Abstract

In the context of Self-Interacting Dark Matter as a solution for the small-scale structure problems, we consider the possibility that Dark Matter could have been produced without being in thermal equilibrium with the Standard Model bath. We discuss one by one the following various dark matter production regimes of this kind: freeze-in, reannihilation and dark freeze-out. We exemplify how these mechanisms work in the context of the particularly simple Hidden Vector Dark Matter model. In contrast to scenarios where there is thermal equilibrium with the Standard Model bath, we find two regimes which can easily satisfy all the laboratory and cosmological constraints. These are dark freeze-out with 3-to-2 annihilations and freeze-in via a light mediator. In the first regime, different temperatures in the visible and the Dark Matter sectors allow us to avoid the constraints coming from cosmic structure formation as well as the use of non-perturbative couplings to reproduce the observed relic density. For the second regime, different couplings are responsible for Dark Matter relic density and self-interactions, permitting to surpass BBN, X-ray, CMB and direct detection constraints.

Highlights

  • If the connector is so tiny that it has never had any practical impact, one can consider two possibilities, depending on whether the Hidden Sector (HS) thermalizes or not. If it does not thermalize, there is a relic density we can not predict its value unless we address the physics responsible for the reheating process [71, 72]

  • We have shown in a systematic way how the various possible DM production regimes, where the DM sector is not in thermal equilibrium with the Standard Model (SM) sector, can be relevant for solving the small scale DM problems

  • Other constraints that are fully relevant for such scenarios come from Big Bang Nucleosynthesis (BBN), Cosmic Microwave Background (CMB), X-ray emission and DM direct detection searches

Read more

Summary

Hidden Vector Dark Matter: description of the model

We provide the essential ingredients of the HVDM model [49], which is the one we will consider explicitly in all subsequent sections. Due to a remnant accidental custodial SO(3) symmetry, these three gauge bosons form a triplet with the same mass mA = gX vφ/2, and are automatically stable. These are the DM candidates of the model. Such a gauge structure is allowed to communicate with the SM through a unique renormalizable interaction, λm, of the Higgs portal type In this setup the η scalar mixes with the SM scalar h , which, after diagonalization, leads to the physical η and h fields. In this model, while DM is stable because of the SO(3) accidental symmetry, still the annihilation of three DM particles into two takes place naturally, induced by the gauge nature of the trilinear term. For the phenomenological study of the following sections, this model is implemented in FeynRules [59, 60] and the output in obtained in CalcHEP [61]

Dark Matter self-interactions
Various possibilities of accounting for the Dark Matter relic density
10-8 Regime 1
Scenario with no light mediator
Regime 4: portal interaction freeze-out
Regime 2: reannihilation
Regime 1: freeze-in
Regime 0: no portal
Scenario with a light mediator
Regime 3A
Conclusions
A Invisible decay of the SM scalar
C Constraints on regimes 2 and 3A with a light mediator
Full Text
Published version (Free)

Talk to us

Join us for a 30 min session where you can share your feedback and ask us any queries you have

Schedule a call