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In this work, we study an extension of the Standard Model (SM) based on the gauge symmetry $SU(3)_C\times SU(2)_L\times U(1)_{Y'}\times U(1)_R$ where only the right-handed fermions have nonzero $U(1)_R$ charge and the $U(1)_Y$ weak…

High Energy Physics - Phenomenology · Physics 2020-01-01 Cao H. Nam

We investigate an extension of the Standard Model (SM) incorporating a gauge $ U(1) $ horizontal symmetry that is free of anomalies. This extension introduces four additional un-Higgsed scalar doublets that do not develop vacuum expectation…

High Energy Physics - Phenomenology · Physics 2024-08-06 We-Fu Chang

In the conventional gauged ${B-L}$ extension of the standard model, the $B-L$ charge of the singlet scalar $\chi$, responsible for the breaking of $U(1)_{B-L}$ symmetry, is taken to be 2 such that it can anchor type-I seesaw by giving…

High Energy Physics - Phenomenology · Physics 2026-01-12 Ernest Ma , Partha Kumar Paul , Narendra Sahu

Lepton number violation and its relation to neutrino masses is investigated in several versions of the $SU(3)_c\otimes SU(3)_L\otimes U(1)_x$ model. Spontaneous and explicit violation and conservation of the lepton number are considered. In…

High Energy Physics - Phenomenology · Physics 2015-03-06 Richard H. Benavides , Luis N. Epele , Huner Fanchiotti , Carlos García Canal , William A. Ponce

The embedding in SU(4)xSU(3)xSU(3) of the well studied gauge groups SU(4)xSU(2)xSU(2) and SU(3)xSU(3)xSU(3) naturally leads to family unification as opposed to simple family replication. An inescapable consequence is the predicted existence…

High Energy Physics - Phenomenology · Physics 2011-05-12 Thomas W. Kephart , Qaisar Shafi

We present exact non-perturbative solutions to chiral gauge theories based on the $E_6$ gauge group and several matter fermions in the fundamental $\bf{27}$-dimensional representation. They are obtained when supersymmetric versions are…

High Energy Physics - Theory · Physics 2025-05-14 Andrew Goh , Hitoshi Murayama , Gup Singh , Bethany Suter , Jason Wong

The possibility of generating neutrino mass through see-saw mechanism involving U(1) chiral Peccei-Quinn and scale symmetries breakdown is discussed. We consider a generic scale invariant model which has three Majorana fermions and a…

High Energy Physics - Phenomenology · Physics 2007-05-23 Alex Gomes Dias

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

We discuss the phenomenology of a three-family supersymmetric Standard-like Model derived from the orientifold construction, in which the ordinary chiral states are localized at the intersection of branes at angles. In addition to the…

High Energy Physics - Phenomenology · Physics 2009-09-17 Mirjam Cvetic , Paul Langacker , Gary Shiu

The three electroweak doublet neutrinos $\nu_{e,\mu,\tau}$ of the Standard Model may acquire small seesaw masses, using either three Majorana fermion singlets $N$ or three Majorana fermion triplets $(\Sigma^+,\Sigma^0,\Sigma^-)$. It is…

High Energy Physics - Phenomenology · Physics 2010-04-15 Rathin Adhikari , Jens Erler , Ernest Ma

We examine charge fractionalization by chiral separation in a one-dimensional fermion system described by Luttinger liquid theory. The focus is on the question of whether the fractional charges are quantum mechanically sharp, and in the…

Strongly Correlated Electrons · Physics 2013-05-29 Jon Magne Leinaas , Mats Horsdal , T. H. Hansson

The observed hierarchical charged fermion masses of three generations seem to imply that these masses are originally universal for three generations and then get exponential suppression with "quantized exponents" by some mechanism. We argue…

High Energy Physics - Phenomenology · Physics 2019-12-06 C. S. Lim

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

We all know that in our family of particle physics we have three generations but still don't know why - the so-called "family problem". On other hand, in view of the masses and oscillations, the neutrinos now present some basic difficulty…

High Energy Physics - Phenomenology · Physics 2008-08-18 W-Y. Pauchy Hwang

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

We propose a new gauged $B-L$ extension of the standard model where light neutrinos are of Dirac type, naturally acquiring sub-eV mass after electroweak symmetry breaking, without any additional global symmetries. This is realised by…

High Energy Physics - Phenomenology · Physics 2020-07-15 Dibyendu Nanda , Debasish Borah

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

We analyse stability of almost massless Dirac mode in gauge models with boundary (domain wall) fermions, and consider the possibility of decoupling one of its chiral component by giving it a Majorana mass of the order of the inverse lattice…

High Energy Physics - Lattice · Physics 2009-10-30 S. Aoki , K. Nagai , S. V. Zenkin

I study, in the leptonic sector, the role of the $SU(2)_V$ custodial symmetry $\ti{\cal G}$ which was shown in ref. [1] to control the quantization of the electric charge in the $J=0$ mesonic sector. The electroweak theory is considered,…

High Energy Physics - Phenomenology · Physics 2015-06-25 B. Machet

Hybrid $SU(2) \times U(1)$ models are the models in which $SU(2) \times U(1)$ symmetry is broken down not only spontaneously (as in the Standard Model), but also explicitely by adding a hard mass term for the U(1) field in the lagrangian.…

High Energy Physics - Phenomenology · Physics 2007-05-23 A. Yu. Ignatiev , G. C. Joshi
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