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Related papers: Mirror Dirac leptogenesis

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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 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 present a purely linear seesaw mechanism in a left-right symmetric framework and then realize a novel leptogenesis scenario for parametrizing the cosmic baryon asymmetty by the charged lepton masses and the light Majorana neutrino mass…

High Energy Physics - Phenomenology · Physics 2020-06-24 Pei-Hong Gu

We consider the Affleck-Dine mechanism for leptogenesis in the minimal MSSM with Dirac or Pseudo-Dirac neutrinos. The rolling of scalars along D-flat directions generates a left-right asymmetry in the sneutrino sector, only the left part of…

High Energy Physics - Phenomenology · Physics 2009-11-11 Steven Abel , Veronique Page

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 compute and compare the baryon asymmetry of the universe in thermal leptogenesis scenario with and without flavour effects for different neutrino mass models namely degenerate, inverted hierarchical and normal hierarchical models, with…

High Energy Physics - Phenomenology · Physics 2009-11-13 H. Zeen Devi , Amal Kr Sarma , N. Nimai Singh

Thermal leptogenesis, in the seesaw model, is a popular mechanism for generating the Baryon Asymmetry of the Universe. It was noticed recently, that including lepton flavour can modify significantly the results. These proceedings aim to…

High Energy Physics - Phenomenology · Physics 2007-05-23 Sacha Davidson

We present a model of leptogenesis that preserves lepton number. The model maintains the important feature of more traditional leptogenesis scenarios: the decaying particles that provide the CP violation necessary for baryogenesis also…

High Energy Physics - Phenomenology · Physics 2009-09-29 Hitoshi Murayama , Aaron Pierce

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

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

We study leptogenesis in two seesaw models where maximal atmospheric neutrino mixing and $U_{e3} = 0$ result from symmetries. Salient features of those models are the existence of three Higgs doublets and a twofold degeneracy of the…

High Energy Physics - Phenomenology · Physics 2009-11-10 W. Grimus , L. Lavoura

Dirac neutrinos with lepton-number-violating interactions can give rise to a new leptogenesis mechanism. In its simplest renormalizable realization, based on a gauged B-L symmetry spontaneously broken by four units, the decay of a new…

High Energy Physics - Phenomenology · Physics 2013-10-10 Julian Heeck

Baryogenesis via leptogenesis is investigated in a specific model of light neutrino masses and mixing angles. The latter was proposed on the basis of an assumed complex-extended scaling property of the neutrino Majorana mass matrix $M_\nu$,…

High Energy Physics - Phenomenology · Physics 2017-03-22 Rome Samanta , Mainak Chakraborty , Probir Roy , Ambar Ghosal

Left-right symmetric models which employ a generalized seesaw mechanism to generate quark and charged lepton masses are known to solve the strong CP problem via parity symmetry, without the need for the axion. These models lead to naturally…

High Energy Physics - Phenomenology · Physics 2025-07-23 K. S. Babu , Ajay Kaladharan

We present here a novel and testable mechanism for leptogenesis, which is characterized by a purely thermal generation of lepton asymmetry via scalar decay. Guided by the thermal mass matrix diagonalization in the finite-temperature regime,…

High Energy Physics - Phenomenology · Physics 2022-01-05 Shao-Ping Li , Xin-Qiang Li , Xin-Shuai Yan , Ya-Dong Yang

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

We analyze lepton asymmetry induced in the decay of right--handed neutrinos in a class of minimal left--right symmetric models. In these models, which assume low energy supersymmetry, the Dirac neutrino mass matrix is proportional to the…

High Energy Physics - Phenomenology · Physics 2015-06-25 K. S. Babu , A. Bachri , H. Aissaoui

The conventional seesaw-leptogenesis can simultaneously explain the suppression of neutrino masses and the generation of cosmic baryon asymmetry, but usually cannot predict an unambiguous relation between these two sectors. In this work we…

High Energy Physics - Phenomenology · Physics 2016-10-12 Pei-Hong Gu , Xiao-Gang He

Dirac leptogenesis (or Dirac neutrinogenesis), in which neutrinos are purely Dirac particles, is an interesting alternative to the standard leptogenesis scenario. In its supersymmetric version, the modified form of the superpotential…

High Energy Physics - Phenomenology · Physics 2008-11-26 Brooks Thomas , Manuel Toharia

We study a model for leptogenesis in which the total CP asymmetries in the decays and scatterings involving the SU(2) singlet seesaw neutrinos $N_\alpha$ vanish ($\epsilon_{N_\alpha}=0$). Leptogenesis is possible due to non-vanishing CP…

High Energy Physics - Phenomenology · Physics 2014-11-18 D. Aristizabal Sierra , Luis Alfredo Muñoz , Enrico Nardi
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