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On the Stable Classification of Certain 4-Manifolds
BULL. AUSTRAL. MATH. SOC. 57N65, 57R67, 57Q10, 57Q20 VOL. 52 (1995) [385-398] ON THE STABLE CLASSIFICATION OF CERTAIN 4-MANIFOLDS ALBERTO CAVICCHIOLI, FRIEDRICH HEGENBARTH AND DUSAN REPOVS We study the s-cobordism type of closed orientable (smooth or PL) 4—manifolds with free or surface fundamental groups. We prove stable classification theorems for these classes of manifolds by using surgery theory. 1. INTRODUCTION In this paper we shall study closed connected (smooth or PL) 4—manifolds with special fundamental groups as free products or surface groups. For convenience, all manifolds considered will be assumed to be orientable although our results work also in the general case, provided the first Stiefel-Whitney classes coincide. The starting point for classifying manifolds is the determination of their homotopy type. For 4- manifolds having finite fundamental groups with periodic homology of period four, this was done in [12] (see also [1] and [2]). The case of a cyclic fundamental group of prime order was first treated in [23]. The homotopy type of 4-manifolds with free or surface fundamental groups was completely classified in [6] and [7] respectively. In particular, closed 4-manifolds M with a free fundamental group IIi(M) = *PZ (free product of p factors Z ) are classified, up to homotopy, by the isomorphism class of their intersection pairings AM : B2{M\K) x H2(M;A) —> A over the integral group ring A = Z[IIi(M)]. For Ui(M) = Z, we observe that the arguments developed in [11] classify these 4-manifolds, up to TOP homeomorphism, in terms of their intersection forms over Z. -
Persistent Obstruction Theory for a Model Category of Measures with Applications to Data Merging
TRANSACTIONS OF THE AMERICAN MATHEMATICAL SOCIETY, SERIES B Volume 8, Pages 1–38 (February 2, 2021) https://doi.org/10.1090/btran/56 PERSISTENT OBSTRUCTION THEORY FOR A MODEL CATEGORY OF MEASURES WITH APPLICATIONS TO DATA MERGING ABRAHAM D. SMITH, PAUL BENDICH, AND JOHN HARER Abstract. Collections of measures on compact metric spaces form a model category (“data complexes”), whose morphisms are marginalization integrals. The fibrant objects in this category represent collections of measures in which there is a measure on a product space that marginalizes to any measures on pairs of its factors. The homotopy and homology for this category allow measurement of obstructions to finding measures on larger and larger product spaces. The obstruction theory is compatible with a fibrant filtration built from the Wasserstein distance on measures. Despite the abstract tools, this is motivated by a widespread problem in data science. Data complexes provide a mathematical foundation for semi- automated data-alignment tools that are common in commercial database software. Practically speaking, the theory shows that database JOIN oper- ations are subject to genuine topological obstructions. Those obstructions can be detected by an obstruction cocycle and can be resolved by moving through a filtration. Thus, any collection of databases has a persistence level, which measures the difficulty of JOINing those databases. Because of its general formulation, this persistent obstruction theory also encompasses multi-modal data fusion problems, some forms of Bayesian inference, and probability cou- plings. 1. Introduction We begin this paper with an abstraction of a problem familiar to any large enterprise. Imagine that the branch offices within the enterprise have access to many data sources. -
Obstructions, Extensions and Reductions. Some Applications Of
