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Related papers: A_4 model for the quark mass matrices

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If a family symmetry exists for the quarks and leptons, the Higgs sector is expected to be enlarged to be able to support the transformation properties of this symmetry. There are however three possible generic ways (at tree level) of…

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

We combine $SO(10)$ Grand Unified Theories (GUTs) with $A_4$ modular symmetry and present a comprehensive analysis of the resulting quark and lepton mass matrices for all the simplest cases. We focus on the case where the three fermion…

High Energy Physics - Phenomenology · Physics 2021-11-24 Gui-Jun Ding , Stephen F. King , Jun-Nan Lu

We calculate quark and lepton masses and quark mixing angles in the framework of a supersymmetric SU(4)$\otimes$SU(2)$_L\otimes$SU(2)$_R$ model where the gauge group is broken at 10$^{16}$ GeV. The model predicts third family top-bottom-tau…

High Energy Physics - Phenomenology · Physics 2010-11-01 B. C. Allanach , S. F. King

We propose a model based on SU(3) family symmetry which leads to a successful description of quark and lepton masses and mixing angles including approximate bi-maximal mixing in the neutrino sector suitable for the LOW or quasi-vacuum solar…

High Energy Physics - Phenomenology · Physics 2009-11-07 S. F. King , G. G. Ross

The mass matrix forms of quarks and leptons are discussed in theory with permutation flavor symmetry. The structure of scalar potential is analyzed in case that electroweak doublet Higgs fields have non-trivial flavor symmetry charges. We…

High Energy Physics - Phenomenology · Physics 2007-05-23 Satoru Kaneko , Hideyuki Sawanaka , Takaya Shingai , Morimitsu Tanimoto , Koichi Yoshioka

We construct a 3-3-1 model based on family symmetry S_4 responsible for the neutrino and quark masses. The tribimaximal neutrino mixing and the diagonal quark mixing have been obtained. The new lepton charge \mathcal{L} related to the…

High Energy Physics - Phenomenology · Physics 2011-02-09 P. V. Dong , H. N. Long , D. V. Soa , V. V. Vien

We propose a supersymmetric model of quark flavor symmetry based on SU(3)colorxSU(3)WxU(1)X x T' where T' (binary tetrahedral group) is a discrete flavor symmetry group. The third (heavy) generation of quarks are assigned to singlet…

High Energy Physics - Phenomenology · Physics 2008-11-26 Sutapa Sen

We investigate the possibility to describe the quark mass hierarchies as well as the CKM quark mixing matrix without fine-tuning in a quark flavour model with modular $A_4$ symmetry. The quark mass hierarchies are considered in the vicinity…

High Energy Physics - Phenomenology · Physics 2023-07-26 S. T. Petcov , M. Tanimoto

We give a detailed description of the model construction procedures about our new approach to the family structure of the standard model. SM-like chiral fermion spectra, largely "derivable" from the gauge anomaly constraints, are formulated…

High Energy Physics - Phenomenology · Physics 2009-10-28 Otto C. W. Kong

We study quark and lepton mass matrices in the $A_4$ modular symmetry towards the unification of the quark and lepton flavors. We adopt modular forms of weights $2$ and $6$ for quarks and charged leptons, while we use modular forms of…

High Energy Physics - Phenomenology · Physics 2021-07-27 Hiroshi Okada , Morimitsu Tanimoto

We consider chiral symmetry breaking AdS / QCD models with cubic and quartic potentials in the scalar sector and a z dependent mass for scalars in the bulk. In these models it is possible to get good mesonic spectra using current quark…

High Energy Physics - Phenomenology · Physics 2011-08-08 Alfredo Vega , Ivan Schmidt

Mass matrix of quarks is studied in the Supersymmetric $E_6$ Grand Unified Theory (GUT). The fundamental representation $\textbf{27}$ in $E_6$ which corresponds to one generation contains two sets of $\textbf{5}^{*}$'s in SU(5), so that…

High Energy Physics - Phenomenology · Physics 2007-05-23 Midori Obara , Gi-Chol Cho , Makiko Nagashima , Akio Sugamoto

A simple specific pattern of the two 3 X 3 quark mass matrices is proposed, resulting in a prediction of the CP phase of the charged-current mixing matrix V_CKM, i.e. sin 2 phi_1 (beta) = 0.733, which is in remarkable agreement with data,…

High Energy Physics - Phenomenology · Physics 2009-11-11 Shao-Long Chen , Ernest Ma

We propose a realistic A4 extension of the Standard Model involving a particular quark-lepton mass relation, namely that the ratio of the third family mass to the geometric mean of the first and second family masses are equal for down-type…

High Energy Physics - Phenomenology · Physics 2013-09-05 S. F. King , S. Morisi , E. Peinado , J. W. F. Valle

We construct a $D_4$ flavor model based on SU(3)_C X SU}(3_L X U(1)_X gauge symmetry responsible for fermion masses and mixings. The neutrinos get small masses from antisextets which are in a singlet and a doublet under $D_4$. If the D_4…

High Energy Physics - Phenomenology · Physics 2014-01-06 V. V. Vien , H. N. Long

We propose a supersymmetric A4 x SU(5) model of quasi-degenerate neutrinos which predicts the effective neutrino mass m_ee relevant for neutrinoless double beta decay to be proportional to the neutrino mass scale, thereby allowing its…

High Energy Physics - Phenomenology · Physics 2011-04-01 Stefan Antusch , Stephen F. King , Martin Spinrath

We propose extended 3HDM and 4HDM models where the SM gauge symmetry is enlarged by the spontaneously broken $S_4$ group, the preserved $Z_2$ and broken $Z_4$ cyclic symmetries. Each model has three active $SU(2)$ scalar doublets, in…

A simple alternative to the usual Pati-Salam model is proposed. The model allows quarks and leptons to be unified with gauge group $SU(4) \otimes SU(2)_L \otimes SU(2)_R$ at a remarkably low scale of about 1 TeV. Neutrino masses in the…

High Energy Physics - Phenomenology · Physics 2009-10-30 R. Foot

Recently, Nishiura and the author have proposed a unified quark-lepton mass matrix model under a family symmetry U(3)$\times$U(3)$'$. The model can give excellent parameter-fitting to the observed quark and neutrino data. The model has a…

High Energy Physics - Phenomenology · Physics 2017-11-22 Yoshio Koide

We impose an $S_3$ symmetry on the quark fields under which two of three quarks transform like a doublet and the remaining one as singlet, and use a scalar sector with the same structure of $SU(2)$ doublets. After gauge symmetry breaking, a…

High Energy Physics - Phenomenology · Physics 2016-01-06 Dipankar Das , Ujjal Kumar Dey , Palash B. Pal