Real and Complex Projective Spaces — 2
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Products in Homology and Cohomology Via Acyclic Models
EILENBERG-ZILBER VIA ACYCLIC MODELS, AND PRODUCTS IN HOMOLOGY AND COHOMOLOGY CHRIS KOTTKE 1. The Eilenberg-Zilber Theorem 1.1. Tensor products of chain complexes. Let C∗ and D∗ be chain complexes. We define the tensor product complex by taking the chain space M M C∗ ⊗ D∗ = (C∗ ⊗ D∗)n ; (C∗ ⊗ D∗)n = Cp ⊗ Dq n2Z p+q=n with differential defined on generators by p @⊗(a ⊗ b) := @a ⊗ b + (−1) a ⊗ @b; a 2 Cp; b 2 Dq (1) and extended to all of C∗ ⊗ D∗ by bilinearity. Note that the sign convention (or 2 something similar to it) is required in order for @⊗ ≡ 0 to hold, i.e. in order for C∗ ⊗ D∗ to be a complex. Recall that if X and Y are CW-complexes, then X × Y has a natural CW- complex structure, with cells given by the products of cells on X and cells on Y: As an exercise in cellular homology computations, you may wish to verify for yourself that CW CW ∼ CW C∗ (X) ⊗ C∗ (Y ) = C∗ (X × Y ): This involves checking that the cellular boundary map satisfies an equation like (1) on products a × b of cellular chains. We would like something similar for general spaces, using singular chains. Of course, the product ∆p × ∆q of simplices is not a p + q simplex, though it can be subdivided into such simplices. There are two ways to do this: one way is direct, involving the combinatorics of so-called \shuffle maps," and is somewhat tedious. The other method goes by the name of \acyclic models" and is a very slick (though nonconstructive) way of producing chain maps between C∗(X) ⊗ C∗(Y ) 1 and C∗(X × Y ); and is the method we shall follow, following [Bre97]. -
Differentiable Manifolds
Prof. A. Cattaneo Institut f¨urMathematik FS 2018 Universit¨atZ¨urich Differentiable Manifolds Solutions to Exercise Sheet 1 p Exercise 1 (A non-differentiable manifold). Consider R with the atlas f(R; id); (R; x 7! sgn(x) x)g. Show R with this atlas is a topological manifold but not a differentiable manifold. p Solution: This follows from the fact that the transition function x 7! sgn(x) x is a homeomor- phism but not differentiable at 0. Exercise 2 (Stereographic projection). Let f : Sn − f(0; :::; 0; 1)g ! Rn be the stereographic projection from N = (0; :::; 0; 1). More precisely, f sends a point p on Sn different from N to the intersection f(p) of the line Np passing through N and p with the equatorial plane xn+1 = 0, as shown in figure 1. Figure 1: Stereographic projection of S2 (a) Find an explicit formula for the stereographic projection map f. (b) Find an explicit formula for the inverse stereographic projection map f −1 (c) If S = −N, U = Sn − N, V = Sn − S and g : Sn ! Rn is the stereographic projection from S, then show that (U; f) and (V; g) form a C1 atlas of Sn. Solution: We show each point separately. (a) Stereographic projection f : Sn − f(0; :::; 0; 1)g ! Rn is given by 1 f(x1; :::; xn+1) = (x1; :::; xn): 1 − xn+1 (b) The inverse stereographic projection f −1 is given by 1 f −1(y1; :::; yn) = (2y1; :::; 2yn; kyk2 − 1): kyk2 + 1 2 Pn i 2 Here kyk = i=1(y ) . -
Homology of Cellular Structures Allowing Multi-Incidence Sylvie Alayrangues, Guillaume Damiand, Pascal Lienhardt, Samuel Peltier
Homology of Cellular Structures Allowing Multi-incidence Sylvie Alayrangues, Guillaume Damiand, Pascal Lienhardt, Samuel Peltier To cite this version: Sylvie Alayrangues, Guillaume Damiand, Pascal Lienhardt, Samuel Peltier. Homology of Cellular Structures Allowing Multi-incidence. Discrete and Computational Geometry, Springer Verlag, 2015, 54 (1), pp.42-77. 10.1007/s00454-015-9662-5. hal-01189215 HAL Id: hal-01189215 https://hal.archives-ouvertes.fr/hal-01189215 Submitted on 15 Dec 2015 HAL is a multi-disciplinary open access L’archive ouverte pluridisciplinaire HAL, est archive for the deposit and dissemination of sci- destinée au dépôt et à la diffusion de documents entific research documents, whether they are pub- scientifiques de niveau recherche, publiés ou non, lished or not. The documents may come from émanant des établissements d’enseignement et de teaching and research institutions in France or recherche français ou étrangers, des laboratoires abroad, or from public or private research centers. publics ou privés. Homology of Cellular Structures allowing Multi-Incidence S. Alayrangues · G. Damiand · P. Lienhardt · S. Peltier Abstract This paper focuses on homology computation over "cellular" structures whose cells are not necessarily homeomorphic to balls and which allow multi- incidence between cells. We deal here with combinatorial maps, more precisely chains of maps and subclasses as generalized maps and maps. Homology computa- tion on such structures is usually achieved by computing simplicial homology on a simplicial analog. But such an approach is computationally expensive as it requires to compute this simplicial analog and to perform the homology computation on a structure containing many more cells (simplices) than the initial one. -
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. -
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. -
0.1 Euler Characteristic
0.1 Euler Characteristic Definition 0.1.1. Let X be a finite CW complex of dimension n and denote by ci the number of i-cells of X. The Euler characteristic of X is defined as: n X i χ(X) = (−1) · ci: (0.1.1) i=0 It is natural to question whether or not the Euler characteristic depends on the cell structure chosen for the space X. As we will see below, this is not the case. For this, it suffices to show that the Euler characteristic depends only on the cellular homology of the space X. Indeed, cellular homology is isomorphic to singular homology, and the latter is independent of the cell structure on X. Recall that if G is a finitely generated abelian group, then G decomposes into a free part and a torsion part, i.e., r G ' Z × Zn1 × · · · Znk : The integer r := rk(G) is the rank of G. The rank is additive in short exact sequences of finitely generated abelian groups. Theorem 0.1.2. The Euler characteristic can be computed as: n X i χ(X) = (−1) · bi(X) (0.1.2) i=0 with bi(X) := rk Hi(X) the i-th Betti number of X. In particular, χ(X) is independent of the chosen cell structure on X. Proof. We use the following notation: Bi = Image(di+1), Zi = ker(di), and Hi = Zi=Bi. Consider a (finite) chain complex of finitely generated abelian groups and the short exact sequences defining homology: dn+1 dn d2 d1 d0 0 / Cn / ::: / C1 / C0 / 0 ι di 0 / Zi / Ci / / Bi−1 / 0 di+1 q 0 / Bi / Zi / Hi / 0 The additivity of rank yields that ci := rk(Ci) = rk(Zi) + rk(Bi−1) and rk(Zi) = rk(Bi) + rk(Hi): Substitute the second equality into the first, multiply the resulting equality by (−1)i, and Pn i sum over i to get that χ(X) = i=0(−1) · rk(Hi). -
Fixed Point Free Involutions on Cohomology Projective Spaces
Indian J. pure appl. Math., 39(3): 285-291, June 2008 °c Printed in India. FIXED POINT FREE INVOLUTIONS ON COHOMOLOGY PROJECTIVE SPACES HEMANT KUMAR SINGH1 AND TEJ BAHADUR SINGH Department of Mathematics, University of Delhi, Delhi 110 007, India e-mail: tej b [email protected] (Received 22 September 2006; after final revision 24 January 2008; accepted 14 February 2008) Let X be a finitistic space with the mod 2 cohomology ring isomorphic to that of CP n, n odd. In this paper, we determine the mod 2 cohomology ring of the orbit space of a fixed point free involution on X. This gives a classification of cohomology type of spaces with the fundamental group Z2 and the covering space a complex projective space. Moreover, we show that there exists no equivariant map Sm ! X for m > 2 relative to the antipodal action on Sm. An analogous result is obtained for a fixed point free involution on a mod 2 cohomology real projective space. Key Words: Projective space; free action; cohomology algebra; spectral sequence 1. INTRODUCTION Suppose that a topological group G acts (continuously) on a topological space X. Associated with the transformation group (G; X) are two new spaces: The fixed point set XG = fx²Xjgx = x; for all g²Gg and the orbit space X=G whose elements are the orbits G(x) = fgxjg²Gg and the topology is induced by the natural projection ¼ : X ! X=G; x ! G(x). If X and Y are G-spaces, then an equivariant map from X to Y is a continuous map Á : X ! Y such that gÁ(x) = Ág(x) for all g²G; x 2 X. -
1 CW Complex, Cellular Homology/Cohomology
