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LemmaStatement: Literature-sourcedProof: AI-adaptedPipeline-generatedprecheck passjudge pass (gpt-6-sol)audited 2026-09-30
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Covariant derivatives commute up to curvature in a two parameter variation

Statement

Use the curvature convention R(X,Y)Z=∇X∇YZ−∇Y∇XZ−∇[X,Y]Z. Let F be a smooth two-parameter variation (in particular, it may be the geodesic variation of Geodesic variation) and let V be a smooth vector field along F. Write Ds,Dt for covariant differentiation along the two parameter curves. Then DsDtV−DtDsV=R(Fs,Ft)V. The identity holds on the parameter interior and extends to included endpoints by the smooth one-sided derivatives. It does not require the longitudinal curves of F to be geodesic.

Facts & Assumptions

Given: A smooth map F from a parameter rectangle to a manifold with an affine connection, and a smooth section V along F.

[F1]

The parameter derivatives and smooth variation field have the meaning in Geodesic variation.

[F2]

Covariant differentiation along a parameter curve is the induced connection derivative, as in Covariant derivative along a curve.

[F3]

Curvature is the bracket-corrected commutator Curvature of an affine connection.

[F4]

Curvature is C∞-linear in its three vector-field slots by Curvature is C-infinity-linear in all three vector fields.

Proof

technique · direct coordinate computation
1.1F1F2given

Fix any point in the parameter rectangle and choose a target coordinate chart near its image. Write F=(xa(s,t)), V=Vi(s,t)∂i, S=Fs, and T=Ft; by [F2], DtV=(∂tVi)∂i+ViDt∂i and DsV=(∂sVi)∂i+ViDs∂i. This is a local calculation, with no frame chosen over the whole rectangle.

1.2F2given

Expand the two iterated derivatives using those coordinate formulas: the mixed ordinary derivatives of Vi and the two cross terms cancel, leaving DsDtV−DtDsV=Vi(DsDt∂i−DtDs∂i). Since Dt∂i=Ftj∇∂j∂i and Ds∂i=Fsk∇∂k∂i, equality of the mixed partials of F cancels the derivatives of Fs,Ft, leaving FskFtjVi(∇∂k∇∂j−∇∂j∇∂k)∂i.

2.1F3F4step 1.2

Coordinate fields commute, so [∂k,∂j]=0; by [F3] the remaining expression is FskFtjViR(∂k,∂j)∂i, and [F4] identifies it with R(Fs,Ft)V. Thus the identity holds in each local chart and on overlaps because both sides are intrinsically defined.

3.1

Smoothness to the parameter boundary extends the identity there by one-sided limits; the empty manifold has no given map F. If V=0, both sides vanish; in dimension zero every field along F is zero, and in dimension one the calculation applies with curvature zero because its first two slots are alternating. Only a chart near an arbitrary point is used, so no choice principle is needed; the claim is an identity, not a biconditional. [F1, F2, F3, step 2.1] □

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