Cosmologies in Horndeski's second-order vector-tensor theory
John D. Barrow, Mikjel Thorsrud, Kei Yamamoto

TL;DR
This paper explores the cosmological implications of Horndeski's second-order vector-tensor theory, focusing on the effects of a free parameter that influences the universe's evolution and observational constraints.
Contribution
It provides a detailed analysis of the cosmological consequences of Horndeski's gauge-invariant vector-tensor theory, including singularity conditions and observational viability.
Findings
Negative coupling leads to finite-time singularities.
Viable cosmological models exist for positive coupling.
Observational constraints on the coupling are weak due to higher-order curvature interactions.
Abstract
Horndeski derived a most general vector-tensor theory in which the vector field respects the gauge symmetry and the resulting dynamical equations are of second order. The action contains only one free parameter, , that determines the strength of the non-minimal coupling between the gauge field and gravity. We investigate the cosmological consequences of this action and discuss observational constraints. For we identify singularities where the deceleration parameter diverges within a finite proper time. This effectively rules out any sensible cosmological application of the theory for a negative non-minimal coupling. We also find a range of parameter that gives a viable cosmology and study the phenomenology for this case. Observational constraints on the value of the coupling are rather weak since the interaction is higher-order in space-time curvature.
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