Cantor's Proof of the Nondenumerability of Perfect Sets
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Descriptive Set Theory
Descriptive Set Theory David Marker Fall 2002 Contents I Classical Descriptive Set Theory 2 1 Polish Spaces 2 2 Borel Sets 14 3 E®ective Descriptive Set Theory: The Arithmetic Hierarchy 27 4 Analytic Sets 34 5 Coanalytic Sets 43 6 Determinacy 54 7 Hyperarithmetic Sets 62 II Borel Equivalence Relations 73 1 8 ¦1-Equivalence Relations 73 9 Tame Borel Equivalence Relations 82 10 Countable Borel Equivalence Relations 87 11 Hyper¯nite Equivalence Relations 92 1 These are informal notes for a course in Descriptive Set Theory given at the University of Illinois at Chicago in Fall 2002. While I hope to give a fairly broad survey of the subject we will be concentrating on problems about group actions, particularly those motivated by Vaught's conjecture. Kechris' Classical Descriptive Set Theory is the main reference for these notes. Notation: If A is a set, A<! is the set of all ¯nite sequences from A. Suppose <! σ = (a0; : : : ; am) 2 A and b 2 A. Then σ b is the sequence (a0; : : : ; am; b). We let ; denote the empty sequence. If σ 2 A<!, then jσj is the length of σ. If f : N ! A, then fjn is the sequence (f(0); : : :b; f(n ¡ 1)). If X is any set, P(X), the power set of X is the set of all subsets X. If X is a metric space, x 2 X and ² > 0, then B²(x) = fy 2 X : d(x; y) < ²g is the open ball of radius ² around x. Part I Classical Descriptive Set Theory 1 Polish Spaces De¯nition 1.1 Let X be a topological space. -
Cantor and Continuity
Cantor and Continuity Akihiro Kanamori May 1, 2018 Georg Cantor (1845-1919), with his seminal work on sets and number, brought forth a new field of inquiry, set theory, and ushered in a way of proceeding in mathematics, one at base infinitary, topological, and combinatorial. While this was the thrust, his work at the beginning was embedded in issues and concerns of real analysis and contributed fundamentally to its 19th Century rigorization, a development turning on limits and continuity. And a continuing engagement with limits and continuity would be very much part of Cantor's mathematical journey, even as dramatically new conceptualizations emerged. Evolutionary accounts of Cantor's work mostly underscore his progressive ascent through set- theoretic constructs to transfinite number, this as the storied beginnings of set theory. In this article, we consider Cantor's work with a steady focus on con- tinuity, putting it first into the context of rigorization and then pursuing the increasingly set-theoretic constructs leading to its further elucidations. Beyond providing a narrative through the historical record about Cantor's progress, we will bring out three aspectual motifs bearing on the history and na- ture of mathematics. First, with Cantor the first mathematician to be engaged with limits and continuity through progressive activity over many years, one can see how incipiently metaphysical conceptualizations can become systemati- cally transmuted through mathematical formulations and results so that one can chart progress on the understanding of concepts. Second, with counterweight put on Cantor's early career, one can see the drive of mathematical necessity pressing through Cantor's work toward extensional mathematics, the increasing objectification of concepts compelled, and compelled only by, his mathematical investigation of aspects of continuity and culminating in the transfinite numbers and set theory. -
Set Ideal Topological Spaces
