Abstract

Models with a tiny coupling $\lambda$ between the dark matter and the Standard Model, $\lambda \sim v/M_\text{Pl}\sim 10^{-16}$, can yield the measured relic abundance through the thermal process known as freeze-in. We propose to interpret this small number in the context of perturbative large $N$ theories, where couplings are suppressed by inverse powers of $N$. Then $N \sim M_{\rm Pl}^2/v^2$ gives the observed relic density. Additionally, the ultimate cutoff of the Standard Model is reduced to $\sim 4\,\pi\, M_\text{Pl}/\sqrt{N} \sim 4\, \pi\, v$, thereby solving the electroweak hierarchy problem. These theories predict a direct relation between the Standard Model cutoff and the dark matter mass, linking the spectacular collider phenomenology associated with the low gravitational scale to the cosmological signatures of the dark sector. The dark matter mass can lie in the range from hundreds of keV to hundreds of GeV. Possible cosmological signals include washing out power for small scale structure, indirect detection signals from dark matter decays, and a continuous injection of electromagnetic and hadronic energy throughout the history of the Universe.

Highlights

  • Dark matter (DM) accounts for 80% of the matter in our Universe, but its microscopic origin is still unknown

  • If the DM is coupled to the standard model (SM) thermal bath, a variety of mechanisms to produce the observed relic abundance are possible

  • The DM production ceases once the SM bath temperature T becomes of order of the mass of the lightest SM particle that interacts with the DM, thereby freezing-in the relic density

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Summary

INTRODUCTIONS

Dark matter (DM) accounts for 80% of the matter in our Universe, but its microscopic origin is still unknown. The freeze-in relic density calculation maps N (and ΛUV) onto a choice for the DM mass, as discussed in Secs. This relation is one of the most appealing features of our framework since it implies that this class of theories is quite predictive: once we fix the large N scaling of the couplings, the DM mass determines both the strength of its interactions with the SM and ΛUV. In the 4D effective theory, this can be viewed as a consequence of a large number of Kaluza-Klein states, comparable to the number of species in our dark sector In this sense, the equivalence of the large N solution to the hierarchy problem can be made sharp.

MODELS
RELIC DENSITY
PHENOMENOLOGY
Equal masses
Findings
OUTLOOK
Full Text
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