Abstract

We study cascade decays of heavy neutral Higgs bosons through vectorlike quarks. We focus on scenarios where decay modes into pairs of vectorlike quarks are not kinematically open which extends the sensitivity of the LHC to larger masses. Assuming only mixing with the third family of standard model quarks the new decay modes of heavy Higgs bosons are: H → t4t → Wbt, Ztt, htt and H → b4b → Wtb, Zbb, hbb, where t4 (b4) is the new up-type (down-type) quark mass eigenstate. In the numerical analysis we assume the CP even Higgs boson in the two Higgs doublet model type-II but the signatures are relevant for many other scenarios. We identify the region of the parameter space where these decay modes are significant or can even dominate, and thus they provide the best opportunities for the simultaneous discovery of a new Higgs boson and vectorlike quarks. We further explore the reach of the High Luminosity LHC for two representative decay modes, t4→ Zt → ℓℓt and b4→ Zb → ℓℓb, and found that cross sections at a 0.1 fb level can be probed with simple cut based analyses. We also find that the rates for Higgs cascade decays can be much larger than the rates for a single production of vectorlike quarks. Furthermore, the reach for vectorlike quarks in Higgs cascade decays and pair production extends to comparable masses.

Highlights

  • We study cascade decays of heavy neutral Higgs bosons through vectorlike quarks

  • We identify the region of the parameter space where these decay modes are significant or can even dominate, and they provide the best opportunities for the simultaneous discovery of a new Higgs boson and vectorlike quarks

  • We find that the rates for Higgs cascade decays can be much larger than the rates for a single production of vectorlike quarks

Read more

Summary

Parameter space scan and experimental constraints

In the numerical study we scan the parameters of the model in the following ranges: MQ,T,B ∈ [900, 4000] GeV , κT , κQ, κ, κ ∈ [−1.0, 1.0] , λB, λQ, λ, λ ∈ [−1.0, 1.0] , tan β ∈ [0.3, 50] ,. Due to current constraints on vectorlike quark masses, all indirect constraints have a minimal impact on our scan. We impose experimental constraints from oblique corrections and Rb [61] following the results presented in section II of ref. We further include bounds from h → (γγ, 4 ) [65,66,67] [68, 69]), and direct searches for pair production of vectorlike quarks at the LHC [70, 71] (for each scan point we calculate the t4 and b4 branching ratios into W , Z and h and compare with the constraint). The width H → hh is given in eq (A.7) which impacts the H → hh branching ratio at the O(0.1%) level; H → hh constraints [78] are negligible

Higgs production cross section and decays
Search strategies and comparison with single productions of t4 and b4
Conclusions
Findings
A Partial decay widths of the heavy Higgs boson
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