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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. -
1.10 Partitions of Unity and Whitney Embedding 1300Y Geometry and Topology
1.10 Partitions of unity and Whitney embedding 1300Y Geometry and Topology Theorem 1.49 (noncompact Whitney embedding in R2n+1). Any smooth n-manifold may be embedded in R2n+1 (or immersed in R2n). Proof. We saw that any manifold may be written as a countable union of increasing compact sets M = [Ki, and that a regular covering f(Ui;k ⊃ Vi;k;'i;k)g of M can be chosen so that for fixed i, fVi;kgk is a finite ◦ ◦ cover of Ki+1nKi and each Ui;k is contained in Ki+2nKi−1. This means that we can express M as the union of 3 open sets W0;W1;W2, where [ Wj = ([kUi;k): i≡j(mod3) 2n+1 Each of the sets Ri = [kUi;k may be injectively immersed in R by the argument for compact manifolds, 2n+1 since they have a finite regular cover. Call these injective immersions Φi : Ri −! R . The image Φi(Ri) is bounded since all the charts are, by some radius ri. The open sets Ri; i ≡ j(mod3) for fixed j are disjoint, and by translating each Φi; i ≡ j(mod3) by an appropriate constant, we can ensure that their images in R2n+1 are disjoint as well. 0 −! 0 2n+1 Let Φi = Φi + (2(ri−1 + ri−2 + ··· ) + ri) e 1. Then Ψj = [i≡j(mod3)Φi : Wj −! R is an embedding. 2n+1 Now that we have injective immersions Ψ0; Ψ1; Ψ2 of W0;W1;W2 in R , we may use the original argument for compact manifolds: Take the partition of unity subordinate to Ui;k and resum it, obtaining a P P 3-element partition of unity ff1; f2; f3g, with fj = i≡j(mod3) k fi;k. -
EXOTIC SPHERES and CURVATURE 1. Introduction Exotic
BULLETIN (New Series) OF THE AMERICAN MATHEMATICAL SOCIETY Volume 45, Number 4, October 2008, Pages 595–616 S 0273-0979(08)01213-5 Article electronically published on July 1, 2008 EXOTIC SPHERES AND CURVATURE M. JOACHIM AND D. J. WRAITH Abstract. Since their discovery by Milnor in 1956, exotic spheres have pro- vided a fascinating object of study for geometers. In this article we survey what is known about the curvature of exotic spheres. 1. Introduction Exotic spheres are manifolds which are homeomorphic but not diffeomorphic to a standard sphere. In this introduction our aims are twofold: First, to give a brief account of the discovery of exotic spheres and to make some general remarks about the structure of these objects as smooth manifolds. Second, to outline the basics of curvature for Riemannian manifolds which we will need later on. In subsequent sections, we will explore the interaction between topology and geometry for exotic spheres. We will use the term differentiable to mean differentiable of class C∞,and all diffeomorphisms will be assumed to be smooth. As every graduate student knows, a smooth manifold is a topological manifold that is equipped with a smooth (differentiable) structure, that is, a smooth maximal atlas. Recall that an atlas is a collection of charts (homeomorphisms from open neighbourhoods in the manifold onto open subsets of some Euclidean space), the domains of which cover the manifold. Where the chart domains overlap, we impose a smooth compatibility condition for the charts [doC, chapter 0] if we wish our manifold to be smooth. Such an atlas can then be extended to a maximal smooth atlas by including all possible charts which satisfy the compatibility condition with the original maps. -
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. -
Simple Stable Maps of 3-Manifolds Into Surfaces
Tqmlogy. Vol. 35, No. 3, pp. 671-698. 1996 Copyright 0 1996 Elsevier Science Ltd Printed in Great Britain. All rights reserved 004@9383,96/315.00 + 0.00 0040-9383(95)ooo3 SIMPLE STABLE MAPS OF 3-MANIFOLDS INTO SURFACES OSAMU SAEKI~ (Receioedjiir publication 19 June 1995) 1. INTRODUCTION LETS: M3 -+ [w2 be a C” stable map of a closed orientable 3-manifold M into the plane. It is known that the local singularities off consist of three types: definite fold points, indefinite fold points and cusp points (for example, see [l, 91). Note that the singular set S(f) offis a smooth l-dimensional submanifold of M. In their paper [l], Burlet and de Rham have studied those stable maps which have only definite fold points as the singularities and have shown that the source manifolds of such maps, called special generic maps, must be diffeomorphic to the connected sum of S3 and some copies of S’ x S2 (see also [14,16]). On the other hand, Levine [9] has shown that we can eliminate the cusp points of any stable mapfby modifying it homotopically; i.e., every orientable 3-manifold admits a stable map into the plane without cusp points. In this paper we investigate an intermediate class of stable maps, namely simple ones [ 171. A stable mapf: M -+ R2 is simple iffhas no cusp points and if every component of the fiberf -l(x) contains at most one singular point for all x E [w’.In the terminology of [S, lo], fis simple if and only if it has no vertices. -
Enumeration of Non-Orientable 3-Manifolds Using Face Pairing Graphs and Union-Find∗
