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Related papers: A Constraint on Yukawa-Coupling Unification from L…

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With the strong experimental evidence for standard neutrino mass and mixings, there exists now a possibility of the lepton flavor violating process e\sup + mu \sup - \arrow W \sup + W \sup -, which would occur via t-channel neutrino…

High Energy Physics - Phenomenology · Physics 2007-05-23 Jai Kumar Singhal , Sardar Singh , A K Nagawat

Lepton flavor violation (LFV) is studied within a realistic unified framework, based on supersymmetric SO(10) or an effective G(224) = SU(2)_L\times SU(2)_R\times SU(4)^c symmetry, that successfully describes (i) fermion masses and mixings,…

High Energy Physics - Phenomenology · Physics 2014-11-18 K. S. Babu , Jogesh C. Pati , Parul Rastogi

Lepton flavour non-conserving processes are examined in the context of unified models with U(1)-family symmetries which reproduce successfully the low-energy hierarchy of the fermion mass spectrum and the Kobayashi - Maskawa mixing. These…

High Energy Physics - Phenomenology · Physics 2009-10-31 G. K. Leontaris , N. D. Tracas

We study the implications of an approximate $U(2)^5$ flavor symmetry at the TeV scale, under the assumption of new physics predominantly coupled to the third-generation fermions, focusing on the breaking of the $U(2)_\ell$ subgroup…

High Energy Physics - Phenomenology · Physics 2025-11-21 Sebastiano Covone , Pol Morell , Arianna Tinari

To address fermion mass hierarchy and flavor mixings in the quark and lepton sectors, a minimal flavor structure without any redundant parameters beyond phenomenological observables is proposed via decomposition of the Standard Model Yukawa…

High Energy Physics - Phenomenology · Physics 2022-01-17 Ying Zhang

The recent discovery of nonzero $\theta_{13}$ (equal to Cabbibo angle $\theta_C$ up to a factor of $\sqrt{2}$), the masses of supersymmetric particles $\gapp$ TeV from LHC data, and the sum of three active neutrino masses $\sum_i…

High Energy Physics - Phenomenology · Physics 2013-11-15 Abhijit Samanta

We investigate the lepton flavor violating (LFV) rare decays in the supersymmetric minimal seesaw model in which the Frampton-Glashow-Yanagida ansatz is incorporated. The branching ratio of $\mu \to e \gamma$ is calculated in terms of the…

High Energy Physics - Phenomenology · Physics 2008-11-26 Wan-lei Guo

We have investigated the lepton flavor violation in the supersymmetric framework assuming the large mixing angle MSW solution with the quasi-degenerate and the inverse-hierarchical neutrino masses. In the case of the quasi-degenerate…

High Energy Physics - Phenomenology · Physics 2009-11-07 A. Kageyama , S. Kaneko , N. Shimoyama , M. Tanimoto

Scalar leptoquarks naturally arise within unified theories, offering a promising avenue for addressing one of the most significant challenges of the Standard Model--the existence of non-zero neutrino masses. In this work, we present a…

High Energy Physics - Phenomenology · Physics 2024-05-22 Kevin Hinze , Shaikh Saad

We consider the lepton-flavor violating(LFV) processes $l_{i}\to l_{j}\gamma$ in the framework of topcolor assisted technicolor(TC2) models. We find that the new gauge boson $Z^{\prime}$ predicted by TC2 models can give significantly…

High Energy Physics - Phenomenology · Physics 2018-01-17 Chongxing Yue , Qingjun Xu , Guoli Liu

In R-parity-violating (RPV) supersymmetric models, light neutralinos with masses from the GeV-scale down to even zero are still allowed by all laboratory constraints. They are further consistent with dark matter observations, as they decay…

High Energy Physics - Phenomenology · Physics 2024-05-15 Herbi K. Dreiner , Dominik Köhler , Saurabh Nangia , Martin Schürmann , Zeren Simon Wang

The group E_6 for grand unification is combined with the generation symmetry group SO(3) x Z(2). The coupling matrices in the Yukawa interaction are identified with the vacuum expectation values of scalar flavons. The symmetric part of this…

High Energy Physics - Phenomenology · Physics 2012-04-20 Berthold Stech

The charged lepton flavour violating (LFV) radiative decays, $\mu\to e+\gamma$, $\tau\to \mu+\gamma$ and $\tau\to e +\gamma$ are investigated in a class of supersymmetric $A_4$ models with three heavy right-handed (RH) Majorana neutrinos,…

High Energy Physics - Phenomenology · Physics 2014-11-20 C. Hagedorn , E. Molinaro , S. T. Petcov

We present a class of warped extra dimensional models whose flavor violating interactions are much suppressed compared to the usual anarchic case due to flavor alignment. Such suppression can be achieved in models where part of the global…

High Energy Physics - Phenomenology · Physics 2013-05-29 Csaba Csaki , Gilad Perez , Ze'ev Surujon , Andreas Weiler

The semileptonic decays $\tau^- \to \mu^- M (M=\pi^0,\eta,\eta')$ could be sensitive probe for new physics scenarios with lepton flavor violation(LFV). Motivated by the recent Belle measurement, we investigate these decays in type III…

High Energy Physics - Phenomenology · Physics 2009-11-11 Wenjun Li , Yadong Yang , Xiangdan Zhang

I analyze the predictions for the strong gauge coupling, $\alpha_3(M_Z) $, and the top quark and light Higgs masses in the framework of gauge and bottom-tau Yukawa coupling unification in the minimal supersymmetric standard model. These…

High Energy Physics - Phenomenology · Physics 2007-05-23 M. Carena

Within low-scale seesaw mechanisms, such as the inverse and linear seesaw, one expects (i) potentially large lepton flavor violation (LFV) and (ii) sizeable non-standard neutrino interactions (NSI). We consider the interplay between the…

High Energy Physics - Phenomenology · Physics 2015-05-30 D. V. Forero , S. Morisi , M. Tortola , J. W. F. Valle

In the supersymmetric left-right model, the light neutrino masses are given by the Type-II seesaw mechanism. A duality property about this mechanism indicates that there exist eight possible Higgs triplet Yukawa couplings which result in…

High Energy Physics - Phenomenology · Physics 2015-05-13 Wei Chao

We interpret anomalies, deviations, from the standard model as being in fact due to effects not given by perturbation, because the top Yukawa coupling is after all so large that not by perturbation effects become important. Most of the…

High Energy Physics - Phenomenology · Physics 2019-05-02 Colin D. Froggatt , Holger Bech Nielsen

Heavy neutral leptons (HNLs) can explain the origin of neutrino masses and oscillations over a wide range of masses. Direct experimental probes of HNLs become unfeasible for masses significantly above the electroweak scale.Consequently, the…

High Energy Physics - Phenomenology · Physics 2025-07-15 Kevin A. Urquía-Calderón , Inar Timiryasov , Oleg Ruchayskiy
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