Fundamentals of Submersions and Immersions Between Infinite
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Codimension Zero Laminations Are Inverse Limits 3
CODIMENSION ZERO LAMINATIONS ARE INVERSE LIMITS ALVARO´ LOZANO ROJO Abstract. The aim of the paper is to investigate the relation between inverse limit of branched manifolds and codimension zero laminations. We give necessary and sufficient conditions for such an inverse limit to be a lamination. We also show that codimension zero laminations are inverse limits of branched manifolds. The inverse limit structure allows us to show that equicontinuous codimension zero laminations preserves a distance function on transver- sals. 1. Introduction Consider the circle S1 = { z ∈ C | |z| = 1 } and the cover of degree 2 of it 2 p2(z)= z . Define the inverse limit 1 1 2 S2 = lim(S ,p2)= (zk) ∈ k≥0 S zk = zk−1 . ←− Q This space has a natural foliated structure given by the flow Φt(zk) = 2πit/2k (e zk). The set X = { (zk) ∈ S2 | z0 = 1 } is a complete transversal for the flow homeomorphic to the Cantor set. This space is called solenoid. 1 This construction can be generalized replacing S and p2 by a sequence of compact p-manifolds and submersions between them. The spaces obtained this way are compact laminations with 0 dimensional transversals. This construction appears naturally in the study of dynamical systems. In [17, 18] R.F. Williams proves that an expanding attractor of a diffeomor- phism of a manifold is homeomorphic to the inverse limit f f f S ←− S ←− S ←−· · · where f is a surjective immersion of a branched manifold S on itself. A branched manifold is, roughly speaking, a CW-complex with tangent space arXiv:1204.6439v2 [math.DS] 20 Nov 2012 at each point. -
Part III : the Differential
77 Part III : The differential 1 Submersions In this section we will introduce topological and PL submersions and we will prove that each closed submersion with compact fibres is a locally trivial fibra- tion. We will use Γ to stand for either Top or PL and we will suppose that we are in the category of Γ–manifolds without boundary. 1.1 A Γ–map p: Ek → Xl betweenΓ–manifoldsisaΓ–submersion if p is locally the projection Rk−→πl R l on the first l–coordinates. More precisely, p: E → X is a Γ–submersion if there exists a commutative diagram p / E / X O O φy φx Uy Ux ∩ ∩ πl / Rk / Rl k l where x = p(y), Uy and Ux are open sets in R and R respectively and ϕy , ϕx are charts around x and y respectively. It follows from the definition that, for each x ∈ X ,thefibre p−1(x)isaΓ– manifold. 1.2 The link between the notion of submersions and that of bundles is very straightforward. A Γ–map p: E → X is a trivial Γ–bundle if there exists a Γ– manifold Y and a Γ–isomorphism f : Y × X → E , such that pf = π2 ,where π2 is the projection on X . More generally, p: E → X is a locally trivial Γ–bundle if each point x ∈ X has an open neighbourhood restricted to which p is a trivial Γ–bundle. Even more generally, p: E → X is a Γ–submersion if each point y of E has an open neighbourhood A, such that p(A)isopeninXand the restriction A → p(A) is a trivial Γ–bundle. -
FOLIATIONS Introduction. the Study of Foliations on Manifolds Has a Long
BULLETIN OF THE AMERICAN MATHEMATICAL SOCIETY Volume 80, Number 3, May 1974 FOLIATIONS BY H. BLAINE LAWSON, JR.1 TABLE OF CONTENTS 1. Definitions and general examples. 2. Foliations of dimension-one. 3. Higher dimensional foliations; integrability criteria. 4. Foliations of codimension-one; existence theorems. 5. Notions of equivalence; foliated cobordism groups. 6. The general theory; classifying spaces and characteristic classes for foliations. 7. Results on open manifolds; the classification theory of Gromov-Haefliger-Phillips. 8. Results on closed manifolds; questions of compact leaves and stability. Introduction. The study of foliations on manifolds has a long history in mathematics, even though it did not emerge as a distinct field until the appearance in the 1940's of the work of Ehresmann and Reeb. Since that time, the subject has enjoyed a rapid development, and, at the moment, it is the focus of a great deal of research activity. The purpose of this article is to provide an introduction to the subject and present a picture of the field as it is currently evolving. The treatment will by no means be exhaustive. My original objective was merely to summarize some recent developments in the specialized study of codimension-one foliations on compact manifolds. However, somewhere in the writing I succumbed to the temptation to continue on to interesting, related topics. The end product is essentially a general survey of new results in the field with, of course, the customary bias for areas of personal interest to the author. Since such articles are not written for the specialist, I have spent some time in introducing and motivating the subject. -
