Connecting Connectedness
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A Sheaf-Theoretic Topos Model of the Physical “Continuum” and Its Cohomological Observable Dynamics
A Sheaf-Theoretic Topos Model of the Physical “Continuum” and its Cohomological Observable Dynamics ELIAS ZAFIRIS University of Athens Department of Mathematics Panepistimiopolis, 15784 Athens Greece Abstract The physical “continuum” is being modeled as a complex of events interconnected by the relation of extension and forming an abstract partially ordered structure. Operational physical procedures for dis- cerning observable events assume their existence and validity locally, by coordinatizing the informational content of those observable events in terms of real-valued local observables. The localization process is effectuated in terms of topological covering systems on the events “con- tinuum”, that do not presuppose an underlying structure of points on the real line, and moreover, respect only the fundamental relation of extension between events. In this sense, the physical “continuum” is represented by means of a fibered topos-theoretic structure, modeled as a sheaf of algebras of continuous real-valued functions. Finally, the dy- namics of information propagation, formulated in terms of continuous real-valued observables, is described in the context of an appropriate sheaf-cohomological framework corresponding to the localization pro- cess. 0E-mail : ezafi[email protected] 1 Keywords: Observables; Modern Differential Geometry; Topos and Sheaf Theory; Functoriality; Connection; De Rham Cohomology. 2 1 Prologue The semantics of the physical “continuum” in the standard interpretation of physical systems theories is associated with the codomain of valuation of physical attributes (Butterfield and Isham (2000)). Usually the notion of “continuum” is tied with the attribute of position, serving as the range of values characterizing this particular attribution. The model adopted to represent these values is the real line R and its powers, specified as a set the- oretical structure of points that are independent and possess the property of infinite distinguishability with absolute precision. -
Homology and Vortices I
The role of homology in fluid vortices I: non-relativistic flow D. H. Delphenich † Spring Valley, OH 45370 Abstract : The methods of singular and de Rham homology and cohomology are reviewed to the extent that they are applicable to the structure and motion of vortices. In particular, they are first applied to the concept of integral invariants. After a brief review of the elements of fluid mechanics, when expressed in the language of exterior differential forms and homology theory, the basic laws of vortex theory are shown to be statements that are rooted in the homology theory of integral invariants. (†) E-mail: [email protected] Contents Page Introduction ……………………………………………………………………………………… 1 Part I: Mathematical preliminaries 1. Elementary homology and cohomology……………………………………………………… 3 a. Singular homology 3 b. Singular cohomology 10 c. De Rham cohomology 12 d. De Rham homology 15 e. Differentiable homotopies of chains. 17 f. Chain homotopies 18 2. Vector homology …………………………………………………………………………… 19 3. Integral invariants ………………………………………………………………………….. 23 Part II: The theory of vortices 4. Basic fluid kinematics ………………………………………………………………………. 26 a. The basic flow region 26 b. Flow velocity vector field 27 c. The velocity gradient 27 d. Flow covelocity 1-form 29 e. Integrability of covelocity 29 f. The convective acceleration 1-form 31 5. Kinematical vorticity 2-form ………………..……………………………………………... 32 a. Basic definition 32 b. Vorticity vector field. 33 c. Vortex lines and tubes. 34 d. Vorticity flux as a 2-coboundary 34 e. The magnetic analogy 35 6. Circulation as a 1-cochain ………………………………………………………………….. 36 a. Basic definition 36 b. Topological sources of vorticity for irrotational flow 37 7. Basic fluid dynamics …………………………………………………………………………. -
Chapter 7 Separation Properties
Chapter VII Separation Axioms 1. Introduction “Separation” refers here to whether or not objects like points or disjoint closed sets can be enclosed in disjoint open sets; “separation properties” have nothing to do with the idea of “separated sets” that appeared in our discussion of connectedness in Chapter 5 in spite of the similarity of terminology.. We have already met some simple separation properties of spaces: the XßX!"and X # (Hausdorff) properties. In this chapter, we look at these and others in more depth. As “more separation” is added to spaces, they generally become nicer and nicer especially when “separation” is combined with other properties. For example, we will see that “enough separation” and “a nice base” guarantees that a space is metrizable. “Separation axioms” translates the German term Trennungsaxiome used in the older literature. Therefore the standard separation axioms were historically named XXXX!"#$, , , , and X %, each stronger than its predecessors in the list. Once these were common terminology, another separation axiom was discovered to be useful and “interpolated” into the list: XÞ"" It turns out that the X spaces (also called $$## Tychonoff spaces) are an extremely well-behaved class of spaces with some very nice properties. 2. The Basics Definition 2.1 A topological space \ is called a 1) X! space if, whenever BÁC−\, there either exists an open set Y with B−Y, CÂY or there exists an open set ZC−ZBÂZwith , 2) X" space if, whenever BÁC−\, there exists an open set Ywith B−YßCÂZ and there exists an open set ZBÂYßC−Zwith 3) XBÁC−\Y# space (or, Hausdorff space) if, whenever , there exist disjoint open sets and Z\ in such that B−YC−Z and . -
Topology Proceedings FOLDERS of CONTINUA 1. Introduction The
