Fundamental Groups of Aspherical Manifolds and Maps of Non-Zero Degree
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Abstract Algebra
Abstract Algebra Paul Melvin Bryn Mawr College Fall 2011 lecture notes loosely based on Dummit and Foote's text Abstract Algebra (3rd ed) Prerequisite: Linear Algebra (203) 1 Introduction Pure Mathematics Algebra Analysis Foundations (set theory/logic) G eometry & Topology What is Algebra? • Number systems N = f1; 2; 3;::: g \natural numbers" Z = f:::; −1; 0; 1; 2;::: g \integers" Q = ffractionsg \rational numbers" R = fdecimalsg = pts on the line \real numbers" p C = fa + bi j a; b 2 R; i = −1g = pts in the plane \complex nos" k polar form re iθ, where a = r cos θ; b = r sin θ a + bi b r θ a p Note N ⊂ Z ⊂ Q ⊂ R ⊂ C (all proper inclusions, e.g. 2 62 Q; exercise) There are many other important number systems inside C. 2 • Structure \binary operations" + and · associative, commutative, and distributive properties \identity elements" 0 and 1 for + and · resp. 2 solve equations, e.g. 1 ax + bx + c = 0 has two (complex) solutions i p −b ± b2 − 4ac x = 2a 2 2 2 2 x + y = z has infinitely many solutions, even in N (thei \Pythagorian triples": (3,4,5), (5,12,13), . ). n n n 3 x + y = z has no solutions x; y; z 2 N for any fixed n ≥ 3 (Fermat'si Last Theorem, proved in 1995 by Andrew Wiles; we'll give a proof for n = 3 at end of semester). • Abstract systems groups, rings, fields, vector spaces, modules, . A group is a set G with an associative binary operation ∗ which has an identity element e (x ∗ e = x = e ∗ x for all x 2 G) and inverses for each of its elements (8 x 2 G; 9 y 2 G such that x ∗ y = y ∗ x = e). -
SUMMARY of PART II: GROUPS 1. Motivation and Overview 1.1. Why
SUMMARY OF PART II: GROUPS 1. Motivation and overview 1.1. Why study groups? The group concept is truly fundamental not only for algebra, but for mathematics in general, as groups appear in mathematical theories as diverse as number theory (e.g. the solutions of Diophantine equations often form a group), Galois theory (the solutions(=roots) of a polynomial equation may satisfy hidden symmetries which can be put together into a group), geometry (e.g. the isometries of a given geometric space or object form a group) or topology (e.g. an important tool is the fundamental group of a topological space), but also in physics (e.g. the Lorentz group which in concerned with the symmetries of space-time in relativity theory, or the “gauge” symmetry group of the famous standard model). Our task for the course is to understand whole classes of groups—mostly we will concentrate on finite groups which are already very difficult to classify. Our main examples for these shall be the cyclic groups Cn, symmetric groups Sn (on n letters), the alternating groups An and the dihedral groups Dn. The most “fundamental” of these are the symmetric groups, as every finite group can be embedded into a certain finite symmetric group (Cayley’s Theorem). We will be able to classify all groups of order 2p and p2, where p is a prime. We will also find structure results on subgroups which exist for a given such group (Cauchy’s Theorem, Sylow Theorems). Finally, abelian groups can be controlled far easier than general (i.e., possibly non-abelian) groups, and we will give a full classification for all such abelian groups, at least when they can be generated by finitely many elements. -
Floer Homology, Gauge Theory, and Low-Dimensional Topology
