2022
DOI: 10.1088/1361-6382/ac387e
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Asymptotic structure with vanishing cosmological constant

Abstract: This is the first of two papers [1] devoted to the asymptotic structure of space-time in the presence of a non-negative cosmological constant Λ. This first paper is concerned with the case of Λ = 0. Our approach is fully based on the tidal nature of the gravitational field and therefore on the ‘tidal energies’ built with the Weyl curvature. In particular, we use the (radiant) asymptotic supermomenta computed from the rescaled Weyl tensor at infinity to provide a novel characterisation of radiation escaping fro… Show more

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Cited by 7 publications
(28 citation statements)
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References 47 publications
(113 reference statements)
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“…Though this is not necessary, in order to concorde with references [29,28,32,31] I am going to partly fix this gauge freedom by choosing Ω such that ∇ µ ∇ µ Ω J = 0, which in turn implies…”
Section: Weakly Asymptotically Simple Spacetimesmentioning
confidence: 99%
See 4 more Smart Citations
“…Though this is not necessary, in order to concorde with references [29,28,32,31] I am going to partly fix this gauge freedom by choosing Ω such that ∇ µ ∇ µ Ω J = 0, which in turn implies…”
Section: Weakly Asymptotically Simple Spacetimesmentioning
confidence: 99%
“…Hence, the existence of gravitational radiation carrying energy-momentum -lost by isolated systems in their dynamical evolutionshould be amenable to a description that considers the strength of the curvature, that is, the strength of the tidal gravitational effects, as the fundamental variable. This is the basic idea to be developed in what follows which was put forward and developed in detail in [29,28,32,31]. The strength 2 of the tidal gravitational forces can be appropriately described by the Bel-Robinson tensor (see Appendix A), defined by…”
Section: Asymptotic (Radiant) Super-momentum: the Radiation Criterionmentioning
confidence: 99%
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