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In this talk we explore the possibility that the smallness of the observed neutrino masses is naturally understood in a modified version of the standard model with N extra generations of fermions and N right-handed neutrinos, in which light…

High Energy Physics - Phenomenology · Physics 2014-10-15 A. Aparici , J. Herrero-Garcia , N. Rius , A. Santamaria

Using a low-energy effective field theory approach, we study some properties of models with large extra dimensions, in which quarks and leptons have localized wave functions in the extra dimensions. We consider models with two types of…

High Energy Physics - Phenomenology · Physics 2021-01-22 S. Girmohanta , R. N. Mohapatra , R. Shrock

The Standard Model has three generations of fermions and although it does not contain any explicit reason for this, the existence of additional generations is now very constrained by experiment. Present measurements are saturating…

High Energy Physics - Phenomenology · Physics 2014-12-17 Alfredo Aranda , Jose A. R. Cembranos

We investigate an one loop radiative neutrino mass model, where the loop particles, notably a singlet fermion ($\chi$), a doublet fermion ($\Psi$) and three generations of singlet scalars ($\phi_i, i=\{1,2,3\}$) are assumed to be odd under…

High Energy Physics - Phenomenology · Physics 2025-11-25 Ujjal Kumar Dey , Santu Kumar Manna , Partha Kumar Paul , Sujit Kumar Sahoo , Narendra Sahu

One of the most important discoveries in particle physics is the observation of nonzero neutrino masses, which dictates that the Standard Model (SM) is incomplete. Moreover, several pieces of evidence of lepton flavor universality violation…

High Energy Physics - Phenomenology · Physics 2022-09-15 J. Julio , Shaikh Saad , Anil Thapa

A brief review of the assignment of elementary fermions and bosons to irreducible multiplets in grand unified $E_6$ models is followed by a discussion of different, hierarchical symmetry breaking chains from $E_6$ down to $SU(3)_C \times…

High Energy Physics - Phenomenology · Physics 2018-05-23 Secil Benli , Tekin Dereli

We propose a leptoquark model with two scalar leptoquarks $S^{}_1 \left( \bar{3},1,\frac{1}{3} \right)$ and $\widetilde{R}^{}_2 \left(3,2,\frac{1}{6} \right)$ to give a combined explanation of neutrino masses, lepton flavor mixing and the…

High Energy Physics - Phenomenology · Physics 2021-07-28 Di Zhang

In this work, we try to explain the neutrino mass and mixing data radiatively at three-loop by extending the standard model (SM) with two charged singlet scalars and three right handed (RH) neutrinos. Here, the lightest RH neutrino is a…

High Energy Physics - Phenomenology · Physics 2015-06-22 Amine Ahriche , Salah Nasri

An anomaly-free U(1) gauge extension of the standard model (SM) is presented. Only one Higgs doublet with a nonzero vacuum expectation is required as in the SM. New fermions and scalars as well as all SM particles transform nontrivially…

High Energy Physics - Phenomenology · Physics 2016-02-23 Rathin Adhikari , Debasish Borah , Ernest Ma

We consider the simplest extension of the standard electroweak model by one sterile neutrino that allows for neutrino masses and mixing. We find that its leptonic sector contains much less free physical parameters than previously realized.…

High Energy Physics - Phenomenology · Physics 2011-09-13 Yi Liao

In the recent note we argued that most of the available positive and negative neutrino oscillation data can be incorporated in a four-neutrino weak interaction model with one physical condition: thorough maximal mixing of the neutrino…

High Energy Physics - Phenomenology · Physics 2007-05-23 E. M. Lipmanov

We consider the neutrino physics of models with a sequentially broken U(2) flavor symmetry. Such theories yield the observed pattern of quark and lepton masses, while maintaining sufficient degeneracies between superparticles of the first…

High Energy Physics - Phenomenology · Physics 2014-11-17 Christopher D. Carone , Lawrence J. Hall

We study a $U(1)_{B-L}$ extension of the Standard Model (SM) in which Dirac neutrino masses are generated radiatively at the one-loop level through the exchange of new beyond the SM fields. This framework establishes a direct connection…

High Energy Physics - Phenomenology · Physics 2026-01-28 Chayan Majumdar , Utkarsh Patel , Supriya Senapati , Sudhanwa Patra

The Dualized Standard Model has scored a number of successes in explaining the fermion mass hierarchy and mixing pattern. This note contains updates to those results including (a) an improved treatment of neutrino oscillation free from…

High Energy Physics - Phenomenology · Physics 2009-11-10 J Bordes , HM Chan , ST Tsou

In this work we prob a class of neutrino mass models at both Large Hadron Collider (LHC) energies 8 TeV and 14 TeV. The focus will be on the new introduced interaction terms between a singlet charged scalar, $S^{\pm}$, and leptons leading…

High Energy Physics - Phenomenology · Physics 2016-11-23 Chahrazed Guella , Dounia Cherigui , Amine Ahriche , Salah Nasri , Rachik Soualah

The mass matrices of charged fermions have a simple structure if expressed in powers of the small parameter sigma=(m_c/m_t)^{1/2}. It is suggested that the mass matrix of the three heavy neutrinos occuring in grand unified theories can be…

High Energy Physics - Phenomenology · Physics 2009-10-31 B. Stech

The Georgi-Glashow model is the simplest possible attempt at grand unification. However, due to its particle content, the model preserves a global $U(1)_{B-L}$ symmetry, where $B$ and $L$ are baryon and lepton numbers, respectively. It thus…

High Energy Physics - Phenomenology · Physics 2026-05-28 Ilja Dorsner , Svjetlana Fajfer , Shaikh Saad

By using the $L_e$ - $L_\mu$ - $L_\tau$ symmetry, we construct an $SU(3)_L\times U(1)_N$ gauge model that provides two-loop radiative neutrino masses as well as one-loop radiative neutrino masses. The generic smallness of two-loop neutrino…

High Energy Physics - Phenomenology · Physics 2009-10-31 Teruyuki Kitabayashi , Masaki Yasue

We propose a supersymmetric extra U(1) model, which can generate small neutrino masses and necessary $\mu$ terms, simultaneously. Fields including quarks and leptons are embedded in three ${\bf 27}$s of $E_6$ in a different way among…

High Energy Physics - Phenomenology · Physics 2014-11-20 Daijiro Suematsu , Takashi Toma , Tetsuro Yoshida

We present radiative one-loop neutrino mass model with hypercharge zero scalar triplet in conjunction with another charged singlet scalar and an additional vectorlike lepton doublet. We study three variants of this mass model: the first one…

High Energy Physics - Phenomenology · Physics 2013-12-23 Vedran Brdar , Ivica Picek , Branimir Radovcic