Floer Homology, Gauge Theory, and Low-Dimensional Topology Clay Mathematics Proceedings Volume 5 Floer Homology, Gauge Theory, and Low-Dimensional Topology Proceedings of the Clay Mathematics Institute 2004 Summer School Alfréd Rényi Institute of Mathematics Budapest, Hungary June 5–26, 2004 David A. Ellwood Peter S. Ozsváth András I. Stipsicz Zoltán Szabó Editors American Mathematical Society Clay Mathematics Institute 2000 Mathematics Subject Classification. Primary 57R17, 57R55, 57R57, 57R58, 53D05, 53D40, 57M27, 14J26. The cover illustrates a Kinoshita-Terasaka knot (a knot with trivial Alexander polyno- mial), and two Kauffman states. These states represent the two generators of the Heegaard Floer homology of the knot in its topmost filtration level. The fact that these elements are homologically non-trivial can be used to show that the Seifert genus of this knot is two, a result first proved by David Gabai. Library of Congress Cataloging-in-Publication Data Clay Mathematics Institute. Summer School (2004 : Budapest, Hungary) Floer homology, gauge theory, and low-dimensional topology : proceedings of the Clay Mathe- matics Institute 2004 Summer School, Alfr´ed R´enyi Institute of Mathematics, Budapest, Hungary, June 5–26, 2004 / David A. Ellwood ...[et al.], editors. p. cm. — (Clay mathematics proceedings, ISSN 1534-6455 ; v. 5) ISBN 0-8218-3845-8 (alk. paper) 1. Low-dimensional topology—Congresses. 2. Symplectic geometry—Congresses. 3. Homol- ogy theory—Congresses. 4. Gauge fields (Physics)—Congresses. I. Ellwood, D. (David), 1966– II. Title. III. Series. QA612.14.C55 2004 514.22—dc22 2006042815 Copying and reprinting. Material in this book may be reproduced by any means for educa- tional and scientific purposes without fee or permission with the exception of reproduction by ser- vices that collect fees for delivery of documents and provided that the customary acknowledgment of the source is given. -
Commentary on Thurston's Work on Foliations
COMMENTARY ON FOLIATIONS* Quoting Thurston's definition of foliation [F11]. \Given a large supply of some sort of fabric, what kinds of manifolds can be made from it, in a way that the patterns match up along the seams? This is a very general question, which has been studied by diverse means in differential topology and differential geometry. ... A foliation is a manifold made out of striped fabric - with infintely thin stripes, having no space between them. The complete stripes, or leaves, of the foliation are submanifolds; if the leaves have codimension k, the foliation is called a codimension k foliation. In order that a manifold admit a codimension- k foliation, it must have a plane field of dimension (n − k)." Such a foliation is called an (n − k)-dimensional foliation. The first definitive result in the subject, the so called Frobenius integrability theorem [Fr], concerns a necessary and sufficient condition for a plane field to be the tangent field of a foliation. See [Spi] Chapter 6 for a modern treatment. As Frobenius himself notes [Sa], a first proof was given by Deahna [De]. While this work was published in 1840, it took another hundred years before a geometric/topological theory of foliations was introduced. This was pioneered by Ehresmann and Reeb in a series of Comptes Rendus papers starting with [ER] that was quickly followed by Reeb's foundational 1948 thesis [Re1]. See Haefliger [Ha4] for a detailed account of developments in this period. Reeb [Re1] himself notes that the 1-dimensional theory had already undergone considerable development through the work of Poincare [P], Bendixson [Be], Kaplan [Ka] and others. -
Classification of 3-Manifolds with Certain Spines*1 )
TRANSACTIONS OF THE AMERICAN MATHEMATICAL SOCIETY Volume 205, 1975 CLASSIFICATIONOF 3-MANIFOLDSWITH CERTAIN SPINES*1 ) BY RICHARD S. STEVENS ABSTRACT. Given the group presentation <p= (a, b\ambn, apbq) With m, n, p, q & 0, we construct the corresponding 2-complex Ky. We prove the following theorems. THEOREM 7. Jf isa spine of a closed orientable 3-manifold if and only if (i) \m\ = \p\ = 1 or \n\ = \q\ = 1, or (") (m, p) = (n, q) = 1. Further, if (ii) holds but (i) does not, then the manifold is unique. THEOREM 10. If M is a closed orientable 3-manifold having K^ as a spine and \ = \mq — np\ then M is a lens space L\ % where (\,fc) = 1 except when X = 0 in which case M = S2 X S1. It is well known that every connected compact orientable 3-manifold with or without boundary has a spine that is a 2-complex with a single vertex. Such 2-complexes correspond very naturally to group presentations, the 1-cells corre- sponding to generators and the 2-cells corresponding to relators. In the case of a closed orientable 3-manifold, there are equally many 1-cells and 2-cells in the spine, i.e., equally many generators and relators in the corresponding presentation. Given a group presentation one is motivated to ask the following questions: (1) Is the corresponding 2-complex a spine of a compact orientable 3-manifold? (2) If there are equally many generators and relators, is the 2-complex a spine of a closed orientable 3-manifold? (3) Can we say what manifold(s) have the 2-complex as a spine? L. -
