Birth of Dark Matter in the Inflationary Furnace express

Original: "Dark Photon Dark Matter from Quantum Fluctuations during Starobinsky Inflation"
· Taiyo Kasamaki, Takeo Moroi
arXiv:2607.29149v1 · 2026-07-31 · CC BY 4.0 · 1 min
Quantum jitters in the first moments of the universe could have spawned dark matter particles with masses of a few millionths of an electronvolt.

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In the first moments after the Big Bang, the universe underwent a rapid expansion — inflation. Space stretched faster than light, and quantum jitters of the vacuum turned into real particles. This is how dark matter, the invisible substance that holds galaxies together, could have been born.

The authors of the study considered a hypothetical particle: the dark photon. It is an analog of the ordinary photon, but with a tiny mass. In models where inflation alters the geometry of space, the properties of the dark photon depend on the course of the expansion itself. Calculations showed that if this dependence is ignored, one could be off by hundreds of times in the number of particles produced.

The mass of the dark photon turns out to be squeezed into a narrow corridor: from 5.6 to 7.4 microelectronvolts. That's about a trillion times lighter than the electron.

The scientists took the inflation model proposed by Alexei Starobinsky in 1980. In this model, the expansion is driven not by a field but by corrections to spacetime curvature. For this scenario, they honestly integrated the particle production equations from the beginning of inflation to the present day. The result is a mass prediction that can be tested in laboratory experiments searching for dark photons.

Thus, quantum jitters of the vacuum, frozen in the first moments, turn out to be the key to unraveling the composition of the modern universe. The narrow mass window is not just a number: it's an invitation to directly test the theory.

Original abstract

as written by the authors arXiv:2607.29149v1

We present a detailed investigation of scenarios in which dark-photon dark matter is produced from quantum fluctuations during inflation. In particular, we focus on inflationary models that necessarily involve a Weyl transformation, dependent on the inflaton amplitude, in order to move to the Einstein frame. In such models, the kinetic function of the longitudinal mode of the dark photon varies throughout, and even after, the inflationary period. We show that this variation of the kinetic function has a substantial impact on the resulting relic abundance of dark photons. As a representative and phenomenologically important example, we analyze the Starobinsky inflation model, for which we perform an accurate computation of the relic dark-photon abundance. By imposing the relevant observational constraints, we find that, in order to reproduce the observed dark-matter density in the present Universe, the dark-photon mass must lie in the range $$5.6 < m < 7.4\,\mu\mathrm{eV}$$ within the framework considered in this work.

Dark photons, if they exist, could mix very weakly with ordinary light. They are being sought by 'listening' to an empty metal cavity with ultra-sensitive radio receivers.

Scientists
Alan GuthAlexander FriedmannAndrei LindeGeorges LemaîtreJames PeeblesStephen Hawking
Concepts
starobinsky inflation dark photon quantum fluctuation inflation inflaton quantum cosmological inhomogeneities inflationary cosmology dark matter inflationary gravitational waves virtual particle stochastic fluctuations magnetophotonic effects neutrino decay cosmic neutrino dynamic casimir effect reheating black hole photon ring density fluctuation galaxy formation Sachs–Wolfe effect particle creation