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The radiative decay of neutrino,such as (\bar{\nu_{\tau}}: \longrightarrow: \nu_{\mu}+\gamma), in the minimal supersymmetric standard model with right-handed neutrinos (MSSMRN) and in the (SU(5)) grand unified theory with right-handed…

High Energy Physics - Phenomenology · Physics 2007-05-23 Marie-Bernadette Causse

After discovery of the Higgs boson at CERN the Standard Model acquired a status of the theory of the elementary particles in the electroweak range (up to about 300 GeV). What general conclusions can be inferred from the Standard Model? It…

High Energy Physics - Phenomenology · Physics 2015-01-05 S. M. Bilenky

In SU(3)_L x U(1)_N gauge models for electroweak interactions, we discuss how to implement a radiative mechanism of generating Majorana neutrino masses by considering the property that the Higgs scalar, which has a coupling to a charged…

High Energy Physics - Phenomenology · Physics 2009-10-31 Yutaka Okamoto , Masaki Yasue

We analyze a scenario where the right-handed neutrinos make part of a strongly coupled conformal field theory and acquire an anomalous dimension \gamma<1 at a large scale \Lambda. Their Yukawa couplings to the Higgs become irrelevant at the…

High Energy Physics - Phenomenology · Physics 2009-07-24 Gero von Gersdorff , Mariano Quiros

The gauge principle is a cornerstone of particle-physics model building. Nevertheless, many constructions leave certain global $U(1)$ redundancies ungauged. In this work, we take the gauge principle to its logical extreme by promoting all…

High Energy Physics - Phenomenology · Physics 2025-12-18 Antonio Herrero-Brocal , Javier Perez-Soler , Avelino Vicente

A remarkable U(1) gauge extension of the supersymmetric standard model was proposed eight years ago. It is anomaly-free, has no mu term, and conserves baryon and lepton numbers automatically. The phenomenology of a specific version of this…

High Energy Physics - Phenomenology · Physics 2010-05-19 Ernest Ma

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

In this work we implement the type II seesaw mechanism into the framework of the $U(1)_{B-L}$ gauge model. As main gain, the right-handed neutrinos of the model get free to play the role of the dark matter of the universe. As side effect,…

High Energy Physics - Phenomenology · Physics 2019-07-15 J. G. Rodrigues , A. C. O. Santos , J. G. Ferreira , C. A. de S. Pires

We study a softly-broken supersymmetric model whose gauge symmetry is that of the standard model (SM) gauge group times an extra Abelian symmetry U(1)'. We call this gauge-extended model U(1)' model, and we study a U(1)' model with a…

High Energy Physics - Phenomenology · Physics 2015-03-17 Durmuş A. Demir , Mariana Frank , Levent Selbuz , Ismail Turan

We demonstrate that almost degenerate Dirac neutrinos of mass of few eV and transition magnetic moment of the order of ${10}^{-11}$ $\mu_B$ can be obtained in an ${SU(2)}_L\times {U(1)}_Y$ model with $S_3\times Z_3\times Z_4$ discrete…

High Energy Physics - Phenomenology · Physics 2007-05-23 Ambar Ghosal , Asim K. Ray

After discovery of the Higgs boson at CERN the Standard Model acquired a status of the full, correct theory of the elementary particles in the electroweak range. What general conclusions can be inferred from the SM? I am suggesting here…

High Energy Physics - Phenomenology · Physics 2014-08-08 S. M. Bilenky

We consider a U(1)' gauge symmetry acting on three generations of right-handed neutrinos. The U(1)' symmetry is broken at the TeV scale and its remnant discrete symmetry makes one of the right-handed neutrinos stable. As a natural…

High Energy Physics - Phenomenology · Physics 2014-01-29 Manfred Lindner , Daniel Schmidt , Atsushi Watanabe

Nonzero masses for the active neutrinos - regardless of their nature or origin - arise only after electroweak symmetry breaking. We discuss the parameterization of neutrino couplings to a Higgs sector consisting of one SU(2)_L scalar…

High Energy Physics - Phenomenology · Physics 2011-09-08 Andre de Gouvea , Wei-Chih Huang , Shashank Shalgar

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

Majorana features of neutrinos and SO(3) gauge symmetry of three families enable us to construct a gauge model of neutrino for understanding naturally the observed smallness of neutrino masses and the nearly tri-bimaximal neutrino mixing…

High Energy Physics - Phenomenology · Physics 2012-03-06 Yue-Liang Wu

Standard model is minimally extended using the unitary group $G'=U(3)\times SU(2)\times U(1)$ of Connes' color-flavor algebra. In place of Connes' unimodularity condition an extra Higgs is assumed to spontaneously break $G'$ down to…

High Energy Physics - Theory · Physics 2007-05-23 Katsusada Morita , Yoshitaka Okumura

We investigate the nature (Dirac vs. Majorana) and size of left-handed neutrino masses in a supersymmetric five-dimensional model compactified in the interval [0,\pi R], where quarks and leptons are localized on the boundaries while the…

High Energy Physics - Phenomenology · Physics 2008-11-26 D. Diego , M. Quiros

We show that the electroweak symmetry can be broken in a natural and phenomenologically acceptable way by a neutrino condensate. Therefore, we assume as particle content only the chiral fermions and gauge bosons of the Standard Model and in…

High Energy Physics - Phenomenology · Physics 2010-04-05 Stefan Antusch , Joern Kersten , Manfred Lindner , Michael Ratz

We investigate a model with an extra $Z_{2}$ gauge symmetry in the Standard Model. We assume that only the scalars and the leptons carry non-zero charge. The symmetry gives a structure to the mass matrix for the neutrinos. With two extra…

High Energy Physics - Phenomenology · Physics 2009-10-22 Jihn E. Kim , B-A Lindholm

We show that experimental results for the masses and mixing of the neutrinos can be understood naturally by a simple grand unification model of SU(5) coupled to N=1 supergravity. No right-handed neutrinos are included. The left-handed…

High Energy Physics - Phenomenology · Physics 2009-11-10 Noriyuki Oshimo