LECTURE 5: SMOOTH MAPS. 1. Smooth Maps

Similar documents
LECTURE 22: INTEGRATION ON MANIFOLDS. 1. Orientations

LECTURE 11: TRANSVERSALITY

Defn 3.1: An n-manifold, M, is a topological space with the following properties:

M4P52 Manifolds, 2016 Problem Sheet 1

Math Topology II: Smooth Manifolds. Spring Homework 2 Solution Submit solutions to the following problems:

The theory of manifolds Lecture 2

0.1 Diffeomorphisms. 0.2 The differential

LECTURE 3: SMOOTH FUNCTIONS

Math 6455 Nov 1, Differential Geometry I Fall 2006, Georgia Tech

LECTURE 16: LIE GROUPS AND THEIR LIE ALGEBRAS. 1. Lie groups

CHAPTER 1. Preliminaries Basic Relevant Algebra Introduction to Differential Geometry. By Christian Bär

Math 598 Feb 14, Geometry and Topology II Spring 2005, PSU

Manifolds and tangent bundles. Vector fields and flows. 1 Differential manifolds, smooth maps, submanifolds

TANGENT VECTORS. THREE OR FOUR DEFINITIONS.

fy (X(g)) Y (f)x(g) gy (X(f)) Y (g)x(f)) = fx(y (g)) + gx(y (f)) fy (X(g)) gy (X(f))

1 Differentiable manifolds and smooth maps

STOKES THEOREM ON MANIFOLDS

THEODORE VORONOV DIFFERENTIABLE MANIFOLDS. Fall Last updated: November 26, (Under construction.)

Integration and Manifolds

(1) Let π Ui : U i R k U i be the natural projection. Then π π 1 (U i ) = π i τ i. In other words, we have the following commutative diagram: U i R k

SMSTC (2017/18) Geometry and Topology 2.

LECTURE 10: THE PARALLEL TRANSPORT

BROUWER FIXED POINT THEOREM. Contents 1. Introduction 1 2. Preliminaries 1 3. Brouwer fixed point theorem 3 Acknowledgments 8 References 8

Math 868 Final Exam. Part 1. Complete 5 of the following 7 sentences to make a precise definition (5 points each). Y (φ t ) Y lim

Worksheet on Vector Fields and the Lie Bracket

LECTURE 9: THE WHITNEY EMBEDDING THEOREM

Notes on Spivak, Differential Geometry, vol 1.

CALCULUS ON MANIFOLDS

1.4 The Jacobian of a map

CALCULUS ON MANIFOLDS. 1. Riemannian manifolds Recall that for any smooth manifold M, dim M = n, the union T M =

The theory of manifolds Lecture 3

Math 396. Bijectivity vs. isomorphism

10. Smooth Varieties. 82 Andreas Gathmann

DIFFERENTIAL GEOMETRY CLASS NOTES INSTRUCTOR: F. MARQUES. September 25, 2015

Math 147, Homework 1 Solutions Due: April 10, 2012

Symplectic and Poisson Manifolds

Definition 5.1. A vector field v on a manifold M is map M T M such that for all x M, v(x) T x M.

Lecture 2. Smooth functions and maps

Bordism and the Pontryagin-Thom Theorem

LECTURE: KOBORDISMENTHEORIE, WINTER TERM 2011/12; SUMMARY AND LITERATURE

Chapter 1. Smooth Manifolds

Let X be a topological space. We want it to look locally like C. So we make the following definition.

Chapter 3. Riemannian Manifolds - I. The subject of this thesis is to extend the combinatorial curve reconstruction approach to curves

LECTURE NOTES ON DIFFERENTIABLE MANIFOLDS

INVERSE FUNCTION THEOREM and SURFACES IN R n

LECTURE 2. (TEXED): IN CLASS: PROBABLY LECTURE 3. MANIFOLDS 1. FALL TANGENT VECTORS.

Analysis II: The Implicit and Inverse Function Theorems

Math 6455 Oct 10, Differential Geometry I Fall 2006, Georgia Tech. Integration on Manifolds, Volume, and Partitions of Unity

LECTURE 28: VECTOR BUNDLES AND FIBER BUNDLES

WEYL INTEGRATION FORMULA

Chap. 1. Some Differential Geometric Tools

LECTURE 5: COMPLEX AND KÄHLER MANIFOLDS

We have the following immediate corollary. 1

Coordinate Systems and Canonical Forms

Math 423 Course Notes

MATH 423/ Note that the algebraic operations on the right hand side are vector subtraction and scalar multiplication.

