Abstract

We study the post-inflationary dynamics of the Standard Model Higgs and a real singlet scalar ss, coupled together through a renormalizable coupling λshh2s2λ_{sh}h^2s^2, in a Z2Z_2 symmetric model that may explain the observed dark matter abundance and/or the origin of baryon asymmetry. The initial values for the Higgs and ss condensates are given by inflationary fluctuations, and we follow their dissipation and relaxation to the low energy vacua. We find that both the lowest order perturbative and the non-perturbative decays are blocked by thermal effects and large background fields and that the condensates decay by two-loop thermal effects. Assuming instant reheating at T=1016T=10^{16} GeV, the characteristic temperature for the Higgs condensate thermalization is found to be Th∼1014T_h \sim 10^{14} GeV, whereas ss thermalizes typically around Ts∼106T_s \sim 10^{6} GeV. By that time, the amplitude of the singlet is driven very close to the vacuum value by the expansion of the universe, unless the portal coupling takes a value λsh≲10−7λ_{sh}\lesssim 10^{-7} and the singlet ss never thermalizes. With these values of the coupling, it is possible to slowly produce a sizeable fraction of the observed dark matter abundance via singlet condensate fragmentation and thermal Higgs scattering. Physics also below the electroweak scale can therefore be affected by the non-vacuum initial conditions generated by inflation.

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