Redshift propagation equations in the $\beta' \neq 0$ Szekeres models
Andrzej Krasi\'nski, Krzysztof Bolejko

TL;DR
This paper derives redshift equations in complex Szekeres spacetimes, showing that most light paths are non-repeatable, with only special symmetric cases allowing repeatable paths, and discusses potential observational implications of sky position drift.
Contribution
It provides the first detailed derivation of redshift propagation equations in general $eta' eq 0$ Szekeres models, highlighting the rarity of repeatable light paths.
Findings
Most Szekeres models lack repeatable light paths.
Only axially symmetric and certain symmetric models have RLPs.
Sky position drift could be observable within a decade.
Abstract
The set of differential equations obeyed by the redshift in the general Szekeres spacetimes is derived. Transversal components of the ray's momentum have to be taken into account, which leads to a set of 3 coupled differential equations. It is shown that in a general Szekeres model, and in a general Lema\^{\i}tre -- Tolman (L--T) model, generic light rays do not have repeatable paths (RLPs): two rays sent from the same source at different times to the same observer pass through different sequences of intermediate matter particles. The only spacetimes in the Szekeres class in which {\em all} rays are RLPs are the Friedmann models. Among the proper Szekeres models, RLPs exist only in the axially symmetric subcases, and in each one the RLPs are the null geodesics that intersect each constant space on the symmetry axis. In the special models with a 3-dimensional…
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