The Cohomology Cup Product

Total Page:16

File Type:pdf, Size:1020Kb

The Cohomology Cup Product The Cohomology Cup Product Dan Hathaway April 24, 2011 1 The Cup Product 1.1 Defining The Cup Product and Showing it is Well Defined Consider cohomology with coefficients in some fixed ring R. This is different from what we have been studying so far in class, because up till now our coefficients were in an arbitrary abelian group. We can L n take the direct sum n≥0 H (X) of all cohomology groups of a topological space X to obtain an abelian group. What we would like to do is add a multiplication operation on this group to get a ring. This multiplication will be the cup product. n n Given 2 Z (X), let [ ] represent the cohomology class of . Recall that C (X) = Hom(Cn(X);R), φ 2 Zn(X) means δ(φ) = 0, and φ 2 Bn(X) means φ = δ(φ0) for some (n − 1)-cochain φ0 2 Cn−1(X). L n n To define the cup product ^ on n≥0 H (X), it suffices to define [φ] ^ [ ] for [φ] 2 H (X) and [ ] 2 Hm(X) where n; m ≥ 0 are arbitrary (because then ^ can be defined component wise). To do this, we will use the symbol ^ to denote a product φ ^ of n and m cohains, and we will show that this operation is well defined on cohomology classes. Given φ 2 Cn(X) and 2 Cm(X), define φ ^ to be the (n + m)-cochain that satisfies the following formula for all σ : ∆n+m ! X: (φ ^ )(σ) = φ(σj[v0; :::; vn]) (σj[vn; :::; nn+m]): This formula makes sense because φ(σj[v0; :::; vn]) and (σj[vn; :::; vn+m]) are both elements of R, so they can be multiplied. What we want is an induced ^ operation Hn(X) × Hm(X) ! Hn+m(X): To get this, we must show that the ^ operation Cn(X) × Cm(X) ! Cn+m(X) maps Zn(X) × Zm(X) to Zn+m, and if [φ] = [φ0] and [ ] = [ 0], then [φ ^ ] = [φ0 ^ 0]. Both of these facts are implied by the following Lemma: Lemma: If φ 2 Cn(X) and 2 Cm(X), then δ(φ ^ ) = δφ ^ + (−1)nφ ^ δ . Proof: We will compute δ(φ ^ )(σ), (δφ ^ )(σ), and (φ ^ δ )(σ) separately for an arbitrary σ : ∆n+m+1 ! X. Computing δ(φ ^ ): n+m+1 X i δ(φ ^ )(σ) = (φ ^ )(@σ) = (φ ^ )( (−1) σj[v0; :::; v^i; :::; vn+m+1]) = i=0 n+m+1 X i (−1) (φ ^ )(σj[v0; :::; v^i; :::; vn+m+1]): i=0 The last equality follows because φ ^ is a homomorphism. Computing (δφ ^ )(σ): (δφ ^ )(σ) = (δφ)(σj[v0; :::; vn+1]) (σj[vn+1; :::; vn+m+1]) = φ(@(σj[v0; :::; vn+1])) (:::) = 1 n+1 n+1 X i X i φ( (−1) σj[v0; :::; v^i; :::; vn+1]) (:::) = (−1) φ(σj[v0; :::; v^i; :::; vn+1]) (:::): i=0 i=0 Computing (φ ^ δ )(σ) in the same way: (φ ^ δ )(σ) = φ(σj[v0; :::; vn])(δ )(σj[vn; :::; vn+m+1]) = φ(:::) (@(σj[vn; :::; vn+m+1])) = n+m+1 n+m+1 X i−n X i−n φ(:::) ( (−1) σj[vn; :::; v^i; :::; vn+m+1]) = (−1) φ(:::) (σj[vn; :::; v^i; :::; vn+m+1]): i=n i=n Thus, n+1 n X i (δφ ^ )(σ) + (−1) (φ ^ δ )(σ) = (−1) φ(σj[v0; :::; v^i; :::; vn+1]) (σj[vn+1; :::; vn+m+1])+ i=0 n+m+1 n X i−n (−1) (−1) φ(σj[v0; :::; vn]) (σj[vn; :::; v^i; :::; vn+m+1]): i=n Notice how the last term of the first sum cancels with the first term of the second sum. Comparing the resulting sum to what we calculated δ(φ ^ ) to be, we find that (δφ ^ )(σ) + (−1)n(φ ^ δ )(σ) = δ(φ ^ ). This completes the proof of the lemma. With this