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. -
LOCAL PROPERTIES of SMOOTH MAPS 1. Submersions And
LECTURE 6: LOCAL PROPERTIES OF SMOOTH MAPS 1. Submersions and Immersions Last time we showed that if f : M ! N is a diffeomorphism, then dfp : TpM ! Tf(p)N is a linear isomorphism. As in the Euclidean case (see Lecture 2), we can prove the following partial converse: Theorem 1.1 (Inverse Mapping Theorem). Let f : M ! N be a smooth map such that dfp : TpM ! Tf(p)N is a linear isomorphism, then f is a local diffeomorphism near p, i.e. it maps a neighborhood U1 of p diffeomorphically to a neighborhood X1 of q = f(p). Proof. Take a chart f'; U; V g near p and a chart f ; X; Y g near f(p) so that f(U) ⊂ X (This is always possible by shrinking U and V ). Since ' : U ! V and : X ! Y are diffeomorphisms, −1 −1 n n d( ◦ f ◦ ' )'(p) = d q ◦ dfp ◦ d''(p) : T'(p)V = R ! T (q)Y = R is a linear isomorphism. It follows from the inverse function theorem in Lecture 2 −1 that there exist neighborhoods V1 of '(p) and Y1 of (q) so that ◦ f ◦ ' is a −1 −1 diffeomorphism from V1 to Y1. Take U1 = ' (V1) and X1 = (Y1). Then f = −1 ◦ ( ◦ f ◦ '−1) ◦ ' is a diffeomorphism from U1 to X1. Again we cannot conclude global diffeomorphism even if dfp is a linear isomorphism everywhere, since f might not be invertible. In fact, now we can construct an example which is much simpler than the example we constructed in Lecture 2: Let f : S1 ! S1 be given by f(eiθ) = e2iθ. -
Nonlinear Structures Determined by Measures on Banach Spaces Mémoires De La S
MÉMOIRES DE LA S. M. F. K. DAVID ELWORTHY Nonlinear structures determined by measures on Banach spaces Mémoires de la S. M. F., tome 46 (1976), p. 121-130 <http://www.numdam.org/item?id=MSMF_1976__46__121_0> © Mémoires de la S. M. F., 1976, tous droits réservés. L’accès aux archives de la revue « Mémoires de la S. M. F. » (http://smf. emath.fr/Publications/Memoires/Presentation.html) implique l’accord avec les conditions générales d’utilisation (http://www.numdam.org/conditions). Toute utilisation commerciale ou impression systématique est constitutive d’une infraction pénale. Toute copie ou impression de ce fichier doit contenir la présente mention de copyright. Article numérisé dans le cadre du programme Numérisation de documents anciens mathématiques http://www.numdam.org/ Journees Geom. dimens. infinie [1975 - LYON ] 121 Bull. Soc. math. France, Memoire 46, 1976, p. 121 - 130. NONLINEAR STRUCTURES DETERMINED BY MEASURES ON BANACH SPACES By K. David ELWORTHY 0. INTRODUCTION. A. A Gaussian measure y on a separable Banach space E, together with the topolcT- gical vector space structure of E, determines a continuous linear injection i : H -> E, of a Hilbert space H, such that y is induced by the canonical cylinder set measure of H. Although the image of H has measure zero, nevertheless H plays a dominant role in both linear and nonlinear analysis involving y, [ 8] , [9], [10] . The most direct approach to obtaining measures on a Banach manifold M, related to its differential structure, requires a lot of extra structure on the manifold : for example a linear map i : H -> T M for each x in M, and even a subset M-^ of M which has the structure of a Hilbert manifold, [6] , [7]. -
Complete Connections on Fiber Bundles