NOTES ON MANIFOLDS ALBERTO S. CATTANEO

The theory of manifolds Lecture 3. Tf : TR n TR m

Solutions to Problem Set 5 for , Fall 2007

i = f iα : φ i (U i ) ψ α (V α ) which satisfy 1 ) Df iα = Df jβ D(φ j φ 1 i ). (39)

KUIPER S THEOREM ON CONFORMALLY FLAT MANIFOLDS

Notes for Math 535 Differential Geometry Spring Francis Bonahon. Department of Mathematics, University of Southern California

with a given direct sum decomposition into even and odd pieces, and a map which is bilinear, satisfies the associative law for multiplication, and

DIFFERENTIAL TOPOLOGY AND THE POINCARÉ-HOPF THEOREM

1 The Local-to-Global Lemma

DEVELOPMENT OF MORSE THEORY

BACKGROUND IN SYMPLECTIC GEOMETRY

Vector fields Lecture 2

Algebraic Varieties. Notes by Mateusz Micha lek for the lecture on April 17, 2018, in the IMPRS Ringvorlesung Introduction to Nonlinear Algebra

Introduction to Topology

PICARD S THEOREM STEFAN FRIEDL

Let V, W be two finite-dimensional vector spaces over R. We are going to define a new vector space V W with two properties:

satisfying the following condition: If T : V V is any linear map, then µ(x 1,,X n )= det T µ(x 1,,X n ).

Transversality. Abhishek Khetan. December 13, Basics 1. 2 The Transversality Theorem 1. 3 Transversality and Homotopy 2

Lecture 8. Connections

NOTES ON DIFFERENTIAL FORMS. PART 1: FORMS ON R n

COMPLEX ANALYSIS AND RIEMANN SURFACES

SYMPLECTIC LEFSCHETZ FIBRATIONS ALEXANDER CAVIEDES CASTRO

LECTURE 8: THE SECTIONAL AND RICCI CURVATURES

Chapter 4. Inverse Function Theorem. 4.1 The Inverse Function Theorem

SARD S THEOREM ALEX WRIGHT

Vector fields and one forms. v : M TM

Differential Topology Solution Set #2

Lecture Notes a posteriori for Math 201

1. Classifying Spaces. Classifying Spaces

REAL AND COMPLEX SMOOTH MANIFOLDS

Differential Geometry (preliminary draft) Massimiliano Mella

An Introduction to Differential Topology, (Subject to permanent revision)

2. Intersection Multiplicities

Lecture 4 Super Lie groups

FOUNDATIONS OF ALGEBRAIC GEOMETRY CLASS 37

Introduction to Computational Manifolds and Applications

Let us recall in a nutshell the definition of some important algebraic structure, increasingly more refined than that of group.

SISSA Differential Geometry

Algebraic geometry of the ring of continuous functions

LECTURE 26: THE CHERN-WEIL THEORY

Lifting Smooth Homotopies of Orbit Spaces of Proper Lie Group Actions

Math 147, Homework 5 Solutions Due: May 15, 2012

THE INVERSE FUNCTION THEOREM

MATH 4030 Differential Geometry Lecture Notes Part 4 last revised on December 4, Elementary tensor calculus

Transcription:

LECTURE 5: SMOOTH MAPS 1. Smooth Maps Recall that a smooth function on a smooth manifold M is a function f : M R so that for any chart 1 {ϕ α, U α, V α } of M, the function f ϕ 1 α is a smooth function on V α. More generally, we can define smooth maps between smooth manifolds: Definition 1.1. Let M, N be smooth manifolds. We say a continuous map f : M N is smooth if for any chart {ϕ α, U α, V α } of M and {ψ β, X β, Y β } of N, the map ψ β f ϕ 1 α : ϕ α (U α f 1 (X β )) ψ β (X β ) is smooth. [Note: Both ϕ α (U α f 1 (X β )) and ψ β (X β ) are Euclidian open sets.] Remark. In the definition we assume that the map f is already a continuous map. In general the smoothness of all ψ β f ϕ 1 α s does not imply the continuity of f. See Problem Set 2. Remark. One can check that if f : (M, A) (N, B) is smooth, A 1 is a chart on M that is compatible with A, and B 1 is a chart on N that is compatible with B, then f : (M, A 1 ) (N, B 1 ) is smooth. Remark. A map f = (f 1,, f n ) : M R k is smooth if and only if each f i C (M). The set of all smooth maps from M to N is denoted by C (M, N). We will leave it as an exercise to prove that if f C (M, N) and g C (N, P ), then g f C (M, P ). As a consequence, any smooth map f : M N induces a pullback map f : C (N) C (M), g g f. The pull-back will play an important role in the future. 1 In this course, when we say any chart of a smooth manifold M, we always mean any chart in a given atlas A that defines the smooth structure of M. 1

