Abstract

The extension of the Standard Model (SM) with two complex $SU(2)_{L}$ scalar triplets enables one to have the Type II seesaw mechanism operative consistently with texture-zero neutrino mass matrices. This framework predicts additional doubly charged, singly charged and neutral spinless states. We show that, for certain values of the model parameters, there is sufficient mass splitting between the two doubly charged states ( $H_1^{\pm\pm}, H_2^{\pm\pm}$) that allows the decay $H_1^{\pm\pm} \to H_2^{\pm\pm} h $, and thus leads to a unique signature of this scenario. We show that the final state $2(\ell^{\pm} \ell^{\pm}) + 4b + \mET~$ arising from this mode can be observed at the high energy, high luminosity (HE-HL) run of the 14 TeV Large Hadron Collider (LHC), and also at a 100 TeV Future Circular Collider (FCC-hh).

Highlights

  • We show that the final state 2ðlÆlÆÞ þ 4b þ =ET arising from this mode can be observed at the high energy, high luminosity (HE-HL) run of the 14 TeV Large Hadron Collider (LHC), and at a 100 TeV Future Circular Collider (FCC-hh)

  • A 125 GeV scalar, with a striking resemblance to the Higgs boson proposed in the standard model (SM) has been observed at the Large Hadron Collider (LHC) [1,2]

  • We have extended the Type-II seesaw model with an extra SUð2ÞL complex triplet scalar and allow a small mixing of the triplets with the SM Higgs doublet as required by electroweak precision measurements

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Summary

INTRODUCTION

A 125 GeV scalar, with a striking resemblance to the Higgs boson proposed in the standard model (SM) has been observed at the Large Hadron Collider (LHC) [1,2]. There is no such bound yet on doubly charged scalar mass for w > 10−4 GeV [29] This is because (a) a relatively large triplet vev implies small ΔL 1⁄4 2 Yukawa couplings from a consideration of neutrino masses, and (b) overcoming standard model (SM) backgrounds for the final state driven by same-sign W-pairs is a challenging task, and requires a large integrated luminosity. One class of such models consists of zero textures, having some vanishing entries in the mass matrix, leading to relations between mass eigenvalues and mixing angles, and ensuring better predictiveness in the neutrino sector It has been shown, that zero textures are inconsistent with Type-II seesaw models with a single scalar triplet [43]. The decay mode Δþþ → ΔþWþ is kinematically not allowed with a single triplet scalar

EXTENSION WITH TWO TRIPLETS
CA: ð25Þ
ANALYSIS
Benchmark points
C1–2 C1–3 C1–4 C1–5 C1–6 C1–7
C2–4 C2–5 C2–6 C2–7 C2–8 tt þ WÆ tt þ Z tt þ h
CONCLUSION
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