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The observed neutrino oscillations and baryon asymmetry, unexplained by the Standard Model (SM), can both be accounted for by extending the SM to include Majorana right-handed neutrinos (RHNs). Tiny neutrino masses naturally arise through…

High Energy Physics - Phenomenology · Physics 2025-06-26 Nobuchika Okada , Digesh Raut

We study leptogenesis in three different realisations of the type Ib seesaw mechanism, where the effective masses of the neutrinos are obtained by the spontaneous symmetry breaking of two different Higgs doublets. In the minimal type Ib…

High Energy Physics - Phenomenology · Physics 2022-04-05 Bowen Fu , Stephen F. King

Knowledge of the mechanism of neutrino mass generation would help understand a lot more about Lepton Number Violation (LNV), the cosmological evolution of the Universe, or the evolu tion of astronomical objects. Here we propose a verifiable…

High Energy Physics - Phenomenology · Physics 2020-03-18 Claudio Dib , Sergey Kovalenko , Ivan Schmidt , Adam Smetana

We describe a "neutrinogenesis" mechanism whereby, in the presence of right-handed neutrinos with sufficiently small pure Dirac masses, (B+L)-violating sphaleron processes create the baryon asymmetry of the Universe, even when B=L=0…

High Energy Physics - Phenomenology · Physics 2009-09-25 Karin Dick , Manfred Lindner , Michael Ratz , David Wright

We studied models of leptogenesis where three right-handed Majorana neutrinos are involved and the minimal-extended seesaw mechanism including an additional singlet field produces four light neutrinos. This study shows that the type of mass…

High Energy Physics - Phenomenology · Physics 2022-12-28 Ki-Young Jung , Kim Siyeon

A non-supersymmetric inverse seesaw model of neutrino mass based on the $A^{\prime}_5$ modular symmetry is presented. This framework provides a combined explanation for neutrino masses, mixing, and the cosmic baryon asymmetry through…

High Energy Physics - Phenomenology · Physics 2026-03-20 Xianshuo Zhang , Yakefu Reyimuaji

We propose a unified explanation for the origin of dark matter and baryon number asymmetry on the basis of a non-supersymmetric model for neutrino masses. Neutrino masses are generated in two distinct ways, that is, a tree-level seesaw…

High Energy Physics - Phenomenology · Physics 2008-11-26 Daijiro Suematsu

We bring the theoretical issue of whether two important cosmological demands, baryon asymmetry and degenerate neutrinos as hot dark matter, can be compatible in the context of the seesaw mechanism. To realize leptogenesis with almost…

High Energy Physics - Phenomenology · Physics 2009-10-31 Eung Jin Chun , Sin Kyu Kang

We study the possibility of connecting leptonic Dirac CP phase $\delta$, lightest neutrino mass and baryon asymmetry of the Universe within the framework of a model where both type I and type II seesaw mechanisms contribute to neutrino…

High Energy Physics - Phenomenology · Physics 2015-06-23 Rupam Kalita , Debasish Borah

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

Numerous recent evidences for neutrino masses have established the leptogenesis mechanism as a very natural possible explanation for the baryon asymmetry of the Universe. The explicit realization of this mechanism depends on the neutrino…

High Energy Physics - Phenomenology · Physics 2015-06-12 Thomas Hambye

We present a novel approach for implementing baryogenesis via leptogenesis at low scale within neutrino seesaw framework where a sufficient lepton asymmetry can be generated via out of equilibrium CP-violating decays of right handed…

High Energy Physics - Phenomenology · Physics 2026-04-14 Dipendu Bhandari , Arunansu Sil

We study the implications for leptogenesis in a class of left-right symmetric model, where all fermion masses are induced through the Universal Seesaw mechanism. Unlike conventional analyses, we do not use the decays of the neutrino…

High Energy Physics - Phenomenology · Physics 2025-12-24 K. S. Babu , Maximilian Berbig , Srubabati Goswami , Drona Vatsyayan

We propose a new nonthermal leptogenesis mechanism triggered by the cosmic first-order phase transition. The Standard Model is extended with two generations of TeV-scale vectorlike leptons. The lighter generation gives rise to an inverse…

High Energy Physics - Phenomenology · Physics 2026-02-26 Wen-Yuan Ai , Peisi Huang , Ke-Pan Xie

We introduce a novel hybrid framework combining type I and type II seesaw models for neutrino mass where a complex vacuum expectation value of a singlet scalar field breaks CP spontaneously. Using pragmatic organizing symmetries we…

High Energy Physics - Phenomenology · Physics 2023-06-21 Rohan Pramanick , Tirtha Sankar Ray , Avirup Shaw

We consider a variant of seesaw mechanism by introducing extra singlet neutrinos, with which we show how the low scale leptogenesis is realized without imposing the tiny mass splitting between two heavy Majorana neutrinos required in the…

High Energy Physics - Phenomenology · Physics 2008-11-26 Sin Kyu Kang , C. S. Kim

We consider leptogenesis induced by soft supersymmetry breaking terms ("soft leptogenesis"), in the context of the inverse seesaw mechanism. In this model there are lepton number (L) conserving and L-violating soft supersymmetry-breaking…

High Energy Physics - Phenomenology · Physics 2010-10-27 J. Garayoa , M. C. Gonzalez-Garcia , N. Rius

In the framework of seesaw models with only two heavy Majorana neutrinos, nonzero leptonic asymmetries can be radiatively generated when exact heavy neutrino mass degeneracy ($M_1=M_2=M$) is imposed at a scale $\Lambda_D > M$. For a…

High Energy Physics - Phenomenology · Physics 2009-11-11 F. R. Joaquim

We propose an alternative mechanism for leptogenesis at the electroweak scale, through the decays of a left-handed sneutrino. This scenario may be realized in supersymmetric models with non-zero Majorana masses for the neutrino superfield…

High Energy Physics - Phenomenology · Physics 2007-05-23 John Ellis , Sin Kyu Kang

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