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Mathematics - Vector Bundles and K-Theory

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"Version 1.3, July 2001 Allen Hatcher Copyright c 2001 by Allen Hatcher Paper or electronic copies for noncommercial use may be made freely without explicit permission from the author. All other rights reserved. Table of Contents Chapter 1. Vector Bundles 1.1. Basic Definitions and Constructions . . . . . . . . . . . . 1 Sections 3. Direct Sums 5. Pullback Bundles 5. Inner Products 7. Subbundles 8. Tensor Products 9. Associated Bundles 11. 1.2. Classifying Vector Bundles . . . . . . . . . . . . . . . . . 12 The Universal Bundle 12. Vector Bundles over Spheres 16. Orientable Vector Bundles 21. A Cell Structure on Grassmann Manifolds 22. Appendix: Paracompactness 24. Chapter 2. Complex K-Theory 2.1. The Functor K(X) 2.2. Bott Periodicity . . . . . . . . . . . . . . . . . . . . . . . 28 Ring Structure 31. Cohomological Properties 32. . . . . . . . . . . . . . . . . . . . . . . . . 38 Clutching Functions 38. Linear Clutching Functions 43. Conclusion of the Proof 45. 2.3. Adams’ Hopf Invariant One Theorem Adams Operations 51. The Splitting Principle 55. . . . . . . . . . . . 48 2.4. Further Calculations The Thom Isomorphism 61. . . . . . . . . . . . . . . . . . . . . . 61 Chapter 3. Characteristic Classes 3.1. Stiefel-Whitney and Chern Classes Applications of w1 and c1 72. . . . . . . . . . . . . 63 Axioms and Construction 64. Cohomology of Grassmannians 69. 3.2. The Chern Character The J–Homomorphism 76. . . . . . . . . . . . . . . . . . . . . . 73 3.3. Euler and Pontryagin Classes . . . . . . . . . . . . . . . . 83 The Euler Class 87. Pontryagin Classes 90. 1. Basic Definitions and Constructions together with a real vector space structure on p −1 (b) for each b ∈ B , such that the following local triviality condition is satisfied: There is a cover of B by open sets Uα for each of which there exists a homeomorphism hα : p −1 (Uα )→Uα × Rn taking p −1 (b) to {b}× Rn by a vector space isomorphism for each b ∈ Uα . Such an hα is E is the total space, and the vector spaces p −1 (b) are the fibers. Often one abbreviates terminology by just calling the vector bundle E , letting the rest of the data be implicit. We could equally well take C in place of R as the scalar field here, obtaining the notion of a complex vector bundle. If we modify the definition by dropping all references to vector spaces and replace R n ture. Here is the basic definition. An n dimensional vector bundle is a map p : E →B Vector bundles are special sorts of fiber bundles with additional algebraic struc- called a local trivialization of the vector bundle. The space B is called the base space, exists a homeomorphism hα : p −1 (Uα )→Uα × F taking p −1 (b) to {b}× F for each b ∈ Uα . Here are some examples of vector bundles: p : E →B such that there is a cover of B by open sets Uα for each of which there by an arbitrary space F , then we have the definition of a fiber bundle: a map (1) The product or trivial bundle E = B × Rn with p the projection onto the first factor. then the projection I × R→I induces a map p : E →S 1 which is a 1 dimensional vector bundle, or line bundle. Since E is homeomorphic to a M¨bius band with its boundary o circle deleted, we call this bundle the M¨bius bundle. o (3) The tangent bundle of the unit sphere S n in Rn+1 , a vector bundle p : E →S n S n by translating it so that its tail is at the head of x , on S n . The map p : E →S n where E = { (x, v) ∈ S n × Rn+1 | x ⊥ v } and we think of v as a tangent vector to (2) If we let E be the quotient space of I × R under the identifications (0, t) ∼ (1, −t) , 2 Chapter 1 Vector Bundles sends (x, v) to x . To construct local trivializations, choose any point b ∈ S n and let Ub ⊂ S n be the open hemisphere containing b and bounded by the hyperplane through