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We propose a model of neutrino mass matrix with large $SU(2)$ multiplets and gauged $U(1)_{L_\mu - L_\tau}$ symmetry, in which we introduce $SU(2)$ quartet scalar and quintet fermions with nonzero $L_\mu - L_\tau$ charge. Then we…

High Energy Physics - Phenomenology · Physics 2018-07-18 Takaaki Nomura , Hiroshi Okada

We construct a scotogenic neutrino mass model introducing large $SU(2)_L$ multiplet fields without adding an extra symmetry. We have introduced extra scalar fields such as a septet, quintet and quartet where we make the vacuum expectation…

High Energy Physics - Phenomenology · Physics 2020-11-26 Nilanjana Kumar , Takaaki Nomura , Hiroshi Okada

We propose an inverse seesaw model with large $SU(2)_L$ multiplet fields which realizes natural mass hierarchies among neutral fermions. Here, lighter neutral fermion mass matrices are induced via two suppression mechanisms; one is small…

High Energy Physics - Phenomenology · Physics 2019-04-10 Takaaki Nomura , Hiroshi Okada

We propose a one-loop neutrino mass model with several $SU(2)_L$ multiplet fermions and scalar fields in which the inert feature of a scalar to realize the one-loop neutrino mass can be achieved by the cancellation among Higgs couplings…

High Energy Physics - Phenomenology · Physics 2019-06-26 Takaaki Nomura , Hiroshi Okada

We propose an inverse seesaw model with large $SU(2)_L$ multiplets applying modular $A_4$ symmetry where $SU(2)_L$ quartet and septet fermions are introduced as triplets under the symmetry. The neutral components of the quartet contribute…

High Energy Physics - Phenomenology · Physics 2020-07-31 Takaaki Nomura , Hiroshi Okada

We propose a model based on the $SU(5)$ grand unification with an extra $A_{4}\otimes Z_{2}\otimes Z_{2}^{\prime }\otimes Z_{2}^{\prime \prime}\otimes U\left( 1\right) _{f}$ flavor symmetry, which accounts for the pattern of the SM fermion…

High Energy Physics - Phenomenology · Physics 2015-06-19 Miguel D. Campos , A. E. Cárcamo Hernández , S. Kovalenko , Iván Schmidt , Erik Schumacher

Motivated by the Super-Kamiokande data, we revisit models with U(1) symmetries and discuss the origin of neutrino masses and mixings in such theories. We show that, in models with just three light neutrinos and a hierarchy of neutrino…

High Energy Physics - Phenomenology · Physics 2009-10-31 Smaragda Lola , Graham G. Ross

We construct two viable extensions of the SM with a heavy vector in the fundamental $SU\left( 2\right) _{L}$ representation and nine SM singlet scalar fields, consistent with the current SM fermion mass spectrum and fermionic mixing…

High Energy Physics - Phenomenology · Physics 2019-09-24 A. E. Cárcamo Hernández , Jonatan Vignatti , Alfonso Zerwekh

The addition of gauge singlet fermions to the Standard Model Lagrangian renders the neutrinos massive and allows one to explain all that is experimentally known about neutrino masses and lepton mixing by varying the values of the Majorana…

High Energy Physics - Phenomenology · Physics 2009-10-29 Andre de Gouvea , Wei-Chih Huang , James Jenkins

In SU(3)_L x U(1)_N gauge models for electroweak interactions, we discuss how to implement a radiative mechanism of generating Majorana neutrino masses by considering the property that the Higgs scalar, which has a coupling to a charged…

High Energy Physics - Phenomenology · Physics 2009-10-31 Yutaka Okamoto , Masaki Yasue

We explore generating the dimension five operator leading to neutrino masses by integrating out heavy SU(2)_L triplet fermions. We exhibit a model that has a neutrino mass matrix consistent with observations. In addition, the model is…

High Energy Physics - Phenomenology · Physics 2008-12-30 Willy Fischler , Raphael Flauger

We propose a realistic model with Majorana neutrinos in the framework of unifying the three generations of fermions by point interactions in an extra dimension. This model can simultaneously explain the origin of fermion generations,…

High Energy Physics - Phenomenology · Physics 2016-02-15 Chengfeng Cai , Hong-Hao Zhang

We have studied the most general neutrino mass matrices in models with SU(2) and SU(3) horizontal symmetries. Without going into the details of the models it is possible to write down the effective operators, which predict the structure of…

High Energy Physics - Phenomenology · Physics 2009-11-07 Asim K. Ray , Utpal Sarkar

We propose a natural realization of linear seesaw model with hidden gauge symmetry in which $SU(2)_L$ triplet fermions, one extra Higgs singlet, doublet and quartet scalar are introduced. Small neutrino mass can be realized by two…

High Energy Physics - Phenomenology · Physics 2019-04-03 Takaaki Nomura , Hiroshi Okada

Assuming three light neutrinos and the see-saw mechanism we present a semiquantitative model of fermion masses based on (SUSY) SU(5) and abelian horizontal charges. A good description of the observed pattern of quark and lepton masses is…

High Energy Physics - Phenomenology · Physics 2008-11-26 Guido Altarelli , Ferruccio Feruglio

The fact that neutrinos are massive suggests that the minimal supersymmetric standard model (MSSM) might be extended in order to include three gauge-singlet neutrino superfields with Yukawa couplings of the type $H_2 L \nu^c$. We propose to…

High Energy Physics - Phenomenology · Physics 2009-11-11 D. E. Lopez-Fogliani , C. Munoz

We study the generation of neutrino masses in the $SU(3)_W$ electroweak unified theory in $M_4\times S_1/(Z_2\times Z'_2)$ spacetime. By appropriate orbifolding, the bulk symmetry $SU(3)_W$ is broken into $SU(2)_L \times U(1)_Y$ at one of…

High Energy Physics - Phenomenology · Physics 2011-07-19 Chia-Hung V. Chang , We-Fu Chang , John N. Ng

We consider an extension of the standard model (SM) with an inert Higgs doublet and three Majorana singlet fermions to address both origin and the smallness of neutrino masses and dark matter (DM) problems. In this setup, the lightest…

High Energy Physics - Phenomenology · Physics 2018-05-22 Amine Ahriche , Adil Jueid , Salah Nasri

We study a model which generates Majorana neutrino masses at tree-level via low-energy effective operator with mass-dimension-9. Introduction of such a higher dimensional operator brings down the lepton number violating mass scale to TeV…

High Energy Physics - Phenomenology · Physics 2026-03-23 Saiyad Ashanujjaman , Kirtiman Ghosh

We study a model in which lepton number violation is solely triggered by a dimension 4 hard breaking term in the scalar potential. A minimal model which contains a SU(2) triplet with hypercharge Y=2, and a pair of singlet doubly charged…

High Energy Physics - Phenomenology · Physics 2008-11-26 Chian-Shu Chen , C. Q. Geng , J. N. Ng
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