2007
DOI: 10.1103/physrevd.76.063504
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Canf(R)modified gravity theories mimic aΛCDMcosmology?

Abstract: We consider f (R) modified gravity theories in the metric variation formalism and attempt to reconstruct the function f (R) by demanding a background ΛCDM cosmology. In particular we impose the following requirements: a. A background cosmic history H(z) provided by the usual flat ΛCDM parametrization though the radiation (w ef f = 1/3), matter (w ef f = 0) and deSitter (w ef f = −1) eras. b. Matter and radiation dominate during the 'matter' and 'radiation' eras respectively i.e. Ωm = 1 when w ef f = 0 and Ωr =… Show more

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Cited by 110 publications
(89 citation statements)
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“…The corresponding classes of scalar potentials may be easily constructed (see an explicit example of such construction in the Appendix). It is interesting that in such unified model it is easier to realize the known classical universe history ( radiation/matter dominance, decceleration-acceleration transition, cosmic acceleration) than in pure F (R) gravity [7,8] or in pure scalar-GB gravity [14,15]. There is no problem to take into account usual matter in such consideration.…”
Section: Cosmic Acceleration In F (R)-scalar-gauss-bonnet Gravitymentioning
confidence: 99%
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“…The corresponding classes of scalar potentials may be easily constructed (see an explicit example of such construction in the Appendix). It is interesting that in such unified model it is easier to realize the known classical universe history ( radiation/matter dominance, decceleration-acceleration transition, cosmic acceleration) than in pure F (R) gravity [7,8] or in pure scalar-GB gravity [14,15]. There is no problem to take into account usual matter in such consideration.…”
Section: Cosmic Acceleration In F (R)-scalar-gauss-bonnet Gravitymentioning
confidence: 99%
“…As clear from (6) or (8), the expressions of V (φ) and ξ 1 (φ) depend on the explicit form of F (R), say µ in (9), and the time-development of the universe g(t), nowH 0 andH 1 , (and f (φ) in case of (6)). Then the form of F (R) is irrelevant to the WMAP data but only g(t) is relevant as long as we use the expressions in (6) or (8).…”
Section: Cosmic Acceleration In F (R)-scalar-gauss-bonnet Gravitymentioning
confidence: 99%
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“…The addition of a non-linear function of the Ricci scalar R to the Einstein-Hilbert action has been demonstrated to cause acceleration for a wide variety of f (R) functions [1,2,3,4,5,6,7,8,9,10,11,12,13,14,15,16,17,18,19,20,21,22,23,24,25,26,27,28,29,30,31,32,33,34,35,36,37,38,39,40,41,42,43,44,45,46,47,48,49,50,51,52,…”
Section: Introductionmentioning
confidence: 99%
“…It is expected that modified gravity (for a review, see [1]) approach which may be related with string/M-theory [2] may help in the understanding of the dark energy origin. For instance, various modified f (R) gravities have been constructed and applied to the description of the late-time cosmic acceleration [3,4,5,6,7,8] with also the check of local tests. Even the form of modified f (R) gravity may be reconstructed from the known universe expansion history [9].…”
mentioning
confidence: 99%