Diffeologies, Differential Spaces, and Symplectic Geometry By
Total Page:16
File Type:pdf, Size:1020Kb
Load more
Recommended publications
-
Algebraic Equations for Nonsmoothable 8-Manifolds
PUBLICATIONS MATHÉMATIQUES DE L’I.H.É.S. NICHOLAAS H. KUIPER Algebraic equations for nonsmoothable 8-manifolds Publications mathématiques de l’I.H.É.S., tome 33 (1967), p. 139-155 <http://www.numdam.org/item?id=PMIHES_1967__33__139_0> © Publications mathématiques de l’I.H.É.S., 1967, tous droits réservés. L’accès aux archives de la revue « Publications mathématiques de l’I.H.É.S. » (http:// www.ihes.fr/IHES/Publications/Publications.html) implique l’accord avec les conditions géné- rales d’utilisation (http://www.numdam.org/conditions). Toute utilisation commerciale ou im- pression 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/ ALGEBRAIC EQUATIONS FOR NONSMOOTHABLE 8-MANIFOLDS by NICOLAAS H. KUIPER (1) SUMMARY The singularities of Brieskorn and Hirzebruch are used in order to obtain examples of algebraic varieties of complex dimension four in P^C), which are homeo- morphic to closed combinatorial 8-manifolds, but not homeomorphic to any differentiable manifold. Analogous nonorientable real algebraic varieties of dimension 8 in P^R) are also given. The main theorem states that every closed combinatorial 8-manifbld is homeomorphic to a Nash-component with at most one singularity of some real algebraic variety. This generalizes the theorem of Nash for differentiable manifolds. § i. Introduction. The theorem of Wall. From the smoothing theory of Thorn [i], Munkres [2] and others and the knowledge of the groups of differential structures on spheres due to Kervaire, Milnor [3], Smale and Gerf [4] follows a.o. -
An Introduction to Differentiable Manifolds
Mathematics Letters 2016; 2(5): 32-35 http://www.sciencepublishinggroup.com/j/ml doi: 10.11648/j.ml.20160205.11 Conference Paper An Introduction to Differentiable Manifolds Kande Dickson Kinyua Department of Mathematics, Moi University, Eldoret, Kenya Email address: [email protected] To cite this article: Kande Dickson Kinyua. An Introduction to Differentiable Manifolds. Mathematics Letters. Vol. 2, No. 5, 2016, pp. 32-35. doi: 10.11648/j.ml.20160205.11 Received : September 7, 2016; Accepted : November 1, 2016; Published : November 23, 2016 Abstract: A manifold is a Hausdorff topological space with some neighborhood of a point that looks like an open set in a Euclidean space. The concept of Euclidean space to a topological space is extended via suitable choice of coordinates. Manifolds are important objects in mathematics, physics and control theory, because they allow more complicated structures to be expressed and understood in terms of the well–understood properties of simpler Euclidean spaces. A differentiable manifold is defined either as a set of points with neighborhoods homeomorphic with Euclidean space, Rn with coordinates in overlapping neighborhoods being related by a differentiable transformation or as a subset of R, defined near each point by expressing some of the coordinates in terms of the others by differentiable functions. This paper aims at making a step by step introduction to differential manifolds. Keywords: Submanifold, Differentiable Manifold, Morphism, Topological Space manifolds with the additional condition that the transition 1. Introduction maps are analytic. In other words, a differentiable (or, smooth) The concept of manifolds is central to many parts of manifold is a topological manifold with a globally defined geometry and modern mathematical physics because it differentiable (or, smooth) structure, [1], [3], [4]. -
Graphs and Patterns in Mathematics and Theoretical Physics, Volume 73
