The H0 tension: Δ GN vs. Δ Neff

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Published 12 November 2020 © 2020 IOP Publishing Ltd and Sissa Medialab
, , Citation Guillermo Ballesteros et al JCAP11(2020)024 DOI 10.1088/1475-7516/2020/11/024

1475-7516/2020/11/024

Abstract

We investigate whether the 4.4σ tension on H0 between SH0ES 2019 and Planck 2018 can be alleviated by a variation of Newton's constant GN between the early and the late Universe. This changes the expansion rate before recombination, similarly to the addition of Δ Neff extra relativistic degrees of freedom. We implement a varying GN in a scalar-tensor theory of gravity, with a non-minimal coupling of the form (M2+β ϕ2)R. If the scalar ϕ starts in the radiation era at an initial value ϕI ∼ 0.5 Mp and with β<0, a dynamical transition occurs naturally around the epoch of matter-radiation equality and the field evolves towards zero at late times. As a consequence, the H0 tension between SH0ES (2019) and Planck 2018+BAO slightly decreases, as in Δ Neff models, to the 3.8σ level. We then perform a fit to a combined Planck, BAO and supernovae (SH0ES and Pantheon) dataset. When including local constraints on Post-Newtonian (PN) parameters, we find H0=69.08−0.71+0.6 km/s/Mpc and a marginal improvement of Δχ2≃−3.2 compared to ΛCDM, at the cost of 2 extra parameters. In order to take into account scenarios where local constraints could be evaded, we also perform a fit without PN constraints and find H0=69.65−0.78+0.8 km/s/Mpc and a more significant improvement Δχ2=−5.4 with 2 extra parameters. For comparison, we find that the Δ Neff model gives H0=70.08−0.95+0.91 km/s/Mpc and Δχ2=−3.4 at the cost of one extra parameter, which disfavors the ΛCDM limit just above 2σ, since Δ Neff=0.34−0.16+0.15. Overall, our varying GN model performs similarly to the Δ Neff model in respect to the H0 tension, if a physical mechanism to remove PN constraints can be implemented.

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10.1088/1475-7516/2020/11/024