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Related papers: Lepton Masses from a TeV Scale in a 3-3-1 Model

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We show that a TeV scale inverse seesaw model for neutrino masses can be realized within the framework of a supersymmetric SO(10) model consistent with gauge coupling unification and observed neutrino masses and mixing. We present our…

High Energy Physics - Phenomenology · Physics 2010-04-06 P. S. Bhupal Dev , R. N. Mohapatra

We consider a TeV scale resonant lepogenesis within type-I seesaw mechanism. We show that a concrete model based on $A_4$ flavor symmetry with a scaling ansatz in the neutrino Dirac mass matrix and a retro-circulant heavy Majorana mass…

High Energy Physics - Phenomenology · Physics 2021-12-03 H. B. Benaoum

In this talk, I present a new mechanism for the generation of neutrino masses via dimension 7 operators: llHH(H*H)/M^3. This leads to new formula for the light neutrino masses, m_\nu~v^4/M^3. This is distinct from the usual see-saw…

High Energy Physics - Phenomenology · Physics 2015-03-17 S. Nandi

Neutrino masses may be generated by the VEV of an $SU(2)_L$ Higgs triplet. We assume that the doubly charged component of such a triplet has a mass in the range of several 100 GeV, such that it is accessible at LHC. Its decay into like-sign…

High Energy Physics - Phenomenology · Physics 2009-01-06 Julia Garayoa , Thomas Schwetz

A simple extension of the Standard Model providing TeV scale seesaw mechanism is presented. Beside the Standard Model particles and right-handed Majorana neutrinos, the model contains a singly charged scalar, an extra Higgs doublet and…

High Energy Physics - Phenomenology · Physics 2010-11-03 Wei Chao

We develop a systematic procedure of constructing lepton mass matrices that satisfy all the experimental constraints in the light lepton sector of the minimal left-right symmetric model with type-I seesaw dominance. This method is unique…

High Energy Physics - Phenomenology · Physics 2017-06-08 Chang-Hun Lee

We explore a realistic supersymmetric SU(2)_L \times SU(2)_R \times U(1)_B-L model spontaneously broken at around 10^12 GeV. The presence of D and F-flat directions gives rise to TeV mass doubly charged particles which can be found at the…

High Energy Physics - Phenomenology · Physics 2011-05-12 Shahida Dar , Qaisar Shafi , Arunansu Sil

We propose a model with one large submm size extra dimension in which the gravity and right-handed (RH) neutrino propagate, but the three Standard Model (SM) families are confined to fat branes of TeV^(-1) size or smaller. The charged…

High Energy Physics - Phenomenology · Physics 2008-11-26 S. Nandi , C. M. Rujoiu

We explore an anomaly-free ${\textrm U}(1)$ gauge extended beyond the Standard model (BSM) framework, to account for the baryon asymmetry of the Universe, along with arranging for tiny neutrino mass. Neutrino masses are generated via…

High Energy Physics - Phenomenology · Physics 2023-05-03 Kuldeep Deka , Tanumoy Mandal , Ananya Mukherjee , Soumya Sadhukhan

The R-symmetry formalism is applied for the supersymmetric SU(3)_C X SU(3)_L X U(1)_X (3-3-1) model with right-handed neutrinos. For this kind of models, we study generalization of the MSSM relation among R-parity, spin and matter-parity.…

High Energy Physics - Phenomenology · Physics 2008-11-26 P. V. Dong , D. T. Huong , M. C. Rodriguez , H. N. Long

The mass matrices of the charged leptons and neutrinos, that had been derived in the framework of a Minimal S_3-invariant Extension of the Standard Model, are here reparametrized in terms of their eigenvalues. The neutrino mixing matrix,…

High Energy Physics - Phenomenology · Physics 2008-11-26 O. Felix , A. Mondragon , M. Mondragon , E. Peinado

We investigate the possibility of expressing the charged leptons and neutrino mass matrices as linear combinations of generators of a single finite group. Constraints imposed on the resulting mixing matrix by current data restrict the group…

High Energy Physics - Phenomenology · Physics 2015-06-17 G. K. Leontaris , N. D. Vlachos

The effects of heavy new particles beyond the Standard Model can be conveniently captured through higher-dimensional effective operators. As noted long ago by Weinberg, the amount of baryon and lepton number an operator can carry is…

High Energy Physics - Phenomenology · Physics 2025-08-08 Julian Heeck , Diana Sokhashvili

We consider a Majorana neutrino mass matrix $\mathcal{M}_\nu$ with $(\mathcal{M}_\nu)_{\mu\mu} = (\mathcal{M}_\nu)_{\tau\tau} = 0$, in the basis where the charged-lepton mass matrix is diagonal. We show that this pattern for the lepton mass…

High Energy Physics - Phenomenology · Physics 2011-07-19 W. Grimus , L. Lavoura

We propose a new model with the Majorana neutrino masses generated at two-loop level, in which the lepton number violation (LNV) processes, such as neutrinoless double beta decays, are mainly induced by the dimension-7 LNV effective…

High Energy Physics - Phenomenology · Physics 2015-07-14 Chao-Qiang Geng , Da Huang , Lu-Hsing Tsai , Qing Wang

We consider a left-right symmetric model with an $SU(2)_L$ and an $SU(2)_R$ scalar doublet but without the scalar bidoublet. The charged fermion masses in this model are generated via a universal seesaw mechanism. We add a set of three…

High Energy Physics - Phenomenology · Physics 2025-05-01 Zafri A. Borboruah , Lekhika Malhotra , Utkarsh Patel , Sudhanwa Patra , S. Uma Sankar

Some years ago it was shown by Ma that in the context of the electroweak standard model there are, at the tree level, only three ways to generate small neutrino masses by the see-saw mechanism via one effective dimension-five operator. Here…

High Energy Physics - Phenomenology · Physics 2009-11-07 J. C. Montero , C. A. de S. Pires , V. Pleitez

We propose a model of TeV-scale resonant leptogenesis based upon recent models of the generation of light neutrino masses from supersymmetry-breaking effects with TeV-scale right-handed (rhd) neutrinos, $N_i$. The model leads to naturally…

High Energy Physics - Phenomenology · Physics 2009-11-10 Thomas Hambye , John March-Russell , Stephen M. West

We propose novel tree level seesaw mechanism with TeV-scale vectorlike Dirac mediators that produce Majorana masses of the known neutrinos. The gauge quantum number assignment to the Dirac mediators allows them to belong to a weak triplet…

High Energy Physics - Phenomenology · Physics 2014-11-20 Ivica Picek , Branimir Radovcic

We propose two 3-3-1 models (with either neutral fermions or right-handed neutrinos) based on S_3 flavor symmetry responsible for fermion masses and mixings. The models can be distinguished upon the new charge embedding (\mathcal{L})…

High Energy Physics - Phenomenology · Physics 2012-03-07 P. V. Dong , H. N. Long , C. H. Nam , V. V. Vien
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