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Cauchy sets are closed, split the manifold into past, set and future, and are locally Lipschitz graphs

Statement

Assume Countable Choice and Dependent Choice (The Axiom of Countable Choice (ACω), The axiom of dependent choice: a relation in which every element is related to something admits an N-indexed chain) for the absolutely continuous causal-curve calculus and the supplied causal results used below.

Let (M,g,N) be a time-oriented smooth Lorentzian four-manifold (Smooth time-oriented Lorentzian four-manifolds: the geometric objects of the model) and let S⊆M be a Cauchy set (Spacelike hypersurfaces, acausal sets, Cauchy sets, domains of dependence and Cauchy horizons clause (c)): every inextendible causal curve γ:I→M has γ−1[S]={t∈I:γ(t)∈S} of exactly one element. Then:

(a) there is no nonconstant future causal curve δ:[a,b]→M with δ(a)=δ(b); in particular S is achronal and acausal, and the three sets I−(S), S, I+(S) are pairwise disjoint with M=I−(S)  ⊔  S  ⊔  I+(S); moreover for x∉S one has x∈I+(S) if and only if some point of S chronologically precedes x;

(b) S is closed in M;

(c) for every p∈S there are a chart (U,x) of the kind produced by Causal cone domination in adapted charts and Lipschitz-graph bounds for causal curves clauses (a) and (d) around p, with x(p)=0 and the supplier constants K≥1 and c=16, and numbers a,ρ,η>0 with c ρ+η<a and W:=x−1((−a,a)×Bρ(0))⊆U such that for every z∈Bρ(0) the coordinate vertical line Lz=x−1((−a,a)×{z}) meets S∩W in exactly one point x−1(φ(z),z), and ∣φ(z)−φ(z′)∣≤c ∣z−z′∣(z,z′∈Bρ(0)), with φ(0)=0 and ∣φ(z)∣≤c ∣z∣<a. The cylinder W may be chosen inside any prescribed neighborhood of p. Consequently the maps z↦x−1(φ(z),z) form a topological atlas on the closed set S, making S a topological 3-manifold in the subspace topology whose inclusion into M is a topological embedding.

Facts & Assumptions

Given: A time-oriented smooth Lorentzian four-manifold (M,g,N) and a Cauchy set S⊆M.

[L1]

S is acausal, hence achronal: no two distinct points of S are causally, respectively chronologically, related in either direction (Convergent causal ends are extendible, maximal geodesics have no limit, and Cauchy sets are acausal clause (d), Spacelike hypersurfaces, acausal sets, Cauchy sets, domains of dependence and Cauchy horizons clause (b)).

[L2]

Every maximal geodesic γq,v with v≠0 is defined on an open interval and does not converge to any point of M as the parameter tends to either end; hence it is an inextendible causal curve whenever v is timelike. Along a geodesic the causal character and time orientation of the tangent are constant, so a geodesic with future timelike initial velocity is a future timelike curve; on its image every point is a value of the parameter (Convergent causal ends are extendible, maximal geodesics have no limit, and Cauchy sets are acausal clauses (b) and (c), Covariant differentiation along curves: metric pairing, parallel transport and geodesic speed clause 3, The geodesic initial-value problem and the exponential map of the metric-selected connection clauses (a) and (d), Causal curves, chronological and causal reachability, and inextendibility clauses (b) and (d)).

[L3]

I+(x) and I−(x) are open for every x, and {(y,z):y≪z} is open in M×M (Openness of the chronological future and past, openness of the chronological relation, and closure of future and past sets clauses (a) and (b)).

[L4]

Adapted chart and flat minorant: around every p there are a chart (U,x) with x(p)=0, a radius r>0 with x(U)=Br(0), a constant K≥1 with n=N/−g(N,N)=∂/∂x0 and g00≡−1 on U, and the flat metric ηc=−(dx0)2+c∑i=13(dxi)2 with c=16 such that every ηc-causal vector is g-timelike and, whenever ηc(q′−q,q′−q)<0 for q,q′∈U, the points q,q′ are chronologically related with q≪q′ if x0(q′)>x0(q) (Causal cone domination in adapted charts and Lipschitz-graph bounds for causal curves clauses (a) and (d), Observers, rest spaces and the spatial projection at an event). The coordinate vertical lines of this chart are the integral curves of n=∂/∂x0, hence future timelike curves, and for s<s′ in (−a,a) one has x−1(s,z)≪x−1(s′,z) (Causal curves, chronological and causal reachability, and inextendibility). The vertical segments have affine coordinates; in any other chart their smooth representatives have bounded derivative on sufficiently small compact segments, hence are Lipschitz and absolutely continuous by the mean value bound.

