Handlebody Complements in the 3-Sphere: a Remark on a Theorem of Fox
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Ricci Curvature and Minimal Submanifolds
Pacific Journal of Mathematics RICCI CURVATURE AND MINIMAL SUBMANIFOLDS Thomas Hasanis and Theodoros Vlachos Volume 197 No. 1 January 2001 PACIFIC JOURNAL OF MATHEMATICS Vol. 197, No. 1, 2001 RICCI CURVATURE AND MINIMAL SUBMANIFOLDS Thomas Hasanis and Theodoros Vlachos The aim of this paper is to find necessary conditions for a given complete Riemannian manifold to be realizable as a minimal submanifold of a unit sphere. 1. Introduction. The general question that served as the starting point for this paper was to find necessary conditions on those Riemannian metrics that arise as the induced metrics on minimal hypersurfaces or submanifolds of hyperspheres of a Euclidean space. There is an abundance of complete minimal hypersurfaces in the unit hy- persphere Sn+1. We recall some well known examples. Let Sm(r) = {x ∈ Rn+1, |x| = r},Sn−m(s) = {y ∈ Rn−m+1, |y| = s}, where r and s are posi- tive numbers with r2 + s2 = 1; then Sm(r) × Sn−m(s) = {(x, y) ∈ Rn+2, x ∈ Sm(r), y ∈ Sn−m(s)} is a hypersurface of the unit hypersphere in Rn+2. As is well known, this hypersurface has two distinct constant principal cur- vatures: One is s/r of multiplicity m, the other is −r/s of multiplicity n − m. This hypersurface is called a Clifford hypersurface. Moreover, it is minimal only in the case r = pm/n, s = p(n − m)/n and is called a Clifford minimal hypersurface. Otsuki [11] proved that if M n is a com- pact minimal hypersurface in Sn+1 with two distinct principal curvatures of multiplicity greater than 1, then M n is a Clifford minimal hypersur- face Sm(pm/n) × Sn−m(p(n − m)/n), 1 < m < n − 1. -
Mapping Class Group of a Handlebody
FUNDAMENTA MATHEMATICAE 158 (1998) Mapping class group of a handlebody by Bronis law W a j n r y b (Haifa) Abstract. Let B be a 3-dimensional handlebody of genus g. Let M be the group of the isotopy classes of orientation preserving homeomorphisms of B. We construct a 2-dimensional simplicial complex X, connected and simply-connected, on which M acts by simplicial transformations and has only a finite number of orbits. From this action we derive an explicit finite presentation of M. We consider a 3-dimensional handlebody B = Bg of genus g > 0. We may think of B as a solid 3-ball with g solid handles attached to it (see Figure 1). Our goal is to determine an explicit presentation of the map- ping class group of B, the group Mg of the isotopy classes of orientation preserving homeomorphisms of B. Every homeomorphism h of B induces a homeomorphism of the boundary S = ∂B of B and we get an embedding of Mg into the mapping class group MCG(S) of the surface S. z-axis α α α α 1 2 i i+1 . . β β 1 2 ε x-axis i δ -2, i Fig. 1. Handlebody An explicit and quite simple presentation of MCG(S) is now known, but it took a lot of time and effort of many people to reach it (see [1], [3], [12], 1991 Mathematics Subject Classification: 20F05, 20F38, 57M05, 57M60. This research was partially supported by the fund for the promotion of research at the Technion. [195] 196 B.Wajnryb [9], [7], [11], [6], [14]). -
Isoparametric Hypersurfaces with Four Principal Curvatures Revisited
ISOPARAMETRIC HYPERSURFACES WITH FOUR PRINCIPAL CURVATURES REVISITED QUO-SHIN CHI Abstract. The classification of isoparametric hypersurfaces with four principal curvatures in spheres in [2] hinges on a crucial charac- terization, in terms of four sets of equations of the 2nd fundamental form tensors of a focal submanifold, of an isoparametric hypersur- face of the type constructed by Ferus, Karcher and Munzner.