Topological Spaces and Manifolds
Total Page:16
File Type:pdf, Size:1020Kb
Load more
Recommended publications
-
Infinite-Dimensional Manifolds Are Open Subsets of Hilbert Space
View metadata, citation and similar papers at core.ac.uk brought to you by CORE provided by Elsevier - Publisher Connector INFINITE-DIMENSIONAL MANIFOLDS ARE OPEN SUBSETS OF HILBERT SPACE DAVID W. HENDERSON+ (Receketl z I Jflmrr,v 1969) IN THIS paper We prove, using Hilbert space microbundles, the THEOREM. If M is n separable metric manifold modeled on the separable injnite- dimensional Hilbert space, H, then M can be embedded as an open subset of H. Each infinite-dimensional separable Frechet space (and therefore each infinite- dimensional separable Banach space) is homeomorphic to H. (See [I].) We shall use “F-manifold ” to denote “ metric manifold modeled on a separable infinite-dimensional Frenchet space “. Thus we have COROLLARY 1. Each separable F-matzifold ccl/zbe embedded as an open subset of H. Recent results of Eells and Elworthy [6] and Kuiper and Burghelea [lo] and Moulis [14] combine to show (see [5]) that every homotopy equivalence between C”-Hilbert manifolds is homotopic to a C” diffeomorphism. Since open subsets of H have an induced C” structure, we have COROLLARY 2. Each F-manifokd has u unique C” Hilbert manifold structure. an d COROLLARY 3. Ecery homotopy eyuicalence betbreen F-manifolds is homotopic to a homeomorphism. Results about open subsets of H in [7] apply to give us COROLLARY 4. For each F-manifold Xl there is a coutltable locally-finite simplicial complex K, such that 1cI is homeomorphic to \l<j x H. an d COROLLARY 5. Each F-manifold is homeomorphic to an opett set U c H, such that H - U is homeomorphic to H and bd(U) is homeomorphic to U and to cl(U). -
I-Sequential Topological Spaces∗
Applied Mathematics E-Notes, 14(2014), 236-241 c ISSN 1607-2510 Available free at mirror sites of http://www.math.nthu.edu.tw/ amen/ -Sequential Topological Spaces I Sudip Kumar Pal y Received 10 June 2014 Abstract In this paper a new notion of topological spaces namely, I-sequential topo- logical spaces is introduced and investigated. This new space is a strictly weaker notion than the first countable space. Also I-sequential topological space is a quotient of a metric space. 1 Introduction The idea of convergence of real sequence have been extended to statistical convergence by [2, 14, 15] as follows: If N denotes the set of natural numbers and K N then Kn denotes the set k K : k n and Kn stands for the cardinality of the set Kn. The natural densityf of the2 subset≤ Kg is definedj j by Kn d(K) = lim j j, n n !1 provided the limit exists. A sequence xn n N of points in a metric space (X, ) is said to be statistically f g 2 convergent to l if for arbitrary " > 0, the set K(") = k N : (xk, l) " has natural density zero. A lot of investigation has been donef on2 this convergence≥ andg its topological consequences after initial works by [5, 13]. It is easy to check that the family Id = A N : d(A) = 0 forms a non-trivial f g admissible ideal of N (recall that I 2N is called an ideal if (i) A, B I implies A B I and (ii) A I,B A implies B I. -
Ergodicity and Metric Transitivity
Chapter 25 Ergodicity and Metric Transitivity Section 25.1 explains the ideas of ergodicity (roughly, there is only one invariant set of positive measure) and metric transivity (roughly, the system has a positive probability of going from any- where to anywhere), and why they are (almost) the same. Section 25.2 gives some examples of ergodic systems. Section 25.3 deduces some consequences of ergodicity, most im- portantly that time averages have deterministic limits ( 25.3.1), and an asymptotic approach to independence between even§ts at widely separated times ( 25.3.2), admittedly in a very weak sense. § 25.1 Metric Transitivity Definition 341 (Ergodic Systems, Processes, Measures and Transfor- mations) A dynamical system Ξ, , µ, T is ergodic, or an ergodic system or an ergodic process when µ(C) = 0 orXµ(C) = 1 for every T -invariant set C. µ is called a T -ergodic measure, and T is called a µ-ergodic transformation, or just an ergodic measure and ergodic transformation, respectively. Remark: Most authorities require a µ-ergodic transformation to also be measure-preserving for µ. But (Corollary 54) measure-preserving transforma- tions are necessarily stationary, and we want to minimize our stationarity as- sumptions. So what most books call “ergodic”, we have to qualify as “stationary and ergodic”. (Conversely, when other people talk about processes being “sta- tionary and ergodic”, they mean “stationary with only one ergodic component”; but of that, more later. Definition 342 (Metric Transitivity) A dynamical system is metrically tran- sitive, metrically indecomposable, or irreducible when, for any two sets A, B n ∈ , if µ(A), µ(B) > 0, there exists an n such that µ(T − A B) > 0. -
