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Related papers: Leptogenesis without CP Violation at Low Energies

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We consider a minimal extension of the Standard Model with one singlet neutrino per generation that can realize resonant leptogenesis at the electroweak scale. In particular, the baryon asymmetry in the Universe can be created by resonant…

High Energy Physics - Phenomenology · Physics 2009-11-10 Apostolos Pilaftsis

A predictive Leptogenesis scenario is presented based on the Minimal Lepton Flavour Violation symmetry. In the realisation with three right-handed neutrinos transforming under the same flavour symmetry of the lepton electroweak doublets,…

High Energy Physics - Phenomenology · Physics 2018-08-01 L. Merlo , S. Rosauro-Alcaraz

We analyze leptogenesis in the context of seesaw models with almost conserved lepton number, focusing on the L-conserving contribution to the flavoured CP asymmetries. We find that, contrary to previous claims, successful leptogenesis is…

High Energy Physics - Phenomenology · Physics 2015-06-05 J. Racker , Manuel Peña , Nuria Rius

In SO(10) models with a vectorial fourth generation of down quarks and leptons, the structure of the neutrino Majorana and Dirac mass matrices generically coincide with those of up- and down-quarks, respectively. Then the small neutrino…

High Energy Physics - Phenomenology · Physics 2007-10-12 Sören Wiesenfeldt

Some models of leptogenesis involve a quasi-degenerate pair of heavy neutrinos $N_{1,2}$ whose masses can be small, $O({\rm GeV})$. Such neutrinos can contribute to the rare lepton-number-violating (LNV) decay $W^\pm \to \ell_1^\pm…

High Energy Physics - Phenomenology · Physics 2021-04-23 Fatemeh Najafi , Jacky Kumar , David London

We discuss neutrino masses and mixing in the context of seesaw type I models with three right-handed Majorana neutrinos and an approximately diagonal Dirac sector. This ansatz is motivated by the idea that the flavor structure in the…

High Energy Physics - Phenomenology · Physics 2014-06-25 Heinrich Päs , Erik Schumacher

In extensions of the Standard Model by Majorana fermions, the presence of additional CP violating phases has been shown to play a crucial role in lepton number violating processes. In this work we show that (Dirac and Majorana) CP violating…

High Energy Physics - Phenomenology · Physics 2021-12-20 A. Abada , J. Kriewald , A. M. Teixeira

We examine the compatibility between the Neutrino Option, in which the electroweak scale is generated by PeV mass type I seesaw Majorana neutrinos, and leptogenesis. We find the Neutrino Option is consistent with resonant leptogenesis.…

High Energy Physics - Phenomenology · Physics 2019-11-11 I. Brivio , K. Moffat , S. Pascoli , S. T. Petcov , J. Turner

Generation of the neutrino masses and leptogenesis (LG) in the Standard Model extended by the heavy Majorana fermions is considered. Classification of LG scenarios according to the new fermion mass spectra is given, where singlet-triplet LG…

High Energy Physics - Phenomenology · Physics 2013-08-13 Dmitry V. Zhuridov

Several beyond the Standard Model scenarios introduce new heavy neutrinos, whose Dirac or Majorana nature could be tested by comparing the rates of lepton number violating and lepton number conserving processes: a Dirac fermion induces only…

High Energy Physics - Phenomenology · Physics 2019-09-27 X. Marcano , A. Abada , C. Hati , A. M. Teixeira

If the baryon asymmetry of the Universe is produced by leptogenesis, CP violation is required in the lepton sector. In the seesaw extension of the Standard Model with three hierarchical right-handed neutrinos, we show that the baryon…

High Energy Physics - Phenomenology · Physics 2008-11-26 Sacha Davidson , Julia Garayoa , Federica Palorini , Nuria Rius

We study variations of the standard leptogenesis scenario that can arise if an additional mass scale related to the breaking of some new symmetry (as for example a flavor or the B-L symmetry) is present below the mass $M_{N_1}$ of the…

High Energy Physics - Phenomenology · Physics 2009-09-29 Diego Aristizabal Sierra , Marta Losada , Enrico Nardi

From the new existing data with not vanishing theta13 mixing angle we determine the possible shape of the Majorana neutrino mass matrix. We assume that CP symmetry is broken and all Dirac and Majorana phases are taken into account. Two…

High Energy Physics - Phenomenology · Physics 2012-04-18 Bartosz Dziewit , Sebastian Zajac , Marek Zralek

We propose a new scenario for baryogenesis through leptogenesis, where the CP phase relevant for leptogenesis is connected directly to the PMNS phase(s) in the light neutrino mixing matrix. The scenario is realized in case only one CP phase…

High Energy Physics - Phenomenology · Physics 2016-09-14 Laura Covi , Jihn E. Kim , Bumseok Kyae , Soonkeon Nam

We investigate the possibility that baryogenesis occurs during the weak phase transition in a minimal extension of the Standard Model which contains extra neutral leptons and conserves total lepton number. The necessary CP-violating phases…

High Energy Physics - Phenomenology · Physics 2009-10-30 P. Hernandez , N. Rius

We review the basic mechanisms of neutrino mass generation and the corresponding structure of the lepton mixing matrix. We summarize the status of three-neutrino oscillation parameters as determined from current observations, using…

High Energy Physics - Phenomenology · Physics 2009-11-13 Hiroshi Nunokawa , Stephen Parke , Jose W. F. Valle

We present a low-scale type-I seesaw scenario with discrete flavor and CP symmetries. This scenario not only explains the measured values of the lepton mixing angles, but also makes predictions for leptonic CP violation, and connects the…

High Energy Physics - Phenomenology · Physics 2023-01-03 Garv Chauhan , P. S. Bhupal Dev

We estimate the effect of leptonic CP violating phases in the minimal seesaw model with two heavy neutrinos $N$ by imposing the approximately $\mu-\tau$ symmetry on the model. For $N$ subject to the $\mu-\tau$ symmetry, we find that…

High Energy Physics - Phenomenology · Physics 2008-07-01 Teppei Baba

Flavor effects due to lepton interactions in the early Universe may have played an important role in the generation of the cosmological baryon asymmetry through leptogenesis. If the only source of high-energy CP violation comes from the…

High Energy Physics - Phenomenology · Physics 2008-11-26 G. C. Branco , R. Gonzalez Felipe , F. R. Joaquim

Once a light axionlike scalar field couples to the electroweak gauge bosons, its classical motion during reheating induces an effective chemical potential for the fermion number. In the presence of rapid lepton number (L)-violating…

High Energy Physics - Phenomenology · Physics 2015-07-08 Alexander Kusenko , Kai Schmitz , Tsutomu T. Yanagida
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