Abstract

Abstract An interesting feature of the next-to-minimal supersymmetric standard model (NMSSM) is that one or more Higgs bosons may be comparably light ( ${M_{{{H_i}}}} < {M_Z}$ ) without being in conflict with current experimental bounds. Due to a large singlet component, their direct production in standard channels at the Large Hadron Collider (LHC) is suppressed. We demonstrate that there are good prospects for observing such a light Higgs boson in decays of heavy neutralinos and charginos. We consider an example scenario with $20\,GeV < {M_H}_{{_1}} < {M_Z}$ and show that a large fraction of the cascade decays of gluinos and squarks involves the production of at least one Higgs boson. Performing a Monte Carlo analysis at the level of fast detector simulation, it is demonstrated how the Higgs signal can be separated from the main backgrounds, giving access to the Yukawa coupling of the Higgs to bottom quarks. Analyzing the resulting $b\overline b$ mass spectrum could provide an opportunity for light Higgs boson discovery already with 5 fb−1 of LHC data at 7 TeV.

Highlights

  • The right size can be generated dynamically from supersymmetry-breaking operators

  • In our analysis we investigate the prospects for production of light CP-even Higgs bosons in the next-to-minimal supersymmetric standard model (NMSSM) through cascade decays of heavy SUSY particles at the Large Hadron Collider (LHC)

  • The NMSSM is both theoretically appealing as an extension of the SM and interesting phenomenologically, as its spectrum may contain Higgs bosons with mass much below the limits in the SM or the MSSM

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Summary

The next-to-minimal supersymmetric standard model

We review briefly the elements of the NMSSM which differ from the MSSM. Our conventions for the other sectors — that remain unchanged when going to the NMSSM — follow those of [37, 38]

The Higgs sector
The neutralino sector
The squark sector
Scenarios with light Higgs bosons
Standard channels
SUSY cascades
LHC analysis
Event generation
Backgrounds
Event selection
Background
TeV 14 TeV
Results
Summary and conclusions
Full Text
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