Set Ideal Topological Spaces W. B. Vasantha Kandasamy Florentin Smarandache ZIP PUBLISHING Ohio 2012 This book can be ordered from: Zip Publishing 1313 Chesapeake Ave. Columbus, Ohio 43212, USA Toll Free: (614) 485-0721 E-mail: [email protected] Website: www.zippublishing.com Copyright 2012 by Zip Publishing and the Authors Peer reviewers: Prof. Catalin Barbu, V. Alecsandri National College, Mathematics Department, Bacau, Romania. Prof. Valeri Kroumov, Okayama Univ. of Science, Japan. Dr. Sebastian Nicolaescu, 2 Terrace Ave., West Orange, NJ 07052, USA. Many books can be downloaded from the following Digital Library of Science: http://www.gallup.unm.edu/~smarandache/eBooks-otherformats.htm ISBN-13: 978-1-59973-193-3 EAN: 9781599731933 Printed in the United States of America 2 CONTENTS Preface 5 Chapter One INTRODUCTION 7 Chapter Two SET IDEALS IN RINGS 9 Chapter Three SET IDEAL TOPOLOGICAL SPACES 35 Chapter Four NEW CLASSES OF SET IDEAL TOPOLOGICAL SPACES AND APPLICATIONS 93 3 FURTHER READING 109 INDEX 111 ABOUT THE AUTHORS 114 4 PREFACE In this book the authors for the first time introduce a new type of topological spaces called the set ideal topological spaces using rings or semigroups, or used in the mutually exclusive sense. This type of topological spaces use the class of set ideals of a ring (semigroups). The rings or semigroups can be finite or infinite order. By this method we get complex modulo finite integer set ideal topological spaces using finite complex modulo integer rings or finite complex modulo integer semigroups. Also authors construct neutrosophic set ideal toplogical spaces of both finite and infinite order as well as complex neutrosophic set ideal topological spaces. -
Introductory Topics in the Mathematical Theory of Continuum Mechanics - R J Knops and R
CONTINUUM MECHANICS - Introductory Topics In The Mathematical Theory Of Continuum Mechanics - R J Knops and R. Quintanilla INTRODUCTORY TOPICS IN THE MATHEMATICAL THEORY OF CONTINUUM MECHANICS R J Knops School of Mathematical and Computer Sciences, Heriot-Watt University, UK R. Quintanilla Department of Applied Mathematics II, UPC Terrassa, Spain Keywords: Classical and non-classical continuum thermomechanics, well- and ill- posedness; non-linear, linear, linearized, initial and boundary value problems, existence, uniqueness, dynamic and spatial stability, continuous data dependence. Contents I. GENERAL PRINCIPLES 1. Introduction 2. The well-posed problem II. BASIC CONTINUUM MECHANICS 3. Introduction 4. Material description 5. Spatial description 6. Constitutive theories III. EXAMPLE: HEAT CONDUCTION 7. Introduction. Existence and uniqueness 8. Continuous dependence. Stability 9. Backward heat equation. Ill-posed problems 10. Non-linear heat conduction 11. Infinite thermal wave speeds IV. CLASSICAL THEORIES 12. Introduction 13. Thermoviscous flow. Navier-Stokes Fluid 14. Linearized and linear elastostatics 15. Linearized Elastodynamics 16. LinearizedUNESCO and linear thermoelastostatics – EOLSS 17. Linearized and linear thermoelastodynamics 18. Viscoelasticity 19. Non-linear Elasticity 20. Non-linearSAMPLE thermoelasticity and thermoviscoelasticity CHAPTERS V. NON-CLASSICAL THEORIES 21. Introduction 22. Isothermal models 23. Thermal Models Glossary Bibliography Biographical sketches ©Encyclopedia of Life Support Systems (EOLSS) CONTINUUM MECHANICS - Introductory Topics In The Mathematical Theory Of Continuum Mechanics - R J Knops and R. Quintanilla Summary Qualitative properties of well-posedness and ill-posedness are examined for problems in the equilibrium and dynamic classical non-linear theories of Navier-Stokes fluid flow and elasticity. These serve as prototypes of more general theories, some of which are also discussed. The article is reasonably self-contained. -
ON BERNSTEIN SETS Let Us Recall That a Subset of a Topological Space
ON BERNSTEIN SETS JACEK CICHON´ ABSTRACT. In this note I show a construction of Bernstein subsets of the real line which gives much more information about the structure of the real line than the classical one. 1. BASIC DEFINITIONS Let us recall that a subset of a topological space is a perfect set if is closed set and contains no isolated points. Perfect subsets of real line R have cardinality continuum. In fact every perfect set contains a copy of a Cantor set. This can be proved rather easilly by constructing a binary tree of decreasing small closed sets. There are continnum many perfect sets. This follows from a more general result: there are continuum many Borel subsets of real. We denote by R the real line. We