INTERACTION BETWEEN CECH COHOMOLOGY and GROUP COHOMOLOGY 1. Cech Cohomology Let I Be Some Index Set and Let U = {U I : I ∈ I}
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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 -
Vector Bundles on Projective Space
Vector Bundles on Projective Space Takumi Murayama December 1, 2013 1 Preliminaries on vector bundles Let X be a (quasi-projective) variety over k. We follow [Sha13, Chap. 6, x1.2]. Definition. A family of vector spaces over X is a morphism of varieties π : E ! X −1 such that for each x 2 X, the fiber Ex := π (x) is isomorphic to a vector space r 0 0 Ak(x).A morphism of a family of vector spaces π : E ! X and π : E ! X is a morphism f : E ! E0 such that the following diagram commutes: f E E0 π π0 X 0 and the map fx : Ex ! Ex is linear over k(x). f is an isomorphism if fx is an isomorphism for all x. A vector bundle is a family of vector spaces that is locally trivial, i.e., for each x 2 X, there exists a neighborhood U 3 x such that there is an isomorphism ': π−1(U) !∼ U × Ar that is an isomorphism of families of vector spaces by the following diagram: −1 ∼ r π (U) ' U × A (1.1) π pr1 U −1 where pr1 denotes the first projection. We call π (U) ! U the restriction of the vector bundle π : E ! X onto U, denoted by EjU . r is locally constant, hence is constant on every irreducible component of X. If it is constant everywhere on X, we call r the rank of the vector bundle. 1 The following lemma tells us how local trivializations of a vector bundle glue together on the entire space X. -
LECTURE 6: FIBER BUNDLES in This Section We Will Introduce The
LECTURE 6: FIBER BUNDLES In this section we will introduce the interesting class of fibrations given by fiber bundles. Fiber bundles play an important role in many geometric contexts. For example, the Grassmaniann varieties and certain fiber bundles associated to Stiefel varieties are central in the classification of vector bundles over (nice) spaces. The fact that fiber bundles are examples of Serre fibrations follows from Theorem ?? which states that being a Serre fibration is a local property. 1. Fiber bundles and principal bundles Definition 6.1. A fiber bundle with fiber F is a map p: E ! X with the following property: every ∼ −1 point x 2 X has a neighborhood U ⊆ X for which there is a homeomorphism φU : U × F = p (U) such that the following diagram commutes in which π1 : U × F ! U is the projection on the first factor: φ U × F U / p−1(U) ∼= π1 p * U t Remark 6.2. The projection X × F ! X is an example of a fiber bundle: it is called the trivial bundle over X with fiber F . By definition, a fiber bundle is a map which is `locally' homeomorphic to a trivial bundle. The homeomorphism φU in the definition is a local trivialization of the bundle, or a trivialization over U. Let us begin with an interesting subclass. A fiber bundle whose fiber F is a discrete space is (by definition) a covering projection (with fiber F ). For example, the exponential map R ! S1 is a covering projection with fiber Z. Suppose X is a space which is path-connected and locally simply connected (in fact, the weaker condition of being semi-locally simply connected would be enough for the following construction). -
Math 210B. Annihilation of Cohomology of Finite Groups 1. Motivation an Important Fact in the Cohomology Theory of Finite Groups
Math 210B. Annihilation of cohomology of finite groups 1. Motivation An important fact in the cohomology theory of finite groups is that if G is a finite group then Hn(G; M) is killed by #G for any n > 0 and any G-module M. This is not at all obvious from the abstract definition (via injective resolutions, say), nor even from the viewpoint of the explicit \bar resolution" method of computing group cohomology. In this handout we present the proof of this fundamental fact as a marvelous concrete application of the abstract fact that erasable δ-functors are universal (Grothendieck's conceptualization of the \degree-shifting" method that had long been used in earlier versions of cohomology theories throughout algebra and topology). Before we turn to the proof, we record a remarkable consequence: Theorem 1.1. If G is finite and M is a G-module that is finitely generated as an abelian group then Hn(G; M) is finite for all n > 0. Proof. From the bar resolution, we see that Hn(G; M) is finitely generated as an abelian group, as the terms of the bar resolution complex are the abelian groups Map(Gj;M) which are visibly finitely generated (as each Gj is a finite set). Hence, since it is also killed by #G, it must be finite! Actually, the finiteness of such higher cohomologies can be seen in an entirely different way, at the cost of losing the precise information of being annihilated by the specific integer #G (which is very useful in some applications). -
