1999
DOI: 10.1103/physrevd.59.124015
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Asymptotic and exact solutions of perfect-fluid scalar-tensor cosmologies

Abstract: We present a method which enables exact solutions to be found for flat homogeneous and isotropic scalar-tensor cosmologies with an arbitrary ω(Φ) function and satisfying the general perfect fluid state equationThis method has been used to analyze a wide range of asymptotic analytical solutions at early and late times for different epochs in the cosmic history:false vacuum inflationary models, vacuum and radiation-dominated models, and matter-dominated models. We also describe the qualitative behavior of models… Show more

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Cited by 14 publications
(16 citation statements)
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“…Exact solutions with κ = 0 have been found to Eqs. ( 134) and (135) in [94,1004,108,942], and vacuum and radiation dominated solutions for arbitrary spatial curvature have been found in [95,899,111]. Some of the methods used in these papers are extended to anisotropic cosmologies in [898], and the asymptotics of FLRW cosmologies in scalar-tensor theories have been studied in [112,1125].…”
Section: General Scalar-tensor Theoriesmentioning
confidence: 99%
“…Exact solutions with κ = 0 have been found to Eqs. ( 134) and (135) in [94,1004,108,942], and vacuum and radiation dominated solutions for arbitrary spatial curvature have been found in [95,899,111]. Some of the methods used in these papers are extended to anisotropic cosmologies in [898], and the asymptotics of FLRW cosmologies in scalar-tensor theories have been studied in [112,1125].…”
Section: General Scalar-tensor Theoriesmentioning
confidence: 99%
“…This has indeed attracted a lot of interest recently and such cosmological models have been studied and possibly confronted with observations like CMB anisotropies, or the growth of energy density perturbations (see for instance [25,26,27,28,29,30,31,32,33,34,35]). However, we emphasize once more that the central point of view adopted here, in analogy with Starobinsky [14], is to constrain the model with the experimental knowledge of the Hubble diagram up to z ∼ (1 − 2).…”
Section: Introductionmentioning
confidence: 99%
“…In the so-called Jordan frame and Brans-Dicke like parametrization STG form a collection of theories which contain two functional degrees of freedom, a coupling function ω(Ψ) and a scalar potential V (Ψ). As has been discussed by many authors previously [7,8,9,10,11,12,13,14,15,16], for a range of choices of ω and V the cosmological evolution of dust and potential dominated STG models naturally converges close to the one expected from GR. On the other hand, cosmological observations and data from the local weak field tests permit to suppose that only these STG models are viable which involve this property.…”
Section: Introductionmentioning
confidence: 52%
“…Note that a necessary condition for crossing the so-called phantom divide, w eff = −1, is vanishing of the second term in Eq. (14). Depending on the model, exponential solutions may cross the phantom divide line at most twice before approaching w eff = −1 from either above or below.…”
Section: Potential Dominated Regimementioning
confidence: 99%