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Related papers: Leptogenesis with Linear, Inverse or Double Seesaw

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In this work, we introduce the minimal set of leptoquarks into the 3-3-1 model with right-handed neutrinos, capable of generating radiative masses for active neutrinos. As a main consequence, the standard neutrinos acquire small Majorana…

High Energy Physics - Phenomenology · Physics 2024-12-23 A. Doff , João Paulo Pinheiro , C. A. de S. Pires

We investigate the scenario of resonant thermal leptogenesis, in which the leptonic asymmetries are generated through renormalization group corrections induced at the leptogenesis scale. In the framework of the standard model extended by…

High Energy Physics - Phenomenology · Physics 2009-11-11 G. C. Branco , R. Gonzalez Felipe , F. R. Joaquim , B. M. Nobre

We discuss the relation between leptogenesis and the MNS phases in the class of see-saw models called light sequential dominance in which the right-handed neutrinos dominate sequentially, with the dominant right-handed neutrino being the…

High Energy Physics - Phenomenology · Physics 2009-11-07 S. F. King

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

If neutrino masses are realized through the see-saw mechanism, can the right-handed neutrinos be produced and detected at present and future colliders? The answer is negative in the most popular see-saw scenarios for the simple reason that…

High Energy Physics - Phenomenology · Physics 2008-11-26 P. Q. Hung

The seesaw mechanism with three heavy Majorana right-handed neutrinos provides an elegant explanation for neutrino masses and, combined with leptogenesis, can generate the baryon asymmetry of the universe (BAU). Naturally embedded in a…

High Energy Physics - Phenomenology · Physics 2025-05-06 Juan Herrero-Garcia , Giacomo Landini , Tsutomu T. Yanagida

We consider a phenomenologically viable SO(10) grand unification model which allows perturbative calculations up to the Planck scale or the string scale. We use a set of Higgs superfields {10 + 16bar + 16 + 45}. In this framework, the data…

High Energy Physics - Phenomenology · Physics 2008-11-26 Tatsuru Kikuchi

We analyze the left-right symmetric type I+II seesaw mechanism, where an eight-fold degeneracy among the mass matrices of heavy right-handed neutrinos M_R is known to exist. Using the stability property of the solutions and their ability to…

High Energy Physics - Phenomenology · Physics 2010-10-27 E. K. Akhmedov , M. Blennow , T. Hallgren , T. Konstandin , T. Ohlsson

We investigate a resonant leptogenesis scenario by quasi-degenerate right-handed neutrinos which have TeV-scale masses. Especially, we consider the case when two right-handed neutrinos are responsible to leptogenesis and the seesaw…

High Energy Physics - Phenomenology · Physics 2019-09-25 Takehiko Asaka , Takahiro Yoshida

We study the thermal leptogenesis in the scenario where the standard model is extended to include one $SU(2)_{L}$ triplet Higgs boson, in addition to three generations of the right-handed neutrinos. And in the model we introduce the…

High Energy Physics - Phenomenology · Physics 2009-11-10 Peihong Gu , Xiao-Jun Bi

It is well-known that thermal leptogenesis through the decays of the lightest right-handed neutrinos encounters serious difficulties when SO(10)-inspired mass conditions are imposed on the Dirac neutrino mass matrix and light neutrino…

High Energy Physics - Phenomenology · Physics 2009-02-02 Pasquale Di Bari , Antonio Riotto

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

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

The seesaw mechanism of neutrino mass generation is analysed under the following assumptions: (1) minimal seesaw with no Higgs triplets, (2) hierarchical Dirac masses of neutrinos, (3) large lepton mixing primarily or solely due to the…

High Energy Physics - Phenomenology · Physics 2008-11-26 E. Kh. Akhmedov

We consider an $SU(3)_c \otimes SU(2)_L \otimes SU(2)_R \otimes U(1)_{B-L}$ left-right symmetric model with three Higgs scalars including an $SU(2)_L$ doublet, an $SU(2)_R$ doublet and an $SU(2)_L \otimes SU(2)_R$ bidoublet. In addition to…

High Energy Physics - Phenomenology · Physics 2015-05-30 Pei-Hong Gu

We extend some two Higgs doublet models, where the Yukawa couplings for the charged fermion mass generation only involve one Higgs doublet, by two singlet scalars respectively carrying a singly electric charge and a doubly electric charge.…

High Energy Physics - Phenomenology · Physics 2017-01-04 Zhen Liu , Pei-Hong Gu

Leptogenesis may be induced by the mixing of extra Higgs doublets with experimentally accessible masses. This mechanism relies on diagrammatic cuts that are kinematically forbidden in the vacuum but contribute at finite temperature. A…

High Energy Physics - Phenomenology · Physics 2012-06-26 Bjorn Garbrecht

Resonant heavy-neutrino mixing and sterile neutrino oscillations are two prominent mechanisms to realize low-scale leptogenesis, with singlet neutrino masses below TeV energies that could be probed in current and future laboratory…

High Energy Physics - Phenomenology · Physics 2026-04-09 Shao-Ping Li , Apostolos Pilaftsis

Extending the Standard Model with right-handed neutrinos provides a minimal explanation for both light neutrino masses (through the type-I seesaw mechanism) and the baryon asymmetry of our universe (through leptogenesis). We map here for…

High Energy Physics - Phenomenology · Physics 2023-05-12 Yannis Georis

In type I seesaw models with flavor symmetries accounting for the lepton mixing angles the CP asymmetry in right-handed neutrino decays vanishes in the limit in which the mixing pattern is exact. We study the implications that additional…

High Energy Physics - Phenomenology · Physics 2015-06-03 D. Aristizabal Sierra , F. Bazzocchi , I. de Medeiros Varzielas
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