Math 527 - Homotopy Theory Cofiber Sequences
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Homological Algebra
Homological Algebra Donu Arapura April 1, 2020 Contents 1 Some module theory3 1.1 Modules................................3 1.6 Projective modules..........................5 1.12 Projective modules versus free modules..............7 1.15 Injective modules...........................8 1.21 Tensor products............................9 2 Homology 13 2.1 Simplicial complexes......................... 13 2.8 Complexes............................... 15 2.15 Homotopy............................... 18 2.23 Mapping cones............................ 19 3 Ext groups 21 3.1 Extensions............................... 21 3.11 Projective resolutions........................ 24 3.16 Higher Ext groups.......................... 26 3.22 Characterization of projectives and injectives........... 28 4 Cohomology of groups 32 4.1 Group cohomology.......................... 32 4.6 Bar resolution............................. 33 4.11 Low degree cohomology....................... 34 4.16 Applications to finite groups..................... 36 4.20 Topological interpretation...................... 38 5 Derived Functors and Tor 39 5.1 Abelian categories.......................... 39 5.13 Derived functors........................... 41 5.23 Tor functors.............................. 44 5.28 Homology of a group......................... 45 1 6 Further techniques 47 6.1 Double complexes........................... 47 6.7 Koszul complexes........................... 49 7 Applications to commutative algebra 52 7.1 Global dimensions.......................... 52 7.9 Global dimension of -
Derived Functors and Homological Dimension (Pdf)
DERIVED FUNCTORS AND HOMOLOGICAL DIMENSION George Torres Math 221 Abstract. This paper overviews the basic notions of abelian categories, exact functors, and chain complexes. It will use these concepts to define derived functors, prove their existence, and demon- strate their relationship to homological dimension. I affirm my awareness of the standards of the Harvard College Honor Code. Date: December 15, 2015. 1 2 DERIVED FUNCTORS AND HOMOLOGICAL DIMENSION 1. Abelian Categories and Homology The concept of an abelian category will be necessary for discussing ideas on homological algebra. Loosely speaking, an abelian cagetory is a type of category that behaves like modules (R-mod) or abelian groups (Ab). We must first define a few types of morphisms that such a category must have. Definition 1.1. A morphism f : X ! Y in a category C is a zero morphism if: • for any A 2 C and any g; h : A ! X, fg = fh • for any B 2 C and any g; h : Y ! B, gf = hf We denote a zero morphism as 0XY (or sometimes just 0 if the context is sufficient). Definition 1.2. A morphism f : X ! Y is a monomorphism if it is left cancellative. That is, for all g; h : Z ! X, we have fg = fh ) g = h. An epimorphism is a morphism if it is right cancellative. The zero morphism is a generalization of the zero map on rings, or the identity homomorphism on groups. Monomorphisms and epimorphisms are generalizations of injective and surjective homomorphisms (though these definitions don't always coincide). It can be shown that a morphism is an isomorphism iff it is epic and monic. -
Lecture 15. De Rham Cohomology
Lecture 15. de Rham cohomology In this lecture we will show how differential forms can be used to define topo- logical invariants of manifolds. This is closely related to other constructions in algebraic topology such as simplicial homology and cohomology, singular homology and cohomology, and Cechˇ cohomology. 15.1 Cocycles and coboundaries Let us first note some applications of Stokes’ theorem: Let ω be a k-form on a differentiable manifold M.For any oriented k-dimensional compact sub- manifold Σ of M, this gives us a real number by integration: " ω : Σ → ω. Σ (Here we really mean the integral over Σ of the form obtained by pulling back ω under the inclusion map). Now suppose we have two such submanifolds, Σ0 and Σ1, which are (smoothly) homotopic. That is, we have a smooth map F : Σ × [0, 1] → M with F |Σ×{i} an immersion describing Σi for i =0, 1. Then d(F∗ω)isa (k + 1)-form on the (k + 1)-dimensional oriented manifold with boundary Σ × [0, 1], and Stokes’ theorem gives " " " d(F∗ω)= ω − ω. Σ×[0,1] Σ1 Σ1 In particular, if dω =0,then d(F∗ω)=F∗(dω)=0, and we deduce that ω = ω. Σ1 Σ0 This says that k-forms with exterior derivative zero give a well-defined functional on homotopy classes of compact oriented k-dimensional submani- folds of M. We know some examples of k-forms with exterior derivative zero, namely those of the form ω = dη for some (k − 1)-form η. But Stokes’ theorem then gives that Σ ω = Σ dη =0,sointhese cases the functional we defined on homotopy classes of submanifolds is trivial. -
