We show that a nonstandard cosmological history with a period of early matter domination driven by a sub-TeV visible-sector particle can arise rather naturally. This scenario involves a long-lived standard model singlet that acquires a thermal abundance at high temperatures from decays and inverse decays of a parent particle with SM charge(s), and subsequently dominates the energy density of the Universe as a frozen species. Entropy generation at the end of early matter domination dilutes the abundance of dangerous relics (such as gravitinos) by a factor as large as 10 4 . The scenario can accommodate the correct dark matter relic abundance for cases with σannv f ≶ 3 × 10 −26 cm 3 s −1 . More importantly, the allowed parameter space can be directly probed by proposed searches for neutral long-lived particles at the energy frontier, allowing us to use particle physics experiments to reconstruct the cosmological history just prior to big bang nucleosynthesis.
I. INTRODUCTIONDespite various lines of evidence for the existence of dark matter (DM) [1], its identity remains a major problem at the interface of cosmology and particle physics. The relic abundance of DM depends on its particle physics origin as well as the thermal history of the early Universe. Thermal freeze-out in a radiation-dominated (RD) Universe can explain the DM content of the Universe if the thermally averaged annihilation rate takes the nominal value σ ann v f = 3 × 10 −26 cm 3 s −1 at the time of freeze-out, when T = T f . However, the correct relic abundance can also be obtained for much larger or smaller values of σ ann v f if the Universe is not in a RD phase at the time of freeze-out [2]. An epoch of early matter domination (EMD), which is a generic feature of early Universe models from string theory constructions [3], provides an important such example. EMD is driven by a matter-like species that comes to dominate the energy density of the Universe and decays to establish RD prior to big bang nucleosynthesis (BBN). Various production mechanisms during EMD can yield the correct DM abundance for both σ ann v f ≶ 3 × 10 −26 cm 3 s −1 .A component whose equation of state is the same as matter can lead to an EMD phase in the postinflationary Universe if it constitutes a sizeable fraction of the total energy density and is sufficiently long lived. In the context of string theory, this can arise from coherent oscillations of string moduli that are displaced from the minimum of their potential during inflation. Modulus fields have long lifetimes due to their gravitationally suppressed couplings to other fields. An EMD era may also be driven by long-lived nonrelativistic quanta that are produced in the postinflationary Universe and dominate the energy density before decaying. This can happen, for example, in models that involve hidden sectors [5][6][7][8]. Scenarios with EMD have interesting observable predictions that can be tested via cosmological observations and DM indirect detection searches [9][10][11][12][13]. A natural question that arises i...