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A variable-time flow through a fixed boundary has the boosted unit normal

Statement

Let a smooth Killing field K vanish on a compact spacelike boundary surface S of a reference spacelike section in a smooth time-oriented Lorentzian four-manifold (M,g) of signature (−,+,+,+). Let nˉ be the future unit reference normal and νˉ the exterior unit boundary normal. Fix κ>0 and impose the signed normal-boost convention ∇nˉK=κνˉ and ∇νˉK=κnˉ on S, where ∇ is the Levi–Civita connection. Let ϕK:D→M be a local flow of K. On a reference neighborhood of S, let u be smooth down to S, with (u(x),x)∈D, and suppose the variable-time map Φ(x)=ϕu(x)K(x) is a smooth embedding with spacelike image, the candidate section. Then on S its future unit normal is n=cosh⁡(κu)nˉ+sinh⁡(κu)νˉ. In particular −g(n,nˉ)=cosh⁡(κu). The derivative of u contributes nothing to the boundary tangent map because K=0 there.

Facts & Assumptions

[F1]

A smooth embedded spacelike section has its unique future unit normal, including at its smooth spacelike boundary. Spacelike sections, maximality and lapse–shift data

[F2]

With the stated signed infinitesimal boost in the ordered normal basis (nˉ,νˉ), the Killing flow fixes S pointwise, its differential is the identity on TS, and its normal-plane differential is the boost with off-diagonal entries sinh⁡(κt). Normal boost action and invariant two-forms at a fixed surface

[F3]

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

[F4]

For composable smooth maps F,G, the differential satisfies d(G∘F)p=dGF(p)∘dFp. The chain rule for differentials of smooth maps

[F5]

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 S, 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.

1.1F1F2F3F4F5

At p∈S, the flow fixes p. Apply the chain rule to x↦(u(x),x)↦ϕu(x)K(x). For every vector X in the reference tangent space at p, this gives dΦp(X)=dϕu(p)K∣p(X)+dup(X)Kϕu(p)K(p)=dϕu(p)K∣p(X), since ϕu(p)K(p)=p and Kp=0. At the boundary this calculation is made using smooth local extensions in boundary charts; smoothness down to S 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 dϕu(p)K∣p, independently of all height derivatives.

2.1F1F2step 1.1algebra∎

The identity action on TpS and the normal-plane boost preserve gp, so dϕu(p)K∣p is a linear isometry. Its image of nˉp is cosh⁡(κu(p))nˉp+sinh⁡(κu(p))νˉp, a future unit timelike vector because cosh⁡(κu(p))>0 and cosh⁡2(κu(p))−sinh⁡2(κu(p))=1. By step 1.1 this vector is orthogonal to the candidate tangent hyperplane, hence is its unique future unit normal. Pairing with nˉp and using g(nˉp,nˉp)=−1 and g(νˉp,nˉp)=0 gives −g(np,nˉp)=cosh⁡(κu(p)).

Depends on

Used by · 3

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