http://dx.doi.org/10.1090/pspum/073 Graphs and Patterns in Mathematics and Theoretical Physics This page intentionally left blank Proceedings of Symposia in PURE MATHEMATICS Volume 73 Graphs and Patterns in Mathematics and Theoretical Physics Proceedings of the Conference on Graphs and Patterns in Mathematics and Theoretical Physics Dedicated to Dennis Sullivan's 60th birthday June 14-21, 2001 Stony Brook University, Stony Brook, New York Mikhail Lyubich Leon Takhtajan Editors Proceedings of the conference on Graphs and Patterns in Mathematics and Theoretical Physics held at Stony Brook University, Stony Brook, New York, June 14-21, 2001. 2000 Mathematics Subject Classification. Primary 81Txx, 57-XX 18-XX 53Dxx 55-XX 37-XX 17Bxx. Library of Congress Cataloging-in-Publication Data Stony Brook Conference on Graphs and Patterns in Mathematics and Theoretical Physics (2001 : Stony Brook University) Graphs and Patterns in mathematics and theoretical physics : proceedings of the Stony Brook Conference on Graphs and Patterns in Mathematics and Theoretical Physics, June 14-21, 2001, Stony Brook University, Stony Brook, NY / Mikhail Lyubich, Leon Takhtajan, editors. p. cm. — (Proceedings of symposia in pure mathematics ; v. 73) Includes bibliographical references. ISBN 0-8218-3666-8 (alk. paper) 1. Graph Theory. 2. Mathematics-Graphic methods. 3. Physics-Graphic methods. 4. Man• ifolds (Mathematics). I. Lyubich, Mikhail, 1959- II. Takhtadzhyan, L. A. (Leon Armenovich) III. Title. IV. Series. QA166.S79 2001 511/.5-dc22 2004062363 Copying and reprinting. Material in this book may be reproduced by any means for edu• cational and scientific purposes without fee or permission with the exception of reproduction by services that collect fees for delivery of documents and provided that the customary acknowledg• ment of the source is given. -
General Topology
General Topology Tom Leinster 2014{15 Contents A Topological spaces2 A1 Review of metric spaces.......................2 A2 The definition of topological space.................8 A3 Metrics versus topologies....................... 13 A4 Continuous maps........................... 17 A5 When are two spaces homeomorphic?................ 22 A6 Topological properties........................ 26 A7 Bases................................. 28 A8 Closure and interior......................... 31 A9 Subspaces (new spaces from old, 1)................. 35 A10 Products (new spaces from old, 2)................. 39 A11 Quotients (new spaces from old, 3)................. 43 A12 Review of ChapterA......................... 48 B Compactness 51 B1 The definition of compactness.................... 51 B2 Closed bounded intervals are compact............... 55 B3 Compactness and subspaces..................... 56 B4 Compactness and products..................... 58 B5 The compact subsets of Rn ..................... 59 B6 Compactness and quotients (and images)............. 61 B7 Compact metric spaces........................ 64 C Connectedness 68 C1 The definition of connectedness................... 68 C2 Connected subsets of the real line.................. 72 C3 Path-connectedness.......................... 76 C4 Connected-components and path-components........... 80 1 Chapter A Topological spaces A1 Review of metric spaces For the lecture of Thursday, 18 September 2014 Almost everything in this section should have been covered in Honours Analysis, with the possible exception of some of the examples. For that reason, this lecture is longer than usual. Definition A1.1 Let X be a set. A metric on X is a function d: X × X ! [0; 1) with the following three properties: • d(x; y) = 0 () x = y, for x; y 2 X; • d(x; y) + d(y; z) ≥ d(x; z) for all x; y; z 2 X (triangle inequality); • d(x; y) = d(y; x) for all x; y 2 X (symmetry). -
Zuoqin Wang Time: March 25, 2021 the QUOTIENT TOPOLOGY 1. The
Topology (H) Lecture 6 Lecturer: Zuoqin Wang Time: March 25, 2021 THE QUOTIENT TOPOLOGY 1. The quotient topology { The quotient topology. Last time we introduced several abstract methods to construct topologies on ab- stract spaces (which is widely used in point-set topology and analysis). Today we will introduce another way to construct topological spaces: the quotient topology. In fact the quotient topology is not a brand new method to construct topology. It is merely a simple special case of the co-induced topology that we introduced last time. However, since it is very concrete and \visible", it is widely used in geometry and algebraic topology. Here is the definition: Definition 1.1 (The quotient topology). (1) Let (X; TX ) be a topological space, Y be