An Introduction to Stable Homotopy Theory
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Algebraic K-Theory and Equivariant Homotopy Theory
Algebraic K-Theory and Equivariant Homotopy Theory Vigleik Angeltveit (Australian National University), Andrew J. Blumberg (University of Texas at Austin), Teena Gerhardt (Michigan State University), Michael Hill (University of Virginia), and Tyler Lawson (University of Minnesota) February 12- February 17, 2012 1 Overview of the Field The study of the algebraic K-theory of rings and schemes has been revolutionized over the past two decades by the development of “trace methods”. Following ideas of Goodwillie, Bokstedt¨ and Bokstedt-Hsiang-¨ Madsen developed topological analogues of Hochschild homology and cyclic homology and a “trace map” out of K-theory that lands in these theories [15, 8, 9]. The fiber of this map can often be understood (by work of McCarthy and Dundas) [27, 13]. Topological Hochschild homology (THH) has a natural circle action, and topological cyclic homology (TC) is relatively computable using the methods of equivariant stable homotopy theory. Starting from Quillen’s computation of the K-theory of finite fields [28], Hesselholt and Madsen used TC to make extensive computations in K-theory [16, 17], in particular verifying certain cases of the Quillen-Lichtenbaum conjecture. As a consequence of these developments, the modern study of algebraic K-theory is deeply intertwined with development of computational tools and foundations in equivariant stable homotopy theory. At the same time, there has been a flurry of renewed interest and activity in equivariant homotopy theory motivated by the nature of the Hill-Hopkins-Ravenel solution to the Kervaire invariant problem [19]. The construction of the norm functor from H-spectra to G-spectra involves exploiting a little-known aspect of the equivariant stable category from a novel perspective, and this has begun to lead to a variety of analyses. -
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. -
Part III 3-Manifolds Lecture Notes C Sarah Rasmussen, 2019
Part III 3-manifolds Lecture Notes c Sarah Rasmussen, 2019 Contents Lecture 0 (not lectured): Preliminaries2 Lecture 1: Why not ≥ 5?9 Lecture 2: Why 3-manifolds? + Intro to Knots and Embeddings 13 Lecture 3: Link Diagrams and Alexander Polynomial Skein Relations 17 Lecture 4: Handle Decompositions from Morse critical points 20 Lecture 5: Handles as Cells; Handle-bodies and Heegard splittings 24 Lecture 6: Handle-bodies and Heegaard Diagrams 28 Lecture 7: Fundamental group presentations from handles and Heegaard Diagrams 36 Lecture 8: Alexander Polynomials from Fundamental Groups 39 Lecture 9: Fox Calculus 43 Lecture 10: Dehn presentations and Kauffman states 48 Lecture 11: Mapping tori and Mapping Class Groups 54 Lecture 12: Nielsen-Thurston Classification for Mapping class groups 58 Lecture 13: Dehn filling 61 Lecture 14: Dehn Surgery 64 Lecture 15: 3-manifolds from Dehn Surgery 68 Lecture 16: Seifert fibered spaces 69 Lecture 17: Hyperbolic 3-manifolds and Mostow Rigidity 70 Lecture 18: Dehn's Lemma and Essential/Incompressible Surfaces 71 Lecture 19: Sphere Decompositions and Knot Connected Sum 74 Lecture 20: JSJ Decomposition, Geometrization, Splice Maps, and Satellites 78 Lecture 21: Turaev torsion and Alexander polynomial of unions 81 Lecture 22: Foliations 84 Lecture 23: The Thurston Norm 88 Lecture 24: Taut foliations on Seifert fibered spaces 89 References 92 1 2 Lecture 0 (not lectured): Preliminaries 0. Notation and conventions. Notation. @X { (the manifold given by) the boundary of X, for X a manifold with boundary. th @iX { the i connected component of @X. ν(X) { a tubular (or collared) neighborhood of X in Y , for an embedding X ⊂ Y . -
HE WANG Abstract. a Mini-Course on Rational Homotopy Theory
RATIONAL HOMOTOPY THEORY HE WANG Abstract. A mini-course on rational homotopy theory. Contents 1. Introduction 2 2. Elementary homotopy theory 3 3. Spectral sequences 8 4. Postnikov towers and rational homotopy theory 16 5. Commutative differential graded algebras 21 6. Minimal models 25 7. Fundamental groups 34 References 36 2010 Mathematics Subject Classification. Primary 55P62 . 