the origin orthogonal to b . Define hb : p −1 (Ub )→Ub × p −1 (b) ≈ Ub × Rn by hb (x, v) = (x, πb (v)) where πb is orthogonal projection onto the tangent plane p −1 (x) onto p −1 (b) for each x ∈ Ub . p −1 (b) . Then hb is a local trivialization since πb restricts to an isomorphism of pairs (x, v) ∈ S n × Rn+1 such that v is perpendicular to the tangent plane to S n at (4) The normal bundle to S n in Rn+1 , a line bundle p : E →S n with E consisting of in the previous example, local trivializations hb : p −1 (Ub )→Ub × R can be obtained by orthogonal projection of the fibers p −1 (x) onto p −1 (b) for x ∈ Ub . (5) The canonical line bundle p : E →RPn . Thinking of RPn as the space of lines in Rn+1 through the origin, E is the subspace of RPn × Rn+1 consisting of pairs ( , v) with v ∈ , and p( , v) = . Again local trivializations can be defined by orthogonal projection. We could also take n = ∞ and get the canonical line bundle E →RP∞ . line bundle. The projection p : E ⊥ →RPn , p( , v) = ⊥ x , i.e., v = tx for some t ∈ R . The map p : E →S n is again given by p(x, v) = x . As (6) The orthogonal complement E ⊥ = { ( , v) ∈ RPn × Rn+1 | v ⊥ the orthogonal subspaces } of the canonical , is a vector bundle with fibers , of dimension n . Local trivializations can be obtained once more by orthogonal projection. −1 base space B is a homeomorphism h : E1 →E2 taking each fiber p1 (b) to the cor- An isomorphism between vector bundles p1 : E1 →B and p2 : E2 →B over the same −1 responding fiber p2 (b) by a linear isomorphism. Thus an isomorphism preserves all the structure of a vector bundle, so isomorphic bundles are often regarded as the same. We use the notation E1 ≈ E2 to indicate that E1 and E2 are isomorphic. For example, the normal bundle of S n in Rn+1 is isomorphic to the product bundle S n × R by the map (x, tx) (x, t) . The tangent bundle to S 1 is also isomorphic (eiθ , t) , for eiθ ∈ S 1 and t ∈ R . to the trivial bundle S 1 × R , via (eiθ , iteiθ ) As a further example, the M¨bius bundle in (2) above is isomorphic to the canono ical line bundle over RP1 ≈ S 1 . Namely, RP1 is swept out by a line rotating through an angle of π , so the vectors in these lines sweep out a rectangle [0, π ]× R with the two ends {0}× R and {π }× R identified. The identification is (0, x) ∼ (π , −x) since rotating a vector through an angle of π produces its negative. The zero section of a vector bundle p : E →B is the union of the zero vectors in all the fibers. This is a subspace of E which projects homeomorphically onto B by p . Moreover, E deformation retracts onto its zero section via the homotopy ft (v) = (1 − t)v given by scalar multiplication of vectors v ∈ E . Thus all vector bundles over B have the same homotopy type. ment of the zero section since any vector bundle isomorphism h : E1 →E2 must take One can sometimes distinguish nonisomorphic bundles by looking at the comple- Basic Definitions and Constructions Section 1.1 3 the zero section of E1 onto the zero section of E2 , hence the complements of the zero o sections in E1 and E2 must be homeomorphic. For example, the M¨bius bundle is not isomorphic to the product bundle S 1 × R since the complement of the zero section in the M¨bius bundle is connected while for the product bundle the complement of o the zero section is not connected. This method for distinguishing vector bundles can also be used with more refined topological invariants such as Hn in place of H0 . We shall denote the set of isomorphism classes of n dimensional real vector bundles over B by Vectn (B) , and its complex analogue by Vectn (B) . For those who C worry about set theory, we are using the term ‘set’ here in a naive sense. It follows from Theorem 1.8 later in the chapter that Vectn (B) and Vectn (B) are indeed sets in C the strict sense when B is paracompact. o For example, Vect1 (S 1 ) contains exactly two elements, the