Obstructions, Extensions and Reductions. Some applications of Cohomology ∗ Luis J. Boya Departamento de F´ısica Te´orica, Universidad de Zaragoza. E-50009 Zaragoza, Spain [email protected] October 22, 2018 Abstract After introducing some cohomology classes as obstructions to ori- entation and spin structures etc., we explain some applications of co- homology to physical problems, in especial to reduced holonomy in M- and F -theories. 1 Orientation For a topological space X, the important objects are the homology groups, H∗(X, A), with coefficients A generally in Z, the integers. A bundle ξ : E(M, F ) is an extension E with fiber F (acted upon by a group G) over an space M, noted ξ : F → E → M and it is itself a Cech˘ cohomology element, arXiv:math-ph/0310010v1 8 Oct 2003 ξ ∈ Hˆ 1(M,G). The important objects here the characteristic cohomology classes c(ξ) ∈ H∗(M, A). Let M be a manifold of dimension n. Consider a frame e in a patch U ⊂ M, i.e. n independent vector fields at any point in U. Two frames e, e′ in U define a unique element g of the general linear group GL(n, R) by e′ = g · e, as GL acts freely in {e}. An orientation in M is a global class of frames, two frames e (in U) and e′ (in U ′) being in the same class if det g > 0 where e′ = g · e in the overlap of two patches. A manifold is orientable if it is ∗To be published in the Proceedings of: SYMMETRIES AND GRAVITY IN FIELD THEORY. -
PIECEWISE LINEAR TOPOLOGY Contents 1. Introduction 2 2. Basic
PIECEWISE LINEAR TOPOLOGY J. L. BRYANT Contents 1. Introduction 2 2. Basic Definitions and Terminology. 2 3. Regular Neighborhoods 9 4. General Position 16 5. Embeddings, Engulfing 19 6. Handle Theory 24 7. Isotopies, Unknotting 30 8. Approximations, Controlled Isotopies 31 9. Triangulations of Manifolds 33 References 35 1 2 J. L. BRYANT 1. Introduction The piecewise linear category offers a rich structural setting in which to study many of the problems that arise in geometric topology. The first systematic ac- counts of the subject may be found in [2] and [63]. Whitehead’s important paper [63] contains the foundation of the geometric and algebraic theory of simplicial com- plexes that we use today. More recent sources, such as [30], [50], and [66], together with [17] and [37], provide a fairly complete development of PL theory up through the early 1970’s. This chapter will present an overview of the subject, drawing heavily upon these sources as well as others with the goal of unifying various topics found there as well as in other parts of the literature. We shall try to give enough in the way of proofs to provide the reader with a flavor of some of the techniques of the subject, while deferring the more intricate details to the literature. Our discussion will generally avoid problems associated with embedding and isotopy in codimension 2. The reader is referred to [12] for a survey of results in this very important area. 2. Basic Definitions and Terminology. Simplexes. A simplex of dimension p (a p-simplex) σ is the convex closure of a n set of (p+1) geometrically independent points {v0, . -
Finite Group Actions on Kervaire Manifolds 3
FINITE GROUP ACTIONS ON KERVAIRE MANIFOLDS DIARMUID CROWLEY AND IAN HAMBLETON M4k+2 Abstract. Let K be the Kervaire manifold: a closed, piecewise linear (PL) mani- fold with Kervaire invariant 1 and the same homology as the product S2k+1 × S2k+1 of M4k+2 spheres. We show that a finite group of odd order acts freely on K if and only if 2k+1 2k+1 it acts freely on S × S . If MK is smoothable, then each smooth structure on M j M4k+2 K admits a free smooth involution. If k 6= 2 − 1, then K does not admit any M30 M62 free TOP involutions. Free “exotic” (PL) involutions are constructed on K , K , and M126 M30 Z Z K . Each smooth structure on K admits a free /2 × /2 action. 1. Introduction One of the main themes in geometric topology is the study of smooth manifolds and their piece-wise linear (PL) triangulations. Shortly after Milnor’s discovery [54] of exotic smooth 7-spheres, Kervaire [39] constructed the first example (in dimension 10) of a PL- manifold with no differentiable structure, and a new exotic smooth 9-sphere Σ9. The construction of Kervaire’s 10-dimensional manifold was generalized to all dimen- sions of the form m ≡ 2 (mod 4), via “plumbing” (see [36, §8]). Let P 4k+2 denote the smooth, parallelizable manifold of dimension 4k+2, k ≥ 0, constructed by plumbing two copies of the the unit tangent disc bundle of S2k+1. The boundary Σ4k+1 = ∂P 4k+2 is a smooth homotopy sphere, now usually called the Kervaire sphere. -
