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Related papers: Nonzero $\theta_{13}$ in $SO(3) \rightarrow A_4$ l…

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In this work, we have proposed a modular $A_4$ symmetric model of neutrino mass which, simultaneously, explains observed baryon asymmetry of the Universe(BAU). In minimal extension of the standard model(SM) with two right-handed neutrinos…

High Energy Physics - Phenomenology · Physics 2021-10-04 Monal Kashav , Surender Verma

We present a new model of the lepton sector that uses a family symmetry A4 to make predictions for lepton mixing which are invariant under any permutation of the three flavours. We show that those predictions broadly agree with the…

High Energy Physics - Phenomenology · Physics 2015-06-16 P. M. Ferreira , L. Lavoura , P. O. Ludl

A possible interplay between the two terms of the general type-II seesaw formula is exercised which leads to the generation of nonzero $\theta_{13}$. The specific flavor structure of the model, guided by the $A_4 \times Z_4 \times Z_3$…

High Energy Physics - Phenomenology · Physics 2016-01-13 Biswajit Karmakar , Arunansu Sil

In a new application of the discrete non-Abelian symmetry A_4 using the canonical seesaw mechanism, a three-parameter form of the neutrino mass matrix is derived. It predicts the following mixing angles for neutrino oscillations:…

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

I review the construction of a model for lepton masses based on the flavour symmetry group A4 x U(1) reproducing the so-called tri-bimaximal lepton mixing scheme, in eccelent agreement with current data. The model predicts a neutrino…

High Energy Physics - Phenomenology · Physics 2009-04-25 Ferruccio Feruglio

I mainly describe neutrino masses and oscillations in the gauge model with $SO(3)_{F}$ lepton flavor symmetry and with two Higgs triplets. It is shown how the maximal mixing between $\nu_{\mu}$ and $\nu_{\tau}$ neutrinos comes out naturally…

High Energy Physics - Phenomenology · Physics 2009-10-31 Yue-Liang Wu

The leptonic Higgs doublet model of neutrino masses is implemented with an A_4 discrete symmetry (the even permutation of 4 objects or equivalently the symmetry of the tetrahedron) which has 4 irreducible representations: 1, 1', 1'', and 3.…

High Energy Physics - Phenomenology · Physics 2009-11-07 Ernest Ma , G. Rajasekaran

Using the type II seesaw approach and properties of discrete flavor symmetry group representations, we build a supersymmetric $A_{4}\times A_{3}$\ neutrino model with $\theta_{13}\neq0$. After describing the basis of this model--which is…

High Energy Physics - Phenomenology · Physics 2016-06-22 R. Ahl Laamara , M. A Loualidi , E. H Saidi

Effects of the 1-3 leptonic mixing on the solar neutrino observables are studied and the signatures of non-zero $\theta_{13}$ are identified. For this we have re-derived the formula for $3\nu$-survival probability including all relevant…

High Energy Physics - Phenomenology · Physics 2009-11-10 Srubabati Goswami , Alexei Yu. Smirnov

Recent experiments indicate a departure from the exact Tri-Bimaximal mixing by measuring definitive non-zero value of $\theta_{13}$. Within the framework of type I seesaw mechanism, we reconstruct the triangular Dirac neutrino mass matrix…

High Energy Physics - Phenomenology · Physics 2012-11-06 H. B. Benaoum

We discuss the neutrino masses and mixings as the realization of an $S_{3}$ flavour permutational symmetry in two models, namely the Standard Model and an extension of the Standard Model with three Higgs doublets. In the $S_3$ Standard…

High Energy Physics - Phenomenology · Physics 2013-03-26 F. Gonzalez Canales , A. Mondragon , M. Mondragon

We revisit the $A_4$ model for leptons in light of new result of NuFIT 3.2. We introduce a new flavon $\eta$ transforming as $A_4$ singlet $1'$ or $1"$ which couples to both charged leptons and neutrinos in next-leading order operators. The…

High Energy Physics - Phenomenology · Physics 2019-12-06 Sin Kyu Kang , Yusuke Shimizu , Kenta Takagi , Shunya Takahashi , Morimitsu Tanimoto

In order to explain the non-hierarchical neutrino mixing angles and the absence of lepton flavor violating processes in the context of warped extra dimensions one needs to introduce bulk flavor symmetries. We present a simple model of…

High Energy Physics - Phenomenology · Physics 2010-05-12 C. Csaki , C. Delaunay , C. Grojean , Y. Grossman

We consider lepton mixing in an extension of the Standard Model with three right-handed neutrino singlets. We require that the three lepton numbers L_e, L_\mu, and L_\tau be separately conserved in the Yukawa couplings, and we assume that…

High Energy Physics - Phenomenology · Physics 2010-02-03 W. Grimus , L. Lavoura

We study a second CP symmetry compatible with the $A_4$ flavor group, which interchanges the representations $\mathbf{1}'$ and $\mathbf{1}"$. We analyze the lepton mixing patterns arising from the $A_4$ and CP symmetry broken to residual…

High Energy Physics - Phenomenology · Physics 2016-11-23 Cai-Chang Li , Jun-Nan Lu , Gui-Jun Ding

Recent observations for a non-zero $\theta_{13}$ have come from various experiments. We study a model of lepton mixing with a 2-3 flavor symmetry to accommodate the sizable $\theta_{13}$ measurement. In this work, we derive deviations from…

High Energy Physics - Phenomenology · Physics 2015-03-19 Ahmed Rashed

Based on the SO(3) gauge symmetry for three family leptons and general see-saw mechanism, we present a simple scheme that allows three nearly degenerate Majorana neutrino masses needed for hot dark matter. The vacuum structure of the…

High Energy Physics - Phenomenology · Physics 2009-10-31 Yue-Liang Wu

The exact solution for the neutrino mass matrix of the Zee-Babu model is derived. Tribimaximal mixing imposes conditions on the Yukawa couplings, from which the normal mass hierarchy is preferred. The derived conditions give a possibility…

High Energy Physics - Phenomenology · Physics 2014-05-08 H. N. Long , V. V. Vien

Recently Babu, Ma and Valle proposed a model of quark and lepton mixing based on $A_4$ symmetry. Within this model the lepton and slepton mixings are intimately related. We perform a numerical study in order to derive the slepton masses and…

High Energy Physics - Phenomenology · Physics 2010-04-06 M. Hirsch , J. C. Romao , S. Skadhauge , J. W. F. Valle , A. Villanova del Moral

The Standard Model does not explain the hierarchy problem. Before the discovery of nonzero lepton mixing angle {\theta}13 high hopes in explanation of the shape of the lepton mixing matrix were combined with non abelian symmetries.…

High Energy Physics - Phenomenology · Physics 2017-05-24 Bartosz Dziewit , Jacek Holeczek , Monika Richter , Sebastian Zając , Marek Zrałek
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