MTH 304: General Topology Semester 2, 2017-2018
MTH 304: General Topology Semester 2, 2017-2018 Dr. Prahlad Vaidyanathan Contents I. Continuous Functions3 1. First Definitions................................3 2. Open Sets...................................4 3. Continuity by Open Sets...........................6 II. Topological Spaces8 1. Definition and Examples...........................8 2. Metric Spaces................................. 11 3. Basis for a topology.............................. 16 4. The Product Topology on X × Y ...................... 18 Q 5. The Product Topology on Xα ....................... 20 6. Closed Sets.................................. 22 7. Continuous Functions............................. 27 8. The Quotient Topology............................ 30 III.Properties of Topological Spaces 36 1. The Hausdorff property............................ 36 2. Connectedness................................. 37 3. Path Connectedness............................. 41 4. Local Connectedness............................. 44 5. Compactness................................. 46 6. Compact Subsets of Rn ............................ 50 7. Continuous Functions on Compact Sets................... 52 8. Compactness in Metric Spaces........................ 56 9. Local Compactness.............................. 59 IV.Separation Axioms 62 1. Regular Spaces................................ 62 2. Normal Spaces................................ 64 3. Tietze's extension Theorem......................... 67 4. Urysohn Metrization Theorem........................ 71 5. Imbedding of Manifolds.......................... -
Defining Physics at Imaginary Time: Reflection Positivity for Certain
Defining physics at imaginary time: reflection positivity for certain Riemannian manifolds A thesis presented by Christian Coolidge Anderson [email protected] (978) 204-7656 to the Department of Mathematics in partial fulfillment of the requirements for an honors degree. Advised by Professor Arthur Jaffe. Harvard University Cambridge, Massachusetts March 2013 Contents 1 Introduction 1 2 Axiomatic quantum field theory 2 3 Definition of reflection positivity 4 4 Reflection positivity on a Riemannian manifold M 7 4.1 Function space E over M ..................... 7 4.2 Reflection on M .......................... 10 4.3 Reflection positive inner product on E+ ⊂ E . 11 5 The Osterwalder-Schrader construction 12 5.1 Quantization of operators . 13 5.2 Examples of quantizable operators . 14 5.3 Quantization domains . 16 5.4 The Hamiltonian . 17 6 Reflection positivity on the level of group representations 17 6.1 Weakened quantization condition . 18 6.2 Symmetric local semigroups . 19 6.3 A unitary representation for Glor . 20 7 Construction of reflection positive measures 22 7.1 Nuclear spaces . 23 7.2 Construction of nuclear space over M . 24 7.3 Gaussian measures . 27 7.4 Construction of Gaussian measure . 28 7.5 OS axioms for the Gaussian measure . 30 8 Reflection positivity for the Laplacian covariance 31 9 Reflection positivity for the Dirac covariance 34 9.1 Introduction to the Dirac operator . 35 9.2 Proof of reflection positivity . 38 10 Conclusion 40 11 Appendix A: Cited theorems 40 12 Acknowledgments 41 1 Introduction Two concepts dominate contemporary physics: relativity and quantum me- chanics. They unite to describe the physics of interacting particles, which live in relativistic spacetime while exhibiting quantum behavior. -
Characterization of Exact Lumpability for Vector Fields on Smooth Manifolds
