Abstract

We develop a low scale left-right symmetric model based on $SU(3)_C\times SU(2)_L\times SU(2)_R\times U(1)_{B-L}\times Z_2$ with a simplified Higgs sector consisting of only one bidoublet and one $SU(2)_R$ doublet. In this model, the tiny values of light neutrino masses are generated through an inverse-seesaw mechanism. We emphasize that in this setup, the tree-level flavor changing neutral current can be strongly suppressed, consistent with the current experimental constraints. We show that the lightest $CP$-even Higgs boson, which is like the standard model Higgs boson, and the next lightest Higgs boson, $h'$, are generated from the neutral components of the bidoublet. We show that the mass of the next lightest Higgs boson can be of an order a few hundred~\text{GeVs}. We analyze the detection of $h'$ at the Large Hadron Collider (LHC) for a center-of-mass energy $\sqrt{s}=14~\text{TeV}$ and integrated luminosity $L_{\text{int}}=300~{\text{fb}}^{-1}$ via di-Higgs channel: $h'\to hh\to b\bar{b}\gamma\gamma$ and also in the $ZZ$ channel: $h'\to ZZ\to 4\ell~(\ell=e,~\mu)$ at an integrated luminosity $L_{\text{int}}=3000~{\text{fb}}^{-1}$. We consider three benchmark points for this analysis with $m_{h'}=250~\text{GeV},~400~\text{GeV}$, and $600~\text{GeV}$. We show that promising signals with good statistical significances can be obtained in di-Higgs channel, with $2\gamma+2b$-jets final states.

Highlights

  • The Standard Model (SM) of particle physics is in an excellent agreement with most of the confirmed experimental results

  • We show that the lightest CP-even Higgs boson, which is like the standard model Higgs boson, and the lightest Higgs boson, h0, are generated from the neutral components of the bidoublet

  • After imposing various sets of cuts to reduce bpacffiffikffi grounds (B) and improve the statistical significance ðS= BÞ, where S refers to the signal, we find that the SM-like Higgs pair production, with bbγγ final states, is the most promising channel for probing our heavy Higgs boson at the Large Hadron Collider (LHC)

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Summary

INTRODUCTION

The Standard Model (SM) of particle physics is in an excellent agreement with most of the confirmed experimental results. We consider an example of a LR model, with a Higgs sector consisting of one scalar bidoublet and a scalar right-handed doublet In this case and in order to generate light neutrino masses, we adopt the inverse-seesaw (IS) mechanism [15,16,17,18,19]. The IS mechanism is quite motivated by having the TeV scale LR model that can be probed in current and future colliders, while in the conventional LR model, the GUT scale is the typical scale of breaking LR symmetry, where right-handed neutrino masses are generated. The physical fermions’ masses are given after diagonalization by Mduiag 1⁄4 VuL†M0uVuR; Mdliag These Yukawa couplings lead to the following interactions between quarks and neutral Higgs bosons: pffiffi

LCKM M ddiag V
HIGGS SECTOR IN THE LRIS
Higgs masses and mixing
Charged Higgs bosons
CP-odd Higgs bosons
SEARCH FOR HEAVY HIGGS BOSONS AT THE LHC
Findings
CONCLUSIONS
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