a set, and p : X ! Y be a surjective map. The co-induced topology on Y induced by the map p is called the quotient topology on Y . In other words, −1 a set V ⊂ Y is open if and only if p (V ) is open in (X; TX ). (2) A continuous surjective map p :(X; TX ) ! (Y; TY ) is called a quotient map, and Y is called the quotient space of X if TY coincides with the quotient topology on Y induced by p. (3) Given a quotient map p, we call p−1(y) the fiber of p over the point y 2 Y . Note: by definition, the composition of two quotient maps is again a quotient map. Here is a typical way to construct quotient maps/quotient topology: Start with a topological space (X; TX ), and define an equivalent relation ∼ on X. -
AN INTRODUCTION to DIFFEOLOGY I Since Its Creation, In
AN INTRODUCTION TO DIFFEOLOGY PATRICK IGLESIAS-ZEMMOUR Abstract. This text presents the basics of Difeology and the main domains: Homotopy, Fiber Bundles, Quotients, Singularities, Cartan-de Rham Calculus — which form the core of diferential geometry — from the point of view of this theory. We show what makes difeology special and relevant in regard to these traditional subjects. Introduction Since its creation, in the early 1980s, Dieology has become an alternative, or rather a natural extension of traditional diferential geometry. With its developments in higher homotopy theory, ber bundles, modeling spaces, Cartan-de Rham calcu- lus, moment map and symplectic1 program, for examples, difeology now covers a large spectrum of traditional elds and deploys them from singular quotients to innite-dimensional spaces — and mixes the two — treating mathematical objects that are or are not strictly speaking manifolds, and other constructions, on an equal footing in a common framework. We shall see some of its achievements through a series of examples, chosen because they are not covered by the geom- etry of manifolds, because they involve innite-dimensional spaces or singular quotients, or both. The growing interest in difeology comes from the conjunction of two strong properties of the theory: 1. Mainly, the category {Difeology} is stable under all set-theoretic construc- tions: sums, products, subsets, and quotients. One says that it is a complete and co-complete category. It is also Cartesian closed, the space of smooth maps in difeology has itself a natural functional dieology. Date: August 25, 2017 – Revision May 15, 2020. Text of the talk given at the Conference “New Spaces in Mathematics & Physics”, September 28 – October 2, 2015 Institut Henri Poincaré Paris, France. -
Topologies on Spaces of Continuous Functions
Topologies on spaces of continuous functions Mart´ınEscard´o School of Computer Science, University of Birmingham Based on joint work with Reinhold Heckmann 7th November 2002 Path Let x0 and x1 be points of a space X. A path from x0 to x1 is a continuous map f : [0; 1] X ! with f(0) = x0 and f(1) = x1. 1 Homotopy Let f0; f1 : X Y be continuous maps. ! A homotopy from f0 to f1 is a continuous map H : [0; 1] X Y × ! with H(0; x) = f0(x) and H(1; x) = f1(x). 2 Homotopies as paths Let C(X; Y ) denote the set of continuous maps from X to Y . Then a homotopy H : [0; 1] X Y × ! can be seen as a path H : [0; 1] C(X; Y ) ! from f0 to f1. A continuous deformation of f0 into f1. 3 Really? This would be true if one could topologize C(X; Y ) in such a way that a function H : [0; 1] X Y × ! is continuous if and only if H : [0; 1] C(X; Y ) ! is continuous. This is the question Hurewicz posed to Fox in 1930. Is it possible to topologize C(X; Y ) in such a way that H is continuous if and only if H¯ is continuous? We are interested in the more general case when [0; 1] is replaced by an arbitrary topological space A. Fox published a partial answer in 1945. 4 The transpose of a function of two variables The transpose of a function g : A X Y × ! is the function g : A C(X; Y ) ! defined by g(a) = ga C(X; Y ) 2 where ga(x) = g(a; x): More concisely, g(a)(x) = g(a; x): 5 Weak, strong and exponential topologies A topology on the set C(X; Y ) is called weak if g : A X Y continuous = × ! ) g : A C(X; Y ) continuous, ! strong if g : A C(X; Y ) continuous = ! ) g : A X Y continuous, × ! exponential if it is both weak and strong. -