2 LECTURE 5: SMOOTH MAPS Example. The inclusion map ι : S n R n+1 is smooth, since ι ϕ 1 ± (y 1,, y n ) = 1 ( 2y 1,, 2y n, ±(1 y 2 ) ) 1 + y 2 are smooth maps from R n to R n+1. Moreover, if g is any smooth function on R n+1, the pull-back function ι g is ust the restriction of g to S n. Example. The proection map π : R n+1 \ {0} RP n is smooth, since ( ) x ϕ i π(x 1,, x n+1 1 ) = x,, xi 1, xi+1,, xn+1 i x i x i x i is smooth on π 1 (U i ) = {(x 1,, x n+1 ) : x i 0} for each i. As in the Euclidean case, we can define diffeomorphisms between smooth manifolds. Definition 1.2. Let M, N be smooth manifolds. A map f : M N is a diffeomorphism if it is smooth, biective, and f 1 is smooth. If there exists a diffeomorphism f : M N, then we say M and N are diffeomorphic. Sometimes we will denote M N. We will regard diffeomorphic smooth manifolds as the same. The following properties can be easily deduced from the corresponding properties in the Euclidean case: The identity map Id : M M is a diffeomorphism. If f : M N and g : N P are diffeomorphisms, so is g f. If f : M N is a diffeomorphism, so is f 1. Moreover, dim M = dim N. So in particular, for any smooth manifold M, Diff(M) = {f : M M f is a diffeomorphism} is a group, called the diffeomorphism group of M. Example. If M is a smooth manifold, then any chart (ϕ, U, V ) gives a diffeomorphism ϕ : U V from U M to V R n. Example. We have seen that on M = R, the two atlas A = {(ϕ 1 (x) = x, R, R)} and B = {(ϕ 2 (x) = x 3, R, R)} define non-equivalent smooth structures. However, the map ψ : (R, A) (R, B), ψ(x) = x 1/3 is a diffeomorphism. So we still think these two smooth structures are the same, although they are not equivalent. Remark. Here are some deep results on the smooth structures: (J. Milnor and M. Kervaire) The topological 7-sphere admits exactly 28 different smooth structures. (S. Donaldson and M. Freedman) For any n 4, R n has a unique smooth structure up to diffeomorphism; but on R 4 there exist uncountable many distinct pairwise non-diffeomorphic smooth structures.

LECTURE 5: SMOOTH MAPS 3 2. The differential of a smooth map We have seen that if U, V are Euclidean open sets, and f : U V is smooth, then for any a U, one naturally gets a linear map df a : T a U T f(a) V, which can be think of as a linearization of f near the point a, and is extremely useful in studying properties of f near a. Now suppose M, N are smooth manifolds, and f : M N smooth. We would like to define its differential df p at p, again as a linear map between tangent spaces, which serves as a linearization of f near p. But the first question is: What is the tangent space of a smooth manifold at a point? Since M is an abstract manifold, we don t have a simple nice geometric picture. To define tangent vectors on smooth manifolds, let s first re-interpret (algebraically) the tangent vectors in the Euclidean case. Recall that for any point a R n and any vector v at a, there is a conception of directional derivative at point a in the direction v, which send a smooth function f defined on R n to the quantity D a vf = lim t 0 f(a + t v) f(a) t = d dt f(a + t v). t=0 So any v gives us an operator D a v : C (R n ) R. In coordinates, if v = v 1,, v n, then D a vf = v i f x i, in other words, as an operator on C (R n ), Observe that for any f, g C (R n ), D v a = v i x. i (linearity) D v a(αf + βg) = αda v f + βda v g for any α, β R. (Leibnitz law) D v a(fg) = f(a)da v g + g(a)da v f. In general, we can define Definition 2.1. Any operator D a : C (R n ) R satisfying these two properties is called a derivative at a. So any vector v at a defines a derivative D v a at a. It is not hard to see that the correspondence v D v a preserves linearity, i.e. Da α v+β w = αda v + βda w. The next proposition tells us that the correspondence v D v a is one-to-one, so that we can identify the set (vector space) of tangent vectors at a with the set of derivatives at a: Proposition 2.2. Any derivative D : C (R n ) R at a is of the form D v a for some vector v at a. Proof. For any f C (R n ), we have f(x) = f(a) + 1 0 d dt f(a + t(x a))dt = f(a) + (x i a i )h i (x), i=1