Our goal is to develop a method to compute cohomology algebra and rational homotopy group of fiber bundles. 1 CW complex, cellular homology/cohomology Definition 1. (Attaching space with maps) Given topological spaces X; Y , closed subset A ⊂ X, and continuous map f : A ! y. We define X [f Y , X t Y / ∼ n n n−1 n where x ∼ y if x 2 A and f(x) = y. In the case X = D , A = @D = S , D [f X is said to be obtained by attaching to X the cell (Dn; f). n−1 n n Proposition 1. If f; g : S ! X are homotopic, then D [f X and D [g X are homotopic. Proof. Let F : Sn−1 × I ! X be the homotopy between f; g. Then in fact n n n D [f X ∼ (D × I) [F X ∼ D [g X Definition 2. (Cell space, cell complex, cellular map) 1. A cell space is a topological space obtained from a finite set of points by iterating the procedure of attaching cells of arbitrary dimension, with the condition that only finitely many cells of each dimension are attached. 2. If each cell is attached to cells of lower dimension, then the cell space X is called a cell complex. Define the n−skeleton of X to be the subcomplex consisting of cells of dimension less than n, denoted by Xn. 3. A continuous map f between cell complexes X; Y is called cellular if it sends Xk to Yk for all k. Proposition 2. 1. Every cell space is homotopic to a cell complex. -
The Real Projective Spaces in Homotopy Type Theory
The real projective spaces in homotopy type theory Ulrik Buchholtz Egbert Rijke Technische Universität Darmstadt Carnegie Mellon University Email: [email protected] Email: [email protected] Abstract—Homotopy type theory is a version of Martin- topology and homotopy theory developed in homotopy Löf type theory taking advantage of its homotopical models. type theory (homotopy groups, including the fundamen- In particular, we can use and construct objects of homotopy tal group of the circle, the Hopf fibration, the Freuden- theory and reason about them using higher inductive types. In this article, we construct the real projective spaces, key thal suspension theorem and the van Kampen theorem, players in homotopy theory, as certain higher inductive types for example). Here we give an elementary construction in homotopy type theory. The classical definition of RPn, in homotopy type theory of the real projective spaces as the quotient space identifying antipodal points of the RPn and we develop some of their basic properties. n-sphere, does not translate directly to homotopy type theory. R n In classical homotopy theory the real projective space Instead, we define P by induction on n simultaneously n with its tautological bundle of 2-element sets. As the base RP is either defined as the space of lines through the + case, we take RP−1 to be the empty type. In the inductive origin in Rn 1 or as the quotient by the antipodal action step, we take RPn+1 to be the mapping cone of the projection of the 2-element group on the sphere Sn [4]. -
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. -
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......... -
Algebraic Topology 565 2016
Algebraic Topology 565 2016 February 21, 2016 The general format of the course is as in Fall quarter. We'll use Hatcher Chapters 3-4, and we'll start using selected part of Milnor's Characteristic classes. One global notation change: From now on we fix a principal ideal domain R, and let H∗X denote H∗(X; R). This change extends in the obvious way to other notations: C∗X means RS·X (singular chains with coefficients in R), tensor products and Tor are over R, cellular homology is with coefficients in R, and so on. Course outline Note: Applications and exercises are still to appear. Some parts of the outline below won't make sense yet, but still serve to give the general idea. 1. Homology of products. There are two steps to compute the homology of a product ∼ X × Y : (i) The Eilenberg-Zilber theorem that gives a chain equivalence C∗X ⊗ C∗Y = C∗(X × Y ), and (ii) the purely algebraic Kunneth theorem that expresses the homology of a tensor product of chain complexes in terms of tensor products and Tor's of the homology of the individual complexes. I plan to only state part (ii) and leave the proof to the text. On the other hand, I'll take a very different approach to (i), not found in Hatcher: the method of acyclic models. This more categorical approach is very slick and yields easy proofs of some technical theorems that are crucial for the cup product in cohomology later. There are explicit formulas for certain choices of the above chain equivalence and its inverse; in particular there is a very simple and handy formula for an inverse, known as the Alexander- Whitney map.