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Connected sum preserves oriented homotopy spheres

Statement

Assume ACω. For n≥3, the oriented connected sum of two oriented smooth homotopy n-spheres is again an oriented smooth homotopy n-sphere.

Facts & Assumptions

Given: Oriented smooth homotopy n-spheres Σ1,Σ2 with n≥3, smoothly embedded oriented disks Di⊆Σi, and the oriented connected sum Σ1#Σ2.

[A1]

Countable choice ACω is assumed (The Axiom of Countable Choice (ACω)).

[L1]

The punctured manifold Pi=Σi∖int⁡Di has boundary Sn−1. Excision and the pair sequence identify Hk(Σi,Pi) with Hk(Di,∂Di); the oriented fundamental class maps to the relative disk generator. Van Kampen applies after enlarging the pieces by collars (Smooth homotopy sphere, Excision for singular homology, Long exact sequence of a pair, Seifert–van Kampen identifies the fundamental group with a group pushout).

[L2]

Under ACω compact smooth manifolds have finite CW homotopy models (Compact smooth manifolds have finite CW models under countable choice). For a homology equivalence f:X→Y between simply connected finite CW complexes, cellular approximation and its finite mapping cylinder give a simply connected finite pair (Mf,X) with zero relative homology (Cellular approximation for maps of CW pairs, Cellular mapping cylinders and relative cylinders are CW complexes, Long exact sequence of a pair). The pair is 1-connected; if it is (r−1)-connected, the choice-free relative Hurewicz comparison makes πr(Mf,X)=Hr(Mf,X)=0 (Relative Hurewicz comparison through a choice-free weak model). Induction and the relative homotopy sequence show that f is weak, and finite Whitehead makes it a homotopy equivalence (Long exact sequence of relative homotopy groups, Whitehead theorem). This criterion uses no full choice.

[L3]

Mayer-Vietoris computes the homology of a union of two subspaces from the homology of the pieces and their intersection (Mayer–Vietoris sequence in singular homology), and van Kampen computes the fundamental group of a union with connected intersection (Seifert–van Kampen identifies the fundamental group with a group pushout).

Proof

technique · direct
1.1L1L2A1given

By [L1] the map Hn(Σi)→Hn(Σi,Pi) is an isomorphism, since it sends the fundamental generator to the local disk generator. Exactness gives H~∗(Pi)=0. Removing a disk leaves a path-connected manifold: paths entering the disk can be diverted along its connected boundary collar. Van Kampen for Pi and the disk, thickened to an open cover, has simply connected overlap Sn−1 for n≥3, and gives π1(Pi)=π1(Σi)=0. Thus [L2], applied on finite models to Pi→{∗}, makes Pi contractible.

2.1step 1.1givenconstruct

Use the fixed orientation-reversing linear reflection between the disk-coordinate boundary spheres to glue P1 and P2. This is the oriented connected sum; no arbitrary boundary diffeomorphism is substituted for that coordinate identification. Collar thickenings of the two pieces form an open cover whose overlap retracts to Sn−1.

3.1step 1.1step 2.1L3

Reduced Mayer–Vietoris for that cover gives H~k(Σ1#Σ2)≅H~k−1(Sn−1) for k≥1, because both pieces are contractible. In degree zero the union is connected. Hence its integral homology is that of Sn.

3.2step 1.1step 2.1L3

Van Kampen for the same open cover, with simply connected pieces and overlap, gives π1(Σ1#Σ2)=0.

4.1step 3.1step 3.2L1L2construct

Choose an oriented coordinate disk D in the connected sum X and collapse X∖int⁡D to a point. The target is D/∂D≅Sn; the map has degree one because it carries the local oriented disk generator to the sphere generator. By step 3.1 it is a homology equivalence. Transport it to the finite CW model of X and use [L2] to obtain X≃Sn.

5.1step 4.1∎

The oriented connected sum is therefore an oriented smooth homotopy n-sphere.

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