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Extending a compact surface metric across its boundary

Statement

Assume ACω. Let M be a compact smooth surface with boundary and let g be a smooth Riemannian metric on M. In the smooth double DM, the metric on either chosen labelled copy extends to a smooth Riemannian metric on an open neighbourhood of that copy.

Facts & Assumptions

Given: ACω, a compact smooth surface M with boundary, and a smooth Riemannian metric g on M. We use the smooth structure on its labelled double supplied by the double theorem.

[F1]

Assuming ACω, collar seam charts and the original interior charts give the labelled double a smooth boundaryless structure (The double has a well-defined smooth structure).

[F2]

A smooth tensor field on a manifold with boundary extends smoothly across each boundary point to some neighbourhood in its double (Smooth functions and tensor fields extend locally across the boundary).

[F3]

Assuming ACω, every open cover of a smooth manifold has a smooth partition of unity subordinate to it (Smooth partitions of unity exist on manifolds).

[F4]

A Riemannian metric is a smooth symmetric covariant two-tensor that is positive on every nonzero tangent vector (Riemannian metric and riemannian manifold).

[F5]

A subordinate partition has functions in [0,1], supports inside the cover members, and pointwise sum one (Smooth partitions of unity subordinate to an open cover).

[F6]

The double is the labelled disjoint union with corresponding boundary points identified; if the boundary is empty, the two copies remain disjoint (The double of a smooth manifold with boundary).

[A1]

ACω asserts that every countable family of nonempty sets has a choice function (The Axiom of Countable Choice (ACω)).

Proof

technique · direct
1.1givenF1F6construct

Write M+ for the chosen labelled copy and B=∂M+. If M=∅, then M+=∅ is open in DM and the unique empty tensor is its own extension. More generally, if B is empty, the double is the disjoint union of its labelled copies, so M+ is open even when it is disconnected; g itself is the required extension. Otherwise B is closed in the compact space M+ and is compact. The seam charts in [F1] identify M+ locally with a closed half-space in DM, and its interior M+∘ is open in DM.

1.2F2F4construct

For each b∈B, [F2] gives a covariant two-tensor extension hb of g on some open neighbourhood of b in DM. Replace hb by its symmetric part (hb+hbT)/2; this remains smooth and still equals g on the original half-space. At b it is positive definite by [F4]. In a local frame, the positive quadratic form has a positive minimum on the Euclidean unit circle; continuity of its finitely many coefficients therefore keeps it positive definite after shrinking the neighbourhood. Thus every b has an open neighbourhood U with a smooth positive-definite symmetric extension gU agreeing with g on U∩M+.

2.1F3F4F5step 1.2choose

The family of all such neighbourhoods covers the compact set B, so choose a finite subcover U1,…,Um and corresponding extensions g1,…,gm; these are only finitely many selections. Set O=⋃i=1mUi. Apply [F3] to the open cover (Ui)i=1m of the smooth manifold O, obtaining a smooth partition (ρi)i=1m. By [F5], each product ρigi extends by zero outside Ui smoothly because supp⁡ρi⊆Ui. Consequently G=∑iρigi is a smooth symmetric tensor on O. For every nonzero tangent vector v at x∈O, each term with positive weight satisfies gi(v,v)>0, at least one weight is positive, and the weights sum to one; hence Gx(v,v)>0. On O∩M+ every gi agrees with g, so G=g there.

3.1A1F1F3step 1.1step 2.1∎

The open set N=O∪M+∘ contains the whole copy M+, since B⊂O. On O use G, and on M+∘ use the original metric g. These tensors agree on their overlap by step 2.1, so they glue to a smooth Riemannian metric on N extending g. This proves the claim. The exact ACω uses are invoking [F1] for the smooth double and [F3] for its partition of unity; the finite subcover and finite local extension selections use only finite choice.

Source locator

Polymerakis, On the spectrum of differential operators under Riemannian coverings, Section 3, Lemma 3.2, printed p. 8 (PDF p. 12), gives the same local metric-extension mechanism: extend the metric coefficients across the boundary, shrink until the matrix remains positive definite, and patch with a partition of unity. Its ambient manifold is built by attaching a boundary cylinder; the double-specific neighbourhood and gluing argument above is supplied here.

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Sources