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Related papers: Leptogenesis in SO(10)

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Baryogenesis appears to require lepton number violation. This is naturally realized in extensions of the standard model containing right-handed neutrinos. We discuss the generation of a baryon asymmetry by the out-of-equilibrium decay of…

High Energy Physics - Phenomenology · Physics 2007-05-23 M. Plumacher

We review the status of thermal leptogenesis in the minimal $SU(5)\times U(1)$ and $SO(10)$ unified models under the assumption that the leptonic asymmetry generated in the out-of-equilibrium decays of heavy Majorana neutrinos (and its…

High Energy Physics - Phenomenology · Physics 2025-07-01 Michal Malinský

We investigate thermal leptogenesis within a supersymmetric grand unified theory (SUSY GUT) based on the $SO(10) \times U(1)_A$ symmetry, where both the doublet--triplet splitting problem and the unrealistic Yukawa relations are resolved…

High Energy Physics - Phenomenology · Physics 2025-11-17 Nobuhiro Maekawa , Kei Shibata , Masato Yamanaka

A non-supersymmetric renormalizable $SO(10)$ model is investigated for its viability in explaining the observed fermion masses and mixing parameters along with the baryon asymmetry produced via thermal leptogenesis. The Yukawa sector of the…

High Energy Physics - Phenomenology · Physics 2021-12-10 V. Suryanarayana Mummidi , Ketan M. Patel

Motivated by the fact that, in some realistic models combining SO(10) GUTs and flavour symmetries, it is not possible to achieve the required baryon asymmetry through the CP asymmetry generated in the decay of right-handed neutrinos, we…

High Energy Physics - Phenomenology · Physics 2009-01-06 E. J. Chun , L. Velasco-Sevilla

Baryogenesis, through the decays of heavy bosons, was considered to be one of the major successes of the grand unified theories (GUTs). It was then realized that the sphaleron processes erased any baryon asymmetry from the GUT-baryogenesis…

High Energy Physics - Phenomenology · Physics 2008-11-26 Pei-Hong Gu , Utpal Sarkar

We consider the see-saw mechanism within a non-supersymmetric SO(10) model. By assuming the SO(10) quark-lepton symmetry, and after imposing suitable conditions that ensure that the right-handed (RH) neutrino masses are at most mildly…

High Energy Physics - Phenomenology · Physics 2013-09-19 Franco Buccella , Domenico Falcone , Chee Sheng Fong , Enrico Nardi , Giulia Ricciardi

A detailed analytic and numerical study of baryogenesis through leptogenesis is performed in the framework of the standard model of electroweak interactions extended by the addition of three right-handed neutrinos, leading to the seesaw…

High Energy Physics - Phenomenology · Physics 2011-07-19 G. C. Branco , R. Gonzalez Felipe , F. R. Joaquim , M. N. Rebelo

Although $SO(10)$ Supersymmetric (SUSY) Grand Unification Theories (GUTs) are very attractive for neutrino mass and mixing, it is often quite difficult to achieve successful leptogenesis from the lightest right-handed neutrino $N_1$ due to…

High Energy Physics - Phenomenology · Physics 2017-03-08 Fredrik Björkeroth , Francisco J. de Anda , Ivo de Medeiros Varzielas , Stephen F. King

Baryogenesis appears to require lepton number violation. This is naturally realized in extensions of the standard model containing right-handed neutrinos. We discuss the generation of a baryon asymmetry by the out-of-equilibrium decay of…

High Energy Physics - Phenomenology · Physics 2007-05-23 W. Buchmuller , M. Plumacher

In this work we demonstrate that what was previously considered as different mechanisms of baryon asymmetry generation involving two right-handed Majorana neutrinos with masses far below the GUT scale -- leptogenesis via neutrino…

High Energy Physics - Phenomenology · Physics 2021-09-15 Juraj Klarić , Mikhail Shaposhnikov , Inar Timiryasov

We present in this talk a model based on SO(10) x SU(2)_{F} having symmetric mass textures with 5 zeros constructed by us recently. The symmetric mass textures arising from the left-right symmetry breaking chain of SO(10) give rise to good…

High Energy Physics - Phenomenology · Physics 2015-06-25 Mu-Chun Chen , K. T. Mahanthappa

We study the prediction for leptogenesis in two renormalizable supersymmetric $SO(10)\times A_4$ modular models in which the neutrino mass is dominantly generated by the type I seesaw mechanism. The evolution of the lepton asymmetries are…

High Energy Physics - Phenomenology · Physics 2022-10-26 Gui-Jun Ding , Stephen F. King , Jun-Nan Lu , Bu-Yao Qu

In the baryogenesis via leptogenesis framework the baryonic asymmetry depends on lepton mass matrices. In a previous paper we used SO(10)-inspired mass matrices and we found few possibilities to obtain a sufficient level of asymmetry. In…

High Energy Physics - Phenomenology · Physics 2009-11-07 D. Falcone , F. Tramontano

We have constructed a SUSY SO(10) x SU(2)_F model in which a set of symmetric mass matrices with five texture zeros (having 11 parameters) leads to 22 measurable fermion masses, mixing angles and CP phases, all in agreement with available…

High Energy Physics - Phenomenology · Physics 2007-05-23 Mu-Chun Chen , K. T. Mahanthappa

By demanding a compact spectrum for the right-handed neutrinos and an approximate quark-lepton symmetry inspired from SO(10) gauge unification (assuming a Dirac neutrino mass matrix close to the up quark mass matrix), we construct a {\it…

High Energy Physics - Phenomenology · Physics 2011-06-02 F. Buccella , D. Falcone , L. Oliver

Lopsided structure in mass matrices of down quarks and leptons gives a simple explanation for the observed large angles of neutrino mixings. We realize such mass matrices by the Froggatt-Nielsen mechanism in the framework of supersymmetric…

High Energy Physics - Phenomenology · Physics 2009-11-10 T. Asaka

We study the thermal leptogenesis in the $E_6\times U(1)_A$ SUSY GUT model in which realistic masses and mixings of quarks and leptons can be realized. We show that the sufficient baryon number can be produced by the leptogenesis in the…

High Energy Physics - Phenomenology · Physics 2016-03-23 Takuya Ishihara , Nobuhiro Maekawa , Mao Takegawa , Masato Yamanaka

A framework based on an effective symmetry that is either G(224)= SU(2)_L x SU(2)_R xSU(4)^c or SO(10) has been proposed (a few years ago) that successfully describes the masses and mixings of all fermions including neutrinos, with seven…

High Energy Physics - Phenomenology · Physics 2009-11-07 Jogesh C. Pati

We point out that, in a class of SO(10) models with matter fields in 16 and 10 representations and type II realization of the seesaw mechanism, the light neutrino masses and the CP asymmetry needed for leptogenesis are controlled by one and…

High Energy Physics - Phenomenology · Physics 2008-11-26 Michele Frigerio , Pierre Hosteins , Stephane Lavignac , Andrea Romanino
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