Radiative gravitational fields in general relativity II. Asymptotic behaviour at future null infinity

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Abstract

We prove that Penrose’s requirements for asymptotic simplicity are formally satisfied by the general metric, (1), which admits both post-Minkowskian and multipolar expansions, (2), which is stationary in the past and asymptotically Minkowskian in the past, (3), which admits harmonic coordinates, and (4), which is a solution of Einstein’s vacuum equations outside a spatially bounded region. The proof is based on the setting up, by using the method of a previous work (L. Blanchet & T. Damour ( Phil . Trans . R . Soc . Lond . A 320, 379-430 (1986))), of an improved algorithm that generates a metric equivalent to the general harmonic metric of that work but written in radiative coordinates, i. e. admitting an expansion in powers of r -1 for r → ∞ and t - r fixed. The arbitrary parameters of the construction are the radiative multipole moments in the sense of K. S. Thorne ( Rev . mod . Phys . 52, 299 (1980)).

Publisher

The Royal Society

Subject

Pharmacology (medical)

Reference34 articles.

1. Anderson J. L. 1979 In Isolated gravitating systems in general relativity (ed. J. Ehlers). Amsterdam: North Holland.

2. Ashtekar A. 1984 In General relativity and gravitation ( et al.). Dordrecht: Reidel.

3. J. math;Bardeen J. M.;Phys.,1973

4. Blanchet L. 1986 In Recent developments of general relativity Proceedings of the Fourth Marcel Grossmann Meeting (ed. R. Ruffini). Amsterdam: North Holland.

5. Radiative gravitational fields in general relativity I. General structure of the field outside the source

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