The Hubble diagram for a system within dark energy: the location of the zero-gravity radius and the global Hubble rate
Pekka Teerikorpi, Arthur Davidovich Chernin

TL;DR
This paper investigates how the local measurement of dark energy using galaxy system dynamics can determine the zero-gravity radius and the global Hubble rate, providing insights into local versus global dark energy density.
Contribution
It introduces a method to relate local galaxy flow measurements to the global dark energy density and Hubble rate, refining understanding of local dark energy effects.
Findings
The outflow reaches the global Hubble rate at a radius related to the zero-gravity radius.
The local flow reaches the global Hubble rate at about 1.5 times the zero-gravity radius.
For the Local Group, the local dark energy density is consistent with the global value.
Abstract
Here we continue to discuss the principle of the local measurement of dark energy using the normalized Hubble diagram describing the environment of a system of galaxies. We calculate the present locus of test particles injected a fixed time ago (\sim the age of the universe), in the standard \Lambda -cosmology and for different values of the system parameters (the model includes a central point mass M and a local dark energy density \rho_{loc}) and discuss the position of the zero-gravity distance R_v in the Hubble diagram. Our main conclusions are: 1) When the local DE density \rho_{loc} is equal to the global DE density \rho_v, the outflow reaches the global Hubble rate at the distance R_2 = (1+z_v)R_v, where z_v is the global zero-acceleration redshift (\approx 0.7 for the standard model). This is also the radius of the ideal Einstein-Straus vacuole. 2) For a wide range of the…
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