¨ The proof of the characterization in [2] is an extremely long calculation by exterior derivatives with remarkable cancellations, which is mo- tivated by the idea that an isoparametric hypersurface is defined by an over-determined system of partial differential equations. There- fore, exterior differentiating sufficiently many times should gather us enough information for the conclusion. In spite of its elemen- tary nature, the magnitude of the calculation and the surprisingly pleasant cancellations make it desirable to understand the under- lying geometric principles. In this paper, we give a conceptual, and considerably shorter, proof of the characterization based on Ozeki and Takeuchi's expan- sion formula for the Cartan-Munzner¨ polynomial. Along the way the geometric meaning of these four sets of equations also becomes clear. 1. Introduction In [2], isoparametric hypersurfaces with four principal curvatures and multiplicities (m1; m2); m2 ≥ 2m1 − 1; in spheres were classified to be exactly the isoparametric hypersurfaces of F KM-type constructed by Ferus Karcher and Munzner¨ [4]. The classification goes as follows. Let M+ be a focal submanifold of codimension m1 of an isoparametric hypersurface in a sphere, and let N be the normal bundle of M+ in the sphere. Suppose on the unit normal bundle UN of N there hold true 1991 Mathematics Subject Classification. -
[Math.GT] 31 Mar 2004
CORES OF S-COBORDISMS OF 4-MANIFOLDS Frank Quinn March 2004 Abstract. The main result is that an s-cobordism (topological or smooth) of 4- manifolds has a product structure outside a “core” sub s-cobordism. These cores are arranged to have quite a bit of structure, for example they are smooth and abstractly (forgetting boundary structure) diffeomorphic to a standard neighborhood of a 1-complex. The decomposition is highly nonunique so cannot be used to define an invariant, but it shows the topological s-cobordism question reduces to the core case. The simply-connected version of the decomposition (with 1-complex a point) is due to Curtis, Freedman, Hsiang and Stong. Controlled surgery is used to reduce topological triviality of core s-cobordisms to a question about controlled homotopy equivalence of 4-manifolds. There are speculations about further reductions. 1. Introduction The classical s-cobordism theorem asserts that an s-cobordism of n-manifolds (the bordism itself has dimension n + 1) is isomorphic to a product if n ≥ 5. “Isomorphic” means smooth, PL or topological, depending on the structure of the s-cobordism. In dimension 4 it is known that there are smooth s-cobordisms without smooth product structures; existence was demonstrated by Donaldson [3], and spe- cific examples identified by Akbulut [1]. In the topological case product structures follow from disk embedding theorems. The best current results require “small” fun- damental group, Freedman-Teichner [5], Krushkal-Quinn [9] so s-cobordisms with these groups are topologically products. The large fundamental group question is still open. Freedman has developed several link questions equivalent to the 4-dimensional “surgery conjecture” for arbitrary fundamental groups. -
Lecture Notes on Foliation Theory
INDIAN INSTITUTE OF TECHNOLOGY BOMBAY Department of Mathematics Seminar Lectures on Foliation Theory 1 : FALL 2008 Lecture 1 Basic requirements for this Seminar Series: Familiarity with the notion of differential manifold, submersion, vector bundles. 1 Some Examples Let us begin with some examples: m d m−d (1) Write R = R × R . As we know this is one of the several cartesian product m decomposition of R . Via the second projection, this can also be thought of as a ‘trivial m−d vector bundle’ of rank d over R . This also gives the trivial example of a codim. d- n d foliation of R , as a decomposition into d-dimensional leaves R × {y} as y varies over m−d R . (2) A little more generally, we may consider any two manifolds M, N and a submersion f : M → N. Here M can be written as a disjoint union of fibres of f each one is a submanifold of dimension equal to dim M − dim N = d. We say f is a submersion of M of codimension d. The manifold structure for the fibres comes from an atlas for M via the surjective form of implicit function theorem since dfp : TpM → Tf(p)N is surjective at every point of M. We would like to consider this description also as a codim d foliation. However, this is also too simple minded one and hence we would call them simple foliations. If the fibres of the submersion are connected as well, then we call it strictly simple. (3) Kronecker Foliation of a Torus Let us now consider something non trivial. -
