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ADM section time and causal spatial speed

Statement

Assume the Axiom of Choice. Equip E=Rv×S, where S is a connected smooth three-manifold, with the canonical product smooth structure. Let h be a smooth Riemannian metric on S, N>0 a smooth function on S, and X a smooth vector field on S, extended independently of v using the product splitting. Give g=−N2dv2+h(dx+Xdv,dx+Xdv) the time orientation of n=N−1(∂v−X). This is a smooth Lorentzian metric of signature (−,+,+,+), and n is its smooth unit timelike normal to the v-slices, declared future-directed. A causal curve means a locally absolutely continuous curve with nonzero causal velocity almost everywhere. Every future causal curve has strictly increasing v and can be written as (v,x(v)) on its v-image. This representation is locally Lipschitz in charts, is future causal, and satisfies ∣x′+X∣h≤N almost everywhere. In particular ∣x′∣h≤N+∣X∣h and ∣(f∘x)′∣≤N∣df∣h+∣X(f)∣ for every smooth real f on S. Here ∣Y∣h=h(Y,Y), ∣df∣h:=∣grad⁡hf∣h, where h(grad⁡hf,Y)=df(Y), and X(f)=df(X) is the action of X on f. Inextendibility as absence of an endpoint is preserved by this change of parameter.

Statement references

Facts & Assumptions

Given: The data and hypotheses in the Statement.

Goal: The conclusions stated there.

[F1]

The Axiom of Choice implies Dependent Choice and Countable Choice, supplying the hypotheses of the causal-curve calculus and absolutely-continuous fundamental theorem used below. The Axiom of Choice AC implies DC implies countable choice

[F2]

Causal curves are locally absolutely continuous, have nonzero future causal velocity almost everywhere, and inextendibility means absence of a limit at a parameter end. Causal exterior, chronological boundaries and Cauchy data

[F3]

A lapse and shift decompose the stationary vector as ∂v=Nn+X with g(n,n)=−1 and X tangent to the spacelike slice. Spacelike sections, maximality and lapse–shift data

[F4]

Smooth composition of a locally absolutely continuous curve is locally absolutely continuous and satisfies the chain rule almost everywhere; strictly increasing continuous changes of parameter preserve the endpoint criterion. Chart independence, concatenation, reparametrization and transitivity for causal curves

[F5]

An absolutely continuous real function is the integral of its almost-everywhere derivative; Lipschitz functions are absolutely continuous. Fundamental theorem of calculus for absolutely continuous functions C¹ implies Lipschitz, Lipschitz implies absolutely continuous, and absolutely continuous implies continuous and bounded variation

[F6]

On a compact coordinate ball, a smooth positive-definite metric bounds the Euclidean norm from below and above. Local comparison of a riemannian metric with the euclidean metric

[F7]

The canonical product charts give E=R×S its smooth four-manifold structure and the splitting T(v,p)E=R∂v⊕TpS. Products of smooth manifolds have a canonical product smooth structure

[F8]

The pointwise norm is ∣Y∣h=h(Y,Y), the gradient satisfies df(Y)=h(grad⁡hf,Y), and the vector-field action is X(f)=df(X). Cauchy–Schwarz in the inner product hp gives ∣df(Y)∣≤∣df∣h∣Y∣h with the norm convention in the Statement. Pointwise norm and angle from a riemannian metric The Riemannian gradient is the metric dual of the differential The action of a vector field on smooth functions Cauchy–Schwarz: |⟨ u,v⟩|≤‖ u‖‖ v‖, with equality exactly for linearly dependent vectors

[F9]

A Riemannian metric is a smooth symmetric covariant two-tensor that is positive definite on each tangent space. Riemannian metric and riemannian manifold

[F10]

A Lorentzian metric in four dimensions is a smooth symmetric nondegenerate covariant two-tensor of signature (−,+,+,+). A time orientation is a smooth timelike vector field n; a nonzero causal vector Y is future-directed exactly when g(Y,n)<0. Smooth time-oriented Lorentzian four-manifolds: the geometric objects of the model