lemma in place, it is clear that if φ 2 Zn(X) and 2 Zm(X), then φ ^ 2 Zn+m(X): if δφ = 0 and δ = 0, then δ(φ ^ ) = δφ ^ + (−1)nφ ^ δ = 0 ^ + (−1)nφ ^ 0 = 0 + 0 = 0. Thus, ^ restricts to a map from Zn(X) × Zm(X) to Zn+m(X). Suppose now that φ, φ0 2 Zn(X), ; 0 2 Zm(X), φ − φ0 2 Bn(X), and − 0 2 Bm(X). We want to show that [φ ^ ] = [φ0 ^ 0]. Let φ − φ0 = δφ~ for some φ~ 2 Cn+1(X). The lemma gives us δ(φ~ ^ ) = δφ~ ^ + (−1)nφ ^ δ . Since 2 Zn(X), this means that δ = 0 so δ(φ~ ^ ) = δφ~ ^ . Thus, δφ~ ^ is a coboundary. That is, δφ~ ^ = (φ − φ0) ^ = (φ ^ ) − (φ0 ^ ) is a coboundary. That is, [φ ^ ] = [φ0 ^ ]. In the same way, we can show [φ0 ^ ] = [φ0 ^ 0]. This establishes [φ ^ ] = [φ0 ^ 0]. That is, ^ is a well defined map from Hn(X) × Hm(X) to Hn+m(X). 1.2 Cohomology Ring L n With the cup product defined, it is worth checking that this operation on n≥0 H (X) indeed gives us a ring structure. We have that ^ is associative because given [φ] 2 Hn(X), [ ] 2 Hm(X), and [γ] 2 Hk(X), we have ((φ ^ ) ^ γ)(σ) = φ(σj[v0; :::; vn]) (σj[vn; :::; vn+m])γ(σj[vn+m; :::; vn+m+k]) = (φ ^ ( ^ γ))(σ) so ([φ] ^ [ ]) ^ [γ] = [φ] ^ ([ ] ^ [γ]). We also have that ^ distributes with addition, because if φ, φ0 2 Zn(X) and 2 Zm(X), then 0 0 0 0 ((φ+φ ) ^ )(σ) = (φ+φ )(σj[v0; :::; vn]) (σj[vn; :::; vn+m]) = φ(:::) (:::)+φ (:::) (:::) = (φ ^ +φ ^ )(σ): The same is true for the second argument. Thus, we do indeed have a ring structure on cohomology. In L n fact, we have more than just a ring structure: n≥0 H (X) forms an R-algebra (which can be easily verified). 1.3 Taking the Cohomology Ring is Functorial We have shown that every topological space has associated with it a cohomology ring. The question arises as to if there is a ring homomorphism induced by a continuous function between topological spaces. This turns out to be the case. 2 That is, let X and Y be topological spaces and let f : X ! Y be a continuous function. For each n, ∗ n n we have an induced group homomorphism fn : H (Y ) ! H (X). This induces a group homomorphism ∗ L n L n ∗ f : n≥0 H (Y ) ! n≥0 H (X). We claim that this map f is also a ring homomorphism. This is because if φ is an i-cochain on Y and is a j-cochain on Y , then ∗ ∗ ∗ ∗ (f (φ) ^ f ( ))(σ) = (f (φ))(σj[v0; :::; vi])(f ( ))(σj[vi; :::; vi+j]) = ∗ φ((f ◦ σ)j[v0; :::; vi]) ((f ◦ σ)j[vi; :::; vi+j]) = (φ ^ )(f ◦ σ) = f (φ ^ )(σ): Thus, on cohomology classes we have [f ∗(φ)] ^ [f ∗( )] = [f ∗(φ ^ )]. Thus, for elements a; b 2 L n ∗ ∗ ∗ ∗ n≥0 H (Y ) we have f (a) ^ f (b) = f (a ^ b). That is, f is a ring homomorphism. We have that if X, Y , and Z are topological spaces with the continuous maps f : X ! Y and ∗ ∗ ∗ ∗ ∗ ∗ g : Y ! Z, then fn ◦gn = (f ◦g)n, for all n. This means that f ◦g = (f ◦g) . The fact that these maps L n L n commute is not affected by the additional ring structure that is put on n≥0 H (X), n≥0 H (Y ), and L n n≥0 H (Z). Thus, the operation F of taking the cohomology ring is a (contravariant) functor from the category of topological spaces to the category of rings. 