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Covariant derivatives commute up to curvature in a two parameter variation
Statement
Use the curvature convention Let be a smooth two-parameter variation (in particular, it may be the geodesic variation of Geodesic variation) and let be a smooth vector field along . Write for covariant differentiation along the two parameter curves. Then 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 to be geodesic.
Facts & Assumptions
Given: A smooth map from a parameter rectangle to a manifold with an affine connection, and a smooth section along .
The parameter derivatives and smooth variation field have the meaning in Geodesic variation.
Covariant differentiation along a parameter curve is the induced connection derivative, as in Covariant derivative along a curve.
Curvature is the bracket-corrected commutator Curvature of an affine connection.
Curvature is -linear in its three vector-field slots by Curvature is C-infinity-linear in all three vector fields.
Proof
Fix any point in the parameter rectangle and choose a target coordinate chart near its image. Write , , , and ; by [F2], and . This is a local calculation, with no frame chosen over the whole rectangle.
Expand the two iterated derivatives using those coordinate formulas: the mixed ordinary derivatives of and the two cross terms cancel, leaving . Since and , equality of the mixed partials of cancels the derivatives of , leaving .
Coordinate fields commute, so ; by [F3] the remaining expression is , and [F4] identifies it with . Thus the identity holds in each local chart and on overlaps because both sides are intrinsically defined.
Smoothness to the parameter boundary extends the identity there by one-sided limits; the empty manifold has no given map . If , both sides vanish; in dimension zero every field along 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]
Depends on
Used by
- Jacobi field Definition
- Second variation formula for energy Theorem
- Variation field of a geodesic variation is a Jacobi field Theorem
Dependency tree · two levels
11 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
- John M. Lee, Riemannian Manifolds: An Introduction to Curvature (1997), Lemma 10.1 (standard reference, not scraped)
- Ved Datar, Lectures on Riemannian Geometry (2025), Lectures 21–24 (standard reference, not scraped)