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Related papers: Charge quantization in the largest leptoquark-bile…

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I build a SU(2)left x U(1) electroweak gauge theory of J=0 mesons, which transform like sets of fermion-antifermion composite fields. SU(2)left x U(1) is embedded in a natural way, compatible with the Glashow-Salam-Weinberg model for…

High Energy Physics - Phenomenology · Physics 2007-05-23 B. Machet

A new flipped $SU(3)_C\otimes SU(4)_L\otimes U(1)_X$ model without exotic electric charges is proposed. All the quarks families are arranged in the same representation while leptons generations are in different representations leading to a…

High Energy Physics - Phenomenology · Physics 2021-07-19 Meriem Djouala , Noureddine Mebarki , Habib Aissaoui

For the particular class of \textbf{$SU(4)_{L}\otimes U(1)_{Y}$} electro-weak models without exotic electric charges, some plausible phenomenological predictions - such as the boson mass spectrum and charges of all the fermions involved…

High Energy Physics - Phenomenology · Physics 2014-11-18 Adrian Palcu

We present a supersymmetric model of fermion masses with SU(4)*SU(2)^2*U(1)_X gauge group with matter in fundamental and antisymmetric tensor representations only. The up, down, charged lepton and neutrino Yukawa matrices are distinguished…

High Energy Physics - Phenomenology · Physics 2009-11-10 Thomas Dent , George Leontaris , John Rizos

We obtain electric charge quantization in the context of models based on the gauge symmetry group SU(3) X SU(4) X U(1). The gauge models studied include three families to cancel out anomalies and a set of scalar fields to break…

High Energy Physics - Phenomenology · Physics 2015-06-15 J. M. Cabarcas , J. -Alexis Rodriguez

We present a model to explain LHCb's recent measurements of $R_K$ and $R_{K^{\ast}}$ based on an anomaly-free, spontaneously-broken $U(1)_F$ gauge symmetry, without any fermionic fields beyond those of the Standard Model (SM). The model…

High Energy Physics - Phenomenology · Physics 2021-08-24 B. C. Allanach , Joe Davighi

Following the pioneering Okubo scrutiny of gauge simple groups for the quantum chromodynamics we show the constraints coming from the wondrous predictive leptoquark-bilepton flavordynamics connecting the number of color charges to solution…

High Energy Physics - Phenomenology · Physics 2007-05-23 A. Doff , F. Pisano

Motivated by the Super-Kamiokande data, we revisit models with U(1) symmetries and discuss the origin of neutrino masses and mixings in such theories. We show that, in models with just three light neutrinos and a hierarchy of neutrino…

High Energy Physics - Phenomenology · Physics 2009-10-31 Smaragda Lola , Graham G. Ross

We propose that all light fermionic degrees of freedom, including the Standard Model (SM) fermions and all possible light beyond-the-standard-model fields, are chiral with respect to some spontaneously broken abelian gauge symmetry.…

High Energy Physics - Phenomenology · Physics 2015-07-06 André de Gouvea , Daniel Hernandez

In this work we explore the possibility to fix the number of new non-sequential chiral-type generations of fermions that could be added to the standard model by combining the condition that arise from the anomalies cancellation with the…

High Energy Physics - Phenomenology · Physics 2020-08-11 Elmer Ramirez Barreto , David Romero Abad

Quarks come in three colors and have electric charges in multiples of one-third. There are also three families of quarks and leptons. Whereas the first two properties can be understood in terms of unification symmetries such as SU(5),…

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

A model for electroweak unification of quarks and leptons, in a gauge group $SU_{C}(3)\times SU(4)\times U_{X}(1)$ is constructed. The model requires, three generations of quarks and leptons which are replicas (mirror) of the standard…

High Energy Physics - Phenomenology · Physics 2015-06-03 Fayyazuddin

We first review the three known chiral anomalies in four dimensions and then use the anomaly free conditions to study the uniqueness of quark and lepton representations and charge quantizations in the standard model. We also extend our…

High Energy Physics - Phenomenology · Physics 2017-08-23 C. Q. Geng

We show that in a self-consistent preon model, where Standard Model quarks and leptons are three-body composites confined at a metacolor scale Lambda_cr ~ 10^14 GeV, both leptoquarks and the Standard Model gauge group SU(3)_c x SU(2)_L x…

High Energy Physics - Phenomenology · Physics 2026-05-01 Risto Raitio

We introduce a new class of $U(1)_X$ symmetries where all Standard Model fermions are ``chiral," i.e., the left- and right-handed components have different charges under the $U(1)_X$ symmetry. Gauge anomaly cancellation is achieved by…

High Energy Physics - Phenomenology · Physics 2026-03-19 Hemant Prajapati , Rahul Srivastava

An extension of the gauge group $SU(2)_L\otimes U(1)_Y$ of the standard model to the symmetry group $SU(4)_L\otimes U(1)_X$ (3-4-1 for short) is presented. The model does not contain exotic electric charges and anomaly cancellation is…

High Energy Physics - Phenomenology · Physics 2008-11-26 Luis A. Sanchez , Luis A. Wills-Toro , Jorge I. Zuluaga

A new mechanism is presented for the generation of quark and lepton masses, based on a heavy fourth family and a new sector of massless fermions. The massless fermions have only discrete chiral symmetries and they are confined by the…

High Energy Physics - Phenomenology · Physics 2009-10-22 B. Holdom

Quark has an electric charge either $-1/3$ or $2/3$ and a baryon number $1/3$, where the divisions $3$'s match the color number. Although the electric charge and the baryon number have a nature distinct from the color charge, the matching…

High Energy Physics - Phenomenology · Physics 2023-03-08 Phung Van Dong , Tran Ngoc Hung , Duong Van Loi

There is no reason why the gauge symmetry extension is family universal as in the standard model and the most well-motivated models, e.g. left-right symmetry and grand unification. Hence, we propose a simplest extension of the standard…

High Energy Physics - Phenomenology · Physics 2023-11-21 Duong Van Loi , Phung Van Dong

We discuss extension of the electroweak gauge group to $SU(3)_L \times SU(3)_R \times U(1)_{XL} \times U(1)_{XR}$. This adds new leptons to the familiar 331-model. The explanation for three light quark-lepton families remains but new…

High Energy Physics - Phenomenology · Physics 2025-01-20 Claudio Corianò , Paul H. Frampton , Dario Melle