Manifolds: Where Do We Come From? What Are We? Where Are We Going
Manifolds: Where Do We Come From? What Are We? Where Are We Going Misha Gromov September 13, 2010 Contents 1 Ideas and Definitions. 2 2 Homotopies and Obstructions. 4 3 Generic Pullbacks. 9 4 Duality and the Signature. 12 5 The Signature and Bordisms. 25 6 Exotic Spheres. 36 7 Isotopies and Intersections. 39 8 Handles and h-Cobordisms. 46 9 Manifolds under Surgery. 49 1 10 Elliptic Wings and Parabolic Flows. 53 11 Crystals, Liposomes and Drosophila. 58 12 Acknowledgments. 63 13 Bibliography. 63 Abstract Descendants of algebraic kingdoms of high dimensions, enchanted by the magic of Thurston and Donaldson, lost in the whirlpools of the Ricci flow, topologists dream of an ideal land of manifolds { perfect crystals of mathematical structure which would capture our vague mental images of geometric spaces. We browse through the ideas inherited from the past hoping to penetrate through the fog which conceals the future. 1 Ideas and Definitions. We are fascinated by knots and links. Where does this feeling of beauty and mystery come from? To get a glimpse at the answer let us move by 25 million years in time. 25 106 is, roughly, what separates us from orangutans: 12 million years to our common ancestor on the phylogenetic tree and then 12 million years back by another× branch of the tree to the present day orangutans. But are there topologists among orangutans? Yes, there definitely are: many orangutans are good at "proving" the triv- iality of elaborate knots, e.g. they fast master the art of untying boats from their mooring when they fancy taking rides downstream in a river, much to the annoyance of people making these knots with a different purpose in mind. -
The Classical Matrix Groups 1 Groups
The Classical Matrix Groups CDs 270, Spring 2010/2011 The notes provide a brief review of matrix groups. The primary goal is to motivate the lan- guage and symbols used to represent rotations (SO(2) and SO(3)) and spatial displacements (SE(2) and SE(3)). 1 Groups A group, G, is a mathematical structure with the following characteristics and properties: i. the group consists of a set of elements {gj} which can be indexed. The indices j may form a finite, countably infinite, or continous (uncountably infinite) set. ii. An associative binary group operation, denoted by 0 ∗0 , termed the group product. The product of two group elements is also a group element: ∀ gi, gj ∈ G gi ∗ gj = gk, where gk ∈ G. iii. A unique group identify element, e, with the property that: e ∗ gj = gj for all gj ∈ G. −1 iv. For every gj ∈ G, there must exist an inverse element, gj , such that −1 gj ∗ gj = e. Simple examples of groups include the integers, Z, with addition as the group operation, and the real numbers mod zero, R − {0}, with multiplication as the group operation. 1.1 The General Linear Group, GL(N) The set of all N × N invertible matrices with the group operation of matrix multiplication forms the General Linear Group of dimension N. This group is denoted by the symbol GL(N), or GL(N, K) where K is a field, such as R, C, etc. Generally, we will only consider the cases where K = R or K = C, which are respectively denoted by GL(N, R) and GL(N, C). -
Boundary Volume and Length Spectra of Riemannian Manifolds: What the Middle Degree Hodge Spectrum Doesn’T Reveal Tome 53, No 7 (2003), P
