Abstract

We conduct a numerical study over the constrained MSSM (CMSSM), Next-to-MSSM (NMSSM) and $U(1)$ extended MSSM (UMSSM) to probe the allowed mass ranges of the charged Higgs boson and its dominant decay patterns, which might come into prominence in near future collider experiments. {We present results obtained from a limited scan for CMSSM} as a basis and compare its predictions with the extended models. We observe within our data that a wide mass range is allowed as $0.5(1) \lesssim m_{H^{\pm}} \lesssim 17$ TeV in UMSSM (NMSSM). We find that the dominant decay channel is mostly $H^{\pm}\rightarrow tb$ such that ${\rm BR}(H^{\pm}\rightarrow tb) \sim 80\%$. While this mode remains dominant over the whole allowed parameter space of CMSSM, we realize some special domains in the NMSSM and UMSSM, in which ${\rm BR}(H^{\pm}\rightarrow tb) \lesssim 10\%$. In this context, the decay patterns of the charged Higgs can play a significant role to distinguish among the SUSY models. In addition to the $tb$ decay mode, we find that the narrow mass scale in CMSSM allows only the decay modes for the charged Higgs boson to $\tau\nu$ ($\sim 16\%$), and their supersymmetric partners $\tilde{\tau}\tilde{\nu}$ ($\sim 13\%$). On the other hand, it is possible to realize the mode in NMSSM and UMSSM in which the charged Higgs boson decays into a chargino and neutralino pair up to about $25\%$. {This decay mode requires non-universal boundary conditions within the MSSM framework to be available, since CMSSM yields ${\rm BR} (H^{\pm}\rightarrow \tilde{\chi}_{1}^{0}\tilde{\chi}_{1}^{\pm}) \lesssim 1\%$.} It can also be probed in near future collider experiments through the missing energy and CP-violation measurements...

Highlights

  • After the null results for the new physics, the current experiments have focused on the Higgs boson properties and analyses have been quite enlarged such that the Higgs boson couplings and decays are being studied precisely

  • We perform numerical analyses for the constrained minimal supersymmetric extension of the SM (MSSM) (CMSSM), NMSSM and Uð1Þ extended MSSM (UMSSM) to probe the allowed mass ranges for the charged Higgs boson and its possible decay modes as well as showing the allowed parameter spaces of these models

  • In addition to the charged Higgs boson, we find mt ≳ 2 TeV in CMSSM, while it can be as light as about 1 TeV in NMSSM and 500 GeV in UMSSM

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Summary

INTRODUCTION

After the null results for the new physics, the current experiments have focused on the Higgs boson properties and analyses have been quite enlarged such that the Higgs boson couplings and decays are being studied precisely. The second term in the square parentheses of Eq (18) reflects the contribution from the Uð1Þ0 sector, where gY0 is the gauge coupling associated with Uð1Þ0, QHu and QHd are the charges of Hu and Hd under the Uð1Þ0 group After these contributions, the tree-level Higgs boson mass can be obtained as large as about 140 GeV for low tan β, while it can be as heavy as about 115 GeV, when tan β is large [19]. In addition to the Higgs sector, the neutralino sector is enlarged in UMSSM Since it has a field whose VEV breaks Uð1Þ0 symmetry, its fermionic superpartner mixes with the MSSM neutralinos, as in the NMSSM case. Similar to NMSSM, UMSSM does not propose any new charged particle; the chargino sector remains the same as that in MSSM

SCANNING PROCEDURE AND EXPERIMENTAL CONSTRAINTS
FUNDAMENTAL PARAMETER SPACE AND MASS SPECTRUM
PRODUCTION AND DECAY MODES OF HÆ
Findings
CONCLUSION
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