Abstract

We investigate the production and decays of doubly-charged Higgs bosons for the Type-II seesaw mechanism at an $e^{+} e^{-}$ collider with two center of mass energies, $\sqrt{s}=380$ GeV and 3 TeV, and analyze the fully hadronic final states in detail. Lower mass ranges can be probed during the 380 GeV run of the collider, while high mass ranges, which are beyond the 13 TeV Large Hadron Collider discovery reach, can be probed with $\sqrt{s}=3$ TeV. For such a heavy Higgs boson, the final decay products are collimated, resulting in fat-jets. We perform a substructure analysis to reduce the background and find that a doubly-charged Higgs boson in the mass range 800-1120 GeV can be discovered during the 3 TeV run, with integrated luminosity $\mathcal{L} \sim 95\, \rm{fb}^{-1}$ of data. For 380 GeV center of mass energy, we find that for the doubly-charged Higgs boson in the range 160-172 GeV, a $5\sigma$ significance can be achieved with only integrated luminosity $\mathcal{L} \sim 24 \, \rm{fb}^{-1}$. Therefore, a light Higgs boson can be discovered immediately during the run of a future $e^{+} e^{-}$ collider.

Highlights

  • With the discovery of the Higgs boson at the Large Hadron Collider (LHC), we start to develop an understanding of how the standard model (SM) fermion and gauge boson masses are generated in terms of the BroutEnglert-Higgs (BEH) mechanism

  • We find that a heavy Higgs boson with a mass up to 1120 GeV can be most optimally discovered with 5σ significance at the 3 TeV run of CLIC with 95 fb−1 of data

  • The Type-II seesaw model consists of an extension of the scalar sector by a Higgs triplet field Δ with hypercharge Y 1⁄4 þ2

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Summary

INTRODUCTION

With the discovery of the Higgs boson at the Large Hadron Collider (LHC), we start to develop an understanding of how the standard model (SM) fermion and gauge boson masses are generated in terms of the BroutEnglert-Higgs (BEH) mechanism. The same Yukawa interaction between the lepton doublet and the triplet scalar field generates Majorana masses for the neutrinos, and dictates the phenomenology of the charged Higgs bosons. [33,34] This is only relevant for a very tiny vev vΔ < 10−4 GeV, where the doubly-charged Higgs boson decays into the same-sign dilepton with 100% branching ratio. For the other SM and BSM searches at CLIC and other linear colliders, see [47,53,54,55,56,57,58,59,60,61,62,63,64,65,66,67] for Higgs physics and effective field theory, [68,69,70,71,72] for different BSM scenarios, and [73,74,75,76,77,78,79,80] for seesaw and radiative neutrino mass model searches.

MODEL DESCRIPTION
DECAY MODES AND EXPERIMENTAL CONSTRAINTS
LARGE TRIPLET VEV AND COLLIDER SIGNATURES
DISCUSSION AND CONCLUSIONS
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