ebook img

Topics in differential geometry (web draft, April 2007) PDF

413 Pages·2.711 MB·English
Save to my drive
Quick download
Download
Most books are stored in the elastic cloud where traffic is expensive. For this reason, we have a limit on daily download.

Preview Topics in differential geometry (web draft, April 2007)

Topics in Differential Geometry Peter W. Michor Institut fu¨r Mathematik der Universit¨at Wien, Strudlhofgasse 4, A-1090 Wien, Austria. Erwin Schr¨odinger Institut fu¨r Mathematische Physik, Boltzmanngasse 9, A-1090 Wien, Austria. [email protected] These notes are from a lecture course Differentialgeometrie und Lie Gruppen whichhasbeenheldattheUniversityofViennaduringtheacademicyear1990/91, again in 1994/95, in WS1997, in a four term seriesin1999/2000 and 2001/02, and parts in WS 2003 It is not yet complete and will be enlarged. TypesetbyAMS-TEX ii Keywords: Corrections and complements to this book will be posted on the internet at the URL http://www.mat.univie.ac.at/~michor/dgbook.html DraftfromApril18,2007 PeterW.Michor, iii TABLE OF CONTENTS CHAPTER I Manifolds and Vector Fields . . . . . . . . . . . . . . . 1 1. Differentiable Manifolds . . . . . . . . . . . . . . . . . . . . . . 1 2. Submersions and Immersions . . . . . . . . . . . . . . . . . . . 13 3. Vector Fields and Flows . . . . . . . . . . . . . . . . . . . . . 18 CHAPTER II Lie Groups and Group Actions . . . . . . . . . . . . 37 4. Lie Groups I . . . . . . . . . . . . . . . . . . . . . . . . . . 37 5. Lie Groups II. Lie Subgroups and Homogeneous Spaces . . . . . . . . 52 6. Transformation Groups and G-manifolds . . . . . . . . . . . . . . 56 7. Polynomial and smooth invariant theory . . . . . . . . . . . . . . 72 CHAPTER III Differential Forms and De Rham Cohomology . . . . . 85 8. Vector Bundles . . . . . . . . . . . . . . . . . . . . . . . . . 85 9. Differential Forms . . . . . . . . . . . . . . . . . . . . . . . . 97 10. Integration on Manifolds . . . . . . . . . . . . . . . . . . . . . 105 11. De Rham cohomology . . . . . . . . . . . . . . . . . . . . . . 111 12. Cohomology with compact supports and Poincar´e duality . . . . . . . 120 13. De Rham cohomology of compact manifolds . . . . . . . . . . . . 131 14. Lie groups III. Analysis on Lie groups . . . . . . . . . . . . . . . 137 15. Extensions of Lie algebras and Lie groups . . . . . . . . . . . . . 147 CHAPTER IV Bundles and Connections . . . . . . . . . . . . . . 155 16. Derivations on the Algebra of Differential Forms and the Fro¨licher-Nijenhuis Bracket . . . . . . . . . . . . . . . . . . 155 17. Fiber Bundles and Connections . . . . . . . . . . . . . . . . . . 163 18. Principal Fiber Bundles and G-Bundles . . . . . . . . . . . . . . 172 19. Principal and Induced Connections . . . . . . . . . . . . . . . . 188 20. Characteristic classes . . . . . . . . . . . . . . . . . . . . . . 207 21. Jets . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . 221 CHAPTER V Riemannian Manifolds . . . . . . . . . . . . . . . . 227 22. Pseudo Riemann metrics and the Levi Civita covariant derivative . . . 227 23. Riemann geometry of geodesics . . . . . . . . . . . . . . . . . . 240 24. Parallel transport and curvature . . . . . . . . . . . . . . . . . 248 25. Computing with adapted frames, and examples . . . . . . . . . . . 258 26. Riemann immersions and submersions . . . . . . . . . . . . . . . 273 27. Jacobi fields . . . . . . . . . . . . . . . . . . . . . . . . . . 287 CHAPTER VI Isometric Group Actions and Riemannian G-Manifolds . 