HOMOLOGICAL ALGEBRA Our Goal Will Be to Get Far Enough to Develop
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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. -
Category Theory
CMPT 481/731 Functional Programming Fall 2008 Category Theory Category theory is a generalization of set theory. By having only a limited number of carefully chosen requirements in the definition of a category, we are able to produce a general algebraic structure with a large number of useful properties, yet permit the theory to apply to many different specific mathematical systems. Using concepts from category theory in the design of a programming language leads to some powerful and general programming constructs. While it is possible to use the resulting constructs without knowing anything about category theory, understanding the underlying theory helps. Category Theory F. Warren Burton 1 CMPT 481/731 Functional Programming Fall 2008 Definition of a Category A category is: 1. a collection of ; 2. a collection of ; 3. operations assigning to each arrow (a) an object called the domain of , and (b) an object called the codomain of often expressed by ; 4. an associative composition operator assigning to each pair of arrows, and , such that ,a composite arrow ; and 5. for each object , an identity arrow, satisfying the law that for any arrow , . Category Theory F. Warren Burton 2 CMPT 481/731 Functional Programming Fall 2008 In diagrams, we will usually express and (that is ) by The associative requirement for the composition operators means that when and are both defined, then . This allow us to think of arrows defined by paths throught diagrams. Category Theory F. Warren Burton 3 CMPT 481/731 Functional Programming Fall 2008 I will sometimes write for flip , since is less confusing than Category Theory F. -
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. -
Homological Mirror Symmetry for the Genus 2 Curve in an Abelian Variety and Its Generalized Strominger-Yau-Zaslow Mirror by Cath
Homological mirror symmetry for the genus 2 curve in an abelian variety and its generalized Strominger-Yau-Zaslow mirror by Catherine Kendall Asaro Cannizzo A dissertation submitted in partial satisfaction of the requirements for the degree of Doctor of Philosophy in Mathematics in the Graduate Division of the University of California, Berkeley Committee in charge: Professor Denis Auroux, Chair Professor David Nadler Professor Marjorie Shapiro Spring 2019 Homological mirror symmetry for the genus 2 curve in an abelian variety and its generalized Strominger-Yau-Zaslow mirror Copyright 2019 by Catherine Kendall Asaro Cannizzo 1 Abstract Homological mirror symmetry for the genus 2 curve in an abelian variety and its generalized Strominger-Yau-Zaslow mirror by Catherine Kendall Asaro Cannizzo Doctor of Philosophy in Mathematics University of California, Berkeley Professor Denis Auroux, Chair Motivated by observations in physics, mirror symmetry is the concept that certain mani- folds come in pairs X and Y such that the complex geometry on X mirrors the symplectic geometry on Y . It allows one to deduce information about Y from known properties of X. Strominger-Yau-Zaslow (1996) described how such pairs arise geometrically as torus fibra- tions with the same base and related fibers, known as SYZ mirror symmetry. Kontsevich (1994) conjectured that a complex invariant on X (the bounded derived category of coherent sheaves) should be equivalent to a symplectic invariant of Y (the Fukaya category). This is known as homological mirror symmetry. In this project, we first use the construction of SYZ mirrors for hypersurfaces in abelian varieties following Abouzaid-Auroux-Katzarkov, in order to obtain X and Y as manifolds. -
Limits Commutative Algebra May 11 2020 1. Direct Limits Definition 1
Limits Commutative Algebra May 11 2020 1. Direct Limits Definition 1: A directed set I is a set with a partial order ≤ such that for every i; j 2 I there is k 2 I such that i ≤ k and j ≤ k. Let R be a ring. A directed system of R-modules indexed by I is a collection of R modules fMi j i 2 Ig with a R module homomorphisms µi;j : Mi ! Mj for each pair i; j 2 I where i ≤ j, such that (i) for any i 2 I, µi;i = IdMi and (ii) for any i ≤ j ≤ k in I, µi;j ◦ µj;k = µi;k. We shall denote a directed system by a tuple (Mi; µi;j). The direct limit of a directed system is defined using a universal property. It exists and is unique up to a unique isomorphism. Theorem 2 (Direct limits). Let fMi j i 2 Ig be a directed system of R modules then there exists an R module M with the following properties: (i) There are R module homomorphisms µi : Mi ! M for each i 2 I, satisfying µi = µj ◦ µi;j whenever i < j. (ii) If there is an R module N such that there are R module homomorphisms νi : Mi ! N for each i and νi = νj ◦µi;j whenever i < j; then there exists a unique R module homomorphism ν : M ! N, such that νi = ν ◦ µi. The module M is unique in the sense that if there is any other R module M 0 satisfying properties (i) and (ii) then there is a unique R module isomorphism µ0 : M ! M 0. -
Some Notes About Simplicial Complexes and Homology II
