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Related papers: The 33311 Left-Right Bilepton Model

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To explain quark and lepton masses and mixing angles, one has to extend the standard model, and the usual practice is to put the quarks and leptons into irreducible representations of discrete groups. We argue that discrete flavor…

High Energy Physics - Phenomenology · Physics 2016-04-27 Carl H. Albright , Robert P. Feger. , Thomas W. Kephart

By extending the electroweak gauge group to $SU(3)_L\times U(1)_Y$, the 331 model incorporates dilepton gauge bosons $Y$ which do not respect individual lepton family number. We point out that, in addition to family diagonal couplings such…

High Energy Physics - Phenomenology · Physics 2010-11-01 James T. Liu , Daniel Ng

Consider the addition of a right-handed SU(2) fermion multiplet (with neither color nor hypercharge) to each family of quarks and leptons. The resultant theory admits a new U(1) gauge symmetry only if the additional multiplet is a singlet…

High Energy Physics - Phenomenology · Physics 2007-05-23 Ernest Ma

In this work we study an effective version of the 3-3-1 model, in which the particle content is the same of the 2HDM. We show that the inherited structure from the $SU(3)_C \otimes SU(3)_L \otimes U(1)_X$ gauge group has a series of…

High Energy Physics - Phenomenology · Physics 2023-04-07 A. L. Cherchiglia , O. L. G. Peres

We present a 3-3-1 model as a subgroup of SU(4)PS X SU(4)L+R gauge symmetry with symmetry-breaking pattern SU(4)->SU(3) X U(1) for both SU(4) groups. A Pleitez-Frampton type of 3C-3L-1X model is obtained with charged heavy leptons and…

High Energy Physics - Phenomenology · Physics 2009-11-10 Sutapa Sen , Aparna Dixit

In order to explain the fermions masses and mixing parameters appearing in the lepton sector of the Standard Model, one proposes the extension of its symmetry. A discrete, non-abelian subgroup of $U(3)$ is added to the gauge group…

High Energy Physics - Phenomenology · Physics 2017-09-13 Bartosz Dziewit , Jacek Holeczek , Monika Richter , Sebastian Zając , Marek Zrałek

The extended electroweak $\mathrm{SU(3)_c \otimes SU(3)_L \otimes U(1)_X}$ symmetry framework "explaining" the number of fermion families is revisited. While $331$-based schemes can not easily be unified within the conventional field theory…

High Energy Physics - Phenomenology · Physics 2016-09-07 Andrea Addazi , J. W. F. Valle , C. A. Vaquera-Araujo

The uniqueness of the hypercharge assignments in the three fermion families leptoquark-bilepton $SU(3)_C \times SU(4)_L \times U(1)_N$ model is established. Although the gauge group contains an explicit U(1) factor, freedom from triangle…

High Energy Physics - Phenomenology · Physics 2008-11-26 A. Doff , F. Pisano

The Standard Model is extended by a SU(2)L singlet of vector leptoquarks. An additional SU(4) gauge symmetry between right-handed up quarks and right-handed leptons is introduced to render the model renormalizable. The arrangement is made…

High Energy Physics - Phenomenology · Physics 2008-11-26 Andreas Blumhofer , Bodo Lampe

We construct a model of quark-lepton unification at the TeV scale based on an $SU(4)$ gauge symmetry, while still having acceptable neutrino masses and enough suppression in flavor changing neutral currents. An approximate $U(2)$ flavor…

High Energy Physics - Phenomenology · Physics 2018-05-16 Admir Greljo , Ben A. Stefanek

We consider an extended gauge group for the electroweak interaction: SU(2)_1 \times SU(2)_2 \times U(1)_Y where the first and second generations of fermions couple to SU(2)_1 while the third generation couples to SU(2)_2. Bounds based on…

High Energy Physics - Phenomenology · Physics 2011-01-25 David Muller , Satya Nandi

We build a supersymmetric version of a recently proposed SU(3)xSU(3)xU(1)X model with heavy charged lepton and no bilepton gauge bosons.The model is an anomaly free, three generation extension of the Standard model with SU(3)L x U(1)gauge…

High Energy Physics - Phenomenology · Physics 2007-05-23 Sutapa Sen , Aparna Dixit

Using the most recent experimental data on parameters of the standard electroweak theory, as well as renormalisation group equations with a boundary matching condition, we derive a refined and more accurate value for the mass of the…

High Energy Physics - Phenomenology · Physics 2021-06-30 Claudio Corianò , Paul H. Frampton

It now appears phenomenologically that the third family of fundamental fermions may be essentially different fron the first two. Particularly the high value (174GeV?) of the top quark mass suggests a special role. In the standard model all…

High Energy Physics - Phenomenology · Physics 2007-05-23 Paul H. Frampton

After some general remarks about SU_L(4) electroweak unification, the model is extended to SU_L(4)xU_X(1) to accomodate fractionally charged quarks. The unification scale is expected to be in TeV region. A right-handed Majorana neutrino…

High Energy Physics - Phenomenology · Physics 2008-11-26 Fayyazuddin , Riazuddin

In the upcoming LHC Run 2, at $\sqrt{s} \sim13$ TeV, it is suggested to seek unusually charged ($Q= -4/3$ and $+5/3$) quarks with mass $M_Q \sim 3$ TeV which carry lepton number ($L = +2$ and $-2$ respectively) and decay superweakly to a…

High Energy Physics - Phenomenology · Physics 2015-04-23 Paul Howard Frampton

Among the particles being searched for at the LHC beyond the Standard Model are bileptons, which are doubly charged gauge bosons. Bileptons are predicted by several Standard Model extensions, including the so-called 331 models with $\beta =…

High Energy Physics - Phenomenology · Physics 2025-07-31 Stefano Morisi , Giovanna Paola Perdonà , Giulia Ricciardi

In the context of the local gauge group $SU(3)_c\otimes SU(3)_L\otimes U(1)_X$, we look for possible four family models, where all the particles carry ordinary electric charges. Thirteen different anomaly-free fermion structures emerge, out…

High Energy Physics - Phenomenology · Physics 2014-11-21 Richard H. Benavides , William A. Ponce , Yithsbey Giraldo

We consider a modification of the standard electroweak model with the third quark generation and the $\tau$-lepton in vector representations of $SU(2)\otimes U(1)_Y$ electroweak symmetry. This is a new way to implement right-handed currents…

High Energy Physics - Phenomenology · Physics 2008-02-03 Vicente Pleitez

We propose a realistic theory based on the $\mathrm{SU(3)_c \otimes SU(3)_L \otimes SU(3)_R \otimes U(1)_{X}}$ gauge group which requires the number of families to match the number of colors. In the simplest realization neutrino masses…

High Energy Physics - Phenomenology · Physics 2017-01-24 Mario Reig , José W. F. Valle , C. A. Vaquera-Araujo