Higgs-Portal Stueckelberg Dark Matter
arXiv:2512.17231 · doi:10.1103/jrrj-qy9w
Abstract
We study dark photon dark matter X associated with a dark gauge symmetry. To evade laboratory and cosmological constraints on kinetic mixing with the Standard Model , we assign a -odd dark parity to X that forbids such mixing. The leading interactions then arise from gauge-invariant dimension-6 Higgs-portal operators, including both parity-even and parity-odd terms. We assume that the dark matter mass is generated via the Stueckelberg mechanism. In the interacting Stueckelberg EFT, a gauge-invariant dimension-6 parent reduces in unitary gauge to the nominal dimension-4 Higgs-portal interaction , with its coefficient correlated with , while additional derivative operators are organized by the same longitudinal-mode power counting. We investigate freeze-in production of X from Higgs-pair annihilations after reheating, incorporating both field-strength and Stueckelberg-allowed operators. First, we consider the case in which the Wilson coefficients of the gauge-invariant dimension-6 operators, C and , are of order unity. Under a conservative single-cutoff power counting in which the strong-coupling scales of the longitudinal mode lie above the cutoff of the field-strength effective theory, we find that the Stueckelberg contributions remain subdominant in dark matter production. We emphasize that this ordering of scales is an explicit assumption rather than a universal consequence of perturbative unitarity. Next, we explore a more general situation in which C and are smaller than unity. In this second case, Stueckelberg-allowed operators can become comparable and generate contributions proportional to , , and , including sign-dependent interference effects. For both cases, we show that there exists a wide parameter space consistent with the observed dark matter relic density.
arXiv comment30 pages, 6 figures, 2 tables. Published version in Phys. Rev. D with a minor clarification