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Strong causality bounds the auxiliary length of causal curves contained in a compact set
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 general absolutely continuous curve calculus and its fundamental theorem. Use the locally absolutely continuous Riemannian length of The auxiliary Riemannian metric h=g+2n-flat tensor n-flat is complete after a proper-exhaustion conformal factor, and its closed bounded sets are compact. Let be a strongly causal time-oriented smooth Lorentzian four-manifold (Chronology, causality, strong causality, global hyperbolicity and time functions clause (b)) and let be a smooth positive definite metric on (Smooth covariant 2-tensor fields on a smooth manifold). Then for every compact set there is such that for every future causal curve (Causal curves, chronological and causal reachability, and inextendibility) with .
Consequently, if is parametrized by -arclength () and its image is contained in the compact set , then .
Facts & Assumptions
Given: Countable Choice, Dependent Choice, a strongly causal spacetime, a smooth positive definite metric , a compact set and a future causal curve .
Strong causality: for every and every open there is an open with such that for every future causal curve and all with one has (Chronology, causality, strong causality, global hyperbolicity and time functions clause (b)).
The pointwise adapted cone chart has and for every nonzero future causal vector (Causal cone domination in adapted charts and Lipschitz-graph bounds for causal curves clauses (a) and (b)). On a closed coordinate ball compactly contained in this chart, smooth positive definite has a finite Euclidean operator-norm bound , so . Its coordinate time range is finite. No boundedness on an unshrunk chart is assumed.
Continuous images of compact sets are compact, and compact subsets of a Hausdorff space are closed; a compact set has a finite subcover from every open cover (Open cover, subcover, and compact topological space; a compact subset is a subspace that is compact in its own right).
Absolutely continuous calculus: under the Riemannian length definition of The auxiliary Riemannian metric h=g+2n-flat tensor n-flat is complete after a proper-exhaustion conformal factor, and its closed bounded sets are compact, the density is nonnegative and integrable, and its integral is additive and monotone over intervals (Absolute continuity on a compact interval, Absolutely continuous functions have integrable derivatives, Fundamental theorem of calculus for absolutely continuous functions).
Proof
(A finite precompact causally convex cover.) For each point of , choose an adapted chart and a closed coordinate ball compactly contained in it. Use its open half-radius ball as the neighborhood in strong causality [L1], obtaining a causally convex open around the point contained in that smaller ball. The collection of all such admissible , charts and radii covers ; compactness selects finitely many members, with no choice of a family indexed by all points of . Write them for , with their open coordinate balls and compactly contained in their respective larger charts. Define , , and . Then [L2] gives almost everywhere on every subarc in . If is empty the conclusion is immediate with ; henceforth use the finite cover for nonempty .
(The visit of a causal curve to one causally convex set is one interval.) Let be future causal and fix . If with , then by the defining property of ; hence the parameter set is an interval in : whenever it contains it contains . In particular has at most one connected component and is an interval , possibly empty.
(Length over a compact part of one visit.) For every compact nondegenerate , the curve image lies in , so the fundamental theorem in [L4] and step 1.1 give . The restricted speed is integrable, since the coordinate derivatives are integrable and dominate it. The relatively open visit need not contain its endpoints; only compact subintervals contained in are used in this argument.
(Finite compact-interval cover and length sum.) The relatively open intervals form a finite cover of the compact parameter interval . A sufficiently fine finite partition has each of its closed subintervals contained in some , by a Lebesgue number of this cover. Assign each partition piece to the least such ; this requires only finitely many choices. For every index used, let be the closed interval from the least left endpoint to the greatest right endpoint of its assigned pieces. As is an interval, ; these finitely many compact intervals cover . Step 3.1 applies on each . The nonnegative integral over their union is at most the sum of their integrals, so the global speed is integrable and , with unused indices contributing no interval. If the length is zero. For an arclength-parametrized curve , giving the second assertion. No possibly missing visit endpoint is evaluated.
(Imprisonment form.) There is no sequence of future causal curves with images in a fixed compact and auxiliary lengths tending to infinity: each length is bounded by the same from step 4.1. Equivalently, there is no family of -arclength-parametrized future causal curves with images in and parameter-domain lengths tending to infinity.
(Conclusion.) The finite causally convex cover, the interval visit estimate and the nonnegative integral bound establish both assertions, with exactly the declared calculus premises.
Remarks
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Strong causality is used only through a finite causally convex cover. No compactness of causal diamonds, no time function and no completeness are used; the metric enters only through the local bound of [L2].
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Sharpness. The conclusion fails without strong causality: on the flat cylinder a closed causal loop contained in a compact set can be traversed with arbitrarily large auxiliary length.
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Instance. The auxiliary metric of The auxiliary Riemannian metric h=g+2n-flat tensor n-flat is complete after a proper-exhaustion conformal factor, and its closed bounded sets are compact is a smooth positive definite metric to which the bound applies; the constant then depends on the choice of .
Depends on
The Axiom of Countable Choice ()
The axiom of dependent choice: a relation in which every element is related to something admits an -indexed chain
Chronology, causality, strong causality, global hyperbolicity and time functions
Causal cone domination in adapted charts and Lipschitz-graph bounds for causal curves
Causal curves, chronological and causal reachability, and inextendibility
Chart independence, concatenation, reparametrization and transitivity for causal curves
The auxiliary Riemannian metric h=g+2n-flat tensor n-flat is complete after a proper-exhaustion conformal factor, and its closed bounded sets are compact
Smooth time-oriented Lorentzian four-manifolds: the geometric objects of the model
Smooth covariant 2-tensor fields on a smooth manifold
Absolute continuity on a compact interval
Absolutely continuous functions have integrable derivatives
Fundamental theorem of calculus for absolutely continuous functions
Continuity of at a point of and on : the - condition, its agreement with at a limit point, and continuity at an isolated point
Intervals of : the nine order-convex forms, nondegeneracy, and length
and smooth maps between smooth manifolds
Open cover, subcover, and compact topological space; a compact subset is a subspace that is compact in its own right
Dependency tree · 2 levels
Sources
- E. Minguzzi, Lorentzian causality theory, Living Reviews in Relativity 22 (2019), article 3: Theorem 2.80 (a strongly causal spacetime is non-partially imprisoning) with proof, printed p. 58, and Theorem 1.35/Definition 1.34 on strong causality, printed p. 24
- S. W. Hawking and G. F. R. Ellis, The Large Scale Structure of Space-Time, Cambridge University Press (1973): strong causality and the finite number of causally convex neighbourhoods met by a causal curve, section 6.2