Lecture 10: Tubular Neighborhood Theorem
LECTURE 10: TUBULAR NEIGHBORHOOD THEOREM 1. Generalized Inverse Function Theorem We will start with Theorem 1.1 (Generalized Inverse Function Theorem, compact version). Let f : M ! N be a smooth map that is one-to-one on a compact submanifold X of M. Moreover, suppose dfx : TxM ! Tf(x)N is a linear diffeomorphism for each x 2 X. Then f maps a neighborhood U of X in M diffeomorphically onto a neighborhood V of f(X) in N. Note that if we take X = fxg, i.e. a one-point set, then is the inverse function theorem we discussed in Lecture 2 and Lecture 6. According to that theorem, one can easily construct neighborhoods U of X and V of f(X) so that f is a local diffeomor- phism from U to V . To get a global diffeomorphism from a local diffeomorphism, we will need the following useful lemma: Lemma 1.2. Suppose f : M ! N is a local diffeomorphism near every x 2 M. If f is invertible, then f is a global diffeomorphism. Proof. We need to show f −1 is smooth. Fix any y = f(x). The smoothness of f −1 at y depends only on the behaviour of f −1 near y. Since f is a diffeomorphism from a −1 neighborhood of x onto a neighborhood of y, f is smooth at y. Proof of Generalized IFT, compact version. According to Lemma 1.2, it is enough to prove that f is one-to-one in a neighborhood of X. We may embed M into RK , and consider the \"-neighborhood" of X in M: X" = fx 2 M j d(x; X) < "g; where d(·; ·) is the Euclidean distance. -
Poincare Complexes: I
Poincare complexes: I By C. T. C. WALL Recent developments in differential and PL-topology have succeeded in reducing a large number of problems (classification and embedding, for ex- ample) to problems in homotopy theory. The classical methods of homotopy theory are available for these problems, but are often not strong enough to give the results needed. In this paper we attempt to develop a branch of homotopy theory applicable to the classification problem for compact manifolds. A Poincare complex is (approximately) a finite cw-complex which satisfies the Poincare duality theorem. A precise definition is given in ? 1, together with a discussion of chain complexes. In Chapter 2, we give a cutting and gluing theorem, define connected sum, and give a theorem on product decompositions. Chapter 3 is devoted to an account of the tangential proper- ties first introduced by M. Spivak (Princeton thesis, 1964). We then start our classification theorems; in Chapter 4, for dimensions up to 3, where the dominant invariant is the fundamental group; and in Chapter 5, for dimension 4, where we obtain a classification theorem when the fundamental group has prime order. It is complicated to use, but allows us to construct two inter- esting examples. In the second part of this paper, we intend to classify highly connected Poin- care complexes; to show how to perform surgery, and give some applications; by constructing handle decompositions and computing some cobordism groups. This paper was originally planned when the only known fact about topological manifolds (of dimension >3) was that they were Poincare com- plexes. -
Two Classes of Slant Surfaces in Nearly Kahler Six Sphere
