English
Related papers

Related papers: Minimal Tree-Level Seesaws with a Heavy Intermedia…

200 papers

The origin of neutrino mass is usually attributed to a seesaw mechanism, either through a heavy Majorana fermion singlet (version 1) or a heavy scalar triplet (version 2). Recently, the idea of using a heavy Majorana fermion triplet…

High Energy Physics - Phenomenology · Physics 2009-04-24 Ernest Ma

We consider a scenario in which additional vectorlike TeV-scale fermions belonging to higher weak-isospin multiplets provide new seesaw mediators. If these fermions have non-zero hypercharge, their tree-level exchange produces novel seesaw…

High Energy Physics - Phenomenology · Physics 2010-03-29 Ivica Picek , Branimir Radovcic

We propose a Majoron-like extension of the Standard Model with an extra global $U(1)_X$-symmetry where neutrino masses are generated through an inverse seesaw mechanism at the 1-loop level. In contrast to the tree-level inverse seesaw, our…

High Energy Physics - Phenomenology · Physics 2024-01-17 Cesar Bonilla , A. E. Cárcamo Hernández , Bastián Díaz Sáez , Sergey Kovalenko , Juan Marchant González

We consider the seesaw mechanism of neutrino mass generation in the light of our present knowledge of the neutrino masses and mixing. We analyse the seesaw mechanism constrained by the following assumptions: (1) minimal seesaw with no Higgs…

High Energy Physics - Phenomenology · Physics 2008-11-26 E. Kh. Akhmedov , G. C. Branco , M. N. Rebelo

An extension of the Standard Model (SM) is studied in which two right-handed (RH) neutrinos per generation are incorporated, but considering the hypothesis of the symmetry of lepton and quark contents in order to deprive the number of RH…

High Energy Physics - Phenomenology · Physics 2015-01-13 Ernesto A. Matute

We examine minimal seesaw mechanism in which the masses of light neutrinos are described with tri/bi-maximal mixing in the basis where the charged-lepton Yukawa matrix and heavy Majorana neutrino mass matrix are diagonal. We search for all…

High Energy Physics - Phenomenology · Physics 2014-11-17 Sanghyeon Chang , Sin Kyu Kang , Kim Siyeon

We build a renormalizable theory where the inverse seesaw mechanism explains the pattern of SM fermion masses. To the best of our knowledge, our model corresponds to the first implementation of the inverse seesaw mechanism for the charged…

High Energy Physics - Phenomenology · Physics 2022-02-04 A. E. Cárcamo Hernández , D. T. Huong , Ivan Schmidt

We propose natural hierarchies among neutral fermions in a framework of inverse seesaw, imposing a $Z_3$ Tambara-Yamagami fusion rule which is applied to our phenomenology. Under the symmetry, the Majorana mass terms for $N_R$ and $N_L$ are…

High Energy Physics - Phenomenology · Physics 2025-08-25 Shilpa Jangid , Hiroshi Okada

We propose a $B-L$ gauged extension of the Standard Model where light neutrino masses arise from type III seesaw mechanism. Unlike the minimal $B-L$ model with three right handed neutrinos having unit lepton number each, the model with…

High Energy Physics - Phenomenology · Physics 2020-03-24 Anirban Biswas , Debasish Borah , Dibyendu Nanda

Seesaw mechanisms are the simplest and the most elegant way of generating small masses for the active neutrinos $(m_\nu)$. In these mechanisms $m_\nu$ is inversely proportional to the lepton number breaking scale $(M)$ that, in the…

High Energy Physics - Phenomenology · Physics 2023-05-01 E. Cabrera , D. Cogollo , C. A. de S. Pires

In the context of Standard Model (SM) extensions, the seesaw mechanism provides the most natural explanation for the smallness of neutrino masses. In this work we consider the most economical type-I seesaw realization in which two…

High Energy Physics - Phenomenology · Physics 2018-06-20 D. M. Barreiros , R. G. Felipe , F. R. Joaquim

A mechanism for generating small tree-level Majorana mass for neutrinos is implemented in the 331 Model. No additional fermions or scalars need to be added, and no mass scale greater than a few TeV is invoked.

High Energy Physics - Phenomenology · Physics 2009-12-31 M. B. Tully , G. C. Joshi

In this letter we address the issue of generating appropriate tiny neutrino masses within the framework of a particular $SU(3)_{c}\otimes SU(3)_{L}\otimes U(1)_{X}$ gauge model by adding three singlet exotic Majorana neutrinos to the ones…

High Energy Physics - Phenomenology · Physics 2016-04-05 Adrian Palcu

We propose a $U(1)_L$ model with $A_4$ symmetry in light of the linear seesaw for majorana neutrino that capable of generating the current lepton and quark mass and mixing patterns. The smallness of Majorana neutrino mass is reproduced…

High Energy Physics - Phenomenology · Physics 2023-03-09 V. V. Vien

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

The seesaw mechanism can be generalized to a Type-III variant and a quintuplet variant. We present two models that provide analogous generalizations of the inverse seesaw mechanism. The first model employs a fermion triplet F ~ (1,3,0) and…

High Energy Physics - Phenomenology · Physics 2013-06-12 Sandy S. C. Law , Kristian L. McDonald

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 construct a model realizing the inverse seesaw mechanism. The model has two types of gauge singlet fermions in addition to right-handed neutrinos. A required Majorana mass scale (keV scale) for generating the light active neutrino mass…

High Energy Physics - Phenomenology · Physics 2015-11-30 Mayumi Aoki , Naoyuki Haba , Ryo Takahashi

We propose a type II seesaw model for light Dirac neutrinos to provide an explanation for the recently reported anomaly in W boson mass by the CDF collaboration with $7\sigma$ statistical significance. In the minimal model, the required…

High Energy Physics - Phenomenology · Physics 2022-08-10 Debasish Borah , Satyabrata Mahapatra , Dibyendu Nanda , Narendra Sahu

In the Standard Model, Yukawa couplings parametrize the fermion masses and mixing angles with the exception of neutrino masses. The hierarchies and apparent regularities among the quark and lepton masses are, however, otherwise a mystery.…

High Energy Physics - Phenomenology · Physics 2022-11-07 Sudip Jana , Sophie Klett , Manfred Lindner