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Modification lemma: prescribed class changes by isotopy of an embedded boundary sphere

Statement

Assume ACω (The Axiom of Countable Choice (ACω)). Let W be a compact smooth (n+1)-manifold with a finite handle decomposition relative to ∂0W in which all handles have index ≥q, where 2≤q≤n−2, and suppose the middle boundary Nq=∂1Wq is connected. Let f:Sq↪∂1∘Wq be an embedded sphere and let x1,…,xr∈Z, where r is the number of (q+1)-handles. Then there is an embedded sphere g:Sq↪∂1∘Wq (Smooth embeddings), isotopic to f in ∂1Wq+1, whose class in Cq satisfies [g]=[f]+∑jxj ∂q+1[φj], where the [φj] are the core classes of the (q+1)-handles and ∂q+1 is the handle-chain differential of the relative complex (The relative handle chain complex computes H∗(W,M0) and has the intersection matrix as its differential). Thus an arbitrary integer combination of boundary classes of higher handles can be added to the class of an embedded sphere by an isotopy that becomes trivial one level higher.

Facts & Assumptions

Given: A compact smooth (n+1)-manifold with all handles of index ≥q, 2≤q≤n−2, connected middle boundary Nq, an embedded sphere f:Sq↪∂1∘Wq, and integers x1,…,xr indexed by the (q+1)-handles; ACω.

[F1]

The class in Cq attached to an embedded sphere is computed by the attaching-belt coefficients, and the boundary class ∂q+1[φ] of a (q+1)-handle is represented in the middle level by the attaching sphere of that handle up to sign (Handle boundary coefficients are attaching-belt intersection numbers, The relative handle chain complex computes H∗(W,M0) and has the intersection matrix as its differential).

[F2]

Disjoint q-spheres in a connected n-manifold admit an embedded band when q≤n−2; only codimension at least two is required. Its construction can take place in a chosen connected open complement and can match local framing germs. Embedded bands joining two framed spheres exist

[F3]

A (q+1)-handle replaces its attaching tube by Dq+1×Sn−q−1. The outgoing boundary of a handle attachment trades the disk factors

Proof

technique · direct
1.1F1F3givenconstruct

Fix a (q+1)-handle φj. Choose a parallel copy Pj of its attaching sphere just outside its closed attaching tube, using the extension over a neighborhood of the normal disk factor. It lies in Nq∘, the open complement of all closed upper attaching tubes. In Nq+1 it bounds the outgoing disk Dq+1×{z}, z∈Sn−q−1, together with the short annular collar from its boundary to Pj. This is an embedded disk with interior in that handle's outgoing piece, disjoint from any sphere in the common part. Its normal disk coordinates give the standard bounding-disk framing. In Cq, [Pj]=∂q+1[φj] with compatible orientations, by [F1].

2.1F1F2step 1.1constructalgebra

Nq∘ is connected: the upper attaching cores have codimension n−q≥2, so paths can be rerouted in finitely many product charts off the cores, and radial retraction in each punctured tube pushes them outside the closed smaller tubes. Apply [F2] within this common part to band-sum f with Pj. The band interior can avoid both spheres and all other attaching tubes. The resulting q-sphere g is embedded and remains in Nq∘. An oriented pair-of-pants bordism in a thin neighborhood of the band has boundary g−f−Pj, so in Cq its fundamental chain gives [g]=[f]+[Pj]. Choose the orientation of the added parallel copy, rather than reverse f, to obtain either sign.

3.1F2F3step 1.1step 2.1construct

In Nq+1, slide the added lobe back along the band and across the embedded disk of step 1.1. The disk interior is in the new handle's outgoing region, whereas f and the band are in the common part. A thin product neighborhood of their union therefore gives the usual embedded isotopy from the band-sum to f, fixed outside that neighborhood. If f has a normal frame, use the bounding-disk frame for Pj and the matching band frame; this isotopy transports the full frame and gives a framed isotopy as well. Thus no implication from a vanishing homology class to embedding triviality is used.

4.1step 2.1step 3.1algebra∎

Repeat with fresh disjoint parallel copies ∣xj∣ times, using the sign of xj, and then over the finite upper-handle list. At every iteration the new sphere is in the common part and is isotopic one level higher to the preceding sphere. The additive computation gives [g]=[f]+∑jxj∂q+1[φj]. In particular, a standard trivial framed starting sphere yields a sphere framed-isotopic to it in Nq+1. This proves the assertion, including zero coefficients and an empty upper-handle list.

Depends on

Used by

Dependency tree · two levels

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Sources