2020
DOI: 10.1007/s10714-020-02690-2
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Cosmological perfect fluids in higher-order gravity

Abstract: We prove that in Robertson-Walker space-times (and in generalized Robertson-Walker spacetimes of dimension greater than 3 with divergence-free Weyl tensor) all higher-order gravitational corrections of the Hilbert-Einstein Lagrangian density F (R, R, ..., k R) have the form of perfect fluids in the field equations. This statement definitively allows to deal with dark energy fluids as curvature effects.PACS numbers: 98.80.-k, 95.35.+d, 95.36.+x

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Cited by 48 publications
(36 citation statements)
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“…first increasing and then decreasing). In a nutshell, without assuming m = 1 , four types of well-known potentials were obtained (Note that µ > 0 ): for all cases of study, then according to [83]…”
Section: Discussionmentioning
confidence: 99%
“…first increasing and then decreasing). In a nutshell, without assuming m = 1 , four types of well-known potentials were obtained (Note that µ > 0 ): for all cases of study, then according to [83]…”
Section: Discussionmentioning
confidence: 99%
“…We consider the mini superspace defined by the dynamic variables {a, φ}. A point-like Lagrangian in the mini superspace of the for field equations (114) and (115) is…”
Section: Scalar-field Cosmologymentioning
confidence: 99%
“…Application of the previous analysis gives the following classification of Noether symmetries of the model for various forms of the effective potential [120] • For arbitrary potential V ef f (x, y), Lagrangian (120) admits the Noether point symmetry ∂ t with first integral the constraint equation (113).…”
Section: Scalar-field Cosmologymentioning
confidence: 99%
“…which allows generalized derivative couplings of H with gravity. The couplings ς and θ in (3.22) were first studied in [31,32]. So far, the Higgs potential V (H) in (3.21) is unidentified.…”
Section: Second Approach: Extended Brans-dicke Modelmentioning
confidence: 99%