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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. -
[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. -
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. -
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. -
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. -
MTH 507 Midterm Solutions
MTH 507 Midterm Solutions 1. Let X be a path connected, locally path connected, and semilocally simply connected space. Let H0 and H1 be subgroups of π1(X; x0) (for some x0 2 X) such that H0 ≤ H1. Let pi : XHi ! X (for i = 0; 1) be covering spaces corresponding to the subgroups Hi. Prove that there is a covering space f : XH0 ! XH1 such that p1 ◦ f = p0. Solution. Choose x ; x 2 p−1(x ) so that p :(X ; x ) ! (X; x ) and e0 e1 0 i Hi ei 0 p (X ; x ) = H for i = 0; 1. Since H ≤ H , by the Lifting Criterion, i∗ Hi ei i 0 1 there exists a lift f : XH0 ! XH1 of p0 such that p1 ◦f = p0. It remains to show that f : XH0 ! XH1 is a covering space. Let y 2 XH1 , and let U be a path-connected neighbourhood of x = p1(y) that is evenly covered by both p0 and p1. Let V ⊂ XH1 be −1 −1 the slice of p1 (U) that contains y. Denote the slices of p0 (U) by 0 −1 0 −1 fVz : z 2 p0 (x)g. Let C denote the subcollection fVz : z 2 f (y)g −1 −1 of p0 (U). Every slice Vz is mapped by f into a single slice of p1 (U), −1 0 as these are path-connected. Also, since f(z) 2 p1 (y), f(Vz ) ⊂ V iff f(z) = y. Hence f −1(V ) is the union of the slices in C. 0 −1 0 0 0 Finally, we have that for Vz 2 C,(p1jV ) ◦ (p0jVz ) = fjVz . -
On Digital Simply Connected Spaces and Manifolds: a Digital Simply Connected 3- Manifold Is the Digital 3-Sphere
On digital simply connected spaces and manifolds: a digital simply connected 3- manifold is the digital 3-sphere Alexander V. Evako Npk Novotek, Laboratory of Digital Technologies. Moscow, Russia e-mail: [email protected]. Abstract In the framework of digital topology, we study structural and topological properties of digital n- dimensional manifolds. We introduce the notion of simple connectedness of a digital space and prove that if M and N are homotopy equivalent digital spaces and M is simply connected, then so is N. We show that a simply connected digital 2-manifold is the digital 2-sphere and a simply connected digital 3-manifold is the digital 3-sphere. This property can be considered as a digital form of the Poincaré conjecture for continuous three-manifolds. Key words: Graph; Dimension; Digital manifold; Simply connected space; Sphere 1. Introduction A digital approach to geometry and topology plays an important role in analyzing n-dimensional digitized images arising in computer graphics as well as in many areas of science including neuroscience, medical imaging, industrial inspection, geoscience and fluid dynamics. Concepts and results of the digital approach are used to specify and justify some important low-level image processing algorithms, including algorithms for thinning, boundary extraction, object counting, and contour filling. Usually, a digital object is equipped with a graph structure based on the local adjacency relations of digital points [5]. In papers [6-7], a digital n-surface was defined as a simple undirected graph and basic properties of n-surfaces were studied. Paper [6] analyzes a local structure of the digital space Zn. -
Critical Values of Homology Classes of Loops and Positive Curvature
CRITICAL VALUES OF HOMOLOGY CLASSES OF LOOPS AND POSITIVE CURVATURE HANS-BERT RADEMACHER Abstract. We study compact and simply-connected Riemannian man- ifolds (M,g) with positive sectional curvature K ≥ 1. For a non-trivial homology class of lowest positive dimension in the space of loops based at a point p ∈ M or in the free loop space one can define a critical length crlp (M,g) resp. crl (M,g) . Then crlp (M,g) equals the length of a geodesic loop with base point p and crl (M,g) equals the length of a closed geodesic. This is the idea of the proof of the existence of a closed geodesic of positive length presented by Birkhoff in case of a sphere and by Lusternik & Fet in the general case. It is the main result of the paper that the numbers crlp (M,g) resp. crl (M,g) attain its maximal value 2π only for the round metric on the n-sphere. Under the additional assumption K ≤ 4 this result for crl (M,g) follows from results by Sugimoto in even dimensions and Ballmann, Thorbergsson & Ziller in odd dimensions. 1. Introduction For a compact Riemannian manifold (M, g) let = γ : [0, 1] M { −→ M ; γ absolutely continuous , 1 γ′ 2(t) dt < be the manifold of paths 0 k k ∞} (H1-paths) on M. We considerR in the sequel the following subspaces: the free loop space Λ = ΛM = γ ; γ(0) = γ(1) and for p,q M the space of paths between p and q :{ Ω ∈= M Ω M = γ } ; γ(0) = p,∈ γ(1) = q .