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We establish a hybrid seesaw mechanism to explain small neutrino masses and predict cold dark matter candidate in the context of the B-L gauge symmetry extension of the Standard Model. In this model a new scalar doublet and two new fermion…

High Energy Physics - Phenomenology · Physics 2015-03-13 Tong Li , Wei Chao

We derive bounds on the Dirac Yukawa couplings of the neutrinos in seesaw models using the recent Large Hadron Collider (LHC) data on Higgs decays for the case where the Standard Model singlet heavy leptons needed for the seesaw mechanism…

High Energy Physics - Phenomenology · Physics 2015-03-20 P. S. Bhupal Dev , Roberto Franceschini , R. N. Mohapatra

The simplest type III seesaw model as originally proposed introduces one lepton triplet. It thus contains four active neutrinos, two massive and two massless at tree level. We determine the radiative masses that the latter receive first at…

High Energy Physics - Phenomenology · Physics 2009-04-22 Yi Liao , Ji-Yuan Liu , Guo-Zhu Ning

In type II seesaw utilized to explain the observed neutrino masses and mixings, one extends the Standard Model (SM) by introducing scalar fields which transform as a triplet under the electroweak gauge symmetry. New scalar couplings…

High Energy Physics - Phenomenology · Physics 2008-11-26 Ilia Gogoladze , Nobuchika Okada , Qaisar Shafi

We construct a model in which the neutrino Dirac mass terms are of order the electron mass and the seesaw mechanism proceeds via right-handed neutrinos with masses of order TeV. In our model the spectra of the three light and of the three…

High Energy Physics - Phenomenology · Physics 2010-07-20 W. Grimus , L. Lavoura

Observation of non-zero neutrino masses at a scale $\sim 10^{-1} - 10^{-2}$ eV is a major problem in the otherwise highly successful Standard Model. The most elegant mechanism to explain such tiny neutrino masses is the seesaw mechanism…

High Energy Physics - Phenomenology · Physics 2016-02-10 S. Chakdar , K. Ghosh , V. Hoang , P. Q. Hung , S. Nandi

The simplest linear seesaw mechanism can accommodate the new CDF-II $W$ mass measurement. In addition to Standard Model particles, the model includes quasi-Dirac leptons, and a second, leptophilic, scalar doublet seeding small neutrino…

High Energy Physics - Phenomenology · Physics 2022-09-07 Aditya Batra , Praveen Bharadwaj , Sanjoy Mandal , Rahul Srivastava , José W. F. Valle

The seesaw mechanism for three neutrinos is discussed, clarifying the situation where the seesaw texture results in three approximately zero mass eigenvalues. The true underlying mechanism is shown to be just the $inverse$ (or $linear$)…

High Energy Physics - Phenomenology · Physics 2010-01-15 Xiao-Gang He , Ernest Ma

We show that in TeV-scale left-right (L-R) symmetric seesaw models, there are new dominant contributions to the collider signals of heavy Majorana neutrinos arising from the heavy-light neutrino mixing, which directly probe the seesaw…

High Energy Physics - Phenomenology · Physics 2013-08-28 Chien-Yi Chen , P. S. Bhupal Dev , R. N. Mohapatra

We obtain limits on generic vector-like leptons at the TeV scale from electroweak precision tests. These limits are complementary to the ones obtained from lepton flavour violating processes. In general, the quality of the global…

High Energy Physics - Phenomenology · Physics 2008-11-26 F. del Aguila , J. de Blas , M. Perez-Victoria

The Lee-Wick (LW) formulation of higher-derivative theories can be extended from one in which the extra degrees of freedom are represented as a single heavy, negative-norm partner for each known particle (N=2), to one in which a second,…

High Energy Physics - Phenomenology · Physics 2013-05-30 Richard F. Lebed , Russell H. TerBeek

The model of heavy neutral leptons (HNLs) is one of the well-motivated models beyond the standard model (BSM) from both theoretical and phenomenological point of views. It is an indispensable ingredient to explain the puzzle of tiny…

High Energy Physics - Phenomenology · Physics 2020-11-04 Kingman Cheung , Yi-Lun Chung , Hiroyuki Ishida , Chih-Ting Lu

There exist tree-level generalizations of the Type-I and Type-III seesaw mechanisms that realize neutrino mass via low-energy effective operators with d>5. However, these generalizations also give radiative masses that can dominate the…

High Energy Physics - Phenomenology · Physics 2015-12-01 Kristian L. McDonald

We study the production of heavy neutrinos at the Large Hadron Collider (LHC) through the dominant s-channel production mode as well as the vector boson fusion (VBF) process. We consider the TeV scale minimal linear seesaw model containing…

High Energy Physics - Phenomenology · Physics 2015-04-13 Gulab Bambhaniya , Srubabati Goswami , Subrata Khan , Partha Konar , Tanmoy Mondal

We propose TeV-scale Dirac fermions producing Majorana masses of the known neutrinos via tree-level seesaw, different from standard type I and III seesaw. The employed weak five-plet with nonzero hypercharge leads to new seesaw formula…

High Energy Physics - Phenomenology · Physics 2011-05-30 Ivica Picek , Branimir Radovcic

Electroweak precision data have been extensively used to constrain models containing physics beyond that of the Standard Model. When the model contains Higgs scalars in representations other than singlets or doublets, and hence rho not…

High Energy Physics - Phenomenology · Physics 2014-11-18 Mu-Chun Chen , Sally Dawson , Tadas Krupovnickas

We generalize the scalar triplet neutrino mass model, the type II seesaw. Requiring fine-tuning and arbitrarily small parameters to be absent leads to dynamical lepton number breaking at the electroweak scale and a rich LHC phenomenology. A…

High Energy Physics - Phenomenology · Physics 2018-09-12 Julia Gehrlein , Dorival Gonçalves , Pedro A. N. Machado , Yuber F. Perez-Gonzalez

We consider extensions of the next-to-minimal supersymmetric model (NMSSM) in which the observed neutrino masses are described in terms of effective dimension six (or seven) rather than dimension five operators. All such operators respect…

High Energy Physics - Phenomenology · Physics 2009-02-18 Ilia Gogoladze , Nobuchika Okada , Qaisar Shafi

The Type II Seesaw model remains a popular and viable explanation of neutrino masses and mixing angles. By hypothesizing the existence of a scalar that is a triplet under the weak gauge interaction, the model predicts strong correlations…

High Energy Physics - Phenomenology · Physics 2023-04-28 Jon Butterworth , Julian Heeck , Si Hyun Jeon , Olivier Mattelaer , Richard Ruiz

The minimal 3-3-1 model is perturbative until energies around 4-5TeV, posing a challenge to generate neutrino masses at eV scale, mainly if one aims to take advantage of the seesaw mechanism. As a means to circumvent this problem we propose…

High Energy Physics - Phenomenology · Physics 2013-05-30 W. Caetano , D. Cogollo , C. A. de S. Pires , P. S. Rodrigues da Silva