Abstract

In hidden sector models, dark matter does not directly couple to the particle content of the Standard Model, strongly suppressing rates at direct detection experiments, while still allowing for large signals from annihilation. In this paper, we conduct an extensive study of hidden sector dark matter, covering a wide range of dark matter spins, mediator spins, interaction diagrams, and annihilation final states, in each case determining whether the annihilations are s-wave (thus enabling efficient annihilation in the universe today). We then go on to consider a variety of portal interactions that allow the hidden sector annihilation products to decay into the Standard Model. We broadly classify constraints from relic density requirements and dwarf spheroidal galaxy observations. In the scenario that the hidden sector was in equilibrium with the Standard Model in the early universe, we place a lower bound on the portal coupling, as well as on the dark matter’s elastic scattering cross section with nuclei. We apply our hidden sector results to the observed Galactic Center gamma-ray excess and the cosmic-ray antiproton excess. We find that both of these excesses can be simultaneously explained by a variety of hidden sector models, without any tension with constraints from observations of dwarf spheroidal galaxies.

Highlights

  • We present the main results of our analysis, identifying which of the hidden sector dark matter models discussed in sections 2 and 3 are capable of producing signals that are consistent with the observed features of the Galactic Center gamma-ray excess and the cosmic-ray antiproton excess

  • We summarize our results for the case of hidden sector dark matter that annihilates into a pair of spin-1 particles that decay to the SM through the hypercharge portal

  • In the upper left frame, we show the regions of the mχ-mZ plane that can produce the observed spectrum and intensity of the Galactic Center gamma-ray excess (GCE), the cosmic-ray antiproton excess (Antip), or both

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Summary

Hidden sector dark matter annihilation

We consider the annihilation of dark matter particles. we are primarily interested in this study in dark matter that resides within a hidden sector, the contents of this section can be applied to non-hidden sector scenarios as well. We can consider interactions involving complex scalars This allows for the possibility of many different interactions, we include in our study only the following case which can potentially lead to s-wave dark matter annihilation: L(Φz) ⊃ λΦz iΦ∗i ∂μ Φi Zμ + h.c. We consider interactions that take place exclusively between spin-1 particles Such interactions can naturally appear in hidden sector models which feature more complex gauge symmetries In tables 1 and 2, we list each of the processes through which a fermionic or bosonic dark matter particle could annihilate through an s-wave amplitude The presence of multiple rows within the same table entry implies that there are multiple interaction combinations that can lead to s-wave annihilation Those cases denoted with a ‘-’ do not correspond to any renormalizable model within our framework.

Portals between the hidden sector and the standard model
Hypercharge portal
Baryon portal
Higgs portal
Two-Higgs doublet portal
Neutrino portal
Characteristics of the gamma-ray and antiproton excesses
The galactic center gamma-ray excess
The cosmic-ray antiproton excess
Energy spectra generation
Constraints from dwarf spheroidal galaxies
B L Portal
Results
Cosmological considerations and prospects for direct detection
Summary and conclusions
Full Text
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