1.4 Cup Product Is Supercommutative L n i j Consider the cohomology ring n≥0 H (X). Let a 2 H and b 2 H . As long as R is commutative (a fact which we are assuming), it turns out that a ^ b = (−1)ijb ^ a. We mention this fact here because we will need this for having a well defined multiplication operation on the tensor product of two cohomology rings. We omit the proof of supercommutivity for brevity. 2 Computing the Cohomology Ring of Simplicial Complexes The definition we gave for ^ can be modified to apply to simplicial complexes. Using this definition, we will compute the cohomology ring of various simplicial complexes. 2.1 Using Z as a Coefficient Ring From now on in this section, we will use Z instead of an arbitrary ring R. Recall an important tool from a past homework assignment for calculating the cohomology of a simplicial complex given that we are using Z for our coefficient group: if all the homology groups Hn(X) are free abelian, then the canonical n homomorphism from the abelian group H (X) to the abelian group Hom(Hn(X); Z) is an isomorphism. We will use this result to compute the cohomology of a space as a first step before we investigate the ring structure induced by the cup product. 2.2 Cohomology Ring of a Point First things first, we will compute the cohomology ring of X where X is a space with a single point. Once this is done, we will know the cohomology ring of any contractible space. In class we showed H0(X) = Z and Hi(X) = 0 for i 6= 0. Since every homology group of X is free abelian, we have i ∼ 0 ∼ H (X) = Hom(Hi(X); Z) for all i. Since H0(X) = Z, we have H (X) = Hom(Z; Z). Since Hi(X) = 0 for i ≥ 0, we have Hi(X) =∼ Hom(0; Z) = 0.
Recommended publications
  • MA3403 Algebraic Topology Lecturer: Gereon Quick Lecture 21
    MA3403 Algebraic Topology Lecturer: Gereon Quick Lecture 21 21. Applications of cup products in cohomology We are going to see some examples where we calculate or apply multiplicative structures on cohomology. But we start with a couple of facts we forgot to mention last time. Relative cup products Let (X;A) be a pair of spaces. The formula which specifies the cup product by its effect on a simplex (' [ )(σ) = '(σj[e0;:::;ep]) (σj[ep;:::;ep+q]) extends to relative cohomology. For, if σ : ∆p+q ! X has image in A, then so does any restriction of σ. Thus, if either ' or vanishes on chains with image in A, then so does ' [ . Hence we get relative cup product maps Hp(X; R) × Hq(X;A; R) ! Hp+q(X;A; R) Hp(X;A; R) × Hq(X; R) ! Hp+q(X;A; R) Hp(X;A; R) × Hq(X;A; R) ! Hp+q(X;A; R): More generally, assume we have two open subsets A and B of X. Then the formula for ' [ on cochains implies that cup product yields a map Sp(X;A; R) × Sq(X;B; R) ! Sp+q(X;A + B; R) where Sn(X;A+B; R) denotes the subgroup of Sn(X; R) of cochains which vanish on sums of chains in A and chains in B. The natural inclusion Sn(X;A [ B; R) ,! Sn(X;A + B; R) induces an isomorphism in cohomology. For we have a map of long exact coho- mology sequences Hn(A [ B) / Hn(X) / Hn(X;A [ B) / Hn+1(A [ B) / Hn+1(X) Hn(A + B) / Hn(X) / Hn(X;A + B) / Hn+1(A + B) / Hn+1(X) 1 2 where we omit the coefficients.
    [Show full text]
  • 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.
