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Related papers: Fermion Masses from SO(10) Hermitian Matrices

200 papers

We have constructed a SUSY SO(10) x SU(2)_F model in which a set of symmetric mass matrices with five texture zeros (having 11 parameters) leads to 22 measurable fermion masses, mixing angles and CP phases, all in agreement with available…

High Energy Physics - Phenomenology · Physics 2007-05-23 Mu-Chun Chen , K. T. Mahanthappa

We study the prediction for leptogenesis in two renormalizable supersymmetric $SO(10)\times A_4$ modular models in which the neutrino mass is dominantly generated by the type I seesaw mechanism. The evolution of the lepton asymmetries are…

High Energy Physics - Phenomenology · Physics 2022-10-26 Gui-Jun Ding , Stephen F. King , Jun-Nan Lu , Bu-Yao Qu

Hermitian mass matrices for the up and down quarks with texture zeroes but with the minimum number of parameters, ten, are investigated. We show how these {\em minimum parameter} forms can be obtained from a general set of hermitian…

High Energy Physics - Phenomenology · Physics 2009-10-31 M. Baillargeon , F. Boudjema , C. Hamzaoui , J. Lindig

General structures of the charged lepton and the neutrino mixing matrices leading to tri-bimaximal leptonic mixing are determined. These are then integrated into an SO(10) model within which detailed fits to fermion masses and mixing angles…

High Energy Physics - Phenomenology · Physics 2011-10-10 Anjan S. Joshipura , Ketan M. Patel

I report the analysis performed on fermion masses and mixing, including neutrino mixing, within the context of a model with hierarchical radiative mass generation mechanism for light charged fermions, mediated by exotic scalar particles at…

High Energy Physics - Phenomenology · Physics 2008-11-26 Albino Hernandez-Galeana

If three right-handed neutrinos are added to the Standard Model, then, for the three known generations, there are six quarks and six leptons. It is then natural to assume that the symmetry considerations that have been applied to the quark…

High Energy Physics - Phenomenology · Physics 2009-11-07 R. Gastmans , Per Osland , Tai Tsun Wu

We study leptogenesis in supersymmetric SO(10) models with a left-right symmetric seesaw mechanism, including flavour effects and the contribution of the next-to-lightest right-handed neutrino. Assuming M_D = M_u and hierarchical light…

High Energy Physics - Phenomenology · Physics 2007-11-01 A. Abada , P. Hosteins , F. -X. Josse-Michaux , S. Lavignac

A complete set of fermion and Higgs superfields is introduced with well-defined SO(10) properties and U(1) x Z_2 x Z_2 family charges from which the Higgs and Yukawa superpotentials are constructed. The structures derived for the four Dirac…

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

We construct two viable extensions of the SM with a heavy vector in the fundamental $SU\left( 2\right) _{L}$ representation and nine SM singlet scalar fields, consistent with the current SM fermion mass spectrum and fermionic mixing…

High Energy Physics - Phenomenology · Physics 2019-09-24 A. E. Cárcamo Hernández , Jonatan Vignatti , Alfonso Zerwekh

Within the framework of unified gauge models, interactions responsible for neutrino masses can also provide mechanisms for nucleon instability. We discuss their implications concretely in the light of recent results on neutrino oscillation…

High Energy Physics - Phenomenology · Physics 2009-08-07 K. S. Babu , Jogesh C. Pati , Frank Wilczek

The phenomenological model that all quark and lepton mass matrices have the same zero texture, namely their (1,1), (1,3) and (3,1) components are zeros, is discussed in the context of SO(10) Grand Unified Theories (GUTs). The mass matrices…

High Energy Physics - Phenomenology · Physics 2009-10-31 K. Matsuda , H. Nishiura , T. Fukuyama

A SUSY SO(10) $\times A_4$ GUT model is constructed for fermion masses and mixing by introducing a minimal set of low dimensional Higgs representations needed to break the guage symmetry down to $SU(3)_c \times U(1)_{em}$. The hierarchy of…

High Energy Physics - Phenomenology · Physics 2015-05-14 Abdelhamid Albaid

We analyze a class of supersymmetric SO(10) grand unified theories with type II seesaw for neutrino masses, where the contribution to PMNS matrix from the neutrino sector has an exact tri-bi-maximal (TBM) form, dictated by a broken S_4…

High Energy Physics - Phenomenology · Physics 2014-10-13 P. S. Bhupal Dev , R. N. Mohapatra , Matt Severson

We consider fermion masses and mixings in a renormalizable SUSY SO(10) GUT with Yukawa couplings of scalar fields in the representation 10 + 120 + 126 bar. We investigate a scenario defined by the following assumptions: i) A single large…

High Energy Physics - Phenomenology · Physics 2008-11-26 W. Grimus , H. Kuhbock

A parameter free, model independent analysis of quark mass matrices is carried out. We find a representation in terms of a diagonal mass matrix for the down (up) quarks and a suitable matrix for the up (down) quarks, such that the mass…

High Energy Physics - Phenomenology · Physics 2011-02-01 D. Falcone , O. Pisanti , L. Rosa

We propose a simple supersymmetric SO(10) GUT model with only doublet Higgs scalars. The fermion mass problem is naturally solved by a new one-loop diagram. R-parity is conserved implying a stable LSP which can explain the dark matter of…

High Energy Physics - Phenomenology · Physics 2009-11-10 Utpal Sarkar

Recently a new mechanism has been proposed to cure the problem of fermion mass hierarchy in the Standard Model (SM) model. In this scenario, all SM charged fermions other than top quark arise from higher dimensional operators involving the…

High Energy Physics - Phenomenology · Physics 2013-05-30 Dilip Kumar Ghosh , R. S. Hundi

A framework based on an effective symmetry that is either G(224)= SU(2)_L x SU(2)_R xSU(4)^c or SO(10) has been proposed (a few years ago) that successfully describes the masses and mixings of all fermions including neutrinos, with seven…

High Energy Physics - Phenomenology · Physics 2009-11-07 Jogesh C. Pati

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

We study the flavour sector in models where the three families of matter are unified in a $(16,3)$ representation of the $SO(10)\times A_4$ group. The necessary ingredients to realize tri-bi-maximal mixing in the lepton sector are…

High Energy Physics - Phenomenology · Physics 2009-01-16 Federica Bazzocchi , Michele Frigerio , Stefano Morisi