303 28. Homogeneous Riemann manifolds and symmetric spaces . . . . . . . 303 29. Riemannian G-manifolds . . . . . . . . . . . . . . . . . . . . . 306 30. Polar actions . . . . . . . . . . . . . . . . . . . . . . . . . . 320 CHAPTER VII Symplectic Geometry and Hamiltonian Mechanics . . . 343 31. Symplectic Geometry and Classical Mechanics . . . . . . . . . . . 343 32. Completely integrable Hamiltonian systems . . . . . . . . . . . . 364 33. Poisson manifolds . . . . . . . . . . . . . . . . . . . . . . . . 369 34. Hamiltonian group actions and momentum mappings . . . . . . . . 379 References . . . . . . . . . . . . . . . . . . . . . . . . . . . . . 403 List of Symbols . . . . . . . . . . . . . . . . . . . . . . . . . . 408 DraftfromApril18,2007 PeterW.Michor, iv DraftfromApril18,2007 PeterW.Michor, 1 CHAPTER I Manifolds and Vector Fields 1. Differentiable Manifolds 1.1. Manifolds. A topological manifold is a separable metrizable space M which is locally homeomorphic to Rn. So for any x M there is some homeomorphism ∈ u : U u(U) Rn, where U is an open neighborhood of x in M and u(U) is an → ⊆ open subset in Rn. The pair (U,u) is called a chart on M. From algebraic topology it follows that the number n is locally constant on M; if n is constant, M is sometimes called a pure manifold. We will only consider pure manifolds and consequently we will omit the prefix pure. A family (U ,u ) of charts on M such that the U form a cover of M is called α α α A α an atlas. The mapp∈ings uαβ :=uα◦u−β1 :uβ(Uαβ)→uα(Uαβ) are called the chart changings for the atlas (U ), where U :=U U . α αβ α β ∩ Anatlas(U ,u ) foramanifoldM issaidtobeaCk-atlas,ifallchartchangings α α α A u :u (U ) u∈(U ) are differentiable of class Ck. Two Ck-atlases are called αβ β αβ α αβ → Ck-equivalent, iftheirunionisagainaCk-atlasforM. AnequivalenceclassofCk- atlasesiscalledaCk-structureonM. FromdifferentialtopologyweknowthatifM has a C1-structure, then it also has a C1-equivalent C -structure and even a C1- ∞ equivalentCω-structure,whereCω isshorthandforrealanalytic,see[Hirsch,1976]. By a Ck-manifold M we mean a topological manifold together with aCk-structure and a chart on M will be a chart belonging to some atlas of the Ck-structure. But there are topological manifolds which do not admit differentiable structures. For example, every 4-dimensional manifold is smooth off some point, but there are such which are not smooth, see [Quinn, 1982], [Freedman, 1982]. There are also topological manifolds which admit several inequivalent smooth structures. The spheres from dimension 7 on have finitely many, see [Milnor, 1956]. But the most surprising result is that on R4 there are uncountably many pairwise inequivalent (exotic)differentiablestructures. Thisfollowsfromtheresultsof [Donaldson,1983] and [Freedman, 1982], see [Gompf, 1983] for an overview. Note that for a HausdorffC -manifold in a more general sensethe following prop- ∞ erties are equivalent: (1) It is paracompact. DraftfromApril18,2007 PeterW.Michor, 2 ChapterI.ManifoldsandVectorFields 1.3 (2) It is metrizable. (3) It admits a Riemannian metric. (4) Each connected component is separable. In this book a manifold will usually mean a C -manifold, and smooth is used ∞ synonymously for C , it will be Hausdorff, separable, finite dimensional, to state ∞ it precisely. NotefinallythatanymanifoldM admitsafiniteatlasconsistingofdimM+1(not connected) charts. This is a consequence of topological dimension theory [Nagata, 1965], a proof for manifolds may be found in [Greub-Halperin-Vanstone, Vol. I]. 