Hopf Algebras and Homology of Loop Suspension Spaces
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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 -
Loop Spaces in Motivic Homotopy Theory A
LOOP SPACES IN MOTIVIC HOMOTOPY THEORY A Dissertation by MARVIN GLEN DECKER Submitted to the Office of Graduate Studies of Texas A&M University in partial fulfillment of the requirements for the degree of DOCTOR OF PHILOSOPHY August 2006 Major Subject: Mathematics LOOP SPACES IN MOTIVIC HOMOTOPY THEORY A Dissertation by MARVIN GLEN DECKER Submitted to the Office of Graduate Studies of Texas A&M University in partial fulfillment of the requirements for the degree of DOCTOR OF PHILOSOPHY Approved by: Chair of Committee, Paulo Lima-Filho Committee Members, Nancy Amato Henry Schenck Peter Stiller Head of Department, Al Boggess August 2006 Major Subject: Mathematics iii ABSTRACT Loop Spaces in Motivic Homotopy Theory. (August 2006) Marvin Glen Decker, B.S., University of Kansas Chair of Advisory Committee: Dr. Paulo Lima-Filho In topology loop spaces can be understood combinatorially using algebraic the- ories. This approach can be extended to work for certain model structures on cate- gories of presheaves over a site with functorial unit interval objects, such as topological spaces and simplicial sheaves of smooth schemes at finite type. For such model cat- egories a new category of algebraic theories with a proper cellular simplicial model structure can be defined. This model structure can be localized in a way compatible with left Bousfield localizations of the underlying category of presheaves to yield a Motivic model structure for algebraic theories. As in the topological context, the model structure is Quillen equivalent to a category of loop spaces in the underlying category. iv TABLE OF CONTENTS CHAPTER Page I INTRODUCTION .......................... 1 II THE BOUSFIELD-KAN MODEL STRUCTURE ....... -
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. -
The Double Suspension of the Mazur Homology 3-Sphere
THE DOUBLE SUSPENSION OF THE MAZUR HOMOLOGY SPHERE FADI MEZHER 1 Introduction The main objects of this text are homology spheres, which are defined below. Definition 1.1. A manifold M of dimension n is called a homology n-sphere if it has the same homology groups as Sn; that is, ( Z if k ∈ {0, n} Hk(M) = 0 otherwise A result of J.W. Cannon in [Can79] establishes the following theorem Theorem 1.2 (Double Suspension Theorem). The double suspension of any homology n-sphere is homeomorphic to Sn+2. This, however, is beyond the scope of this text. We will, instead, construct a homology sphere, the Mazur homology 3-sphere, and show the double suspension theorem for this particular manifold. However, before beginning with the proper content, let us study the following famous example of a nontrivial homology sphere. Example 1.3. Let I be the group of (orientation preserving) symmetries of the icosahedron, which we recall is a regular polyhedron with twenty faces, twelve vertices, and thirty edges. This group, called the icosahedral group, is finite, with sixty elements, and is naturally a subgroup of SO(3). It is a well-known fact that we have a 2-fold covering ξ : SU(2) → SO(3), where ∼ 3 ∼ 3 SU(2) = S , and SO(3) = RP . We then consider the following pullback diagram S0 S0 Ie := ι∗(SU(2)) SU(2) ι∗ξ ξ I SO(3) Then, Ie is also a group, where the multiplication is given by the lift of the map µ ◦ (ι∗ξ × ι∗ξ), where µ is the multiplication in I. -
L22 Adams Spectral Sequence