Some notes about simplicial complexes and homology II J´onathanHeras J. Heras Some notes about simplicial homology II 1/19 Table of Contents 1 Simplicial Complexes 2 Chain Complexes 3 Differential matrices 4 Computing homology groups from Smith Normal Form J. Heras Some notes about simplicial homology II 2/19 Simplicial Complexes Table of Contents 1 Simplicial Complexes 2 Chain Complexes 3 Differential matrices 4 Computing homology groups from Smith Normal Form J. Heras Some notes about simplicial homology II 3/19 Simplicial Complexes Simplicial Complexes Definition Let V be an ordered set, called the vertex set. A simplex over V is any finite subset of V . Definition Let α and β be simplices over V , we say α is a face of β if α is a subset of β. Definition An ordered (abstract) simplicial complex over V is a set of simplices K over V satisfying the property: 8α 2 K; if β ⊆ α ) β 2 K Let K be a simplicial complex. Then the set Sn(K) of n-simplices of K is the set made of the simplices of cardinality n + 1. J. Heras Some notes about simplicial homology II 4/19 Simplicial Complexes Simplicial Complexes 2 5 3 4 0 6 1 V = (0; 1; 2; 3; 4; 5; 6) K = f;; (0); (1); (2); (3); (4); (5); (6); (0; 1); (0; 2); (0; 3); (1; 2); (1; 3); (2; 3); (3; 4); (4; 5); (4; 6); (5; 6); (0; 1; 2); (4; 5; 6)g J. Heras Some notes about simplicial homology II 5/19 Chain Complexes Table of Contents 1 Simplicial Complexes 2 Chain Complexes 3 Differential matrices 4 Computing homology groups from Smith Normal Form J. -
Higher-Dimensional Instantons on Cones Over Sasaki-Einstein Spaces and Coulomb Branches for 3-Dimensional N = 4 Gauge Theories
Two aspects of gauge theories higher-dimensional instantons on cones over Sasaki-Einstein spaces and Coulomb branches for 3-dimensional N = 4 gauge theories Von der Fakultät für Mathematik und Physik der Gottfried Wilhelm Leibniz Universität Hannover zur Erlangung des Grades Doktor der Naturwissenschaften – Dr. rer. nat. – genehmigte Dissertation von Dipl.-Phys. Marcus Sperling, geboren am 11. 10. 1987 in Wismar 2016 Eingereicht am 23.05.2016 Referent: Prof. Olaf Lechtenfeld Korreferent: Prof. Roger Bielawski Korreferent: Prof. Amihay Hanany Tag der Promotion: 19.07.2016 ii Abstract Solitons and instantons are crucial in modern field theory, which includes high energy physics and string theory, but also condensed matter physics and optics. This thesis is concerned with two appearances of solitonic objects: higher-dimensional instantons arising as supersymme- try condition in heterotic (flux-)compactifications, and monopole operators that describe the Coulomb branch of gauge theories in 2+1 dimensions with 8 supercharges. In PartI we analyse the generalised instanton equations on conical extensions of Sasaki- Einstein manifolds. Due to a certain equivariant ansatz, the instanton equations are reduced to a set of coupled, non-linear, ordinary first order differential equations for matrix-valued functions. For the metric Calabi-Yau cone, the instanton equations are the Hermitian Yang-Mills equations and we exploit their geometric structure to gain insights in the structure of the matrix equations. The presented analysis relies strongly on methods used in the context of Nahm equations. For non-Kähler conical extensions, focusing on the string theoretically interesting 6-dimensional case, we first of all construct the relevant SU(3)-structures on the conical extensions and subsequently derive the corresponding matrix equations. -
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. -
Abelian Categories
Abelian Categories Lemma. In an Ab-enriched category with zero object every finite product is coproduct and conversely. π1 Proof. Suppose A × B //A; B is a product. Define ι1 : A ! A × B and π2 ι2 : B ! A × B by π1ι1 = id; π2ι1 = 0; π1ι2 = 0; π2ι2 = id: It follows that ι1π1+ι2π2 = id (both sides are equal upon applying π1 and π2). To show that ι1; ι2 are a coproduct suppose given ' : A ! C; : B ! C. It φ : A × B ! C has the properties φι1 = ' and φι2 = then we must have φ = φid = φ(ι1π1 + ι2π2) = ϕπ1 + π2: Conversely, the formula ϕπ1 + π2 yields the desired map on A × B. An additive category is an Ab-enriched category with a zero object and finite products (or coproducts). In such a category, a kernel of a morphism f : A ! B is an equalizer k in the diagram k f ker(f) / A / B: 0 Dually, a cokernel of f is a coequalizer c in the diagram f c A / B / coker(f): 0 An Abelian category is an additive category such that 1. every map has a kernel and a cokernel, 2. every mono is a kernel, and every epi is a cokernel. In fact, it then follows immediatly that a mono is the kernel of its cokernel, while an epi is the cokernel of its kernel. 1 Proof of last statement. Suppose f : B ! C is epi and the cokernel of some g : A ! B. Write k : ker(f) ! B for the kernel of f. Since f ◦ g = 0 the map g¯ indicated in the diagram exists. -
Homological Algebra Over the Representation Green Functor
Homological Algebra over the Representation Green Functor SPUR Final Paper, Summer 2012 Yajit Jain Mentor: John Ullman Project suggested by: Mark Behrens February 1, 2013 Abstract In this paper we compute Ext RpF; F q for modules over the representation Green functor R with F given to be the fixed point functor. These functors are Mackey functors, defined in terms of a specific group with coefficients in a commutative ring. Previous work by J. Ventura [1] computes these derived k functors for cyclic groups of order 2 with coefficients in F2. We give computations for general cyclic groups with coefficients in a general field of finite characteristic as well as the symmetric group on three elements with coefficients in F2. 1 1 Introduction Mackey functors are algebraic objects that arise in group representation theory and in equivariant stable homotopy theory, where they arise as stable homotopy groups of equivariant spectra. However, they can be given a purely algebraic definition (see [2]), and there are many interesting problems related to them. In this paper we compute derived functors Ext of the internal homomorphism functor defined on the category of modules over the representation Green functor R. These Mackey functors arise in Künneth spectral sequences for equivariant K-theory (see [1]). We begin by giving definitions of the Burnside category and of Mackey functors. These objects depend on a specific finite group G. It is possible to define a tensor product of Mackey functors, allowing us to identify ’rings’ in the category of Mackey functors, otherwise known as Green functors. We can then define modules over Green functors.