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Homology lemma: a handle-basis class is realized by a sphere meeting the belt sphere once

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−3, and suppose the outgoing boundary ∂1Wq is simply connected (Simply connected topological spaces). Let f:Sq↪∂1Wq be an embedded sphere whose class in Cq=Hq(Wq,Wq−1;Z) equals ±[φ] for the basis element [φ] of some q-handle φ (The relative handle chain complex computes H∗(W,M0) and has the intersection matrix as its differential). Then f is isotopic in ∂1Wq to an embedding that meets the belt sphere of φ transversely in exactly one point and is disjoint from the belt spheres of all other q-handles (K handle core cocore attaching region and belt sphere). In the special case that the presentation consists of two adjacent index classes q,q+1, the hypothesis on the class says exactly that the intersection vector of f with the belt spheres is ± a standard basis vector.

For q=2, also assume that π1(∂0W)→π1(W2) is injective. In the h-cobordism applications this follows from the incoming homotopy equivalence and the absence of later handles below index three; nullhomotopic 2-handle attaching circles also suffice.

Facts & Assumptions

Given: A compact smooth (n+1)-manifold with all handles of index ≥q, 2≤q≤n−3, simply connected outgoing boundary ∂1Wq, and an embedded sphere f:Sq↪∂1Wq with [f]=±[φ]; ACω.

[F1]

In the relative handle chain complex the class of a sphere in Cq has intersection coordinates given by the attaching-belt intersection numbers: the local collapse-to-core calculation also applies to the map Hq(∂1Wq)→Hq(Wq,Wq−1), so the coefficient of a handle in [f] is the signed sum against its belt sphere; transverse representatives are obtained by isotopy (The relative handle chain complex computes H∗(W,M0) and has the intersection matrix as its differential, proof step 5.1; Attaching-belt intersection matrix of adjacent-index handles).

[F2]

In a connected embedded submanifold of dimension at least two, two distinct points can be joined by embedded arcs in the submanifold avoiding any prescribed finite set (Arcs joining two points of a connected submanifold avoiding finitely many points).

[F3]

The high-dimensional Whitney trick removes a pair of transverse intersection points of opposite sign, one for each of two embedded spheres of dimensions a,b≥3 in an ambient manifold of dimension a+b, when the Whitney circle is null-homotopic (The high-dimensional Whitney trick).

[F4]

The two-dimensional Whitney construction requires the fixed-sheet complement injection. For the actual 2-handle belts it follows from the stated incoming injection, by deleting the belts and retracting to the incoming boundary minus the attaching circles. It is not a consequence of simple connectivity of the outgoing level alone. Belt-sphere complements in low handle levels preserve the fundamental group, The Whitney trick in the codimension-two borderline case.

Proof

1.1F1given

Isotope f transverse to the finitely many belt spheres. By [F1] its signed intersection coordinates are ±1 at the distinguished belt and zero at every other belt. Unless the required configuration already holds, one belt therefore has an opposite-sign surplus pair.

2.1F2F3F4step 1.1

Choose sheet arcs avoiding every other intersection by [F2]. Their circle is nullhomotopic because the outgoing level is simply connected. For 3≤q≤n−3, both sheet dimensions are at least three and [F3] supplies the Whitney move; choose the disk and tube disjoint from all other spheres by their codimension-at-least-three dimension counts. For q=2, [F4] gives the full belt-complement injection from the explicit incoming assumption, fills the shifted circle in that complement and clears all other 2-sphere attaching images. The helper supplies the clean admissibly framed disk and pair removal.

3.1F1F4step 2.1∎

Each move lowers the finite intersection count by two, preserves the other intersections and transports any given normal frame. Iterating leaves one point at the distinguished belt and none at the others, because the signed sums remain ±1 and zero. This proves the stated generic range with its exact q=2 condition.

Remarks

The wider arbitrary-sphere endpoint q=n−2 from the source is not proved by this lemma: it would require an additional argument controlling the complement of the arbitrary codimension-two sphere. Actual two-index h-cobordism attaching spheres admit that control by reversing the handles, and the geometric middle-cancellation lemma proves that endpoint directly.

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