What Is the Fundamental Group?
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The Fundamental Group
The Fundamental Group Tyrone Cutler July 9, 2020 Contents 1 Where do Homotopy Groups Come From? 1 2 The Fundamental Group 3 3 Methods of Computation 8 3.1 Covering Spaces . 8 3.2 The Seifert-van Kampen Theorem . 10 1 Where do Homotopy Groups Come From? 0 Working in the based category T op∗, a `point' of a space X is a map S ! X. Unfortunately, 0 the set T op∗(S ;X) of points of X determines no topological information about the space. The same is true in the homotopy category. The set of `points' of X in this case is the set 0 π0X = [S ;X] = [∗;X]0 (1.1) of its path components. As expected, this pointed set is a very coarse invariant of the pointed homotopy type of X. How might we squeeze out some more useful information from it? 0 One approach is to back up a step and return to the set T op∗(S ;X) before quotienting out the homotopy relation. As we saw in the first lecture, there is extra information in this set in the form of track homotopies which is discarded upon passage to [S0;X]. Recall our slogan: it matters not only that a map is null homotopic, but also the manner in which it becomes so. So, taking a cue from algebraic geometry, let us try to understand the automorphism group of the zero map S0 ! ∗ ! X with regards to this extra structure. If we vary the basepoint of X across all its points, maybe it could be possible to detect information not visible on the level of π0. -
[Math.AT] 4 Sep 2003 and H Uhri Ebro DE Eerhtann Ewr HPRN-C Network Programme
ON RATIONAL HOMOTOPY OF FOUR-MANIFOLDS S. TERZIC´ Abstract. We give explicit formulas for the ranks of the third and fourth homotopy groups of all oriented closed simply con- nected four-manifolds in terms of their second Betti numbers. We also show that the rational homotopy type of these manifolds is classified by their rank and signature. 1. Introduction In this paper we consider the problem of computation of the rational homotopy groups and the problem of rational homotopy classification of simply connected closed four-manifolds. Our main results could be collected as follows. Theorem 1. Let M be a closed oriented simply connected four-manifold and b2 its second Betti number. Then: (1) If b2 =0 then rk π4(M)=rk π7(M)=1 and πp(M) is finite for p =46 , 7 , (2) If b2 =1 then rk π2(M)=rk π5(M)=1 and πp(M) is finite for p =26 , 5 , (3) If b2 =2 then rk π2(M)=rk π3(M)=2 and πp(M) is finite for p =26 , 3 , (4) If b2 > 2 then dim π∗(M) ⊗ Q = ∞ and b (b + 1) b (b2 − 4) rk π (M)= b , rk π (M)= 2 2 − 1, rk π (M)= 2 2 . 2 2 3 2 4 3 arXiv:math/0309076v1 [math.AT] 4 Sep 2003 When the second Betti number is 3, we can prove a little more. Proposition 2. If b2 =3 then rk π5(M)=10. Regarding rational homotopy type classification of simply connected closed four-manifolds, we obtain the following. Date: November 21, 2018; MSC 53C25, 57R57, 58A14, 57R17. -
The Calabi Complex and Killing Sheaf Cohomology
The Calabi complex and Killing sheaf cohomology Igor Khavkine Department of Mathematics, University of Trento, and TIFPA-INFN, Trento, I{38123 Povo (TN) Italy [email protected] September 26, 2014 Abstract It has recently been noticed that the degeneracies of the Poisson bra- cket of linearized gravity on constant curvature Lorentzian manifold can be described in terms of the cohomologies of a certain complex of dif- ferential operators. This complex was first introduced by Calabi and its cohomology is known to be isomorphic to that of the (locally constant) sheaf of Killing vectors. We review the structure of the Calabi complex in a novel way, with explicit calculations based on representation theory of GL(n), and also some tools for studying its cohomology in terms of of lo- cally constant sheaves. We also conjecture how these tools would adapt to linearized gravity on other backgrounds and to other gauge theories. The presentation includes explicit formulas for the differential operators in the Calabi complex, arguments for its local exactness, discussion of general- ized Poincar´eduality, methods of computing the cohomology of locally constant sheaves, and example calculations of Killing sheaf cohomologies of some black hole and cosmological Lorentzian manifolds. Contents 1 Introduction2 2 The Calabi complex4 2.1 Tensor bundles and Young symmetrizers..............5 2.2 Differential operators.........................7 2.3 Formal adjoint complex....................... 