will work in the theory ZFC. Definition 1. A subset B of the real line R is a Bernstein set if for every perfect subset P of R we have (P \ B 6= ;) ^ (P n B 6= ;) : Bernstein sets are interesting object of study because they are Lebesgue nonmeasurable and they do not have the property of Baire. The classical construction of a Berstein set goes as follows: we fix an enumeration (Pα)α<c of all perfect sets, we define a transfinite sequences (pα), (qα) of pairwise different points such that fpα; qαg ⊆ Pα, we put B = fpα : α < cg and we show that B is a Bernstein set. This construction can be found in many classical books. The of this note is to give slightly different construction, which will generate simultanously a big family of Bermstein sets.We start with one simple but beautifull result: Lemma 1. -
Topology JonPaul Cox Connected Spaces May 11, 2016
Topology JonPaul Cox Connected Spaces May 11, 2016 Connected Spaces JonPaul Cox 5/11/16 6th Period Topology Parallels Between Calculus and Topology Intermediate Value Theorem If is continuous and if r is a real number between f(a) and f(b), then there exists an element such that f(c) = r. Maximum Value Theorem If is continuous, then there exists an element such that for every . Uniform Continuity Theorem If is continuous, then given > 0, there exists > 0 such that for every pair of numbers , of [a,b] for which . 1 Topology JonPaul Cox Connected Spaces May 11, 2016 Parallels Between Calculus and Topology Intermediate Value Theorem If is continuous and if r is a real number between f(a) and f(b), then there exists an element such that f(c) = r. Connected Spaces A space can be "separated" if it can be broken up into two disjoint, open parts. Otherwise it is connected. If the set is not separated, it is connected, and vice versa. 2 Topology JonPaul Cox Connected Spaces May 11, 2016 Connected Spaces Let X be a topological space. A separation of X is a pair of disjoint, nonempty open sets of X whose union is X. E.g. Connected Spaces A space is connected if and only if the only subsets of X that are both open and closed in X are and X itself. 3 Topology JonPaul Cox Connected Spaces May 11, 2016 Subspace Topology Let X be a topological space with topology . If Y is a subset of X (I.E. -
Lecture 8: the Real Line, Part II February 11, 2009
Lecture 8: The Real Line, Part II February 11, 2009 Definition 6.13. a ∈ X is isolated in X iff there is an open interval I for which X ∩ I = {a}. Otherwise, a is a limit point. Remark. Another way to state this is that a is isolated if it is not a limit point of X. Definition 6.14. X is a perfect set iff X is closed and has no isolated points. Remark. This definition sounds nice and tidy, but there are some very strange perfect sets. For example, the Cantor set is perfect, despite being nowhere dense! Our goal will be to prove the Cantor-Bendixson theorem, i.e. the perfect set theorem for closed sets, that every closed uncountable set has a perfect subset. Lemma 6.15. If P is a perfect set and I is an open interval on R such that I ∩ P 6= ∅, then there exist disjoint closed intervals J0,J1 ⊂ I such that int[J0] ∩ P 6= ∅ and int[J1] ∩ P 6= ∅. Moreover, we can pick J0 and J1 such that their lengths are both less than any ² > 0. Proof. Since P has no isolated points, there must be at least two points a0, a1 ∈ I ∩ P . Then just pick J0 3 a0 and J1 3 a1 to be small enough. SDG Lemma 6.16. If P is a nonempty perfect set, then P ∼ R. Proof. We exhibit a one-to-one mapping G : 2ω → P . Note that 2ω can be viewed as the set of all infinite paths in a full, infinite binary tree with each edge labeled by 0 or 1. -
Generalizations and Properties of the Ternary Cantor Set and Explorations in Similar Sets
