Abstract

In extended supersymmetric models with a hidden sector the lightest R-parity odd particle can reside in the hidden sector and act as dark matter. We consider the case when the hidden sector has ultraweak interactions with the visible sector. An interesting phenomenon arises if the LSP of the visible sector is charged in which case it will decay to the hidden sector dark matter. Due to the ultraweak interactions, the LSP of the visible sector will be long-lived decaying outside the detector after leaving a track inside. We investigate this possibility in the framework of a U(1)X-extended MSSM/SUGRA model with a small gauge kinetic mixing and mass mixing between the U(1)X and U(1)Y where U(1)Y is the gauge group of the hypercharge. Specifically we investigate the case when the LSP of MSSM is a stop which decays into the hidden sector dark matter and has a lifetime long enough to traverse the LHC detector without decay. It is shown that such a particle can be detected at the HL-LHC and HE-LHC as an R-hadron which will look like a slow moving muon with a large transverse momentum pT and so can be detected by the track it leaves in the inner tracker and in the muon spectrometer. Further, due to the ultraweak couplings between the hidden sector and the MSSM fields, the dark matter particle has a relic density arising from a combination of the freeze-out and freeze-in mechanisms. It is found that even for the ultraweak or feeble interactions the freeze-out contribution relative to freeze-in contribution to the relic density is substantial to dominant, varying between 30% to 74% for the model points considered. It is subdominant to freeze-in for relatively small stop masses with relatively larger stop annihilation cross-sections and the dominant contribution to the relic density for relatively large stop masses and relatively smaller stop annihilation cross-sections. Our analysis shows that the freeze-out contribution must be included for any realistic analysis even for dark matter particles with ultraweak or feeble interactions with the visible sector. A discovery of a long-lived stop as the lightest particle of the MSSM may point to the nature of dark matter and its production mechanism in the early universe.

Highlights

  • Mass of the LSP the relic density is controlled by coannihilation between the stau and the neutralino

  • It is shown that such a particle can be detected at the HL-LHC and HE-LHC as an R-hadron which will look like a slow moving muon with a large transverse momentum pT and so can be detected by the track it leaves in the inner tracker and in the muon spectrometer

  • Further we assume that the hidden sector neutralino interacts with the visible sector with ultraweak interactions

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Summary

The model

As discussed above we consider an extension of the standard model gauge group by an additional abelian gauge group U(1)X. We allow gauge kinetic mixing between the U(1)X and U(1)Y sectors through terms of the form δ 2. Since the mixing parameter δ is very small, the first two neutralinos ξ10 and ξ20 reside mostly in the hidden sector while the remaining four χ0i (i = 1 · · · 4) reside mostly in the MSSM sector. In the limit of small mixings between the hidden and the MSSM sectors the masses of the hidden sector neutralinos are mξ10 =. With cW (cθ)(cφ) ≡ cos θW (cos θ)(cos φ) and sW (sθ)(sφ) ≡ sin θW (sin θ)(sin φ), where θW represents the mixing angle between the new gauge sector and the standard model gauge bosons while the other angles are given by tan φ = α, tan θ gY g2 cδ cos φ,

Dark matter relic density from freeze-in and freeze-out
Model implementation and long-lived stop
Stop pair production at the LHC
Signal and background simulation and event preselection
Selection criteria and results
Findings
Conclusions
Full Text
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