Complete connections on fiber bundles Matias del Hoyo IMPA, Rio de Janeiro, Brazil. Abstract Every smooth fiber bundle admits a complete (Ehresmann) connection. This result appears in several references, with a proof on which we have found a gap, that does not seem possible to remedy. In this note we provide a definite proof for this fact, explain the problem with the previous one, and illustrate with examples. We also establish a version of the theorem involving Riemannian submersions. 1 Introduction: A rather tricky exercise An (Ehresmann) connection on a submersion p : E → B is a smooth distribution H ⊂ T E that is complementary to the kernel of the differential, namely T E = H ⊕ ker dp. The distributions H and ker dp are called horizontal and vertical, respectively, and a curve on E is called horizontal (resp. vertical) if its speed only takes values in H (resp. ker dp). Every submersion admits a connection: we can take for instance a Riemannian metric ηE on E and set H as the distribution orthogonal to the fibers. Given p : E → B a submersion and H ⊂ T E a connection, a smooth curve γ : I → B, t0 ∈ I, locally defines a horizontal lift γ˜e : J → E, t0 ∈ J ⊂ I,γ ˜e(t0)= e, for e an arbitrary point in the fiber. This lift is unique if we require J to be maximal, and depends smoothly on e. The connection H is said to be complete if for every γ its horizontal lifts can be defined in the whole domain. In that case, a curve γ induces diffeomorphisms between the fibers by parallel transport. -
Ehresmann's Theorem
Ehresmann’s Theorem Mathew George Ehresmann’s Theorem states that every proper submersion is a locally-trivial fibration. In these notes we go through the proof of the theorem. First we discuss some standard facts from differential geometry that are required for the proof. 1 Preliminaries Theorem 1.1 (Rank Theorem) 1 Suppose M and N are smooth manifolds of dimen- sion m and n respectively, and F : M ! N is a smooth map with a constant rank k. Then given a point p 2 M there exists charts (x1, ::: , xm) centered at p and (v1, ::: , vn) centered at F(p) in which F has the following coordinate representation: F(x1, ::: , xm) = (x1, ::: , xk, 0, ::: , 0) Definition 1.1 Let X and Y be vector fields on M and N respectively and F : M ! N a smooth map. Then we say that X and Y are F-related if DF(Xjp) = YjF(p) for all p 2 M (or DF(X) = Y ◦ F). Definition 1.2 Let X be a vector field on M. Then a curve c :[0, 1] ! M is called an integral curve for X if c˙(t) = Xjc(t), i.e. X at c(t) forms the tangent vector of the curve c at t. Theorem 1.2 (Fundamental Theorem on Flows) 2 Let X be a vector field on M. For each p 2 M there is a unique integral curve cp : Ip ! M with cp(0) = p and c˙p(t) = Xcp(t). t Notation: We denote the integral curve for X starting at p at time t by φX(p). -
Homotopy Theory of Infinite Dimensional Manifolds?
Topo/ogy Vol. 5. pp. I-16. Pergamon Press, 1966. Printed in Great Britain HOMOTOPY THEORY OF INFINITE DIMENSIONAL MANIFOLDS? RICHARD S. PALAIS (Received 23 Augrlsf 1965) IN THE PAST several years there has been considerable interest in the theory of infinite dimensional differentiable manifolds. While most of the developments have quite properly stressed the differentiable structure, it is nevertheless true that the results and techniques are in large part homotopy theoretic in nature. By and large homotopy theoretic results have been brought in on an ad hoc basis in the proper degree of generality appropriate for the application immediately at hand. The result has been a number of overlapping lemmas of greater or lesser generality scattered through the published and unpublished literature. The present paper grew out of the author’s belief that it would serve a useful purpose to collect some of these results and prove them in as general a setting as is presently possible. $1. DEFINITIONS AND STATEMENT OF RESULTS Let V be a locally convex real topological vector space (abbreviated LCTVS). If V is metrizable we shall say it is an MLCTVS and if it admits a complete metric then we shall say that it is a CMLCTVS. A half-space in V is a subset of the form {v E V(l(u) L 0} where 1 is a continuous linear functional on V. A chart for a topological space X is a map cp : 0 + V where 0 is open in X, V is a LCTVS, and cp maps 0 homeomorphically onto either an open set of V or an open set of a half space of V. -
Stacky Lie Groups,” International Mathematics Research Notices, Vol