On the Cohomology of the Finite Special Linear Groups, I
View metadata, citation and similar papers at core.ac.uk brought to you by CORE provided by Elsevier - Publisher Connector JOURNAL OF ALGEBRA 54, 216-238 (1978) On the Cohomology of the Finite Special Linear Groups, I GREGORY W. BELL* Fort Lewis College, Durango, Colorado 81301 Communicated by Graham Higman Received April 1, 1977 Let K be a finite field. We are interested in determining the cohomology groups of degree 0, 1, and 2 of various KSL,+,(K) modules. Our work is directed to the goal of determining the second degree cohomology of S&+,(K) acting on the exterior powers of its standard I + l-dimensional module. However, our solution of this problem will involve the study of many cohomology groups of degree 0 and 1 as well. These groups are of independent interest and they are useful in many other cohomological calculations involving SL,+#) and other Chevalley groups [ 11. Various aspects of this problem or similar problems have been considered by many authors, including [l, 5, 7-12, 14-19, 211. There have been many techni- ques used in studing this problem. Some are ad hoc and rely upon particular information concerning the groups in question. Others are more general, but still place restrictions, such as restrictions on the characteristic of the field, the order of the field, or the order of the Galois group of the field. Our approach is general and shows how all of these problems may be considered in a unified. way. In fact, the same method may be applied quite generally to other Chevalley groups acting on certain of their modules [l]. -
Local Topological Properties of Asymptotic Cones of Groups
Local topological properties of asymptotic cones of groups Greg Conner and Curt Kent October 8, 2018 Abstract We define a local analogue to Gromov’s loop division property which is use to give a sufficient condition for an asymptotic cone of a complete geodesic metric space to have uncountable fundamental group. As well, this property is used to understand the local topological structure of asymptotic cones of many groups currently in the literature. Contents 1 Introduction 1 1.1 Definitions...................................... 3 2 Coarse Loop Division Property 5 2.1 Absolutely non-divisible sequences . .......... 10 2.2 Simplyconnectedcones . .. .. .. .. .. .. .. 11 3 Examples 15 3.1 An example of a group with locally simply connected cones which is not simply connected ........................................ 17 1 Introduction Gromov [14, Section 5.F] was first to notice a connection between the homotopic properties of asymptotic cones of a finitely generated group and algorithmic properties of the group: if arXiv:1210.4411v1 [math.GR] 16 Oct 2012 all asymptotic cones of a finitely generated group are simply connected, then the group is finitely presented, its Dehn function is bounded by a polynomial (hence its word problem is in NP) and its isodiametric function is linear. A version of that result for higher homotopy groups was proved by Riley [25]. The converse statement does not hold: there are finitely presented groups with non-simply connected asymptotic cones and polynomial Dehn functions [1], [26], and even with polynomial Dehn functions and linear isodiametric functions [21]. A partial converse statement was proved by Papasoglu [23]: a group with quadratic Dehn function has all asymptotic cones simply connected (for groups with subquadratic Dehn functions, i.e. -
[Math.AT] 2 May 2002
WEAK EQUIVALENCES OF SIMPLICIAL PRESHEAVES DANIEL DUGGER AND DANIEL C. ISAKSEN Abstract. Weak equivalences of simplicial presheaves are usually defined in terms of sheaves of homotopy groups. We give another characterization us- ing relative-homotopy-liftings, and develop the tools necessary to prove that this agrees with the usual definition. From our lifting criteria we are able to prove some foundational (but new) results about the local homotopy theory of simplicial presheaves. 1. Introduction In developing the homotopy theory of simplicial sheaves or presheaves, the usual way to define weak equivalences is to require that a map induce isomorphisms on all sheaves of homotopy groups. This is a natural generalization of the situation for topological spaces, but the ‘sheaves of homotopy groups’ machinery (see Def- inition 6.6) can feel like a bit of a mouthful. The purpose of this paper is to unravel this definition, giving a fairly concrete characterization in terms of lift- ing properties—the kind of thing which feels more familiar and comfortable to the ingenuous homotopy theorist. The original idea came to us via a passing remark of Jeff Smith’s: He pointed out that a map of spaces X → Y induces an isomorphism on homotopy groups if and only if every diagram n−1 / (1.1) S 6/ X xx{ xx xx {x n { n / D D 6/ Y xx{ xx xx {x Dn+1 −1 arXiv:math/0205025v1 [math.AT] 2 May 2002 admits liftings as shown (for every n ≥ 0, where by convention we set S = ∅). Here the maps Sn−1 ֒→ Dn are both the boundary inclusion, whereas the two maps Dn ֒→ Dn+1 in the diagram are the two inclusions of the surface hemispheres of Dn+1. -