Introduction to Topology
Introduction to Topology Randall R. Holmes Auburn University Typeset by AMS-TEX 1 Chapter 1. Metric Spaces 1. De¯nition and Examples. As the course progresses we will need to review some basic notions about sets and functions. We begin with a little set theory. Let S be a set. For A; B ⊆ S, put A [ B := fs 2 S j s 2 A or s 2 Bg A \ B := fs 2 S j s 2 A and s 2 Bg S ¡ A := fs 2 S j s2 = Ag 1.1 Theorem. Let A; B ⊆ S. Then S ¡ (A [ B) = (S ¡ A) \ (S ¡ B). Exercise 1. Let A ⊆ S. Prove that S ¡ (S ¡ A) = A. Exercise 2. Let A; B ⊆ S. Prove that S ¡ (A \ B) = (S ¡ A) [ (S ¡ B). (Hint: Either prove this directly as in the proof of Theorem 1.1, or just use the statement of Theorem 1.1 together with Exercise 1.) Exercise 3. Let A; B; C ⊆ S. Prove that A M C ⊆ (A M B) [ (B M C), where A M B := (A [ B) ¡ (A \ B). 1.2 De¯nition. A metric space is a pair (X; d) where X is a non-empty set, and d is a function d : X £ X ! R such that for all x; y; z 2 X (1) d(x; y) ¸ 0, (2) d(x; y) = 0 if and only if x = y, (3) d(x; y) = d(y; x), and (4) d(x; z) · d(x; y) + d(y; z) (\triangle inequality"). In the de¯nition, d is called the distance function (or metric) and X is called the underlying set. -
Sufficient Generalities About Topological Vector Spaces
(November 28, 2016) Topological vector spaces Paul Garrett [email protected] http:=/www.math.umn.edu/egarrett/ [This document is http://www.math.umn.edu/~garrett/m/fun/notes 2016-17/tvss.pdf] 1. Banach spaces Ck[a; b] 2. Non-Banach limit C1[a; b] of Banach spaces Ck[a; b] 3. Sufficient notion of topological vector space 4. Unique vectorspace topology on Cn 5. Non-Fr´echet colimit C1 of Cn, quasi-completeness 6. Seminorms and locally convex topologies 7. Quasi-completeness theorem 1. Banach spaces Ck[a; b] We give the vector space Ck[a; b] of k-times continuously differentiable functions on an interval [a; b] a metric which makes it complete. Mere pointwise limits of continuous functions easily fail to be continuous. First recall the standard [1.1] Claim: The set Co(K) of complex-valued continuous functions on a compact set K is complete with o the metric jf − gjCo , with the C -norm jfjCo = supx2K jf(x)j. Proof: This is a typical three-epsilon argument. To show that a Cauchy sequence ffig of continuous functions has a pointwise limit which is a continuous function, first argue that fi has a pointwise limit at every x 2 K. Given " > 0, choose N large enough such that jfi − fjj < " for all i; j ≥ N. Then jfi(x) − fj(x)j < " for any x in K. Thus, the sequence of values fi(x) is a Cauchy sequence of complex numbers, so has a limit 0 0 f(x). Further, given " > 0 choose j ≥ N sufficiently large such that jfj(x) − f(x)j < " . -
Scale and the Differential Structure of Images
Scale and the differential structure of images Luc M J Florack, Bat M ter Haar Romeny, Jan J Koenderink and Max A Viergever capture the crucial observation of the inherently multi- Why and how one should study a scale-space is scale character of image structure. prescribed by the universal physical law of scale For some time there has been discussion on the invariance, expressed by the so-called Pi-theorem. question of how to generate a scale-space, the con- The fact that any image is a physical observable with an tinuous analogue of the pyramid, in a unique way, as inner and outer scale bound, necessarily gives rise to a there seemed to exist no clear way to choose among the 'scale-space representation', in wphich a given image is many possible scale-space filters' *. One obviously represented by a one-dimensiond family of images needed a set of natural, a priori scale-space constraints. representing that image on vurious levels of inner spatial A fundamental approach was adopted by scale. An early vision system is completely ignorant of Koenderink', Witkin" and Yuille and Poggio', who the geometry of its input. Its primary task is to establish formulated an a priori conttraint in the form of a this geometry at any available scale. The absence of causality requirement: no 'spurious detail' should be geometrical knowledge poses additional constraints on generated upon increasing scale. This, together with the construction of a scale-space, notably linearity, some symmetry constraints, unambiguously established spatial shift invariance and isotropy, thereby defining a the Gaussian kernel (i.e. -