Proof

1.1F2F3F6F7F9F10algebra

In the product splitting, the map (a,W)↦(a,W+aX) is invertible and carries the quadratic form of g to −N2a2+h(W,W). Smoothness, N>0 and positive definiteness of h therefore make g smooth and Lorentzian of the asserted signature. Direct substitution gives g(n,n)=−1 and g(n,W)=0 for spatial W, while the restriction to each slice is h; hence n is the asserted smooth unit normal. For a nonzero future causal vector Y=a∂v+W, its pairing with n is −Na<0, so a>0. The metric identity gives ∣W+aX∣h≤Na. Applied almost everywhere to the original curve parameter s, these identities give vs>0 and the coordinate estimate ∣xs∣e≤Bvs on any relatively compact coordinate neighborhood, for some finite B. The bound follows from smoothness of N,X,h and the metric comparison.

2.1F1F4F5F8step 1.1algebra

Integrating vs>0 on any nondegenerate compact parameter interval shows that v is strictly increasing. It therefore has a continuous inverse on its image interval. To justify the required vector estimate using scalar integration, let z:[a,b]→R3 have absolutely continuous coordinates, let w:[a,b]→R be absolutely continuous with ws≥0 almost everywhere, and suppose ∣zs∣H≤Cws almost everywhere for a fixed inner product H and constant C≥0. Put D=z(b)−z(a). If D≠0, fix e=D/∣D∣H and the real function ϕ(s)=H(e,z(s)). This fixed linear combination of coordinates is absolutely continuous, and ϕs=H(e,zs) almost everywhere. The scalar fundamental theorem makes ϕs,ws integrable; Cauchy–Schwarz gives ϕs≤Cws. Consequently ∣D∣H=ϕ(b)−ϕ(a)=∫abϕs ds≤C∫abws ds=C(w(b)−w(a)). If D=0, the same bound follows from w(b)≥w(a). On each compact chart subarc apply this estimate with z=x, w=v, H the Euclidean inner product and C=B, obtaining ∣x(s2)−x(s1)∣e≤B(v(s2)−v(s1)). Thus x as a function of v is locally Lipschitz; each coordinate is therefore locally absolutely continuous. This argument does not assume absolute continuity of the inverse of v.

3.1F1F4F5F6F8step 1.1step 2.1algebra

At an interior differentiability point v0 of x(v), put p=x(v0) and, in a spatial chart, freeze H=hp, N0=N(p) and c=X(p), identifying coordinate tangent vectors with R3. On a sufficiently short subarc about p, continuity of the coefficients and the coordinate speed bound imply ∣xs+vsc∣H≤(N0+ϵ)vs almost everywhere, where ϵ→0 as the subarc shrinks. On each compact subarc the coordinates of z(s)=x(s)+v(s)c are absolutely continuous, since they are fixed linear combinations of the original absolutely continuous coordinates. Their derivatives and vs are integrable by the scalar fundamental theorem. Apply the scalar-projection estimate proved in step 2.1 with this z, w=v, the fixed inner product H and C=N0+ϵ; it yields ∣x(s2)−x(s1)+(v(s2)−v(s1))c∣H≤(N0+ϵ)(v(s2)−v(s1)). Take one endpoint at v0, divide by the positive increase of v, and shrink the subarc to v0. The differentiability of x(v) gives ∣xv(v0)+X(p)∣hp≤N(p). By local Lipschitz continuity and the scalar fundamental theorem applied to the three coordinates, such differentiability points have full measure in the v-interval. Hence ∣xv+X∣h≤N almost everywhere. Its time component is one, so the reparametrized velocity is nonzero future causal. This proves the reparametrized causal inequality.

4.1F4F8step 2.1step 3.1algebra∎

The triangle inequality gives ∣xv∣h≤N+∣X∣h. For a smooth real f, the smooth-composition chain rule gives (f∘x)′=df(xv)=df(xv+X)−X(f) almost everywhere. Applying the gradient identity and Cauchy–Schwarz of [F8] to xv+X yields ∣(f∘x)′∣≤∣df∣h∣xv+X∣h+∣X(f)∣≤N∣df∣h+∣X(f)∣. Finally the increasing homeomorphism of parameter intervals preserves all endpoint limits in either direction, proving the inextendibility assertion.

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