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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 (), The axiom of dependent choice: a relation in which every element is related to something admits an -indexed chain) for the absolutely continuous causal-curve calculus and the supplied causal results used below.
Let be a time-oriented smooth Lorentzian four-manifold (Smooth time-oriented Lorentzian four-manifolds: the geometric objects of the model) and let be a Cauchy set (Spacelike hypersurfaces, acausal sets, Cauchy sets, domains of dependence and Cauchy horizons clause (c)): every inextendible causal curve has of exactly one element. Then:
(a) there is no nonconstant future causal curve with ; in particular is achronal and acausal, and the three sets , , are pairwise disjoint with moreover for one has if and only if some point of chronologically precedes ;
(b) is closed in ;
(c) for every there are a chart of the kind produced by Causal cone domination in adapted charts and Lipschitz-graph bounds for causal curves clauses (a) and (d) around , with and the supplier constants and , and numbers with and such that for every the coordinate vertical line meets in exactly one point , and with and . The cylinder may be chosen inside any prescribed neighborhood of . Consequently the maps form a topological atlas on the closed set , making a topological -manifold in the subspace topology whose inclusion into is a topological embedding.
Facts & Assumptions
Given: A time-oriented smooth Lorentzian four-manifold and a Cauchy set .
is acausal, hence achronal: no two distinct points of 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)).
Every maximal geodesic with is defined on an open interval and does not converge to any point of as the parameter tends to either end; hence it is an inextendible causal curve whenever 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)).
and are open for every , and is open in (Openness of the chronological future and past, openness of the chronological relation, and closure of future and past sets clauses (a) and (b)).
Adapted chart and flat minorant: around every there are a chart with , a radius with , a constant with and on , and the flat metric with such that every -causal vector is -timelike and, whenever for , the points are chronologically related with if (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 , hence future timelike curves, and for in one has (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.
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 pieces, use tolerance 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
(No closed causal curve.) Let be a future causal curve with , nonconstant. Define the periodic extension by . On each interval the curve is the restriction of 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: is a future causal curve. It is future-inextendible: if as , then for every the sequence converges to , so for all , contradicting the nonconstancy of on ; the same argument at (using ) gives past-inextendibility. Hence is an inextendible causal curve, and by the Cauchy property has exactly one element ; but then as well, since , and . This contradiction shows that no such exists.
(A vertical line meets at most once.) Fix and the chart , constants and , and minorant of [L4]. Write . Choose , and . Then and , so . These choices can be made arbitrarily small: for any prescribed neighborhood of , first reduce so that , retaining the same adapted coordinate functions, cone constants and , and then choose as above. For the vertical line is the image of a future timelike curve [L4]; two distinct points and of with would be chronologically related, contradicting [L1]. Hence has at most one point.
(Disjointness and the decomposition.) Let . Choose a future timelike vector and let be the maximal geodesic through with ; by [L2] it is an inextendible future timelike curve, and . By the Cauchy property there is exactly one with . If , then . If and , then is a future timelike curve from a point of to , so ; if , then is a future timelike curve from to a point of , so . Hence . The sets are pairwise disjoint: if , there is with , and because forces ; this contradicts acausality [L1]. If , there are with ; if this contradicts acausality [L1], while if then transitivity of gives , that is, a closed future timelike curve through , which is excluded by step 1.1 applied to that closed curve. This proves (a), including the characterization of membership in .
(Closedness.) Let with , and suppose . Choose a maximal geodesic with future timelike as in [L2]; it is an inextendible future timelike curve and meets in exactly one point , with because . Let be the parameter of . If then is a future timelike curve from to , so ; since is open [L3] and , for all large we have , that is, with ; since for large (as ), this contradicts the acausality of [L1]. If then is a future timelike curve from to , so ; since is open [L3], for large we have , that is, with and , again contradicting acausality. Hence : is closed. This proves (b).
(A vertical line meets at least once.) With as in step 1.2, fix and put and . Both are in since . In coordinate differences from one has , and the same value for . Thus [L4] gives , so and . The vertical segment joining them is connected. If it avoided , step 2.1 would partition it into the disjoint relatively open sets and , open by [L3] and both nonempty by their endpoints. This contradicts connectedness. Hence , and step 1.2 gives exactly one intersection.
(The graphing function is Lipschitz.) For let be the -coordinate of the unique point of , so that , and by step 3.2. Since , uniqueness on gives . If with , set and suppose (the other case is symmetric); then , and both and lie in , so [L4] gives : two distinct points of chronologically related, contradicting acausality [L1]. Hence . Taking and using gives .
(Topological hypersurface.) For and its chart as above, the map , is continuous (a Lipschitz function into Euclidean space followed by the continuous chart inverse), injective and surjective onto by step 4.1, and the restriction of the continuous coordinate projection to is its inverse, because a point of lies on exactly one vertical line and has the form by step 1.2; hence is a homeomorphism onto the relatively open set . For two such graph charts the transition is continuous on its domain, so these charts form a topological atlas on ; consequently is a topological -manifold in the subspace topology and its inclusion into is a topological embedding. This proves (c) and completes the proof.
Remarks
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What is and is not proved. No smoothness of 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.
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The role of the minorant cone. The flat form is used only to produce chronological relations: to find points of 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 is turned into the inequality for .
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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
The axiom of dependent choice: a relation in which every element is related to something admits an -indexed chain
The Axiom of Countable Choice ()
Spacelike hypersurfaces, acausal sets, Cauchy sets, domains of dependence and Cauchy horizons
Convergent causal ends are extendible, maximal geodesics have no limit, and Cauchy sets are acausal
Openness of the chronological future and past, openness of the chronological relation, and closure of future and past sets
Causal cone domination in adapted charts and Lipschitz-graph bounds for causal curves
Covariant differentiation along curves: metric pairing, parallel transport and geodesic speed
The geodesic initial-value problem and the exponential map of the metric-selected connection
Observers, rest spaces and the spatial projection at an event
Causal curves, chronological and causal reachability, and inextendibility
Smooth time-oriented Lorentzian four-manifolds: the geometric objects of the model
Continuity of at a point of and on : the - condition, its agreement with at a limit point, and continuity at an isolated point
and smooth maps between smooth manifolds
Intervals of : the nine order-convex forms, nondegeneracy, and length
Dependency tree · 2 levels
Sources
- E. Minguzzi, Lorentzian causality theory, Living Reviews in Relativity 22 (2019), article 3: Cauchy sets and domains of dependence, Definitions 3.33-3.35 and the elementary properties of Cauchy sets printed pp. 93-97; Proposition 3.42 printed p. 96
- S. W. Hawking and G. F. R. Ellis, The Large Scale Structure of Space-Time, Cambridge University Press (1973): Proposition 6.5.1 and the elementary theory of Cauchy surfaces, section 6.5; achronal sets and their local structure, section 6.3