Abstract

We study simple effective models of fermionic WIMP dark matter, where the dark matter candidate is a mixture of a Standard Model singlet and an n-plet of SU2L with n ≥ 3, stabilized by a discrete symmetry. The dark matter mass is assumed to be around the electroweak scale, and the mixing is generated by higher-dimensional operators, with a cutoff scale ≳TeV. For appropriate values of the mass parameters and the mixing we find that the observed dark matter relic density can be generated by coannihilation. Direct detection experiments have already excluded large parts of the parameter space, and the next-generation experiments will further constrain these models.

Highlights

  • From some extension of the Standard Model which solves the electroweak hierarchy problem

  • We study simple effective models of fermionic WIMP dark matter, where the dark matter candidate is a mixture of a Standard Model singlet and an n-plet of SU2L with n ≥ 3, stabilized by a discrete symmetry

  • We have studied simple effective models for WIMP dark matter, where the electroweakscale particle content is given by a fermionic singlet and a fermionic SU(2) n-plet with n ≥ 3 in addition to that of the Standard Model

Read more

Summary

Models

Can we reproduce the observed dark matter relic density with a single electroweak-scale singlet χ, with all other states substantially heavier (e.g. with masses Λ TeV) such that they should be integrated out at low energies, thereby inducing the coupling κ?. (We will see that (M − m) ∼ few · 10 GeV for the cases of interest.) eq (2.10) may be a poor approximation to the true mixing angle if the coupling λ is accidentally so small that the higher-order terms in the v/Λ expansion dominate This is e.g. the case in the bino-wino scenario of the MSSM if either μ is small or tan β is large, roughly for μ mZ tan β.

Dark matter properties
The relic density
Freeze-in
Direct and indirect detection
Results
Conclusions and outlook
A The triplet-singlet model
B W3 we obtain the effective neutralino Lagrangian
B The quadruplet-singlet model
C The quintuplet-singlet model
Full Text
Paper version not known

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

Disclaimer: All third-party content on this website/platform is and will remain the property of their respective owners and is provided on "as is" basis without any warranties, express or implied. Use of third-party content does not indicate any affiliation, sponsorship with or endorsement by them. Any references to third-party content is to identify the corresponding services and shall be considered fair use under The CopyrightLaw.