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A variable-time flow through a fixed boundary has the boosted unit normal
Statement
Let a smooth Killing field vanish on a compact spacelike boundary surface of a reference spacelike section in a smooth time-oriented Lorentzian four-manifold of signature . Let be the future unit reference normal and the exterior unit boundary normal. Fix and impose the signed normal-boost convention and on , where is the Levi–Civita connection. Let be a local flow of . On a reference neighborhood of , let be smooth down to , with , and suppose the variable-time map is a smooth embedding with spacelike image, the candidate section. Then on its future unit normal is . In particular . The derivative of contributes nothing to the boundary tangent map because there.
Statement references
Facts & Assumptions
A smooth embedded spacelike section has its unique future unit normal, including at its smooth spacelike boundary. Spacelike sections, maximality and lapse–shift data
With the stated signed infinitesimal boost in the ordered normal basis , the Killing flow fixes pointwise, its differential is the identity on , and its normal-plane differential is the boost with off-diagonal entries . Normal boost action and invariant two-forms at a fixed surface
The derivative of a smooth flow with respect to its time is its generating field at the image point. Local and global flows generated by a vector field
For composable smooth maps , the differential satisfies . The chain rule for differentials of smooth maps
A smooth embedding between manifolds with boundary is an immersion and a homeomorphism onto its image; its differential on the full tangent spaces is injective at every point, including boundary points. Immersions and embeddings for manifolds with boundary
Proof
Given: The reference section, its boundary , the signed boost hypotheses, and the smooth variable-time embedding with spacelike image in the Statement.
Goal: Establish the boundary normal formula, the angle identity, and independence of height derivatives in the boundary tangent map.
At , the flow fixes . Apply the chain rule to . For every vector in the reference tangent space at , this gives , since and . At the boundary this calculation is made using smooth local extensions in boundary charts; smoothness down to ensures that the resulting differentials agree with those of the given maps. Thus the candidate tangent hyperplane is the image of the reference tangent hyperplane under , independently of all height derivatives.
The identity action on and the normal-plane boost preserve , so is a linear isometry. Its image of is , a future unit timelike vector because and . By step 1.1 this vector is orthogonal to the candidate tangent hyperplane, hence is its unique future unit normal. Pairing with and using and gives .
Depends on
- Spacelike sections, maximality and lapse–shift data
- Killing fields of a Lorentzian metric
- Normal boost action and invariant two-forms at a fixed surface
- Local and global flows generated by a vector field
- The chain rule for differentials of smooth maps
- Immersions and embeddings for manifolds with boundary
Dependency tree · 2 levels
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