    [Show full text]
  • D-Branes, RR-Fields and Duality on Noncommutative Manifolds
    D-BRANES, RR-FIELDS AND DUALITY ON NONCOMMUTATIVE MANIFOLDS JACEK BRODZKI, VARGHESE MATHAI, JONATHAN ROSENBERG, AND RICHARD J. SZABO Abstract. We develop some of the ingredients needed for string theory on noncommutative spacetimes, proposing an axiomatic formulation of T-duality as well as establishing a very general formula for D-brane charges. This formula is closely related to a noncommutative Grothendieck-Riemann-Roch theorem that is proved here. Our approach relies on a very general form of Poincar´eduality, which is studied here in detail. Among the technical tools employed are calculations with iterated products in bivariant K-theory and cyclic theory, which are simplified using a novel diagram calculus reminiscent of Feynman diagrams. Contents Introduction 2 Acknowledgments 3 1. D-Branes and Ramond-Ramond Charges 4 1.1. Flat D-Branes 4 1.2. Ramond-Ramond Fields 7 1.3. Noncommutative D-Branes 9 1.4. Twisted D-Branes 10 2. Poincar´eDuality 13 2.1. Exterior Products in K-Theory 13 2.2. KK-Theory 14 2.3. Strong Poincar´eDuality 16 2.4. Duality Groups 18 arXiv:hep-th/0607020v3 26 Jun 2007 2.5. Spectral Triples 19 2.6. Twisted Group Algebra Completions of Surface Groups 21 2.7. Other Notions of Poincar´eDuality 22 3. KK-Equivalence 23 3.1. Strong KK-Equivalence 24 3.2. Other Notions of KK-Equivalence 25 3.3. Universal Coefficient Theorem 26 3.4. Deformations 27 3.5. Homotopy Equivalence 27 4. Cyclic Theory 27 4.1. Formal Properties of Cyclic Homology Theories 27 4.2. Local Cyclic Theory 29 5.
    [Show full text]
  • Combinatorial Topology and Applications to Quantum Field Theory
    Combinatorial Topology and Applications to Quantum Field Theory by Ryan George Thorngren 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 Vivek Shende, Chair Professor Ian Agol Professor Constantin Teleman Professor Joel Moore Fall 2018 Abstract Combinatorial Topology and Applications to Quantum Field Theory by Ryan George Thorngren Doctor of Philosophy in Mathematics University of California, Berkeley Professor Vivek Shende, Chair Topology has become increasingly important in the study of many-body quantum mechanics, in both high energy and condensed matter applications. While the importance of smooth topology has long been appreciated in this context, especially with the rise of index theory, torsion phenomena and dis- crete group symmetries are relatively new directions. In this thesis, I collect some mathematical results and conjectures that I have encountered in the exploration of these new topics. I also give an introduction to some quantum field theory topics I hope will be accessible to topologists. 1 To my loving parents, kind friends, and patient teachers. i Contents I Discrete Topology Toolbox1 1 Basics4 1.1 Discrete Spaces..........................4 1.1.1 Cellular Maps and Cellular Approximation.......6 1.1.2 Triangulations and Barycentric Subdivision......6 1.1.3 PL-Manifolds and Combinatorial Duality........8 1.1.4 Discrete Morse Flows...................9 1.2 Chains, Cycles, Cochains, Cocycles............... 13 1.2.1 Chains, Cycles, and Homology.............. 13 1.2.2 Pushforward of Chains.................. 15 1.2.3 Cochains, Cocycles, and Cohomology.........
    [Show full text]
  • The Decomposition Theorem, Perverse Sheaves and the Topology Of
    The decomposition theorem, perverse sheaves and the topology of algebraic maps Mark Andrea A. de Cataldo and Luca Migliorini∗ Abstract We give a motivated introduction to the theory of perverse sheaves, culminating in the decomposition theorem of Beilinson, Bernstein, Deligne and Gabber. A goal of this survey is to show how the theory develops naturally from classical constructions used in the study of topological properties of algebraic varieties. While most proofs are omitted, we discuss several approaches to the decomposition theorem, indicate some important applications and examples. Contents 1 Overview 3 1.1 The topology of complex projective manifolds: Lefschetz and Hodge theorems 4 1.2 Families of smooth projective varieties . ........ 5 1.3 Singular algebraic varieties . ..... 7 1.4 Decomposition and hard Lefschetz in intersection cohomology . 8 1.5 Crash course on sheaves and derived categories . ........ 9 1.6 Decomposition, semisimplicity and relative hard Lefschetz theorems . 13 1.7 InvariantCycletheorems . 15 1.8 Afewexamples.................................. 16 1.9 The decomposition theorem and mixed Hodge structures . ......... 17 1.10 Historicalandotherremarks . 18 arXiv:0712.0349v2 [math.AG] 16 Apr 2009 2 Perverse sheaves 20 2.1 Intersection cohomology . 21 2.2 Examples of intersection cohomology . ...... 22 2.3 Definition and first properties of perverse sheaves . .......... 24 2.4 Theperversefiltration . .. .. .. .. .. .. .. 28 2.5 Perversecohomology .............................. 28 2.6 t-exactness and the Lefschetz hyperplane theorem . ...... 30 2.7 Intermediateextensions . 31 ∗Partially supported by GNSAGA and PRIN 2007 project “Spazi di moduli e teoria di Lie” 1 3 Three approaches to the decomposition theorem 33 3.1 The proof of Beilinson, Bernstein, Deligne and Gabber .
