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Related papers: mu-tau symmetry in Zee-Babu model

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The Superkamiokande experiment suggests the large flavor mixing between nu_mu and nu_tau. We show that the mixing angle receives significant corrections from the renormalization group equation (RGE) when both the second and the third…

High Energy Physics - Phenomenology · Physics 2011-03-10 N. Haba , N. Okamura , M. Sugiura

The neutrino $\mu$-$\tau$ reflection symmetry has been attracting a lot of attention as it predicts the interesting results $\theta^{}_{23} = \pi/4$ and $\delta = \pm \pi/2$. But it is reasonable to consider breakings of such a symmetry…

High Energy Physics - Phenomenology · Physics 2017-10-11 Zhen-hua Zhao

We find that the lepton flavor mixing matrix $U$ should possess a partial $\mu$-$\tau$ permutation symmetry $|U^{}_{\mu 1}| = |U^{}_{\tau 1}|$, and the latter predicts a novel correlation between the Dirac CP-violating phase $\delta$ and…

High Energy Physics - Phenomenology · Physics 2014-09-01 Zhi-zhong Xing , Shun Zhou

We examine in detail the neutrino masses and mixing patterns in an extension of the minimal supersymmetric standard model with three gauge-singlet neutrinos and R-parity violation. The Majorana masses for the gauge-singlet neutrinos as well…

High Energy Physics - Phenomenology · Physics 2010-04-30 Pradipta Ghosh , Sourov Roy

Recent atmospheric neutrino data at Super-Kamiokande suggest the large flavor mixing of neutrinos. Models for the lepton mass matrix, which give the near-maximal flavor mixing, are discussed in the three family model. Especially, details of…

High Energy Physics - Phenomenology · Physics 2008-11-26 Morimitsu Tanimoto

Many neutrino mixing scenarios that have \mu-\tau symmetry with \theta_{13}=0 are in disagreement with recent experimental results that indicate a nonzero value for \theta_{13}. We investigate the effect of small perturbations on Majorana…

High Energy Physics - Phenomenology · Physics 2013-01-07 Jiajun Liao , D. Marfatia , K. Whisnant

We develop a see-saw model for neutrino masses and mixing with an S3\times Z3 symmetry. It involves an interplay of Type-I and Type-II see-saw contributions of which the former is subdominant. The S3 \times Z3 quantum numbers of the fermion…

High Energy Physics - Phenomenology · Physics 2017-02-01 Soumita Pramanick , Amitava Raychaudhuri

The observed pattern of neutrino mixing may be the result of a 2-3($ \mu- \tau$) symmetry in the leptonic sector. We consider a two Higgs doublet model with a 2-3 symmetry in the down type quark and the charged lepton sector. The breaking…

High Energy Physics - Phenomenology · Physics 2009-11-11 Alakabha Datta , Patrick J. O'Donnell

We demonstrate that, for every grand unified model based on a conventional type I seesaw mechanism leading to a normal light neutrino mass hierarchy, one can easily generate a corresponding model with an inverted hierarchy which yields the…

High Energy Physics - Phenomenology · Physics 2009-11-10 Carl H. Albright

The $\mu$-$\tau$ exchange symmetry in the neutrino mass matrix and its breaking as a perturbation are discussed. The exact $\mu$-$\tau$ symmetry restricts the 2-3 and 1-3 neutrino mixing angles as $\theta_{23} = \pi/4$ and $\theta_{13} = 0$…

High Energy Physics - Phenomenology · Physics 2020-07-15 Takeshi Fukuyama , Yukihiro Mimura

We review recent developments in theoretical models for neutrino masses and mixing. Emphases are given to models based on finite group family symmetries. In particular, we describe one recent model based on SU(5), in which both the…

High Energy Physics - Phenomenology · Physics 2009-04-17 Mu-Chun Chen , K. T. Mahanthappa

To generate the minimal neutrino Majorana mass matrix that has a free solar mixing angle and Delta m_sol^2 = 0 it suffices to implement an O(2) symmetry, or one of its subgroups SO(2), Z_N (N>2), or D_N (N>2). This O(2) generalizes the…

High Energy Physics - Phenomenology · Physics 2012-02-23 Julian Heeck , Werner Rodejohann

The naturalness of maximal mixing between myon- and tau-neutrinos is investigated. A spontaneously broken nonabelian generation symmetry can explain a small parameter which governs the deviation from maximal mixing. In many cases all three…

High Energy Physics - Phenomenology · Physics 2008-11-26 C. Wetterich

We consider an $U(1)_{L_\mu -L_\tau}$ extended left-right symmetric gauge theory where the neutrino masses are generated through inverse seesaw mechanism. In this model the muon $(g-2)$ anomaly is accounted for by the mediation of…

High Energy Physics - Phenomenology · Physics 2022-11-04 Chayan Majumdar , Supriya Senapati , S. Uma Sankar , Urjit A. Yajnik

Non-vanishing U_{e3} has been theoretically related to a certain flavor symmetry breaking in the neutrino sector. We propose a scenario to break the mu-tau symmetry so as to accommodate the non-vanishing U_{e3}. Our scenario is constructed…

High Energy Physics - Phenomenology · Physics 2011-07-19 Y. H. Ahn , Sin Kyu Kang , C. S. Kim , Jake Lee

The Zee-Babu model is a minimal realization of radiative neutrino mass generation mechanism at the two-loop level. We study the phenomenology of this model at future multi-TeV muon colliders. After imposing all theoretical and low-energy…

High Energy Physics - Phenomenology · Physics 2024-03-14 Adil Jueid , Talal Ahmed Chowdhury , Salah Nasri , Shaikh Saad

Models of neutrino masses are discussed capable of explaining in a natural way the maximal mixing between $\nu_{\mu}$ and $\nu_{\tau}$ observed by the Super-Kamiokande collaboration. For three generations of leptons two classes of such…

High Energy Physics - Phenomenology · Physics 2009-10-31 M. Jezabek , Y. Sumino

We built an extended 2HDM theory with a spontaneously broken $U(1) _{X}$ global symmetry, where the tree level Universal Seesaw Mechanism generates the mass hierarchy of the Standard Model charged fermions and the Zee-Babu mechanism…

High Energy Physics - Phenomenology · Physics 2024-10-25 A. E. Cárcamo Hernández , Diego Restrepo , Ivan Schmidt , Óscar Zapata

If the neutrino mass spectrum turns out to be m^{}_3 < m^{}_1 < m^{}_2, one may choose to relabel it as m^{\prime}_1 < m^{\prime}_2 < m^{\prime}_3 such that all the masses of fundamental fermions with the same electrical charges are in…

High Energy Physics - Phenomenology · Physics 2018-01-17 Zhi-zhong Xing , Jing-yu Zhu

We study the Zee model in the framework of the split fermion model in $M_4\times S_1/Z_2$ spacetime. Neutrino masses are generated through 1-loop diagrams without the right-handed neutrinos introduced. By assuming an order one anarchical…

High Energy Physics - Phenomenology · Physics 2011-02-15 We-Fu Chang , I-Ting Chen , Siao-Cing Liou