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Characteristic numbers are cobordism invariants

Statement

Assume AC (The Axiom of Choice), inherited from the characteristic-number definitions and the boundary-vanishing propositions, and used only there. Let M0 and M1 be closed smooth n-manifolds. If M0 and M1 are unoriented-cobordant, then wI[M0]=wI[M1] for every monomial wI of total degree n. If M0 and M1 are closed oriented 4k-manifolds that are oriented-cobordant, then pJ[M0]=pJ[M1] for every partition J of k; the same equality holds for their Stiefel-Whitney numbers. Hence the characteristic numbers define functions on the unoriented and oriented bordism groups ΩnO and Ω4kSO.

Facts & Assumptions

Given: Closed smooth manifolds M0,M1 of dimension n, either unoriented or oriented with orientations o0,o1, and a bordism (W,θ0,θ1) from M0 to M1 as in the respective cobordism definitions.

[F1]

Unoriented smooth cobordism of closed manifolds and Oriented smooth cobordism define a bordism as a compact smooth (n+1)-manifold W with a decomposition ∂W=(∂W)0⊔(∂W)1 into open and closed boundary parts and collars θ0,θ1 onto open neighbourhoods of the two parts, whose zero-slice restrictions identify Mi diffeomorphically with (∂W)i; in the oriented case W carries an orientation whose induced boundary orientation on (∂W)0 is −o0 and on (∂W)1 is o1. Null-cobordant closed manifolds records the special case of a bordism to the empty manifold.

[F2]

Boundaries have zero Stiefel-Whitney numbers: for a closed smooth n-manifold M=∂W that is the boundary of a compact smooth (n+1)-manifold, every Stiefel-Whitney number vanishes, wI[M]=0. Oriented boundaries have zero Pontryagin numbers: for a closed oriented 4k-manifold that is an oriented boundary, every Pontryagin number vanishes, pJ[M]=0.

[F3]

Stiefel-Whitney numbers of a closed manifold defines wI[M] for a closed smooth n-manifold as the componentwise sum over the finitely many connected components, with the canonical mod-two orientation; Pontryagin numbers of a closed oriented manifold defines pJ[M] as the componentwise sum over the components and records that replacing the orientation o by −o negates every Pontryagin number.

[F4]

Disjoint union makes bordism classes abelian groups and Cartesian product makes bordism a graded ring define the bordism groups ΩnO and ΩnSO as the sets of cobordism classes with the operations of disjoint union and product, and prove these operations well defined.

Proof

1.1givenF1F2F3

Unoriented case. Let (W,θ0,θ1) be a bordism from M0 to M1 [F1]. The collars identify [0,1)×M0 and (−1,0]×M1 with collar neighbourhoods, and their zero-slice restrictions identify the boundary parts with M0 and M1, so ∂W with its canonical mod-two fundamental class is, up to the diffeomorphisms θi∣{0}×Mi, the disjoint union M0⊔M1; in particular ∂W is a closed smooth n-manifold of the boundary type covered by [F2]. Applying the boundary-vanishing proposition [F2] to the boundary ∂W of W gives wI[∂W]=0 for every monomial of total degree n, while the componentwise definition of the Stiefel-Whitney number [F3] gives wI[∂W]=wI[M0]+wI[M1] in F2, the identification of the two boundary parts with M0 and M1 being a diffeomorphism and the mod-two numbers carrying no orientation sign. Hence wI[M0]=wI[M1] for every monomial of total degree n.

2.1givenF1F2F3step 1.1

Oriented case. Let (W,θ0,θ1) now be an oriented bordism from (M0,o0) to (M1,o1) [F1]. The induced boundary orientation of ∂W restricts to −o0 on (∂W)0 and to o1 on (∂W)1, so by [F2] applied to the oriented boundary ∂W of W we have pJ[∂W]=0 for every partition J of k. The componentwise additivity [F3] and the collar identifications give pJ[∂W]=pJ[(∂W)0]+pJ[(∂W)1]=−pJ[M0]+pJ[M1], where the sign uses the orientation-reversal rule of [F3] and the fact that θ0 identifies (∂W)0 with M0 carrying the negative orientation. Hence pJ[M0]=pJ[M1]. For the Stiefel-Whitney numbers of the oriented pair, the same bordism is in particular an unoriented bordism, so step 1.1 applies and gives wI[M0]=wI[M1] for every monomial of total degree 4k.

3.1F2F3F4step 1.1step 2.1∎

The numbers therefore descend to the cobordism-class groups of [F4]. This includes dimension zero: the empty monomial is point parity in the unoriented theory and signed count in the oriented theory, and the same boundary-vanishing argument proves invariance without assuming a classification of compact one-manifolds. Empty manifolds have zero numbers. AC is inherited from [F2, F3]; the comparison itself uses only the supplied bordism and finite component sums.

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