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Gluing continuation solutions gives collar neighbourhoods of the broken ends

Statement

Assume the Axiom of Choice (The Axiom of Choice). Let (fs,gs) be a regular continuation datum on a closed manifold M, let ind⁡(p)−ind⁡(q)=1, and let β=(γ−,v)∈M−(p,a)×C(a,q),ind⁡(a)=ind⁡(q), or β=(v,γ+)∈C(p,b)×M+(b,q),ind⁡(b)=ind⁡(p), be a once-broken continuation trajectory (Broken continuation trajectories and geometric convergence). Then there are δ>0 and a continuous injection ψ:[0,δ)→C‾(p,q) with ψ(0)=β,ψ(t)∈C(p,q) (t>0), that is smooth on (0,δ), whose parameter t is a neck-length (gluing) parameter, and whose image is a neighbourhood of β; moreover every sequence in C(p,q) converging geometrically to β lies eventually in ψ((0,δ)). Consequently every once-broken boundary point of the compactification of Continuation trajectories are compact up to breaking has a one-sided collar chart, and C‾(p,q) is a compact one-dimensional topological manifold with boundary whose boundary is exactly the disjoint union of these once-broken products.

Facts & Assumptions

Given: The Axiom of Choice, the stated regular datum and index-drop-one once-broken configuration.

[F1]

Its geometric compactification is compact metrizable, and the only added configurations are the two displayed once-broken products. The rigid middle and metric-end tail sets are finite (Continuation trajectories are compact up to breaking, Broken continuation trajectories and geometric convergence).

[F2]

The local exact flow-matching chart has one coordinate ρ=1/T at a single break, with a fixed-time anchor adjacent to the unshifted middle. It includes constant connectors. The chart is a homeomorphism onto a geometric neighbourhood and every sufficiently close trajectory has the unique inverse crossing-time coordinate (Finite flow matching gives local charts at metric-end broken trajectories).

[F3]

The regular unbroken space has dimension one (A regular continuation datum between Morse--Smale pairs).

Proof

technique · direct
1.1F1F2givenconstruct

At the specified once-broken point, the two rigid piece spaces have singleton local charts by [F1]. The broken-stratum chart B of [F2] is therefore a point. Its one-neck matching chart is a homeomorphism ψ:[0,δ)→U, taking zero to the broken point and positive ρ to exact unbroken solutions. It is smooth on the positive interval. No middle translation is used: the passage ends, or starts in the positive-break case, at the fixed-time anchor. This remains valid if the middle is a constant solution at the intermediate critical point.

2.1F2step 1.1

By the inverse coverage of [F2], any ordinary trajectory geometrically sufficiently close to the broken point has the unique entry-crossing time relative to that anchor, hence the unique T and ρ=1/T. It is the matched trajectory ψ(ρ). Thus the image is a neighbourhood, the map is injective, and every sequence converging to that broken point lies eventually in its positive image.

3.1F1F3step 1.1step 2.1∎

Apply steps 1.1–2.1 at each added point. By [F1] these are exactly the once-broken products, and every such point has a half-interval neighbourhood. The unbroken points have ordinary one-dimensional charts by [F3]. Together with compactness and metrizability of [F1], these charts make the compactification a compact one-dimensional topological manifold with boundary in the sense of Topological manifolds with boundary, with the stated boundary and collars.

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