f = x X f(x) =0 . { 2 | 6 } 9.1. PARTITIONS OF UNITY 507 Proposition 9.1. There is a smooth function, b: Rn R, so that ! 1 if x B(1) b(x)= 2 0 if x Rn B(2). ⇢ 2 − See Figures 9.1 and 9.2. 1 0.8 0.6 0.4 0.2 K3 K2 K1 0 1 2 3 Figure 9.1: The graph of b: R R used in Proposition 9.1. ! 508 CHAPTER 9. PARTITIONS OF UNITY, COVERING MAPS ~ > Figure 9.2: The graph of b: R2 R used in Proposition 9.1. ! Proposition 9.1 yields the following useful technical result: 9.1. PARTITIONS OF UNITY 509 Proposition 9.2. Let M be a smooth manifold. -
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. -
Graded-And-Microformal-Prop
The University of Manchester Research Graded Geometry, Q-Manifolds, and Microformal Geometry DOI: 10.1002/prop.201910023 Document Version Accepted author manuscript Link to publication record in Manchester Research Explorer Citation for published version (APA): Voronov, T. (2019). Graded Geometry, Q-Manifolds, and Microformal Geometry: LMS/EPSRC Durham Symposium on Higher Structures in M-Theory. Fortschritte der Physik. https://doi.org/10.1002/prop.201910023 Published in: Fortschritte der Physik Citing this paper Please note that where the full-text provided on Manchester Research Explorer is the Author Accepted Manuscript or Proof version this may differ from the final Published version. If citing, it is advised that you check and use the publisher's definitive version. General rights Copyright and moral rights for the publications made accessible in the Research Explorer are retained by the authors and/or other copyright owners and it is a condition of accessing publications that users recognise and abide by the legal requirements associated with these rights. Takedown policy If you believe that this document breaches copyright please refer to the University of Manchester’s Takedown Procedures [http://man.ac.uk/04Y6Bo] or contact [email protected] providing relevant details, so we can investigate your claim. Download date:06. Oct. 2021 Graded geometry, Q-manifolds, and microformal geometry 1,2 Theodore Th. Voronov ¤ below), to which we give a brief introduction as well. We give an exposition of graded and microformal ge- “Thick morphisms” (defined for ordinary manifolds, ometry, and the language of Q-manifolds. Q-manifolds supermanifolds or graded manifolds) generalize ordinary are supermanifolds endowed with an odd vector field of maps or supermanifold morphisms, but are not maps square zero.