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Related papers: Neutrino mixing in a left-right model

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We show that the neutrino masses with large mixing between \nu_\mu and \nu_\tau are naturally reproduced in a supersymmetric E_6 grand unification model with an anomalous U(1)_X symmetry. We propose a simple scenario which incorporates a…

High Energy Physics - Phenomenology · Physics 2009-10-31 Masako Bando , Taichiro Kugo

We study a possibility to explain neutrino masses and mixings based on supersymmetry. If we introduce a flavor diagonal but generation dependent extra U(1) gauge interaction at a TeV region, we can obtain masses and mixings of neutrinos…

High Energy Physics - Phenomenology · Physics 2007-05-23 Daijiro Suematsu

We estimate the magnitude of Lepton Flavour Violation (LFV) from the phase of the neutrino Yukawa matrix. In the minimal supersymmetric standard model with right-handed neutrinos, the LFV processes l_i \to l_j \gamma can appear through the…

High Energy Physics - Phenomenology · Physics 2009-11-10 S. Kanemura , K. Matsuda , T. Ota , T. Shindou , E. Takasugi , K. Tsumura

Starting from the original Majorana's article of 1937, the see-saw mechanism is illustrated, first for one and later for three neutrino generations, and neutrinoless double beta decay is considered. Neutrino mixing and oscillations in three…

High Energy Physics - Phenomenology · Physics 2020-04-22 Luciano Maiani

F-theory is one of the frameworks where up-type Yukawa couplings of SU(5) unified theories are naturally generated. As charged matter fields have localized zero modes in F-theory, a study of flavor structure could be easier in F-theory than…

High Energy Physics - Theory · Physics 2009-10-31 Radu Tatar , Yoichi Tsuchiya , Taizan Watari

We suggest a supersymmetric (SUSY) explanation of neutrino masses and mixing, where nonrenormalizable interactions in the hidden sector generate lepton number violating Majorana mass terms for both right-chiral sneutrinos and neutrinos. It…

High Energy Physics - Phenomenology · Physics 2009-11-11 Biswarup Mukhopadhyaya , Probir Roy , Raghavendra Srikanth

We consider various possibilities for generating neutrino masses in supersymmetric models with an additional U(1)' gauge symmetry. One class of models involves two extra U(1)' x U(1)'' gauge symmetries, with U(1)'' breaking at an…

High Energy Physics - Phenomenology · Physics 2009-11-10 Junhai Kang , Paul Langacker , Tianjun Li

The addition of gauge singlet fermions to the Standard Model Lagrangian renders the neutrinos massive and allows one to explain all that is experimentally known about neutrino masses and lepton mixing by varying the values of the Majorana…

High Energy Physics - Phenomenology · Physics 2009-10-29 Andre de Gouvea , Wei-Chih Huang , James Jenkins

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

If neutrinos have masses, why are they so tiny? Are these masses of the Dirac type or of the Majorana type? We are already familiar with the mechanism of how to obtain a tiny Majorana neutrino mass by the famous see-saw mechanism. The…

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

We consider a neutrino mass model where all leptonic mixing is induced by a heavy Majorana sector through the seesaw type I mechanism, while the Dirac mass matrices are diagonal. Such a pattern occurs naturally in grand unified theories.…

High Energy Physics - Phenomenology · Physics 2011-08-11 Philipp Leser , Heinrich Päs

We construct a gauge $B-L$ model with $D_4\times Z_4\times Z_2$ symmetry that can explain the quark and lepton mass hierarchies and their mixings with the realistic CP phases via the type-I seesaw mechanism. Six quark mases, three quark…

High Energy Physics - Phenomenology · Physics 2024-05-02 V. V. Vien

We propose a model of fermion masses and mixings based on $SU(5)$ grand unified theory (GUT) and a $D_{4}$ flavor symmetry. This is a highly predictive 4D $SU(5)$ GUT with a flavor symmetry that does not contain a triplet irreducible…

High Energy Physics - Phenomenology · Physics 2021-11-29 M. Miskaoui , M. A. Loualidi

We present a new mechanism to explain naturally and through a common flavour symmetry the mildly hierarchical neutrino masses with large mixings and the hierarchical Yukawa matrices with small mixing angles. Although this mechanism is not…

High Energy Physics - Phenomenology · Physics 2007-05-23 Oscar Vives

The fact that neutrinos are massive suggests that the minimal supersymmetric standard model (MSSM) might be extended in order to include three gauge-singlet neutrino superfields with Yukawa couplings of the type $H_2 L \nu^c$. We propose to…

High Energy Physics - Phenomenology · Physics 2009-11-11 D. E. Lopez-Fogliani , C. Munoz

In spite of enormous experimental progress in determination of the neutrino parameters, theory of neutrino mass and mixing is still on the cross-roads. Guidelines could be (i) the connection between zero neutrino charges (and therefore a…

High Energy Physics - Phenomenology · Physics 2022-03-02 Alexei Yu. Smirnov

We present a comprehensive analysis of neutrino mass and lepton mixing in theories with $A_4$ modular symmetry, where the only flavon field is the single modulus field $\tau$, and all masses and Yukawa couplings are modular forms. Similar…

High Energy Physics - Phenomenology · Physics 2019-10-02 Gui-Jun Ding , Stephen F. King , Xiang-Gan Liu

We discuss an inverse seesaw model based on right-handed fermion specific $U(1)$ gauge symmetry and $A_4$-modular symmetry. These symmetries forbid unnecessary terms and restrict structures of Yukawa interactions which are relevant to…

High Energy Physics - Phenomenology · Physics 2019-12-03 Takaaki Nomura , Hiroshi Okada , Sudhanwa Patra

Within the framework of a local SU(3) family symmetry model, we report a general analysis of the mechanism for neutrino mass generation and mixing, including light sterile neutrinos. In this scenario, ordinary heavy fermions, top and bottom…

High Energy Physics - Phenomenology · Physics 2014-12-23 Albino Hernandez-Galeana

We have studied the most general neutrino mass matrices in models with SU(2) and SU(3) horizontal symmetries. Without going into the details of the models it is possible to write down the effective operators, which predict the structure of…

High Energy Physics - Phenomenology · Physics 2009-11-07 Asim K. Ray , Utpal Sarkar
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