4 LECTURE 5: SMOOTH MAPS where 1 f h i (x) = (a + t(x a))dt. 0 xi Note that the Leibnitz property implies D(1) = 0 since D(1) = D(1 1) = 2D(1). By linearity, D(c) = 0 for any constant c. So D(f) = 0 + D(x i )h i (a) + (a i a i )D(h i ) = It follows that as an operator on C (R n ), D = D(x i ) x i. x=a In other words, if we let v = D(x 1 ),, D(x n ), then D = D a v. i=1 D(x i ) f x i (a). This motivates the following definition: Definition 2.3. Let M be an n-dimensional smooth manifold. A tangent vector at a point p M is a R-linear map X p : C (M) R satisfying the Leibnitz law (1) X p (fg) = f(p)x p (g) + X p (f)g(p) for any f, g C (M). It is easy to see that the set of all tangent vectors of M at p is a linear space. We will denote this set by T p M, and call it the tangent space T p M to M at p.. As argued above, if f is a constant function, then X p (f) = 0. More generally, Lemma 2.4. If f = c in a neighborhood of p, then X p (f) = 0. Proof. Let ϕ be a smooth function on M that equals 1 near p, and equals 0 at points where f c. (The existence of such f is guaranteed by partition of unity.) Then (f c)ϕ 0. So 0 = X p ((f c)ϕ) = (f(p) c)x p (ϕ) + X p (f)ϕ(p) = X p (f). As a consequence, we see that if f = g in a neighborhood of p, then X p (f) = X p (g). In other words, X p (f) is determined by the values of f near p. So one can replace C (M) in Definition 2.3 by C (U), where U is any open set that contains p. In other words, as linear spaces, T p M is isomorphic to T p U. Finally we are ready to define the differential of a smooth map between smooth manifolds. Recall that the differential of a smooth map f : U V between open sets in Euclidean spaces at a U is a linear map df a : T a U = R n x T f(a) V = R m y whose matrix is the Jacobian matrix ( f i ) of f at a. To transplant this conception to x smooth maps, we need to take a closer look at the two interpretation of T a U: We have

LECTURE 5: SMOOTH MAPS 5 seen that we can identify the (geometric )vector v at a with the (algebraic) derivative D v a = v i. Note that geometrically, x i ( ) fi f 1 df a ( v) = v = x x v,, f n x v. The vector in the right hand side is a vector in R m y. When interpreted as a derivative on C (R m y ), it is a map that maps g C (R m y ) to v f i g x y = v i x (g f) = Da v(g f). i In other words, the derivative that corresponds to the vector df a ( v) is the derivative at f(a) that maps g C (R m ) to D v a (g f). Motivated by these computations, we define Definition 2.5. Let f : M N be a smooth map. Then for each p M, the differential of f is the linear map df p : T p M T f(p) N defined by for all X p T p M and g C (N). df p (X p )(g) = X p (g f) The chain rule still holds for composition of smooth maps: Theorem 2.6 (Chain rule). Suppose f : M N and g : N P are smooth maps, then d(g f) p = dg f(p) df p. Proof. For any X p T p M and h C (P ), d(g f) p (X p )(h) = X p (h g f) = df p (X p )(h g) = dg f(p) (df p (X p ))(h). So the theorem follows. Obviously the differential of the identity map is the identity map between tangent spaces. By repeating the proof of Theorem 1.2 in Lecture 2 we get Corollary 2.7. If f : M N is a diffeomorphism, then df p : T p M T f(p) N is a linear isomorphism. In particular, we have Corollary 2.8. If dim M = n, then T p M is an n-dimensional linear space. Proof. Let {ϕ, U, V } be a chart near p. Then ϕ : U V is a diffeomorphism. It follows that dim T p M = dim T p U = dim T f(p) V = n. In particular, we see that the tangent vectors i := dϕ 1 ( x i ) form a basis of T p M. In coordinates, one has the following explicit formula for i : i : C (U) R, i (f) = (f ϕ 1 ) (ϕ(p)). x i