1.2. Example: Spheres. We consider the space Rn+1, equipped with the stan- dardinnerproduct x,y = xiyi. Then-sphereSn isthenthesubset x Rn+1 : h i { ∈ x,x = 1 . Since f(x) = x,x , f : Rn+1 R, satisfies df(x)y = 2 x,y , it is of h i } hP i → h i rank 1 off 0 and by (1.12) the sphere Sn is a submanifold of Rn+1. In order to get some feeling for the sphere we will describe an explicit atlas for Sn, the stereographic atlas. Choose a Sn (‘south pole’). Let ∈ U+ :=Sn\{a}, u+ :U+ →{a}⊥, u+(x)= x1−hxx,,aaia, −h i U− :=Sn\{−a}, u− :U− →{a}⊥, u−(x)= x1−+hhxx,,aaiia. From an obvious drawing in the 2-plane through 0, x, and a it is easily seen that u is the usual stereographic projection. + -a x 1 0 z=u- (x) y=u (x) + x-<x,a>a a We also get u−+1(y)= |yy|22−+11a+ y22+1y for y ∈{a}⊥\{0} | | | | uansidng(u‘−St◦ruah−+l1e)n(sya)t=z’.|yy|2. Thelatterequationcandirectlybeseenfromthedrawing 1.3. Smooth mappings. Amappingf :M N betweenmanifoldsissaidtobe → Ck if for each x M and one (equivalently: any) chart (V,v) on N with f(x) V ∈ ∈ there is a chart (U,u) on M with x U, f(U) V, and v f u 1 is Ck. We will − ∈ ⊆ ◦ ◦ denote by Ck(M,N) the space of all Ck-mappings from M to N. DraftfromApril18,2007 PeterW.Michor, 1.5 1. DifferentiableManifolds 3 ACk-mappingf :M N iscalledaCk-diffeomorphismiff 1 :N M existsand − → → is also Ck. Two manifolds are called diffeomorphic if there exists a diffeomorphism betweenthem. Fromdifferentialtopology(see[Hirsch,1976])weknowthatifthere isaC1-diffeomorphismbetweenM andN,thenthereisalsoaC -diffeomorphism. ∞ There are manifolds which are homeomorphic but not diffeomorphic: on R4 there are uncountably many pairwise non-diffeomorphic differentiable structures; on ev- eryotherRn thedifferentiablestructureisunique. Therearefinitelymanydifferent differentiable structures on the spheres Sn for n 7. ≥ A mapping f : M N between manifolds of the same dimension is called a local → diffeomorphism, if each x M has an open neighborhood U such that f U : U ∈ | → f(U) N is a diffeomorphism. Note that a local diffeomorphism need not be ⊂ surjective. 1.4. Smooth functions. The set of smooth real valued functions on a manifold M will be denoted by C (M), in order to distinguish it clearly from spaces of ∞ sections which will appear later. C (M) is a real commutative algebra. ∞ The support of a smooth function f is the closure of the set, where it does not vanish,supp(f)= x M :f(x)=0 . Thezerosetoff isthesetwheref vanishes, { ∈ 6 } Z(f)= x M :f(x)=0 . { ∈ } 1.5. Theorem. Any (separable, metrizable, smooth) manifold admits smooth par- titions of unity: Let (U ) be an open cover of M. α α A ∈ Then there is a family (ϕ ) of smooth functions on M, such that: α α A ∈ (1) ϕ (x) 0 for all x M and all α A. α ≥ ∈ ∈ (2) supp(ϕ ) U for all α A. α α ⊂ ∈ (3) (supp(ϕ )) is a locally finite family (so each x M has an open neigh- α α A ∈ ∈ borhood which meets only finitely many supp(ϕ )). α (4) ϕ =1 (locally this is a finite sum). α α P Proof. Any (separable metrizable) manifold is a ‘Lindelo¨f space’, i. e. each open cover admits a countable subcover. This can be seen as follows: Let be an open cover of M. Since M is separable there is a countable dense U subsetS inM. Choose a metric on M. Foreach U and each x U there isan ∈U ∈ y S andn NsuchthattheballB (y)withrespecttothatmetricwithcenter 1/n ∈ ∈ y and radius 1 contains x and is contained in U. But there are only countably n many of these balls; for each of them we choose an open