2017
DOI: 10.1140/epjc/s10052-017-4682-3
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General scalar–tensor cosmology: analytical solutions via noether symmetry

Abstract: We analyze the cosmology of a general scalartensor theory which encompasses generalized Brans-Dicke theory, Gauss-Bonnet gravity, non-minimal derivative gravity, generalized Galilean gravity and also the general kessence type models. Instead of taking into account phenomenological considerations we adopt a Noether symmetry approach, as a physical criterion, to single out the form of undetermined functions in the action. These specified functions symmetrize equations of motion in the simplest possible form whic… Show more

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Cited by 8 publications
(8 citation statements)
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“…Such probes include weak lensing [21][22][23][24][25][26] and redshift space distortion observations [16,[27][28][29][30][31]. A simple way to account for this tension is to allow [27] for the possibility of extensions of GR in the form of modified theories of gravity [32][33][34][35][36][37][38][39][40][41][42][43][44]. RSD measurements in galaxy redshift surveys [46][47][48][49][50] measure the peculiar velocities of matter and thus infer [51] the growth rate of cosmological perturbations on a range of redshifts and scales.…”
Section: Introductionmentioning
confidence: 99%
“…Such probes include weak lensing [21][22][23][24][25][26] and redshift space distortion observations [16,[27][28][29][30][31]. A simple way to account for this tension is to allow [27] for the possibility of extensions of GR in the form of modified theories of gravity [32][33][34][35][36][37][38][39][40][41][42][43][44]. RSD measurements in galaxy redshift surveys [46][47][48][49][50] measure the peculiar velocities of matter and thus infer [51] the growth rate of cosmological perturbations on a range of redshifts and scales.…”
Section: Introductionmentioning
confidence: 99%
“…was provided. Likewise, Massaeli et al [90] found exact solutions by taking ceratin assumptions in Horndeski theory and explored the possible constraints on free parameters using effective EoS parameter only which turned out as a constant quantity in each case. In [72], Capozziello et.…”
Section: Discussionmentioning
confidence: 99%
“…where the left-hand equation is for the cosh-like potential, while the right-hand one is for the sinh-like potential. Since at the GR-de Sitter point: x = ξ = 0, then, from the above equations it follows that this critical point exists for the cosh and sinh-like potentials only if kµ = 1, in which case the mentioned potentials (183) asymptotically approach to the exponential as ϕ → ∞:…”
Section: (Non)emergence Of the λCdm Phase From The Brans-dicke Cosmologymentioning
confidence: 99%
“…Scalar-tensor theories of gravity 41,64,65,[175][176][177][178][179][180][181][182][183][184][185][186][187] are a generalization of the Brans-Dicke theory to allow the BD coupling to be a function of the scalar field: ω BD → ω(φ), i. e., to be a varying parameter:…”
Section: Scalar-tensor Theoriesmentioning
confidence: 99%