Manifolds of Mappings for Continuum Mechanics
MANIFOLDS OF MAPPINGS FOR CONTINUUM MECHANICS PETER W. MICHOR Abstract. After an introduction to convenient calculus in infinite dimensions, the foundational material for manifolds of mappings is presented. The central character is the smooth convenient manifold C1(M; N) of all smooth mappings from a finite dimensional Whitney manifold germ M into a smooth manifold N. A Whitney manifold germ is a smooth (in the interior) manifold with a very general boundary, but still admitting a continuous Whitney extension operator. This notion is developed here for the needs of geometric continuum mechanics. 2010 Mathematics Subject Classification: 58B20, 58D15, 35Q31 Keywords and Phrases: Convenient calculus, Manifolds of map- pings, Diffeomorphism groups, Shape spaces, weak Riemannian met- rics. Contents 1. Introduction 2 2. A short review of convenient calculus in infinite dimensions 3 3. Manifolds with corners 8 4. Whitney manifold germs 12 5. Manifolds of mappings 20 6. Regular Lie groups 28 7. Spaces of embeddings or immersions, and shape spaces 35 8. Weak Riemannian manifolds 47 9. Robust weak Riemannian manifolds and Riemannian submersions 56 References 62 Peter W. Michor: Universit¨atWien, Oskar-Morgenstern-Platz 1, A-1090 Wien, Austria. In: Geometric Continuum Mechanics. Editors: Reuven Segev, Marcelo Epstein. Series: Advances in Continuum Mechanics, Vol. 42. pp. 3-75. Birkh¨auserBasel 2020. doi:10.1007/978-3-030-42683-5. 1 2 PETER W. MICHOR 1. Introduction At the birthplace of the notion of manifolds, in the Habilitationsschrift [93, end of section I], Riemann mentioned infinite dimensional manifolds ex- plicitly. The translation into English in [94] reads as follows: There are manifoldnesses in which the determination of posi- tion requires not a finite number, but either an endless series or a continuous manifoldness of determinations of quantity. -
Non-Commutative Toric Varieties
Non-commutative toric varieties Ludmil Katzarkov, Ernesto Lupercio, Laurent Meersseman, and Alberto Verjovsky Abstract. In this short note, we introduce a new family of non-commutative spaces that we call non-commutative toric varieties. We also briefly describe some of their main properties. The main technical tool in this investigation is a natural extension of LVM-theory for the irrational case. This note, aimed at graduate students, primarily consists of a brief survey of the required back- ground for the definition of a non-commutative toric variety, plus further re- sults at the end. An definitve version os this paper is to appear in Contempo- rary Mathematics. 1. Introduction Non-commutative toric varieties are to toric varieties what non-commutative tori are to tori and, as such, they can be interpreted in multiple ways: As (non- commutative) topological spaces, they are C∗-algebras associated to dense folia- tions, that is to say, deformations of the commutative C∗-algebras associated to tori. But while non-commutative tori correspond to foliations (deformations) on classical tori, non-commutative toric varieties correspond to foliations on so-called LVM-manifolds, which are certain intersections of real quadrics in complex pro- jective spaces of a very explicit nature. The homotopy type of LVM-manifolds is described by moment angle complexes [11] that provides us with the basic topo- logical information regarding non-commutative toric varieties. Non-commutative toric varieties can be interpreted as stratified parametrized families of non-commutative tori over a simple polytope: indeed, while for a classical toric variety the inverse image of a point µ−1(p) under the moment map µ : X ! P arXiv:1308.2774v2 [math.SG] 8 Nov 2013 is an ordinary torus, a non-commutative toric variety still has a moment map µ : X! P (landing in an irrational simple polytope) but then µ−1(p) is a non- commutative torus.