Can varying the gravitational constant alleviate the tensions ?
Ziad Sakr,
Domenico Sapone
Abstract:Constraints on the cosmological concordance model parameters from observables at different redshifts are usually obtained using the locally measured value of the gravitational constant G N . Here we relax this assumption, by considering G as a free parameter, either constant over the redshift range or dynamical but limited to differ from fiducial value only above a certain redshift. Using CMB data and distance measurements from galaxy clustering BAO feature, we constrain the cosmological parameters, along with… Show more
“…While this clearly happens for the (w 0 , w a ) parametrisations in section 2, DE EFTs, even those that permit w DE < −1, are evidently more rigid, and as we have seen, the scope is limited, at least within our assumptions. In that sense, our analysis agrees with [67,74] that a varying Newton's constant may be a viable approach to alleviating H 0 tension, but this window can be expected to be severely restricted as observational constraints improve.…”
Section: Classsupporting
confidence: 84%
“…For this reason, one would expect increases in H 0 due to linear evolution of F(φ) with cosmic time to be marginal, and this is indeed what we found. Even though the outlook may not be good [67,74], at a technical level it is imperative to identify models that increase H 0 without relying heavily on a local H 0 prior, e. g. [72,73]. Finally, we note that increasing H 0 requires Ḟ > 0 (F 1 < 0), which implies the Newton's constant must decrease in the late universe in line with the findings of Ref.…”
Section: Discussionsupporting
confidence: 71%
“…On the minimal assumption that the coupling G 4 (φ) evolves linearly with cosmic time, while employing model agnostic techniques for the Quintessence sector, G 2 (φ, X) = X − V(φ), we show in section 3 that any increase in H 0 is expected to be negligible. In other words, despite ongoing debate about whether non-minimal couplings can alleviate H 0 tension [71][72][73], in line with [67,74], we find that a non-minimal coupling can only marginally alleviate H 0 tension, at least within reasonable assumptions. Concretely, we observe that the class of models largely fails to penetrate into the phantom regime w DE < −1 at z = 0, so it is consistent with our (w 0 , w a ) expectations.…”
Local H 0 determinations currently fall in a window between H 0 ∼ 70 km/s/Mpc (TRGB) and H 0 ∼ 76 km/s/Mpc (Tully-Fisher). In contrast, BAO data calibrated in an early ΛCDM universe are largely consistent with Planck-ΛCDM, H 0 ∼ 67.5 km/s/Mpc. Employing a generic two parameter family of evolving equations of state (EoS) for dark energy (DE) w DE (z) and mock BAO data, we demonstrate that if i) w DE (z = 0) < −1 and ii) integrated DE density less than ΛCDM, then H 0 increases. EoS that violate these conditions at best lead to modest H 0 increases within 1σ. Tellingly, Quintessence and K-essence satisfy neither condition, whereas coupled Quintessence can only satisfy ii). Beyond these seminal DE Effective Field Theories (EFTs), we turn to explicit examples. Working model agnostically in an expansion in powers of redshift z, we show that Brans-Dicke/ f (R) and Kinetic Gravity Braiding models within the Horndeski class can lead to marginal and modest increases in H 0 , respectively. We confirm that as far as increasing H 0 is concerned, no DE EFT model can outperform the phenomenological two parameter family of the DE models. Evidently, the late universe may no longer be large enough to accommodate H 0 , BAO and DE described by EFT.
