A phantom transition at as a resolution of the Hubble tension
arXiv:2012.13932 · doi:10.1103/PhysRevD.103.083517
Abstract
A rapid phantom transition of the dark energy equation of state parameter at a transition redshift of the form with can lead to a higher value of the Hubble constant while closely mimicking a Planck18/CDM form of the comoving distance for . Such a transition however would imply a significantly lower value of the SnIa absolute magnitude than the value imposed by local Cepheid calibrators at . Thus, in order to resolve the tension it would need to be accompanied by a similar transition in the value of the SnIa absolute magnitude as with . This is a Late phantom transition (). It may be achieved by a sudden reduction of the value of the normalized effective Newton constant by about assuming that the absolute luminosity of SnIa is proportional to the Chandrasekhar mass which varies as . We demonstrate that such an ultra low abrupt feature of provides a better fit to cosmological data compared to smooth late time deformations of that also address the Hubble tension. For we find , . This model also addresses the growth tension due to the predicted lower value of at . A prior of (no transition) can still resolve the tension with a larger amplitude transition with at . This implies a larger reduction of for (about ). The can be generically induced by a scalar field non-minimally coupled to gravity with no need of a screening mechanism since in this model at .
14 pages, 9 Figures. Accepted in Physical Review D (to appear). Typos corrected, a new figure and references added. The Mathematica files used for the construction of the figures may be downloaded from https://github.com/GeorgeAlestas/LwMPT
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