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Related papers: Neutrino mixing with broken $S_3$ symmetry

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We investigate the implications of one vanishing minor in neutrino mass matrix using trimaximal mixing matrix. In this context, we analyse all six patterns of one vanishing minor zero in neutrino mass matrix and present correlations of the…

High Energy Physics - Phenomenology · Physics 2023-09-14 Iffat Ara Mazumder , Rupak Dutta

Minimal SO(10) grand unified models provide phenomenological predictions for neutrino mass patterns and mixing. These are the outcome of the interplay of several features, namely: i) the seesaw mechanism; ii) the presence of an intermediate…

High Energy Physics - Phenomenology · Physics 2017-04-10 F. Buccella , M. Chianese , G. Mangano , G. Miele , S. Morisi , P. Santorelli

Using the seesaw mechanism, we construct a model for the light-neutrino Majorana mass matrix which yields trimaximal lepton mixing together with maximal CP violation and maximal atmospheric-neutrino mixing. We demonstrate that, in our…

High Energy Physics - Phenomenology · Physics 2010-04-21 W. Grimus , L. Lavoura

We develop a model-independent "box" parameterization of neutrino oscillations. Oscillation probabilities are linear in these new parameters, so measurements can straightforwardly determine the box parameters which can then be manipulated…

High Energy Physics - Phenomenology · Physics 2009-10-31 DJ Wagner , Thomas J. Weiler

A proposal for the neutrino mass, based on neutrino-scalar field interaction, is introduced. The scalar field is also non-minimally coupled to the Ricci scalar and hence relates the neutrino mass to the matter density. In a dense region,…

High Energy Physics - Phenomenology · Physics 2018-04-17 H. Mohseni Sadjadi , A. P. Khosravi Karchi

If the neutrino mass spectrum turns out to be m^{}_3 < m^{}_1 < m^{}_2, one may choose to relabel it as m^{\prime}_1 < m^{\prime}_2 < m^{\prime}_3 such that all the masses of fundamental fermions with the same electrical charges are in…

High Energy Physics - Phenomenology · Physics 2018-01-17 Zhi-zhong Xing , Jing-yu Zhu

In view of the recent neutrino oscillation data pointing to a non-vanishing value for the smallest mixing angle ($\theta_z$), we derive and find explicit realizations of the $(Z_2)^3$ flavor symmetry which characterizes, for the neutrino…

High Energy Physics - Phenomenology · Physics 2013-05-30 E. I. Lashin , M. Abbas , N. Chamoun , S. Nasri

We study neutrino masses and mixing in the context of flavor models with A4 symmetry, three scalar doublets in the triplet representation, and three lepton families. We show that there is no representation assignment that yields a…

High Energy Physics - Phenomenology · Physics 2013-09-10 R. Gonzalez Felipe , H. Serodio , Joao P. Silva

We simplify and extend our previous model for the masses and mixing matrix of three Majorana neutrinos based on permutation symmetry $S_3$ and the perturbations which violate this symmetry. The perturbations are arranged such that we get…

High Energy Physics - Phenomenology · Physics 2013-04-09 Renata Jora , Joseph Schechter , M. Naeem Shahid

We discuss all possible schemes with four massive neutrinos inspired by the existing experimental indications in favour of neutrino mixing, namely the atmospheric, solar and LSND neutrino experiments. We argue that the scheme with a…

High Energy Physics - Phenomenology · Physics 2011-04-15 W. Grimus

We propose a novel framework that simultaneously addresses three critical issues: tiny neutrino masses and their mixing patterns, dark matter, and the strong CP problem. Our model extends the Peccei-Quinn (PQ) symmetry by incorporating…

High Energy Physics - Phenomenology · Physics 2025-08-15 Sin Kyu Kang , Hiroshi Okada

We demonstrate that under the "symmetric zero texture" with minimal Majorana mass matrix, neutrino masses and mixing angles are expressed in terms of up-quark masses, $m_t,m_c,m_u$. This provides interesting relations among neutrino mixing…

High Energy Physics - Phenomenology · Physics 2017-08-23 Masako Bando , Midori Obara

A search for the parameter constraint in the three-parameter empirical mass formula proposed recently for active neutrinos is described. Without any parameter constraint the formula is a formal transformation of three free parameters into…

High Energy Physics - Phenomenology · Physics 2007-05-23 Wojciech Krolikowski

We generalize the democratic neutrino mixing Ansatz by incorporating the type-II seesaw mechanism with S(3) flavor symmetry. We find that bilarge neutrino mixing can naturally appear if the flavor democracy contribution is strongly…

High Energy Physics - Phenomenology · Physics 2009-11-10 Werner Rodejohann , Zhi-zhong Xing

The 3 X 3 Majorana neutrino mass matrix is written as a sum of 3 terms, i.e. M_nu = M_A + M_B + M_C, where M_A is proportional to the identity matrix and M_B and M_C are invariant under different Z_3 transformations. This M_nu is very…

High Energy Physics - Phenomenology · Physics 2009-11-10 Ernest Ma

The elements (squared) of the neutrino mixing matrix are found to satisfy, as functions of the induced mass, a set of differential equations. They show clearly the dominance of pole terms when the neutrino masses "cross". Using the known…

High Energy Physics - Phenomenology · Physics 2018-03-22 S. H. Chiu , T. K. Kuo

A new framework for handling flavor symmetry breaking in the neutrino sector is discussed where the source of symmetry breaking is traced to the global property of right-handed neutrinos in extra-dimensional space. Light neutrino…

High Energy Physics - Phenomenology · Physics 2009-11-11 Naoyuki Haba , Atsushi Watanabe , Koichi Yoshioka

We discuss a neutrino mass model based on the S4 discrete symmetry where the symmetry breaking is triggered by the boundary conditions of the bulk right-handed neutrino in the fifth spacial dimension. While the symmetry restricts bare mass…

High Energy Physics - Phenomenology · Physics 2011-02-21 Hajime Ishimori , Yusuke Shimizu , Morimitsu Tanimoto , Atsushi Watanabe

One loop corrections to the neutrino mass matrix within the MSSM with Bilinear R Parity Violation are calculated, paying attention to the approach in which an effective $3\times 3$ neutrino mass matrix is used. The full mass matrix is block…

High Energy Physics - Phenomenology · Physics 2014-09-18 Marco A. Diaz , Maximiliano A. Rivera , Nicolas Rojas

It is proposed that light neutrinos form a triplet in a global SU(3) flavor symmetry. Within this framework, a symmetry principle predicts sin^2 theta_{23}=0.5 and gives the so called inverted neutrino mass hierarchy, theta _{13}=0 and a…

High Energy Physics - Phenomenology · Physics 2007-05-23 Riazuddin