1 2 HE WANG 1. Introduction One of the goals of topology is to classify the topological spaces up to some equiva- lence relations, e.g., homeomorphic equivalence and homotopy equivalence (for algebraic topology). In algebraic topology, most of the time we will restrict to spaces which are homotopy equivalent to CW complexes. We have learned several algebraic invariants such as fundamental groups, homology groups, cohomology groups and cohomology rings. Using these algebraic invariants, we can seperate two non-homotopy equivalent spaces. Another powerful algebraic invariants are the higher homotopy groups. Whitehead the- orem shows that the functor of homotopy theory are power enough to determine when two CW complex are homotopy equivalent. A rational coefficient version of the homotopy theory has its own techniques and advan- tages: 1. fruitful algebraic structures. 2. easy to calculate. RATIONAL HOMOTOPY THEORY 3 2. Elementary homotopy theory 2.1. Higher homotopy groups. Let X be a connected CW-complex with a base point x0. Recall that the fundamental group π1(X; x0) = [(I;@I); (X; x0)] is the set of homotopy classes of maps from pair (I;@I) to (X; x0) with the product defined by composition of paths. Similarly, for each n ≥ 2, the higher homotopy group n n πn(X; x0) = [(I ;@I ); (X; x0)] n n is the set of homotopy classes of maps from pair (I ;@I ) to (X; x0) with the product defined by composition. -
The Suspension X ∧S and the Fake Suspension ΣX of a Spectrum X
Contents 41 Suspensions and shift 1 42 The telescope construction 10 43 Fibrations and cofibrations 15 44 Cofibrant generation 22 41 Suspensions and shift The suspension X ^S1 and the fake suspension SX of a spectrum X were defined in Section 35 — the constructions differ by a non-trivial twist of bond- ing maps. The loop spectrum for X is the function complex object 1 hom∗(S ;X): There is a natural bijection 1 ∼ 1 hom(X ^ S ;Y) = hom(X;hom∗(S ;Y)) so that the suspension and loop functors are ad- joint. The fake loop spectrum WY for a spectrum Y con- sists of the pointed spaces WY n, n ≥ 0, with adjoint bonding maps n 2 n+1 Ws∗ : WY ! W Y : 1 There is a natural bijection hom(SX;Y) =∼ hom(X;WY); so the fake suspension functor is left adjoint to fake loops. n n+1 The adjoint bonding maps s∗ : Y ! WY define a natural map g : Y ! WY[1]: for spectra Y. The map w : Y ! W¥Y of the last section is the filtered colimit of the maps g Wg[1] W2g[2] Y −! WY[1] −−−! W2Y[2] −−−! ::: Recall the statement of the Freudenthal suspen- sion theorem (Theorem 34.2): Theorem 41.1. Suppose that a pointed space X is n-connected, where n ≥ 0. Then the homotopy fibre F of the canonical map h : X ! W(X ^ S1) is 2n-connected. 2 In particular, the suspension homomorphism 1 ∼ 1 piX ! pi(W(X ^ S )) = pi+1(X ^ S ) is an isomorphism for i ≤ 2n and is an epimor- phism for i = 2n+1, provided that X is connected. -
Directed Algebraic Topology and Applications
Directed algebraic topology and applications Martin Raussen Department of Mathematical Sciences, Aalborg University, Denmark Discrete Structures in Algebra, Geometry, Topology and Computer Science 6ECM July 3, 2012 Martin Raussen Directed algebraic topology and applications Algebraic Topology Homotopy Homotopy: 1-parameter deformation Two continuous functions f , g : X ! Y from a topological space X to another, Y are called homotopic if one can be "continuously deformed" into the other. Such a deformation is called a homotopy H : X × I ! Y between the two functions. Two spaces X, Y are called homotopy equivalent if there are continous maps f : X ! Y and g : Y ! X that are homotopy inverse to each other, i.e., such that g ◦ f ' idX and f ◦ g ' idY . Martin Raussen Directed algebraic topology and applications Algebraic Topology Invariants Algebraic topology is the branch of mathematics which uses tools from abstract algebra to study topological spaces. The basic goal is to find algebraic invariants that classify topological spaces up to homeomorphism, though usually most classify (at best) up to homotopy equivalence. An outstanding use of homotopy is the definition of homotopy groups pn(X, ∗), n > 0 – important invariants in algebraic topology. Examples Spheres of different dimensions are not homotopy equivalent to each other. Euclidean spaces of different dimensions are not homeomorphic to each other. Martin Raussen Directed algebraic topology and applications Path spaces, loop spaces and homotopy groups Definition Path space P(X )(x0, x1): the space of all continuous paths p : I ! X starting at x0 and ending at x1 (CO-topology). Loop space W(X )(x0): the space of all all continuous loops 1 w : S ! X starting and ending at x0. -
[DRAFT] a Peripatetic Course in Algebraic Topology
