Abstract

In this study we explore the LHC's Run II potential to the discovery of heavy Majorana neutrinos, with luminosities between $30$ and $3000$ fb$^{-1}$ in the $l^{\pm}l^{\pm}j~j$ final state. Given that there exist many models for neutrino mass generation, even within the Type I seesaw framework, we use a simplified model approach and study two simple extensions to the Standard Model, one with a single heavy Majorana neutrino, singlet under the Standard Model gauge group, and a limiting case of the left-right symmetric model. We then extend the analysis to a future hadron collider running at $100$ TeV center of mass energies. This extrapolation in energy allows us to study the relative importance of the resonant production versus gauge boson fusion processes in the study of Majorana neutrinos at hadron colliders. We analyze and propose different search strategies designed to maximize the discovery potential in either the resonant production or the gauge boson fusion modes.

Highlights

  • Within the SM, lepton number violating processes are absent at zero temperature

  • In this study we explore the LHC’s Run II potential to the discovery of heavy Majorana neutrinos, with luminosities between 30 and 3000 fb−1 in the l±l±j j final state

  • This extrapolation in energy allows us to study the relative importance of the resonant production versus gauge boson fusion processes in the study of Majorana neutrinos at hadron colliders

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Summary

Two simplified models

To study same-sign leptons production in association with jets at the LHC run II and future higher energy colliders, we examine two simplified models that give rise to this final. The first one consists only of SM gauge interactions and the only added new degree of freedom is the singlet heavy Majorana NR fermion which mixes with the 3 active SM neutrinos. The mass of NR and its mixing with the active neutrinos are taken to be free parameters. The second model implements an additional SU(2) gauge symmetry under which the right-handed leptons and quarks are charged unlike the lefthanded chirality. NR partners with the right-handed charged leptons. This can be part of a left-right symmetric model that can give rise to realistic masses for the active neutrinos. We review different aspect of these two theoretical approaches and indicate how they can be related to more complete models

Single Majorana fermion extension to the standard model
Gauge bosons beyond the Standard Model
Constraints
Background
Left-right symmetric model: collider reach at 13 and 100 TeV
Discussion
A T-channel amplitudes
Findings
B The E 4-particle kinematical variable
Full Text
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