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In this work we show that we can generate neutrino masses through the type-II see-saw mechanism working at TeV scale in the context of a 331 model.

High Energy Physics - Phenomenology · Physics 2014-11-17 J. C. Montero , C. A. de S. Pires , V. Pleitez

We study a scale invariant inverse seesaw model that radiatively generates the electroweak scale, the Standard Model (SM) neutrino masses, and stabilizes the electroweak vacuum. Previous studies have noted that the SM Higgs potential and…

High Energy Physics - Phenomenology · Physics 2025-11-07 Aqeel Ahmed , Juan P. Garcés , Manfred Lindner

The triplet or type-II seesaw mechanism is the simplest way to endow neutrinos with mass in the Standard Model (SM). Here we review its associated theory and phenomenology, including restrictions from $S$, $T$, $U$ parameters, neutrino…

High Energy Physics - Phenomenology · Physics 2022-06-01 Sanjoy Mandal , O. G. Miranda , G. Sanchez Garcia , J. W. F. Valle , Xun-Jie Xu

The type II seesaw mechanism is an attractive way to generate the observed light neutrino masses. It postulates a SU(2)$_\mathrm{L}$-triplet scalar field, which develops an induced vacuum expectation value after electroweak symmetry…

High Energy Physics - Phenomenology · Physics 2019-03-01 Stefan Antusch , Oliver Fischer , A. Hammad , Christiane Scherb

We propose a Standard Model (SM) extension where neutrinos get masses through a two-loop inverse seesaw mechanism. This naturally explains the smallness of the neutrino masses and allows seesaw mediators to be at the TeV scale with testable…

With just the Standard Model Higgs doublet, there are only three types of seesaw models that generate light Majorana neutrino masses at tree level after electroweak spontaneous symmetry breaking. However, if there exist additional TeV…

High Energy Physics - Phenomenology · Physics 2024-08-13 Alessio Giarnetti , Juan Herrero-Garcia , Simone Marciano , Davide Meloni , Drona Vatsyayan

We consider different extensions of the standard model which can give rise to the small active neutrino masses through seesaw mechanisms, and their mixing. These tiny neutrino masses are generated at some high energy scale by the heavy…

High Energy Physics - Phenomenology · Physics 2015-03-17 Shamayita Ray

We present a ``gravity-induced'' seesaw mechanism, which accommodates neutrino masses ($m_\nu\propto m_u^2/M_I$, with $m_u$ the corresponding quark mass and $M_I\simeq 4\times10^{11}$ GeV) compatible with the MSW study of the Solar neutrino…

High Energy Physics - Phenomenology · Physics 2007-05-23 Mirjam Cvetic

We investigate an alternative seesaw mechanism for neutrino mass generation. Neutrino mass is generated at loop level but the basic concept of usual seesaw mechanism is kept. One simple model is constructed to show how this mechanism is…

High Energy Physics - Phenomenology · Physics 2011-02-24 Zhi-jian Tao

Alternatives to the see-saw mechanism are explored in supersymmetric models with three right-handed or sterile neutrinos. Tree-level Yukawa couplings can be drastically suppressed in a natural way to give sub-eV Dirac neutrino masses. If,…

High Energy Physics - Phenomenology · Physics 2009-09-29 Francesca Borzumati , Yasunori Nomura

Two Higgs Doublet Models (2HDM) are popular extensions of the Standard Model for several reasons, but do not explain neutrino masses. In this work, we investigate how one can incorporate neutrino masses within the framework of the…

High Energy Physics - Phenomenology · Physics 2019-07-31 D. Cogollo , Ricardo D. Matheus , Tessio B. de Melo , Farinaldo S. Queiroz

One of the interesting properties of the NMSSM is that it can accommodate a light pseudoscalar of order 10 GeV. However, such scenarios are challenged by several experimental constraints, especially those related to the fermionic decays of…

High Energy Physics - Phenomenology · Physics 2011-07-15 Asmaa Abada , Gautam Bhattacharyya , Debottam Das , Cédric Weiland

If there is no new physics beyond the TeV energy scale, such as in a theory of large extra dimensions, the smallness of the seesaw neutrino mass, i.e. $m_\nu = m_D^2/m_N$, cannot be explained by a very large $m_N$. In contrast to previous…

High Energy Physics - Phenomenology · Physics 2009-10-31 Ernest Ma

We propose a model for leptons based on the smallest modular finite group $\Gamma_2\cong S_3$ that, for the first time, accounts for both the hints of large low-energy CP-violation in the lepton sector and the matter-antimatter asymmetry of…

High Energy Physics - Phenomenology · Physics 2024-05-09 Simone Marciano , Davide Meloni , Matteo Parriciatu

We consider a version of the low-scale type I seesaw mechanism for generating small neutrino masses, as an alternative to the standard seesaw scenario. It involves two right-handed (RH) neutrinos $\nu_{1R}$ and $\nu_{2R}$ having a Majorana…

High Energy Physics - Phenomenology · Physics 2018-04-27 J. T. Penedo , S. T. Petcov , Tsutomu T. Yanagida

We suggest new simple model of generating tiny neutrino masses through a TeV-scale seesaw mechanism without requiring tiny Yukawa couplings. This model is a simple extension of the standard model by introducing extra one Higgs singlet, and…

High Energy Physics - Phenomenology · Physics 2014-11-21 Naoyuki Haba , Masaki Hirotsu

After the LHC is turning on and accumulating more data, the TeV scale seesaw mechanisms for small neutrino masses in the form of inverse seesaw mechanisms are gaining more and more attention once they provide neutrino masses at sub-eV scale…

High Energy Physics - Phenomenology · Physics 2019-08-14 Carlos Antônio de Sousa Pires , Felipe Ferreira de Freitas , Jing Shu , Li Huang , Pablo Wagner Vasconcelos Olegário

Given that the two-Higgs-doublet model of type III (2HDM-III) has the potential to address the $R_{D^{(\ast)}}$ anomalies while the resolution to the $R_{K^{(\ast)}}$ deficits requires new degrees of freedom within this framework, we…

High Energy Physics - Phenomenology · Physics 2018-10-17 Shao-Ping Li , Xin-Qiang Li , Ya-Dong Yang , Xin Zhang

We propose an extension of the standard model with a B-L global symmetry that is broken softly at the TeV scale. The neutrinos acquire masses through a type-II seesaw while the lepton (L) asymmetry arises in the {\it singlet sector} but…

High Energy Physics - Phenomenology · Physics 2010-05-27 John McDonald , Narendra Sahu , Utpal Sarkar

The quasi-degeneracy of heavier sterile neutrino masses in the Neutrino Minimal Standard Model ($\nu$MSM) facilitates the production of lepton asymmetry below the electroweak scale. The first order loop corrections to this mass-difference…

High Energy Physics - Phenomenology · Physics 2010-06-22 Ananda Roy