The expansion history of the Universe can found by measuring the differential age evolution of cosmic chronometers. This yields a measurement of the Hubble parameter H(z) as a function of redshift.
see: Jimenez & Loeb (2002); Moresco et al. (2018).
The basic idea of the Cosmic Chronometer method is that the Hubble parameter is related to the differential redshift-time relation as $H(z) = \frac{-1}{1+z}\times\frac{dz}{dt}\tag1$
(1) is derived from
$H(z)= \frac{\dot a}{a}$
$a=\frac{1}{1+z}$ and
$\frac{da}{dt}=\frac{da}{dz} \times \frac{dz}{dt}$
Then the quantities $dz$ and $dt$ need to be measured for a passively evolving system such as a group of stars, $dz$ is found from spectroscopic measurements.
For $dt$ the ‘cosmic chronometer’ was a direct spectroscopic observable (the 4000 ˚A break) known to be linearly related with the age of the stellar population
and a plot of $H(z)$ against $z$ can be obtained like the one above.
“The solid line and the dashed regions...show the fiducial flat LCDM cosmology... H0 = 67.8 km/s/Mpc, m = 0.308. For comparison an Einstein-de Sitter model is shown...”
• Moresco et al DOI:10.1088/1475-7516/2016/05/014
The method doesn’t need absolute ages of stars, but the difference in ages of the stars.
The question is this:
Since both the actual age of a star and the difference in ages of a pair of stars are both subject to time dilation, has this properly been accounted for in the method?
For example, with easy numbers.
If time dilation caused a 10.2 million year old star at a redshift of $z$ to appear to be 5.1 million years old, and a 10 million year old star further away at redshift $z+dz$ to appear to be 5 million years old, the $dt$ would be measured as 0.1 million years, but in reality it should be 0.2 million years.
It doesn’t seem to be taken into account, or is it already there in equation (1)?