[L5]

Restrictions to subintervals and finite concatenations of locally absolutely continuous closed curve pieces retain absolute continuity and the almost-everywhere causal velocity condition. This follows directly from the finite epsilon-delta definition: for a compact interval meeting k pieces, use tolerance ε/k on each piece and the minimum of the finitely many corresponding deltas, split each finite test family at the junctions, and sum the variation bounds. The exceptional velocity sets are a finite union of null sets together with finitely many junctions. Thus no general absolutely continuous integration theorem or additional choice is used in this finite step (Causal curves, chronological and causal reachability, and inextendibility).

Proof

technique · direct
1.1L1L5givenalgebra

(No closed causal curve.) Let δ:[0,1]→M be a future causal curve with δ(0)=δ(1), nonconstant. Define the periodic extension β:R→M by β(t):=δ(t−⌊t⌋). On each interval (n,n+1) the curve β is the restriction of δ up to an increasing affine reparametrization, so it is locally absolutely continuous with future causal velocity almost everywhere, and by [L5] this persists across the finitely many junctions of every compact interval: β is a future causal curve. It is future-inextendible: if β(t)→z as t→+∞, then for every s∈(0,1) the sequence β(s+n)=β(s) converges to z, so β(s)=z for all s∈(0,1), contradicting the nonconstancy of δ on [0,1]; the same argument at −∞ (using β(s−n)=β(s)) gives past-inextendibility. Hence β is an inextendible causal curve, and by the Cauchy property β−1[S] has exactly one element t0; but then t0+1∈β−1[S] as well, since β(t0+1)=β(t0)∈S, and t0+1≠t0. This contradiction shows that no such δ exists.

1.2L1L4givenconstruct

(A vertical line meets S at most once.) Fix p∈S and the chart (U,x), constants K≥1 and c=16, and minorant ηc of [L4]. Write x(U)=Br(0). Choose 0<a<r/2, 0<ρ<a/(4c) and η:=a/2. Then a2+ρ2<r and c ρ+η<a, so W:=x−1((−a,a)×Bρ(0))⊆U. These choices can be made arbitrarily small: for any prescribed neighborhood V of p, first reduce r so that x−1(Br(0))⊆V, retaining the same adapted coordinate functions, cone constants and g00=−1, and then choose a,ρ,η as above. For z∈Bρ(0) the vertical line Lz is the image of a future timelike curve [L4]; two distinct points x−1(s,z) and x−1(s′,z) of S with s<s′ would be chronologically related, contradicting [L1]. Hence S∩Lz has at most one point.

2.1step 1.1L1L2L3given

(Disjointness and the decomposition.) Let x∈M. Choose a future timelike vector w∈TxM and let γ:=γx,w:I→M be the maximal geodesic through x with γ′(0)=w; by [L2] it is an inextendible future timelike curve, and γ(0)=x. By the Cauchy property there is exactly one t0∈I with γ(t0)∈S. If x=γ(t0), then x∈S. If x≠γ(t0) and 0>t0, then γ∣[t0,0] is a future timelike curve from a point of S to x, so x∈I+(S); if 0<t0, then γ∣[0,t0] is a future timelike curve from x to a point of S, so x∈I−(S). Hence M=I−(S)∪S∪I+(S). The sets are pairwise disjoint: if s∈S∩I+(S), there is s′∈S with s′≪s, and s′≠s because s′≪s forces s′≠s; this contradicts acausality [L1]. If x∈I+(S)∩I−(S), there are s1,s2∈S with s1≪x≪s2; if s1≠s2 this contradicts acausality [L1], while if s1=s2 then transitivity of ≪ gives s1≪s1, that is, a closed future timelike curve through s1, which is excluded by step 1.1 applied to that closed curve. This proves (a), including the characterization of membership in I±(S).