Generalizations and Properties of the Ternary Cantor Set and Explorations in Similar Sets by Rebecca Stettin A capstone project submitted in partial fulfillment of graduating from the Academic Honors Program at Ashland University May 2017 Faculty Mentor: Dr. Darren D. Wick, Professor of Mathematics Additional Reader: Dr. Gordon Swain, Professor of Mathematics Abstract Georg Cantor was made famous by introducing the Cantor set in his works of mathemat- ics. This project focuses on different Cantor sets and their properties. The ternary Cantor set is the most well known of the Cantor sets, and can be best described by its construction. This set starts with the closed interval zero to one, and is constructed in iterations. The first iteration requires removing the middle third of this interval. The second iteration will remove the middle third of each of these two remaining intervals. These iterations continue in this fashion infinitely. Finally, the ternary Cantor set is described as the intersection of all of these intervals. This set is particularly interesting due to its unique properties being uncountable, closed, length of zero, and more. A more general Cantor set is created by tak- ing the intersection of iterations that remove any middle portion during each iteration. This project explores the ternary Cantor set, as well as variations in Cantor sets such as looking at different middle portions removed to create the sets. The project focuses on attempting to generalize the properties of these Cantor sets. i Contents Page 1 The Ternary Cantor Set 1 1 2 The n -ary Cantor Set 9 n−1 3 The n -ary Cantor Set 24 4 Conclusion 35 Bibliography 40 Biography 41 ii Chapter 1 The Ternary Cantor Set Georg Cantor, born in 1845, was best known for his discovery of the Cantor set. -
Big Homotopy Theory
University of Tennessee, Knoxville TRACE: Tennessee Research and Creative Exchange Doctoral Dissertations Graduate School 5-2013 Big Homotopy Theory Keith Gordon Penrod [email protected] Follow this and additional works at: https://trace.tennessee.edu/utk_graddiss Part of the Geometry and Topology Commons Recommended Citation Penrod, Keith Gordon, "Big Homotopy Theory. " PhD diss., University of Tennessee, 2013. https://trace.tennessee.edu/utk_graddiss/1768 This Dissertation is brought to you for free and open access by the Graduate School at TRACE: Tennessee Research and Creative Exchange. It has been accepted for inclusion in Doctoral Dissertations by an authorized administrator of TRACE: Tennessee Research and Creative Exchange. For more information, please contact [email protected]. To the Graduate Council: I am submitting herewith a dissertation written by Keith Gordon Penrod entitled "Big Homotopy Theory." I have examined the final electronic copy of this dissertation for form and content and recommend that it be accepted in partial fulfillment of the equirr ements for the degree of Doctor of Philosophy, with a major in Mathematics. Jurek Dydak, Major Professor We have read this dissertation and recommend its acceptance: Jim Conant, Nikolay Brodskiy, Morwen Thistletwaite, Delton Gerloff Accepted for the Council: Carolyn R. Hodges Vice Provost and Dean of the Graduate School (Original signatures are on file with official studentecor r ds.) Big Homotopy Theory A Dissertation Presented for the Doctor of Philosophy Degree The University of Tennessee, Knoxville Keith Gordon Penrod May 2013 c by Keith Gordon Penrod, 2013 All Rights Reserved. ii This dissertation is dedicated to Archimedes, who was my inspiration for becoming a mathematician. -
UC Berkeley UC Berkeley Electronic Theses and Dissertations
UC Berkeley UC Berkeley Electronic Theses and Dissertations Title Mechanical Behaviors of Alloys From First Principles Permalink https://escholarship.org/uc/item/1xv2n9dw Author Hanlumyuang, Yuranan Publication Date 2011 Peer reviewed|Thesis/dissertation eScholarship.org Powered by the California Digital Library University of California Mechanical Behaviors of Alloys From First Principles by Yuranan Hanlumyuang A dissertation submitted in partial satisfaction of the requirements for the degree of Doctor of Philosophy in Materials Sciences and Engineering in the Graduate Division of the University of California, Berkeley Committee in charge: Professor Daryl C. Chrzan, Chair Professor John W. Morris, Jr. Professor Tarek I. Zohdi Fall 2011 Mechanical Behaviors of Alloys From