R AN IE N R A U L E O S F D T E U L T I ’ I T N S ANNALES DE L’INSTITUT FOURIER Carolyn S. GORDON & Juan Pablo ROSSETTI Boundary volume and length spectra of Riemannian manifolds: what the middle degree Hodge spectrum doesn’t reveal Tome 53, no 7 (2003), p. 2297-2314. <http://aif.cedram.org/item?id=AIF_2003__53_7_2297_0> © Association des Annales de l’institut Fourier, 2003, tous droits réservés. L’accès aux articles de la revue « Annales de l’institut Fourier » (http://aif.cedram.org/), implique l’accord avec les conditions générales d’utilisation (http://aif.cedram.org/legal/). Toute re- production en tout ou partie cet article sous quelque forme que ce soit pour tout usage autre que l’utilisation à fin strictement per- sonnelle du copiste est constitutive d’une infraction pénale. Toute copie ou impression de ce fichier doit contenir la présente mention de copyright. cedram Article mis en ligne dans le cadre du Centre de diffusion des revues académiques de mathématiques http://www.cedram.org/ 2297- BOUNDARY VOLUME AND LENGTH SPECTRA OF RIEMANNIAN MANIFOLDS: WHAT THE MIDDLE DEGREE HODGE SPECTRUM DOESN’T REVEAL by C.S. GORDON and J.P. ROSSETTI (1) To what extent does spectral data associated with the Hodge Laplacian dd* + d*d on a compact Riemannian manifold M determine the geometry and topology of M? Let specp (M) denote the spectrum of the Hodge Laplacian acting on the space of p-forms on M, with absolute boundary conditions in case the boundary of M is non-empty. -
Recent Advances in Topological Manifolds
Recent Advances in Topological Manifolds Part III course of A. J. Casson, notes by Andrew Ranicki Cambridge, Lent 1971 Introduction A topological n-manifold is a Hausdorff space which is locally n-Euclidean (like Rn). No progress was made in their study (unlike that in PL and differentiable manifolds) until 1968 when Kirby, Siebenmann and Wall solved most questions for high dimensional manifolds (at least as much as for the PL and differentiable cases). Question: can compact n-manifolds be triangulated? Yes, if n 6 3 (Moise 1950's). This is unknown in general. However, there exist manifolds (of dimension > 5) which don't have PL structures. (They might still have triangulations in which links of simplices aren't PL spheres.) There is machinery for deciding whether manifolds of di- mension > 5 have a PL structure. Not much is known about 4-manifolds in the topological, differentiable, and PL cases. n n+1 Question 2: the generalized Sch¨onfliestheorem. Let B = x 2 R : kxk 6 1 , n n+1 n n S = x 2 R : kxk = 1 . Given an embedding f : B ! S (i.e. a 1-1 con- tinuous map), is Sn n f(Bn) =∼ Bn? No{the Alexander horned sphere. n n+1 0 n n ∼ n Let λB = x 2 R : kxk 6 λ . Question 2 : is S n f(λB ) = B (where 0 < λ < 1)? Yes. In 1960, Morton Brown, Mazur, and Morse proved the following: if g : Sn−1× n n n−1 [−1; 1] ! S is an embedding, then S ng(S ×f0g) has 2 components, D1;D2, ∼ ∼ n 0 such that D1 = D2 = B , which implies 2 as a corollary. -
Notes on Geometry and Topology
Lecture Notes on Geometry and Topology Kevin Zhou [email protected] These notes cover geometry and topology in physics. They focus on how the mathematics is applied, in the context of particle physics and condensed matter, with little emphasis on rigorous proofs. For instance, no point-set topology is developed or assumed. The primary sources were: • Nakahara, Geometry, Topology, and Physics. The standard textbook on the subject for physi- cists. Covers the usual material (simplicial homology, homotopy groups, de Rham cohomology, bundles), with extra chapters on advanced subjects like characteristic classes and index theo- rems. The material is developed clearly, but there are many errata, and the most comprehensive list is available here. At MIT I co-led an undergraduate reading group on this book with Matt DeCross, who wrote problem sets available here. • Robert Littlejon's Physics 250 notes. These notes primarily follow Nakahara, with some extra physical applications. They are generally more careful and precise. • Nash and Sen, Topology and Geometry for Physicists. A shorter alternative to Nakahara which covers the usual material from a slightly more mathematical perspective. For instance, topological spaces are defined, and excision and long exact sequences are used. However, many propositions are left unproven, and some purported proofs are invalid. • Schutz, Geometrical Methods of Mathematical Physics. A basic introduction to differential geometry that focuses on differential forms. • Baez, Gauge Fields, Knots, and Gravity. Covers differential geometry and fiber bundles as applied in gauge theory. Like Nash and Sen, it has a \math-style" presentation, but not rigorous proofs. Also contains neat applications to Chern-Simons theory and knot theory. -