M¨bius bundle and the product bundle. This will be a rather trivial application of later theory, but it might be an interesting exercise to prove it now directly from the definitions. Sections s(b) ∈ p −1 (b) for all b ∈ B . We have already mentioned the zero section, which is the section whose values are all zero. At the other extreme would be a section whose values are all nonzero. Not all vector bundles have such a nonvanishing section. Consider for example the tangent bundle to S n . Here a section is just a tangent vector field to S n . One of the standard first applications of homology theory is the theorem that S n has a nonvanishing vector field iff n is odd. From this it follows that the tangent bundle of S n is not isomorphic to the trivial bundle if n is even and nonzero, since the trivial bundle obviously has a nonvanishing section, and an isomorphism between vector bundles takes nonvanishing sections to nonvanishing sections. In fact, an n dimensional bundle p : E →B is isomorphic to the trivial bundle iff each fiber p −1 (b) . For if one has such sections si , the map h : B × Rn →E given by h(b, t1 , ··· , tn ) = i ti si (b) A section of a bundle p : E →B is a map s : B →E such that ps = 1 , or equivalently, 1 it has n sections s1 , ··· , sn such that s1 (b), ··· , sn (b) are linearly independent in is a linear isomorphism in each fiber, and is continuous, as can be verified by composing with a local trivialization p −1 (U )→U × Rn . Hence h A continuous map h : E1 →E2 between vector bundles over the same is an isomorphism by the following useful technical result: −1 base space B is an isomorphism if it takes each fiber p1 (b) to the corresponding −1 fiber p2 (b) by a linear isomorphism. Lemma 1.1. Proof: The hypothesis implies that h is one-to-one and onto. What must be checked is that h−1 is continuous. This is a local question, so we may restrict to an open set to the case of an isomorphism h : U × Rn →U × Rn of the form h(x, v) = (x, gx (v)) . U ⊂ B over which E1 and E2 are trivial. Composing with local trivializations reduces 4 Chapter 1 Vector Bundles Here gx is an element of the group GLn (R) of invertible linear transformations of Rn which depends continuously on x . This means that if gx is regarded as an n× n −1 matrix, its n2 entries depend continuously on x . The inverse matrix gx also depends continuously on x since its entries can be expressed algebraically in terms of the −1 Therefore h−1 (x, v) = (x, gx (v)) is continuous. −1 entries of gx , namely, gx is 1/(det gx ) times the classical adjoint matrix of gx . As an example, the tangent bundle to S 1 is trivial because it has the section (x1 , x2 ) (−x2 , x1 ) for (x1 , x2 ) ∈ S 1 . In terms of complex numbers, if we set iz since iz = −x2 + ix1 . z = x1 + ix2 then this section is z There is an analogous construction using quaternions instead of complex numbers. Quaternions have the form z = x1 + ix2 + jx3 + kx4 , and form a division algebra H via the multiplication rules i2 = j 2 = k2 = −1 , ij = k , jk = i , ki = j , ji = −k , kj = −i , and ik = −j . If we identify H with R4 via the coordinates (x1 , x2 , x3 , x4 ) , then the unit sphere is S 3 and we can define three sections of its tangent bundle by the formulas z z z iz jz kz or or or (x1 , x2 , x3 , x4 ) (x1 , x2 , x3 , x4 ) (x1 , x2 , x3 , x4 ) (−x2 , x1 , −x4 , x3 ) (−x3 , x4 , x1 , −x2 ) (−x4 , −x3 , x2 , x1 ) It is easy to check that the three vectors in the last column are orthogonal to each other and to (x1 , x2 , x3 , x4 ) , so we have three linearly independent nonvanishing tangent vector fields on S 3 , and hence the tangent bundle to S 3 is trivial. The underlying reason why this works is that quaternion multiplication satisfies |zw| = |z||w| , where | · | is the usual norm of vectors in R4 . Thus multiplication by a quaternion in the unit sphere S 3 is an isometry of H . The quaternions 