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The reflection of an outward field extends over the double

Statement

Assume countable choice ACω (The Axiom of Countable Choice (ACω)). Let M be a compact smooth n-manifold with boundary, n≥1, and let X be a smooth vector field that is nonzero and points strictly outward along ∂M (Inward, outward, and boundary-tangent vectors). Choose the collar generated by the inward field −X. Let DM be the smooth double defined by this collar, with seam involution τ interchanging the two labelled halves (The double of a smooth manifold with boundary, The double has a well-defined smooth structure). Then X+(y)=X(y)  (y∈M+),X+(τy)=−dτy(X(y))  (y∈M+) defines a smooth vector field on this double (an arbitrary fixed collar need not give a smooth field); its zeros are exactly the two copies of the zeros of X, and for every isolated zero p∈int⁡M ind⁡τp(X+)=(−1)nind⁡pX.

Facts & Assumptions

Given: A compact smooth n-manifold M with boundary, a smooth field X nonzero and strictly outward along ∂M, and the labelled double (DM,τ).

[F1]

DM is the quotient of M+⊔M− identifying the two copies of ∂M, with τ the involution interchanging the labelled halves; smooth collar data near the seam give it the structure of a smooth boundaryless manifold, and two collar choices give structures related by a diffeomorphism fixing the seam pointwise and preserving the halves (The double of a smooth manifold with boundary, The double has a well-defined smooth structure).

[F3]

Because X is strictly outward and nonzero on the compact boundary, there is δ>0 such that X has no zero in the δ-neighbourhood of ∂M; the zeros of X therefore lie in the interior at positive distance from ∂M (Inward, outward, and boundary-tangent vectors).

[F4]

The inward field −X has smooth local forward semiflows at boundary points, using smooth coordinate extensions across the face (Inward-pointing fields have local forward semiflows at the boundary). Their differentials at time zero are invertible because −X is transverse to the boundary. Compactness supplies a uniform short time. Uniqueness and strict inwardness make the map c(x,u)=Φu −X(x) injective: a trajectory cannot return to the boundary, since its boundary defining coordinate has positive derivative at any putative return. Thus c is a global collar for short time, and X=−∂u in its coordinates.

[F5]

The index is independent of the chart and of a trivialization with matching base and fibre orientations, and negation scales it by (−1)n (The local index is independent of chart, ball and trivialization, Negation scales the local index by (−1)n).

Proof

1.1F1F4givenconstruct

If ∂M=∅, the double is the disjoint union of two copies, and the two fields are X and −X. Otherwise use the single global flow collar c(x,u) of [F4] to define the double's smooth structure. Its seam charts have signed coordinate u, with τ(x,u)=(x,−u). This is the collar-defined double of [F1], rather than a replacement of an already fixed smooth structure while keeping X unchanged.

2.1F1F4step 1.1algebra

In these charts X=−∂u on the first half. Reflection followed by negation gives −dτ(−∂u)=−∂u on the second half. The prescriptions therefore agree at the seam and give one smooth nonzero expression there. Off the seam they are X and the push-forward of −X, so they are smooth globally.

3.1F3F5step 1.1step 2.1algebra∎

There are no seam zeros, and off the seam the zero set consists precisely of the two copies of X−1(0). For any isolated zero p, a chart at p transported by τ identifies the second field with −X. Chart invariance and [F5] give ind⁡τpX+=ind⁡p(−X)=(−1)nind⁡pX. The same computation applies to the two disjoint copies when the boundary is empty.

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