Lecture 22: Adams Spectral Sequence for HZ=p 4/10/15-4/17/15 1 A brief recall on Ext We review the definition of Ext from homological algebra. Ext is the derived functor of Hom. Let R be an (ordinary) ring. There is a model structure on the category of chain complexes of modules over R where the weak equivalences are maps of chain complexes which are isomorphisms on homology. Given a short exact sequence 0 ! M1 ! M2 ! M3 ! 0 of R-modules, applying Hom(P; −) produces a left exact sequence 0 ! Hom(P; M1) ! Hom(P; M2) ! Hom(P; M3): A module P is projective if this sequence is always exact. Equivalently, P is projective if and only if if it is a retract of a free module. Let M∗ be a chain complex of R-modules. A projective resolution is a chain complex P∗ of projec- tive modules and a map P∗ ! M∗ which is an isomorphism on homology. This is a cofibrant replacement, i.e. a factorization of 0 ! M∗ as a cofibration fol- lowed by a trivial fibration is 0 ! P∗ ! M∗. There is a functor Hom that takes two chain complexes M and N and produces a chain complex Hom(M∗;N∗) de- Q fined as follows. The degree n module, are the ∗ Hom(M∗;N∗+n). To give the differential, we should fix conventions about degrees. Say that our differentials have degree −1. Then there are two maps Y Y Hom(M∗;N∗+n) ! Hom(M∗;N∗+n−1): ∗ ∗ Q Q The first takes fn to dN fn. -
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. -
A Suspension Theorem for Continuous Trace C*-Algebras
proceedings of the american mathematical society Volume 120, Number 3, March 1994 A SUSPENSION THEOREM FOR CONTINUOUS TRACE C*-ALGEBRAS MARIUS DADARLAT (Communicated by Jonathan M. Rosenberg) Abstract. Let 3 be a stable continuous trace C*-algebra with spectrum Y . We prove that the natural suspension map S,: [Cq{X), 5§\ -* [Cq{X) ® Co(R), 3 ® Co(R)] is a bijection, provided that both X and Y are locally compact connected spaces whose one-point compactifications have the homo- topy type of a finite CW-complex and X is noncompact. This is used to compute the second homotopy group of 31 in terms of AMheory. That is, [C0(R2), 3] = K0{30) i where 3fa is a maximal ideal of 3 if Y is com- pact, and 3o = 3! if Y is noncompact. 1. Introduction For C*-algebras A, B let Hom(^4, 5) denote the space of (not necessarily unital) *-homomorphisms from A to 5 endowed with the topology of point- wise norm convergence. By definition <p, w e Hom(^, 5) are called homotopic if they lie in the same pathwise connected component of Horn (A, 5). The set of homotopy classes of the *-homomorphisms in Hom(^, 5) is denoted by [A, B]. For a locally compact space X let Cq(X) denote the C*-algebra of complex-valued continuous functions on X vanishing at infinity. The suspen- sion functor S for C*-algebras is defined as follows: it takes a C*-algebra A to A ® C0(R) and q>e Hom(^, 5) to <P0 idem € Hom(,4 ® C0(R), 5 ® C0(R)). -
A Radius Sphere Theorem
Invent. math. 112, 577-583 (1993) Inventiones mathematicae Springer-Verlag1993 A radius sphere theorem Karsten Grove 1'* and Peter Petersen 2'** 1 Department of Mathematics, University of Maryland, College Park, MD 20742, USA 2 Department of Mathematics, University of California, Los Angeles, CA 90024-1555, USA Oblatum 9-X-1992 Introduction The purpose of this paper is to present an optimal sphere theorem for metric spaces analogous to the celebrated Rauch-Berger-Klingenberg Sphere Theorem and the Diameter Sphere Theorem in Riemannian geometry. There has lately been considerable interest in studying spaces which are more singular than Riemannian manifolds. A natural reason for doing this is because Gromov-Hausdorff limits of Riemannian manifolds are almost never Riemannian manifolds, but usually only inner metric spaces with various nice properties. The kind of spaces we wish to study here are the so-called Alexandrov spaces. Alexan- drov spaces are finite Hausdorff dimensional inner metric spaces with a lower curvature bound in the distance comparison sense. The structure of Alexandrov spaces was studied in [BGP], [P1] and [P]. We point out that the curvature assumption implies that the Hausdorff dimension is equal to the topological dimension. Moreover, if X is an Alexandrov space and peX then the space of directions Zp at p is an Alexandrov space of one less dimension and with curvature > 1. Furthermore a neighborhood of p in X is homeomorphic to the linear cone over Zv- One of the important implications of this is that the local structure of n-dimensional Alexandrov spaces is determined by the structure of (n - 1)-dimen- sional Alexandrov spaces with curvature > 1.