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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

Based on the $SU(3)_{F}$ gauge family symmetry model which was proposed to explain the observed mass and mixing pattern of neutrinos, we investigate the symmetry breaking, the mixing pattern in quark and lepton sectors, and the contribution…

High Energy Physics - Phenomenology · Physics 2016-01-20 Shou-Shan Bao , Zhuo Liu , Yue-Liang Wu

Within the framework of the two-Higgs Doublet Model (2HDM), we attempt to find some discrete, non-abelian flavour symmetry which could provide an explanation for the masses and mixing matrix elements of leptons. Unlike the Standard Model,…

High Energy Physics - Phenomenology · Physics 2018-09-12 Piotr Chaber , Bartosz Dziewit , Jacek Holeczek , Monika Richter , Marek Zrałek , Sebastian Zając

Why the charged lepton mass formula m_e +m_\mu +m_\tau = {2/3} (\sqrt{m_e}+\sqrt{m_\mu} +\sqrt{m_\tau})^2 is mysterious is reviewed, and guiding principles to solve the mystery are presented. According to the principles, an example of such…

High Energy Physics - Phenomenology · Physics 2007-05-23 Yoshio Koide

We present an SU(12) unification model with three light chiral families, avoiding any external flavor symmetries. The hierarchy of quark and lepton masses and mixings is explained by higher dimensional Yukawa interactions involving Higgs…

High Energy Physics - Phenomenology · Physics 2013-05-30 Carl H. Albright , Robert P. Feger , Thomas W. Kephart

We consider the possibility that the neutral-current $B$ anomalies are due to radiative corrections generated by Yukawa interactions of quarks and leptons with new vector-like quark and lepton electroweak doublets and new Standard Model…

High Energy Physics - Phenomenology · Physics 2018-12-27 B. Grinstein , S. Pokorski , G. G. Ross

Lepton flavour violation has been proposed as a significant test of supersymmetric unification. Here we show that such signals are also a generic feature of supersymmetric string unified models in which there is no simple unified gauge…

High Energy Physics - Phenomenology · Physics 2016-08-25 S. F. King , M. Oliveira

Fermion masses and mixing matrices can be described in terms of spontaneously broken (global or gauge) flavor symmetries. We propose a little-Higgs inspired scenario in which an SU(2)xU(1) gauge flavor symmetry is spontaneously (and…

High Energy Physics - Phenomenology · Physics 2009-11-10 F. Bazzocchi , S. Bertolini , M. Fabbrichesi , M. Piai

We show that the mass matrix of electrically neutral gauge bosons in the recently proposed model based on SU(3)_C X SU(3)_L X U(1)_X group with three lepton singlets [1] has two exact eigenvalues: a zero corresponding the photon mass and…

High Energy Physics - Phenomenology · Physics 2015-05-08 Hoang Ngoc Long

Leptophobic Z^\prime gauge boson appears naturally in many grand unified theories, such as flipped SU(5) or string-inspired E_6 models. This elusive particle easily escapes the direct/indirect detections because it does not couple to…

High Energy Physics - Phenomenology · Physics 2014-11-18 Seungwon Baek , Jong Hun Jeon , C. S. Kim

We proposed a viable and predictive model based on the $SU(3)_C \times SU(3)_L \times U(1)_X$ gauge symmetry, supplemented by the global $U(1)_{Lg}$ symmetry, the $S_4$ family symmetry and several auxiliary cyclic symmetries, which…

High Energy Physics - Phenomenology · Physics 2024-06-14 A. E. Cárcamo Hernández , Juan Marchant González , M. L. Mora-Urrutia , Daniel Salinas-Arizmendi

A U(3) family gauge boson model is investigated based on U(3)$\times$[U(1)]$^3$ gauge symmetry. In this model, of nine U(3) family gauge bosons $A_i^{\ j}$, those with $i=j$ are considerable heavy compared with those with $i \neq j$, so…

High Energy Physics - Phenomenology · Physics 2013-09-25 Yoshio Koide

We propose new lepton-mixing textures that may be enforced through well-defined symmetries in renormalizable models. Each of our textures has four sum rules for the neutrino mass observables. The models are based on the type-I seesaw…

High Energy Physics - Phenomenology · Physics 2019-09-04 D. Jurciukonis , L. Lavoura

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

We postulate that the neutrino mass matrix in the lepton flavour basis is an S3 group matrix in the natural representation of S3. This immediately requires one neutrino to be trimaximally mixed, as suggested by the solar neutrino data. We…

High Energy Physics - Phenomenology · Physics 2009-11-10 P. F. Harrison , W. G. Scott

Assuming the existence of a gauge boson $X$ which couples to $B - 3 L_\tau$, we discuss the present experimental constraints on $g_X$ and $m_X$ from $Z \to l^+ l^-$ and $Z \to \bar f f X~(f = q, \nu_\tau, \tau)$. We also discuss the…

High Energy Physics - Phenomenology · Physics 2009-10-31 Ernest Ma , D. P. Roy

We consider an $SU(3)_L\otimes U(1)_N$ model for the electroweak interactions which includes extra charged leptons which do not mix with the known leptons. These new leptons couple to $Z^0$ only through vector currents. We consider…

High Energy Physics - Phenomenology · Physics 2009-10-22 V. Pleitez , M. D. Tonasse

We present a common explanation of the fermion mass hierarchy and the large lepton mixing angles in the context of a grand unified flavor and gauge theory (GUTF). Our starting point is a SU(3)xU(1) flavor symmetry and a SO(10) GUT, a basic…

High Energy Physics - Phenomenology · Physics 2008-11-26 F. Bazzocchi , S. Morisi , M. Picariello , E. Torrente-Lujan

We present a simple $U(1)_{B_3-3L_\mu}$ gauge Standard Model extension that can easily account for the anomalies in $R(K)$ and $R(K^*)$ reported by LHCb. The model is economical in its setup and particle content. Among the Standard Model…

High Energy Physics - Phenomenology · Physics 2018-11-07 Cesar Bonilla , Tanmoy Modak , Rahul Srivastava , Jose W. F. Valle

Brannen has recently pointed out that the observed charged lepton masses satisfy the relation m_e +m_\mu +m_\tau = {2/3} (\sqrt{m_e}+\sqrt{m_\mu}+\sqrt{m_\tau})^2, while the observed neutrino masses satisfy the relation m_{\nu 1} +m_{\nu 2}…

High Energy Physics - Phenomenology · Physics 2008-11-26 Yoshio Koide