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Related papers: An Asymmetric TBM Texture

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\noindent We revisit the \textit{minimal seesaw model}, i.e., the type-I seesaw mechanism involving only two right-handed neutrinos. % This model represents an important minimal benchmark scenario for future experimental updates on neutrino…

High Energy Physics - Phenomenology · Physics 2017-04-05 Thomas Rink , Kai Schmitz

A minimal and predictive neutrino mass matrix texture for Majorana neutrino is proposed. The texture favours the normal hierarchy of neutrino mass eigenvalues. It further predicts the octant of $\theta_{23}$, constraints $\delta$, gives…

High Energy Physics - Phenomenology · Physics 2026-05-19 Sagar Tirtha Goswami , Pralay Chakraborty , Subhankar Roy

Recent measurements of the neutrino solar mixing angle and the Cabibbo angle satisfy the empirical relation theta_{sol} + theta_{C} ~ 45^{o}. This relation suggests the existence of a correlation between the mixing matrices of leptons and…

High Energy Physics - Phenomenology · Physics 2009-11-11 F. Gonzalez-Canales , A. Mondragon

We present the general form of the unitary matrices keeping invariant the Majorana neutrino mass matrix of specific texture suitable for explaining oscillation data. In the case of the Tri-bimaximal pattern with two degenerate masses we…

High Energy Physics - Phenomenology · Physics 2011-02-01 E. I. Lashin , S. Nasri , E. Malkawi , N. Chamoun

In an attempt at explaining the observed neutrino mass-squared differences and leptonic mixing, lepton mass matrices with zero textures have been widely studied. In the weak basis where the charged lepton mass matrix is diagonal, various…

High Energy Physics - Phenomenology · Physics 2014-07-18 R. Gonzalez Felipe , H. Serodio

We study the possibility of generating non-zero reactor mixing angle $\theta_{13}$ by perturbing the $\mu-\tau$ symmetric neutrino mass matrix. The leading order $\mu-\tau$ symmetric neutrino mass matrix originates from type I seesaw…

High Energy Physics - Phenomenology · Physics 2015-06-22 Manikanta Borah , Debasish Borah , Mrinal Kumar Das , Sudhanwa Patra

We study the origin of neutrino masses and mixing angles which can accomodate the LMA MSW solutions of the solar neutrino anomaly as well as the solution of the atmospheric neutrino problem, within the framework of the see-saw mechanism. We…

High Energy Physics - Phenomenology · Physics 2014-11-17 N. Nimai Singh , Mahadev Patgiri

The Tri-Bimaximal (TBM) mixing predicts a vanishing $\theta_{13}$. This can be attributed to the inherited $\mu-\tau$ symmetry of TBM mixing. We break its $\mu-\tau$ symmetry by adding a complex magic matrix with one variable to TBM…

High Energy Physics - Phenomenology · Physics 2018-12-27 Kanwaljeet S. Channey , Sanjeev Kumar

We study all possible neutrino mass matrices with one zero element and two equal non-zero elements, known as hybrid texture neutrino mass matrices. In the diagonal charged lepton basis, we consider thirty nine such possible cases which are…

High Energy Physics - Phenomenology · Physics 2016-03-23 Rupam Kalita , Debasish Borah

Phenomenological aspects of non-invertible symmetries, in particular the flavor structure of quarks and leptons, are studied. We start with a $\mathbb{Z}_M$ discrete symmetry and gauge $\mathbb{Z}_2$ so as to obtain a non-invertible…

High Energy Physics - Phenomenology · Physics 2024-09-10 Tatsuo Kobayashi , Hajime Otsuka , Morimitsu Tanimoto

We analyze the different parametrizations of a general four-zero texture mass matrices for quarks and leptons, that are able to reproduce the CKM and PMNS mixing matrices. This study is done through a Chi-Square analysis. In quark sector,…

High Energy Physics - Phenomenology · Physics 2012-10-04 J. Barranco , D. Delepine , L. Lopez-Lozano

The minimum seesaw model with two right-handed neutrinos is considered, where the lightest neutrino is naturally massless. Instead of adopting texture zeros in the lepton Yukawa matrices, which cause both theoretical and experimental…

High Energy Physics - Phenomenology · Physics 2024-10-17 Yu-Cheng Qiu , Jin-Wei Wang , Tsutomu T. Yanagida

We analyze neutrino mass matrices having one texture zero, assuming that the neutrino mixing matrix has either its first (TM$_1$) or second (TM$_2$) column identical to that of the tribimaximal mixing matrix. We found that all the six…

High Energy Physics - Phenomenology · Physics 2018-03-20 Radha Raman Gautam

A seesaw mass matrix model is reviewed as a unification model of quark and lepton mass matrices. The model can understand why top-quark mass m_t is so singularly enhanced compared with other quark masses, especially, why m_t >> m_b in…

High Energy Physics - Phenomenology · Physics 2007-05-23 Yoshio Koide

We study the symmetric 2-zero texture of the neutrino mass matrix, which is obtained from the symmetric Dirac neutrino mass matrix with 2-zeros and right-handed Majorana neutrino mass matrix with the general form via the see-saw mechanism,…

High Energy Physics - Phenomenology · Physics 2009-11-10 Masako Bando , Satoru Kaneko , Midori Obara , Morimitu Tanimoto

We systematically analyze the radiative corrections to the $S_3$ symmetric neutrino mass matrix at high energy scale, say the GUT scale, in the charged lepton basis. There are significant corrections to the neutrino parameters both in the…

High Energy Physics - Phenomenology · Physics 2015-06-22 Shivani Gupta , C. S. Kim , Pankaj Sharma

We study neutrino mass matrices with one texture equality and the neutrino mixing matrix having either its first (TM$_1$) or second (TM$_2$) column identical to that of the tribimaximal mixing matrix. We found that out of total fifteen…

High Energy Physics - Phenomenology · Physics 2022-10-07 S. Dev , Desh Raj

Based on a supersymmetric Yukawaon model with O(3) family symmetry, possible forms of quark and lepton mixing matrices are systematically investigated under a condition that the up-quark mass matrix form leads to the observed nearly…

High Energy Physics - Phenomenology · Physics 2013-11-26 Hiroyuki Nishiura , Yoshio Koide

We suggest an approach to explain the observed pattern of the neutrino masses and mixing which employs the weakly broken quark-lepton symmetry and does not require introduction of an ad hoc symmetry of the neutrino sector. The mass matrices…

High Energy Physics - Phenomenology · Physics 2009-11-10 I. Dorsner , A. Yu. Smirnov

With the recent observation of nonzero \theta_{13}, five neutrino oscillation parameters are now known. By imposing four zeros in the Yukawa coupling matrix of the type I seesaw model, the number of parameters in the neutrino mass matrix is…

High Energy Physics - Phenomenology · Physics 2013-04-26 Jiajun Liao , D. Marfatia , K. Whisnant