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Related papers: A flipped 331 model

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We analyze the structure of quark and lepton mass matrices under the hypothesis that they are determined from a minimum principle applied to a generic potential invariant under the $\left[U(3)\right]^5\otimes {\mathcal O}(3)$ flavor…

High Energy Physics - Phenomenology · Physics 2014-05-23 Rodrigo Alonso

It is shown that embedding a four-dimensional flipped SU(5) model in a five-dimensional SO(10) model, preserves the best features of both flipped SU(5) and SO(10). The missing partner mechanism, which naturally achieves both doublet-triplet…

High Energy Physics - Phenomenology · Physics 2011-05-12 S. M. Barr , Ilja Dorsner

Motivated by the $b\to s\ell^+\ell^-$ anomalies recently reported by the LHCb collaboration, I present a class of flavored U(1)' gauge extensions of the Standard Model that naturally accommodates them and possesses a rich phenomenology.…

High Energy Physics - Phenomenology · Physics 2015-12-22 Javier Fuentes-Martin

It is proposed that supersymmetry (SUSY) maybe used to understand fermion mass hierarchies. A family symmetry Z_{3L} is introduced, which is the cyclic symmetry among the three generation SU(2) doublets. SUSY breaks at a high energy scale ~…

High Energy Physics - Phenomenology · Physics 2014-11-18 Chun Liu

We give a detailed description of the model construction procedures about our new approach to the family structure of the standard model. SM-like chiral fermion spectra, largely "derivable" from the gauge anomaly constraints, are formulated…

High Energy Physics - Phenomenology · Physics 2009-10-28 Otto C. W. Kong

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

Contributions of flavour-changing neutral currents in the 3 3 1 model with right-handed neutrinos to mass difference of the neutral meson system $\Delta m_P (P = K, D, B)$ are calculated. Using the Fritzsch anzats on quark mixing, we show…

High Energy Physics - Phenomenology · Physics 2008-11-26 Hoang Ngoc Long , Vo Thanh Van

In a model with a gauge group $G_{SM}\otimes U(1)_X$, where $G_{SM} \equiv SU(3)_C \otimes SU(2)_L \otimes U(1)_Y$ is the standard model gauge group and $U(1)_X$ is a horizontal local gauge symmetry, the spectrum of charged fermion masses…

High Energy Physics - Phenomenology · Physics 2016-09-06 E. Garcia-Reyes , A. Hernandez-Galeana , A. Vargas , A. Zepeda

The flipped trinification, a framework for unifying the 3-3-1 and left-right symmetries, has recently been proposed in order to solve profound questions, the weak parity violation and the number of families, besides the implication for…

High Energy Physics - Phenomenology · Physics 2019-03-11 D. N. Dinh , D. T. Huong , N. T. Duy , N. T. Nhuan , L. D. Thien , Phung Van Dong

An algebraic representation of three generations of fermions with $SU(3)_C$ color symmetry based on the Cayley-Dickson algebra of sedenions $\mathbb{S}$ is constructed. Recent constructions based on division algebras convincingly describe a…

General Physics · Physics 2024-02-16 Niels G. Gresnigt , Liam Gourlay , Abhinav Varma

We include the standard-model (SM) leptons in a recently proposed framework for the generation of quark mass ratios and Cabibbo-Kobayashi-Maskawa (CKM) mixing angles from an SU(3) family gauge interaction. The set of SM-singlet scalar…

High Energy Physics - Phenomenology · Physics 2008-11-26 Thomas Appelquist , Yang Bai , Maurizio Piai

In this paper, we introduce an extension of the Standard Model, based on SU(3)$_\mathrm{C}\times $SU(3)$_\mathrm{L}\times $U(1)$_X$ gauge symmetry (331-model). The 331-models traditionally explain the number of fermion familes in nature. In…

High Energy Physics - Phenomenology · Physics 2019-03-29 Katri Huitu , Niko Koivunen , Timo J. Kärkkäinen

We consider the mass generation for the usual quarks and leptons in some supersymmetric models. The masses of the top, the bottom, the charm, the tau and the muon are given at the tree level. All the other quarks and the electron get their…

High Energy Physics - Phenomenology · Physics 2009-11-11 C. M. Maekawa , M. C. Rodriguez

We present the study of the quark sector of the universal seesaw model with $\mathrm{SU(2)_L \times SU(2)_R \times U(1)_{Y'}}$ gauge symmetry in the massless case of the two lightest quark families. This model aims to explain the mass…

High Energy Physics - Phenomenology · Physics 2024-09-19 Takuya Morozumi , Albertus Hariwangsa Panuluh

We study Flipped $SU(5)\times U(1)$ Grand Unified Theories (GUTs) with $\Gamma_3\simeq A_4$ modular symmetry. We propose two models with different modular weights assignments, where the fermion mass hierarchy can arise from weighton fields.…

High Energy Physics - Phenomenology · Physics 2021-12-22 Georgianna Charalampous , Stephen F. King , George K. Leontaris , Ye-Ling Zhou

We consider an $SU(3)_c \otimes SU(2)_L \otimes SU(2)_R \otimes U(1)_{B-L}$ left-right symmetric model with three Higgs scalars including an $SU(2)_L$ doublet, an $SU(2)_R$ doublet and an $SU(2)_L \otimes SU(2)_R$ bidoublet. In addition to…

High Energy Physics - Phenomenology · Physics 2015-05-30 Pei-Hong Gu

We do not know why there are three fermion families in the Standard Model (SM), nor can we explain the observed pattern of fermion masses and mixing angles. Standard grand unified theories based on the SU(5) and SO(10) groups fail to shed…

High Energy Physics - Phenomenology · Physics 2020-12-16 Renato M. Fonseca

Here we propose models with $SU(2)_L\otimes SU(2)_R\otimes U(1)_{B-L}$ electroweak gauge symmetry in which parity (or charge conjugation) is broken explicitly and the interactions of left- and right-handed fermions are completely different…

High Energy Physics - Phenomenology · Physics 2021-08-11 Henry Diaz , E. Castillo-Ruiz , O. P. Ravinez , V. Pleitez

We study a supersymmetric SO(10) gauge theory in six dimensions compactified on an orbifold. Three sequential quark-lepton families are localized at the three fixpoints where SO(10) is broken to its three GUT subgroups. Split bulk…

High Energy Physics - Phenomenology · Physics 2010-11-19 T. Asaka , W. Buchmuller , L. Covi

In an SU(9) model of gauged family unification, we propose an explanation for why angles observed in the lepton flavor ({\it PMNS}) mixing matrix are significantly larger than those measured for any analagous quark flavor ({\it KM}) mixing…

High Energy Physics - Phenomenology · Physics 2009-11-05 Paul H. Frampton , Thomas W. Kephart