1960
DOI: 10.1103/physrevlett.4.431
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Spherical Gravitational Waves

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Cited by 214 publications
(245 citation statements)
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“…The last equation in (17) can be put into the form d dl (ln A) = −Θ, where l is the affine parameter, and Θ = 1 2 k µ ;µ is the expansion of the null congruence. This determines the behaviour of the amplitude A in the above spacetimes (22), (31), (43). The remaining equations (17) enables one to deduce the polarization tensors.…”
Section: Discussionmentioning
confidence: 99%
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“…The last equation in (17) can be put into the form d dl (ln A) = −Θ, where l is the affine parameter, and Θ = 1 2 k µ ;µ is the expansion of the null congruence. This determines the behaviour of the amplitude A in the above spacetimes (22), (31), (43). The remaining equations (17) enables one to deduce the polarization tensors.…”
Section: Discussionmentioning
confidence: 99%
“…The metric (generally of the Petrov type II) in the standard coordinates has the form, see e.g. [22,23,28,39],…”
Section: Expanding Wavesmentioning
confidence: 99%
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“…This is the conventional peeling behavior when compared with models of vacuum gravitational fields due to isolated gravitating systems in general (cf. [4]- [8] and (2.20)-(2.24) below). The purpose of the present paper is to explain the unconventional peeling behavior described above by putting it in the context of light-like signals emitted by a general class of isolated gravitating systems.…”
Section: Introductionmentioning
confidence: 99%