Sheaf Theory and Paschke Duality
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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 . -
3D Holography: from Discretum to Continuum
3D Holography: from discretum to continuum Bianca Dittrich (Perimeter Institute) V. Bonzom, B. Dittrich, to appear V. Bonzom, B.Dittrich, S. Mizera, A. Riello, w.i.p. ILQGS Sep 2015 1 Overview 1.Is quantum gravity fundamentally holographic? 2.Continuum: dualities for 3D gravity. 3.Regge calculus. 4.Computing the 3D partition function in Regge calculus. One loop correction. Boundary fluctuations. 2 1 1 S = d3xpgR d2xphK −16⇡G − 8⇡G Z Z@ 1 M β M = Ar(torus) r=1 = no ↵ dependence (0.217) sol −8⇡G | −4G 1 1 S = d3xpgR d2xphK −16⇡G − 8⇡G dt Z Z@ ln det(∆ m2)= 1 d3xK(t,1 x, x)M β(0.218)M − − 0 t = Ar(torus) r=1 = no ↵ dependence (0.217) Z Z sol −8⇡G | −4G 1 K = r dt Is quantum gravity fundamentallyln det(∆ m2)= holographic?1 d3xK(t, x, x) (0.218) i↵ − − t q = e Z0 (0.219)Z • In the last years spin1 foams have made heavily use of the K = r Generalized Boundary Formulation [Oeckl 00’s +, Rovelli, et al …] Region( bdry) i↵ (0.220) • Encodes dynamicsA into amplitudes associated to (generalized)q = e space time regions. (0.219) (0.221) bdry ( ) (0.220) ARegion bdry boundary -should satisfy (the dualized) Wheeler de Witt equation Hilbert space -gives no boundary (Hartle-Hawking) wave function • This looks ‘holographic’. However in the standard formulation one has the gluing axiom: ‘Gluing axiom’: essential to get more complicated from simpler amplitudes Amplitude for bigger region = glued from amplitudes for smaller regions This could be / is also called ‘locality axiom’. -
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. -
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. -
Notes on Categorical Logic
Notes on Categorical Logic Anand Pillay & Friends Spring 2017 These notes are based on a course given by Anand Pillay in the Spring of 2017 at the University of Notre Dame. The notes were transcribed by Greg Cousins, Tim Campion, L´eoJimenez, Jinhe Ye (Vincent), Kyle Gannon, Rachael Alvir, Rose Weisshaar, Paul McEldowney, Mike Haskel, ADD YOUR NAMES HERE. 1 Contents Introduction . .3 I A Brief Survey of Contemporary Model Theory 4 I.1 Some History . .4 I.2 Model Theory Basics . .4 I.3 Morleyization and the T eq Construction . .8 II Introduction to Category Theory and Toposes 9 II.1 Categories, functors, and natural transformations . .9 II.2 Yoneda's Lemma . 14 II.3 Equivalence of categories . 17 II.4 Product, Pullbacks, Equalizers . 20 IIIMore Advanced Category Theoy and Toposes 29 III.1 Subobject classifiers . 29 III.2 Elementary topos and Heyting algebra . 31 III.3 More on limits . 33 III.4 Elementary Topos . 36 III.5 Grothendieck Topologies and Sheaves . 40 IV Categorical Logic 46 IV.1 Categorical Semantics . 46 IV.2 Geometric Theories . 48 2 Introduction The purpose of this course was to explore connections between contemporary model theory and category theory. By model theory we will mostly mean first order, finitary model theory. Categorical model theory (or, more generally, categorical logic) is a general category-theoretic approach to logic that includes infinitary, intuitionistic, and even multi-valued logics. Say More Later. 3 Chapter I A Brief Survey of Contemporary Model Theory I.1 Some History Up until to the seventies and early eighties, model theory was a very broad subject, including topics such as infinitary logics, generalized quantifiers, and probability logics (which are actually back in fashion today in the form of con- tinuous model theory), and had a very set-theoretic flavour. -
Arxiv:2012.08669V1 [Math.CT] 15 Dec 2020 2 Preface
Sheaf Theory Through Examples (Abridged Version) Daniel Rosiak December 12, 2020 arXiv:2012.08669v1 [math.CT] 15 Dec 2020 2 Preface After circulating an earlier version of this work among colleagues back in 2018, with the initial aim of providing a gentle and example-heavy introduction to sheaves aimed at a less specialized audience than is typical, I was encouraged by the feedback of readers, many of whom found the manuscript (or portions thereof) helpful; this encouragement led me to continue to make various additions and modifications over the years. The project is now under contract with the MIT Press, which would publish it as an open access book in 2021 or early 2022. In the meantime, a number of readers have encouraged me to make available at least a portion of the book through arXiv. The present version represents a little more than two-thirds of what the professionally edited and published book would contain: the fifth chapter and a concluding chapter are missing from this version. The fifth chapter is dedicated to toposes, a number of more involved applications of sheaves (including to the \n- queens problem" in chess, Schreier graphs for self-similar groups, cellular automata, and more), and discussion of constructions and examples from cohesive toposes. Feedback or comments on the present work can be directed to the author's personal email, and would of course be appreciated. 