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Openness of the chronological future and past, openness of the chronological relation, and closure of future and past sets

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, with the relations ≪, ≤ and the sets I±, J± of Causal curves, chronological and causal reachability, and inextendibility and the future and past sets of Future sets, past sets, achronal boundaries and their elementary properties. Then:

(a) Openness. For every x∈M the chronological future I+(x) and the chronological past I−(x) are open subsets of M.

(b) The chronological relation is open. The set {(x,y)∈M×M: x≪y} is open in the product topology of M×M.

(c) Closure of future and past sets. Let F⊆M be a future set, that is I+(F)⊆F. Then every q∈F‾ satisfies I+(q)⊆F. Dually, if P is a past set (I−(P)⊆P) and q∈P‾, then I−(q)⊆P.

Facts & Assumptions

Given: A time-oriented smooth Lorentzian four-manifold (M,g,N) and the points and sets of the claims.

[L1]

In every strictly convex normal ball B, and for every base point p∈B, the set IB+(p) of endpoints of future timelike curves in B starting at p is open in B and equals the exponential image of the future timelike vectors in exp⁡p−1(B) (Local causality in a convex normal ball: causal reachability is the exponential cone, the Lorentzian length is bounded by the displacement radius, and null endpoints force the null geodesic clause (b), Existence of strictly convex normal neighborhoods: small coordinate balls are normal neighborhoods of each of their points). Since B is open in M, this set is also open in M.

[L2]

If γ:[a,b]→M is a future timelike curve and a≤s<t≤b, then γ∣[s,t] is a future timelike curve, because the set of parameters at which the velocity exists and is future timelike is of full measure and restricts to a set of full measure in [s,t]; also γ(s)≪γ(t) (Causal curves, chronological and causal reachability, and inextendibility clause (b) and clause (c)).

[L3]

Concatenation and transitivity: a finite concatenation of future timelike curves is a future timelike curve, and from x≪z and z≪y it follows that x≪y (Chart independence, concatenation, reparametrization and transitivity for causal curves clauses (d) and (f)).

[L4]

A future set F satisfies I+(F)⊆F, and then also I+(q)⊆I+(F)⊆F for any q∈F (Future sets, past sets, achronal boundaries and their elementary properties clause (a)); a past set satisfies I−(P)⊆P.

Proof

technique · direct
1.1L1L2L3given

(Openness of I+(x).) Let y∈I+(x) and let γ:[0,1]→M be a future timelike curve from x to y. Choose a strictly convex normal ball B about y. By continuity, choose a fixed t0∈(0,1) sufficiently near 1 that γ([t0,1])⊆B, and put p0:=γ(t0). The tail is a future timelike curve in B, so y∈IB+(p0). By [L1], IB+(p0) is open in M; choose a neighborhood V of y contained in it. For every z∈V, we have x≪p0 by [L2] and p0≪z by the definition of IB+(p0); transitivity [L3] gives x≪z. Thus V⊆I+(x) and I+(x) is open. The time-reversed argument gives openness of I−(x). The center p0 is fixed throughout the neighborhood argument; continuity is used only to place the original curve tail in the ball around y.

2.1step 1.1L3given

(Openness of the chronological relation.) Let x≪y and choose a future timelike curve γ from x to y; pick t0∈(0,1) and put z:=γ(t0), so that x≪z≪y by [L2] and [L3]. By step 1.1 the sets I−(z)={a:a≪z} and I+(z) are open, and I−(z)×I+(z) is an open neighborhood of (x,y) in M×M; every (a,b) in it satisfies a≪z≪b, hence a≪b by [L3]. This proves (b).

3.1step 2.1L4given

(Future sets are closed under the chronological future of their closure.) Let F be a future set and q∈F‾. Let r∈I+(q). By step 2.1, the set I−(r) is an open neighborhood of q, so it meets F; choose one f∈F∩I−(r). Then f≪r, and r∈I+(f)⊆I+(F)⊆F by [L4]. Hence I+(q)⊆F; the past statement is the time reverse. No sequence of chosen points is needed.

4.1step 1.1step 2.1step 3.1∎

(Conclusion.) Step 1.1 proves (a), step 2.1 proves (b) and step 3.1 proves (c).

Remarks

  • Where local causality enters. The only input from the local theory is the openness of the cone image IB+(p) in a strictly convex normal ball; everything else is transitivity and the definition of the relations.

  • Scope. The result is a statement about the causal structure of the smooth Lorentzian model; it asserts no global causality condition and no physical interpretation.

Depends on

Dependency tree · 2 levels

Sources