TWO CLASSES OF SLANT SURFACES IN NEARLY KAHLER¨ SIX SPHERE K. OBRENOVIC´ AND S. VUKMIROVIC´ Abstract. In this paper we find examples of slant surfaces in the nearly K¨ahler six sphere. First, we characterize two-dimensional small and great spheres which are slant. Their description is given in terms of the associative 3-form in Im O. Later on, we classify the slant surfaces of S6 which are orbits of maximal torus in G2. We show that these orbits are flat tori which are linearly S5 S6 1 π . full in ⊂ and that their slant angle is between arccos 3 and 2 Among them we find one parameter family of minimal orbits. 1. Introduction It is known that S2 and S6 are the only spheres that admit an almost complex structure. The best known Hermitian almost complex structure J on S6 is defined using octonionic multiplication. It not integrable, but satisfies condition ( X J)X = 0, for the Levi-Civita connection and every vector field X on S6. Therefore,∇ sphere S6 with this structure J is usually∇ referred as nearly K¨ahler six sphere. Submanifolds of nearly Kahler¨ sphere S6 are subject of intensive research. A. Gray [7] proved that almost complex submanifolds of nearly K¨ahler S6 are necessarily two-dimensional and minimal. In paper [3] Bryant showed that any Riemannian surface can be embedded in the six sphere as an almost complex submanifold. Almost complex surfaces were further investigated in paper [1] and classified into four types. Totally real submanifolds of S6 can be of dimension two or three. -
Reference Ic/88/392
REFERENCE IC/88/392 INTERNATIONAL CENTRE FOR THEORETICAL PHYSICS THE LOCAL STRUCTURE OF A 2-CODIMENSIONAL CONFORMALLY FLAT SUBMANIFOLD IN AN EUCLIDEAN SPACE lRn+2 G. Zafindratafa INTERNATIONAL ATOMIC ENERGY AGENCY UNITED NATIONS EDUCATIONAL, SCIENTIFIC AND CULTURAL ORGANIZATION IC/88/392 ABSTRACT International Atomic Energy Agency and Since 1917, many mathematicians studied conformally flat submanifolds (e.g. E. Cartan, B.Y. Chen, J.M. Morvan, L. Verstraelen, M. do Carmo, N. Kuiper, etc.). United Nations Educational Scientific and Cultural Organization In 1917, E. Cartan showed with his own method that the second fundamental form INTERNATIONAL CENTRE FOR THEORETICAL PHYSICS of a conforraally flat hypersurface of IR™+1 admits an eigenvalue of multiplicity > n — 1. In order to generalize such a result, in 1972, B.Y. Chen introduced the notion of quasiumbilical submanifold. A submanifold M of codimensjon JV in 1R"+W is quasiumbilical if and only if there exists, locally at each point of M, an orthonormal frame field {d,...,£jv} of the normal space so that the Weingarten tensor of each £„ possesses an eigenvalue of multiplicity > n — 1. THE LOCAL STRUCTURE OF A 2-CODIMENSIONAL CONFORMALLY FLAT SUBMANIFOLD The first purpose of this work is to resolve the following first problem: IN AN EUCLIDEAN SPACE JRn+;1 * Is there any equivalent definition of quasiumbilictty which does not use either any local frame field on the normal bundle or any particular sections on the tangent bundle? B.Y. Chen and K. Yano proved in 1972 that a quasiumbilical submanifold of G. Zafmdratafa, ** codimension N > 1 in JR"+" is conformally flat; moreover in the case of codimension International Centre for Theoretical Physics, Trieste, Italy. -
How to Depict 5-Dimensional Manifolds
HOW TO DEPICT 5-DIMENSIONAL MANIFOLDS HANSJORG¨ GEIGES Abstract. We usually think of 2-dimensional manifolds as surfaces embedded in Euclidean 3-space. Since humans cannot visualise Euclidean spaces of higher dimensions, it appears to be impossible to give pictorial representations of higher-dimensional manifolds. However, one can in fact encode the topology of a surface in a 1-dimensional picture. By analogy, one can draw 2-dimensional pictures of 3-manifolds (Heegaard diagrams), and 3-dimensional pictures of 4- manifolds (Kirby diagrams). With the help of open books one can likewise represent at least some 5-manifolds by 3-dimensional diagrams, and contact geometry can be used to reduce these to drawings in the 2-plane. In this paper, I shall explain how to draw such pictures and how to use them for answering topological and geometric questions. The work on 5-manifolds is joint with Fan Ding and Otto van Koert. 1. Introduction A manifold of dimension n is a topological space M that locally ‘looks like’ Euclidean n-space Rn; more precisely, any point in M should have an open neigh- bourhood homeomorphic to an open subset of Rn. Simple examples (for n = 2) are provided by surfaces in R3, see Figure 1. Not all 2-dimensional manifolds, however, can be visualised in 3-space, even if we restrict attention to compact manifolds. Worse still, these pictures ‘use up’ all three spatial dimensions to which our brains are adapted by natural selection. arXiv:1704.00919v1 [math.GT] 4 Apr 2017 2 2 Figure 1. The 2-sphere S , the 2-torus T , and the surface Σ2 of genus two. -