Mapping Surgery to Analysis III: Exact Sequences
K-Theory (2004) 33:325–346 © Springer 2005 DOI 10.1007/s10977-005-1554-7 Mapping Surgery to Analysis III: Exact Sequences NIGEL HIGSON and JOHN ROE Department of Mathematics, Penn State University, University Park, Pennsylvania 16802. e-mail: [email protected]; [email protected] (Received: February 2004) Abstract. Using the constructions of the preceding two papers, we construct a natural transformation (after inverting 2) from the Browder–Novikov–Sullivan–Wall surgery exact sequence of a compact manifold to a certain exact sequence of C∗-algebra K-theory groups. Mathematics Subject Classifications (1991): 19J25, 19K99. Key words: C∗-algebras, L-theory, Poincare´ duality, signature operator. This is the final paper in a series of three whose objective is to construct a natural transformation from the surgery exact sequence of Browder, Novikov, Sullivan and Wall [17,21] to a long exact sequence of K-theory groups associated to a certain C∗-algebra extension; we finally achieve this objective in Theorem 5.4. In the first paper [5], we have shown how to associate a homotopy invariant C∗-algebraic signature to suitable chain complexes of Hilbert modules satisfying Poincare´ duality. In the second paper, we have shown that such Hilbert–Poincare´ complexes arise natu- rally from geometric examples of manifolds and Poincare´ complexes. The C∗-algebras that are involved in these calculations are analytic reflections of the equivariant and/or controlled structure of the underlying topology. In paper II [6] we have also clarified the relationship between the analytic signature, defined by the procedure of paper I for suitable Poincare´ com- plexes, and the analytic index of the signature operator, defined only for manifolds. -
Math 527 - Homotopy Theory Obstruction Theory
Math 527 - Homotopy Theory Obstruction theory Martin Frankland April 5, 2013 In our discussion of obstruction theory via the skeletal filtration, we left several claims as exercises. The goal of these notes is to fill in two of those gaps. 1 Setup Let us recall the setup, adopting a notation similar to that of May x 18.5. Let (X; A) be a relative CW complex with n-skeleton Xn, and let Y be a simple space. Given two maps fn; gn : Xn ! Y which agree on Xn−1, we defined a difference cochain n d(fn; gn) 2 C (X; A; πn(Y )) whose value on each n-cell was defined using the following \double cone construction". Definition 1.1. Let H; H0 : Dn ! Y be two maps that agree on the boundary @Dn ∼= Sn−1. The difference construction of H and H0 is the map 0 n ∼ n n H [ H : S = D [Sn−1 D ! Y: Here, the two terms Dn are viewed as the upper and lower hemispheres of Sn respectively. 1 2 The two claims In this section, we state two claims and reduce their proof to the case of spheres and discs. Proposition 2.1. Given two maps fn; gn : Xn ! Y which agree on Xn−1, we have fn ' gn rel Xn−1 if and only if d(fn; gn) = 0 holds. n n−1 Proof. For each n-cell eα of X n A, consider its attaching map 'α : S ! Xn−1 and charac- n n−1 teristic map Φα :(D ;S ) ! (Xn;Xn−1). -
Arxiv:2101.06841V2 [Math.AT] 1 Apr 2021
