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Can I read A $w-M$ phantom transition at $z_t<0.1$ as a resolution of the Hubble tension on EtoBox?

A $w-M$ phantom transition at $z_t<0.1$ as a resolution of the Hubble tension by Alestas, George; Kazantzidis, Lavrentios; Perivolaropoulos, Leandros is a scholarly article available to read on EtoBox.

What is A $w-M$ phantom transition at $z_t<0.1$ as a resolution of the Hubble tension about?

A rapid phantom transition of the dark energy equation of state parameter $w$ at a transition redshift $z_t<0.1$ of the form $w(z)=-1+\Delta w\;\Theta (z_t-z)$ with $\Delta w<0$ can lead to a higher value of the Hubble constant while closely mimicking a Planck18/$\Lambda$CDM form of the comoving distance $r(z)=\int_0^z\frac{dz'}{H(z')}$ for $z>z_t$. Such a transition however would imply a significantly lower value of the SnIa absolute magnitude $M$ than the value $M_C$ imposed by local Cepheid calibrators at $z<0.01$. Thus, in order to resolve the $H_0$ tension it would need to be accompanied by a similar transition in the value of the SnIa absolute magnitude $M$ as $M(z)=M_C+\Delta M \;\Theta (z-z_t)$ with $\Delta M<0$. This is a Late $w-M$ phantom transition ($LwMPT$). It may be achieved by a sudden reduction of the value of the normalized effective Newton constant $\mu=G_{\rm{eff}}/G_{\rm{N}}$ by about $6\%$ assuming that the absolute luminosity of SnIa is proportional to the Chandrasekhar mass which varies as $\mu^{-3/2}$. We demonstrate that such an ultra low $z$ abrupt feature of $w-M$ provides a better fit to cosmological data compared to smooth late time deformations of $H(

Author
Alestas, George; Kazantzidis, Lavrentios; Perivolaropoulos, Leandros
Published
2020
Language
EN