2020
DOI: 10.1088/1361-6382/abbc43
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Brans–Dicke cosmology with a Λ-term: a possible solution to ΛCDM tensions*

Abstract: We present a full-fledged analysis of Brans–Dicke cosmology with a cosmological constant and cold dark matter (BD-ΛCDM for short). We extend the scenarios where the current cosmological value of the BD-field is restricted by the local astrophysical domain to scenarios where that value is fixed only by the cosmological observations, which should be more natural in view of the possible existence of local screening mechanism. Our analysis includes both the background and perturbations equations in different gauge… Show more

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Cited by 89 publications
(162 citation statements)
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References 364 publications
(788 reference statements)
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“…The aim of the work is to find a cosmological scenario of the model in BD theory with varying cosmological term which would be capable to link the dynamics of the early Universe with that of our late Universe. This work extends the successful approach recently presented on BD cosmology with a rigid cosmological term [61,62], and reinforces the idea that dynamical models of the vacuum energy can be very helpful to improve the fit to cosmological and cosmographical observations [63][64][65][66][67]. In particular, they help alleviating the so-called H 0 and σ 8 tensions [68][69][70][71], see e.g.…”
Section: Introductionsupporting
confidence: 82%
“…The aim of the work is to find a cosmological scenario of the model in BD theory with varying cosmological term which would be capable to link the dynamics of the early Universe with that of our late Universe. This work extends the successful approach recently presented on BD cosmology with a rigid cosmological term [61,62], and reinforces the idea that dynamical models of the vacuum energy can be very helpful to improve the fit to cosmological and cosmographical observations [63][64][65][66][67]. In particular, they help alleviating the so-called H 0 and σ 8 tensions [68][69][70][71], see e.g.…”
Section: Introductionsupporting
confidence: 82%
“…cosmological observations (and in alleviating the tensions afflicting the latter) provided the effective value of ν eff is positive and of order ν eff = O(10 −3 ) > 0 [22][23][24][25][26][27][28][29]31,32]. Amazingly, this value is also of the order of the predicted one in (92).…”
Section: String-inspired-rvm Evolution In the Presence Of Stiff Mattermentioning
confidence: 97%
“…Let us, however, note that one may also obtain an effective RVM evolution in a Brans-Dicke (BD) context with a cosmological constant, hence within a gravity paradigm different from GR. It turns out that in this latter form (in which there is an evolution of the effective gravitational coupling as well) the RVM is particularly efficient in solving the main tensions, above all the one associated with the local value of the Hubble parameter, H 0 [31,32]. In either framework (GR or BD), the dynamical vacuum energy density associated with the RVM is based on the following general renormalisation-group (RG)-like form of the vacuum energy density in terms of powers of the Hubble parameter H(t) =ȧ/a, which is a function of the cosmic time t, and its cosmic-time derivativeḢ [12][13][14][15]: (1) where the coefficients A i , B i are dimensionless, whereas the C i ones and higher are dimensionful.…”
Section: General Structure Of the Rvm And Its Connection To The Renormalisation Group In Curved Spacetimementioning
confidence: 99%
“…The former ones, however, seem to be preferred over since reduce the value of the comoving size of the sound horizon at baryon drag r s , without spoiling the fit to CMB and BAO data [30][31][32]. Two well studied frameworks to modify the early time dynamics of the Universe and inject the required energy into the cosmic fluid to lower r s with respect to the ΛCDM one are modified gravity (MG) [33][34][35][36][37][38][39][40][41][42][43][44][45] and early dark energy (EDE) models [46][47][48][49][50][51][52][53][54][55][56][57][58][59][60][61][62][63]. 1 In this paper, we extend the model with a scalar field on-minimally coupled to the Ricci scalar of the form FðσÞ ¼ M 2 pl þ ξσ 2 in presence of a cosmological constant Λ [41,42], by providing it with a small effective mass.…”
Section: Introductionmentioning
confidence: 99%