COFIBRATIONS in This Section We Introduce the Class of Cofibration
SECTION 8: COFIBRATIONS In this section we introduce the class of cofibration which can be thought of as nice inclusions. There are inclusions of subspaces which are `homotopically badly behaved` and these will be ex- cluded by considering cofibrations only. To be a bit more specific, let us mention the following two phenomenons which we would like to exclude. First, there are examples of contractible subspaces A ⊆ X which have the property that the quotient map X ! X=A is not a homotopy equivalence. Moreover, whenever we have a pair of spaces (X; A), we might be interested in extension problems of the form: f / A WJ i } ? X m 9 h Thus, we are looking for maps h as indicated by the dashed arrow such that h ◦ i = f. In general, it is not true that this problem `lives in homotopy theory'. There are examples of homotopic maps f ' g such that the extension problem can be solved for f but not for g. By design, the notion of a cofibration excludes this phenomenon. Definition 1. (1) Let i: A ! X be a map of spaces. The map i has the homotopy extension property with respect to a space W if for each homotopy H : A×[0; 1] ! W and each map f : X × f0g ! W such that f(i(a); 0) = H(a; 0); a 2 A; there is map K : X × [0; 1] ! W such that the following diagram commutes: (f;H) X × f0g [ A × [0; 1] / A×{0g = W z u q j m K X × [0; 1] f (2) A map i: A ! X is a cofibration if it has the homotopy extension property with respect to all spaces W . -
Zuoqin Wang Time: March 25, 2021 the QUOTIENT TOPOLOGY 1. The
Topology (H) Lecture 6 Lecturer: Zuoqin Wang Time: March 25, 2021 THE QUOTIENT TOPOLOGY 1. The quotient topology { The quotient topology. Last time we introduced several abstract methods to construct topologies on ab- stract spaces (which is widely used in point-set topology and analysis). Today we will introduce another way to construct topological spaces: the quotient topology. In fact the quotient topology is not a brand new method to construct topology. It is merely a simple special case of the co-induced topology that we introduced last time. However, since it is very concrete and \visible", it is widely used in geometry and algebraic topology. Here is the definition: Definition 1.1 (The quotient topology). (1) Let (X; TX ) be a topological space, Y be a set, and p : X ! Y be a surjective map. The co-induced topology on Y induced by the map p is called the quotient topology on Y . In other words, −1 a set V ⊂ Y is open if and only if p (V ) is open in (X; TX ). (2) A continuous surjective map p :(X; TX ) ! (Y; TY ) is called a quotient map, and Y is called the quotient space of X if TY coincides with the quotient topology on Y induced by p. (3) Given a quotient map p, we call p−1(y) the fiber of p over the point y 2 Y . Note: by definition, the composition of two quotient maps is again a quotient map. Here is a typical way to construct quotient maps/quotient topology: Start with a topological space (X; TX ), and define an equivalent relation ∼ on X. -
INTRODUCTION to ALGEBRAIC TOPOLOGY 1 Category And
INTRODUCTION TO ALGEBRAIC TOPOLOGY (UPDATED June 2, 2020) SI LI AND YU QIU CONTENTS 1 Category and Functor 2 Fundamental Groupoid 3 Covering and fibration 4 Classification of covering 5 Limit and colimit 6 Seifert-van Kampen Theorem 7 A Convenient category of spaces 8 Group object and Loop space 9 Fiber homotopy and homotopy fiber 10 Exact Puppe sequence 11 Cofibration 12 CW complex 13 Whitehead Theorem and CW Approximation 14 Eilenberg-MacLane Space 15 Singular Homology 16 Exact homology sequence 17 Barycentric Subdivision and Excision 18 Cellular homology 19 Cohomology and Universal Coefficient Theorem 20 Hurewicz Theorem 21 Spectral sequence 22 Eilenberg-Zilber Theorem and Kunneth¨ formula 23 Cup and Cap product 24 Poincare´ duality 25 Lefschetz Fixed Point Theorem 1 1 CATEGORY AND FUNCTOR 1 CATEGORY AND FUNCTOR Category In category theory, we will encounter many presentations in terms of diagrams. Roughly speaking, a diagram is a collection of ‘objects’ denoted by A, B, C, X, Y, ··· , and ‘arrows‘ between them denoted by f , g, ··· , as in the examples f f1 A / B X / Y g g1 f2 h g2 C Z / W We will always have an operation ◦ to compose arrows. The diagram is called commutative if all the composite paths between two objects ultimately compose to give the same arrow. For the above examples, they are commutative if h = g ◦ f f2 ◦ f1 = g2 ◦ g1. Definition 1.1. A category C consists of 1◦. A class of objects: Obj(C) (a category is called small if its objects form a set). We will write both A 2 Obj(C) and A 2 C for an object A in C. -