C2-EQUIVARIANT TOPOLOGICAL MODULAR FORMS DEXTER CHUA Abstract. We compute the homotopy groups of the C2 fixed points of equi- variant topological modular forms at the prime 2 using the descent spectral sequence. We then show that as a TMF-module, it is isomorphic to the tensor product of TMF with an explicit finite cell complex. Contents 1. Introduction 1 2. Equivariant elliptic cohomology 5 3. The E2 page of the DSS 9 4. Differentials in the DSS 13 5. Identification of the last factor 25 6. Further questions 29 Appendix A. Connective C2-equivariant tmf 30 Appendix B. Sage script 35 References 38 1. Introduction Topological K-theory is one of the first examples of generalized cohomology theories. It admits a natural equivariant analogue — for a G-space X, the group 0 KOG(X) is the Grothendieck group of G-equivariant vector bundles over X. In 0 particular, KOG(∗) = Rep(G) is the representation ring of G. As in the case of non-equivariant K-theory, this extends to a G-equivariant cohomology theory KOG, and is represented by a genuine G-spectrum. We shall call this G-spectrum KO, omitting the subscript, as we prefer to think of this as a global equivariant spectrum — one defined for all compact Lie groups. The G-fixed points of this, written KOBG, is a spectrum analogue of the representation ring, BG 0 BG −n with π0KO = KOG(∗) = Rep(G) (more generally, πnKO = KOG (∗)). These fixed point spectra are readily computable as KO-modules. For example, KOBC2 = KO _ KO; KOBC3 = KO _ KU: arXiv:2101.06841v2 [math.AT] 1 Apr 2021 This corresponds to the fact that C2 has two real characters, while C3 has a real character plus a complex conjugate pair. -
ON TOPOLOGICAL and PIECEWISE LINEAR VECTOR FIELDS-T
ON TOPOLOGICAL AND PIECEWISE LINEAR VECTOR FIELDS-t RONALD J. STERN (Received31 October1973; revised 15 November 1974) INTRODUCTION THE existence of a non-zero vector field on a differentiable manifold M yields geometric and algebraic information about M. For example, (I) A non-zero vector field exists on M if and only if the tangent bundle of M splits off a trivial bundle. (2) The kth Stiefel-Whitney class W,(M) of M is the primary obstruction to obtaining (n -k + I) linearly independent non-zero vector fields on M [37; 0391. In particular, a non-zero vector field exists on a compact manifold M if and only if X(M), the Euler characteristic of M, is zero. (3) Every non-zero vector field on M is integrable. Now suppose that M is a topological (TOP) or piecewise linear (IX) manifold. What is the appropriate definition of a TOP or PL vector field on M? If M were differentiable, then a non-zero vector field is just a non-zero cross-section of the tangent bundle T(M) of M. In I%2 Milnor[29] define! the TOP tangent microbundle T(M) of a TOP manifold M to be the microbundle M - M x M G M, where A(x) = (x, x) and ~(x, y) = x. If M is a PL manifold, the PL tangent microbundle T(M) is defined similarly if one works in the category of PL maps of polyhedra. If M is differentiable, then T(M) is CAT (CAT = TOP or PL) microbundle equivalent to T(M). -
Symmetric Obstruction Theories and Hilbert Schemes of Points On
Symmetric Obstruction Theories and Hilbert Schemes of Points on Threefolds K. Behrend and B. Fantechi March 12, 2018 Abstract Recall that in an earlier paper by one of the authors Donaldson- Thomas type invariants were expressed as certain weighted Euler char- acteristics of the moduli space. The Euler characteristic is weighted by a certain canonical Z-valued constructible function on the moduli space. This constructible function associates to any point of the moduli space a certain invariant of the singularity of the space at the point. In the present paper, we evaluate this invariant for the case of a sin- gularity which is an isolated point of a C∗-action and which admits a symmetric obstruction theory compatible with the C∗-action. The an- swer is ( 1)d, where d is the dimension of the Zariski tangent space. − We use this result to prove that for any threefold, proper or not, the weighted Euler characteristic of the Hilbert scheme of n points on the threefold is, up to sign, equal to the usual Euler characteristic. For the case of a projective Calabi-Yau threefold, we deduce that the Donaldson- Thomas invariant of the Hilbert scheme of n points is, up to sign, equal to the Euler characteristic. This proves a conjecture of Maulik-Nekrasov- Okounkov-Pandharipande. arXiv:math/0512556v1 [math.AG] 24 Dec 2005 1 Contents Introduction 3 Symmetric obstruction theories . 