Group Theory
Group theory March 7, 2016 Nearly all of the central symmetries of modern physics are group symmetries, for simple a reason. If we imagine a transformation of our fields or coordinates, we can look at linear versions of those transformations. Such linear transformations may be represented by matrices, and therefore (as we shall see) even finite transformations may be given a matrix representation. But matrix multiplication has an important property: associativity. We get a group if we couple this property with three further simple observations: (1) we expect two transformations to combine in such a way as to give another allowed transformation, (2) the identity may always be regarded as a null transformation, and (3) any transformation that we can do we can also undo. These four properties (associativity, closure, identity, and inverses) are the defining properties of a group. 1 Finite groups Define: A group is a pair G = fS; ◦} where S is a set and ◦ is an operation mapping pairs of elements in S to elements in S (i.e., ◦ : S × S ! S: This implies closure) and satisfying the following conditions: 1. Existence of an identity: 9 e 2 S such that e ◦ a = a ◦ e = a; 8a 2 S: 2. Existence of inverses: 8 a 2 S; 9 a−1 2 S such that a ◦ a−1 = a−1 ◦ a = e: 3. Associativity: 8 a; b; c 2 S; a ◦ (b ◦ c) = (a ◦ b) ◦ c = a ◦ b ◦ c We consider several examples of groups. 1. The simplest group is the familiar boolean one with two elements S = f0; 1g where the operation ◦ is addition modulo two. -
Arxiv:1509.03920V2 [Cond-Mat.Str-El] 10 Mar 2016 I.Smayaddsuso 16 Discussion and Summary VII
Topological Phases on Non-orientable Surfaces: Twisting by Parity Symmetry AtMa P.O. Chan,1 Jeffrey C.Y. Teo,2 and Shinsei Ryu1 1Institute for Condensed Matter Theory and Department of Physics, University of Illinois at Urbana-Champaign, 1110 West Green St, Urbana IL 61801 2Department of Physics, University of Virginia, Charlottesville, VA 22904, USA We discuss (2+1)D topological phases on non-orientable spatial surfaces, such as M¨obius strip, real projective plane and Klein bottle, etc., which are obtained by twisting the parent topological phases by their underlying parity symmetries through introducing parity defects. We construct the ground states on arbitrary non-orientable closed manifolds and calculate the ground state degeneracy. Such degeneracy is shown to be robust against continuous deformation of the underlying manifold. We also study the action of the mapping class group on the multiplet of ground states on the Klein bottle. The physical properties of the topological states on non-orientable surfaces are deeply related to the parity symmetric anyons which do not have a notion of orientation in their statistics. For example, the number of ground states on the real projective plane equals the root of the number of distinguishable parity symmetric anyons, while the ground state degeneracy on the Klein bottle equals the total number of parity symmetric anyons; In deforming the Klein bottle, the Dehn twist encodes the topological spins whereas the Y-homeomorphism tells the particle-hole relation of the parity symmetric anyons. CONTENTS I. INTRODUCTION I. Introduction 1 One of the most striking discoveries in condensed mat- A.Overview 2 ter physics in the last few decades has been topolog- B.Organizationofthepaper 3 ical states of matter1–4, in which the characterization of order goes beyond the paradigm of Landau’s sym- II.