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A simple extension of the Standard Model (SM), based on the gauge group $SU(3)_C\otimes SU(3)_L\otimes U(1)_Y$ with $Y$ being the hypercharge, is considered. We show that, by imposing an approximate global $SU(2)_L\times SU(2)_R$ custodial…

High Energy Physics - Phenomenology · Physics 2016-03-30 Le Tho Hue , Le Duc Ninh

The quartic gauge boson couplings in the ${SU(3)}_C \otimes {SU(3)}_L \otimes {U(1)}_N$ models are presented. We find that the couplings of four {\it differrent} gauge bosons may have unusual Lorentz structure and the couplings sastify the…

High Energy Physics - Phenomenology · Physics 2008-11-26 D. T. Binh , D. T. Huong , Tr. T. Huong , H. N. Long , D. V. Soa

Many models beyond the Standard Electroweak Theory, top-down or bottom-up, contain extensions of the gauge symmetry group by extra U(1)' factors which can be understood or treated as subgroups of E(6). A brief overview of such models is…

High Energy Physics - Phenomenology · Physics 2011-08-04 Jens Erler , Paul Langacker , Shoaib Munir , Eduardo Rojas

Recently, ``Higgsless'' models of electroweak symmetry breaking have been proposed. Based on compactified five-dimensional gauge theories, these models achieve unitarity of electroweak boson self-interactions through the exchange of a tower…

High Energy Physics - Phenomenology · Physics 2009-11-10 R. Sekhar Chivukula , Hong-Jian He , Masafumi Kurachi , Elizabeth H. Simmons , Masaharu Tanabashi

The totality of present neutrino data seems to require four light neutrinos, but only three of them can be the neutral components of left-handed lepton doublets. To accommodate one or more naturally light singlet neutrino(s), an extra U(1)…

High Energy Physics - Phenomenology · Physics 2015-06-25 Ernest Ma

Some versions of the electroweak SU(3)$_L\otimesU(1)_X$ models cannot be treated within perturbation theory at energies of few TeV. An extended version for these models is proposed which is perturbative even at TeV scale posing no…

High Energy Physics - Phenomenology · Physics 2009-11-10 Alex G. Dias

We define a new class of Z' models with neutral flavour-changing interactions at tree level in the down-quark sector. They are related in an exact way to elements of the quark mixing matrix due to an underlying flavoured U(1)' gauge…

High Energy Physics - Phenomenology · Physics 2016-06-30 Martin Jung

We study the path from the string scale physics to the low-energy physics in the $SU(6) \times SU(2)_R$ string-inspired model with the flavor symmetry ${\bf Z}_M \times {\bf Z}_N \times \tilde{D}_4$. The flavor symmetry controls the mass…

High Energy Physics - Phenomenology · Physics 2009-11-10 Takemi Hayashi , Masahisa Matsuda , Takeo Matsuoka

We propose a new model with flavor-dependent gauged $U(1)_{B-L_1}\times U(1)_{B-L_{2}-L_{3}}$ symmetry in addition to the flavor-blind one in the standard model. The model contains three right-handed neutrinos to cancel gauge anomalies and…

High Energy Physics - Phenomenology · Physics 2018-12-05 Linping Mu , Hiroshi Okada , Chao-Qiang Geng

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

Massive neutrino is an evidence of new physics beyond the Standard Model. One of the well motivated new physics scenarios is a model with gauged lepton flavor symmetry. We investigate neutrino properties in the minimal…

High Energy Physics - Phenomenology · Physics 2018-09-12 W. Sreethawong , W. Treesukrat , P. Uttayarat

We construct an anomaly-free extension of the left-right symmetric model, where the maximal flavor group is gauged and anomaly cancellation is guaranteed by adding new vectorlike fermion states. We address the question of the lowest allowed…

High Energy Physics - Phenomenology · Physics 2011-06-16 Diego Guadagnoli , Rabindra N. Mohapatra , Ilmo Sung

The electroweak currents of quarks and leptons in the $SO(5) \times U(1)$ gauge-Higgs unification model in the Randall-Sundrum warped space are determined. The 4D gauge couplings deviate from those in the standard model and the weak…

High Energy Physics - Phenomenology · Physics 2014-11-20 Yutaka Hosotani , Shusaku Noda , Nobuhiro Uekusa

We consider the neutrino physics of models with a sequentially broken U(2) flavor symmetry. Such theories yield the observed pattern of quark and lepton masses, while maintaining sufficient degeneracies between superparticles of the first…

High Energy Physics - Phenomenology · Physics 2014-11-17 Christopher D. Carone , Lawrence J. Hall

The small neutrino mass observed in neutrino oscillations is nicely explained by the seesaw mechanism. Rich phenomenology is generally expected if the heavy neutrinos are not much heavier than the electroweak scale. A model with this…

High Energy Physics - Phenomenology · Physics 2008-11-26 Jian-Ping Bu , Yi Liao , Ji-Yuan Liu

We introduce the sequence of spontaneous symmetry breaking of a coupling between Pati-Salam and electroweak symmetries $SU(4)_{PS} \otimes SU(4)_{EW}$ in order to establish a mathematically consistent relation among the coupling constants…

High Energy Physics - Phenomenology · Physics 2009-11-10 Alex E. Bernardini

I report low energy results on the study of fermion masses and mixing for quarks and leptons, including neutrinos within a SU(3) flavor symmetry model, where ordinary heavy fermions, top and bottom quarks and tau lepton become massive at…

High Energy Physics - Phenomenology · Physics 2012-12-20 Albino Hernandez-Galeana

We consider a recent proposal by Dimopoulos and Kaplan to embed the electroweak SU(2)_L X U(1)_Y into a larger group SU(3)_W X SU(2) X U(1) at a scale above a TeV. This idea is motivated by the prediction for the weak mixing angle sin^2…

High Energy Physics - Phenomenology · Physics 2009-09-17 Csaba Csaki , Joshua Erlich , Graham D. Kribs , John Terning

We explore the parameter space of a U(1) extension of the standard model -- also called the super-weak model -- from the point of view of explaining the observed dark matter energy density in the Universe. The new particle spectrum contains…

High Energy Physics - Phenomenology · Physics 2022-01-25 Sho Iwamoto , Károly Seller , Zoltán Trócsányi

We propose a natural realization of inverse seesaw model with right-handed and flavor dependent $U(1)$ gauge symmetries, in which we formulate the neutrino mass matrix to reproduce current neutrino oscillation data in a general way. Also we…

High Energy Physics - Phenomenology · Physics 2018-08-21 Takaaki Nomura , Hiroshi Okada
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