3.1step 2.1L1L2L3given

(Closedness.) Let sk∈S with sk→q∈M, and suppose q∉S. Choose a maximal geodesic γ:=γq,w with future timelike w as in [L2]; it is an inextendible future timelike curve and meets S in exactly one point r:=γ(t0), with r≠q because q∉S. Let tq:=0 be the parameter of q. If t0<0 then γ∣[t0,0] is a future timelike curve from r to q, so r≪q; since I+(r) is open [L3] and sk→q, for all large k we have sk∈I+(r), that is, r≪sk with r,sk∈S; since sk≠r for large k (as sk→q≠r), this contradicts the acausality of S [L1]. If t0>0 then γ∣[0,t0] is a future timelike curve from q to r, so q≪r; since I−(r) is open [L3], for large k we have sk∈I−(r), that is, sk≪r with sk,r∈S and sk≠r, again contradicting acausality. Hence q∈S: S is closed. This proves (b).

3.2step 2.1step 1.2L3L4givenalgebra

(A vertical line meets S at least once.) With p,W,a,ρ,η as in step 1.2, fix z∈Bρ(0) and put q−:=x−1(−c ∣z∣−η,z) and q+:=x−1(c ∣z∣+η,z). Both are in W since c ∣z∣+η<c ρ+η<a. In coordinate differences from p one has ηc(q+−p,q+−p)=−(c ∣z∣+η)2+c∣z∣2=−2c ∣z∣η−η2<0, and the same value for ηc(p−q−,p−q−). Thus [L4] gives q−≪p≪q+, so q−∈I−(S) and q+∈I+(S). The vertical segment Jz joining them is connected. If it avoided S, step 2.1 would partition it into the disjoint relatively open sets Jz∩I−(S) and Jz∩I+(S), open by [L3] and both nonempty by their endpoints. This contradicts connectedness. Hence Jz∩S≠∅, and step 1.2 gives exactly one intersection.

4.1step 3.2L1L4givenalgebra

(The graphing function is Lipschitz.) For z∈Bρ(0) let φ(z)∈(−a,a) be the x0-coordinate of the unique point of S∩Lz, so that S∩W={x−1(φ(z),z):z∈Bρ(0)}, and ∣φ(z)∣≤c ∣z∣+η<a by step 3.2. Since p=x−1(0,0)∈S, uniqueness on L0 gives φ(0)=0. If z,z′∈Bρ(0) with ∣φ(z)−φ(z′)∣>c∣z−z′∣, set δ:=(φ(z)−φ(z′),z−z′) and suppose φ(z)>φ(z′) (the other case is symmetric); then ηc(δ,δ)=−(φ(z)−φ(z′))2+c∣z−z′∣2<0, and both x−1(φ(z),z) and x−1(φ(z′),z′) lie in S∩W⊆U, so [L4] gives x−1(φ(z′),z′)≪x−1(φ(z),z): two distinct points of S chronologically related, contradicting acausality [L1]. Hence ∣φ(z)−φ(z′)∣≤c∣z−z′∣. Taking z′=0 and using φ(0)=0 gives ∣φ(z)∣≤c ∣z∣<a.

5.1step 1.2step 4.1givenconstruct∎

(Topological hypersurface.) For p∈S and its chart as above, the map ψ:Bρ(0)→S∩W, ψ(z)=x−1(φ(z),z) is continuous (a Lipschitz function into Euclidean space followed by the continuous chart inverse), injective and surjective onto S∩W by step 4.1, and the restriction of the continuous coordinate projection π:x−1(s,z)↦z to S∩W is its inverse, because a point of S∩W lies on exactly one vertical line and has the form x−1(φ(π(⋅)),π(⋅)) by step 1.2; hence ψ is a homeomorphism onto the relatively open set S∩W. For two such graph charts ψ,ψ′ the transition ψ′−1∘ψ=π′∘ψ is continuous on its domain, so these charts form a topological atlas on S; consequently S is a topological 3-manifold in the subspace topology and its inclusion into M is a topological embedding. This proves (c) and completes the proof.

Remarks

  • What is and is not proved. No smoothness of S is asserted: the transition maps are only continuous, and no normal vector field is constructed. The proof uses only the Cauchy property, the acausality of Cauchy sets, the openness of chronology and the flat minorant cone of the adapted chart.

  • The role of the minorant cone. The flat form ηc is used only to produce chronological relations: to find points of I±(S) on every vertical line (step 3.2) and to force the Lipschitz bound (step 4.1), where the absence of a chronological relation between two points of S is turned into the inequality for φ.

  • Use. Clauses (a) and (b) are used in The existence of a Cauchy set implies strong causality and compact causal diamonds and clause (c) records the terminology of Cauchy sets as embedded topological hypersurfaces; the graph representation is also the model for the local Cauchy-neighbourhood lemma of this page.

Depends on

Dependency tree · 2 levels

Sources