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Related papers: Seesaw and leptogenesis: a triangular ansatz

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The presence of domain walls separating regions of unbroken $SU(2)_L$ and $SU(2)_R$ is shown to provide necessary conditions for leptogenesis which converts later to the observed Baryon aymmetry. The strength of lepton number violation is…

High Energy Physics - Phenomenology · Physics 2008-11-26 U. A. Yajnik , J. Cline , M. Rabikumar

Leptogenesis is an appealing framework to account for the baryon asymmetry in the universe. To this end physics beyond the Standard Model is demanded. In this paper we investigate the possibility to attain successful leptogenesis with…

High Energy Physics - Phenomenology · Physics 2017-10-02 Simone Biondini , Orlando Panella

We show that the U(1)-prime models linked with the seesaw mechanism at TeV scale can lead to a successful baryogenesis through soft leptogenesis with a resonant behavior in the B parameter. Such a consideration constrains the Z-prime mass…

High Energy Physics - Phenomenology · Physics 2013-05-29 Eung Jin Chun

We give a general analysis of neutrino mixing in the seesaw mechanism with three flavors. Assuming that the Dirac and u-quark mass matrices are similar, we establish simple relations between the neutrino parameters and individual Majorana…

High Energy Physics - Phenomenology · Physics 2009-12-30 T. K. Kuo , Guo-Hong Wu , Sadek W. Mansour

Dirac leptogenesis, in which neutrinos are purely Dirac and develop small but nonzero effective masses without the aid of the see-saw mechanism, provides an interesting alternative to the standard leptogenesis picture. Here we review the…

High Energy Physics - Phenomenology · Physics 2007-12-27 Brooks Thomas

Understanding the disparate mixing patterns between quarks and leptons is one of the major challenges in particle theory today. I discuss some of the ways to understand this difference within the seesaw framework using new symmetries of…

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

We propose a simple ansatz for neutrino phenomenology, in which the relevant lepton mass matrices take the universal Fritzsch-like form and the seesaw relation holds under a particular condition. There exist six textures of this nature, but…

High Energy Physics - Phenomenology · Physics 2009-11-10 Zhi-zhong Xing , Shun Zhou

The possible extension of generation structure is investigated on the basis of a composite model, in which leptons and quarks are composed of rishons $T$ with charge 1/3 and purely neutral $V$. In this sub-system, we regard $V$ as the…

High Energy Physics - Phenomenology · Physics 2009-11-07 K. Koike

In this talk we show how a natural neutrino mass hierarchy can follow from the type I see-saw mechanism, and a natural neutrino mass degeneracy from the type II see-saw mechanism, where the bi-large mixing angles can arise from either the…

High Energy Physics - Phenomenology · Physics 2009-11-10 S. F. King

We propose a baryo- and leptogenesis mechanism in which the B-L asymmetry is produced in the conversion of ordinary leptons into particles of some depleted hidden sector. In particular, we consider the lepton number violating reactions, l…

High Energy Physics - Phenomenology · Physics 2009-09-25 Luis Bento , Zurab Berezhiani

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

Discrete symmetries being preferred to explain the neutrino phenomenology, we chose the simplest $S_3$ group and explore the implication of its modular form on neutrino masses and mixing. Non-trivial transformations of Yukawa couplings…

High Energy Physics - Phenomenology · Physics 2020-08-06 Subhasmita Mishra

We study the possibility of generating non-zero reactor mixing angle $\theta_{13}$ and baryon asymmetry of the Universe within the framework of an $A_4$ flavour symmetric model. Using the conventional type I seesaw mechanism we construct…

High Energy Physics - Phenomenology · Physics 2018-06-13 Debasish Borah , Mrinal Kumar Das , Ananya Mukherjee

The Type II Seesaw Mechanism provides a minimal framework to explain the neutrino masses involving the introduction of a single triplet Higgs to the Standard Model. However, this simple extension was believed to be unable to successfully…

High Energy Physics - Phenomenology · Physics 2022-06-08 Neil D. Barrie , Chengcheng Han , Hitoshi Murayama

In this third part of our EFT-consistent analysis of electromagnetic leptogenesis, we confront the dipole operator that sources the baryon asymmetry with constraints from light-neutrino masses and low-energy observables. Starting from the…

High Energy Physics - Phenomenology · Physics 2025-12-13 Rin Takada

We propose two versions of radiative linear seesaw models, where electrically charged scalars and vector-like leptons generate the Dirac neutrino mass submatrix at one and two loop levels. In these models, the SM charged lepton masses are…

High Energy Physics - Phenomenology · Physics 2024-07-31 A. E. Cárcamo Hernández , Yocelyne Hidalgo Velásquez , Sergey Kovalenko , Nicolás A. Pérez-Julve , Ivan Schmidt

Hybrid leptogenesis framework combining type I and type II seesaw mechanism for neutrino mass necessarily include scattering topologies involving both the scalar triplet and the right handed neutrino. We demonstrate that a systematic…

High Energy Physics - Phenomenology · Physics 2024-06-26 Rohan Pramanick , Tirtha Sankar Ray , Arunansu Sil

In an $SU(3)_{c}\times SU(2)_{L}\times SU(2)_{R}\times U(1)_{B-L}$ left-right symmetric framework, we present a new leptogenesis scenario parametrized by Dirac neutrino mass matrix. Benefited from the parity symmetry motivated to solve the…

High Energy Physics - Phenomenology · Physics 2017-10-25 Pei-Hong Gu

We discuss the various incarnations of a gauged B-L symmetry: 1) unbroken, it features Dirac neutrinos, neutrinogenesis to create the baryon asymmetry of our Universe, and a potentially light Z' boson; 2) broken by two units, we obtain the…

High Energy Physics - Phenomenology · Physics 2015-03-27 Julian Heeck

We perform a thermal unflavored leptogenesis analysis on minimal left-right symmetric models with discrete left-right symmetry identified as generalized parity or charge conjugation. When left-right symmetry is unbroken in the lepton Yukawa…

High Energy Physics - Phenomenology · Physics 2023-02-24 Xinyi Zhang , Jiang-Hao Yu , Bo-Qiang Ma
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