1, i, j, k form the standard orthonormal basis for R4 , so when we multiply them by an arbitrary unit quaternion z ∈ S 3 we get a new orthonormal basis z, iz, jz, kz . The same constructions work for the Cayley octonions, a division algebra structure on R8 . Thinking of R8 as H× H , multiplication of octonions is defined by (z1 , z2 )(w1 , w2 ) = (z1 w1 − w 2 z2 , z2 w 1 + w2 z1 ) and satisfies the key property |zw| = |z||w| . This leads to the construction of seven orthogonal tangent vector fields on the unit sphere S 7 , so the tangent bundle to S 7 is also trivial. As we shall show in §2.3, the only spheres with trivial tangent bundle are S 1 , S 3 , and S 7 . One final general remark before continuing with our next topic: Another way of characterizing the trivial bundle E ≈ B × Rn is to say that there is a continuous projection map E →Rn which is a linear isomorphism on each fiber, since such a projection together with the bundle projection E →B gives an isomorphism E ≈ B × Rn . Basic Definitions and Constructions Section 1.1 5 Direct Sums As a preliminary to defining a direct sum operation on vector bundles, we make two simple observations: (a) Given a vector bundle p : E →B and a subspace A ⊂ B , then p : p −1 (A)→A is clearly a vector bundle. We call this the restriction of E over A . (b) Given vector bundles p1 : E1 →B1 and p2 : E2 →B2 , then p1 × p2 : E1 × E2 →B1 × B2 −1 −1 is also a vector bundle, with fibers the products p1 (b1 )× p2 (b2 ) . For if we have −1 −1 local trivializations hα : p1 (Uα )→Uα × Rn and hβ : p2 (Uβ )→Uβ × Rm for E1 and E2 , then hα × hβ is a local trivialization for E1 × E2 . Now suppose we are given two vector bundles p1 : E1 →B and p2 : E2 →B over the same base space B . The restriction of the product E1 × E2 over the diagonal B = {(b, b) ∈ B × B} is then a vector bundle, called the direct sum E1 ⊕ E2 →B . Thus E1 ⊕ E2 = { (v1 , v2 ) ∈ E1 × E2 | p1 (v1 ) = p2 (v2 ) } The fiber of E1 ⊕ E2 over a point b ∈ B is the product, or direct sum, of the vector −1 −1 spaces p1 (b) and p2 (b) . The direct sum of two trivial bundles is again a trivial bundle, clearly, but the direct sum of nontrivial bundles can also be trivial. For example, the direct sum of the tangent and normal bundles to S n in Rn+1 is the trivial bundle S n × Rn+1 since elements of the direct sum are triples (x, v, tx) ∈ S n × Rn+1 × Rn+1 with x ⊥ v , and the map (x, v, tx) S ×R n n+1 (x, v + tx) gives an isomorphism of the direct sum bundle with . So the tangent bundle to S n is stably trivial: it becomes trivial after taking the direct sum with a trivial bundle. As another example, the direct sum E ⊕ E ⊥ of the canonical line bundle E →RPn with its orthogonal complement, defined in example (6) above, is isomorphic to the trivial bundle RPn × Rn+1 via the map ( , v, w) Specializing to the case n = 1 , both E and E 1 1 ⊥ ( , v + w) for v ∈ and w ⊥ . are isomorphic to the M¨bius bundle o o over RP = S , so the direct sum of the M¨bius bundle with itself is the trivial bundle. This is just saying that if one takes a slab I × R2 and glues the two faces {0}× R2 and {1}× R2 to each other via a 180 degree rotation of R2 , the resulting vector bundle over S 1 is the same as if the gluing were by the identity map. In effect, one can gradually decrease the angle of rotation of the gluing map from 180 degrees to 0 without changing the vector bundle. Pullback Bundles bundles over B into vector bundles over A . Given a vector bundle p : E →B , let Next we describe a procedure for using a map f : A→B to transform vector 6 Chapter 1 Vector Bundles f ∗ (E) = { (a, v) ∈ A× E | f (a) = p(v) } . This subspace of A× E fits into the communot hard to see that π : f (E)→A is also a vector bundle with fibers ∗ tative diagram at the right where π (a, v) = a and f (a, v) = v . It is ∼ f ∗ f ( E ) −− E −→ − − π − − → p − − → of the same dimension as in E . For