11 2.4 Equations of finite type, twisted de Rham complex........ 14 3 Cohomology of locally constant sheaves 16 3.1 Locally constant sheaves....................... 16 3.2 Acyclic resolution by a differential complex............ 18 3.3 Generalized Poincar´eduality................... -
Sheaf Theory
Sheaf Theory Anne Vaugon December 20, 2013 The goals of this talk are • to define a generalization denoted by RΓ(F) of de Rham cohomology; • to explain the notation RΓ(F) (here F is a sheaf and RΓ is a derived functor). 1 Presheaves and sheaves 1.1 Definitions and examples Let X be a topological space. Definition 1.1. A presheaf of k-modules F on X is defined by the following data: • a k-module F(U) for each open set U of X; • a map rUV : F(U) → F(V ) for each pair V ⊂ U of open subsets such that – rWV ◦ rVU = rWU for all open subsets W ⊂ V ⊂ U; – rUU = Id for all open subsets U. Therefore, a presheaf is a functor from the opposite category of open sets to the category of k-modules. If F is a presheaf, F(U) is called the set of sections of U and rVU the restriction from U to V . Definition 1.2. A presheaf F is a sheaf if • for any family (Ui)i∈I of open subsets of X • for any family of elements si ∈ F(Ui) such that rUi∩Uj ,Ui (si) = rUi∩Uj ,Uj (sj) for all i, j ∈ I there exists a unique s ∈ F(U) where U = ∪i∈I Ui such that rUi,U (s) = si for all i ∈ I. This means that we can extend a locally defined section. Definition 1.3. A morphism of presheaves f : F → G is a natural trans- formation between the functors F and G: for each open set U, there exists a morphism f(U): F(U) → G(U) such that the following diagram is commutative for V ⊂ U. -
A TEXTBOOK of TOPOLOGY Lltld
SEIFERT AND THRELFALL: A TEXTBOOK OF TOPOLOGY lltld SEI FER T: 7'0PO 1.OG 1' 0 I.' 3- Dl M E N SI 0 N A I. FIRERED SPACES This is a volume in PURE AND APPLIED MATHEMATICS A Series of Monographs and Textbooks Editors: SAMUELEILENBERG AND HYMANBASS A list of recent titles in this series appears at the end of this volunie. SEIFERT AND THRELFALL: A TEXTBOOK OF TOPOLOGY H. SEIFERT and W. THRELFALL Translated by Michael A. Goldman und S E I FE R T: TOPOLOGY OF 3-DIMENSIONAL FIBERED SPACES H. SEIFERT Translated by Wolfgang Heil Edited by Joan S. Birman and Julian Eisner @ 1980 ACADEMIC PRESS A Subsidiary of Harcourr Brace Jovanovich, Publishers NEW YORK LONDON TORONTO SYDNEY SAN FRANCISCO COPYRIGHT@ 1980, BY ACADEMICPRESS, INC. ALL RIGHTS RESERVED. NO PART OF THIS PUBLICATION MAY BE REPRODUCED OR TRANSMITTED IN ANY FORM OR BY ANY MEANS, ELECTRONIC OR MECHANICAL, INCLUDING PHOTOCOPY, RECORDING, OR ANY INFORMATION STORAGE AND RETRIEVAL SYSTEM, WITHOUT PERMISSION IN WRITING FROM THE PUBLISHER. ACADEMIC PRESS, INC. 11 1 Fifth Avenue, New York. New York 10003 United Kingdom Edition published by ACADEMIC PRESS, INC. (LONDON) LTD. 24/28 Oval Road, London NWI 7DX Mit Genehmigung des Verlager B. G. Teubner, Stuttgart, veranstaltete, akin autorisierte englische Ubersetzung, der deutschen Originalausgdbe. Library of Congress Cataloging in Publication Data Seifert, Herbert, 1897- Seifert and Threlfall: A textbook of topology. Seifert: Topology of 3-dimensional fibered spaces. (Pure and applied mathematics, a series of mono- graphs and textbooks ; ) Translation of Lehrbuch der Topologic. Bibliography: p. Includes index. 1. -
Picard Groupoids and $\Gamma $-Categories
