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Within the type II see-saw mechanism the light neutrino mass matrix is given by a sum of a direct (or triplet) mass term and the conventional (type I) see-saw term. Both versions of the see-saw mechanism explain naturally small neutrino…

High Energy Physics - Phenomenology · Physics 2010-10-27 Manfred Lindner , Werner Rodejohann

We propose a simple, testable, SU(5) model within the context of the type II neutrino see-saw mechanism. It is based on requiring renormalizability, the absence of any other matter fields besides those already present in the Standard Model…

High Energy Physics - Phenomenology · Physics 2008-11-26 Ilja Dorsner , Irina Mocioiu

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

The original Standard Model has massless neutrinos, but the observation of neutrino oscillations requires that neutrinos are massive. The simple extension of adding gauge singlet fermions to the particle spectrum allows normal Yukawa mass…

High Energy Physics - Phenomenology · Physics 2011-12-14 Thomas Gajdosik , Andrius Juodagalvis , Darius Jurciukonis , Tomas Sabonis

A beautiful understanding of the smallness of the neutrino masses may be obtained via the seesaw mechanism, whereby one takes advantage of the key qualitative distinction between the neutrinos and the other fermions: right-handed neutrinos…

High Energy Physics - Phenomenology · Physics 2015-06-03 Brian Feldstein , William Klemm

We explore the neutrino sector of the minimal left-right symmetric model, with the additional charge conjugation discrete symmetry, in the tuned regime where type-I and type-II seesaw mechanisms are equally responsible for the light…

High Energy Physics - Phenomenology · Physics 2022-08-17 Gustavo F. S. Alves , Chee Sheng Fong , Luighi P. S. Leal , Renata Zukanovich Funchal

We consider the minimal 3-3-1 model with a heavy scalar sextet and realize, at the tree level, an effective dimension-five interaction that contributes to the mass of the charged leptons. In this case the charged leptons masses arise from a…

High Energy Physics - Phenomenology · Physics 2015-10-22 G. De Conto , A. C. B. Machado , V. Pleitez

In contrast to the original type I seesaw mechanism that requires right-handed Majorana neutrinos at energies much higher than the electroweak scale, the so-called low scale seesaw models allow lighter masses for the additional neutrinos.…

High Energy Physics - Phenomenology · Physics 2020-02-11 A. E. Cárcamo Hernández , Marcela González , Nicolás A. Neill

The future muon collider can play as an ideal machine to search for new physics at high energies. In this work, we study the search potential of the heavy Higgs triplet in the Type II Seesaw mechanism at muon colliders with high collision…

High Energy Physics - Phenomenology · Physics 2023-04-05 Tong Li , Chang-Yuan Yao , Man Yuan

We show how the use of a see-saw mechanism based on a $3 \times 3$ neutrino mass matrix texture can considerably simplify Higgs sectors for quark-lepton symmetric models (and for Standard Model extensions generally). The main theory we…

High Energy Physics - Phenomenology · Physics 2009-10-28 R. Foot , R. R. Volkas

The type II seesaw mechanism introduces a hypercharged Higgs triplet to explain the observed neutrino masses and mixing. Among three triplet components, the doubly charged Higgs boson can be the lightest and decay mainly to same-sign…

High Energy Physics - Phenomenology · Physics 2012-09-07 Eung Jin Chun , Pankaj Sharma

We investigate neutrino magnetic moment, triplet scalar dark matter in a Type-II radiative seesaw scenario. With three vector-like fermion doublets and two scalar triplets, we provide a loop level setup for the electromagnetic vertex of…

High Energy Physics - Phenomenology · Physics 2024-04-17 Shivaramakrishna Singirala , Dinesh Kumar Singha , Rukmani Mohanta

Neutrinos are the most elusive particles of the Standard Model. The physics behind their masses remains unknown and requires introducing new particles and interactions. An elegant solution to this problem is provided by the seesaw…

High Energy Physics - Phenomenology · Physics 2024-11-19 Bartosz Fornal , Dyori Polynice , Luka Thompson

After outlining some popular ways to go beyond the standard model so as to generate non-zero but tiny neutrino masses, I focus on several typical seesaw mechanisms and discuss how to get a balance between their theoretical naturalness and…

High Energy Physics - Phenomenology · Physics 2011-04-15 Zhi-zhong Xing

We elaborate on an earlier proposal by Ernest Ma of a type II seesaw mechanism for suppressing the vacuum expectation values of some Higgs doublets. We emphasize that, by nesting this form of seesaw mechanism into various other seesaw…

High Energy Physics - Phenomenology · Physics 2010-04-23 W. Grimus , L. Lavoura , B. Radovcic

The type-II seesaw mechanism with an isospin-triplet scalar $\Delta_L$ provides one of the most compelling explanations for the observed smallness of neutrino masses. The triplet contains a doubly-charged component $H_L^{\pm\pm}$, which…

High Energy Physics - Phenomenology · Physics 2018-11-14 P. S. Bhupal Dev , Yongchao Zhang

We extend the Type I and Type III seesaw mechanisms to generate neutrino masses within the left-right symmetric theories where parity is spontaneously broken. We construct a next to minimal left-right symmetric model where neutrino masses…

High Energy Physics - Phenomenology · Physics 2010-03-17 Joydeep Chakrabortty

We study the possibility to test the Type I seesaw mechanism for neutrino masses at the CERN Large Hadron Collider. The inclusion of three generations of right-handed neutrinos (N_i) provides an attractive option of gauging the B-L…

High Energy Physics - Phenomenology · Physics 2009-10-29 Pavel Fileviez Perez , Tao Han , Tong Li

We consider an extension of the Standard Model (SM) augmented by two neutral singlet fermions per generation and a leptoquark. In order to generate the light neutrino masses and mixing, we incorporate inverse seesaw mechanism. The right…

High Energy Physics - Phenomenology · Physics 2018-02-07 Debottam Das , Kirtiman Ghosh , Manimala Mitra , Subhadeep Mondal

If neutrino masses are obtained via the canonical seesaw mechanism, based on an underlying 2X2 mass matrix, unitarity violation of the neutrino mixing matrix is unavoidable, but its effect is extremely small. On the other hand, in the…

High Energy Physics - Phenomenology · Physics 2010-11-15 Ernest Ma