Math 704: Part 1: Principal Bundles and Connections
MATH 704: PART 1: PRINCIPAL BUNDLES AND CONNECTIONS WEIMIN CHEN Contents 1. Lie Groups 1 2. Principal Bundles 3 3. Connections and curvature 6 4. Covariant derivatives 12 References 13 1. Lie Groups A Lie group G is a smooth manifold such that the multiplication map G × G ! G, (g; h) 7! gh, and the inverse map G ! G, g 7! g−1, are smooth maps. A Lie subgroup H of G is a subgroup of G which is at the same time an embedded submanifold. A Lie group homomorphism is a group homomorphism which is a smooth map between the Lie groups. The Lie algebra, denoted by Lie(G), of a Lie group G consists of the set of left-invariant vector fields on G, i.e., Lie(G) = fX 2 X (G)j(Lg)∗X = Xg, where Lg : G ! G is the left translation Lg(h) = gh. As a vector space, Lie(G) is naturally identified with the tangent space TeG via X 7! X(e). A Lie group homomorphism naturally induces a Lie algebra homomorphism between the associated Lie algebras. Finally, the universal cover of a connected Lie group is naturally a Lie group, which is in one to one correspondence with the corresponding Lie algebras. Example 1.1. Here are some important Lie groups in geometry and topology. • GL(n; R), GL(n; C), where GL(n; C) can be naturally identified as a Lie sub- group of GL(2n; R). • SL(n; R), O(n), SO(n) = O(n) \ SL(n; R), Lie subgroups of GL(n; R). -
Algebraic Number Theory II
Algebraic number theory II Uwe Jannsen Contents 1 Infinite Galois theory2 2 Projective and inductive limits9 3 Cohomology of groups and pro-finite groups 15 4 Basics about modules and homological Algebra 21 5 Applications to group cohomology 31 6 Hilbert 90 and Kummer theory 41 7 Properties of group cohomology 48 8 Tate cohomology for finite groups 53 9 Cohomology of cyclic groups 56 10 The cup product 63 11 The corestriction 70 12 Local class field theory I 75 13 Three Theorems of Tate 80 14 Abstract class field theory 83 15 Local class field theory II 91 16 Local class field theory III 94 17 Global class field theory I 97 0 18 Global class field theory II 101 19 Global class field theory III 107 20 Global class field theory IV 112 1 Infinite Galois theory An algebraic field extension L/K is called Galois, if it is normal and separable. For this, L/K does not need to have finite degree. For example, for a finite field Fp with p elements (p a prime number), the algebraic closure Fp is Galois over Fp, and has infinite degree. We define in this general situation Definition 1.1 Let L/K be a Galois extension. Then the Galois group of L over K is defined as Gal(L/K) := AutK (L) = {σ : L → L | σ field automorphisms, σ(x) = x for all x ∈ K}. But the main theorem of Galois theory (correspondence between all subgroups of Gal(L/K) and all intermediate fields of L/K) only holds for finite extensions! To obtain the correct answer, one needs a topology on Gal(L/K): Definition 1.2 Let L/K be a Galois extension. -
Remarks on the Cohomology of Finite Fundamental Groups of 3–Manifolds
Geometry & Topology Monographs 14 (2008) 519–556 519 arXiv version: fonts, pagination and layout may vary from GTM published version Remarks on the cohomology of finite fundamental groups of 3–manifolds SATOSHI TOMODA PETER ZVENGROWSKI Computations based on explicit 4–periodic resolutions are given for the cohomology of the finite groups G known to act freely on S3 , as well as the cohomology rings of the associated 3–manifolds (spherical space forms) M = S3=G. Chain approximations to the diagonal are constructed, and explicit contracting homotopies also constructed for the cases G is a generalized quaternion group, the binary tetrahedral group, or the binary octahedral group. Some applications are briefly discussed. 57M05, 57M60; 20J06 1 Introduction The structure of the cohomology rings of 3–manifolds is an area to which Heiner Zieschang devoted much work and energy, especially from 1993 onwards. This could be considered as part of a larger area of his interest, the degrees of maps between oriented 3– manifolds, especially the existence of degree one maps, which in turn have applications in unexpected areas such as relativity theory (cf Shastri, Williams and Zvengrowski [41] and Shastri and Zvengrowski [42]). References [1,6,7, 18, 19, 20, 21, 22, 23] in this paper, all involving work of Zieschang, his students Aaslepp, Drawe, Sczesny, and various colleagues, attest to his enthusiasm for these topics and the remarkable energy he expended studying them. Much of this work involved Seifert manifolds, in particular, references [1, 6, 7, 18, 20, 23]. Of these, [6, 7, 23] (together with [8, 9]) successfully completed the programme of computing the ring structure H∗(M) for any orientable Seifert manifold M with 1 2 3 3 G := π1(M) infinite. -
