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Related papers: From Fermion Mass Matrices to Neutrino Oscillation…

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We discuss whether quark, charged lepton and neutrino masses and mixing angles may be related by an extended flavour and family symmetry group. We show that current measurements of all fermion masses and mixing angles are consistent with a…

High Energy Physics - Phenomenology · Physics 2010-04-05 G. G. Ross , L. Velasco-Sevilla

It was recently shown by the authors that the Fritzsch ansatz for the quark mass matrices prescribed at the supersymmetric grand unified scale is compatible with a moderately heavy top quark ($m_t \simeq 120-150~GeV$). Here we extend the…

High Energy Physics - Phenomenology · Physics 2011-05-12 K. S. Babu , Q. Shafi

I discuss a SUSY-GUT model with a non-Abelian discrete family symmetry that explains the observed hierarchical pattern of quark and lepton masses. This $SO(10) \times \Delta(75)$ model predicts modified quadratic seesaw neutrino masses and…

High Energy Physics - Phenomenology · Physics 2016-08-24 Martin Schmaltz

In drawing on an analogy with the flavor mixing observed in the quark sector we discuss a pattern of large flavor mixing angles in the lepton sector. Simple arguments based on a democratic symmetry and its violation in the lepton sector…

High Energy Physics - Phenomenology · Physics 2007-05-23 Harald Fritzsch , Zhi-Zhong Xing

Under the assumptions that 1) the quark/lepton mass matrices take Froggatt-Nielsen's factorized power form \lambda^{\psi_i+\psi_j} with anomalous U(1) charges \psi_i, and 2) the U(1) charges \psi_i respect the SU(5) GUT structure, we show…

High Energy Physics - Phenomenology · Physics 2007-05-23 Masako Bando , Taichiro Kugo

We consider the Grand Unification (GU) scenario for neutrino masses which is based on the see-saw mechanism with the mass of the heaviest right handed (RH) neutrino at the GU-scale: $M_3 \sim \Lambda_{GU}$, and on the quark-lepton symmetry…

High Energy Physics - Phenomenology · Physics 2009-10-30 K. S. Babu , Q. Y. Liu , A. Yu. Smirnov

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

In this talk I discuss the qualitative features of an SO(10) SUSY GUT with an SU(2)x U(1)$^n$ family symmetry. I then describe the global fit of this theory to precision electroweak data [including charged fermion masses and mixing angles].…

High Energy Physics - Phenomenology · Physics 2009-10-31 Stuart Raby

The recent experimental results indicating the neutrino oscillations may strongly suggest that at least one more light neutrino species is required in order to reconcile the existing data. In the simple GUT frameworks, this fact seems…

High Energy Physics - Phenomenology · Physics 2009-10-31 Masako Bando , Koichi Yoshioka

We develop a bottom-up approach to constructing a theory of fermion masses and mixing angles based on the gauge group $SU(3)\times G$ where SU(3) is a family symmetry and $G$ contains a unified group such as SO(10) or its Pati-Salam…

High Energy Physics - Phenomenology · Physics 2015-06-25 S. F. King , G. G. Ross

An alternative supersymmetric SO(10) grand unification model with lopsided fermion mass matrices is introduced. It generates a large solar-neutrino-mixing angle through the neutrinos' Dirac mass matrix constrained by the SO(10) group…

High Energy Physics - Phenomenology · Physics 2009-11-11 Xiangdong Ji , Yingchuan Li , R. N. Mohapatra

Extrapolating the tau and b masses in the MSSM tends to give for their ratio at the GUT scale a number around 1.2, for most viable values \tan \beta, rather than the minimal SU(5) prediction of 1. We suggest that this may be due to large…

High Energy Physics - Phenomenology · Physics 2011-01-27 S. M. Barr , I. Dorsner

We discuss a supersymmetric unified model based on a product gauge group SU(5)\times SU(5)\times SU(5), where the gauge symmetry breaking is achieved without the adjoint or higher-dimensional Higgs field, and the doublet-triplet splitting…

High Energy Physics - Phenomenology · Physics 2007-05-23 Takehiko Asaka , Y. Takanishi

We propose simple phenomenological lepton mass matrices which describe the three neutrinos almost degenerate in mass, leading to a very large mixing angle between $\nu_\mu$ and $\nu_\tau$, as consistent with a recent report on atmospheric…

High Energy Physics - Phenomenology · Physics 2009-10-30 M. Fukugita , M. Tanimoto , T. Yanagida

The atmospheric neutrino data imply large mixing between the $\nu_\mu$ and $\nu_\tau$ states, $\theta_{23} = (45\pm 12)^\circ$, while the MSW solution to the solar neutrino problem needs very small mixing angle $\theta_{12} = (2\pm…

High Energy Physics - Phenomenology · Physics 2010-02-03 Zurab Berezhiani , Anna Rossi

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 to…

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

Neutrino masses and mixings are investigated on the basis of a universal seesaw mass matrix model, in which quark (except for top) and charged lepton mass matrices M_f and neutrino mass matrix M_\nu are given by M_f \simeq m_L M_F^{-1} m_R…

High Energy Physics - Phenomenology · Physics 2009-10-30 Yoshio Koide

A structure is proposed for the mass matrices of the quarks and leptons that arises in a natural way from the assumption that the breaking of SO(10) gauge symmetry is achieved by the smallest possible set of vacuum expectation values. This…

High Energy Physics - Phenomenology · Physics 2011-05-12 Carl H. Albright , K. S. Babu , S. M. Barr

Current solar and atmospheric neutrino oscillation data seem to favor a bimaximal pattern for neutrino mixings where the matrix elements U_{e2} and U_{\mu 3} are of order one, while U_{e3} is much smaller. We show that such a pattern can be…

High Energy Physics - Phenomenology · Physics 2011-05-12 K. S. Babu , S. M. Barr

We describe a supersymmetric Grand Unified Theory based on the gauge group $\SU(5)^3$, or $\SO(10)^3$, invariant under the interchange of any~SU(5), or~SO(10), with each family multiplet transforming non trivially under one different…

High Energy Physics - Phenomenology · Physics 2009-10-09 Riccardo Barbieri , Gia Dvali , Alessandro Strumia
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