Enumeration of non-orientable 3-manifolds using face pairing graphs and union-find∗ Benjamin A. Burton Author’s self-archived version Available from http://www.maths.uq.edu.au/~bab/papers/ Abstract Drawing together techniques from combinatorics and computer science, we improve the census algorithm for enumerating closed minimal P2-irreducible 3-manifold triangulations. In particular, new constraints are proven for face pairing graphs, and pruning techniques are improved using a modification of the union-find algorithm. Using these results we catalogue all 136 closed non-orientable P2-irreducible 3-manifolds that can be formed from at most ten tetrahedra. 1 Introduction With recent advances in computing power, topologists have been able to construct exhaustive tables of small 3-manifold triangulations, much like knot theorists have constructed exhaustive tables of simple knot projections. Such tables are valuable sources of data, but they suffer from the fact that enormous amounts of computer time are required to generate them. Where knot tables are often limited by bounding the number of crossings in a knot pro- jection, tables of 3-manifolds generally limit the number of tetrahedra used in a 3-manifold triangulation. A typical table (or census) of 3-manifolds lists all 3-manifolds of a particular type that can be formed from n tetrahedra or fewer. Beyond their generic role as a rich source of examples, tables of this form have a number of specific uses. They still offer the only general means for proving that a triangulation is minimal (i.e., uses as few tetrahedra as possible), much in the same way as knot tables are used to calculate crossing number. -
A New Explicit Way of Obtaining Special Generic Maps Into the 3
A NEW EXPLICIT WAY OF OBTAINING SPECIAL GENERIC MAPS INTO THE 3-DIMENSIONAL EUCLIDEAN SPACE NAOKI KITAZAWA Abstract. A special generic map is a smooth map regarded as a natural gen- eralization of Morse functions with just 2 singular points on homotopy spheres. Canonical projections of unit spheres are simplest examples of such maps and manifolds admitting special generic maps into the plane are completely deter- mined by Saeki in 1993 and ones admitting such maps into general Euclidean spaces are determined under appropriate conditions. Moreover, if the difference of dimensions of source and target manifolds are not so large, then the diffeomorphism types of source manifolds are often limited; for example, homotopy spheres except standard spheres do not admit special generic maps into Euclidean spaces whose dimensions arenot so low. As another example, 4-dimensional simply connected manifolds admitting special generic maps are only manifolds represented as the connected sum of the total spaces of 2-dimensional sphere bundles over the 2-dimensional sphere (or the 4-dimensional standard sphere) and there are many manifolds homeomorphic and not diffeomorphic to these manifolds. These explicit facts make special generic maps attractive objects in the theory of Morse functions and higher dimensional versions and application to algebraic and differentiable topology of manifolds, which is an important study in both singuarity theory of maps and algebraic and differential topology of manifolds. In this paper, we demonstrate a way of construction of special generic maps into the 3-dimensional Euclidean space. For this, first we prepare maps onto 2-dimensional polyhedra regarded as simplicial maps naturally called pseudo quotient maps, which are generalizations of the quotient maps to the spaces of all the connected components of inverse images, so-called Reeb spaces of original smooth maps, being fundamental and important tools in the studies. -
Examples of Bireducible Dehn Fillings
Pacific Journal of Mathematics EXAMPLES OF BIREDUCIBLE DEHN FILLINGS James A. Hoffman and Daniel Matignon Volume 209 No. 1 March 2003 PACIFIC JOURNAL OF MATHEMATICS Vol. 209, No. 1, 2003 EXAMPLES OF BIREDUCIBLE DEHN FILLINGS James A. Hoffman and Daniel Matignon If an irreducible manifold M admits two Dehn fillings along distinct slopes each filling resulting in a reducible manifold, then we call these bireducible Dehn fillings. The first example of bireducible Dehn fillings is due to Gordon and Litherland. More recently, Eudave-Mu˜noz and Wu presented the first in- finite family of manifolds which admit bireducible Dehn fill- ings. We present another infinite family of hyperbolic man- ifolds which admit bireducible Dehn fillings. The manifolds obtained by the fillings are always the connect sum of two lens spaces. 0. Introduction. Let M be an orientable 3-manifold with toroidal boundary T . Given a slope r on T , the Dehn filling of M along r, denoted by M(r), is the manifold obtained by identifying T with the boundary of a solid torus V so that r bounds a meridian disk in V . In this paper, we are especially interested in those Dehn fillings which produce reducible manifolds. Recall that a manifold is reducible if it contains an essential 2-sphere, that is, a 2-sphere which does not bound a 3-ball. If an irreducible manifold M admits two Dehn fillings along distinct slopes each filling resulting in a reducible manifold, then we call these bireducible Dehn fillings. The first example of bireducible Dehn fillings is due to Gordon and Lither- land [GLi]. -
