Particle decay in post inflationary cosmology
arXiv:1808.02539 · doi:10.1103/PhysRevD.98.083503
Abstract
We study scalar particle decay during the radiation and matter dominated epochs of a standard cosmological model. An adiabatic approximation is introduced that is valid for degrees of freedom with typical wavelengths much smaller than the particle horizon (~Hubble radius) at a given time. We implement a non-perturbative method that includes the cosmological expansion and obtain a cosmological Fermi's Golden Rule that enables one to compute the decay law of a parent particle of mass , along with the build up of the population of daughter particles of mass . The survival probability of the decaying particle is with being an \emph{effective momentum and time dependent decay rate}. It features a transition time scale between the relativistic and non-relativistic regimes and for is always smaller than the analogous rate in Minkowski spacetime, as a consequence of (local) time dilation and the cosmological redshift. For the decay law is a "stretched exponential" , whereas for the non-relativistic stage with , we find . The Hubble time scale introduces an energy uncertainty which relaxes the constraints of kinematic thresholds. This opens new decay channels into heavier particles for , with the (local) comoving energy of the decaying particle. As the expansion proceeds this channel closes and the usual two particle thresholds restrict the decay kinematics.
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