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Related papers: A flipped 331 model

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What we call the Anti-GUT model is extended a bit to include also right-handed neutrinos and thus make use of the see-saw mechanism for neutrino masses. This model consists in assigning gauge quantum numbers to the known Weyl fermions and…

High Energy Physics - Phenomenology · Physics 2009-10-31 C. D. Froggatt , H. B. Nielsen , Y. Takanishi

We explore the unification of gauge couplings and fermion masses in two different types of supersymmetric left-right models, one with Higgs triplets and the other with both Higgs triplets as well as bitriplets. The minimal versions of these…

High Energy Physics - Phenomenology · Physics 2011-05-30 Debasish Borah , Urjit A. Yajnik

A Hexad Preon model where leptons, quarks and W Z bosons are composite is proposed. Six Hexad Preons transform under $U(3)\otimes U(3)$ local gauge theory which is identified with $U(1)_Q\otimes SU(3)_C\otimes SU(3)_f\otimes U(1)_w$. All…

High Energy Physics - Phenomenology · Physics 2011-12-02 Shun-Zhi Wang

We construct a three family flipped SU(5) model from the heterotic string theory compactified on the $\Z_{12-I}$ orbifold with one Wilson line. The gauge group is $\rm SU(5)\times U(1)_X\times U(1)^2\times[SU(2)\times SO(10)\times…

High Energy Physics - Theory · Physics 2008-11-26 Jihn E. Kim , Bumseok Kyae

The framed standard model (FSM) suggested earlier, which incorporates the Higgs field and 3 fermion generations as part of the framed gauge theory structure, is here developed further to show that it gives both quarks and leptons…

High Energy Physics - Phenomenology · Physics 2012-06-14 Michael J. Baker , J. Bordes , H. M. Chan , S. T. Tsou

As was shown in 1984 by Caneschi, Farrar, and Schwimmer, decomposing representations of the supergroup SU(M|N), can give interesting anomaly-free sets of fermion representations of SU(M) x SU(N) x U(1). It is shown here that such groups can…

High Energy Physics - Phenomenology · Physics 2017-11-22 S. M. Barr , Heng-Yu Chen

We posit that the distinct patterns observed in fermion masses and mixings are due to a minimally broken $\mathrm{U}(2)_{q+e}$ flavor symmetry acting on left-handed quarks and right-handed charged leptons, giving rise to an accidental…

High Energy Physics - Phenomenology · Physics 2024-02-28 Stefan Antusch , Admir Greljo , Ben A. Stefanek , Anders Eller Thomsen

The old issue of why there are more than one family of quarks and leptons is reinvestigated with an eye towards the use of anomaly as a tool for constraining the number of families. It is found that, by assuming the existence of…

High Energy Physics - Phenomenology · Physics 2009-10-31 P. Q. Hung

The approach unifying all the internal degrees of freedom--proposed by one of us--is offering a new way of understanding families of quarks and leptons: A part of the starting Lagrange density in d(=1+13), which includes two kinds of spin…

High Energy Physics - Phenomenology · Physics 2008-11-26 G. Bregar , M. Breskvar , D. Lukman , N. S. Mankoc Borstnik

Flavour changing neutral currents arise in the $SU(3)_c\otimes SU(4)_L\otimes U(1)_X$ extension of the standard model because anomaly cancellation among the fermion families requires one generation of quarks to transform differently from…

High Energy Physics - Phenomenology · Physics 2009-10-06 Jorge L. Nisperuza , Luis A. Sanchez

We construct a 3-3-1 model based on family symmetry S_4 responsible for the neutrino and quark masses. The tribimaximal neutrino mixing and the diagonal quark mixing have been obtained. The new lepton charge \mathcal{L} related to the…

High Energy Physics - Phenomenology · Physics 2011-02-09 P. V. Dong , H. N. Long , D. V. Soa , V. V. Vien

In 3-3-1 models anomaly cancellation requires that one of the three families of quarks transforms as triplet by $\text{SU}(3)_\text{L}$ with the other two transforming necessarily as anti-triplet. This is an important feature of the model…

High Energy Physics - Phenomenology · Physics 2023-08-23 Vinícius Oliveira , C. A. de S. Pires

We suggest a model which addresses both the fermion mass hierarchy problem and the family problem in two-layer warped extra dimensions. In this model, 3 family fermions in 4 dimensions (4D) generate from 1 family in two-layer warped 6D by…

High Energy Physics - Phenomenology · Physics 2009-12-10 Zhi-Qiang Guo , Bo-Qiang Ma

We present a model based on the $SU(3)_{C}\otimes SU(3)_{L}\otimes U(1)_{X}$ gauge symmetry having an extra $T_{7}\otimes Z_{2}\otimes Z_{3}\otimes Z_{14} $ flavor group, which successfully describes the observed SM fermion mass and mixing…

High Energy Physics - Phenomenology · Physics 2016-02-25 A. E. Cárcamo Hernández , R. Martinez

We propose a $B-L$ gauged extension of the Standard Model where light neutrino masses arise from type III seesaw mechanism. Unlike the minimal $B-L$ model with three right handed neutrinos having unit lepton number each, the model with…

High Energy Physics - Phenomenology · Physics 2020-03-24 Anirban Biswas , Debasish Borah , Dibyendu Nanda

We review our recent development of family replicated gauge group model, which generates the Large Mixing Angle MSW solution. The model is based on each family of quarks and leptons having its own set of gauge fields, each containing a…

High Energy Physics - Phenomenology · Physics 2007-05-23 H. B. Nielsen , Y. Takanishi

In light of the recent $R_{K^{(*)}}$ data on neutral current flavour anomalies in $B \to K^{(*)} \ell^+ \ell^-$ decays, we re-examine their quantitative interpretation in terms of an extended 331 gauge theory framework. We achieve this by…

High Energy Physics - Phenomenology · Physics 2022-08-29 Andrea Addazi , Giulia Ricciardi , Simone Scarlatella , Rahul Srivastava , José W. F. Valle

A complete set of postulates of the standard model of the electroweak interaction and mass generation is formulated and confirmed deriving the Lagrangian for the standard model. A massive fermion is formed by a right-handed and a…

General Physics · Physics 2014-06-06 Walter Schmidt-Parzefall

We present a renormalizable fermion mass model based on the symmetry $Q_4$ that accommodates all fermion masses and mixing angles in both the quark and lepton sectors. It requires the presence of only four SU(2) doublet scalar fields…

High Energy Physics - Phenomenology · Physics 2011-08-12 Alfredo Aranda , Cesar Bonilla , Raymundo Ramos , Alma D. Rojas

We develop a ${\rm SU}(3)_C\otimes {\rm SU}(3)_L\otimes {\rm U}(1)_X$ model where the number of fermion generations is fixed by cancellation of gauge anomalies, being a type of 3-3-1 model with new charged leptons. Similarly to the…

High Energy Physics - Phenomenology · Physics 2018-04-04 E. R. Barreto , A. G. Dias , J. Leite , C. C. Nishi , R. L. N. Oliveira , W. C. Vieira
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