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We investigate the resonant leptogenesis scenario in the minimally $U(1)_{B-L}$ extended standard model with minimal flavor violation. In our model, the $U(1)_{B-L}$ gauge symmetry is broken at the TeV scale and standard model singlet…

High Energy Physics - Phenomenology · Physics 2015-06-05 Nobuchika Okada , Yuta Orikasa , Toshifumi Yamada

Nontrivial topological vacua of non-Abelian gauge symmetry $SU(3)\times SU(2)_{L}$ of the Standard Model play an important role in baryogenesis. In particular, the baryon (and lepton) number violation from $SU(2)_{L}$ sphaleron is a crucial…

High Energy Physics - Phenomenology · Physics 2024-01-19 Chee Sheng Fong

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

We propose a novel mechanism for generating the baryon asymmetry of the Universe through leptogenesis in a scenario where the right-handed neutrinos are heavier than the maximal temperature of the Universe, and are never produced on-shell…

High Energy Physics - Phenomenology · Physics 2026-05-26 Simon Cléry , Alejandro Ibarra , Onur Yonar

The inclusion of two triplet scalars in the Standard Model (SM) enables to accommodate neutrino mass generation as well as baryogenesis through leptogenesis. One of the essential ingredients of leptogenesis is the violation of charge…

High Energy Physics - Phenomenology · Physics 2024-07-17 Sreerupa Chongdar , Sasmita Mishra

Low scale leptogenesis scenarios are difficult to verify due to our inability to relate the parameters involved in the early universe processes with the low energy or collider observables. Here we show that one can in principle relate the…

High Energy Physics - Phenomenology · Physics 2021-07-28 Piyali Banerjee , Urjit Yajnik

It has been recently shown that the quantum Boltzmann equations may be relevant for the leptogenesis scenario. In particular, they lead to a time-dependent CP asymmetry which depends upon the previous dynamics of the system. This memory…

High Energy Physics - Phenomenology · Physics 2008-11-26 Andrea De Simone , Antonio Riotto

We study the supersymmetric leptogenesis via $LH_{u}$ flat direction with a gauged $U(1)_{B-L}$ symmetry. We find that the resultant baryon asymmetry is enhanced compared with the case without a gauged $U(1)_{B-L}$ symmetry. The baryon…

High Energy Physics - Phenomenology · Physics 2009-11-07 Masaaki Fujii , K. Hamaguchi , T. Yanagida

We investigate the generation of the baryon asymmetry of the Universe within a SUSY SU(5) x T' model of flavour, which gives rise to realistic masses and mixing patterns for quarks and leptons. The model employs the see-saw mechanism for…

High Energy Physics - Phenomenology · Physics 2012-03-21 A. Meroni , E. Molinaro , S. T. Petcov

We study the consequence of the neutrino mass anarchy on cosmology, in particular the total mass of neutrinos and baryon asymmetry through leptogenesis. We require independence of measure in each mass matrix elements in addition to the…

High Energy Physics - Phenomenology · Physics 2015-01-06 Xiaochuan Lu , Hitoshi Murayama

In thermal leptogenesis, the cosmic matter-antimatter asymmetry is produced by CP violation in the decays N --> l + \Phi of heavy right-handed Majorana neutrinos N into ordinary leptons l and Higgs particles \Phi. If some charged-lepton…

High Energy Physics - Phenomenology · Physics 2010-10-27 S. Blanchet , P. Di Bari , G. G. Raffelt

Leptogenesis is a class of scenarios in which the cosmic baryon asymmetry originates from an initial lepton asymmetry generated in the decays of heavy sterile neutrinos in the early Universe. We explain why leptogenesis is an appealing…

High Energy Physics - Phenomenology · Physics 2013-01-16 Chee Sheng Fong , Enrico Nardi , Antonio Riotto

The possibility to explain the CMB measurement of the baryon asymmetry with leptogenesis results in a stringent bound on the neutrino masses such that [(m_1)^2+(m_2)^2+(m_3)^2]^(1/2) < 0.30 eV. We discuss the implications of such a bound…

High Energy Physics - Phenomenology · Physics 2009-11-07 P. Di Bari

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

We propose a new electroweak baryogenesis scenario in high-scale supersymmetric (SUSY) models. We consider a singlet extension of the minimal SUSY standard model introducing additional vector-like multiplets. We show that the strongly…

High Energy Physics - Phenomenology · Physics 2015-03-05 Kazuya Ishikawa , Teppei Kitahara , Masahiro Takimoto

Up until now the works regarding leptogenesis have discussed different mechanisms to explain the observed baryon asymmetry of the universe (BAU). The type-$II$ seesaw mechanism employing triplet scalars has been well studied in this context…

High Energy Physics - Phenomenology · Physics 2025-04-22 Rituparna Ghosh , Biswarup Mukhopadhyaya , Utpal Sarkar

Using the closed-time-path formalism we quantify gradient corrections to the kinetic equations for leptogenesis, that are neglected in the standard Boltzmann approach. In particular we show that an additional CP-violating source term…

High Energy Physics - Phenomenology · Physics 2010-06-01 M. Garny , A. Hohenegger , A. Kartavtsev

We argue that \Delta L=2 neutrino spin flavor precession, induced by the primordial magnetic fields, could have a significant impact on the leptogenesis process that accounts for the baryon asymmetry of the universe. Although the extra…

High Energy Physics - Phenomenology · Physics 2015-06-05 Juan Barranco , Roberto Cota , David Delepine , Shaaban Khalil

Assuming only a hierarchical structure of the heavy Majorana neutrino masses and of the neutrino Dirac mass matrix m_D of the see-saw mechanism, we find that in order to produce the observed baryon asymmetry of the Universe via…

High Energy Physics - Phenomenology · Physics 2009-11-10 S. Pascoli , S. T. Petcov , W. Rodejohann

Scalar fields can play a dominant role in the dynamics of the Universe until shortly before nucleosynthesis. Examples are provided by domination by a kinetic mode of a scalar field, which may be both the inflaton and the late time…

High Energy Physics - Phenomenology · Physics 2009-10-31 M. Joyce , T. Prokopec