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Observable consequences of partially degenerate leptogenesis

In the context of the seesaw mechanism, it is natural that the large solar and atmospheric neutrino mixing angles originate separately from large 2 by 2 mixings in the neutrino and charged-lepton sectors, respectively, and large mixing in the neutrino couplings is in turn more plausible if two of th...

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Detalles Bibliográficos
Autores principales: Ellis, John R., Raidal, Martti, Yanagida, T.
Lenguaje:eng
Publicado: 2002
Materias:
Acceso en línea:https://dx.doi.org/10.1016/S0370-2693(02)02691-6
http://cds.cern.ch/record/565367
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author Ellis, John R.
Raidal, Martti
Yanagida, T.
author_facet Ellis, John R.
Raidal, Martti
Yanagida, T.
author_sort Ellis, John R.
collection CERN
description In the context of the seesaw mechanism, it is natural that the large solar and atmospheric neutrino mixing angles originate separately from large 2 by 2 mixings in the neutrino and charged-lepton sectors, respectively, and large mixing in the neutrino couplings is in turn more plausible if two of the heavy singlet neutrinos are nearly degenerate. We study the phenomenology of this scenario, calculating leptogenesis by solving numerically the set of coupled Boltzmann equations for out-of-equilibrium heavy singlet neutrino decays in the minimal supersymmetric seesaw model. The near-degenerate neutrinos may weigh < 10^8 GeV, avoiding the cosmological gravitino problem. This scenario predicts that Br(mu to e gamma) should be strongly suppressed, because of the small singlet neutrino masses, whilst Br(tau to mu gamma) may be large enough to be observable in B-factory or LHC experiments. If the light neutrino masses are hierarchical, we predict that the neutrinoless double-beta decay parameter m_{ee} is approximately sqrt{Delta m_{sol}^2} times sin^2 theta_{12}.
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institution Organización Europea para la Investigación Nuclear
language eng
publishDate 2002
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spelling cern-5653672023-03-14T20:18:53Zdoi:10.1016/S0370-2693(02)02691-6http://cds.cern.ch/record/565367engEllis, John R.Raidal, MarttiYanagida, T.Observable consequences of partially degenerate leptogenesisParticle Physics - PhenomenologyIn the context of the seesaw mechanism, it is natural that the large solar and atmospheric neutrino mixing angles originate separately from large 2 by 2 mixings in the neutrino and charged-lepton sectors, respectively, and large mixing in the neutrino couplings is in turn more plausible if two of the heavy singlet neutrinos are nearly degenerate. We study the phenomenology of this scenario, calculating leptogenesis by solving numerically the set of coupled Boltzmann equations for out-of-equilibrium heavy singlet neutrino decays in the minimal supersymmetric seesaw model. The near-degenerate neutrinos may weigh < 10^8 GeV, avoiding the cosmological gravitino problem. This scenario predicts that Br(mu to e gamma) should be strongly suppressed, because of the small singlet neutrino masses, whilst Br(tau to mu gamma) may be large enough to be observable in B-factory or LHC experiments. If the light neutrino masses are hierarchical, we predict that the neutrinoless double-beta decay parameter m_{ee} is approximately sqrt{Delta m_{sol}^2} times sin^2 theta_{12}.In the context of the seesaw mechanism, it is natural that the large solar and atmospheric neutrino mixing angles originate separately from large 2 by 2 mixings in the neutrino and charged-lepton sectors, respectively, and large mixing in the neutrino couplings is in turn more plausible if two of the heavy singlet neutrinos are nearly degenerate. We study the phenomenology of this scenario, calculating leptogenesis by solving numerically the set of coupled Boltzmann equations for out-of-equilibrium heavy singlet neutrino decays in the minimal supersymmetric seesaw model. The near-degenerate neutrinos may weigh < 10^8 GeV, avoiding the cosmological gravitino problem. This scenario predicts that Br(mu to e gamma) should be strongly suppressed, because of the small singlet neutrino masses, whilst Br(tau to mu gamma) may be large enough to be observable in B-factory or LHC experiments. If the light neutrino masses are hierarchical, we predict that the neutrinoless double-beta decay parameter m_{ee} is approximately sqrt{Delta m_{sol}^2} times sin^2 theta_{12}.In the context of the seesaw mechanism, it is natural that the large solar and atmospheric neutrino mixing angles originate separately from large 2×2 mixings in the neutrino and charged-lepton sectors, respectively, and large mixing in the neutrino couplings is in turn more plausible if two of the heavy singlet neutrinos are nearly degenerate. We study the phenomenology of this scenario, calculating leptogenesis by solving numerically the set of coupled Boltzmann equations for out-of-equilibrium heavy singlet neutrino decays in the minimal supersymmetric seesaw model. The near-degenerate neutrinos may weigh ≲10 8  GeV, avoiding the cosmological gravitino problem. This scenario predicts that Br ( μ → eγ ) should be strongly suppressed, because of the small singlet neutrino masses, whilst Br ( τ → μγ ) may be large enough to be observable in B-factory or LHC experiments. If the light neutrino masses are hierarchical, we predict that the neutrinoless double- β decay parameter m ee ≈ Δm sol 2 sin 2 θ 12 .hep-ph/0206300CERN-TH-2002-139CERN-TH-2002-139oai:cds.cern.ch:5653672002-06-28
spellingShingle Particle Physics - Phenomenology
Ellis, John R.
Raidal, Martti
Yanagida, T.
Observable consequences of partially degenerate leptogenesis
title Observable consequences of partially degenerate leptogenesis
title_full Observable consequences of partially degenerate leptogenesis
title_fullStr Observable consequences of partially degenerate leptogenesis
title_full_unstemmed Observable consequences of partially degenerate leptogenesis
title_short Observable consequences of partially degenerate leptogenesis
title_sort observable consequences of partially degenerate leptogenesis
topic Particle Physics - Phenomenology
url https://dx.doi.org/10.1016/S0370-2693(02)02691-6
http://cds.cern.ch/record/565367
work_keys_str_mv AT ellisjohnr observableconsequencesofpartiallydegenerateleptogenesis
AT raidalmartti observableconsequencesofpartiallydegenerateleptogenesis
AT yanagidat observableconsequencesofpartiallydegenerateleptogenesis