    [Show full text]
  • GROUP and GALOIS COHOMOLOGY Romyar Sharifi
    GROUP AND GALOIS COHOMOLOGY Romyar Sharifi Contents Chapter 1. Group cohomology5 1.1. Group rings5 1.2. Group cohomology via cochains6 1.3. Group cohomology via projective resolutions 11 1.4. Homology of groups 14 1.5. Induced modules 16 1.6. Tate cohomology 18 1.7. Dimension shifting 23 1.8. Comparing cohomology groups 24 1.9. Cup products 34 1.10. Tate cohomology of cyclic groups 41 1.11. Cohomological triviality 44 1.12. Tate’s theorem 48 Chapter 2. Galois cohomology 53 2.1. Profinite groups 53 2.2. Cohomology of profinite groups 60 2.3. Galois theory of infinite extensions 64 2.4. Galois cohomology 67 2.5. Kummer theory 69 3 CHAPTER 1 Group cohomology 1.1. Group rings Let G be a group. DEFINITION 1.1.1. The group ring (or, more specifically, Z-group ring) Z[G] of a group G con- sists of the set of finite formal sums of group elements with coefficients in Z ( ) ∑ agg j ag 2 Z for all g 2 G; almost all ag = 0 : g2G with addition given by addition of coefficients and multiplication induced by the group law on G and Z-linearity. (Here, “almost all” means all but finitely many.) In other words, the operations are ∑ agg + ∑ bgg = ∑ (ag + bg)g g2G g2G g2G and ! ! ∑ agg ∑ bgg = ∑ ( ∑ akbk−1g)g: g2G g2G g2G k2G REMARK 1.1.2. In the above, we may replace Z by any ring R, resulting in the R-group ring R[G] of G. However, we shall need here only the case that R = Z.
    [Show full text]
  • K-Theory for Group C -Algebras
    K-theory for group C∗-algebras Paul F. Baum1 and Rub´enJ. S´anchez-Garc´ıa2 1 Mathematics Department 206 McAllister Building The Pennsylvania State University University Park, PA 16802 USA [email protected] 2 Mathematisches Institut Heinrich-Heine-Universit¨atD¨usseldorf Universit¨atsstr. 1 40225 D¨usseldorf Germany [email protected] Final draft (Last compiled on July 30, 2009) Introduction These notes are based on a lecture course given by the first author in the Sedano Winter School on K-theory held in Sedano, Spain, on January 22- 27th of 2007. They aim at introducing K-theory of C∗-algebras, equivariant K-homology and KK-theory in the context of the Baum-Connes conjecture. We start by giving the main definitions, examples and properties of C∗- algebras in Section 1. A central construction is the reduced C∗-algebra of a locally compact, Hausdorff, second countable group G. In Section 2 we define K-theory for C∗-algebras, state the Bott periodicity theorem and establish the connection with Atiyah-Hirzebruch topological K-theory. Our main motivation will be to study the K-theory of the reduced C∗- algebra of a group G as above. The Baum-Connes conjecture asserts that these K-theory groups are isomorphic to the equivariant K-homology groups of a certain G-space, by means of the index map. The G-space is the universal example for proper actions of G, written EG. Hence we procceed by discussing proper actions in Section 3 and the universal space EG in Section 4. Equivariant K-homology is explained in Section 5.
