1986
DOI: 10.1007/bf01205488
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On the existence ofn-geodesically complete or future complete solutions of Einstein's field equations with smooth asymptotic structure

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Cited by 475 publications
(626 citation statements)
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“…Up to questions of extensibility, all such solutions which are smooth have been characterized here by initial data on a space-like hypersurface and boundary data on 2-. As has been recognized before in the case of a negative cosmological constant [5,7], it is seen now that the concept of asymptotic simplicity is natural for Einstein's field equations also in the case of a positive cosmological constant.…”
Section: With Positive Cosmological Constant )~ Which Has Conformal Ementioning
confidence: 71%
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“…Up to questions of extensibility, all such solutions which are smooth have been characterized here by initial data on a space-like hypersurface and boundary data on 2-. As has been recognized before in the case of a negative cosmological constant [5,7], it is seen now that the concept of asymptotic simplicity is natural for Einstein's field equations also in the case of a positive cosmological constant.…”
Section: With Positive Cosmological Constant )~ Which Has Conformal Ementioning
confidence: 71%
“…In a suitable representation the equations for the rescaled metric retain their hyperbolicity even under conformal rescalings with conformal factors which vanish on subsets of space-time. The consequences of this property for the longtime behaviour of gravitational fields have been worked out in detail for de Sitter-type space-times [5,7], i.e. for solutions to Einstein's field equations…”
Section: Introductionmentioning
confidence: 99%
“…Hence, the respective cone is Minkowski. This implies in particular that the solution g ij = δ ij in (3.20) is also Minkowski and the direct transformation of coordinates is given by: 25) such that:…”
Section: Ricci-flat Asymptoticsmentioning
confidence: 99%
“…26 The holographic Ward identities for the 24 Here and in equation (4.28) we have performed the intermedium step: δS/δq AB = (z/β) 2 δS/δq AB , where:qAB := (z/β) 2 qAB, and performed the decomposition of δ/δq AB in the same way as in (4.23)-(4.25). 25 Notice that the term QAB as well as: ∂Cn/∂q AB and: (4.21) are purely spatial and therefore vanish when contracted with n A . The expression for E follows from an explicit computation of (4.28) for each value of d and has been verified up to d = 6.…”
Section: Holographic Stress Tensorsmentioning
confidence: 99%
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