2019
DOI: 10.1007/s11005-019-01213-8
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The future is not always open

Abstract: We demonstrate the breakdown of several fundamentals of Lorentzian causality theory in low regularity. Most notably, chronological futures (defined naturally using locally Lipschitz curves) may be non-open, and may differ from the corresponding sets defined via piecewise C 1 -curves. By refining the notion of a causal bubble from [CG12], we characterize spacetimes for which such phenomena can occur, and also relate these to the possibility of deforming causal curves of positive length into timelike curves (pus… Show more

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Cited by 35 publications
(50 citation statements)
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“…The latter reaches down to C 1,1 -at least as far as convexity and causality are concerned [16,13,14,5]. However, the Lipschitz property is decisive since it prevents the most dramatic downfalls in causality theory which are known to occur for Hölder continuous metrics [9,3,30,6,17]. More specifically, in the context of the initial value problem for the geodesic equation, the Lipschitz property guarantees the existence of solutions [35] which, due to the special geometry of the models at hand, are even (globally) unique [27].…”
Section: Introductionmentioning
confidence: 99%
“…The latter reaches down to C 1,1 -at least as far as convexity and causality are concerned [16,13,14,5]. However, the Lipschitz property is decisive since it prevents the most dramatic downfalls in causality theory which are known to occur for Hölder continuous metrics [9,3,30,6,17]. More specifically, in the context of the initial value problem for the geodesic equation, the Lipschitz property guarantees the existence of solutions [35] which, due to the special geometry of the models at hand, are even (globally) unique [27].…”
Section: Introductionmentioning
confidence: 99%
“…While convexity fails below that regularity [26,43], nevertheless, most aspects of causality theory can be maintained even under Lipschitz regularity of the metric. Further below some significant changes occur [5,16], while some robust features continue to hold even in more general settings [2,15,27,35]. In particular, for C 1 -spacetimes, the push-up principle is still valid and I + (A) is open for any set A ⊆ M.…”
Section: Low Regularitymentioning
confidence: 97%
“…Hence γ is a timelike curve. Definition 2.5 Given a set S within an open neighborhood U , we define the causal future and timelike future of S within U as [9]). This is the main distinction between timelike curves and timelike almost everywhere curves.…”
Section: Proposition 24 Letmentioning
confidence: 99%