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Penrose null geodesic incompleteness

Physical scope

A conditional Lorentzian-geometric theorem. The null Ricci inequality is assumed directly; no Einstein equation, matter-energy condition, event horizon, curvature blow-up, or singular point in the manifold is concluded.

Statement

Assume the Axiom of Choice. Let (M,g,N) be a smooth time-oriented Lorentzian four-manifold of signature (−,+,+,+) that is globally hyperbolic (strongly causal with compact causal diamonds). Let Σ⊂M be a connected noncompact smooth spacelike Cauchy hypersurface, meaning that every inextendible causal curve meets Σ exactly once. Let S⊂M be a nonempty compact smooth spacelike two-surface on which both future null expansions are negative for the two local future null normal rays. Assume directly that Ric⁡p(v,v)≥0 for every point p∈M and every null vector v∈TpM. Then (M,g,N) is future null geodesically incomplete: at least one maximal future-directed affinely parametrized null geodesic has an affine parameter interval with finite upper endpoint. This conclusion asserts no curvature divergence or singular point belonging to M.

Statement references

Facts & Assumptions

Given: Axiom of Choice; a globally hyperbolic time-oriented smooth Lorentzian four-manifold; a connected noncompact smooth spacelike Cauchy hypersurface Σ; a compact future trapped surface S; and the pointwise null Ricci inequality.

[A1]

The Axiom of Choice: AC is the assertion that every family of nonempty sets has a choice function.

[F1]

AC implies DC implies countable choice: in ZF, AC⇒DC⇒ACω, so the Countable Choice and Dependent Choice hypotheses of the causal suppliers follow from [A1].

[F2]

Existence of a positive smooth volume density of total mass one on a smooth Lorentzian four-manifold, The Geroch volume function: a continuous strictly increasing time function whose levels are Cauchy sets, and Smooth Cauchy temporal splitting: a global temporal function with Cauchy levels and an orthogonal complete flow: under Countable Choice and Dependent Choice, a nonempty time-oriented smooth Lorentzian four-manifold has a normalized smooth volume measure; global hyperbolicity and that measure give the volume time input required by the splitting theorem; the latter then gives a smooth temporal function T with Cauchy levels and a complete future timelike flow diffeomorphism Ψ:R×S0→M satisfying T(Ψ(s,z))=s.

[F3]

A complete temporal flow identifies smooth Cauchy slices: for this complete timelike product flow, projection along its flow lines identifies any smooth spacelike Cauchy hypersurface Σ diffeomorphically with the slice S0. Thus S0 is connected and noncompact.

[F4]

Compactness of the future horismos under null completeness: under the stated trapped-surface, null Ricci, global-hyperbolicity, and future-null-completeness assumptions, E+(S)=∂I+(S) is a compact topological three-manifold without boundary.

[F5]

Achronal boundaries are locally Lipschitz graphs, topological hypersurfaces and null for smooth volume densities: the boundary of an open future set is achronal; in particular no two distinct points of E+(S)=∂I+(S) are chronologically related.

[F6]

Temporal functions are time functions, and time functions forbid closed causal curves: a temporal function strictly increases along every nonconstant future causal curve, hence along every future timelike curve.

[F7]

Invariance of domain: assuming AC, a continuous injective map between open subsets of R3 has open image; applying this in charts makes a continuous injective map between topological three-manifolds an open map.

[F10]

Future null geodesic completeness and incompleteness: future null geodesic incompleteness means the existence of a maximal future null affine interval with finite upper endpoint.

[A2]

The inequality Ric⁡(v,v)≥0 for null v is a direct mathematical premise. It is not derived from a matter model, energy condition, or Einstein equation.

Proof

technique · contradiction

Given: [A1]–[A2] and [F1]–[F10]. Assume, for contradiction, that every future-directed null geodesic is future complete.

1.1A1F1assume-contragiven

Assume for contradiction that every future-directed null geodesic is future complete. By [F1], Countable Choice and Dependent Choice hold under the assumed Axiom of Choice, so the hypotheses of the volume-time, Cauchy-splitting and causal-boundary suppliers are satisfied.

2.1F2step 1.1given

Apply [F2] to obtain a volume time input, a temporal function T, a smooth Cauchy slice S0=T−1(0), and a complete timelike product flow Ψ. The splitting satisfies T(Ψ(s,z))=s. Hence T tends to +∞ and −∞ along the two ends of every orbit; continuity prevents an endpoint in M, so each orbit is an inextendible timelike curve.

3.1F3step 2.1given

Apply [F3] to identify the given hypersurface Σ diffeomorphically with S0 by projection along these flow lines. Therefore S0 is connected and noncompact.

3.2F2F4F6F8step 2.1givencontradiction

The restriction T∣S is continuous and S is nonempty compact, so [F8] gives a point s0∈S at which T∣S is minimal. If s0∈I+(S), some s1∈S satisfies s1≪s0; since T is temporal, [F6] gives T(s1)<T(s0), contradicting minimality. Thus s0∉I+(S). As s0∈S⊆J+(S) by reflexivity, s0∈E+(S), so this boundary is nonempty.

3.3F2F5step 2.1givenconstruct

Define π:M→S0 by π(Ψ(s,z))=z. This is continuous because Ψ−1 is smooth. If x,y∈E+(S) have π(x)=π(y) and x≠y, their flow coordinates differ, so the timelike orbit between them makes them chronologically related. This contradicts the achronality in [F5]. Hence π∣E+(S) is injective.

4.1F2F4F7step 3.3construct

The domain E+(S) is a topological three-manifold without boundary by [F4], and S0 is a smooth three-manifold by [F2]. For each x∈E+(S), choose manifold charts about x and π(x) and shrink the source chart so its image lies in the target chart. In these coordinates π is continuous and injective between open subsets of R3; [F7] makes its image open. Taking the union over x shows π(E+(S)) is open in S0.

4.2F2F4F8F9step 3.3

By [F4], E+(S) is compact, and π is continuous, so [F8] makes π(E+(S)) compact. The smooth manifold S0 is Hausdorff; [F9] therefore makes this image closed in S0.

5.1F9F10step 3.1step 3.2step 4.1step 4.2contradictiondischarge-contradiction∎

The image π(E+(S)) is nonempty by step 3.2 and both open and closed by steps 4.1 and 4.2. Since S0 is connected by step 3.1, [F9] implies π(E+(S))=S0. But π(E+(S)) is compact by step 4.2, which would make S0 compact, contradicting step 3.1. Thus the assumed future null completeness is false. By [F10], at least one maximal future-directed null geodesic has finite upper affine endpoint, which is the asserted conclusion.

Remarks

The null Ricci condition is a geometric hypothesis in the library curvature convention; it is not silently replaced by an Einstein equation or a matter energy condition. The conclusion is affine incompleteness only. It neither identifies an incomplete endpoint inside M nor asserts curvature blow-up, cosmic censorship, or the existence of an event horizon. A trapped surface is not itself an event horizon; that comparison requires separate asymptotic and global hypotheses.

Depends on

Dependency tree · 2 levels

Sources