1988
DOI: 10.1088/0264-9381/5/6/002
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Do non-linear metric theories of gravitation really exist?

Abstract: Earlier results of Higgs (1959), Stelle (1978) and Whitt (1984) on the dynamical equivalence between Einstein's theory and a class of quadratic theories of gravitation are analysed in view of a more general result, implying the same conclusion for a much larger class of theories (essentially all those which depend arbitrarily on the Ricci tensor). It is shown that all previously known cases of conformal equivalence follow from the prescription of a general Legendre transform, which is in fact suggested by an e… Show more

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Cited by 69 publications
(46 citation statements)
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“…In summary, a fourth-order theory is conformally equivalent to the standard second-order Einstein theory plus a scalar field (see also [26,27]). If the theory is higher than fourth order, we have Lagrangian densities of the form [28][29][30],…”
Section: Conformal Transformations and Higher-order Gravitymentioning
confidence: 99%
See 1 more Smart Citation
“…In summary, a fourth-order theory is conformally equivalent to the standard second-order Einstein theory plus a scalar field (see also [26,27]). If the theory is higher than fourth order, we have Lagrangian densities of the form [28][29][30],…”
Section: Conformal Transformations and Higher-order Gravitymentioning
confidence: 99%
“…It is evident that the trace equation (the fourth in the system (27)), provides a differential equation with respect to the Ricci scalar which allows to solve exactly the system (27) at O(1) -order. Finally, one gets the general solution :…”
Section: A Yukawa-like Corrections In F (R)-gravitymentioning
confidence: 99%
“…Regarding the dynamical field content of the theory, the fact that quadratic corrections to the Einstein-Hilbert action introduce a massive scalar field was noted in (Buchbinder et al, 1992;Stelle, 1978Stelle, , 1977Strominger, 1984;Utiyama and DeWitt, 1962;Vilkovisky, 1992); this applies to any f (R) gravity theory in the metric formalism [see, e.g., (Ferraris et al, 1988;Hindawi et al, 1996;Olmo, 2007)]. The metric tensor contains, in principle, various degrees of freedom: spin 2 modes, and vector and scalar modes, which can all be massless or massive.…”
Section: Metric F (R) Gravitymentioning
confidence: 99%
“…Due to the Gauss-Bonnet identity, one can reduce the theory under consideration to 22 f (R, R µν R µν ) which, in general, contains a massive spin 2 ghost field in addition to the usual massless graviton and the massive scalar. f (R) theories have no ghosts (Buchbinder et al, 1992;Ferraris et al, 1988;Stelle, 1978Stelle, , 1977Strominger, 1984;Utiyama and DeWitt, 1962;Vilkovisky, 1992), and the stability condition f ′′ (R) ≥ 0 of (Dolgov and Kawasaki, 2003a;Faraoni, 2006a) essentially amounts to guarantee that the scalaron is not a ghost. Theories of the kind f (R, R µν R µν , R µνρσ R µνρσ ) in general are plagued by ghosts [this is the case, for example, of conformal gravity, as noticed long before the 1998 discovery of the cosmic acceleration (Riegert, 1984)], but models with only f R, R 2 − 4R µν R µν + R µνρσ R µνρσ terms in the action are ghost-free (Comelli, 2005;Navarro and Van Acoleyen, 2006).…”
Section: Ghost Fieldsmentioning
confidence: 99%
“…Under suitable regularity conditions on the Lagrangian and using a Legendre transformation on the metric, higher order theories take the form of GR in which one or more scalar field(s) source of the gravitational field (see, e .g., [9,[57][58][59]). On the other hand, as discussed above, the mathematical equivalence between models with variable gravitational coupling and Einstein gravity has been studied using suitable conformal transformations [60,61].…”
Section: Introductionmentioning
confidence: 99%