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Equivalent characterizations of a totally geodesic submanifold
Statement
Assume . Let be an embedded Riemannian submanifold, and assume both manifolds are boundaryless so that the library's two-sided geodesic convention applies. The following conditions are equivalent:
- , so is totally geodesic;
- is tangent to for all local tangent fields ;
- every intrinsic affinely parametrized geodesic of , viewed in , is an ambient affinely parametrized geodesic on every common interval of definition.
The choice hypothesis is inherited exactly from the smooth submanifold projections and geodesic existence.
Facts & Assumptions
Given: Countable choice and the boundaryless embedded Riemannian submanifold.
Total geodesicity means . Totally geodesic submanifold.
The Gauss decomposition is . Induced connection and second fundamental form.
The induced connection is the intrinsic Levi–Civita connection. The induced connection is Levi–Civita.
The second fundamental form is symmetric and bilinear. The second fundamental form is a symmetric normal-bundle-valued two-tensor.
A geodesic is characterized by vanishing covariant acceleration, with the derivative along a curve defined by the pullback connection. Geodesic of an affine connection, Covariant derivative along a curve.
Under , every supplied initial tangent vector has a unique local intrinsic geodesic. Existence uniqueness and smooth dependence of geodesics.
Proof
By [F2], the normal component of is exactly . Thus condition 1 holds if and only if condition 2 holds.
Pulling [F2] back along a smooth curve in and evaluating on its velocity gives the curvewise Gauss formula This follows in a local frame directly from the pullback derivative in [F5], so it is independent of field extensions. If condition 1 holds and is an intrinsic geodesic, [F3] and [F5] make the first term zero and [F1] makes the second zero. Hence is an ambient geodesic, proving condition 3.
Conversely assume condition 3. Fix and . By [F6] there is an intrinsic geodesic with . Condition 3 and [F5] make both covariant accelerations in step 1.2 zero, so . Since were arbitrary, this holds for every tangent vector.
By symmetry and bilinearity [F4], polarization gives Thus , proving condition 1 and completing the equivalence.
On the empty manifold all three universal conditions hold. In dimension zero all geodesics are constant and is zero; the proof applies unchanged in dimension one and in codimension zero. Both manifolds are explicitly boundaryless because [F5] uses that convention; parameter intervals have nonempty interior and any included endpoints use their stated one-sided derivative. Positive definiteness supplies the orthogonal decomposition. The only choice is the declared inherited through [F1]–[F3] and used by [F6]; step 2.1 invokes existence for one supplied at a time.
Depends on
- Totally geodesic submanifold
- Induced connection and second fundamental form
- The induced connection is Levi–Civita
- The second fundamental form is a symmetric normal-bundle-valued two-tensor
- Geodesic of an affine connection
- Covariant derivative along a curve
- Existence uniqueness and smooth dependence of geodesics
Used by
Nothing in the library uses this result yet.
Dependency tree · two levels
21 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 (standard reference, not scraped)