Effective Actions of the Unitary Group on Complex Manifolds
Canad. J. Math. Vol. 54 (6), 2002 pp. 1254–1279 Effective Actions of the Unitary Group on Complex Manifolds A. V. Isaev and N. G. Kruzhilin Abstract. We classify all connected n-dimensional complex manifolds admitting effective actions of the unitary group Un by biholomorphic transformations. One consequence of this classification is a characterization of Cn by its automorphism group. 0 Introduction We are interested in classifying all connected complex manifolds M of dimension n ≥ 2 admitting effective actions of the unitary group Un by biholomorphic trans- formations. It is not hard to show that if dim M < n, then an action of Un by biholo- morphic transformations cannot be effective on M, and therefore n is the smallest possible dimension of M for which one may try to obtain such a classification. One motivation for our study was the following question that we learned from S. Krantz: assume that the group Aut(M) of all biholomorphic automorphisms of M and the group Aut(Cn) of all biholomorphic automorphisms of Cn are isomorphic as topological groups equipped with the compact-open topology; does it imply that M is biholomorphically equivalent to Cn? The group Aut(Cn) is very large (see, e.g., [AL]), and it is not clear from the start what automorphisms of Cn one can use to approach the problem. The isomorphism between Aut(M) and Aut(Cn) induces a continuous effective action on M of any subgroup G ⊂ Aut(Cn). If G is a Lie group, then this action is in fact real-analytic. We consider G = Un which, as it turns out, results in a very short list of manifolds that can occur. -
Solving Variational Problems and Partial Differential Equations Mapping Into General Target Manifolds
Journal of Computational Physics 195 (2004) 263–292 www.elsevier.com/locate/jcp Solving variational problems and partial differential equations mapping into general target manifolds Facundo Memoli a, Guillermo Sapiro a,*, Stanley Osher b a Electrical and Computer Engineering, University of Minnesota, 200 Union Street, Minneapolis, MN 55455, USA b UCLA Mathematics Department, Los Angeles, CA 90095, USA Received 6 May 2003; received in revised form 30 September 2003; accepted 4 October 2003 Abstract A framework for solving variational problems and partial differential equations that define maps onto a given ge- neric manifold is introduced in this paper. We discuss the framework for arbitrary target manifolds, while the domain manifold problem was addressed in [J. Comput. Phys. 174(2) (2001) 759]. The key idea is to implicitly represent the target manifold as the level-set of a higher dimensional function, and then implement the equations in the Cartesian coordinate system where this embedding function is defined. In the case of variational problems, we restrict the search of the minimizing map to the class of maps whose target is the level-set of interest. In the case of partial differential equations, we re-write all the equationÕs geometric characteristics with respect to the embedding function. We then obtain a set of equations that, while defined on the whole Euclidean space, are intrinsic to the implicitly defined target manifold and map into it. This permits the use of classical numerical techniques in Cartesian grids, regardless of the geometry of the target manifold. The extension to open surfaces and submanifolds is addressed in this paper as well. -
DIFFERENTIABLE MANIFOLDS Course C3.1B 2012 Nigel Hitchin
DIFFERENTIABLE MANIFOLDS Course C3.1b 2012 Nigel Hitchin [email protected] 1 Contents 1 Introduction 4 2 Manifolds 6 2.1 Coordinate charts . .6 2.2 The definition of a manifold . .9 2.3 Further examples of manifolds . 11 2.4 Maps between manifolds . 13 3 Tangent vectors and cotangent vectors 14 3.1 Existence of smooth functions . 14 3.2 The derivative of a function . 16 3.3 Derivatives of smooth maps . 20 4 Vector fields 22 4.1 The tangent bundle . 22 4.2 Vector fields as derivations . 26 4.3 One-parameter groups of diffeomorphisms . 28 4.4 The Lie bracket revisited . 32 5 Tensor products 33 5.1 The exterior algebra . 34 6 Differential forms 38 6.1 The bundle of p-forms . 38 6.2 Partitions of unity . 39 6.3 Working with differential forms . 41 6.4 The exterior derivative . 43 6.5 The Lie derivative of a differential form . 47 6.6 de Rham cohomology . 50 2 7 Integration of forms 57 7.1 Orientation . 57 7.2 Stokes' theorem . 62 8 The degree of a smooth map 68 8.1 de Rham cohomology in the top dimension . 68 9 Riemannian metrics 76 9.1 The metric tensor . 76 9.2 The geodesic flow . 80 10 APPENDIX: Technical results 87 10.1 The inverse function theorem . 87 10.2 Existence of solutions of ordinary differential equations . 89 10.3 Smooth dependence . 90 10.4 Partitions of unity on general manifolds . 93 10.5 Sard's theorem (special case) . 94 3 1 Introduction This is an introductory course on differentiable manifolds.