3 4 Contents Introduction 7 0.1 An Invitation . .7 0.2 A First Pass at the Idea of a Sheaf . 11 0.3 Outline of Contents . 20 1 Categorical Fundamentals for Sheaves 23 1.1 Categorical Preliminaries . -
Topological Quantum Field Theory with Corners Based on the Kauffman Bracket
TOPOLOGICAL QUANTUM FIELD THEORY WITH CORNERS BASED ON THE KAUFFMAN BRACKET R˘azvan Gelca Abstract We describe the construction of a topological quantum field theory with corners based on the Kauffman bracket, that underlies the smooth theory of Lickorish, Blanchet, Habegger, Masbaum and Vogel. We also exhibit some properties of invariants of 3-manifolds with boundary. 1. INTRODUCTION The discovery of the Jones polynomial [J] and its placement in the context of quantum field theory done by Witten [Wi] led to various constructions of topological quantum field theories (shortly TQFT's). A first example of a rigorous theory which fits Witten's framework has been produced by Reshetikhin and Turaev in [RT], and makes use of the representation theory of quantum deformations of sl(2; C) at roots of unity (see also [KM]). Then, an alternative construction based on geometric techniques has been worked out by Kohno in [Ko]. A combinatorial approach based on skein spaces associated to the Kauffman bracket [K1] has been exhibited by Lickorish in [L1] and [L2] and by Blanchet, Habegger, Masbaum, and Vogel in [BHMV1]. All these theories are smooth, in the sense that they define invariants satisfying the Atiyah-Segal set of axioms [A], thus there is a rule telling how the invariants behave under gluing of 3-manifolds along closed surfaces. In an attempt to give a more axiomatic approach to such a theory, K. Walker described in [Wa] a system of axioms for a TQFT in which one allows gluings along surfaces with boundary, a so called TQFT with corners. This system of axioms includes the Atiyah-Segal axioms, but works for a more restrictive class of TQFT's. -
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. -
On Different Geometric Formulations of Lagrangian Formalism
Published in Differential Geom. Appl., 10 n. 3 (1999), 225–255 Version with some corrections/improvements On different geometric formulations of Lagrangian formalism Raffaele Vitolo1 Dept. of Mathematics “E. De Giorgi”, Universit`adi Lecce, via per Arnesano, 73100 Italy email: [email protected] Abstract We consider two geometric formulations of Lagrangian formalism on fibred manifolds: Krupka’s theory of finite order variational sequences, and Vinogradov’s infinite order variational sequence associated with the C–spectral sequence. On one hand, we show that the direct limit of Krupka’s variational bicomplex is a new infinite order variational bicomplex which yields a new infinite order variational sequence. On the other hand, by means of Vinogradov’s C–spectral sequence, we provide a new finite order variational sequence whose direct limit turns out to be the Vinogradov’s infinite order variational sequence. Finally, we provide an equivalence of the two finite order and infinite order variational sequences up to the space of Euler–Lagrange morphisms. Key words: Fibred manifold, jet space, infinite order jet space, variational bicomplex, variational sequence, spectral sequence. 1991 MSC: 58A12, 58A20, 58E30, 58G05. 1 This paper has been partially supported by Fondazione F. Severi, INdAM ‘F. Severi’ through a senior research fellowship, GNFM of CNR, MURST, University of Florence. 1 2 On formulations of Lagrangian formalism Introduction The theory of variational bicomplexes can be regarded as the natural geometrical set- ting for the calculus of variations [1, 2, 10, 11, 15, 19, 20, 21, 22, 23, 24]. The geometric objects which appear in the calculus of variations find a place on the vertices of a varia- tional bicomplex, and are related by the morphisms of the bicomplex. -
On Phi-Families
