Many late time approaches for the solution of the Hubble tension use a late time smooth deformation of the Hubble expansion rate H (z) of the Planck18/ΛCDM best fit H (z) to match the locally measured value of H0 while effectively keeping the comoving distance to the last scattering surface r (zrec) and ωm ≡ Ω0mh fixed to maintain consistency with Planck CMB measurements. A well known problem of these approaches is that they worsen the fit to low z distance probes (BAO and SnIa). Here we show that another problem of these approaches is that they worsen the level of the Ω0m − σ8 growth tension. We use the CPL parametrization of H (z) corresponding to evolving dark energy equation of state parameter w(z) = w0 + w1 z 1+z with local measurements H0 prior and fixed values of Ω0mh and r (zrec) and identify the pairs (w0, w1) that satisfy these conditions. We show that for these models theΩ0m −σ8 tension between dynamical probe data (redshift space distortions) and CMB constraints is worse than the corresponding tension that appears in the case of the standard Planck18/ΛCDM model. We justify this feature using a full numerical solution of the growth equation and fit to the data, as well as by using approximate analytic properties of the growth factor of perturbations δρ ρ (z) solution. A similar problem has been pointed out for early time approaches to the Hubble crisis. The problem does not affect recent proposed solutions of the Hubble crisis involving a SnIa intrinsic luminosity transition at zt ' 0.01 that can fully resolve both the Hubble and the growth tensions while being consistent with the Cepheid distance calibrators at z < 0.01.
Late-time approaches to the Hubble tension deforming H(z), worsen the growth tension
G. Alestas,L. Perivolaropoulos
Published 2021 in Unknown venue
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2021
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Unknown venue
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2021-03-06
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Physics
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