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We present a model based on the $SU(3)_C\otimes SU(3)_L\otimes U(1)_X$ gauge symmetry that relates the mass hierarchy of the fermions with the solution to the strong CP problem through the $U(1)_{PQ}$ Peccei-Quinn symmetry. This last…

High Energy Physics - Phenomenology · Physics 2018-12-19 A. G. Dias , J. Leite , D. D. Lopes , C. C. Nishi

We construct a new gauged $U(1)_\ell$ lepton number model which is anomaly-free for each SM generation. The active neutrino masses are radiatively generated with a minimal scalar sector. The phenomenology and collider signals are studied.…

High Energy Physics - Phenomenology · Physics 2018-08-15 We-Fu Chang , John N. Ng

The Substandard theory deals with the standard model of leptons, electro-weak gauge bosons and Higgs, excluding the chromodynamics of quarks. The theory gives a geometric and algebraic interpretation of its U(2) symmetry based on the…

High Energy Physics - Theory · Physics 2007-05-23 E. L. Schucking

We propose a simple, testable, SU(5) model within the context of the type II neutrino see-saw mechanism. It is based on requiring renormalizability, the absence of any other matter fields besides those already present in the Standard Model…

High Energy Physics - Phenomenology · Physics 2008-11-26 Ilja Dorsner , Irina Mocioiu

The asymmetric Higgs sector of one $SU(2)_L \times SU(2)_R$ bidoublet $(\phi_1^0,\phi_1^-;\phi_2^+,\phi_2^0)$ and one $SU(2)_R$ doublet [but no $SU(2)_L$ doublet] is considered in a nonsupersymmetric left-right extension of the standard…

High Energy Physics - Phenomenology · Physics 2009-12-14 Alfredo Aranda , J. Lorenzo Diaz-Cruz , Ernest Ma , Roberto Noriega , Jose Wudka

We propose a new anomaly-free and family nonuniversal $\mathrm{U}(1)'$ extension of the standard model with the addition of two scalar singlets and a new scalar doublet. The quark sector is extended by adding three exotic quark singlets,…

High Energy Physics - Phenomenology · Physics 2017-06-07 S. F. Mantilla , R. Martinez , F. Ochoa

The electroweak model is formulated on the nonlinearly realized gauge group SU(2) X U(1). This implies that in perturbation theory no Higgs field is present. The paper provides the effective action at the tree level, the Slavnov Taylor…

High Energy Physics - Phenomenology · Physics 2010-11-22 Daniele Bettinelli , Ruggero Ferrari , Andrea Quadri

We study a model in which lepton number violation is solely triggered by a dimension 4 hard breaking term in the scalar potential. A minimal model which contains a SU(2) triplet with hypercharge Y=2, and a pair of singlet doubly charged…

High Energy Physics - Phenomenology · Physics 2008-11-26 Chian-Shu Chen , C. Q. Geng , J. N. Ng

The 3-3-1 model with neutral leptons contains four CP-even Higgs bosons when some constraints are imposed on the Higgs potential. Two Higgs bosons of this type are identified with the corresponding ones in the Two-Higgs-Doublet model…

High Energy Physics - Phenomenology · Physics 2023-07-04 H. T. Hung , A. B. Arbuzov

The supersymmetric $SU(6)$ model equipped by the flavour-blind discrete gauge symmetry $Z_3$ is considered. It provides simultaneous solution to the doublet-triplet splitting problem, $\mu$-problem and leads to natural understanding of…

High Energy Physics - Phenomenology · Physics 2016-09-01 Zurab Berezhiani

We systematically study and classify scotogenic models with a local U(1) gauge symmetry. These models give rise to radiative neutrino masses and a stable dark matter candidate, but avoid the theoretical problems of global and discrete…

High Energy Physics - Phenomenology · Physics 2023-12-19 T. de Boer , M. Klasen , S. Zeinstra

A realistic scheme for masses and mixing of leptons is investigated in the model with gauged SO(3) lepton flavor symmetry. Within this scheme, a nearly `bi-maximal' neutrino mixing pattern with maximal CP-violating phase is found to be the…

High Energy Physics - Phenomenology · Physics 2011-09-13 Yue-Liang Wu

We propose two models based on the $SU(3)_C \times SU(3)_L \times U(1)_X$ gauge symmetry, each incorporating distinct inverse seesaw mechanisms for generating neutrino masses at the radiative level. Therefore, neutrino masses are suppressed…

High Energy Physics - Phenomenology · Physics 2024-10-30 V. H. Binh , Cesar Bonilla , A. E. Cárcamo Hernández , D. T. Huong , Vishnudath K. N. , H. N. Long , P. N. Thu , Iván Schmidt

Based on the SO(3) gauge symmetry for three family leptons and general see-saw mechanism, we present a simple scheme that allows three nearly degenerate Majorana neutrino masses needed for hot dark matter. The vacuum structure of the…

High Energy Physics - Phenomenology · Physics 2009-10-31 Yue-Liang Wu

We propose a predictive model based on the $SU(3)_C\times SU(3)_L\times U(1)_X$ gauge symmetry, which is supplemented by the $D_4$ family symmetry and several auxiliary cyclic symmetries whose spontaneous breaking produces the observed SM…

High Energy Physics - Phenomenology · Physics 2022-09-02 A. E. Cárcamo Hernández , H. N. Long , M. L. Mora-Urrutia , N. H. Thao , V. V. Vien

We investigate the possibility to find the simplest renormalizable grand unified theory based on the SU(5) gauge symmetry. We find that it is possible to generate all fermion masses with only two Higgs bosons, 5_H and 45_H. In this context…

High Energy Physics - Phenomenology · Physics 2007-10-04 Pavel Fileviez Perez

In the Standard Model of elementary particles the fermions are assumed to be intrinsically massless. Here we propose a new theoretical idea of fermion mass generation (other than by the Higgs mechanism) through the coupling with the vector…

High Energy Physics - Phenomenology · Physics 2025-08-26 Eckart Marsch , Yasuhito Narita

We present a supersymmetric model of fermion masses with SU(4)*SU(2)^2*U(1)_X gauge group with matter in fundamental and antisymmetric tensor representations only. The up, down, charged lepton and neutrino Yukawa matrices are distinguished…

High Energy Physics - Phenomenology · Physics 2009-11-10 Thomas Dent , George Leontaris , John Rizos

We find constraints on the highest scale of symmetry breaking of a model with gauge symmetry $SU(3)_C \otimes SU(3)_L \otimes U(1)_X$ with heavy neutral leptons in the fermion triplets, calculating the anomalous magnetic moment of the muon…

High Energy Physics - Phenomenology · Physics 2021-03-03 C. E. Alvarez-Salazar , O. L. G. Peres

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