ON PHI-FAMILIES CHARLES E. WATTS 1. Introduction. The purpose of this note is to show that the notion of sections with support in a phi-family in the Cartan version of the Leray theory of sheaves can be avoided by the following expedient. One uses the phi-family to construct a new space in the manner of a one-point compactification. Then a sheaf on the original space is shown to yield a new sheaf on the new space whose cohomology (with unrestricted supports) is that of the original sheaf with restricted supports. A partial generalization to the Grothendieck cohomology theory is given. 2. Phi-families. A family 5 of subsets of a topological space X is a family of supports [l ] provided: (I) each member of 5 is closed; (II) if FE$, then each closed subset of F is E$; (III) if Fi, F2E5, then Fi\JF2E5- Given a family of supports 5, we choose an object co (^X, and define X' = \}$, X*=X'VJ{ oo }. We then topologize X* by saying that a subset U oi X* is open iff either U is open in X' or else X*— UE%- It is readily verified that these open sets in fact form a topology for X* and that the inclusion X'EX* is a topological imbedding. The family of supports JF is a phi-family [3] provided also: (IV) each member of fJ has a closed neighborhood in J; (V) each member of J is paracompact. Proposition 1. If ff is a phi-family, then X* is paracompact. -
Sheaf Theory 1 Introduction and Definitions
Sheaf Theory Tom Lovering September 24, 2010 Abstract In this essay we develop the basic idea of a sheaf, look at some simple examples and explore areas of mathematics which become more transpar- ent and easier to think about in light of this new concept. Though we attempt to avoid being too dependent on category theory and homological algebra, a reliance on the basic language of the subject is inevitable when we start discussing sheaf cohomology (but by omitting proofs when they become too technical we hope it is still accessible). 1 Introduction and Denitions Mathematics is a curious activity. Most of us probably see it as some giant blob of knowledge and understanding, much of which is not yet understood and maybe never will be. When we study mathematics we focus on a certain `area' together with some collection of associated theorems, ideas and examples. In the course of our study it often becomes necessary to restrict our study to how these ideas apply in a more specialised area. Sometimes they might apply in an interesting way, sometimes in a trivial way, but they will always apply in some way. While doing mathematics, we might notice that two ideas which seemed disparate on a general scale exhibit very similar behaviour when applied to more specic examples, and eventually be led to deduce that their overarching essence is in fact the same. Alternatively, we might identify similar ideas in several dierent areas, and after some work nd that we can indeed `glue them together' to get a more general theory that encompasses them all. -
Uniformly Continuous Partitions of Unity on a Metric Space
Canad. Math. Bull. Vol. 26 (1), 1983 UNIFORMLY CONTINUOUS PARTITIONS OF UNITY ON A METRIC SPACE BY STEWART M. ROBINSON AND ZACHARY ROBINSON ABSTRACT. In this paper, we construct, for any open cover of a metric space, a partition of unity consisting of a family of uniformly continuous functions. It is a well-known characterization of paracompact spaces that every open covering admits a partition of unity subordinate to it. In a series of lectures on "Non-Linear Analysis on Banach Spaces" given at both Dalhousie University and Cleveland State University, K. Sundaresan posed the following question: If (X, d) is a metric space, may one select this partition of unity to consist of uniformly continuous functions? In this note we provide an affirmative answer to this question. THEOREM. Let X be a paracompact space in which each open set is the support of a Lipschitz continuous function. Then there is a Lipschitz continuous partition of unity subordinate to any open cover of X. Proof. Let X be a space which satisfies the hypotheses and let °U be an open cover of X. Since X is paracompact, °U admits an open refinement that is both o--discrete and locally finite; denote this refinement by Unez+ °ttn> where each %n is a discrete family of open sets. Let Sn = UAG^^- We may select a gn : X —» [0,1] to be a Lipschitz continuous function with support Sn. For / e Z+, define k, : [0,1]-> [0,1] by fc(jc)f/-x if x e [0,1//] J 11 otherwise, and define gnj : X —» [0, 1] by g„,y(x) = ^.(gn(x)).