2005
DOI: 10.1007/s00220-005-1346-1
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Smoothness of Time Functions and the Metric Splitting of Globally Hyperbolic Spacetimes

Abstract: To Professor P.E. Ehrlich, wishing him a continued recovery and good health Abstract The folk questions in Lorentzian Geometry which concerns the smoothness of time functions and slicings by Cauchy hypersurfaces, are solved by giving simple proofs of: (a) any globally hyperbolic spacetime (M, g) admits a smooth time function T whose levels are spacelike Cauchy hyperfurfaces and, thus, also a smooth global splitting M = R × S, g = −β(T , x)dT 2 +ḡ T , (b) if a spacetime M admits a (continuous) time function t t… Show more

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Cited by 350 publications
(435 citation statements)
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“…(For background material on globally hyperbolic spacetimes the reader may consult, e.g., Hawking and Ellis [11]. The fact that the original definition of global hyperbolicity is equivalent to the existence of a foliation into smooth Cauchy surfaces was completely proven only recently by Bernal and Sánchez [12].) Then M can be written as a product of a 3-dimensional manifold S, which serves as the prototype for each Cauchy surface, and a time-axis,…”
Section: A Results From Morse Theorymentioning
confidence: 99%
See 1 more Smart Citation
“…(For background material on globally hyperbolic spacetimes the reader may consult, e.g., Hawking and Ellis [11]. The fact that the original definition of global hyperbolicity is equivalent to the existence of a foliation into smooth Cauchy surfaces was completely proven only recently by Bernal and Sánchez [12].) Then M can be written as a product of a 3-dimensional manifold S, which serves as the prototype for each Cauchy surface, and a time-axis,…”
Section: A Results From Morse Theorymentioning
confidence: 99%
“…On M + , the coordinates ϕ and ϑ range over S 2 , the coordinate t ranges over R, and the coordinate r ranges over an open interval which is diffeomorphic to R; hence M + ≃ S 2 × R 2 . From now on we will consider the spacetime (M + , g), where g denotes the restriction of the Kerr-Newman metric (8) with (10) to the domain M + given by (12). For the sake of brevity, we will refer to (M + , g) as to the exterior Kerr-Newman spacetime.…”
Section: Centrifugal and Coriolis Force In The Kerr-newman Spacementioning
confidence: 99%
“…There has been some imprecision in the literature concerning the proof of the smoothness of the splitting of globally hyperbolic spacetimes. See [27,28,29] for a survey of this question, and a complete proof of the smoothness of the splitting M ≈ S × R.…”
Section: N5 Domains Of Dependence and Geodesic Laminationsmentioning
confidence: 99%
“…There exists a global time function t on M. The level surfaces Σ t , t ∈ R, of the function t define a foliation of M, all Σ t being Cauchy surfaces and homemorphic to a given smooth 3−manifold Σ (see Geroch [25]). Geroch's theorem does not say anything about the regularity of the leaves Σ t ; the time function is only proved to be continuous and they are thus simply understood as topological submanifolds of M. A regularization procedure for the time function can be found in [8], [9]. In the concrete cases which we consider in this paper the time function is smooth and all the leaves are diffeomorphic to Σ.…”
Section: Spin Structuresmentioning
confidence: 99%