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Related papers: Master Majorana neutrino mass parametrization

200 papers

We introduce three right-handed neutrinos and three sterile neutrinos, and consider an inverse seesaw mechanism for neutrino mass generation. From naturalness point of view, their Majorana masses should be small, while it induces a large…

High Energy Physics - Phenomenology · Physics 2016-11-10 Naoyuki Haba , Hiroyuki Ishida , Yuya Yamaguchi

We reconstruct the neutrino mass matrix in the flavor basis, using experimental data on neutrino oscillations. Both normal and inverted hierarchy (ordering) of the mass spectrum are considered. The dependence of the matrix structure on CP…

High Energy Physics - Phenomenology · Physics 2007-05-23 Michele Frigerio

Flavor mixings together with fermion mass spectra are studied in detail in the $SU(6) \times SU(2)_R$ model, in which state-mixings beyond the minimal supersymmetric standard model (MSSM) take place. Characteristic patterns of fermion…

High Energy Physics - Phenomenology · Physics 2013-06-26 Chuichiro Hattori , Mamoru Matsunaga , Takeo Matsuoka

We present an updated and improved global fit analysis of precision and flavor observables so as to derive constraints on deviations from unitarity in the leptonic mixing matrix. We focus on the case in which these deviations are sourced by…

High Energy Physics - Phenomenology · Physics 2024-05-24 Daniel Naredo-Tuero

Lepton flavour violation and neutrino masses are a signal for new Physics beyond the Standard Model and are deeply related. The minimal extension of the Standard Model to make it include neutrino masses is not satisfactory from a conceptual…

High Energy Physics - Phenomenology · Physics 2011-07-29 J. N. Esteves

It is found that the seesaw mechanism not only explain the smallness of neutrino masses but also account for the large mixing angles simultaneously, even if the unification of the neutrino Dirac mass matrix with that of up-type quark sector…

High Energy Physics - Phenomenology · Physics 2007-05-23 H. Tsujimoto

The determination of CP violating phases in the Majorana neutrino mixing matrix using phenomenological constraints from neutrino oscillations, neutrinoless double beta decay, ($\mu^-, e^+$) conversion and few other processes is discussed.…

High Energy Physics - Phenomenology · Physics 2007-05-23 M. K. Samal

With the help of current neutrino oscillation data, we illustrate the three-dimensional (3D) profiles of all the six distinct effective Majorana neutrino masses $|\langle m\rangle^{}_{\alpha \beta}|$ (for $\alpha, \beta = e, \mu, \tau$)…

High Energy Physics - Phenomenology · Physics 2021-09-15 Ce-ran Hu , Zhi-zhong Xing

Large mixing parameters of neutrino mass eigenstates in the neutrino flavor eigenstates are determined, and interpreted as closely related to the neutrino and charged lepton mass-ratio patterns. The three known seemingly different charged…

High Energy Physics - Phenomenology · Physics 2007-07-10 E. M. Lipmanov

The exponential parameterization of Pontecorvo-Maki-Nakagawa-Sakata mixing matrix for neutrino is used for comparative analysis of different neutrino mixing data. The UPMNS matrix is considered as the element of the SU(3) group and the…

High Energy Physics - Phenomenology · Physics 2016-12-21 Konstantin Zhukovsky , Anatoly Borisov

The fact that neutrinos are massive suggests that the minimal supersymmetric standard model (MSSM) might be extended in order to include three gauge-singlet neutrino superfields with Yukawa couplings of the type $H_2 L \nu^c$. We propose to…

High Energy Physics - Phenomenology · Physics 2009-11-11 D. E. Lopez-Fogliani , C. Munoz

We consider the scheme with mixing of three neutrinos and a mass hierarchy. We shown that, under the natural assumptions that massive neutrinos are Majorana particles and there are no unlikely fine-tuned cancellations among the…

High Energy Physics - Phenomenology · Physics 2009-10-31 Carlo Giunti

We present a new mechanism to explain naturally and through a common flavour symmetry the mildly hierarchical neutrino masses with large mixings and the hierarchical Yukawa matrices with small mixing angles. Although this mechanism is not…

High Energy Physics - Phenomenology · Physics 2007-05-23 Oscar Vives

For the purpose of deriving the observed nearly tribimaximal neutrino mixing, a possible quark mass matrix model is investigated based on a yukawaon model. The neutrino mass matrix is related to the up-quark mass matrix. Five observable…

High Energy Physics - Phenomenology · Physics 2010-03-31 Yoshio Koide

We revisit the WMAP dark matter constraints on Yukawa Unification in the presence of massive neutrinos. The large neutrino mixing indicated by the data modifies the predictions for the bottom quark mass, and enables Yukawa also for large…

High Energy Physics - Phenomenology · Physics 2009-05-01 M. E. Gomez , S. Lola , P. Naranjo , J. Rodriguez-Quintero

We reconsider the possibility that Majorana masses for the three known neutrinos are generated radiatively by the presence of a fourth generation and one right-handed neutrino with Yukawa couplings and a Majorana mass term. We find that the…

High Energy Physics - Phenomenology · Physics 2011-08-01 Alberto Aparici , Juan Herrero-García , Nuria Rius , Arcadi Santamaria

One can describe cosmological relic neutrinos by adding Lagrange multipliers to the Standard Model Lagrangian for them. The two possible Lagrange multipliers are a chemical potential, which fixes the mean neutrino/anti-neutrino asymmetry,…

High Energy Physics - Phenomenology · Physics 2013-02-13 Bob McElrath

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

A neutrino mass matrix model with a bilinear form $M_\nu = k_\nu (M_D M_R^{-1} M_D^T)^2$ is proposed within the framework of the so-called yukawaon model, which has been proposed for the purpose of a unified description of the lepton mixing…

High Energy Physics - Phenomenology · Physics 2015-06-12 Yoshio Koide , Hiroyuki Nishiura

Lepton-flavour symmetry in the Standard Model is broken by small masses for charged leptons and neutrinos. Introducing neutrino masses via dimension-5 operators associated to lepton-number violation at a very high scale, the corresponding…

High Energy Physics - Phenomenology · Physics 2008-11-26 Th. Feldmann , Th. Mannel
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