Group Cohomology in Lean
BEng Individual Project Imperial College London Department of Computing Group Cohomology in Lean Supervisor: Prof. Kevin Buzzard Author: Anca Ciobanu Second Marker: Prof. David Evans July 10, 2019 Abstract The Lean project is a new open source launched in 2013 by Leonardo de Moura at Microsoft Research Redmond that can be viewed as a programming language specialised in theorem proving. It is suited for formalising mathematical defini- tions and theorems, which can help bridge the gap between the abstract aspect of mathematics and the practical part of informatics. My project focuses on using Lean to formalise some essential notions of group cohomology, such as the 0th and 1st cohomology groups, as well as the long exact sequence. This can be seen as a performance test for the new theorem prover, but most im- portantly as an addition to the open source, as group cohomology has yet to be formalised in Lean. Contents 1 Introduction3 1.1 About theorem provers.......................3 1.2 Lean as a solution.........................4 1.3 Achievements............................4 2 Mathematical Background6 2.1 Basic group theory.........................6 2.2 Normal subgroups and homomorphisms.............7 2.3 Quotient groups..........................7 3 Tutorial in Lean9 3.1 Tactics for proving theorems....................9 3.2 Examples.............................. 10 4 Definitions and Theorems of Group Cohomology 13 4.1 Motivation............................. 13 4.2 Modules............................... 14 4.3 0th cohomology group....................... 14 4.4 First cohomology group...................... 16 5 Group Cohomology in Lean 19 5.1 Exact sequence with H0(G; M) only............... 19 5.2 Long exact sequence........................ 22 6 Evaluation 24 6.1 First impressions on Lean.................... -
The Cohomology of Automorphism Groups of Free Groups
The cohomology of automorphism groups of free groups Karen Vogtmann∗ Abstract. There are intriguing analogies between automorphism groups of finitely gen- erated free groups and mapping class groups of surfaces on the one hand, and arithmetic groups such as GL(n, Z) on the other. We explore aspects of these analogies, focusing on cohomological properties. Each cohomological feature is studied with the aid of topolog- ical and geometric constructions closely related to the groups. These constructions often reveal unexpected connections with other areas of mathematics. Mathematics Subject Classification (2000). Primary 20F65; Secondary, 20F28. Keywords. Automorphism groups of free groups, Outer space, group cohomology. 1. Introduction In the 1920s and 30s Jakob Nielsen, J. H. C. Whitehead and Wilhelm Magnus in- vented many beautiful combinatorial and topological techniques in their efforts to understand groups of automorphisms of finitely-generated free groups, a tradition which was supplemented by new ideas of J. Stallings in the 1970s and early 1980s. Over the last 20 years mathematicians have been combining these ideas with others motivated by both the theory of arithmetic groups and that of surface mapping class groups. The result has been a surge of activity which has greatly expanded our understanding of these groups and of their relation to many areas of mathe- matics, from number theory to homotopy theory, Lie algebras to bio-mathematics, mathematical physics to low-dimensional topology and geometric group theory. In this article I will focus on progress which has been made in determining cohomological properties of automorphism groups of free groups, and try to in- dicate how this work is connected to some of the areas mentioned above. -
Modules and Cohomology Over Group Algebras: One Commutative Algebraist’S Perspective
