Alphabeta Math
CorollaryStatement: AI-adaptedProof: AI-adaptedPipeline-generatedjudge pass (gpt-5.6-terra)audited 2026-09-13
How statement and proof provenance work

The first chip identifies the source of the statement or construction; the second identifies the source of its local proof or verification.

  • Literature-sourced: the exact statement appears in a cited source; only wording and notation differ.
  • AI-adapted: a semantically identical restatement of literature-sourced material, modulo indexing, notation, and boundary cases adopted by the library.
  • AI-generated: a genuinely novel statement formulated by AI, with no source for the claim itself.

These labels describe origin, not correctness: citations and verification chips remain separate evidence.

A local isometry from a complete connected manifold has geodesically complete target image

Statement

Assume ACω. Let F:(M,g)→(N,h) be a local Riemannian isometry between boundaryless Riemannian manifolds. Suppose M is connected and complete for its Riemannian distance, and put O=F(M).

Then O is open in N and, with the restricted Riemannian metric, is geodesically complete. More strongly, for every q∈O and w∈TqN, the maximal N-geodesic with initial data (q,w) is defined for all real time and its entire image lies in O.

No injectivity, surjectivity onto N, or covering-map conclusion is asserted.

Facts & Assumptions

Given: The local isometry and completeness hypotheses in the statement.

[A1]

The Axiom of Countable Choice (ACω) is the assumed ACω, and Boundaryless convention for geodesic flow and Hopf–Rinow fixes the boundaryless convention.

[F1]

Riemannian isometry and local isometry says that a local Riemannian isometry is a smooth local diffeomorphism satisfying F∗h=g; in particular every dFp is a linear isomorphism and every p has a neighbourhood mapped diffeomorphically onto an open subset of N.

[F2]

Under [A1], Hopf–Rinow theorem makes a nonempty connected boundaryless Riemannian manifold that is complete for its Riemannian distance geodesically complete. Geodesically complete Riemannian manifold says this means that every maximal geodesic has domain R.

[F3]

Under [A1], Existence uniqueness and smooth dependence of geodesics supplies the unique maximal geodesic for each initial tangent vector and identifies every other geodesic with the same initial data as its restriction.

[F4]

Local isometries send geodesics to geodesics says that a local Riemannian isometry sends affinely parametrized geodesics to affinely parametrized geodesics and intertwines their velocities.

Proof

technique · lift initial data
1.1F1given

For q∈O, choose p∈M with F(p)=q. By [F1], some neighbourhood of p maps diffeomorphically onto an open neighbourhood V of q in N, and V⊆F(M)=O. Thus every point of O is interior and O is open. The choice of p instantiates one existential statement for one fixed q.

2.1F1F2step 1.1

If O=∅, it has no initial tangent vectors and is geodesically complete vacuously by [F2]; the stronger assertion is vacuous as well. Suppose q∈O and fix w∈TqN. Choose one p∈M with F(p)=q. Since O is open, TqO=TqN, and [F1] gives the unique vector v=(dFp)−1w∈TpM.

3.1F2F3step 2.1

The point p shows that M is nonempty, so [F2] applies to the assumed metric completeness of M. By [F3], the maximal source geodesic η:R→M with initial data (p,v) is therefore defined for every real time.

4.1F1F3F4step 3.1

Regard F first as a map M→O with the restricted target metric. It is still a local Riemannian isometry by [F1], so [F4] makes σ=F∘η:R→O a geodesic. It has σ(0)=q and σ′(0)=dFp(v)=w. By [F3], the maximal geodesic in O with data (q,w) contains this global geodesic and hence has domain R. Since (q,w) was arbitrary, O is geodesically complete.

5.1F3F4step 4.1

Regard the same σ as an N-valued geodesic. It has the same initial data (q,w), so uniqueness in [F3] identifies it with the maximal N-geodesic on that geodesic's domain. Because σ itself is defined on all of R, maximality makes the N-geodesic global; its value at every time is F(η(t))∈O. This proves the stronger assertion.

6.1A1F1F2F3step 1.1step 2.1step 3.1step 4.1step 5.1∎

The empty case was settled in step 2.1. In dimension zero, every tangent vector is zero and the relevant geodesics are constant; dimension one is unchanged. The zero vector and both positive and negative infinite-time directions are included because η has domain all of R. The statement is one-way and does not infer a covering map. Assumption [A1] is used through [F2] and [F3]; choosing one preimage after fixing (q,w) and applying one inverse linear map require no family-wide choice.

Source locator

Datar, Theorem 20.1.1 and its geodesic-lifting step, pp.147--149, prove the stronger covering and target-completeness theorem for a complete source local isometry. The present corollary retains only the initial-data lifting and geodesic-complete-image consequences.

Depends on

Used by

Nothing in the library uses this result yet.

Dependency tree · two levels

45 results within two dependency steps of this one, each drawn at its shortest distance from it. An arrow runs from a result to what uses it, so the chart reads left to right and ends at this result, which carries a heavier outline. Every node is a link to that result. Click elsewhere on the chart to enlarge it.

Sources