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Related papers: The Type-II Singular See-Saw Mechanism

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We consider the see-saw mechanism for hierarchical Dirac and Majorana neutrino mass matrices m_D and M_R, including the CP violating phases. Simple arguments about the structure of the neutrino mass matrix and the requirement of successful…

High Energy Physics - Phenomenology · Physics 2011-07-19 Werner Rodejohann

The see-saw mechanism of neutrino mass generation may enhance lepton mixing up to maximal even if the Dirac mass matrices of leptons have structure similar to that in the quark sector. Two sets of conditions for such an enhancement are…

High Energy Physics - Phenomenology · Physics 2009-10-22 Alexei Yu. Smirnov

A novel scenario is presented within the Type-I seesaw mechanism in which no other beyond Standard Model fields except three heavy right handed neutrinos, have been considered. Light neutrino masses around sub eV scale, could be possible at…

High Energy Physics - Phenomenology · Physics 2024-11-26 Kunal Pandey , Rathin Adhikari

The possibility of generating neutrino mass through see-saw mechanism involving U(1) chiral Peccei-Quinn and scale symmetries breakdown is discussed. We consider a generic scale invariant model which has three Majorana fermions and a…

High Energy Physics - Phenomenology · Physics 2007-05-23 Alex Gomes Dias

In this talk we show how a natural neutrino mass hierarchy can follow from the type I see-saw mechanism, and a natural neutrino mass degeneracy from the type II see-saw mechanism, where the bi-large mixing angles can arise from either the…

High Energy Physics - Phenomenology · Physics 2009-11-10 S. F. King

The seesaw mechanism is the preferred methodology to obtain light neutrino masses by the introduction of a Majorana mass matrix. Moreover, radiative corrections can be done in order to improve the predictions of the model. However, when…

High Energy Physics - Phenomenology · Physics 2018-02-12 Carlos E. Diaz , S. F. Mantilla , R. Martinez

It is often said that neutrino mass is a window to a new physics beyond the standard model (SM). This is certainly true if neutrinos are Majorana particles since the SM with Majorana neutrino mass is not a complete theory. The classical…

High Energy Physics - Phenomenology · Physics 2010-03-25 Goran Senjanovic

Starting from a complete set of possible parametrisations of the quark-mass matrices that have the maximum number of texture zeros at the grand unification scale, and the Georgi-Jarlskog mass relations, we classify the neutrino spectra with…

High Energy Physics - Phenomenology · Physics 2015-06-25 E. Papageorgiu

The simplest possibility to generate small Majorana neutrino masses is the seesaw mechanism. However, the smallness of the observed neutrino masses can also be understood, if neutrino masses are generated by higher-dimensional operators…

High Energy Physics - Phenomenology · Physics 2020-05-20 Ricardo Cepedello , Renato Fonseca , Martin Hirsch

A minimal extension of the Standard Model is proposed, where the observed left-handed neutrinos obtain naturally small Majorana masses from a one-loop radiative seesaw mechanism. This model has two candidates (one bosonic and one fermionic)…

High Energy Physics - Phenomenology · Physics 2010-04-06 Ernest Ma

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

In the framework of type II seesaw mechanism we propose two simple but instructive ansatze for neutrino mixing and leptogenesis. In each ansatz, the effective Majorana neutrino mass matrix is composed of two parts -- the part with Z_2…

High Energy Physics - Phenomenology · Physics 2008-11-26 Wan-lei Guo

We give a general analysis of neutrino mixing in the seesaw mechanism with three flavors. Assuming that the Dirac and u-quark mass matrices are similar, we establish simple relations between the neutrino parameters and individual Majorana…

High Energy Physics - Phenomenology · Physics 2009-12-30 T. K. Kuo , Guo-Hong Wu , Sadek W. Mansour

The see-saw mechanism is a very attractive explanation for small neutrino masses, parametrized at the GUT scale by the right-handed Majorana mass matrix, ${\cal M}$, and the neutrino Yukawa matrix, ${\bf Y_\nu}$. We show that in a SUSY…

High Energy Physics - Phenomenology · Physics 2010-02-03 Sacha Davidson , Alejandro Ibarra

We present a detailed discussion on neutrinoless double beta decay within a class of left-right symmetric models where neutrino mass originates by natural type-II seesaw dominance. The spontaneous symmetry breaking is implemented with…

High Energy Physics - Phenomenology · Physics 2016-11-23 Prativa Pritimita , Nitali Dash , Sudhanwa Patra

In this study, we implement the type-II seesaw mechanism for Dirac neutrino masses within the framework of a 3-3-1 model. To this end, we introduce a scalar sextet and impose both lepton number conservation and invariance under a discrete…

High Energy Physics - Phenomenology · Physics 2025-06-06 Vinícius Oliveira , Patricio Escalona , Lucia Angel , C. A. de S. Pires , Farinaldo S. Queiroz

We study the possibility of realizing the neutrino seesaw mechanism in the E8XE8 heterotic string. In particular, we consider its Z_6 orbifold compactifications leading to the supersymmetric standard model gauge group and matter content. We…

High Energy Physics - Phenomenology · Physics 2008-11-26 Wilfried Buchmuller , Koichi Hamaguchi , Oleg Lebedev , Saul Ramos-Sanchez , Michael Ratz

In this brief review we discuss the generation of Majorana neutrino masses through the see-saw mechanism, the theory of neutrinoless double-beta decay, the implications of neutrino oscillation data for the effective Majorana mass, taking…

High Energy Physics - Phenomenology · Physics 2015-06-04 S. M. Bilenky , C. Giunti

It is shown that the Majorana nature of the heavy neutrinos $N_j$ having masses in the range of $M_j \sim (100 - 1000)$ GeV and present in the TeV scale type I and inverse see-saw scenarios of neutrino mass generation, is unlikely to be…

High Energy Physics - Phenomenology · Physics 2014-11-21 A. Ibarra , E. Molinaro , S. T. Petcov

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