[DRAFT] A Peripatetic Course in Algebraic Topology Julian Salazar [email protected]• http://slzr.me July 22, 2016 Abstract These notes are based on lectures in algebraic topology taught by Peter May and Henry Chan at the 2016 University of Chicago Math REU. They are loosely chrono- logical, having been reorganized for my benefit and significantly annotated by my personal exposition, plus solutions to in-class/HW exercises, plus content from read- ings (from May’s Finite Book), books (e.g. May’s Concise Course, Munkres’ Elements of Algebraic Topology, and Hatcher’s Algebraic Topology), Wikipedia, etc. I Foundations + Weeks 1 to 33 1 Topological notions3 1.1 Topological spaces.................................3 1.2 Separation properties...............................4 1.3 Continuity and operations on spaces......................4 2 Algebraic notions5 2.1 Rings and modules................................6 2.2 Tensor products..................................7 3 Categorical notions 11 3.1 Categories..................................... 11 3.2 Functors...................................... 13 3.3 Natural transformations............................. 15 3.4 [DRAFT] Universal properties.......................... 17 3.5 Adjoint functors.................................. 20 1 4 The fundamental group 21 4.1 Connectedness and paths............................. 21 4.2 Homotopy and homotopy equivalence..................... 22 4.3 The fundamental group.............................. 24 4.4 Applications.................................... 26 -
Poincar\'E Duality for $ K $-Theory of Equivariant Complex Projective
POINCARE´ DUALITY FOR K-THEORY OF EQUIVARIANT COMPLEX PROJECTIVE SPACES J.P.C. GREENLEES AND G.R. WILLIAMS Abstract. We make explicit Poincar´eduality for the equivariant K-theory of equivariant complex projective spaces. The case of the trivial group provides a new approach to the K-theory orientation [3]. 1. Introduction In 1 well behaved cases one expects the cohomology of a finite com- plex to be a contravariant functor of its homology. However, orientable manifolds have the special property that the cohomology is covariantly isomorphic to the homology, and hence in particular the cohomology ring is self-dual. More precisely, Poincar´eduality states that taking the cap product with a fundamental class gives an isomorphism between homology and cohomology of a manifold. Classically, an n-manifold M is a topological space locally modelled n on R , and the fundamental class of M is a homology class in Hn(M). Equivariantly, it is much less clear how things should work. If we pick a point x of a smooth G-manifold, the tangent space Vx is a represen- tation of the isotropy group Gx, and its G-orbit is locally modelled on G ×Gx Vx; both Gx and Vx depend on the point x. It may happen that we have a W -manifold, in the sense that there is a single representation arXiv:0711.0346v1 [math.AT] 2 Nov 2007 W so that Vx is the restriction of W to Gx for all x, but this is very restrictive. Even if there are fixed points x, the representations Vx at different points need not be equivalent. -
4 Homotopy Theory Primer
4 Homotopy theory primer Given that some topological invariant is different for topological spaces X and Y one can definitely say that the spaces are not homeomorphic. The more invariants one has at his/her disposal the more detailed testing of equivalence of X and Y one can perform. The homotopy theory constructs infinitely many topological invariants to characterize a given topological space. The main idea is the following. Instead of directly comparing struc- tures of X and Y one takes a “test manifold” M and considers the spacings of its mappings into X and Y , i.e., spaces C(M, X) and C(M, Y ). Studying homotopy classes of those mappings (see below) one can effectively compare the spaces of mappings and consequently topological spaces X and Y . It is very convenient to take as “test manifold” M spheres Sn. It turns out that in this case one can endow the spaces of mappings (more precisely of homotopy classes of those mappings) with group structure. The obtained groups are called homotopy groups of corresponding topological spaces and present us with very useful topological invariants characterizing those spaces. In physics homotopy groups are mostly used not to classify topological spaces but spaces of mappings themselves (i.e., spaces of field configura- tions). 4.1 Homotopy Definition Let I = [0, 1] is a unit closed interval of R and f : X Y , → g : X Y are two continuous maps of topological space X to topological → space Y . We say that these maps are homotopic and denote f g if there ∼ exists a continuous map F : X I Y such that F (x, 0) = f(x) and × → F (x, 1) = g(x). -
Some Finiteness Results for Groups of Automorphisms of Manifolds 3