PICARD GROUPOIDS AND Γ-CATEGORIES AMIT SHARMA Abstract. In this paper we construct a symmetric monoidal closed model category of coherently commutative Picard groupoids. We construct another model category structure on the category of (small) permutative categories whose fibrant objects are (permutative) Picard groupoids. The main result is that the Segal’s nerve functor induces a Quillen equivalence between the two aforementioned model categories. Our main result implies the classical result that Picard groupoids model stable homotopy one-types. Contents 1. Introduction 2 2. The Setup 4 2.1. Review of Permutative categories 4 2.2. Review of Γ- categories 6 2.3. The model category structure of groupoids on Cat 7 3. Two model category structures on Perm 12 3.1. ThemodelcategorystructureofPermutativegroupoids 12 3.2. ThemodelcategoryofPicardgroupoids 15 4. The model category of coherently commutatve monoidal groupoids 20 4.1. The model category of coherently commutative monoidal groupoids 24 5. Coherently commutative Picard groupoids 27 6. The Quillen equivalences 30 7. Stable homotopy one-types 36 Appendix A. Some constructions on categories 40 AppendixB. Monoidalmodelcategories 42 Appendix C. Localization in model categories 43 Appendix D. Tranfer model structure on locally presentable categories 46 References 47 arXiv:2002.05811v2 [math.CT] 12 Mar 2020 Date: Dec. 14, 2019. 1 2 A. SHARMA 1. Introduction Picard groupoids are interesting objects both in topology and algebra. A major reason for interest in topology is because they classify stable homotopy 1-types which is a classical result appearing in various parts of the literature [JO12][Pat12][GK11]. The category of Picard groupoids is the archetype exam- ple of a 2-Abelian category, see [Dup08]. -
3-Manifold Groups
3-Manifold Groups Matthias Aschenbrenner Stefan Friedl Henry Wilton University of California, Los Angeles, California, USA E-mail address: [email protected] Fakultat¨ fur¨ Mathematik, Universitat¨ Regensburg, Germany E-mail address: [email protected] Department of Pure Mathematics and Mathematical Statistics, Cam- bridge University, United Kingdom E-mail address: [email protected] Abstract. We summarize properties of 3-manifold groups, with a particular focus on the consequences of the recent results of Ian Agol, Jeremy Kahn, Vladimir Markovic and Dani Wise. Contents Introduction 1 Chapter 1. Decomposition Theorems 7 1.1. Topological and smooth 3-manifolds 7 1.2. The Prime Decomposition Theorem 8 1.3. The Loop Theorem and the Sphere Theorem 9 1.4. Preliminary observations about 3-manifold groups 10 1.5. Seifert fibered manifolds 11 1.6. The JSJ-Decomposition Theorem 14 1.7. The Geometrization Theorem 16 1.8. Geometric 3-manifolds 20 1.9. The Geometric Decomposition Theorem 21 1.10. The Geometrization Theorem for fibered 3-manifolds 24 1.11. 3-manifolds with (virtually) solvable fundamental group 26 Chapter 2. The Classification of 3-Manifolds by their Fundamental Groups 29 2.1. Closed 3-manifolds and fundamental groups 29 2.2. Peripheral structures and 3-manifolds with boundary 31 2.3. Submanifolds and subgroups 32 2.4. Properties of 3-manifolds and their fundamental groups 32 2.5. Centralizers 35 Chapter 3. 3-manifold groups after Geometrization 41 3.1. Definitions and conventions 42 3.2. Justifications 45 3.3. Additional results and implications 59 Chapter 4. The Work of Agol, Kahn{Markovic, and Wise 63 4.1. -
Lecture 2: Spaces of Maps, Loop Spaces and Reduced Suspension
