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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. -
DIFFERENTIAL GEOMETRY Contents 1. Introduction 2 2. Differentiation 3
DIFFERENTIAL GEOMETRY FINNUR LARUSSON´ Lecture notes for an honours course at the University of Adelaide Contents 1. Introduction 2 2. Differentiation 3 2.1. Review of the basics 3 2.2. The inverse function theorem 4 3. Smooth manifolds 7 3.1. Charts and atlases 7 3.2. Submanifolds and embeddings 8 3.3. Partitions of unity and Whitney’s embedding theorem 10 4. Tangent spaces 11 4.1. Germs, derivations, and equivalence classes of paths 11 4.2. The derivative of a smooth map 14 5. Differential forms and integration on manifolds 16 5.1. Introduction 16 5.2. A little multilinear algebra 17 5.3. Differential forms and the exterior derivative 18 5.4. Integration of differential forms on oriented manifolds 20 6. Stokes’ theorem 22 6.1. Manifolds with boundary 22 6.2. Statement and proof of Stokes’ theorem 24 6.3. Topological applications of Stokes’ theorem 26 7. Cohomology 28 7.1. De Rham cohomology 28 7.2. Cohomology calculations 30 7.3. Cechˇ cohomology and de Rham’s theorem 34 8. Exercises 36 9. References 42 Last change: 26 September 2008. These notes were originally written in 2007. They have been classroom-tested twice. Address: School of Mathematical Sciences, University of Adelaide, Adelaide SA 5005, Australia. E-mail address: [email protected] Copyright c Finnur L´arusson 2007. 1 1. Introduction The goal of this course is to acquire familiarity with the concept of a smooth manifold. Roughly speaking, a smooth manifold is a space on which we can do calculus. Manifolds arise in various areas of mathematics; they have a rich and deep theory with many applications, for example in physics. -
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. -
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. -
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. -
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. -
Tangent Spaces
CHAPTER 4 Tangent spaces So far, the fact that we dealt with general manifolds M and not just embedded submanifolds of Euclidean spaces did not pose any serious problem: we could make sense of everything right away, by moving (via charts) to opens inside Euclidean spaces. However, when trying to make sense of "tangent vectors", the situation is quite different. Indeed, already intuitively, when trying to draw a "tangent space" to a manifold M, we are tempted to look at M as part of a bigger (Euclidean) space and draw planes that are "tangent" (in the intuitive sense) to M. The fact that the tangent spaces of M are intrinsic to M and not to the way it sits inside a bigger ambient space is remarkable and may seem counterintuitive at first. And it shows that the notion of tangent vector is indeed of a geometric, intrinsic nature. Given our preconception (due to our intuition), the actual general definition may look a bit abstract. For that reason, we describe several different (but equivalent) approaches to tangent m spaces. Each one of them starts with one intuitive perception of tangent vectors on R , and then proceeds by concentrating on the main properties (to be taken as axioms) of the intuitive perception. However, before proceeding, it is useful to clearly state what we expect: • tangent spaces: for M-manifold, p 2 M, have a vector space TpM. And, of course, m~ for embedded submanifolds M ⊂ R , these tangent spaces should be (canonically) isomorphic to the previously defined tangent spaces TpM. • differentials: for smooths map F : M ! N (between manifolds), p 2 M, have an induced linear map (dF )p : TpM ! TF (p)N; m called the differential of F at p. -
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). -
MAT 531: Topology&Geometry, II Spring 2011
MAT 531: Topology&Geometry, II Spring 2011 Solutions to Problem Set 1 Problem 1: Chapter 1, #2 (10pts) Let F be the (standard) differentiable structure on R generated by the one-element collection of ′ charts F0 = {(R, id)}. Let F be the differentiable structure on R generated by the one-element collection of charts ′ 3 F0 ={(R,f)}, where f : R−→R, f(t)= t . Show that F 6=F ′, but the smooth manifolds (R, F) and (R, F ′) are diffeomorphic. ′ ′ (a) We begin by showing that F 6=F . Since id∈F0 ⊂F, it is sufficient to show that id6∈F , i.e. the overlap map id ◦ f −1 : f(R∩R)=R −→ id(R∩R)=R ′ from f ∈F0 to id is not smooth, in the usual (i.e. calculus) sense: id ◦ f −1 R R f id R ∩ R Since f(t)=t3, f −1(s)=s1/3, and id ◦ f −1 : R −→ R, id ◦ f −1(s)= s1/3. This is not a smooth map. (b) Let h : R −→ R be given by h(t)= t1/3. It is immediate that h is a homeomorphism. We will show that the map h:(R, F) −→ (R, F ′) is a diffeomorphism, i.e. the maps h:(R, F) −→ (R, F ′) and h−1 :(R, F ′) −→ (R, F) are smooth. To show that h is smooth, we need to show that it induces smooth maps between the ′ charts in F0 and F0. In this case, there is only one chart in each. So we need to show that the map f ◦ h ◦ id−1 : id h−1(R)∩R =R −→ R is smooth: −1 f ◦ h ◦ id R R id f h (R, F) (R, F ′) Since f ◦ h ◦ id−1(t)= f h(t) = f(t1/3)= t1/3 3 = t, − this map is indeed smooth, and so is h. -
Chapter 9 Partitions of Unity, Covering Maps ~
Chapter 9 Partitions of Unity, Covering Maps ~ 9.1 Partitions of Unity To study manifolds, it is often necessary to construct var- ious objects such as functions, vector fields, Riemannian metrics, volume forms, etc., by gluing together items con- structed on the domains of charts. Partitions of unity are a crucial technical tool in this glu- ing process. 505 506 CHAPTER 9. PARTITIONS OF UNITY, COVERING MAPS ~ The first step is to define “bump functions”(alsocalled plateau functions). For any r>0, we denote by B(r) the open ball n 2 2 B(r)= (x1,...,xn) R x + + x <r , { 2 | 1 ··· n } n 2 2 and by B(r)= (x1,...,xn) R x1 + + xn r , its closure. { 2 | ··· } Given a topological space, X,foranyfunction, f : X R,thesupport of f,denotedsuppf,isthe closed set! supp f = x X f(x) =0 . { 2 | 6 } 9.1. PARTITIONS OF UNITY 507 Proposition 9.1. There is a smooth function, b: Rn R, so that ! 1 if x B(1) b(x)= 2 0 if x Rn B(2). ⇢ 2 − See Figures 9.1 and 9.2. 1 0.8 0.6 0.4 0.2 K3 K2 K1 0 1 2 3 Figure 9.1: The graph of b: R R used in Proposition 9.1. ! 508 CHAPTER 9. PARTITIONS OF UNITY, COVERING MAPS ~ > Figure 9.2: The graph of b: R2 R used in Proposition 9.1. ! Proposition 9.1 yields the following useful technical result: 9.1. PARTITIONS OF UNITY 509 Proposition 9.2. Let M be a smooth manifold.