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Vector dark matter production during inflation in the gradient-expansion formalism

A. V. Lysenko1,*, O. O. Sobol2,1,†, and S. I. Vilchinskii3,1,‡

  • *Contact author: lysenkoktp@knu.ua
  • †Contact author: oleksandr.sobol@knu.ua
  • ‡Contact author: stanislav.vilchinskii@cern.ch
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Phys. Rev. D 113, 063525 – Published 9 March, 2026

DOI: https://doi.org/10.1103/lpph-hrdr

Abstract

A massive vector field is a highly promising candidate for dark matter in the Universe. A salient property of dark matter is its negligible or null coupling to ordinary matter, with the exception of gravitational interaction. This poses a significant challenge in producing the requisite amount of dark particles through processes within the Standard Model. In this study, we examine the production of a vector field during inflation due to its direct interaction with the inflaton field through kinetic and axionlike couplings as well as the field-dependent mass. The gradient-expansion formalism, previously proposed for massless Abelian gauge fields, is extended to include the longitudinal polarization of a massive vector field. We derive a coupled system of equations of motion for a set of bilinear functions of the vector field. This enables us to address the nonlinear dynamics of inflationary vector field production, including backreaction on background evolution. To illustrate this point, we apply our general formalism to a low-mass vector field whose kinetic and mass terms are coupled to the inflaton via the Ratra-type exponential function. The present study investigates the production of its transverse and longitudinal polarization components in a benchmark inflationary model with a quadratic inflaton potential. It has been demonstrated that pure mass coupling is able to enhance only the longitudinal components. By turning on also the kinetic coupling, one can get different scenarios. As the coupling function decreases, the primary contribution to the energy density is derived from the transverse polarizations of the vector field. Conversely, for an increasing coupling function, the longitudinal component becomes increasingly significant and rapidly propels the system into the strong backreaction regime.

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Phys. Rev. D 113, 063525– Published 9 March, 2026
  • Received 6 October 2025
  • Accepted 23 February 2026
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