LECTURE 2: SPACES OF MAPS, LOOP SPACES AND REDUCED SUSPENSION In this section we will give the important constructions of loop spaces and reduced suspensions associated to pointed spaces. For this purpose there will be a short digression on spaces of maps between (pointed) spaces and the relevant topologies. To be a bit more specific, one aim is to see that given a pointed space (X; x0), then there is an entire pointed space of loops in X. In order to obtain such a loop space Ω(X; x0) 2 Top∗; we have to specify an underlying set, choose a base point, and construct a topology on it. The underlying set of Ω(X; x0) is just given by the set of maps 1 Top∗((S ; ∗); (X; x0)): A base point is also easily found by considering the constant loop κx0 at x0 defined by: 1 κx0 :(S ; ∗) ! (X; x0): t 7! x0 The topology which we will consider on this set is a special case of the so-called compact-open topology. We begin by introducing this topology in a more general context. 1. Function spaces Let K be a compact Hausdorff space, and let X be an arbitrary space. The set Top(K; X) of continuous maps K ! X carries a natural topology, called the compact-open topology. It has a subbasis formed by the sets of the form B(T;U) = ff : K ! X j f(T ) ⊆ Ug where T ⊆ K is compact and U ⊆ X is open. Thus, for a map f : K ! X, one can form a typical basis open neighborhood by choosing compact subsets T1;:::;Tn ⊆ K and small open sets Ui ⊆ X with f(Ti) ⊆ Ui to get a neighborhood Of of f, Of = B(T1;U1) \ ::: \ B(Tn;Un): One can even choose the Ti to cover K, so as to `control' the behavior of functions g 2 Of on all of K. -
Riemann Mapping Theorem
Riemann surfaces, lecture 8 M. Verbitsky Riemann surfaces lecture 7: Riemann mapping theorem Misha Verbitsky Universit´eLibre de Bruxelles December 8, 2015 1 Riemann surfaces, lecture 8 M. Verbitsky Riemannian manifolds (reminder) DEFINITION: Let h 2 Sym2 T ∗M be a symmetric 2-form on a manifold which satisfies h(x; x) > 0 for any non-zero tangent vector x. Then h is called Riemannian metric, of Riemannian structure, and (M; h) Riemannian manifold. DEFINITION: For any x:y 2 M, and any path γ :[a; b] −! M connecting R dγ dγ x and y, consider the length of γ defined as L(γ) = γ j dt jdt, where j dt j = dγ dγ 1=2 h( dt ; dt ) . Define the geodesic distance as d(x; y) = infγ L(γ), where infimum is taken for all paths connecting x and y. EXERCISE: Prove that the geodesic distance satisfies triangle inequality and defines metric on M. EXERCISE: Prove that this metric induces the standard topology on M. n P 2 EXAMPLE: Let M = R , h = i dxi . Prove that the geodesic distance coincides with d(x; y) = jx − yj. EXERCISE: Using partition of unity, prove that any manifold admits a Riemannian structure. 2 Riemann surfaces, lecture 8 M. Verbitsky Conformal structures and almost complex structures (reminder) REMARK: The following theorem implies that almost complex structures on a 2-dimensional oriented manifold are equivalent to conformal structures. THEOREM: Let M be a 2-dimensional oriented manifold. Given a complex structure I, let ν be the conformal class of its Hermitian metric. Then ν is determined by I, and it determines I uniquely. -
Remarks on the Cohomology of Finite Fundamental Groups of 3–Manifolds
Geometry & Topology Monographs 14 (2008) 519–556 519 arXiv version: fonts, pagination and layout may vary from GTM published version Remarks on the cohomology of finite fundamental groups of 3–manifolds SATOSHI TOMODA PETER ZVENGROWSKI Computations based on explicit 4–periodic resolutions are given for the cohomology of the finite groups G known to act freely on S3 , as well as the cohomology rings of the associated 3–manifolds (spherical space forms) M = S3=G. Chain approximations to the diagonal are constructed, and explicit contracting homotopies also constructed for the cases G is a generalized quaternion group, the binary tetrahedral group, or the binary octahedral group. Some applications are briefly discussed. 57M05, 57M60; 20J06 1 Introduction The structure of the cohomology rings of 3–manifolds is an area to which Heiner Zieschang devoted much work and energy, especially from 1993 onwards. This could be considered as part of a larger area of his interest, the degrees of maps between oriented 3– manifolds, especially the existence of degree one maps, which in turn have applications in unexpected areas such as relativity theory (cf Shastri, Williams and Zvengrowski [41] and Shastri and Zvengrowski [42]). References [1,6,7, 18, 19, 20, 21, 22, 23] in this paper, all involving work of Zieschang, his students Aaslepp, Drawe, Sczesny, and various colleagues, attest to his enthusiasm for these topics and the remarkable energy he expended studying them. Much of this work involved Seifert manifolds, in particular, references [1, 6, 7, 18, 20, 23]. Of these, [6, 7, 23] (together with [8, 9]) successfully completed the programme of computing the ring structure H∗(M) for any orientable Seifert manifold M with 1 2 3 3 G := π1(M) infinite. -
