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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

We investigate the hierarchical flavor structure of the Standard Model in a Froggatt-Nielsen (FN) framework, where the spontaneous breaking of a $U(1)_{\rm FN}$ symmetry by a complex flavon field generates fermion masses and mixing patterns…

High Energy Physics - Phenomenology · Physics 2026-03-06 Cheshta Batra , Rusa Mandal , Kunal Rawat , Tom Tong

Taking into account the recent progress in the understanding of the lepton flavour effects in leptogenesis, we investigate in detail the possibility that the CP-violation necessary for the generation of the baryon asymmetry of the Universe…

High Energy Physics - Phenomenology · Physics 2008-11-26 S. Pascoli , S. T. Petcov , Antonio Riotto

The CP-violation necessary for the generation of the baryon asymmetry of the Universe $Y_B$ in the "flavoured" leptogenesis scenario can arise from the "low energy" PMNS neutrino mixing matrix $U$ and/or from the "high energy" part of…

High Energy Physics - Phenomenology · Physics 2010-09-20 E. Molinaro , S. T. Petcov

Neutrino Physics is a mature branch of science with all the three neutrino mixing angles and two mass squared differences determined with high precision. Inspite of several experimental verifications of neutrino oscillations and precise…

High Energy Physics - Phenomenology · Physics 2018-06-28 Gayatri Ghosh , Kalpana Bora

We study the model with three right-handed neutrinos which masses are smaller than the weak scale ${\cal O}(10^2)$ GeV (called as the $\nu$MSM). The model can explain the origin of neutrino masses by the seesaw mechanism, offer a candidate…

High Energy Physics - Phenomenology · Physics 2015-06-02 Takehiko Asaka , Shintaro Eijima , Kazuhiro Takeda

We investigate baryogenesis via leptogenesis and generation of neutrino masses and mixings through the Type I plus Type III seesaw plus an one-loop mechanism in the context of Renormalizable Adjoint SU(5) theory. One light neutrino remains…

High Energy Physics - Phenomenology · Physics 2011-07-26 Kristjan Kannike , Dmitry Zhuridov

We consider leptogenesis in a left-right-symmetric seesaw scenario in which neutrino mass generation and leptogenesis are dominated by the type-II seesaw term. Motivated by grand unification, we assume that the neutrino Dirac mass matrix is…

High Energy Physics - Phenomenology · Physics 2021-09-29 Thomas Rink , Werner Rodejohann , Kai Schmitz

We revisit minimal non-supersymmetric models of SU(5) Grand Unification with the type II seesaw mechanism as the origin of neutrino masses. Imposing the requirement of gauge coupling unification and the proton lifetime bounds, we perform a…

High Energy Physics - Phenomenology · Physics 2022-12-02 Lorenzo Calibbi , Xiyuan Gao

We study the possibility of generating the observed baryon asymmetry via leptogenesis in the decay of heavy Standard Model singlet fermions which carry lepton number, in a framework without Majorana masses above the electroweak scale. Such…

High Energy Physics - Phenomenology · Physics 2009-12-14 M. C. Gonzalez-Garcia , J. Racker , N. Rius

The tiny neutrino masses measured in the neutrino oscillation experiments can be naturally explained by the supersymmetric see-saw mechanism. If the supersymmetry breaking is mediated by gravity, the see-saw models may predict observable…

High Energy Physics - Phenomenology · Physics 2009-11-07 Xiao-Jun Bi , Yuan-Ben Dai

In this work we study a predictive model based on a partially unified theory possessing the gauge symmetry of the Pati-Salam group, $SU(2)_L\times SU(2)_R\times SU(4)_C$ supplemented by a global Peccei-Quinn symmetry, $U(1)_{PQ}$. A…

High Energy Physics - Phenomenology · Physics 2019-05-14 Shaikh Saad

We propose two models based on the $SU(3)_C \times SU(3)_L \times U(1)_X$ gauge symmetry, each incorporating distinct inverse seesaw mechanisms for generating neutrino masses at the radiative level. Therefore, neutrino masses are suppressed…

High Energy Physics - Phenomenology · Physics 2024-10-30 V. H. Binh , Cesar Bonilla , A. E. Cárcamo Hernández , D. T. Huong , Vishnudath K. N. , H. N. Long , P. N. Thu , Iván Schmidt

We study a $\mu - \tau$ reflection symmetry in neutrino sector realized at the GUT scale in the context of the seesaw model. In our scenario, the exact $\mu - \tau$ reflection symmetry realized in the basis where the charged lepton and…

High Energy Physics - Phenomenology · Physics 2015-05-13 Y. H. Ahn , Sin Kyu Kang , C. S. Kim , T. Phong Nguyen

Leptogenesis is a class of scenarios where the baryon asymmetry of the Universe is produced from a lepton asymmetry generated in the decays of a heavy sterile neutrino. We explain the motivation for leptogenesis. We review the basic…

High Energy Physics - Phenomenology · Physics 2008-11-26 Sacha Davidson , Enrico Nardi , Yosef Nir

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

Thermal leptogenesis, that can be viewed as a consequence of the seesaw model, is a very natural mechanism to explain the matter anti-matter asymmetry of the Universe. Recently, lepton flavours have been included in the Boltzmann equations,…

High Energy Physics - Phenomenology · Physics 2007-10-11 F. X. Josse-Michaux

We calculate the baryonic asymmetry of the universe in the baryogenesis-via-leptogenesis framework, assuming first a quark-lepton symmetry and then a charged-neutral lepton symmetry. We match the results with the experimentally favoured…

High Energy Physics - Phenomenology · Physics 2009-10-31 D. Falcone , F. Tramontano

We study a set of textures giving rise to correct masses and mixings of the charged fermions in the context of leptogenesis. The Dirac neutrino texture pattern is assumed to be identical with the up quark texture. The heavy Majonana…

High Energy Physics - Phenomenology · Physics 2011-07-19 Micheal S. Berger , Biswajoy Brahmachari

We propose a new mechanism of baryogenesis which proceeds via a CP-violating phase transition. During this phase transition, the coupling of the Weinberg operator is dynamically realised and subsequently a lepton asymmetry is generated via…

High Energy Physics - Phenomenology · Physics 2017-04-28 Silvia Pascoli , Jessica Turner , Ye-Ling Zhou
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