“…While this clearly happens for the (w 0 , w a ) parametrisations in section 2, DE EFTs, even those that permit w DE < −1, are evidently more rigid, and as we have seen, the scope is limited, at least within our assumptions. In that sense, our analysis agrees with [67,74] that a varying Newton's constant may be a viable approach to alleviating H 0 tension, but this window can be expected to be severely restricted as observational constraints improve.…”
Section: Classsupporting
confidence: 84%
“…For this reason, one would expect increases in H 0 due to linear evolution of F(φ) with cosmic time to be marginal, and this is indeed what we found. Even though the outlook may not be good [67,74], at a technical level it is imperative to identify models that increase H 0 without relying heavily on a local H 0 prior, e. g. [72,73]. Finally, we note that increasing H 0 requires Ḟ > 0 (F 1 < 0), which implies the Newton's constant must decrease in the late universe in line with the findings of Ref.…”
Section: Discussionsupporting
confidence: 71%
“…On the minimal assumption that the coupling G 4 (φ) evolves linearly with cosmic time, while employing model agnostic techniques for the Quintessence sector, G 2 (φ, X) = X − V(φ), we show in section 3 that any increase in H 0 is expected to be negligible. In other words, despite ongoing debate about whether non-minimal couplings can alleviate H 0 tension [71][72][73], in line with [67,74], we find that a non-minimal coupling can only marginally alleviate H 0 tension, at least within reasonable assumptions. Concretely, we observe that the class of models largely fails to penetrate into the phantom regime w DE < −1 at z = 0, so it is consistent with our (w 0 , w a ) expectations.…”
Local H 0 determinations currently fall in a window between H 0 ∼ 70 km/s/Mpc (TRGB) and H 0 ∼ 76 km/s/Mpc (Tully-Fisher). In contrast, BAO data calibrated in an early ΛCDM universe are largely consistent with Planck-ΛCDM, H 0 ∼ 67.5 km/s/Mpc. Employing a generic two parameter family of evolving equations of state (EoS) for dark energy (DE) w DE (z) and mock BAO data, we demonstrate that if i) w DE (z = 0) < −1 and ii) integrated DE density less than ΛCDM, then H 0 increases. EoS that violate these conditions at best lead to modest H 0 increases within 1σ. Tellingly, Quintessence and K-essence satisfy neither condition, whereas coupled Quintessence can only satisfy ii). Beyond these seminal DE Effective Field Theories (EFTs), we turn to explicit examples. Working model agnostically in an expansion in powers of redshift z, we show that Brans-Dicke/ f (R) and Kinetic Gravity Braiding models within the Horndeski class can lead to marginal and modest increases in H 0 , respectively. We confirm that as far as increasing H 0 is concerned, no DE EFT model can outperform the phenomenological two parameter family of the DE models. Evidently, the late universe may no longer be large enough to accommodate H 0 , BAO and DE described by EFT.
“…Other approaches considering varying gravitational constant are analysed in [907], that considering G N as a free parameter, and in [908] in the context of a cuscuta-galileon gravity theory. Finally, Ref [909] implements a sharp transition in the value of the effective gravitational constant prior recombination, effectively lowering the sound horizon at CMB last scattering and addressing both the H 0 and the S 8 tensions.…”
This White Paper has been prepared to fulfill SNOWMASS 2021 requirements and it extends the material previously summarized in the four Letters of Interest [1][2][3][4]. The Particle Physics Community Planning Exercise (a.k.a. SNOWMASS ) is organized by the Division of Particles and Fields of the American Physical Society, and this is an effort to bring together the community of theoretical physicists and cosmologists and identify promising opportunities to address the questions described.This White Paper was initiated with the aim of identifying the opportunities in the cosmological field for the next decade, and strengthening the coordination of the community. It is addressed to identifying the most promising directions of investigation, and rather than attempting a long review of the current status of the whole field of research, it focuses on the upcoming theoretical opportunities and challenges described. The White Paper is a collaborative effort led by Eleonora Di Valentino and Luis Anchordoqui, and it is organized in the topics listed below, each of them coordinated by the scientists indicated (alphabetical order):
“…Refs. [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] in the recent literature. This is a rather controversial topic [29,30,31].…”
The CPC (Covariant Physical Couplings) framework is a modified gravity set up assuming Einstein Field Equations wherein the quantities {G, c, Λ} are promoted to spacetime functions. Bianchi identity and the requirement of stress-energy tensor conservation entangle the possible variations of the couplings {G, c, Λ}, which are forced to co-vary as dictated by the General Constraint (GC). In this paper we explore a cosmological model wherein G, c and Λ are functions of the redshift respecting the GC of the CPC framework. We assume a linear parameterization of Λ in terms of the scale factor a. We use the ansatz Ġ/G = σ ( ċ/c) with σ = constant to deduce the functional forms of c = c(z) and G = G(z). We show that this varying-{G, c, Λ} model fits SNe Ia data and H(z) data with σ = 3. The model parameters can be constrained to describe dark energy at the background level.
scite is a Brooklyn-based organization that helps researchers better discover and understand research articles through Smart Citations–citations that display the context of the citation and describe whether the article provides supporting or contrasting evidence. scite is used by students and researchers from around the world and is funded in part by the National Science Foundation and the National Institute on Drug Abuse of the National Institutes of Health.