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The $\mu\tau$-reflection symmetry is a simple symmetry capable of predicting all the unknown CP phases of the lepton sector and the atmospheric angle but too simple to predict the absolute neutrino mass scale or the mass ordering. We show…

High Energy Physics - Phenomenology · Physics 2017-01-23 C. C. Nishi , B. L. Sánchez-Vega

Under the assumption that the neutrinos are Majorana particles we study how the lepton mass matrices can be transformed into the simple form which has the same physical quantities by removing redundant parameters. We propose the exact…

High Energy Physics - Phenomenology · Physics 2014-11-17 K. Kimura , A. Takamura

Assuming that the neutrino mass matrix is diagonalized by the tribimaximal mixing matrix, we explore the textures for the charged lepton mass matrix that render an $U_{PMNS}$ lepton mixing matrix consistent with data. In particular we are…

High Energy Physics - Phenomenology · Physics 2014-06-10 J. Alberto Acosta , Alfredo Aranda , Manuel A. Buen-Abad , Alma D. Rojas

In view of the recent measurement of nonzero $\theta_{13}$, we carry out a systematic study of a simple class of neutrino models that has one diagonal texture or cofactor zero in the mass matrix. There are seven free parameters in the model…

High Energy Physics - Phenomenology · Physics 2013-08-27 Jiajun Liao , Danny Marfatia , Kerry Whisnant

Several popular Ans\"atze of lepton mass matrices that contain texture zeros are confronted with current neutrino observational data. We perform a systematic $\chi^2$-analysis in a wide class of schemes, considering arbitrary Hermitian…

High Energy Physics - Phenomenology · Physics 2015-07-08 Luís M. Cebola , David Emmanuel-Costa , Ricardo González Felipe

We have realized different two-zero textures within the framework of the left right symmetric model using the $\Gamma_{3}\cong A_{4}$ modular group. The matter multiplets of the model are assigned as three singlet representations of the…

High Energy Physics - Phenomenology · Physics 2025-12-29 Bhabana Kumar , Debajyoti Dutta , Mrinal Kumar Das

We discuss consequences of assuming ($i$) that the (Majorana) neutrino mass matrix $M_\nu$ displays flavour antisymmetry, $S_\nu^T M_\nu S_\nu=-M_\nu$ with respect to some discrete symmetry $S_\nu$ contained in $SU(3)$ and ($ii$) $S_\nu$…

High Energy Physics - Phenomenology · Physics 2016-01-27 Anjan S. Joshipura

In this work we have investigated the phenomenological consequences of two-zero textures of \textit{inverse} neutrino mass matrix ($M_{\nu}^{-1}$) in light of the large mixing angle (LMA) and large mixing angle-\textit{dark} (LMA-D)…

High Energy Physics - Phenomenology · Physics 2022-10-19 Labh Singh , Monal Kashav , Surender Verma

In this paper, we derive in a novel approach the possible textures of neutrino mass matrix that can lead us to maximal atmospheric mixing angle and Dirac CP phase which are consistent with the current neutrino oscillation data. A total of…

High Energy Physics - Phenomenology · Physics 2018-11-14 Zhi-Cheng Liu , Chong-Xing Yue , Zhen-hua Zhao

We diagonalize Majorana neutrino mass matrix with the help of PMNS matrix and obtain analytical relations between the mass matrix elements and mixing parameters, viz., three mixing angles- $\theta_{12}, \theta_{23}, \theta_{13}$ and Dirac…

High Energy Physics - Phenomenology · Physics 2019-05-21 Chandan Duarah

We investigate the prospects for scenarios with vanishing determinant neutrino mass matrices and vanishing $\theta_{13}$ mixing angle. Normal and inverse mass hierarchies are considered separately. For normal hierarchy it is found that…

High Energy Physics - Phenomenology · Physics 2013-05-29 Bhag C. Chauhan , Joao Pulido , Marco Picariello

We assume there to be precisely three left-handed neutrino states whose Majorana masses are generated by an unspecified mechanism. Were CP conserved, the symmetric neutrino mass matrix M would be real and all six of its distinct entries…

High Energy Physics - Phenomenology · Physics 2009-11-07 Paul H. Frampton , Sheldon L. Glashow , Danny Marfatia

In theories with three light neutrinos, certain simplicity assumptions allow the construction of a complete list of leading order lepton mass matrices. These matrices are consistent with m_{tau} \neq 0, Delta m^2_{12} \ll Delta m^2_{23},…

High Energy Physics - Phenomenology · Physics 2008-11-26 Lawrence J. Hall , David Smith

In this work we have realized texture zero structures of neutrino mass matrix through our study of neutrino phenomenology and dark matter. For analysing these processes, we have constructed a model in minimal inverse seesaw, ISS(2,3) by…

High Energy Physics - Phenomenology · Physics 2025-03-05 Jotin Gogoi , Mrinal Kumar Das

We study the phenomenological implications of the presence of two zeros in a magic neutrino mass matrix. We find that only two such patterns of the neutrino mass matrix are experimentally acceptable. We express all the neutrino observables…

High Energy Physics - Phenomenology · Physics 2020-12-29 Radha Raman Gautam , Sanjeev Kumar

Taking into account the latest neutrino oscillation data, we study texture zeros of the lepton mass matrices. Assuming the Dirac neutrino mass matrix M_D, the charged-lepton mass matrix M_l and the mass matrix of heavy right-handed Majorana…

High Energy Physics - Phenomenology · Physics 2013-02-01 Harald Fritzsch , Shun Zhou

A class of neutrino mass matrices with texture zeros realizable using the group $Z_3$ within the framework of type (I+II) seesaw mechanism naturally admits a non-zero $\theta_{13}$ and allows for deviations from maximal mixing. The…

High Energy Physics - Phenomenology · Physics 2015-05-30 Sanjeev Kumar

An explicit form of charged--lepton mass matrix, predicting $ m_\tau = 1776.80 $~MeV from the experimental values of $ m_e $ and $ m_\mu$ (in good agreement with the experimental figure $ m_\tau = 1777.05^{+0.29}_{-0.26}$ MeV), is applied…

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

We study constraints on neutrino properties from texture zeros in bi-large mixing See-Saw mass matrix and also from leptogenesis. Texture zeros may occur in the light (class a)) or in the heavy (class b)) neutrino mass matrices. Each of…

High Energy Physics - Phenomenology · Physics 2008-11-26 Wei Chao , Xiao-Gang He , Xue-Qian Li

With the accumulation of many years of solar and atmospheric neutrino oscillation data, the approximate form of the 3 times 3 neutrino mixing matrix is now known. What is not known is the (presumably Majorana) neutrino mass matrix M_{nu}…

High Energy Physics - Phenomenology · Physics 2007-05-23 Ernest Ma
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