Notes for Math 227A: Algebraic Topology
NOTES FOR MATH 227A: ALGEBRAIC TOPOLOGY KO HONDA 1. CATEGORIES AND FUNCTORS 1.1. Categories. A category C consists of: (1) A collection ob(C) of objects. (2) A set Hom(A, B) of morphisms for each ordered pair (A, B) of objects. A morphism f ∈ Hom(A, B) f is usually denoted by f : A → B or A → B. (3) A map Hom(A, B) × Hom(B,C) → Hom(A, C) for each ordered triple (A,B,C) of objects, denoted (f, g) 7→ gf. (4) An identity morphism idA ∈ Hom(A, A) for each object A. The morphisms satisfy the following properties: A. (Associativity) (fg)h = f(gh) if h ∈ Hom(A, B), g ∈ Hom(B,C), and f ∈ Hom(C, D). B. (Unit) idB f = f = f idA if f ∈ Hom(A, B). Examples: (HW: take a couple of examples and verify that all the axioms of a category are satisfied.) 1. Top = category of topological spaces and continuous maps. The objects are topological spaces X and the morphisms Hom(X,Y ) are continuous maps from X to Y . 2. Top• = category of pointed topological spaces. The objects are pairs (X,x) consisting of a topological space X and a point x ∈ X. Hom((X,x), (Y,y)) consist of continuous maps from X to Y that take x to y. Similarly define Top2 = category of pairs (X, A) where X is a topological space and A ⊂ X is a subspace. Hom((X, A), (Y,B)) consists of continuous maps f : X → Y such that f(A) ⊂ B. -
Fibrations II - the Fundamental Lifting Property
Fibrations II - The Fundamental Lifting Property Tyrone Cutler July 13, 2020 Contents 1 The Fundamental Lifting Property 1 2 Spaces Over B 3 2.1 Homotopy in T op=B ............................... 7 3 The Homotopy Theorem 8 3.1 Implications . 12 4 Transport 14 4.1 Implications . 16 5 Proof of the Fundamental Lifting Property Completed. 19 6 The Mutal Characterisation of Cofibrations and Fibrations 20 6.1 Implications . 22 1 The Fundamental Lifting Property This section is devoted to stating Theorem 1.1 and beginning its proof. We prove only the first of its two statements here. This part of the theorem will then be used in the sequel, and the proof of the second statement will follow from the results obtained in the next section. We will be careful to avoid circular reasoning. The utility of the theorem will soon become obvious as we repeatedly use its statement to produce maps having very specific properties. However, the true power of the theorem is not unveiled until x 5, where we show how it leads to a mutual characterisation of cofibrations and fibrations in terms of an orthogonality relation. Theorem 1.1 Let j : A,! X be a closed cofibration and p : E ! B a fibration. Assume given the solid part of the following strictly commutative diagram f A / E |> j h | p (1.1) | | X g / B: 1 Then the dotted filler can be completed so as to make the whole diagram commute if either of the following two conditions are met • j is a homotopy equivalence. • p is a homotopy equivalence. -
When Is the Natural Map a a Cofibration? Í22a
transactions of the american mathematical society Volume 273, Number 1, September 1982 WHEN IS THE NATURAL MAP A Í22A A COFIBRATION? BY L. GAUNCE LEWIS, JR. Abstract. It is shown that a map/: X — F(A, W) is a cofibration if its adjoint/: X A A -» W is a cofibration and X and A are locally equiconnected (LEC) based spaces with A compact and nontrivial. Thus, the suspension map r¡: X -» Ü1X is a cofibration if X is LEC. Also included is a new, simpler proof that C.W. complexes are LEC. Equivariant generalizations of these results are described. In answer to our title question, asked many years ago by John Moore, we show that 7j: X -> Í22A is a cofibration if A is locally equiconnected (LEC)—that is, the inclusion of the diagonal in A X X is a cofibration [2,3]. An equivariant extension of this result, applicable to actions by any compact Lie group and suspensions by an arbitrary finite-dimensional representation, is also given. Both of these results have important implications for stable homotopy theory where colimits over sequences of maps derived from r¡ appear unbiquitously (e.g., [1]). The force of our solution comes from the Dyer-Eilenberg adjunction theorem for LEC spaces [3] which implies that C.W. complexes are LEC. Via Corollary 2.4(b) below, this adjunction theorem also has some implications (exploited in [1]) for the geometry of the total spaces of the universal spherical fibrations of May [6]. We give a simpler, more conceptual proof of the Dyer-Eilenberg result which is equally applicable in the equivariant context and therefore gives force to our equivariant cofibration condition.