posted on 2016-05-11, 00:00authored byL Randall, J Scholtz, J Unwin
Most dark matter models set the dark matter relic density by some interaction
with Standard Model particles. Such models generally assume the existence of Standard
Model particles early on, with the dark matter relic density a later consequence of those
interactions. Perhaps a more compelling assumption is that dark matter is not part of
the Standard Model sector and a population of dark matter too is generated at the end of
inflation. This democratic assumption about initial conditions does not necessarily provide
a natural value for the dark matter relic density, and furthermore superficially leads to too
much entropy in the dark sector relative to ordinary matter. We address the latter issue
by the late decay of heavy particles produced at early times, thereby associating the dark
matter relic density with the lifetime of a long-lived state. This paper investigates what it
would take for this scenario to be compatible with observations in what we call Flooded
Dark Matter (FDM) models and discusses several interesting consequences. One is that
dark matter can be very light and furthermore, light dark matter is in some sense the most
natural scenario in FDM as it is compatible with larger couplings of the decaying particle.
A related consequence is that the decay of the field with the smallest coupling and hence
the longest lifetime dominates the entropy and possibly the matter content of the Universe,
a principle we refer to as “Maximum Baroqueness”. We also demonstrate that the dark
sector should be colder than the ordinary sector, relaxing the most stringent free-streaming
constraints on light dark matter candidates. We will discuss the potential implications for
the core-cusp problem in a follow-up paper. The FDM framework will furthermore have
interesting baryogenesis implications. One possibility is that dark matter is like the baryon
asymmetry and both are simultaneously diluted by a late entropy dump. Alternatively,
FDM is compatible with an elegant non-thermal leptogenesis implementation in which
decays of a heavy right-handed neutrino lead to late time reheating of the Standard Model
degrees of freedom and provide suitable conditions for creation of a lepton asymmetry.