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The index sum of an outward field is the Gauss degree

Statement

Assume ACω (The Axiom of Countable Choice (ACω)). Let N⊂Rm be a compact smooth m-dimensional submanifold with boundary, m≥1 (Embedded smooth submanifolds with boundary), and let Y be a smooth vector field on N with only isolated zeros and Y≠0 on ∂N. Then, summing the componentwise degrees over the components of ∂N with the boundary orientation (Induced boundary orientation), ∑x∈N, Y(x)=0ind⁡xY=deg⁡(∂N→Sm−1, x↦Y(x)∣Y(x)∣). For m=1 the right-hand side is read as the reduced degree of the map ∂N→S0: the oriented boundary of a compact oriented 1-manifold is balanced (Oriented boundary counts of a compact oriented 1-manifold cancel), so the reduced degree of The reduced degree of a map into the 0-sphere applies. If in addition Y points strictly outward along ∂N (Inward, outward, and boundary-tangent vectors), the right-hand side equals deg⁡(g) for the Gauss map g:∂N→Sm−1 sending x to the outward unit normal. In particular the index sum is independent of Y.

Facts & Assumptions

Given: A compact smooth m-manifold with boundary N⊂Rm, oriented by the ambient orientation of Rm, and a smooth field Y on N with Y≠0 on ∂N and only isolated zeros.

[F1]

The zeros of Y are finitely many: the zero set is closed, and an infinite closed discrete subset of the compact space N would have an accumulation point x∈N at which continuity gives Y(x)=0 while every neighbourhood of x contains other zeros, contradicting isolatedness. (Isolated zero and local index of a vector field)

[F2]

The index of an isolated zero is the degree of x↦Y(x)/∣Y(x)∣ on a small sphere around the zero, with the standard orientations, and for m=1 the reduced degree of that map S0→S0 (Isolated zero and local index of a vector field, The reduced degree of a map into the 0-sphere).

[F3]

For m≥2, a regular value exists by Morse-Sard for smooth manifolds and Regular values have null complement and are dense. For a proper smooth map F:C→Sm−1 from a nonempty connected closed oriented (m−1)-manifold C and a top form ω on Sm−1, ∫CF∗ω=deg⁡(F)∫Sm−1ω, where the degree is the closed-manifold degree of Degree of a map between oriented closed manifolds, equal to the compact-support cohomological degree of Regular-value formula for degree, and where a normalized volume form with integral one exists (Positive volume form on an oriented manifold, Integral of a compactly supported top form, Degree is well defined and independent of the normalized top form).

[F4]

Under ACω, manifold Stokes holds for a compact oriented manifold with boundary and a smooth (m−1)-form α: ∫∂N′α=∫N′dα, the boundary carrying the induced boundary orientation (The general Stokes theorem, Induced boundary orientation).

[F5]

For m=1: ∂N consists of finitely many points with signs ε(x), and ∑x∈∂Nε(x)=0; the reduced degree of a map h:∂N→S0 is 12∑x∈∂Nε(x)h(x) (Oriented boundary counts of a compact oriented 1-manifold cancel, The reduced degree of a map into the 0-sphere).

[F6]

If Y is strictly outward on ∂N, with outward unit normal g (Inward, outward, and boundary-tangent vectors), then ⟨Y/∣Y∣,g⟩>0 pointwise, so t↦(tY/∣Y∣+(1−t)g)/∣⋯∣ is a homotopy from Y/∣Y∣ to g; homotopic maps have equal degree, and for m=1 a homotopy S0×[0,1]→S0 is constant in the time variable, so the reduced degrees agree (Degree is invariant under proper smooth homotopy, Reduced degree into the 0-sphere is homotopy invariant and multiplicative).

Proof

1.1F1F2algebra

By [F1] the zeros p1,…,pk of Y are finite; choose pairwise disjoint closed coordinate balls D1,…,Dk⊆N around them, so small that Y≠0 on Di‾∖{pi} and ∂Di∩∂N=∅, and let N′:=N∖⋃iint⁡Di, a compact oriented m-manifold with boundary on which the normalized field f:=Y/∣Y∣:N′→Sm−1 is smooth. Its boundary is ∂N′=∂N⊔⨆i∂Di, where each ∂Di carries, as a piece of ∂N′, the orientation opposite to the boundary orientation of the removed ball Di, since the outward normals of N′ and of Di are opposite along ∂Di.

2.1F2F3F4step 1.1algebra

For m≥2 choose a volume form ω on Sm−1 with ∫Sm−1ω=1 and apply [F4] to α=f∗ω: since dω=0, ∫∂N′f∗ω=∫N′f∗dω=0. Evaluating the boundary integral componentwise with [F3] gives 0=deg⁡(∂N→Sm−1)−∑iind⁡piY, because each small sphere ∂Di is mapped by f with degree ind⁡piY in its own boundary orientation by [F2] and therefore contributes −ind⁡piY to ∂N′.

3.1F2F4F5step 1.1algebra

For m=1 use instead the 0-form ω on S0 with ω(±1)=±1, so that ∫S0ω=2 and ∫∂N′f∗ω=∑x∈∂N′ε(x)f(x); Stokes gives ∑x∈∂N′ε(x)f(x)=0, and each removed pair contributes f(pi−δi)−f(pi+δi)=−2ind⁡piY with the orientation of step 1.1 by [F2], so ∑iind⁡piY=12∑x∈∂Nε(x)f(x)=deg⁡(∂N→S0) by [F5], the claimed formula; this and step 2.1 prove the first assertion in both dimensions, and with it the index sum depends only on the boundary values of the normalized field.

4.1F3F6step 3.1algebra∎

If Y is strictly outward, [F6] gives a homotopy from x↦Y(x)/∣Y(x)∣ to the Gauss map g, so their degrees agree and the right-hand side equals deg⁡(g); since deg⁡(g) does not involve Y, the index sum is independent of the choice of the outward field.

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