    [Show full text]
  • The Baum-Connes Conjecture: an Extended Survey
    The Baum-Connes conjecture: an extended survey Maria Paula GOMEZ APARICIO, Pierre JULG, and Alain VALETTE May 27, 2019 To Alain Connes, for providing lifelong inspiration Contents 1 Introduction 3 1.1 Building bridges . 3 1.2 In a nutshell - without coefficients... 4 1.3 ... and with coefficients . 5 1.4 Structureofthesenotes ......................... 5 1.5 Whatdoweknowin2019? ....................... 6 1.6 Agreatconjecture?............................ 7 1.7 Whichmathematicsareneeded? . 7 2 Birth of a conjecture 8 2.1 Elliptic (pseudo-) differential operators . 8 2.2 Square-integrablerepresentations . 9 2.3 Enters K-theory for group C∗-algebras................. 11 2.4 TheConnes-Kasparovconjecture . 12 2.5 TheNovikovconjecture .. .. .. .. .. .. .. .. .. .. .. 15 3 Index maps in K-theory: the contribution of Kasparov 17 3.1 Kasparovbifunctor............................ 17 3.2 DiracinductioninKK-theory . 19 arXiv:1905.10081v1 [math.OA] 24 May 2019 3.3 The dual Dirac method and the γ-element............... 19 3.4 FromK-theorytoK-homology . 21 3.5 Generalisation to the p-adiccase .................... 23 4 Towards the official version of the conjecture 25 4.1 Time-dependentleft-handside . 25 4.2 The classifying space for proper actions, and its K-homology . 27 4.3 The Baum-Connes-Higson formulation of the conjecture . .. 27 4.4 Generalizing the γ-elementmethod. .. .. .. .. .. .. .. .. 29 4.4.1 Thecaseofgroupsactingonbolicspaces . 29 1 4.4.2 Tu’sabstractgammaelement . 30 4.4.3 Nishikawa’s new approach . 32 4.5 Consequences of the Baum-Connes conjecture . .. 33 4.5.1 Injectivity: theNovikovconjecture . 33 4.5.2 Injectivity: the Gromov-Lawson-Rosenberg conjecture . .. 35 4.5.3 Surjectivity: the Kadison-Kaplansky conjecture . 35 4.5.4 Surjectivity: vanishing of a topological Whitehead group .
    [Show full text]
  • The Duality Theorem
    Poincar´e Duality Section 3.3 239 The Duality Theorem The form of Poincar´e duality we will prove asserts that for an R orientable closed k → n manifold, a certain naturally defined map H (M; R) Hn−k(M; R) is an isomor- phism. The definition of this map will be in terms of a more general construction called cap product, which has close connections with cup product. Cap Product Let us see how cup product leads naturally to cap product. For an arbitrary space X and coefficient ring R let us for simplicity write Ck(X; R) as Ck and its k = k ∈ k ∈ ` dual C (X; R) HomR(Ck,R) as C . For cochains ϕ C and ψ C we have their + cup product ϕ ` ψ ∈ Ck ` . When we regard ϕ ` ψ as a function of ψ for fixed ϕ, + + we get a map C`→Ck ` , ψ , ϕ ` ψ. One might ask whether this map C`→Ck ` is → the dual of a map Ck+` C` . The answer turns out to be yes, and this map on chains will be the cap product map α , α a ϕ. In order to define α a ϕ it suffices by linearity to take α to be a singular simplex + σ : ∆k `→X , and then the formula for σ a ϕ is rather like the formula defining cup product: a = | ··· | ··· σ ϕ ϕ σ [v0, ,vk] σ [vk, ,vk+`] To say that for fixed ϕ the map α , α a ϕ has as its dual the map ψ , ϕ ` ψ is --------------a→ϕ -----→ψ ` to say that the composition Ck+` C ` R is the map α , (ϕ ψ)(α),orin other words, (∗)ψ(αaϕ) = (ϕ ` ψ)(α) + This holds since for σ : ∆k `→X we have | | ψ(σ a ϕ) = ψ ϕ σ|[v , ···,v ] σ|[v , ···,v + ] 0 k k k ` = | ··· | ··· = ` ϕ σ [v0, ,vk] ψ σ [vk, ,vk+`] (ϕ ψ)(σ ) Another way to write the formula (∗) that may be more suggestive is in the form hα a ϕ, ψi=hα, ϕ ` ψi h− −i × i→ where , is the map Ci C R evaluating a cochain on a chain.
