Radiative neutrino mass with electroweak scale Majorana dark matter in the Scotogenic model

Non-zero neutrino mass and dark matter (DM) overshadow the success of the Standard Model (SM) of particle physics. The most straightforward extension of the SM to explain these two issues is the Scotogenic model, where the SM particle spectrum extends with three isospin singlet right-handed neutrino...

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Main Authors: Avnish, Kirtiman Ghosh
Format: Article
Language:English
Published: Elsevier 2024-05-01
Series:Nuclear Physics B
Online Access:http://www.sciencedirect.com/science/article/pii/S0550321324000907
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author Avnish
Kirtiman Ghosh
author_facet Avnish
Kirtiman Ghosh
author_sort Avnish
collection DOAJ
description Non-zero neutrino mass and dark matter (DM) overshadow the success of the Standard Model (SM) of particle physics. The most straightforward extension of the SM to explain these two issues is the Scotogenic model, where the SM particle spectrum extends with three isospin singlet right-handed neutrinos and one doublet scalar, all odd under a Z2 symmetry. The neutrino masses and mixings result from the Weinberg operator induced at one-loop level. The particle spectrum of this model contains a few weakly interacting stable massive particles, each of which can be a good candidate for DM. In this work, we have considered the lightest right-handed neutrino as DM candidate. The Yukawa couplings that give rise to the observed flavor mixings in the neutrino sector also lead to flavor violation in the SM charged lepton sector and hence, get tightly constrained from the charged lepton flavor violating (CLFV) observables. The same Yukawa couplings also contribute to the DM annihilation in the early universe and hence, determine the relic density of the DM. In this work, we address the tension between the constraints from CLFV observables and measured DM relic density to obtain the large Yukawa couplings with the help of a parameterization that reduces the phenomenology relevant parameters to merely three and enhances the detection prospect at the collider experiments. We have explored the parameter space consistent with current CLFV bounds, the observed DM relic density, and the absolute neutrino mass limit. To search for these scenarios, we have identified two promising signals at the proposed lepton colliders: the mono-photon plus missing energy and di-lepton plus missing energy signals. We have studied the collider phenomenology of these signatures and estimated the 5σ detection required luminosity for the center of mass energies at 500 GeV and 1 TeV.
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spelling doaj.art-7268943e8e1c44d4848209eb0956224a2024-03-30T04:38:44ZengElsevierNuclear Physics B0550-32132024-05-011002116524Radiative neutrino mass with electroweak scale Majorana dark matter in the Scotogenic model Avnish0Kirtiman Ghosh1Institute of Physics, Bhubaneswar, Sachivalaya Marg, Sainik School, Bhubaneswar 751005, India; Homi Bhabha National Institute, Training School Complex, Anushakti Nagar, Mumbai 400094, India; Corresponding author.Institute of Physics, Bhubaneswar, Sachivalaya Marg, Sainik School, Bhubaneswar 751005, India; Homi Bhabha National Institute, Training School Complex, Anushakti Nagar, Mumbai 400094, IndiaNon-zero neutrino mass and dark matter (DM) overshadow the success of the Standard Model (SM) of particle physics. The most straightforward extension of the SM to explain these two issues is the Scotogenic model, where the SM particle spectrum extends with three isospin singlet right-handed neutrinos and one doublet scalar, all odd under a Z2 symmetry. The neutrino masses and mixings result from the Weinberg operator induced at one-loop level. The particle spectrum of this model contains a few weakly interacting stable massive particles, each of which can be a good candidate for DM. In this work, we have considered the lightest right-handed neutrino as DM candidate. The Yukawa couplings that give rise to the observed flavor mixings in the neutrino sector also lead to flavor violation in the SM charged lepton sector and hence, get tightly constrained from the charged lepton flavor violating (CLFV) observables. The same Yukawa couplings also contribute to the DM annihilation in the early universe and hence, determine the relic density of the DM. In this work, we address the tension between the constraints from CLFV observables and measured DM relic density to obtain the large Yukawa couplings with the help of a parameterization that reduces the phenomenology relevant parameters to merely three and enhances the detection prospect at the collider experiments. We have explored the parameter space consistent with current CLFV bounds, the observed DM relic density, and the absolute neutrino mass limit. To search for these scenarios, we have identified two promising signals at the proposed lepton colliders: the mono-photon plus missing energy and di-lepton plus missing energy signals. We have studied the collider phenomenology of these signatures and estimated the 5σ detection required luminosity for the center of mass energies at 500 GeV and 1 TeV.http://www.sciencedirect.com/science/article/pii/S0550321324000907
spellingShingle Avnish
Kirtiman Ghosh
Radiative neutrino mass with electroweak scale Majorana dark matter in the Scotogenic model
Nuclear Physics B
title Radiative neutrino mass with electroweak scale Majorana dark matter in the Scotogenic model
title_full Radiative neutrino mass with electroweak scale Majorana dark matter in the Scotogenic model
title_fullStr Radiative neutrino mass with electroweak scale Majorana dark matter in the Scotogenic model
title_full_unstemmed Radiative neutrino mass with electroweak scale Majorana dark matter in the Scotogenic model
title_short Radiative neutrino mass with electroweak scale Majorana dark matter in the Scotogenic model
title_sort radiative neutrino mass with electroweak scale majorana dark matter in the scotogenic model
url http://www.sciencedirect.com/science/article/pii/S0550321324000907
work_keys_str_mv AT avnish radiativeneutrinomasswithelectroweakscalemajoranadarkmatterinthescotogenicmodel
AT kirtimanghosh radiativeneutrinomasswithelectroweakscalemajoranadarkmatterinthescotogenicmodel