Rational Homotopy Theory: a Brief Introduction
Contemporary Mathematics Rational Homotopy Theory: A Brief Introduction Kathryn Hess Abstract. These notes contain a brief introduction to rational homotopy theory: its model category foundations, the Sullivan model and interactions with the theory of local commutative rings. Introduction This overview of rational homotopy theory consists of an extended version of lecture notes from a minicourse based primarily on the encyclopedic text [18] of F´elix, Halperin and Thomas. With only three hours to devote to such a broad and rich subject, it was difficult to choose among the numerous possible topics to present. Based on the subjects covered in the first week of this summer school, I decided that the goal of this course should be to establish carefully the founda- tions of rational homotopy theory, then to treat more superficially one of its most important tools, the Sullivan model. Finally, I provided a brief summary of the ex- tremely fruitful interactions between rational homotopy theory and local algebra, in the spirit of the summer school theme “Interactions between Homotopy Theory and Algebra.” I hoped to motivate the students to delve more deeply into the subject themselves, while providing them with a solid enough background to do so with relative ease. As these lecture notes do not constitute a history of rational homotopy theory, I have chosen to refer the reader to [18], instead of to the original papers, for the proofs of almost all of the results cited, at least in Sections 1 and 2. The reader interested in proper attributions will find them in [18] or [24]. The author would like to thank Luchezar Avramov and Srikanth Iyengar, as well as the anonymous referee, for their helpful comments on an earlier version of this article. -
Fibrations I
Fibrations I Tyrone Cutler May 23, 2020 Contents 1 Fibrations 1 2 The Mapping Path Space 5 3 Mapping Spaces and Fibrations 9 4 Exercises 11 1 Fibrations In the exercises we used the extension problem to motivate the study of cofibrations. The idea was to allow for homotopy-theoretic methods to be introduced to an otherwise very rigid problem. The dual notion is the lifting problem. Here p : E ! B is a fixed map and we would like to known when a given map f : X ! B lifts through p to a map into E E (1.1) |> | p | | f X / B: Asking for the lift to make the diagram to commute strictly is neither useful nor necessary from our point of view. Rather it is more natural for us to ask that the lift exist up to homotopy. In this lecture we work in the unpointed category and obtain the correct conditions on the map p by formally dualising the conditions for a map to be a cofibration. Definition 1 A map p : E ! B is said to have the homotopy lifting property (HLP) with respect to a space X if for each pair of a map f : X ! E, and a homotopy H : X×I ! B starting at H0 = pf, there exists a homotopy He : X × I ! E such that , 1) He0 = f 2) pHe = H. The map p is said to be a (Hurewicz) fibration if it has the homotopy lifting property with respect to all spaces. 1 Since a diagram is often easier to digest, here is the definition exactly as stated above f X / E x; He x in0 x p (1.2) x x H X × I / B and also in its equivalent adjoint formulation X B H B He B B p∗ EI / BI (1.3) f e0 e0 # p E / B: The assertion that p is a fibration is the statement that the square in the second diagram is a weak pullback.