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Local freedom in the gravitational field revisited

María Jesús Pareja1 and Malcolm A H MacCallum2

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Maartens et al (1997 Class. Quantum Grav. 14 1927) gave a covariant characterization, in a (1 + 3) formalism based on a perfect fluid's velocity, of the parts of the first derivatives of the curvature tensor in general relativity which are 'locally free', i.e. not pointwise determined by the fluid energy–momentum and its derivative. The full decomposition of independent curvature derivative components given in earlier work on the spinor approach to the equivalence problem enables analogous general results to be stated for any order: the independent matter terms can also be characterized. Explicit relations between the two sets of results are obtained. The 24 Maartens et al locally free data are shown to correspond to the ∇Ψ quantities in the spinor approach, and the fluid terms are similarly related to the remaining 16 independent quantities in the first derivatives of the curvature.


PACS

04.20.-q Classical general relativity

MSC

83D05 Relativistic gravitational theories other than Einstein's, including asymmetric field theories

83C60 Spinor and twistor methods; Newman-Penrose formalism

15A72 Vector and tensor algebra, theory of invariants (See also 13A50, 14L24)

83C05 Einstein's equations (general structure, canonical formalism, Cauchy problems)

Subjects

Gravitation and cosmology

Dates

Issue 15 (7 August 2006)

Received 26 May 2006

Published 19 July 2006



  1. Local freedom in the gravitational field revisited

    María Jesús Pareja and Malcolm A H MacCallum 2006 Class. Quantum Grav. 23 5039

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