    [Show full text]
  • Algebraic Topology Iv Epiphany Term Lecture
    ALGEBRAIC TOPOLOGY IV k EPIPHANY TERM LECTURE NOTES MARK POWELL This course is about cohomology of spaces, products on cohomology, and man- ifolds. Cohomology is useful primarily because it can be made into a ring using the cup product. We will study the cohomology ring and apply it to manifolds, especially of dimension 2, 3 and 4. For manifolds homology and cohomology can be related to each other in two different ways, using Poincar´eduality and using the universal coefficient theorem. The interplay between these two relations can be extremely powerful. Contents 1. CW complexes and manifolds 2 1.1. CW complexes 2 1.2. Manifolds 2 1.3. Smooth manifolds 3 1.4. Manifolds with boundary 4 2. Homology groups of manifolds 4 2.1. Recap of singular and cellular homology 4 2.2. Top dimensional homology of a manifold 6 2.3. Fundamental classes and degrees of maps 7 3. Cohomology 8 3.1. Hom groups 8 3.2. Algebra of cochain complexes 9 3.3. Cohomology of a topological space 11 3.4. CW cohomology 12 3.5. Understanding cohomology 13 3.6. Properties of cohomology 15 4. Relationships between homology and cohomology 17 4.1. Universal coefficient theorem 17 4.2. Poincar´eduality 18 4.3. An application of both 19 5. Universal coefficient theorem 19 5.1. Ext groups 19 5.2. Examples and properties 23 5.3. The universal coefficient theorem for cohomology 25 6. Univeral coefficients for homology and the K¨unneththeorem 27 6.1. Tensor products 27 6.2. Tor groups 28 1 ALGEBRAIC TOPOLOGY IV k EPIPHANY TERM LECTURE NOTES 2 6.3.
    [Show full text]
  • Real and Complex Projective Spaces — 2
    Real and complex projective spaces | 2 This is a sequel to the file projspaces1.pdf, and the purpose here is to compute the homology and cohomology of real and complex projective spaces. We shall frequently refer to Hatcher for some of the details, but there are also places in which we give alternative approaches. Throughout this document F will denote the real or complex numbers, and d will denote the real dimension dimR F, which of course is 1 if F = R and 2 if F = C. Similar considerations yield analogous results for projective spaces over the quaternions (this is noted at various places in Hatcher), but these are omitted in order to simplify the discussion at a few places. DEFAULT CONVENTION. If no coefficient groups are specified for homology or cohomology groups, the coefficients are assumed to be some commutative ring with unit. Cell decompositions of projective spaces These are described explicitly in Examples 0.4 and 0.6 on pages 6{7 of Hatcher. For each k such that 0 ≤ k ≤ n, this cell decomposition has exactly one k-cell edl in dimension d · k, and the union of all cells through dimension d · k is just the standardly embedded FPk corresponding to the image of the composite Sdk+d−1 ⊂ Sdn+d−1 ! FPk. The explicit attaching maps Sdk ! FPk are described on the cited pages of Hatcher. n Suppose now that n ≥ 2 and F = R, so that π1(FP ) =∼ Z2. Then the give cell decomposition E lifts to a cell decomposition E 0 of the double covering Sn with the following properties: k k 0 (i) For each k such that 0 ≤ k ≤ n there are two k-cells e ⊂ S in E , and they correspond to the upper and lower hemispheres in Sk consisting of all points whose (k + 1)st coordinates k k are nonnegative for e+ and nonpositive for e−.
    [Show full text]
  • The Discrete Hodge Star Operator and Poincaré Duality
    The Discrete Hodge Star Operator and Poincar´eDuality Rachel F. Arnold Dissertation submitted to the Faculty of the Virginia Polytechnic Institute and State University in partial fulfillment of the requirements for the degree of Doctor of Philosophy in Mathematics Peter E. Haskell, Chair William J. Floyd John F. Rossi James E. Thomson May 1, 2012 Blacksburg, Virginia Keywords: Poincar´eDuality, Discrete Hodge Star, Cell Complex, Cubical Whitney Forms Copyright 2012, Rachel F. Arnold The Discrete Hodge Star Operator and Poincar´eDuality Rachel F. Arnold (ABSTRACT) This dissertation is a unification of an analysis-based approach and the traditional topological- based approach to Poincar´eduality. We examine the role of the discrete Hodge star operator in proving and in realizing the Poincar´eduality isomorphism (between cohomology and ho- mology in complementary degrees) in a cellular setting without reference to a dual cell complex. More specifically, we provide a proof of this version of Poincar´eduality over R via the simplicial discrete Hodge star defined by Scott Wilson in [19] without referencing a dual cell complex. We also express the Poincar´eduality isomorphism over both R and Z in terms of this discrete operator. Much of this work is dedicated to extending these results to a cubical setting, via the introduction of a cubical version of Whitney forms. A cubical setting provides a place for Robin Forman's complex of nontraditional differential forms, defined in [7], in the unification of analytic and topological perspectives discussed in this dissertation. In particular, we establish a ring isomorphism (on the cohomology level) be- tween Forman's complex of differential forms with his exterior derivative and product and a complex of cubical cochains with the discrete coboundary operator and the standard cubical cup product.
    [Show full text]