3 Weighted Euler characteristics and Gm-actions . .. .. 4 Anexample........................... 5 Lagrangian intersections . 5 Hilbertschemes......................... 6 Conventions........................... 6 Acknowledgments. .. .. .. .. .. .. 7 1 Symmetric Obstruction Theories 8 1.1 Non-degenerate symmetric bilinear forms . -
Almost Complex Structures and Obstruction Theory
ALMOST COMPLEX STRUCTURES AND OBSTRUCTION THEORY MICHAEL ALBANESE Abstract. These are notes for a lecture I gave in John Morgan's Homotopy Theory course at Stony Brook in Fall 2018. Let X be a CW complex and Y a simply connected space. Last time we discussed the obstruction to extending a map f : X(n) ! Y to a map X(n+1) ! Y ; recall that X(k) denotes the k-skeleton of X. n+1 There is an obstruction o(f) 2 C (X; πn(Y )) which vanishes if and only if f can be extended to (n+1) n+1 X . Moreover, o(f) is a cocycle and [o(f)] 2 H (X; πn(Y )) vanishes if and only if fjX(n−1) can be extended to X(n+1); that is, f may need to be redefined on the n-cells. Obstructions to lifting a map p Given a fibration F ! E −! B and a map f : X ! B, when can f be lifted to a map g : X ! E? If X = B and f = idB, then we are asking when p has a section. For convenience, we will only consider the case where F and B are simply connected, from which it follows that E is simply connected. For a more general statement, see Theorem 7.37 of [2]. Suppose g has been defined on X(n). Let en+1 be an n-cell and α : Sn ! X(n) its attaching map, then p ◦ g ◦ α : Sn ! B is equal to f ◦ α and is nullhomotopic (as f extends over the (n + 1)-cell). -
Surgery on Compact Manifolds, Second Edition, 1999 68 David A
http://dx.doi.org/10.1090/surv/069 Selected Titles in This Series 69 C. T. C. Wall (A. A. Ranicki, Editor), Surgery on compact manifolds, Second Edition, 1999 68 David A. Cox and Sheldon Katz, Mirror symmetry and algebraic geometry, 1999 67 A. Borel and N. Wallach, Continuous cohomology, discrete subgroups, and representations of reductive groups, Second Edition, 1999 66 Yu. Ilyashenko and Weigu Li, Nonlocal bifurcations, 1999 65 Carl Faith, Rings and things and a fine array of twentieth century associative algebra, 1999 64 Rene A. Carmona and Boris Rozovskii, Editors, Stochastic partial differential equations: Six perspectives, 1999 63 Mark Hovey, Model categories, 1999 62 Vladimir I. Bogachev, Gaussian measures, 1998 61 W. Norrie Everitt and Lawrence Markus, Boundary value problems and symplectic algebra for ordinary differential and quasi-differential operators, 1999 60 Iain Raeburn and Dana P. Williams, Morita equivalence and continuous-trace C*-algebras, 1998 59 Paul Howard and Jean E. Rubin, Consequences of the axiom of choice, 1998 58 Pavel I. Etingof, Igor B. Frenkel, and Alexander A. Kirillov, Jr., Lectures on representation theory and Knizhnik-Zamolodchikov equations, 1998 57 Marc Levine, Mixed motives, 1998 56 Leonid I. Korogodski and Yan S. Soibelman, Algebras of functions on quantum groups: Part I, 1998 55 J. Scott Carter and Masahico Saito, Knotted surfaces and their diagrams, 1998 54 Casper Goffman, Togo Nishiura, and Daniel Waterman, Homeomorphisms in analysis, 1997 53 Andreas Kriegl and Peter W. Michor, The convenient setting of global analysis, 1997 52 V. A. Kozlov, V. G. Maz'ya> and J. Rossmann, Elliptic boundary value problems in domains with point singularities, 1997 51 Jan Maly and William P.