SOME FINITENESS RESULTS FOR GROUPS OF AUTOMORPHISMS OF MANIFOLDS ALEXANDER KUPERS Abstract. We prove that in dimension =6 4, 5, 7 the homology and homotopy groups of the classifying space of the topological group of diffeomorphisms of a disk fixing the boundary are finitely generated in each degree. The proof uses homological stability, embedding calculus and the arithmeticity of mapping class groups. From this we deduce similar results for the homeomorphisms of Rn and various types of automorphisms of 2-connected manifolds. Contents 1. Introduction 1 2. Homologically and homotopically finite type spaces 4 3. Self-embeddings 11 4. The Weiss fiber sequence 19 5. Proofs of main results 29 References 38 1. Introduction Inspired by work of Weiss on Pontryagin classes of topological manifolds [Wei15], we use several recent advances in the study of high-dimensional manifolds to prove a structural result about diffeomorphism groups. We prove the classifying spaces of such groups are often “small” in one of the following two algebro-topological senses: Definition 1.1. Let X be a path-connected space. arXiv:1612.09475v3 [math.AT] 1 Sep 2019 · X is said to be of homologically finite type if for all Z[π1(X)]-modules M that are finitely generated as abelian groups, H∗(X; M) is finitely generated in each degree. · X is said to be of finite type if π1(X) is finite and πi(X) is finitely generated for i ≥ 2. Being of finite type implies being of homologically finite type, see Lemma 2.15. Date: September 4, 2019. Alexander Kupers was partially supported by a William R. -
The Real Projective Spaces in Homotopy Type Theory
The real projective spaces in homotopy type theory Ulrik Buchholtz Egbert Rijke Technische Universität Darmstadt Carnegie Mellon University Email: [email protected] Email: [email protected] Abstract—Homotopy type theory is a version of Martin- topology and homotopy theory developed in homotopy Löf type theory taking advantage of its homotopical models. type theory (homotopy groups, including the fundamen- In particular, we can use and construct objects of homotopy tal group of the circle, the Hopf fibration, the Freuden- theory and reason about them using higher inductive types. In this article, we construct the real projective spaces, key thal suspension theorem and the van Kampen theorem, players in homotopy theory, as certain higher inductive types for example). Here we give an elementary construction in homotopy type theory. The classical definition of RPn, in homotopy type theory of the real projective spaces as the quotient space identifying antipodal points of the RPn and we develop some of their basic properties. n-sphere, does not translate directly to homotopy type theory. R n In classical homotopy theory the real projective space Instead, we define P by induction on n simultaneously n with its tautological bundle of 2-element sets. As the base RP is either defined as the space of lines through the + case, we take RP−1 to be the empty type. In the inductive origin in Rn 1 or as the quotient by the antipodal action step, we take RPn+1 to be the mapping cone of the projection of the 2-element group on the sphere Sn [4]. -
Math 231Br: Algebraic Topology
algebraic topology Lectures delivered by Michael Hopkins Notes by Eva Belmont and Akhil Mathew Spring 2011, Harvard fLast updated August 14, 2012g Contents Lecture 1 January 24, 2010 x1 Introduction 6 x2 Homotopy groups. 6 Lecture 2 1/26 x1 Introduction 8 x2 Relative homotopy groups 9 x3 Relative homotopy groups as absolute homotopy groups 10 Lecture 3 1/28 x1 Fibrations 12 x2 Long exact sequence 13 x3 Replacing maps 14 Lecture 4 1/31 x1 Motivation 15 x2 Exact couples 16 x3 Important examples 17 x4 Spectral sequences 19 1 Lecture 5 February 2, 2010 x1 Serre spectral sequence, special case 21 Lecture 6 2/4 x1 More structure in the spectral sequence 23 x2 The cohomology ring of ΩSn+1 24 x3 Complex projective space 25 Lecture 7 January 7, 2010 x1 Application I: Long exact sequence in H∗ through a range for a fibration 27 x2 Application II: Hurewicz Theorem 28 Lecture 8 2/9 x1 The relative Hurewicz theorem 30 x2 Moore and Eilenberg-Maclane spaces 31 x3 Postnikov towers 33 Lecture 9 February 11, 2010 x1 Eilenberg-Maclane Spaces 34 Lecture 10 2/14 x1 Local systems 39 x2 Homology in local systems 41 Lecture 11 February 16, 2010 x1 Applications of the Serre spectral sequence 45 Lecture 12 2/18 x1 Serre classes 50 Lecture 13 February 23, 2011 Lecture 14 2/25 Lecture 15 February 28, 2011 Lecture 16 3/2/2011 Lecture 17 March 4, 2011 Lecture 18 3/7 x1 Localization 74 x2 The homotopy category 75 x3 Morphisms between model categories 77 Lecture 19 March 11, 2011 x1 Model Category on Simplicial Sets 79 Lecture 20 3/11 x1 The Yoneda embedding 81 x2 82