First Principles Copyright 2011 by Yuranan Hanlumyuang 1 Abstract Mechanical Behaviors of Alloys From First Principles by Yuranan Hanlumyuang Doctor of Philosophy in Materials Sciences and Engineering University of California, Berkeley Professor Daryl C. Chrzan, Chair Several mesoscale models have been developed to consider a number of mechanical prop- erties and microstructures of Ti-V approximants to Gum Metal and steels from the atomistic scale. In Gum Metal, the relationships between phonon properties and phase stabilities are studied. Our results show that it is possible to design a BCC (β-phase) alloy that deforms near the ideal strength, while maintaining structural stability with respect to the formation of the ! and α00 phases. Theoretical diffraction patterns reveal the role of the soft N−point phonon and the BCC!HCP transformation path in post-deformation samples. The total energies of the path explain the formation of the giant faults and nano shearbands in Gum Metal. -
Definition in Terms of Order Alone in the Linear
DEFINITION IN TERMS OF ORDERALONE IN THE LINEAR CONTINUUMAND IN WELL-ORDERED SETS* BY OSWALD VEBLEN First definition of the continuum. A linear continuum is a set of elements { P} which we may call points, sub- ject to a relation -< which we may read precedes, governed by the following conditions, A to E : A. General Postulates of Order. 1. { P} contains at least two elements. 2. If Px and P2 are distinct elements of {P} then either Px -< P2 or P < P . 3. IfP, -< F2 then Px is distinct from P2. f 4. IfPx <. P2 and P2 < P3, then P, < P3. f B. Dedekind Postulate of Closure. J If {P} consists entirely of two infinite subsets, [P] and [P"] such that P' -< P", then there is either a P'0 of [PJ such that P' -< P'0 whenever P + P'0 or a P'J of [P"J such that P'0' < P" whenever P" +- P'¡. C. Pseudo-Archimedean postulate. 1. If { P} is an infinite set then there exists a subset [ P„ ] , such that P„ -< P„+ ,(^==1, 2, 3, ■••) and if P is any element of { P} for which Px "C P, then there exists a v such that P -< Pv. * Presented to the Society December 30, 1904, uuder the title, Non-Metrictd Definition of the Linear Continuum. Received for publication January 26, 1905. |The propositions As and At say that -< is "non-reflexive" and "transitive." It follows immediately that it is "non-symmetric," for if Px -< P2 and P,A. Pi could occur simultaneously, 4 would lead to P¡^P¡, contrary to 3. -
Arxiv:1703.05470V1 [Math.LO] 16 Mar 2017 Coding Polish Spaces
Coding Polish spaces Diego Alejandro Mej´ıa Faculty of Science Shizuoka University 836 Ohya, Suruga-ku, 422-8529 Shizuoka, Japan [email protected] Abstract We use countable metric spaces to code Polish metric spaces and evaluate the complexity of some statements about these codes and of some relations that can be determined by the codes. Also, we propose a coding for continuous functions between Polish metric spaces. 1 Introduction A Polish metric space is a separable complete metric space hX,di and a Polish space is a topological space X which is homeomorphic to some Polish metric space (in the first notion the complete metric is required). As any Polish metric space is the completion of a countable metric space and the latter can be coded by reals in Rω×ω, we can use such reals to code Polish metric spaces. This coding was used by Clemens [Cle12] to formalize the isometry relation and to study other equivalence relations that can be reduced to that one. In this paper, we take a closer look to this coding and study the complexity of some statements about codes, some of them characterizing relations between Polish metric spaces. In particular, we provide a different proof of [Cle12, Lemma 4] that states that the isometry relation is analytic (Theorem 3.5(f)). We also code continuous functions between Polish metric spaces by Cauchy-continuous functions between the corresponding separable metric spaces and, like in the case of Polish metric spaces, we study the complexity of arXiv:1703.05470v1 [math.LO] 16 Mar 2017 some statements about this coding.