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Related papers: Leptogenesis in $\Delta(27)$ with a Universal Text…

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We study the role played in leptogenesis by the equilibration of lepton flavors, as could be induced in supersymmetric models by off diagonal soft breaking masses for the scalar lepton doublets $\tilde m_{\alpha\beta}$, or more generically…

High Energy Physics - Phenomenology · Physics 2009-12-17 D. Aristizabal Sierra , Marta Losada , Enrico Nardi

In this paper, we would like to point out that in the scenario that the right-handed neutrinos suddenly gain some masses much larger than the temperature of the Universe at that time so that the washout effects for the lepton asymmetry…

High Energy Physics - Phenomenology · Physics 2024-09-18 Zhen-hua Zhao , Jing Zhang , Xiang-Yi Wu

In the context of the type-I seesaw mechanism, it is known that $\theta_{13}$ is zero and leptogenesis can not be realized if there exists a residual flavor symmetry resulting in the Tri-Bimaximal neutrino mixing pattern. We propose a…

High Energy Physics - Phenomenology · Physics 2015-06-19 Wei-Chih Huang

The generation of the right amount of baryon asymmetry $\eta$ of the Universe from supersymmetric leptogenesis is studied within the type-I seesaw framework with three heavy singlet Majorana neutrinos $N_i\,\,(i = 1,2,3)$ and their…

High Energy Physics - Phenomenology · Physics 2011-01-28 Biswajit Adhikary , Ambar Ghosal , Probir Roy

Seesaw models with a slightly broken lepton number symmetry can explain small neutrino masses, and allow for low-scale leptogenesis. We make a thorough analysis of leptogenesis within the simplest model with two right-handed (RH) neutrinos…

High Energy Physics - Phenomenology · Physics 2010-04-21 Takehiko Asaka , Steve Blanchet

We discuss how seesaw neutrino models can be graphically represented in lepton flavour space. We examine various popular models and show how this representation helps understanding their properties and connection with experimental data…

High Energy Physics - Phenomenology · Physics 2019-05-22 Pasquale Di Bari , Michele Re Fiorentin , Rome Samanta

Assuming that the neutrino mass matrix is diagonalized by the tribimaximal mixing matrix, we explore the textures for the charged lepton mass matrix that render an $U_{PMNS}$ lepton mixing matrix consistent with data. In particular we are…

High Energy Physics - Phenomenology · Physics 2014-06-10 J. Alberto Acosta , Alfredo Aranda , Manuel A. Buen-Abad , Alma D. Rojas

We present a mechanism of leptogenesis based on the out-of-equilibrium decay of a scalar particle into heavy virtual Majorana neutrinos. This scheme presents many conceptual advantages over the conventional scenario of Fukugita and…

High Energy Physics - Phenomenology · Physics 2009-10-31 J. -M. Frere , F. -S. Ling , M. H. G. Tytgat , V. Van Elewyck

We show that the neutrino models, as suggested by Low, which have an additional Abelian family symmetry and a real Higgs singlet to the default see-saw do not hinder the possibility of successful thermal leptogenesis. For these models…

High Energy Physics - Phenomenology · Physics 2008-11-26 Sandy S. C. Law , Raymond R. Volkas

In the context of Standard Model (SM) extensions, the seesaw mechanism provides the most natural explanation for the smallness of neutrino masses. In this work we consider the most economical type-I seesaw realization in which two…

High Energy Physics - Phenomenology · Physics 2018-06-20 D. M. Barreiros , R. G. Felipe , F. R. Joaquim

We present a simple extension of the Standard Model with three right-handed neutrinos in a SUSY framework, with an additional U(1$)_\text{F}$ abelian flavor symmetry with a non standard leptonic charge $L_e-L_\mu-L_\tau$ for lepton doublets…

High Energy Physics - Phenomenology · Physics 2023-03-01 Giorgio Arcadi , Simone Marciano , Davide Meloni

In this paper we investigate the parallel texture structures containing texture zeros in charged lepton mass matrix $M_{l}$ and cofactor zeros in neutrino mass matrix $M_{\nu}$. These textures are interesting since they are related to the…

High Energy Physics - Phenomenology · Physics 2014-08-27 Weijian Wang

We investigate non-resonant thermal leptogenesis in the context of the $SU(5) \times \mathcal{T}_{13}$ "asymmetric texture", where both Dirac and Majorana ${CP}$ violation arise from a single phase in the tribimaximal seesaw mixing matrix.…

High Energy Physics - Phenomenology · Physics 2021-02-24 Moinul Hossain Rahat

We consider sub-TeV scale flavoured resonant leptogenesis within the minimal type-I seesaw scenario with two right-handed singlet neutrinos $N_{1,2}$ forming a pseudo-Dirac pair, concentrating on the case of masses of the pseudo-Dirac pair…

High Energy Physics - Phenomenology · Physics 2021-11-09 A. Granelli , K. Moffat , S. T. Petcov

Leptogenesis, i.e. the creation of a lepton asymmetry in the early Universe, may occur through the decay of heavy singlet (right-handed) neutrinos. If we require it not to be erased by physics beyond the Standard Model at the TeV energy…

High Energy Physics - Phenomenology · Physics 2007-05-23 Ernest Ma

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

Leptogenesis is an attractive scenario in which neutrino masses and baryon asymmetry of the Universe are explained together under a minimal set of assumptions. After formulating the problem of initial conditions and introducing the strong…

High Energy Physics - Phenomenology · Physics 2014-10-22 Luca Marzola

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

Four is the maximum number of texture zeros allowed in the Yukawa coupling matrix of three massive neutrinos. These completely fix the high scale CP violation needed for leptogenesis in terms of that accessible at laboratory energies.…

High Energy Physics - Phenomenology · Physics 2017-08-23 Probir Roy

We examine the compatibility between the Neutrino Option, in which the electroweak scale is generated by PeV mass type I seesaw Majorana neutrinos, and leptogenesis. We find the Neutrino Option is consistent with resonant leptogenesis.…

High Energy Physics - Phenomenology · Physics 2019-11-11 I. Brivio , K. Moffat , S. Pascoli , S. T. Petcov , J. Turner