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Related papers: Neutrino masses in SU(5) grand unified model

200 papers

A grand unified model based on SO(10) and supersymmetry is presented to account for the masses and mixing of the neutrinos observed in experiments.

High Energy Physics - Phenomenology · Physics 2007-05-23 Noriyuki Oshimo

Motivated by the atmospheric and solar neutrino anomalies, we study neutrino masses in a parity invariant SU(5)xSU(5)' grand unified model. Constraints from photon-mirror photon kinetic mixing are discussed.

High Energy Physics - Phenomenology · Physics 2009-10-31 M. Collie , R. Foot

We briefly review models of neutrino masses and mixings. In view of the existing experimental ambiguities many possibilities are still open. After an overview of the main alternative options we focus on the most constrained class of models…

High Energy Physics - Phenomenology · Physics 2007-05-23 Guido Altarelli

We discuss some models of neutrino masses and mixings in the context of fermion masses in Grand Unified Theories.

High Energy Physics - Phenomenology · Physics 2009-10-31 G. Altarelli

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

The symmetry between quarks and leptons suggests that neutrinos should have mass. As embodied in the grand unified theory SO(10) this yields masses that can only be detected by neutrino oscillations. Such oscillations could be very…

High Energy Physics - Phenomenology · Physics 2008-11-26 Lincoln Wolfenstein

A grand unified model based on SU(5) and supersymmetry is presented. Pairs of superfields belonging to 15 and 15* representations are newly introduced, while gauge coupling unification is satisfied. Improper mass relations in the minimal…

High Energy Physics - Phenomenology · Physics 2009-10-29 Noriyuki Oshimo

Seesaw mechanism appears to be the simplest and most appealing way to understand small neutrino masses observed in recent experiments. It introduces three right handed neutrinos with heavy masses to the standard model, with at least one…

High Energy Physics - Phenomenology · Physics 2014-11-18 R. N. Mohapatra

Assuming three light neutrinos and the see-saw mechanism we present a semiquantitative model of fermion masses based on (SUSY) SU(5) and abelian horizontal charges. A good description of the observed pattern of quark and lepton masses is…

High Energy Physics - Phenomenology · Physics 2008-11-26 Guido Altarelli , Ferruccio Feruglio

We discuss a grand unified model based on SUSY SU(5) in extra dimensions and on the flavour group A4xU(1) which, besides reproducing tri-bimaximal mixing for neutrinos with the accuracy required by the data, also leads to a natural…

High Energy Physics - Phenomenology · Physics 2010-02-03 Guido Altarelli , Ferruccio Feruglio , Claudia Hagedorn

We review the problem of neutrino masses and mixings in the context of Grand Unified Theories. After a brief summary of the present experimental status of neutrino physics, we describe how the see-saw mechanism can automatically account for…

High Energy Physics - Phenomenology · Physics 2009-02-23 Isabella Masina

Near maximal neutrino mixing needed to understand atmospheric neutrino data can be interpreted to be a consequence of an interchange symmetry between the muon and tau neutrinos in the neutrino mass matrix in the flavor basis. This idea can…

High Energy Physics - Phenomenology · Physics 2009-11-11 R. N. Mohapatra , S. Nasri , Hai-Bo Yu

We discuss the implications of large neutrino mixings for grand unified theories based on the seesaw mechanism. In SU(5) GUTs large mixings can be accomodated by means of $U(1)_F$ flavour symmetries. In these models the heavy Majorana…

High Energy Physics - Phenomenology · Physics 2007-05-23 W. Buchmüller

We propose a simple renormalizable grand unified theory based on the $SU(5)$ gauge symmetry where the neutrino masses are generated at the quantum level through the Zee mechanism. In this model the same Higgs needed to correct the mass…

High Energy Physics - Phenomenology · Physics 2016-10-26 Pavel Fileviez Perez , Clara Murgui

We review theoretical ideas, problems and implications of neutrino masses and mixing angles. We give a general discussion of schemes with three light neutrinos. Several specific examples are analyzed in some detail, particularly those that…

High Energy Physics - Phenomenology · Physics 2009-11-10 Guido Altarelli , Ferruccio Feruglio

The problem of neutrino masses and mixing angles is analysed in a class of supersymmetric grand unified models, with SO(10) gauge symmetry and global U(2) flavour symmetry. Adopting the seesaw mechanism for the generation of the neutrino…

High Energy Physics - Phenomenology · Physics 2009-10-30 G. Costa , E. Lunghi

We review theoretical ideas, problems and implications of different models for neutrino masses and mixing angles. We give a general discussion of schemes with three or more light neutrinos. Several specific examples are analyzed in some…

High Energy Physics - Phenomenology · Physics 2009-07-09 Guido Altarelli , Ferruccio Feruglio

There are strong indications for neutrino masses and mixings in the data on solar neutrinos, the observed deficit of the muon neutrinos from the atmosphere as well as the discussions of the dark matter of the universe after COBE data. It is…

High Energy Physics - Phenomenology · Physics 2007-05-23 R. N. Mohapatra

We consider neutrino mixings in supersymmetric SU(5) supplemented by a U(1) flavor symmetry. In particular, we show how bi-maximal neutrino mixings can be realized. Two scenarios for implementing the small mixing angle MSW solution, with…

High Energy Physics - Phenomenology · Physics 2011-05-12 Qaisar Shafi , Zurab Tavartkiladze

A new supersymmetric grand unified model based on the gauge group $SU(5)\times SU(5)$ is discussed. The model has the feature that the conventional seesaw mechanism for neutrino masses is implemented using the $(15, 1)+(1,\bar{15)}$…

High Energy Physics - Phenomenology · Physics 2009-10-28 R. N. Mohapatra
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