Preprint. Final version in: Differ.Geom.Appl. 48 (2016) 46-60 doi: 10.1016/j.difgeo.2016.06.001 Characterization of Exact Lumpability for Vector Fields on Smooth Manifolds Leonhard Horstmeyer∗ † Fatihcan M. Atay‡ Abstract We characterize the exact lumpability of smooth vector fields on smooth man- ifolds. We derive necessary and sufficient conditions for lumpability and express them from four different perspectives, thus simplifying and generalizing various re- sults from the literature that exist for Euclidean spaces. We introduce a partial connection on the pullback bundle that is related to the Bott connection and be- haves like a Lie derivative. The lumping conditions are formulated in terms of the differential of the lumping map, its covariant derivative with respect to the con- nection and their respective kernels. Some examples are discussed to illustrate the theory. PACS numbers: 02.40.-k, 02.30.Hq, 02.40.Hw AMS classification scheme numbers: 37C10, 34C40, 58A30, 53B05, 34A05 Keywords: lumping, aggregation, dimensional reduction, Bott connection 1 Introduction Dimensional reduction is an important aspect in the study of smooth dynamical systems and in particular in modeling with ordinary differential equations (ODEs). Often a reduction can elucidate key mechanisms, find decoupled subsystems, reveal conserved quantities, make the problem computationally tractable, or rid it from redundancies. A dimensional reduction by which micro state variables are aggregated into macro state variables also goes by the name of lumping. Starting from a micro state dynamics, this arXiv:1607.01237v2 [math.DG] 6 Jul 2016 aggregation induces a lumped dynamics on the macro state space. Whenever a non- trivial lumping, one that is neither the identity nor maps to a single point, confers the ∗Max Planck Institute for Mathematics in the Sciences, Inselstraße 22, 04103 Leipzig, Germany. -
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). -
Dirichlet Character Difference Graphs 1
DIRICHLET CHARACTER DIFFERENCE GRAPHS M. BUDDEN, N. CALKINS, W. N. HACK, J. LAMBERT and K. THOMPSON Abstract. We define Dirichlet character difference graphs and describe their basic properties, includ- ing the enumeration of triangles. In the case where the modulus is an odd prime, we exploit the spectral properties of such graphs in order to provide meaningful upper bounds for their diameter. 1. Introduction Upon one's first encounter with abstract algebra, a theorem which resonates throughout the theory is Cayley's theorem, which states that every finite group is isomorphic to a subgroup of some symmetric group. The significance of such a result comes from giving all finite groups a common ground by allowing one to focus on groups of permutations. It comes as no surprise that algebraic graph theorists chose the name Cayley graphs to describe graphs which depict groups. More formally, if G is a group and S is a subset of G closed under taking inverses and not containing the identity, then the Cayley graph, Cay(G; S), is defined to be the graph with vertex set G and an edge occurring between the vertices g and h if hg−1 2 S [9]. Some of the first examples of JJ J I II Cayley graphs that are usually encountered include the class of circulant graphs. A circulant graph, denoted by Circ(m; S), uses Z=mZ as the group for a Cayley graph and the generating set S is Go back m chosen amongst the integers in the set f1; 2; · · · b 2 cg [2]. -
Daniel Irvine June 20, 2014 Lecture 6: Topological Manifolds 1. Local
Daniel Irvine June 20, 2014 Lecture 6: Topological Manifolds 1. Local Topological Properties Exercise 7 of the problem set asked you to understand the notion of path compo- nents. We assume that knowledge here. We have done a little work in understanding the notions of connectedness, path connectedness, and compactness. It turns out that even if a space doesn't have these properties globally, they might still hold locally. Definition. A space X is locally path connected at x if for every neighborhood U of x, there is a path connected neighborhood V of x contained in U. If X is locally path connected at all of its points, then it is said to be locally path connected. Lemma 1.1. A space X is locally path connected if and only if for every open set V of X, each path component of V is open in X. Proof. Suppose that X is locally path connected. Let V be an open set in X; let C be a path component of V . If x is a point of V , we can (by definition) choose a path connected neighborhood W of x such that W ⊂ V . Since W is path connected, it must lie entirely within the path component C. Therefore C is open. Conversely, suppose that the path components of open sets of X are themselves open. Given a point x of X and a neighborhood V of x, let C be the path component of V containing x. Now C is path connected, and since it is open in X by hypothesis, we now have that X is locally path connected at x. -
ERGODIC THEORY and ENTROPY Contents 1. Introduction 1 2