Trends in Commutative Algebra MSRI Publications Volume 51, 2004 Modules and Cohomology over Group Algebras: One Commutative Algebraist's Perspective SRIKANTH IYENGAR Abstract. This article explains basic constructions and results on group algebras and their cohomology, starting from the point of view of commu- tative algebra. It provides the background necessary for a novice in this subject to begin reading Dave Benson's article in this volume. Contents Introduction 51 1. The Group Algebra 52 2. Modules over Group Algebras 56 3. Projective Modules 64 4. Structure of Projectives 69 5. Cohomology of Supplemented Algebras 74 6. Group Cohomology 77 7. Finite Generation of the Cohomology Algebra 79 References 84 Introduction The available accounts of group algebras and group cohomology [Benson 1991a; 1991b; Brown 1982; Evens 1991] are all written for the mathematician on the street. This one is written for commutative algebraists by one of their own. There is a point to such an exercise: though group algebras are typically noncommutative, module theory over them shares many properties with that over commutative rings. Thus, an exposition that draws on these parallels could benefit an algebraist familiar with the commutative world. However, such an endeavour is not without its pitfalls, for often there are subtle differences be- tween the two situations. I have tried to draw attention to similarities and to Mathematics Subject Classification: Primary 13C15, 13C25. Secondary 18G15, 13D45. Part of this article was written while the author was funded by a grant from the NSF. 51 52 SRIKANTH IYENGAR discrepancies between the two subjects in a series of commentaries on the text that appear under the rubric Ramble1. -
WHAT IS a CONNECTION, and WHAT IS IT GOOD FOR? Contents 1. Introduction 2 2. the Search for a Good Directional Derivative 3 3. F
WHAT IS A CONNECTION, AND WHAT IS IT GOOD FOR? TIMOTHY E. GOLDBERG Abstract. In the study of differentiable manifolds, there are several different objects that go by the name of \connection". I will describe some of these objects, and show how they are related to each other. The motivation for many notions of a connection is the search for a sufficiently nice directional derivative, and this will be my starting point as well. The story will by necessity include many supporting characters from differential geometry, all of whom will receive a brief but hopefully sufficient introduction. I apologize for my ungrammatical title. Contents 1. Introduction 2 2. The search for a good directional derivative 3 3. Fiber bundles and Ehresmann connections 7 4. A quick word about curvature 10 5. Principal bundles and principal bundle connections 11 6. Associated bundles 14 7. Vector bundles and Koszul connections 15 8. The tangent bundle 18 References 19 Date: 26 March 2008. 1 1. Introduction In the study of differentiable manifolds, there are several different objects that go by the name of \connection", and this has been confusing me for some time now. One solution to this dilemma was to promise myself that I would some day present a talk about connections in the Olivetti Club at Cornell University. That day has come, and this document contains my notes for this talk. In the interests of brevity, I do not include too many technical details, and instead refer the reader to some lovely references. My main references were [2], [4], and [5]. -
Group Cohomology
Group Cohomology I will define group cohomology H*(G, N) for any group G and any G-module N, and relate this to Hilbert Theorem 90. ∗ The context is ExtR(M; N), for a ring R and two (left) R-modules M; N. This ∗ is a long theory to do everything, but one computation of ExtR goes as follows: (1) Choose a free R-module resolution complex F∗ ! M ! 0 (resolution means exact) ∗ (2) Form the cocomplex of abelian groups HomR(F∗;N). Then ExtR(M; N) is ∗ the cohomology H (HomR(F∗;N)) 0 (3) It is easy to see from half-exactness property of Hom that H = HomR(M; N). (4) The codifferentials HomR(Fk;N) ! HomR(Fk+1;N) are given by `adjoints' of the differentials in F∗. Namely, the codifferential of an R-hom z : Fk ! N is the composition zd : Fk+1 ! Fk ! N. In particular, z is a k-cocycle exactly when this composition zd = 0. The k-coboundaries are all compositions Fk ! Fk−1 ! N, where first map is d. (5) Take M = Z with trivial G action and take R = Z[G]. Note R-modules and G-modules are the same thing. Then H∗(G; N) is defined to be Ext∗ ( ;N). Z[G] Z (6) I will write down a free Z[G] module resolution F∗ ! Z ! 0: As a free abelian group, Fk has Z-basis fg0 < g1; ··· gk >g with the gi 2 G.A plain bracket < a; b; ··· ; x > is interpreted to have the identity e 2 G in front.