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Related papers: Neutrino Mass in TeV-Scale New Physics Models

200 papers

We propose a model for neutrino mass generation in wich no physics beyond a TeV is required. We extend the standard model by adding two charged singlet fields with lepton number two. Dirac neutrino masses $m_{\nu_D} \leq MeV$ are generated…

High Energy Physics - Phenomenology · Physics 2009-11-07 Salah Nasri , Sherif Moussa

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

Neutrino mass generation may affect the basic structure of the electroweak symmetry breaking sector. We consider a broad class of elementary particle theories where neutrinos get mass at a low mass scale. We show how these can be made…

High Energy Physics - Phenomenology · Physics 2007-05-23 F. Bazzocchi , J. W. F. Valle

The seesaw and leptogenesis commonly depend on the masses of same particles, and thus are both realized at the same scale. In this work, we demonstrate a new possibility to realize a TeV-scale neutrino seesaw and a natural high-scale…

High Energy Physics - Phenomenology · Physics 2019-01-23 Pei-Hong Gu , Hong-Jian He

We present a new model of radiative neutrino mass generation wherein TeV scale leptoguark scalars induce tiny neutrino masses as two-loop radiative corrections. The neutrino oscillation parameter \sin^2\theta_{13} is predicted to be close…

High Energy Physics - Phenomenology · Physics 2014-11-21 K. S. Babu , J. Julio

We discuss the connection between the origin of neutrino masses and their mixings which arises in a class of scenarios with radiatively induced neutrino masses. In these scenarios, the neutrino mass matrix acquires textures with two entries…

High Energy Physics - Phenomenology · Physics 2014-07-18 Michael Gustafsson , Jose M. No , Maximiliano A. Rivera

We show that under a new U(1) gauge symmetry, which is non-anomalous in the presence of one ``right-handed neutrino'' per generation and consistent with the standard model Yukawa couplings, the most general fermion charges are determined in…

High Energy Physics - Phenomenology · Physics 2008-11-26 Mu-Chun Chen , Andre de Gouvea , Bogdan A. Dobrescu

In this brief review, I discuss the new physics unveiled by neutrino oscillation experiments over the past several years, and discuss several attempts at understanding the mechanism behind neutrino masses and lepton mixing. It is fair to…

High Energy Physics - Phenomenology · Physics 2009-11-11 Andre de Gouvea

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

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 obtain model independent relations among neutrino masses and leptogenesis parameters. We find exact relations that involve the CP asymmetries $\epsilon_{N_\alpha}$, the washout parameters $\tilde m_\alpha$ and $\theta_{\alpha\beta}$, and…

High Energy Physics - Phenomenology · Physics 2010-02-03 Guy Engelhard , Yuval Grossman , Yosef Nir

Little Higgs models are formulated as effective theories with a cut-off of up to 100 times the electroweak scale. Neutrino masses are then a puzzle, since the usual see-saw mechanism involves a much higher scale that would introduce…

High Energy Physics - Phenomenology · Physics 2009-11-11 F. del Aguila , M. Masip , J. L. Padilla

We investigate the tree-level neutrino mass generation in the gauged $U(1)_\ell$ lepton model recently proposed by us [arXiv:1805.10382]. With the addition of one Standard Model(SM) singlet, $\phi_1(Y=0, \ell=1)$, and one SM triplet scalar,…

High Energy Physics - Phenomenology · Physics 2018-10-05 We-Fu Chang , John N. Ng

We present theories of `Natural Neutrinos' in which neutral fermionic top partner fields are simultaneously the right-handed neutrinos (RHN), linking seemingly disparate aspects of the Standard Model structure: a) The RHN top partners are…

High Energy Physics - Phenomenology · Physics 2015-11-04 Brian Batell , Matthew McCullough

With the start of the LHC, interest in electroweak scale models for the neutrino mass has grown. In this letter, we review two specific models that simultaneously explain neutrino masses and provide a suitable DM candidate. We discuss the…

High Energy Physics - Phenomenology · Physics 2011-11-10 Yasaman Farzan

We consider a possibility to naturally explain tiny neutrino masses without the lepton number violation. We study a simple model with SU(2)_L singlet charged scalars (s_1^+, s_2^+) as well as singlet right-handed neutrino (nu_R). Yukawa…

High Energy Physics - Phenomenology · Physics 2011-08-24 Shinya Kanemura , Takehiro Nabeshima , Hiroaki Sugiyama

One puzzle of neutrino masses and mixings is that they do not exhibit the kind of strong "hierarchy" that is found for the quarks and charged leptons. Neutrino mass ratios and mixing angles are not small. A possible reason for this is…

High Energy Physics - Phenomenology · Physics 2011-05-12 S. M. Barr

We show that by adding to the standard model plus the type I seesaw different types of scalars, it is possible to construct models that satisfy the three requirements of (i) generating neutrino masses at the TeV scale, (ii) being testable…

High Energy Physics - Phenomenology · Physics 2015-06-16 Chee Sheng Fong , M. C. Gonzalez-Garcia , Enrico Nardi , Eduardo Peinado

Neutrino masses can be generated by fermion triplets with TeV-scale mass, that would manifest at LHC as production of two leptons together with two heavy SM vectors or higgs, giving rise to final states such as 2 leptons + 4 jets (that can…

High Energy Physics - Phenomenology · Physics 2008-11-26 Roberto Franceschini , Thomas Hambye , Alessandro Strumia

We discuss the implications for lepton mixing and CP violation of structure in the lepton mass matrices, for the case that neutrino masses are generated by the see-saw mechanism with an hierarchical structure for the Majorana masses. For a…

High Energy Physics - Phenomenology · Physics 2015-06-25 A. Ibarra , G. G. Ross