To appear in Topology Proceedings FOLDERS OF CONTINUA C.L. HAGOPIAN, M.M. MARSH, AND J.R. PRAJS Abstract. This article is motivated by the following unsolved fixed point problem of G. R. Gordh, Jr. If a continuum X ad- mits a map onto an arc such that the preimage of each point is either a point or an arc, then must X have the fixed point prop- erty? We call such a continuum an arc folder. This terminology generalizes naturally to the concept of a continuum folder. We give several partial solutions to Gordh's problem. The an- swer is yes if X is either planar, one dimensional, or an approx- imate absolute neighborhood retract. We establish basic proper- ties of both continuum folders and arc folders. We provide several specific examples of arc folders, and give general methods for con- structing continuum folders. Numerous related questions are raised for further research. 1. Introduction The main focus of this paper is arc folders; that is, continua admit- ting maps onto an arc with point preimages being an arc or a point. In conversation (circa 1980) with a number of topologists, G. R. Gordh, Jr. asked the following question, which is still open. Question 1. Do all arc folders have the fixed point property? We find this question challenging and intriguing, and the class of arc folders interesting and more diverse than its rather restrictive definition may suggest. In this paper, we give some partial answers to Gordh's 2010 Mathematics Subject Classification. Primary 54F15, 54B15, 54D80; Sec- ondary 54C10, 54B17. -
METRIC SPACES and SOME BASIC TOPOLOGY
Chapter 3 METRIC SPACES and SOME BASIC TOPOLOGY Thus far, our focus has been on studying, reviewing, and/or developing an under- standing and ability to make use of properties of U U1. The next goal is to generalize our work to Un and, eventually, to study functions on Un. 3.1 Euclidean n-space The set Un is an extension of the concept of the Cartesian product of two sets that was studied in MAT108. For completeness, we include the following De¿nition 3.1.1 Let S and T be sets. The Cartesian product of S and T , denoted by S T,is p q : p + S F q + T . The Cartesian product of any ¿nite number of sets S1 S2 SN , denoted by S1 S2 SN ,is j b ck p1 p2 pN : 1 j j + M F 1 n j n N " p j + S j . The object p1 p2pN is called an N-tuple. Our primary interest is going to be the case where each set is the set of real numbers. 73 74 CHAPTER 3. METRIC SPACES AND SOME BASIC TOPOLOGY De¿nition 3.1.2 Real n-space,denotedUn, is the set all ordered n-tuples of real numbers i.e., n U x1 x2 xn : x1 x2 xn + U . Un U U U U Thus, _ ^] `, the Cartesian product of with itself n times. nofthem Remark 3.1.3 From MAT108, recall the de¿nition of an ordered pair: a b a a b . def This de¿nition leads to the more familiar statement that a b c d if and only if a bandc d. -
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. -
Appendix: Sites for Topoi
Appendix: Sites for Topoi A Grothendieck topos was defined in Chapter III to be a category of sheaves on a small site---or a category equivalent to such a sheaf cate gory. For a given Grothendieck topos [; there are many sites C for which [; will be equivalent to the category of sheaves on C. There is usually no way of selecting a best or canonical such site. This Appendix will prove a theorem by Giraud, which provides conditions characterizing a Grothendieck topos, without any reference to a particular site. Gi raud's theorem depends on certain exactness properties which hold for colimits in any (cocomplete) topos, but not in more general co complete categories. Given these properties, the construction of a site for topos [; will use a generating set of objects and the Hom-tensor adjunction. The final section of this Appendix will apply Giraud's theorem to the comparison of different sites for a Grothendieck topos. 1. Exactness Conditions In this section we consider a category [; which has all finite limits and all small colimits. As always, such colimits may be expressed in terms of coproducts and coequalizers. We first discuss some special properties enjoyed by colimits in a topos. Coproducts. Let E = It, Ea be a coproduct of a family of objects Ea in [;, with the coproduct inclusions ia: Ea -> E. This coproduct is said to be disjoint when every ia is mono and for every 0: =I- (3 the pullback Ea XE E{3 is the initial object in [;. Thus in the category Sets the coproduct, often described as the disjoint union, is disjoint in this sense. -
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. -
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. -
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. -
Topology: the Journey Into Separation Axioms
TOPOLOGY: THE JOURNEY INTO SEPARATION AXIOMS VIPUL NAIK Abstract. In this journey, we are going to explore the so called “separation axioms” in greater detail. We shall try to understand how these axioms are affected on going to subspaces, taking products, and looking at small open neighbourhoods. 1. What this journey entails 1.1. Prerequisites. Familiarity with definitions of these basic terms is expected: • Topological space • Open sets, closed sets, and limit points • Basis and subbasis • Continuous function and homeomorphism • Product topology • Subspace topology The target audience for this article are students doing a first course in topology. 1.2. The explicit promise. At the end of this journey, the learner should be able to: • Define the following: T0, T1, T2 (Hausdorff), T3 (regular), T4 (normal) • Understand how these properties are affected on taking subspaces, products and other similar constructions 2. What are separation axioms? 2.1. The idea behind separation. The defining attributes of a topological space (in terms of a family of open subsets) does little to guarantee that the points in the topological space are somehow distinct or far apart. The topological spaces that we would like to study, on the other hand, usually have these two features: • Any two points can be separated, that is, they are, to an extent, far apart. • Every point can be approached very closely from other points, and if we take a sequence of points, they will usually get to cluster around a point. On the face of it, the above two statements do not seem to reconcile each other. In fact, topological spaces become interesting precisely because they are nice in both the above ways. -
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.