Types of Integrability on a Submanifold and Generalizations of Gordon’S Theorem
Trudy Moskov. Matem. Obw. Trans. Moscow Math. Soc. Tom 66 (2005) 2005, Pages 169–241 S 0077-1554(05)00149-4 Article electronically published on November 9, 2005 TYPES OF INTEGRABILITY ON A SUBMANIFOLD AND GENERALIZATIONS OF GORDON’S THEOREM N. N. NEKHOROSHEV Abstract. At the beginning of the paper the concept of Liouville integrability is analysed for systems of general form, that is, ones that are not necessarily Hamil- tonian. On this simple basis Hamiltonian systems are studied that are integrable only on submanifolds N of the phase space, which is the main subject of the paper. The study is carried out in terms of k-dimensional foliations and fibrations defined on N by the Hamiltonian vector fields corresponding to k integrals in involution. These integrals are said to be central and may include the Hamiltonian function of the system. The parallel language of sets of functions is also used, in particular, sets of functions whose common level surfaces are the fibres of fibrations. Relations between different types of integrability on submanifolds of the phase space are established. The main result of the paper is a generalization of Gordon’s theorem stating that in a Hamiltonian system all of whose trajectories are closed the period of the solutions depends only on the value of the Hamiltonian. Our generalization asserts that in the case of the strongest “Hamiltonian” integrability the frequencies of a conditionally periodic motion on the invariant isotropic tori that form a fibration of an integrability submanifold depend only on the values of the central integrals. Under essentially weaker assumptions on the fibration of the submanifold into such tori it is proved that the circular action functions also have the same property. -
Lecture 9: the Whitney Embedding Theorem
LECTURE 9: THE WHITNEY EMBEDDING THEOREM Historically, the word \manifold" (Mannigfaltigkeit in German) first appeared in Riemann's doctoral thesis in 1851. At the early times, manifolds are defined extrinsi- cally: they are the set of all possible values of some variables with certain constraints. Translated into modern language,\smooth manifolds" are objects that are (locally) de- fined by smooth equations and, according to last lecture, are embedded submanifolds in Euclidean spaces. In 1912 Weyl gave an intrinsic definition for smooth manifolds. A natural question is: what is the difference between the extrinsic definition and the intrinsic definition? Is there any \abstract" manifold that cannot be embedded into any Euclidian space? In 1930s, Whitney and others settled this foundational problem: the two ways of defining smooth manifolds are in fact the same. In fact, Whitney's result is much more stronger than this. He showed that not only one can embed any smooth manifold into some Euclidian space, but that the dimension of the Euclidian space can be chosen to be (as low as) twice the dimension of the manifold itself! Theorem 0.1 (The Whitney embedding theorem). Any smooth manifold M of di- mension m can be embedded into R2m+1. Remark. In 1944, by using completely different techniques (now known as the \Whitney trick"), Whitney was able to prove Theorem 0.2 (The Strong Whitney Embedding Theorem). Any smooth man- ifold M of dimension m ≥ 2 can be embedded into R2m (and can be immersed into R2m−1). We will not prove this stronger version in this course, but just mention that the Whitney trick was further developed in h-cobordism theory by Smale, using which he proved the Poincare conjecture in dimension ≥ 5 in 1961! Remark.