example, we could say that 1× f ∗ (E) is the restriction of the vector bundle 1 p : A× E →A× B (a, f (a)) A −− B −− −→ f over the graph of f , {(a, f (a)) ∈ A× B} , which we identify with A via the projection a . The vector bundle f ∗ (E) is called the pullback or induced bundle. v , since the condition As a trivial example, if f is the inclusion of a subspace A ⊂ B , then f ∗ (E) is isomorphic to the restriction p −1 (A) via the map (a, v) f (a) = p(v) just says that v ∈ p case of pullback. pullback of the M¨bius bundle E →S 1 by the two-to-one covering map f : S 1 →S 1 , o An interesting example which is small enough to be visualized completely is the −1 (a) . So restriction over subspaces is a special f (z) = z2 . In this case the pullback f ∗ (E) is a two-sheeted covering space of E which can be thought of as a coat of paint applied to ‘both sides’ of the M¨bius bundle. o Since E has one half-twist, f ∗ (E) has two half-twists, hence is the trivial bundle. More o generally, if En is the pullback of the M¨bius bundle by the map z the trivial bundle for n even and the M¨bius bundle for n odd. o Some elementary properties of pullbacks, whose proofs are one-minute exercises in definition-chasing, are: (i) (f g)∗ (E) ≈ g ∗ (f ∗ (E)) . (iii) f ∗ (E1 ⊕ E2 ) ≈ f ∗ (E1 ) ⊕ f ∗ (E2 ) . (ii) If E1 ≈ E2 then f ∗ (E1 ) ≈ f ∗ (E2 ) . zn , then En is Now we come to our first important result: ∗ ∗ then the induced bundles f0 (E) and f1 (E) are isomorphic if A is paracompact. Theorem 1.2. Given a vector bundle p : E →B and homotopic maps f0 , f1 : A→B , All the spaces one ordinarily encounters in algebraic and geometric topology are paracompact, for example compact Hausdorff spaces and CW complexes; see the Appendix to this chapter for more information about this. Let F : A× I →B be a homotopy from f0 to f1 . The restrictions of F ∗ (E) over 1.3. The restrictions of a vector bundle E →X × I over X × {0} and Proof: ∗ ∗ A× {0} and A× {1} are then f0 (E) and f1 (E) . So the theorem will follow from: Proposition Proof: X × {1} are isomorphic if X is paracompact. We need two preliminary facts: (1) A vector bundle p : E →X × [a, b] is trivial if its restrictions over X × [a, c] and X × [c, b] are both trivial for some c ∈ (a, b) . To see this, let these restrictions be E1 = p −1 (X × [a, c]) and E2 = p −1 (X × [c, b]) , and let h1 : E1 →X × [a, c]× Rn Basic Definitions and Constructions Section 1.1 7 the isomorphism X × [c, b]× Rn →X × [c, b]× Rn which on each slice X × {x}× Rn is define a trivialization of E . p −1 (X × {c}) , but they can be made to agree by replacing h2 by its composition with and h2 : E2 →X × [c, b]× Rn be isomorphisms. These isomorphisms may not agree on given by h1 h−1 : X × {c}× Rn →X × {c}× Rn . Once h1 and h2 agree on E1 ∩ E2 , they 2 (2) For a vector bundle p : E →X × I , there exists an open cover {Uα } of X so that each open neighborhoods Ux,1 , ··· , Ux,k in X and a partition 0 = t0 < t1 < ··· < tk = 1 of restriction p −1 (Uα × I)→Uα × I is trivial. This is because for each x ∈ X we can find [0, 1] such that the bundle is trivial over Ux,i × [ti−1 , ti ] , using compactness of [0, 1] . Then by (1) the bundle is trivial over Uα × I where Uα = Ux,1 ∩ ··· ∩ Ux,k . Now we prove the proposition. By (2), we can choose an open cover {Uα } of X so that E is trivial over each Uα × I . Lemma 1.19 in the Appendix to this chapter asserts that there is a countable cover {Vk }k≥1 of X and a partition of unity {ϕk } with ϕk supported in Vk , such that each Vk is a disjoint union of open sets each contained in some Uα . This means that E is trivial over each Vk × I . so Xk = { (x, ψk (x)) ∈ X × I } , and let pk : Ek →Xk be the restriction of the bunFor k ≥ 0 , let ψk = ϕ1 + ··· + ϕk , wi..."

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Mathematics - Vector Bundles and K-Theory

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