ERGODIC THEORY AND ENTROPY JACOB FIEDLER Abstract. In this paper, we introduce the basic notions of ergodic theory, starting with measure-preserving transformations and culminating in as a statement of Birkhoff's ergodic theorem and a proof of some related results. Then, consideration of whether Bernoulli shifts are measure-theoretically iso- morphic motivates the notion of measure-theoretic entropy. The Kolmogorov- Sinai theorem is stated to aid in calculation of entropy, and with this tool, Bernoulli shifts are reexamined. Contents 1. Introduction 1 2. Measure-Preserving Transformations 2 3. Ergodic Theory and Basic Examples 4 4. Birkhoff's Ergodic Theorem and Applications 9 5. Measure-Theoretic Isomorphisms 14 6. Measure-Theoretic Entropy 17 Acknowledgements 22 References 22 1. Introduction In 1890, Henri Poincar´easked under what conditions points in a given set within a dynamical system would return to that set infinitely many times. As it turns out, under certain conditions almost every point within the original set will return repeatedly. We must stipulate that the dynamical system be modeled by a measure space equipped with a certain type of transformation T :(X; B; m) ! (X; B; m). We denote the set we are interested in as B 2 B, and let B0 be the set of all points in B that return to B infinitely often (meaning that for a point b 2 B, T m(b) 2 B for infinitely many m). Then we can be assured that m(B n B0) = 0. This result will be proven at the end of Section 2 of this paper. In other words, only a null set of points strays from a given set permanently. -
Introducing the Mini-DML Project Thierry Bouche
Introducing the mini-DML project Thierry Bouche To cite this version: Thierry Bouche. Introducing the mini-DML project. ECM4 Satellite Conference EMANI/DML, Jun 2004, Stockholm, Sweden. 11 p.; ISBN 3-88127-107-4. hal-00347692 HAL Id: hal-00347692 https://hal.archives-ouvertes.fr/hal-00347692 Submitted on 16 Dec 2008 HAL is a multi-disciplinary open access L’archive ouverte pluridisciplinaire HAL, est archive for the deposit and dissemination of sci- destinée au dépôt et à la diffusion de documents entific research documents, whether they are pub- scientifiques de niveau recherche, publiés ou non, lished or not. The documents may come from émanant des établissements d’enseignement et de teaching and research institutions in France or recherche français ou étrangers, des laboratoires abroad, or from public or private research centers. publics ou privés. Introducing the mini-DML project Thierry Bouche Université Joseph Fourier (Grenoble) WDML workshop Stockholm June 27th 2004 Introduction At the Göttingen meeting of the Digital mathematical library project (DML), in May 2004, the issue was raised that discovery and seamless access to the available digitised litterature was still a task to be acomplished. The ambitious project of a comprehen- sive registry of all ongoing digitisation activities in the field of mathematical research litterature was agreed upon, as well as the further investigation of many linking op- tions to ease user’s life. However, given the scope of those projects, their benefits can’t be expected too soon. Between the hope of a comprehensive DML with many eYcient entry points and the actual dissemination of heterogeneous partial lists of available material, there is a path towards multiple distributed databases allowing integrated search, metadata exchange and powerful interlinking. -
DIFFERENTIAL GEOMETRY COURSE NOTES 1.1. Review of Topology. Definition 1.1. a Topological Space Is a Pair (X,T ) Consisting of A
DIFFERENTIAL GEOMETRY COURSE NOTES KO HONDA 1. REVIEW OF TOPOLOGY AND LINEAR ALGEBRA 1.1. Review of topology. Definition 1.1. A topological space is a pair (X; T ) consisting of a set X and a collection T = fUαg of subsets of X, satisfying the following: (1) ;;X 2 T , (2) if Uα;Uβ 2 T , then Uα \ Uβ 2 T , (3) if Uα 2 T for all α 2 I, then [α2I Uα 2 T . (Here I is an indexing set, and is not necessarily finite.) T is called a topology for X and Uα 2 T is called an open set of X. n Example 1: R = R × R × · · · × R (n times) = f(x1; : : : ; xn) j xi 2 R; i = 1; : : : ; ng, called real n-dimensional space. How to define a topology T on Rn? We would at least like to include open balls of radius r about y 2 Rn: n Br(y) = fx 2 R j jx − yj < rg; where p 2 2 jx − yj = (x1 − y1) + ··· + (xn − yn) : n n Question: Is T0 = fBr(y) j y 2 R ; r 2 (0; 1)g a valid topology for R ? n No, so you must add more open sets to T0 to get a valid topology for R . T = fU j 8y 2 U; 9Br(y) ⊂ Ug: Example 2A: S1 = f(x; y) 2 R2 j x2 + y2 = 1g. A reasonable topology on S1 is the topology induced by the inclusion S1 ⊂ R2. Definition 1.2. Let (X; T ) be a topological space and let f : Y ! X.