paper

A reanalysis of the latest SH0ES data for : Effects of new degrees of freedom on the Hubble tension

arXiv:2208.11169

Abstract

We reanalyze the recently released SH0ES data for the determination of . We focus on testing the homogeneity of the Cepheid+SnIa sample and the robustness of the results in the presence of new degrees of freedom in the modeling of Cepheids and SnIa. We thus focus on the four modeling parameters of the analysis: the fiducial luminosity of SnIa and Cepheids and the two parameters ( and ) standardizing Cepheid luminosities with period and metallicity. After reproducing the SH0ES baseline model results, we allow for a transition of the value of any one of these parameters at a given distance or cosmic time thus adding a single degree of freedom in the analysis. When the SnIa absolute magnitude is allowed to have a transition at (about ago), the best fit value of the Hubble parameter drops from to in full consistency with the Planck value. Also, the best fit SnIa absolute magnitude for drops to the Planck inverse distance ladder value while the low distance best fit parameter remains close to the original distance ladder calibrated value . Similar hints for a transition behavior is found for the other three main parameters of the analysis (, and ) at the same critical distance even though in that case the best fit value of is not significantly affected. When the inverse distance ladder constraint on is included in the analysis, the uncertainties for reduce dramatically () and the transition model is strongly preferred over the baseline SH0ES model (, ) according to AIC and BIC model selection criteria.

49 pages, 21 Figures, 7 Tables. Invited submission to Universe (accepted for publication, to appear). 5 Figures added including an explicit demonstration of hints for M transition in the data (Fig. 17). The numerical analysis Mathematica (v. 11 and v. 12) files that lead to the production of the figures may be found at https://github.com/FOTEINISKARA/A-reanalysis-of-the-SH0ES-data-for-H_0