set U containing it. ∈ U This is then a countable subcover of . U Now let (U ) be the given cover. Let us fix first α and x U . We choose a α α A α chart (U,u) ce∈ntered at x (i. e. u(x) = 0) and ε > 0 such that∈εDn u(U U ), α ⊂ ∩ where Dn = y Rn : y 1 is the closed unit ball. Let { ∈ | |≤ } e 1/t for t>0, − h(t):= 0 for t 0, (cid:26) ≤ DraftfromApril18,2007 PeterW.Michor, 4 ChapterI.ManifoldsandVectorFields 1.7 a smooth function on R. Then h(ε2 u(z)2) for z U, f (z):= −| | ∈ α,x 0 for z / U (cid:26) ∈ is a non negative smooth function on M with support in U which is positive at x. α We choose such a function f for each α and x U . The interiors of the α,x α ∈ supportsofthesesmoothfunctions formanopencoverofM whichrefines(U ), so α by the argument at the beginning of the proof there is a countable subcover with corresponding functions f ,f ,.... Let 1 2 W = x M :f (x)>0 and f (x)< 1 for 1 i<n , n { ∈ n i n ≤ } anddenotebyW theclosure. Then(W ) isanopencover. Weclaimthat(W ) n n n n n is locally finite: Let x M. Then there is a smallest n such that x W . Let n ∈ ∈ V := y M :f (y)> 1f (x) . If y V W then we have f (y)> 1f (x) and { ∈ n 2 n } ∈ ∩ k n 2 n f (y) 1 for i<k, which is possible for finitely many k only. i ≤ k Considerthenonnegativesmoothfunctiong (x)=h(f (x))h(1 f (x))...h(1 n n n− 1 n− f (x)) for each n. Then obviously supp(g ) = W . So g := g is smooth, n 1 n n n n − since it is locally only a finite sum, and everywhere positive, thPus (gn/g)n∈N is a smooth partition of unity on M. Since supp(g )=W is contained in some U n n α(n) we may put ϕ = gn to get the required partition of unity which is α n:α(n)=α g subordinated to (U ){ . (cid:3) } αPα∈A 1.6. Germs. Let M and N be manifolds and x M. We consider all smooth ∈ mappings f : U N, where U is some open neighborhood of x in M, and we f f → put f g if there is some open neighborhood V of x with f V = g V. This is an ∼x | | equivalence relation on the set of mappings considered. The equivalence class of a mapping f is called the germ of f at x, sometimes denoted by germ f. The set of x all these germs is denoted by C (M,N). x∞ Note that for a germs at x of a smooth mapping only the value at x is defined. We may also consider composition of germs: germ g germ f :=germ (g f). f(x) ◦ x x ◦ If N = R, we may add and multiply germs of smooth functions, so we get the real commutative algebra C (M,R) of germs of smooth functions at x. This x∞ constructionworksalsoforothertypesoffunctionslikerealanalyticorholomorphic ones, if M has a real analytic or complex structure. Usingsmoothpartitionsofunity((1.4))itiseasilyseenthateachgermofasmooth functionhasarepresentativewhichisdefinedonthewholeofM. Forgermsofreal analytic or holomorphic functions this is not true. So C (M,R) is the quotient of x∞ the algebra C (M) by the ideal of all smooth functions f : M R which vanish ∞ → on some neighborhood (depending on f) of x. 1.7. The tangent space of Rn. Let a Rn. A tangent vector with foot point a ∈ is simply a pair (a,X) with X Rn, also denoted by X . It induces a derivation a ∈ DraftfromApril18,2007 PeterW.Michor, 1.8 1. DifferentiableManifolds 5 X :C (Rn) R by X (f)=df(a)(X ). The value depends only on the germ of a ∞ a a → f ataandwehaveX (f g)=X (f) g(a)+f(a) X (g)(thederivationproperty). a a a · · · If conversely D :C (Rn) R is linear and satisfies D(f g)=D(f) g(a)+f(a) ∞ → · · · D(g) (a derivation at a), then D is given by the action of a tangent vector with foot point a. This can be seen as follows. For f C (Rn) we have ∞ ∈ 1 f(x)=f(a)+ df(a+t(x a))dt dt − Z0 n 1 =f(a)+ ∂f (a+t(x a))dt(xi ai) ∂xi − − i=1Z0 X n =f(a)+ h (x)(xi ai). i − i=1 X D(1)=D(1 1)=2D(1), so D(constant)=0. Thus · n D(f)=D(f(a)+ h (xi ai)) i − i=1 X n n =0+ D(h )(ai ai)+ h (a)(D(xi) 0) i i − − i=1 i=1 X X n = ∂f (a)D(xi), ∂xi i=1 X where xi is the i-th coordinate function on Rn. So we have n n D(f)= D(xi) ∂ (f), D = D(xi) ∂ . ∂xi|a ∂xi|a i=1 i=1 X X Thus D is induced by the tangent vector (a, n D(xi)e ), where (e ) is the stan- i=1 i i dard basis of Rn. P 1.8. The tangent space of a manifold. Let M be a manifold and let x M ∈ and dimM =n. Let T M be the vector space of all derivations at x of C (M,R), x x∞ the algebra of germs of smooth functions on M at x. (Using (1.5) it may easily be seen that a derivation of C (M) at x factors to a derivation of C (M,R).) ∞ x∞ So T M consists of all linear mappings X : C (M) R with the property x x ∞ → X (f g)=X (f) g(x)+f(x) X (g). The space T M is called the tangent space x x x x · · · of M at x. If(U,u)isachartonM withx U,thenu :f f uinducesanisomorphismof ∗ ∈ 7→ ◦ algebras C (Rn,R) = C (M,R), and thus also an isomorphism T u : T M u∞(x) ∼ x∞ x x → T Rn, given by (T u.X )(f) = X (f u). So T M is an n-dimensional vector u(x) x x x x ◦ space. We will use the following notation: u=(u1,... ,un), so ui denotes the i-th coordi- nate function on U, and ∂ :=(T u) 1( ∂ )=(T u) 1(u(x),e ). ∂ui|x x − ∂xi|u(x) x − i DraftfromApril18,2007 PeterW.Michor, 6 ChapterI.ManifoldsandVectorFields 1.10 So ∂ T M is the derivation given by ∂ui|x ∈ x ∂(f u 1) ∂ (f)= ◦ − (u(x)). ∂ui|x ∂xi From (1.7) we have now n n T u.X = (T u.X )(xi) ∂ = X (xi u) ∂ x x x x ∂xi|u(x) x ◦ ∂xi|u(x) i=1 i=1 X X n = X (ui) ∂ , x ∂xi|u(x) i=1 X n X =(T u) 1.T u.X = X (ui) ∂ . x x − x x x ∂ui|x i=1 X 1.9. The tangent bundle. For a manifold M of dimension n we put TM := T M,thedisjointunionofalltangentspaces. Thisisafamilyofvectorspaces x M x par∈ameterized by M, with projection π :TM M given by π (T M)=x. F M → M x For any chart (Uα,uα) of M consider the chart (πM−1(Uα),Tuα) on TM, where Tuα : πM−1(Uα) → uα(Uα)×Rn is given by Tuα.X = (uα(πM(X)),TπM(X)uα.X). Then the chart changings look as follows: Tuβ ◦(Tuα)−1 :Tuα(πM−1(Uαβ))=uα(Uαβ)×Rn → →uβ(Uαβ)×Rn =Tuβ(πM−1(Uαβ)), ((Tu (Tu ) 1)(y,Y))(f)=((Tu ) 1(y,Y))(f u ) β α − α − β ◦ ◦ =(y,Y)(f u u 1)=d(f u u 1)(y).Y ◦ β ◦ −α ◦ β ◦ −α =df(u u 1(y)).d(u u 1)(y).Y β ◦ −α β ◦ −α =(u u 1(y),d(u u 1)(y).Y)(f). β ◦ α− β ◦ −α So the chart changings are smooth. We choose the topology on TM in such a way that all Tu become homeomorphisms. This is a Hausdorff topology, since X, α Y TM maybeseparatedinM ifπ(X)=π(Y),andinonechartifπ(X)=π(Y). ∈ 6 So TM is again a smooth manifold in a canonical way; the triple (TM,π ,M) is M called the tangent bundle of M. 1.10. Kinematic definition of the tangent space. Let C (R,M) denote the 0∞ space of germs at 0 of smooth curves R M. We put the following equivalence → relation on C (R,M): the germ of c is equivalent to the germ of e if and only if 0∞ c(0) = e(0) and in one (equivalently each) chart (U,u) with c(0) = e(0) U we ∈ have d (u c)(t)= d (u e)(t). The equivalence classes are also called velocity dt|0 ◦ dt|0 ◦ vectors of curves in M. We have the following mappings C (R,M)/ C (R,M) 0∞ ∼ u 0∞ α AAAC ev0 Aβ A uA u TM M, π M w DraftfromApril18,2007 PeterW.Michor,

See more

The list of books you might like

Most books are stored in the elastic cloud where traffic is expensive. For this reason, we have a limit on daily download.