2014
DOI: 10.1007/s00023-014-0371-z
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Smoothness of Compact Horizons

Abstract: Abstract. We prove that compact Cauchy horizons in a smooth spacetime satisfying the null energy condition are smooth. As an application, we consider the problem of determining when a cobordism admits Lorentzian metrics with certain properties. In particular, we prove a result originally due to Tipler without the smoothness hypothesis necessary in the original proof.

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Cited by 13 publications
(9 citation statements)
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“…14, was posted on the Archive (arXiv: 1406.5919) as the last of a series of three papers (the others being [58,59]). The very next day a related work by E. Larsson (arXiv:1406.6194 recently published in [54]), reaching similar conclusions on smoothness of Cauchy horizons and topology change, was also posted ( [54] mentions that it also appeared some days before on a public web repository of theses of the KTH Institute, Stockholm). This work and Larsson's follow quite different lines of proof.…”
Section: Acknowledgmentsmentioning
confidence: 93%
“…14, was posted on the Archive (arXiv: 1406.5919) as the last of a series of three papers (the others being [58,59]). The very next day a related work by E. Larsson (arXiv:1406.6194 recently published in [54]), reaching similar conclusions on smoothness of Cauchy horizons and topology change, was also posted ( [54] mentions that it also appeared some days before on a public web repository of theses of the KTH Institute, Stockholm). This work and Larsson's follow quite different lines of proof.…”
Section: Acknowledgmentsmentioning
confidence: 93%
“…Some specific or technical topics of causality theory have not been discussed in this review. I give a list here pointing the reader to some literature -Chronology violation (time machines) and topology change (Geroch 1967;Tipler 1974Tipler , 1977Yodzis 1972Yodzis , 1973Galloway 1983bGalloway , 1995Kriele 1989;Hawking 1992;Ori 1993Ori , 2007Borde 1997Borde , 2004Krasnikov 1995Krasnikov , 2002Minguzzi 2015aMinguzzi , 2016aLarsson 2015;Lesourd 2018). -Spacetime boundaries (Penrose 1964(Penrose , 1965cSchmidt 1971a, b;Geroch et al 1972;Sachs 1973;Budic and Sachs 1974;Geroch 1977a;Szabados 1987Szabados , 1988Rácz 1987Rácz , 1988; Liang 1988, 1992;Scott and Szekeres 1994;Harris 1998Harris , 2000Harris , 2004Harris , 2017Marolf and Ross 2003;García-Parrado and Senovilla 2005;Low 2006;Flores 2007;Flores and Sánchez 2008;Flores and Harris 2007;Sánchez 2009;…”
Section: History and Peculiarities Of Causality Theorymentioning
confidence: 99%
“…M \ C = I ∪ H, where H is a maximal globally hyperbolic spacetime with a compact and boundaryless Cauchy surface Σ. In this context C is a smooth [6], [8], [9], and totally geodesic null hypersurface, hence ruled by inextensible null geodesics called the null generators. We say that C is non-degenerate if there is at least one future or past incomplete generator (i.e.…”
Section: Introductionmentioning
confidence: 99%