Blohmann, C. (2008) “Stacky Lie Groups,” International Mathematics Research Notices, Vol. 2008, Article ID rnn082, 51 pages. doi:10.1093/imrn/rnn082 Stacky Lie Groups Christian Blohmann Department of Mathematics, University of California, Berkeley, CA 94720, USA; Fakultat¨ fur¨ Mathematik, Universitat¨ Regensburg, 93040 Regensburg, Germany Correspondence to be sent to: [email protected] Presentations of smooth symmetry groups of differentiable stacks are studied within the framework of the weak 2-category of Lie groupoids, smooth principal bibundles, and smooth biequivariant maps. It is shown that principality of bibundles is a categor- ical property which is sufficient and necessary for the existence of products. Stacky Lie groups are defined as group objects in this weak 2-category. Introducing a graphic nota- tion, it is shown that for every stacky Lie monoid there is a natural morphism, called the preinverse, which is a Morita equivalence if and only if the monoid is a stacky Lie group. As an example, we describe explicitly the stacky Lie group structure of the irrational Kronecker foliation of the torus. 1 Introduction While stacks are native to algebraic geometry [11, 13], there has recently been increas- ing interest in stacks in differential geometry. In analogy to the description of moduli problems by algebraic stacks, differentiable stacks can be viewed as smooth structures describing generalized quotients of smooth manifolds. In this way, smooth stacks are seen to arise in genuinely differential geometric problems. For example, proper etale´ differentiable stacks, the differential geometric analog of Deligne–Mumford stacks, are Received April 11, 2007; Revised June 29, 2008; Accepted July 1, 2008 Communicated by Prof. -
Solution 1(A): True. If F : S 1 × S1 → S2 Is an Imme
SOLUTIONS MID-SEMESTER EXAM B-MATH-III 2015-2016 (DIFFERENTIAL TOPOLOGY) Solution 1(a): True. If f : S1 × S1 ! S2 is an immersion then because of dimension count, it is also submersion. By Submersion Theorem, it is a local diffeomorphism. Hence the image f(S1 × S1) is an open subset of S2. As S1 × S1 is compact, the image f(S1 × S1) is also closed subset of S2. This implies that f(S1 × S1) = S2. Now using the fact that S1 × S1 is compact, we conclude that f is a covering map. But, as S2 is simply connected, we get a contradiction. Solution 1(b): True. Consider the standard inclusion i : S1 × S1 ! R3. As R3 is a submanifold of R5, and R5 is an open subset of S5, we compose all these inclusion to get a 1-1 inclusion of S1 × S1 into S5. Solution 1(c): True. As f : X ! Y is a diffeomorphism, for an p 2 X, the derivative map Dp(f): TpX ! Tf(p)Y is an isomorphism. Hence, it is now easy to see that f is transversal to any submanifold Z of Y . Thus is true irrespective to the dimension of Z. Solution 1(d): True. If f : S2 ! S1 do not have any critical point then the map f is a submersion. 2 2 1 That means, for any point p 2 S , the derivative map Dpf : TpS ! Tf(p)S is surjective. We denote the kernel of this homomorphsim by Kp. Next we induce the standard Reimannian metric on S2. As the tangent bundle of S1 is trivial, there exits a nowhere vanishing vector field ξ on S1. -
Lecture 5: Submersions, Immersions and Embeddings
LECTURE 5: SUBMERSIONS, IMMERSIONS AND EMBEDDINGS 1. Properties of the Differentials Recall that the tangent space of a smooth manifold M at p is the space of all 1 derivatives at p, i.e. all linear maps Xp : C (M) ! R so that the Leibnitz rule holds: Xp(fg) = g(p)Xp(f) + f(p)Xp(g): The differential (also known as the tangent map) of a smooth map f : M ! N at p 2 M is defined to be the linear map dfp : TpM ! Tf(p)N such that dfp(Xp)(g) = Xp(g ◦ f) 1 for all Xp 2 TpM and g 2 C (N). Remark. Two interesting special cases: • If γ :(−"; ") ! M is a curve such that γ(0) = p, then dγ0 maps the unit d d tangent vector dt at 0 2 R to the tangent vectorγ _ (0) = dγ0( dt ) of γ at p 2 M. • If f : M ! R is a smooth function, we can identify Tf(p)R with R by identifying d a dt with a (which is merely the \derivative $ vector" correspondence). Then for any Xp 2 TpM, dfp(Xp) 2 R. Note that the map dfp : TpM ! R is linear. ∗ In other words, dfp 2 Tp M, the dual space of TpM. We will call dfp a cotangent vector or a 1-form at p. Note that by taking g = Id 2 C1(R), we get Xp(f) = dfp(Xp): For the differential, we still have the chain rule for differentials: Theorem 1.1 (Chain rule). Suppose f : M ! N and g : N ! P are smooth maps, then d(g ◦ f)p = dgf(p) ◦ dfp.